2016 • 16–21 October 2016 1 Conference Schedule-At-A-Glance Note: Dates and Times Are Subject to Change

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Table of Contents

Schedule at a Glance ...... 2 Laser Science Symposium on Undergraduate Research . . . . 16 FiO/LS Chairs’ Welcome Letters ...... 3 Symposium on Mesoscopic Optics of Disordered Media . . . 17 A Tribute to Steve Jacobs ...... 17 General Information ...... 5 Symposium on Mid-Infrared Fiber Sources ...... 17 Conference Services ...... 5 Symposium on 100 Years of vision at OSA: Most Cited Papers First Aid and Emergency Information ...... 6 in OSA Journals ...... 18 Sponsoring Society Booths ...... 6 Symposium on Integrated Photonic Manufacturing . . . . . 18 Stay Connected Symposium on Integrated Quantum Optics ...... 18 Conference Materials ...... 9 Special Events ...... 19 FiO/LS Mobile App ...... 9 Exhibition Information ...... 23 Conference Plenary Session and Awards Ceremony FiO/LS Committees ...... 25 Plenary Presentations ...... 11 APS Arthur L. Schawlow Prize and Lecture ...... 12 Explanation of Session Codes ...... 26 Frederic Ives Medal /Jarus W. Quinn Prize Presentation FiO/LS Agenda of Sessions ...... 27 and Lecture ...... 12 FiO/LS Abstracts ...... 36 OSA Awards and Honors FiO/LS Subject Index ...... 132 OSA and APS Awards and Special Recognitions ...... 12 OSA Foundation Student Travel Grants ...... 14 Key to Authors and Presiders ...... 142 OSA Foundation Boris P. Stoicheff Memorial Scholarship . . . 14 OSA Foundation Emil Wolf Outstanding Student Paper Competition ...... 14 OSA and APS thank the following sponsors OSA Foundation Incubic/Milton Chang Travel Grant . . . . . 14 for their generous support of this meeting: OSA Foundation Jean Bennett Memorial Student Travel Grant . 15 OSA Foundation Robert S. Hilbert Memorial Student Travel Grant ...... 15 Carl E. Anderson Award for Outstanding Doctoral Dissertation ...... 15 Special Symposia Symposium on 100 Years of Optical Design, Fabrication, Testing and Instrumentation – A Historical Look Back . . . . . 16 Symposium on 50th Anniversary of Low-Loss Optical Fibers . . 16

Check the Mobile App for regular updates. Program updates and changes through 13 October may be found on the Conference Program Update Sheet distributed in the registration bags.

FiO/LS 2016 • 16–21 October 2016 1 Conference Schedule-at-a-Glance Note: Dates and Times are subject to change. Check the Mobile App for regular updates. All times reflect Eastern time zone. Monday Tuesday Wednesday Thursday Friday 17 October 18 October 19 October 20 October 21 October General & Exhibits Registration 15:00–20:00 07:00 –17:00 07:00–18:00 07:00–17:00 07:30–16:30 WORKinOPTICS.com Kiosk & E-Center 15:00–20:00 07:00 –17:00 07:00–17:00 07:00–17:00 07:30–16:30 Speaker Preparation Room 15:00–18:00 07:00–18:00 07:00–18:00 07:00–18:00 07:30–16:00 Coffee Breaks 10:00–10:30 09:30–10:30 09:30–10:00 10:00–10:30 15:30–16:00 14:30–15:00 16:00–16:30 15:30–16:00 Exhibit Hall Open 09:30–16:00 09:30–14:00 Unopposed Exhibit-only Time 09:30–10:30 09:30–11:00 12:00–13:00 12:30–14:00 14:30–16:00 Glass Art Contest & Auction 09:30–16:00 09:30–14:00 OSA Student Chapter Competition 14:00–16:00 Programming FiO/LS Technical Sessions 08:00–18:00 10:30–18:00 14:00–18:30 08:00–18:00 Laser Science Symposium on Undergraduate Research 12:15–18:00 Joint FiO/LS Plenary & Awards Sessions 08:00–09:30 08:00–09:30 FiO Poster Sessions 14:30–16:00 09:30–11:00 OSA Light the Future Speaker Series featuring Michio Kaku and Nobel Laureates 11:00–12:30 Postdeadline Paper Sessions 10:30–12:30 Special Events Women of Light, a Special Program for Women in Optics hosted by WiSTEE CONNECT 11:00–17:00 Make Optics Career Roundtable 17:00–18:00 Diversity & Inclusion Reception: A Look at the LGBT Climate in Physics 17:00–18:00 FiO/LS Welcome Reception 18:30–20:30 Optics in Digital Systems Technical Group Networking Breakfast 07:30–08:30 OSA Fellow Members Lunch 12:00–13:15 Optical Material Studies Technical Group Special Talk 12:00–13:30 Polarization Technical Group Special Talk 12:00–13:30 OSA Friends and Family Event 13:45–16:00 Meet the OSA Editors’ Reception 15:30–16:30 Photonics Clambake 2016 17:30–20:30 Optics & Energy: Reflections on the Past and Lighting the Future 18:00–19:00 OSA Student Member Party 19:00–22:00 Optics Alumni Networking Reception 19:00–22:00 AIM Photonics Northeast Supply Conference (NESCO) 08:00–17:00 Environmental Sensing Technical Group Special Talk 12:00–13:00 Meet the Editors of the APS Journals Reception 15:30–17:00 OIDA Member and Exhibitor Appreciation Reception 16:00–17:00 OSA Annual Business Meeting 17:00–17:45 DLS Annual Business Meeting 17:00–18:00 OSA 100 Year BASH 18:30–21:30 VIP Industry Leaders Networking Event 12:30–14:00

2 FiO/LS 2016 • 16–21 October 2016 Welcome to Frontiers in Optics 2016

We are pleased that you have chosen to join us to celebrate The Optical Society’s centennial year • Be sure to join us for the OSA 100 Year BASH on Wednesday, 19 October from 18:30–21:30. as we return to the organization’s birthplace, Rochester, New York. The 2016 Frontiers in Optics • The Light the Future Speaker Series featuring a presentation by Michio Kaku will be held on th (FiO) Conference, the 100 Annual meeting of The Optical Society, will encompass the breadth of Thursday, 20 October from 11:00–12:30 optical science and engineering and provide an atmosphere that fosters the exchange of information between those working on fundamental research and those looking for solutions to engineer- • Late-breaking advances in optics will be presented on Friday, 21 October, in the FiO ing problems. On behalf of the FiO Subcommittee Chairs, we would like to thank our colleagues Postdeadline Paper Sessions, running from 10:30–12:30. from the Division of Laser Science (DLS) of the American Physical Society (APS) for assisting in • The OSA Foundation is pleased to announce the 8th annual Emil Wolf Outstanding cultivating joint topics and sessions that will greatly enhance the experience of the attendees at Student Paper Competition. One award winner will be selected from each of the seven FiO FiO 2016. subcommittees. Selections will be made based on the quality of the submitted technical summary and presentation. Winners will be announced at the end of the conference and in The technical program features nearly 900 invited, tutorial, and contributed oral and poster the next issue of Optics & Photonics News (OPN). presentations by celebrated members of the community describing some of the most exciting advances in their fields. Special symposia and other major events further highlight major advances • Wednesday and Thursday, while you are enjoying the poster sessions and the coffee breaks in many selected areas. This year’s program also features two renowned Plenary speakers. Lukas in the Exhibit Hall and/or taking breaks from the presentations, please see the latest in Novotny, ETH Zurich, Switzerland, will give the presentation, “Controlling Light-matter Interac- scientific and optical instrumentation and information that our exhibitors have on display! tions on the Nanometer Scale” during Wednesday’s Plenary session. Michal Lipson, Columbia We welcome you to FiO 2016 and encourage you to take full advantage of the benefits of this University, USA, will discuss “Next Generation Silicon Photonics” at the Thursday Plenary session. year’s social and networking opportunities, technical sessions, corporate programming, poster Our Plenary session programming will also include the award presentations from two individuals sessions and exhibition! receiving two of the highest honors for OSA and APS. Gerard Mourou, University of Michigan, USA, winner of the OSA 2016 Frederic Ives Medal/Jarus W. Quinn Prize, will give an address at the Wednesday Plenary session. Robert W. Boyd, recipient of the APS 2016 Arthur L. Schawlow Prize will present during Thursday’s Plenary session. In addition to these distinguished speakers, OSA will celebrate our 100th Anniversary with a continuation of the Light the Future Speaker series. This event will feature Michio Kaku, Futurist and theoretical Physicist, City College of New York, USA. FiO is pleased to offer several special symposia – The Symposium on 100 Years of Optical Design, Fabrication, Testing and Instrumentation – A Historical Look Back (Tuesday, 18 October, 08:00–14:30); The Symposium on the 50th Anniversary of Low-Loss Optical Fibers (Tuesday, 18 October, 08:00–15:30); The Symposium on Mesoscopic Optics of Disordered Media (Wednesday, Urs Utzinger 19 October, 10:30–14:00); A Tribute to Steve Jacobs (Wednesday, 19 October, 10:30–14:00); The Scott Carney Symposium on Mid-Infrared Fiber Sources (Thursday, 20 October, 14:00–18:30); The Symposium University of Illinois at University of Arizona, USA on 100 Years of Vision at OSA: Most Cited Vision Papers in OSA Journals (Thursday, 20 October, Urbana-Champaign, USA General Chair 14:00–16:00); The Symposium on Integrated Photonic Manufacturing (Friday, 21 October, 08:00– General Chair 14:30); and the Symposium on Integrated Quantum Optics (Friday, 21 October, 14:30–17:30). Details about all the symposia are listed on the Symposia pages of this program. This year’s meeting is filled with many informational and networking events. Some of the highlights of FiO 2016 include the following: • OSA’s Science Educators’ Day will be held on Sunday, 16 October, from 13:30–16:30, in the Grand Ballroom of the Hyatt Regency Rochester. Hosted by The Optical Society, Science Educator’s Day (EDAY) provides middle and high school science teachers with a wide variety of optics-focused lesson plans and classroom demonstration guides. EDAY attendees receive materials that can be used in middle and high school classrooms. • The Conference Welcome Reception will be held on Monday, 17 October, from 18:30–20:30. Tom Brown Chris Dainty Ling Fu • OSA Students will be welcomed at the OSA Student Member Party Tuesday, 18 October University of Rochester, USA University College Wuhan National Lab for from 19:00–22:00 Program Chair London, UK Optoelectronics, China Program Chair Program Chair

FiO/LS 2016 • 16–21 October 2016 3 Welcome to Laser Science 2016

The leadership of the Division of Laser Science (DLS) of the American Physical Soci- Integrated Quantum Photonics; Nonreciprocal and Topological Photonic Devices; ety (APS) is pleased to welcome you to our 32nd annual meeting, Laser Science Nano-Plasmonics for Spectroscopy and Imaging; Advances in X-ray and XUV Laser (LS) 2016, in Rochester, New York. We are grateful for the help of our colleagues Science and Applications; and General Laser Science. The DLS Business meeting and technical program Subcommittee Chairs, David Reis, Robert Alfano, Bo Zhen, will be held Wednesday, 19 October from 17:00–18:00. We welcome you to the Nick Vamivakas, Mohammad Hafezi, Carlos Baiz, Dirk Englund, and Christopher Laser Science 2016 Meeting and encourage you to take full advantage of this year’s Milne, in organizing a broad range of topics in physics, biology and chemistry. This technical and poster sessions, symposia, and plenary lectures, as well as an exhibit year’s program includes many of the areas at the forefront of laser science that are hall showcasing leading suppliers to the laser science community. Enjoy! customarily found at the annual DLS meeting. We have collaborated with our colleagues in The Optical Society to coordinate schedules to encourage your intellec- tual wanderings between DLS and OSA sessions. In addition to an outstanding technical program with over 100 Laser Science presentations, there are many exciting special symposia and events scheduled for the meeting this year. Special attention is appropriate for the Symposium on Under- graduate Research on Tuesday, which showcases the work of some of our youngest scientists. The Symposium will feature a special poster session to present the work of selected undergraduate researchers. The technical sessions for the Laser Sci- ence meeting are organized around several broad themes: High Harmonic Gen- Kevin J. Kubarych Edo Waks eration from Solids to Gases; Multiphoton Effects and High Resolution Imaging; University of Michigan, USA, University of Maryland, USA, Advanced Nano-Photonic Lasers: Science and Application; Quantum Light Souces; Laser Science Co-Chair Laser Science Co-Chair

4 FiO/LS 2016 • 16–21 October 2016 General Information General Information

Conference Services Media Room Business Center Aqueduct A/B Hyatt Regency Rochester and Radisson Rochester Riverside Registration A staffed media room is available for credentialed Galleria members of the media. Badges for pre-registered The Radisson Rochester Riverside Business Center is Registration Hours reporters and reporter registration are in the media located in the hotel Lobby and features four comput- room along with media kits kits, internet connectiv- ers for guest use as well as printers. Copying, and Monday, 17 October 15:00–20:00 ity and printer, quiet work space and conference faxing services are offered through the Radisson Tuesday, 18 October 07:00–17:00 information. Rochester Riverside Front Desk. These services are available 24 Hours a Day. Wednesday, 19 October 07:00–18:00 Media Room Hours The Hyatt Regency Rochester’s in-house Business Thursday, 20 October 07:00–17:00 Monday, 17 October 12:00–17:00 Center, operated by CMI Communications, offers Friday, 21 October 07:30–16:30 Tuesday, 18 October 08:00–17:00 one-stop shopping for all of your business needs, Wednesday, 19 October 08:00–17:00 including e-mail and high-speed Internet access, secretarial/transcription services, photocopying, and Speaker Preparation Room Thursday, 20 October 08:00–12:00 Aqueduct C/D faxing. Guests of the Hyatt Regency Rochester have extended access to the business center which is avail- Speakers and presenters are encouraged to stop by E-Center able 24 hours a day, 7 days a week. the Speaker Preparation Room to test their computers Empire Lobby and presentations prior to their session. The room will Lost and Found be equipped with LCD projectors and screens. Com- The E-Center, offering free internet connectivity, will puters will be available to test presentations. be open Monday through Friday during registration For Lost and Found please check first at the confer- hours. ence registration counter in the Gallieria. Please put Speaker Preparation Hours your name on all conference materials (including your Monday, 17 October 15:00–18:00 Exhibition Conference Program), as they will only be replaced for a fee. Tuesday, 18 October 07:00–18:00 Empire Hall Wednesday, 19 October, 09:30–16:00 Wednesday, 19 October 07:00–18:00 Thursday, 20 October, 09:30–14:00 Special Needs Thursday, 20 October 07:00–18:00 Exhibit Hours Exclusive If you have a disability and require special accommo- Friday, 21 October 07:30–16:00 dations in order to fully participate in this conference, Wednesday, 19 October 09:30–10:30 please contact Conference Management at the regis- 12:00–13:00 tration desk. Your specific needs will be addressed. 14:00–16:00 Thursday, 20 October 09:30–11:00 12:30–14:00

The FiO Exhibit is open to all registered attendees. Visit a diverse group of companies representing every facet of the optics and photonics industries. For more information, see page 23.

FiO/LS 2016 • 16–21 October 2016 5 WiFi Access Instructions Highland Hospital OSA Booth 1000 South Avenue Rochester, New York 14620 Galleria To access the complimentary wifi services during the +1 585.473.2200 FiO/LS Conference, use the following information All FiO attendees are invited to stop by the OSA to log in. If you require more detailed instructions, Park Ridge Hospital Booth. Not a Member? Join on-site and take advan- a step-by-step access guide is available at the FiO 1555 Long Pond Road Rochester, New York 14626 tage of a 50 percent dues discount on the Individual registration desk. +1 585.723.7000 Member category. Sign up at the OSA Booth, which is located near Registration. Rochester Riverside Convention Center Wifi information: Sponsoring Society Membership Booths Galleria SSID: FiO2016 General Information Password: OSA100proud APS and OSA Society Booth Hours Radisson Rochester Riverside Wifi Information: Monday, 17 October 15:00–20:00 CAM Lounge Empire Lounge SSID: RadissonRochesterRiverside Tuesday, 18 October 07:00–17:00 Password: none OSA is turning 100 in 2016! We’re asking all OSA Wednesday, 19 October 07:00–17:00 members to be a part of the celebration by partici- WORKinOPTICS.com Kiosk Thursday, 20 October 07:00–17:00 pating in short videos. CAM (Centennial Authentic Empire Lobby Friday, 21 October 07:30–16:30 Moments) is an ongoing program of collecting scientific selfies where members will talk about what it WORKinOPTICS.com provides a state-of-the-art plat- means to be an OSA Member, how has OSA helped form to efficiently connect employers and job seekers APS Booth in their careers, what inspired them to get into the within the optics and photonics community. Galleria field of optics and what excites them about their current work in three minutes or less. The collection of Your next job opportunity or new hire is just a click Founded in 1899, the American Physical Society (APS) these short videos will be featured on OSA’s centen- away. is a non-profit membership organization working nial website. • Post your resume at no charge to reach top to advance and diffuse the knowledge of physics. employers. APS publishes the world’s most widely read physics CAM Lounge Hours research and review journals: Physical Review Let- • OSA Industry Development Associates ters, Physical Review X, Reviews of Modern Physics, Tuesday, 18 October 09:00–14:00 Members get 20 free job postings. Physical Review A-E, Physical Review Fluids, Physical Wednesday, 19 October 09:00–14:30 Review Applied, Physical Review Accelerators and First Aid and Emergency Information Beams, Physical Review Physics Education Research, and Physics. Please stop by our table near Registra- In the event of an emergency at the Rochester Riv- tion to learn more about the prestigious Physical erside Convention Center, please dial “0” from any Review collection and Physical Review Fluids, our black courtesy phone. newest journal dedicated to publishing innovative Medical Facilities research that will significantly advance the fundamental understanding of fluid dynamics. Strong Memorial Hospital 601 Elmwood Avenue Rochester, New York 14642 +1 585.275.2100 Rochester General Hospital 1425 Portland Avenue Rochester, New York 14621 +1 585.922.4000

6 FiO/LS 2016 • 16–21 October 2016 OSA100 Exhibit Looking for Lunch? Food Trucks and General Information Empire Hall Booth #101 and Galleria Concessions! We have planned some new exciting lunch options. On Tuesday, 18 October and Friday, 21 October a variety of food trucks will be available during lunch OSA is marking a century of sparking inspiration hours (cash and credit accepted) outside of the Roch- and smart innovation driven by 270,000 scientists, ester Riverside Convention Center. On Wednesday, students, engineers and business leaders around 19 October, cash concessions will be available in the the world. Visit the OSA100 Exhibit in the registra- exhibit hall from 12:00–13:00, visit with the exhibitors tion area to experience 100 iconic images from the and enjoy lunch (cash only please). history of optics, photonics and The Optical Society. A smaller version of the exhibit will also be featured at booth #101. To see the interactive version of the OSA100 Exhibit and learn more about OSA Centen- Free Lunch Provided by OSA nial Activities, go to osa.org/100. On Thursday, 20 October, join your FiO colleagues OSA100 Empire Hall Booth Hours for a FREE lunch in the Exhibit Hall from 12:30– 14:00. This is a great opportunity to meet the Wednesday, 19 October 09:30–16:00 exhibitors who have contributed to our success Thursday, 20 October 09:30–14:00 over the last 100 years.

OSA100 Galleria Booth Hours Monday, 17 October 15:00–20:00 Tuesday, 18 October 07:00–17:00 Wednesday, 19 October 07:00–17:00 Thursday, 20 October 07:00–17:00 Friday, 21 October 07:30–16:30

FiO/LS 2016 • 16–21 October 2016 7 8 FiO/LS 2016 • 16–21 October 2016 Stay Connected

Conference Materials Exhibit Buyers’ Guide Schedule The Exhibit Buyers’ Guide is composed of descrip- Search for conference presentations by day, topic, Technical Digest and Postdeadline Papers tions and contact information for exhibiting com- speaker or program type. Plan your schedule by set- Technical attendees have EARLY (at least one week panies at this year’s conference, and exhibit hall ting bookmarks on programs of interest. Technical prior to the conference) and FREE continuous online activities. Guides will be provided to every FiO/LS attendees can access technical papers within session access to the FiO/LS 2016 technical digest and attendee as part of registration. All exhibitor infor- descriptions. mation changes will be communicated in the FiO/ Postdeadline papers. These 1-2-page summaries of Exhibit Hall tutorial, invited, and accepted contributed papers can LS mobile application. We encourage you to review be downloaded individually or by downloading daily the mobile application carefully to stay informed of Search for exhibitors in alphabetical order, and set a

.zip files. (.zip files are available for 60 days.) changes to the program. bookmark reminder to stop by their booth. Tap on Stay Connected the map icon within a description, and you’ll find their 1. Visit the conference website at http://www.fron- Program Updates Board location on an expo floor map. View a daily schedule tiersinoptics.com of all activities occurring on the show floor. Onsite Program changes will be posted on an update 2. Select the “Access Digest Papers” link on the board located at the registration desk. Check daily for Attendees right side of the web page new information and/or reference the FiO/LS mobile All FiO/LS registered attendees are listed in the app. 3. Log in using your email address and password app. Send a contact request to an attendee, and initiate used for registration. Access is limited to Full another valuable networking opportunity. Technical Attendees only. If you need assistance Join the Social Conversation at FiO/LS 2016! with your login information, please use the “for- Download the App We will be providing the latest updates throughout got password” utility or “Contact Help” link. the conference using Twitter. Do you have a Twitter The app is compatible with iPhone, iPad, iPod Touch handle? Follow @Opticalsociety on Twitter. Tweet and Android devices. To get the guide, choose one Conference Program Update Sheet about your conference experience using #FIO16 in of the methods below: Technical program changes received just prior to the your tweets. Stop by the OSA booth for more details. 1. Visit www.frontiersinoptics.com/app to download meeting will be communicated in the onsite Confer- Join the conversation. Follow @Opticalsociety on the application. ence Program Update Sheet distributed with your Twitter. Use hashtag #FIO16. Celebrate 100 years of onsite registration materials. In addition, all updates optics at #OSA100. 2. Scan the following image with your mobile phone will be made in the FiO/LS mobile app. We encour- (QR-Code reader required, e.g. ‘Red Laser’, ‘Bar- age you to review them carefully to stay informed on Join the conversation. code Scanner’) changes to the program. Follow @Opticalsociety on Twitter. 3. Search for OSA Events in the app stores. Use hashtag #FIO16 and #OSA100 Poster Presentation PDFs Authors presenting posters have the option to submit FiO/LS Mobile Application the PDF of their poster, which will be attached to their Frontiers in Optics/Laser Science 2016 (FiO/LS 2016) papers in OSA Publishing’s Digital Library. If submit- has gone mobile again this year using CrowdCom- ted, poster PDFs will be available about three weeks pass! We strongly encourage you to download our after the conference end date. While accessing the mobile guide to enhance your experience at FiO/LS papers in OSA Publishing’s Digital Library, look for the 2016. You’ll be able to plan your day with a person- multimedia symbol (above). alized schedule and browse exhibitors, maps and general show info.

FiO/LS 2016 • 16–21 October 2016 9 2017 OSA Optics and Photonics Topical Meetings and Congresses

Submit your Submit your abstract by: abstract by: OFC 19 - 23 March 11 October 2016 Freeform Optics (Freeform) OSA Design and 8 March 2017 Los Angeles, International Optical Design Conference Fabrication Congress California, USA (IODC) 9 - 13 July ofcconference.org Optical Fabrication and Testing (OF&T) Denver, Colorado, USA Optical Trapping Applications (OTA) OSA Biophotonics 29 November 2016 osa.org/ Novel Techniques in Microscopy (NTM) Congress: Optics in DesignFabOPC Bio-Optics: Design and Application the Life Sciences OSA Nonlinear Optics Topical Meeting 17 - 21 July 2017 14 March 2017 (BODA) 2 - 5 April Waikoloa, Hawaii, USA Optical Molecular Probes, Imaging and San Diego, California, osa.org/nlo Drug Delivery (OMP) USA Integrated Photonics Research, Silicon, OSA Advanced 4 April 2017 Optics and the Brain (BRAIN) osa.org/ and Nano-Photonics (IPR) Photonics Congress LifeSciencesOPC Novel Optical Materials and Applications 24 - 27 July OSA Quantum Information and 5 - 7 April 6 December 2016 (NOMA) New Orleans, Measurement (QIM) - IV: Quantum Paris, France Optical Sensors (Sensors) Louisiana, USA Technologies osa.org/qim Photonic in Switching (PS) osa.org/PhotonicsOPC

Stay Connected CLEO: 2017 14 - 19 May 14 December 2016 Photonic Networks and Devices San Jose, California, (Networks) USA Signal Processing in Photonic cleoconference.org Communications (SPPCom) OSA Digital Holography and 3-D Imaging 29 May - 1 June 24 January 2017 CLEO/Pacific Rim 31 July - 4 August 1 January 2017 Topical Meeting Jeju Island, South Singapore, Singapore Korea photonics2017.org osa.org/dh Frontiers in Optics/Laser Science 17 - 21 September 2 May 2017 CLEO/Europe - EQEC 25 - 29 June 19 January 2017 Washington, D.C., USA Munich, Germany frontiersinoptics.com www.cleoeurope.org Advanced Solid State Lasers Conference OSA Laser Congress 30 May 2017 European Conferences on Biomedical 25 - 29 June 19 January 2017 and Exhibition (ASSL) 1 - 5 October Optics Munich, Germany Laser Applications Conference Nagoya, Aichi, Japan www.osa.org/ecbo osa.org/assl 3D Image Collection and Display OSA Imaging and 15 February 2017 Solid State Lighting (SSL) OSA Light, Energy 5 July 2017 Applied Industrial Optics (AIO) Applied Optics Optical Nanostructures and Advanced and the Environment Computational Optical Sensing and Congress Materials for Photovoltaics (PV) Congress Imaging (COSI) 26 - 29 June Optical and Photonics for Energy & the 6 - 9 November Imaging Systems and Applications (IS) San Francisco, Environment (E2) Boulder, Colorado, Mathematics in Imaging California Optics for Solar Energy (SOLAR) USA Propagation Through and Characterization osa.org/ImagingOPC osa.org/EnergyOPC of Atmospheric and Oceanic Phenomena (pcAOP)

10 FiO/LS 2016 • 16–21 October 2016 Conference Plenary Sessions and Awards Ceremony

Wednesday, 19 October, 08:00–09:30 and Plenary Presentations Next Generation Silicon Photon- Thursday, 20 October, 08:00–09:30 ics, Michal Lipson, Columbia Lilac Ballroom Controlling Light-matter Interac- University, USA tions on the Nanometer Scale, Join your colleagues to recognize recent OSA and Lukas Novotny, ETH Zürich, In the past decade, silicon pho- APS/Division of Laser Science award and honor recipi- Switzerland tonics has recently been shown as ents. The sessions include the Ives Medal Address, a platform for high-performance the Schawlow Prize Lecture and two plenary presenta- The past 20 years have brought optical devices that can be tions. The order of events: exceptional control over light-mat- monolithically integrated with ter interactions on the nanoscale. state-of-the-art microelectronics. Wednesday, 19 October Today, localized optical fields are The toolbox of integrated nanophotonics today is Welcome and Opening Remarks being probed with nanoscale rich: from the ability to modulate, guide and amplify materials and, vice versa, nanoscale materials are multiple wavelength sources at GHz bandwidths, to Controlling Light-matter Interactions on the being controlled and manipulated with localized optomechanical MEMS and nonlinear devices. Nanometer Scale, Lukas Novotny, ETH Zurich, fields. Switzerland In this talk, Michal Lipson will review the current chal- In this talk, Lukas Novotny will discuss both early and lenges and recent achievements in the field of silicon OSA Award and Medal Presentations recent developments in near-field optical spectros- nanophotonics and present recent results. Using copy and optical nanomanipulation. Ives Medal Address – Extreme Light: From highly-confined photonic structures, her team has Multiphoton Ionization to Light Materialization About the Speaker demonstrated ultra-compact passive and active sili- and Beyond, Gérard Mourou, IZEST, Ecole con photonic components that enhance the electro- Lukas Novotny is a Professor of Photonics at ETH optical, mechanical and nonlinear properties of the

Polytechnique Palaiseau, France Plenary and Awards Zürich. His research is focused on understanding and material. Closing Remarks controlling light-matter interactions on the nanometer scale. Novotny did his PhD at ETH Zürich and from About the Speaker Thursday, 20 October 1996-99 he was a postdoctoral fellow at the Pacific Prof. Michal Lipson is the Eugene Higgins Profes- Welcome Northwest National Laboratory, working on new sor at Columbia University. She completed her B.S., schemes of single molecule detection and nonlin- Next Generation Silicon Photonics M.S. and Ph.D. degrees in Physics in the Technion , Michal ear spectroscopy. In 1999 he joined the faculty of Lipson, Columbia Univ., USA in 1998. Following a Postdoctoral position in MIT in the Institute of Optics at the University of Rochester the Material Science department from 1998 to 2001, OSA Fellow Member Recognition where he started one of the first research programs she joined the School of Electrical and Computer to focus on nano-optics. Novotny is the author of the APS Fellow Member Recognition Engineering at Cornell University and was named textbook Principles of Nano-Optics, which is cur- the Given Foundation Professor of Engineering at Schawlow Prize Lecture – Nonlinear Optics and rently in its second edition. He is a Fellow of The the School of Electrical and Computer Engineering Laser Science, Robert W. Boyd, University of Optical Society and the American Association for the in 2012. In 2015 she joined the electrical engineer- Ottawa, Canada Advancement of Science. ing department at Columbia University. Lipson is one of the pioneers of the field of silicon photonics. She Closing Remarks holds over 20 patents and is the author of over 200 technical papers. Prof. Lipson’s honors and awards include Macarthur Fellow, Blavatnik Award, IBM Fac- ulty Award, and NSF Early Career Award. She is a Fel- low of both the OSA and of IEEE. She was named by Thomson Reuters as a top 1% highly cited researcher in the field of Physics.

FiO/LS 2016 • 16–21 October 2016 11 Awards Ceremony 2016 Frederic Ives Medal / Jarus Quinn Prize APS/Division of Laser Science Award APS and OSA will present awards and honors during Extreme Light: From Multipho- Arthur L. Schawlow Prize the Plenary Session. ton Ionization to Light Material- Robert Boyd, Univ. of Ottawa, Canada ization and Beyond, Gérard 2016 Arthur L. Schawlow Prize in Laser Mourou, École Polytechnique, DLS sponsored APS Fellows: Science France Andrea Alu, Univ. of Texas, Austin, USA Nonlinear Optics and Laser The laser provides a convenient Citation: For seminal contributions to electromagnetic Science, way to generate formidable Robert W. Boyd, Univer- theory and applications, nano optics, plasmonics, and sity of Ottawa, Canada fields—enough to break atomic bonds, drive particles relativisti- metamaterials. The interplay between nonlinear cally over short distances or generate high energy Hiroshi Amano, Nagoya Univ., Japan optics and the field of laser sci- radiations. A new way to compress large energy Citation: For pioneering the materials science and ence will be reviewed. Topics to pulses into the attosecond-zeptosecond range has device physics leading to the invention of blue light- be stressed include the develop- emerged. X-Ray pulses in the exawatt regime would emitting diodes with III nitride-based semiconductor ment of approaches for controlling ensue opening unfathomable possibilities for nuclear heterostructures. the velocity of light, of quantum physics, high energy physics, astrophysics and cos- imaging methods, and composite nonlinear optical mology, showing that the best in laser physics is yet Hou-Ton Chen, Los Alamos National Laboratory, USA materials. to come. Citation: For contributions to the development of active metamaterials and devices, and the develop- About the Speaker About the Speaker ment and understanding of few-layer metamaterials Robert W. Boyd received the B.S. degree in physics Gérard Mourou was the founding Director of the and metasurfaces, especially in the terahertz fre- in 1969 from Massachusetts Institute of Physics (MIT) Center for Ultrafast Optical Science at the University quency range. and his Ph.D. in physics in 1977 from the University of of Michigan. For forty years, Mourou has pioneered Zhingang Chen, San Francisco State Univ., USA California, Berkeley. He joined the faculty of the Uni- the field of ultrafast lasers and their applications in Citation: For seminal contributions on spatial soli- versity of Rochester in 1977, and in 2001 became the scientific, engineering and medical disciplines. He is tons, photonic lattices, and beam shaping, and for M. Parker Givens Professor of Optics and Professor of also the initiator of the Extreme Light Infrastructure promoting world-class research at an undergraduate Physics. In 2010, he became Professor of Physics and (ELI) in Europe. With his student Donna Strickland institution. Canada Excellence Research Chair at the University he is the inventor of the chirped pulses amplification of Ottawa. His research interests include studies of technique which allows ultrashort laser pulses to be Stefan Hell, Max Planck Institute, Germany “slow” and “fast” light, orbital angular momentum amplified to petawatt optical powers, with the laser Citation: For pioneering contributions to the devel- of light, quantum communication, quantum imag- pulse being stretched out temporarily and spectrally opment and application of superresolved, far-field ing, nonlinear optical interactions and materials, and before amplification. Mourou has recieved the Wood optical microscopy.

Plenary and Awards nanofabrication of photonic devices. He has written Prize from OSA, the Edgerton Prize from the SPIE, Mackillo Kira, Philipps Univ. Marburg, Germany two books, co-edited two anthologies, published the Sarnoff Prize from the IEEE, and the 2004 IEEE/ Citation: For contributions to theoretical semiconduc- over 400 research papers (≈29,000 citations, Google LEOS Quantum Electronics Award. He is a Fellow tor quantum optics. h-index 71), and been awarded nine patents. He of OSA and IEEE, as well as a member of the U.S. is the 2009 recipient of the Willis E. Lamb Award National Academy of Engineering. Currently he is a Xiaogin Li, Univ. of Texas, Austin, USA for Laser Science and Quantum Optics, the 2010 distinguished professor emeritus at the University of Citation: For contributions to quantum information, recipient of a Humboldt Research Prize, and the 2014 Michigan, USA, and at the École Polytechnique in multidimensional coherent spectroscopy, nanopho- recipient of the Quantum Electronics Award of the Palaiseau, France. tonics based on AFM assembly, and spin dynamics in IEEE Photonics Society. ferromagnetic nanostructures.

12 FiO/LS 2016 • 16–21 October 2016 OSA Awards and Honors Stephen D. Fantone Distinguished Service Award William F. Meggers Award G. Michael Morris, RPC Photonics Inc., USA Brooks H. Pate, University of Virginia, USA OSA Fellowships For extraordinary contributions to the OSA, includ- For the invention of the chirped- pulse Fourier Irene Georgakoudi, Tufts University, USA ing distinguished service as OSA President and a transform microwave technique, which revolutionized Elizabeth M. C. Hillman, Columbia University, USA key role in the formation and leadership of the OSA rotational spectroscopy, leading to an explosion of Foundation novel spectroscopic, astrochemical, analytical, dynam- Cristina Masoller, Universitat Politecnica de Catalunya, ical, and chemical kinetics applications Spain Paul F. Forman Team Engineering Excellence Award David D. Smith, NASA Marshall Space Flight Center, Advanced LIGO Engineering Team David Richardson Medal USA For innovative engineering creating the most sensi- Francisco J. Duarte, Interferometric Optics, USA tive measurement instrument ever built, leading to For seminal contributions to the physics and technol- H. Philip Stahl, NASA Marshall Space Flight Center, the first direct detection of gravitational waves. ogy of multiple-prism arrays for narrow-linewidth tun- USA able laser oscillators and laser pulse compression. David Stork, Rambus Inc., USA Joseph Fraunhofer Award/Robert M. Burley Prize Demetri Psaltis, École Polytechnique Fédérale de R. W. Wood Prize Andrey A. Sukhorukov, Australian National University, Lausanne, Switzerland Kishan Dholakia, University of St. Andrews, U.K. Australia For pioneering contributions to the fields of photon- For pioneering research into optical micromanipula- Mourad Zghal, University of Carthage, Tunisia ics engineering and optofluidics. tion using shaped light for interdisciplinary photonics- based applications. 2016 Frederic Ives Medal/Jarus W. Quinn Prize Nick Holonyak, Jr. Award Gérard Mourou, École Polytechnique, France Chennupati Jagadish, Australian National University, The Treasurer’s Award: An OSA Employee For numerous pioneering contributions to the Australia Recognition Program development of ultrafast and ultrahigh intensity laser For pioneering work and sustained contributions to The Treasurer’s Award, in recognition of the unique science and for outstanding leadership of the inter- quantum-well, quantum-dot and nanowire optoelec- perspective our Treasurers have on the staff and their national and commercial communities impacted by tronic devices and their integration these technologies impact to the operations of the Society, will honor an Emmett Leith Medal employee who has made significant contributions to Plenary and Awards Esther Hoffman Beller Medal Francis T.S. Yu, Pennsylvania State University, USA organizational excellence, who promotes and enacts Bishnu P. Pal, Mahindra École Centrale, India For life-long important contributions to holography, innovative solutions or who exemplifies inspirational For over thirty-five years of guided wave photonics white-light holography, partially coherent signal pro- leadership. education, including the development of graduate cessing, optical correlators, and information optics. and continuing education teaching programs and Congratulations to the 2016 Treasurer’s Award laboratories in optoelectronics and optical communi- Ellis R. Lippincott Award Recipient: Thomas Elsaesser, Max Born Institute, Germany cations at IIT-Delhi, and for inspiring a generation of Deborah Herrin, The Optical Society, USA leading academic and industrial scientists For seminal contributions to the understanding of the ultrafast coherent and incoherent vibrational dynam- Max Born Award ics of hydrogen bonds in liquids and biomolecules Xiang Zhang, University of California, Berkeley, USA For the experimental realization of major theoretical Michael S. Feld Biophotonics Award predictions in the field of metamaterials and For leadership and pioneering contributions in the graphene optics field of biphotonics, comprising the diverse use of label-free native fluorescence, Raman spectroscopy and optical imaging for cancer detection in tissues and cells

FiO/LS 2016 • 16–21 October 2016 13 Awards and Special Recognitions

OSA Foundation Grant Recipients cheff, an internationally renowned laser spectrosco- FiO 5: Integrated Photonics pist who also served as President of OSA (1976) and Clément Javerzac-Galy, Ecole Polytechnique Federale The OSA Foundation would like to congratulate our CAP (1983-84).This $3,000 scholarship is awarded De Lausanne, Switzerland 2016 grant recipients. Through the following pro- annually to a graduate student who has demonstrated Moritz Merklein, Centre for Ultrahigh Bandwidth grams we have been able to provide over 30 grants, both research excellence and significant service to the Devices for Optical Systems (CUDOS), The Univ. of scholarships and prizes to help students attending optics or physics community. Sydney, Australia FiO. Mengjie Yu, Cornell Univ., USA Congratulations to the 2016 award recipient: You can help to inspire and support the next genera- Christopher Pugh, Univ. of Waterloo, Canada FiO 6: Quantum Electronics tion of science and engineering innovators by making Lior Cohen, Hebrew Univ. of Jerusalem, Israel a donation to the OSA Foundation. All donations are OSA Foundation Emil Wolf Outstanding Rick Leijssen, FOM Inst. AMOLF, the Netherlands matched 100% by the Optical Society—so your gift Christian Reimer, INRS-EMT, Canada has twice the impact. To learn more and to make a Student Paper Competition donation online, visitwww.osa.org/foundation, or stop FiO 7: Vision and Color This competition recognizes the innovation, research by the OSA booth. Amanda Bares, Cornell Univ., USA excellence and presentation abilities of students pre- Michelle Victoria, Univ. of Illinois at Urbana- senting their work during FiO and honors Emil Wolf OSA Foundation Travel Grant Recipients Champain, USA for his many contributions to science and The Optical Tao Jin,Univ. of Waterloo, Canada Fernando Arturo Araiza Sixtos, Faculty of Sciences, Society. One winner is selected from each of the Mexico seven FiO subcommittees. Winners receive a complimentary OSA three-year student membership, an OSA Foundation Incubic/Milton Chang Pegah Asgari, Zanjan Univ., Iran Travel Grant Gabriel Castillo-Santiago, UNAM, Mexico award stipend of $300 USD and an award certificate. Jin-hui Chen, Nanjing Univ., China Congratulations to our finalists competing at FiO: Funded by an endowment from Milton and Rosalind Andrew Huzortey, Univ. of Cape Coast, Ghana Chang, this program provides 10 grants of $500 USD Jem Teresa John, Indian Inst. of Sciences, India FiO 1: Optical Design and Instrumentation each to enable students who present papers to travel Ivan Kam, Instituto de Estudos Avançados (IEAv), Wenzhe Li, Clemson Univ., USA to the Frontiers in Optics. Grants are awarded to the Universidade Federal de São Paulo, Brazil Maria Papaioannou, Univ. of Southampton, UK presenter and usually the first author of the paper. Apurv Chaitanya Nellikka, Physical Research Piotr Tyczkowski, Tampere Univ. of Technology, Congratulations to the 2015 Incubic/Milton Chang Laboratory, India Finland Yousef Pourvais, Univ. of Tehran, Iran Di Xu, Univ. of Rochester, USA Travel Grant Recipients: Nirmal Punjabi, Indian Inst. of Technology, Bombay, FiO 2: Optical Sciences Mahbub Alam, Georgia Inst. of Technology, USA India Zhe Guang, Georgia Inst. of Technology, USA Surekha Barkur, Manipal University, India Zhuo Wang, Huazhong Univ. of Sciences & Nihal Jhajj, Univ. of Maryland, USA Gabriel Castillo, Universidad Nacional Autonoma de Technology, China Roman Khakimov, Australian National Univ., USA Mexico, Mexico Jin-Min Wu, Beijing Inst. of Technology, Beijing Key Bethany Little, Univ. of Rochester, USA Xiaobo Han, Huazhong Univ. of Science and Laboratory or Fractional Signals and Systems, Technology, China China FiO 3: Optics in Biology and Medicine Tong Lin, National Univ. of Singapore, Singapore William Eldridge, Duke Univ., USA Sara Magdi, American Univ. in Cairo, Egypt OSA Foundation Boris P. Stoicheff Aleks Klimas, George Washington Univ., USA Emerson Melo, Univ. of Sao Paulo, Brazil Memorial Scholarship FiO 4: Fiber Optics and Optical Communications Patrick Stockton, Colorado State Univ., USA Krysta Boccuzzi, Univ. of Rochester, USA Denise Valente, Univ. College Dublin, Ireland Established in 2011 by the OSAF and the Canadian Zhanwei Liu, Cornell Univ., USA Hengyun Zhou, Harvard Univ., USA Association of Physicists Educational Trust Fund

Special R ecognitions Samantha Nowierski, Northwestern Univ., USA (CAPETF), this program pays tribute to Boris P. Stoi-

14 FiO/LS 2016 • 16–21 October 2016 OSA Foundation Jean Bennett Memorial Carl E. Anderson Award for Outstanding Student Travel Grant Doctoral Dissertation Established in 2008, in memory of Jean M. Ben- The Carl E. Anderson Award for Outstanding Doc- nett, a highly decorated research physicist who was toral Dissertation in Laser Science was established in recognized for her contributions to the studies of 2013 by the American Physical Society (APS) Division optical surfaces and served as OSA’s first female presi- of Laser Science (DLS). Its purpose is to recognize dent, this $1,000 USD grant is awarded to a student doctoral research in the Laser Science area and to presenting their work at FiO. This competition is encourage effective written and oral presentation of administered by the OSA Foundation and is made research results. The award consists of $1,000 USD possible through the generous support of Nanoptek and a certificate citing the contribution made by the Corporation, the Pennsylvania State Univ. Department recipient. The finalists will present their work at a of Physics and individual contributors. special session of the Laser Science conference on Tuesday, 18 October from 08:00-10:00 in the High- Congratulations to our 2016 grant recipient: land Room E. The winner will be announced at the Roxana Rezvani Naraghi, University of Central Florida, DLS business meeting Wednesday. USA The following presentations will be given during this OSA Foundation Robert S. Hilbert special session: Memorial Student Travel Grant Giulio Vampa, Univ. of Ottawa, Canada, Identifying and Using Recollision-based High Harmonics from Established in 2009 by Optical Research Associates Bulk Semiconductors (ORA), now the Optical Solutions Group at Synopsys, as a memorial to ORA’s former President and Chief Christoph Heyl, Lund Univ., Sweden, Power-scaling Executive Officer Robert S. Hilbert, this $1,100 USD Attosecond Sources Using Universal Scaling grant recognizes the research excellence of students Principles for Nonlinear Optical Processes in Gases in the areas of optical engineering, lens design and Mohammad Mirhosseini, California Inst. of illumination design. Technology, USA, Quantum Information with Congratulations to our 2016 grant recipients: Structured Light Jin-hui Chen, Nanjing University, China Sylvain Ravets, Joint Quantum Institute, USA, Ahmed Dorrah, University of Toronto, Canada Development of Tools for Quantum Engineering Denise Valente, University College Dublin, Ireland Using Individual Atoms: Optical Nanofibers and Controlled Rydberg Interactions Special R ecognitions

FiO/LS 2016 • 16–21 October 2016 15 Special Symposia

Symposium on 100 Years of Optical Robert Wiederhold, Optimax Systems, Inc., USA, The Don Keck, Retired, USA, Glass and Light: Enabling Design, Fabrication, Testing, and History of Optical Fabrication in Rochester NY the Information Age Instrumentation - A Historical Look Back Jim Wyant, Univ. of Arizona, USA, Short History of Ming Jun Li, Corning Inc., USA, Recent Development Tuesday, 18 October, 08:00–10:00 (Part I), Interferometric Optical Metrology in Optical Fibers for High Capacity Transmission 10:30–12:00 (Part II), 13:30–14:30 (Part III) Systems

Special Symposia Grand Ballroom A (Radisson) Symposium on 50th Anniversary of Low- John MacChesney, John B. MacChesney Optical Symposium Organizer: Julie Bentley, Univ. of Loss Optical Fibers Materials, USA, AT&T’s Contributions to Fiber Rochester, USA Tuesday, 18 October, 08:00–10:00 (Part I), Optics 10:30–12:00 (Part II), 13:30–15:30 (Part III) Trans This symposium celebrates 100 years of advances Grand Ballroom B (Radisson) Stojan Radic, Univ. of California San Diego, in optical design, optical fabrication and testing, mitting Beyond The Fictitious Nonlinear Capacity and instrumentation by taking a historical look back. Symposium Organizer: Alan F. Evans, Corning, USA Limit Topics to be discussed include the development of Optical fibers have changed our society by connect- David Richardson, Univ. of Southampton, UK, Recent optical design software, the optical design of tele- ing the world. This fundamental global transforma- Advances in Microstructured Optical Fibers and scopes at NASA, the evolution of optical design and tion occurred due to the advent of low-loss optical their Applications metrology at Tropel, a look into optical manufactur- fiber for high-bandwidth transmission of optical data. ing at Kodak, the history of the Steward Mirror Lab, High-Capacity This symposium celebrates the 50th anniversary of Robert Tkach, Nokia Bell Labs, USA, APOMA, and COM, and the ever changing landscape Optical Communications – Can We Guess the Charles K. Kao’s seminal paper unfolding the alluring of optical metrology and optical instrumentation. Future from the Past? possibilities and opportunities of low-loss silica fiber. Invited Speakers: The presentations in this symposium will focus on the history of the development of silica fiber technolo- Laser Science Symposium on , History of Optical John Bruning, Retired, USA gies, highlight significant milestones and advances Undergraduate Research Design and Metrology at Tropel to emerge from this paradigm shift in the way light Tuesday, 18 October, 12:15–18:00 Joseph Howard, NASA, USA, Large-data Center is transmitted, and describe recent developments of Highland Room A Interconnect: Emerging Technologies and Scaling low-loss fibers with advanced designs and materials. Organizer: Harold Metcalf, Stony Brook Univ., USA Challenges Invited Speakers: The Symposium on Undergraduate Research has John Grievenkamp, The Univ. of Arizona, USA, Optics John Ballato, Clemson Univ., USA, Back to the been a feature of the annual meeting of the Divi- Goes to the Movies Future - Why Boring Old Materials and Designs are sion of Laser Science of the American Physical Dae Wook Kim, Univ. of Arizona, USA, 30 Years of the Answer to Next Generation Optical Fibers Society (APS-DLS) for more than ten years, and has Mirror Making at the Richard F. Caris Mirror Lab showcased the research work of approximately 400 Richard Epworth, Retired, UK, The Birth of Optical students during that time. Students’ presentations John Schoen, US Dept. of Defense, USA, History of Fiber Communications often describe their work during the previous sum- the Center for Optics Manufacturing Yoel Fink, MIT, USA, Realizing a Moore’s Law for mer. The Symposium has been supported by the DLS, Jim Sydor, Sydor Optics, USA, APOMA: Past & Fibers OSA, and the NSF, along with several corporate spon- Present sors. The NSF has played a vital role by providing Randy Giles, Nokia Bell Labs, USA, Origins of the the research opportunities for many of the students Erbium-Doped Fiber Amplifier Ed White, Consultant, USA, History of Optical Manu- through its REU programs, as well as by direct sup- facturing at Kodak Takemi Hasegawa, Sumitomo Electric Industries Ltd., port of the event. Japan, Advances in Ultra-low Loss Silica Fibers

16 FiO/LS 2016 • 16–21 October 2016 Symposium on Mesoscopic Optics of A Tribute to Steve Jacobs Aric Shorey, Corning Inc., USA, Materials Develop- Disordered Media Wednesday, 19 October, 10:30–12:00 (Part I), ment in Magnetorheological Finishing: The Work of Special Symposia Wednesday, 19 October, 10:30–12:00 (Part I), 13:00–14:00 (Part II) Dr. Stephen Jacobs 13:00–14:00 (Part II) Highland Room C Grand Ballroom D (Radisson) Organizer: Julie Bentley, Univ. of Rochester, USA Symposium on Mid-Infrared Fiber Sources Thursday, 20 October, 14:00–16:00 (Part I), Organizers: Aristide Dogariu, CREOL, Univ. of Florida, The Stephen D. Jacobs Symposium has been 16:30–18:30 (Part II) USA; Remi Carminati, ESPCI ParisTech, France; and organized to honor the late Dr. Stephen D. Jacobs’s Grand Ballroom A (Radisson) Juan Jose Saenz, Donostia International Physics contributions to the fields of optical materials, liquid Center, Spain crystals, optics manufacturing and educational out- Organizer: Morten Ibsen, Univ. of Southhampton, UK In extreme environments, electromagnetic fields reach. Steve spent his entire career at the University Optical sources in the mid-infrared wavelength range couple strongly to matter. Recent advances in under- of Rochester with appointments at the Laboratory have become key for enabling applications in remote standing the complex phenomenology of multiple for Laser Energetics (LLE), Institute of Optics, Materi- sensing, biomedical, materials processing, and home- scattering offer unique opportunities for retrieving als Science and Chemical Engineering departments. land security. Specific applications in metrology, structural information and for controlling the propa- His research included topics such as phosphate laser tomography, and isotope separation are enabled by gation of light. At photonic mesoscales, fascinating glass, frequency conversion crystals, liquid crystal optical access to the molecular fingerprint region. To interaction and confinement phenomena occur across laser optics, optical finishing of glass, ceramics and date, mid-infrared fiber sources span the performance different temporal and spatial scales. This sympo- crystals, magnetorheological finishing (MRF), cho- space from ultrafast pulses to kilowatts of power, from sium will gather international experts to discuss the lesteric liquid crystal flakes for display applications, single-frequency to supercontinuum bandwidths, and experimental and theoretical progress in unveiling the and laser damage in multilayer dielectric coatings. cover spectral bands that cannot be addressed by properties of light propagating through and emitted In addition to his significant technical contributions other sources (e.g., QCLs). This symposium will focus in disordered media as well as a range of novel phe- Steve also had a passion for educational outreach. on recent developments in mid-infrared fiber sources nomena related to light-matter interaction. He volunteered as the educational outreach chair for and related technologies, with the most advanced the OSA-Rochester Section for over 15 years during progress in the field including materials, devices, and Invited Speakers: which time he developed and organized the Optics applications. Suitcase program that has been instrumental in Girish Agarwal, Oklahoma State Univ., USA, Long Invited Speakers: Range Light Matter Interactions at Hyperbolic introducing hundreds of thousands of young children Meta Surface to the fields of optics and materials science through- Caroline Amiot, Tampere Univ. of Technology, Fin- out the US and globally in over 40 countries. Steve land, Mid-IR Source for Ultra-broadband Cavity Hui Cao, Yale Univ., USA, Control of Optical Inten- Jacobs touched many lives, we are honored to have Enhanced Spectroscopy sity Distribution inside a Disordered Waveguide this special symposium in memory of our great col- league, friend and mentor. Martin Bernier, Université Laval, Canada, All-fiber Mathias Fink, Ecole Sup Physique Chimie Industri- Sources Operating in the Mid-infrared elles, France, Wave Control and Holography with Invited Speakers: Time Transformations Stuart Jackson, Macquarie Univ., Australia, Power Tanya Kosc, Univ. of Rochester, USA, Steve Jacobs: Scaling Concepts for Mid-infrared Fibre Lasers Allard Mosk, Universiteit Twente, Netherlands, Open The Optics Outreach Innovator Using Fluoride Glass Channels in Scattering Media: See the Light Inside John Lambropoulos, Univ. of Rochester, USA, Nano- Khanh Kieu, Univ. of Arizona, USA, Mid-IR Ultrafast Silvia Vignolini, Cambridge Univ., UK, Cellulose Bio- mechanics in Optical Manufacturing Fibre Laser Sources inspired Hierarchical Structures Ken Marshall, Univ. of Rochester, USA, Thirty-five Christian Rosenberg Petersen, DTU, Denmark, Gen- Years of Liquid Crystal Research at LLE: From Laser eration and Applications of High Average Power Fusion to Electronic Paper Mid-IR Supercontinuum in Chalcogenide Fibres Kathleen Richardson, UCF-CREOL, USA, Optical Angela Seddon, Univ. of Nottingham, UK, Medical Glass Science – The How and Why We Got Here Applications of Mid-IR Fibre Laser Technologies

FiO/LS 2016 • 16–21 October 2016 17 Brandon Shaw, Naval Research Labs, USA, Highly Symposium on Integrated Photonic Symposium on Integrated Quantum Nonlinear Fibre for Applications in the Mid-IR Manufacturing Optics Thibaut Sylvestre, Univ. of Franche-Comté, France, Friday, 21 October, 08:00–10:00 (Part I), Friday, 21 October, 14:30 - 15:30 (Part I); 16:00–17:30 Tutorial: Mid-IR Wavelength Conversion in Tapered 13:30–14:30 (Part II) (Part II) Chalcogenide Fibres Highland Room A Highland Room A Symposium Organizer: Stefan Preble, Rochester Inst. Symposium Organizer: Stefan Preble, Rochester Inst. Symposium on 100 Years of Vision at of Technology, USA of Technology, USA OSA: Most Cited Vision Papers in OSA This symposium gathers experts from academia, Quantum optics technologies have the potential Special Symposia Journals industry and foundries to discuss the progress that to revolutionize computing, communication and Thursday, 20 October 2016, 14:00–16:00 has been made and the challenges that remain to sensing systems. Chip-scale implementations have Highland Room E realize commercially successful integrated photonic resulted in rapid progress by integrating high quality Organizer: Susana Marcos, Consejo Sup Investigacio- manufacturing platforms. photon sources, circuits and single photon detectors together. This symposium will focus on recent nes Cientificas, Spain Invited Speakers: developments and the progress that is being made Vision Science has been an active community at Roel Baets, Universiteit Gent, Belgium, Silicon Pho- towards the realization of complex, chip-scale, quan- OSA, and a large percentage of publications on tonics Plaforms: To Standardize or to Diversify? tum information systems. vision have been among the most top cited in OSA Journals (JOSA, JOSA A, Applied Optics, Optics Let- Keren Bergman, Columbia Univ., USA, Manufacturing Invited Speakers: Silicon Photonics for High-performance Datacom ters, Optics Express and Biomedical Optics Express, Benjamin Eggleton, Univ. of Sydney, Australia, Multi- Systems among others). The symposium hig,lights some clas- plexing of Integrated Single Photon Sources sic vision science papers and their impact on today’s Peter de Dobbelaere, Luxtera, USA, Silicon Photon- Dirk Englund, MIT, USA, Quantum Information research in the field. Selected thems range from the ics: Applications and High Volume Manufacturing Processing Using Programmable Silicon Photonic sensitivity of the eye and motion perception to wave- Platform front sensing in the eye. Integrated Circuits Michael Liehr, AIM Photonics, USA, AIM Photonics - Jeremy O’Brien, Univ. of Briston, UK, Title to be Invited Speakers: Manufacturing Challenges for Photonic Integrated Announced Edward H. Adelson, MIT, USA, Motion, Early Vision, Circuits Christine Silberhorn, Universitat Paderborn, Germany, and the Plenoptic Function Sylvie Menezo, CEA-LETI, France, Providing Silicon- Quantum Information Processing with Photon Photonic Transceivers with an Efficient Laser Denis Pelli, New York Univ., USA, Visual Sensitivity Temporal Modes and Object Recognition Source: Where does “III-V/Silicon Heterogeneous Integration” Stand? Jelena Vuckovic, Stanford Univ., USA, Quantum Andrew Beau Watson, NASA, USA, Fourier, Gabor, Nanophotonics: From Inverse Design to Peter O’Brien, Tyndall Institute, Ireland, Development Reichardt, Hilbert: Guides on the Path to a Model Implementations of Human Motion Perception of Integrated Photonic Packaging Standards and Foundry Capabilities David Williams, Univ. of Rochester, USA, Emerging Ocular Applications of Wavefront Correction

18 FiO/LS 2016 • 16–21 October 2016 Special Events

Science Educators Day (EDAY) 2016 Women of Light, a Special Program for join your colleagues for a networking reception to Sunday, 16 October, 13:30–16:30 Women in Optics hosted by WiSTEE discuss ways the optics and photonics community can Grand Ballroom A-C, Hyatt Regency Rochester CONNECT improve diversity and inclusion. We encourage you to attend this program to learn what OSA is doing to Monday, 17 October, 11:00–17:00 The Optical Society Foundation (OSAF) in partnership improve the experience of underrepresented mem- Grand Ballroom F-G, Hyatt Regency Rochester with the American Association of Physics Teach- bers and support your colleagues as we continue this ers (AAPT) and The Optical Society (OSA) Roches- WiSTEE Connect is an organization which serves to important conversation. First 50 attendees will receive ter Local Section are hosting a special community connect female students, faculty members, and engi- a printed copy of APS’s LGBT Report. outreach program and training for K-12 educators! neers in Science, Technology, Engineering, and Entre- This session will focus on light and color through fun, preneurship (STEE) from regional universities and hands-on, and even *edible* science experiences. Make Optics Career Roundtable private companies in upstate New York. The vision Monday, 17 October 2016, 17:00–18:00 Special Events • Learn about the components of white light of WiSTEE Connect is to promote women leadership Grand Ballroom E, Hyatt Regency Rochester with a “Rainbow Peephole,” how some in STEE and assist women involved in these areas to animals see patterns invisible to the human gain regional and/or global connections and recog- Hosted by the OSA Opti- eye with “Magic Stripes,” and how materials nition. This organization helps to bridge the gap cal Fabrication and Testing can change color with the “Magic Patch.” between science and entrepreneurship while provid- Technical Group, this event ing a forum though which women in these fields may will provide students and recent graduates with the • Learn about color absorption and reflection as learn, connect, and lead. opportunity to connect with experienced profession- we predict the colors of M&M’s under different als working in academia, industry and government colors of light and as we observe how light The overall goal of the “Women of Light” special roles. Contact [email protected] to register for this travels through colored gummy bears. session is to shine light upon women’s careers in career roundtable event. science, technology, engineering, mathematics, and • Learn about color transmission as we observe entrepreneurship, recruit women across career ranks FiO/LS Welcome Reception the world through filters made of Jell-O. and disciplines, and build a sustainable community Monday, 17 October, 18:30–20:30 of women in both academia and industry from which • Participants will walk away with a variety of Galleria, Riverside Court, and Empire Lobby resources for their students and multiple career growth, mobility, and leadership opportunities lesson plans appropriate for K-12. may be sought out. Get the FiO/LS 2016 conference off to a great start by attending the Welcome Reception. Meet with col- Diversity and Inclusion Program and leagues from around the world and enjoy light hors Student Leadership Conference Reception: A Look at the LGBT Climate in d’oeuvres. This event is complimentary for FiO/LS Technical attendeees only. Non-technical attendees (Invitation only) Physics Monday, 17 October, 07:00–17:00 and guest tickets are available for $75 USD each. Monday, 17 October, 17:00–18:00 Grand Ballroom, Holiday Inn Rochester Downtown Grand Ballroom A-B, Hyatt Regency Rochester Sponsored by The OSA Student Leadership Conference (SLC) at FiO/LS brings together chapter officers from around the globe each year to network amongst their peers and to learn more about successful chapter management and careers in optics and photonics. This year’s Speaker: Ramon Barthelemy, American Institute of event will feature professional development, chapter Physics Statistical Research Center, USA management and education outreach programming. Please join Barthelemy as he shares highlights from the 2016 American Physical Society’s (APS) LGBT Climate in Physics Report. Following the presentation

FiO/LS 2016 • 16–21 October 2016 19 Optics in Digital Systems Technical Group OSA Fellow Members Lunch Photonics Clambake 2016 Networking Breakfast (Advance Registration Required) (Ticket Required) Tuesday, 18 October 2016, 07:30–08:30 Tuesday, 18 October, 12:00–13:15 Tuesday, 18 October, 17:30–20:30 Genesee Suite G, Radisson Rochester Riverside Grand Ballroom A-C, Hyatt Regency Rochester Grand Ballroom, Hyatt Regency Rochester Members of the OSA Optics OSA Fellow Members are invited to join their col- The Photonics Clambake is a melting pot of optics in Digital System Technical leagues for lunch. Advance registration is required. & photonics professionals who gather to enjoy one Group are invited to join us of the industry’s premier networking events while for a networking breakfast on Tuesday morning. The OSA Members, Family and Friends Tour – relaxing with refreshing beverages, great food and event will provide an opportunity to connect with fel- Susan B. Anthony Museum & House lots of clams. low attendees who share an interest in this field and (Advance Registration Required) Reservations and payments must be made in to learn more about this technical group. An RSVP is Tuesday, 18 October, 13:45–16:00 advance, no payments will be accepted at the door. required for this technical group event as breakfast will be provided. Contact [email protected] to OSA members and their families are welcome to Questions? Contact Mike Naselaris of Sydor Optics, register, pending availability. attend a 90-minute tour of the National Susan B. Inc. at [email protected] or +1.585.271.7300. Anthony Museum & House, which is the home of Polarization Technical Group Special Talks the legendary American women’s rights leader dur- Optics & Energy: Reflections on the Past Tuesday, 18 October, 12:00–13:30 ing the most politically active period of her life. The and Lighting the Future home was the headquarters of the National American Genesee Suite G, Radisson Rochester Riverside Tuesday, 18 October, 18:00–19:00 Woman Suffrage Association when Susan B. Anthony Organized by the OSA Genesee Suite F, Radisson Riverside Rochester Special Events was its president. Come learn how she and fellow suf- Polarization Technical fragists changed history for women’s rights. Join the OSA Optics for Group, this event will Energy Technical Group Shuttle transportation will depart from the Rochester feature a series of special talks by three high impact for this special event Convention Center at 13:45 and guests will return at speakers working in this field. Join us to hear about highlighting the major milestones of the optics and 16:00. our speakers’ recent research and discuss advances energy partnership through the last century. Visionar- in the field of polarization over lunch. An RSVP is ies in the field will be invited to share their thoughts required for this technical group event as lunch will be Meet the OSA Editors’ Reception and provide insight into the future of energy-related provided. Contact [email protected] to register, Tuesday, 18 October, 15:30–16:30 research and applications. Brief presentations will be pending availability. Empire Lobby followed by informal discussions and networking over Join OSA Publishing’s Journal Editors for conversation refreshments. Optical Material Studies Technical Group and refreshments. The Editors welcome your ques- Special Talk tions, concerns, and ideas for any of OSA’s Journals. OSA Student Member Party Tuesday, 18 October 2016, 12:00–13:30 Topics that may be covered include best practices Tuesday, 18 October, 19:00–22:00 Grand Ballroom D, Radisson Riverside Rochester when submitting a manuscript; elements of a useful Grand Ballroom, Holiday Inn Rochester Downtown manuscript review; criteria editors look for in sub- Join the OSA Optical OSA Student Members who are full technical regis- mitted manuscripts; and how to propose a Feature Material Studies Technical trants of FiO/LS are invited to attend the OSA Stu- Issue topic for publication in an OSA Journal. All are Group for a special talk dent Member Party. This birthday party will celebrate welcome. focused on photonics and optical materials. Dr. the next 100 years of leaders in the society with food, Michal Lipson of Columbia University will by the drinks and entertainment. featured speaker. An RSVP is required for this technical group event as lunch will be provided. Contact [email protected] to register, pending availability.

20 FiO/LS 2016 • 16–21 October 2016 Optics Alumni Networking Reception Glass Art Contest & Auction Meet the APS Journal Editors Reception Tuesday, 18 October, 19:00–22:00 Wednesday, 19 October, 09:30–16:00 Wednesday, 19 October, 15:30–17:00 Riverside Ballroom and Lounge, Radisson Riverside Thursday, 20 October, 09:30–14:00 Riverside Court Rochester Empire Hall The Institute of Optics, University of Rochester; The Hosted by the OSA Rochester Section College of Optical Sciences, University of Arizona; and the OSA Foundation The College of Optics & Photonics, University of Optical fabricators and glass artists will showcase Central Florida; Rochester Institute of Technology; their unique approaches to the design and manufac- The Editors of the APS journals invite you to join them and Stanford Photonics Research Center, Stanford ture of glass artwork. Pieces will be displayed in the for conversation and light refreshments. The Editors University, are honored to host our alumni and invited Frontiers in Optics Exhibition Hall, 19–20 October. All will be available to answer questions, hear your ideas, friends for a reception in conjunction with OSA FiO. attendees are invited to vote for their favorite piece and discuss any comments about the journals. All are Remarks from Optics Leaders will be featured at 8 in the contest, and several of the pieces are available welcome. We hope you will be able to join us. PM, including Xi-Cheng Zhang, Thomas Koch, Bahaa

for auction. Proceeds will go to the OSA Rochester Special Events Saleh and Thomas Baer. Section to support the Optics Suitecase and the OSA OIDA Member and Exhibitor Invitation only; registration is required. Foundation to support the Explore Optics Kit. Appreciation Reception (OIDA Members and Exhibitors Only) AIM Photonics Northeast Supply Environmental Sensing Technical Group Wednesday, 19 October, 16:00–17:00 Conference (NESCO) Special Talk Empire Hall Wednesday, 19 October, 08:00–17:00 Wednesday, 19 October, 12:00–13:00 Hyatt Regency Rochester, Grand Ballroom Salons A-D Genesee Suite G, Radisson Hotel Rochester Riverside Sponsored by The AIM Photonics Northeast Supply Conference Join the OSA Environmental (NESCO) provides a stage for established Photonics Sensing Technical Group supply chain companies, new and emerging innova- for a special talk focused Exhibitors, finish up your first day and come relax and tors, industry leaders, strategic investors, and venture on open-path sensing and the application of UAVs mingle with your colleagues. Join us in the exhibit hall capitalists to discuss the needs and requirements in environmental sensing. Dr. Azer Yalin of Colorado immediately following the close of the show for some of the industry’s future growth. Participants will gain State University will be the featured speaker. An RSVP food and beverages sponsored by OSA Industry insights into technology, capital, partnership, and col- is required for this technical group event as lunch will Development Associates. Join OSA and discover the laboration strategies necessary for mutual success. be provided. Contact [email protected] to regis- benefits of Industry Membership. OSA can help cor- ter, pending availability. porations optimize product development resources Who should attend? and reduce time to market by giving professionals access to quality information, quality interactions and • Entrepreneurs involved or interested in Student Chapter Competition Photonics innovation premium opportunities for collaboration. Join today! Wednesday, 19 October, 14:00–16:00 Contact [email protected] or +1.202.416.1474 for more • Emerging Optics and Photonics companies Empire Hall information. seeking to network with technology partners and investors OSA challenges its student chapters to an annual competition where they showcase their unique • Investment professionals from the angel, and innovative skills with youth education outreach venture, corporate and institutional demonstrations. Each competing chapter will use the communities OSA Foundation & LASER Classroom Explore Optics • R&D, purchasing, supply chain managers, Kit and any easily obtained items to create a new and manufacturing senior executives from the demonstration that is not already a part of these kits. Photonics industry Competitors will have their sights set on three cash Questions? Please contact Frank Tolic at prizes of up to $500, so it’s a show you don’t want to [email protected] miss.

FiO/LS 2016 • 16–21 October 2016 21 Division of Laser Science Annual Business Nonmembers who are not planning to attend as a Meeting Technical registrant can register for the free Exhibit Wednesday, 19 October, 17:00–18:00 Hall Only option then select the option to purchase a Genesee Suite F, Radisson Rochester Riverside BASH ticket for $100 USD. All members and interested parties are invited to Additional guest BASH tickets are available for $100 attend the annual business meeting of the Division USD each. of Laser Science (DLS). The DLS officers will report on the activities of the past year and on plans for the OSA Light the Future Speaker Series future. Questions will be taken from the floor. This featuring Michio Kaku and Nobel is your opportunity to help define the operations of Laureates the DLS and the LS Conference. The Carl E. Ander- Thursday, 20 October, 11:00–12:30 son Dissertation award will also be presented at this Lilac Ballroom meeting. This event will feature Michio Kaku, futurist and OSA Annual Business Meeting theoretical physicist, City College of New York, with Wednesday, 19 October, 17:00–7:45 Sir Peter L. Knight, emeritus professor, Imperial Regency Ballroom C, Hyatt Regency Rochester College, London, OSA Fellow, 2004 President. Learn more about OSA and join the OSA Board of Kaku’s talk “Optics of the Future: Exploring the Directors for the Society’s annual business meeting. Universe and the Brain” will be followed by a discus- Special Events An update on the Society’s 2015 activities will be sion featuring a panel of Nobel Laureates including presented and the results of the Board of Directors Roy Glauber, Nicolaas Bloembergen, Robert F. Curl, election will be announced. John L. Hall, W.E. Moerner, William D. Phillips and David J. Wineland. OSA 100 Year BASH Wednesday, 19 October, 18:30–21:30 VIP Industry Leaders Networking Event: The Sibley Building, 228 East Main Street, Rochester, Connecting Corporate Executives, Young New York Professionals & Students Thursday, 20 October, 12:30–14:00 Grand Ballroom C, Hyatt Regency Rochester This session brings together Industry Executives to In celebration of the OSA Centennial, join OSA in share their business experience with Young Profes- acknowledging the innovators and inventions that sionals, Recent Graduates and Students – how they inspire the future. This reception is sure to be a high started their careers, lessons learned and using their point in a year of celebration. We’ve waited a century degree in an executive position. Informal network- for this, and we want you to be a part of it! ing during lunch is followed by a transition to “speed Entry is free for registered attendees of Frontiers meetings” – brief, small-group visits with each execu- in Optics. tive to discuss industry trends or career topics. OSA Members who are not planning to attend as a Sponsored by Technical registrant can register for the free Exhibit Hall Only option and receive complimentary entry to the party.

22 FiO/LS 2016 • 16–21 October 2016 Exhibition Information

Visit the Frontiers in Optics 2016 Exhibit in Empire E-Posters Hall and get a glimpse of the latest optical innova- Wednesday, 19 October, 14:30–16:00 tions! The FiO 2016 exhibit floor will feature compa- Thursday, 20 October, 09:30–11:00 nies representing a broad range of the best products Empire Hall and applications in the optics and photonics industry. Don’t miss this opportunity to learn about new As a new feature of the 2016 FiO/LS Meeting, we have offered selected presenters the opportunity to present products, find technical and business solutions and their paper as an E-poster. Like a conventional poster, an e-poster will convey an author’s introduction, moti- gain the most up-to-date market perspective of your vation, results, and conclusions, on one screen. However, e-posters will provide the author with the option to industry. There is no charge to attend the exhibit—it’s digitally bring up supplemental details for deeper discussion. E-posters will be presented in the Exhibit Hall open to all registered attendees! (Empire Hall) during the two Joint Poster sessions. Each author selected for an E-poster will be given 45 minutes to present an E-poster. The remaining 45 minutes, the author will present their traditional poster within their designated poster slot. Please find a schedule of presentation times below. Exhibit Hours Wednesday, 19 October, 09:30–16:00 Joint Poster Session I E-Poster Presentation Times Thursday, 20 October 09:30–14:00 Wednesday, 19 October, 14:30–16:00 Empire Hall Screen 1 Screen 2 Screen 3 Screen 4 Screen 5 Exhibit Hall Unopposed Exhibit-Only Times 14:30– 15:15 JW4A.117 JW4A.49 FW4A.196 JW4A.43 JW4A.83 Wednesday, 19 October 09:30–10:30 12:00–13:00 15:15–16:00 JW4A.106 JW4A.9 JW4A.158 JW4A.132 14:30–16:00

Thursday, 20 October 09:30–11:00 Joint Poster Session II E-Poster Presentation Times Exhibit Information 12:30–14:00 Thursday, 20 October, 09:30–11:00 Screen 1 Screen 2 Screen 3 Screen 4 Screen 5 Joint FiO/LS Poster Sessions 09:30–10:15 JTh2A.131 JTh2A.198 JTh2A.78 JTh2A.74 JTh2A.99 Wednesday, 19 October 14:30–16:00 Thursday, 20 October 09:30–11:00 10:15–11:00 JTh2A.104 JTh2A.57 JTh2A.64 Empire Hall Poster presentations offer an effective way to communicate new research findings and provide an opportunity for lively and detailed discussion between presenters and interested viewers. Make sure to visit the poster sessions in the Exhibit Hall to see the more than 390 posters scheduled for presentation.

FiO/LS 2016 • 16–21 October 2016 23 FiO 2016 Participating Companies: (as of August 29, 2016) 4D Technology Corporation MegaWatt Lasers Toptica Photonics, Inc. American Institute of Physics Menlo Systems, Inc. TRIOPTICS USA Apollo Optical Systems, LLC Metrology Concepts, LLC UltraFast Innovations Applied Image, Inc. New Scale Technologies, Inc. United Lens Co, Inc. Asphericon Newport Corporation University of Arizona, College of Optics Axiom Optics NiCoForm, Inc. University of Central Florida, CREOL Bayside Photonics, Inc. Nufern Wiley Bristol Instruments, Inc. Ophir-Spiricon, LLC Wordingham Technologies Chroma Technology Corp. Optikos Corporation Wuhan National Lab for Optoelectronics Class 5 Photonics Optimax Systems, Inc. Xiamen Freeform Optical Technology Co., Ltd. ComTec Solutions OptiPro Systems Xonox Technology GmbH Daheng New Epoch Technology, Inc. OPTOCRAFT GmbH Zygo Corporation De Gruyter OSA Energetiq Technology, Inc. OSA Centennial Fianium, Inc. OSA Foundation Future Photon Initiative PHASICS Corp. Glass Fab, Inc. Photonic Cleaning Technologies G-S Plastic Optics Photonics Media/Laurin Publishing Hamamatsu Corporation Precision Optical Transceivers, Inc. Imagine Optic, Inc. QED Technologies International, Inc. Exhibit Information IOP Publishing Ltd. RPC Photonics Inrad Optics SPIE: The Intl Society for Optics Iridian Spectral Technologies Springer Nature Jasper Display Corporation Sydor Optics, Inc. Laser Focus World Synopsys, Inc. Learning Glass Solutions Syntec Optics LEUKOS The Institute of Optics, University of Rochester Mahr-ESDI Thorlabs

24 FiO/LS 2016 • 16–21 October 2016 FiO/LS Committee Thanks to the technical program committee members! Your time and efforts are appreciated! Frontiers in Optics General Chairs Carlos Lopez Mariscal, Naval Research Laboratory, Lukas Chrostowski, University of British Columbia, Scott Carney, University of Illinois at Urbana- USA Canada Champaign, USA Jie Qiao, Rochester Institute of Technology, USA Po Dong, Alcatel-Lucent Bell Labs, USA Urs Utzinger, University of Arizona, USA Shivanand, Intel, USA Sasan Fathpour, University of Central Florida, CREOL, Laura Sinclair, NIST, USA USA Laszlo Veisz, Max Planck Institute for Quantum Optics, Christian Grillet, CNRS Ecole Centrale de Lyon, Frontiers in Optics Program Chairs Germany France Chris Dainty, University College London, UK Wei Guo, University of Massachusetts Lowell, USA Tom Brown, University of Rochester, USA FiO 3: Optics in Biology and Medicine Wolfram Pernice, Karlsruher Institut fur Technologie, Ling Fu, Wuhan National Lab for Optoelectronics, Elizabeth Hillman, Columbia University, USA, Germany China Subcommittee Chair Lin Zhu, Clemson University, USA J. Quincy Brown, Tulane University, USA Frontiers in Optics Subcommittees Irene Georgakoudi, Tufts University, USA FiO 6: Quantum Electronics Christine Hendon, Columbia University, USA Alexander V. Sergienko, Boston University, USA, FiO 1: Optical Design and Instrumentation Martin Leahy, National University of Ireland Galway, Subcommittee Chair Julie Bentley, University of Rochester, USA, Ireland Antonio Badolato, University of Rochester, USA Subcommittee Chair Jonathan (Teng-Chieh) Liu, University of Washington, Sara Ducci, University of Paris VII, France Rob Bates, FiveFocal LLC, USA USA Alexander Gaeta, Columbia University, USA Dewen Chang, Beijing Institute of Technology, China Junle Qu, Shenzhen University, China Nobuyuki Imoto, Osaka University, Japan Jessica DeGroote Nelson, Optimax, USA Gang Zheng, University of Toronto, Canada Gerd Leuchs, University of Erlangen Nuremberg, Groot Gregory, Synopsys, USA Germany FiO 4: Fiber Optics and Optical Communications John Koshel, University of Arizona, USA Jian-Wei Pan, University of Science and Technology of Byoungho Lee, Seoul National University, South John Marciante, University of Rochester, USA, China, China Korea Subcommittee Chair Andrew Shields, Toshiba, UK Rongguang Liang, University of Arizona, USA Goëry Genty, Univ. of Tempere, Finland Mark Thompson, University of Bristol, UK Xinye Lou, Microsoft, USA John Ballato, Clemson University, USA Michael Vasilyev, University of Texas Arlington, USA Mike Marcus, Lumetrics, USA James Dailey, Vencore Labs, USA FiO 7: Vision and Color Simon Thibault, Laval University, Canada Iyad Dajani, Air Force Research Lab., USA Qiwen Zhan, University of Dayton, USA Fabrizio Di Pasquale, Scuola Superiore Sant’Anna, Susana Marcos, Consejo Sup Investigaciones Italy Cientificas, Spain, Subcommittee Chair FiO 2: Optical Sciences Diego Grosz, Instituto Balseiro, Argentina Melanie Campbell, University of Waterloo, Canada

Jake Bromage, University of Rochester, USA, Morten Ibsen, Univ. of Southampton, UK Stacy Choi, Ohio State University, USA FiO/LS Committees Subcommittee Chair Bill (Ping Piu) Kuo, University of California San Diego, Dan Neal, Advanced Medical Optics, USA Cameron Geddes, Lawrence Berkeley National Lab, USA Ram Sabesan, University of California Berkeley, USA USA, Subcommittee Chair Drew Maywar, RIT, USA Frank Schaeffel, University of Tubingen, Germany Selçuk Aktürk, Istanbul Technical University, Turkey Armando Pinto, Aveiro University, Portugal Duje Tadin, University of Rochester, USA Judith Dawes, Macquarie University, Australia Brian Vohnsen, University College Dublin, Ireland FiO 5: Integrated Photonics Greg Gbur, UNC Charlotte, USA Vicki Volbrecht, University of Colorado, USA Cristina Hernandez-Gomez, STFC Rutherford Stefan Preble, Rochester Institute of Technology, Yudong Zhang, Institute of Optics and Electronics, Appleton Laboratory, UK USA, Subcommittee Chair Chinese Academy of Sciences, China Igor Jovanovic, Pennsylvania State University, USA Paul Barclay, University of Calgary, Canada

FiO/LS 2016 • 16–21 October 2016 25 Laser Science Committee Explanation of Session Codes

Laser Science Co-Chairs Kevin J. Kubarych, University of Michigan, USA FTu1A.4 Edo Waks, University of Maryland, USA

Laser Science Subcommittee Chairs Session Designation 1. High Harmonic Generation from Solids to (alphabetically) Gases David Reis, Stanford Univ., USA, Subcommittee Number Chair Meeting Name F = Frontier in Optics (FiO) Series Number (presentation 2. Multiphoton Effects and High Resolution L = Laser Science (LS) 1 = First Series of Sessions order within Imaging J = Joint 2 = Second Series of Sessions the session) Robert Alfano, CCNY, USA, Subcommittee Chair 3. Advanced Nano-Photonic Lasers: Science and Day of the Week Application M = Monday Bo Zhen, MIT, USA, Subcommittee Chair Tu = Tuesday 4. Quantum Light Sources W = Wednesday Th = Thursday Nick Vamivakas, University of Rochester, USA, Subcommittee Chair 5. Integrated Quantum Photonics Dirk Englund, Columbia University, USA, Subcommittee Chair The first letter of the code designates the meeting (For instance, F = Frontiers in Optics, L = Laser Science, J=Joint). The second element denotes the day of the week (Monday = M, Tuesday = Tu, 6. Nonreciprocal and Topological Photonic Wednesday = W, Thursday = Th). The third element indicates the session series in that day (for instance, Devices 1 would denote the first parallel sessions in that day). Each day begins with the letter A in the fourth Mohammad Hafezi, University of Maryland, USA, element and continues alphabetically through a series of parallel sessions. The lettering then restarts with Subcommittee Chair each new series. The number on the end of the code (separated from the session code with a period) 7. Nano-Plasmonics for Spectroscopy and Imaging signals the position of the talk within the session (first, second, third, etc.). For example, a presentation Carlos Baiz, University of Texas, Austin, USA, coded FW1A.4 indicates that this paper is part of the Frontiers in Optics Meeting and is being presented Subcommittee Chair on Wednesday (W) in the first series of sessions (1), and is the first parallel session (A) in that series and 8. Advances in X-ray and XUV Laser Science and the fourth paper (4) presented in that session. Applications Christopher Milne, Paul Scherer Inst, USA, Subcommittee Chair FiO/LS Committees

26 FiO/LS 2016 • 16–21 October 2016 Agenda of Sessions — Sunday, 16 October

13:30–16:30 Science Educator’s Day, Hyatt Regency Rochester, Grand Ballroom A-C

Monday, 17 October

07:00–17:00 OSA Annual Student Chapter Leadership (Invitation only), Holiday Inn Hotel Rochester, Grand Ballroom

11:00–17:00 Women of Light, a Special Program for Women in Optics hosted by WiSTEE CONNECT, Hyatt Regency Rochester, Grand Ballroom F-G

15:00–20:00 Registration, Galleria

17:00–18:00 Diversity & Inclusion Program and Reception: A Look at the LGBT Climate in Physics, Hyatt Regency Rochester, Grand Ballroom A-B

17:00–18:00 Make Optics Career Roundtable, Hyatt Regency Rochester, Grand Ballroom E Agenda of Sessions 18:30–20:30 FiO/LS Welcome Reception, Galleria, Riverside Court, and Empire Lobby

FiO/LS 2016 • 16–21 October 2016 27 Agenda of Sessions — Tuesday, 18 October

Grand Ballroom A Grand Ballroom B Grand Ballroom C Grand Ballroom D Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E (Radisson) (Radisson) (Radisson) (Radisson) 07:00–17:00 Registration, Galleria Registration, Galleria 07:30–08:30 Optics in Digital Systems Technical Group Networking Breakfast, Radisson Rochester, Riverside, Genessee Suite G Optics in Digital Systems Technical Group Networking Breakfast, Radisson Rochester, Riverside, Genessee Suite G 08:00–10:00 FTu1A • Symposium on 100 FTu1B • Symposium on FTu1C • Laser-Plasma FTu1D • Silicon Photonics I LTu1E • Carl E. Anderson Award FTu1F • Three-Dimensional FTu1G • Quantum Effects LTu1H • Nanophotonics I FTu1I • Novel Light Years Optical Fabrication I 50th Anniversary of Low- Interactions and Acceleration for Outstanding Doctoroal Optical Design in Metamaterials Generation and Manipulation Loss Optical Fibers I Dissertation Session in Fiber Devices I 10:00–10:30 Coffee Break, West Corridor and Skyway Lobby (Radisson) Coffee Break, West Corridor and Skyway Lobby (Radisson) 10:30–12:00 FTu2A • Symposium on 100 FTu2B • Symposium on 50th FTu2C • Laser-Matter Interactions FTu2D • Silicon Photonics II LTu2E • X-ray and XUV I FTu2F • Resolution and FTu2G • Optics and Photonics LTu2H • Multiphoton Effects I FTu2I • Novel Fiber Devices Years Optical Fabrication II Anniversary of Low-Loss Measuring Limits of Disordered Systems (ends at 11:30) Optical Fibers II 12:00–13:30 Lunch Break (on your own) Lunch Break (on your own) 12:00–13:30 Polarization Technical Group Special Talks, Radisson Rochester Riverside, Genesee Suite G Polarization Technical Group Special Talks, Radisson Rochester Riverside, Genesee Suite G 12:00–13:15 OSA Fellow Members Lunch (Advance Registration Required), Hyatt Regency Rochester, Grand Ballroom, A-C OSA Fellow Members Lunch (Advance Registration Required), Hyatt Regency Rochester, Grand Ballroom, A-C 12:00–13:30 Optical Material Studies Technical Group Special Talk, Radisson Riverside Rochester, Grand Ballroom B Optical Material Studies Technical Group Special Talk, Radisson Riverside Rochester, Grand Ballroom B 12:15–14:55 LTu2J • Laser Science Symposium on Undergraduate Research Poster Session, Riverside Court LTu2J • Laser Science Symposium on Undergraduate Research Poster Session, Riverside Court 13:30–15:30 FTu3A • Symposium on 100 Years FTu3B • Symposium on 50th FTu3C • Ultrafast and THz Souces FTu3D • Plasmonic and LTu3E • Laser Science Symposium FTu3F • Optical Properties FTu3G • Integrated LTu3H • Quantum Light Sources I FTu3I • Novel Light Optical Fabrication III Anniversary of Low-Loss Photonic Crystal Devices on Undergraduate Research I of Materials Quantum Optics (ends at 15:00) Generation and Manipulation (ends at 14:30) Optical Fibers III (15:00–16:30) in Fiber Devices II ______FTu4A • Tutorial: Bill Casserly (begins at 14:45) 13:45–16:00 OSA Members, Family and Friends Tour – Susan B. Anthony Museum & House, Shuttle transportation will depart from the Hyatt Regency Rochester at 13:45 OSA Members, Family and Friends Tour – Susan B. Anthony Museum & House, Shuttle transportation will depart from the Hyatt Regency Rochester at 13:45 15:30–16:00 Coffee Break, West Corridor and Skyway Lobby (Radisson) Coffee Break, West Corridor and Skyway Lobby (Radisson)

Agenda of Sessions 15:30–16:30 Meet the OSA Editors’ Reception, Empire Lobby Meet the OSA Editors’ Reception, Empire Lobby 16:00–18:00 FTu5A • Optics in FTu5B • Laser Material Processing FTu5C • Frequency Combs and FTu5D • Mid-Infrared LTu5E • Laser Science Symposium LTu5F • X-ray and XUV II FTu5G • Nonlinear Optics in FTu5H • Nano-Plasmonics FTu5I • Novel Light Consumer Electronics High Harmonic Generation Integrated Photonics on Undergraduate Research II Micro/Nano-Optical Structures I for Spectroscopy Generation and Manipulation (ends at 17:30) (ends at 17:45) (starts at 16:45) in Fiber Devices III 17:30–20:30 Photonics Clambake 2016 (ticket required), Hyatt Regency Rochester, Grand Ballroom Photonics Clambake 2016 (ticket required), Hyatt Regency Rochester, Grand Ballroom 18:00–19:00 Optics & Energy: Reflections on the Past and Lighting the Future, Radisson Rochester Riverside, Genesee Suite F Optics & Energy: Reflections on the Past and Lighting the Future, Radisson Rochester Riverside, Genesee Suite F 19:00–22:00 OSA Student Member Party, Holiday Inn Hotel Rochester, Grand Ballroom OSA Student Member Party, Holiday Inn Hotel Rochester, Grand Ballroom 19:00–22:00 Optics Alumni Networking Reception, Radisson Rochester Riverside, Riverview Ballroom and Lounge Optics Alumni Networking Reception, Radisson Rochester Riverside, Riverview Ballroom and Lounge

Key to Shading Frontiers in Optics Laser Science Joint

28 FiO/LS 2016 • 16–21 October 2016 Grand Ballroom A Grand Ballroom B Grand Ballroom C Grand Ballroom D Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E (Radisson) (Radisson) (Radisson) (Radisson) 07:00–17:00 Registration, Galleria Registration, Galleria 07:30–08:30 Optics in Digital Systems Technical Group Networking Breakfast, Radisson Rochester, Riverside, Genessee Suite G Optics in Digital Systems Technical Group Networking Breakfast, Radisson Rochester, Riverside, Genessee Suite G 08:00–10:00 FTu1A • Symposium on 100 FTu1B • Symposium on FTu1C • Laser-Plasma FTu1D • Silicon Photonics I LTu1E • Carl E. Anderson Award FTu1F • Three-Dimensional FTu1G • Quantum Effects LTu1H • Nanophotonics I FTu1I • Novel Light Years Optical Fabrication I 50th Anniversary of Low- Interactions and Acceleration for Outstanding Doctoroal Optical Design in Metamaterials Generation and Manipulation Loss Optical Fibers I Dissertation Session in Fiber Devices I 10:00–10:30 Coffee Break, West Corridor and Skyway Lobby (Radisson) Coffee Break, West Corridor and Skyway Lobby (Radisson) 10:30–12:00 FTu2A • Symposium on 100 FTu2B • Symposium on 50th FTu2C • Laser-Matter Interactions FTu2D • Silicon Photonics II LTu2E • X-ray and XUV I FTu2F • Resolution and FTu2G • Optics and Photonics LTu2H • Multiphoton Effects I FTu2I • Novel Fiber Devices Years Optical Fabrication II Anniversary of Low-Loss Measuring Limits of Disordered Systems (ends at 11:30) Optical Fibers II 12:00–13:30 Lunch Break (on your own) Lunch Break (on your own) 12:00–13:30 Polarization Technical Group Special Talks, Radisson Rochester Riverside, Genesee Suite G Polarization Technical Group Special Talks, Radisson Rochester Riverside, Genesee Suite G 12:00–13:15 OSA Fellow Members Lunch (Advance Registration Required), Hyatt Regency Rochester, Grand Ballroom, A-C OSA Fellow Members Lunch (Advance Registration Required), Hyatt Regency Rochester, Grand Ballroom, A-C 12:00–13:30 Optical Material Studies Technical Group Special Talk, Radisson Riverside Rochester, Grand Ballroom B Optical Material Studies Technical Group Special Talk, Radisson Riverside Rochester, Grand Ballroom B 12:15–14:55 LTu2J • Laser Science Symposium on Undergraduate Research Poster Session, Riverside Court LTu2J • Laser Science Symposium on Undergraduate Research Poster Session, Riverside Court 13:30–15:30 FTu3A • Symposium on 100 Years FTu3B • Symposium on 50th FTu3C • Ultrafast and THz Souces FTu3D • Plasmonic and LTu3E • Laser Science Symposium FTu3F • Optical Properties FTu3G • Integrated LTu3H • Quantum Light Sources I FTu3I • Novel Light Optical Fabrication III Anniversary of Low-Loss Photonic Crystal Devices on Undergraduate Research I of Materials Quantum Optics Generation and Manipulation

(ends at 15:00) Agenda of Sessions (ends at 14:30) Optical Fibers III (15:00–16:30) in Fiber Devices II ______FTu4A • Tutorial: Bill Casserly (begins at 14:45) 13:45–16:00 OSA Members, Family and Friends Tour – Susan B. Anthony Museum & House, Shuttle transportation will depart from the Hyatt Regency Rochester at 13:45 OSA Members, Family and Friends Tour – Susan B. Anthony Museum & House, Shuttle transportation will depart from the Hyatt Regency Rochester at 13:45 15:30–16:00 Coffee Break, West Corridor and Skyway Lobby (Radisson) Coffee Break, West Corridor and Skyway Lobby (Radisson) 15:30–16:30 Meet the OSA Editors’ Reception, Empire Lobby Meet the OSA Editors’ Reception, Empire Lobby 16:00–18:00 FTu5A • Optics in FTu5B • Laser Material Processing FTu5C • Frequency Combs and FTu5D • Mid-Infrared LTu5E • Laser Science Symposium LTu5F • X-ray and XUV II FTu5G • Nonlinear Optics in FTu5H • Nano-Plasmonics FTu5I • Novel Light Consumer Electronics High Harmonic Generation Integrated Photonics on Undergraduate Research II Micro/Nano-Optical Structures I for Spectroscopy Generation and Manipulation (ends at 17:30) (ends at 17:45) (starts at 16:45) in Fiber Devices III 17:30–20:30 Photonics Clambake 2016 (ticket required), Hyatt Regency Rochester, Grand Ballroom Photonics Clambake 2016 (ticket required), Hyatt Regency Rochester, Grand Ballroom 18:00–19:00 Optics & Energy: Reflections on the Past and Lighting the Future, Radisson Rochester Riverside, Genesee Suite F Optics & Energy: Reflections on the Past and Lighting the Future, Radisson Rochester Riverside, Genesee Suite F 19:00–22:00 OSA Student Member Party, Holiday Inn Hotel Rochester, Grand Ballroom OSA Student Member Party, Holiday Inn Hotel Rochester, Grand Ballroom 19:00–22:00 Optics Alumni Networking Reception, Radisson Rochester Riverside, Riverview Ballroom and Lounge Optics Alumni Networking Reception, Radisson Rochester Riverside, Riverview Ballroom and Lounge

FiO/LS 2016 • 16–21 October 2016 29 Agenda of Sessions — Wednesday, 19 October

Grand Ballroom A Grand Ballroom B Grand Ballroom C Grand Ballroom D Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E (Radisson) (Radisson) (Radisson) (Radisson) 07:00–18:00 Registration, Galleria Registration, Galleria 08:00–09:30 JW1A • Joint Plenary Session, Lilac Ballroom JW1A • Joint Plenary Session, Lilac Ballroom 08:00–17:00 AIM Photonics Northeast Supply Conference (NESCO), Hyatt Regency Rochester, Grand Ballroom A-D AIM Photonics Northeast Supply Conference (NESCO), Hyatt Regency Rochester, Grand Ballroom A-D 09:30–16:00 Exhibit Hall Open, Empire Hall Exhibit Hall Open, Empire Hall 09:30–16:00 Glass Art Contest, Empire Hall Glass Art Contest, Empire Hall 09:30–10:30 Unopposed Exhibit Only Time and Coffee Break, Empire Hall Unopposed Exhibit Only Time and Coffee Break, Empire Hall 10:30–12:00 FW2A • Novel Design Concepts for FW2B • Quantum Communications I FW2C • Biomedical Optics FW2D • Symposium on Mesoscopic FW2E • Exotic States FW2F • Optical Fibers FW2G • Symposium: FW2H • Adaptive Optics LW2I • Integrated Quantum Eye Correction and Vision Simulators I Optics of Disordered Media I and Applications I for Space Projects Tribute to Steve Jacobs I and Inferometry Photonics I (ends at 12:30) 12:00–13:00 Lunch Break (on your own) and Unopposed Exhibit Only Time, Empire Hall Lunch Break (on your own) and Unopposed Exhibit Only Time, Empire Hall 12:00–13:00 Environmental Sensing Technical Group Special Talk, Genesee Suite G, Radisson Hotel Rochester Riverside Environmental Sensing Technical Group Special Talk, Genesee Suite G, Radisson Hotel Rochester Riverside 13:00–14:30 FW3A • Novel Design Concepts for FW3B • Quantum Communications II FW3C • Diffuse Imaging and FW3D • Symposium on Mesoscopic FW3E • Plasmonics FW3F • Quantum Entanglement FW3G • Symposium: Tribute FW3H • Optical Design LW3I • Multiphoton Effects II Eye Correction and Vision Simulators II Optical Propertiesv Optics of Disordered Media II to Steve Jacobs II and GRIN Materials (ends at 14:00) (ends at 14:00) 14:00–16:00 Student Chaper Competition, Empire Hall Student Chaper Competition, Empire Hall 14:30–15:00 Coffee Break, Empire Hall Coffee Break, Empire Hall 14:30–16:00 JW4A • Joint Poster Session I and Unopposed Exhibit Only Time, Empire Hall (see page 23 for specific e-poster viewing times) JW4A • Joint Poster Session I and Unopposed Exhibit Only Time, Empire Hall (see page 23 for specific e-poster viewing times) 15:30–17:00 Meet the Editors of the APS Journals, Riverside Court Meet the Editors of the APS Journals, Riverside Court

Agenda of Sessions 16:00–17:00 OIDA Members and Exhibitor Appreciation Reception (OIDA members and exhibitors only), Empire Hall OIDA Members and Exhibitor Appreciation Reception (OIDA members and exhibitors only), Empire Hall 16:00–18:00 FW5A • Understanding FW5B • High Power Fiber FW5C • Optical Coherence FW5D • Integrated Photonics FW5E • Ultrafast Lasers FW5F • Nonlinear Optics in FW5G • Optical Fabrication FW5H • Freeform Design LW5I • Integrated Myopia Development Lasers and Beam Combining Tomography and Applications Micro/Nano-Optical Structures II and Metrology and Metrology Quantum Photonics II (ends at 17:30) (ends at 18:15) 17:00–17:45 OSA Annual Business Meeting, Hyatt Regency Rochester, Regency Ballroom C OSA Annual Business Meeting, Hyatt Regency Rochester, Regency Ballroom C 17:00–18:00 APS Division of Laser Science Annual Business Meeting, Radisson Hotel Rochester Riverside, Genesee Suite F APS Division of Laser Science Annual Business Meeting, Radisson Hotel Rochester Riverside, Genesee Suite F 18:30–21:30 OSA 100 Year BASH, The Sibley Building, 228 East Main Street, Rochester, New York OSA 100 Year BASH, The Sibley Building, 228 East Main Street, Rochester, New York

Key to Shading Frontiers in Optics Laser Science Joint

30 FiO/LS 2016 • 16–21 October 2016 Grand Ballroom A Grand Ballroom B Grand Ballroom C Grand Ballroom D Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E (Radisson) (Radisson) (Radisson) (Radisson) 07:00–18:00 Registration, Galleria Registration, Galleria 08:00–09:30 JW1A • Joint Plenary Session, Lilac Ballroom JW1A • Joint Plenary Session, Lilac Ballroom 08:00–17:00 AIM Photonics Northeast Supply Conference (NESCO), Hyatt Regency Rochester, Grand Ballroom A-D AIM Photonics Northeast Supply Conference (NESCO), Hyatt Regency Rochester, Grand Ballroom A-D 09:30–16:00 Exhibit Hall Open, Empire Hall Exhibit Hall Open, Empire Hall 09:30–16:00 Glass Art Contest, Empire Hall Glass Art Contest, Empire Hall 09:30–10:30 Unopposed Exhibit Only Time and Coffee Break, Empire Hall Unopposed Exhibit Only Time and Coffee Break, Empire Hall 10:30–12:00 FW2A • Novel Design Concepts for FW2B • Quantum Communications I FW2C • Biomedical Optics FW2D • Symposium on Mesoscopic FW2E • Exotic States FW2F • Optical Fibers FW2G • Symposium: FW2H • Adaptive Optics LW2I • Integrated Quantum Eye Correction and Vision Simulators I Optics of Disordered Media I and Applications I for Space Projects Tribute to Steve Jacobs I and Inferometry Photonics I (ends at 12:30) 12:00–13:00 Lunch Break (on your own) and Unopposed Exhibit Only Time, Empire Hall Lunch Break (on your own) and Unopposed Exhibit Only Time, Empire Hall 12:00–13:00 Environmental Sensing Technical Group Special Talk, Genesee Suite G, Radisson Hotel Rochester Riverside Environmental Sensing Technical Group Special Talk, Genesee Suite G, Radisson Hotel Rochester Riverside 13:00–14:30 FW3A • Novel Design Concepts for FW3B • Quantum Communications II FW3C • Diffuse Imaging and FW3D • Symposium on Mesoscopic FW3E • Plasmonics FW3F • Quantum Entanglement FW3G • Symposium: Tribute FW3H • Optical Design LW3I • Multiphoton Effects II Eye Correction and Vision Simulators II Optical Propertiesv Optics of Disordered Media II to Steve Jacobs II and GRIN Materials

(ends at 14:00) (ends at 14:00) Agenda of Sessions 14:00–16:00 Student Chaper Competition, Empire Hall Student Chaper Competition, Empire Hall 14:30–15:00 Coffee Break, Empire Hall Coffee Break, Empire Hall 14:30–16:00 JW4A • Joint Poster Session I and Unopposed Exhibit Only Time, Empire Hall (see page 23 for specific e-poster viewing times) JW4A • Joint Poster Session I and Unopposed Exhibit Only Time, Empire Hall (see page 23 for specific e-poster viewing times) 15:30–17:00 Meet the Editors of the APS Journals, Riverside Court Meet the Editors of the APS Journals, Riverside Court 16:00–17:00 OIDA Members and Exhibitor Appreciation Reception (OIDA members and exhibitors only), Empire Hall OIDA Members and Exhibitor Appreciation Reception (OIDA members and exhibitors only), Empire Hall 16:00–18:00 FW5A • Understanding FW5B • High Power Fiber FW5C • Optical Coherence FW5D • Integrated Photonics FW5E • Ultrafast Lasers FW5F • Nonlinear Optics in FW5G • Optical Fabrication FW5H • Freeform Design LW5I • Integrated Myopia Development Lasers and Beam Combining Tomography and Applications Micro/Nano-Optical Structures II and Metrology and Metrology Quantum Photonics II (ends at 17:30) (ends at 18:15) 17:00–17:45 OSA Annual Business Meeting, Hyatt Regency Rochester, Regency Ballroom C OSA Annual Business Meeting, Hyatt Regency Rochester, Regency Ballroom C 17:00–18:00 APS Division of Laser Science Annual Business Meeting, Radisson Hotel Rochester Riverside, Genesee Suite F APS Division of Laser Science Annual Business Meeting, Radisson Hotel Rochester Riverside, Genesee Suite F 18:30–21:30 OSA 100 Year BASH, The Sibley Building, 228 East Main Street, Rochester, New York OSA 100 Year BASH, The Sibley Building, 228 East Main Street, Rochester, New York

FiO/LS 2016 • 16–21 October 2016 31 Agenda of Sessions — Thursday, 20 October

Grand Ballroom A Grand Ballroom B Grand Ballroom C Grand Ballroom D Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E (Radisson) (Radisson) (Radisson) (Radisson)

07:00–17:00 Registration, Galleria Registration, Galleria

08:00–09:30 JTh1A • Joint Plenary Session, Lilac Ballroom JTh1A • Joint Plenary Session, Lilac Ballroom

09:30–14:00 Exhibits Open, Empire Hall Exhibits Open, Empire Hall

09:30–14:00 Glass Art Contest, Empire Hall Glass Art Contest, Empire Hall

09:30–10:00 Coffee Break, Empire Hall Coffee Break, Empire Hall

09:30–11:00 JTh2A • Joint Poster Session II and Unopposed Exhibit Only Time, Empire Hall (see page 23 for specific e-poster viewing times) JTh2A • Joint Poster Session II and Unopposed Exhibit Only Time, Empire Hall (see page 23 for specific e-poster viewing times)

11:00–12:30 JTh3A • OSA Light the Future Speaker Series featuring Michio Kaku and Nobel Laureates, Lilac Ballroom JTh3A • OSA Light the Future Speaker Series featuring Michio Kaku and Nobel Laureates, Lilac Ballroom

12:30–14:00 Free Lunch (provided by OSA), Exhibit Hall, Empire Hall Free Lunch (provided by OSA), Exhibit Hall, Empire Hall

14:00–16:00 FTh4A • Symposium on Mid- FTh4B • Optical Vortices FTh4C • Computational Imaging I FTh4D • Optics Meets Neuroscience I FTh4E • High Capacity FTh4F • Quantum Communication FTh4G • Integrated FTh4H • Probing Ocular FTh4I • Symposium on 100 Years Infrared Fiber Sources I Optical Communications and Networking I Nonlinear Optics I Biomechanics with Imaging of Vision at OSA: Most Cited and Data Centers I Techniques / Novel Applications Vision Papers in OSA Journals of Femtosecond Lasers in Ophthalmology

16:00–16:30 Coffee Break, West Corridor and Skyway Lobby (Radisson) Coffee Break, West Corridor and Skyway Lobby (Radisson) Agenda of Sessions 16:30–18:30 FTh5A • Symposium on Mid- FTh5B • Optical Vortices, FTh5C • Computational Imaging II FTh5D • Optics Meets Neuroscience II FTh5E • High Capacity FTh5F • Quantum Communication FTh5G • Integrated LTh5H • Topological Photonics I LTh5I • High Harmonic Generation Infrared Fiber Sources II Polarization and Mode Shaping Optical Communications and Networking II Nonlinear Optics II and Data Centers II

Key to Shading Frontiers in Optics Laser Science Joint

32 FiO/LS 2016 • 16–21 October 2016 Grand Ballroom A Grand Ballroom B Grand Ballroom C Grand Ballroom D Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E (Radisson) (Radisson) (Radisson) (Radisson)

07:00–17:00 Registration, Galleria Registration, Galleria

08:00–09:30 JTh1A • Joint Plenary Session, Lilac Ballroom JTh1A • Joint Plenary Session, Lilac Ballroom

09:30–14:00 Exhibits Open, Empire Hall Exhibits Open, Empire Hall

09:30–14:00 Glass Art Contest, Empire Hall Glass Art Contest, Empire Hall

09:30–10:00 Coffee Break, Empire Hall Coffee Break, Empire Hall

12:30–14:00 Free Lunch (provided by OSA), Exhibit Hall, Empire Hall Free Lunch (provided by OSA), Exhibit Hall, Empire Hall

12:30–14:00 VIP Industry Leaders Networking Event: Connecting Corporate Executives, Young Professionals & Students, Hyatt Regency Rochester, Grand Ballroom B-C VIP Industry Leaders Networking Event: Connecting Corporate Executives, Young Professionals & Students, Hyatt Regency Rochester, Grand Ballroom B-C Agenda of Sessions 14:00–16:00 FTh4A • Symposium on Mid- FTh4B • Optical Vortices FTh4C • Computational Imaging I FTh4D • Optics Meets Neuroscience I FTh4E • High Capacity FTh4F • Quantum Communication FTh4G • Integrated FTh4H • Probing Ocular FTh4I • Symposium on 100 Years Infrared Fiber Sources I Optical Communications and Networking I Nonlinear Optics I Biomechanics with Imaging of Vision at OSA: Most Cited and Data Centers I Techniques / Novel Applications Vision Papers in OSA Journals of Femtosecond Lasers in Ophthalmology

16:00–16:30 Coffee Break, West Corridor and Skyway Lobby (Radisson) Coffee Break, West Corridor and Skyway Lobby (Radisson)

16:30–18:30 FTh5A • Symposium on Mid- FTh5B • Optical Vortices, FTh5C • Computational Imaging II FTh5D • Optics Meets Neuroscience II FTh5E • High Capacity FTh5F • Quantum Communication FTh5G • Integrated LTh5H • Topological Photonics I LTh5I • High Harmonic Generation Infrared Fiber Sources II Polarization and Mode Shaping Optical Communications and Networking II Nonlinear Optics II and Data Centers II

FiO/LS 2016 • 16–21 October 2016 33 Agenda of Sessions — Friday, 21 October

Grand Ballroom A Grand Ballroom B Grand Ballroom C Grand Ballroom D Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E (Radisson) (Radisson) (Radisson) (Radisson)

07:30–16:30 Registration, Galleria Registration, Galleria

08:00–10:00 FF1A • Imaging and Therapy FF1B • Optical Fiber Sensors I FF1C • Quantum Information FF1D • Quantum Optical Technologies FF1E • Symposium on Integrated FF1F • Strongly Confined FF1G • Wavefront Sensing and FF1H • General Optical Sciences I LF1I • Nanophotonics II Inside the Human Body Processing in Integrated Systems Photonic Manufacturing I Nanoscale Waveguides, Photonic Phase Retrieval Crystals and Resonator Devices (begins at 08:30)

10:00–10:30 Coffee Break, West Corridor and Skyway Lobby (Radisson) Coffee Break, West Corridor and Skyway Lobby (Radisson)

10:30–12:30 FF2A • Postdeadline Session I FF2B • Postdeadline Session II FF2C • Postdeadline Session III LF2D • General Laser Science I LF2E • General Laser Science II LF2F • Quantum Light Sources II LF2G • General Laser Science III LF2H • High Harmonic (begins at 10:45) Generation II

12:30–13:30 Lunch (on your own) Lunch (on your own)

13:30–15:30 FF3A • Advanced Microscopy FF3B • Optical Fiber Sensors II FF3C • Quantum Electronics I FF3D • Quantum Optical measurement FF3E • Symposium on Integrated FF3F • Ultrafast Dynamics FF3G • Polarization Control FF3H • General Optical Sciences II LF3I • X-ray and XUV III Methods and Applications and Quantum Technologies I Photonic Manufacturing II and laser Ion Acceleration and Measurements (ends at 14:30) ______FF4A • Symposium on Integrated Quantum Optics I (begins at 14:30)

15:30–16:00 Coffee Break, West Corridor and Skyway Lobby (Radisson) Coffee Break, West Corridor and Skyway Lobby (Radisson)

16:00–18:00 FF5A • In-vivo Spectroscopy, FF5B • Optical Manipulation, FF5C • Quantum Electronics II FF5D • Quantum Optical Measurement FF5E • Symposium on FF5F • Hybrid Integration FF5G • Beams and FF5H • Exotic States LF5I • Topological Photonics II Metabolism and Raman Processing and Applications and Quantum Technologies II Integrated Quantum Optics II (ends at 18:15) Optical Coherence and Applications II (ends at 17:30) Agenda of Sessions

Key to Shading Frontiers in Optics Laser Science Joint

34 FiO/LS 2016 • 16–21 October 2016 Grand Ballroom A Grand Ballroom B Grand Ballroom C Grand Ballroom D Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E (Radisson) (Radisson) (Radisson) (Radisson)

07:30–16:30 Registration, Galleria Registration, Galleria

10:00–10:30 Coffee Break, West Corridor and Skyway Lobby (Radisson) Coffee Break, West Corridor and Skyway Lobby (Radisson)

12:30–13:30 Lunch (on your own) Lunch (on your own)

FF4A • Symposium on Agenda of Sessions Integrated Quantum Optics I (begins at 14:30)

15:30–16:00 Coffee Break, West Corridor and Skyway Lobby (Radisson) Coffee Break, West Corridor and Skyway Lobby (Radisson)

FiO/LS 2016 • 16–21 October 2016 35 Tuesday, 18 October Instrumentation -AHistoricalLookBackI Optical Design,Fabrication,Testing, and FTu1A •Symposium on100Years of 08:00–10:00 36 C. Wyant Short HistoryofInterferometric OpticalMetrology, FTu1A.2 •08:30 ard Optical DesignsofNASATelescopes, FTu1A.1 •08:00 USA Presider: JannickRolland,Univ. ofRochester, optical designforms. with an emphasis on their science applications and resulting historical summary of NASA’s space telescopes is presented enhancements provided by lasersandcomputers. talk gives a short history of interferometric metrology and the was introduced the same year OSA was founded, 1916. This use of the Twyman-Green interferometer for optical metrology 1 ; Grand Ballroom A(Radisson) 1 brief A NASA Goddard SpaceFlightCenter, USA. 1 ; 1 Univ. ofArizona,CollOptSciences,USA. The Invited Invited

Follow @Opticalsociety onTwitter. 07:30–08:30 oeh . How M. Joseph Join theconversation. Use hashtag#FIO16 and #OSA100 James James

- Optics inDigitalSystemsTechnical Group NetworkingBreakfast, RadissonRochesterRiverside,GenesseeSuiteG small team at a British research laboratory. This is their story. a of work the frequencies”, optical for waveguides surface tion began with the pioneering publication: “Dielectric-fibre Keck Glass and Light: Enabling the Information Age, FTu1B.2 •08:30 worth The BirthofOpticalFiberCommunications, FTu1B.1 •08:00 USA Presider: Incorporated, AlanEvans;Corning Anniversary ofLowLossOpticalFibersI FTu1B •Symposium onthe50th 08:00–10:00 impact ofopticaltelecommunications. world-changing the and milestone, remarkable that revisit We’ll Age. Information the created – fiber optical low-loss syzygy of four inventions/breakthroughs – including Corning’s 1 ; Grand Ballroom B(Radisson) 1 ; 1 Consultant, USA. 1 Retired, UK. Fifty years ago the optical fiber revolu-

Invited Invited Forty-six years ago, a technological

FiO/LS 2016 07:00–17:00 Registration, Richard Ep- Richard Donald B.

• FiO 16–21 October 2016 practical machines. to forward path the and discussed be will plasmas in fields meter per gigavolt of tens excite that pulses laser intense physics and status of electron acceleration of electrons using the APS,IEEE,andAAAS. Achievement Award for the BELLA Project and is a Fellow of Secretary’sDOE 2014 the 2012, in Award Concepts erator Accel- Advanced the DOE, the from Award Lawrence E.O. received numerous awards including has most recently He the 2009 applications. and accelerators plasma driven laser of development the on focuses research main His 1991. in LBNL joined and UCLA from Ph.D. his obtained He LBNL. at Center Accelerator) Laser Lab (Berkeley BELLA the of tor Technology(ATAP)Physics Applied and Direcand - Division Biography: Leemans Wim is the Director of the Accelerator ser, La- PW-classBELLA the Using Acceleration Plasma Laser FTu1C.1 •08:00 Presider: To beAnnounced Photon Sources FTu1C •Laser-Plasma Acceleration and 08:00–10:00 E. Esarey Cameron G. Geddes Mittelberger E. Daniel Hann-Shin Mao Wim Leemans Wim Grand Ballroom C(Radisson) 1 ; 1 Lawrence Berkeley National Laboratory, USA.The Galleria 1 , Sven Steinke 1 , Anthony J. Gonsalves 1 , Jean-Luc Vay

Tutorial 1 , Carlo Benedetti Carlo , 1 , Csaba Toth

1 , Carl B. Schroeder 1 , Stepan Bulanov Stepan , 1 , Kei Nakamura 1 , Josst Daniels 1 , Eric 1 1 1 , , , 0.8dB penalty over a ~100nm bandwidth and all polarizations. with transmission peak -1.4dB show We interface. polymer nanophotonic waveguides through a mechanically with compliant fibers standard interfacing in performance improved USA; Gen. Div., AsahiGlassCo,Japan; Barwicz standard fibers and nanophotonic waveguides, A compliantpolymerinterfacewith1.4dBlossbetween FTu1D.2 •08:30 chal Lipson Photonics, Silicon Generation TechnologiesNext for FTu1D.1 •08:00 Lowell, USA Presider: Wei Guo;Univ. ofMassachusetts FTu1D •Silicon PhotonicsI 08:00–10:00 Jean-Francois Morissette Canada; new materials such as graphene for ultra high speed devices. with integration back-end and scaling bandwidth enabling multiplexing communications multi-mode include These photonics. silicon bandwidth high ultra for technologies Numata Fortier 2 Grand Ballroom D(Radisson) IBM Bromont, Canada; 2 , Nicolas Boyer Nicolas , 1 5 , Alexander Janta-Polczynski Alexander , , Swetha Kamlapurkar 5 e demonstrate WeIBM Research -Tokyo, Japan. 1 ; 1 Columbia Univ., USA. We have demonstrated Invited 2 ; 2,4 1 IBM TJWatson Research Center, , Bo Peng 1 , Sebastian Engelmann

3 AGC Electronics, Technol. 4 Universite deSherbrooke, 1

, Yoichi Taira 2 , Shotaro TakenobuShotaro , 1 , Hidetoshi Tymon. 1 , Paul Mi- 3 , Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E Tuesday, 18 October LS FiO LS FiO

07:00–17:00 Registration, Galleria

07:30–08:30 Optics in Digital Systems Technical Group Networking Breakfast, Radisson Rochester Riverside, Genessee Suite G

08:00–10:00 08:00–10:00 08:00–10:00 08:00–10:00 08:00–10:00 LTu1E • Carl E. Anderson Award FTu1F • Three-Dimensional FTu1G • Quantum Effects in LTu1H • Nanophotonics I FTu1I • Novel Light Generation for Outstanding Doctoroal Optical Structure Design, Metamaterials Presider: Bo Zhen; MIT, USA and Manipulation in Fiber Dissertation Award Session Fabrication and Nanopatterning Presider: Gerd Leuchs; Univ. Devices I Presider: Kristan L. Corwin, Kansas Presider: Jaime Cardenas, Univ. of Erlangen-Numberg, Germany Presider: Benjamin Wetzel; INRS - State Univ., USA Rochester, USA EMT, Canada

LTu1E.1 • 08:00 Invited FTu1F.1 • 08:00 Invited FTu1G.1 • 08:00 Invited LTu1H.1 • 08:00 Invited FTu1I.1 • 08:00 Tutorial Identifying and Using Recollision-Based High Reconfigurable Photonics Metasurfac- Nonlinear Metamaterial Nanophoton- Spatial Coherence Engineering of Lasers, Hui UV Generation in Silica Fibres, Yun Wang1, Harmonics From Bulk Semiconductors, Giulio es , Nikolay I. Zheludev1,2; 1ORC, Univ. of ics, Anatoly Zayats1; 1King’s College London, Cao1; 1Yale Univ., USA. We develop lasers with M.I.M. Abdul Khudus1, Francesco De Lucia1, Qi Vampa1; 1Univ. of Ottawa, Canada. In the Southampton, UK; 2CDPT/TPI/SPMS, Nanyang UK. Metamaterials and metasurfaces open up low spatial coherence to achieve speckle-free Sun1, Jing He1, Pier J. A. Sazio1, Rand Ismaeel1, generation of high harmonics from ZnO and Si Technological Univ., Singapore.The chang- opportunities to design the enhanced nonlinear imaging. We also invent a fast and efficient Martynas Beresna1, Peter Horak1, Gilberto crystals we find that “generalized recollisions” ing balance of forces at the nanoscale offers properties in a desired spectral range beyond method of switching the spatial coherence of a Brambilla1,2; 1Univ. of Southampton, UK; 2The between electrons and their holes dominate the opportunity to develop reconfigurable nonlinear response of the constituents. We laser for multimodality Future Manufacturing Hub, UK. The generation the emission, and show how they can be used. nanomembrane metamaterials in which ther- overview second and third-order nonlinearities microscopy. of UV light in solid core silica fibres has been mal, electromagnetic Coulomb, Lorentz and in plasmonic metamaterials. achieved using intermodal phase matched four Ampère forces can be used to control their wave mixing in optical fibre tapers or rare earth optical properties. doping with Gd.

LTu1E.2 • 08:30 Invited FTu1F.2 • 08:30 FTu1G.2 • 08:30 Invited LTu1H.2 • 08:30 Invited Power-scaling Attosecond Sources Using Ni-TaN Nanocomposite Absorber For Next- Photonic Hyperctystals. Evgenii E. Nari- InGaN/GaN Dot-in-Nanowire Lasers on Sili- Universal Scaling Principles for Nonlinear Generation Extreme Ultraviolet Lithogra- manov1; 1Purdue Univ., USA. Photonic con, Pallab K. Bhattacharya1; 1Univ. of Michigan, 1 1 1 Optical Processes in Gases, Christoph Heyl1,2, phy, Darrick Hay , Patrick Bagge , Ian Khaw , hypercrystals form a new universality class USA. The fabrication and characteristics of 2 3 3 H. Coudert-Alteirac1, M. Miranda1, M. Louisy1, Lei Sun , Obert Wood , Yulu Chen , Ryoung-Han of artificial optical media. These hyperbolic monolithic edge-emitting InGaN/GaN dot-in- 3 3 1 1 P. Rudawski1, F. Brizuela1, K. Kovacs3,4, V. Tosa3,4, Kim , Zhengqing Qi , Zhimin Shi ; Department metamaterials with a periodic spatial variation nanowire array diode lasers on (001)Si will be 2 E. Balogh4,5, K. Varju4,5, P. Johnsson1, A. of Physics, Univ. of South Florida, USA; Glo- of permittivity on subwavelength scale, combine presented. 3 Couairon6, C. L. Arnold1, A. L. Huillier1; 1Lund balFoundries Inc. , USA; GlobalFoundries Inc. the features of metamaterials and photonic Univ., Sweden; 2JILA, NIST, Univ. of Colorado, , USA. A thin Ni-TaN nano-composite absorber crystals. USA; 3National Inst. for R&D Isotopic and is studied for next-generation EUV lithography. Molecular Technologies, Romania; 4ELI-ALPS, We show that the performance is insensitive to Hungary; 5Dept. of Optics and Quantum the size and location of nano-particles, and that Biography: Gilberto Brambilla is a professor Electronics, Univ. of Szeged, Hungary; 6Centre such an absorber can greatly reduce HV bias. at the Optoelectronics Research Centre at de Physique Theorique, Ecole Polytechnique, the University of Southampton, where he has CNRS, France. Scaling attosecond sources been employed as a researcher since 2002. He to higher pulse energy and/or repetition rate obtained his MSc (Material Engineering) with can benefit many applications. We present a honours from Politecnico di Milano (Italy) and his scaling framework for nonlinear light-matter PhD degree in Optoelectronics from the ORC in interactions, applicable to attosecond pulse 2002. In 2007 he was awarded the prestigious generation and other nonlinear phenomena as Research Fellowship from the Royal Society. e.g. filamentation. He has been the director of the EPSRC Centre for Innovative Manufacturing in Photonics until 2015. As co-director for the Future Photonics Hub he has responsibility for the research on the platforms in the Hub.

FiO/LS 2016 • 16–21 October 2016 37 Tuesday, 18 October 38 Bruning Tropel, at Metrology and Optics Precision FTu1A.3 •09:00 Back I and Instrumentation-AHistoricalLook Optical Design,Fabrication,Testing, FTu1A •Symposiumon100Years of their impact on microelectronics, photonics and healthcare. applications of computers, lasers and microlithography, and early highlighting Rochester, in Tropel at metrology and optics precision of evolution the on perspective Grand Ballroom A(Radisson) — 1 ; Continued 1 hs ak s personal a is talk This Retired, USA. Corning, Invited

on H. John systems. transmission high-capacity and WDM areaof the in leaders networks. MSB has been widely. transmission ATR Bell Labs for are fibers the continuing optical low-loss produces and invents labs Bell MacChesney OpticalMaterials,USA. at Peet n Future, and Present Past, Bell Lab’s SeminalTesting toofOpticalFiberSystems: FTu1B.3 •09:00 Fibers I Anniversary ofLowLossOptical FTu1B •Symposiumonthe50th Grand Ballroom B(Radisson) — Continued Invited on MacChesney John

FiO/LS 2016 1 ; 1 John B. • FiO 16–21 October 2016 imaging ofinverse-Comptonscattered x-rays. spectroscopic employing technique novel a via performed electron beam transverse emittance, as well as its evolution, laser-wakefield-acceleratedof measurement first the report Seller Umstadter 10^3 laserphotonsperelectron. to close of strengthsscattering field the ultra-high and with multiphoton regime.The experimental results are consistent laser light is used to study Thomson scattering in the highly FTu1C.2 •08:45 ergy, En- Ponderamotive High with Event Recollision Single FTu1C.4 •09:15 Scattered X-rays, Beams withSpectroscopic ImagingofInverse-Compton- Electron Laser-Driven of Emittance Ultralow Measuring FTu1C.3 •09:00 tering, Thomsonscat- multiphoton of observation Experimental an octaveintheextreme ultraviolet. pulses, tuneable in energy by the carrier envelope phase over synthesize a sub-cycle pulse. It generates isolated attosecond interplay of nonlinear optics and spatio-temporal coupling to ig Zhang Ping Liu Cheng Liu Cheng Haden Daniel Photon Sources FTu1C •Laser-Plasma Accelerationand T J. Hammond Grand Ballroom C(Radisson) 2 , Donald P.Umstadter Donald , Wenchao YanWenchao 1 1 1 , Shouyuan Chen Shouyuan , , Shouyuan Chen Shouyuan , ; 1 1 ih power High Univ. ofNebraskaLincoln,USA. Mthw Veale Matthew , 1 Pn Zhang Ping , 1 rgr Golovin Grigory ; — 1 1 JAS Labs,U.Ottowa,USA. We use the , Grigory Golovin Grigory , Continued 1 1 1 Jn Zhang Jun , , Sudeep Banerjee Sudeep , 1 , Jun Zhang Jun , ; 1 2 UNL, USA; Mthw Wilson Matthew , 1 Sde Banerjee Sudeep , 1 , Colton Fruhling Colton , 1 1 Bohn Zhao Baozhen , , Baozhen Zhao Baozhen , 2 We We STFC, UK. 1 , Donald P.Donald , 2 Paul , 1 1 1 1 , , , , USA; than 10 pm/K thermal sensitivity. than 10pm/Kthermal less achieving while tolerance, error fabrication its increase to arms the of one in waveguide grating subwavelength with interferometer Mach-Zehnder athermal broadband a of validation experimental an present We Arab Emirates. Bristol, UK; in ourbestdesign. tuning and 130ps/mm/V for voltage tuning has been achieved wavelength for 140ps/mm of delay tunable A applications. line delay for waveguides grating silicon apodized of designs three investigated We Research Laboratory, USA. Jiang Apodized GratingforSiliconTunable DelayLines, FTu1D.5 •09:15 Range, Spectral Wide and Tolerance Error Fabrication Enhanced With Interferometer Photonics Silicon Mach-Zehnder Athermal Grating Subwavelength FTu1D.4 •09:00 Optimising Beam-Splitters, 60.5 dB Silicon Mach-Zehnder Interferometer using Self- FTu1D.3 •08:45 photonic quantum information applications. photonic quantuminformation splitters. This result paves the way for large-scale integrated beam- variable adjust to approach self-optimising a using high extinction MZI on a reconfigurable silicon photonic chip, Qiang Jaime P.Jaime Viegas Thompson G. Mark Xiaoqi Zhou FTu1D •SiliconPhotonicsI London, UK; Zhou 2 2 Grand Ballroom D(Radisson) Zarn . Huang R. Zhaoran , Sensors &Electron Devices Directorate, USArmy 1 1 , Jianwei Wang Sehn Anderson Stephen , 2 , Pete Shadbolt 2 4 Sun Yat-Sen Univ., China; Stanford Univ., USA. We demonstrate an ultra- 1 ; 1 Masdar Inst. of Science and Tech, United 1 Jrm L O’Brien L. Jeremy , 1 , Raffaele Santagati 1 ; 3 , Terry Rudolph 1 Callum M. Wilkes M. Callum Rensselaer PolytechnicInst., 1 Yug . Kim H. Young , — Continued 3 1 Imperial College, 1,4 , Stefano Paesani ; 3 1 , David Miller CQP, Univ. of eg Xing Peng 1 , Xiaogang , 1 Weimin , Lingjun 1 4 1 , , , Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E Tuesday, 18 October LS FiO LS FiO

LTu1E • Carl E. Anderson FTu1F • Three-Dimensional FTu1G • Quantum Effects in LTu1H • Nanophotonics I— FTu1I • Novel Light Generation Award for Outstanding Optical Structure Metamaterials—Continued Continued and Manipulation in Fiber Doctoroal Dissertation Award Design, Fabrication and Devices I—Continued Session—Continued Nanopatterning—Continued

FTu1F.3 • 08:45 Invited FTu1I.2 • 08:45 Inverse Methods and the Design of Sub- Mid-IR Supercontinuum up to 5.4 μm in a wavelength Scattering Elements for Super- 15 meter-long Fluoroindate Fiber, Jean- 1 1 resolution, Michael A. Fiddy1; 1Univ of North Christophe Gauthier , Vincent Fortin , Jean-Yves 2 2 2 Carolina at Charlotte, USA. Subwavelength- Carrée , Samuel Poulain , Marcel Poulain , 1 1 1 scale scatterers convert evanescent into Réal Vallée , Martin Bernier ; Universite Laval, 2 propagating waves. Nonlinear inverse scattering Canada; Le Verre Fluoré, France. We present algorithms may reveal these processes leading a simple approach for supercontinuum (SC) to superresolved images but they may be generation up to 5.4 μm using a low-loss replaced by propagating through designed fluoroindate fiber. It is pumped by an erbium- optical structures. doped fluoride fiber amplifier seeded with 400 ps pulses at 2.75 μm.

LTu1E.3 • 09:00 Invited FTu1G.3 • 09:00 LTu1H.3 • 09:00 Invited FTu1I.3 • 09:00 Quantum Information with Structured Trapped Ultracold Atoms Make Perfect Quan- Title to be Announced, Steven G. John- Formation of Cascading Solitons in Fiber 1 1 Light, Mohammad Mirhosseini1,2, O. S. Magana- tum Metamaterials, Pankaj K. Jha , Michael son1; 1Massachusetts Inst. of Technology, Amplifiers, Francisco Rodrigo Arteaga Sierra , 1 1 1 1 1 1 Loaiza2, M. N. O’Sullivan2, Brandon Rodenburg2, Mrejen , Jeongmin Kim , Chihhui Wu , Yuan USA. Abstract not available. Aku J. Antikainen , Govind P. Agrawal ; The Inst. 1 2 1 1 Zhimin Shi3, Mehul Malik2,4, M. P. Lavery5, Wang , Yuri Rostovtsev , Xiang Zhang ; Univ. of Optics, Univ. of Rochester, USA. We study 2 Miles J. Padgett6, D. J. Gauthier7, Robert W. of California, Berkeley, USA; Univ. of North numerically the formation of cascading solitons Boyd8; 1California Inst. of Technology, USA; 2The Texas, USA. We introduce a novel platform when a single femtosecond pulse is launched Inst. of Optics, Univ. of Rochester, USA; 3Dept. for quantum metamaterial by engineering the into a fiber amplifier. Because of Raman spectral of Physics, Univ. of South Florida, USA; 4Inst. electromagnetic response of ultracold atoms shifts, the output spectrum is relatively broad for Quantum Optics and Quantum Information loaded in an artificial crystal of light. Our and exhibits high coherence. (IQOQI), Austrian Academy of Sciences, Aus- proposal opens the door for applications at tria; 5School of Enginering, Univ. of Glasgow, single-photon level with metamaterials. UK; 6School of Physics and Astronomy, Univ. FTu1F.4 • 09:15 FTu1G.4 • 09:15 FTu1I.4 • 09:15 of Glasgow, UK; 7Dept. of Physics, Duke Characteristics of Three-Dimensional Bicontin- Engineering a Giant Nonlinear Optical Intracavity Dissipative Four-Wave Mixing at Univ., USA; 8Dept. of Physics, Univ. of Ottawa, uous Periodic Structures Produced by Multi- Response for a Meta-Surface on an Epsilon- Different Dispersion Regimes of an Ultrafast Canada. We investigate structured photons as Beam Interference, Shruthi Kumara Vadivel1, Near-Zero Material, Mohammad Z. Alam1, Fiber Laser, Sinem Yilmaz1,2, Hakan S. Sayinc2, carriers of quantum information. We describe Matthieu Leibovici1, Thomas K. Gaylord1; 1Geor- Israel de Leon1,2, Sebastian A. Schulz1, Jeremy Fatih Ömer Ilday1,3, Jörg Neumann2, Dietmar our implementation of quantum cryptography gia Inst. of Technology, USA. The ranges of Upham1, Robert W. Boyd1; 1Univ. of Ottawa, Kracht2; 1Physics department, Bilkent Univ., with orbital angular momentum, and present our bicontinuity for three-dimensional, periodic Canada; 2Tecnológico de Monterrey, Mexico. A USA; 2Laser Zentrum Hannover e.V., Germa- results on efficient implementation of quantum structures made by multi-beam interference are meta-surface of plasmonic antennas on a ny; 3Department of Electrical and Electronics En- state tomography for structured light fields. reported, along with their volume fractions and thin epsilon-near-zero substrate exhibits a gineering, Bilkent Univ., Turkey. We investigated

surface areas. Corresponding results for sphere- broadband nonlinear response with |n2| values a system which generates ultrahigh repetition based models are presented for comparison. up to eight orders of magnitude larger than that rate of 100 GHz stable pulse trains for different of silica glass and |Δn|>3.0. dispersion regimes in combination of a high- finesse Fabry Perot filter inside the laser setup.

FiO/LS 2016 • 16–21 October 2016 39 Tuesday, 18 October 40 Optics Goesto the Movies, FTu1A.4 •09:30 Back I and Instrumentation-AHistoricalLook Optical Design,Fabrication,Testing, FTu1A •Symposiumon100Years of Portions ofseveralthesemovieswillbeshown. fabrication. and design optical of history the into windows interesting provide that movies of number a acquired has Arizona, USA. The Museum of Optics at the Univ. of Arizona Grand Ballroom A(Radisson) — Continued Invited John Greivenkamp John

1 ; 1 Univ. of Giles Amplifier, Fiber Erbium-Doped the of Origins FTu1B.4 •09:30 bandwidth expansionofcommercial lightwavesystems. dramatic a in resulting deployment wide its to experiments and the enabling technologies that took the EDFA from lab This talk will trace the early work on the erbium-doped fiber the Erbium-doped Fiber Amplifier (EDFA) in the late 1980s. of invention the with practical became systems lightwave Fibers I Anniversary ofLowLossOptical FTu1B •Symposiumonthe50th 1 Grand Ballroom B(Radisson) ; 1 pia apiiain in amplification Optical Nokia Bell Labs, USA. — Continued 10:00 -10:30 Invited

FiO/LS 2016 Coffee Break, West CorridorandSkywayLobby(Radisson) Randy • FiO 16–21 October 2016 FTu1C.5 •09:30 Staging ofLaser-plasma Accelerators, Gonsalves an 100MeVenergy gain. Electron beam trapping in the second stage was varified by plasma accelerators where coupled by an active plasma lens. USA. We present an experiment where two indepedant laser- van Tilborg van B. Schroeder i Leemans Wim Photon Sources FTu1C •Laser-Plasma Accelerationand Grand Ballroom C(Radisson) 1 , Kei Nakamura Kei , 1 , Carlo Benedetti Carlo , 1 , Joost Daniels 1 ; 1 Lawrence BerkeleyNationalLaboratory, — Invited Continued 1 , Brian H. Shaw H. Brian , 1 , Kelly K. Swanson 1 , Cameron G. Geddes G. Cameron ,

Sven Steinke 1 , Eric E. EsareyE. Eric , 1 , Anthony J. 1 , Jeoren 1 , Carl , 1 , switching time. microsecondwith switches large-scale(64x64) our describe the current state-of-the-art of silicon photonic switches, and review We chip. a on switches optical large-scale integrate to capability unprecedented offers photonics USA. Silicon Silicon Photonic Switches for Datacenters, for Switches Photonic Silicon FTu1D.6 •09:30 Tae Joon Seok FTu1D •SiliconPhotonicsI Grand Ballroom D(Radisson) 1 , Sangyoon Han Invited 1

; 1 Univ. Berkeley, ofCalifornia — Continued Ming C. Wu C. Ming 1 , Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E Tuesday, 18 October LS FiO LS FiO

LTu1E.4 • 09:30 Invited FTu1F.5 • 09:30 FTu1G.5 • 09:30 Invited LTu1H.4 • 09:30 FTu1I.5 • 09:30 Development of Tools for Quantum Engi- Using Near IR Scattering Nanoparticles to Gain Optical Nonlinearities and Non-volatile Random laser dynamics with temporally Near-Gaussian Spatial Mode from a Mid- 1 neering Using Individual Atoms: Optical Improve Transparent Solar Cell Efficien- Switching in Photonic Metamaterials, Nikolay modulated pumping, Stefan Bittner , Sebas- IR Acetylene-filled Hollow-Core Fiber La- 1 1 1 1 1 1 Nanofibers and Controlled Rydberg Interac- cy, Duncan C. Wheeler , Yichen Shen , Marin I. Zheludev2,1; 1CDPT/TPI/SPMS, Nanyang Tech- tian Knitter , Hui Cao ; Yale Univ., USA. We ser, Neda Dadashzadeh , Manasa Thirugnana- 1 1 1 1 tions, Sylvain Ravets2,1, Jonathan E. Hoffman2, Soljacic ; Physics, MIT, USA. We use near IR nological Univ., Singapore; 2ORC, Univ. of South- present a detailed experimental study of the sambandam , Kushan Weerasinghe , Benoit 2 2 2 Fredrik K. Fatemi3, Steve L. Rolston2, Luis A. Oro- scattering nanoparticles and a wavelength ampton, UK. Extremely large nonlinearities can temporal dynamics of lasing in disordered Debord , Matthieu Chafer , Frédéric Gérôme , 2 1 zco2, Daniel Barredo1, Henning Labuhn1, Thierry selective mirror to create a light trapping be obtained in all-dielectric and plasmonic dielectric nanostructures. The irregular temporal Fetah Benabid , Brian Washburn , Kristan L. Cor- 1 1 2 Lahaye1, Antoine Browaeys1; 1Institut d’optique, effect. When used with a transparent solar cell, metamaterials through the exploitation of modulations of the pump intensity lead to win ; Kansas State Univ., USA; Univ. of Limo- France; 2Joint Quantum Inst., USA; 3Naval Re- theoretical calculations show that efficiency can optomechanical and thermal response of strong fluctuations of the emission intensity and ges, France. We report good beam quality with 2 search Laboratory, USA. Robust hybrid quantum double without decreasing transparency. the nanostructures, that can be additionally lasing spectrum. M = 1.14±0.02 for a 3μm output pulse energy systems have been imagined to combine the enhances by the use of superconductors of 1.15μJ from an acetylene-filled hollow-core strengths of multiple approaches while hopefully fiber laser. Beam quality was characterized as a compensating for their weaknesses. This paper function of 3μm pulse energy. reports on the progress made on two different FTu1F.6 • 09:45 LTu1H.5 • 09:45 FTu1I.6 • 09:45 setups that are developed toward this goal. Reversibly tunable hydrophilic nano/micro- Lasing Using Bound States in the Con- Supercontinuum Generation in Photonic porous polymer photonic crystal, Dengxin Ji1, tinuum, Ashok Kodigala1, Thomas Lepetit1, Crystal Fibers with Longitudinally Varying Haomin Song1, Borui Chen1, Alec Cheney1, Nan Qing Gu1, Babak Bahari1, Yeshaiahu Fainman1, Dispersion Using Dual-Wavelength Pump- Zhang1, Tim Thomay1, Chi Zhou1, Qiaoqiang Boubacar Kante1; 1Univ. of California, San ing, Aku J. Antikainen1, Francisco Rodrigo Gan1, Alexander Cartwright1; 1State Univ. of Diego, USA. We have designed a high quality Arteaga Sierra1, Govind P. Agrawal1; 1Univ. of New York at Buffalo, USA. Here we report a low factor cavity that is based on a bound state in Rochester, USA. We demonstrate extension cost fabrication method to finely manipulate the the continuum and harnessed its properties to of supercontinuum bandwidth through dual- pore size of nano/microporous materials and demonstrate a novel type of surface emitting pumping and longitudinally varying dispersion demonstrate its application for reversible color laser in the c-band (~1550nm). in photonic crystal fiber and explain the spectral tuning of porous polymer photonic crystals features in terms of accelerated soliton self- based on atmosphere humidity condensation. frequency shift and temporal reflections.

10:00 -10:30 Coffee Break, West Corridor and Skyway Lobby (Radisson)

FiO/LS 2016 • 16–21 October 2016 41 Tuesday, 18 October history, enablingaseriesiconictelescopes,ispresented. making mirror of years 30 Its telescopes. largest world’s the of some for mirrors honeycomb lightweight made has RichardF. USA. The Univ.the at MirrorLab Caris Arizona of and implementationofmanufacturingtechnology. from 1990–2004 Excellence as a of focal point Center for development, Army demonstration, U.S. a was Rochester of USA. The Center for Optics Manufacturing (COM) at the Univ. 42 Schoen History oftheCenterforOpticsManufacturing, FTu2A.2 •11:00 Lab, F.Richard Mirrorthe Caris at Making YearsMirror 30 of FTu2A.1 •10:30 Presider: KateMedicus,Optimax, USA Back II Instrumentation -AHistoricalLook Optical Design,Fabrication,Testing, and FTu2A •Symposium on100Years of 10:30–12:00 of Arizona,USA; Hubert M. Martin M. Hubert Grand Ballroom A(Radisson) 1 ;

1 Laboratory forLaserEnergetics, Univ. ofRochester, 2 Large BinocularTelescope Observatory, Invited Invited 1 , John Hill John ,

2 , Dae Wook Kim Wook Dae , John M. John 1 ; 1 Univ. and nextgenerationfibersforspacedivisionmultiplexing. capacity system increasing for fibers multimode and mode long haul and short reach for applications. We fibers discuss optical new single in development recent present USA. We Hasegawa Fibers, Silica Loss Ultra-low in Advances FTu2B.2 •11:00 Transmission Systems, Recent DevelopmentinOpticalFibersforHighCapacity FTu2B.1 •10:30 USA Presider: Incorporated, AlanEvans;Corning Fibers II Anniversary ofLow-LossOptical FTu2B •Symposium onthe50th 10:30–12:00 0.158dB/km loss. technologies are further applied to SDM fiber Thesewith ultra-low design. waveguide advanced to due losses splice km loss in commercial products, along with low bending and pan. Advances in silica-core fiber realizes ultra-low 0.152dB/ esy Hayashi Tetsuya Grand Ballroom B(Radisson)

1 Ysioi Yamamoto Yoshinori , 1 ; 1 Sumitomo Electric Industries Ltd, Ja Invited Invited Ming-Jun Li

FiO/LS 2016 1 ; 1 1 Corning Incorporated, Incorporated, Corning Ysik Tamura Yoshiaki , Takemi • FiO 1 - , 16–21 October 2016 numerically byusingKeldyshandmulti-rateequations. interpreted and recorded were movies phase-contrast and damage process in dielectric thin films. Ultrafast amplitude- femtosecond of dynamics capture to used was microscopy holographic- Digital stitut Fresnel -UMR7249,France. Sirutkaitis USA Presider: JakeBromage, Univ. ofRochester, FTu2C •Laser-Matter Interactions 10:30–12:00 Parameters Temporal Dependence, Ablation Pulses Ultrashort BK7 of Determination D-Scan FTu2C.2 •11:00 Melninkaitis drius Laser-induced Damage Process in Dielectric Thin Films, Time-resolved HolographicImagingofFemtosecond FTu2C.1 •10:30 Wagner de Rossi Smalakys Linas the pulsesduration. on dependence parameters ablation the of determination the allowing widths, temporal pulses ultrashort and measure the BK7 ablation threshold for many superpositions CNEN-SP, Brazil. The D-Scan technique was used to quickly Grand Ballroom C(Radisson) 1 ; 1 Vilnius Univ.Vilnius LaserResearch Center, Lithuania; 1 Nrjs Šiaulys Nerijus , 1 , Nilson D. Vieira 1 , Balys Momgaudis Balys , Invited

1 1 Luet Gallais Laurent , , Ricardo E. Samad Leandro M. Machado 1 , Robertas Grigutis Robertas ,

2 Valdas , 1 ; 1 IPEN/ An- 2 In- 1 1 , , Martin bandwidth measured. 60nm the over 27dB than better is extinction the polarization and 1.0dB ≤ is loss insertion measured The process. photonic Si CMOS-integrated production a in fabricated splitter-rotator polarization adiabatic an demonstrate 100nm-radius particlesusing2×2microring CROWs based on light-scattering imaging show real-time binding of experiments Our (CROWs). optical-waveguides resonator coupled- two-dimensional nitride silicon using detection nanoparticle single report & Technology, HongKong. We Integrated Silicon Photonics Platform, CMOS- a in Splitter-Rotator Polarization O-band An FTu2D.2 •11:00 drewW. Poon Dimensional Coupled-Resonator Optical-Waveguides, Single Nanoparticle Detection Using Silicon Nitride Two- FTu2D.1 •10:30 Central Florida,USA Presider: SasanFathpour;CREOL, Univ. of FTu2D •Silicon PhotonicsII 10:30–12:00 Tymon . Barwicz Peng Bo Grand Ballroom D(Radisson) 1 , Jason S. Orcutt 1 Jsi C Rosenberg C. Jessie , 1 , Jiawei WangJiawei , 1 ; 1 IBM TJWatson Research Center, USA. We Invited 1 , Yurii A. Vlasov 1 ; 1

Hong KongUnivofScience 1 Mra Khater Marwan ,

1 , William M. Green Wesley D. Sacher . 1

Yves , An- 1 1 , , Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E Tuesday, 18 October LS FiO LS FiO

10:30–12:00 10:30–12:00 10:30–12:00 10:30–11:30 10:30–12:00 LTu2E • X-ray and XUV I FTu2F • Resolution and FTu2G • Optics and Photonics of LTu2H • Multiphoton Effects I FTu2I • Novel Fiber Devices Presider: Christopher Milne; Paul Measurement Limits Disordered Systems Presider: Robert Alfano; CUNY City Presider: John Ballato; Clemson Scherrer Institut, Switzerland Presider: Simon Thibault; Presider: Akira Furusawa; Univ. of College, USA Univ., USA Universite Laval, Canada Tokyo, Japan

LTu2E.1 • 10:30 Invited FTu2F.1 • 10:30 FTu2G.1 • 10:30 Invited LTu2H.1 • 10:30 Invited FTu2I.1 • 10:30 1 1 Super-Resolving Two Point Sources Using a 1 1 CO Laser Structuring of Semiconductor- Title to be Announced, Yoann Pertot ; ETH Speckle-Based Spectrometers, Hui Cao ; Yale Multiphoton Interactions in Nonlinear Opti- 2 3 Zurich, Switzerland. Abstract not available. Single Tailored Spatial Projective Measure- Univ., USA. The speckle pattern, produced by cal Waveguides, Govind P. Agrawal1; 1Univ. core Glass Fibers, Michael Fokine , Thomas 1,2 1,2 2 2,4 2 ment, Hugo M. Ferretti , Weng-Kian Tham , a random scattering medium or a multimode of Rochester, USA. We review the role of Hawkins , Maxwell Jones , John Ballato , Ursula 1,2 1 1 1 Aephraim M. Steinberg ; Department of Phys- fiber/waveguide, is sensitive to wavelength and multiphoton interactions when ultrashort optical J. Gibson ; Norges Teknisk Naturvitenskapelige 2 3 ics, Univ. of Toronto, Centre for Quantum Infor- used as a fingerprint to recover the spectrum. pulses propagate inside nonlinear optical Univ, Norway; Clemson Univ., USA; KTH 4 mation and Quantum Control and Inst. for Opti- We achieve high spectral resolution with small waveguides. Topics covered include self-phase Royal Inst. of Technology, Sweden; Nufern, cal Sciences, Canada; 2Canadian Inst. For Ad- Inc, USA. A scanning CO laser system is used footprint. modulation, two-photon absorption, and four- 2 vanced Research, Canada. We introduce a new wave mixing. to process semiconductor core glass fibers. The technique for estimating the distance between conditions can be tuned to melt the core and two point sources. We present progress soften the glass, producing resonators, tapers towards an experimental demonstration of the and bends. advantages of this technique over the more traditional Image Plane Counting.

FTu2F.2 • 10:45 FTu2I.2 • 10:45 Simultaneous fluorescent and quantitative Self-Cleaning of Femtosecond-Pulsed Beams phase imaging through spatial frequency in Graded-Index Multimode Fiber, Zhanwei projections, Patrick A. Stockton1, Randy Liu1, Logan G. Wright1, Demetrios Christodou- Bartels1, Jeffrey J. Field1; 1Colorado State Un- lides2, Frank W. Wise1; 1Cornell Univ., USA; 2Univ. versity, USA. We introduce a new imaging of Central Florida, USA. We observe a nonlinear technique to simultaneously image fluorescence spatial self-cleaning process in multimode fiber. and phase with a single element detector. Experiments and simulations show this effect is This is accomplished by taking advantage caused by Kerr nonlinear interactions between of modulation transfer and Fourier optics to the modes. Several important applications will reconstruct the fluorescence and phase. be discussed.

LTu2E.2 • 11:00 Invited FTu2F.3 • 11:00 FTu2G.2 • 11:00 LTu2H.2 • 11:00 Invited FTu2I.3 • 11:00 HHG Generated Soft X-ray Supercontinuum Retrieving Inter-Segment Piston Error Using Anderson Localization in the Deep Subwave- An in vivo Two-Photon Fluorescence Composite Material Hollow Antiresonant Fi- 1 1 1 1 for Absorption Spectroscopy, A.S. Johnson1, Broadband Light, Scott Paine , James R. Fien- length Regime, Hanan H. Herzig Sheinfux , Approach to Quantify the Blood-Brain Barrier bers, Walter Belardi , Pier Sazio , Francesco De 1 1 1 1 2 1 1 1 L. Miseikis1, D.A. Wood1, D.R. Austin1, C. up ; Univ. of Rochester, USA. Traditional phase Yaakov Lumer , Guy Ankonina , Azriel Genack , Permeability for Drug Delivery in Brain, Ling- Lucia , Francesco Poletti ; ORC, Univ. of South- 1 1 1 Brahms1, S. Jarosch1, C.S. Stuber1, P. Ye1, Jona- retrieval methods fail to retrieve piston errors Guy Bartal , Mordechai Segev ; Technion Israel yan Shi1; 1Columbia Univ., USA. A new method ampton, UK. We analyze air-core fiber designs 2 than P. Marangos1; 1Imperial College London, greater than 0.5 waves in segmented systems Inst. of Technology, Israel; Physics, Queens Col- was developed to quantify the blood-brain with different materials in the cladding, including UK. We report the generation of a soft X-ray because of 2-pi ambiguities. We present and lege and Graduate Center of CUNY, USA. We barrier (BBB) solute permeability postnatal rat structures with an extended bandwidth and supercontinuum in the 150 – 450 eV photon characterize an algorithm that uses broadband experimentally demonstrate, for the first time, brain and adult by using two-photon imaging hybrid semiconductor/glass fibers with very low energy range using HHG from a 1.5 cycle CEP light to determine such piston errors. that localization of visible light can occur in deep system in vivo. attenuation. We report on the first realization of stable intense laser pulse at 1800 nm which was subwavelength disordered multilayers with ~15 this fiber type. used to measure XANES spectra of a 200 nm nm layer thicknesses. Transmission is shown to polythiophene (P3HT) film. be sensitive to 2 nm thickness variations.

FiO/LS 2016 • 16–21 October 2016 43 Tuesday, 18 October Inc, USA; the future apoma.org holds.Visit formore info. of APOMA, past accomplishments, current events and what Association) including why APOMA was the formed, history related to APOMA (American Precision Optics Manufacturers 44 APOMA: Past & Present, FTu2A.3 •11:30 Back II–Continued Instrumentation -AHistoricalLook Optical Design,Fabrication,Testing, and FTu2A •Symposiumon100Years of 12:00–13:30 Grand Ballroom A(Radisson) 2 Sydor Technologies, USA. Overview and updates 12:00–13:30 Invited Polarization Technical Group Special Talks, RadissonRochesterRiverside, James M. Sydor Radisson RochesterRiverside,Grand Ballroom D

12:00–13:30 Optical MaterialStudiesTechnical Group SpecialTalk, 1,2 ; 1 Sydor Optics Genessee SuiteG Lunch Break (onyourown) Fibers II–Continued Anniversary ofLow-LossOptical FTu2B •Symposiumonthe50th h Ftr fo te Past?, the from Future the Guess We Can – Communications Optical High-Capacity FTu2B.3 •11:30 how thefuture willevolve. guess to try and trends past at look will talk capacity. This technologies have enabled over a of thousand-fold increase in range amazing An decades. few last the over progress incredible made has communications Optical Labs, USA. Grand Ballroom B(Radisson) Invited

oet Tkach Robert FiO/LS 2016 1 ; 1 Nokia Bell • FiO 16–21 October 2016 Continued FTu2C •Laser-Matter Interactions– formation ofanewmetallicalloy. formation photo-initiated solid-state diffusional mixing resulting in the reveal patterns diffractionresulting The presented.are film probe experiments on an optically excited metallic multilayer Australia; Control ofelectron localizationindissociatingH FTu2C.3 •11:15 using femtosecondinfrared pulses, Ferroelectric domainsinversion inlithiumniobatecrystal FTu2C.5 •11:45 diffusional mixing, Optical pump/x-rayprobe measurements ofsolid-state FTu2C.4 •11:30 manipulating two-statepopulationdynamics, Schrödinger equation. time-dependent the solving by simulation the perform We few-cycle midinfrared laser pulse and a low-frequency field. phase-stabilized a of combination the using by localization electron the steer to scheme a nology,propose China. We ra Mitchell Arnan Xin Chen Pengfei Lan Brian Kelly Brian ware, USA; a channelwaveguide. in demonstrated is @815nm doubling frequency matched Quasi-phase fabricated. are patterns two-dimensional and a lithium niobate by focused femtosecond laser beam. One tralia. Periodic inversion of ferroelectric domains is realized in 12:00–13:15 13:45–16:00 Grand Ballroom C(Radisson) House, Shuttletransportation willdepartfrom theHyatt RegencyRocehsterat13:45 1 12:15–14:55 2 , Pawel Karpinski Texas A&MUniv. atQatar, Qatar; 1 2 1 , Karl Unruh Karl , Argonne NationalLabs,USA. Optical pump/x-ray , Peixiang Lu 3 Yn Sheng Yan , Matthew F.DeCamp Matthew OSA FellowMembersLunch(AdvanceRegistrationRequired), HyattRegency 1 OSA Members,FamilyandFriends Tour –SusanB.AnthonyMuseum& , Anthony DiChiara Anthony , 1 ; 1 Huazhong Univ of Science&Tech- 1 , Vlad Shvedov 1 ; LTu2J •LaserScienceSymposiumonUndergraduate Research 1 Australian National Univ., Wieslaw Wieslaw Z. Krolikowski Rochester, GrandBallroom, A-C Poster Session,RiversideCourt 1 , Aaron Loether Aaron , 1 3 , Andreas Boes 2 RMIT Univ., Aus- ; 1 Univ. ofDela- Zhuo Wang 2 + via 3 1 1 2 , , , , ricated withphotolithography, fab demultiplexer crystal photonic in-plane Ultrasmall FTu2D.3 •11:15 demonstrated withhighwavelengthtunability. crystal. Eight-port demultiplexing with a 267 GHz spacing is photonic photolithographic a using obtained tunability and spacing dense footprint, small a with demultiplexer a nabe photonic structure group, Japan. . Daud B. FTu2D •SiliconPhotonicsII–Continued aimn Purnawirman nawirman Watts htnc b Csae f Al of Cascade by Photonics Silicon for Source Light WDM of Integration Monolithic FTu2D.5 •11:45 Mixing, Wave Four via Amplification Parametric Non-Hermitian FTu2D.4 •11:30 Univ. ofNewYork, USA; Nanoscale ScienceandEngineering,Univ. atAlbany, State optical attenuation. of Hermitian phase absence matching condition the if the in idler beam even suffers amplified strongly be can beam signal the waveguides, silicon in mixing wave four for that USA; thomas adam singh gurpreet El-Ganainy Ramy pm/ operation of four channels is achieved with photonics by silicon cascade for of Al source light WDM of integration monolithic a o C temperature dependent wavelength shift. 2 Grand Ballroom D(Radisson) 1 Michigan Technologicaldemonstrate Univ., USA. We ; 1 Massachusetts Inst.ofTechnology, USA; 1 Tmhr Tetsumoto Tomohiro , sf Ahmed Asif 2 , Gerard Leake 1 jnta D bradley D. jonathan , 2 Rcad . Osgood M. Richard , 1 3 Xag Meng Xiang , Harvard Univ., USA. We demonstrate 1 Nni Li Nanxi , 2 O 2 3 , Douglas Coolbaugh : Er 2 O 3+ 1 YutaOoka Tksm Tanabe Takasumi , 3 Er : DFB lasers. Simultaneous 3 ei slh magden salih emir , 1 3+ mcee moresco michele , 1 Jry . Dadap I. Jerry , 1 DFBLasers, ; e demonstrate We 1 dl/dT = 15.3±0.1 Columbia Univ., 1 , Nurul Ashikin Nurul , 2 College of 2 , Michael 1 ; Pur 1 Ta 1 1 1 - - - , , , Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E Tuesday, 18 October LS FiO LS FiO

LTu2E • X-ray and XUV I– FTu2F • Resolution and FTu2G • Optics and Photonics of LTu2H • Multiphoton Effects I– FTu2I • Novel Fiber Devices– Continued Measurement Limits–Continued Disordered Systems–Continued Continued Continued

FTu2F.4 • 11:15 FTu2G.3 • 11:15 FTu2I.4 • 11:15 Weak Value Measurements with Pulse Recy- Replica Symmetry Breaking in Random Lasers Characteristics of Dissimilar-Fiber Long-Peri- cling, Courtney Byard1, Trent Graham1, Andrew Based on Colloidal Rh-6G and Specially De- od Fiber Gratings, Pengfei Wang1,2, Thomas K. 2 1 1 2 2 1 2 Jordan , Paul Kwiat ; Univ. of Illinois at UC, signed TiO2 Nanoparticles, Pablo I. Pincheira , Gaylord ; Beijing Jiaotong Univ., China; Geor- USA; 2Physics and Astronomy, Univ. of Roch- Andréa Silva2, Sandra Carreño2, Serge Fewo3, gia Inst. of Technology, USA. A new kind of ester, USA. Recycling undetected photons in a Andre de Lima Moura2,1, Ernesto Raposo2, long-period fiber grating that contains dissimilar weak measurement can substantially improve Anderson Gomes2, Cid B. de Araújo2; 1Universi- fiber types is fabricated and demonstrated. the signal-to-noise ratio. We demonstrate a dade Federal de Alagoas, USA; 2Departamento This dissimilar-fiber long-period fiber grating preliminary improvement by a factor of 1.36 over de Física, Universidade Federal de Pernambuco, (DF-LPFG) is shown to exhibit good resonant a system with no recycling, potentially reaching Brazil; 3Univ. of Yaounde I, Yaoundé, Camer- attenuation and an acceptable insertion loss. a factor of 3.2. oon. Replica symmetry break and a photonic paramagnetic to spin-glass phase transition in a random laser based on ethanol solution of Rhodamine 6G and specially designed

amorphous TiO2 nanoparticles is demonstrated.

LTu2E.3 • 11:30 Invited FTu2F.5 • 11:30 FTu2G.4 • 11:30 FTu2I.5 • 11:30 Exploiting the Longitudinal Coherence of Common Path Heterodyne Interferometer for Multiple Most-Likely Path Solutions for Con- Maskless photolithography using a photon 1 FERMI: Coherent Control with Multicolor FEL Single Nanoparticle Detection in Fluids, Sarah tinuously Monitored, Driven Qubits, Philippe sieve on an optical fiber tip, Raquel Flores , 1 1 1 1 1 1 1 Pulses, Kevin Prince1; 1Intl Centre for Theoretical Kurmulis , Lukas Novotny ; Photonics Labora- Lewalle , Areeya Chantasri , Andrew Jor- Ricardo Janeiro , Dionísio Pereira , Jaime 1 1 1 1 Physics, Italy. FELs based on SASE have poor tory, ETH Zurich, Switzerland.Sensitivity of dan ; Univ. of Rochester, USA. We examine Viegas ; Masdar Inst., United Arab Emirates.A longitudinal coherence, whereas the seeded interferometric detection of nanoparticles is most-likely paths for continuously monitored photon sieve inscribed on a single mode optical FEL FERMI is nearly transform limited. This limited by path length fluctuations. We present a pure-state qubits, obtained as an extremum fiber tip by focused ion beam milling is demon- opens the way to performing coherent control common path heterodyne interferometer using of a stochastic path integral. By considering strated for maskless lithography of a photoresist experiments, as demonstrated recently, Nature a vibrating plate that allows stable and sensitive the evolution of the Lagrange Manifold, we with a 405 nm wavelength laser. Photonics 10 (2016) 176. sizing of single nanoparticles in solution. locate multiple-path solutions, analogous to optical caustics.

FTu2F.6 • 11:45 FTu2G.5 • 11:45 FTu2I.6 • 11:45 Fault-tolerant and finite-error localization Using Polarized Light to Investigate Shell The Reflectivity Measurement of a Dynami- for point emitters within the diffraction lim- Structure of Sea Dwelling Organisms, Joshua cally Formed Fiber Bragg Grating Inside an it, Zong Sheng Tang1, Kadir Durak1, Alexander A. Jones1, Enrique J. Galvez1, Rebecca A. Yb-doped Fiber, Ivan A. Lobach1, Roman V. Ling1,2; 1Center for Quantum Technologies, Sin- Metzler1, Anthony J. D’Addario1, Carrie Bur- Drobyshev1, Andrei A. Fotiadi2,3, Sergey I. Kablu- gapore; 2Department of Physics, National Univ. gess1, Brian Regan1, Samantha Spano1, Ben kov1, Sergey A. Babin1; 1Inst. of Automation and of Singapore, Singapore. We implement a finite- Cvarch1; 1Colgate Univ., USA. We present our Electrometry, Russian Federation; 2Electromag- error estimator for determining the separation work on using polarized light to investigate netism and Telecommunication department, between two incoherent point sources even the structure of nacre in three shelled species: Univ. of Mons, Belgium;3Ulyanovsk State Univ., with small separation. This technique has good bivalve, cephalopod and gastropods. Data Russian Federation. Spatial hole burning in an tolerance to error, making it an interesting were collected using imaging polarimetry of active medium of a linear cavity Yb-doped fiber consideration for high resolution instruments. monochromatic light passing through thin laser leads to formation of a dynamical fiber samples. Bragg grating. Reflectivity of the grating (~5%) is measured for the first time.

12:00–13:30 Lunch Break (on your own) 12:00–13:15 OSA Fellow Members Lunch (Advance Registration Required), Hyatt Regency Rochester, Grand Ballroom, A-C 12:00–13:30 Optical Material Studies Technical Group Special Talk, Radisson Rochester Riverside, Grand Ballroom D 12:15–14:55 LTu2J • Laser Science Symposium on Undergraduate Research Poster Session, Riverside Court 12:00–13:30 Polarization Technical Group Special Talks, Radisson Rochester Riverside, Genessee Suite G 13:45–16:00 OSA Members, Family and Friends Tour – Susan B. Anthony Museum & House, Shuttle transportation will depart from the Hyatt Regency Rocehster at 13:45

FiO/LS 2016 • 16–21 October 2016 45 Tuesday, 18 October 46 Title tobeAnnounced, FTu3A.2 •14:00 York, History ofOpticsManufacturinginRochester, New FTu3A.1 •13:30 USA Presider: DaeWook Kim,Univ. ofArizona, Back III Instrumentation -AHistoricalLook Optical Design,Fabrication,Testing, and FTu3A •Symposium on100Years of 13:30–14:30 Company USA,USA. Abstractnotavailable. using current businesses. examples few a as well as overview historical an presents paper This companies. other off spun and developed companies how of stories interesting with Rochester in history long a has manufacturing Systems Inc, USA. Optics Grand Ballroom A(Radisson) Jim VanKouwenberg

Invited Invited 1 dad White Edward , Robert Wiederhold

1 ; 1 CDGM Glass 1 ; 1 Optimax tions incommunications,lasersandsensing. applica- emerging and conventional both in improvements significant deliver to core) hollow a and/or cores/channels, spatial multiple either exploiting particular (in technology fiber microstructured in advances recent review ton, UK. I Limit, Transmitting BeyondTheFictitiousNonlinearCapacity FTu3B.2 •14:00 their Applications, DavidRichardson Recent AdvancesinMicrostructured OpticalFibers and FTu3B.1 •13:30 USA Presider: Incorporated, AlanEvans;Corning Fibers III Anniversary ofLow-LossOptical FTu3B •Symposium onthe50th 13:30–15:30 recognize “nonlinearShannon limit”. of this misconception and describe the physics that does not capacity is limited by Kerr response. We discuss the genesis introduction of low-loss fibers, it appears that the transmission Grand Ballroom B(Radisson) Stojan Radic

1 ; 1 Univ. SanDiego,USA. With ofCalifornia Invited Invited FiO/LS 2016 1 ; 1 Univ. ofSouthamp- • FiO 16–21 October 2016 related techniqueswillbedescribed. and spectroscopy absorption resolved time to their appication and HHG and XFELs upon based sources X-ray soft on progress Recent explained. be will dynamics electron ultrafast measuring of challenge College London,UK. The Technology, USA Presider: JieQiao,Rochester Inst.of Applications FTu3C •Ultrafast Sources and 13:30–15:30 ties, Limitations,andTrade-offs, Dynamics of Large Femtosecond Filament Arrays: Possibili- FTu3C.3 •14:15 in experimentsatX-rayFELsUSA,JapanandEurope. participant active an is and 2008-2010 from Project Source Light New UK the led having science laser electron free in involved is He sources. light sub-femtosecond power high developing in and fields laser strong by systems complex at looking been problemsthe controllingof electronthe in driven dynamics has he Recently Fellow. OSA an is and College Imperial at Physics in Chair Lockyer the holds he from Imperial College in 1982 and a PhD in 1986. Currently Physics in BSc a with graduated Marangos Jon Biography: and the Condensed Phase, Towards AttosecondMeasurement inComplexMolecules FTu3C.1 •13:30 . Litchinitser M. optimal parametersensuringhigharraystability. the find We power. initial and them, between separation relative phase of the generating beams, number of filaments, by affected is propagation array multifilament of dynamics Grand Ballroom C(Radisson) 1 ;

1 Univ. at Buffalo, USA. Tutorial Jonathan P. Marangos

Wiktor Walasik Wiktor e hw ht the that show We 1 ; 1 1 , Natalia , Imperial Imperial Computer Engineering,George Washington Univ., USA; and electricaltradeoffs. assess the quality of link performance based-on both optical to Footprint)] x (Energy/bit / [Speed metric the define and length critical with non-monotonically scales performance device nanophotonic that show We of Washington, USA. Sun On-Chip Plasmonic Spectrometer, FTu3D.3 •14:15 Shi Modulator, Plasmonic Field-Effect Ultracompact FTu3D.2 •14:00 Nanophotonics, of Laws Scaling Physical FTu3D.1 •13:30 Switzerland Presider: Jeurg Leuthold;ETHZurich, Devices FTu3D •Plasmonic andPhotonicCrystal 13:30–15:45 at highspeed. work potentially can and 800nm, only of length effective an has modulator The structure. (MIC) oxide conductive modulator based on the field effect inside a metal-insulator- plasmonic (EA) electro-absorption ultracompact an present micro-particle spectroscopy. improve potentially to field-enhancement plasmonic the spectroscopy,Raman compact harnesses enable and can It demonstrated. is polaritons, plasmon surface propagating utilizing spectrometer on-chip first The Aviv Univ., Israel. 1 , Zhaolin Lu Zhaolin , 1 Ak Majumdar Arka , Grand Ballroom D(Radisson)

1 ; 1 Rochester Inst.ofTechnology, USA. We Invited 2 Vle J Sorger J. Volker ,

Yuval Tsur 1 ; 1 1 , Ady Arie e Liu Ke Electrical and 1 Kaifeng Shuai , 2 1 Univ. ; 1 Tel Tel Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E Tuesday, 18 October LS FiO LS FiO

15:00–16:30 13:30–15:30 13:30–15:30 14:00–15:30 13:30–15:30 LTu3E • Laser Science Symposium FTu3F • Optical Properties of FTu3G • Integrated Quantum LTu3H • Quantum Light Sources I FTu3I • Novel Light Generation on Undergraduate Research I Materials Optics Presider: A. Nick Vamivakas, Univ. and Manipulation in Fiber Presider: Hal Metcalf, SUNY, Stony Presider: Christopher Dorrer, Univ. Presider: Tobias Kippenberg; of Rochester, USA Devices II Brook, USA of Rochester, USA Ecole Polytechnique Federale de Presider: Shankar Pidishety, Indian Lausanne, Switzerland Inst. of Technology Madras, India See the program distributed with registration materials for complete information.

FTu3F.1 • 13:30 FTu3G.1 • 13:30 Invited FTu3I.1 • 13:30 Invited Resonant cavity-enhanced holographic Artificial Gauge Fields and Photonic Topo- The Inviscid Burgers’ Equation in Nonlinear imaging in ultrathin topological insulator logical Phenomena, Vaakov Lumer1, Miguel Fiber Optics, Benjamin Wetzel1,2, Domenico 1 1 1 1 films, Zengji Yue , Gaolei Xue , Min Gu ; Phys- Bandres1, Yonatan Plotnik1, Hanan H. Herzig Bongiovanni1, Michael Kues1, Yi Hu3, Zhigang ics, RMIT, Australia. We report computer- Sheinfux1, Alexander Szameit2, Mikael C. Chen3,4, Stefano Trillo5, John M. Dudley6, generated holography in ultrathin topological Rechtsman3, Mordechai Segev1; 1Technion Stefano Wabnitz7, Roberto Morandotti1; 1INRS insulator films, which serve as natural optical Israel Inst. of Technology, Israel; 2Univ. of Jena, - EMT, Canada; 2Univ. of Sussex, UK; 3Nan- resonant cavities and remarkably enhances the Germany; 3Penn State, USA. Artificial gauge kai Univ., China; 4San Francisco State Univ., phase modulations in the holograms. fields allow unprecedented control of light flow USA; 5Universita di Ferrara, Italy; 6Université de in photonic systems, enabling the observation Franche-Comté, France; 7Università degli Studi of topological insulators and other topological di Brescia, Italy. We report on the experimental FTu3F.2 • 13:45 phenomena in photonics. We present an generation of Riemann waves in an optical fiber Tailoring the Optical Properties of Boron overview of this area along with new results. system, allowing for the controlled formation Doped μc-Si:H Thin Films by Changing the of shock waves, as analytically described by a SiH /H Ratio Using RF-PECVD Process, Ghada 4 2 seminal equation of fluid dynamics: the so-called 1 1 Dushaq , Ammar Nayfeh , Mahmoud Ras- Inviscid Burgers’ Equation. ras1; 1Masdar Inst., United Arab Emirates. This

paper depicts the effect of SiH4/H2 dilution ratio (R) on the structural and optical properties of amorphous silicon matrix with embedded microcrystals of silicon. The thin films are prepared using RF-standard PECVD process.

FTu3F.3 • 14:00 FTu3G.2 • 14:00 Invited LTu3H.1 • 14:00 Invited FTu3I.2 • 14:00 2D Coherent Spectroscopy of Strained Hybrid Quantum Information Process- Single Defect Centers in Wide-Bandgap Multi-peak Dispersive Wave Generation 1 1 GaAs, Alan D. Bristow , Brian L. Wilmer , Daniel ing, Akira Furusawa1; 1The Univ. of Tokyo, Materials: Stable, Bright and Pure Quantum in Single-Capillary-Assisted Chalcogenide 2 2 1 2 Webber , Kimberley Hall ; West Virginia Univ., Japan. Hybridization of qubit and continuous- Light Sources, Tim Schroder1; 1Massachusetts Optical Fibers, Satya P. Singh , Vishwatosh 2 2 2,1 1 USA; Dalhousie Univ., Canada.2D coherent variable quantum information processing (QIP) Inst. of Technology, USA. A promising class Mishra , Shailendra K. Varshney ; Department 2 spectroscopy explore low- and high-strain GaAs enables us to realize high-fidelity and efficient of single photon emitters consists of crystal of E&ECE, IIT Kharagpur, India; Department layers. The interplay of many-body effecs and QIP. I will show our research activities for that defect centers in wide-bandgap materials. of Physics, IIT Kharagpur, India. We propose strain is shown through polarization. Low strain direction. Here, we introduce, discuss, and compare such methodology to generate multi-peak dispersive has similar, closer spaced excitons. For high color centers in established and new materials waves in capillary chalcogenide optical fiber with strain, many-body effects appear bestronger. including diamond, silicon carbide, and boron the aid of longitudinal thermal-gradient and and gallium nitride. thermal-tuning of dispersion of fiber, which is only possible in cascaded fiber system.

FTu3F.4 • 14:15 FTu3I.3 • 14:15 Intermediate Time Relaxation in super Optomechanical contribution to the intensity- cooled liquid studied by optical Kerr effect dependent refractive index of optical microfi- spectroscopy, Miaochan Zhi1, Marcus T. Cice- bers and nanofibers, Wei Luo1, Yun-chao Shi1, rone1; 1National Inst. of Standards and Technol- Fei Xu1, Yan-qing Lu1; 1Nanjing Univ., China. We ogy, USA. We performed optical Kerr effect carefully examine the Lorentz optical force in (OKE) experiments in propylene carbonate and silica microfibers and nanofibers and show that showed that the ubiquitously observed but yet optomechanical effect contributes significantly unexplained intermediate relaxation process in to the value of the nonlinear index. OKE response is due to cooperative molecular motion in liquids.

FiO/LS 2016 • 16–21 October 2016 47 Tuesday, 18 October FTu4A •Tutorial -BillCasserly 14:45–15:30 48 the IlluminationDesignProblem. Conferences, Dr. Cassarly submitted the winning solution for Design Optical International 2010 and 2006 the At Optics. engineering in the Optical illumination Society of on America’s chapter Handbook a of and papers numerous authored US patents, and teaches illumination design courses. Bill has ties for illumination systems. Bill is an SPIE Fellow, holds 48 development of practical and effective optimization capabili- computer-aided illumination engineering, particularly in the of advancement the to contributor key a is Bill Biography: tions, Applica- Electronic Consumer for Design Illumination FTu4A.1 •14:45 USA Presider: JulieBentley;Univ. ofRochester, demonstrations usingMonte-Carlosimulations. ‘virtual’ and demonstrations hardware both using concepts illumination fundamental explain will tutorial This products. electronic consumer many of part core a is design Grand Ballroom A(Radisson) William William J. Cassarly Tutorial 1 ; 1 Synopsys, Inc,USA. Illumination

communicate, store andconvertenergy andchange color. sense, hear, see, will that systems and devices functional highly into materials fabric and fiber of transformation the enabling Law” “AFFOA the creating of vision the share will Fink sachusetts Inst.ofTechnology, Professor USA. Ballato are the Answer to Next Generation Optical Fibers, Back to the Future - Why Boring Old Materials and Designs FTu3B.4 •15:00 Realizing aMoore’s LawforFibers, FTu3B.3 •14:30 Fibers III—Continued Anniversary ofLow-LossOptical FTu3B •Symposiumonthe50th addressing continuedpower scaling. for best are designs simple and glasses old how discusses provocative, purposefully talk, This fiber. optical down never envisioned the optical power levels that today coursing Grand Ballroom B(Radisson) 1 ; 1 Kao and Hockham probably Hockham Clemson Univ.,and USA. Kao Invited Invited FiO/LS 2016 ol Fink Yoel 1 ; 1 • Mas- John FiO 16–21 October 2016 Applications—Continued FTu3C •UltrafastSources and Science andTechnology, China; National LaboratoryforOptoelectronics, HuazhongUnivof supercontinuum generation. for used effectively were oscillator the from directly pulses fs sub-160 2nJ, duration. limit transform Fourier their to oscillator which, delivers high energy pulses recompressible fiber dispersion all-normal an present We ences, Poland. Stepanenko land; the artificial structures caused by plane wave approximation. This method shows a significant improvement in eliminating Coulomb-correctedmethod. tomography orbital molecular a using by N$_2$ of orbital molecular the reconstruct Univ ofScienceandTechnology,experimentally China. We FTu3C.2 •14:30 Pronin Generation, Ultraviolet Extreme and Mid-infrared High-power FemtosecondThin-diskOscillatorsfor FTu3C.1 •15:00 oscillator, limit generatedfromdispersionfiber theall-normal Sub-160-fs pulsesdechripedtoitsFouriertransform FTu3C.2 •14:45 Functions, Wave Coulomb SpectroscopyHigh Harmonic forMolecularImagingwith is described. comb frequency mid-infrared W-level of generation The presented. is Kerr-lenses distributed on relying technique mode-locking novel A reported. are oscillators thin-disk many. Recent advances in the development of femtosecond eec Krausz Ferenc ejn Shi Wenjing Lan Pengfei Germany; Grand Ballroom C(Radisson) 2 1 Inst. ofPhysicalChemistry, PolishAcademyofSci- Jnta Brons Jonathan , 2 Ludwig-Maximilians-Universität München,Ger a Szczepanek Jan 1,2 1,2 2 ; Xasn Zhu Xiaosong , 1 Qnbn Zhang Qingbin , Faculty ofPhysics,Univ. ofWarsaw, Po- 1,2 ; 1 Max Planck Inst. of Quantum Optics, Invited 1 Mru Seidel Marcus , 1 hnag Zhai Chunyang Tms M Kardas M. Tomasz , 1,2

2 School of Physics, Huazhong School ofPhysics,Huazhong Yn Li Yang , 1,2 Piin Lu Peixiang , 1,2 1 Jne Zhang Jinwei , Fn Wang Feng , 1,2 Lxn He Lixin , 1,2 ; 1 2 Wuhan Yuriy , Oleg 1,2 1,2 1 - , , , a square wavelength. within nanoantennas of number the with linearly scales that observed in be a planar array can of nanoantennas, with superradiance a linewidth that model analytical simple a and Ottawa, Canada. We demonstrate by experiment, simulation, y Choudhary mya Superradiance in Arrays of Plasmonic Nanoantennas, FTu3D.4 •14:30 Univ. ofToronto, Canada; ences, Tecnológico deMonterrey, Mexico; Sebastian A. Schulz W. Boyd Devices—Continued FTu3D •PlasmonicandPhotonicCrystal Siong Chau Siong Singapore; vacuum, in excitations mechanical of mixing Quasi-coherent FTu3D.6 •15:00 Platform, Plasmomechanical able Subdiffraction OpticalMotionTransduction usingaScal- FTu3D.5 •14:45 coherent mixingofmechanical excitationsinvacuum. quasi- the demonstrate and platform silicon-on-insulator a on resonators nanobeam coupled the of optomechanics Vladimir Aksyuk subdiffraction region. deep a from motion of measurement plasmon-based sensitive, demonstrate we factors, quality large exhibiting plasmonic devices. Using localized-gap plasmon resonators reconfigurable producing for platform scalable a present ogy, NationalInst.ofStandards andTechnology, USA. We Grand Ballroom D(Radisson) 1,4 og Lin Tong ; 1 2 1 Inst. ofOptics,Univ. ofRochester, USA; Zhejiang Univ. ,China. We investigate the cavity , Guangya Zhou Guangya , 1 ; 1 1 Sli D Swiecicki D. Sylvia , Center for Nanoscale Science and Technol 1,2 4 , Jeremy Upham Xnwn Zhang Xingwang , 3 School ofEngineeringandSci- 1 ; 1 National Univ. ofSingapore, 4 , John E. Sipe ra J Roxworthy J. Brian 2 1 Ire d Leon de Israel , Fn Tian Feng , 4 Physics, Univ. of 2 2 , Robert Physics, 1 Fook , Sau- 3,4 1 - , , Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E Tuesday, 18 October LS FiO LS FiO

LTu3E • Laser Science Symposium FTu3F • Optical Properties of FTu3G • Integrated Quantum LTu3H • Quantum Light FTu3I • Novel Light Generation on Undergraduate Research I— Materials—Continued Optics—Continued Sources I—Continued and Manipulation in Fiber Continued Devices II—Continued

FTu3F.5 • 14:30 FTu3G.3 • 14:30 LTu3H.3 • 14:30 Invited FTu3I.4 • 14:30 High-order hyper-Rayleigh scattering in BBO Configurable heralded two-photon states on New Types of Artificial Atoms and Molecules Direct Measurement of Temporal Rogue nanocrystals, 1 2 1 2 Igor P. de Miranda , Lauro Maia , a chip, Panagiotis Vergyris , Thomas Meany , for Quantum Information Technologies, Han Waves Generated by Spontaneous Modu- 1 1 1 1 2 1 Cid B. de Araújo , Edilson L. Falcao-Filho ; Uni- Tommaso Lunghi , James Downes Downes , Mi- Htoon1; 1Center for Integrated Nanotech- lation Instability, Mikko Narhi , Benjamin 2 2 2 1 2 3 3 versidade Federal de Pernambuco, Brazil; Insti- chael Steel , Michael Withford , Olivier Alibart , nologies, Los Alamos National Laboratory, USA. Wetzel , Cyril Billet , Jean-Marc Merolla , 1 1 3 3 tuto de Física, Universidade Federal de Goiás, Sébastien Tanzilli ; Laboratoire de Physique de Quantum light emission from solitary oxygen Shanti Toenger , Thibaut Sylvestre , Roberto 2 4 1 Brazil. We report on the high-order hyper- la Matiére Condensée, Universite Nice Sophia dopants of carbon nanotubes and plasmonically Morandotti , Frederic Dias , Goëry Genty , 2 3 1 Rayleigh emission in BBO nanocrystals with Antipolis - CNRS UMR 7336, France; Depart- coupled core/thick-shell nanocrystal quantum John M. Dudley ; Tampere Univ. of Technol- 2 dimensions of ~8 nm. The samples excitation ment of Physics and Astronomy, Macquarie dot molecules will be presented as evidences ogy, Finland; Institut National de la Recherche 3 4 was performed at 2000 nm, emission up to the Univ., Australia. We show the potential of a of their potential in quantum information Scientifique, Canada; Femto-ST, France; Univ. fifth harmonic, i.e., 400 nm was detected. hybrid technology for realizing highly complex technologies. College Dublin, Ireland. We measure the real circuits for quantum photonic applications. We time intensity profiles of localized structures demonstrate the most advanced chip enabling emerging from spontaneous modulation four photon generation and manipulation for instability. We show that the results can be heralding tunable two-photon states. interpreted in terms of analytical solutions of the nonlinear Schrödinger equation.

FTu3F.6 • 14:45 FTu3G.4 • 14:45 FTu3I.5 • 14:45 Optical birefringence from P3HT nanofibers High Performance Photon Sources for Quan- Leveraging Birefringence and Gain An- in alternating electric field, Gleb Lobov1, tum Silicon Photonics, Jeffrey A. Steidle1, isotropy in a Nonlinear Fabry-Perot Reso- Yichen Zhao1, Alleksandrs Marinins1, Min Yan1, Michael L. Fanto1,2, Christopher C. Tison2, Zihao nator to Achieve a High-Contrast Opti- Jiantong Li1, Abhilash Sugunan2, Lars Thylen1, Wang1, Paul Alsing2, Stefan F. Preble1;1Rochester cal AND Gate, Saif A. Al Graiti1, Drew N. Lech Wosinski1, Michael Östling1, Muhammet Inst. of Technology, USA; 2Air Force Research Maywar1;1Rochester Inst. of Technology, USA. A Toprak1, Sergei Popov1; 1Royal Inst. of Technol- Lab, USA. High performance silicon ring 60.9-degree polarization rotation on the ogy, Sweden; 2SP Technical Research Inst. of resonator photon-pair sources have been Poincare sphere produced by the anisotropic Sweden, Sweden. AC poling allowing to control realized to produce entangled states and response of a nonlinear Fabry-Perot resonator the orientation of P3HT nanofibers, result in by balancing the losses in the resonator we is leveraged with an in-line polarizer to achieve strong optical birefringence with promising achieved heralding efficiencies of ~96%. a 31.2-dB-contrast optical AND gate. implementation in a novel type of optical modulator, without necessary embedding into any hosting matrix, e.g. liquid crystal.

FTu3F.7 • 15:00 FTu3G.5 • 15:00 LTu3H.4 • 15:00 Invited FTu3I.6 • 15:00 Polarization Dependence of the Second Bayesian quantum phase estimation on an Engineering Quantum Emitters for Integrated Torsional modes of a nanofiber: polarimetric 1 Harmonic Generation and Raman Scattering integrated Silicon photonic device, Stefano Quantum Networks, Mete Atature1; 1Cam- excitation and read out., Eliot Fenton , Ad- from Atomically Thin MoTe , 1 1 1 1 1 1 2 Ryan Beams , Paesani , Antonio Andreas Gentile , Raffaele bridge Univ., UK. Solid-state quantum emitters nan Khan , Burkley Patterson , Pablo Solano , 2 1 1 1 2 1 1 Luiz Gustavo Cançado , Sergiy Krylyuk , Irina Santagati , Jianwei Wang , Nathan Wiebe , possess multiple advantages including high- Steve L. Rolston , Luis A. Orozco , Fredrik K. 1,3 4 1 3 1 2 1 Kalish , Patrick Vora , Albert Davydov , Stephan David Tew , Jeremy L. O’Brien , Mark G. bandwidth operation and on-chip integration. Fatemi ; Univ. of Maryland at College Park, 1 1 1 1 2 J. Stranick ; National Inst of Standards & Tech- Thompson ; Centre for Quantum Photonics, I will cover recent progress in InGaAs quantum USA; Army Research Laboratory, USA. We 2 2 nology, USA; Departamento de Fisica, Univer- Univ. of Bristol, UK; Quantum Architectures dots for optically coupled spin networks as well present a study of the torsional modes of a 3 sidade Federal de Minas Gerais, Brazil; Irina and Computation Group, Microsoft Research, as new emitters in layered materials. nanofiber excited with AM circularly polarized Kalish, LLC, USA; 4Physics Department, George USA; 3School of Chemistry, Univ. of Bristol, driving laser propagating through the fiber. Mason Univ., USA. We study the symmetry UK. We demonstrate a Bayesian approach We resolve the frequencies of the modes using

properties of 1T’ MoTe2 using polarized Raman for practical and robust implementation of polarimetry in a heterodyne configuration. and second harmonic generation. We find that the quantum phase estimation algorithm. while the inversion symmetry is broken for even We implement it on a reconfigurable Silicon numbers of layers, the Raman modes are nearly quantum photonic device, demonstrating its unchanged. importance for future quantum applications.

FiO/LS 2016 • 16–21 October 2016 49 Tuesday, 18 October FTu4A •Tutorial -BillCasserly—Continued 50 Grand Ballroom A(Radisson) Fibers III—Continued Anniversary ofLow-LossOptical FTu3B •Symposiumonthe50th Grand Ballroom B(Radisson) 15:30–16:00 15:30–16:30 FiO/LS 2016 Coffee Break, West CorridorandSkywayLobby (Radisson) www.frontiersinoptics.com Meet theOSAEditors’Reception,Empire Lobby FiO/LS 2016Program for more information. now available in mobile formats! Reminder:  • Visit FiO 16–21 October 2016 Applications—Continued FTu3C •UltrafastSources and Grand Ballroom C(Radisson) for optimizingsuchstructures. are known analytically, bringing out the physical requirements with a set of one-dimensional geometries for which the fields use of a Figure of Merit for nonlinear plasmonic waveguides fano Palomba fano photonic crystalstructures, Active control ofthevacuumfieldinnanomechanical FTu3D.7 •15:15 Kerr nonlinearity, Figure ofMeritforplanarplasmonicwaveguideswitha FTu3D.8 •15:30 Q-factor are predicted andexperimentallydemonstrated. optical the of modulations field.Large electromagnetic which allows controlling the spatial localization of the vacuum photonic-crystal-based nano-opto-electro-mechanical system Eindhoven Univ. ofTechnology, Netherlands. We investigate a Leonardo . . a Otten van M. W. Devices—Continued FTu3D •PlasmonicandPhotonicCrystal Grand Ballroom D(Radisson) 1 , Maurangelo Petruzzella 1 ; 1 Univ. ofSydney, Australia. Wethe illustrate 1 Ade Fiore Andrea , C. Martijn de Sterke ihl Cotrufo Michele 1 ; 1 1 , Zarko Zobenica COBRA Research Inst., 1 , Guangyuan Li 1 Midolo , 1 , Frank 1 , Ste - Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E Tuesday, 18 October LS FiO LS FiO

FTu3F.8 • 15:15 FTu3G.6 • 15:15 FTu3I.7 • 15:15 Controlling Dipole Orientation Near A Di- Rogue-soliton generation via Anderson Microwave Beam Steering System with electric Interface Via Substrate and Buffer localisation, Mohammed F. Saleh1, Claudio Simultaneous Spectral Bandpass Filtering Layer, Xuan Long Ho1, Po-Jui Chen1, Wei Yen Conti2, Fabio Biancalana1; 1Heriot Watt Univ., Using Optical True Time Delay, Wenjing Woon2, Jonathon David White1; 1Department UK; 2Department of Physics, Univ. Sapienza, Xu1; 1Beijing Univ. of Posts and Telecomm, of Photonics Engineering, Yuan Ze Univ., Inst. for Complex Systems (ISC-CNR), Italy. We China.A novel microwave beam steering system Taiwan; 2Department of Physics, National offer a new explanation of how rogue-solitons with spectral filtering using optical true time Central Univ., Taiwan. Fluorescence lifetime generated during the modulation instability delay is proposed. 90 degrees beam steering of Rhodamine 6G on an air-dielectric interface process in optical fibres are formed. Our novel with four elements and spectral filtering with increased by a factor of three as thickness point of view is based on Anderson localisation 26-dB passband-to-stopband contrast ratio are of a PMMA layer increased suggesting a effect assisted by an optical-event horizon. simultaneously obtained. change in dipole orientation from isotropic to perpendicular.

15:30–16:00 Coffee Break, West Corridor and Skyway Lobby (Radisson)

15:30–16:30 Meet the OSA Editors’ Reception, Empire Lobby

FiO/LS 2016 • 16–21 October 2016 51 Tuesday, 18 October addressing size,weightandpowerconstrains. while requirements such for enabler key a is design optical centric Human experience. AR/VR ultimate the to key are USA. High resolution over large FOV with accurate 3D cues with HMPD. used when calculated is conditions viewing different for formulated and experimentally validated. Screen luminance is cone reflection of expression Analytical explored. are screen transparent based microbeads of features reflective Electrical engineeringdepartment,KocUniv., Turkey. Retro- 52 angle, Flexible holographic 3D display with wide viewing FTu5A.3 •16:45 Soomro Displays, Projection Mounted Head for Retro-reflective CharacteristicsofTransparent Screen FTu5A.2 •16:30 Wearable Displays, Human Centric Optical Design Enabling Next Generation FTu5A.1 •16:00 USA Presider: JulieBentley;Univ. ofRochester, FTu5A •Optics inConsumerElectronics 16:00–17:30 Wang numerically demonstrated. matically increased viewing angle of the curved hologram is dra- The substrate. flexible a on materials index refractive high the on based designed been has display holographic 3D flexible Inst. ofTechnology,Melbourne A Australia. Grand Ballroom A(Radisson) 1 , Min Gu Min , ali Xue Gaolei 1 Hkn Urey Hakan , 2 ; 1 Beijing Inst.ofTechnology, China; 2,1 Bernard Kress Qmn Zhang Qiming , Invited 1 ; 1 Optical Microsystems Laboratory,

1 ; 1 Microsoft Corporation, 2 Ja Liu Juan , 1 hab R. Shoaib Yongtian , 2

Royal mized processing parameters to mitigate heat accumulation. oxidation. A thermal model was constructed and to predict opti- heating from resulting artifacts detrimental with but laser processing of silicon showed effective material removal, for producing herringbonestructures. femtosecond laser. We find the ideal experimental conditions periodic surface structures (LIPSS) are observed on Cu using a laser-induced patterned Herringbone of Rochester, USA. Femtosecond Laser Processing of Silicon, of Processing Laser Femtosecond Determining Optimized Laser Parameters for Non-Thermal FTu5B.3 •16:45 (LIPSS), Structures Surface Periodic Laser-Induced Patterned Herringbone FTu5B.2 •16:30 Optoelectronic Devices, Laser DopingandTexturing ofSiliconforAdvanced FTu5B.1 •16:00 Technology, USA Presider: JieQiao,Rochester Inst.of FTu5B •Laser MaterialProcessing 16:00–18:00 applications indetectionandenergy harvesting. material, and electronic optical, sample’sproperties. The the resulting changes material has dopants of presence the in pulses laser intense with semiconductor a USA. Irradiating Jie Qiao Grand Ballroom B(Radisson) 1 ; 1 Rochester Inst.ofTechnology, USA.Femtosecond rk . Garcell M. Erik Invited rc Mazur Eric

FiO/LS 2016 1 Culi Guo Chunlei , 1 ; 1 Harvard Univ., Lauren TaylorLauren

1 ; 1 • Univ. FiO 1 , 16–21 October 2016 ny; - SolidsandNanostructures, Georg-August Univ.,- Germa ston emission from thebulkemission. harmonic localized distinguishing of robustmethod a show ZnO-crystal by spectral analysis and microscopic imaging. We localization of high harmonic generation in a nanostructured and enhancement the investigate We Council, Canada. the twocolourfield. enhancement occurs due to scaling of the ionization rate by compared with single fields,colour fields of laser equivalent energy. colour two The by driven efficiency generation Israel. We demonstrate large enhancements in high harmonic Presider: LauraSinclair, NIST, USA Generation Harmonic FTu5C •Frequency CombsandHigh 16:00–18:00 Nanostructures, GenerationinSemiconductor Localized HighHarmonic FTu5C.3 •16:45 using incommensuratetwocolourfields, efficiency generation harmonic high of Enhancement FTu5C.2 •16:30 Chang WaterWindow, the in Sources Light Attosecond FTu5C.1 •16:00 characterized. wereeV producedmore400 energyand to than extending polarization gating, isolated attosecond pulses with photon implementing and μm 1.7 at Amplifier Pulse Chirped Parametric Optical an with generation high-orderharmonic rn Pedatzur Oren Villeneuve Orenstein 2 Joint Attosecond ScienceLaboratory, National Research 2 , Giulio Vampa Grand Ballroom C(Radisson) 1 ; 1 By driving Univ. ofCentralFlorida,CREOL,USA. By 1 2 Nrt Dudovich Nirit , , Claus Ropers 1 Drn Azoury Doron , ua Sivis Murat 2 , Andre Staudte Invited 1 , Paul Corkum 1 ;

2,1 1 Mro Taucer Marco , Weizmann Inst.ofScience,

1 Mcal Krueger Michael , 2 , Andrei Naumov 2 ; 1 Barry D. Bruner 4th PhysicalInst. 2 Kl John - Kyle , Zenghu 2 , David 1 Gal , 1 , North guide pumped at 1.55 micron, 1.55 at pumped guide Mid-infrared supercontinuum generationinaSiNwave- FTu5D.3 •16:45 nator, Mid-Infrared Dual-Comb Source Using a Silicon Microreso- FTu5D.2 •16:30 Mid IR Silicon Photonics, FTu5D.1 •16:00 Technology, USA Presider: StefanPreble; RochesterInst.of Photonics FTu5D •Mid-Infrared Integrated 16:00–17:45 control andfree-carrier injection. sourcepump continuous-wave single a thermal using simultaneously achieved is Modelocking microresonators. silicon two in modelocking soliton using mid-infrared the in source dual-comb a lumbia Univ.,demonstrate USA. We Billat Michal Lipson potential asmid-infrared source. is a bandwidth record for the platform and demonstrates its span The micron. 1.55 at source commercial a by pumped waveguides silicon-nitride in micron 3.6 to extending generation supercontinuum report We Switzerland. and silicononinsulator(SOI). material platforms: germanium on silicon, suspended silicon and active photonic devices passive in threeof mid-IR review silicon a photonics present we paper this ampton, UK. In 1 Grand Ballroom D(Radisson) , Martin Hubert Peter Pfeiffer Peter Hubert Martin , 1 , Tobias J. Kippenberg Mengjie YuMengjie

2 , Alexander L. Gaeta 1,2 , Yoshitomo, Okawachi Invited Graham T. Reed 1 , Camille-Sophie Bres

2 Davide Grassani Davide ; 1 1 , Hairun Guo Hairun , Cornell Univ.,Cornell USA; 2 1 , Austin GriffithAustin , ; 1 Univ. ofSouth- 1 , Thibault , 1 1 , Adrien , ; 1 EPFL, 2 Co- 1 , Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E Tuesday, 18 October LS FiO

16:45–18:00 16:00–18:00 16:00–18:00 16:00–18:00 16:00–18:00 LTu5E • Laser Science Symposium LTu5F • X-ray and XUV II FTu5G • Nonlinear Optics in LTu5H • Nano-Plasmonics for FTu5I • Novel Light Generation on Undergraduate Research II Presider: Jonathan P. Marangos; Micro/Nano-Optical Structures I Spectroscopy and Manipulation in Fiber Presider: Hal Metcalf, SUNY, Stony Imperial College London, UK Presider: Anatoly Zayats; King’s Presider: Kevin Kubarych; Univ. of Devices III Brook, USA College London, UK Michigan, USA Presider: Gilberto Brambilla; Univ. of Southampton, UK See the program distributed with registration materials for complete information. LTu5F.1 • 16:00 Invited FTu5G.1 • 16:00 Invited LTu5H.1 • 16:00 Invited FTu5I.1 • 16:00 Tutorial Shrinking the Synchrotron: Tabletop Extreme Hybrid Silicon Photonic Circuits for Chip- Ultrafast Microscopy of Plasmonic Modes Polarization Effects in Optical Fibers For Ultraviolet Absorption of Transition Metal Scale Quantum Optics, Hong Tang1; 1Yale of Ag Nanocrystals Grown on Si Sub- Distributed Sensing, Andrea Galtarossa1, Luca Complexes, Josh Vura-Weis1; 1Department of Univ., USA. I will present the heterogeneous strates, Hrvoje Petek1; 1Univ. of Pittsburgh, Palmieri1; 1Universita degli Studi di Padova, Chemistry, UIUC, USA. High-harmonic extreme integration of active nanostructured materials USA. We investigate the plasmonic modes of Italy. We show that the analysis of the state of ultraviolet spectroscopy is shown to be sensitive on silicon chips for low-loss waveguiding and Ag nanocrystals grown in situ on Si(001) sub- polarization of Rayleigh backscattered light may to the electronic structure of molecular transition the exploitation of hybrid photonic circuits for strate by time-resolved photoelectron emission be useful in developing distributed polarization metal complexes, distinguishing the oxidation efficient light conversion, manipulation and microscopy. Spectromicroscopic measurements sensitive optical fiber sensors able to measure state, spin state, and ligand field, and metal detection on silicon platform. reveal high-order plasmonic modes of Ag mechanical parameters, electric current and identity of coordination systems. nanowires and Ag/Si interface. magnetic field.

LTu5F.2 • 16:30 Invited FTu5G.2 • 16:30 Invited LTu5H.2 • 16:30 Invited Transient Wave Mixing Spectroscopy Using Photonic Quantum Networks, Ian A. Walms- Nanoscale Characterization and Control of High Order Harmonic Attosecond Pulses ley1, Joshua Nunn1, Brian J. Smith1, Steve Functional Materials Using Near-field Spec- and Few-cycle NIR Laser, Wei Cao1,2, Erika R. Kolthammer1, Dylan Saunders1, Stefanie troscopy, Joanna M. Atkin1; 1Univ. of North Car- Warrick1,2, Ashley Fidler1,2, Stephen R. Leone1,3, Barz1, Jelmer Renema1, Patrick Ledingham1, olina - Chapel Hi, USA. Scattering-based near- Daniel M. Neumark1,2; 1Chemical Sciences Divi- Andreas Eckstein1, Benjamin Brecht1, Amir field spectroscopy allows for measurements sion, Lawrence Berkeley National Laboratory, Feizpour1, Helen Chrzanowski1; 1Univ. of Ox- of nanometer heterogeneity in a wide variety USA; 2Dept. of Chemistry, Univ. of California, ford, UK. Photonic networks offer the promise of materials. I will discuss the use of near-field USA; 3Department of Chemistry, Univ. of Cali- for delivering robust quantum information spectroscopy to probe the functional properties fornia, USA. We demonstrate the wave mixing processing technologies, from sensor arrays to of nanostructured electronic materials. process between weak extreme ultraviolet (XUV) quantum simulators. New sources, detectors attosecond pulses and strong near-infrared and memories illustrate progress towards Biography: Andrea Galtarossa is full professor (NIR) few-cycle laser pulses in gas phase atoms. building scalable quantum network. at Department of Information Engineering, It offers a means for ultrafast nonlinear XUV University of Padova, Italy. He is co-author spectroscopy. of about 150 regular and invited papers in propagation effects of polarized signals in single- mode optical fibers. He has been member of the Technical Program Committee of European Conference on Optical Communication (ECOC) and Optical Fiber Conference (OFC) and Technical co-chair of ECOC 2010. He was Topical Editor of OSA Optics Letters (2008-2012) and he is Deputy Editor of OSA Optics Letters (since 2013). He is Fellow of OSA and Senior Member of IEEE.

FTu5I.2 • 16:45 Observation of surface Brillouin scattering in microstructured optical fibers, Joel Cabrel Tchahame1, Jean-Charles Beugnot1, Kien Phan Huy1, Vincent Laude1, alexandre Kudlinski1, Thibaut Sylvestre1; 1CNRS, France. We report the observation of surface Brillouin scattering in a small-core microstructured optical fiber and show that this new type of scattering is highly sensitive to the air-hole microstructure, thus providing an efficient way to control it.

FiO/LS 2016 • 16–21 October 2016 53 Tuesday, 18 October USA; ber Betzold 54 tems, Sys Photovoltaic in Management Light Holographic FTu5A.5 •17:15 Generator, EfficientStructuredLight FTu5A.4 •17:00 Continued FTu5A •OpticsinConsumerElectronics— systems withvolumeandcomputergeneratedholograms. splitting spectrum and concentrators broadband including reviewed is conversion energy photovoltaic for elements optical holographic of application the paper this In USA. eig Zhang Deming field-of-view, highefficiency, andnozero order. 3D sensing applications. The optical element provides wide random structured light for pattern gesture recognition and describe a refractive micro-structure that generates a pseudo- Grand Ballroom A(Radisson) 2 Luminit, USA; amn K Kostuk K. Raymond 1 , Michael Morris 3 Seb Vorndran Shelby , 3 Seagate Technology, USA; 1 1 Ja Russo Juan , ; 1 We RPC PhotonicsInc,USA. We 1 ; TassoSales R. 1 Univ. ofArizona, 2 Js Castro Jose , 4 Panduit, 1 , Am- , 4 - , Continued FTu5B •LaserMaterialProcessing— Monash Univ., Australia; tralia. An enhancement of 10 photonic applications. flexible and weight light ultrathin, for platform integratable emerging an as potentials great their demonstrating films oxide graphene from made devices photonic functional present we technology, printing laser direct Using tralia. Thekkekara Flexible LaserScribedBiomimeticSupercapacitors , FTu5B.5 •17:30 Devices, Photonic Functional for Films Thin Oxide Graphene FTu5B.4 •17:00 Technology, Australia; Yang electrode counterpart. planar its with comparison in structures leaf Fern from adopted structures biomimetic the using supercapacitors oxide graphene scribed laser the for attained was density 1 , Scott Fraser Scott , Grand Ballroom B(Radisson) aha Jia Baohua 1 , Dan Li 1 2 ; , Ling Qiu Invited 1 Swinburne Univ.Swinburne of Technology, Aus- 2 1 Department of Material Engineering, Department ofMaterialEngineering, Xari Zheng Xiaorui , 3 School ofScience,RMITUniv., Aus- 1 Whcm 2 , Min Gu

FiO/LS 2016 -3 in the energy storage 3 ; 1 1 Swinburne Univ.Swinburne of Hn Lin Han , 1 Yunyi , • Litty FiO 16–21 October 2016 for fastmultispeciesdetection. mid-infrared in Vernierspectroscopy continuous-filtering of implementation first the spectroscopy,and high-resolution broadband for near-infrared in spectroscopy transform Fourier comb frequency optical present We Sweden. Ramaiah-Badarla copy withOpticalFrequency Combs, Cavity-Enhanced Fourier Transform and Vernier Spectros- FTu5C.4 •17:00 mr Khodabakhsh Amir Harmonic Generation—Continued Harmonic FTu5C •Frequency CombsandHigh shikawa on Electro-Optics-Modulators, Wide Frequency Range by Using a a Frequency in Comb Waves based Millimeter Low-Phase-Noise of Generation FTu5C.5 •17:30 Hideki Gotoh 72 GHzcanbedramaticallyreduced. noise in a commercially available signal generator from 6 to wavelengths, we have successfully demonstrated that phase telecommunications at comb frequency optical based electro-optics-modulator-kyo DenkiUniv.,an Japan. Using Grand Ballroom C(Radisson) 2 , Takahiro Goto 1 ; 1 NTT BasicResearch Laboratories, Japan; 1 Aesnr Foltynowicz Aleksandra , 1 Aeada . Johansson C. Alexandra , Invited 2 , Kenichi Hitachi

Atsushi Ishizawa 1 , Tetsuomi Sogawa uie Rutkowski Lucile 1 ; 1 Umeå Univ., 1 , Tadashi Ni- 1 Venkata , 2 To 1 1 - , , Photonics—Continued FTu5D •Mid-Infrared Integrated plain Polytechnique FederaledeLausanne,Switzerland; microresonators, crystalline fluoride in factors Q high ultra Mid-infrared FTu5D.5 •17:30 Arrays, Antimonid Based Mid-Infrared Detectors and Focal Plane FTu5D.4 •17:00 demonstrated usingType IIsuperlattices. be structurewill detector metamaterial A discussed. be will arrays plane focal and detectors infrared performance high als, USA. The use of “unipolar barrier engineering” to realize Quantum Center, RussianFederation; optical finesse. mid-IR highest the obtain we absorption multiphonon low to Due microresonators. crystalline with mid-infrared the in deep factors quality ultra-high demonstrate coupler,we ideality high as fiber tapered chalcogenide uncoated an V. LomonosovMoscowStateUniv., RussianFederation. Using 1 Grand Ballroom D(Radisson) , Michael L. Gorodetsky Sanjay Krishna lmn Javerzac-Galy Clément Invited 1 ; 1 Center forHighTechnology Materi- 2,3 , Tobias J. Kippenberg

3 Faculty ofPhysics,M. 1 Crln Leca- Caroline , 2 1 Russian ; 1 Ecole Ecole Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E Tuesday, 18 October LS FiO

LTu5E • Laser Science Symposium LTu5F • X-ray and XUV II— FTu5G • Nonlinear Optics in LTu5H • Nano-Plasmonics for FTu5I • Novel Light Generation on Undergraduate Research II— Continued Micro/Nano-Optical Structures I— Spectroscopy—Continued and Manipulation in Fiber Continued Continued Devices III—Continued

LTu5F.3 • 17:00 Invited FTu5G.3 • 17:00 LTu5H.3 • 17:00 Invited FTu5I.3 • 17:00 Frontiers of X-ray Science Developed with Tunable Cavity-Enhanced Quantum Light Withdrawn. Ultra-Long DFB Fiber Bragg Grating for an XFEL Facility SACLA, Tetsuo Katayama2, Sources for Integrated Quantum Photon- Stimulated Brillouin Scattering in Standard Makina Yabashi1; 1RIKEN SPring-8 Center, ics, Maurangelo Petruzzella1, Birindelli Simone1, Fiber, Sébastien Loranger1, Victor Lambin Japan; 2Japan Synchrotron Radiation Research Francesco Pagliano1, Zarko Zobenica1, Midolo Iezzi1, Raman Kashyap1,2; 1Ecole Polytechnique Institute (JASRI) Advanced Light Source and Leonardo1, Lianhe Lianhe2, Edmund Linfield2, de Montreal, Canada; 2Electrical Engineer- Optics Research Group XFEL, Japan. I will Andrea Fiore1; 1Applied Physics, Eindhoven ing Department, Polytechnique Montreal, present latest status and perspective on a Univ. of Technology, Netherlands; 2School of Canada. We demonstrate stimulated Brillouin Japanese XFEL facility SACLA, including recent Electronic and Electrical Engineering, Univ. scattering (SBS) in standard fiber using ultra- relocation of the SCSS test accelerator to the of Leeds, UK. We report the control over the long distributed feedback (DFB) fiber Bragg SACLA facility in order to enhance a capability spontaneous emission of energy-tunable gratings (FBG). This is the first observation of in softer x-ray region. quantum emitters embedded in passive SBS in standard fiber with a DFB. waveguide circuits, realized by coupling Stark- tunable quantum dots to electromechanically- compliant photonic crystal molecules.

FTu5G.4 • 17:15 FTu5I.4 • 17:15 Measurement of photon-pair generation Multiband RF Filter Enabled Through Opti- in waveguide arrays with specialized pol- cal Phase-Sensitive Amplification, James M. ing, Francesco Lenzini1, James Titchener2, Paul Dailey1, Anjali Agarwal1, Paul Toliver1; 1Ven- Fisher1, Andreas Boes3, Alexander Poddubny4,5, core Labs, USA. We report experimental Sachin Kasture1, Ben Haylock1, Matteo Villa1, measurements on an RF photonic multiband Arnan Mitchell3, Alexander S. Solntsev2, An- filter realized using a simple, passive spectral drey A. Sukhorukov2, Mirko Lobino1; 1Griffith phase mask and fiber-based optical phase- Univ., Australia; 2The Australian National Univ., sensitive amplifier resulting in 1 GHz bands with Australia; 3RMIT Univ., Australia; 4ITMO Univ., an extinction given by amplifier-gain-squared. Russian Federation; 5Ioffe Physical-Technical Inst. of the Russian Academy of Science, Russian Federation. We present the realization of an inhomogeneously poled nonlinear waveguide array for the generation of photon pairs. The device is characterized by coincidence counting and a novel method based on reversed sum- frequency generation measurements.

LTu5F.4 • 17:30 Invited FTu5G.5 • 17:30 LTu5H.4 • 17:30 Invited FTu5I.5 • 17:30 Single Particle Imaging at the Linac Coher- High Efficiency Superconducting Single-Pho- Ultrafast Methods for Investigating Structure Generation of Radially and Azimuthally ent Light Source, Andy Aquila1; 1LCLS, SLAC, ton Detectors Evanescently Coupled to Laser and Dynamics of Biological Systems, Carlos Polarized Beams using All-fiber Fused 1 3,1 USA. Results from LCLS’s Single Particle Imaging Written Waveguides, Rubayet Al Maruf , Chris- Baiz1; 1Univ. of Texas at Austin, USA. We Couplers, Shankar Pidishety , Gilberto 1 1 1 1 2 Initiative, a community-involved program tasked topher Haapamaki , Michal Bajcsy ; Inst. for describe a suite of ultrafast IR spectroscopy Brambilla , Siddharth Ramachandran , Balaji 3 1 with the goal of overcoming the technical Quantum Computing, Department of Electrical tools and molecular models designed to probe Srinivasan ; Optoelectronics Research Centre, 2 challenges for reaching ultimately atomic and Computer Engineering, Canada. SNSPDs biological interfaces, including membrane Univ. of Southampton , UK; Electrical and Com- resolution in X-ray imaging of single-particles, evanescently coupled to silicon waveguides protein structure, and interfacial environments puter Engineering Department, Boston Univ. , 3 will be discussed. can have low system efficiency due to mode surrounding the lipid bilayer. USA; Department of Electrical Engineering, mismatch issue. We propose to improved this Indian Inst. of Technology Madras, India. We by substituting the silicon waveguides with demonstrate the generation of radially and silica waveguides, such as fibers or laser-written azimuthally polarized beams using an all-fiber waveguides. fused coupler fabricated using single mode fiber (SMF) and air-core fiber. The generated beams exhibit high stability with ~85% power coupling efficiency.

FiO/LS 2016 • 16–21 October 2016 55 Tuesday, 18 October 56 Continued FTu5A •OpticsinConsumerElectronics— Grand Ballroom A(Radisson) 18:00–19:00 19:00–22:00 17:30–20:30 Optics &Energy: Reflections onthePastandLightingFuture, RadissonRochesterRiverside,GeneseeSuiteF the resulting absorptionandpolymerization. Continued FTu5B •LaserMaterialProcessing— lah topolymer duringholographicrecording, An investigationoflightbehaviourinthemultilayerpho- FTu5B.6 •17:45 lymerization by varying the dye concentration. The 3D technique multilayer the using process photpolymerization for calculation the show We College Dublin,Ireland. 1 19:00–22:00 , Haoyu Li Haoyu , Optics AlumniNetworkingReception,RadissonRochesterRiverside,RiverviewBallroom andLounge Grand Ballroom B(Radisson) Driven 1 , Inbarasan Muniraj Inbarasan , Photonics Clambake2016,(ticketrequired), HyattRegencyRochester, GrandBallroom iffusion model is applied to calculate to applied is model Diffusion OSA StudentMemberParty, HolidayInnHotelRochester, GrandBallroom FiO/LS 2016 1 , John T.John , Sheridan N onlocal Ra’ed A. Malal- A. Ra’ed P hotopo 1 ; 1 • Univ. FiO - 16–21 October 2016 molecular hydrogen fortestingQED. and krypton, in spectroscopy two-photon accurate highly to leading excitation, Ramsey-Comb deep-UV developed frequency comb laser pulses with Ramsey-spectroscopy, we amplified of upconversion combining By Netherlands. deep-UV range, the in spectroscopy Ramsey-Comb with QED Testing FTu5C.6 •17:45 S. Dreissen Harmonic Generation—Continued Harmonic FTu5C •Frequency CombsandHigh Grand Ballroom C(Radisson) 1 , Kjeld S. Eikema Sandrine Galtier 1 ; 1 Vrije Universiteit Amsterdam, 1 , Robert K. Altmann 1 , Laura Photonics—Continued FTu5D •Mid-Infrared Integrated Grand Ballroom D(Radisson) Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E Tuesday, 18 October LS FiO

FTu5G.6 • 17:45 FTu5I.6 • 17:45 Inherently Non-Reciprocal On The Na- Period-doubling vector soliton generation noscale: Nonlinear Generation Via Multipole from a linear cavity mode-locked laser us- Interference, Ekaterina Poutrina1,2, Augustine ing a faraday rotator mirror, Yingling Pan1, Urbas1; 1Air Force Research Laboratories, Xin Zhao1, Ya Liu1,2, Meng Zhang1, Zheng USA;2UES, Inc., USA. We show that nonreciprocal Zheng1,2; 1School of Electronic and Informa- directionality of nonlinear generation, where tion Engineering, Beihang Univ., China; 2Col- the generation direction is preserved when laborative Innovation Center of Geospatial reversing the fundamental beam(s), is inherent Technology, China. Experimental observation of and realistically observable in the nonlinear high-contrast, period-doubling vector solitons multipolar response of nanostructures. generated by a linear cavity mode-locked fiber laser is reported, which is mode-locked with a carbon nanotube modelocker and has a faraday rotator end mirror.

17:30–20:30 Photonics Clambake 2016, (ticket required), Hyatt Regency Rochester, Grand Ballroom

18:00–19:00 Optics & Energy: Reflections on the Past and Lighting the Future, Radisson Rochester Riverside, Genesee Suite F

19:00–22:00 OSA Student Member Party, Holiday Inn Hotel Rochester, Grand Ballroom

19:00–22:00 Optics Alumni Networking Reception, Radisson Rochester Riverside, Riverview Ballroom and Lounge

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07:00–18:00 Registration, Galleria

08:00–09:30 JW1A • Joint Plenary Session, Lilac Ballroom

08:00–17:00 AIM Photonics Northeast Supply Conference (NESCO), Hyatt Regency Rochester, Grand Ballroom A-D

09:30–16:00 Exhibit Hall Open, Empire Hall

09:30–16:00 Glass Art Contest, Empire Hall

09:30–10:30 Unopposed Exhibit Time and Coffee Break, Empire Ballroom

10:30–12:00 10:30–12:00 10:30–12:00 10:30–12:00 Wednesday, 19 October Wednesday, FW2A • Novel Design Concepts for Eye FW2B • Quantum Communications I FW2C • Biomedical Optics FW2D • Symposium on Mesoscopic Optics Correction and Vision Simulators I Presider: Rainer Steinwandt; Florida Atlantic Presider: Mike Marcus, Lumetrics, USA of Disordered Media I Presider: Brian Vohnsen, Univ. College Univ., USA Presider: Aristide Dogariu, CREOL, Univ. of Dublin, Ireland Florida, USA

FW2A.1 • 10:30 Invited FW2B.1 • 10:30 Invited FW2C.1 • 10:30 Invited FW2D.1 • 10:30 Invited Myopia Control Off-Axis Correction Lenses, Earl The Interplay between Cryptography and Quantum 3D High-definition Wide Field-of-view Optical Coherence Control of Optical Intensity Distribution inside a Disor- Smith1; 1Univ. of Houston, USA. The defocus-sensitive Technology - Challenges and Opportunities, Rainer Stein- Microscopy Advancing Real-time in-vivo Cellular Imag- dered Waveguide, Hui Cao1, R. Sarma1, Yaron Bromberg1, mechanisms that regulate ocular growth operate in a wandt1; 1Florida Atlantic Univ., USA. Quantum technology ing, Cristina Canavesi1, Andrea Cogliati2, Adam Hayes3, Pa- Alexey Yamilov2, Sasha Petrenko2; 1Yale Univ., USA; 2 Dept. of regionally selective manner. Optical manipulations of has substantial potential for cryptology. This talk discusses trice Tankam3, Anand Santhanam4, Kevin Rolland-Thompson5, Physics, Missouri Univ. of Science & Technology, USA. We use peripheral vision can influence growth, potentially slowing cryptanalytic implications – how common hardness Jannick P. Rolland3,1; 1LighTopTech Corp., USA; 2Electrical and the adaptive wavefront shaping technique to vary the total myopia progression, without altering central vision. assumptions are invalidated and security models deserve to Computer Engineering, Univ. of Rochester, USA; 3The Inst. of energy inside a disordered silicon waveguide, and change be revisited – and how quantum technology can transcend Optics, Univ. of Rochester, USA; 4Radiation Oncology, Univ. of the energy density distribution across the sample by selective limitations of classical cryptography. California, USA; 5Synopsys Inc., USA. In-vivo imaging requires coupling to high or low transmission eigenchannels. micron-scale resolution in 3D, ~1 mm depth of imaging and large field-of-view (≥1 mm). Optical coherence microscopy breaks the cellular lateral resolution limit of optical coherence tomography, enabling advances in biotech.

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07:00–18:00 Registration, Galleria

08:00–09:30 JW1A • Joint Plenary Session, Lilac Ballroom

08:00–17:00 AIM Photonics Northeast Supply Conference (NESCO), Hyatt Regency Rochester, Grand Ballroom A-D Wednesday, 19 October 09:30–16:00 Exhibit Hall Open, Empire Hall

09:30–16:00 Glass Art Contest, Empire Hall

09:30–10:30 Unopposed Exhibit Time and Coffee Break, Empire Ballroom

10:30–12:00 10:30–12:00 10:30–12:00 10:30–12:00 10:30–12:30 FW2E • Exotic States and FW2F • Optical Fibers for Space FW2G • A Tribute to Steve FW2H • Adaptive Optics and LW2I • Integrated Quantum Applications I Projects Jacobs I Interferometry Photonics I Presider: Shivanand, Purdue Univ., Presider: Morten Ibsen; Univ. of Presider: Jonathan Zuegel, Univ. of Presider: Christina Schwartz, Univ. Presider: To be Announced USA Southampton, UK Rochester, USA of Rochester, USA

FW2E.1 • 10:30 Invited FW2F.1 • 10:30 Tutorial FW2G.1 • 10:30 Invited FW2H.1 • 10:30 LW2I.1 • 10:30 Invited Exotic States of Light for Microscopy, Monika Recent Advances in Radiation Hardened Optical Glass Science – the How and Why We Wavefront Shaping For Measurements Quantum Silicon Photonics: Photon sources A. Ritsch-Marte1; 1Medical Univ. of Innsbruck, Fiber-Based Technologies, Sylvain Girard1, You- Got There, Kathleen A. Richardson1; 1Univ. of Through Diffusing Phase Boundaries, Nektar- and Circuits, Stefan F. Preble1, Jeffrey A. 1 1 2 Austria. Using tailored optical wavefronts or cef Ouerdane1, Thierry Robin2, Benoit Cadier2, Central Florida, CREOL, USA. Optical glasses ios Koukourakis , Bob Fregin , Jörg König , Lars Steidle1, Michael Fanto1,2, Christopher C. 1 1 1 “exotic” optical beams in a microscope leads to Aziz Boukenter1; 1Laboratoire Hubert Curien, play a critical role in photonic systems and Buettner , Jürgen Czarske ; TU Dresden, Ger- Tison2, Gregory A. Howland2, Edwin Hach 1, 2 a wealth of opportunities to modify the imaging Universite Saint Etienne, France; 2Photonics Divi- components. Know-how in glass manufacturing many; IFW, Germany. We show that aberrations Paul Alsing2; 1Rochester Inst. of Technology, performance. Advantages and problematic sion, Photonics Division, IXBlue, France. Several and characterization realized at LLE in the early introduced by diffusing phase boundaries can USA; 2Air Force Research Laboratory, USA. We issues of recent approaches and general trade- recent techniques are presented allowing to 1980’s led by Steve Jacobs, continue to yield be compensated by using guide-stars. Flow report high performance ring resonator photon offs will be discussed. increase the radiation tolerance of fibers and advancement throughout our community. field measurements based on image correlation sources and the integration of the sources into fiber-based sensors to the harsh radiation through rough phase boundaries are presented. quantum photonic circuits. We also discuss ring constraints associated with space, high energy resonators as a building block for compact, physics or nuclear power plants. reconfigurable, linear quantum optical circuits.

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FW2A • Novel Design Concepts for Eye FW2B • Quantum Communications I— FW2C • Biomedical Optics—Continued FW2D • Symposium on Mesoscopic Optics Correction and Vision Simulators I— Continued of Disordered Media I—Continued Continued

FW2A.2 • 11:00 Invited FW2B.2 • 11:00 FW2C.2 • 11:00 FW2D.2 • 11:00 Invited 1 New Technologies to Increase the Range of Vision of In- Hyperdense Coding with Single Photons, Alexander Hill , Tomographic Coaxial Scanning Microscopy Using a Conical Wave Control and Holography with Time Transforma- 1 1 1 1 1 1 traocular Lenses, Aixa Alarcon1, Marrie H. van der Mooren1, Trent Graham , Paul Kwiat ; Univ. of Illinois (UIUC), USA. We Lens (Axicon) , Boris Y. Zeldovich , Bahaa E. Saleh ; Univ. of tions, Mathias Fink1; 1Ecole Sup Physique Chimie Indus- Carmen Canovas1, Henk Weeber1, Patricia Piers1; 1Abbott present current progress on an experimental implementation Central Florida, CREOL, USA. A new form of tomographic trielles, France. Because time and space play a similar role Medical Optics Inc, Netherlands. Traditional methods to of quantum hyperdense coding, a quantum communication coaxial scanning microscopy is proposed by replacing the in wave propagation, wave control can be achieved or by increase depth of focus result in the reduction of distance protocol which is capable of transmitting up to 2.58 bits per standard lens in confocal microscopy with a conical lens manipulating spatial boundaries or by manipulating time

Wednesday, 19 October Wednesday, vision and increased side-effects. We present how the hyperentangled photon pair. (axicon) that generates pencil-like illumination and detection boundaries. Here we emphasize the role of time boundaries combination of different technologies can significantly along lines through the object. manipulation. We show that sudden changes of the medium improve depth of focus and visual performance. properties generate instant wave sources that emerge in- stantaneously from the entire wavefield and can be used to control wavefield and to revisit the holographic principles.

FW2B.3 • 11:15 FW2C.3 • 11:15 Reminder: Comparing the Information Capacity of Entangled Stokes vector based Second Harmonic Generation Mi- Laguerre-Gaussian and Hermite-Gaussian Modal Sets in a croscopy reveals molecular structure, Nirmal Mazumder3,1, FiO/LS 2016 Program Finite Aperture System, Sara Restuccia1, Daniel Giovannini2, Jianjun Qiu1,2, Fu J. Kao1; 1biophotonics, national yang ming Miles J. Padgett1; 1Glasgow Univ., UK; 2The Edward S. Rogers Univ., Taiwan; 2Huazhong Univ. of Science and Technology, now available in Department of Electrical and Computer Engineering, Univ. Key Laboratory of Biomedical Photonics, China; 3Biophysics, of Toronto, Canada. Within a parametric down-conversion Manipal Univ., India. We developed a four-channel photon mobile formats! process we compare information capacity associated with counting based Stokes polarimeter for spatial characterization the entangled spatial modes as measured in the Hermitte- of polarization properties of Second Harmonic (SH) light. Gaussian and Lagueere-Gaussian modal basis in an optical Thus, the critical polarization parameters can be obtained.  system of finite aperture. Visit www.frontiersinoptics.com for more information.

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FW2E • Exotic States and FW2F • Optical Fibers for Space FW2G • A Tribute to Steve FW2H • Adaptive Optics and LW2I • Integrated Quantum Applications I—Continued Projects—Continued Jacobs I—Continued Interferometry—Continued Photonics I—Continued

FW2H.2 • 10:45 A Versatile Method for Precise Control of Non-Uniform Beam Front Polarizations, Mat- thew T. Runyon1, Lambert Giner1, Alicia Sit1, Marissa Granados-Baez1, Ebrahim Karimi1, Jeff Lundeen1; 1Univ. of Ottawa, Canada. The Wednesday, 19 October generation of customized, non-uniform beam front polarization profiles are accomplished through the use of two incidences on a spatial light modulator and traditional optical components such as waveplates, lenses, mirrors, and beam splitters. Biography: Sylvain Girard got his PhD degree FW2E.2 • 11:00 from Saint-Etienne University (UJM), France in FW2G.2 • 11:00 Invited FW2H.3 • 11:00 LW2I.2 • 11:00 Invited Topological Darkness of Tamm Plasmons 2003. He joined CEA bas a post-doctoral fellow, Thirty-Five Years of Liquid Crystal Research Improvements in accuracy and process ef- Title to be Announced, Alexander L. Gae- for High-Sensitivity Singular-Phase Optical was recruited in 2004 and became a senior at LLE: From Laser Fusion to Electronic ficiency with multimode measurements of ta1; 1Columbia Univ., USA. Abstract not available. 1 Detection, Svetlana V. Boriskina , Jonathan member of technical staff. He was in charge of Paper, Kenneth L. Marshall1; 1Univ. of Roch- ophthalmic contact lenses, David C. Com- 1 1 2 1 1 Tong , Yoichiro Tsurimaki , Victor N. Boriskin , vulnerability and radiation hardening studies ester, USA. This presentation chronicles the pertore ; Lumetrics, USA. Typically, qualifying 3 2 Alexander Semenov , Mykola I. Ayzatskiy , Yuri of photonics for the Laser Mégajoule. In 2012, collaborations and events that lead to Steve a contact lens requires four different types of 4 1 1 P. Machekhin , Gang Chen ; Massachusetts Inst. Sylvain joined UJM as Full Professor to work on Jacobs’ efforts in the 1980’s to develop high- equipment, resulting in excessive handling of 2 of Technology, USA; Kharkiv Inst. of Physics and the development of predictive models for the peak-power liquid crystal (LC) optics for OMEGA the contact lens. Combining measurements 3 Technology, Ukraine; Inst. for Single Crystals behavior of optical materials and components and the LC applications research spawned at LLE strongly reduces the risks and increases the 4 NASU, Ukraine; Kharkiv National Univ. of Radio under irradiation. He has co-authored more from that pioneering work. efficiency of the quality control processes. Electronics, Ukraine. Multilayered photonic- than 140 journal papers and is the recipient of plasmonic structures exhibit topologically the 2013 IEEE NPSS Early Achievement and protected zero reflection if they are designed the 2014 IEEE Léon-Nicolas Brillouin Awards. to support Tamm plasmon modes. Sharp phase changes associated with the Tamm mode excitation dramatically improve sensitivity of detectors.

FW2E.3 • 11:15 FW2F.2 • 11:15 FW2H.4 • 11:15 Invited Creating `Optics’ for Singular Atom Optics Small Diameter Polarization Maintaining Pho- Advances in Adaptive Optics for Microscopy with Spinor Bose–Einstein Condensates, Jus- tonic Crystal Fiber for Spaceborne Miniatur- and Nanoscopy, Martin J. Booth1,2; 1Univ. of 1 1 1 1 tin T. Schultz , Azure Hansen , Joseph D. ized Gyroscopes, Cai Wei , Jing Jin , Jingming Oxford, UK; 2SAOT, Univ. of Erlangen Nurnberg, 1 1 1 2 2 1 Murphree , Maitreyi Jayaseelan , Nicholas P. Song , Wei Li , Wenyong Luo , Ningfang Song , Germany.Adaptive optics has been widely ap- 1 1 1 1 2 Bigelow ; Univ. of Rochester, USA. We present Chunxi Zhang ; Beihang Univ., China; Fi- plied to microscopes to compensate specimen- methods to create waveplates and phase plates berHome Telecommunication Technologies induced aberrations. We report on recent for pseudo-spin-1/2 atomic systems via two- CO., Ltd., China. An optimized small diameter developments extending these techniques to photon Raman interactions. The interactions polarization maintaining photonic crystal fiber more challenging methods, including to super- are geometrically represented as rotations on (PM-PCF) is proposed. Radiation response of resolution microscopes, or nanoscopes. the Bloch sphere. the PM-PCF and the performance of a 300-m mini coil demonstrate that the fiber is suitable for spaceborne gyroscopes.

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FW2A.3 • 11:30 FW2B.4 • 11:30 FW2C.4 • 11:30 FW2D.3 • 11:30 Invited Temporal multiplexing and simulation of multifocal Observation of Intrinsic Spin-Orbit Interaction of Light Synthetic holographic phase imaging in confocal micros- Open Channels in Scattering Media: See the Light 1 1 1 1,2 3 intraocular lenses, Vyas Akondi , Carlos Dorronsoro , En- in Few-Mode Optical Fiber, Dashiell L. Vitullo , Cody C. copy and applications, Martin Schnell , Sam Buercklin , Inside, Allard Mosk1; 1Debye Inst. for Nanomaterials Sci- 1 1 1 1 3 2 1 1 1 1 rique Gambra , Maria Vinas , Daniel Pascual , Sara Aissati , Leary , Patrick Gregg , Roger Smith , Dileep V. Reddy , Paulo Sarriugarte , Maria Jesus Perez-Roldan , Rainer Hil- ence, Universiteit Utrecht, Netherlands. Open channels are 1 1 2 1 1 4,5 2,3 1 Susana Marcos ; Consejo Sup Investigaciones Cientificas, Siddharth Ramachandran , Michael G. Raymer ; Univ. of lenbrand , P. Scott Carney ; CIC nanoGUNE Consolider, remarkable solutions of the wave equationthat carry light 2 2 Spain. Tunable lenses can simulate multifocal intraocular Oregon, USA; Electrical & Computer Engineering, Boston Spain; Beckman Inst. for Advanced Science and Technol- through a thick scattering sample. We measure the energy 3 3 lenses through temporal multiplexing. The effect of sampling, Univ., USA; Physics, College of Wooster, USA. Interaction ogy, Univ. of Illinois Urbana-Champaign, USA; Department density and frequency width of open channels and use them response time of tunable lens and choice of the through-focus between spin and intrinsic orbital angular momentum of light of Electrical and Computer Engineering, Univ. of Illinois as a sensitive probe of the scattering strength. optical quality metric in evaluating the temporal profile are in a straight few-mode fiber is observed to generate rotation Urbana-Champaign, USA; 4CIC nanoGUNE Consolider and investigated. for both polarization and spatial profiles, in agreement with EHU/UPV, Spain; 5IKERBASQUE, Basque Foundation for recent prediction. Science, Spain. We present synthetic optical holography for amplitude and phase-resolved confocal imaging. We apply our technique to optical topography mapping and numerical refocusing of out-of-focus confocal data.

FW2A.4 • 11:45 FW2B.5 • 11:45 FW2C.5 • 11:45 Light Sword Lens as Effective Method of Presbyopia Experimentally Demonstrating Quantum Data Locking Sensing pH in a Microfluidic Channel with a Lab-on-a- Compensation, Krzysztof Petelczyc1, Karol Kakarenko2,3, with a Quantum Enigma Machine, Daniel Lum1, Michael Smartphone Fluorescence Spectrometer, Jiajie Chen1, Andrzej Kolodziejczyk1, Zbigniew Jaroszewicz2,3, Marek T. Allman2, Thomas Gerrits2, Varun Verma2, Cosmo Lupo3, Ruoyu Wang1, Abhishek Renganathan1, Anurag Rattan1,

Wednesday, 19 October Wednesday, Rekas5, Alejandro Mira-Agudelo4, John Fredy Barrera 4, Seth Lloyd3, Sae Woo Nam2, John Howell1; 1Univ. of Roch- Xiangyue Meng1, Ranjith Rajasekharan Unnithan1, Kenneth Rodrigo Henao4; 1Faculty of Physics, Warsaw Univ of Tech, ester, USA; 2National Inst. of Standards and Technology, Crozier1,2; 1Electrical and Electronic Engineering, Univ. of Poland; 2Inst. of Aplied Optics, Poland; 3National Inst. of USA; 3Massachusetts Inst. of Technology, USA. We present Melbourne, Australia; 2School of Physics, Univ. of Melbourne, Telecomunications, Poland; 4Facultad de Ciencias Exactas y an experimental demonstration of quantum data locking as Australia. We demonstrate a smartphone unit for measuring Naturales, Universidad de Antioquia UdeA, Colombia; 5Oph- a quantum enigma machine that encrypts 6 bits per photon pH. The dye-mixed sample is input to a microfluidic chip and thalmology Department, Military Inst. of Medicine, Poland. with less than 6 bits per photon of encryption key while inserted into the unit. The smartphone image sensor records The monocular vision tests of 34 presbyopic patients was remaining information-theoretically secure. the fluorescence spectrum, and an app determines pH. performed for defocused BCDVA vision, stenopia and Light Sword Lens correction. We show that visual acuity in the LSL case is better than others while contrast sensitivity matches normal vision.

12:00–13:00 Lunch Break (on your own)

12:00–13:00 Environmental Sensing Technical Group Special Talk, Genesee Suite G, Radisson Hotel Rochester Riverside

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FW2E.4 • 11:30 FW2F.3 • 11:30 Invited FW2G.3 • 11:30 Invited LW2I.3 • 11:30 Invited 1 Dark Matter Optics, Humberto Michinel , An- Miniaturized Interferometric Fiber Optical Steve Jacobs: The Optics Outreach In- Experimental Photonic Quantum State 1 1 gel Paredes ; Universidad de Vigo, Spain. We Gyroscopes for Space Application, Jing novator, Tanya Z. Kosc2,1; 1Univ. of Roches- Transfer and Self-guided Tomography, Alberto explain galactic offsets in the Abell 3827 cluster Jin1, Cai Wei1, Song Jingming1, Xiaobin Xu1, ter, USA; 2Laboratory for Laser Energetics, Peruzzo1, Andreas Boes1, Robert Chapman1, by considering Dark Matter as a coherent Ningfang Song1, Chunxi Zhang1; 1Beihang USA. Steve Jacobs’ achievements extended to Zixin Huang1, Akib Karim1, Inna Krasnokutska1,

condensate of ultra-light axions forming Univ., China. The configurations of miniaturized the often overlooked realm of education and Jean-Luc Tambasco1; 1Quantum Photonics Labo- Wednesday, 19 October solitons, which display interference properties interferometric fiber optical gyroscopes (IFOG), outreach when he developed the innovative, ratory, Royal Melbourne Inst. of Technology, similar to those observed in nonlinear optics. miniaturized components, high reliability interactive Optics Suitcase. Initially conceived Australia. Integrated optics offers an attractive techniques and performance test results of for local middle schoolers, the Optics Suitcase platform for generating, manipulating and typical IFOG products are introduced in this has expanded worldwide. detecting quantum states of light. We report on paper. the experimental realization of the perfect state transfer protocol and the self-guided quantum tomography.

FW2E.5 • 11:45 FW2H.5 • 11:45 LW2I.4 • 12:00 Invited Measuring Exotic Looped Trajectories of Cost-Effective Adaptive Optics with the High Performances Integrated Single Photon 1 3,2 Light, Omar S. Magana Loaiza , Israel de Leon , Digital Light Ophthalmoscope, Matthew Sources, Pascale Senellart1; 1CNRS, Centre for 1 1 1 2,1 1 Mohammad Mirhosseini , Brian McIntyre , S. Muller , Ann E. Elsner ; Aeon Imaging, Nanoscience and Nanotechnology – C2N – 3 1,2 1 2 Brandon Rodenburg , Robert W. Boyd ; Univ. LLC, USA; School of Optometry, Indiana CNRS UMR9001, Site de Marcoussis, Route de 2 of Rochester, USA; Department of Physics and Univ., USA. A novel adaptive optics system for Nozay, France. Resonantly-excited quantum Max Planck Centre for Extreme and Quantum imaging the retina is presented. The system dots inserted in an electrically controlled pillar 3 Photonics, Univ. of Ottawa, Canada; School uses a digital light projector and rolling shutter cavity are shown to produce single photons with of Physics and Astronomy, Rochester Inst. of detector, permitting real-time adjustments to a purity and indistinguishability exceeding 99% Technology, USA. The probability of a photon the confocal aperture and a compact and cost- and a brightness 20 times higher than SPDC to follow looped trajectories in a three-slit effective layout. based single-photon sources. interferometer is extremely small and difficult to measure. We unveil the underlying physics and implications behind these trajectories and present their first observation.

12:00–13:00 Lunch Break (on your own)

12:00–13:00 Environmental Sensing Technical Group Special Talk, Genesee Suite G, Radisson Hotel Rochester Riverside

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13:00–14:15 13:00–14:30 13:00–14:30 13:00–14:00 FW3A • Novel Design Concepts for FW3B • Quantum Communications II FW3C • Diffuse Imaging and Optical FW3D • Symposium on Mesoscopic Optics Eye Correction and Vision Simulators II Presider: To be Announced Properties of Disordered Media II Presider: Filipp Ignatovich, Lumetrics Presider: Christine Hendon, Columbia Univ., Presider: Aristide Dogariu, CREOL, Univ. of Inc., USA and Vyas Akondi, Consejo Sup USA Florida, USA Investigaviones Cientificas, Spain

FW3A.1 • 13:00 Invited FW3B.1 • 13:00 Tutorial FW3C.1 • 13:00 Invited FW3D.1 • 13:00 Invited SimVis: See-through Simulation of Presbyopic Correc- Quantum-crypto Systems in the Commercial Service Net- Bedside Mapping of Human Brain Function with High Long Range Light Matter Interactions at Hyperbolic Meta tions, Carlos Dorronsoro1, Aiswaryah Radhakrishnan1, Jose work, Jeong-sik Cho2, Sean Kwak1; 1Univ. of Southampton, Density Diffuse Optical Tomography, Adam T. Egg- Surface, Girish Agarwal1; 1Oklahoma State Univ., USA. We Ramon Alonso-Sanz1, Daniel Pascual1, Enrique Gambra1, Vyas UK; 2Quantum Tech Lab, SK Telecom, Korea. Quantum-crypto ebrecht1; 1Washington Univ. in St Louis, USA. I will present show how long range light matter interactions can be realized Akondi1, Susana Marcos1; 1INSTITUTO DE OPTICA - CSIC, system has to evolve to provide customers with substantial our custom high density optical imaging system and at hyperbolic metasurfaces. We concentrate on the dipole- Spain. We developed a see-through portable binocular visual benefits such as low-cost, compactness and scalability as well analytical pipelines that enable optical mapping of human dipole interactions which are important for energy transfer simulator capable of simulating presbyopic corrections. as robustness, high service availability. brain function in the intensive care unit, the operating room, studies and in quantum entanglement between qubits at Subjects performed visual tests with 17 corrections (bifocal, and in sensitive populations including chidren with autism. metasurfaces. trifocal, monovision). Perceived quality differed across patients/corrections. Wednesday, 19 October Wednesday,

Biography: Jeong-sik Cho is an engineer and a manger in SK telecom. He has developed the optics part of the quantum key distribution system. Before he joined SK telecom, He worked in the optical fiber division of Samsung Electronics and in the optical communications lab of the Electronics and Telecommunications Research Institute. He received a Ph.D from the Korea Advanced Institute of Science and Technology, South Korea in 2008.

Join the conversation. Follow @Opticalsociety on Twitter. Use hashtag #FIO16 and #OSA100

64 FiO/LS 2016 • 16–21 October 2016 Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E

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13:00–14:30 13:00–14:30 13:00–14:00 13:00–14:30 13:00–14:30 FW3E • Plasmonics FW3F • Quantum Entanglement FW3G • A Tribute to Steve FW3H • Optical Design and GRIN LW3I • Multiphoton Effects II Presider: Volker Sorger; George Presider: Fabio Sciarrino; Univ Jacob II Materials Presider: Lingyan Shi; CUNY City Washington Univ., USA degli Studi di Roma La Sapienza, Presider: Jonathan Zuegel, Univ. of Presider: Blair Unger, Rochester College, USA Italy Rochester, USA Precision Optics, USA

FW3F.1 • 13:00 FW3E.1 • 13:00 Invited FW3G.1 • 13:00 Invited FW3H.1 • 13:00 Invited LW3I.1 • 13:00 Invited Wednesday, 19 October Plasmonics - Ultra-Fast Communications at the Multi-Photon Entanglement in High Dimen- Nanomechanics in Optical Manufactur- Tolerance Eigenmode Analysis of Optical Sys- Non-linear wavelength extension of Fibre 1,2 1,2 Microscale, Juerg Leuthold1; 1ETH Zurich, Swit- sions, Mehul Malik , Manuel Erhard , Marcus ing, John C. Lambropoulos1; 1Univ. of Roch- tems, John R. Rogers1; 1Synopsys, Inc, USA. We Laser Systems, J. R. Taylor1; 1Imperial College 3,4 1,2 1,2 zerland. Plasmonics has emerged as a solution Huber , Mario Krenn , Robert Fickler , Anton ester, USA. Nanomechanics addresses nm- describe a tolerance eigenmode analysis for London, UK. Spectral and temporal versatility 1,2 1 for monolithic integration of THz bandwidth Zeilinger ; Inst. for Quantum Optics and Quan- level material properties, including fracture, optical systems. This analysis indicates, in order is achieved using compact master oscillator photonic components at the microscale. In this tum Information, Austrian Academy of Sciences, mechanical-chemical interactions, and of importance, the combinations of aberrations power fibre amplifier schemes to drive nonlinear 2 talk we review recent advances in the field of Austria; Faculty of Physics, Univ. of Vienna, deformation. Nanomechanics applies to optical that will be induced by tolerances, thus allowing processes both fibre integrated and in bulk 3 optical communications and the microwave Austria; Universitat Autonoma de Barcelona, manufacturing from grinding, to finishing, better tolerance assignment and compensator allowing power scaled operation throughout 4 photonics enabled by plasmonics. Spain; ICFO-Institut de Ciencies Fotoniques, to polishing, including magnetorheological selection. the visible and mid infra-red. Spain. We create the first entangled state of finishing (MRF), as all these material removal more than two particles entangled in greater mechanisms essentially break atomic bonds. than two dimensions. Our state consists of three photons entangled in 3 × 3 × 2 dimensions of their orbital angular momentum.

FW3F.2 • 13:15 Generation of multi-photon entangled states with integrated optical frequency comb sources, Christian Reimer1, Michael Kues1, Piotr Roztocki1, Lucia Caspani1,2, Yaron Bromberg3, Benjamin Wetzel1,7, Brent Little4, Sai T. Chu5, David J. Moss6, Roberto Morandotti1; 1INRS- EMT, Canada; 2Heriot-Watt Univ., UK; 3Yale Univ., USA;4Xi’an Inst. of Optics and Precision Mechanics of CAS, China; 5City Univ. Hong Kong, China; 6Swinburne Univ. of Technology, Australia; 7Univ. of Sussex, UK. We demonstrate that four-photon entangled qubit states can be generated from an optical frequency combs source. This state generation is evidenced by four-photon quantum interference, and quantum state tomography reveals a fidelity above 64%.

FiO/LS 2016 • 16–21 October 2016 65 Grand Ballroom A (Radisson) Grand Ballroom B (Radisson) Grand Ballroom C (Radisson) Grand Ballroom D (Radisson)

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FW3A • Novel Design Concepts for FW3B • Quantum Communications II— FW3C • Diffuse Imaging and Optical FW3D • Symposium on Mesoscopic Optics Eye Correction and Vision Simulators II— Continued Properties—Continued of Disordered Media II—Continued Continued

FW3A.2 • 13:30 FW3C.2 • 13:30 Invited FW3D.2 • 13:30 Invited Surface-changing Accommodating Intraocular Lens Diffuse Optics for Monitoring Bone Healing and Cancer Cellulose Bio-inspired Hierarchical Structures, Silvia Vi- 1 for Presbyopia Correction, Andres De La Hoz , Eduardo Treatments, Regine Choe1; 1Univ. of Rochester, USA. Diffuse gnolini1; 1Cambridge Univ., UK. In this talk the route for the 1 1 1 Martinez-Enriquez , Carlos Dorronsoro , Nandor Bekesi , optical and correlation tomography have a great potential fabrication of complex bio-mimetic cellulose-based photonic 1 1 1 Nicolas Alejandre , Hrebesh Subhash , Daniel Pascual , to monitor and predict treatment efficacy. We demonstrate structures will be presented and the optical properties of 1 1 Susana Marcos ; CSIC - Inst. of Optics, Spain. An AIOL feasibility for chemotherapy on breast cancer and tissue artificial structures will be analysed and compared with the design that changes the shape of its surfaces thru application engineering based treatments for bone healing using natural ones. of equatorial forces is proposed. Its viability is evaluated murine models. using mechanical and optical simulations, and experimental measurements of focal length and surface shape change.

FW3A.3 • 13:45 FW3B.2 • 13:45 Retina-simulating phantom produced by chemically Generation and Reconstruction of Time-Bin Entangled Wednesday, 19 October Wednesday, amplified photolithography, Denise V. dos Santos1, Ququarts, Samantha Nowierski1, Neal N. Oza1, Prem Kumar1, Brian Vohnsen1; 1Univ. College Dublin, Ireland. To emulate Gregory S. Kanter1; 1Northwestern Univ., USA. We generate photoreceptors for an eye model, an array of dielectric and reconstruct a maximally-entangled time-bin ququart cylinders in a uniform matrix has been developed by using quantum state tomography and polarization-projective photolithography. Preparation details and sample analysis measurements. We measure a fidelity of 93.7 ± 0.4% to a are discussed in this work. maximally-entangled ququart with accidental coincidences subtracted.

FW3A.4 • 14:00 FW3B.3 • 14:00 FW3C.3 • 14:00 Measuring Temporal Integration in Human Vision with All-optical synchronization for quantum networks, Bruno Precisely Discerning the Bilirubin Concentration of Turbid Single Photons, Michelle M. Victora1, Rebecca M. Holmes1, Fedrici1, Lutfi A. Ngah1, Florian Kaiser1, Olivier Alibart1, Samples Using Diffuse Reflectance Spectroscopy, Ying Y. Ranxio Frances Wang1, Paul Kwiat1; 1Univ. of Illinois at Laurent Labonté1, Virginia D’Auria1, Sébastien Tanzilli1; 1Lab. Chen1, Shih-Yu Tzeng1, Kang-Yu Chu1, Yi-Ling Lin1, Sheng-Hao Urbana-Champai, USA. We discuss techniques using a de Physique de la Matière Condensée, France. We report Tseng1,2; 1Biophotonics Lab, Department of Photonic, Tai- heralded single-photon source to study the lower limit of an all-optical realization of a quantum relay experiment at a wan; 2Advanced Optoelectronic Technology Center, National human vision, specifically measuring temporal integration telecom wavelength. Our synchronization scheme is validated Cheng-Kung Univ., Tainan, Taiwan 701, R.O.C., Taiwan.We using multi-photon trials, and report preliminary results at by a two-photon interference visibility greater than 99% at demonstrated the use of our diffuse reflectance spectroscopy the few-photon level. the relay station. system to determine the absorption spectra of turbid samples containing bilirubin. The absorption spectra at 500nm were found to be highly correlated with the bilirubin concentration.

66 FiO/LS 2016 • 16–21 October 2016 Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E

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FW3E • Plasmonics—Continued FW3F • Quantum Entanglement— FW3G • A Tribute to Steve FW3H • Optical Design and GRIN LW3I • Multiphoton Effects II— Continued Jacob II—Continued Materials—Continued Continued

FW3E.2 • 13:30 Invited FW3F.3 • 13:30 FW3G.2 • 13:30 Invited FW3H.2 • 13:30 LW3I.2 • 13:30 Invited Novel Applications of Plasmonic Bowtie Einstein-Podolsky-Rosen Position-Momen- Materials Development in Magnetorheo- Implementation of a Scattering Method Medical Applications of Mid-IR Fibre Laser Nanoantennas in the Presence of Enhanced tum Entanglement in a Quantum Mem- logical Finishing: The work of Dr. Stephen for Rough Surfaces in a Raytracing Soft- Technologies, Giovanni Milione1; 1NEC Labo- 1 Local Heating, Kimani C. Toussaint1; 1Univ of ory Setup, Michal Dabrowski , Michal Par- Jacobs, Aric B. Shorey1; 1Corning Incorpo- ware linked with a CAD (Computer-Aided ratories America Inc, USA. 1 1 1 Illinois at Urbana-Champaign, USA. Increased niak , Radoslaw Chrapkiewicz , Wojciech rated, USA. The materials development in Design) Toolbox, Florian Loosen , Carsten 1 1 1 1 2 interests in optical nanoantennas have led Wasilewski ; Faculty of Physics, Univ. of Warsaw, Magnetorheological Finishing (MRF) has been Backhaus , Norbert Lindlein , Jochen Zeitler , Wednesday, 19 October 2 1 to recent novel applications that exploit the Poland. Raman scattering emissive multimode substantial over the past few decades. In this Jörg Franke ; Inst. of Optics, Information and enhanced local heating. We highlight select quantum memory setup is presented. The presentation, we will review the considerable Photonics (IOIP), Friedrich-Alexander-Universität 2 applications from low-input optical power memory enables storage of photonic position- contributions from Dr. Stephen Jacobs. Erlangen-Nürnberg (FAU), Germany; Inst. density tweezing to fabrication of planar optical momentum entanglement, demonstrating a for Factory Automation and Production Sys- components. time-delayed Einstein-Podolsky-Rosen paradox. tems (FAPS), Friedrich-Alexander-Universität Erlangen-Nürnberg (FAU), Germany. The design and simulation of printed polymer optical waveguides is a new approach in the field of raytracing techniques, to link the CAD routines with the simulation process of the waveguides via raytracing methods.

FW3F.4 • 13:45 FW3H.3 • 13:45 Measuring Non-Commuting Observables of Is the Maxwell-Shafer fish eye lens able to a Single Photon via Sequential Weak Values form super-resolved images?, Miguel A. Evaluation, Marco Gramegna1; 1Physical Metrol- Alonso1; 1Univ. of Rochester, USA. The Maxwell- ogy, INRiM, Italy. First experimental realization Shafer fish eye lens (a so-called absolute system) of a sequential weak value evaluation of two are studied theoretically to determine if it incompatible observable of a single photon. can form super-resolved images or obeys the diffraction limit. A modal analysis shows that the latter is true.

FW3E.3 • 14:00 FW3F.5 • 14:00 FW3H.4 • 14:00 LW3I.3 • 14:00 Invited Real-space mapping of chiral antennas and Few-photon induced transient entangle- Achromatic Design of Gradient Index Lenses Method for Transient Modulation of Refrac- 1,2 1 metasurfaces, Martin Schnell , Paulo Sarri- ment in multi-qubit bi-directional chiral using Ternary Blends, Guy Beadie , Jo- tive Index under Exposure to High-Power 1 3 1 2 1 ugarte , Tomas Neuman , Alexander B. Khani- waveguide QED, Imran M. Mirza , John C. seph N. Mait , Richard A. Flynn , Predrag Laser Pulses, Stavros G. Demos1; 1Labora- 4 5 3 1 1 2 1 kaev , Gennady Shvets , Javier Aizpurua , Rainer Schotland ; Univ. of Michigan, USA. We study Milojkovic ; US Naval Research Laboratory, tory for Laser Energetics, Univ. of Rochester, 6,7 1 2 Hillenbrand ; CIC nanoGUNE Consolider, transient entanglement generation and control USA; US Army Research Laboratory, USA. The USA. Optical elements that enable tailored 2 Spain; Beckman Inst. for Advanced Science and in multiple-qubit bi-directional waveguide addition of a third material to a binary blend modification of their refractive index during Technology, Univ. of Illinois Urbana-Champaign, QED utilizing single or two-photon Gaussian allows designers to specify refractive index exposure to laser pulses can help better control 3 USA; Materials Physics Center CSIC-UPV/ wavepackets. Particularly, we show how chirality and dispersion independently in gradient index beam characteristics. Our approach is based on 4 EHU and DIPC, Spain; Department of Physics, can enhance the maximum generated multi- optics. The effectiveness is demonstrated via activation of defect centers in large-bandgap Queens College of the City Univ. of New York, qubit entanglement. a diffraction-limited, f/1 achromatic singlet materials. USA; 5Department of Physics, The Univ. of Texas design. at Austin, USA; 6CIC nanoGUNE Consolider and EHU/UPV, Spain; 7IKERBASQUE, Basque Foun- dation for Science, Spain. We apply near-field microscopy (s-SNOM) to infrared Archimedean spiral antennas and resolve circular polarization resolved nanofocusing. We near-field image chiral metasurfaces and connect the observed near-field response with circular dichroism.

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FW3B.4 • 14:15 FW3C.4 • 14:15 Withdrawn. Development of an advanced model for determining the optical properties below and beyond 600 to 1000 nm wavelength range from frequency domain diffuse reflectance, Yu-Wen Chen1, Chien-Chih Chen1, Po-Jung Huang1, Sheng-Hao Tseng1,2; 1Department of Photonics, Na- tional Cheng-Kung Univ., Taiwan; 2Advanced Optoelectronic Technology Center, National Cheng-Kung Univ., Taiwan. We developed an artificial neural networks trained by frequency domain-based Monte Carlo simulation, which could work with a least-square optimized algorithm to recover an extensive range (below and beyond 600-1000nm) of sample’s optical properties.

Wednesday, 19 October Wednesday, 14:00–16:00 Student Chaper Competition, Empire Hall

14:30–15:00 Coffee Break, Empire Hall

14:30–16:00 JW4A • Joint Poster Session I and Unopposed Exhibit Time, Empire Hall (see page 23 for specific e-poster viewing times)

15:30–17:00 Meet the Editors of the APS Journals Reception, Riverside Court

16:00–17:00 OIDA Members and Exhibitor Appreciation Reception (OiDA members and exhibitors only), Empire Hall

68 FiO/LS 2016 • 16–21 October 2016 Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E

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FW3E.4 • 14:15 FW3F.6 • 14:15 FW3H.5 • 14:15 Deep Subwavelength and Broadband Light Generation of Path-Entangled Photons Using Design and Fabrication of Gradient-Index Delivery using an All-Fiber Plasmonic Nanotip- an Arrayed Waveguide Grating, Nobuyuki Optical Elements for Beam Shaping, James Enhanced Near-Field Probe, Alessandro Tuniz1, Matsuda1,2, Hidetaka Nishi1,3, Peter Karkus2, R. Leger1, Mint Kunkel1, Glen Douglass2, Simon Mario Chemnitz1,3, Jan Dellith1, Stefan Weidlich2, Tai Tsuchizawa1,3, Koji Yamada1,3, William J. Gross2, Michael Withford2; 1Univ. of Minne- 1,3 1 2 2 2 1 2 Markus Schmidt ; Inst. of Photonic Technology, Munro , Kaoru Shimizu , Hiroki Takesue ; NTT sota Twin Cities, USA; Physics and Astronomy, Wednesday, 19 October Germany; 2Heraeus Quarzglas GmbH & Co. Nanophotonics Center, Japan; 2NTT Basic Re- Macquarie Univ., Australia. We describe a new KG, Quarzstr. 8, Germany; 3Abbe School of search Laboratories, Japan; 3NTT Device Tech- method of generalized beam shaping based Photonics and Faculty of Physics, Germany. We nology Laboratories, Japan. We demonstrate on gradient index optics in waveguides. Phase experimentally demonstrate a monolithic the on-chip generation of path-entangled retrieval is used in the design and femtosecond nanowire-enhanced fiber-based plasmonic photon pairs using an arrayed-waveguide laser writing is used in the fabrication of the nanoprobe for broadband excitation (550- grating with nonlinear input waveguides. The waveguides. 730 nm) of short range surface plasmons and scheme can be extended to the generation of delivery of subwavelength radiation to a gold high-dimensional entanglement. nanotip with sub-100 nm apex radius.

14:00–16:00 Student Chaper Competition, Empire Hall

14:30–15:00 Coffee Break, Empire Hall

14:30–16:00 JW4A • Joint Poster Session I and Unopposed Exhibit Time, Empire Hall (see page 23 for specific e-poster viewing times)

15:30–17:00 Meet the Editors of the APS Journals Reception, Riverside Court

16:00–17:00 OIDA Members and Exhibitor Appreciation Reception (OiDA members and exhibitors only), Empire Hall

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14:30–16:00 JW4A • Joint Poster Session I

JW4A.1 JW4A.5 JW4A.9 E-Poster JW4A.13 JW4A.17 Simulating Phase-Only Pupil Plane Masks On the Microscopic Origins of Optical Mag- Experimental Observation of Second Har- Imaging Moving Objects Hidden in Arbi- Mode Amplification and Nonlinear Mode for Laser Suppression, Jacob H. Wirth1, netism - Insight from Mie Theory, Mengren monic Generation in polymeric Carbon trarily Heavily ScatteringMedia, Qiaoen Luo1, Conversion in Few Mode Fibers, Abderrah- Abbie Watnik2, Garreth Ruane1, Grover A. Man1, Kevin J. Webb1; 1Purdue Univ., USA. We Dioxide, Amartya Sengupta1, Choong-Shik Jason A. Newman1, Kevin J. Webb1; 1Purdue men Trichili1, Mourad Zghal1, Luca Palmieri2, Swartzlander1; 1Rochester Inst. of Technology, identify the microscopic origins for optical Yoo 2; 1Indian Inst. of Technology Delhi, Univ., USA. We show an image of a moving Marco Santagiustina2; 1Engineering School USA; 2U.S. Naval Research Laboratory, USA. A magnetism in dielectric metamaterials. Features India;2Washington State Univ., USA. Close to object (pi-shaped mask) embedded in heavily of Comm of Tunis, Tunisia; 2Dipartimento di phase-only pupil plane mask is tested to protect in the homogenized permeability are found to 20% efficiency of second harmonic generation scattering media using a coherent imaging Ingegneria dell’Informazione, Università di Pa-

sensors from powerful coherent radiation. Masks correspond to the magnetic dipole resonance of is observed in polymeric CO2 synthesized under approach. Spatial speckle intensity correlation dova, Italy. We demonstrate phase sensitive and are simulated to reduce the peak irradiance individual particles, which will have far-reaching novel conditions. This polymeric phase of measurements in relation to object position are insensitive amplification and nonlinear mode

of the point spread function while images are impacts. CO2 retains its non-linear optical properties over used to reconstruct the pi-shaped mask. conversion in few mode fibers by studying the reconstructed in post processing. a broad range of pressures and temperatures. four wave mixing effect. JW4A.6 This presentation will be presented as an JW4A.14 JW4A.2 Asymmetric Transport of Light through E-Poster on Screen 2 from 15:15–16:00 Towards the generation of entangled photon JW4A.18 Scalable and Gray-Coded Optical M-ary QAM All-dielectric Structured Media, Roxana pairs using a tapered fiber coupler, Lambert Spectral narrowing in the propagation of Using QPSK Modulators with Binary Elec- Rezvani Naraghi1,2, Sergey Sukhov1, Aristide JW4A.10 Giner1,2, Xinru Cheng1,2, Chams Baker1, Jef- unchirped pulses in two-core fibers, Nestor tronic Driving Signals, Naji A. Albakay1, Lim Dogariu1; 1Univ. of Central Florida, CREOL, Diffraction Compensation of Finite Beams in ferson Flórez1,2, Duncan G. England3, Philip J. Lozano-Crisostomo1,2, Julio Cesar Garcia Nguyen1; 1Electrical and Computer Engineering, USA; 2Department of Physics,, Univ. of Central Hyperbolic Metamaterials, Jisha C. Pannian1, Bustard3, Benjamin J. Sussman3, Xiaoyi Bao1, Jeff Melgarejo1,2, Miguel Torres Cisneros4, Daniel Univ. of Nebraska Lincoln, USA. We present Florida, USA. Asymmetric transmission of light Alessandro Alberucci2, Allan Boardman3, Gaeta- Lundeen1,2; 1Department of Physics, Univ. of Ot- Alberto May Arrioja3, Javier Sanchez Mon- a novel square M-ary QAM transmitter using usually requires chiral materials or grating- no Assanto2; 1Univ. of Porto, Portugal; 2Tampere tawa, Canada; 2Max Planck-uOttawa Center for dragon1; 1Departamento de Óptica, Instituto QPSK modulators driven by binary electronic like structures that make them sensitive to all Univ. of Technology, Finland; 3Univ. of Salford, Extreme and Quantum Photonics, Canada; 3Na- Nacional de Astrofísica, Óptica y Electrónica, signals. The proposed configuration generates parameters of incident light. Here we show UK. The propagation of finite size beams in tional Research Council of Canada, Canada. We Mexico; 2Universidad Autónoma de Coahuila, Wednesday, 19 October Wednesday, Gray-coded symbol constellations and is asymmetric transport of light that is broadband a hyperbolic metamaterial is modeled as a present the first steps towards the generation Mexico;3Centro de Investigaciones en Óptica, scalable for high order optical M-ary QAM. and polarization-insensitive. moving particle of negative mass. We show the of entanglement photon pairs by spontaneous Mexico; 4Departamento de Electrónica, Univer- occurrence of anomalous diffraction, diffraction four wave mixing inside a microcoupler device sidad de Guanajuato, Mexico. We demonstrate JW4A.3 JW4A.7 compensation and profile recovery for any input made by tapering two touching silica fibers until spectral narrowing in the propagation of an Proposal for Generation of Hybrid Entangled Estimation of atom loading efficiency into excitation. their core diameter reaches a few micrometers. initial unchirped optical pulse through a two- States in Waveguide Using Polarization a hollow core fiber, Taehyun Yoon1,2, Michal core fiber (TCF). Our results show that the linear Convertor, Divya Bharadwaj1, Krishna Thyaga- Bajcsy1,2; 1Inst. for Quantum Computing, Univ. JW4A.11 JW4A.15 coupling between both TCF cores induces that rajan1; 1Indian Inst. of Technology, Delhi, India. In of Waterloo, Canada; 2Department of Electrical Modeling the Evolution of Spatial En- A Statistical Analysis of Spatial and Spectral spectral narrowing. this paper we describe a scheme for generation and Computer Engineering, Univ. of Waterloo, tanglement with non-Gaussian Beams, Mat- Control with Binary Irregular Nanostruc- of hybrid spatial modal– polarization entangled Canada. We simulate the motion of Cs atoms thew Reichert1, Xiaohang Sun1, Jason W. tures, Yu-Chun Hsueh1, Kevin J. Webb1; 1Purdue JW4A.19 photon pairs using type-II spontaneous in a dipole potential created by a red detuned Fleischer1; 1Princeton Univ., USA. We study Univ., USA. We study the degrees of freedom Characterizing a 10×10 OAM propagation parametric down conversion process and the laser diverging from a hollow core photonic the dynamics of spatial entanglement during from a 2-D binary nanostructured material, as matrix of few-mode fiber by a dual-interfer- electro optic effect in a domain engineered KTP crystal fiber (HCPCF) and estimate the loading propagation and experimentally observe its they impact the achievable spectral and spatial ence pattern metho, Guoxuan Zhu1, Yuehan channel waveguide. efficiency into the fiber. migration between amplitude and phase. To control. This statistical analysis provides design Liu1, Yujie Chen1, Yuanhui Wen1, Yanfeng Zhang1, accommodate non-Gaussian biphotons, we strategies for applications. Hui Chen1, Siyuan Yu1; 1Sun Yat-sen Univ., JW4A.4 JW4A.8 generalize the “beam quality factor” M 2 from China. A dual-interference pattern method is Effect of Nonlinearity on the Formation of Generation of variable sized “perfect” vortex classical laser theory. JW4A.16 proposed for measuring OAM spiral spectrum, Spatial Optical Rogue Waves, Akbar Safari1, and its effect in parametric down conversion Phase Sensitive Amplification in Metastable including amplitude and phase information. Robert Fickler1, Miles J. Padgett2, Robert W. process, Jabir M. V.1, Apurv Chaitanya Nel- JW4A.12 Helium at Room Temperature, Jasleen Lugani1, With this method, we characterize the output Boyd1,3; 1Univ. of Ottawa, Canada;2Univ. of likka1, A. Aadhi1, Goutam K. Samanta1;1Physical Nonperturbative Nonlinear Optics in Liquid Chitram Banerjee1, Marie-Aude Maynard1, Pas- field of a few-mode fiber and obtain its 10×10 Glasgow, UK; 3The Inst. of Optics, Univ. of Research Laboratory, India. We report a novel Crystals, Alessandro Alberucci2, Armando Pic- cal Neveu1, Ram Soorat2, Rupamanjari Ghosh2, OAM propagation matrix. Rochester, USA. Randomness plays a crucial scheme to generate variable sized “perfect” cardi4, Nina Kravets4, Oleksandr Buchnev3, Jisha Fabien Bretenaker1, Fabienne Goldfarb1; 1Labo- role in the formation of optical seas. We observe vortices, having radius and order as mutually C. Pannian1, Gaetano Assanto2;1Univ. of Porto, ratoire Aime Cotton, France; 2Shiv Nadar Univ., JW4A.20 that when the random phase shift is not strong independent parameters, and prove that Portugal; 2Tampere Univ. of Technology, Fin- India. We have performed phase sensitive Portable Multiplexer Supporting Three Spa- enough, nonlinear propagation has a significant angular-spectrum of down-converted-photons land; 3Univ. of Southampton, UK; 4Univ. of Rome amplification (PSA) in metastable helium. The tially Multiplexed Optical Channels , Syed H. effect on the formation of rogue waves. does not depend on OAM of pump vortices. (RomaTre), Italy. We show that reorientational maximum and minimum gain behaviors and Murshid1, Saud Alanzi1, Guilherme Cavalcante1, nematic liquid crystals are an ideal workbench their values compared to the gain for the Phase Bilas Chowdhury1, Rayan Enaya1;1Florida Inst. of for the investigation of non-perturbative Insensitive Amplification (PIA), correspond to a Technology, USA. Design of the input end of a nonlinear optical effects and report light self- very pure PSA. portable spatial multiplexer supporting three steering, power-controlled negative refraction spatially multiplexed optical channels over a and spontaneous symmetry breaking. multimode fiber is presented. Screen projection of the output beam and its intensity profile is also reported.

70 FiO/LS 2016 • 16–21 October 2016 Empire Hall

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JW4A • Joint Poster Session I—Continued

JW4A.21 JW4A.25 JW4A.29 JW4A.33 JW4A.37 Demonstration of Optical Sensing with LPGs Influence of Two Weak Continuous Wave D-Shaped Polarization Maintaining Fiber Design of BCD to Excess 3 code converter An improved FRFT-based method for esti- Inscribed on Polymer Functionalized Optical Triggers on Picosecond Supercontinuum Sensor for Simultaneous Monitoring of using electro-optic effect of Mach-Zehnder mating physical parameters from Newton’s Microfibers, Yuhang Li1, Zhongyang Xu2, Lijun Generation, Ji Zhu1, Cai Wen1, Qian Li1; 1School Refractive Index and Temperature, Hummad Interferometers, Chanderkanta Chauhan1, San- rings, Jin-Min Wu1,2, Ming-Feng Lu1,2, Ran Wang1; 1Department of Precision Instrument, of Electronic and Computer Engineering, Peking Qazi1, Abu B. Mohammad1, Harith B. Ahmad2, tosh Kumar1, Angela Amphawan2,3; 1DIT Univ., Tao 1,2, Feng Zhang1,2; 1Beijing Inst. of Tech- Tsinghua Univ., China; 23Shanghai Inst. of Univ., China. We numerically demonstrate the Mohd Z. Zulkifli2; 1Universiti Teknologi Malaysia, India, India; 2School of Computing, Universiti nology, China; 2Beijing Key Laboratory of Laser Plasma, China. We demonstrated LPG improvement in the pulse-to-pulse stability in USA; 2Univ. of Malaya, Malaysia. A D-shaped Utara Malaysia, Malaysia; 3Massachusetts Inst. Fractional Signals and Systems, China. This inscription on polymer functionalized optical the picosecond supercontinuum generation PMF as fiber optic sensor is presented for of Technology, USA. In this paper, a four bit BCD paper proposes a novel method for estimating

microfibers via point-by-point ultraviolet laser by using two weak continuous wave triggers. simultaneous monitoring of RI and surrounding to Excess 3 code convertor using electro-optic parameters from Newton fringe patterns often Wednesday, 19 October exposure. Also presented are its potential temperature. Experimental results show that effect of lithium niobate based Mach Zehnder encountered in interferometry. The presented applications in optical sensing of strain, axial JW4A.26 proposed sensor has high sensitivity of 0.03nm/ interferometer (MZI) is proposed. The results are results demonstrate that the method is robust force and temperature. Combination and compression of eight RIU and 0.13nm/oC for RI and temperature verified using beam propagation method and to noise and has applications in interferometric pulses in nonlinear fibers with exponentially respectively. MATLAB simulation. measurements. JW4A.22 decreasing dispersion, Ziyun Jian1, Wei Lu1, Intensity Distribution of Spatially Multiplexed Qian Li1; 1School of Electronic and Computer En- JW4A.30 JW4A.34 JW4A.38 Architectures Supplementing Wavelength gineering, Peking Univ., China. We demonstrate Dielectric-grating-coupled surface plasmon Mode Conversion of Four-Mode Fiber with Polarization Independent Single-PD Coherent 1 Division Multiplexing, Syed H. Murshid , combination and compression of eight chirped resonance for ultrasensitive sensing, Shaohua CO2-Laser Written Long-Period Fiber Grat- Receiver without Synchronous Processing Saud Alanzi1, Bilas Chowdhury1; 1Florida Inst. raised cosine pulses. The initial 1 ps pulse can Pi1,2, Xie Zeng1, Nan Zhang1, Dengxin Ji1, Hao- ings, Yunhe Zhao1, Yunqi Liu1, Chenyi Zhang1, for OOK System, Ke Wen1, Junjie Tu1, Yanli of Technology, USA. Intensity distribution of be compressed to 83 fs, and its peak power is min Song1, Suhua Jiang2, Qiaoqiang Gan1;1State Jianxiang Wen1, Tingyun Wang1;1Shanghai Univ., Zhao1; 1Wuhan Natianal Lab. for optoelectronics, spatially multiplexed system complementing nearly 51 times compared to the initial pulse. Univ. of New York at Buffalo, USA; 2Fudan Univ., China. We demonstrate the mode conversion China. In this paper, we present a polarization- WDM channels is presented. Results show that China. We proposed a dielectric grating that between the fundamental core mode and independent (PI) single-PD coherent receiver energy distribution of SDM is independent of JW4A.27 can launch surface plasmon resonance mode different higher-order core modes of four-mode without synchronous processing. The proposed wavelength. They supplement each other and Measurement Dependence and Limited efficiently on the other side of flat metal films fiber with high efficiency of more than 98.5% by receiver can achieve PI in frequency domain and 1 have potential to increase fiber data capacity. Detection Nonlocality, Djeylan Aktas , Gilles with normal incident light, which is suitable for the CO2-laser written long-period fiber gratings. improve the performance without increasing Pütz2, Anthony Martin2, Rob Thew2, Bruno Fe- the integration with optical fiber tips. system complexity. JW4A.23 drici1, Nicolas Gisin2, Sébastien Tanzilli1;1LPMC, JW4A.35 Mathematical Representation of Spatially France; 2GAP, Switzerland. We investigate two JW4A.31 Optimal Measure for the Polarization Estima- JW4A.39 Multiplexed Channels Using Azimuthal Index approaches to attest quantum nonlocality. We Synchronous dual-wavelength pulse gen- tion of Light with Arbitrary Photon Statis- Analysis dynamics of optical speckles in and Modified Laguerre Gaussian Beams, Syed assume, first, limited measurement dependence, eration in an Er-doped fiber laser with tics, Lu Zhang1, Kam Wai C. Chan1, Pramode the study pure liquids, Danylo Babich1, Val- H. Murshid1, Ahmed Kadhim1, Bilas Chowdhury1, and then introduce limited detection efficiency. near-zero dispersion, Guoqing Hu1, Ru- K. Verma1; 1Univ. of Oklahoma, USA. We entina Pobiedina1, Artem Levchuk1, Andrey Gregory L. Lovell1, Saud Alanzi1; 1Florida Inst. of In both cases, we show experimental violations liu Wang1, Yingling Pan1, Xin Zhao1, Meng present an optimal measure for the estimation Yakunov1; 1Taras Shevchenko National Univ., Technology, USA. This presents a mathematical of the corresponding Bell-type inequality. Zhang1, Zheng Zheng1,2; 1School of Electronic of the polarization of light with arbitrary photon Ukraine. Laser-speckle patterns dynamics model relating incident angle of a spatially and Information Engineering, Beihang Univ., statistics. The success probability and the mean caused by transmission irradiation through multiplexed system to the azimuthal index of JW4A.28 China; 2Collaborative Innovation Center of fidelity are calculated, and comparisons against the liquid have been studied. Frame by frame a modified Laguerre-Gaussian beam equation. All Normal As2S5-Borosilicate Hybrid Photonic Geospatial Technology, China. We demonstrate an adaptive measurement are made. analysis of speckle video has shown that the Preliminary data shows good correlation Crystal Fiber for Ultra Flat-Top Mid-Infrared synchronous dual-wavelength pulse generation decaying of the amplitude of the correlation between experimental results and the model. Supercontinuum , Amine Ben Salem1, Mbaye in a CNT modelocked Er fiber laser with reduced JW4A.36 functions depends on liquids parameters. Diouf2,1, Rim Cherif1, Abderrahmen Trichili1, Ah- dispersion based on polarization-dependent Study on Toxic Chromium (VI) metal ion Sens- JW4A.24 madou Wague2, Mourad Zghal1; 1Engineering spectral filtering, and four-wave mixing between ing with Hydrogel Coated Fiber Bragg Grat- JW4A.40 Modal Dispersion of Helically Propagating School of Communication of Tunis (Sup’Com), the synchronized pulses is observed. ing, Pabbisetti Vayu Nandana Kishore1, Madhu- Numerical Modeling of a Mode Selective Spatially Multiplexed Optical Channels Oper- Tunisia; 2Univ. of Cheikh Anta Diop, Department varasu Sai Shankar1, C Hari Krishna1;1National Photonic Lanterns using the Beam Propaga- ating at 1550nm, Syed H. Murshid1, Gregory L. of Physics, Laboratoire Atome-Laser, Dakar, JW4A.32 Inst of Technology, Warangal, India. The Paper tion Method, Gisela Lopez-Galmiche1, Jesús Lovell1, Saud Alanzi1, Bilas Chowdhury1;1Florida Senegal, Senegal. Ultra flat-top broadband Factorable photon-pair generation in mul- discusses a chemo- mechanical- optical sensing Escobedo-Alatorre2, Miguel Basurto-Pensado2, Inst. of Technology, USA. Modal dispersion for supercontinuum spanning 1 to 5 µm with high timode optical fibers, Hamed Pourbeyram approach for sensing harmful Chromium ions Javier Sanchez Mondragon1; 1Inst Nat Astrofisica a two channel spatially multiplexed system is spectral flatness of 8 dB is obtained in 4-mm- Kaleibar1, Arash Mafi1; 1Univ. of New Mexico, in environment. FBG is functionalized with a Optica Electronica, Mexico; 2Centro de Inves-

calculated using effective area based normalized long all-normal-dispersion As2S5-Borosilicate USA. We present a theoretical study of multiple stimulus responsive hydrogel which swells or tigación en Ingeniería y Ciencias Aplicadas ,

frequency parameter (Veff), which shows that such hybrid photonic crystal fiber by injecting 50 factorable photon-pairs generation in SMF- deswells depending on ambient chromium ion Mexico. A mode selective photonic lantern,

systems can significantly reduce modal delay of fs-1.6 nJ pulses at 2.5 µm. 28 optical fiber and show the capability concentrations. which is able to generate the LP01, LP11a and

multimode optical fiber channels. of multimode optical fibers as sources for LP11b modes with a linear taper, is modeled using wavelength-tunable factorable photon pairs. the beam propagation method. Modal analysis is also estimated.

FiO/LS 2016 • 16–21 October 2016 71 Empire Hall

JOINT FiO/LS

JW4A • Joint Poster Session I—Continued

JW4A.41 JW4A.45 JW4A.49 E-Poster JW4A.54 JW4A.58 Tailoring light by 3D direct laser-writing Multiplexing three-dimensional optically Lensless Measurements of Optical Field Microsphere Stabilized Plane-Parallel Resona- Accurate Determination of Inner Diameter 1 of micron-scale phase elements, Shlomi encrypted data, Alejandro Velez , Roberto Correlations, Katelynn Sharma1, Thomas G. tors Fabricated via Convective Assembly, Jose for X-Ray Mono-Capillary Optics, Kwon Su 1,2 1 2 1 1,3 2 1 1 1 1 1 1 2 1 Lightman , Raz Gvishi , Ady Arie ; NRC, Torroba , John Fredy Barrera ; CIOp, Argen- Brown1, Miguel Alonso1; 1Univ. of Rochester, A. Rivera , Tom Galvin , James G. Eden ; UIUC, Chon , Yoshiharu Namba ; Catholic Univ. of 2 2 2 Israel; Electrical Engineering, Tel-Aviv Univ., tina; Instituto de Física, Universidad de Antio- USA. We investigate a method to measure USA. An array of microspheres, situated near Daegu, Korea; Chubu Univ., Japan. Small 3 Israel. We demonstrate experimentally phase quia, Colombia; Facultad de Ingenieria, UNLP, spatial coherence that uses no lenses in the one mirror of a critically-stable cavity, stabilize inner diameter of a mono-capillary optics modulation of light beams by fabricating Argentina. We introduce a multiplexing method measurement. Three variations of this method the cavity at positions occupied by the spheres. was precisely measured by using synchrotron arbitrary microstructures using a 3D-Direct for three-dimensional data experimentally are compared, and we find one using three Each microlaser in the resulting array exhibits beamline which provided images of high Laser writing method. This approach produces encrypted using a joint transform correlator. amplitude masks to be the most robust. strong mode confinement and unique spectral resolution. The measurement accuracy was 0.67 complex structured light beams, in a compact, Encrypted data are individually filtered and This presentation will be presented as an characteristics. μm, and diameters along the axis direction were stable and cost effective manner. added forming a multiplexed package. Each E-Poster on Screen 2 from 14:30–15:15 also measured. object is retrieved using a key object. JW4A.55 JW4A.42 JW4A.50 Increasing the Speed of CCD-Based Ther- JW4A.59 Square Holey Cladding Dielectric THz JW4A.46 A simple wavefront re-construction optical moreflectance Imaging: Theory and Ex- Partially polarized speckle of light scattered 1 1 1 Waveguides for Chip-to-Chip Communica- Observation of two state behavior in elements combination, Hai Lin1; 1Shanghai periment, Mark Hallman , Kyle Allison , from depolarizing media, Gabriel Soriano , 1 2 1 1 2 2 1 tion, Nafiseh Aflakian , Naixin Yang , Timothy the Supercontinuum Generation induced Inst of Optics & Fine Mechanics, China. A Janice A. Hudgings ; Physics and Astronomy, Myriam Zerrad , Claude Amra ; Institut Fres- 1 2 2 LaFave , Rashaunda Henderson , Kenneth K. by insability in Saturable Nonlinear Me- simple wavefront re-construction optical Pomona College, USA. We experimentally and nel, Aix-Marseille Université, France; Institut 2 1 1 1 O , Duncan MacFarlane ; Electrical Engineer- dia, Kanagaraj Nithyanandan , Porsezian element is designed.It uses uniaxial optical theoretically examine methods for increasing Fresnel, CNRS, France. The spatial distribution 2 1 1 ing, Southern Methodist Univ., USA; Electrical Kuppusamy ; Pondicherry Univ., India. The crystals to re-arrange a beam with transverse the image acquisition speed in CCD-based of the time-averaged intensity is theoretically Engineering, Univ. of Texas at Dallas, USA. The supercontinuum generation is observed to inhomogeneous intensity profile but thermoreflectance measurements by increasing and numerically studied when light of arbitrary development of a square holey cladding behave in a unique in saturable nonlinearity, homogeneous state-of-polarization. the sampling rate, for signal amplitudes both partial polarization state is strongly scattered dielectric waveguide for chip-to-chip THz such that the broadband is observed at above and below the quantization limit. from a depolarizing medium.

Wednesday, 19 October Wednesday, communication is presented. Designed to shortest distance for pumping at saturation JW4A.51 operate in the range of 180-360GHz, measured power, in comparison to all other pump power Withdrawn. JW4A.56 JW4A.60 and simulated mode profiles of fabricated configurations. Discussions on advantages of ghost imag- A Simple Method to Measure the Complex waveguides are in good agreement. JW4A.52 ing compared to traditional optical imag- Refractive Index of Conducting Media, Fer- 1 1 2 JW4A.47 Thermal Imaging Microscope and Applica- ing, WeiTao Liu ; College of Science, NUDT, nando Arturo Araiza Sixtos , Maximino Avenda- 1 1 2 JW4A.43 E-Poster Nonuniform Laguerre-Gaussian Correlated tions to Microelectronic Devices, Ki Soo China. Ghost imaging promises higher spatial ño-Alejo ; CCADET-UNAM, Mexico; Faculty of 1 1 Image Processing Applied to Photon Sparse Partially Coherent Beam, Jiayi Yu ; Soochow Chang1; 1Korea Basic Science Inst., Korea. We resolution, higher robustness against harsh Sciences, Mexico. A simple method to measure 1 1 Data, Lena Mertens , Matthias Sonnleitner , Univ., China. A new kind of partially coherent demonstrate a thermal imaging microscope environment, higher detection sensitivity, and the refractive index of metals considering 2 2 Jonathan Leach , Megan Agnew , Miles beam called a nonnuiform Laguerre-Gaussian system that measures the temperature more options in system designing due to the the Fresnel coefficients for reflectance and 1 1 2 Padgett ; Univ. of Glasgow, UK; Dept. of correlated partially coherent beam have distribution over the surface of microelectronic controllability of the source. Our results on this expanding in Taylor’s series is proposed. We Physics, Heriot-Watt Univ. , UK. We present an been introduced. It is found that the intensity devices. It enables hot spot detection and will be reported. present measurements, which could be in image reconstruction algorithm for producing distribution exhibits self-focusing, self-shifting thermal analysis of microelectronics devices. agreement with other optical methods. grey-scale images derived from binary photon- and self-splitting effect. JW4A.57 sparse data. The algorithm is based upon a JW4A.53 The Origin of Asymmetric Transmission in JW4A.61 1 likelihood of Poissonian distribution combined JW4A.48 Additive random noise in generalized phase- Chiral Photonic Crystals, Nikhil Parappurath , Determination of width of subapertures in 1 1 with a measure of image smoothness. Scattered-Light Analysis of Birefringent shifting algorithms, Gastón Ayubi1, José A. Fer- Filippo Alpeggiani , Kobus Kuipers , Ewold Lattice design for stitching interferometry 1 1 1 This presentation will be presented as an Coatings for Distributed Polarization Rota- rari1; 1Universidad de la Republica, Uruguay. The Verhagen ; FOM Inst. AMOLF, Netherlands. We of aspheric surfaces, Junzheng Peng , Xiaoli 1,2 3 1 2 1 1 E-Poster on Screen 4 from 14:30–15:15 tors, Katelynn Sharma , Thomas Germer , purpose of the present work is study the phase present a fundamental limit to asymmetric Liu , Yingjie Yu , Xiang Peng ; Shenzhen Univ., 2 2 2 Christopher Smith , Jonathan Zuegel , James extraction from interferograms with additive transmission (AT) in strongly chiral photonic China; Shanghai Univ., China. Determination 2 1 1 JW4A.44 Oliver , Thomas G. Brown ; Univ. of Rochester, random noise, and deduce the conditions to crystals. We develop a theory that fully predicts of the width of subapertures is a key issue in 2 Solitonic Self-Spectral Compression of Noisy USA; Laboratory for Laser Energetics, Univ. be satisfied for minimizing the phase-retrieval AT from eigenmode properties, and show stitching interferometry of aspheric surface. This 1,2 3 Supercontinuum Radiation, Hrach Toneyan , of Rochester, USA; Sensor Science Division, error. Simulations are presented. that near-unity AT can be reached in suitable paper proposed a method to solve this problem Minas Sukiasyan1,2, Vardan Avetisyan1, Aghavni National Inst. of Standards and Technology, designs. based on the slope resolution capability of Kutuzyan1, Arsham Yeremyan2, Levon Moura- USA. Novel, birefringent thin-film coatings interferometer. dian1,2; 1Yerevan State Univ., Armenia; 2CANDLE have been developed for improved irradiation Synchrotron Research Inst., Armenia. We uniformity by polarization smoothing in direct- experimentally demonstrate solitonic self- drive fusion. Forward scatter distribution of 351 spectral compression for noisy supercontinuum nm radiation is characterized and its operational radiation in a single-mode fiber. The numerical impact analyzed. modeling of the process shows the prospects of the noise nonlinear suppression for partially coherent pulses.

72 FiO/LS 2016 • 16–21 October 2016 Empire Hall

JOINT FiO/LS

JW4A • Joint Poster Session I—Continued

JW4A.62 JW4A.65 JW4A.69 JW4A.73 JW4A.77 Resting-State Functional Connectivity Mea- Compact hyper-spectrometer based on meta- Diffraction at the grating and appearance of Nonlinear dynamics, bifurcation maps, signal Optical Vortex Microscope-Analytical Model surement in the Mouse Brain using a Low Cost surfaces at visible wavelengths, Alexander Y. “spirits” from the view of radiooptics, Vasily encryption and decryption using acousto- and its Experimental Verification, Agnieszka Photoacoustic Computed Tomography, Ali Zhu1, Wei-Ting Chen1, Mohammadreza Kho- Kazakov1, Oleg Moskaletz1, Nadezhda Firono- optic chaos under a variable aperture il- Popiolek-Masajada1, Jan Masajada1, Lukasz Hariri1, Parsa Omidi1, Mohammadreza Nasi- rasaninejad1, Jaewon Oh1,2, Rober Devlin1, Ishan va1; 1St. Petersburg State Univ. of Aerospace lumination, Monish R. Chatterjee1, Suman Plociniczak1; 1Wroclaw Univ. of Technology, riavanaki1; 1BME, Wayne state Univ., USA. We Mishra1,2, Federico Capasso1; 1John A Paulson Instrumentation, Russian Federation. Diffraction Chaparala1; 1Univ. of Dayton, USA. Bragg cell Poland. Model of the microscopic optical system use photoacoustic technology to noninvasively School of Engineering and Applied Science, at the grating from the view of radiooptics nonlinear dynamics and bifurcation properties in which the optical vortex is embedded within image Resting-State Functional Connectivity Harvard Univ., USA; 2Univ. of Waterloo, Cana- is considered. The properties of spectrum in under first-order feedback with variable the Gaussian beam and focused to the sample

(RSFC) in the mouse brain, with a high frame da. We present a compact hyper-spectrometer different diffraction orders are established. aperture are examined. Chaotic encryption plane is considered. The analytical solutions are Wednesday, 19 October rate, large field of view and high spatial resolu- using only planar metasurface lenses and a The mathematical justification for appearance and recovery of low-bandwidth signals, and verified in the experimental setup. tion at different depths. CMOS camera. Spectral resolutions as small as of “spirits” at diffraction on the grating is optimal performance are evaluated for fixed approximately 300 pm (detector-limited) and proposed. and variable apertures. JW4A.78 JW4A.63 an overall working range exceeding 130nm at Withdrawn. High Numerical Aperture Meta-lenses at Vis- visible wavelengths are achieved. JW4A.70 JW4A.74 ible Wavelengths, Mohammadreza Khorasani- Negative Index in Chiral Metamaterials under Revival of Hanbury Brown-Twiss Effect and JW4A.79 nejad1, Wei-Ting Chen1, Alexander Zhu1, Jaewon JW4A.66 Conductive Loss and First-Order Material Its Application on Single-Arm Ghost Imaging Blueshift in the Near Band Edge Emission Oh1,2, C. Roques-Carmes1,3, Ishan Mishra1, Rober Undergraduate Laboratory on Polarization Dispersion Using Lorentzian, Condon and Based on Discrete Chaotic Light, Liming Li1, and in the Optical Band Gap of Sr Doped Devlin1, Federico Capasso1; 1Harvard Univ., Using Poincaré Beams, Joshua A. Jones1, Drude Models, Monish R. Chatterjee1, Tarig Peilong Hong2, Guoquan Zhang1;1Nankai Univ., ZnO Films, Vandana Masih1, Anchal Srivas- USA; 2Univ. of Waterloo, Canada; 3École Poly- Anthony J. D’Addario1, Enrique J. Galvez1; 1Col- Algadey1; 1Univ. of Dayton, USA. Emergence China; 2Nanjing Univ. of Science and Technol- tava1; 1Univ. of Lucknow, Lucknow, India, India. A technique, France. We report high numerical gate Univ., USA. Gaussian and higher order of negative index (NIM) in chiral materials ogy, School of Science, China. Based on a blueshift in the near band edge emission in aperture meta-lenses in the visible spectrum Laguerre-Gauss mode beams are combined to with conductive loss using standard dispersive discrete chaotic light source, we demonstrated the strontium doped zinc oxide thin films with focal spots as small as 0.65λ. Meta-lenses form Poincaré beams having spatially varying models is reported. Positive and negative phase the revival effect of second-order spatial deposited by sol-gel method is observed. The are based on titanium dioxide metasurface polarization. We developed a new lab using and group indices are realized as expected correlation pattern with multiple bunching nanocrystalline films show an enhancement in phase masks.They operate in transmission mode Poincaré beams as an exercise to teach states for NIM behavior for sidebands with opposite peaks, which can be used to achieve ghost the optical band gap by 6.6%. and are polarization-insensitive. of polarization. polarities. imaging in a single-arm configuration. JW4A.80 JW4A.64 JW4A.67 JW4A.71 JW4A.75 Imaging Darkness, Adam Selyem1, Thomas Enhanced Spectral Sensitivity of a Chip- Multifilter Phase Imaging with Partially Coher- High-output-power third-harmonic genera- In-line system for intensity and topological W. Clark1, Neal Radwell1, Sonja Franke-Ar- 1 1 1 Scale Photonic-Crystal Slow-Light Inter- ent Light: Nonparaxial Case, Yijun Bao , Thom- tion at 355nm based on La2CaB10O19 (LCB) charge characterization of optical vorti- nold ; Univ. of Glasgow, UK. We present ferometer, Boshen Gao2, Omar S. Magana as K. Gaylord1; 1Georgia Inst. of Technology, crystal in yz plane, Lirong Wang1; 1Inst. of Semi- ces, Edgar Rueda1, Jorge Gomez2, Dafne a technique for reconstructing bright and Loaiza2, Sebastian A. Schulz1, Kashif M. Awan3, USA. The existing quantitative phase imaging conductors, China. Third-harmonic generation Amaya3, Alberto Lencina4; 1Universidad de dark light sculptures. The method is based Jeremy Upham1, Ksenia Dolgaleva1,3, Robert method Multifilter Phase Imaging with Partially based on LCB crystal was investigated in yz Antioquia, Colombia; 2Politécnico Colombiano on recording fluorescence from a thermal W. Boyd2,1; 1Department of Physics and Max Coherent light (MFPI-PC) has been extended plane. The maximum output power at 355 nm Jaime Isaza Cadavid, Colombia; 3Centro de rubidium gas directly or after atomic depletion Planck Centre for Extreme and Quantum to nonparaxial case. Its improved accuracy has was 11.5W . The angular bandwidth and tem- investigaciones ópticas, Argentina; 4Universidad respectively. Photonics, Univ. of Ottawa, Canada; 2The Inst. been verified using simulations and microlens perature bandwidth were measured, which are Nacional del Centro de la Provincia de Buenos of Optics, Univ. of Rochester, USA; 3School of experimental measurements. larger than the previous reports also. Aires, Laboratorio de análisis de suelos, Argen- JW4A.81 Electrical Engineering and Computer Science, tina. An in-line system to recover simultaneously Withdrawn. Univ. of Ottawa, Canada. By placing a slow-light JW4A.68 JW4A.72 topological charge and intensity of an optical- photonic-crystal waveguide in one arm of a Light Scattering Spectroscopy of Nanosilica Experimental study of the vortex phase vortex is presented. It is based on adding a JW4A.82 fiber-based Mach–Zehnder (MZ) interferometer, Particles Aggregating in Single, Freely Sus- induced-change of the polarization structure Fresnel lens to a vortex-producing lens. The Persistence and fidelity of phase singularities we experimentally demonstrate that structural pended Micrometer-Sized Evaporating Drop- of a radially polarized beam, Lina Guo1,2, need of an interferometer is eliminated. in optical random waves, Lorenzo De Angelis1, slow light can be used to enhance the spectral let, Mariusz P. Wozniak1, Justice Archer1, Daniel Yangjian Cai1, Fei Wang1, Xianlong Liu1, Lin Filippo Alpeggiani1, Andrea Di Falco2, L. Kuipe- sensitivity of the interferometer Jakubczyk1, Gennadiy Derkachov1, Krystyna Liu1;1School of Physical Science and Technol- JW4A.76 rs1; 1Center for Nanophotonics, AMOLF, Nether- Kolwas1, Maciej Kolwas1; 1Inst. of Physics Pol- ogy and Collaborative Innovation Center of Withdrawn. lands; 2SUPA, School of Physics and Astronomy, ish Academy of Sciences, Poland. The light Suzhou Nano Science and Technology, So- Univ. of St Andrews, UK. As the wavelength is scattering spectroscopy of single, micrometer- ochow Univ., China; 2School of Electronics and varied, phase singularities in random waves are sized evaporating droplet was developed. Information, GuangDong Polytechnic Normal created, diffuse and annihilate. With near-field We report a well-pronounced change in the Univ., China. We carried out the theoretical experiments we map their trajectories as a visible spectrum of the nanosilica suspension and experimental study on the propagation of function of wavelength and study correlations corresponding to different stages of aggregate a focused radially polarized vortex beam. It is between creation and annihilation events. formation. found that the state of polarization of such beam rotates and changes on propagation.

FiO/LS 2016 • 16–21 October 2016 73 Empire Hall

JOINT FiO/LS

JW4A • Joint Poster Session I—Continued

JW4A.83 E-Poster JW4A.87 JW4A.90 JW4A.94 JW4A.99 Formation of LIPSS in nanocomposites of Poly Quantitative Measurement of the Average Anisoplanatic Electromagnetic Image Propa- New algorithm of adaptive focusing of laser Local and nonlocal nonlinear response of (ethylene terephthalate)/Expanded Graphite Orbital Angular Momentum of Light with a Cy- gation through Narrow or Extended Phase beam developed on conservation laws of its Ag nanocubes in solution as function of size 1 1 1 1 by using UV nanosecond laser pulses, Rene I. lindrical Lens, Samuel Alperin , Robert Nieder- Turbulence using Altitude-Dependent Struc- propagation, V. A. Trofimov , Artem Kotkov , and concentration, Emma V. García Ramírez , 2 3,2 1 1 1 1 1 1 Rodriguez Beltran1, Margarita Hernandez2, Tibe- riter , Juliet T. Gopinath , Mark Siemens ; Univ. ture Parameter, Monish R. Chatterjee , Ali Tatiana Lysak ; M. V. Lomonosov Moscow State Jorge alejandro Reyes Esqueda , Daysi Ramírez 2 1 1 1 1 rio A. Ezquerra2, Anna Szymczyk3, Sandra Pasz- of Denver, USA; Physics, Univ. of Colorado, Mohamed ; Univ. of Dayton, USA. The effects Univ., Russian Federation. We propose a new Martínez , Sergio Sabinas Hernandez , Gabriela 3 1 1 kiewicz3, Zbigniew Roslaniec3, Marta Castillejo4, USA; Electrical, Computer, and Energy En- of turbulence on anisoplanatic imaging are algorithm of adaptive focusing of laser beam by Díaz Guerrero ; Univ Nacional Autonoma de Pablo Moreno1, Esther Rebollar4; 1Universidad gineering, Univ. of Colorado, USA. We show often modeled through the use of a sequence using the conservation laws of optical radiation Mexico, Mexico. Cubic silver nanoparticles were de Salamanca, Spain;2Instituto de Estructura de that the average orbital angular momentum of phase screens distributed along the optical propagation in linear and non-linear medium. analyzed by Z-scan technique in the resonant la Materia (IEM-CSIC), Spain; 3West Pomeranian (OAM) of twisted light can be measured with path. We implement the split-step wave and no-resonant regimes. These results were Univ. of Technology, Poland; 4Instituto de Quími- a single stationary cylindrical lens and camera. algorithm to examine turbulence-corrupted JW4A.95 done with picosecond pulse as function of the ca Física Rocasolano (IQFR-CSIC), Spain. We Our method can be calibrated absolutely and images. Withdrawn. size and concentration of the samples. report the formation of Laser Induced Periodic measure arbitrary (non-integer) average OAM. Surface Structures in Poly(ethylene terephthal- JW4A.91 JW4A.96 JW4A.100 ate) and Poly(ethylene terephthalate)/Expanded JW4A.88 Self-Healing of Laguerre-Gauss Beams A Point Spread Function for Fourier Teles- Robust Statistical Parity-Time Symmetric 1 1 Graphite films. Some physical properties of Diffraction Gratings Prepared by HR-LIPSS Described by Superposition of Conical-Like copy, William T. Rhodes ; Florida Atlantic Univ., Lasers in Fiber Cavities, Ali Kazemi Jah- 1 1 1 the surfaces improve in the presence of these for New Surface Plasmon-Polariton Pho- Traveling Waves, Jorge A. Ugalde-Ontive- USA. A spatial frequency domain point spread romi , Absar U. Hassan , Ayman Abouraddy , 1 1 3 1 1 nanostructures. todetectors & Sensors, Iaroslav Gnilitskyi , ros , Alfonso Jaimes-Najera , Job Mendoza- function for Fourier telescopy imaging is defined Demetrios Christodoulides ; Univ. of Central 2 3 4 1 This presentation will be presented as an Sergiy Mamykin , Mykhaylo Dusheyko , Tatiana Hernández , Marcelo D. Iturbe-castillo , Sabino and its properties discussed. The function is Florida, CREOL, USA. We demonstrate that 4 3 1,2 1 E-Poster on Screen 5 from 14:30–15:15 Borodinova , Nataliya Maksimchuk , Leonardo Chavez-Cerda ; Inst Nat Astrofisica Optica given by the inverse Fourier transform of the many features of PT-symmetric lasing, such Orazi1; 1UNIMORE, Italy; 2V. E. Lashkaryov Inst. Electronica, Mexico; 2Centro de Investigaciones object illumination intensity distribution. as the lower predicted lasing threshold and 3 JW4A.84 of Semiconductor Physics, National Academy of en Optica, Mexico; Departamento de Fisica, PT-symmetric phase transition, are sufficiently 3 4 Wednesday, 19 October Wednesday, A 10-GHz Optical Frequency Comb from a Sciences of Ukraine, Ukraine; National Techni- CINVESTAV, Mexico; Facultad de Ciencias JW4A.97 robust to be observed in a long fiber cavity (>1 SCOWA-Based Mode-Locked Laser with 600- cal Univ. of Ukraine “Kiev Polytechnic Inst.”, Fisico-Matematicas, Benemerita Universidad A system to control the energy of a high- km) despite random phase fluctuations. 4 Hz Optical Mode Linewidth, Kristina Bagnell1, Ukraine; National Academy of Sciences of Autonoma de Puebla, Mexico. We demonstrate power laser system and its application to x-ray Anthony Klee1, Peter Delfyett1;1Univ. of Central Ukraine, F. D. Ovcharenko Inst. of Biocolloid that propagation of Laguerre-Gaussian beams generation at ultra-high intensity, Baozhen JW4A.101 1 1 1 Florida, CREOL, USA. We present a harmonically Chemistry, Ukraine.New method based on has not been fully understood since some Zhao , Wenchao Yan , Ping Zhang , Sudeep Transparent Perfect Mirror via Non-Hermitian 1 1 1 1 mode-locked laser at 10-GHz repetition rate HR-LIPSS for diffraction grating on preliminary observed phenomena with them cannot be Banerjee , Grigory Golovin , Colton Fruhling , Systems, Ali Kazemi Jahromi , Soroush Sha- 1 1 1 1 1 with high saturation power SCOWA gain, with fabricated p-n junction on Si substrate are explained without the use of transverse traveling Daniel Haden , Jun Zhang , Cheng Liu , bahang , H. Esat Kondakci , Ayman Abou- 1 1 1 1 1 a long external fiber cavity and intracavity etalon suggested. This allows to produce surface wave features similar to those of Bessel beams. Shouyuan Chen , Donald P. Umstadter ; Univ. raddy ; Univ. of Central Florida, CREOL, for supermode suppression, with optical mode plasmonic photodetectors based on periodically of Nebraska Lincoln, USA. We demonstrate a USA. We have experimentally demonstrated an linewidth of 600 Hz. corrugated thin metal plasmon-carrying films. JW4A.92 system to control the output energy of a high- optical device that provides 100% broadband Magnetic response of split nanotube type energy, ultrashort pulse laser system by an reflection, yet transmits light. The device JW4A.85 JW4A.89 metamaterial at near infrared frequency, Nis- order-of-magnitude. This technique is used to is a sub-lasing active cavity in which the 2 1 Optical Nonlocal nonlinear properties in Raman spectroscopy for CVD monolayer gra- hant Shankhwar , Ravindra K. Sinha , Yogita Kal- control the brightness of an Inverse-Compton resonances in reflection disappear at a critical 2 1 2 [EMIM][B ], Israel Severiano Carrillo1, Edgar phene: Fermi levels depending on different ra ; CSIR-CSIO, India; Department of Applied x-ray source. gain threshold. 4 1 Alvarado Méndez1, Monica Trejo Durán1; 1DI- substrates material, Solveyga Azbite , Alaudi Physics, Delhi Technological Univ., India. In this 1 1 1 CIS, Universidad de Guanajuato, Mexico. We Denisultanov , Mikhail Khodzitsky ; Univ. ITMO, paper, we present the design of a split nanotube JW4A.98 JW4A.102 used the nonlocal nonlinear model by the Russian Federation. Energies of Fermi level of type metamaterial which shows strong magnetic Generation and Switching of Phase Vortices ZnO Films Photoluminiscence and Nonlinear 1 1 characterization of Ionics liquid ([EMIM][BF ] monolayer graphene on quartz, polyethylene resonance at infrared frequency. Its operation is in Cylindrical Vector Beams, C Hari Krishna , Optical Properties, Emma V. García Ramírez , 4 1 1 1 by the z-scan technique to nonlinear refraction terephthalate (PET) and Si were calculated using similar to that of split ring resonator (SRR) but is Sourabh Roy ; Physics, National Inst. of Jorge Alejandro Reyes Esqueda , Roberto Lo- 2 2 and nonlinear absorption curves. Numerical Raman spectroscopy data. The dependence of easier to fabricate at nanoscale. Technology Warangal, India. Cylindrical vector péz , Enrique Vigueras-Santiago , Daysi Ramírez 1 1 and experimental results show ionic liquid as Fermi level energy on refractive index of the beams are generated using a two mode optical Martínez ; Univ Nacional Autonoma de Mexico, 2 nonlocal medium. substrate was shown. JW4A.93 fiber. Vortex and anti-vortex are observed in Mexico; Universidad Autónoma del Estado de Electro-optic dual-comb vibrometry, Vicente interferograms formed by helical and plane México, Mexico. We study photoluminescence 1 1 JW4A.86 D. Durán , Elena L. Teleanu , Víctor Torres- wavefronts.Switching between them is achieved properties of direct-gap of ZnO films for 1 1 Spectral Analysis of Bragg and non-Bragg Company ; Chalmers Univ. of Technology, by changing input polarization state. different grain size and we obtained lasing Orders in Dynamic Holography using Photore- Sweden. We use an ultrafast electro-optic dual threshold. The crystalline structure, surface fractive Materials, Akash Kota1, Ujitha Abey- comb interferometer to perform single-point morphology and optical properties of the thin wickrema1, Partha P. Banerjee1; 1Univ. of Dayton, vibrometry on the submillisecond time scale. We films have been investigated. USA. Interaction of Bragg and non-Bragg orders resolve the vibration of an ultrasound speaker in a photorefractive material during two-beam driven at 50 kHz, achieving a sub-nanometer coupling is studied by numerically solving the axial resolution. coupled differential equations for the angular plane wave spectra of all interacting orders.

74 FiO/LS 2016 • 16–21 October 2016 Empire Hall

JOINT FiO/LS

JW4A • Joint Poster Session I—Continued

JW4A.103 JW4A.106 E-Poster JW4A.110 JW4A.114 JW4A.117 E-Poster Subluminal speed of higher orders of physi- Alternative Fusing Algorithm for High Beam Shaping through Turbid Media by Self-trapping of Light Through Red Blood Filtering Doppler OCT Improves Unwrapping 1,2 1 cal light beams, Nestor Jr. Bareza , Nathaniel Speed Gabor Domain Optical Coherence Feedback-based Wavefront Shaping, Jix- Cell Suspensions, Rekha Gautam , Joshua Lam- and Extends Range of Microscopic Fluid Ve- 1,2 1 1 1 1 1 1 1 1 Hermosa ; National Inst. of Physics, Philip- Microscopy, Panomsak Meemon1, Pornthep iong Pu , Lipeng Wan , Ziyang Chen , Huiling stein , Anna Bezryadina , Zhigang Chen ; San locity Measurement, Yang Xu1,2, Donald Darga2, 2 1 1 pines; Univ. of the Philippines-Diliman, Philip- Pongchalee1, Joewono Widjaja1, Jannick P. Huang ; College of Information Science Francisco State Univ., USA. We observe self- Jason Smid2, Adam Zysk2, Daniel Teh1, Stephen pines. We report the dependence of light’s Rolland2;1School of Physics, Suranaree Univ. of and Engineering, Huaqiao Univ., China. We trapping and deep penetration of a laser beam Boppart1,2, P. Scott Carney1,2; 1Univ of Illinois at speed delay to the mode indices of higher beam Technology, Thailand; 2Inst. of Optics, Univ. of demonstrate that the focusing of light into in human red blood cell (RBC) suspensions Urbana-Champaign, USA; 2Diagnostic Photon- orders. We demonstrated this by calculating the Rochester, USA. An alternative Gabor-based desired patterns through turbid media can under isotonic, hypotonic, and hypertonic ics, Inc., USA. Using the modified Robust Phase group velocity of Laguerre Gauss beam with fusing algorithm that improves the processing be realized using feedback-based wavefront conditions, in spite of the intrinsic absorption Tracker algorithm for denoising, we demonstrate Wednesday, 19 October orbital order and radial order. speed of the GD-OCM is presented. The fusion shaping. The desired focused patterns, such as and scattering loss due to RBCs. DOCT velocity unwrapping of datasets with is performed in spectral domain and hence a triangle-shape beam, are obtained. peak velocity up to 14.5 cm/s. This technique JW4A.104 could enable hardware-based fusion, which is JW4A.115 significantly extends the measureable range of Extending the high-order harmonic genera- promising for real time GD-OCM. JW4A.111 Two-dimensional correlation between blood DOCT velocity. tion cutoff by means of self-phase-modulated This presentation will be presented as an Superresolution Second Harmonic Generation glucose and optical scattering for noninvasive This presentation will be presented as an 1,2 1,3 chirped pulses, E. Neyra , F. Videla , J.A. E-Poster on Screen 1 from 15:15–16:00 Microscopy based on Point-scanning Struc- blood glucose sensing with optical coherence E-Poster on Screen 1 from 14:30–15:15 Perez-Hernandez4, M.F. Ciappina5, L. Roso4, tured Illumination, Szu-Yu Chen1, Chia-Hua tomography, Ya Su1, Huiqing Liu1, X. Steve 1 1 1 1 1 1,2 1 3 1 Gustavo Torchia ; Centro de Investigaciones JW4A.107 Yeh , Cheng-Zn Tan ; National Central Univ., Tai- Yao , Changjiang Wei , Zhihong Li ; Hebei JW4A.118 2 2 Opticas, Argentina; Departamento de Física, Indirect Zinc Phthalocyanine excitation due wan. Since fluorescence-based superresolution Univ., China; General Photonics Corporation, Deep-Tissue Optical Imaging and Pho- 3 Facultad de Ciencias Exactas Universidad Na- nonradiative quantum dots couppling, Guil- techniques can’t be applied to second harmonic USA; Suzhou Optoring Co. Ltd., China. We toactivation Activities at Biophotonics@ 3 cional de La Plata, Argentina; Departamento de herme A. Alves2,1, Arnaldo F. Reis1, Adamo F. generation microscopy (SHGM), a system propose an algorithm of using two-dimensional Tyndall, Stefan Andersson-Engels2,1, Moni- Ciencias Básicas,, Facultad de Ingeniería Univer- Monte1, José Maria Villas-Bôas1, Djalmir N. combing structured illumination and SHGM correlation analysis between blood glucose and rehalsadat Mousavi1, Haichun Liu3, Andreas 4 sidad Nacional de La Plata, Argentina; Centro Messias 1; 1Universidade Federal de Uberlândia, was introduced to get a 1.41 resolution optical scattering coefficient of skin tissues for Walther1, Lars Rippe1, Stefan Kröll1; 1Lund Univ., 5 de Láseres Pulsados (CLPU), Spain; Max Planck Brazil; 2Instituto Federal de Ciência e Tecnologia improvement factor in the chicken tendon. the noninvasive blood glucose measurement Sweden; 2Tyndall National Inst., Univ. College Inst. of Quantum Optics, Germany. In this work de Goiás, Brazil. This work reports the study of with optical coherence tomography (OCT). Cork, Ireland; 3Biomedical Engineering, National we propose a new approach to extend the the energy transfer from CdSe/ZnS core-shell JW4A.112 Univ. of Singapore, Singapore.Activities for cutoff in high-order harmonic generation (HHG) quantum dots to Zinc Phthalocyanine dye. It Raman Spectral Histopathology of Breast JW4A.116 deep tissue imaging and photoactivation will 1 spectra beyond the well established limits.We was found the ZnPc emitted wavelength which Cancer Recession Margins, Dustin W. Shipp , Quantification of Fluorescence Enhance- be presented. Wihin Biophotonics@Tyndall proj- 1 2 3 achieved this extension by using driven pulses travels the longest distance along the samples. Kenny Kong , Emad Rakha , Ian Ellis , Ioan ment Due to Dielectrophoresis and the ects based on upconverting nanoparticles and 1 1 obtained by means of self-phase-modulation Notingher ; School of Physics and Astronomy, Plasmonic Effect Using Time-Resolved ultrasound optical tomography will be pursued. 2 1 (SPM). JW4A.108 Univ. of Nottingham, UK; Department of Pa- Fluorescence, Ivan T. Lima , Logeeshan Velman- Data from collaborative research will be given. 1 2 High-throughput Characterization of thology, Nottingham Univ. Hospitals NHS Trust, ickam , Michael Fondakowski , Dharmakeerthi 3 1 1 JW4A.105 Nanoparticle Stability Using Near-field Optical UK; School of Molecular Medical Sciences, Univ. Nawarathna ; Department of Electrical and JW4A.119 Laser Quest : A Laser-Based Education and Trapping, Perry Schein1, David Erickson1; 1Cor- of Nottingham, UK. We demonstrate a Raman Computer Engineering, North Dakota State Study of Photodynamic Therapy applied to 2 Outreach Program - Coupling Practice with nell Univ., USA. We show high-throughput spectroscopy system that quickly maps tumors Univ., USA; Department of Mechanical Engi- the treatment and fluorescence-based diag- 1,2 1 Content (URACE), Sumit Ghosh ; Physics, measurements of the interactions between in thick pieces of breast tissue immediately neering, North Dakota State Univ., USA. We nosis of infiltrative Basal Cell Carcinoma in- 2 Andhra Vidyalaya College, India; Physics, nanoparticles and surfaces, characterizing following excision. Diagnostic accuracy is used time-resolved fluorescence to show that cluding gold nanoparticles, Félix Fanjul-Vélez1, Andhra Vidyalaya College - Osmania Univ., colloidal stability based on fluctuations in high with the potential to increase with more dielectrophoresis can increases the fluores- Jose L. Arce-Diego1; 1TEISA, Univ. of Cantabria, India. More than five decades have passed scattered light during interaction with a database samples. cence emission due to the plasmonic effect Spain. Photodynamic Therapy dosimetry is an since the first laser was demonstrated, it still waveguide on particles with <100 nm diameters. near nanostructured metallic electrodes by a unresolved issue for treatment effectiveness, continues to amaze and delight with its power JW4A.113 factor of 3, which can significantly reduce the particularly when using nanoparticles. In this and applications. An outreach program was JW4A.109 Conditions Leading to Eryptosis in Eryth- detection sensitivity. work the treatment and fluorescence-based organised to teach optics using laser light. Exploiting Optical Asymmetry for Frequency- rocytes: A Raman Tweezers Study, Surekha diagnosis is analyzed when applied to infiltrative 1 1 controlled Guiding of Particles with Light, Og- Barkur , Aseefhali Bankapur , Santhosh Chi- Basal Cell Carcinoma. 1 1 njen Ilic1, Ido Kaminer1, Yoav Lahini1, Hrvoje dangil ; Department of Atomic and Molecular Buljan2, Marin Soljacic1;1Massachusetts Inst. of Physics, Manipal Univ., India. Raman tweezers JW4A.120 Technology, USA; 2Department of Physics, Univ. was used to study eryptosis in erythrocytes Enhanced Scaffold Guided Cellular Motion Us- of Zagreb, Croatia. We propose a novel method induced by different reasons. Our study shows ing Polarized Light, Colin Constant1, Kiminobu to guide particles that is controllable by the that, though the main cause of eryptosis may be Sugaya2, Daniel Ng2, Aristide Dogariu1; 1Univ. of frequency of light. With detailed simulations, oxidative stress, the consequences of different Central Florida, CREOL, USA; 2Burnett School we demonstrate exceptional degree of control, stressors may be different. of Biomedical Sciences, Univ. of Central Florida, independent of the direction of the light beam USA. Cellular motion along substrate channels and insensitive to scattering. confines the cellular motion linearly. The addition of an optical field linearly polarized parallel to the substrate channel enhances this motion due to optical torques applied to subcellular elements.

FiO/LS 2016 • 16–21 October 2016 75 Empire Hall

JOINT FiO/LS

JW4A • Joint Poster Session I—Continued

JW4A.121 JW4A.127 JW4A.131 JW4A.136 JW4A.140 Super-Resolved Microscopy with Spatial Grating Design for 3-D Interconnections of Transverse electric surface mode in atomically Study of Energy Transfer between Quantum Surface-lattice resonances in 2d arrays of Frequency-Modulated Imaging, Keith Werns- Waveguides in Overlaid Chips Using the thin Boron-Nitride, Michele Merano1; 1Uni- Dots and a Two-Dimensional Semiconduc- spheres: multipolar couplings and normal ing1, Jeffrey J. Field1, Randy Bartels1; 1Colorado RCWA-EIS Method, Congshan Wan1, Thomas versita degli Studi di Padova, Italy. Atomically tor, Kenneth M. Goodfellow1, Chitraleema modes, Sylvia Swiecicki1, John E. Sipe1; 1Univ. State Univ., USA. We present a super-resolved K. Gaylord1, Muhannad S. Bakir1; 1Georgia Inst. thin Boron-Nitride is predicted to support a Chakraborty1, Kelly Sowers1, Pradeep Waduge2, of Toronto, Canada. We present a multipolar imaging technique for real and virtual state of Technology, USA. The rigorous coupled-wave transverse electric non-radiating surface mode Meni Wanunu2, Todd Krauss1, Kristina Driscoll3, model of the surface - lattice resonances in interactions, which measures object spatial analysis–equivalent-index-slab (RCWA-EIS) in the visible spectrum. This mode has a spatial A. Nick Vamivakas1; 1Univ. of Rochester, arrays of spheres. We show the importance frequency projections at bandwidths exceeding method is used to determine the diffraction confinement of 15 microns and an intensity- USA; 2Northeastern Univ., USA; 3Rochester Inst. of couplings between multipoles of different the diffraction limit by a factor of approximately efficiencies of gratings for 3-D coupling between propagation distance greater than 2 cm. of Technology, USA. We explore the efficiency of polarity and characterize the dispersion of twice the interaction nonlinearity. overlaid chips. The simulation results are energy transfer between colloidal quantum dots multipolar modes. validated by FDTD calculations. JW4A.132 E-Poster with a cadmium selenide core and cadmium JW4A.122 Gain-Assisted Surface Plasmon Polaritons: sulfide shell and monolayer molybdenum JW4A.141

Withdrawn. JW4A.128 Time Domain Analysis with Experimentally diselenide (MoSe2), separating them by thin Plasmon enhanced whispering gallery mode Fresnel coefficients of a two-dimensional Fitted Organic Dye Models, Shaimaa Azzam1, layers of hexagonal boron nitride (h-BN). sensor using Nanostructure, Seunghun JW4A.123 atomic crystal, Michele Merano1; 1Universita Nikita Arnold2, Ludmila Prokopeva3, Zhaxylyk Lee1, Hyerin Song1, Tae Young Kang1, Seon- Surface Plasmon-enhanced Super-resolution degli Studi di Padova, Italy. I compare the slab Kudyshev1, Alexander Kildishev1; 1Purdue Univ., JW4A.137 hee Hwang1, Taerim Yoon1, Heesang Ahn1, Imaging Using Silver Nanoislands, Taehwang model and the surface conductivity model of USA; 2Johannes Kepler Univ., Austria; 3Novosi- Plasmonic Nanoantenna Array with Single- Kyujung Kim1; 1NanoBioPhotonics Lab, Ko- Son1, Yougjin Oh1, Wonju Lee1, Donghyun graphene to interpret the most remarkable birsk State Univ., Russian Federation. Kinetic Chip Integrated Metal-Organic Framework rea. Whispering gallery mode optical sensor Kim1; 1Yonsei Univ., Korea. Surface plasmon- experiments in graphene optics. Only the parameters of a six-level model are obtained by for Infrared Absorption Gas Sensing, Xinyuan has detected sub-micron sized molecules by enhanced super-resolution imaging has been surface conductivity model is able to explain matching the experimental data for a fluorescent Chong1, Ki-Joong Kim1, Erwen Li1, Yujing mornitoring the resonance peak shift. We studied using silver nanoislands. The size of the overall experimental data. dye to study loss-compensation in the surface Zhang1, Paul Ohodnicki2, Chih-Hung Chang1, described ‘plasmonic enhanced’ whispering localized near-field was in the range of 100- plasmon-polariton propagating along a silver Alan X. Wang1; 1Oregon State Univ., USA; 2Na- gallery mode sensor using nanostructure and it

Wednesday, 19 October Wednesday, 150nm, which affects the resolution. Fluorescent JW4A.129 film covered with a gain layer. tional Energy Technology Lab, USA. Plasmonics confirmed by computer simulations. actin filament of J774 cells was imaged. Optical control with large-scale assembly of This presentation will be presented as an devices are usually not suitable for gas highly aligned silver nanowires, Yunsheng E-Poster on Screen 5 from 15:15–16:00 spectroscopy due to the limited enhancement JW4A.142 JW4A.124 Fang1, Yuanpeng Wu2, Jun Zhou1, Qing Yang2, length. Here, we demonstrate a plasmonic Mid-IR Resonant Cavity Detectors, Trevor Driving force that controls a protein reaction Bin Hu1; 1Wuhan National Laboratory for Op- JW4A.133 nanopatch array coated with metal-organic A. O’Loughlin1, Gregory Savich1,2, Daniel for optogenetics, Masahide Terazima1; 1Chem- toelectronics, Huazhong Univ. of Science and Withdrawn. framework for CO2 sensing, with enhancement Sidor1, Brendan Marozas3, Gary Wicks1, Terry istry, Kyoto Univ., Japan. Driving force of a Technology, China; 2College of Optical Science factor over 1100 times. Golding4, Keith Jamison4, Leis Fredin4, Bert photo-reaction of a photosensor protein were and Engineering, Zhejiang Univ., China. Large- JW4A.134 Fowler4, Weerasinghe Priyantha4; 1Inst. of investigated by a time-resolved transient grating scale aligned silver nanowires arrays was Silicon On-chip Nanobeam Bandstop Filters JW4A.138 Optics, USA; 2Air Force Research Laboratory, method. The result indicates that the enhanced obtained using controlled capillary printing for the Parallel Multiplexing of Integrated 1D Light extraction efficiency enhancement of USA; 3Materials Science, Univ. of Rochester, fluctuation of the conformation is a key factor. technology. Optical simulations were conducted Photonic Crystal Nanobeam Cavity Sensors organic light-emitting diodes fabricated on USA; 4Amethyst Research, Inc., USA.Resonant to gain the single silver nanowire and nanowires Array, Daquan Yang1; 1Beijing Univ. of Posts silica network substrate, Dong B. To1; 1Na- cavity detectors have been grown by MBE. They JW4A.125 arrays optical behaviors. and Telecom., China. We propose a novel tional Chung Cheng Univ., Taiwan. This research offer a low noise, narrow response detector in Magnetic field enhancement in dielectric is- method for the dense integration of nanoscale focuses on the improvement of internal light the mid-infrared region, with possible applica- land assisted by metal nanoslit arrays, Jeong- JW4A.130 1D photonic crystal (1D-PC) sensors array, which out-coupling of organic light emitting diodes tions in spectroscopy, gas sensing, and optical Geun Yun1, Sun-Je Kim1, Joonsoo Kim1, Bragg Grating Encrypted Metal Clad Ridge can be interrogated simultaneously between a (OLED) with enhancement factor about 2.25 communications. Byoungho Lee1; 1Seoul National Univ., Korea. In Waveguide as an Highly Sensitive & Compact single input and output port. The footprint is times compared with a conventional OLED. this paper, we propose a structure that consists Bio-Sensor, Nabarun Saha1, Arun Kumar1; 1In- ultra-compact of 4.5μm×50μm. JW4A.143 of a dielectric island and a metal nanoslit array. dian Inst. of Technology, Delhi, India. It is shown JW4A.139 Spontaneous emission studies of blue In numerical simulation, the proposed structure that the RI sensitivity of a Bragg grating based JW4A.135 Withdrawn. and green InGaN-based laser diode struc- shows a huge magnetic field enhancement up ridge waveguide can be increased significantly Analysis of various ZrN plasmonic nano- ture, Gyu-Jae Jeong1, Sung-Nam Lee1; 1Korea to a factor of 61. by including a thin metal layer between the core structures and their effect on the absorption Polytechnic Univ., Korea.Blue/green LEDs and substrate. of organic solar cells, Sara Al Menabawy1, represented higher efficiency droop than blue/ JW4A.126 Qiaoqiang Gan2, Mohamed Swillam1; 1American green LDs under the same injection current Single CdTe Nanowire Optical Correla- Univ. in Cairo, Egypt; 2Electrical Engineering, density. Because of same epi-structures, we tor, Chenguang Xin1, Limin Tong1; 1Zhejiang Univ. at Buffalo, The State Univ. of New York, suggested that efficiency droop may be due Univ., China. Based on second harmonic USA. We incorporated ZrN nanoparticles, to the difference of heat dissipation structure. generation in a 800-nm diameter CdTe nanow- nanocubes and nanoshells in organic solar cell ire, we demonstrated an optical correlator for and theoretically demonstrated broadband femto-second pulse measurement. Benefitted absorption enhancement due to high scattering from the high optical nonlinearity, pulse energy and near field enhancement. Their extinction goes down to several femtojoules per pulse. cross sections are also analyzed.

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JW4A • Joint Poster Session I—Continued

JW4A.144 JW4A.148 JW4A.152 JW4A.155 JW4A.159 Design of a Wavefront Control Type Compact Design of SOI Rib Slot Waveguide with Phase-Sensitive Amplification with Net Gain Enhanced nonlinear-optical response of Free-standing SU-8 optical waveguides for Silicon Wavelength Selective Switch, Fumi Enhanced Evanescent Field for Optical in Low-Loss Integrated Waveguides, Young composites based on plasmonic nanopar- dense photonic integration, Alleksandrs Mari- Nakamura1, Kyosuke Muramatsu1, Hiroyuki Sensing , Babita Kumari1, Ravi K. Varshney1, Zhang1, Jenny Wu1, Christian Reimer1, Piotr ticles, Nikolai Mitetelo1, Sergey Svyakhovskiy1, nins1, Nicolas Knudde1, Sergei Popov1; 1Royal Tsuda1; 1Electronics and Electrical Engineering, Bishnu P. Pal2; 1Physics Department, Indian Roztocki1, Benjamin Wetzel1,2, Brent Little6, Sai Alexandra Gartman1, Stanislav Evlashin1, Anton Inst. of Technology, Sweden. Suspended Keio Univ., Japan. A 200-GHz channel spacing, Inst. of Technology, Delhi, India; 2School of T. Chu3, David J. Moss4, Michael Kues1, Roberto Maydykovskiy1; 1Moscow State Univ., Russian polymeric waveguides of small footprint suitable 16-channel, 1×2 wavefront control type silicon Natural Science, Mahindra École Centrale, Morandotti1,5; 1INRS, Canada; 2Department of Federation. We demonstrate experimentally for dense photonic integrated circuits were wavelength selective switch is designed, which India. We propose a novel SOI rib horizontal Physics and Astronomy, Univ. of Sussex, UK; 3De- that introduction of plasmonic nanoparticles developed and evaluated. Low propagation have two-step etched rib structure to reduce loss slot waveguide geometry to achieve larger partment of Physics and Materials Science,, in dielectric materials (quartz, graphene-based and bending losses at 1550 nm reported. The Wednesday, 19 October in the boundary parts between the slab and the than 10% enhancement in evanescent field vis- City Univ. of Hong Kong, Hong Kong; 4Center films) leads to a strong and spectrally selective waveguides are suitable for telecommunications arrayed-waveguide. à-vis a conventional horizontal slot waveguide for Micro-Photonics,, Swinburne Univ. of Tech- enhancement of local optical fields and increase applications. and hence yielding higher sensitivity in its nology,, Australia; 5Inst. of Fundamental and nonlinear optical effects. JW4A.145 environment sensing applications. Frontier Sciences, Univ. of Electronic Science JW4A.160 Phase-Resolved Characterization of Reflec- and Technology of China, China; 6Chinese JW4A.156 Conjugation-Length Dependence of the High tive Infrared Nanostructured Half- and JW4A.149 Academy of Science, State Key Laboratory of Silicon/Graphene Oxide Hybrid Photonic Two-Photon Absorption of Small Donor- Quarter-Wave Plates, Carol L. Baumbauer1, Thermo-optic Tuning of Silicon Photonic Multi- Transient Optics and Photonics, China. We Waveguide Filter, Chia-Wei Huang1, Jyun- Acceptor Substituted Molecules, Michael Benjamin Moon1, Andrew Hohne1, Ethan mode Waveguide for Post-Fabrication Optimi- demonstrate phase-sensitive amplification Fu Shih1, Chong-Jia Wu1, Tzu-Hsiang Yen1, Erickson1, Marten Beels1, Ivan Biaggio1; 1Lehigh Keeler1, Marquette A. Stevenson1, David L. zation, Christine P. Chen1, Brian Souhan2, Rich- based on pump-degenerate four-wave mixing in Chun-Hu Chen2, Ya-Ching Liang1, Yung-Jr Univ., USA. We report on the exceptionally Dickensheets1, Wataru Nakagawa1; 1Electrical ard M. Osgood1, Keren Bergman1;1Columbia highly nonlinear low-loss waveguides. A net gain Hung1;1Department of Photonics, National Sun strong two-photon transition in an optimized and Computer Engineering, Montana State Univ., USA; 2West Point, USA. We examine the of 6 dB (including propagation loss) is achieved, Yat-sen Univ., Taiwan; 2Department of Chemistry, family of small donor-acceptor substituted Univ., USA. Fabrication and characterization of effect of thermo-optically varying the effective with an extinction ratio of 16 dB. National Sun Yat-sen Univ., Taiwan. The enabling molecules and show how both strength and both half- and quarter-wave plates operating mode index of an asymmetric y-junction that of graphene oxide nanopatterning prompts the shape of the two-photon resonance varies with in reflection at infrared wavelengths is multiplexes three modes. This work aims JW4A.153 realization of silicon/graphene oxide hybrid conjugation length. presented. The phase delay between TE/TM to optimize multimode operation, thereby New Architectures for Photonic Doppler Ve- waveguide filters for the first time. A reflection polarization components can be controlled by improving performance. locimetry: High Velocities at Lower Cost, Levi bandwidth of 3 nm and an extinction ratio of 15 JW4A.161 the subwavelength grating fill factor. Neukirch1, Amy M. Tainter1, Dale Tupa1, Philip J. dB are experimentally obtained. Design, develop and operation of an ampli- JW4A.150 Rae2, David B. Holtkamp1, Brian Glover2; 1Phys- tude modulator fabricated by laser writing in JW4A.146 Generation and Characterization of Breather ics Division, Los Alamos National Laboratory, JW4A.157 Lithium Niobate, Gustavo Torchia1,2, D. Presti1,2, Strong coupling of hybrid and plasmonic Solitons in an On-Chip Microresonator, Chen- USA; 2Explosive Science and Shock Physics Photon Entropy Control and Near-Field A. Fasciszewski3, V. Guarepi1; 1Centro de Inves- resonances in liquid core plasmonic micro- gying Bao1, Jose Jaramillo-Villegas1, Yi Xuan1, Division, Los Alamos National Laboratory, Radiative Coupling Improve Efficiency of tigaciones Opticas, Argentina; 2Departamento bubble cavities, Liying Liu1, Qijing Lu1, Lei Xu1, Daniel E. Leaird1, Minghao Qi1, Andrew USA. Doppler velocimetry is used extensively Thermoradiative Cells, Wei-Chun Hsu1, Jona- de Ciencia y Tecnología, Universidad Nacional Sheng Liu1, Xiang Wu1; 1Fudan Univ., China. A M. Weiner1; 1Purdue Univ., USA. We show to measure velocities in dynamic experiments, than Tong1, Bolin Liao1, Yi Huang1, Svetlana V. de Quilmes Quilmes, Argentina; 3Departamento novel thin wall fluidic plasmonic micro-bubble the generation of breather solitons and but Doppler shifts of ≈1.3 GHz/km/s demand Boriskina1, Gang Chen1; 1Massachusetts Inst. of de Nano y Microelectrónica, Comisión de En- resonator is proposed and fabricated to characterization of the spectral dynamics in an expensive digitizers. We discuss methods Technology, USA. Efficiency of thermoradiative ergía Atómica Sede Constituyentes, Argen- manipulate coupling between various types of on-chip SiN microresonator. The breather soliton leveraging frequency down-mixing to reduce cells can be increased by selecting high-entropy tina. In this paper, we describe the design and resonant modes by changing its wall thickness exhibits asymmetric breathing with respect to digitization requirements and costs. infrared photons for radiative energy exchange. development of a Mach Zehnder interferometer and refractive index of the liquid in the core. the center of the spectrum. Near-field coupling to phonon polaritons in (MZI) fabricated in Lithium Niobate by means JW4A.154 the heat sink further increases both conversion of fs laser writing.The main MZI working JW4A.147 JW4A.151 Electric and magnetic hotspots in the efficiency and power density. characteristics, as amplitude modulator, are also Full Particulars of Surface Plasmon Polariton Large-Area Lithography-Free Metamaterial Silicon Bow-Tie nanocavity, Reena Reena2, presented and discussed. Dispersion Relation in Multi-Layered Me- Thermophotovoltaic Emitters with Oxygen Yogita Kalra2, Ravindra K. Sinha1,2; 1CSIR-CSIO, JW4A.158 E-Poster dia, Huseyin S. Tetikol1, M. Irsadi Aksun1; 1Koc Tolerance, Zachary Coppens1, Ivan Kravchenko2, India; 2Delhi Technological Univ., India. We Optimizing Third-Order Optical Nonlineari- Univ., Turkey. We show that the wavevector Jason Valentine1; 1Vanderbilt Univ., USA; 2Oak report enhancement of electric and magnetic ties Using Small Molecules, Michael Erickson1, and frequency of surface plasmon polaritons Ridge National Laboratory, USA. We present fields in the silicon bow-tie nanocavity at Marten Beels1, Ivan Biaggio1; 1Lehigh Univ., (SPPs) can simultaneously have complex values, a large-area metamaterial thermal emitter visible wavelength. For our design, electric USA. Donor-acceptor substituted molecules can providing better resolution/confinement. We that is fabricated using facile, lithography-free and magnetic resonances have been optically achieve record high third-order nonlinearities analyze SPPs in layered media and provide the techniques. The device shows stable, selective induced at the wavelength of 620 nm. relative to the size of their conjugated system, complete description of their dispersion. emission after exposure to 1173 K for 22 hours reaching a maximum efficiency for a linear in oxidizing and inert atmospheres. conjugated system of ~3 multiple bonds between donor and acceptor. This presentation will be presented as an E-Poster on Screen 4 from 15:15–16:00

FiO/LS 2016 • 16–21 October 2016 77 Empire Hall

JOINT FiO/LS

JW4A • Joint Poster Session I—Continued

JW4A.162 JW4A.166 JW4A.170 JW4A.174 JW4A.178 Perfect Light Absorption in Ultra-thin Silicon Phase-contrast ghost imaging using an orbital Light Slowing Down and Chirped Soliton For- Rapid Delay Modulation of Biphotons, Ogaga Fabrication and Second-harmonic Generation Optical Nanocavity and its Application for angular momentum phase-filter , Peter A. mation in a Medium with Gold Nanorods, V. D. Odele1, Joseph M. Lukens1,2, Jose A. Imaging of Oriented Ion-shaped Nanopar- Color Filters, Seyed Sadreddin Mirshafieyan1, Morris1, Reuben Aspden1, Ruiqing He2, Qian A. Trofimov1, Tatiana Lysak1; 1M. V. Lomonosov Jaramillo-Villegas1,3, Poolad Imany1, Carsten ticles, Abdallah Slablab1, Léo Turquet1, Tero Ting S. Luk2, Junpeng Guo1; 1Department of Chen2, Miles J. Padgett1; 1Univ. of Glasgow, Moscow State Univ., Russian Federation. We Langrock4, Martin M. Fejer4, Daniel E. Leaird1, Isotalo2, Jouni Mäkitalo1, Pierre Eugène Coulon3, Electrical and Computer Engineering, The UK; 2Nanjing Univ. of Science and Technology, show a possibility for light slowing down Andrew M. Weiner1; 1Purdue Univ., USA; 2Oak Tapio Niemi2, Mathieu Kociak4, Giancarlo Rizza3, Univ. of Alabama in Huntsville, USA; 2Center China. Position and orbital angular momentum accompanied by a novel type soliton – chirped Ridge National Laboratory, USA; 3Universidad Martti Kauranen1; 1Tampere Univ. of Technology, for Integrated Nanotechnologies, Sandia correlations are used to image phase-objects. soliton - formation at a femtosecond pulse Tecnologica de Pereira, Colombia; 4Stanford Finland; 2Optoelectronics Research Centre, National Laboratories, Albuquerque, USA. We Using a non-local phase-filter, ghost images propagation in a medium with gold nanorods Univ., USA. We demonstrate delay modulation Tampere Univ. of Technology, Finland; 3Labora- investigated perfect light absorption in silicon show isotropic edge-enhancement allowing under the nanorods reshaping and negative of entangled photons over a full 32-ns span, toire des solides Irradiés, Ecole Polytechnique, optical nanocavity comprising of ultrathin imaging using significantly fewer photons than phase-amplitude grating. utilizing pump frequency tuning and ultralong France; 4Laboratoire de Physique des Solides, aluminum and silicon films deposited on an standard phase-contrast imaging. fiber Bragg gratings. Electro-optic modulators Univ. Paris-Sud, France. We use ion irradiation aluminum surface. The thickness of the silicon JW4A.171 enable time-bin switching rates as fast as 2.5 to fabricate anisotropic gold nanorods oriented film cavity is 1/18 of the perfect absorption JW4A.167 Cavity QED with Collective Excitations of MHz. in three dimensions. Their orientation is wavelength. Modeling Structural Features of Single-Mode, Warm, 3-Level Atoms, Garrett Hickman1, subsequently determined by second-harmonic Q-Switched Pulse Ensembles, Graham Martin1, Todd B. Pittman1, James D. Franson1; 1Univ. of JW4A.175 generation microscopy relying on linear and JW4A.163 Troy J. Siemers1, John R. Thompson1; 1Virginia Maryland, Baltimore County, USA. We derive a Two-photon Absorption Induced Emission of radial polarizations. Optimized Mid-Infrared Thermal Emitters for Military Inst., USA. Stochastic, single-mode, simplified Hamiltonian describing an ensemble InAs/GaAs Quantum Dots, Xian Hu1,2, Dorel Applications in Aircraft Countermeasures, Si- rate equations are solved to generate pulse of three-level room-temperature atoms in a Guzun2, Morgan E. Ware3,2, Yuriy I. Mazur2, JW4A.179 mon Lorenzo2,1, Chenglong You2,1, Georgios ensembles for comparison with experiments. two-mode cavity. If one transition is driven with Gregory J. Salamo1,2; 1Department of Physics, Boundary-concentrated Modes of a 2-D Opto- Veronis3,4, Jonathan Dowling2,1;1Louisiana Structural features of the ensembles depend a single photon, the ensemble behaves as if it Univ. of Arkansas, USA; 2Inst. of Nano Science fluidic Random Laser Mapped Using a Pump- State Univ., USA; 2Hearne Inst. for Theoretical on the switching time for cavity losses and the were a single atom. and Engineering, Univ. of Arkansas, USA; 3De- probe Technique, Anirban Sarkar1, Jonathan 2 1 1 Wednesday, 19 October Wednesday, Physics and Department of Physics and As- statistical characteristics of noise sources. partment of Electrical Engineering, Univ. of Andreasen , Shivakiran Bhaktha B. N. ; Indian tronomy, Louisiana State Univ., USA; 3Center for JW4A.172 Arkansas, USA.Direct two-photon absorption Inst. of Technology Kharagpur, India; 2Georgia Computation and Technology, Louisiana State JW4A.168 Conservative Classical and Quantum Resolu- induced emission of MBE grown undoped Tech Research Inst., USA. We spatially map Univ., USA; 4School of Electrical Engineering Photonic Microwave Generation Using a tion Limits for Incoherent Imaging, Mankei InAs/GaAs quantum dots (QDs) is investigated the lasing modes of a weakly scattering 2-D and Computer Science, Louisiana State Univ., VCSEL Subject to Orthogonal Optical Injec- Tsang1; 1National Univ. of Singapore, Singa- by power dependent photoluminescence and optofluidic random laser by a pump-probe USA. An optimized aperiodic photonic crystal tion, Salim Ourari1, Tianyao Huang1, Hong pore. We propose classical and quantum limits two-photon photoluminescence excitation technique. We conclude that the lasing modes structure is capable of near-blackbody and Lin1; 1Bates College, USA. We have generated to the resolution of two incoherent sources study with excitation energy near the QDs are concentrated at the boundaries of the gain broad angle thermal emission at aircraft engine tunable photonic microwave signals ranging from the perspective of minimax estimation. half-bandgap. region as predicted by computational analysis. temperatures over the three to five micron from 6 to 62 GHz in a vertical-cavity surface- Our limits are valid for any biased or unbiased atmospheric transmission band. emitting laser operating with three transverse estimator and numerically demonstrated to be JW4A.176 JW4A.180

modes by using period one dynamics and approachable. Withdrawn. Monoblock He-Ne/CH4 laser with the short- JW4A.164 dual-beam injection separately. term and long-term frequency stability better Feedback-induced Bistability of an Opti- JW4A.173 JW4A.177 than 1×10-14, Alexey N. Kireev2, Alexander S. cally Levitated Nanoparticle: A Fokker-Planck JW4A.169 Qubit-Detuning Impacted Entanglement Withdrawn. Shelkovnikov2, Dmitry A. Tyurikov2, Vladimir A. Treatment, Wenchao Ge1, Brandon Roden- A Novel Observation of Optical Bistability Mediated by the Surface Plasmon, Fan Lazarev1, Mikhail A. Gubin2,3; 1Science and Edu- burg1, Mishkatual Bhattacharya1; 1Rochester in Oppositely Directed Coupler, Kanagaraj Zhang1, Dongxing Zhao1, Ying Gu1, Hongyi cation Center for Photonics and IR-Technology, Inst. of Technology, USA. The Fokker-Planck Nithyanandan1, A.K. Shafeeque Ali1, Porsezian Chen1, He Hao1, Qihuang Gong1,2; 1Peking Bauman Moscow State Technical Univ., Russian equation for an optically levitated nanoparticle Kuppusamy1; 1Pondicherry Univ., India.We Univ., China; 2Collaborative Innovation Center Federation;2Frequency Standards Laboratory, P. with feedback damping is investigated. We observe that the oppositely directed coupler of Extreme Optics, Shanxi Univ., China. We N. Lebedev Physical Inst. of the Russian Acad- recover previous theoretical and experimental possesses Bistability. This property arises due have theoretically demonstrated the influence emy of Sciences, Russian Federation; 3National works in the low-damping regime and predict a to effective feedback mechanism as a result of qubit entanglement induced by the detunings Research Nuclear Univ. MEPhI, Russian Fed- bimodal distribution in the overdamped regime. of opposite directionality of the phase velocity among two qubits and surface plasmons in a eration. We reported on the optical frequency and energy flow in the negative index materials. hybrid qubits-metallic nanoparticle system. standard based on a compact monoblock

JW4A.165 Enhancement appears when nanoparticle is He-Ne/CH4 laser with the short-term and long- Bistable mode of THG at non-zero ampli- placed between qubits. term frequency stability better than 1×10-14, that tudes of incident waves, V. A. Trofimov1, was obtained form a direct comparison of two Pavel Sidorov1, Igor Kuchik1; 1M. V. Lomonosov identical monoblock lasers. Moscow State Univ., Russian Federation. We demonstrate and compare the numerical and analytical solutions of THG problem in the case of non-zero input intensity. Also we consider the solution on the boundaries of areas.

78 FiO/LS 2016 • 16–21 October 2016 Empire Hall

JOINT FiO/LS

JW4A • Joint Poster Session I—Continued

JW4A.181 JW4A.184 JW4A.188 JW4A.192 JW4A.196 Controlling Mandel’s Q-parameter in Dis- Analytical Description of Nonlinear Refrac- Experimental and Numerical Study on Valley Trion Dynamics in Monolayer Multimode Solitons in Few-Mode Fiber, Zimu 1 1 1 1 ordered Lattices via Excitation-Symmetry tion Index Measurements with the D4\ Stimulated Raman Scattering in AsSe2- MoSe2, Michael Titze , Feng Gao , Raybel Zhu , Logan G. Wright , Demetrios Christo- 1 3 1 1 2,3 2,3 2 1 1 Breaking, Hasan E. Kondakci , Robert Keil , sigma Technique, Anderson M. Amaral , Hans As2S5 Microstructured Optical Fiber, Weiqing Almeida , Yongji Gong , Pulickel M. Ajayan , doulides , Frank W. Wise ; Cornell Univ., Armando Perez-Leija2, Alexander Szameit2, A. Mejía2, Edilson L. Falcao-Filho1, Cid B. de Gao1,2, Xue Li2, Qiang Xu2, Xiangcai Chen2, Hebin Li1; 1Department of Physics, Florida Inter- USA; 2CREOL, College of Optics and Photonics, Ayman Abouraddy1, Demetrios Christodou- Araújo1; 1Universidade Federal de Pernambuco, Chenquan Ni 2, Li Chen2, Zhengqiang Wen2, national Univ., USA; 2Department of Chemistry, Univ. of Central Florida, USA. We experimentally lides1, Bahaa E. Saleh1; 1CREOL, Univ. of Central Brazil; 2Departamento de Física, Universidade Tonglei Cheng1, Xiaojie Xue1, Takenobu Su- Rice Univ., USA; 3Department of Materials Sci- isolate and measure multimode Raman solitons Florida, USA; 2Inst. of Applied Physics, Friedrich- Federal do Piauí, Brazil. We obtained analytical zuki1, Yasutake Ohishi1; 1Research Center for ence and NanoEngineering, Rice Univ., USA. We in few-mode graded-index fiber. We show that 3 Schiller-Universitat Jena, Germany; Institut expressions for the far-field beam width due to Advanced Photon Technology, Toyota Techno- report an ultrafast two-color pump-probe these waves are spatiotemporal solitary waves, Wednesday, 19 October fur Experimentalphysik, Universitat Innsbruck, elliptical and astigmatic beams propagating logical Inst., Japan; 2School of Electronic Science experiment measuring transient differential and are qualitatively distinct from stationary Austria. We experimentally demonstrate inside Kerr media, and performed experiments & Applied Physics, Hefei Univ. of Technology, reflection of trions in monolayer MoSe2. We solutions of the NLSE in integer-dimensions.

deterministic control of Mandel’s Q-parameter in with CS2 and silica. A good agreement between China. We demonstrate the stimulated Raman explain our results using a model

off-diagonal disordered lattices while the mean theory and experiment was found. scattering effect in AsSe2-As2S5 microstructured based on a set of rate equations. JW4A.197 photon number remains fixed. We achieve this optical fiber. The first-order Stokes wave is Construction of Arbitrary Vortex and Su- by gradually breaking the excitation symmetry JW4A.185 obtained with the conversion efficiency of -15.0 JW4A.193 peroscillatory Fields, Matt Smith1, Gregory of the chiral mode pairs. Evolution of Averaged Speckle Pat- dB. The simulated results agree well with the Self-healing optical beams with snake-like and J. Gbur1; 1Univ. of North Carolina at Charlott, terns, Xiaojun Cheng1,2; 1CUNY Queens Col- experiments. spiral paths in free space, Ahmed Dorrah1, Mi- USA. A simple Fourier method for constructing JW4A.182 lege, USA; 2Graduate Center, CUNY, USA. We chel Zamboni-Rached2, Mo Mojahedi1; 1Univ. of superoscillatory fields with arbitrarily located Quantum resources for optical phase estima- show that intensity maxima in speckle patterns JW4A.189 Toronto, Canada; 2Electrical Engineering, State optical vortices is presented. Examples are tion, Jaspreet Sahota1, Nicolas Quesada2, Dan- averaged over a frequency interval diffuses with Calculation of Power Spectral Density in Univ. of Campinas, Brazil. We experimentally given and mathematical properties of the fields iel F. James1; 1Univ. of Toronto, Canada; 2Phys- a diffusion coefficient decreasing linearly with Passively Modelocked Lasers with Slow demonstrate a class of non-diffracting beams, are explained. ics, Universite de Sherbrooke, Canada.We the width of the frequency interval, providing a Saturable Absorbers, Shaokang Wang1, Curtis known as Frozen Waves, whose central spot can determine how phase sensitivity depends on method in imaging for dynamic samples. R. Menyuk1; 1Computer Science and Electrical be made to follow an arbitrary off-axis curved JW4A.198 quantum entanglement (particle entangle- Engineering, Univ. of Maryland, Baltimore path. These beams can be utilized in material Optically Trapped Microscopic Particles in a ment and mode entanglement) by employing JW4A.186 County, USA. We calculate the power spectral processing and optical trapping applications. Perfect Fractional Vortex Beam, Mingzhou the particle description (first quantization) and Nonlinear Modal Interactions in PT-Symmetric density for a passively modelocked fiber laser Chen1, Georgiy Tkachenko1, Kishan Dholakia1, the mode description (second quantization) of Lasers, Li Ge1,2, Ramy El-Ganainy3; 1College with a semiconductor saturable absorber using JW4A.194 Michael Mazilu1; 1Univ. of St Andrews, UK. We bosonic probe states. of Staten Island, CUNY, USA; 2The Graduate spectral methods. We obtained frequency Quantum Multiple Phase Estimation Using experimentally generated a perfect vortex Center, CUNY, USA; 3Department of Physics sidebands that agrees with experimental Balanced Multi-mode Entangled States, Lu beam with fractional topological charges. The JW4A.183 and Henes Center for Quantum Phenomena, observations. Zhang1, Kam Wai C. Chan1, Pramode K. local orbital angular momentum density in such Electronic nature of new Ir(III)-complexes: Michigan Technological Univ., USA. We discuss Verma1; 1Univ. of Oklahoma, USA. We present beams was probed with an optical trapped linear spectroscopic and nonlinear optical nonlinear modal interactions in PT-symmetric JW4A.190 a generalized entangled state that can approach microscopic particle. properties, Salimeh Tofighi1, Peng Zhao1, laser systems under steady state conditions, and Observation of Ince-Gaussian beams and the Heisenberg limit in quantum metrology. We Mykhailo Bondar2, Ryan O’Donnell3, Jianmin we demonstrate several gain clamping scenarios their polarizaions properties, Sean M. No- prove the entangled squeezed vacuum state JW4A.199 Shi3, David Hagan1, Eric Van Stryland1; 1CREOL in both the PT-symmetric and PT-broken phases. moto1, Adam Goldstein1, Reeta Vyas1, Surendra can achieve a higher precision than entangled Supercontinuum Generation in an AsSe2- Univ. of Central Florida, USA; 2Inst. of Physics Singh1; 1Univ. of Arkansas, USA. Ince-Gaussian (squeezed) coherent state and NOON state. As2S5 Step-Index Fiber, Weiqing Gao1, NASU, Ukraine; 3US Army Research Labora- JW4A.187 (IG) beam solutions of Maxwell’s equations and Qiang Xu1, Xue Li1, Li Chen1, Xiangcai Chen1, tory, USA. Linear photophysical properties Dynamic Ferroelectricity of Trojan Electrons their polarization and propagation properties JW4A.195 Chenquan Ni 1, Zhengqiang Wen1, Tonglei and two-photon absorption spectra of new on Face-Centered Square Lattice, Matt Ka- were studied experimentally for lower order IG Electron spin interaction with the angu- Cheng2, Xiaojie Xue2, Takenobu Suzuki2, Ya- Ir(III)-complexes in liquid media are presented. linski1; 1Utah State Univ., USA. We show that beams for several different eccentricities. lar momentum of the electromagnetic sutake Ohishi2; 1School of Electronic Science The excited-state potential surface of new hydrogen atoms placed on the face-centered field, Charles Paillard2, Brahim Dkhil2, Reeta & Applied Physics, Hefei Univ. of Technology, compounds was revealed by steady-state and two-dimensional square lattice and excited JW4A.191 Vyas1, Laurent Bellaiche1, Surendra Singh1; 1Univ. China; 2Research Center for Advanced Photon time resolved spectroscopic data. to Trojan electron states exhibit dynamic fer- An efficient numerical method for the calcu- of Arkansas, USA; 2Laboratoire SPMS, Cen- Technology, Toyota Technological Inst., Japan. roelectric order when all Trojan Wave Packets lation of global discord of coupled quantum traleSupelec, CNRS-UMR 8580, Universite We demonstrate the supercontinuum genera- move coherently in phase dots, Willa Rawlinson1, Reeta Vyas1; 1Univ. Paris-Saclay, France. Consequences of the tion in an AsSe2-As2S5 step-index fiber. The on circular orbits. of Arkansas, USA. We present an efficient recently introduced interaction between the SCs are investigated by changing the pump numerical method for calculating global electron spin and the angular momentum of wavelength and the fiber length. The maximum discord for coupled quantum dots interacting the electromagnetic field for atomic and optical spectral range covers one octave from 1550 with a quantized cavity field. Speed tests and physics are discussed. to 3300 nm. interesting results are presented for two, three, and four quantum dots.

16:00–17:00 Exhibitor Appreciation Reception, Empire Hall

FiO/LS 2016 • 16–21 October 2016 79 Grand Ballroom A (Radisson) Grand Ballroom B (Radisson) Grand Ballroom C (Radisson) Grand Ballroom D (Radisson)

FiO

16:00–17:30 16:00–18:15 16:00–18:00 16:00–18:00 FW5A • Understanding Myopia FW5B • High-Power Fiber Lasers and Beam FW5C • Optical Coherence Tomograpy FW5D • Integrated Photonics Development Combining Presider: Jerome Mertz, Boston Univ., USA Presider: Michael Fanto, Rochester Inst. of Presider: Frank Schaeffel, Eberhard-Karls_ Presider: Iyad Dajani; US Air Force Research Technology, USA Universitat Tubingen, Germany and Earl Laboratory, USA Smith, Univ. of Houston, USA

FW5A.1 • 16:00 Invited FW5B.1 • 16:00 Invited FW5C.1 • 16:00 Invited FW5D.1 • 16:00 Invited Control of Myopia Progression in Children: Inside and Coherent Beam Combining and Nonlinear Suppression Live Imaging of Reproductive and Developmental Events Nanophotonics Technology and Applications, Yeshaiahu Outside, Donald O. Mutti1; 1Ohio State Univ. Optometry, of Multi-Kilowatt All-Fiber Amplifiers, Angel Flores1, Iyad in Mouse Model with Optical Coherence Tomogra- Fainman1; 1Univ. of California, San Diego, USA. We discuss USA. Positive results using peripheral myopia-based optical Dajani1, Nader N. Naderi1, Brian Anderson1; 1US Air Force Re- phy, Irina Larina1; 1Baylor College of Medicine, USA. Toward integration of a photonic information processing system therapies have motivated their evaluation in longer-term search Laboratory, USA. We present multi-kW power scaling understanding of mammalian reproduction and early onto a single chip focusing on nanoscale engineered clinical trials. This presentation will review these studies results of narrow line Yb-doped fiber amplifiers. Nonlinear embryonic development, we are working on development optical nonlinearities and metal-dielectric-semiconductor and whether time outdoors alters risk of myopia onset and suppression is attained through pseudo-random modulation. of imaging tools based on structural and functional optical nanostructures and compositions to construct nanoemitters. progression rate. Subsequently, 5 pseudo-random modulated kW amplifiers coherence tomography in mouse models. were coherently combined into a 5kW beam. Wednesday, 19 October Wednesday,

FW5A.2 • 16:30 Invited FW5B.2 • 16:30 FW5C.2 • 16:30 Invited FW5D.2 • 16:30 Myopia Development inGuinea Pigs, Sally A. McFadden1, Singlemode Raman Lasing in Graded-Index Fiber Monitoring and Guidance of Arrhythmia Therapy with Supra-octave-spanning single-mode and single-polariza- 1 Guang Zeng1; 1Univ. of Newcastle, Australia. Myopia is in- Pumped by High-Power 915-nm Laser Diode, Ekaterina Optics, Christine P. Hendon1; 1Columbia Universitry, USA. In tion operation in nanophotonic waveguides, Jeff Chiles , 1 1 1 1 1 duced when growing eyes are exposed to hyperopic defocus A. Zlobina , Sergey I. Kablukov , Alexey A. Wolf , Alexander this talk, I will describe my laboratory’s efforts towards Sasan Fathpour ; Univ. of Central Florida, USA.Nanophotonic 1,2 1,2 1 or reduced vision. The associated changes and factors that V. Dostovalov , Sergey A. Babin ; Inst. of Automation translation of optical coherence tomography and near anchored-membrane waveguides utilizing a semi-infinite and 2 influence the development of myopia in the guinea pig eye and Electrometry, Russian Federation; Novosibirsk State infrared spectroscopy for monitoring and guidance of asymmetric geometry are fabricated and shown to exhibit are described. Univ., Russian Federation. Raman lasing in graded-index arrhythmia therapy. single-mode and single-polarization operation over a record fibers pumped by a multimode 915-nm laser diode enables span exceeding 1.27 octaves. single-transverse-mode output due to special FBG inscribed by femtosecond technique. 954-nm output power of >10 W with narrow spectrum has been obtained.

80 FiO/LS 2016 • 16–21 October 2016 Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E

FiO LS

16:00–18:00 16:00–18:00 16:00–18:00 16:00–18:00 16:00–18:00 FW5E • Ultrafast Lasers and FW5F • Nonlinear Optics in FW5G • Optical Fabrication and FW5H • Freeform Design and LW5I • Integrated Quantum Applications Micro/Nano-Optical Structures II Metrology Metrology Photonics II Presider: Jake Bromage, Univ. of Presider: Miles Padgett; Univ. of Presider: Ted Tienviri, Corning, Presider: Joe Howard, NASA Presider: Alexander L. Gaeta; Rochester, USA Glasgow, UK USA Goddard Space Flight Center, USA Columbia Univ., USA

FW5E.1 • 16:00 Tutorial FW5F.1 • 16:00 Invited FW5G.1 • 16:00 Invited FW5H.1 • 16:00 LW5I.1 • 16:00 Invited High Power Fiber-laser Based High Harmonic Compact Freeform Offner-Chrisp Imag- 1 1 Optical Antenna Spontaneous Emission: How Optical Fabrication Science & Technology Title to be Announced, Milos Popovic ; Univ. of Wednesday, 19 October 1 Sources for Nanoscale Imaging and Spec- Much Faster Than Stimulated Emission?, Eli for High Energy Laser Optics, Tayyab I. Surat- ing Spectrometer, Jacob Reimers , Kevin Colorado Boulder, USA. Abstract not available. 1,2 3 troscopy, Jan Rothhardt1,2, Steffen Hädrich3, Yablonovitch1; 1Univ. of California Berkeley, wala1; 1Lawrence Livermore National Laboratory, P. Thompson , Kevin L. Whiteaker , Dennis 4 1 1 Robert Klas1,2, Getnet Tadesse1,2, Stefan Dem- USA. With optical antennas, spontaneous USA. Optical fabrication Science & Technology Yates , Jannick P. Rolland ; Univ. of Rochester, 2 3 mler1,2, Maxim Tschernajew1,2, Jens Limpert2,3, light emission becomes faster than stimulated (specifically sub-surface damage, surface figure, USA; Synopsys Inc., USA; Ball Aerospace & 4 Andreas Tünnermann3,2; 1Helmholtz Inst. Jena, emission, but the enhancement is limited by & roughness) and its impact on fabricating Technologies Corp., USA; PerkinElmer Health Germany; 2Inst. of Applied Physics, Friedrich- optical losses through the “anomalous skin economical high quality, laser damage resistant Sciences, USA. A freeform Offner-Chrisp Schiller-Univ. Jena, Germany; 3Fraunhofer effect”. Maintaining 50% efficiency, a 10x optics for use in high energy, high power lasers imaging spectrometer is demonstrated to be IOF, Germany. We report on table-top XUV speedup beyond stimulated emission should are reviewed. 5x more compact than traditional surfaces. The sources based on high harmonic generation be possible. performance was analyzed using spectral full- with high average power fiber lasers delivering field display. Furthermore, we show distortion record average powers from 20 eV up to the correction without decrease in performance. water window for applications in imaging and spectroscopy. FW5H.2 • 16:15 Sharp images from freeform optics and extended light sources, Matthew Brand1, Aydan Aksoylar2; 1MERL, USA; 2ECE, Boston Univ., USA. We introduce a class of pictorial irradiance patterns that freeform optics can render sharply despite the blurring effect of extended light sources; show how to solve for the freeform geometry; and demonstrate a fabricated lens.

FW5F.2 • 16:30 Invited FW5G.2 • 16:30 FW5H.3 • 16:30 LW5I.2 • 16:30 Invited Soliton Kerr Frequency Combs on a Chip, To- Brittle-Ductile Transition in Shape Adap- Comparing Three-Mirror Freeform Tele- Nanophotonic Resonators for Quantum Fre- 1 bias J. Kippenberg1; 1Ecole Polytechnique tive Grinding (SAG), Peter Simon , Anthony scopes to Traditional TMAs by Exploring quency Conversion, Kartik Srinivasan1, Qing 1 2 1 Federale de Lausanne, Switzerland. The ability Beaucamp , Phillip Charlton , Yoshiharu Nam- TMA Solution Space, Eric M. Schiesser , Li1,2, Marcelo Davanco1; 1Center for Nanoscale 3 1 2 3 1 1,2 Biography: Dr. Jan Rothhardt received his PhD to generate optical frequency combs using ba ; Kyoto Univ., Japan; Zeeko LTD, UK; Chu- Jonathan Papa , Kevin P. Thompson , Jannick Science and Technology, National Inst. of 1 1 2 in Physics in 2010 from the Friedrich-Schiller- dissipative soliton formation in microresonators bu Univ., Japan. Shape Adaptive Grinding (SAG) P. Rolland ; Univ. of Rochester, USA; Synopsis, Standards and Technology, USA; 2Maryland University Jena. Since 2014 he is a Young will be reviewed. In addition higher order soliton is novel process for rapid finishing of ceramic USA. Tilted freeform mirrors allow the removal Nanocenter, Univ. of Maryland, USA. We present Investigators Group leader at the Helmholtz- effects discussed in views of generating an freeform optics. In this paper, we report results of obscuration in otherwise 100% obscured the development of nanophotonic resonators Institute Jena. His group is applying table-top microwave to optical link on a chip. from an investigation into the brittle-ductile coaxial designs. We explore the design space for for quantum frequency conversion, including coherent high photon flux XUV and soft X-ray transition observable on ceramic materials such three mirror freeform telescopes by reviewing efficient, low-noise conversion of single-photon- sources to ultrafast nanoscale imaging and as silicon carbide. the coaxial single-conic TMA space, including level signals and progress towards use with spectroscopy. convex primary solutions. quantum dot single-photon-sources.

FiO/LS 2016 • 16–21 October 2016 81 Grand Ballroom A (Radisson) Grand Ballroom B (Radisson) Grand Ballroom C (Radisson) Grand Ballroom D (Radisson)

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FW5A • Understanding Myopia FW5B • High-Power Fiber Lasers and Beam FW5C • Optical Coherence Tomograpy— FW5D • Integrated Photonics—Continued Development—Continued Combining—Continued Continued

FW5B.3 • 16:45 FW5D.3 • 16:45 ~900W Single-mode CW Power From an 60μm-core On-Chip Optical Neuromorphic Computing, Yichen Shen1, Ytterbium-doped All-solid Photonic Bandgap Fiber Marin Soljacic1, Nicholas Harris1, Dirk . Englund1; 1Massachu- Laser, Fanting Kong1, Guancheng Gu1, Thomas Hawkins1, setts Inst. of Technology, USA. We propose a nanophotonic Maxwell Jones2, Joshua Parsons1, Monica Kalichevsky-Dong1, system that do the neural network computing in optical Benjamin Pulford3, Iyad Dajani3, Liang Dong1; 1Clemson domain. Our system is able to give equivalent learning Univ., USA; 2Nufern, USA; 3Air Force Research Laboratory, performance, while potentially achieve much better speed USA.~900W single-mode power was obtained from an Yb- and efficiency than conventional computer. doped, ~60µm-core all-solid photonic bandgap fiber with multiple-cladding-resonant design, with 90% efficiency vs. launched pump. This is a record single-mode power from a micro-structured fiber laser.

FW5A.3 • 17:00 FW5B.4 • 17:00 FW5C.3 • 17:00 FW5D.4 • 17:00 Invited Modelling Cones in the Macula from AOSLO Data: Aging Brillouin Gain Spectroscopy on LMA Yb-Doped Photonic Long-range, wide-field, functional optical coherence Towards an Integrated Quantum Photonics Platform on 1 1 1,2 3 and Myopia, Ann E. Elsner , Christopher A. Clark , Burns A. Bandgap Fiber, Cody Mart , Benjamin Ward , Benjamin tomography imaging for clinical otology in live patients GaAs, Sven Höfling1; 1Univ. of St. Andrew, UK. Integrated 1 1 2 2 4 1 1 1 1 Stephen ; Indiana Univ., USA. Cone densities of both older Pulford , Iyad Dajani , Liang Dong , Khanh Kieu ; Univ. of and healthy normals, Dan MacDougall , Joshua Farrell , quantum photonics promises a chip-scale implementation 2 1 1 1 and younger subjects are well fit by an exponential model in Arizona, College of Optical Sciences, USA; Directed Energy Nicholas Jufas , Manohar Bance , Jeremy Brown , Robert of quantum circuits. We discuss recent progress towards all meridians except nasal, where the optic nerve head has no Directorate, Air Force Research Laboratory , USA; 3Depart- Adamson1; 1Dalhousie Univ., Canada. We present results

Wednesday, 19 October Wednesday, the realization of a platform on GaAs, including single 4 photoreceptors. This permits modelling of cone contribution ment of Physics, USA Air Force Academy, USA; Clemson from a real-time, phase-sensitive swept-source OCT system photon sources, detectors and other key elements towards to myopia progression. Univ., Center for Optical Materials and Engineering Technol- used for middle ear imaging in live patients with co-registered a functional platform. ogy, USA. We interrogate stimulated Brillouin scattering in functional Doppler vibrography. This is the first system to large mode area photonic bandgap fiber. Theoretical and successfully produce such images in vivo.

experimental studies reveal a gB less than 0.7 cm/GW, which represents a significant reduction over commercial Yb-doped LMA step-index fibers.

FW5A.4 • 17:15 FW5B.5 • 17:15 FW5C.4 • 17:15 Changes in anterior segment 3-D geometry in normal Power Scaling and Coherent Beam Combination of a Broadband Swept-Source Laser in 1.1 to 1.3 µm with InAs and myopic guinea pig eyes, Susana Marcos1, Pablo Narrow-Linewidth, Monolithic Two-Tone Fiber ampli- Quantum Dot Gain Chip Devices, Ruizhe Yao1, Nicholas Perez-Merino1, Miriam Velasco-Ocana1, Eduardo Martinez- fier, Nader N. Naderi1, Angel Flores1, Brian Anderson1, Weir1, Chi-Sen Lee1, Zihao Wang2, Stefan F. Preble2, Wei Enriquez1, Luis Revuelta2, Sally A. McFadden3; 1Consejo Sup Kenneth Rowland1, Iyad Dajani1; 1US Air Force Research Guo1;1Univ. of Massachusetts Lowell, USA; 2Microsystems Investigaciones Cientificas, Spain; 2School of Veterinary, Uni- Laboratory, USA. Power scaling results of a phase modulated Engineering, Rochester Inst. of Technology, USA. We have versidad Complutense de Madrid, Spain; 3Univ. of Newcastle, two-tone fiber amplifier at clock rate of 2.5GHz are presented. demonstrated mode-hopping-free broadband swept-source Australia.We quantified anterior segment geometry in both Coherent beam combination performance of the two-tone laser with ~ 100 nm wavelength tuning range centered at 1.2 control and lens-treated eyes of a guinea pig model in vivo amplifier yielded ~90% combining efficiency with no sign of µm by using novel InAs quantum dot (QD) gain chip devices. using custom-developed OCT. Myopic eyes showed longer linewidth broadening. axial lengths, thinner corneas, longer anterior chamber depth and steeper anterior lens.

82 FiO/LS 2016 • 16–21 October 2016 Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E

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FW5E • Ultrafast Lasers and FW5F • Nonlinear Optics in FW5G • Optical Fabrication and FW5H • Freeform Design and LW5I • Integrated Quantum Applications—Continued Micro/Nano-Optical Structures II— Metrology—Continued Metrology—Continued Photonics II—Continued Continued

FW5E.2 • 16:45 FW5G.3 • 16:45 FW5H.4 • 16:45 Measuring ultrafast lighthouse effect in A 12 decades goniometric instrument for Transverse Translation Diverse Phase Retrieval femtosecond pulses, Zhe Guang1, Michelle the comprehensive characterization of the for Reflective and Freeform Surface Metrolo- Rhodes1, Rick Trebino1; 1Georgia Inst. of spectral properties of thin-film filters, Michel gy, Aaron Michalko1, James R. Fienup1; 1Univ. of Technology, USA. Using the STRIPED FISH Lequime1, Simona Liukaityte1, Myriam Zerrad1, Rochester, USA. The performance of transverse 1 1 technique, we measured ultrafast lighthouse Claude Amra ; Institut Fresnel - UMR 7249, translation diverse phase retrieval is assessed Wednesday, 19 October effect, which corresponds to pulse amplitude France. This paper describes an innovative in two different scenarios. First, performance coupling in the spatial-frequency-temporal (k,t) instrument that allows to measure the optical is compared between a hard-edged and soft- domain. The effect was analyzed and displayed features of a thin-film filter (transmission, edged subaperture. Second, performance is by a spatiotemporal movie in 3D. reflection, blocking, steepness, scattering) with analyzed on a highly aberrated wavefront. 12 decades detection range and sub-nanometer spectral resolution.

FW5E.3 • 17:00 FW5F.3 • 17:00 FW5G.4 • 17:00 Invited FW5H.5 • 17:00 LW5I.3 • 17:00 Invited Harmonic Generation in Graphene and Superconducting Nanowire Single-photon Optical Metrology Systems Spanning the Full Optical Differentiation Wavefront Sensing Advances in Silicon Quantum Photon- 1 1,2 Carbon Nanotubes, Marco Taucer , T J. Detector with Spot-size Converter on Si Spatial Frequency Spectrum, Dae Wook Kim1, for Freeform Optics Metrology, Jie Qiao , ics, D. Bonneau1, J.W. Silverstone1, J. Wang1, 1 1 3 2,1 2,1 1 2 1 Hammond , Giulio Vampa , Nicolas Thire , platform, Tatsurou Hiraki , Tai Tsuchizawa , Maham Aftab1, Heejoo Choi1, Logan Graves1, Zachary Mulhollan , Christophe Dorrer ; Roch- P. Sibson1, R. Santagati1, C. Erven1, J.L. 3 3 1 3 2 Bruno Schmidt , Charles-Andre Couture , Tsuyoshi Yamamoto , Hiroyuki Shibata , Shinji Isaac Trumper1; 1Univ. of Arizona, USA. We ester Inst. of Technology, USA; Aktiwave LLC, O’Brien1, M.G. Thompson1; 1Univ. of Bristol, 3 1,2 1 2,1 1 François Légaré , Paul Corkum ; Univ. of Matsuo ; NTT Device Technology labs., present a collection of unique, collaborative USA. High resolution, high dynamic range UK. Silicon quantum photonics has emerged 2 2 Ottawa, Canada; National Research Council, Japan; NTT Nanophotonics Center, Ja- optical metrology systems that are fully capable optical differentiation wavefront sensor using as a promising approach to realising complex 3 3 Canada; INRS, Canada. We report experimental pan; Kitami Inst. of Technology, Japan. We have of measuring the extensive spectrum of low-to- binary pixelated filters has been developed for and compact quantum circuits for applications observations of non-perturbative harmonic integrated an SNSPD with a spot-size converter mid-to-high spatial frequencies, corresponding the metrology of freeform optics. Wavefront in communication and computation. Highlights generation from graphene and from thin films on the Si photonics platform. A system detection to surface shape information. reconstruction precision and accuracy will be include chip-to-chip quantum communications, of aligned semiconducting carbon nanotubes. efficiency of 32% and a dark count rate of 96 presented. programmable quantum circuits and chip-based We investigate the dependence of harmonic Hz are achieved with a fiber coupled module. quantum simulations. generation on polarization of driving field.

FW5E.4 • 17:15 FW5F.4 • 17:15 FW5H.6 • 17:15 Amplification and Compression of Fem- Generation of non-classical light via self- Scanning Customized Swept-source Optical tosecond Pulses by Fiber Parabolic Pre- induced transparency in mercury-filled Coherence Tomography (SS-OCT) for the Shaping, Walter P. Fu1, Yuxing Tang1, Timothy hollow core photonic crystal fibers, Ulrich Metrology of Freeform Optical Surfaces, Di S. McComb2, Tyson L. Lowder2, Frank W. Vogl1, Florian Sedlmeir1, Nicolas Joly1, Chris- Xu1, Jianing Yao1, Nan Zhao1,2, Jannick P. Rol- Wise1;1Cornell Univ., USA; 2nLIGHT Corpora- toph Marquardt1, Gerd Leuchs1; 1MPI for the land1; 1The Inst. of Optics, Univ. of Rochester, tion, USA. We present a combined pulse Science of Light, Germany. We successfully USA; 2Changchun Inst. of Optics, Fine Mechan- amplification and compression scheme utilizing demonstrate squeezing of nanosecond pulses ics and Physics, Chinese Academy of Sciences, parabolic pre-shaping in optical fiber. Clean, via self-induced transparency in a system China. A high-precision SS-OCT system with near-transform-limited, 300 fs pulses are of mercury vapor confined in a hollow core custom scanning configuration was developed generated from 9 ps seeds, accompanied by kagomé-style fiber. for the point cloud metrology of freeform optical amplification to the few-microjoule level. surfaces. Capabilities were demonstrated on an Alvarez surface and a measurement precision of λ/20 was achieved.

FiO/LS 2016 • 16–21 October 2016 83 Grand Ballroom A (Radisson) Grand Ballroom B (Radisson) Grand Ballroom C (Radisson) Grand Ballroom D (Radisson)

FiO

FW5B.6 • 17:30 FW5C.5 • 17:30 Invited FW5D.5 • 17:30 Optimization of Coaxial Tm/Ho-Doped Fiber Lasers, Krysta Double-clad Fiber Couplers: Novel Devices for Multimodal Orbital Angular Momentum Multiplexing using Low-Cost 1 2 1 1 VCSELs for Datacenter Applications, 1 Boccuzzi , G. A. Newburgh , John R. Marciante ; Univ. Imaging., Caroline Boudoux1; 1Engineering Physics, Ecole Mehdi Nouri , Hiva 2 1 1 1 of Rochester, USA; U.S. Army Research Laboratory, USA. Polytechnique Montreal, Canada. Innovation in double-clad Shahoie , Timothy LaFave , Solyman Ashrafi , Duncan Mac- 1 1 Simulations of a novel coaxial fiber having a Ho-doped core fiber couplers allow for efficient separation (or combination) Farlane ; Electrical Engineering, Southern Methodist Univ., surrounded by a Tm-doped ring resulted in 52% laser effi- of coherent and diffuse light, which makes them ideally suited USA. Development of 428 Gb/s free space data communica- ciency. The conventional method, a Tm:fiber laser pumping to perform multimodal endoscopic optical imaging. tions link based on OAM multiplexing using 850nm VCSELs a Ho:fiber laser, yielded a maximum 43% efficiency. is presented. Passive optical mode sorters are used for MUX (transmit) and DeMUX (receive).

FW5B.7 • 17:45 Invited FW5D.6 • 17:45 All-fiber Combining Concepts in the Wavelength Range Wavelength Selective External Cavity Laser Using an Around 2 µm, Hakan S. Sayinc1, Katharina Hausmann1, InAs Quantum Dot Gain Chip and an Arrayed-Waveguide 1 Wednesday, 19 October Wednesday, Christoph Ottenhues1, Okan Isik1, Michael Steinke1, Saniye Grating for T-band Optical Communication, Yudai Okuno , 2 3 S. Yilmaz1,2, Samir Lamrini3, Jörg Neumann1, Fatih Ömer Yasunori Tomomatsu , Yoshinori Sawado , Katsumi Yo- 3 1 1 1 Ilday2, Dietmar Kracht1; 1Laser Zentrum Hannover e.V., Ger- shizawa , Hideaki Shibutani , Hiroyuki Tsuda ; Keio Univ., 2 3 many; 2Department of Physics, Bilkent Univ., Turkey; 3Laser Japan; Koshinkogaku Corporation, Japan; Pioneer Micro Development, Lisa Laser OHG, Germany. We investigated Technology Corporation, Japan. The wavelength selective combining in the 2 µm wavelength range. Tapered fused external cavity laser using an InAs quantum dot gain chip bundles enabled multi-mode combining, while coupling and an arrayed-waveguide grating for T-band communication of single-mode sources to a truly single mode fiber was is proposed and the output wavelength can be tuned from performed employing cascades of wavelength division 1041.8 nm to 1090.5 nm. multiplexers.

17:00–17:45 OSA Annual Business Meeting, Hyatt Regency Rochester, Regency Ballroom C

17:00–18:00 APS Division of Laser Science Annual Business Meeting, Radisson Hotel Rochester Riverside, Genesee Suite F

18:30–21:30 OSA 100 Year BASH, The Sibley Building, 228 East Main Street, Rochester, New York

84 FiO/LS 2016 • 16–21 October 2016 Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E

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FW5E.5 • 17:30 Invited FW5F.5 • 17:30 FW5G.5 • 17:30 FW5H.7 • 17:30 LW5I.4 • 17:30 Zernike Coefficient Measurement Using Subradiance in a nanofiber mode by an en- Prospects for Multi-kJ Plasma Amplifiers, Pe- Comb-Like Frequency-Bin Entangled Photon Windshield Metrology: Simultaneous Geometric Phase shifting Radial Shearing semble of a few cold Rb atoms, 1 ter A. Norreys1,2, James Sadler1, Raoul M. Pair Generation in Silicon Nitride Micror- measurement of wedge angle and layer Pablo Solano , 1,2 1 1 Interferometer, 1 1 Trines2, Robert Bingham2, Muhammad Kasim1, ing Resonators, Jose A. Jaramillo-Villegas , thickness, Michael A. Marcus ; Lumetrics, Chittur S. Narayanamur- Burkley Patterson , Steve L. Rolston , Luis A. 1 1 1 1 1 1 2 3 Luke Ceurvorst1, Naren Ratan1; 1Department Poolad Imany , Ogaga D. Odele , Xiaoxiao Xue , Inc, USA. An interferometric apparatus to thy ; Indian Inst. of Space Sci & Tech, India. Orozco , Fredrik K. Fatemi , James Clemens , 1 1 1 3 5 of Physics, Univ. of Oxford, UK; 2Central Laser Yi Xuan , Kyunghun Han , Daniel E. Leaird , simultaneously measure layer thickness and Geometric phase shifting radial shearing inter- Perry Rice , Pablo Barberis Blostein , Howard Wednesday, 19 October 1 1 1 4 1 Facility, STFC Rutherford Appleton Labora- Minghao Qi , Andrew M. Weiner ; Purdue wedge angle profiles in multilayer windshields ferometer method is used to determine Zernike Carmichael ; Univ. of Maryland at College Park, 2 2 3 tory, UK. Plasma amplifiers potentially offer a Univ., USA; Universidad Tecnológica de Pereira, is described along with its measurement Co-efficients of Kolmogorov type turbulence USA; Army Research Laboratory, USA; Physics, 4 route to low cost, high efficiency, multi-kJ laser Colombia. We report a comb-like frequency- reproducibility. A hand-held probe simplifies affected wavefront with detailed comparison Miami Univ., USA; Physics, Univ. of Auckland, 5 pulses. I will describe numerical simulations bin entangled photon pair source with a high alignment to the windshield surface. with SHWS data. New Zealand; IIMAS, UNAM, Mexico. The underpinning careful experiment design and coincidence to accidental ratio in a silicon nitride excitation-decay from a few cold Rb atoms into interpretation to optimize this process at the microring resonator. We measured a Schmidt the mode of an optical nanofiber shows two Univ. of Rochester. number of 4.0, thus verifying high degree of distinct time-scales: First the normal lifetime, time-frequency entanglement. and then a longer subradiant lifetime that scales linearly with optical density.

FW5F.6 • 17:45 FW5G.6 • 17:45 FW5H.8 • 17:45 LW5I.5 • 17:45 Direct Compressive Imaging of Joint Quan- Multifunctional Optics Testing Using Wave- Achromatic Resonances in an Optical Micro- Frequency Modes of Ultrafast Pumped, tum States with Strong Projections, Samuel H. front Technology, Johannes Pfund1, Christian cavity, Soroush Shabahang1, H. Esat Kondakci1, High-Gain Modulational Instability: Chirp Knarr1, Daniel Lum1, James Schneeloch2, John Brock1, Ralf Dorn1; 1Optocraft Metrology Massimo L. Villinger1, Joshua Perlstein2, Ayman Tuning & Characterization, Martin A. Finger1, Howell1; 1Univ. of Rochester, USA;2Air Force Re- GmbH, Germany. Consumer optics require Abouraddy1,2; 1Univ. of Central Florida, CREOL, Nicolas Joly2,1, Philip S. Russell1,2, Maria V. search Laboratory , USA. We are performing an multifunctional and high performance test USA; 2Materials Science and Engineering, Univ. Chekhova1,2; 1Max Planck Inst for the Science experiment to incorporate compressive sensing equipment. Latest developments and examples of Central Florida, USA. Achromatic transmission of Light, Germany; 2Department of Physics, into a direct measurement protocol to measure are described and how multifunctional optics in a Fabry-Perot microcavity is demonstrated Univ. of Erlangen-Nuremberg, Germany. The general transverse joint-states using strong testing can be realized on basis of wave-front by angularly-multiplexed phase-matching. A effective number of frequency modes for twin projections. We present simulation results of a sensing combined with other techniques. 0.7-nm-wide resonance is broadened to 60nm, beams generated in a gas-filled PCF can be 256 × 256 system using 9% sampling. spanning multiple cavity FSRs, by assigning each continuously tuned via the pump-pulse chirp. wavelength to an appropriate incidence angle. Spectral covariance measurements yield the shapes and relative weights of the modes.

17:00–17:45 OSA Annual Business Meeting, Hyatt Regency Rochester, Regency Ballroom C

17:00–18:00 APS Division of Laser Science Annual Business Meeting, Radisson Hotel Rochester Riverside, Genesee Suite F

18:30–21:30 OSA 100 Year BASH, The Sibley Building, 228 East Main Street, Rochester, New York

FiO/LS 2016 • 16–21 October 2016 85 07:00–17:00Empire Registration, Hall Galleria JOINT FiO/LS 08:00–09:30 JTh1A • Joint Plenary Session II, Lilac Ballroom

09:30–14:00 Exhibits Open, Empire Hall

09:30–14:00 Glass Art Contest, Empire Hall

09:30–10:00 Coffee Break, Empire Hall

09:30–10:30 Unopposed Exhibit Only Time, Empire Hall

Empire Hall

JOINT FiO/LS

09:30–11:00 JTh2A • Joint Poster Session II

JTh2A.1 JTh2A.3 JTh2A.5 JTh2A.7 JTh2A.10

Optical surface profilometry using Fresnel Stimulated Low-Frequency Raman Scat- Zero Rabi Flopping in the presence of a An Experimental study of Odd-Order Disper- Nonlinear absorption in WS2 and MoS2 mono- diffraction from a 2D array of reflective tering, Anna Kudryavtseva1, Nikolay V. Tch- Field, Julio Cesar Garcia Melgarejo1,2, Edgar sion Effects in Propagation of Long-Range and few-layer films, Saifeng Zhang1, Yuanxin phase-steps, Pegah Asgari1, Yousef Pourvais2, erniega1, Konstantin I. Zemskov1; 1P.N. Lebedev Samuel Arroyo Rivera2, Ricardo Martínez Surface Plasmon Polaritons Using a Hong- Li1, Niall McEvoy2, Jun Wang1; 1Shanghai Inst Ahmad Darudi1; 1Zanjan Univ., Iran2Physics, Univ. Physical Inst., Russian Federation. Stimulated Martínez2, José Alfredo Ramírez Flores2, Ou-Mandel Interferometer, Naoto Name- of Optics & fine Mechanics, USA;2Centre for of Tehran, Iran. In this paper, a novel method low-frequency Raman scattering, caused by Javier Sanchez Mondragon1; 1Inst Nac Astro- kata1, Ryo Kobayashi1, Takahide Sakaidani1, Research on Adaptive Nanostructures and is presented for optical surface profilometry, laser pulses interaction with acoustic vibrations fisica Optica Electronica, Mexico; 2Universidad Shuichiro Inoue1; 1Nihon Univ., Japan. Higher- Nanodevices (CRANN) and Advanced Materi- based on phase-step diffractometry. The of nanoparticles, has been studied in the wide Autónoma de Coahuila, Mexico. The idle role order dispersion effects on long-range surface- als and BioEngineering Research (AMBER)

technique combines the advantages of range of nanoobjects both in high-ordered of the photonic dark state of the X-Cavity plasmon-polariton waveguide have been Centre, Trinity College Dublin, Ireland.WS2 and

Hartamnn and Fizeau methods and is tolerant and random materials, in inorganic and organic JCM is quite an interesting feature because investigated using a quantum interferometer. MoS2 mono- and few-layer films were fabricated with environmental noises. substances. arises from dipole orientation. We discuss the We observed degradation of the quantum by vapor phase sulfurization or chemical vapor zero Rabi flopping in its presence and discuss indistinguishability which originated from the deposition method. The nonlinear absorption JTh2A.2 JTh2A.4 its evidence. odd-order dispersions. (saturable absorption, two-photon absorption)

Thursday, 20 October Thursday, Spatial Squeezing in Bright Twin Light Constant intensity waves and transmission properties in VIS to NIR range were investigated. Beams using a CCD Camera, Ashok Kumar1, through non-Hermitian disordered me- JTh2A.6 JTh2A.8 Hayden Nunley1, Alberto Marino1; 1The Univ. dia, Konstantinos Makris1, Andre Brandstotter2, Plasmonic Effect of Low-Dimensional Elec- Withdrawn. JTh2A.11 of Oklahoma , USA. We report the direct Phillip Ambichl2, Ziad Musslimani3, Stefan Rot- tron Gas in Core-Shell Nanowires, Kiana Mon- Nonlinear optical response of a two-dimen- measurement of 2 dB of spatial squeezing ter2; 1Univ. of Crete, Greece; 2Inst. for Theoreti- tazeri1, Zhihuan Wang1, Bahram Nabet1; 1Drexel JTh2A.9 sional atomic crystal, Michele Merano1; 1Uni- with an EMCCD camera. We use bright twin cal Physics, Vienna Univ. of Technology, Aus- Univ., USA. We analyze the plasmonic effect of Ambient-condition growth of high-pressure versita degli Studi di Padova, Italy. The theory beams of light generated through four-wave tria; 3Mathematics, Florida State Univ., USA. By core-shell nanowires explaining how metallic phase centrosymmetric crystalline KDP of Bloembergen and Pershan for the light mixing in a double-lambda configuration in Rb using the concept of constant-intensity waves, layers and low-dimensional electron gas microstructures for efficient optical second waves at the boundary of nonlinear media is atomic vapor. we show that perfect transmission through the formed at the heterojunction of the core and harmonic generation, Y. Ren2, Lu Deng1, extended to a nonlinear two-dimensional atomic disordered media is possible. Such scattering the shell affect the optical cavity and mode E.W. Hagley1, X. Zhao2; 1National Inst of crystal. A comparison with experimental results states can exist in non-Hermitian scattering generations. Standards & Technology, USA; 2State Key is reported. landscapes with suitably engineered gain-loss Laboratory of Crystal Materials, Shandong distributions. Univ., China. We report ambient-condition growth of one-dimensional, self-assembled, single-crystalline KDP hexagonal hollow/solid core microstructures having molecular structure and symmetry identical to the type-IV KDP monoclinic crystal phase.

86 FiO/LS 2016 • 16–21 October 2016 Empire Hall

JOINT FiO/LS

JTh2A • Joint Poster Session II—Continued

JTh2A.12 JTh2A.16 JTh2A.20 JTh2A.24 JTh2A.29 Optical Pumping of Alkali Hyperfine States via Effect of Spin Squeezing Followed by Revivals in the Jaynes-Cummings model in Highly-sensitive detection of the lattice dis- Numerical Algorithm for Finding Optimal Free-Free Molecular Absorption: Demonstra- Anti-Squeezing in a Collective State Atomic terms of characteristic functions, Hudson tortion in single bent ZnO nanowires by sec- Experimental Setup for Arbitrary Uni- tion of Circularly Polarized Stimulated Emis- Clock, Resham Sarkar1, Minchuan Zhou1, Ren- Pimenta1, Daniel F. James1; 1Univ. of Toronto, ond-harmonic generation microscopy, Xiaobo tary Operator, Sushovit Adhikari1, Jona- 1 1 1 1 1 1 1 1 1 1 sion on the Alkali D2 Lines, Andrey Mironov , peng Fang , Selim Shahriar ; Northwestern USA. Through the periodicity of characteristic Han , Kai Wang , Peixiang Lu ; HUST, China. A than Dowling ; Louisiana State Univ., USA. A James G. Eden1; 1Electrical and Computer Engi- Univ., USA. Two-axes counter-twist (TACT) spin- functions, we find that atomic population high detection sensitivity of ~0.001 nm on the numerical algorithm to generate an optimal neering, Univ. of Illinois at Urbana-Champaign, squeezing can significantly reduce the quantum revivals in the Jaynes-Cummings model are bending distortion is obtained by measuring experimental setup for arbitrary unitary matrix USA. We report a novel method for the pumping projection noise in an ensemble of two-level replicas of each other that have experienced the SHG polarimetric patterns. The twisting has been developed. Given an unitary operator, of alkali hyperfine states by using circularly atoms. Here, we investigate the effect of TACT dispersion akin to that of free particles in distortion can also be detected by observing the algorithm designs the experiment with the polarized pump light absorbed by alkali-rare followed by an anti-TACT pulse in a collective quantum mechanics. the extraordinary non-axisymmetrical SHG least number of beam splitters used. gas atomic pairs. state atomic clock. polarimetric patterns. JTh2A.21 JTh2A.30 JTh2A.13 JTh2A.17 The cross-cavity micromaser., Julio Cesar Gar- JTh2A.25 Optimal Architectures for Single Photon Effect of Purcell Enhancement on Internal Entanglement Constraints with Quan- cia Melgarejo1,2, Nestor Lozano-Crisostomo1,2, Optical Image Cloning based on Electro- Metrology, Margarite L. LaBorde1, Jonathan P. Quantum Efficiency of InGaN Green Light- tum Background Parties, Xiao-Feng Qian1, José Alfredo Ramírez Flores1, Ricardo Martínez magnetically Induced Absorption, Sha- Olson1, Keith R. Motes2, Patrick Birchall3, Nick Emitting Diode Structures, Han-Youl Ryu1, Miguel A. Alonso1, Joseph H. Eberly1; 1Univ. Martínez1, Javier Sanchez Mondragon1;1Inst Nac maila Manzoor1, Ulices F. Apolinario1, Luis E. M. Studer1, Todd Moulder1, Peter P. Rohde4, Guen-Hwan Ryu1, Young-Hwan Choi1; 1Inha of Rochester, USA. We include the usually Astrofisica Optica Electronica, Mexico; 2Uni- Araujo1; 1Instituto de Física “Gleb Wataghin,” Jonathan Dowling1; 1Hearne Inst. for Theoretical Univ., Korea. We theoretically investigate the neglected unidentified non-interacting quantum versidad Autónoma de Coahuila, Mexico. The Universidade Estadual de Campinas, Brazil. We Physics and Department of Physics & Astronomy, modification of internal quantum efficiency background in the analysis of open system experimental and QED dynamics of a JCM experimentally demonstrate, for the first time, Louisiana State Univ., USA; 2Department of (IQE) in InGaN green flip-chip LED structures dynamics. A set of generic inequalities of micromaser relies on the JCM fully solvability. imaging cloning of the spatial profile of a strong Physics and Astronomy, Macquarie Univ., as a result of the Purcell effect that is found to entanglement dynamics is discovered and their We discuss an analogous case, an X-cavity, coupling beam onto that of a weak probe beam Australia; 3Centre for Quantum Photonics, H. be quite advantageous for improving the IQE novel geometric representations are presented. where a new quantum feature produced by the via electromagnetically induced absorption in a H. Wills Physics Laboratory and Department of InGaN green LEDs. x-cavity has not been accounted. warm Rb vapor cell. Electrical and Electronic Engineering, Univ. of JTh2A.18 Bristol, UK; 4Centre for Quantum Computation JTh2A.14 Control of spatial distribution of entangled JTh2A.22 JTh2A.26 and Intelligent Systems, Faculty of Engineering Non-local angular double-slit ghost diffrac- photons by the spatial structure of classical The cross-cavity photon dark state., Julio Nondegenerate Nonlinear Refraction in Semi- & Information Technology, Univ. of Technology, Thursday, 20 October tion with thermal light, Lu Gao1, J.P. Zhao2, pump beam, Jabir M. V.1, N. Apurv Chaitanya1,2, Cesar Garcia Melgarejo1,2, Edgar Samuel conductors, Peng Zhao1, Matthew Reichert2, Australia. Passive linear optics are utilized to Omar S. Magaña-Loaiza2, Seyed Mohammad Goutam K. Samanta1; 1Physical Research Labora- Arroyo Rivera1, Daniel Alberto May Arrioja3, David Hagan1, Eric Van Stryland1; 1CREOL determine an interferometer with single-photon Hashemi Rafsanjani2, Mohammad Mirhosseini2, tory, India; 2Indain Inst. of Technology, India. We Miguel Torres Cisneros4, Javier Sanchez Mon- Univ. of Central Florida, USA; 2Princeton inputs capable of high phase sensitivity. This Yiyu Zhou2, Robert W. Boyd2; 1School of Science, control the spatial distribution of entangled dragon1; 1Inst Nac Astrofisica Optica Electronica, Univ., USA. The dispersion of nondegenerate structure was optimized to maximize phase Univ. of Geosciences (Beijing), China; 2The Inst. photons generated through SPDC process by Mexico; 2Universidad Autónoma de Coahuila, nonlinear refraction in semiconductors is sensitivity and furthermore to explicitly compute of Optics, Univ. of Rochester, USA. We report manipulating spatial structure of classical pump Mexico; 3Centro de Investigaciones en Óptica, measured using our beam-deflection method. this sensitivity. 4 an experimental observation of ghost diffraction beam. Using vortex pump beam, we show that A. C., Mexico; Universidad de Guanajuato, With high nondegeneracy, n2 is significantly with non-local angular double-slit by making use the entangled photons have doughnut spatial Mexico. The photonic dark state of the X-Cavity enhanced over degenerate case, and rapidly JTh2A.31 of thermal light OAM correlation measurement. distribution. JCM is one of the interesting joint features of switches sign to negative near the bandgap. Dark gap polariton solitons in a one-di- Correlated angular interference patterns of the the orthogonal single cavity modes pair. We mensional periodic potential, Ting-Wei distributed angular double-slit are measured. JTh2A.19 test its quantum nature by introducing a second JTh2A.27 Chen1, Szu-Cheng Cheng1; 1Chinese Culture Wideband Suppression of Local Density Two Level Atom. Withdrawn. Univ., Taiwan. The dark polariton solitons are JTh2A.15 of States in Random Waveguides, Xiaojun investigated in a 1D periodic potential. The The Effect of Misaligned Modal Loss on Cheng1,2; 1CUNY Queens College, USA; 2Gradu- JTh2A.23 JTh2A.28 effective-mass approximation is used to obtain Entangled Qubits, Brian T. Kirby1, Michael ate Center of CUNY, USA. We find the local Choice of the Detection Location in a Three- Caustic and wavefronts produced by arbi- the numerical dark solitons in the zone center Brodsky1; 1US Army Research Laboratory, density of states inside quasi-1D random Party Measurement-Device-Independent trary reflecting surfaces, Maximino Avendaño and edge under a diversity of potential depths USA. Quantum Networks require the ability to waveguide is increasingly suppressed in the Quantum Key Distribution System, Yucheng Alejo1; 1Universidad Nacional Autonoma de and pump powers. distribute entanglement to remote nodes, which middle of the sample over a wide frequency Qiao1, Zhengyu Li1, Ziyang Chen1, Bin Luo2, México, Mexico. We provide a simple formulas could be degraded by the mode dependent loss range with increasing sample length and Xiang Peng1, Hong Guo1; 1Peking Univ., for reflected caustics and wavefronts through in transmission channels. We offer an elegant decreasing waveguide cross section. China; 2Beijing Univ. of Posts and Telecom- smooth surfaces considering an incident plane way to account for the mode loss impact. munications, China. We propose a method of wavefront propagating along the optical axis, choosing the detection location for a three-party having a wide potential of non-imagining optical measurement-device-independent quantum systems for solar concentrators. key distribution system, which can simplify the parameter optimization problem for practical applications.

FiO/LS 2016 • 16–21 October 2016 87 Empire Hall

JOINT FiO/LS

JTh2A • Joint Poster Session II—Continued

JTh2A.32 JTh2A.36 JTh2A.40 JTh2A.44 JTh2A.49 Highly Efficient Self-Q-Switched Erbium- Design and Analysis of high bandwidth Bragg Tomographic studies of polymer optical bridg- Molecular Imprinting and SPR Based Fiber Optically Bound Micro-Particle Arrays near Ytterbium Fiber Laser Operating at High Fiber having Triangular Refractive Index Core es produced by photopolymerization, Michal Optic Sensor for 1-Naphthol, Banshi D. Gupta1, Ultrathin Optical Fibers, Aili Maimaiti1, Daniela Output Powers, Luis F. Samano Aguilar1, Profile for Broadband Applications, Vikram Dudek1, Malgorzata Kujawinska1; 1Inst. of Anand M. Shrivastav1, Sruthi P. Usha1; 1Indian Holzmann2, Viet Giang Truong1, Helmut Ritsch 2, Juan C. Hernandez Garcia 1,2, Julian Moises Palodiya1, Sanjeev K. Raghuwanshi1;1Indian Micromechanics and Photonics, Warsaw Univ. Inst. of Technology, Delhi, India. We introduce Sile Nic Chormaic1; 1Okinawa Inst of Science Estudillo Ayala1, Roberto Rojas Laguna1, Olivier School of Mines, Dhanbad, India. In this paper, of Technology, Poland. The studies of 3D an approach to develop an optical fiber sensor & Technology, Japan; 2Univ. of Innsbruck, Pottiez3, Jose David Filoteo Razo1, Jesus Pablo we have studied performance of Bragg fiber refractive index distribution in polymer optical for 1-naphthol using molecular imprinting and Austria. Particles trapped in the evanescent Lauterio Cruz3, Daniel Jauregui Vazquez1; 1Uni- having different type of core profile. Its disper- bridges are presented. Digital holographic SPR phenomenon. Wavelength interrogation field of ultrathin optical fibers can interact via versidad De Guanajuato, Mexico; 2CONACYT, sion, power confinement, group delay, bending system in shearing interferometer configuration method is used for sensor characterization. scattering of the fiber-guided light fields. Here, Mexico; 3CIO, Mexico. Ring self-Q-switched losses, effective nonlinear refractive index and for projections capture and detailed procedure The sensor operates for concentration range we study the difference between fundamental Er3+/Yb3+ fiber laser operated at 1565 nm is polarization mode dispersion are studied. of tomographic reconstruction are described. of 0-100µM. and higher order mode optical binding of presented. The configuration has: high efficient polystyrene beads. (~62%), high output power (10 W) and short JTh2A.37 JTh2A.41 JTh2A.45 pulses generation (ns), allowing a stable multiple Tunable wavelength Thulium-doped fiber Polarization Evolution of Vector Wave Pulses Narrow-linewidth monolithic CW 2 kW fiber JTh2A.50 pulsing regime. laser based in a Hi-Bi Fiber Optical Loop in Twisted Fibers Pumped by Single and Cou- laser with near diffraction-limited beam Soliton-Mediated Dispersive Wave Re- Mirror, Manuel Duran-Sanchez1,2, Ricardo Iván pled Solitons, Mohammad Almanee1, Joseph quality, Wei Shi1; 1Tianjin Univ., China. We flection for Multimode Supercontinuum JTh2A.33 Alvarez-Tamayo1, Baldemar Ibarra-Escamilla1, Haus1, Ivan Armas-Rivera3, Georgina Beltran- demonstrate a monolithic CW fiber laser source Generation, Vishwatosh Mishra1,2, Satya Optical reversible gate based on lithium Evgeny Kuzin1, Antonio Barcelata-Pinzón3; 1IN- Perez3, Baldemar Ibarra-Escamilla2, Manuel at 1070.25 nm, producing 2 kW laser power with P. Singh1, Raktim Haldar2, Shailendra K. niobate based Mach Zehnder Interfer- AOE, Mexico; 2CONACyT, Mexico; 3UTP, Duran-Sanchez2, Ricardo I. Álvarez-Tamayo2, very narrow spectral linewidth (<0.3 nm) and Varshney1,2;1Department of Physics, IIT Kharag- ometers, Chander kanta1, Santosh Kumar1, Mexico. A tunable wavelength operation of a Evgeny Kuzin2, Yazmin Bracamontes-Rodríguez4, near diffraction-limited beam quality (M2 =~1.3). pur, India; 2Department of E&ECE, IIT Kharag- Angela Amphawan2,3; 1DIT Univ., India; 2School linear cavity Thulium-doped fiber laser based Olivier Pottiez4; 1Univ. of Dayton, USA; 2Optics, pur, India. Femtosecond pulse propagation in of Computing, Universiti Utara Malaysia, Malay- on the use of a fiber optical loop mirror with Instituto Nacional de Astrofisica, Optica y JTh2A.46 multi-mode PCF has been studied numerically 3 3 sia; Massachusetts Inst. of Technology, USA. In high birefringence (Hi-Bi) fiber in the loop is Electronica, Mexico; Benemérita Universidad Strain Manipulation of Hybrid Graphene- including azimuthally symmetric modes LP01 and 4 1 this paper, basic reversible logic gate (Peres experimentally demonstrated. Autónoma de Puebla, Mexico; Centro de Microfiber Waveguide, Jin-hui Chen , Fei LP02. The presence of LP02-mode facilitates par- gate) using the lithium niobate based Mach- Investigaciones en Optica, Mexico. Nonlinear Xu1; 1Nanjing Univ., China. Here the strain tial reflection of dispersive wave by the soliton

Zehnder Interferometer is proposed. The results JTh2A.38 polarization dynamics of single and coupled characteristics of a hybrid graphene-microfiber in LP01-mode. are verified using beam propagation method Mid-infrared Dispersive Waves Generation solitons in twisted fibers is experimentally and waveguide structure is first investigated. By in-

and MATLAB simulations. in an All-solid AsSe2-As2S5 Microstructured numerically studied. The output polarization line loading strain, we can achieve modulating JTh2A.51 Optical Fiber, Tonglei Cheng1, Hoang Tuan for two solitons evolves towards a circular transmission of the device as high as 30% with Self-similar Propagation in a Dispersion Man- JTh2A.34 Tong1, Lai Liu1, Xiaojie Xue1, Morio Matsumoto2, polarization and shows a jump at linear input ~5% strain. aged and Highly Nonlinear Segmented Band- Atom-photon interface using the higher order Hiroshige Tezuka2, Takenobu Suzuki1, Yasutake ellipticity. gap Fiber in the mid-IR, Piyali Biswas1, Somnath modes of an ultrathin optical fiber, Thomas Ohishi1; 1ofmlab, Japan; 2Furukawa Denshi Co., JTh2A.47 Ghosh1, Abhijit Biswas1, Bishnu P. Pal2; 1Univ. Nieddu1, Jinjin Du1, Sile Nic Chormaic1; 1Oki- Ltd., Japan. We design an all-solid chalcogenide JTh2A.42 Soliton Interaction in Nearly Degenerate of Calcutta, India; 2Mahindra École Centrale, nawa Inst. of Science and Technology Gradu- microstructured optical fiber with four rods in the Fabrication and characterization of a tel- Modes of a Multimode Fiber, Shaival Buch1, School of Natural Sciences, India. Rapidly ate School, Japan. We create an atom-photon cladding in order to generate the mid-infrared lurite all-solid photonic bandgap fiber with Govind P. Agrawal1; 1Univ. of Rochester, varying but of nearly-mean-zero longitudinal interface using the higher order modes (HOM) of dispersive waves. three rings of high index rods, Hoang Tuan USA. We numerically investigate soliton dispersion profile has been adopted to achieve an ultrathin optical fiber. We explore interactions Tong 1, Kenichi Hashimoto1, Shunta Tanaka1, interaction in nearly degenerate modes of a self-similar propagation of parabolic optical between HOMs and a cold atomic ensemble, JTh2A.39 Kenshiro Nagasaka1, Takenobu Suzuki1, Yasutake multimode fiber. Periodic intermodal power pulses through a chalcogenide glass based and Thursday, 20 October Thursday, with aim to transfer and store orbital angular Chromatic dispersion engineering in chalco- Ohishi1; 1Optical Functional Materials Labora- transfer is observed and its dependence on segmented highly-nonlinear bandgap optical momentum. genide multi-step index fiber for mid-infrared tory, Toyota Technological Inst., Japan. We phase, temporal delay, propagation constant fiber at 2.8 µm. supercontinuum generation, Kenshiro Naga- demonstrate a tellurite all-solid photonic and group velocity difference is studied. JTh2A.35 saka1, Hoang Tuan Tong1, Lai Liu1, Takenobu bandgap fiber (AS-PBF) with three rings of JTh2A.52 High power phase-locked four cores fiber Suzuki1, Yasutake Ohishi1; 1Research Center for high-index rods. It has lower confinement loss JTh2A.48 FO-LMR Based Chlorine Gas Sensor Using laser, Liu YeHui1, Wang Yibo1, Liao Lei1, Li Advanced Photon Technology, Toyota Techno- and better performance as compared with the Hybrid Fiber Optic Probe for Fluidized Zinc Oxide Nanostructure, Sruthi P. Usha1, Haiqing1, Peng jinggang1, Yang lvyun1, Li Jin- logical Inst., Japan. Chalcogenide multi-step previously reported tellurite AS-PBF. Gas-Solid Beds, Jorge Galvis1, Pedro Torres1, Anand M. Shrivastav1, Banshi D. Gupta1; 1Indian yan1; 1Huazhong Univ. of Science&Technolog, index fiber with zero-flattened chromatic Alejandro Molina1; 1Universidad Nacional de Inst. of Technology, Delhi, India. Lossy mode China. We demonstrate a high power 4 cores dispersion is developed to realize mid-infrared JTh2A.43 Colombia-Medelli, Colombia. We present the resonance based fiber optic chlorine gas sensor Yb-doped fiber amplifier which is operated in an supercontinuum generation. We simulate mid- Guided Acoustic Wave Brillouin Scattering concept of hybrid fiber optic probe for fluidized using ZnO nanoparticles is reported. A shift of 14 in-phase supermode and does not need other infrared supercontinuum generation covering (GAWBS) and Slow Light in Optical Fi- gas-solid beds. We found that the hybrid fiber nm in peak absorbance wavelength is observed mode selection mechanisms.The maximum 2-19 μm in the designed fiber. bers, Christopher K. Horne1, Chung Yu1, Zhijian optic probes are promising to simultaneously for the change in chlorine concentration from output power is 9.75 W. Xie1; 1North Carolina A&T State Univ., USA. We measure solids concentration and particle 10 to100 ppm. report the nonlinear effects of Guided Acoustic velocity. Wave Brillouin Scattering on pulse delay and distortion in a special low light device.

88 FiO/LS 2016 • 16–21 October 2016 Empire Hall

JOINT FiO/LS

JTh2A • Joint Poster Session II—Continued

JTh2A.53 JTh2A.57 E-Poster JTh2A.63 JTh2A.67 JTh2A.70 Optical Fiber SPR Sensor for Simultaneous Spatial Frequency Modulated Imaging (SPIFI) Photon sieve on an optical fiber tip for Reconstruction of refractive index profile of Laser-induced localized photothermal con- Determination of Cu(II) and Pb(II) Ions Using in Amplitude with a Spatial Light Modula- improved light coupling into a submicron photonic crystal fiber using intensity based version of vanadium into vanadium ox- 1 1 1 1 Molecular Imprinting, Anand M. Shrivastav , tor, Michael D. Young1, Jeffrey J. Field2, Randy silicon waveguide, Ricardo Janeiro , Raquel optical diffraction tomography, Jem Teresa ides, Giwan Seo , Jong-Bum You , Shin ho 1 1 1 1 1 1 1 1 1 1 1 1 2 1 1 Sruthi P. Usha , Banshi D. Gupta ; Indian Inst. Bartels2, Jeff Squier1; 1Colorado School of Mines, Flores , Pabitra Dahal , Jaime Viegas ; Mas- John , Ram M. Vasu , Rajan Kanhirodan ; Indian Kim , Bong-Jun Kim , Kyoungsik Yu ; Korea 2 of Technology, Delhi, India. Fabrication and USA; 2Colorado State Univ., USA. Previous work dar Inst., United Arab Emirates. The superior Inst. of Science, India. An iterative Gauss- Advanced Inst of Science & Tech, Korea; Mo- characterization of SPR based fiber optic sensor has demonstrated modulated imaging with performance over a commercial tapered fiber Newton algorithm which uses normal derivative brik Co. Ltd., Korea. In situ laser patterning by for detection of copper and lead ions using binary masks. We present a new microscope for light coupling at 1550 nm into a silicon of intensity(without estimating phase) as the localized photothermal heating is proposed for molecular imprinting in the operating range of that provides continuous modulation with a waveguide has been demonstrated using a measurement, to reconstruct the cross-sectional facile fabrication of vanadium oxide devices 0-10 mg/L and 0.100µg/L for Cu(II) and Pb(II) spatial light modulator, which can modulate photon sieve fabricated by focused ion beam refractive index profile of a photonic crystal fiber. with phase transition property. Optically- ions are reported through multiple methods: amplitude, phase, on an optical fiber tip. controlled resistance switching properties of the polarization, etc. JTh2A.68 synthesized devices are investigated. JTh2A.54 This presentation will be presented as an JTh2A.64 E-Poster Refraction-compensating algorithm for a Measurement of Back-reflection and Back- E-Poster on Screen 4 from 10:15–11:00 Pico-watt radiant flux detection by smart- 3D glass structure exhibiting multiple 2D JTh2A.71 scattering Noise in High Sensitivity Photonic phone, Youngkee Jung1,2, Iyll-Joon K. Doh2, images, Ryuji Hirayama1, Hirotaka Nakayama2, Withdrawn. 1 2 1 2 3 1 Crystal Fibre-optic Gyroscope, Teng Fei , Jing JTh2A.58 Euiwon Bae ; graduate student, USA; Me- Atsushi Shiraki , Takashi Kakue , Tomoyoshi 1 1 1 1 1 1 1 Jin , Zuchen Zhang , Chunxi Zhang ; Beihang Withdrawn. chanical engineering, Purdue Univ., USA. We Shimobaba , Tomoyoshi Ito ; Graduate School JTh2A.72 Univ., USA. The incoherent back-reflected present a smartphone based analytical device of Engineering, Chiba Univ., Japan; 2Center for Analysis of Hollow Core De-multiplexer and backscattered light in PCF IFOG was JTh2A.59 for detecting sub nano-watt level of radiant flux. Computational Astrophysics, National Astro- for Spatially Multiplexed Systems, Syed H. 3 1 1 1 investigated. A more accurate noise model Evaluation Of Transverse Aberration By A 3D printed optical cradle and a new algorithm nomical Observatory of Japan, Japan; Inst. of Murshid , Gregory L. Lovell ; Florida Inst. for PCF IFOG which takes incoherent back- Spatial Modulators, Maria Elizabeth Per- to improve SNR level is suggested. Management and Information Technologies, of Technology, USA. Analysis and simulated reflection and backscattering noise into account cino1; 1INAOE, Mexico. The evaluation process This presentation will be presented as an Chiba Univ., Japan. The 3D structure designed results of hollow core, all optical de-multiplexer was proposed and verified by experiments. of concave surfaces, some methods used E-Poster on Screen 5 from 10:15–11:00 by our algorithm exhibits multiple 2D images architecture is presented that tests the coupling are Hartmann and Ronchi test, which use to different directions. However, refraction efficiency of the structure as the bevel angle of JTh2A.55 spatial modulators. This paper presented the JTh2A.65 at the curved surface of glasses causes the the design is varied for common optical indices. Projective Measurement of the Lagueurre- comparison between them evaluationsalong the Twist phase-induced changes of the polariza- deterioration in the image quality. We proposed Thursday, 20 October Gaussian Spectrum, Seyed Mohammad Hash- diameter perpendicular to the patterns fringes. tion degree and state of a stochastic elec- a refraction-compensating algorithm. JTh2A.73 emi Rafsanjani1, Omar S. Magana Loaiza1, Mo- tromagnetic beam, Lin Liu1; 1Soochow Univ., A design approach of the image map- 1 1 1 hammad Mirhosseini , Robert W. Boyd ; Univ. JTh2A.60 China. A radially polarized partially coherent JTh2A.69 per for the image mapping spectrom- 1 1 of Rochester, USA. We propose a protocol for Withdrawn. twist beam propagating in uniaxial crystal have Experimental Validation of Nodal Aberration eter (IMS), Xiaoming Ding , Yan Yuan , Lijuan measuring the radial index of Laguerre-Gaussian been explored based on the unified theory of Theory with a Customized Ritchey–Chrétien Su1; 1Beihang Univ., China. A design approach of 1,2 1,3 modes, and provide evidence of lossless and JTh2A.61 coherence and polarization.The twist factor Telescope, Nan Zhao , Kevin P. Thompson , the image mapper used in the image mapping 1,4 1,5 unitary transformation of these modes into a Withdrawn. and the anisotropy induced the change of the Jun Zhu , Michael Pomerantz , Jannick P. spectrometer (IMS) is introduced to reduce Gaussian mode. statistical properties. Rolland1; 1The Inst. of Optics, Univ. of Roch- the cross talk and improve the quality of the 2 JTh2A.62 ester, USA; Changchun Inst. of Optics, Fine reconstructed images and spectral information. JTh2A.56 Relationship Between Hermite-Gaussian and JTh2A.66 Mechanics and Physics, Chinese Academy of 3 4 Hybrid Wireless Communication Net- Ince-Gaussian Laser Beams, Allison Hine1, Jes- Employing the Ichikawa-Takeda’s Method Sciences, China; Synopsys, Inc., USA; Tsing- JTh2A.74 E-Poster 5 works: Integrating Free-Space Optics and sica P. Conry1; 1Arkansas Tech Univ., USA. We Applied to Irradiance Transport Equation hua Univ., China; Department of Mechanical Testing cylindrical lenses placing a CCD sensor 1 1 WiFi, Spencer T. Liverman , Qiwei Wang , Yu- generate Ince-Gaussian (IG) laser beams from (ITE): Filtering and Tilt Grid Analysis, Jesús Engineering, Univesity of Rochester, USA. To inside the caustic region, Gabriel Castillo-San- 1 1 1 1 2 1 1 Jung Chu , Arun Natarajan , Thinh Nguyen , Hermite-Gaussian (HG) laser beams using A. Arriaga Hernández , Alejandro Cornejo experimentally validate Nodal Aberration tiago , Maximino Avendaño-Alejo ; CCADET- 1 1 1 1 2 Alan X. Wang ; Oregon State Univ., USA. We an astigmatic mode converter (AMC). The Rodriguez , Elizabeth Percino Zacarias , Fermin Theory, third order spherical, coma, and UNAM, Mexico; Facultad de Ingeniería, UNAM, 1 1 describe WiFO: A hybrid free-space optical relationship between the HG order, IG order S. Granados ; INAOE, Mexico. From Irradiance astigmatism are investigated in a custom Mexico. A method to evaluate the shape of fast and radio frequency system, which will provide and ellipticity, and the rotation of the AMC is Transport Equation, derived by Teague [1]. A Ritchey–Chrétien telescope with precisely plano-convex cylindrical lenses is presented, by downlink speeds of up to 60Mbps over a discussed. detailed analysis was realized to the Ichikawa controlled misalignments achieved with a using null bi-Ronchi type screens, which allows distance of three meters using light emitting [2], arrangement for lens testing; the aspects secondary mirror mounted on a hexapod. to have uniform patterns at detection’s plane diodes while maintaining a high level of mobility studied were filters shape, period and tilt of inside the caustic region. via a WiFi uplink. ruling used experimentally. This presentation will be presented as an E-Poster on Screen 4 from 09:30–10:15

FiO/LS 2016 • 16–21 October 2016 89 Empire Hall

JOINT FiO/LS

JTh2A • Joint Poster Session II—Continued

JTh2A.75 JTh2A.78 E-Poster JTh2A.81 JTh2A.85 JTh2A.89 Quasicylindrical waves at dielectric in- Dynamic surface profiling with synthetic holo- Scattering in PT and RT Symmetric Multimode Coherent Frequency Combs for Dual-Comb Clausius-Mossotti Lorentz-Lorenz rela- 1 2 terfaces, Oliver Higbee , Choon H. Gan , graphic confocal microscopy, Martin Schnell1,2, Waveguides: Generalized Conservation Laws Spectroscopy Spanning 3 to 5.2 µm, Daniel tions and retardation effects for two-di- 1 1 1,2 3 1,2 1 1,3 1 Geoff R. Nash ; College of Engineering, P. Scott Carney2,3, Rainer Hillenbrand4,5; 1CIC beyond 1D, Li Ge , Konstantinos Makris , Maser , Gabriel Ycas , Flavio Cruz , Scott mensional crystals, Michele Merano , Luca 4 5 1 1 1 1 1 Mathematics and Physical Sciences, Univ. of nanoGUNE Consolider, Spain;2Beckman Inst. Demetrios Christodoulides , Liang Feng ; Col- Diddams ; National Inst. of Standards & Dell’Anna ; Universita degli Studi di Padova, 2 2 2 Exeter, UK; Seagate, UK. The contribution for Advanced Science and Technology, Univ. of lege of Staten Island, CUNY, USA; The Tech, USA; Physics, Univ. of Colorado Boul- Italy. We model a single-layer two dimensional 3 3 of quasicylindrical waves to beam collimation Illinois Urbana-Champaign, USA; 3Department Graduate Center, CUNY, USA; Crete Center der, USA; Instituto de Fisica Gleb Wataghin, atomic crystal as a distribution of electric is investigated at a dielectric interface. A of Electrical and Computer Engineering, Univ. for Quantum Complexity and Nanotechnology, Universidade Estadual de Campinas, Brazil. A dipoles on a regular lattice. We evidence a 4 subwavelength aperture surrounded by 1D of Illinois Urbana-Champaign, USA; 4CIC nano- Univ. of Crete, Greece; College of Optics and tunable mid-infrared frequency comb was manifestation of retardation-field effects in the resonant nanogrooves is patterned into a GUNE Consolider and EHU/UPV, Spain; 5IK- Photonics - CREOL, Univ. of Central Florida, created via difference frequency generation. optical response of these crystals. 5 dielectric stack and its far field radiation pat- ERBASQUE, Basque Foundation for Science, USA; Department of Electrical Engineering, Pulses between 1 and 1.5 μm were mixed to tern measured. Spain. We present vibration mode mapping The State Univ. of New York at Buffalo, USA. We make idlers of 3-5.2 μm. Two such combs were JTh2A.90 3+ of a micrometer sized cantilever with confocal derive generalized conservation laws for light heterodyned at 5 μm to show their coherence Spectroscopic Changes of Cr Doped JTh2A.76 Al O Precursors Due to Irreversible microscopy which is based on the combination propagating in a multimode system with Parity- and potential for spectroscopy. 2 3 Quantitative analysis of stainless steel corro- of synthetic optical holography with fast light Time (PT) or Rotation-Time (RT) symmetry. Phase Changes During Subsecond Laser 1 sion by reflective digital holographic micros- detection. These conservation laws can be expressed as JTh2A.86 Heating, Benjamin R. Anderson , Ray Guna- 2 1 1 1 1 1 copy, Yousef Pourvais , Pegah Asgari , Pedram This presentation will be presented as an scalar equalities for generalized transmittance Mimicking explosive heating profiles: feed- widjaja , Patrick Price , Hergen Eilers ; Wash- 1 1 1 Abdollahi , Ali-Reza Moradi , Ramin Khamedi , E-Poster on Screen 3 from 09:30–10:15 and reflectance. back controlled sub-second laser heating us- ington State Univ., USA. We measure the Ahmad Darudi1; 1Zanjan Univ., Iran (the Islamic ing a three-color NIR pyrometer, Benjamin R. subsecond laser-heating-induced spectroscopic 2 JTh2A.82 1 1 1 Republic of); Physics, Univ. of Tehran, Iran (the JTh2A.79 Anderson , Patrick Price , Ray Gunawidjaja , Her- changes of Cr:Al2O3 precursors and find that Introducing an Innovative Active Learning 1 1 Islamic Republic of). Using digital holographic Enhancement in Light-Matter Interac- gen Eilers ; Washington State Univ., USA. We Cr:Al2O3 is a promising candidate for an ex-situ microscopy technique, we suggest a novel tion within Atomic MoS Monolayers on Technique: Flipping Optics Classroom, Sumit develop a feedback controlled sub-second temperature sensor. 2 1 1 quantitative criterion to distinguish between Nanocavities, Corey Janisch1, Haomin Song2, Ghosh ; Physics, Andhra Vidyalaya College, Os- laser heating system to subject materials to intergranular and transgranular corrosion in Chanjing Zhou1, Zhong Lin1, Ana Laura Elías1, mania Univ., India. A higher order thinking, self- temperature profiles mimicking those inside of JTh2A.91 stainless steels. The method can be used to Dengxin Ji2, Mauricio Terrones1, Qiaoqiang regulated methodology – Flipped classroom explosive fireballs. Optical properties of heterogeneous systems 1 study several other metallurgical phenomena. Gan2, Zhiwen Liu1; 1The Pennsylvania State has been employed for teaching optics to the with Ag nanoparticles, Ievgen Brytavskyi , Va- 2 1 Univ., USA; 2Univ. at Buffalo, USA. We report a undergraduate students. Qualitative analysis JTh2A.87 lentyna Skobeeva , Valentyn Smyntyna , Nikolay 2 1 1 JTh2A.77 fundamental strategy to enhance light-matter on the efficacy of this model within the Indian Measurements of the Temperature Depen- Malushin , Klara Vergeles ; Odessa Nationa 2 A New Photoanisotropic-copies-based interaction of atomically-thin films based on context has been presented. dence of the Optical Anisotropy Parameter lI. I. Mechnikov Univ., Ukraine; Research Inst. Pattern Recognition System, of CaF , BaF and SrF Crystals, Barbara N. strong interference in planar nanocavities, 2 2 2 Alexey Ya- of Physics, Odessa National I. I. Mechnikov 1 1 1 1 1 1 Kilosanidze , George Kakauridze , Irina Kobu- which is validated experimentally by absorption JTh2A.83 kovlev , Ilya Snetkov , Oleg Palashov ; Inst. of Univ., Ukraine. The optical properties of 1 1 lashvili ; Laboratory of Hologarphic Recording and photoluminescence enhancement of Invisible Structures as Particular Solutions of Applied Physics RAS, Russian Federation. The heterogeneous systems, including organic (dye) and Processing of Information, Georgian Techni- MoS monolayers. Devaney-Wolf Theorem on Non-Radiating temperature dependence of the material and inorganic (Ag and CdS) compounds were 2 1 cal Univ., Inst. of Cybernetics, Georgia. A new Sources, Giuseppe Labate , Ladislau Mateko- constant – parameter ξ of CaF2, BaF2 and studied. The effect of Ag nanoparticles influence 1 1 pattern recognition method is suggested based JTh2A.80 vits ; Politecnico di Torino, Italy. Starting SrF2 crystals in range (80 – 300) °K at wavelength on molecular structuring and on luminescence on determining the parameters of the integral 3D Printed Long Period Grating Filters, Vic- from Devaney-Wolf theorem on non-radiating 1070 nm was measured, also, Euler angles intensity of quantum dots was found. polarization ellipse at the Fraunhofer diffraction tor Lambin Iezzi1, Jean-Sébastien Boisvert1, sources, a general theory for invisible structures of «zero depolarization» orientation were of nonactinic circularly polarized light on the 1 1 1 is presented, compactly deriving non-scattering determined. JTh2A.92

Thursday, 20 October Thursday, Sébastien Loranger , Raman Kashyap ; Poly- photoanisotropic copy of the object image. technique Montreal, Canada. We have created devices based on Directional Invisibility, Tailoring Accelerating Beams with Wigner 1 affordable tunable optical fiber filters using 3D Plasmonic Cloaking, Mantle Cloaking and JTh2A.88 Distribution Function, Yuanhui Wen , Yujie 1 1 1 printed periodic structures acting as long fiber Anapole modes. Ultrafast intramolecular charge transfer Chen , Guoxuan Zhu , Yanfeng Zhang , Hui 1 1 1 period grating. dynamics in low band gap Isoindigo based co- Chen , Siyuan Yu ; Sun Yat-sen Univ., USA. We JTh2A.84 polymers, Newayemedhin A. Tegegne1; 1Univ. proposed a Wigner distribution function to Raman - EDS Coupling for identification of of Stellenbosch, South Africa. Ultrafast Charge construct accelerating beams along both 2D and unknown substances in Archaeology applied transfer dynamics of a low band gap copolymer 3D curves. We unify previous caustic methods in to the Turin Shroud, Jean-Pierre Laude1; 1Laude in solution was studied by fs-transient absorp- real space and Fourier space, and also introduce Consulting, France. Coupled Raman and tion spectroscopy. Intramolecular charge a class of 3D caustics. Energy Dispersive Spectra show a substance transfer characteristics (ICT) were observed. fully compatible with oxidative ring cleavage The intersystem conversion time to ICT state products of the heme of blood, namely was 13ps. biliverdin-derived compounds. A weak line is tentatively attributed to amide I of proteins.

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JTh2A • Joint Poster Session II—Continued JTh2A.93 JTh2A.97 JTh2A.101 JTh2A.105 JTh2A.110 Enhanced modulation of spontaneous emis- Ultra-Realistic Imaging and OptoClon- ArF Excimer Laser Filamentation Induced Sub-100 fs All-PM Er-doped Soliton Mode- On the performance of β-BaB2O4 and BiB3O6 sion via gap plasmon with low index metama- esTM, Hans I. Bjelkhagen1, Alkiviadis Lembes- Damage in Fused Silica, Haibo Zhang1, Zhijun Locked Fiber Oscillator Based on Graphene as an intra-cavity frequency-doubling element terials and liquid crystals, He Hao1, Ying Gu1, sis2, Andreas Sarakinos2; 1CURI, Glyndwr Univ., Yuan1, Ren Ye1, Jun Zhou1; 1Shanghai Inst of Saturable Absorber, Jaroslaw Z. Sotor1, in optical parametric oscillators, Mukesh K. Juanjuan Ren1, Hongyi Chen1, Iam C. Khoo2, UK; 2Hellenic Inst. of Holography, Greece. CW Optics and Fine Mech, China. Filamentation Grzegorz Sobon1, Aleksandra Przewolka2, Alek- Shukla1, Partha Maji1, Ritwick Das1;1National Qihuang Gong1; 1Peking Univ., China; 2Pennsyl- RGB lasers, nano-size SH recording materials induced damage in the fused silica excited by sandra Krajewska2, Iwona Pasternak2, Wlodek Inst of Sci Education & Res., India. We vania State Univ., USA. We theoretically dem- and special RGB LED lights for recording and nanosecond DUV laser pulses with microscope Strupinski2, Krzysztof Abramski1; 1Politechnika report a comparison on the performance of 2 onstrate an active modulation of spontaneous displaying Denisyuk color holograms (Opto- objective lens are demonstrated. The evaluation Wroclawska, Poland; Inst. of Electronic Ma- β-BaB2O4 and BiB3O6 as intra-cavity second- emission in LC-metal-LIM structure. With gap ClonesTM) are described. Mobile equipment of damage growth and that of mitigation on terials Technology, Poland. We demonstrate harmonic-generation of single-frequency, plasmon, the spontaneous emission rate can at the museum was used to record the famous fused silica are investigated. a self-starting Er-doped mode-locked fiber high-power visible radiation in singly-resonant be modulated from 105γ0 to 5741γ0. Fabergé Eggs. laser generating soliton pulses with: duration, MgO-doped periodically-poled LiNbO3 based JTh2A.102 repetition frequency and output power of 95 fs, optical-parametric-oscillator. JTh2A.94 JTh2A.98 Realization of a superluminal Raman laser 99.6 MHz, 8 mW, respectively. As a saturable liquid crystal-tuned spontaneous emission Enhancing THz radiation from two-color using adjacent transitions in two isotopes of absorber a PMMA/graphene composite was JTh2A.111 via plasmon waveguide cladded with low laser-induced air-plasma by using abruptly Rb, Zifan Zhou1, Joshua Yablon1, Selim Shah- used. Mobius Polarization in Non-collinear Poincare- index metamaterials, He Hao1, Ying Gu1, autofocusing beams, Kang Liu1, Anastasios riar1,2; 1Electrical Engineering and Computer beam Superpositions, Enrique J. Galvez1, Juanjuan Ren1, Hongyi Chen1, Iam C. Khoo2, D. Koulouklidis2,3, Dimitrios G. Papazoglou2,3, Science, Northwestern Univ., USA; 2Physics and JTh2A.106 Kory Beach1, Jonathan J. Zeosky1, Ishir Dutta1, Qihuang Gong1; 1Peking Univ., China; 2Penn- Stelios Tzortzakis2,3, Xi-Cheng Zhang1; 1The Astronomy, Northwestern Univ., USA. We show Withdrawn. Joshua A. Jones1, Behzad Khajavi1,2;1Colgate sylvania state Univ., USA. Using the liquid Inst. of Optics, Univ. of Rochester, USA; 2Inst. how to realize a superluminal Raman laser using Univ., USA; 2Physics and Astronomy, Florida crystal-metal-low index metamaterial waveguide of Electronic Structure and Laser, Founda- adjacent transitions in two isotopes of Rb, with JTh2A.107 Atlantic Univ., USA. We investigated the which supports surface plasmon polaritons, we tion for Research and Technology-Hellas, an enhancement in sensitivity due to change A Self-Consistent Method for the Deter- noncollinear superposition of optical beams theoretically demonstrate an active modulation Greece; 3Department of Material Science and in cavity length by a factor of nearly a million. mination of the Complex Refractive Index bearing optical vortices in orthogonal states of of spontaneous emission. It can be modulated Technology, Univ. of Crete, Greece. By using of Arbitrary Absorptance Thin Films, Serge circular polarization. Projective measurements from 131γ0 to 327γ0 by varying optical axis. abruptly autofocusing beams, as opposed to JTh2A.103 Gauvin1, Jean Desforges1; 1Université de Monc- are consistent with the polarization ellipse the conventional Gaussian beams, to generate Universality of optical-field-induced semimet- ton, Canada. A self-consistent formalism that describing Mobius loops in 3 dimensions. 1,2 JTh2A.95 plasma in the ambient air, an enhancement of allization in dielectrics, Ojoon Kwon , Vadym accurately gives the complex index of arbitrary Thursday, 20 October Designed and Developed Low Cost Raman the terahertz radiation from the plasma in the Apalkov3, Mark Stockman3, D. Kim1,2; 1De- absorptance thin films, on an arbitrary substrate, JTh2A.112 Spectroscopic System, Andrew Huzortey1, low frequency region is observed. partment of Physics, Center for Attosecond is described. This method only requires a Dual-wavelength, dual-comb fiber laser Benjamin Anderson1, Alfred Owusu1; 1Laser and Science and Technology, POSTECH, Ko- single transmittance curve. The only source of based on a nearly-adiabatic fiber-taper Fibre Optics Centre, College of Agriculture and JTh2A.99 E-Poster rea; 2Max Planck Center for Attosecond Sci- uncertainty is experimental. filter, Jie Chen1, Tianlei Zhang1, Ruliu Wang1, 1 1 1 Natural Sciences, Univ. of Cape Coast, Ghana. A Optical Properties of MoS2 / ence, Max Planck POSTECH/Korea Res. Init., Guoqing Hu , Xin Zhao , Jiansheng Liu , Zheng 1 3 1,2 1 simple Raman setup which offers a cost-efficient MoSe2 Heterostructures, Tianren Fan , Ali Korea; Center for Nano-Optics and Depart- JTh2A.108 Zheng ; School of Electronic and Information alternative to a commercial Raman system has Eftekhar1, Hossein Taghinejad1, Pulickel Ajay- ment of Physics and Astronomy, Georgia State Freestyle laser traps as a perfect tool for Engineering, Beihang Univ., China; 2Collabora- been developed. The results obtained from the an2, Ali Adibi1; 1Georgia Inst. of Technol- Univ., USA. The transition of dielectrics into all-optical transport of small particles, Jose tive Innovation Center of Geospatial Technol- 2 1 1 1 analysis showed good correlation with literature. ogy, USA; Rice Univ., USA. We present MoS2/ semimetallic states by light field is studied. A. Rodrigo , Tatiana Alieva ; Universidad ogy, China. A simple, turn-key dual-comb laser

MoSe2 heterostructures formed through Despite distinction among substances, the Complutense de Madrid, Spain. We introduce is realized by leveraging a fiber-taper filter JTh2A.96 dry transfer method. We report significant generality of semimetallization is observed, the freestyle 3D laser traps which are strongly based on multi-mode interference. The low Enhancement in Energy of THz Emission From quenching of the photoluminescence in agreeing with theoretical prediction, taking focused curved beams of arbitrary form with modulation depth of the filter with a nearly

Gas Plasma Induced By Two-Color Chirped MoS2 and a red shift of the photoluminescence intraband transition into account. independent phase control. This tool paves the adiabetic profile improves the bandwidth of the 1 2 Laser Pulses, Vera A. Andreeva , Tie-Jun Wang , in MoSe2 as signs of interlayer charge transfer. way for simultaneous all-optical trapping and generated pulses. Nikolay A. Panov1, Daniil E. Shipilo1, Mikhail N. This presentation will be presented as an JTh2A.104 E-Poster transport of small particles along 3D trajectories. Esaulkov3, Aleksander P. Shkurinov1,3, Vladimir E-Poster on Screen 5 from 09:30–10:15 The phase structure evolution of singular JTh2A.113 A. Makarov1, Ruxin Li2, Olga G. Kosareva1, beams spreading in uniaxial crystal, Bohdan JTh2A.109 Formation and Application of highly-regular See Leang Chin4; 1M. V. Lomonosov Moscow JTh2A.100 V. Sokolenko1; 1V I Vernadsky Crimean Federal Hydrophobic Surface Production by Laser LIPSS on Surface of Silicon Crystals, Iaro- State Univ., Russian Federation; 2Shanghai Luminescent Properties of Nd3+/Cr3+-doped Univ, Russian Federation. A process of coherent Ablation on Titanium Alloy, Ivan Kam2,1, slav Gnilitskyi1, Leonardo Orazi1, Nadezhda 2 1 2 3 1 Inst. of Optics and Fine Mechanics, Chinese LiCaAlF6 Flower-like Microcrystals, Xiaojie optical vortex beams propagation and their Jonas Jakutis Neto ; Universidade Federal de Bulgakova , Vitaly Gruzdev ; UNIMORE, Academy of Sciences, China; 3Inst. on Laser Xue1, Tonglei Cheng1, Takenobu Suzuki1, transformation in anisotropic media is studied. São Paulo, Brazil; 2Departamento de Ciência e Italy;2HiLASE Centre, Inst. of Physics ASCR, and Information Technologies of the Russian Yasutake Ohishi1; 1Toyota Technological Inst., Structural disturbance of phase and intensity Tecnologia da Aeronáutica, Instituto de Estudos Czech Republic; 3Department of Mechanical Academy of Sciencies (ILIT RAS), Russian Fed- Japan. Under the excitation of a 650 nm laser, distribution in anisotropic media is implemented Avançados (IEAv), Brazil. The present work & Aerospace Engineering, Univ. of Missouri, 4 3+ 3+ eration; Centre d’Optique, Photonique et Laser the Nd /Cr -doped LiCaAlF6 flower-like by shift at the beam polarization states. studies the production of super hydrophobic USA. Femtosecond laser pulses of sub-MHz (COPL), Université Laval, Canada. Enhancement microcrystals showed an intense near-infrared This presentation will be presented as an surfaces with laser ablation on Ti6Al4V. After a repetition rate induce highly regular periodic in THz emission energy is observed both emission at 1045 nm attributed to sufficient E-Poster on Screen 1 from 10:15–11:00 few hours of low pressure exposure, the textured surface structures on silicon by combining experimentally and theoretically by creating energy transfer from Cr3+ to Nd3+. surface showed a contact angle above 150°. electron emission and ultrafast heating. They gas plasma with two-color (800nm+400nm) are favorable for photovoltaic, optoelectronic, chirped laser pulses. THz yield increases when and biomedical applications. laser pulse is chirped positively.

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JTh2A • Joint Poster Session II—Continued JTh2A.114 JTh2A.117 JTh2A.123 JTh2A.127 JTh2A.130 Aluminum nitride microring resonator for Femtosecond optical tweezers as sensitive na- Optical Study of Dual-width Plasmon- Detection of Organic Matter in Simulant FRET-Modulated Cell Lasers, Qiushu Chen1, efficient frequency comb doubling, Hojoong no-thermometer, Dipankar Mondal1, Debabrata ic Nanogap Gratings for Biosensor Ap- Martian Soil using Plasmonic-Biosilica SERS Michael Ritt2, Biming Wu1, Rhima Coleman1, Jung1, Xiang Guo1, Na Zhu1, Scott Papp2, Scott Goswami1; 1Indian Inst. of Technology, Kanpur, plications, Stephen Bauman1, Ahmad A. Substrate, Kenneth Squire1, Xianming Kong1, Sivaraj Sivaramakrishnan2, Xudong Fan1; 1Bio- Diddams2, Hong Tang1; 1Yale Univ., USA; 2NIST, India. Nanovolume temperature around optical Darweesh1, David A. French2, Joseph B. Paul Leduff1, Gregory Rorrer1, Suning Tang2, medical Engineering, Univ. of Michigan, USA. We demonstrate efficient frequency-comb trap is measured by exploiting nonradiative Herzog2,1;1Microelectronics & Photonics, Bin Chen3, Christopher McKay3, Rafael Navarro- USA; 2Genetics, Cell Biology, and Development, doubling of input IR mode locked fiber comb relaxation in solvents. Copropagating 1560nm Univ. of Arkansas, USA; 2Physics, Univ. of Gonzalez4, Alan X. Wang1; 1Oregon State Univ. of Minnesota, USA. Lasing from living cells with a high-Q phase matched AlN microring femtosecond laser pulses change solvent Arkansas, USA. Plasmonic grating (1D) and Univ., USA; 2Crystal Research, USA; 3NASA, expressing fluorescent protein FRET pairs were resonator. The sinusoidal phase dependent temperature and viscosity while trap-stiffness grid (2D) structures with two unique widths USA; 4UNAM, Mexico. We fabricate a surface- studied. Experimental results and theoretical interference is well matched with theory. is unaffected during 780nm trapping. and sub-10 nm gaps have been fabricated, enhanced Raman spectroscopy (SERS) substrate analysis showed that difference in FRET energy and electromagnetic simulations and Raman using plasmonic-biosilica diatoms and gold transfer efficiency resulted in distinct cell lasing JTh2A.115 JTh2A.118 spectroscopy results have been performed to nanoparticles to detect organic matter down behavior. Withdrawn. Presentation of OSA student chapter Cam- optimize the geometry for optical enhancement. to part-per-billion levels in soil samples that eroon, Murielle Vanessa Tchakui1; 1Universite simulate conditions of soil on Mars. JTh2A.131 E-Poster JTh2A.116 de Yaounde I, Cameroon. In this poster we JTh2A.124 Optical Coherence Elastography of the Cor- Improving the signal-to-noise ratio of ghost present the OSA student chapter Cameroon. In Vivo Assessment of Molecular Aging by JTh2A.128 nea by Tracking the Propagation of Surface imaging with thermal light background by We focus on its mission and its organigram. Quasi-Elastic Light Scattering in the Human Video-rate volume imaging confocal mi- Acoustic Waves, Jose F. Zvietcovich1, Jianing narrow band optical filtering, Dongyue Yang1, Some outreach and recruitment activities done Lens, Olga V. Minaeva1,2, Srikant Sarangi3,1, Juliet croscope based on wavelength / space Yao 1, Jannick P. Rolland1, Kevin Parker1;1Univ. Junhui Li3, Guohua Wu1, Bin Luo2, Longfei Yin3, recently are also developed. A. Moncaster3,1, Danielle M. Ledoux2,4, Caitlin conversion by use of multichannel spec- of Rochester, USA. We measure the speed of Hong Guo3; 1School of Electronic Engineering, A. Rook2, Frank J. Weng2, John I. Clark5, David trometer, Shuji Miyamoto1, Eiji Hase1,2, Takeo surface acoustic waves propagating in a porcine Beijing Univ. of Posts and Telecommunications, JTh2A.119 G. Hunter2,4, Lee E. Goldstein1,3; 1Boston Univ., Minamikawa1,2, Takeshi Yasui1,2, Hirotsugu cornea using optical coherence tomography China; 2State Key Laboratory of Information Optics Research Activity in LAMSEBP, Murielle USA; 2Boston Children’s Hospital, USA; 3Boston Yamamoto3; 1Tokushima Univ., Japan; 2ERATO since it provides of depth-resolved elastic Photonics and Optical Communications, Bei- Vanessa Tchakui1; 1Universite de Yaounde I, Univ. School of Medicine, USA; 4Harvard Medical Intelligent Optical Synthesizer Project, JST, modulus which is important for the study of jing Univ. of Posts and Telecommunications, Cameroon. In this poster we start by presenting School, USA; 5Univ. of Washington, USA. Quasi- Japan; 3Utsunomiya Univ., Japan.Video-rate ocular diseases and treatments. China; 3State Key Laboratory of Advanced the LAMSEBP group at the Univ. of Yaounde1 elastic light scattering analysis of long-lived volume imaging confocal microscopy em- This presentation will be presented as an Optical Communication Systems and Networks, Cameroonon and the staff members. After that lens proteins provides a practical, noninvasive ploying line-focused confocal microscopy, E-Poster on Screen 1 from 09:30–10:15 School of Electronics Engineering and Com- many topics investigated there in the area of technique and quantitative biomarker for wavelength/1D-space conversion and a PZT puter Science, and Center for Quantum Informa- optics and photonics are given. objective, point-of-care assessment of molecular objective scanner was proposed. The system JTh2A.132 tion Technology, Peking Univ., China. In ghost aging in a human body. enables 1.4 volumes/s (13 slices) with the axial Z-scan technique: A new concept for Diag- imaging with narrow-band pseudo-thermal JTh2A.120 resolution of 8.4 µm. nosis of Prostate Cancer in blood, Camila T. signal embedded in thermal light background, Withdrawn. JTh2A.125 Nabeshima2, Flávia R. Silva3, Antonio M. Neto4, signal-arm narrow band optical filters bring New Trend in Terahertz Medicine, Vyacheslav JTh2A.129 Sarah I. Alves2, Ricardo E. Samad5, Lilia C. Cour- higher value and converging upper limit of the JTh2A.121 I. Fedorov1,2; 1Inst. of Laser Physics RAS, Rus- Galvanometer Scanning for Optical Coher- rol1,2; 1Ciências Exatas e da Terra, Universidade imaging signal-to-noise ratio (SNR). Withdrawn. sian Federation; 2ITMO Univ., Russian Federa- ence Tomography, Virgil-Florin Duma1,2, Pa- Federal de São Paulo, Brazil; 2Departamento tion. Fundamental study of biological effects trice Tankam3, Jinxin Huang3, Jungeun Won3, de Ciências Exatas e da Terra, Universidade JTh2A.122 of terahertz radiation may be the basis for Jannick P. Rolland3; 1Universitatea Aurel Vlaicu Federal de São Paulo, Brazil; 3Centro de Ciência Localization analysis and dimensional scaling therapeutic and diagnostic use of laser terahertz Arad, Romania; 2Doctoral School, Polytechnic e Tecnologia de Materias, Instituo de Pesquisas in a disordered optical waveguide, Behnam radiation in medicine. Examples of application Univ. of Timisoara, Romania; 3The Inst. of Energéticas e Nucleares, Brazil; 4Instituto de Thursday, 20 October Thursday, Abaie1, Arash Mafi1; 1Univ. of New Mexico, for treatment and diagnostics will be presented. Optics, Univ. of Rochester, USA. Galvanometer Física, Universidade de São Paulo, Brazil; 5Cen- USA. Anderson localization properties of a scanning was optimized for maximum duty tro de Lasers e Aplicações, Instituto de Pesqui- disordered optical waveguide are studied using JTh2A.126 cycle and distortion-free mosaic images in sas Energéticas e Nucleares, Brazil. Porphyrin the mode-width probability density function The Nuclear Refractive Index from Quantita- Gabor Domain Optical Coherence Microscopy accumulate substantially more in tumors than (PDF). The scaling and convergence of the tive Phase Imaging: Corrupting Factors and (GD-OCM). Mathematical models for sawtooth in normal tissues. The optical nonlinearity of PDF with the transverse size of the waveguide Application to a/LCI, Zachary A. Steelman1, and triangular scanning were obtained and the blood porphyrin was analyzed using Z-scan is explored. William J. Eldridge1, Han Sang Park1, Adam confirmed experimentally. technique. The results showed a decrease in Wax1; 1Duke Univ., USA. Recent Quantitative nonlinear refractive index value for tumor blood. Phase Microscopy experiments have measured the refractive index of a cell nucleus to be lower than the cytoplasm. We suggest a potential error capable of corrupting these measurements.

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JTh2A • Joint Poster Session II—Continued JTh2A.133 JTh2A.137 JTh2A.141 JTh2A.145 JTh2A.149 High-Speed Stimulated Brillouin Scattering Quantitative Phase Microscopy of Live Cells Optical Simulation of Nonlinear Twisted- An efficiency breakthrough in perovskite Nano-scatter enabled Optical Mapping of Profilometry, Itay Remer1, Lear Cohen1, Alberto Flowing in a Micro-Channel Using Flipping In- Ring Defect States with Planar Waveguide solar cells realized by Al-coated Cu nanopar- Orbital Angular Momentum of Broadband Bilenca1,2; 1Biomedical Engineering Department, terferometry, Natan T. Shaked1, Bahram Javidi2, Arrays, Alexander A. Dovgiy1, Andrey E. ticles, Xi Chen1,2, Min Gu2,1; 1Swinburne Univ. Light, Haoran Ren1, Min Gu2,1; 1Centre for Ben-Gurion Univ. of the Negev, Israel; 2Ilse Nir Turko1, Darina Roithstain1; 1Tel-Aviv Univ., Miroshnichenko1, Alexander Moroz2, Alex- of Technology, Australia; 2RMIT Univ., Austra- Micro-Photonics, Faculty of Science, Engi- Katz Inst. for Nanoscale Science and Technol- Israel; 2Univ. of Connecticut , USA. We present ander Szameit3, Demetrios Christodoulides4, lia. Al-coated Cu nanoparticles with strong light- neering and Technology, Swinburne Univ. of ogy, Ben-Gurion Univ. of the Negev, Israel. We wide-field off-axis interferometry for rapid Andrey A. Sukhorukov1; 1Nonlinear Physics trapping effects were synthesized. An efficiency Technology, Australia; 2Artificial Intelligence show high-speed stimulated Brillouin scattering quantitative phase microscopy of biological Centre, RSPE, Australian National Univ., Aus- boost of 21% in perovskite solar cells has been Nanophotonics Laboratory, School of Science, (SBS) profilometry of layered liquids at 30 ms cells during flow in microfluidic channel, tralia; 2Wave-scattering.com, Germany; 3Inst. demonstrated, which is significantly higher than RMIT Univ., Australia. We demonstrate a nano- pixel-dwell-time – 100-fold faster than current with potential of integration into cell sorting of Applied Physics, Abbe Center of Photon- those from other plasmonic nanostructures. scatter enabled single-path wavefront sensing backward SBS methods. This is a step forward to devices. Various experimental demonstrations ics, Friedrich-Schiller-Universitat Jena, Ger- approach capable of distinguishing of arbitrary rapid SBS profilometry in biomedical mechanics. are presented. many; 4CREOL, The College of Optics and JTh2A.146 integer or fractional topological charges of Photonics, Univ. of Central Florida, USA. We Interactions of two counter-propagating orbital angular momentum of broadband light. JTh2A.134 JTh2A.138 introduce a concept of universal optical waveguides in the dry photopolymer material An achromatic system for multi-wavelength Nanometer-class Optical Coherence To- simulators based on experimentally accessible using fibre optics, Ra’ed A. Malallah1, Inbarasan JTh2A.150 fluorescence lifetime imaging of the lung in mography for In Vivo Tear Film Thickness planar waveguide arrays, where the light Muniraj1, Haoyu Li1, Derek Cassidy1, John T. Numerical modeling of the generation of a intensive care units, Fiona M. Kenny1, Laura Estimation, Jinxin Huang1, Holly B. Hind- evolution exactly replicates nonlinear defect Sheridan1; 1Univ. College Dublin, Ireland. Self- Kerr comb in a coupled cavity system using Young1, Timothy Morris1, Chris Saunter1, John man1, Jannick P. Rolland1; 1Univ. of Rochester, state dynamics governed by topologically Writing optical waveguides (SWWs) have been coupled mode equations, Yusuke Okabe1, M. Girkin1; 1Durham Univ., UK. This work used USA. To advance the Dry Eye management, nontrivial Hamiltonians. demonstrated in the photopolymerizable Takumi Kato1, Shun Fujii1, Ryo Suzuki1, Taka- an endoscopic fiber bundle for lifetime imaging we developed a technique to simultaneously materials. Nonlinearity and diffraction limit sumi Tanabe1; 1Keio Univ., Japan. We show of lung tissue which provided information on estimate the thickness of both the lipid and JTh2A.142 of a propagated wave in nonlinear-materials the modeling of Kerr comb generation in a bacterial infections. The system was designed aqueous layers of the tear film in vivo using Withdrawn. effectively compensated by light diffusion coupled cavity system and perform a numerical with reflective optics to maximise efficiency optical coherence tomography and maximum- during the creation of SWWs. simulation in a normal dispersion regime. We of emission detection and wavelength range. likelihood estimation. JTh2A.143 show the repetition rate is selectable and soliton Vertical Split-Ring Resonator based Meta- JTh2A.147 generation is possible. 1

JTh2A.135 JTh2A.139 surface for Light Manipulation, Mu Ku Chen , High Stability and Higher Poling Efficiency Thursday, 20 October 1 1 1 Multi-Species Coherent Anti-Stokes Raman Withdrawn. Wei-Lun Hsu , Pin Chieh Wu , Jia-Wern Chen , for Electro-Optic Polymer/TiO2 Vertical Slot JTh2A.151 Spectroscopy in Gas-Filled Hollow-Core Ting-Yu Chen1, Wei Ting Chen1, Yao-Wei Waveguide Modulators, Yasufumi Enami1, An Electrostatic Actuated 2-D MEMS Scanner Photonic Crystal Fiber, Robert J. Hupfer1, JTh2A.140 Huang1, Chun Yen Liao1, Greg Sun2, Din Ping Jingdong Luo2, Alex Jen2; 1School of System for Potential Image Display Application, Wei- Barbara M. Trabold1, Amir Abdolvand1, Philip Investigating Corneal Disease Using High Tsai3,1; 1National Taiwan Univ., Taiwan; 2De- Engineering, Kochi Univ. of Technology, Ja- chih Wang1,2, Kebin Gu1; 1Univ. of Washington, S. Russell1; 1Max Planck Inst. for the Science of Resolution Gabor-domain Optical Coherence partment of Engineering, Univ. of Massa- pan; 2Department of Materials Science and USA; 2National Tsinghua Univ., Taiwan. Paper Light, Germany. Coherent anti-Stokes Raman Microscopy, Patrice Tankam1, Zhiguo He2, Gilles chusetts Boston, USA; 3Research Center for Engineering, Univ. of Washington, USA. We presents an electrostatic actuated 2-D cantilever 2 3 4 spectroscopy is conducted on gas-mixtures Thuret , Holly B. Hindman , Thierry Lepine , Applied Sciences, Academia Sinica, Taiwan. We demonstrate stable half wave voltage (Vπ) waveguide scanner. A 2-D scanning motion in kagomé-PCF. Pressure-tunable dispersion Cristina Canavesi5, Philippe Gain2, Jannick P. used e-beam process for the deposition of and electrode length (L) product for a elec- has been successfully demonstrated with two 1,5 1 2 enables broadband phase-matching which, Rolland ; Univ. of Rochester, USA; Faculty of 3D nanostructures called vertical split-ring tro-optic (EO)/TiO2 vertical slot waveguide fundamental resonances found at 202(V) and 3 combined with broadband Stokes seeding, Medicine, Jean Monnet Univ., France; Oph- resonators to explore the functionality of beam modulator. VπL product of 2.5 Vcm for the 536(H) Hz with corresponding FOV of 0.062 allows simultaneous detection of multiple thalmology, Univ. of Rochester Medical Center, steering with phase modulation by tuning only modulators shows the same value for two years. and 0.009 rad. trace gases. USA; 4Institut d’Optique, France; 5LighTop- the vertical dimension. Tech, USA. We demonstrate the capability of JTh2A.148 JTh2A.152 JTh2A.136 Gabor-domain optical coherence microscopy JTh2A.144 Focusing grating coupler for integration Long-Range Higher-Order Surface-Plasmon Optimized Endoscopic Laser Surgery in in identifying key features of the structural Electro-Absorption Modulators Based on Car- of a liquid-crystal spatial light modulator Polaritons, Andreas Norrman1, Tero Setälä1, Colon Tumors, Félix Fanjul-Vélez1, Jose L. modification of the cornea in three diseases rier Depletion in Epsilon-Near-Zero Films, Kai- onto a Si photonic circuit, Takahiro Inaba1, Ari T. Friberg1; 1Univ. of Eastern Finland, Fin- Arce-Diego1; 1TEISA, Univ. of Cantabria, including Fuchs’ endothelial corneal dystrophy, feng Shi1, Peichuan Yin1, Zhaolin Lu1; 1Rochester Ryutaro Eguchi1, Hiroyuki Tsuda1; 1Keio Univ., land. We show how a higher-order metal-slab Spain. Common colonoscopic techniques lattice dystrophy and keratoconus. Inst. of Technology, USA. We report field effect Japan. Focusing grating couplers for integrating mode turns into a strongly confined long-range present disadvantages. Laser surgery, including electro-absorption modulators, made of a thin a liquid-crystal spatial light modulator to Si surface-plasmon polariton in situations where ablation and thermal effects, is analyzed, epsilon-near-zero (ENZ) film sandwiched in a optical circuit were designed, which had the the fundamental long-range mode does not considering several wavelengths, pulse silicon or plasmonic waveguide. The significant total loss of 4.6 dB. exist. durations and irradiances. A short pulse Nd:YAG bias-induced reduction of absorption of the ENZ laser is considered to be optimum. film may promise nanoscale modulators.

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JTh2A • Joint Poster Session II—Continued JTh2A.153 JTh2A.157 JTh2A.161 JTh2A.165 JTh2A.170 Giant circular dichroism enhancement and Adjusting Spectrum of MIM Optical Filters Bent Metal-Clad Waveguides for Fiber-to- Avoided Resonance Crossing and Non- Design and Fabrication of Heterogeneously strong superchiral field in hybrid molecule- by Stub Inclination, Shuhao Wu1, Dingxin Waveguide and 3D Chip-to-Chip Light Cou- Reciprocal Nearly Perfect Absorption in Integrated Planar Triplexer for Optical Net- plasmonic nanostructures, Yi N. Liu1; 1Xiamen Wu1; 1Columbia Univ., USA. We analyze the pling Applications, Zhaolin Lu1, Peichuan Yin1, Plasmonic Nanodisks with Near-field and Far- works, Pallav Kanukuntla1, Ayodeji Kuti1, Geddis Univ., China. We have demonstrated a direct stub inclination on stub-based MIM optical Kaifeng Shi1; 1Rochester Inst. of Technology, field Couplings, Shih-Hui G. Chang1; 1National Demetris1; 1Norfolk State Univ., USA.We report correlation between the strong chirality of the filters. Analytical analysis and simulation results USA. We report efficient fiber-to-waveguide and Cheng Kung Univ., Taiwan. Avoided resonance the design and fabrication of heterogeneously local field and the giant CD response at the show that inclination of stub generally causes a 3D chip-to-chip light coupling devices based crossings in plasmonic nanodisk structures integrated silicon based planar triplexer, using plasmon resonance bands induced by chiral blue shift to the transmission spectrum, while on bent metal-clad waveguides. According to due to near field or far field couplings were a self-assembly integration technique which can molecules in the hot spots. emphasizing certain resonances. our FDTD simulation, the coupling efficiency numerically demonstrated. The observed non- be used in data centers and access networks for is over 80% within a broad range of working reciprocal absorption spectra are well explained short wavelength applications. JTh2A.154 JTh2A.158 wavelengths. by a FSS-Fabry-Perot model. Design of Compact Plasmonic Polarim- Si-ITO solar cells with CdTe quantum JTh2A.171 eter Based on Polarization-Sensitive Nano- dots, Marianna Kovalova1, Serhiy Kondratenko1, JTh2A.162 JTh2A.166 A Linearization Technique in Silicon Modula- Grooves, Kyookeun Lee1, Joonsoo kim1, Vasyl Lendel1; 1Taras Shevchenko National Univ. Dual-Layer Plasmonic Metasurfaces for Thermo-optic oscillatory behavior in on-chip tors for Analog Signal Processing, Lingjun Sang-Eun Mun1, Gun-Yeal Lee1, Byoungho . of Kyiv, Ukraine. We’ve investigated p-Si/ITO Phase-Hologram Generation, Yohan Lee1, lithium-niobate microdisk resonators, Jie Jiang1, Pengfei Wu1, Young H. Kim1, Ste- Lee1; 1Seoul National Univ., USA. A compact with CdTe quantum dots. The J-V characteristics Joonsoo Kim1, Byoungho Lee1; 1Seoul National Wang1, Bowen Zhu2, Zhenzhong Hao1, Fang phen Anderson1, Weimin Zhou2, Zhaoran plasmonic polarimeter is proposed. The was found to be nonlinear. The photocurrent Univ., USA. A dual-layer plasmonic metasurface Bo1, Xiaolei Wang2, Guoquan Zhang1, Jingjun R. Huang1; 1Rensselaer Polytechnic Inst., polarization state of the incident light is spectra in spectral range above band gap of Si which offers effective control of the phase of the Xu1; 1The MOE Key Laboratory of Weak Light USA; 2Sensors &Electron Devices Director- measured using interference between surface is caused by presence of CdTe quantum dots. transmitted wave by simple translational motion Nonlinear Photonics, TEDA Applied Physics Inst. ate, US Army Research Laboratory, USA. We plasmon polaritons, excited by nano-grooves. is proposed. It can operate on phase-mode and School of Physics, Nankai Univ. , China; 2Key investigate a linearization technique in silicon The design method and simulation results will JTh2A.159 and is controlled by adjusting the lateral shift Laboratory of Optical Information Science electro-optic (EO) modulator for spur-free be shown. Radiative lifetime changes in the vicinity of of lower surface. and Technology, Ministry of Education, Inst. dynamic range (SFDR) improvement. Using 3rd- a nanofiber: dielectric, and alignment ef- of Modern Optics,, Nankai Univ. , China. We order derivative of the transfer function, an opti- JTh2A.155 fects, Pablo Solano1, Jeffrey Grover1, Burkley JTh2A.163 report the first experimental observation of an mal DC bias is applied to get a maximum SFDR. 1 1 Eu-doped ZnO-HfO2 hybrid nanocrystals Patterson , Steve L. Rolston , Luis A. Oro- Supercontinuum generation beyond 2µm oscillatory behavior of transmission of on-chip embedded glass-ceramic waveguides as zco1, Yunlu Xu1, Jeremy N. Munday1; 1Univ. of in GeSbS waveguides, Ju Won Choi1, Zhao- lithium-niobate microdisk resonators, which was JTh2A.172 blue-light emitting source, Subhabrata Ghosh1, Maryland at College Park, USA. We measure hong Han2, Byoung-Uk Sohn1, George F. attributed to the competition between a fast Coherent perfect absorption in chiral ma- 1 1 1 2 2,1 1 Shivakiran Bhaktha B. N. ; Indian Inst. of the radiative lifetime of the D2 line of atomic R. Chen , Lionel C. Kimerling , Kathleen A. thermo-optic effect and a slow heat dissipation terials, Yuqian Ye , Darrick Hay , Zhimin 3 2,4 1 1 Technology Kharagpur, India. Eu-doped SiO2- rubidium in the evanescent mode of a nanofiber Richardson , Anuradha M. Agarwal , Dawn T. process. Shi ; Department of Physics, Univ. of South 1 1 2 HfO2-ZnO hybrid glass-ceramic waveguides and find enhancements and suppressions H. Tan ; Engineering Product Development, Florida, USA; Department of Physics, Hangzhou have been fabricated for on-chip blue-light depending on the nanofiber size and the Singapore Univ. of Technology and Design, Sin- JTh2A.167 Normal Univ., China. We derive analytically emitting source application. The reduction of atomic-dipole orientation. gapore; 2Department of Materials Science and Withdrawn. the coherent perfect absorption condition of Eu3+→Eu2+ in the presence of ZnO nanocrystals Engineering, Massachusetts Inst. of Technology, a transversely isotropic chiral structure. We leads to enhanced blue-emission in the low-loss JTh2A.160 USA; 3College of Optics and Photonics, Univ. JTh2A.168 use a THz chiral metamaterial structure to waveguides. Optical Bistability in a VCSEL Connect- of Central Florida, USA; 4Materials Processing A Compact and Highly Sensitive Bio-sensor numerically demonstrate coherent absorption ed Across Serially-Coupled PIN Photo- Center, Massachusetts Inst. of Technology, using Directional Coupling between Metal and polarization control. JTh2A.156 diodes, Sanaz Faryadras1, Azad Siahmak- USA. SPM-induced nonlinear phase shift in Clad Ridge Waveguides, Ranjeet Dwivedi1, High-Q and Small Mode-Volume Oxide- oun1; 1Department of Physics and Optical GeSbS chalcogenide waveguides allows us Arun Kumar1; 1Indian Inst. of Technology, JTh2A.173 Thursday, 20 October Thursday, Cladding Aluminum Nitride Photonic Crystal Engineering, Rose-Hulman Inst. of Technology to extract a nonlinear parameter of ~7 W-1/m. Delhi, India. We propose a compact and highly Nanocoatings of Cerium Oxide and Platinum Nanocavity, Emerson G. Melo1, Marcelo N. , USA. Two serially-coupled PIN-PDs connected Supercontinuum is generated with a 14 fold sensitive bio-sensor based on directional on Black Silicon Substrate for Enhanced Pho- Carreño1, Marco I. Alayo1; 1Univ. of São Paulo, to a VCSEL is theoretically modeled and spectral broadening with respect to the input coupling between two metal under-clad ridge tocurrent Generation, Pabitra Dahal1, Dionísio Brazil. A high bandgap material is very attractive experimentally demonstrated to exhibit optical spectrum, which is close to an octave. waveguides. The sensitivity of the proposed Pereira1, Elangovan Elamurugu1, Jaime P. Vie- in some photonic applications. Therefore, we bistability. The bistable device operates in MHz sensor is found to be 6500 nm/RIU for the gas1; 1Masdar Inst. of Science and Tech, United propose a high-quality-factor and small mode- range mainly due to parasitic inductance and JTh2A.164 ambient RI ~1.33. Arab Emirates. We demonstrate a 32-times volume oxide-cladding AlN photonic crystal capacitance of the circuit. Low-loss and low-crosstalk Si polarization photocurrent improvement on nanolayers of nanocavity and assess the effects of fabrication splitters with two-step etching, shigeaki sakai1, JTh2A.169 platinum and cerium oxide on black silicon induced disorder. Hiroyuki Tsuda1, Naotaka Iwamoto 1; 1Keio Mid-Infrared TE-pass and TM-pass polar- due to the combined plasmonic effect with Univ., Japan. The waveguide-type three-line izer based on Silicon on Sapphire (SOS) the multiple pathway photon scattering events Si polarization splitter is designed and it has a waveguide, Raghi El Shamy1, Hany Mossad1, leading to significant absorption improvement. polarization extinction ratio of more than 40dB Mohamed Swillam1; 1The American Univ. in and a loss of less than 0.4 dB for the wavelength Cairo, USA. An easy to fabricate, wideband range from 1.45µm to 1.65µm. and compact silicon-based TE-pass and TM- pass integrated MIR polarizers are proposed. The polarizers covers the whole mid-infrared transparency region of the SOS waveguide.

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JTh2A • Joint Poster Session II—Continued JTh2A.174 JTh2A.179 JTh2A.183 JTh2A.187 JTh2A.191 Optically reconfigurable chirp in micro/nano- Nonlinear Waveguides Based on III-V Semi- In-Vivo Three-Photon Excited Fluorescence Simultaneous CW three laser wavelengths Theoretical Analysis of Temperature Char- fiber Bragg gratings, Wei Luo1, Fei Xu1, Yan- conductors, Shayan Saeidi1, Kashif M. Awan1, Imaging in the Spinal Cord of Awake, Lo- generation using precise gain control by acteristics of Coupled Quantum Dot La- qing Lu1; 1Nanjing Univ., China. We theoretically Lilian Sirbu1, Ksenia Dolgaleva1; 1Univ. of Ot- comoting Mouse, Yu-Ting Cheng1, SallyAnne VBGs , Ching-Nien Chen1, Yu-Hua Hsieh1, sers, Zhiyuan Lin1, Guohui Yuan1, Zhuoran demonstrate the optomechanical effect of tawa, Canada. We propose nonlinear integrated L. Ness2, Sofia H. Hu3, Jared Raikin3, Lillyan D. Te-Yuan Chung1; 1National Central Univ., Tai- Wang1; 1UESTC, China. Spectra of coupled optically reconfigurable chirp in silica micro/ waveguide designs based on semiconductors Pan3, Tianyu Wang4, Dimitre G. Ouzounov4, wan. Three wavelength operation of a diode quantum dot lasers at different temperatures nano-fiber Bragg gratings. The fiber grating not widely used for nonlinear photonics previ- Jean C. Cruz-Hernandez3, Isle M. Bastille3, pumped Nd-based laser was constructed are calculated using a probabilistically coupled devices utilizing the optically reconfigurable ously. The materials belong to the group III-V Nozomi Nishimura3, Joseph R. Fetcho1, Chris using three volume Bragg gratings (VBGs) as model. Calculated results show that the spectra chirp may offer a means for all-optical. and are expected to demonstrate interesting Xu4, Chris B. Schaffer3; 1Neurobiology and the output couplers. By precisely controlling at low temperatures are much flatter than the nonlinear optical properties. Behavior, Cornell Univ., USA; 2Veterinary the temperatures of the VBGs, the laser output ones at high temperatures. JTh2A.175 Medicine, Cornell Univ., USA; 3Meinig School of wavelengths and power are stable. Withdrawn. JTh2A.180 Biomedical Engineering, Cornell, USA; 4School JTh2A.192 Elastic Scattering from a Sapphire Micro- of Applied and Engineering Physics, Cornell JTh2A.188 Nanosecond passively mode-locked laser JTh2A.176 sphere in the THz Region, Syed Sultan Shah Univ. , USA. We constructed a system for in-vivo Superfluid in helical container as a sensor of with a hundred megahertz spectral band- Self-Assembled Plasmonic Core-Shell Clusters Bukhari1, Muhammad Rehan Chaudhry1, three-photon deep imaging in the spinal cord of metric disturbances, Alex Okulov1; 1Russian width, Michael Kues1, Christian Reimer1, for Infrared Resonators, Kan Yao1, Yong- Mustafa Mert Bayer1, Ali Serpengüzel1; 1KOC awake, locomoting mice that facilitates detailed Academy of Sciences, Russian Federation. The Benjamin Wetzel1,2, Piotr Roztocki1, Brent min Liu1; 1Northeastern Univ., USA. Infrared Univ., Turkey. We analyze numerically TE and studies of neural firing patterns correlated with quantum fluid in double-helix pipe is analyzed in Little3, Sai T. Chu4, David J. Moss5, Roberto resonators are key building blocks of optical TM polarization 0° transmission and 90° elastic rhythmic locomotion. accelerated reference frame. The slow Morandotti1,6; 1INRS-EMT, Canada; 2School of devices for widespread applications. We show scattering from a sapphire microsphere with a rotations and small modulations of free-fall ac- Mathematical and Physical Sciences, Univ. of that self-assembled core-shells exhibit unique radius of 2000 µm in terahertz region from 790 JTh2A.184 celeration are taken into account. Sussex, UK; 3Xi’an Inst. of Optics and Preci- spectral features determined by the number, µm to 850 µm by utilizing generalized Lorenz- Challenges in appearance characterization sion Mechanics, Chinese Academy of Science, configuration, and dielectric properties of the Mie theory. of coatings with effect pigments, Alejandro JTh2A.189 China; 4Department of Physics and Materi- particles. Ferrero1, Joaquin Campos1; 1CSIC, Spain. New Characterization of C-band SOA-based als Science, City Univ. of Hong Kong, Hong JTh2A.181 methods to characterize coatings with effect bidirectional tunable fiber laser with two Kong; 5Center for Micro-Photonics, Swinburne JTh2A.177 In Vitro Neuronal Depolarization And In- pigments are necessary to quantify their nested fiber ring cavities, Simeon Bikorimana1, Univ. of Technology, Australia; 6Inst. of Funda- 2 Right-Angle Bends and Splitters for Inter- creased Synaptic Activity Induced By Infrared complex appearance. A description of the Muhammad A. Ummy , Nicholas Madamopou- mental and Frontier Sciences, Univ. of Electronic Thursday, 20 October layer Optical Links of Transverse Electric Neural Stimulation, Blake Entwisle1, Simon challenges faced by their characterization is los1, Roger Dorsinville1; 1Electrical Engineer- Science and Technology of China, China. We Waves, Peichuan Yin1, Kaifeng Shi1, Zhaolin McMullan1, Phillip Bokiniec1, Simon Gross1, given in this contribution. ing, CUNY City College, USA; 2Electrical & demonstrate a passively mode-locked laser Lu1; 1Rochester Inst. of Technology, USA. We Roger Chung1, Michael Withford1; 1Macquarie Telecommunications Engineering Technology, emitting 4.3 nanosecond quasi-Fourier-limited demonstrate the implementation of Metal- Univ., Australia. Neural responses to infrared JTh2A.185 New York City College of Technology, USA. We pulses with a record low (104.9 MHz) spectral Dielectric-Metal structures to design wavelength laser stimulation are explored in single cells. We Optical Fiber based Methods for Deep report a simple, stable, inexpensive SOA-based bandwidth, based on simultaneous filtering size H-plane waveguide bends and power examined synaptic events of Sprague-Dawley Brain Calcium Signal Measurements in Be- bidirectional tunable fiber laser, which consists and cavity-enhanced nonlinear interactions in splitters for TE modes. These designs can be rat neurons, stimulated using an 1890 nm laser. having Mice, Ling Fu1; 1Wuhan National Lab of three SOAs and two nested fiber ring cavities. an on-chip microcavity. implemented as layer-to-layer links or sharp We show that infrared radiation increased for Optoelectronics, China. The traditional A beam combining gain of more than + 4.77 dB bends in the same layer. spontaneous synaptic event frequency. optical systems are not suitable for recording is demonstrated. JTh2A.193 of neuronal activity. Here a multichannel fiber Multiplexing and Amplification of 2 μm Vor- JTh2A.178 JTh2A.182 photometry and a GRIN lens based confocal JTh2A.190 tex Beams, Yuan Li1, Wenzhe Li1, Keith Miller1, Estimation and Compensation of Coupling Simulation of Vision Corrected by the Light microscope are developed to acquire calcium Spatio-temporal dynamics of broad-area semi- Eric G. Johnson1; 1Clemson Univ., USA. The Loss between Bend and Straight Silicon Sword Lens., Karol Kakarenko1, Krzysztof signals in deep brain of behaving mice. conductor lasers, Stefan Bittner1, Brandon Red- multiplexing and amplification of optical Waveguides, Vikash Kumar1, Nishit Malviya1, Petelczyc1, Andrzej Kolodziejczyk1, Zbigniew ding1, Hui Cao1, Daehwan Jung1, Minjoo Larry vortices with orbital angular momentum (OAM) Vishnu Priye1; 1Indian School of Mines, Dhan- Jaroszewicz2,3, Alejandro Mira-Agudelo4, John JTh2A.186 Lee1; 1Yale Univ., USA. We study experimentally is demonstrated in a Ho:YAG rod amplifier. The bad, India. To optimize space utilization in Fredy Barrera 4, Rodrigo Henao4; 1Warsaw Univ. Age- and Glaucoma-Related Changes in the spatio-temporal dynamics of broad-area phase of the amplified vortex is also studied and interconnects of Photonic Integrated Circuits, of Technology Faculty of Physics, Poland; 2Inst. Corneal Deformation Dynamics Utilizing semiconductor lasers. Fast random and periodic proven to be well maintained. estimation and compensation of coupling of Applied Optics, Poland; 3National Inst. of Scheimpflug Imaging, Marta E. Musial1; 1De- oscillations of the laser emission are observed. loss between junction of straight and bend Telecommunications, Poland;4Grupo de Óptica partment of Biomedical Engineering, Wroclaw Their dependence on the pump strength and JTh2A.194 waveguide using Multiple Scaling Method y Fotónica, Instituto de Física, Colombia. The Univ. of Science and Technology, Poland. Our cavity size are investigated. Theoretical analysis on fast saturable-ab- having great effect on the data transceiver. monofocal vision corrected by LSL provide a experimental and statistical research have sorber effects in a mode-locked laser with homogenous performance in a wide range shown that high speed Scheimpflug imaging an intra-cavity nonlinear medium, Toru Sato1, of defocus. We show the simulated visual is a potential tool to determine and register Sakae Kawato1; 1Fukui Univ., Japan. We analyzed performance by means of objective and changes in corneal biomechanics associated fast saturable-absorber effects in a mode-locked subjective assessment of images created in with age and glaucoma occurrence. laser with an intra-cavity highly nonlinear optical system emulating the human eye. medium. The nonlinear effects were required to obtain shorter output pulse widths below the Fourier-transform-limit of the gain spectra.

FiO/LS 2016 • 16–21 October 2016 95 Empire Hall

JOINT FiO/LS

JTh2A • Joint Poster Session II—Continued

JTh2A.195 JTh2A.196 JTh2A.197 JTh2A.198 E-Poster Theoretical Investigation of Laser-diode- Spectral selectivity in capillary dye la- Withdrawn. Surface Profilometry Using Vortex Beams, Ale- 1 1 pumped High Efficiency CW Ti:sapphire sers, Esmaeil Mobini , Behnam Abaie , Arash jandra Serrano1, Jan L. Chaloupka2, Matthw 1 1 1 1 Laser, Motoki Morioka ; Fukui Univ., Japan. The Mafi ; Univ. of New Mexico, USA. The free ANderson3; 1Universidad Autónoma de Baja efficiency of laser-diode-pumped cw Ti:sapphire spectral range (FSR) of the spectral features in California, Mexico; 2Physics, Univ. of Northern laser was investigated theoretically. The optical a fluidic capillary dye laser appears considerably Colorado, USA; 3Physics, San Diego State Univ., to optical conversion efficiency was obtained to larger than what is expected from a Fabry-Perot USA. We explore the use of scanning vortex be higher than 19%. cavity analysis. We theoretically explain the beams to reveal the surface profile of sub- reason behind this phenomenon. micron scale topological features. It is shown that a 200 nm step is easily discernible using this technique. This presentation will be presented as an E-Poster on Screen 2 from 09:30–10:15

11:00–12:30 JTh3A • Light the Future Speaker Series featuring Michio Kaku, Lilac Ballroom

12:30–14:00 Free Lunch (provided by OSA), Exhibit Hall, Empire Hall

12:30–14:00 VIP Industry Leaders Networking Event: Connecting Corporate Executives, Young Professionals & Students, Hyatt Regency Rochester, Grand Ballroom B-C

Thursday, 20 October Thursday,  Thank you for attending FiO/LS. Look for your post-conference survey via email and let us know your thoughts on the program.

96 FiO/LS 2016 • 16–21 October 2016 NOTES ______Thursday, 20 October ______

FiO/LS 2016 • 16–21 October 2016 97 Grand Ballroom A (Radisson) Grand Ballroom B (Radisson) Grand Ballroom C (Radisson) Grand Ballroom D (Radisson)

FiO

14:00–16:00 14:00–16:00 14:00–16:00 14:00–16:00 FTh4A • Symposium on Mid-Infrared Fiber FTh4B • Optical Vortices FTh4C • Computational Imaging I FTh4D • Optics Meets Neuroscience I Sources I Presider: Carlos Lopez Mariscal, Underwater Presider: Marc Christensen, SMU, USA Presider: Elizabeth Hillman, Columbia Univ., Presider: Morten Ibsen; Univ. of Photonics, Mexico USA Southampton, UK

FTh4A.1 • 14:00 Invited FTh4B.1 • 14:00 Tutorial FTh4C.1 • 14:00 Invited FTh4D.1 • 14:00 Invited Highly Nonlinear Fibre for Applications in the Mid-IR, Bran- Spinning Light on the Nanoscale, Natalia M. Litchinitser1, Nanoparticle and Virus Sensing Enabled by Computa- Multi Scale Morpho-functional Characterization of Damage don Shaw1; 1US Naval Research Laboratory, USA. Highly Jingbo Sun1, Mikhail Shalaev1; 1State Univ. of New York at tional Lensfree Imaging, Euan McLeod1; 1Optical Sciences, and Rehabilitation after Stroke, Francesco S. Pavone1; 1Eu- nonlinear fibre for applications in the Mid-IR are explored. Buffalo, USA. We discuss fundamental optical phenomena at Univ. of Arizona, USA. More than 105 individual viruses and ropean Lab for Non-Linear Spectroscopy, Italy. Here we use a the interface of singular and nonlinear optics in engineered nanoparticles <40 nm are detected using on-chip digital multi-level approach to investigate complementary aspects optical media and show that the unique optical properties of lensfree holography. The weak scattered waves from these of brain plasticity after stroke. metamaterials and metasurfaces open unlimited prospects objects are enhanced by self-assembled liquid polymer to “engineer” light itself. nanolenses that boost signal-to-noise ratio.

FTh4A.2 • 14:30 Invited FTh4C.2 • 14:30 FTh4D.2 • 14:30 Invited Generation and Applications of High Average Power Improvement of experimental methods for studying Chemical Sectioning: High Throughput Imaging Brain 1 Mid-IR Supercontinuum in Chalcogenide Fibres, Christian dust plasma and colloidal systems, Nikita P. Kryuchkov , Networks ex vivo at Synaptic Resolution, Shaoqun 1 1 1 Rosenberg Petersen1; 1Denmark. Mid-infrared supercon- Anatoly Kislov , Egor Yakovlev , Kirill Zaytsev , Stanislav Zeng1,2; 1Huazhong Univ of Science & Technology, Chi- 1 1 tinuum with up to 54.8 mW average power, and maximum Yurchenko ; Bauman Moscow State Technical Univ., Russian na; 2Biomedcial Potonics, Wuhan National Lab for Optoelec- bandwidth of 1.77-8.66 μm is demonstrated as a result of Federation. Software package for real-time post-processing tronics, China. We present Chemical Sectioning (CS) method pumping tapered chalcogenide photonic crystal fibers with of the dusty plasma systems experiments is designed. This to systematically reconstruct the integral morphology of a a MHz parametric source at 4 μm. Biography: Natalia Litchinitser is a Professor of Electrical package able to perform automatic particle tracking on the neuron. This method will pave the way towards single cell pro- Engineering at University at Buffalo, The State University of video stream from the experimental station and calculate jectome, and other studies involving neuronal organization. New York. Her research focuses on fundamental properties different parameters. and applications structured light in engineered nanosctruc- tures, biomedical imaging, optical communications and nonlinear optics. She previously held a position of a Member

Thursday, 20 October Thursday, of Technical Staff at Bell Laboratories, Lucent Technologies and of a Senior Member of Technical Staff at Tyco Submarine Systems. She authored 7 invited book chapters and over 150 research papers. She is a Fellow of the Optical Society of America, Fellow of the American Physical Society, and a Senior Member of the IEEE.

Join the conversation. Follow @Opticalsociety on Twitter. Use hashtag #FIO16 and #OSA100

98 FiO/LS 2016 • 16–21 October 2016 Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E

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14:00–16:00 14:00–16:00 14:00–16:00 14:00–16:00 14:00–16:00 FTh4E • High-Capacity Optical FTh4F • Quantum Communication FTh4G • Integrated Nonlinear FTh4H • Probing Ocular FTh4I • Symposium on 100 Years Communications and Data and Networking I Optics I Biomechanics with Imaging of Vision at OSA: Most Cited Centers I Presider: Natalia Litchinitser; State Presider: Stefan Preble; Rochester Techniques / Novel Applications Vision Papers in OSA Journals Presider: Fernando Guiomar; Univ. of New York at Buffalo, USA Inst. of Technology, USA of Femtosecond Lasers in Presider: Susana Marcos, Consejo Politecnico di Torino, Italy Ophthalmology Sup Investigaciones Cientificas, Presider: Andy Yun, Harvard Spain and Scott Carney, Univ. of Medical School, USA Illinois at Urbana-Champaign, USA

FTh4E.1 • 14:00 Invited FTh4F.1 • 14:00 Invited FTh4G.1 • 14:00 Invited FTh4H.1 • 14:00 Invited FTh4I.1 • 14:00 Invited Advanced Techniques for Digital Nonlin- Quantum Teleportation across the Calgary An Unspoofable Ultrafast Silicon Pho- Air-puff Swept-Source Optical Coherence Emerging Ocular Applications of Wavefront ear Compensation in Multi-carrier Optical Fibre Network, Wolfgang Tittel1, Raju Val- tonic Physical Key, Mark A. Foster1; 1Johns Tomography, Maciej Wojtkowski1,2, Ewa Correction, David R. Williams1; 1Univ. of Roch- Transmission Systems, Fernando Guio- ivarthi1, Marcel.li Grimau Puigibert1, Qiang Hopkins Univ., USA. Physical keys store Mączyńska1, Bartłomiej Kałużny3, Ireneusz ester, USA. The correction of the eye›s wave mar1; 1Politecnico di Torino, Italy. High-capacity Zhou1, Gabriel Aguilar1, Daniel Oblak1, Varun secret information in their structure. Here we Grulkowski1; 1Nicolaus Copernicus Univ., Inst. of aberration is enabling advances ranging from optical communications are currently evolving Verma2, Francesco Marsili3, Matthew Shaw3, demonstrate an unclonable key based on a Physics, Poland; 2Polish Academy of Sciences, laser refractive surgery without removing tissue towards multi-carrier transmission. We review Sae Woo Nam2; 1Univ. of Calgary, Cana- nonlinear reverberant silicon photonic micro- Inst. of Physical Chemistry, Poland; 3Nicolaus to retinal imaging tools capable of capturing the new challenges and opportunities for da; 2NIST, USA; 3JPL, USA. We report quantum cavity. Beyond cloning this key also cannot be Copernicus Unive., Collegium Medicum, Po- retinal function at a cellular spatial scale. digital nonlinear mitigation in these systems, teleportation between telecom and 795 nm emulated due to its ultrafast response. land. We studied the response of porcine eyes optimizing the performance versus complexity photons. This improves the distance over which to air pulse at well-controlled levels of intraocu- trade-off. teleportation takes place from 818 m to 6.2 km lar pressure (IOP) using air-puff OCT instrument. and constitutes a milestone towards a global We observed significant changes of hysteresis quantum internet. after cross-linking for higher levels of IOP.

FTh4E.2 • 14:30 FTh4G.2 • 14:30

FTh4F.2 • 14:30 Invited FTh4H.2 • 14:30 Invited FTh4I.2 • 14:30 Invited Thursday, 20 October Diffractive Orbital Angular Momentum De- Interference for Quantum Time-Bin States Nonlinear optic induced transparency and Brillouin Microscopy for Ocular Biomechan- Visual Sensitivity and Object Recognition, De- multiplexing Elements for Underwater Optical in Satellite Channels, Giuseppe Vallone1, Dan- frequency conversion on a chip, Chang- ics, Seok-Hyun A. Yun1; 1Harvard Medical School nis G. Pelli1; 1New York Univ., USA. The limits 1 1 1 1 Communications, Indumathi R. Srimathi , Keith iele Dequal1, Marco Tomasin1, Matteo Schiavon1, Ling Zou , Xiang Guo , Hojoong Jun , Hong and Massachusetts General Hospital, USA. We to human visual sensitivity can be factored into 1 1 1 1 1 Miller , Wenzhe Li , Kaitlyn S. Morgan , Joshua Francesco Vedovato1, Vincenza Luceri2, Gi- Tang ; Yale Univ., China. Nonlinear optic will review the progress and prospect of Brillouin equivalent input noise, mostly due to unreliable 1 1 1 Baghdady , Eric G. Johnson ; Clemson Univ., useppe Bianco3, Paolo Villoresi1; 1Universita de- induced transparency by second order optical microscopy, which combines confocal imaging communication, and efficiency, mostly due to USA. Diffractive elements based on coordinate gli Studi di Padova, Italy; 2E-GEOS, Italy; 3MLRO, nonlinearity on an aluminum nitride photonic and Brillouin light scattering spectroscopy suboptimal algorithms. transformations have been realized at 450 nm Agenzia spaziale Italiana, Italy. The single chip is demonstrated experimentally, with a to map the hydromechanical properties of for demultiplexing orbital angular momentum photon interference of states that propagate in 14% external efficiency frequency conversion ocular tissues to help improve diagnosis and states and can be applied to an underwater Space along a 5000km channel is reported. The between visible and telecom photons. treatments. communications link. System efficiency of ~80% modulation phase is dependent on the satellite was obtained experimentally. velocity, expanding the degree-of-freedom available in Space Quantum Communications and Metrology.

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FTh4A • Symposium on Mid-Infrared Fiber FTh4B • Optical Vortices—Continued FTh4C • Computational Imaging I— FTh4D • Optics Meets Neuroscience I— Sources I—Continued Continued Continued

FTh4B.2 • 14:45 FTh4C.3 • 14:45 Fractional Vortex Hilbert’s Hotel, Gregory J. Gbur1; 1Phys- Motion Artefact Detection in Structured Illumination ics and Optical Science, Univ of North Carolina at Char- Microscopy, Ronny Förster1,2, Kai Wicker3, Walter Müller1,2, lotte, USA. We demonstrate theoretically how the unusual Aurélie Jost1,2, Rainer Heintzmann1,2; 1Microscopy, Leibniz mathematics of infinite sets appears in the propagation of Inst. of Photonic Technology, Germany; 2Friedrich Schiller light through fractional vortex spiral waveplates. It is shown Univ. Jena, Germany; 3Corporate Research and Technology, how Hilbert’s famous hotel is manifested in a singularity of Carl Zeiss AG, Germany. The necessary image processing in vortices. structured illumination microscopy generates high resolution artefacts if the sample has moved during the acquisition. Our algorithm locates motion and distinguishes artefacts from real high resolution cell features.

FTh4A.3 • 15:00 Tutorial FTh4B.3 • 15:00 FTh4C.4 • 15:00 FTh4D.3 • 15:00 Invited Mid-infrared Wavelength Conversion in Chalcogenide Spatio-Temporal Optical Vortices, Nihal Jhajj1, Ilia Larkin1, Integrating sphere based speckle generation for wave- Imaging Activity in the Spinal Cord, Daniel C. Cote1; 1Uni- Optical Microfibers, Thibaut Sylvestre1, Thomas Godin1, Eric Rosenthal1, Sina Zahedpour1, Jared Wahlstrand1, Howard length determination and laser stabilization, Nikolaus K. versite Laval, Canada. We will show various strategies (both John M. Dudley1, Raja Ahmad2, Martin Rochette2; 1Optics, Milchberg1; 1Univ. of Maryland at College Park, USA.We pres- Metzger1, Roman Spesyvtsev1, Bill Miller2, Gareth Maker2, for surgery and imaging techniques) to image activity in the CNRS FEMTO-ST Inst., France; 2Department of Electrical and ent the first measurements of spatio-temporal optical vortices Graeme Malcolm2, Michael Mazilu1, Kishan Dholakia1; 1Univ. spinal cord using genetically encoded calcium indicators Computer Engineering, McGill Univ., Canada. Chalcogenide (STOVs). STOV generation/propagation is a universal feature of St Andrews, UK; 2M-Squared Lasers, UK. An integrating for neuronal activity and monitoring dendrites for microglial fibers have been identified as very attractive nonlinear of nonlinear pulse collapse and collapse arrest. sphere generates wavelength dependent speckle patterns activity. waveguides for mid-infrared applications. We review our that realizes an ultra-sensitive wavemeter with sub- recent achievements on mid-IR frequency conversion femtometre resolution. Utilizing this wavemeter, we stabilize and supercontinuum generation in chalcogenide tapered a laser for atom cooling of Rubidium to better than 1 MHz. optical fibers. Thursday, 20 October Thursday,

FTh4B.4 • 15:15 FTh4C.5 • 15:15 Partially Coherent Vortex Beams of Arbitrary Order, Char- Withdrawn. lotte Stahl1, Gregory J. Gbur1; 1Univ of North Carolina at Char- lotte, USA. We derive analytic solutions for an infinite set of partially coherent vortex beams of any azimuthal order. Such beams may be useful for free space optical communication and understanding them is a necessary first step.

Biography: Thibaut Sylvestre is leading the nonlinear photonics group at the Femto-ST institute in France and he is super- vising studies of nonlinear optical phenomena in specialty fibers with the aim of investigating potential applications to telecommunications, lasers and sensors.

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FTh4E • High-Capacity Optical FTh4F • Quantum Communication FTh4G • Integrated Nonlinear FTh4H • Probing Ocular FTh4I • Symposium on 100 Years Communications and Data and Networking I—Continued Optics I—Continued Biomechanics with Imaging of Vision at OSA: Most Cited Centers I—Continued Techniques / Novel Applications Vision Papers in OSA Journals— of Femtosecond Lasers in Continued Ophthalmology—Continued

FTh4E.3 • 14:45 FTh4G.3 • 14:45 Pump-Phase-Noise Tolerant Wavelength Photonic-chip based widely tunable micro- Multicasting for Coherent Communications wave source using a Brillouin opto-electronic using Kerr Frequency Combs, Peicheng Liao1, oscillator, Moritz Merklein1, Birgit Stiller1, Changjing Bao1, Arne Kordts2, Maxim Karpov2, Irina Kabakova2, Udara Mutugala3, Khu Vu4, Martin Hubert Peter Pfeiffer2, Lin Zhang3, Stephen Madden4, Benjamin J. Eggleton1, Yinwen Cao1, Ahmed Almaiman1, Amirhossein Radan Slavik3; 1Centre for Ultrahigh bandwidth Mohajerin-Ariaei1, Morteza Ziyadi1, Tobias J. Devices for Optical Systems (CUDOS), The Kippenberg2, Alan Willner1;1Univ. of Southern Univ. of Sydney, Australia; 2Blacket Laboratory, California, USA; 2Ecole Polytechnique Federale Imperial College London, UK; 3Optoelectronics Lausanne, Switzerland; 3Tianjin Univ., China. We Research Centre (ORC), Univ. of Southampton, experimentally demonstrate the pump-phase- UK; 4CUDOS, Australian National Univ., Aus- noise-tolerant wavelength multicasting for 20 tralia. We demonstrate the first widely tunable GBaud/s QPSK signals using Kerr frequency chip-based opto-electronic microwave source combs. The EVM of multicasted copy almost based on stimulated Brillouin scattering. The stays unchanged when the pump linewidth is output frequency can be tuned over 40 GHz and broadened to 2 MHz. the phase-noise performance is comparable to high-range RF sources.

FTh4E.4 • 15:00 Invited FTh4G.4 • 15:00 Invited FTh4F.3 • 15:00 FTh4H.3 • 15:00 Invited FTh4I.3 • 15:00 Thursday, 20 October Underwater Optical Communication Link Quantum Networks with Optical Fre- Asymmetric Light-Light Interaction by Non- Multiphoton Retinal Imaging, Jennifer J. Motion, Early Vision, and the Plenoptic Func- 1 Using Wavelength Division Multiplexing, quency Combs, Nicolas Treps1, Clément Hermitian Photonics, Han Zhao , William Feg- Hunter1; 1Univ. of Rochester, USA. Cellular- tion, Edward H. Adelson1; 1Massachusetts Inst. 2 1 1 3 Polarization Division Multiplexing and Orbital Jacquard1, Young-Sik Ra1, Adrien Dufour1, adolli , Jiaka Yu , Zhifeng Zhang , Li Ge , Axel scale non-linear imaging of the living retina of Technology, USA. If you generalize edge 2 1 1 2 Angular Momentum Multiplexing, Joshua Francesco Arzani1, Valentina Parigi1, Claude Scherer , Liang Feng ; SUNY Buffalo, USA; De- has made it possible to non-invasively image detection to space-time, you get motion. If you 1 1 1 Baghdady , Kaitlyn Morgan , Keith Miller , Fabre1;1Laboratoire Kastler Brossel, France. The partment of Physics and Kavli Nanoscience Inst., the ganglion cell mosaic and to interrogate keep generalizing you get color opponency, 1 1 3 Joseph Kelly , Indumathi R. Srimathi , Wenzhe intrinsic multimode character of optical California Inst. of Technology, USA; Depart- molecular processes such as the visual cycle stereopsis, flicker, and much more. The 1 1 1 Li , Eric G. Johnson ; Clemson Univ., USA. We frequency combs is demonstrated to be an ideal ment of Engineering Science and Physics, CUNY, within rods and cones. plenoptic function captures everything that report on the direct modulation of blue laser candidate for quantum information processing. USA. Effective light-light interaction enables can be seen; its derivatives yield early vision. diodes for underwater optical communication Generation of on demand quantum networks energy-efficient optical networks. By non- utilizing wavelength, polarization and space and versatile mode-dependant non-gaussian Hermitian on-chip engineering, we demonstrate division multiplexing. Using this scalable operations are demonstrated. asymmetric light control where intense laser architecture, we demonstrate an effective data field is manipulated by weak control with an rate of 10 Gbit/s. extinction ratio up to 60 dB.

FTh4E.5 • 15:15 FTh4G.5 • 15:15 Modal Properties of Perturbed Few-Mode Wideband spectral broadening in ultra-short Optical Fibers, Werner Klaus1, Katsunori ultra-silicon rich nitride waveguides, Ju Imamura2, Ryuichi Sugizaki2, Yoshinari Awaji1, Won Choi1, George F. R. Chen1, D. K. T. Ng2, Naoya Wada1; 1National Inst of Information Kelvin J. A. Ooi1, Dawn T. H. Tan1;1Engineering & Comm Tech, Japan; 2Furukawa Electric Co. Product Development, Singapore Univ. of Ltd., Japan. We examine the modal properties Technology and Design, Singapore; 2Data of few-mode optical fibers with respect to two Storage Inst., Agency for Science, Technology common fiber perturbations, birefringence and Research (A*STAR), Singapore. Ultra-silicon and core non-circularity, and investigate the rich nitride (USRN) waveguide with 1-mm-length relationship of the fiber’s true and LP modes in possessing high Kerr nonlinearity and low two a quantitative way. photon absorption achieved femtosecond spectral bandwidth of 225 nm at near-infrared wavelength range, which is a 4 fold spectral broadening.

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FTh4A.4 • 15:30 Invited FTh4B.5 • 15:30 Invited FTh4C.6 • 15:30 FTh4D.4 • 15:30 Mid-Infrared Photonics in Healthcare, Angela Sed- Quantum and Classical Properties of Vector Modes, An- Imaging Quality of Intensity-Interferometric Spectral- A Miniaturized Optical System for Monitoring Cerebrovas- 1 don1; 1Univ. of Nottingham, UK. We set a record in drew Forbes1, Bereneice Sephton2; 1Univ. of Witwatersrand, Domain Optical Coherence Tomography with Dispersion cular Perfusion during Deep Brain Stimulation, Linhui Yu , 1 1 1,2 2 1,2 1 demonstrating extreme broad-band supercontinuum South Africa, 2CSIR Natiional Laser Centre, South Africa. Insensitivity, Tomohiro Shirai ; Natl Inst of Adv Industrial M. Sohail Noor , Zelma H. Kiss , Kartikeya Murari ; Electrical generated light 1.4 to 13.3 microns in a specially engineered Vector beams are non-separable light fields. By borrowing Sci & Tech, Japan. We demonstrate that unwanted artifacts and Computer Engineering, Schulich School of Engineering, 2 MIR fibre, a key first step towards bright, portable, broadband tools from quantum mechanics, we show how to create, observed in dispersion-insensitive optical coherence to- Univ. of Calgary, Canada; Hotchkiss Brain Inst., Department MIR sources for applications in healthcare. define and measure them, and demonstrate how they may mography based on spectral intensity interferometry can be of Clinical Neurosciences, Cumming School of Medicine,, be used to simulate quantum processes. reduced by means of a relative displacement between the Univ. of Calgary, Canada. We present the design of a detector and the spectrum to be captured. miniaturized optical system to measure changes in cortical perfusion in response to deep brain stimulation. The system design and preliminary results are presented. Reminder: FiO/LS 2016 Program

now available in FTh4C.7 • 15:45 FTh4D.5 • 15:45 Digital refocusing of fluorescent light intensity with spatial A diamond-based, hybrid optrode for multisite optogenet- mobile formats! frequency modulated imaging, Jeffrey J. Field1, Randy ics, Antoine Boudet1, Robert Scharf1, Martin Dawson1, Keith Bartels1; 1Colorado State Univ., USA. We present an imaging Mathieson1; 1Univ. of Strathclyde, UK. Ideal for multi-depth method that transfers the spatial phase difference between optogenetics, current monolithic LED neuroprobes show two coherent illumination beams into temporal modulations inherent limits, notably for heat extraction. Here we present of fluorescent light emission collected on a single-pixel a diamond optrode integrating transfer-printed GaN µLEDs,  detector, enabling refocusing of fluorescent light. allowing extended/high-power emission and versatility. Visit www.frontiersinoptics.com

Thursday, 20 October Thursday, for more information.

16:00–16:30 Coffee Break, West Corridor and Skyway Lobby (Radisson)

102 FiO/LS 2016 • 16–21 October 2016 Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E

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FTh4E.6 • 15:30 Invited FTh4F.4 • 15:30 FTh4G.6 • 15:30 FTh4H.4 • 15:30 Invited FTh4I.4 • 15:30 Invited Ultra-broadband Nonlinear Optical Signal Multi-user Quantum Key Distribution with 3C Silicon Carbide Nanophotonics, Francesco IRIS – A New Paradigm in Laser Refractive Fourier, Gabor, Reichardt, Hilbert: Guides Processing for Optical Communications, Hao Entangled Photons from a Semiconduc- Martini1, Alberto Politi1; 1Univ. of Southamp- Correction, Jonathan D. Ellis1,2, Gustavo on the Path to a Model of Human Motion 1 Hu1, Francesco Da Ros1, Minhao Pu1, Michael tor Chip, Claire Autebert , Julien Trapa- ton, UK. The development of novel photonic A. Gandara-Montano2, Daniel R. Brooks2, Perception, Andrew B. Watson1; 1NASA Ames 2 2 3 Galili1, Kresten Yvind1, Toshio Morioka1, Leif teau , Adeline Orieux , Aristide Lemaître , materials can offer new capabilities for non- Kaitlin T. Wozniak2, Sara M. Gearhart2, Len A. Research Center, USA. The visual motion 3 2 Katsuo Oxenløwe1; 1DTU Fotonik, Technical Carme Gomez-Carbonnel , Eleni Diamanti , linear and quantum optics. We demonstrate key Zheleznyak2,3, Paul D. Funkenbusch1, Wayne H. sensing model developed by Albert Ahumada 2 1 1 Univ. of Denmark, Denmark. Nonlinear optics Isabelle Zaquine , Sara Ducci ; Université components for a photonic platform in 3C-SiC, Knox2, Krystel R. Huxlin4; 1Dept. of Mechanical and myself relied on four concepts: motion in 2 enables ultra-broadband, ultra-fast and phase- Paris Diderot-Paris7, France; Laboratoire including high-confinement waveguides, Engineering, Univ. of Rochester, USA; 2The the frequency domain; localization in space, preserving applications that can be very useful traitement et communication de l’information, grating couplers and high-Q resonators. Inst. of Optics, Univ. of Rochester, USA; 3Clerio time, and frequency; comparing space and time; 3 in optical communications. A single-source Télécom ParisTech, France; Laboratoire de Vision, Inc., USA; 4Flaum Eye Inst., Univ. of and the Hilbert transform. frequency comb can enable a large number Photonique et Nanostructure, France. We Rochester, USA. Altering the refractive index of of WDM channels, reducing required number experimentally demonstrate a multi-user both hydrogel materials and living cornea shows of lasers. quantum key distribution scheme based on promise for ophthalmic applications. Here we polarization entangled photons emitted from an show our recent developments in the use of AlGaAs chip and standard telecom wavelength femtosecond lasers in a mode that induces division multiplexers. nonlinear multi-photon absorption and alters the refractive index of transparent materials. FTh4F.5 • 15:45 FTh4G.7 • 15:45 Generation and analysis of correlated pairs On-chip Turing pattern formation for coherent of photons on a satellite, 1 high-power THz radiation, 1

Alexander Ling , Shu-Wei Huang , Thursday, 20 October Zhongkan Tang1, Rakhitha Chandrasekara1, Yue Jinghui Yang1, Shang-Hua Yang2, Mingbin Yu2, Chuan Tan1, Cliff Cheng1, Daniel Oi2; 1Centre for Dim-Lee Kwong2, Mona Jarrahi1, Chee Wei Quantum Technologies, Singapore; 2SUPA Dept Wong1; 1UCLA, USA; 2The Inst. of Microelec- of Physics, Univ. of Strathclyde, UK. We report tronics, Singapore. We report efficient on-chip the operation of a photon pair source on board Turing pattern formation, uniquely enabled by a nanosatellite: an important milestone towards mode-hybridization induced phase matching. compact entangled photon pair sources for The robustness, tunability, coherence, and future space-based quantum communication. efficiency lend itself to an excellent pump for high-power narrow-linewidth THz radiation.

16:00–16:30 Coffee Break, West Corridor and Skyway Lobby (Radisson)

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16:30–18:30 16:30–18:30 16:30–18:30 16:30–18:30 FTh5A • Symposium on Mid-Infrared Fiber FTh5B • Optical Vortices, Polarization and FTh5C • Computational Imaging II FTh5D • Optics Meets Neuroscience II Sources II Mode Shaping Presider: David Hasenauer, Synopsys, USA Presider: Ann E. Elsner, Indiana Univ., USA Presider: Morten Ibsen; Univ. of Presider: Greg Gbur, Univ. of North Carolina Southampton, UK at Charlotte, USA

FTh5A.1 • 16:30 Invited FTh5B.1 • 16:30 Invited FTh5C.1 • 16:30 Invited FTh5D.1 • 16:30 Invited All-fiber Sources Operating in the Mid-infrared, Martin Towards Chiral Materials Science Based on Optical Imaging Beyond the Limits: Active Imaging for Enhancing Cone Signals, Adaptive Optics, and the Brain, Lawrence Bernier1; 1Université Laval, Canada. The architecture of an Vortices Illumination, Takashige Omatsu1; 1Chiba Univ., Resolution, 3D Information, and Indirect Imaging, Marc Sincich1; 1Optometry and Vision Science, Univ. of Alabama all-fiber laser operating at 2.94 microns at a continuous output Japan. Illumination of optical vortoces enables us to twist P. Christensen1, Prasanna Rangarajan1; 1Southern Method- at Birmingham, USA. Cone-targeted microstimulation using power of 30W will be detailed. Different recent technical melted materials to establish chiral strutures on a nanoscale. ist Univ., USA. We present a technique of utilizing active adaptive optics provides access to the processing of single achievements based on the same mastered technology will Such structured materials will open the door to develop illumination to surpass the limitations of passive imaging cone signals in the visual system. Recent progress revealing also be discussed. chirality sensors, chiral chemical reactors, and metamaterials. systems alone. An approach to combine super resolution and cone signal variability and summation in the human and profilometery is presented. Recent applications to indirect macaque brain will be presented. imaging will be discussed.

FTh5A.2 • 17:00 Invited FTh5B.2 • 17:00 FTh5C.2 • 17:00 FTh5D.2 • 17:00 Invited 1,2 Power Scaling Concepts for Mid-infrared Fibre Lasers Generation of tunable orbital angular momentum in Experimental x-ray ghost imaging, Daniele Pelliccia , Parallel Processing in the Visual System, Bart Bor- 1 2 1 2 Using Fluoride Glass, Stuart D. Jackson1; 1Engineering, polarization maintaining fiber, Robert Niederriter , Mark David M. Paganin ; Science, RMIT Univ., Australia; Phys- ghuis1; 1Univ. of Louisville, USA. Optical imaging is transform- 3 1,2 1 Macquarie Univ., Australia. I will briefly overview the field of Siemens , Juliet T. Gopinath ; Department of Physics, ics and Astronomy, Monash Univ., Australia. We report the ing the study of neural circuit function in the brain, including 2 mid-infrared fibre lasers with a focus on recent developments Univ. of Colorado at Boulder, USA; Department of Electri- experimental demonstration of x-ray ghost imaging using the retina. Here, I will show how 2-photon fluorescence aimed at increasing the output power. I will mainly focus cal, Computer, and Energy Engineering, Univ. of Colorado synchrotron emission. Our experiment opens a clear path imaging revealed key properties of information processing 3 on fibre gain elements involving fluoride glass as the host Boulder, USA; Department of Physics and Astronomy, Univ. towards low dose x-ray medical diagnostics, and also towards in retinal bipolar cell pathways. material. of Denver, USA. We demonstrate tunable orbital angular single-molecule diffraction imaging at Free Electron Lasers. momentum (OAM) in two-mode polarization-maintaining optical fiber. The OAM and spatial beam profile can be varied as the relative phase and coherence between fiber modes is adjusted. Thursday, 20 October Thursday,

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16:30–18:30 16:30–18:30 16:30–18:30 16:30–18:30 16:30–18:30 FTh5E • High-Capacity Optical FTh5F • Quantum Communication FTh5G • Integrated Nonlinear LTh5H • Topological Photonics I LTh5I • High Harmonic Communications and Data and Networking II Optics II Presider: Mohammad Hafezi, Univ. Generation I Centers II Presider: Paolo Villoresi; Universita Presider: Sasan Fathpour; CREOL, of Maryland, College Park, USA Presider: David Reis; Stanford Presider: Benyuan Zhu; OFS degli Studi di Padova, Italy Univ. of Central Florida, USA Univ., USA Laboratories, USA

FTh5E.1 • 16:30 Invited FTh5F.1 • 16:30 Invited FTh5G.1 • 16:30 Invited LTh5H.1 • 16:30 Invited LTh5I.1 • 16:30 Invited Large-data Center Interconnect: Emerging Nonlinear Light-Matter Interactions in Engi- Soliton Mode Locking in Optical Microcavi- Majorana-like Zero Modes in a Two-di- Extreme Ultraviolet Generation in Bulk Solids: Technologies and Scaling Challenges, Xiang neered Optical Media, Natalia M. Litchinitser1, ties, Kerry J. Vahala1; 1California Inst. of Tech- mensional Photonic Topological Insula- Linking Multi-PHz Electronics and Photon- Zhou1; 1Google, USA. In this talk I will present a Wiktor Walasik1, Salih Silahli1, Jingbo Sun1, nology, USA. Progress on soliton frequency tor, Jiho Noh1, Wladimir Benalcazar2, Sheng ics, Eleftherios Goulielmakis1; 1Max-Planck-Insti- high-level review on emerging technologies and Yun Xu1; 1State Univ. of New York at Buffalo, microcombs is described including review Huang3, Kevin Chen3, Taylor Hughes2, Mikael tut fur Quantenoptik, Germany. We will present scaling challenges for large-scale data center USA. Here, we discuss novel opportunities of dissipative Kerr cavity soliton physics. C. Rechtsman1; 1Physics, The Pennsylvania how electron motion in solids, driven by intense, interconnection networks. for structured light manipulation in nonlinear Dispersive-wave generation and Raman self- State Univ., USA; 2Physics, Univ. of Illinois, precisely-sculpted, optical fields give rise to soft-matter, gaseous and negative-index media. frequency shift will be discussed. Progress USA; 3Electrical Engineering, Univ. of Pittsburgh, controllable electric currents, of multi-Petahertz towards octave-spanning microcombs is USA. Constructing highly confined defect frequency, advancing lightwave electronics to overviewed. modes in photonic crystal slabs and fibers new realms of speed and precision. is a major challenge in photonics. We use a photonic topological insulator to realize mid- gap (maximally confined) disorder-insensitive defect modes.

FTh5E.2 • 17:00 FTh5F.2 • 17:00 Invited FTh5G.2 • 17:00 LTh5H.2 • 17:00 Invited LTh5I.2 • 17:00 Invited Can information Capacity be Increased with Practical Continuous Variable QKD in Fiber Experimental Demonstration of Inserting Title to be Announced, Shanhui Fan1; 1Stanford Plasmonic-enhanced High Harmonic Genera- Orbital Angular Momentum?, Mingzhou and Free Space Systems, Christoph Mar- Phase-Locked Lines into Kerr Combs using Univ., USA. Abstract not available. tion from Bulk Silicon, Giulio Vampa1; 1Univ. 1 1 1 1 1 Chen , Kishan Dholakia , Michael Mazilu ; Univ. quardt2,1; 1Department of Physics, Univ. of Electro-Optical Modulation, Changjing Bao , of Ottawa, Canada. The near-field of a surface Thursday, 20 October 1 1 1 of St Andrews, UK. We demonstrate that using Erlangen-Nuremberg, Germany; 2Max Planck Peicheng Liao , Yinwen Cao , Guodong Xie , plasmon polariton generates high harmonics of 2 3 2 orbital angular momentum (OAM) does not Inst. for the Science of Light, Germany. I will Arne Kordts , Lin Zhang , Maxim Karpov , Mar- an infrared laser from the silicon substrate that 2 1 increase the telecommunication capacity of an review recent activities in continuous variable tin Hubert Peter Pfeiffer , Cong Liu , Morteza hosts an array of gold nanoantennas. 1 1 1 optical system. QKD that aims for the deployment of QKD Ziyadi , Yan Yan , Ahmed Almaiman , Amirhos- 1 1 equipment compatible with current telecom sein Mohajerin-Ariaei , Fatemeh Alishahi , 2 1 1 standards and research in satellite QKD that Tobias J. Kippenberg , Alan Willner ; Univ. of 2 will make it possible to bridge long distances. Southern California, USA; Ecole Polytechnique Federale de Lausanne (EPFL) Lausanne, Switzer- land; 3School of Precision Instrument and Opto- electronics Engineering, Tianjin Univ., China. We experimentally demonstrate the flexibility of inserting one or two lines into Kerr combs. The effect of the spacing between two sidebands (260 KHz and 770 KHz) from EO modulation on the communication system is studied.

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FTh5A • Symposium on Mid-Infrared Fiber FTh5B • Optical Vortices, Polarization and FTh5C • Computational Imaging II— FTh5D • Optics Meets Neuroscience II— Sources II—Continued Mode Shaping—Continued Continued Continued

FTh5B.3 • 17:15 FTh5C.3 • 17:15 Radial poarisation and more from a glass cone., Neal Shape Reconstruction and Orientation Estimation of Radwell1, Ryan D. Hawley1, Joerg B. Goette1, Sonja Franke- Transparent Microscopic Object using Light Field Micros- Arnold1; 1Univ. of Glasgow, UK. Beams with polarisation copy, Xiaopeng Peng1, Grover A. Swartzlander1; 1Rochester structure are interesting due to their ability to produce Inst. of Technology, USA. This paper reports a framework for unconventional light fields. Here we show that a simple glass high speed volumetric imaging and orientation estimation cone can create such beams and we explore the mechanisms of transparent microscopic objects using light field behind this, as well as its potential uses. microscopy.The framework provides a potentiality for kinetic characterization of microscopic objects.

FTh5A.3 • 17:30 Invited FTh5B.4 • 17:30 FTh5C.4 • 17:30 FTh5D.3 • 17:30 Invited Mid-Infrared Sources for Ultra-Broadband Cavity Enhanced High-Order Monstar Disclinations in the Polarization of Multi-spectral visible-to-shortwave infrared smart cam- Imaging Microglia in the Physiological Brain, Anna Ma- 1 1,2 1 Spectroscopy, Caroline G. Amiot1,2, Piotr Ryczkowski1, Antti Light, Enrique J. Galvez , Behzad Khajavi ; Colgate Univ., era built on a compressive sensing platform, Lenore jewska1; 1Univ. of Rochester, USA. Microglia are traditionally 2 1 1 1 1 Aalto1, Juha Toivonen1, Goëry Genty1; 1Tampere Univ. of Tech- USA; Physics and Astronomy, Florida Atlantic Univ., USA. We McMackin , Matthew A. Herman , Tyler Weston ; InView thought to be the immune cells of the brain. Here we present nology, Finland; 2Institut FEMTO-ST, France. We developed investigated high-order polarization disclinations using a Technology Corporation, USA. We describe development evidence from in vivo imaging experiments, that microglia an all-fiber based supercontinuum source spanning from 900 beam prepared in a non-separable superposition of high- of a multi-spectral camera built on a compressive sensing have critical roles in normal brain function. to 3700 nm. We performed incoherent broadband cavity order spatial and polarization modes. Our findings include platform. Its novel yet simple design takes advantage of enhanced absorption spectroscopy using that source and high-order monstar patterns that have a negative index. the diffractive properties of a micromirror array used in the were able to detect multicomponent simultaneously. well-known single-pixel camera architecture.

FTh5B.5 • 17:45 FTh5C.5 • 17:45 Nonlinear Generation of High Power and Higher order Hol- Computational imaging with adaptive spatially-variable low Gaussian Beam, Apurv Chaitanya Nellikka1, Jabir M. V.1, resolution, David B. Phillips1, Ming-Jie Sun1, Matthew Edgar1, Jay Banerji1, Goutam K. Samanta1; 1Physical Research Labo- Jonathan Taylor1, Graham Gibson1, Stephen Barnett1, Miles ratory, India. We demonstrate novel experimental scheme Padgett1; 1Univ. of Glasgow, UK. We describe a single-pixel generating high-power, higher-order hollow-Gaussian-Beam imaging system with an enhanced frame-rate, achieved by Thursday, 20 October Thursday, (HGB) through annihilation of OAM of interacting photons in reconstructing images with a variable resolution across the nonlinear process. Also, report a new and only method for field-of-view. Resolution can be adaptively changed from characterizing the order of HGBs. frame to frame to track moving objects.

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FTh5E • High-Capacity Optical FTh5F • Quantum Communication FTh5G • Integrated Nonlinear LTh5H • Topological Photonics I— LTh5I • High Harmonic Communications and Data and Networking II—Continued Optics II—Continued Continued Generation I—Continued Centers II—Continued

FTh5E.3 • 17:15 FTh5G.3 • 17:15 Effective Area Measurement of Few-Mode Silica-Chip-Based Continuum Generation for Fiber Using Far Field Scan Technique with Frequency Comb Self-Referencing, Connor Hankel Transform Generalized for Circularly- Frederick1, Dong Yoon Oh2, Ki Youl Yang2, Gabri- Asymmetric Mode, Tetsuya Hayashi1, Yoshiaki el Ycas1, Kerry J. Vahala2, Scott Diddams1; 1Time Tamura1, Takuji Nagashima1, Kazuhiro Yone- and Frequency Division, National Inst. of zawa1, Toshiki Taru1, Koji Igarashi2, Daiki Soma2, Standards and Technology, USA; 2T. J. Watson Yuta Wakayama2, Takehiro Tsuritani2; 1Sumitomo Laboratory of Applied Physics, California Inst. of Electric Industries, Ltd., Japan; 2KDDI R&D Technology, USA.Dispersion-engineered silica Laboratories, Inc., Japan. We developed an ridge waveguides are employed for dispersive wave generation from 275 nm to 575 nm. When Aeff measurement method for the few-mode fiber. A newly derived NFP–FFP transform placed at the pump harmonic, the dispersive wave enables frequency comb self-referencing equation enabled Aeffmeasurement of circularly- asymmetric modes using high-dynamic-range in a collinear, zero delay geometry. far-field scan technique and low-crosstalk mode multiplexer.

FTh5E.4 • 17:30 FTh5F.3 • 17:30 Invited FTh5G.4 • 17:30 LTh5H.3 • 17:30 Invited LTh5I.3 • 17:30 Invited Energy equalization of a set of coherent Optical Realisation of Communication Proto- On-chip photon pair source based on Mixing and Matching Photonic Topological Strong-Field High Harmonic and Sideband OAM states by means of optimal phase grat- cols with a Quantitative Quantum Communi- spontaneous parametric down conver- Phases: From Robust Delay Lines to Generation in Solids and Atoms, Stephan W. 1 1 1 1 ings, Jaime A. Anguita , Jaime E. Cisternas , cation Advantage, Norbert Lutkenhaus1; 1Univ. sion, Xiang Guo , Chang-Ling Zou , Carsten Topological Cavities, Tsuhsuan Ma1; Kueifu Koch1, Mackillo Kira1, Ulrich Huttner1; 1Philipps 1 1 1 1 1 Gustavo L. Funes ; Universidad de los Andes of Waterloo, Canada. Quantum Fingerprinting Schuck , Hojoong Jung , Risheng Cheng , Lai1,2; Gennady Shvets1,2; 1Dept. of Physics, Universitat Marburg, Germany. High-harmonic 1 1 - Chile, Chile. We propose a method to design offers a exponential advantage over classical Hong Tang ; Yale Univ., USA. We demonstrate Univ. of Texas at Austin, USA; 2School of and sideband generation in solids and atoms is Thursday, 20 October phase gratings that will generate a uniform protocols in comparing two remote files by a an on-chip parametric down conversion photon Applied and Engineering Physics, Cornell Univ., analyzed using a microscopic many-body theory. energy distribution among the constituent OAM referee in the simultaneous message passing pair source based on second order nonlinearity. USA. I will describe our recent work on the Solid-state HHG exhibits a novel quantum- states after illumination, while minimizing the protocol. We show how to realize this advan- High brightness, low noise, high purity photon photonic emulation of three topological phases interference of electrons which is absent in content of radial modes. tange using optical communication techniques. pairs are generated in a microring resonator on corresponding to quantum Hall, spin-Hall, and atomic systems. Aluminum nitride-on-Insulator platform. valley-Hall interactions. New topology-enabled paradigms for a variety of photonic devices FTh5E.5 • 17:45 Tutorial FTh5G.5 • 17:45 are proposed. Recent Advances on Fibers for Optical Com- Blue light emission via harmonic generation munications, Benyuan Zhu1; 1OFS Laboratories, by stimulated Raman scattering in a silica USA. In this tutorial, we will review recent toroid microcavity, Shun Fujii1, Takumi Kato1, advances on optical fibers including ultra-low- Atsuhiro Hori1, Yusuke Okabe1, Akihiro Kubota1, loss ultra-large-area fibers for systems, multicore Takasumi Tanabe1; 1Keio Univ., Japan. We fibers and few-mode fibers for space-division- experimentally investigate blue light emission multiplexing transmissions. Their optical fiber in a silica toroid microcavity. We show the blue properties and performance are provided. light as the harmonic generation from anti- Stokes light of higher order stimulated Raman scattering.

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FTh5A.4 • 18:00 Invited FTh5B.6 • 18:00 FTh5C.6 • 18:00 FTh5D.4 • 18:00 Mid-IR Ultrafast Fibre Laser Sources, Khanh Kieu1; 1Univ. Generation of wavelength-independent and sub-wave- Single Shot Time Domain Ghost Imaging using Wavelength Mapping the birefringence of amyloid deposits found 1 1 1 of Arizona, USA. I will review mid-IR fiber laser sources and length Bessel beams by meta-axicons, Wei-Ting Chen , Multiplexing, Piotr Ryczkowski , Margaux Barbier , Ari Tapio in retinas in association with Alzheimer’s disease, Tao 1 1 2 3 1 1 1 1 1 present different schemes to generate ultrafast pulses in this Mohammadreza Khorasaninejad , Alexander Y. Zhu , Jaewon Friberg , John M. Dudley , Goëry Genty ; Optics Laboratory, Jin , Laura Emptage , David DeVries , Melanie C. 1,2 1 1 1 1 2 1,2 1 spectral range. Some interesting applications of ultrafast Oh , Rober Devlin , Aun Zaidi , Federico Capasso ; Harvard Tampere Univ. of Technology, Finland; Inst. of Photonics,, Campbell ; Department of Physics and Astronomy, Univ. of 2 3 2 mid-IR sources will be also discussed. Univ., USA; Univ. of Waterloo, Canada. We report meta- Univ. of Eastern Finland, Finland; Institut FEMTO-ST, CNRS– Waterloo , Canada; School of Optometry and Visual Science, axicons with high numerical aperture for generating Bessel Université de Franche-Comté, France. We report on the first Univ. of Waterloo, Canada. A new method is established for beams with λ/3 spot size. The spot size of the generated demonstration of computational ghost imaging in the time mapping birefringence of the amyloid plaques found in the Bessel beams is independent of wavelength of incident light domain using wavelength multiplexing. The wavelength- retinas of subjects in association with Alzheimer’s disease because of tailored phase profile. multiplexed Hadamard patterns used to probe a time-varying using fluorescence confocal microscopy and Mueller matrix waveform enables image reconstruction in real time. polarimetry.

FTh5B.7 • 18:15 FTh5C.7 • 18:15 FTh5D.5 • 18:15 Custom-Tailored Sorting of Structured Light by Controlled Image Quality of Compressive Imaging with Quan- Hyperspectral Imaging in Live Mouse Cortex Using a Scattering, Robert Fickler1, Robert W. Boyd1,2; 1Univ. of tum Light, Kam Wai C. Chan1, Vamsi Manthapuram1, Lu 48-Channel Multiphoton Microscope, Amanda Bares1, Ottawa, Canada; 2Institut of Optics, Univ. of Rochester, Zhang1; 1Univ. of Oklahoma - Tulsa, USA. Several common Mitchell A. Pender1, Menansili A. Mejooli1, Steven Tilley1, USA. Light with a complex structure is interesting for reconstruction algorithms were used to perform compressive Kuang E. Chen1, Jingyuan Dong1, Peter C. Doerschuk1, foundations and applications in classical and quantum optics. quantum imaging with Fock states, coherent states, and Chris B. Schaffer1; 1Cornell Univ., USA. We constructed a We investigate controlled scattering processes to realize squeezed light. It was found that the different light sources hyperspectral multiphoton microscope collecting 48 channels novel transformations such as custom-tailored sorting of gave the same scaling law for the root-mean-squared error. of excitation/emission spectral data, while retaining the structured photons. imaging depth of nonlinear microscopy. We demonstrate imaging of multiple overlapping fluorophores in vivo.

Reminder: FiO/LS 2016 Program Thursday, 20 October Thursday, now available in mobile formats!  Visit www.frontiersinoptics.com for more information.

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FTh5F.4 • 18:00 FTh5G.6 • 18:00 LTh5H.4 • 18:00 Invited LTh5I.4 • 18:00 Invited Chip-scale MOT for Microsystems Technol- Ultraviolet Second Harmonic Generation Topological Theory of Disallowed Cou- Upper Limits to Near-field Radiative Heat 1 1 ogy, Argyrios Dellis , Matthew T. Hummon , in Aluminum Nitride Microring Resona- plings, Bo Zhen1,2, Hengyun Zhou1, Chia Wei Transfer: Generalizing the Blackbody Con- 1 1 1,2 1 Songbai Kang , Elizabeth A. Donley , John tors, Michael l. fanto , Jeffrey A. Steidle , Hsu3, Ling Lu1, A. . Stone3, Mordechai Segev2, cept, Owen Miller1; 1Yale Univ., USA. I describe 1 1 3 1 3 Kitching ; NIST, USA. We are developing Tsung-ju J. Lu , Stefan F. Preble , Dirk Englund , John Joannopoulos1, Marin Soljacic1; 1MIT, energy-conservation principles that answer a 2 2 a micro-fabricated platform to support the Christopher C. Tison , A. Matthew Smith , USA;2Technion, Israel; 3Yale Univ., USA. We basic question: what is the maximum radiative 2 2 creation of laser cooled samples. We are able Gregory A. Howland , Kathy-Anne Soderberg , reveal the topological nature of disallowed heat transfer rate between closely separated 2 1 to cool and trap ~5x10^5 atoms. We are in the Paul Alsing ; Rochester Inst. of Technology, couplings. We first show “bound states in the bodies? The new bounds offer the possibility 2 process of replacing the actively pumped cell USA; Information Directorate, Air Force Re- continuum” are fundamentally vortices in the for significant future enhancements, for 3 with a passively pumped cell. search Laboratory, USA; Massachusetts Inst. polarization directions carrying topological thermophotovoltaics and beyond. of Technology, USA. Aluminum nitride, with a charges. We then reveal their connections to (2) bandgap of 6.2 eV, and a χ of ~10’s of pm/V Chern numbers. can generate ultraviolet photons. This article Biography: Benyuan Zhu joined Bell Laborato- describes using aluminum nitride microring ries, Lucent Technologies in Holmdel, NJ USA resonators to produce second harmonic as a Member of Technical Staff (MTS) in 1999, photons below 400nm. then became a MTS at OFS Labs in 2002, and he was promoted to a Distinguished Member of Technical Staff in 2011. His research interests FTh5F.5 • 18:15 FTh5G.7 • 18:15 include DWDM transmission, advanced modula- Optical quantum computing with spectral Second-Hamonic Generation in Periodi- 1 tion, novel fibers and optical amplifier technolo- qubits, Joseph M. Lukens , Pavel Lougov- cally-Poled Thin Film Lithium Niobate on 1 1 1 1 gies. He has authored/coauthored +180 journal/ ski ; Oak Ridge National Laboratory, USA. We Silicon, Ashutosh Rao , Marcin Malinowski , 1 conference papers, one book chapter, and he formulate a universal platform for optical Amirmahdi Honardoost , Javed Rouf Taluk- 1 2 1 Thursday, 20 October has +18 US patents. He has served as TPC quantum information processing based on der , Payam Rabiei , Peter Delfyett , Sasan 1 1 members or chair for the conferences of OFC, spectral qubits, pulse shapers, and electro- Fathpour ; CREOL, Univ Central Florida, 2 IPC, WOCC, ACP. He is an Associate Editor of optic modulators. Our approach is compatible USA; Partow Technologies LLC, USA. Thin the Electronics Letters. Benyuan Zhu received with fiber networks and offers new potential for films of lithium niobate are wafer-bonded onto Ph.D. degree in Physics from Bath University, UK. interfacing matter qubits. oxidized silicon substrates and periodically poled for quasi-phase matching to demonstrate second-harmonic generation in submicron waveguides with a record-high conversion efficiency of 730%W-1cm-2.

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07:30–16:30 Registration, Galleria

08:00–10:00 08:00–10:00 08:00–10:00 08:00–10:00 FF1A • Imaging and Therapy Inside the FF1B • Optical Fiber Sensors I FF1C • Quantum Information Processing in FF1D • Quantum Optical Technologies Human Body Presider: Armando Ricciardi; Univ. of Sannio, Integrated Systems Presider: Alexander Sergienko; Boston Univ., Presider: Irene Georgakoudi, Tufts Univ., USA Italy Presider: Andrew White; Univ. of USA Queensland, Australia

FF1A.1 • 08:00 Invited FF1B.1 • 08:00 Tutorial FF1C.1 • 08:00 Invited FF1D.1 • 08:00 Invited Chemophototherapy with Porphyrin-Phospholipid Lipo- New Opportunities with, and Future Challenges of, Optical Implementation and Certification of Boson Sampling with The Promise of Quantum Imaging, Robert W. Boyd1; 1Univ. somes: A Treatment Possibility for Solid Tumors, Jonathan Fiber Sensor Technology, Jose Luis Santos1; 1Universidade Integrated photonics, Fabio Sciarrino1; 1Univ degli Studi di of Ottawa, Canada. Quantum Imaging strives to form Lovell1; 1SUNY Buffalo, USA. Liposomes containing small do Porto, Portugal. Optical sensing has been associated with Roma La Sapienza, Italy. Boson sampling is a computational improved images based on quantum phenomena. We give amounts of porphyrin-phospholipid are developed that high performance and recent developments indicate this task hard for classical computers, but efficiently solvable via examples of how these quantum images can be superior to otherwise have similar composition and pharmacokinetics trend will continue. The talk elaborates on challenges and bosonic interference in a specialized quantum computer. We conventional images in terms of sharpness, signal-to-noise to FDA-approved liposomal doxorubicin. Laser irradition opportunities facing this field, in particular when the sensor report several experiments of boson sampling implemented ratio, and low-light-level image formation. potently induces tumor ablation via chemophototherapy. platform is the optical fiber. with integrated quantum photonics.

Biography: José Luís Santos received his graduation in Physics from University of Porto, Portugal, and Ph.D. degree from the same University, benefiting from collaboration with the University of Kent at Canterbury, UK. He is currently a Professor of Physics at the Physics and Astronomy Department of Faculty of Sciences of University of Porto, FF1A.2 • 08:30 Invited Portugal. Optical fiber sensing is the main area of his research, FF1C.2 • 08:30 Invited FF1D.2 • 08:30 Invited Kagome Fiber Based Ultrafast Laser Microsurgery with focus on interferometric and wavelength encoded Boson Sampling with Continuous Variable Measure- First-Photon 3D Imaging with a Single-Pixel Camera, Mat- Probes, Adela Ben-Yakar1; 1Univ. of Texas at Austin, USA. I devices. He is author or co-author of more than 230 scientific ments, Timothy C. Ralph1; 1Univ. of Queensland, Austra- thew Edgar1, Ming-Jie Sun1, Gabriel Spalding1, Graham will present our efforts towards achieving a fully hand-held, 5 articles and co-author of 5 patents. With Professor Faramarz lia. We show that it is classically hard to sample the output Gibson1, Miles J. Padgett1; 1Univ. of Glasgow, UK. We use mm, ultrafast laser scalpel for microsurgery with a capability to Farahi of University of North Carolina was Editor of Handbook distribution of certain continuous variable measurements an ultrashort-pulsed laser and a high-speed spatial light deliver energies in excess of 5 μJ per pulse using large-area, of Optical Sensors, CRC Press 2014. from a BosonSampling device. Our argument is presented modulator to illuminate a scene with a series of patterns. A hollow-core kagome fibers. for exact BosonSampling. We discuss extending this result photomultiplier and fast electronics are used to histogram the to approximate sampling. first-photon backscattered from which a computer algorithm can reconstruct 3D images. Friday, 21 October Friday,

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07:30–16:30 Registration, Galleria

08:00–10:00 08:00–10:00 08:30–10:00 08:00–10:00 08:00–10:00 FF1E • Symposium on Integrated FF1F • Strongly Confined FF1G • Wavefront Sensing and FF1H • General Optical Sciences I LF1I • Nanophotonics II Photonic Manufacturing I Nanoscale Waveguides, Photonic Phase Retrieval Presider: To be Announced Presider: Yichen Shen; MIT, USA Presider: Stefan Preble; Rochester Crystals and Resonator Devices Presider: Len Zheleznyak, Univ. of Inst. of Technology, USA Presider: Andrew Poon; Hong Rochester, USA Kong Univ of Science & Technology, Hong Kong

FF1E.1 • 08:00 Invited FF1F.1 • 08:00 Invited FF1G.1 • 08:00 Invited FF1H.1 • 08:00 LF1I.1 • 08:00 Invited AIM Photonics – Manufacturing Challenges High-Q Photonic Crystal Resonators for Withdrawn. KALEXUS - a Potassium Laser System with Enhanced Lasing Through Tailoring of Photon- for Photonic Integrated Circuits, Michael Nonlinear Optics, Aude Martin2,1, Gregory Autonomous Frequency Stabilization on a ic Density of States, Marin Soljacic1; 1Massachu- 1 Liehr1,2; 1AIM Photonics, USA; 2SUNY Poly- Moille1, Sylvain Combrié1, Gaelle Lehoucq1, Sounding Rocket, Aline N. Dinkelaker , Max setts Inst. of Technology, USA. Nanophotonics 1 1 technic Inst., USA. The recently established Thierry Debuisschert1, Allard, P. Mosk3, Alfredo Schiemangk , Vladimir Schkolnik , Andrew offers unprecedented opportunities for tailoring 1 1 1,2 1 American Inst. for Manufacturing Photonics is De Rossi1,2; 1Thales Research & Technology, Kenyon , Markus Krutzik , Achim Peters ; In- photonic density of states. Weyl and Dirac a manufacturing consortium headquartered in France; 2Laboratoire de Photonique et de Nano- stitut für Physik, Humboldt-Universität zu dispersions could thus enable single-mode 2 NY, to advance the state of the art in the design, structures, CNRS UPR 20, France; 3Physics of Berlin, Germany; Ferdinand-Braun-Institut, lasing for substantially larger lasers. Novel gain manufacture, testing, assembly, and packaging Light in Complex Systems(LINX), Debye Inst. Leibniz-Institut für Höchstfrequenztechnik, Ger- media can be enabled as well. of integrated photonic devices. for Nanomaterials Science,, Utrecht Univ., many. Autonomous laser frequency stabilization Netherlands. Small volume cavities and cavity is a prerequisite for future space-borne atomic arrays made of III-V semiconductor with large physics experiments. The KALEXUS experiment electronic gap allow very large optical fields performed frequency stabilization of two 767 to be established. The spectral alignment of a nm extended cavity diode lasers onboard the triplet of resonances results into ultra-efficient TEXUS 53 sounding rocket. four-wave-mixing. FF1H.2 • 08:15 Controlling the Direction of Optical Power Flow in an Active Photonic Cavity, Ali Ka- zemi Jahromi1, Ayman Abouraddy1; 1Univ. of Central Florida, CREOL, USA. We demonstrate experimentally that the direction of Poynting’s vector and thus power flow in an optical cavity provided with net gain can be controllably reversed by modulating a passive intra-cavity loss element.

FF1E.2 • 08:30 Invited FF1F.2 • 08:30 FF1G.2 • 08:30 FF1H.3 • 08:30 LF1I.2 • 08:30 Invited Silicon Photonics Platforms: to Standardize Exceptional contours and band structure Multi-plane Phase Retrieval in Generalized Optical Characteristics of Bio-Inspired Recent Progress in Photonic Crystals, Susumu 1 or to Diversify?, Roel G. F. Baets1,2; 1Photonics design in parity-time symmetric photonic Two-Path Interferometry, Wesley Farriss , Lasers Based on Fluorescent Biomaterials Noda1; 1Kyoto Univ., Japan. I will report on 1 1 1 1 Friday, 21 October Research Group, Ghent Univ., Belgium; 2IMEC, crystals, Alexander Cerjan , Aaswath Ra- James R. Fienup , Tanya Malhotra , A. Nick and Bioconjugates, Jose A. Rivera , James G. recent progresses in manipulation of photons by 1 1 1 1 1 1 1 Belgium. Silicon photonics has emerged as a man , Shanhui Fan ; Stanford Univ., USA. We Vamivakas ; Univ. of Rochester, USA. Gener- Eden ; UIUC, USA. Changes in the chemical photonic crystals. They include (1) ultrahigh-Q major PIC-technology because it builds on the investigate the properties of 2D parity-time alized interferometry is a novel technique that environment of a biolaser were detected by nanocavities and their applications, (2) thermal maturity and infrastructure of the CMOS world. symmetric periodic systems whose periodicity is decomposes fields into transverse basis set analyzing spectral, temporal, and polarization emission control with a very fast modulation But where is the middle ground between yield- an integer multiple of the underlying Hermitian components and weighting coefficient magni- properties. Such detailed characterizations speed, and (3) broad-area coherent photonic- and cost-driven standardization and application- system’s periodicity. Such systems possess tudes. Nonlinear optimization phase retrieval are fundamental for biolasers to realize their crystal lasers with a high output-power. driven diversification? novel band structure engineering, and yield algorithms using multiple intensity planes are potential as diagnostics tools. supercollimation. developed.

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FF1A • Imaging and Therapy Inside the FF1B • Optical Fiber Sensors I—Continued FF1C • Quantum Information Processing in FF1D • Quantum Optical Technologies— Human Body—Continued Integrated Systems—Continued Continued

FF1B.2 • 08:45 Fast-light Enhanced Brillouin Laser Based Active Fiber Optics Sensor for Simultaneous Measurement of Rotation and Acceleration, Minchuan Zhou1, Zifan Zhou1, Mohammad Fouda1, Jacob Scheuer2, Selim Shahriar1; 1Northwestern Univ., USA; 2Tel Aviv Univ., Israel. We show an enhancement of ~358 for two counter-propagating Brillouin lasers in the sensitivity of an Active Fast Light Fiber Optic Sensor, which performs as a gyroscope and a sensor for acceleration, strain and temperature.

FF1A.3 • 09:00 Invited FF1B.3 • 09:00 FF1C.3 • 09:00 FF1D.3 • 09:00 1 1 Scanning Fiber Endoscopy with New Technologies and A Kind of Mechanical Robust Photonic Crystal Fiber A Quantum Fredkin Gate, Raj Patel , Joseph Ho , Franck A Variable Partially-Polarizing Beamsplitter, Jefferson Flo- 1,2 3 1 1 1 1 1 1 Forward-Viewing Applications, Eric Seibel1; 1Univ. of with Dual Luna Buffer Structure for Fiber Optic Gyro- Ferreyrol , Timothy C. Ralph , Geoff J. Pryde ; Griffith rez , Codey Nacke , Nathan John Carlson , Lambert Giner , 1 1 1 2 2 1 1 Washington, USA. Scanning fiber endoscopy with new scope, Song Jingming , Weile Li , Cai Wei , Wenyong Luo , Univ., Australia; Laboratoire Photonique, Institut d’Optique, Jeff S. Lundeen ; Univ. of Ottawa, Canada. We present a 2 1 2 3 technologies and forward-viewing applications are discussed. Wei Li ; Beihang Univ., China; FiberHome Telecommunica- France; School of Mathematics and Physics, Univ. of variable partially-polarizing beamsplitter that allows for the tion Technologies CO., Ltd, China. A kind of mechanical Queensland, Australia. We report the first demonstration complete and independent control of the horizontal and robust photonic crystal fiber with dual luna buffer structure of a quantum Fredkin gate using linear optics. In addition vertical polarization splitting ratios. It is based on a Sagnac for fiber optic gyroscope (FOG) is proposed, which offers a to excellent performance in the logical basis, the gate can interferometer and two liquid crystal cells. new possibility to further optimize the condition character- generate high-fidelity GHZ states and is used in small-scale istics of FOG. algorithms.

FF1B.4 • 09:15 Tutorial FF1C.4 • 09:15 FF1D.4 • 09:15 3D Shape Sensing using Optical Fiber, Brian Soller, Luna Detection-loophole-free heralded quantum steering over a Spectral Compression of Single Photon Wavepackets Innovations, Inc., USA. 3D shape sensing using optical fibers high-loss quantum channel, Sergei Slussarenko1, Morgan M. by an Electro-optic Time Lens, Michal Jachura1,2, Michal is discussed. Weston1, Helen M. Chrzanowski1,2, Sabine Wollmann1, Geoff Karpinski1,2, Brian J. Smith2,3; 1Department of Physics, Univ. J. Pryde1; 1Griffith Univ., Australia; 2Clarendon Laboratory, of Warsaw, Poland; 2Clarendon Laboratory, Univ. of Oxford, Univ. of Oxford, UK. We demonstrate a single step quantum UK; 3Department of Physics, Univ. of Oregon, USA. We relay, allowing quantum steering for verifying entanglement demonstrate sixfold spectral bandwidth compression of a between distant parties with detection loophole closed even single photon by employing electro-optic time lens. The in the presence of very high channel loss. device increases photon flux through a narrowband spectral feature, making a key step in developement of hybrid quantum networks.

Biography: Dr. Soller joined the executive team as Vice President in April 2014. Prior to joining Luna he served as Vice President of Marketing for Micron Optics & VP of global sales and business development for Lightpath Technologies. Previously he spent ten years in fiber optics with Luna, be- Join the conversation. ginning as a scientist and ultimately moving up through the organization to General Manager of the Products Division. Follow @Opticalsociety on Twitter. Dr. Soller co-developed the instrumentation for fiber optic Use hashtag #FIO16 devices manufactured by Luna today. He has over 15 issued patents in optics with an expertise in the interferometric and #OSA100 Friday, 21 October Friday, measurement field. He received a bachelor’s and master’s degree in mathematics and physics from the University of Wisconsin– La Crosse, and a doctoral degree from the Institute of Optics, University of Rochester.

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FF1E • Symposium on Integrated FF1F • Strongly Confined FF1G • Wavefront Sensing and FF1H • General Optical LF1I • Nanophotonics II— Photonic Manufacturing I— Nanoscale Waveguides, Photonic Phase Retrieval—Continued Sciences I—Continued Continued Continued Crystals and Resonator Devices— Continued FF1F.3 • 08:45 FF1G.3 • 08:45 FF1H.4 • 08:45 Highly Directional Radiation from Photonic Transmission of Individual Optical Signals Flat, High Power VUV (hν ≈ 7.2 eV) Lamp Crystal Slabs, Hengyun Zhou1, Bo Zhen1,2, Chia through a Multimode Fiber Using Digital Tiles Comprising Large Arrays of Microcav- Wei Hsu3, Owen Miller1, Steven G. Johnson1, Optical Phase Conjugation, Lars Buettner1, ity Plasmas, Sung-Jin Park1,2, Cyrus Herring2, John Joannopoulos1, Marin Soljacic1;1MIT, Daniel Haufe1, Nektarios Koukourakis1, Jürgen James G. Eden1,2;1Univ of Illinois at Urbana- USA; 2Technion, Israel; 3Yale Univ., USA. We Czarske1; 1Technische Universität Dresden, Ger- Champaign, USA; 2Eden Park Illumination, Inc., develop a general temporal coupled-mode many. Transmission through a multimode fiber is USA. Flat lamps generating more than 20 W of theory formalism to derive bounds on the demonstrated using phase conjugation. Using average power in the vacuum ultraviolet with an asymmetric radiation from a photonic crystal multiple windows of a spatial light modulator efficiency above 10% have been realized. These slab for arbitrary geometries and wavevectors, allows asynchronous imaging through the fiber. narrowband lamps produce > 500 W of peak and present designs with asymmetry ratios Potential for optogenetics and communications power in ~100 ns FWHM pulses at a repetition exceeding 104. engineering is outlined. frequency up to 135 kHz.

FF1E.3 • 09:00 Invited FF1F.4 • 09:00 Invited FF1G.4 • 09:00 FF1H.5 • 09:00 LF1I.3 • 09:00 Invited Providing Silicon-Photonic Transceivers Diamond Photonics, Marko Loncar1; 1Har- Wide-Field Imaging Interferometer Testbed An Orbiting Laserport for Low Mass Sailcraft Combinatorial Optimization with Coherent 1 1 1 with an Efficient Laser Source: Where does vard Univ., USA. I will review advances in Phase Retrieval, Alexander S. Iacchetta , James Propulsion, Grover A. Swartzlander ; Rochester Ising Machines based on Degenerate Optical 1 2 “III-V/Silicon Heterogeneous Integration” nanotechnology that have enabled fabrication R. Fienup , David T. Leisawitz , Matthew R. Bol- Inst. of Technology, USA. Navigating a sailcraft Parametric Oscillators, Yoshihisa Yamamoto2,1, 2 1 2 Stand?, Sylvie Menzo1; 1CEA-LETI, France. of nanoscale optical devices in diamond, as car ; Univ. of Rochester, USA; NASA Goddard by means of lasers on an orbiting “laserport” Peter McMahon1; 1Stanford Univ., USA; 2Japan Packaging of finished III-V-chips (SOAs and DFB well as discuss the applications of diamond Space Flight Center, USA. We discuss the results afford an opportunity to launch hundreds of Science and Technology Agency, Japan. The Lasers) is the strategy adopted for providing photonic platform in nonlinear and quantum of an experiment to recover system aberrations miniaturized kilogram scale science packages basic concept, principle and implementation of Si-Photonic-transceivers with a laser source. nanophotonics, optomechanics, and high- from Wide-field Imaging Interferometer Testbed to Mars and other Earth neighbors. coherent Ising machines are presented. A fully With the capability for increased integration power optics. images. We model the system with a unifying programmable 100 spin machine with all-to-all and reduced cost, where does heterogeneous- wavefront for all wavelengths, allowing slowly connections solves ground states and randomly integration stand? varying axial chromatic aberrations. samples low-energy excited states of NP-hard Ising problems. FF1G.5 • 09:15 FF1H.6 • 09:15 Towards Wavefront Sensing with Metamateri- Withdrawn. als, Brian Vohnsen1, Denise Valente1, Rucha A. Deshpande2, Anders Pors2, Sergey Bozhevol- nyi2; 1Univ. College Dublin, Ireland;2Department of Technology and Innovation, Univ. of Southern Denmark, Denmark. Rapid phase variations caused by higher-order aberrations contain information that may not be captured using  standard wavefront sensing techniques. We examine the possibilities for ultradense Thank you for wavefront sensing using nanostructured metamaterials. attending FiO/LS. Friday, 21 October Look for your post-conference survey via email and let us know your thoughts on the program.

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FF1A.4 • 09:30 FF1C.5 • 09:30 FF1D.5 • 09:30 Multispectral Endoscopic Imaging Enabled by Mapping Photon-pair generation and sum-frequency conversion in Demonstration of a Bit-Flip Correction for Enhanced Spectral Bands into the Time Domain, Sarah A. Locknar1, nonlinear dielectric nanoresonators, Alexander S. Solntsev1, Sensitivity Measurements, Lior Cohen1, Yehuda Pilnyak 1, John B. Barton1, Gary E. Carver1; 1Omega Optical, Inc., USA. Luca Carletti2, Lei Xu1, Alexander Poddubny3,4, Costantino Daniel Istrati1, Alex Retzker1, Hagai Eisenberg1; 1Hebrew Univ. Rapid multispectral confocal imaging is performed with a sin- De Angelis2, Giuseppe Leo5, Yuri S. Kivshar1, Dragomir N. of Jerusalem, Israel. Error correction can be used to recover gle shot-limited detector. This approach uses fiber delay lines Neshev1, Andrey A. Sukhorukov1; 1Nonlinear Physics Centre, the sensitivity in a noisy environment. We implement such to map spectral bands into the time domain, and has been Australian National Univ., Australia; 2Department of Informa- correction after a bit-flip error. Our results show 87% recovery integrated with fiber bundles for endoscopic applications. tion Engineering, Univ. of Brescia, Italy; 3ITMO Univ., Russian of the sensitivity, independent of the noise rate. Federation; 4Ioffe Physical-Technical Inst. of the Russian Acad- emy of Science, Russian Federation;5Univ. Diderot-CNRS, France. We predict photon-pair generation with non-classical angular correlations through spontaneous parametric down- conversion in quadratic nonlinear AlGaAs nanoresonators, and establish a quantum-classical correspondence with sum-frequency conversion.

FF1A.5 • 09:45 FF1C.6 • 09:45 FF1D.6 • 09:45 Single-Shot Polarimetry Imaging of Multicore Fi- Measurement of Incompatible Observables via the Weak Values and Balanced Homodyne Detection Work- bers, Miguel A. Alonso1, Siddharth Sivankutty2, Esben Cloning of Quantum States, Rebecca Saaltink1,2, Lambert ing Together, Julian Martinez1, Weitao Liu2, Gerardo Viza1, R. Andresen3, Géraud Bouwmans3, Thomas G. Brown1, Giner1,2, Jeff S. Lundeen1,2; 1Univ. of Ottawa, Canada; 2Max John Howell1; 1Univ. of Rochester, USA; 2National Univ. of Hervé Rigneault2;1Univ. of Rochester, USA; 2Institut Fresnel, Planck Centre for Extreme and Quantum Photonics, Cana- Defense Technology, China. We present a metrological France; 3Université Lille 1, France. We report an experimental da. We experimentally measure a complementary pair of technique which, without discarding of data, resembles a test of single-shot polarimetry to monitor in real time the observables, one on each of two optimally cloned photons. larger anomalous amplification than weak-value-amplification output polarization of multicore fibers. With this technique Just as in a classical version of this procedure, the results give (WVA). The protocol surpasses WVA techniques by amplifying we characterize the Jones matrices of up to 180 fiber cores the original state of the photon. an almost-balanced homodyne signal. simultaneously.

10:00–10:30 Coffee Break, West Corridor and Skyway Lobby (Radisson) Friday, 21 October Friday,

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FF1E.4 • 09:30 Invited FF1F.5 • 09:30 Invited FF1G.6 • 09:30 FF1H.7 • 09:30 LF1I.4 • 09:30 Invited Manufacturing Silicon Photonics for High- Silicon Optomechanical Structures and Coher- Segmented Spherical Space Telescope, Sam- Nonisochronism of Material Vibrations in Title to be Announced, Takashi Yabe1; 1To- 1 2 1 performance Datacom Systems, Keren Berg- ent Microwave-to-optical Converters, Amir uel T. Thurman , Richard Kendrick ; Lockheed Stimulated Raman Scattering, Valeri I. Kova- kyo Inst. of Technology, Japan. Abstract not 2 1,2 1 man1; 1Columbia Univ., USA. Manufacturing Safavi-Naeini1; 1Stanford Univ., USA. In this Martin Coherent Technologies, USA; Lockheed lev ; P.N. Lebedev Physical Inst., Russian available. 2 silicon photonics for high-performance datacom talk I will outline on-going experiments at the Martin Advanced Technology Center, USA.We Federation; National Research Nuclear Univ. systems is discussed. intersection of optomechanics, nonlinear optics, present a space telescope concept based on (MEPhI), Russian Federation. Evidence is found and quantum electromechanics. a spherical primary mirror that is composed of for decrease of the Raman shift in stimulated segments mounted on small satellites that dock Raman scattering with increase of the pump together. The telescope design and an on-orbit intensity. It is shown that in fused silica the alignment approach will be discussed. nonisochronism corresponds to saturation-type nonlinearity of material vibrations.

FF1G.7 • 09:45 FF1H.8 • 09:45 A Water Phase Mask for Optical Encryp- Realization of Gain with Electromagneti- tion Applications, David R. Schipf1, Wei-Chih cally Induced Transparency using Zeeman Wang1,2; 1Univ. of Washington, USA; 2National Sublevels in 87Rb for Gravitational Wave Tsinghua Univ., Taiwan. A new analog optical Detection, Minchuan Zhou1, Zifan Zhou1, Selim encryption scheme is presented that uses Shahriar1; 1Northwestern Univ., USA. We show a parametrically driven shallow fluid as an how to realize a negative dispersion medium oscillating phase mask in the Fourier domain. A using Zeeman sublevels in 87Rb, which pro- simulation of the proposed encryption scheme duces a broad gain with an electromagnetically is presented. induced transparency dip, for enhancing the sensitivity-bandwidth product of a gravitational wave detector.

10:00–10:30 Coffee Break, West Corridor and Skyway Lobby (Radisson) Friday, 21 October

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10:30–12:30 10:30–12:30 10:30–12:30 FF2A • Postdeadline FF2B • Postdeadline Session II FF2C • Postdeadline Session III Session I

Please check the Program Update Sheet for the Postdeadline abstracts.

NOTES ______Friday, 21 October Friday, ______

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10:30–12:30 10:30–12:30 10:30–12:30 10:45–12:30 10:30–12:30 LF2D • General Laser Science I LF2E • General Laser Science II LF2F • Quantum Light Sources II LF2G • General Laser Science III LF2H • High Harmonic Presider: Joanna M. Atkin; Univ. of Presider: Owen Miller; Yale Univ. Presider: TSusumu Noda; Kyoto Presider: Andy Aquila; Stanford Generation II North Carolina-Chapel Hill, USA USA Univ., Japan Univ. USA Presider: Eleftherios Goulielmakis; Max-Planck-Inst. fur Quantenoptik, Germany

LF2D.1 • 10:30 LF2E.1 • 10:30 LF2F.1 • 10:30 Invited LF2G.1 • 10:30 LF2H.1 • 10:30 Invited Ultrafast XANES of Excited State Dy- Brillouin scattering induced transparency Quantum Light From Individual Defects in Withdrawn. Strong Field Physics in the Condensed Matter 1 namics in Vitamin B , and non-reciprocal light storage, 1 1 1 12 Nicholas A. Miller , Chunhua Atomically Thin Semiconductors, Chitraleema Phase, Ch. McDonald ; Thomas Brabec ; Univ. 1 1 2 2 2,1 Roseanne J. Sension ; Univ. of Michigan, Dong , Zhen Shen , Chang-Ling Zou , Yan- Chakraborty1, Kenneth M. Goodfellow1, Sajal of Ottawa, Canada. Recent experiments have 2 2,1 2 1 USA. Ultrafast x-ray and UV-visible transient Lei Zhang , Wei Fu , Guang-Can Guo ; Yale Dhara1, Anthony Yoshimura2, Vincent Meunier2, opened the path to extending attosecond 2 absorption spectroscopies were used to Univ., China; Univ. of Science and Technol- A. Nick Vamivakas1; 1Univ. of Rochester, science from atomic gases to solids. In this characterize the excited state dynamics of ogy of China, China. The Brillouin scattering USA; 2Rensselaer Polytechnic Inst., USA. 2D talk the basic mechanisms driving strong field vitamin B cobalamin compounds. Polarized induced transparency in a high quality 12 materials are being actively investigated for processes in solids, such as ionization and HHG, XANES was used to separate in-plane and out- optical microresonantor is experimentally novel optoelectronic devices. We present will be discussed. of-plane contributions. demonstrated. Due to the phase matching single photon emission from localalized defects condition, the circulating acoustic phonon leads in monolayers of WSe2. We perform optical to non-reciprocal light storage and retrieval. spectroscopy and demonstrate Stark effect in these emitters.

LF2D.2 • 10:45 LF2E.2 • 10:45 LF2G.2 • 10:45 Single-pulse 2D Raman spectroscopy and Controllable Unidirectional Anti-Laser, Hami- Predictability of Optical Rogue Waves in Op- improved coupling analysis using sparsity- dreza Ramezani1,2, Yuan Wang1, Eli Yablo- tically Injected Semiconductor Lasers, Nuria based algorithms, Hadas Frostig1, Tim Bayer1,3, novitch1, Xiang Zhang1; 1Univ. of California, Martinez Alvarez1, Jose Reinoso1, Cristina Nirit Dudovich1, Yonina C. Eldar2; 1Weizmann Berkeley, USA; 2Physics, Univ. of Texas,Rio Masoller1; 1Universitat Politecnica de Catalunya, Inst., Israel; 2Technion, Israel; 3Uni Oldenburg, Grande Valley, USA. We propose controllable Spain. The predictability of ultra-high pulses Germany. We present a single-pulse 2D Raman unidirectional anti-laser in a one dimensional emitted by optically injected semiconductor spectroscopy scheme, which is both simpler coupled cavities where an interplay between lasers is studied by using symbolic time-series than the conventional scheme and rejects Fano resonances and a judicious absorption analysis. Pulse patterns that are likely to occur a strong background signal. We achieve mechanism leads to a unidirectional perfect before the rogue wave are identified. quantitative analysis of the coupling strength absorber. using a sparsity-based signal analysis method.

LF2D.3 • 11:00 LF2E.3 • 11:00 LF2F.2 • 11:00 Invited LF2G.3 • 11:00 LF2H.2 • 11:00 Invited Two-Photon Absorption Spectrum of Flu- Optomechanical nonreciprocity and mag- Coherent Polariton Lasing in a Designable Spatial coherence degradation in high power HHG in Solids: Multi-band Couplings Leading 1 1 orenone-based Molecules, Jessica Dipold , netic-free photonic isolation, Freek Ruesink , Microcavity, Hui Deng1, Seonghoon Kim1, external-cavity diode laser arrays, Mario to Multiple Plateaus, Mette Gaarde1; 1Louisi- 2 1 2 2 1 1 1 Rebeca J. Batista , Ruben D. Fonseca , Daniel Mohammad A. Miri , Andrea Alu , Ewold Ver- Zhaorong Wang1, Bo Zhang1, Sebastian Brod- Niebuhr , Axel Heuer ; Univ. of Potsdam, ana State Univ., USA. We discuss the theory of 3 2 1 1 2 L. Silva , Alfredo M. Simas , Leonardo de hagen ; FOM Inst. AMOLF, Netherlands; Univ. beck2, Christian Schneider2, Martin Kamp2, Germany. The low inter-emitter coherence still HHG in solids, relevant to recent experimental 1 1 1 Boni , Cleber R. Mendonça ; Instituto de of Texas at Austin, USA. Optomechanical Sven Höfling2; 1Univ. of Michigan, USA; 2Univ. excludes efficient diode laser arrays as scalable observations of multiple plateaus in HHG from Física de São Carlos, Brazil; 2Departamento interactions can break optical time-reversal competitors in several high power applications.

of Wuerzberg, Germany. We demonstrate solid argon. A multi-band model explains the Friday, 21 October de Química Fundamental, Universidade Fed- symmetry, allowing non-reciprocal light a single-mode polariton laser with Poisson We present an experimental approach to quickly cutoff energies and relative strengths of the 3 eral de Pernambuco, Brazil; Departamento de transmission. We demonstrate a multimode intensity noise and intrinsic phase coherence measure and better understand these typical different plateaus. Ciências da Natureza, Matemática e Educação, system that breaks Lorentz-reciprocity without using a designable cavity. Strong interactions in coherence properties. Universidade Federal de São Carlos, Brazil. Two- an applied magnetic field, yielding a 10 dB the polariton condensate manifest in Gaussian photon absorption cross-section spectra of 9 optical isolator. dephasing at high condensate densities. Fluorenone composites were measured using the open-aperture Z-Scan technique. Their maxima cross-sections values are between 100-230 GM at 710 nm, which are desired for applications as cellular probes.

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LF2D • General Laser Science I— LF2E • General Laser Science II— LF2F • Quantum Light Sources II— LF2G • General Laser Science III— LF2H • High Harmonic Continued Continued Continued Continued Generation II—Continued

LF2D.4 • 11:15 LF2E.4 • 11:15 LF2G.4 • 11:15 Wide-band-gap semiconductor oxide optical Theory of Loss in a Distributed Feedback Cav- Temporal Superoscillatory Pulse Genera- microcavities, Hongxing Dong1, Yang Liu1, ity-Enhanced Single-Photon SPDC Source, Mi- tion, Hao Chenglong2,1, Hao Li2, Xia Yu2, Ying Zhanghai Chen2, Long Zhang1; 1Shanghai Inst. chael G. Raymer1, Dileep V. Reddy1; 1Univ. of Zhang2, Changyuan Yu3,1, ChengWei Qiu1; 1Na- of Optics and Fine Me, China; 2Fudan Univ., Oregon, USA. A nonlinear-optical waveguide tional Univ. of Singapore, Singapore;2Singapore China. High quality ZnO microstructure optical with distributed optical feedback serves as a Inst. of Manufacturing Technology, Singa- cavities with different morphologies were compact, high-brightness, narrowband SPDC pore; 3The Hong Kong Polytechnic Univ., fabricated by various physical/chemical vapor source if the losses are low enough. A new Hong Kong. We report the design of temporal deposition methods. Optical resonant modes theoretical formalism shows how to include superoscillatory pulse (TSP) generation. were directly observed experimentally. distributed loss in such systems. Theoretical model is analyzed. Simulation shows that a TSP with full width at half maximum (FWHM) is 65% of Fourier transform limited pulse is generated.

LF2D.5 • 11:30 LF2E.5 • 11:30 LF2F.3 • 11:30 Invited LF2G.5 • 11:30 LF2H.3 • 11:30 Invited Phase Mask-Based Superresolution Non- Turning Forbidden Transitions into Dominant Quantum Light on Silicon Photonic Single Longitudinal Mode Green Diode Intense Laser-cluster Interactions in Mid- 1 1 1 linear Microscopy, Ryan Beams , Stephan J. Transitions: Towards Efficient Sources of En- Chips, Qiang Lin1; 1Univ. of Rochester, USA. In Laser, Yi-Hsi Chen , Wei-Chen Lin , Jow-Tsong infrared Wavelengths, Louis F. DiMauro1; 1Ohio 1 1 1 1 2 1 1 Stranick ; National Inst of Standards & Technol- tangled Light, Nicholas Rivera , Ido Kaminer , this talk, we will discuss our recent progress Shy , Hsiang-Chen Chui ; National Cheng State Univ. , USA. High-order harmonic 1 1 2 ogy, USA. We experimentally and theoretically Marin Soljacic ; Massachusetts Inst. of Technol- in developing silicon photonic devices for Kung Univ., Taiwan; National Tsing Hua Univ., generation and electron energy distribution explore various phase-masks for superresolution ogy, USA. We demonstrate that using phonon- producing non-classical light for quantum Taiwan. We observed that a green diode laser are investigated in rare gases from atom to nonlinear microscopy. By engineering the polaritons in thin (quasi-2D) polar dielectrics, photonic applications. shows single longitudinal mode output at nano-scale clusters using intense mid-infrared excitation and collection volumes, we can it is possible to turn forbidden transitions into low operation current, and can be frequency fields. We discuss the size dependence of achieve resolutions of ≈λ/7 for a wide range of dominant transitions, allowing for emitters tuned by adjusting the operation temperature the harmonics and photoelectrons at various nonlinear processes. of entangled light with quantum efficiencies and current. The behavior of laser modes with wavelengths. exceeding 90%. operational current was investigated.

LF2D.6 • 11:45 LF2E.6 • 11:45 LF2G.6 • 11:45 Plasmonic Bowtie Nanoantennas with Nano- Nonlinear Interferometic Plasmonic Sens- Absolute Measurements of the Electronic, crystal Quantum Dots for Single-Photon ing, Emily M. Layden1,2, Tabitha Coulter3, Joseph Rotational, and Rovibrational Optical Non- Source Applications, Svetlana G. Lukishova1, M. Lukens1, Nicholas Peters1, Benjamin Lawrie1, linearity in Gases, Jared K. Wahlstrand1, Sina Dilyana Mihaylova1, Huiqing Zhu1, Andreas Raphael Pooser1; 1Quantum Information Sci- Zahedpour1, Yu-Hsiang Cheng1,2, John Palas- Liapis1,2, Robert W. Boyd1,3; 1Univ. of Roches- ence Group, Oak Ridge National Laboratory, tro1,3, Howard Milchberg1; 1Univ. of Maryland at ter, USA; 2Brookhaven National Laboratory, USA; 2Department of Physics and Astronomy, College Park, USA; 2National Inst. for Standards USA; 3Dept. of Physics and School of Electrical Univ. of Tennessee, USA; 3Department of and Technology, USA; 3Naval Research Labora- Engineering, Univ. of Ottawa, Canada. Photon Physics, Furman Univ., USA. The sensitivity of tory, USA. Absolute, ultrafast measurements of antibunching was observed from CdSeTe plasmonic sensors is limited by photon statistics, the optical nonlinearity in gases are performed nanocrystal quantum dots within gold bowtie which are thermally constrained under typical using spectral interferometry in thin targets. plasmonic nanoantennas. We also showed probe powers. We will demonstrate improved Notably, we are able to isolate the rovibrational polarization selectivity in photoluminescence sensitivity for constant probe power with component of the nonlinearity using resonant of gold bowtie nanoantennas. nonlinear interferometric plasmonic sensors. two-beam coupling. Friday, 21 October Friday,

118 FiO/LS 2016 • 16–21 October 2016 Highland Room A Highland Room B Highland Room C Highland Room D Highland Room E

LF2D • General Laser Science I— LF2E • General Laser Science II— LF2F • Quantum Light Sources II— LF2G • General Laser Science III— Generation II—Continued Continued Continued Continued Continued

LF2D.7 • 12:00 LF2E.7 • 12:00 LF2F.4 • 12:00 Invited LF2G.7 • 12:00 LF2H.4 • 12:00 Invited The Influence of an Electric Field on Revers- Giant Enhancement in Nonlinear Optical- Single Photons from Weakly Nonlinear Pho- Toward BCF on small molecules, Scott E. Gali- Title to be Announced, David A. Reis1; 1Stan- 1 1,2 1 1 1 ible Photodegradation of a Dye-Doped Atomic Magnetometry, Lu Deng , F Zhou , tonic Structures, Vincenzo Savona1, Hugo Flay- ca , Leland Aldridge , Donal Sheets , Edward E. ford Univ., USA. Abstract not available. 1 1 1 1 1 Polymer, Benjamin R. Anderson , Mark G. E.W. Hagley ; National Inst of Standards & ac1; 1Ecole Polytechnique Federale de Lausanne, Eyler ; Univ. of Connecticut , USA. Theoretical 1 1 2 Kuzyk ; Washington State Univ., USA. We Technology, USA; Wuhan Inst. of Physics & Switzerland. It was predicted that a quantum work suggests that the optical bichromatic force generalize the statistical mechanical domain Mathematics, Chinese Academy of Sciences, optical system with arbitrarily weak nonlinearities (BCF) should be an effective method for slowing model of self healing dye-doped polymers to China. We demonstrate a cross-polarization can generate strongly subpoissonian light. I molecular species. We describe this together include the effects of an electric field and find wave-mixing nonlinear atomic magnetometer will review this phenomenon, present recent with progress on experimental application of that it predicts all experimental observations. that results in >500X optical signal signal-to- results, and discuss possible implementations the BCF to the diatomic molecule CaF. noise ratio enhancement with perfect field in photonic platforms. sensitivity preservation and significant reduction of laser power.

LF2D.8 • 12:15 LF2E.8 • 12:15 LF2G.8 • 12:15 Ionization Dynamics in Intense Two-Color White-light laser based on an organo– Radiance Enhancement of Diode Laser Arrays Circularly Polarized Laser Fields, Jan L. Cha- inorganic photonic structure, Yu-Cheng Using Advanced Micro-optics and Passive loupka1, Daniel D. Hickstein2, Christopher A. Hsiao1, Jui-Chieh Huang1, Yu-Ting Lin1, Wei Phase-locking Techniques, Sheldon S. Wu1, Mancuso2, Kevin M. Dorney2, Henry C. Kapteyn2, Lee1; 1National Chiao Tung Univ., Taiwan. This Frank Ravizza1, Raymond J. Beach1, Kurt Cut- Margaret M. Murnane2; 1Department of Physics study demonstrates the lasing modes in ter1, Michael A. Johnson1, William Molander1, and Astronomy, Univ. of Northern Colorado, organo–inorganic photonic (OIP) structure. Mark Rotter1; 1Lawrence Livermore National USA; 2JILA - Department of Physics, Univ. of The OIP is composed of dye-doped cholesteric Laboratory, USA. Significant advancements Colorado and NIST, USA.Ionization in intense liquid crystal and photonic crystals. Through were made in the last decade in area of optical two-color circularly polarized laser pulses is ex- this device, a white-light laser source can be radiance conditioning for laser diode arrays. We plored numerically and experimentally. Double produced. present experimental results on single-bar arrays ionization is enhanced with counterrotating leveraging recent advances in several external- fields, and diverse dynamics are uncovered that cavity phase-locking schemes. are impossible with linear polarization.

12:30–13:30 Lunch Break (on your own) Friday, 21 October

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13:30–15:30 13:30–15:30 13:30–15:30 13:30–15:30 FF3A • Advanced Microscopy Methods and FF3B • Optical Fiber Sensors II FF3C • Quantum Electronics I FF3D • Quantum Optical Measurement and Applications Presider: Jose Luis Santos, Universidade do Presider: Christoph Marquardt; Max-Planck- Quantum Technologies I Presider: Daniel C. Cote, Universite Laval, Porto, Portugal. Inst Physik des Lichts, Germany Presider: Nicolas Treps; Laboratoire Kastler Canada Brossel, France

FF3A.1 • 13:30 Invited FF3B.1 • 13:30 Invited FF3C.1 • 13:30 Invited FF3D.1 • 13:30 Invited High Dynamic Range Imaging in Brain Tissue, Jerome C. Lab-on-Fiber Technology for Biological Sensing Applica- Towards attosecond pulse generation in the X-ray re- New Frontiers in Quantum Optomechanics: From Levita- Mertz1, Rouhui Yang1, Timothy Weber1, Ian Davison1; 1Boston tions, Armando Ricciardi1, Andrea Cusano1; 1Univ. of San- gime, Hanieh Fattahi1, Ferenc Krausz1; 1Max-Planck-Institut tion to Gravitation , Markus Aspelmeyer1; 1Universitat Wien, Univ., USA. An electronic add-on is described that vastly nio, Italy. Lab-on-Fiber technology is an emerging research fur Quantenoptik, Germany. A laser architecture based on Austria. The quantum optical control of levitated massive improves the dynamic range of a multiphoton microscope field envisaging the integration of functionalized materials the frequency synthesis of optical parametric chirped-pulse systems may enable a completely new class of experiments while reducing potential photodamage. The add-on provides and devices with optical fibers, aimed at developing a new amplifiers is demonstrated. The apparatus keeps promise to at the interface between quantum physics and gravity. real-time feedback to regulate the laser power delivered to generation of advanced all-in-fiber probes exploitable for generate multi-TW, high-power, light-transients, presenting the sample. biosensing applications. a new route toward keV attosecond pulses.

FF3A.2 • 14:00 FF3B.2 • 14:00 FF3C.2 • 14:00 FF3D.2 • 14:00 Invited Higher-Order Multiphoton Microscopy of the Beating Integrated FBG Sensor Interrogator in SOI Platform using Holographic Reconstruction of Single Photon Spatial Putting the Photon into Photonics, Andrew G. White1; 1Univ. 1 1 1 1 Mouse Heart Using Resonant Scanning, Jason S. Jones , Passive Phase Demodulation, Yisbel Marin , Tiziano Nannip- Wavefunction, Michal Jachura , Radoslaw Chrapkiewicz , of Queensland, Australia. Realising the disruptive applications 1 1 1 1 1 1 1 1 1 1 David M. Small , Nozomi Nishimura ; Cornell Univ., USA. ieri , Fabrizio Di Pasquale , Claudio Oton ; Scuola Superiore Konrad Banaszek , Wojciech Wasilewski ; Department offered by quantum photonics requires efficient production, Contractile motion and tissue light-scattering properties Sant’Anna, Italy. We present a Fiber Bragg Grating sensor of Physics, Univ. of Warsaw, Poland. We experimentally processing, and detection of single photons. Here we review make in vivo microscopy studies of the heart difficult. We interrogator in silicon-on-insulator (SOI) platform based on show that the complex transversal wavefunction of the significant recent progress in efficient photon generation have developed a microscopy platform that uses 3PE excita- interferometric wavelength-shift detection. A commercial unknown photon can be fully recovered from the spatially- and processing—using quantum-dot systems—and discuss tion and fast acquisition techniques to make this possible. FBG readout unit is used as a reference for validation of resolved coincidence pattern resulting from its two-photon attractive near-term applications. dynamic strain measurement. interference with the reference photon. Friday, 21 October Friday,

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13:30–14:30 13:30–15:30 13:30–15:30 13:30–15:30 13:30–15:30 FF3E • Symposium on Integrated FF3F • Ultrafast Dynamics and FF3G • Polarization Control and FF3H • General Optical Sciences II LF3I • X-ray and XUV III Photonic Manufacturing II Laser Ion Acceleration Measurements Presider: To be Announced Presider: Barry Bruner, Weizmann Presider: Stefan Preble; Rochester Presider: Christian Reimer; NRS_ Presider: Katelynn Sharma; Univ. of Inst. of Science, Israel Inst. of Technology, USA EMT, Canada Rochester, USA

FF3E.1 • 13:30 Invited FF3F.1 • 13:30 Tutorial FF3G.1 • 13:30 Invited FF3H.1 • 13:30 LF3I.1 • 13:30 Invited Silicon Photonics: Applications and High Molecular Dynamics Simulations of Laser-Ma- Propagation-invariant Beams: A Ray-optical Removing Pulse Jitter with Temporal Wave- Influence of the Material Band Structure on 1,2 1,2 Volume Manufacturing Platform, Peter de terials Interactions, Leonid V. Zhigilei1; 1Univ. Perspective, Miguel A. Alonso1; 1Univ. of Roch- guides, Brent Plansinis , Govind P. Agrawal , Attosecond Electron Dynamics in Transition 2 1 Dobbelaere1; 1Luxtera, USA. We start with an of Virginia, USA. In this lecture, the atomistic ester, USA. A ray-based description of beams William R. Donaldson ; Inst. of Optics, Univ. Metals, Zhensheng Tao1, Cong Chen1, Adra 2 introduction on applications of silicon photonics and coarse-grained computational methods whose transverse shape is preserved under of Rochester, USA; Laboratory for Laser carr1, Piotr Matyba1, Tibor Szilvási2, Sebastian in high speed data connectivity and highlight the developed for simulation of laser-materials propagation (e.g. HG, LG, IG, Airy, Mathieu Energetics, Univ. of Rochester, USA. A pair of Emmerich3, Martin Piecuch3, Mark Keller4, advantages compared with other technologies. interactions will be reviewed and the capabilities and Bessel beams) is given, which clarifies their temporal boundaries separated in time acts as Dmitriy Zusin1, Steffen Eich3, Markus Rollinger3, After that we will present our silicon photonics of these methods will be illustrated by the results sometimes strange behavior and shows their the temporal analog of planar waveguides. We Wenjing You1, Stefan Mathias3, Uwe Thumm4, technology platform and how it enables high of recent simulation studies. surprising hidden geometry. show numerically how such a waveguide can Manos Mavrikakis2, Martin Aeschlimann3, Peter volume, high performance manufacturing of be used to remove pulse jitter and synchronize M. Oppeneer5, Henry C. Kapteyn1, Margaret silicon photonics products. Amongst others two pulses. M. Murnane1; 1Univ. of Colorado at Boulder, we will address: wafer manufacturing, device USA; 2Dept. of Chemical and Biological libraries, light source integration, packaging FF3H.2 • 13:45 Engineering, Univ. of Wisconsin-Madison, and assembly. We will illustrate the technology Experimental Demonstration of Reflection USA; 3Dept. of Physics and Research Center OP- with some examples. and Refraction of Optical Pulses from Tempo- TIMAS, Univ. of Kaiserlautern, Germany; 4Dept. 1 ral Boundaries, Bethany J. Little , Brent Plansi- of Physics, Kansas State Univ., USA; 5Dept. of 1 1 1 1 nis , Govind P. Agrawal , John Howell ; Univ. of Physics and Astronomy, Uppsala Univ., Swe- Rochester, USA. We experimentally implement den. We use attosecond pulse trains to directly the proposal of Plansinis et al. [PRL 115, (2015)] measure photoelectron lifetimes in Ni(111) and using slow light in Rb vapor. Time-dependent Cu(111). We observe a strong influence of mate- frequency shifts on probe pulses behave like rial band structure on the measured lifetimes, angles in the analogous spatial reflection and which reveal attosecond timescale electron Biography: Leonid V. Zhigilei studied materials refraction from classical optics. screening and scattering. science at the Leningrad Polytechnic Institute, FF3E.2 • 14:00 Invited Russia, and did is Ph.D. dissertation work on FF3G.2 • 14:00 FF3H.3 • 14:00 LF3I.2 • 14:00 Invited Development of Integrated Photonic Packag- the structure of metallic glasses at Tomsk State Hilbert-Space Analyzers: Basis-Neutral A new waveguiding mechanism based upon Time-Resolved XUV and X-Ray Spectroscopy 2,1 ing Standards and Foundry Capabilities, Peter University and St. Petersburg State University, Modal Analysis via Generalized Optical geometric phase, Alessandro Alberucci , Jisha at the Free-Electron Laser Facility FLASH, Wil- 1 3 5,4 A. O’Brien1; 1Photonics, Tyndall National Inst., Russia (Ph.D. degree 1991). After several years Interferometry, Lane Martin , Walker D. C. Pannian , Sergei Slussarenko , Bruno Pic- fried Wurth1,2; 1Universität Hamburg, Ger- 1 1 5 5 5,6 Ireland. An overview of PIC packaging standards of industrial work in Russia and Lithuania, Larson , Hasan E. Kondakci , Davood Mar- cirillo , Enrico Santamato , Lorenzo Marrucci , many; 2DESY Photon Science, Germany.Recent 2 1 1 2,1 1 and foundry capabilities led by researchers at and postdoctoral work at the Department of dani , Soroush Shabahang , Ali Jahromi , Tanya Gaetano Assanto ; Tampere Univ. of Technol- results from time-resolved spectroscopy studies 3 4 2 2 3 the Tyndall Inst. in collaboration with European Chemistry at the Pennsylvania State University, Malhotra , A. Nick Vamivakas , George Atia , ogy, Finland; Univ. Roma Tre, Italy; Univ. of in the XUV and soft x-ray regime on ultrafast 1 1 4 5 partners will be presented. Details of optical in 2000 he joined the Department of Materials Ayman Abouraddy ; CREOL, Univ. of Central Porto, Portugal; Griffith Univ., Australia; Univ. dynamics in solids and at surfaces obtained at 2 6 and electrical packaging technologies will be Science and Engineering at the University of Florida, USA; Dept. Electrical Engineering and of Naples Federico II, Italy; CNR ISASI, FLASH at DESY in Hamburg will be presented. reviewed. Virginia. His research interests are in the general Computer Science, Univ. of Central Florida, Italy. We demonstrate light guiding in a locally area of computational materials science. Zhigilei USA; 3Department of Physics and Astronomy, twisted anisotropic medium in the absence of a gave more than 80 invited talks and authored Univ. of Rochester, USA; 4Inst. of Optics, Univ. refractive index gradient. The transverse phase more than 100 journal papers that have been of Rochester, USA. We demonstrate a ‘Hilbert- modulation required to compensate diffraction Friday, 21 October cited more than 7000 times (his current h-index space analyzer’ capable of projecting optical is provided by the Pancharatnam-Berry phase. is 44). beams onto any modal basis by exploiting an inherently stable interferometer in which the traditional delay is replaced by optical implementations of fractional transforms.

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FF3A • Advanced Microscopy Methods and FF3B • Optical Fiber Sensors II—Continued FF3C • Quantum Electronics I—Continued FF3D • Quantum Optical Measurement and Applications—Continued Quantum Technologies I—Continued

FF3A.3 • 14:15 FF3B.3 • 14:15 FF3C.3 • 14:15 Disease Modeling in Human Induced Pluripotent Stem A fiber-optic probe based on quantum dots integrated Enhanced Second-Order Optical Nonlinearity in Doped Cell Derived Cardiomyocytes Using High-Throughput All- cavity for temperature sensing, Qi Zhang1, Hai Xiao1, Lei Graphene on a Two-Dimensional Diffraction Grating, Tet- Optical Dynamic Cardiac Electrophysiology, Aleks Klimas1,2, Yuan1; 1Clemson Univ. COMSET, USA. We report a trumpet- suyuki Ochiai1; 1National Inst. for Materials Science, Japan. Yiyang Wu3,4, Christina Ambrosi1,2, Jinzhu Yu2, John Williams2, shape micro-cavity probe based on quantum dots for Doped graphene placed on a diffraction grating can exhibit Harold Bien2, Gholson Lyon3,4, Emilia Entcheva1,2; 1Biomedical temperature sensing. By analyzing the fluorescence signals a strong modulation of graphene plasmon polariton in the Engineering, George Washington Univ., USA;2Biomedical generated from the quantum dots, the temperature of the THz range. We present a theoretical analysis of the enhanced Engineering, Stony Brook Univ., USA; 3Cold Spring Harbor micro-cavity structure could be correlated. second-harmonic generation in doped graphene for plane- Laboratory, USA; 4Department of Molecular Genetics and Mi- wave irradiation. crobiology, Stony Brook Univ., USA. We present an all-optical high-throughput system for phenotyping and monitoring iPSC-CMs, with capabilities for performing personalized cardiotoxicity screening. We demonstrate the system’s utility for characterizing a new disease model in iPSC-CMs.

FF3A.4 • 14:30 FF3B.4 • 14:30 FF3C.4 • 14:30 FF3D.3 • 14:30 Cell Ablation in a Single Plane Illumination Micro- Dual-LSPR based Optical-Fiber Sensor Platform for Linear Amplifier Noise and Which-Path Information, James Overcoming Vacuum Noise: The Unforeseen Benefits of scope, John M. Girkin1, Charlotte Buckley2, Mariana Torres- Multiplexed Biosensing Application, Nirmal S. Punjabi1, D. Franson1, Richard A. Brewster1; 1Univ. of Maryland Balti- Quantum Heterodyne Detection, Christian R. Mueller1,2, Carvalho1, Laura Young1, Sebastien Rider2, Clare McFadden2, Soumyo Mukherji1; 1Indian Inst. of Technology, Bombay, more County, USA. Linear amplifiers are generally assumed Christian Peuntinger1,2, Thomas Dirmeier1,2, Imran Khan1,2, Caroline Berlarge1, Rachel Verdon2, Jonathan Taylor3, John India.Gold and silver nanoparticle decorated LSPR based to add noise that is independent of the signal. We show that Ulrich Vogl1,2, Christoph Marquardt1,2, Gerd Leuchs1,2, Luis Mullins2; 1Physics, Univ. of Durham, UK; 2Queen’s Medical fiber-optic probe has been designed for multiplexing. The which-path information left in the idler mode can produce L. Sánchez-Soto3,1, Yong Siah Teo4, Zdenek Hradil4, Jaroslav Research Inst., Edinburgh Univ., UK; 3Physics, Glasgow Univ., dual nanoparticle coated probe is evaluated for RI sensitivity decoherence effects that cannot be described by that model. Rehacek4; 1Max-Planck-Inst Physik des Lichts, Germany; 2Inst. UK. We have developed a SPIM system with the ability to and multiplexed biosensing is demonstrated. of Optics, Information and Photonics, Univ. of Erlangen- ablate single or groups of cells either through a photo- Nuremberg, Germany; 3Departamento de Óptica, Facultad activated dye or direct cell ablation. Results will be presented de Física, Universidad Complutense, Spain; 4Department of demonstrating cellular ablation in the heart and kidney. Optics, Palacký Univ., Czech Republic. We experimentally demonstrate that heterodyne detection outperforms homodyne tomography for almost all Gaussian states. Our results reveal the operational differences between the theoretically equivalent concepts of Wigner- and Husimi Q-functions.

FF3A.5 • 14:45 FF3B.5 • 14:45 Tutorial FF3C.5 • 14:45 FF3D.4 • 14:45 Fast DMD based super-resolution structured illumination Distributed Vibration Sensing: Principles, Techniques and Center-Of-Mass Interpretation for Bi-Partite Purity Analy- Linear Mode-Mixing of Trapped Ion Motion: can a microscopy, Ming Lei1; 1Xi’an Inst of Optics and Precision Applications, Vincent Handerek1; 1Fotech Solutions Ltd., sis of N-Party Entanglement, Miguel A. Alonso1, Xiao-Feng Hong-Ou-Mandel experiment be performed with pho- Mech, China. We propose an alternative reconstruction UK. This tutorial introduces the fundamental principles of Qian1, Joseph H. Eberly1; 1Univ. of Rochester, USA. We nons?, Kevin A. Marshall1, Daniel F. James1; 1Univ. of Toronto, algorithm based on image recombination transform (IRT), distributed vibration sensing and technical elements that provide a graphical description of multi-party entanglement Canada. We propose a method to manipulate the normal which provides an alternative solution to address this problem have enabled commercial development. Some limitations based on a center-of-mass analogy. This description clarifies modes in a chain of trapped ions using two lasers. The internal even in a weak modulation depth. of the technology and possible ways to overcome them will the existence of entanglement restrictions in the form levels mediate a second-order interaction to construct the also be discussed. of inequalities. Connections with optical polarization are acoustic equivalent of a beam splitter. discussed. Friday, 21 October Friday,

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14:30–15:30 FF3F • Ultrafast Dynamics FF3G • Polarization Control and FF3H • General Optical LF3I • X-ray and XUV III— FF4A • Symposium on Integrated and Laser Ion Acceleration— Measurements—Continued Sciences II—Continued Continued Quantum Optics I Continued Presider: Stefan Preble, Rochester Inst. of Technology, USA FF3F.2 • 14:15 FF3G.3 • 14:15 FF3H.4 • 14:15 Ultrafast Terahertz Scanning Tunneling Probing Spatial Disorder with Light Po- Optical Energy Transfer from Relative Mo- Microscopy with Atomic Resolution, Vedran larization, Claude Amra1,2, Myriam Zerrad3, tion, Alexandra B. Artusio-Glimpse1, Jacob Jelic1, Krzysztof Iwaszczuk2, Peter Nguyen1, Gabriel Soriano3; 1Fresnel Inst., France; 2CNRS, H. Wirth1, Grover A. Swartzlander1; 1Rochester Christopher Rathje3, Graham Hornig1, Haille France; 3Institut Fresnel, Aix-Marseille Univer- Inst. of Technology, USA. By intersecting a Sharum1, James Hoffman1, Mark Freeman1, sité, France. Enpolarization and depolarization moving optical potential, a small particle may Frank Hegmann1; 1Department of Physics, Univ. histograms are calculated and measured gain or loss kinetic energy. We describe this of Alberta, Canada; 2Department of Photonics within different speckle patterns. The results energy transfer for a Gaussian beam gradient Engineering, Technical Univ. of Denmark, Den- are related to the samples microstructures. potential and a Rayleigh particle smaller than mark; 34th Physical Inst., Univ. of Göttingen, Spatial depolarization is investigated in regard the beam radius. Germany. We demonstrate that THz-STM can to temporal enpolarization. probe single atoms on a silicon surface with simultaneous sub-nm and sub-ps resolution. THz-STM is established as a new technique for exploring high-field nonequilibrium tunneling phenomena with single atom precision. FF4A.1 • 14:30 Invited Title to be Announced, Jeremy L. FF3F.3 • 14:30 FF3G.4 • 14:30 FF3H.5 • 14:30 LF3I.3 • 14:30 Invited O’Brien1; 1Univ. of Bristol, UK. Abstract not Study on THz-Radiation-Enhanced Emission of Polarization-sensitive Off-null Measurements Scattering properties of one-dimensional non- Soft X-ray Free Electron Laser Science at available. Fluorescence from plasma in a counter-propa- Applied to Process Monitoring Using Fo- hermitian dispersive heterostructures, Oksana LCLS and Opportunities at LCLS II, William 1 1 1 1 1 gating geometry, Kang Liu , Fabrizio Buccheri , cused Beam Scatterometry, Anthony Vella , V. Shramkova , Konstantinos G. Makris , Giorgos F. Schlotter1; 1Linac Coherent Light Source, 1 1 1 1 1 2 1 Xi-Cheng Zhang ; The Inst. of Optics, Univ. of Stephen Head , Thomas G. Brown , Miguel P. Tsironis , Demetrios Christodoulides ; De- SLAC National Accelerator Laboratory, USA. 1 1 Rochester, USA. We studied THz-Radiation- A. Alonso ; Univ. of Rochester, USA. We partment of physics, CCQCN, Univ. of Crete, The Linac Coherent Light Source (LCLS) is an 2 Enhanced Fluorescence from air plasma with present a scatterometry experiment for the Greece; College of Optics & Photonics- X-ray Free Electron Laser that generates ultrafast THz pulse traveling in the opposite direction simultaneous retrieval of multiple parameters CREOL, Univ. of Central Florida, USA. The x-ray pulses for myriad science experiments. A of the optical excitation pulses. Comparison of a subwavelength structure. The input optical properties of scattering non-Hermitian planned upgrade (LCLS-II) will extend the en- between the co-propagation and the counter- beam is tailored with a spatially varying input systems with material dispersion are examined. ergy range to 25 keV and increase the average propagation geometries is reported. polarization state to enhance the sensitivity of We demonstrate that an on-average lossy intensity by 104. the measurement. heterostructure can amplify an incident plane wave, and analyse the exceptional points of the scattering matrix.

FF3F.4 • 14:45 FF3G.5 • 14:45 FF3H.6 • 14:45 The steering of THz pulses using thin emitters Wavefront-Aberration Correction Using Examination of the nonlinear dynamics and excited by tilted optical pulse-fronts, Bradley Binary Amplitude and Polarization Modula- possible chaos encryption in a zeroth-order Smith1, John Whitaker1, Stephen Rand1; 1Univ. of tion, Yunqi Li1, Christophe Dorrer1; 1Univ. acousto-optic Bragg modulator with feed- Friday, 21 October Michigan, USA. A potentially scalable, efficient, of Rochester, USA. We investigate a simple back, Fares S. Almehmadi1, Monish R. Chat- and rapid method of steering THz pulses method to correct aberrations using binary- terjee2; 1Univ. of Tabuk, Saudi Arabia; 2Univ. of emitted from thin media using optical pulse- amplitude and binary-polarization pupil masks. Dayton, USA. Zeroth-order chaos modulation front tilt is developed theoretically and verified A Cr-on-quartz mask and liquid crystal device in a Bragg cell is examined such that tracking in a proof-of-concept experiment. This method experimentally lead to a significant Strehl ratio problems due to spatial deflections of the can also measure pulse-front tilt. improvement for an aberrated laser beam. first-order AO beam at the receiver may be avoided by switching to the undeviated zeroth- order beam.

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FF3A.6 • 15:00 FF3C.6 • 15:00 FF3D.5 • 15:00 Linking Cellular Disorder Strength and Shear Stiffness us- Novel Single-photon Fringes from Momentum-Correlated Non-linear Optomechanical Measurement in Sliced Pho- ing Quantitative Phase Imaging, William Eldridge1, Brianna Photon Pairs, Mayukh Lahiri2, Armin Hochrainer2, Gabriela tonic Crystal Nanobeams, Rick Leijssen1, Lars Freisem1, Loomis1, Adam Wax1; 1Duke Univ., USA. Quantitative phase Lemos3, Radek Lapkiewicz1, Anton Zeilinger3,2; 1Faculty of Giada La Gala1, Juha Muhonen1, Ewold Verhagen1; 1FOM imaging (QPI) was implemented to image cells before and Physics, Univ. of Warsaw, Poland; 2Faculty of Physics, Univ. Inst. AMOLF, Netherlands. We develop silicon sliced photonic during subjugation of shear flow. Simultaneous evaluation of of Vienna, Austria; 3IQOQI, Austrian Academy of Science, crystal nanobeams with extreme coupling between light and disorder strength and cellular stiffness showed a correlation Austria. We create a novel single-photon fringe pattern motion. We demonstrate that measurements of the nanoscale between the two metrics. using non-degenerate photon pairs. Although one photon thermal motion in these structures enter a new regime, where in each pair is not detected, its wavelength characterizes the the readout is highly non-linear. fringe shift. The fringe visibility depends on the two-photon momentum correlation.

Biography: Vincent Handerek studied electrical engineering at Imperial College London, gaining a B.Sc.(Eng.) in 1975 and FF3A.7 • 15:15 a PhD on polarised light in optical fibres. After researching FF3C.7 • 15:15 FF3D.6 • 15:15 Simultaneous Determination of 3D Orientation and 3D fibre measurements in UK industry, he moved to the USA Directly Measuring the Density Matrix Using Weak Mea- Quantum correlations in measurement-based control Localization in Single Emitter Microscopy Imaging, Miguel to work on polarisation maintaining components and fibre surements, Guillaume S. Thekkadath1, Lambert Giner1, Yamn of a mechanical oscillator, Vivishek Sudhir1, Dalziel Wil- A. Alonso1, Sophie Brasselet2, Thomas G. Brown1; 1Univ. gyroscopes. In 1988, he joined King’s College London, Chalich1, Matthew Horton1, Jash Banker1, Jeff Lundeen1;1Univ. son1, Sergey Fedorov1, Ryan Schilling1, Hendrik Schuetz1, of Rochester, USA; 2Institut Fresnel, France. We present a concentrating on distributed optical fibre sensor research. of Ottawa, Canada. We demonstrate a method to measure Amir Ghadimi1, Andreas Nunnenkamp2, Tobias J. Kip- microscopy technique that encodes molecule orientation In 1999, he returned to industry, developing optical any chosen density matrix element of a quantum system. penberg1; 1Ecole Polytechnique Federale de Lausanne, and fluctuations as well as off-plane displacements into the amplification, communication, and sensing systems. Dr. We determine a photon’s mixed or pure polarization state Switzerland; 2Cambridge Univ., UK. Quantum correlations are PSF, allowing the simultaneous determination of six spatial/ Handerek joined Fotech Solutions Ltd. in 2008 to develop by sequentially weakly measuring three observables, each distilled by feedback on a mechanical oscillator. Feedback directional properties for many molecules simultaneously. distributed acoustic vibration sensing systems. He has complimentary to the last. back-action is observed to destroy these correlations. A authored over 90 publications, three book chapters and a generalized uncertainty relation characterizes this transition range of patents. between efficient and inefficient feedback.

15:30–16:00 Coffee Break, West Corridor and Skyway Lobby (Radisson) Friday, 21 October Friday,

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FF4A • Symposium on Integrated FF3F • Ultrafast Dynamics FF3G • Polarization Control and FF3H • General Optical LF3I • X-ray and XUV III— Quantum Optics I—Continued and Laser Ion Acceleration— Measurements—Continued Sciences II—Continued Continued Continued

FF4A.2 • 15:00 Invited FF3F.5 • 15:00 Invited FF3G.6 • 15:00 FF3H.7 • 15:00 LF3I.4 • 15:00 Invited Quantum information processing with photon Recent advances in laser-driven ion accel- Highly Asymmetric Polarization-Independent Ghost Imaging with Atoms, Roman I. Khaki- Opportunities for Research at the SwissFEL 1 1 temporal modes, Christine Silberhorn1; 1Depar- eration research, Marco Borghesi1; 1Queen’s Near Infrared Light Transmission In An mov ; Research School of Physics and Engineer- Hard X-ray Free Electron Laser, Christopher ment of Physics,, Universitaet Paderborn, Ger- Univ. of Belfast, UK. We will present recent All-Dielectric Photonic Structure, Lukasz J. ing, Australian National Univ., Australia. Here we J. Milne1; 1Paul Scherrer Inst., Switzerland. In 1 1 2 many. We present quantum information coding experimental progress in ion acceleration Zinkiewicz , Michal Nawrot , Jakub Haberko , report the first realisation of ghost imaging of this talk I will present an overview of the design 1 1 based on temporal modes of pulsed quantum driven by ultra-intense laser pulses, including Piotr Wasylczyk ; Faculty of Physics, Univ. of using atoms. The correlated pairs of ultracold of SwissFEL and examples of some of our 2 light with different spectral-temporal shapes. optimization of the established Target Warsaw, Poland; Faculty of Physics and Ap- metastable helium atoms are originating from recent XFEL research, including nonlinear hard These span a high-dimensional Hilbert space Normal Sheath Acceleration process, as plied Computer Science, AGH Univ. of Science two colliding (BECs) to generate the correlated X-ray spectroscopy and time-resolved serial and are ideally suited for efficient quantum well as investigations of Radiation Pressure and Technology, Poland. We designed and atom pairs required for creation of a ghost femtosecond crystallography. information coding in networks. Acceleration. 3D-printed a dielectric structure, exhibiting image. significant difference in transmittance for the opposite incident wave vectors. Measured asymmetry is polarization-independent and spans over 70 nm in the near infrared (780 nm).

FF3G.7 • 15:15 FF3H.8 • 15:15 The Phenomenon of Vector Polyphoto- A liquid of optical vortices in a photonic sea chromism in Polarization-sensitive Materi- of vector waves, Lorenzo De Angelis1, Filippo als, Barbara N. Kilosanidze1, Irakli Chaganava1, Alpeggiani1, Andrea Di Falco2, L. Kuipers1; 1Cen- George Kakauridze1, Luis Oriol2, Milagros ter for Nanophotonics, AMOLF, Nether- Piñol2, Alfonso Martinez-Felipe2; 1Laboratory lands; 2SUPA, School of Physics and Astronomy, of Holographic Recording and Processing of Univ. of St Andrews, UK. Phase singularities arise Information, Georgian Technical Univ., Inst. in scalar random waves, with spatial distribution of Cybernetics, Georgia; 2Faculty of Science., reminiscent of particles in liquids. Supporting Inst. of Materials Science of Aragon (ICMA), near-field experiment with analytical theory Univ. of Zaragoza-CSIC, , Spain. Phenomenon we show how such spatial distribution changes of vector polyphotochromism was observed when considering vector waves. in some high-efficient polarization-sensitive materials dependent on the radiant exposure when material is illuminated with linearly polarized actinic light. The phenomenon has purely vector nature.

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16:00–18:00 16:00–18:00 16:00–18:00 16:00–18:00 FF5A • In-vivo Spectroscopy, Metabolism FF5B • Optical Manipulation, Processing FF5C • Quantum Electronics II FF5D • Quantum Optical Measurement and and Raman and Applications Presider: Nickolas Vamivakas, Univ. of Quantum Technologies II Presider: Jonathan Lovell, SUNY Buffalo, Presider: Shivanand, Purdue Univ., USA Rochester, USA Presider: Paolo Villoresi, Universita degli USA Studi di Padova, Italy

FF5A.1 • 16:00 Invited FF5B.1 • 16:00 FF5C.1 • 16:00 FF5D.1 • 16:00 Invited Integrated Dual-modal Microscope for Imaging of Key Optical Manipulation of Thermally Generated Microbub- Tailoring of Four-Wave Mixing by Ground-State Coher- Title to be Announced, Andreas Wallraff1; 1ETH Zurich, 1 1 1 Metabolic and Vascular Endpoints in Preclinical Cancer bles in a Liquid, Arjun Krishnappa , Ujitha abeywickrema , ence and Resonant Dispersion, Michal Parniak , Adam Switzerland. Abstract not available. 1 2 1 1 1 1 models, Caigang Zhu1, Amy F. Martinez1, Fangyao Hu1, Partha P. Banerjee , Uttam Sinha ; Univ. of Dayton, Electro- Leszczynski , Wojciech Wasilewski ; Faculty of Physics, 2 Martin Li 1, Megan C. Madonna1, Marianne Lee1, Helen Optics, USA; Keck School of Medicine, USA. The behavior Univ. of Warsaw, Poland. Quantum light-atom interface with Murphy1, Nirmala Ramanujam1; 1Biomedical Engineering, of thermally generated microbubbles in the presence of internal frequency conversion facilitating storage of light Duke Univ., USA. We have developed and utilized a wide a weakly focused laser beam is theoretically studied by based on four-wave mixing in atomic vapor is presented. field, high resolution microscope to capture multiple key developing an equivalent force model. Possible applications Phase-matching in the four-wave mixing process is shown metabolic and vascular endpoints to different indolent from of these bubbles are also discussed. to enable subtle control of light emission. metastatic disease.

FF5B.2 • 16:15 FF5C.2 • 16:15 Microkelvin Control of an Optically Levitated Nanoparti- Opto-coherent-electronics in graphene: photocur- cle, Vijay Jain1,2, Felix Tebbenjohanns1, Lukas Novotny1; 1Pho- rent direction switching based on illumination wave- tonics Laboratory, ETH Zürich, Switzerland; 2Physics, Univ. length, Mahbub Alam1,2, Paul L. Voss1,2; 1Georgia Inst. of Rochester, USA. Here, a high-power photodetector is of Technology, France; 2GT-CNRS, UMI 2958, Georgia used in conjunction with parametric feedback in an optical Tech Lorraine, France. Recent plasmonics experiments tweezer trap to cool the center-of-mass motion of a levitated focus light to 10 nm focal spots. We show that with such nanoparticle from room temperature to 145 µK, or n = 21. illumination, electrostatically gated graphene nanoribbon photoconductors produce photocurrents whose direction depends on illumination wavelength.

FF5A.2 • 16:30 Invited FF5B.3 • 16:30 FF5C.3 • 16:30 FF5D.2 • 16:30 Unraveling Tissue Metabolism using Endogenous, Two- Quantifying Defect Densities in Monolayer Graphene Us- Thick-crystal regime in photon pair sources, Alexander Quantum controlled phase shift with a single 4π mir- 1 1 1 1 1 1,2 1,2 1 photon Imaging: Mechanisms and Diagnostic Biomark- ing Near-field Coherence Measurements., Roxana Rezvani Ling , James Grieve , Kadir Durak , Brigitta Septriani ; Cen- ror, Lucas Alber , Martin Fischer , Bharath Srivathsan , 1,2 3 4 1 1,2 1,2 1 ers, Irene Georgakoudi1; 1Tufts Univ., USA. Changes in optical Naraghi , Luiz Gustavo Cançado , Félix Salazar-Bloise , Aris- tre for Quantum Technologies, Singapore. We present a Markus Weber , Markus Sondermann , Gerd Leuchs ; Max 1 1 2 2 metabolic signals related to the intensity, lifetime and spatial tide Dogariu ; Univ. of Central Florida, CREOL, USA; Depart- thorough exploration of photon pair sources built around Planck Inst. for the Science of Light, Germany; Department 3 localization of endogenous fluorescence are associated with ment of Physics, Univ. of Central Florida, USA; Departamento thick crystals, achieving concurrently high brightness and of Physics, Univ. Erlangen-Nürnberg, Germany. We report alterations in specific biosynthetic and bioenergetic cellular de Física,, Universidade Federal de Minas Gerais (UFMG), , efficiency, despite pump beam walk-off. This surprising result on the experimental implementation of a free-space setup 4 pathways, which can serve as diagnostic and therapeutic Brazil; Departamento de Energia y Combustibles, Univer- is important when designing practical sources. for phase shifts controlled by a single ion. We determine the targets. sidad Politécnica de Madrid, Spain. We show that defect phase shift of a weak coherent beam to 2.2°. density in 2D crystalline lattices determines the extent of near- field spatial coherence. Measurements show the relationship between the spatial coherence length of scattered light and that of photo-excited electrons in graphene. Friday, 21 October Friday,

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16:00–17:30 16:00–18:15 16:00–18:00 16:00–18:00 16:00–18:00 FF5E • Symposium on Integrated FF5F • Hybrid Integration FF5G • Beams and Optical FF5H • Exotic States and LF5I • Topological Photonics II Quantum Photonics II Presider: Liang Feng, Caltech, USA Coherence Applications II Presider: Hui Deng; Univ. of Presider: Stefan Preble, Rochester Presider: Miguel Alonso, Univ. of Presider: Greg Gbur, Univ. of North Michigan, USA Inst. of Technology, USA Rochester, USA Carolina at Charlotte, USA

FF5E.1 • 16:00 Invited FF5F.1 • 16:00 Invited FF5G.1 • 16:00 Invited FF5H.1 • 16:00 LF5I.1 • 16:00 Invited Quantum Information Processing Using 3D Hybrid Integration for Silicon Photon- Generation and propagation of a partially Generation of Surface Plasmon Polaritons Topological Cavity QED: Landau Levels in Programmable Silicon Photonic Integrated ics, Jonathan Klamkin1; 1Univ. of California coherent beam, Yangjian Cai1, Lin Liu1, Jiayi with Controlled States of Partial Coher- Curved Space to Microwave Chern Insula- 1 Circuits, Dirk Englund1; 1Massachusetts Inst. of Santa Barbara, USA. A 3D hybrid integration Yu1; 1College of Physics, Optoelectronics and ence, Andreas Norrman , Sergey Ponomaren- tors, Jonathan Simon1; 1Univ. of Chicago, 2 1 1 Technology, USA. Photonic integrated circuits platform for silicon photonics is discussed. This Energy, Soochow Univ., China. Partially coherent ko , Ari Tapio Friberg ; Univ. of Eastern Finland, USA. We demonstrate Landau levels for optical 2 (PICs) provide a stable, compact, and potentially platform merges indium phosphide and silicon beams with prescribed correlation function, Finland; Dalhausie Univ., Canada. We formulate photons in a twisted cavity and explore the scalable architecture for generating, manipulat- photonics in an elegant and effective manner, phase and state of polarization display many a framework to generate polychromatic surface impact of placing these photons in curved ing, and measuring optical quantum states. We providing a path to low cost, high yield, and extraordinary properties. In this talk, we present plasmon polaritons with any states of partial space. We further realize a microwave Chern- describe recent progress on programmable high performance. a review of recent progress on generation and electromagnetic coherence at a metal-air insulator. We conclude with work to mediate silicon PICs for quantum communications and propagation of a partially coherent beam. interface by controlling the correlations of the photon-photon interactions. quantum simulation. exciting stationary or pulsed light beam. FF5H.2 • 16:15 Room temperature exciton polaritons in 1 2 thin WS2 flakes, Liaoxin Sun , Qi Wang , changqing Chen2, Bo Zhang1, Xuechu Shen1, Wei Lu1; 1Shanghai Inst. of Technical Physics, China; 2Wuhan National Laboratory for Op- toelectronics, Huazhong Univ. of Science and Technology,, China. The anti-crossing behavior

of exciton polaritons in WS2 thin layers was spectrally observed. Giant Rabi splitting of ~270 meV for A exciton and ~780 meV for B exciton were obtained from the fitting of the cavity polariton dispersions.

FF5E.2 • 16:30 Invited FF5F.2 • 16:30 FF5G.2 • 16:30 FF5H.3 • 16:30 LF5I.2 • 16:30 Invited Multiplexing of Integrated Single Photon Monolithic High-Index-Contrast Stretchable Optical beam spatial modal analysis using a Generation of path-polarization hyperen- All-dielectric Photonic Topological Insula- 1 1 Sources, Benjamin J. Eggleton1; 1Univ. of Photonics, Hongtao Lin , Lan Li , Yizhong two-path generalized Michelson interferom- tanglement using quasi-phase-matching tors and Metasurfaces, Alexander B. Khani- 1 1 2 1 2 Sydney, Australia. We present recent progress Huang , Junying Li , Carlos Ramos , Laurent eter, Tanya Malhotra , Wesley Farriss , James in quasi-periodic nonlinear photonic crys- kaev1,2; 1City Univ. of New York, USA; 2Gradu- 2 3 2 3 1 1 1 on increasing the probability of heralded single Vivien , Jason Lonergan , Kathleen A. Rich- R. Fienup , Ayman Abouraddy , A. Nick Vami- tal , Chengrui Zhu , Xikun Chen , Linxi Hu , ate Center of the City Univ. of New York, 3 1 1 2 1 2 1 1 photon generation from integrated photonic ardson , Juejun Hu ; Materials Science and vakas ; Department of Physics and Astronomy, Jietai Jing , Guangqiang He ; Shanghai Jiao- USA. Symmetry protected topological phases 2 2 devices through active spatial and temporal Engineering, Massachusetts Inst. of Technology, Univ. of Rochester, USA; Inst. of Optics, Univ. of tong Univ., China; East China Normal Univ., are engineered in all-dielectric metamaterials 2 3 multiplexing. USA; Institut d’Electronique Fondamentale, Rochester, USA; CREOL, The College of Optics China. A compact scheme for the generation in the presence of electromagnetic duality. 3 France; The College of Optics & Photonics, and Photonics, Univ. of Central Florida, USA. A of path-polarization entangled photon pairs is Synthetic gauge field induced by magneto- Univ. of Central Florida, USA. We demonstrated spatial mode-sorting two-path generalized proposed by using a quasi-periodic nonlinear electric coupling gives rise to Dirac-like surface stretchable, high-index-contrast photonic Michelson interferometer based on a fractional photonic crystal to simultaneously accomplish states in two and three dimensions. Friday, 21 October devices monolithically integrated on a PDMS Fourier Transform generalized delay line is four spontaneous parametric down-conversion elastomer substrates. The devices can sustain experimentally implemented. Progress on processes. 42% strain and 3,000 stretching cycles without recovering the phase of the modal coefficients measurable optical performance degradation. will be reported.

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FF5A • In-vivo Spectroscopy, Metabolism FF5B • Optical Manipulation, Processing FF5C • Quantum Electronics II—Continued FF5D • Quantum Optical Measurement and and Raman—Continued and Applications—Continued Quantum Technologies II—Continued

FF5B.4 • 16:45 FF5C.4 • 16:45 FF5D.3 • 16:45 Structural Fire Forensics: Using Optically Active Nanopar- Quantum-Coherence Emergent Self-Organized Criticality Entangled-State Quantum Gates With Directionally Unbi- ticles to Determine a Fire’s Thermal Impulse, Benjamin R. and Nonequilibrium Light Localization, Pankaj K. Jha1, ased Linear-Optical Multiports, Alexander V. Sergienko1, Da- Anderson1, Ray Gunawidjaja1, Natalie J. Gese1, Gediminas Kosmas Tsakmakidis1, Yuan Wang1, Xiang Zhang1; 1Univ. vid S. Simon2, Casey A. Fitzpatrick1; 1Electrical and Computer Markevicius1, Helena Diez-y-Riega1, Hergen Eilers1; 1Washing- of California, Berkeley, USA. We introduce a quantum- Engineering, Boston Univ., USA; 2Physics and Astronomy, ton State Univ., USA. One difficulty in structural fire forensics coherence driven many-body photonic nanostructure, in Stonehill College, USA. The concept of directionally unbiased is accurately determining a fire’s thermal impulse. To address which we observe self-organized phase-transitions to a new optical multiport is introduced, in which photons may reflect this difficulty we develop optically active nanoparticles whose type of non-potential light localization, resilient to dissipation, back out the input direction. It acts as universal Bell-state spectral properties irreversibly change when heated. fluctuations, and nonlinear interactions. processor to implement probabilistic quantum gates acting on state symmetries.

FF5A.3 • 17:00 Invited FF5B.5 • 17:00 FF5C.5 • 17:00 FF5D.4 • 17:00 Raman Spectroscopic Tools for Medical Applications, Nich- Far-field super-resolution recording and reading towards Photo-electron streaking for synchronization of laser High-dimensional quantum cloning of orbital angular 1 3 1 1 1 olas Stone1,2; 1Univ. of Exeter, UK; 2Royal Devon and Exeter petabyte optical discs, Zongsong Gan , Richard Evans , pulses with radiofrequency fields, Thomas Juffmann , momentum qudits, Frederic Bouchard , Robert Fickler , 1,2 1 1 1 1 1 1 1 Hospital, UK. Raman spectroscopy can provide unlabelled Min Gu ; Centre for Microphotonics, Faculty of Science, Brannon B Klopfer , Mark A. Kasevich ; Stanford Univ., Robert W. Boyd , Ebrahim Karimi ; Univ. of Ottawa, Canada. discrimination of early and late malignancies. Various novel Engineering and Technology, Swinburne Univ. of Technology, USA.Synchronization of cavity enhanced RF fields with laser We present high-dimensional quantum cloning of orbital 2 methodologies are being developed for minimally invasive Australia; Artifical-Intelligence Nanophotonics Laboratory, triggered electron pulses is crucial in electron acceleration angular momentum quantum states of light. Moreover, we 3 tissue analysis. Here we demonstrate a novel Raman clini- School of Science, RMIT Univ., Australia; CSIRO, Manufactur- and temporal refocussing. We propose to measure jitter characterize the cloning machine for various dimensions cal toolbox. ing, Australia. To significantly increase the capacity of optical in situ and with femtosecond accuracy based on photo- and by performing full quantum state tomography on the discs for petabyte data storage, we report a dual-beam super- electron streaking. cloned states. resolution approach to break the diffraction limit barrier for both far-field super-resolution data recording and reading.

FF5B.6 • 17:15 FF5C.6 • 17:15 FF5D.5 • 17:15 Ferroelectric nanoparticles tailored for electro-optical and Time ordering in nonlinear interferometers, Enno Giese1, Light-Matter Interactions using a Nanofiber-Segment nano-imaging applications, Olena Zribi1, Yuriy Garbovskiy1, Samuel Lemieux1, Robert Fickler1, Robert W. Boyd1,2; 1Univ. Ring Resonator, Todd B. Pittman1, Daniel E. Jones1, Garrett Anatoliy Glushchenko1; 1Univ of Colorado at Colorado of Ottawa, Canada; 2Univ. of Rochester, USA. In high-gain Hickman1, James D. Franson1; 1Univ. of Maryland Baltimore Springs, USA. We report an implementation of the ball parametric down-conversion the Hamiltonian generating County, USA. We describe work on a nanofiber-based ring milling method to produce stable colloids of ferroelectric light with macroscopic photon numbers is time dependent. resonator that enables strong interactions between the cavity- nanoparticles tailored for electro-optical and nano-imaging We therefore investigate the influence of time ordering enhanced field and atoms near the nanofiber surface. This applications. Optical and ferroelectric properties of the on nonlinear interferometers and the emitted radiation ``all fiber’’ cavity has applications in nonlinear spectroscopy produced colloids are discussed. properties. and quantum optics. Friday, 21 October Friday,

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FF5E • Symposium on Integrated FF5F • Hybrid Integration— FF5G • Beams and Optical FF5H • Exotic States and LF5I • Topological Photonics II— Quantum Photonics II—Continued Continued Coherence—Continued Applications II—Continued Continued

FF5F.3 • 16:45 FF5G.3 • 16:45 FF5H.4 • 16:45 Demonstration of Self-Aligned Flip-Chip Beam shaping under extreme focusing condi- Dispersion Engineering in Whispering Gallery Photonic Assembly with 1.1dB Loss and tions: Generalization of the Richards-Wolf for- Mode Microbubble Resonators, Nicolas N. Ri- >120nm Bandwidth, Tymon Barwicz1, Yves malism, Denis Panneton1, Guillaume St-Onge1, esen1,2, Wen Qi Zhang2, Tanya M. Monro2,1; 1Inst. Martin1, Jae-Woong Nah1, Swetha Kamlapur- Michel Piché1, Simon Thibault1;1Universite Laval, for Photonics and Advanced Sensing (IPAS), kar1, Robert L. Bruce1, Sebastian Engelmann1, Canada. We rigorously model nonparaxial Univ. of Adelaide, Australia; 2Univ. of South Yurii A. Vlasov1; 1IBM TJ Watson Research focusing of electromagnetic beams by arbitrary Australia, Australia. The opportunities for Center, USA. We demonstrate direct flip-chip axisymmetric surfaces such as spheres, ellipses engineering dispersion in whispering gallery assembly of photonic dies with solder-induced and hyperbolae. We consider light’s diffraction microbubbles are explored. Using certain self-alignment to sub-micron accuracy. We find and polarization properties. materials it is shown that dispersion equalization a peak chip-to-chip transmission of -1.1 dB can be realized at interesting wavelengths such with 0.2 dB penalty over the 120 nm spectrum as deep within the visible or mid-infrared. measured.

FF5E.3 • 17:00 Invited FF5F.4 • 17:00 Invited FF5G.4 • 17:00 FF5H.5 • 17:00 LF5I.3 • 17:00 Invited Quantum Nanophotonics: From Inverse III-V-on-silicon Photonic Integrated Cir- Evolution of coherence singularities of beams Vortex beam characterization in terms of New Ideas on Photonic Topological Insula- Design to Implementations, Jelena Vuckovic1, cuits for Optical Communication and Sens- associated with structurally stable Gaussian Hypergeometric-Gaussian modes, Bereneice tors, Miguel Bandres1, Gal Harari1, Yaakov 1 2 1,2 1,2 Konstantinos Lagoudakis1; 1Stanford Univ., ing, Gunther Roelkens1; 1Universiteit Gent, modes, Tatiana Alieva , Eugeny Abramochkin , C. Sephton , Angela Dudley , Andrew Lumer1, Eran Lustig1, Yonatan Plotnik1, Moshe- 1 1 2 1 USA. By exploring the full parameter space Belgium. The integration of III-V sources, Jose A. Rodrigo ; Universidad Complutense Forbes ; CSIR National Laser Centre, South Ishay Cohen1, Rivka Bekenstein1, Mordechai 2 2 in nanophotonics design, one can implement high-speed germanium optical modulators and de Madrid, Spain; Lebedev Physical Inst., Rus- Africa; Physics, Univ. of Witwatersrand, South Segev1; 1Technion Israel Inst. of Technology, structures for studies of new regimes in quantum photodetectors on silicon waveguide circuits, sian Federation. The propagation of partially Africa. Q-plates are commonly used for Israel. Recent progress on photonic topological and nonlinear optics, and for new applications and the co-integration with electronic integrated coherent Schell model beams associated with uncomplicated generation of polarization insulators will be presented, with new ideas in communications, computing, and sensing. circuits will be discussed in this paper. structurally stable Gaussian modes is studied controlled vortex beams. Here we show ranging from topo lasers and photonic using ambiguity function. This allows deriving experimentally that the output is not a pure topological quasicrystals to curved-space topo a simple expression for the cross-correlation vortex but rather a Hypergeometric-Gaussian photonics and effects of disorder on photonic function in near and far field. mode. Results are in good agreement with topological phenomena. theory.

FF5G.5 • 17:15 FF5H.6 • 17:15 Multiple Wavelength Concentric Vortex Op- A Simple Hubbard Model for the Excited tics: λ = 1064 nm and 2090 nm, Wenzhe Li1, States of π Conjugated -acene Molecules, Za- Yuan Li1, Keith Miller1, Eric G. Johnson1; 1Clem- heen S. Sadeq1, John E. Sipe1; 1Physics, son Univ., USA. Using a single concentric vortex Univ. of Toronto, Canada. We investigate the optic to generate vortices with multiplexed 1064 excited states of tetracene, pentacene, and nm and 2090 nm laser sources is studied and hexacene using a truncated Hubbard model; experimentally confirmed. The rotation of the our technique yields reasonable energies and resulting diffracted patterns is also explored. oscillator strengths. We show that the lowest doubly excited state acts like two triplets. Friday, 21 October

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FF5A.4 • 17:30 FF5B.7 • 17:30 FF5C.7 • 17:30 FF5D.6 • 17:30 Identification of Single Human Immune Cells with Wave- Efficiency Enhancement in Organic Solar Cell using Dielec- Theory of Intense-Broadband-Pulse Storage and Re- Ancilla–aided recovery of quantum super–sensitivity 1 1 1 length Modulation Raman Spectroscopy, Mingzhou Chen1, tric Nanoparticles, Vidhi Mann1, Vipul Rastogi1; 1Physics, trieval, Rodrigo Gutiérrez-Cuevas , Joseph H. Eberly ; Univ. diminished by decoherence, Walker D. Larson1, Bahaa E. Naomi McReynolds1, E. C. Campbell1, Michael Mazilu1, Kishan IIT Roorkee, India. We propose to incorporate the dielectric of Rochester, USA. We study the storage and retrieval of Saleh1; 1UCF CREOL, USA. The quantum super-sensitivity Dholakia1, Simon J. Powis1; 1Univ. of St Andrews, UK. We nanoparticles at anode to increase the efficiency of organic intense-broadband pulses in hot atomic gases through of phase esttimation in two-photon interferometery is present a completely label-free optical method, wavelength solar cells. 20% enhancement in efficiency could be achieved analytical and numerical solutions. We show how the spin- diminished by decoherence. We show that this quantum modulation Raman spectroscopy (WMRS), for identifying using the proposed organic solar cell structure. wave can be manipulated and the storage of multiple pulses advantage can be restored by employing an ancillary closely related single human immune cells. can be accommodated. optical mode.

FF5A.5 • 17:45 FF5B.8 • 17:45 FF5C.8 • 17:45 FF5D.7 • 17:45

Rapid detection of HIV1-p24 antigen in human blood Raman spectroscopy of few-layer MoSe2 in wide range Frequency Comb Generation at Near Visible Wavelengths Theoretical Intepretation of Light Storage by Coherent plasma using Raman spectroscopy, Ben O. Otange2, Ron- of temperature, Malgorzata M. Zinkiewicz1, Magda- in a Microbubble Resonator, Yong Yang1, Xuefeng Jiang2, Population Oscillation, Pascal Neveu1, Marie-Aude May- ald Rop2, Julius O. Oyugi3, Zephania Birech1; 1Department lena Grzeszczyk1, Katarzyna Golasa1, Karol Nogajewski2, Sho Kasumie1, Guangming Zhao2, Linhua Xu2, Jonathan nard1, Chitram Banerjee1, Jasleen Lugani1, Etienne Brion1, of Physics, Univ. of Nairobi, Kenya; 2Department of Physics, Adam Babinsk1;1Faculty of Physics, Univ. of Warsaw, Po- Ward1, Lan Yang2, Sile Nic Chormaic1; 1Okinawa Inst of Sci- Fabienne Goldfarb1, Fabien Bretenaker1; 1Laboratoire Aimé Egerton Univ., Kenya; 3Department of medical microbiology, land; 2LNCMI, CNRS-UJF-UPS-INSA, France. We focus on ence & Technology, Japan; 2Washington Univ. , USA. We Cotton, France. We report a theoretical interpretation of an

Univ. of Nairobi, Kenya. Raman spectroscopy together with MoSe2 micro-Raman analysis in wide range of temperature demonstrate frequency comb generation with 14 lines for optical memory based on Coherent Population Oscillation principal component analysis (PCA) has been applied in (4-300 K) for sample- thickness varying: 1 to 4 layers. Results visible wavelengths in a silica microbubble resonator, with a (CPO). We introduce a new quantity superposition of light detecting HIV1-p24 antigen in plasma. PCA distinguished are compared with previously studied excitation resonances Q-factor of 107, via dispersion engineering. The visible wave- and matter that propagates with a controlled group velocity. Raman data of human blood Plasma contaminated with at room temperature in this material. length comb has applications in metrology and bioimaging. HIV1-p24 antigens from plasma without the antigen. Friday, 21 October Friday,

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FF5F.5 • 17:30 FF5G.6 • 17:30 FF5H.7 • 17:30 LF5I.4 • 17:30 Invited InAs quantum dot mode-locked lasers on Tunable Bessel Beam in 2D PPLT Crystal, Dong- Bimodal Phase-Matching in Nonlinear Plas- Robust Transport of Time-Bin Entangled 1 1 monics, 1,2 a Si substrate by Pd-GaAs wafer bond- mei Liu ; Nanjing Univ., USA. We demonstrate Alessandro Salandrino , Kevin P. Photons in a 2D Topological System, Sunil 1 1 2 2 2 ing, Zihao Wang , Stefan F. Preble , Michael the generation of a tunable diffraction-free O’Brien , Taiki Hatakeyama , Yuan Wang , Mittal1, Venkata Vikram Orre1, Mohammad 1,2 1 3 2 1 2 Fanto , Jeffrey A. Steidle , Chi-Sen Lee , Wei Bessel beam from a 2D periodically-poled Xiang Zhang ; Univ. of Kansas, USA; Univ. Hafezi1; 1JQI/IREAP/Department of Electrical 3 1 2 LiTaO crystal. Our observation not only enriches of California, Berkeley, USA. Bimodal phase- Guo ; Rochester Inst. of Technology, USA; Air 3 and Computer Engineering, Univ. of Maryland, 3 Force Research Laboratory, USA; Univ. of Mas- the diffraction-free optics, but also has potential matching exploits the interplay between College Park, USA. We study transport of sachusetts- Lowell, USA. Room temperature applications for photolithography and imaging. nonlinear scattering modes and waveguide entangled photons in a topological system operation of passively mode locked InAs modes to provide perfect phase-matching of of coupled-ring resonators and show that quantum dot lasers integrated on a Si substrate second harmonic generation in hybrid photonic- the edge states could enable robust on-chip are demonstrated by using low-temperature plasmonic waveguides. quantum communication channels. We report palladium-GaAs wafer bonding. on the experimental progress towards this demonstration. FF5F.6 • 17:45 FF5G.7 • 17:45 FF5H.8 • 17:45 Efficient extraction of zero-phonon-line All-Optical Image Recognition Using Meta- Experimental Generation of Attenuation- photons from single nitrogen vacancy materials, Maria Papaioannou1, Eric Plum1, resistant Frozen Waves Inside an Absorbing centers in an integrated GaP-on-diamond Edward T F Rogers1, João Valente1, Nikolay I. Medium, Ahmed Dorrah1, Michel Zamboni- platform, Emma Schmidgall1, Michael Gould1, Zheludev1,2; 1Univ. of Southampton, UK; 2Nan- Rached2, Mo Mojahedi1; 1Univ. of Toronto, Shabnam Dadgostar2, Fariba Hatami2, Kai-Mei yang Technological Univ., Singapore. Coherent Canada; 2Electrical Engineering, State Univ. of Fu1; 1Univ. of Washington, USA; 2Humboldt Univ. interaction of waves on a thin absorbing film Campinas , Brazil. We generate non-diffracting Berlin, Germany. We demonstrate coupling allows performance of ultrafast, low energy beams, known as Frozen Waves (FWs), which of single NV center zero phonon emission to logical functions with two-dimensional images, consist of co-propagating Bessel beams and can integrated GaP-on-diamond waveguides, with adaptive filtering and pattern recognition that maintain a desired longitudinal intensity profile estimated total quantum efficiency values above we demonstrate with a plasmonic metamaterial in absorbing fluids. FWs can be utilized in optical 10% due to Purcell enhancement and efficient absorber. trapping and micromanipulation. coupling between the cavities and waveguides.

FF5F.7 • 18:00 Graphene-based electrostatic control of InAs quantum dots, Laura Kinnischtzke1,2, Kenneth M. Goodfellow3,2, Chitraleema Chakraborty4, Yi- Ming Lai1, Antonio Badolato1, Stefan Fält5, Wer- ner Wegscheider5, A. Nick Vamivakas3,2; 1De- partment of Physics and Astronomy, Univ. of Rochester, USA; 2Center for Coherence and Quantum Optics, Univ. of Rochester, USA; 3Inst. of Optics, Univ. of Rochester, USA; 4Materi- als Science, Univ. of Rochester, USA; 5Solid State Physics Laboratory, ETH Zurich, Swit- zerland. We characterize voltage-dependent photoluminescence from single InAs quantum Friday, 21 October dots gated by graphene. Our device also exhibits a higher photon count rate than devices using thin-metallic films due to graphene’s low absorption.

FiO/LS 2016 • 16–21 October 2016 131 FiO/LS Sessions, Symposia and Invited/Tutorial Speakers by Topic

FiO 1 Optical Design and Instrumentation FW5G.4 • Optical Metrology Systems Spanning the Full Spatial Frequency Spectrum, Dae Wook Kim, Univ. of Arizona, USA, Wednesday, Technical Sessions 17:00–17:30 ...... page 81 FTu1F • Three-Dimensional Optical Structure Design, Fabrication and FTu5A.1 • Human Centric Optical Design Enabling Next Generation Nanopatterning, Tuesday, 08:00–10:00 ...... page 37 Wearable Displays, Bernard Kress, Microsoft Corporation, USA, Tuesday, Subject Index FTu2F • Resolution and Measurement Limits, Tuesday, 10:30–12:00 . . . . . page 43 16:00–16:30 ...... page 52 FTu4A • Tutorial - Bill Casserly, Tuesday, 14:45–15:30 ...... page 48 FTh4C.1 • Nanoparticle and Virus Sensing Enabled by Computational Lensfree FTu5A • Optics in Consumer Electronics, Tuesday, 16:00–17:30 ...... page 52 Imaging, Euan McLeod, Univ. of Arizona, USA, Thursday, 14:00–14:30 . . . . . page 98 FW2C • Biomedical Optics, Wednesday, 10:30–12:00 ...... page 58 FW3H.1 • Tolerance Eigenmode Analysis of Optical Systems, John Rogers, FW2H • Adaptive Optics and Interferometry, Wednesday, 10:30–12:00 . . . page 59 Synopsys, Inc, USA, Wednesday, 13:00–13:30 ...... page 65 FW3H • Optical Design and GRIN Materials, Wednesday, 13:00–14:30 . . . . page 65 FW5G.1 • Optical Fabrication Science & Technology for High Energy Laser FW5G • Optical Fabrication and Metrology, Wednesday, 16:00–18:00 . . . . page 81 Optics, Tayyab Suratwala, Lawrence Livermore National Laboratory, USA, Wednesday, 16:00–16:30 ...... page 81 FW5H • Freeform Design and Metrology, Wednesday, 16:00–18:00 . . . . . page 81 FTu1F.1 • Reconfigurable Photonics Metasurfaces, Nikolay Zheludev, Univ. of FTh4C • Computational Imaging I, Thursday, 14:00–16:00 ...... page 98 Southampton, Nanyang Technological Univ., UK, Tuesday, 08:00–08:30 . . . . page 37 FTh5C • Computational Imaging II, Thursday, 16:30–18:30 ...... page 104 FF1G • Wavefront Sensing and Phase Retrieval, Friday, 08:30–10:00 . . . . page 111 FiO 2 Optical Sciences FF3G • Polarization Control and Measurements, Friday, 13:30–15:30 . . . . page 121 Technical Sessions FF5G • Beams and Optical Coherence, Friday, 16:00–18:00 ...... page 127 FTu1C • Laser-Plasma Acceleration and Photon Sources, Tuesday, Tutorial Speaker 08:00–10:00 ...... page 38 FTu4A.1• Illumination Design for Consumer Electronic Applications, William FTu2C • Laser-Matter Interactions, Tuesday, 10:30–12:00 ...... page 42 Cassarly, Synopsys, Inc, USA, Tuesday, 14:45–15:30 ...... page 48 FTu3C • Ultrafast Sources and Applications, Tuesday, 13:30–15:30 . . . . . page 46 Invited Speakers FTu3F • Optical Properties of Materials, Tuesday, 13:30–15:30 ...... page 47 FF3G.1 • Propagation-invariant Beams: A Ray-optical Perspective, Miguel FTu5B • Laser Material Processing, Tuesday, 16:00–18:00 ...... page 52 Alonso, Univ. of Rochester, USA, Friday, 13:30–14:00 ...... page 121 FTu5C • Frequency Combs and High Harmonic Generation, Tuesday, FW2H.4 • Advances in Adaptive Optics for Microscopy and Nanoscopy, 16:00–18:00 ...... page 52 Martin Booth, Univ. of Oxford, Univ. of Erlangen Nurnberg, UK, Wednesday, FW2E • Exotic States and Applications I, Wednesday, 10:30–12:00 . . . . . page 59 11:15–11:45 ...... page 61 FW5E • Ultrafast Lasers and Applications, Wednesday, 16:00–18:00 . . . . . page 81 FF5G.1 • Generation and propagation of a partially coherent beam, FTh4B • Optical Vortices, Thursday, 14:00–16:00 ...... page 98 Yangjian Cai, Soochow Univ., China, Friday, 16:00–16:30 ...... page 127 FTh5B • Optical Vortices, Polarization and Mode Shaping, Thursday, FW2C.1 • 3D High-definition Wide Field-of-view Optical Coherence Microscopy 16:30–18:30 ...... page 104 Advancing Real-time in-vivo Cellular Imaging, Cristina Canavesi, LighTopTech FF1H • General Optical Sciences I, Friday, 08:00–10:00 ...... page 111 Corp., USA, Wednesday, 10:30–11:00 ...... page 58 FF3F • Ultrafast Dynamics and Laser Ion Acceleration, Friday, FTh5C.1 • Imaging Beyond the Limits: Active Imaging for Enhancing 13:30–15:30 ...... page 121 Resolution, 3D Information, and Indirect Imaging, Marc Christensen, Southern Methodist Univ., USA, Thursday, 16:30–17:00 ...... page 104 FF3H • General Optical Sciences II, Friday, 13:30–15:30 ...... page 121 FTu1F.3 • Inverse Methods and the Design of Subwavelength Scattering FF5B • Optical Manipulation, Processing and Applications, Friday, Elements for Superresolution, Michael Fiddy, Univ of North Carolina at Charlotte, 16:00–18:00 ...... page 126 USA, Tuesday, 08:45–09:15 ...... page 39 FF5H • Exotic States and Applications II, Friday, 16:00–18:00 ...... page 127

132 FiO/LS 2016 • 16–21 October 2016 Tutorial Speakers FTu1C.5 • Staging of Laser-plasma Accelerators, Sven Steinke, Lawrence FTu1C.1• Laser Plasma Acceleration Using the PW-class BELLA Laser, Wim Berkeley National Laboratory, USA, Tuesday, 09:30–10:00 ...... page 40 Leemans, Lawrence Berkeley National Laboratory, USA, Tuesday, Subject Index 08:00–08:45 ...... page 36 FiO 3 Optics in Biology and Medicine FTh4B.1• Spinning Light on the Nanoscale, Natalia Litchinitser, State Univ. Technical Sessions of New York at Buffalo, USA, Thursday, 14:00–16:00 ...... page 98 FW3C • Diffuse Imaging and Optical Properties, Wednesday, 13:00–14:30 . page 64 FTu3C.1• Towards Attosecond Measurement in Complex Molecules and the FW5C • Optical Coherence Tomograpy, Wednesday, 16:00–18:00 ...... page 80 Condensed Phase, Jonathan Marangos, Imperial College London, UK, Tuesday, 13:30–14:15 ...... page 46 FTh4D • Optics Meets Neuroscience I, Thursday, 14:00–16:00 ...... page 98 FW5E.1• High Power Fiber-laser Based High Harmonic Sources for Nanoscale FTh5D • Optics Meets Neuroscience II, Thursday, 16:30–18:30 ...... page 104 Imaging and Spectroscopy, Jan Rothhardt, Helmholtz Inst. Jena, Friedrich-Schiller- FF1A • Imaging and Therapy Inside the Human Body, Friday, Univ. Jena, Germany, Wednesday, 16:00–16:45 ...... page 81 08:00–10:00 ...... page 110 FF3F.1• Molecular Dynamics Simulations of Laser-Materials Interactions, FF3A • Advanced Microscopy Methods and Applications, Friday, Leonid Zhigilei, Univ. of Virginia, USA, Friday, 13:30–14:15 ...... page 121 13:30–15:30 ...... page 120 FF5A • In-vivo Spectroscopy, Metabolism and Raman, Friday, Invited Speakers 16:00–18:00 ...... page 126 FF3F.5 • Recent Advances in Laser-driven Ion Acceleration Research, Marco Borghesi, Queen’s Univ. of Belfast, UK, Friday, 15:00–15:30 ...... page 125 Invited Speakers FTu5C.1 • Attosecond Light Sources in the Water Window, Zenghu Chang, FF1A.2 • Kagome Fiber Based Ultrafast Laser Microsurgery Probes, Adela Univ. of Central Florida, CREOL, USA, Tuesday, 16:00–16:30 ...... page 52 Ben-Yakar, Univ. of Texas at Austin, USA, Friday, 08:30–09:00 ...... page 110 FTu5B.4 • Graphene Oxide Thin Films for Functional Photonic Devices, FTh5D.2 • Parallel Processing in the Visual System, Bart Borghuis, Univ. of Baohua Jia, Swinburne Univ. of Technology, Australia, Tuesday, 17:00–17:30 . . page 54 Louisville, USA, Thursday, 17:00–17:30 ...... page 104 FTu5B.1 • Laser Doping and Texturing of Silicon for Advanced Optoelectronic FW5C.5 • Double-clad Fiber Couplers: Novel Devices for Multimodal Devices, Eric Mazur, Harvard Univ., USA, Tuesday, 16:00–16:30 ...... page 53 Imaging, Caroline Boudoux, Ecole Polytechnique Montreal, Canada, Wednesday, FTu2C.1 • Time-resolved Holographic Imaging of Femtosecond Laser-induced 17:30–18:00 ...... page 84 Damage Process in Dielectric Thin Films, Andrius Melninkaitis, Vilnius Univ. FW3C.2 • Diffuse Optics for Monitoring Bone Healing and Cancer Treatments, Laser Research Center, Lithuania, Tuesday, 10:30–11:00 ...... page 42 Regine Choe, Univ. of Rochester, USA, Wednesday, 13:30–14:00 ...... page 66 FW5E.5 • Prospects for Multi-kJ Plasma Amplifiers, Peter Norreys, Univ. of FTh4D.3 • Imaging Activity in the Spinal Cord, Daniel Cote, Universite Laval, Oxford, STFC Rutherford Appleton Laboratory, UK, Wednesday, Canada, Thursday, 15:00–15:30 ...... page 100 17:30–18:00 ...... page 85 FW3C.1 • Bedside Mapping of Human Brain Function with High Density FTh5B.1 • Towards Chiral Materials Science Based on Optical Vortices Diffuse Optical Tomography, Adam Eggebrecht, Washington Univ. in St Louis, Illumination, Takashige Omatsu, Chiba Univ., Japan, Thursday, USA, Wednesday, 13:00–13:30 ...... page 64 16:30–18:30 ...... page 104 FF5A.2 • Unraveling Tissue Metabolism using Endogenous, Two-photon FTu3C.1 • High-power Femtosecond Thin-disk Oscillators for Mid-infrared Imaging: Mechanisms and Diagnostic Biomarkers, Irene Georgakoudi, Tufts and Extreme Ultraviolet Generation, Oleg Pronin, Max Planck Inst. of Quantum Univ., USA, Friday, 16:30–17:00 ...... page 126 Optics, Germany, Tuesday, 15:00–15:30 ...... page 46 FW5C.2 • Monitoring and Guidance of Arrhythmia Therapy with Optics, FW2E.1 • Exotic States of Light for Microscopy, Monika Ritsch-Marte, Medical Christine Hendon, Columbia Universitry, USA, Wednesday, 16:30–17:00 . . . . page 80 Univ. of Innsbruck, Austria, Wednesday, 10:30–11:00 ...... page 59 FW5C.1 • Live Imaging of Reproductive and Developmental Events in Mouse FTu5C.4 • Cavity-Enhanced Fourier Transform and Vernier Spectroscopy with Model with Optical Coherence Tomography, Irina Larina, Baylor College of Optical Frequency Combs, Lucile Rutkowski, Umeå Univ., Sweden, Tuesday, Medicine, USA, Wednesday, 16:00–16:30 ...... page 80 17:00–17:30 ...... page 54 FF1A.1 • Chemophototherapy with Porphyrin-Phospholipid Liposomes: A FTh4B.5 • Quantum and Classical Properties of Vector Modes, Bereneice Treatment Possibility for Solid Tumors, Jonathan Lovell, SUNY Buffalo, USA, Sephton, Univ. of Witwatersrand, South Africa, Thursday, 14:00–16:00 . . . . page 102 Friday, 08:00–08:30 ...... page 110

FiO/LS 2016 • 16–21 October 2016 133 FTh5D.3 • Imaging Microglia in the Physiological Brain, Anna Majewska, Tutorial Speakers Univ. of Rochester, USA, Thursday, 17:30–18:00 ...... page 106 FTu1I.1 • UV Generation in Silica Fibres, Gilberto Brambilla, Univ. of FF3A.1 • High Dynamic Range Imaging in Brain Tissue, Jerome Mertz, Boston Southampton, The Future Manufacturing Hub, UK, Tuesday, 08:00–08:45 . . . page 37 Univ., USA, Friday, 13:30–14:00 ...... page 120 FTu5I.1 • Polarization Effects in Optical Fibers For Distributed Sensing, FTh4D.1 • Multi Scale Morpho-functional Characterization of Damage and Andrea Galtarossa, Universita degli Studi di Padova, Italy, Tuesday, Rehabilitation After Stroke, Francesco Pavone, European Lab for Non-Linear 16:00–16:45 ...... page 53 Spectroscopy, Italy, Thursday, 14:00–14:30 ...... page 98 FW2F.1 • Recent Advances in Radiation Hardened Fiber-Based Technologies, FF5A.1 • Integrated Dual-modal Microscope for Imaging of Key Metabolic Sylvain Girard, Universite Saint Etienne, USA, Wednesday, 10:30–11:15 . . . . page 59 Subject Index and Vascular Endpoints in Preclinical Cancer Models, Nirmala Ramanujam, FF3B.5 • Distributed Vibration Sensing: Principles, Techniques and Duke Univ., USA, Friday, 16:00–16:30 ...... page 126 Applications, Vincent Handerek, Fotech Solutions Ltd., UK, Friday, FF1A.3 • Scanning Fiber Endoscopy with New Technologies and Forward- 14:45–15:30 ...... page 122 Viewing Applications, Eric Seibel, Univ. of Washington, USA, Friday, FW3B.1 • Quantum-crypto Systems in the Commercial Service Network, 09:00–09:30 ...... page 112 Jeongsik Cho, Univ. of Southampton, UK, Wednesday, 13:00–13:45 ...... page 64 FTh5D.1 • Cone Signals, Adaptive Optics, and the Brain, Lawrence Sincich, FF1B.1 • New Opportunities with, and Future Challenges of, Optical Fiber Univ. of Alabama at Birmingham, USA, Thursday, 16:30–17:00 ...... page 104 Sensor Technology, Jose Luis Santos, Universidade do Porto, Portugal, Friday, FF5A.3 • Raman spectroscopic tools for medical applications., Nicholas Stone, 08:00–08:45 ...... page 110 Univ. of Exeter, Royal Devon and Exeter Hospital, UK, Friday, 17:00–17:30 . . . page 128 FF1B.4 • 3D Shape Sensing using Optical Fiber, Brian Soller, Luna Innovations, FTh4D.2 • Chemical Sectioning: high throughput imaging brain networks Inc., USA, Friday, 09:15–10:00 ...... page 112 ex vivo at synaptic resolution, Shaoqun Zeng, Huazhong Univ of Science & FTh5E.5 • Recent Advances on Fibers for Optical Communications, Benyuan Technology, Wuhan National Lab for Optoelectronics, China, Thursday, Zhu, OFS Laboratories, USA, Thursday, 17:45–18:30 ...... page 107 14:30–15:00 ...... page 98 Invited Speakers FiO 4 Fiber Optics and Optical Communications FW5B.1 • Coherent Beam Combining and Nonlinear Suppression of Multi- Kilowatt All-Fiber Amplifiers, Angel Flores, US Air Force Research Laboratory, Technical Sessions USA, Wednesday, 16:00–16:30 ...... page 80 FTu1I • Novel Light Generation and Manipulation in Fiber Devices I, Tuesday, FTh4E.1 • Advanced Techniques for Digital Nonlinear Compensation in 08:00–10:00 ...... page 37 Multi-carrier Optical Transmission Systems, Fernando Guiomar, Politecnico FTu2I • Novel Fiber Devices, Tuesday, 10:30–12:00 ...... page 43 di Torino, Italy, Thursday, 14:00–14:30 ...... page 99 FTu3I • Novel Light Generation and Manipulation in Fiber Devices II, Tuesday, FTh4E.6 • Ultra-broadband Nonlinear Optical Signal Processing for Optical 13:30–15:30 ...... page 47 Communications, Hao Hu, , Technical Univ. of Denmark, Denmark, Thursday, FTu5I • Novel Light Generation and Manipulation in Fiber Devices III, Tuesday, 15:30–16:00 ...... page 103 16:00–18:00 ...... page 53 FW2F.3 • Miniaturized Interferometric Fiber Optical Gyroscopes for Space FW2B • Quantum Communications I, Wednesday, 10:30–12:00 ...... page 58 Application, Jing Jin, Beihang Univ., China, Wednesday, 11:30–12:00 . . . . . page 63 FW2F • Optical Fibers for Space Projects, Wednesday, 10:30–12:00 . . . . . page 59 FF3B.1 • Lab-on-Fiber Technology for Biological Sensing Applications, FW3B • Quantum Communications II, Wednesday, 13:00–14:15 ...... page 64 Armando Ricciardi, Univ. of Sannio, Italy, Friday, 13:30–14:00 ...... page 120 FW5B • High-Power Fiber Lasers and Beam Combining, Wednesday, FW5B.7 • All-fiber Combining Concepts in the Wavelength Range Around 16:00–18:15 ...... page 80 2 µm, Hakan Sayinc, Laser Zentrum Hannover e.V., Germany, Wednesday, 17:45–18:15 ...... page 84 FTh4E • High-Capacity Optical Communications and Data Centers I, Thursday, 14:00–16:00 ...... page 99 FW2B.1 • The Interplay Between Cryptography and Quantum Technology - Challenges and Opportunities, Rainer Steinwandt, Florida Atlantic Univ., USA, FTh5E • High-Capacity Optical Communications and Data Centers II, Thursday, Wednesday, 10:30–11:00 ...... page 58 16:30–18:30 ...... page 105 FTu3I.1 • The Inviscid Burgers’ Equation in Nonlinear Fiber Optics, Benjamin FF1B • Optical Fiber Sensors I, Friday, 08:00–10:00 ...... page 110 Wetzel, INRS - EMT, Univ. of Sussex, Canada, Tuesday, 13:30–14:00 ...... page 47 FF3B • Optical Fiber Sensors II, Friday, 13:30–15:30 ...... page 120

134 FiO/LS 2016 • 16–21 October 2016 FTh5E.1 • Large-data Center Interconnect: emerging technologies and scaling FTu5D.1 • Mid IR Silicon Photonics, Graham Reed, Univ. of Southampton, UK, challenges, Xiang Zhou, Google, USA, Thursday, 16:30–17:00 ...... page 105 Tuesday, 16:00–16:30 ...... page 52 FF5F.4 • III-V-on-silicon photonic integrated circuits for optical communication Subject Index FiO 5 Integrated Photonics and sensing, Gunther Roelkens, Universiteit Gent, Belgium, Friday, 17:00–17:30 ...... page 129 Technical Sessions FF1F.5 • Silicon Optomechanical Structures and Coherent Microwave-to- FTu1D • Silicon Photonics I, Tuesday, 08:00–10:00 ...... page 36 optical Converters, Amir Safavi-Naeini, Stanford Univ., USA, Friday, FTu2D • Silicon Photonics II, Tuesday, 10:30–12:00 ...... page 42 09:30–10:00 ...... page 115 FTu3D • Plasmonic and Photonic Crystal Devices, Tuesday, 13:30–15:45 . . . page 46 FTu3D.1 • Physical Scaling Laws of Nanophotonics, Volker Sorger, George FTu5D • Mid-Infrared Integrated Photonics, Tuesday, 16:00–17:45 . . . . . page 52 Washington Univ., USA, Tuesday, 13:30–14:00 ...... page 46 FW3E • Plasmonics, Wednesday, 13:00–14:30 ...... page 65 FW3E.2 • Novel Applications of Plasmonic Bowtie Nanoantennas in the FW5D • Integrated Photonics, Wednesday, 16:00–18:00 ...... page 80 Presence of Enhanced Local Heating, Kimani Toussaint, Univ of Illinois at Urbana- FTh4G • Integrated Nonlinear Optics I, Thursday, 14:00–16:00 ...... page 99 Champaign, USA, Wednesday, 13:30–14:00 ...... page 67 FTh5G • Integrated Nonlinear Optics II, Thursday, 16:30–18:30 ...... page 105 FTh5G.1 • Soliton Mode Locking in Optical Microcavities, Kerry Vahala, California Inst. of Technology, USA, Thursday, 16:30–17:00 ...... page 105 FF1F • Strongly Confined Nanoscale Waveguides, Photonic Crystals and Resonator Devices, Friday, 08:00–10:00 ...... page 111 FTu1D.6 • Silicon Photonic Switches for Datacenters, Ming Wu, , Univ. of California Berkeley, USA, Tuesday, 09:30–10:00 ...... page 40 FF5F • Hybrid Integration, Friday, 16:00–18:15 ...... page 127 Invited Speakers FiO 6 Quantum Electronics FF1F.1 • High-Q photonic crystal resonators for nonlinear optics, Alfredo Technical Sessions De Rossi, Thales Research & Technology, Laboratoire de Photonique et de Nanostructures, CNRS UPR 20, France, Friday, 08:00–08:30 ...... page 111 FTu1G • Quantum Effects in Metamaterials, Tuesday, 08:00–10:00 . . . . . page 41 FW5D.1 • Nanophotonics Technology and Applications, Yeshaiahu Fainman, FTu2G • Optics and Photonics of Disordered Systems, Tuesday, Univ. of California, San Diego, USA, Wednesday, 16:00–16:30 ...... page 80 10:30–12:00 ...... page 43 FTh4G.1 • An Unspoofable Ultrafast Silicon Photonic Physical Key, Mark FTu3G • Integrated Quantum Optics, Tuesday, 13:30–15:30 ...... page 47 Foster, Johns Hopkins Univ., USA, Thursday, 14:00–14:30 ...... page 99 FTu5G • Nonlinear Optics in Micro/Nano-Optical Structures I, Tuesday, FW5D.4 • Towards an Integrated Quantum Photonics Platform on GaAs, Sven 16:00–18:00 ...... page 53 Höfling, Univ. of St. Andrew, Germany, Wednesday, 17:00–17:30 ...... page 82 FW3F • Quantum Entanglement, Wednesday, 13:00–14:30 ...... page 65 FF5F.1 • 3D Hybrid Integration for Silicon Photonics, Jonathan Klamkin, FW5F • Nonlinear Optics in Micro/Nano-Optical Structures II, Wednesday, Univ. of California Santa Barbara, USA, Friday, 16:00–16:30 ...... page 127 16:00–18:00 ...... page 81 FTu5D.4 • Antimonid Based Mid-Infrared Detectors and Focal Plane Arrays, FTh4F • Quantum Communication and Networking I, Thursday, Sanjay Krishna, Center for High Technology Materials, USA, Tuesday, 14:00–16:00 ...... page 99 17:00–17:30 ...... page 54 FTh5F • Quantum Communication and Networking II, Thursday, FW3E.1 • Plasmonics - Ultra-Fast Communications at the Microscale, Juerg 16:30–18:30 ...... page 105 Leuthold, ETH Zurich, Switzerland, Wednesday, 13:00–13:30 ...... page 65 FF1C • Quantum Information Processing in Integrated Systems, Friday, FTu1D.1 • Technologies for Next Generation Silicon Photonics, Michal Lipson, 08:00–10:00 ...... page 110 Columbia Univ., USA, Tuesday, 08:00–08:30 ...... page 36 FF1D • Quantum Optical Technologies, Friday, 08:00–10:00 ...... page 110 FF1F.4 • Diamond Photonics, Marko Loncar, Harvard Univ., USA, Friday, FF3C • Quantum Electronics I, Friday, 13:30–15:30 ...... page 120 09:00–09:30 ...... page 113 FF3D • Quantum Optical Measurement and Quantum Technologies I, FTu2D.1 • Single Nanoparticle Detection Using Silicon Nitride Two-Dimensional Friday, 13:30–15:30 ...... page 120 Coupled-Resonator Optical-Waveguides, Andrew Poon, Hong Kong Univ of FF5C • Quantum Electronics II, Friday, 16:00–18:00 ...... page 126 Science & Technology, Hong Kong, Tuesday, 10:30–11:00 ...... page 42 FF5D • Quantum Optical Measurement and Quantum Technologies II, Friday, 16:00–18:00 ...... page 126

FiO/LS 2016 • 16–21 October 2016 135 Invited Speakers FTu5G.1 • Hybrid Silicon Photonic Circuits for Chip-Scale Quantum Optics, FTh4F.1 • Quantum Teleportation across the Calgary Fibre Network, Gabriel Hong Tang, Yale Univ., USA, Tuesday, 16:00–16:30 ...... page 53 Aguilar, Univ. of Calgary, Canada, Thursday, 14:00–14:30 ...... page 99 FTh4F.3 • Quantum Networks with Optical Frequency Combs, Nicolas Treps, FF3D.1 • New Frontiers in Quantum Optomechanics: From Levitation to Laboratoire Kastler Brossel, France, Thursday, 15:00–15:30 ...... page 101 Gravitation, Markus Aspelmeyer, Universitat Wien, Austria, Friday, FTh4F.2 • Interference for Quantum Time-Bin States in Satellite Channels, 13:30–14:00 ...... page 120 Paolo Villoresi, Universita degli Studi di Padova, Italy, Thursday, 14:30–15:00 . . page 99 FF1D.1 • The Promise of Quantum Imaging, Robert Boyd, Univ. of Ottawa, FF5D.1 • Title to be Announced, Andreas Wallraff, ETH Zurich, Switzerland, Canada, Friday, 08:00–08:30 ...... page 110 Friday, 16:00–16:30 ...... page 126 Subject Index FTu2G.1 • Speckle-Based Spectrometers, Hui Cao, Yale Univ., USA, Tuesday, FTu5G.2 • Photonic Quantum Networks, Ian Walmsley, Univ. of Oxford, UK, 10:30–11:00 ...... page 43 Tuesday, 16:30–17:00 ...... page 53 FF3C.1 • Towards Attosecond Pulse Generation in the X-ray Regime, FF3D.2 • Putting the Photon into Photonics, Andrew White, Univ. of Hanieh Fattahi, Max-Planck-Institut fur Quantenoptik, Germany, Friday, Queensland, Australia, Friday, 14:00–14:30 ...... page 120 13:30–14:00 ...... page 120 FW5F.1 • Optical Antenna Spontaneous Emission: How Much Faster Than FTu3G.2 • Hybrid Quantum Information Processing, Akira Furusawa, The Stimulated Emission?, Eli Yablonovitch, Univ. of California Berkeley, USA, Univ. of Tokyo, Japan, Tuesday, 14:00–14:30 ...... page 47 Wednesday, 16:00–16:30 ...... page 81 FW5F.2 • Soliton Kerr Frequency Combs on a Chip, Tobias Kippenberg, FTu1G.1 • Nonlinear Metamaterial Nanophotonics, Anatoly Zayats, King’s Ecole Polytechnique Federale de Lausanne, Switzerland, Wednesday, College London, UK, Tuesday, 08:00–08:30 ...... page 37 16:30–17:00 ...... page 81 FTu1G.5 • Gain optical nonlinearities and non-volatile switching in photonic FTh5F.1 • Nonlinear Light-Matter Interactions in Engineered Optical Media, metamaterials, Nikolay Zheludev, Univ. of Southampton , Nanyang Natalia Litchinitser, State Univ. of New York at Buffalo, USA, Thursday, Technological Univ., UK, Tuesday, 09:30–10:00 ...... page 41 16:30–17:00 ...... page 105 FTh5F.3 • Optical Realisation of Communication Protocols with an Quantitative FiO 7 Vision & Color Quantum Communication Advantage, Norbert Lutkenhaus, Univ. of Waterloo, Technical Sessions Canada, Thursday, 17:30–18:00 ...... page 107 FW2A • Novel Design Concepts for Eye Correction and Vision Simulators I, FTh5F.2 • Practical Continuous Variable QKD in Fiber and Free Space Wednesday, 10:30–12:00 ...... page 58 Systems, Christoph Marquardt, Max Planck Inst. for the Science of Light, Univ. of Erlangen-Nuremberg, Germany, Thursday, 17:00–17:30 ...... page 105 FW3A • Novel Design Concepts for Eye Correction and Vision Simulators II, Wednesday, 13:00–14:30 ...... page 64 FTu1G.2 • Photonic Hyperctystals, Evgenii Narimanov, Purdue Univ., USA, Tuesday, 08:30–09:00 ...... page 37 FW5A • Understanding Myopia Development, Wednesday, 16:00–17:30 . . . page 80 FF1D.2 • First-Photon 3D Imaging with a Single-Pixel Camera, Miles Padgett, FTh4D • Optics Meets Neuroscience I, Thursday, 14:00–16:00 ...... page 98 Univ. of Glasgow, UK, Friday, 08:30–09:00 ...... page 110 FTh4H • Probing Ocular Biomechanics with Imaging Techniques / Novel FTh4D.1 • Multi Scale Morpho-functional Characterization of Damage and Applications of Femtosecond Lasers in Ophthalmology, Thursday, Rehabilitation After Stroke, Francesco Pavone, European Lab for Non-Linear 14:00–16:00 ...... page 99 Spectroscopy, Italy, Thursday, 14:00–14:30 ...... page 98 FTh5D • Optics Meets Neuroscience II, Thursday, 16:30–18:30 ...... page 104 FF1C.2 • Boson Sampling with Continuous Variable Measurements, Timothy Invited Speakers Ralph, Univ. of Queensland, Australia, Friday, 08:30–09:00 ...... page 110 FTh5D.2 • Parallel Processing in the Visual System, Bart Borghuis, Univ. of FF1C.1 • Implementation and certification of Boson Sampling with integrated Louisville, USA, Thursday, 17:00–17:30 ...... page 104 photonics, Fabio Sciarrino, Univ degli Studi di Roma La Sapienza, Italy, Friday, FW3A.1 • SimVis: See-through Simulation of Presbyopic Corrections, Carlos 08:00–08:30 ...... page 110 Dorronsoro, Instituto de Optica - CSIC, Spain, Wednesday, 13:00–13:30 . . . . page 64 FTu3G.1 • Artificial Gauge Fields and Photonic Topological Phenomena, FTh4D.3 • Imaging Activity in the Spinal Cord, Daniel Cote, Universite Laval, Mordechai Segev, Technion Israel Inst. of Technology, Israel, Tuesday, Canada, Thursday, 15:00–15:30 ...... page 100 13:30–14:00 ...... page 47 FTh4H.4 • IRIS – A New Paradigm in Laser Refractive Correction, Jonathan Ellis, Univ. of Rochester, Univ. of Rochester, USA, Thursday, 15:30–16:00 . . . page 103

136 FiO/LS 2016 • 16–21 October 2016 FTh4H.1 • Air-puff Swept-Source Optical Coherence Tomography, Ireneusz LF2D • General Laser Science I, Friday, 10:30–12:30 ...... page 117 Grulkowski, Nicolaus Copernicus Univ., Thursday, 14:00–14:30 ...... page 99 LF2E • General Laser Science II, Friday, 10:30–12:30 ...... page 117 Subject Index FTh4H.3 • Multiphoton Retinal Imaging, Jennifer Hunter, Univ. of Rochester, LF2F • Quantum Light Sources II, Friday, 10:30–12:30 ...... page 117 USA, Thursday, 15:00–15:30 ...... page 101 LF2H • High Harmonic Generation II, Friday, 10:30–12:30 ...... page 117 FTh5D.3 • Imaging Microglia in the Physiological Brain, Anna Majewska, LF2G • General Laser Science III, Friday, 10:45–12:30 ...... page 117 Univ. of Rochester, USA, Thursday, 17:30–18:00 ...... page 106 LF3I • X-ray and XUV III, Friday, 13:30–15:30 ...... page 121 FW5A.2 • Myopia Development in Guinea Pigs, Sally McFadden, Univ. of LF5I • Topological Photonics II, Friday, 16:00–18:00 ...... page 127 Newcastle, Australia, Wednesday, 16:30–17:00 ...... page 80 FW5A.1 • Control of Myopia Progression in Children: Inside and Outside, Invited Speakers Donald Mutti OD PhD, Ohio State Univ. Optometry, USA, Wednesday, LTu2H.1 • Multiphoton interactions in nonlinear optical waveguides, Govind 16:00–16:30 ...... page 80 Agrawal, Univ. of Rochester, USA, Tuesday, 10:30–11:00 ...... page 43 FTh5D.1 • Cone Signals, Adaptive Optics, and the Brain, Lawrence Sincich, LTu5F.4 • Single Particle Imaging at the Linac Coherent Light Source, Andy Univ. of Alabama at Birmingham, USA, Thursday, 16:30–17:00 ...... page 104 Aquila, SLAC, USA, Tuesday, 17:30–18:00 ...... page 55 FW2A.1 • Myopia Control Off-Axis Correction Lenses, Earl Smith, Univ. of LTu3H.4 • Engineering Quantum Emitters for Integrated Quantum Networks, Houston, USA, Wednesday, 10:30–11:00 ...... page 58 Mete Atature, Cambridge Univ., UK, Tuesday, 15:00–15:30 ...... page 49 FW2A.2 • New Technologies to Increase the Range of Vision of Intraocular LTu5H.2 • Nanoscale Characterization and Control of Functional Materials Lenses, Marrie van der Mooren, Abbott Medical Optics Inc., Netherlands, Using Near-field Spectroscopy, Joanna Atkin, Univ. of North Carolina - Chapel Wednesday, 11:00–11:30 ...... page 60 Hill, USA, Tuesday, 16:30–17:00 ...... page 53 FTh4H.2 • Brillouin Microscopy for Ocular Biomechanics, Seok-Hyun Yun, LTu5H.4 • Ultrafast Methods for Investigating Structure and Dynamics of Harvard Medical School and Massachusetts General Hospital, USA, Thursday, Biological Systems, Carlos Baiz, Univ. of Texas at Austin, USA, Tuesday, 14:30–15:00 ...... page 99 17:30–18:00 ...... page 55 FTh4D.2 • Chemical Sectioning: High Throughput Imaging Brain Networks LTu1H.2 • InGaN/GaN Dot-in-Nanowire Lasers on Silicon, Pallab Bhattacharya, ex vivo at Synaptic Resolution, Shaoqun Zeng, Huazhong Univ of Science & Univ. of Michigan, USA, Tuesday, 08:30–09:00 ...... page 37 Technology, Wuhan National Lab for Optoelectronics, China, Thursday, LF2H.1 • Strong Field Physics in the Condensed Matter Phase, Thomas 14:30–15:00 ...... page 98 Brabec, Univ. of Ottawa, Canada, Friday, 10:30–11:00 ...... page 117 LTu1H.1 • Spatial Coherence Engineering of Lasers, Hui Cao, Yale Univ., USA, Laser Science Categories Tuesday, 08:00–08:30 ...... page 37 Technical Sessions LTu5F.2 • Transient Wave Mixing Spectroscopy Using High Order Harmonic LTu1E • Carl E. Anderson Award for Outstanding Doctoral Dissertation Award Attosecond Pulses and Few-cycle NIR Laser, Wei Cao, Lawrence Berkeley Session, Tuesday, 08:00–10:00 ...... page 37 National Laboratory, Univ. of California, USA, Tuesday, 16:30–17:00 ...... page 53 LTu1H • Nanophotonics I, Tuesday, 08:00–10:00 ...... page 37 LF2F.1 • Quantum light from individual defects in atomically thin semiconductors, Chitraleema Chakraborty, Univ. of Rochester, USA, Friday, LTu2H • Multiphoton Effects I, Tuesday, 10:30–11:30 ...... page 43 10:30–11:00 ...... page 117 LTu2E • X-ray and XUV I, Tuesday, 10:30–12:00 ...... page 43 LW3I.3 • Method for Transient Modulation of Refractive Index Under LTu3H • Quantum Light Sources I, Tuesday, 14:00–15:30 ...... page 47 Exposure to High-Power Laser Pulses, Stavros Demos, Univ. of Rochester, LTu5F • X-ray and XUV II, Tuesday, 16:00–18:00 ...... page 53 USA, Wednesday, 14:00–14:30 ...... page 67 LTu5H • Nano-Plasmonics for Spectroscopy, Tuesday, 16:00–18:00 . . . . . page 54 LF2F.2 • Coherent Polariton Lasing in a Designable Microcavity, Hui Deng, LW2I • Integrated Quantum Photonics I, Wednesday, 10:30–12:30 . . . . . page 59 Univ. of Michigan, USA, Friday, 11:00–11:30 ...... page 117 LW3I • Multiphoton Effects II, Wednesday, 13:00–14:30 ...... page 65 LTh5H.2 • Title to be Announced, Shanhui Fan, Stanford Univ., USA, LW5I • Integrated Quantum Photonics II, Wednesday, 16:00–18:00 . . . . . page 81 Thursday, 17:00–17:30 ...... page 105 LTh5H • Topological Photonics I, Thursday, 16:30–18:30 ...... page 105 LF2H.2 • HHG in Solids: Multi-band Couplings Leading to Multiple Plateaus, LTh5I • High Harmonic Generation I, Thursday, 16:30–18:30 ...... page 106 Mette Gaarde, Louisiana State Univ., USA, Friday, 11:00–11:30 ...... page 105 LF1I • Nanophotonics II, Friday, 08:00–10:00 ...... page 111

FiO/LS 2016 • 16–21 October 2016 137 LW2I.2 • Title to be Announced, Alexander Gaeta, Columbia Univ., USA, LF2H.3 • Intense Laser-cluster Interactions in Mid-infrared Wavelengths, Wednesday, 11:00–11:30 ...... page 61 Hyunwook Park, Ohio State Univ. , Friday, 11:30–12:00 ...... page 118 LTh5I.1 • Extreme Ultraviolet Generation in Bulk Solids: Linking Multi-PHz LTu2E.1 • Title to be Announced, Yoann Pertot, ETH Zurich, Switzerland, Electronics and Photonics, Eleftherios Goulielmakis, Max-Planck-Institut fur Tuesday, 10:30–11:00 ...... page 43 Quantenoptik, Germany, Thursday, 16:30–17:00 ...... page 105 LW2I.3 • Experimental Photonic Quantum State Transfer and Self-guided LTu1E.2 • Power-scaling Attosecond Sources Using Universal Scaling Principles Tomography, Alberto Peruzzo, Quantum Photonics Laboratory, Royal Melbourne for Nonlinear Optical Processes in Gases, Christoph Heyl, Lund Univ., Univ. of Inst. of Technology, Australia, Wednesday, 12:00–12:30 ...... page 63 Colorado, Sweden, Tuesday, 08:30–09:00 ...... page 37 LTu5H.1 • Ultrafast Microscopy of Plasmonic Modes of Ag Nanocrystals Subject Index LTu3H.3 • New Types of Artificial Atoms and Molecules for Quantum Grown on Si Substrates, Hrvoje Petek, Univ. of Pittsburgh, USA, Tuesday, Information Technologies, Han Htoon, Los Alamos National Laboratory, USA, 16:00–16:30 ...... page 53 Tuesday, 14:30–15:00 ...... page 49 LW5I.1 • Title to be Announced, Milos Popovic, Univ. of Colorado Boulder, LTh5I.3 • Strong-Field High Harmonic and Sideband Generation in Solids USA, Wednesday, 16:00–16:30 ...... page 81 and Atoms, Ulrich Huttner, Philipps Universitat Marburg, Thursday, LW2I.1 • Quantum Silicon Photonics: Photon Sources and Circuits, Stefan 17:30–18:00 ...... page 107 Preble, Rochester Inst. of Technology, USA, Wednesday, 10:30–11:00 . . . . . page 59 LTu1H.3 • Title to be Announced, Steven Johnson, Massachusetts Inst. of LTu2E.3 • Exploiting the Longitudinal Coherence of FERMI: Coherent Control Technology, USA, Tuesday, 09:00–09:30 ...... page 39 with Multicolor FEL Pulses, Kevin Prince, Elettra Sincrotrone Trieste, Italy, LTu5F.3 • Frontiers of X-ray Science Developed with an XFEL Facility SACLA, Tuesday, 11:30–12:00 ...... page 45 Tetsuo Katayama, Japan Synchrotron Radiation Research Inst. (JASRI), Tuesday, LTh5H.1 • Majorana-like Zero Modes in a Two-dimensional Photonic 17:00–17:30 ...... page 55 Topological Insulator, Mikael Rechtsman, The Pennsylvania State Univ., USA, LF5I.2 • All-dielectric Photonic Topological Insulators and Metasurface, Thursday, 16:30–17:00 ...... page 105 Alexander Khanikaev, City Univ. of New York, Univ. of New York, USA, Friday, LF2H.4 • Title to be Announced, David Reis, Stanford Univ., USA, Friday, 16:30–17:00 ...... page 127 12:00–12:30 ...... page 119 LF2F.3 • Quantum Light on Silicon Photonic Chips, Qiang Lin, Univ. of LF2F.4 • Single Photons from Weakly Nonlinear Photonic Structures, Rochester, USA, Friday, 11:30–12:00 ...... page 118 Vincenzo Savona, Ecole Polytechnique Federale de Lausanne, Switzerland, LTu2E.2 • HHG Generated Soft X-ray Supercontinuum for Absorption Friday, 12:00–12:30 ...... page 119 Spectroscopy, Jonathan Marangos, Imperial College London, UK, Tuesday, LF3I.3 • Soft X-ray Free Electron Laser Science at LCLS and Opportunities 11:00–11:30 ...... page 43 at LCLS II, William Schlotter, SLAC National Accelerator Laboratory, USA, Friday, LW3I.2 • Medical Applications of Mid-IR Fibre Laser Technologies, Giovanni 14:30–15:00 ...... page 123 Milione, NEC Laboratories America Inc, USA, Wednesday, 13:30–14:00 . . . . page 67 LTu3H.1 • Single Defect Centers in Wide-bandgap Materials: Stable, Bright LTh5I.4 • Upper Limits to Near-field Radiative Heat Transfer: Generalizing the and Pure Quantum Light Sources, Tim Schroder, Massachusetts Inst. of Blackbody Concept, Owen Miller, Yale Univ., USA, Thursday, 18:00–18:30 . . page 109 Technology, USA, Tuesday, 14:00–14:30 ...... page 47 LF3I.4 • Opportunities for Research at the SwissFEL Hard X-ray Free LF5I.3 • New Ideas on Photonic Topological Insulators, Mordechai Segev, Electron Laser, Christopher Milne, Paul Scherrer Inst., Switzerland, Friday, Technion Israel Inst. of Technology, Israel, Friday, 17:00–17:30 ...... page 129 15:00–15:30 ...... page 125 LW2I.4 • High Performances Integrated Single Photon Sources, Pascale LTu1E.3 • Quantum Information with Structured Light, Mohammad Senellart, Centre for Nanoscience and Nanotechnology – C2N – CNRS UMR9001, Mirhosseini, California Inst. of Technology, Univ. of Rochester, USA, Tuesday, Site de Marcoussis, Route de Nozay, France, Wednesday, 11:30–12:00 . . . . page 63 09:00–09:30 ...... page 39 LTu2H.2 • An in vivo Two-Photon Fluorescence Approach to Quantify the LF5I.4 • Robust Transport of Time-Bin Entangled Photons in a 2D Blood-Brain Barrier Permeability for Drug Delivery in Brain, Lingyan Shi, Topological System, Sunil Mittal, Univ. of Maryland, College Park, USA, Friday, CUNY City College, USA, Tuesday, 11:00–11:30 ...... page 43 17:30–18:00 ...... page 131 LTh5H.3 • Mixing and Matching Photonic Topological Phases: From Robust LF1I.2 • Recent Progress in Photonic Crystals, Susumu Noda, Kyoto Univ., Delay Lines to Topological Cavities, Gennady Shvets, Univ. of Texas at Austin, Japan, Friday, 08:30–09:00 ...... page 111 Cornell Univ., USA, Thursday, 17:30–18:00 ...... page 107

138 FiO/LS 2016 • 16–21 October 2016 LF5I.1 • Topological Cavity QED: Landau Levels in Curved Space to FTu1B • Symposium on the 50th Anniversary of Low Loss Optical Fibers I, Microwave Chern Insulators, Jonathan Simon, Univ. of Chicago, USA, Tuesday, 08:00–10:00 ...... page 36 Friday, 16:00–16:30 ...... page 127 FTu2B • Symposium on the 50th Anniversary of Low-Loss Optical Fibers II, Subject Index LF1I.1 • Enhanced Lasing Through Tailoring of Photonic Density of States, Tuesday, 10:30–12:00 ...... page 42 Marin Soljacic, Massachusetts Inst. of Technology, USA, Friday, FTu3B • Symposium on the 50th Anniversary of Low-Loss Optical Fibers III, 08:00–08:30 ...... page 111 Tuesday, 13:30–15:30 ...... page 46 LW5I.2 • Nanophotonic Resonators for Quantum Frequency Conversion, FW2G • A Tribute to Steve Jacobs I, Wednesday, 10:30–12:00 ...... page 59 Kartik Srinivasan, National Inst. of Standards and Technology, USA, Wednesday, FW3G • A Tribute to Steve Jacob II, Wednesday, 13:00–14:00 ...... page 65 16:30–17:00 ...... page 81 FW2D • Symposium on Mesoscopic Optics of Disordered Media I, LF3I.1 • Influence of the Material Band Structure on Attosecond Electron Wednesday, 10:30–12:00 ...... page 58 Dynamics in Transition Metals, Zhensheng Tao, Univ. of Colorado at Boulder, FW3D • Symposium on Mesoscopic Optics of Disordered Media II, USA, Friday, 13:30–14:00 ...... page 121 Wednesday, 13:00–14:00 ...... page 64 LW3I.1 • Non-linear Wavelength Extension of Fibre Laser Systems, J. Taylor, FTh4A • Symposium on Mid-Infrared Fiber Sources I, Thursday, Imperial College London, UK, Wednesday, 13:00–13:30 ...... page 65 14:00–16:00 ...... page 98 LW5I.3 • Advances in Silicon Quantum Photonics, Mark Thompson, Univ. of FTh5A • Symposium on Mid-Infrared Fiber Sources II, Thursday, Bristol, USA, Wednesday, 17:00–17:30 ...... page 83 16:30–18:30 ...... page 104 LTh5I.2 • Plasmonic-enhanced High Harmonic Generation from Bulk Silicon, FTh4I • Symposium on 100 Years of Vision at OSA: Most Cited Vision Papers Giulio Vampa, Univ. of Ottawa, Canada, Thursday, 17:00–17:30 ...... page 105 in OSA Journals, Thursday, 14:00–16:00 ...... page 99 LTu1E.1 • Identifying and Using Recollision-based High Harmonics from FF1E • Symposium on Integrated Photonic Manufacturing I, Friday, Bulk Semiconductors, Giulio Vampa, Univ. of Ottawa, Canada, Tuesday, 08:00–10:00 ...... page 111 08:00–08:30 ...... page 37 FF3E • Symposium on Integrated Photonic Manufacturing II, Friday, LTu5F.1 • Shrinking the Synchrotron: Tabletop Extreme Ultraviolet 13:30–14:30 ...... page 121 Absorption of Transition Metal Complexes, Josh Vura-Weis, Department of Chemistry, UIUC, USA, Tuesday, 16:00–16:30 ...... page 53 FF4A • Symposium on Integrated Quantum Optics I, Friday, 14:30–15:30 ...... page 123 LF3I.2 • Time-Resolved XUV and X-Ray Spectroscopy at the Free-Electron Laser Facility FLASH, Wilfried Wurth, Universität Hamburg, DESY Photon Science, FF5E • Symposium on Integrated Quantum Optics II, Friday, Germany, Friday, 14:00–14:30 ...... page 121 16:00–17:30 ...... page 127 LF1I.4 • Title to be Announced, Takashi Yabe, Tokyo Inst. of Technology, Japan, Tutorial Speakers Friday, 09:30–10:00 ...... page 115 FTh4A.3• Mid-infrared Wavelength Conversion in Chalcogenide Optical LF1I.3 • Combinatorial Optimization with Coherent Ising Machines based on Microfibers, Thibaut Sylvestre, CNRS FEMTO-ST Inst., France, Thursday, Degenerate Optical Parametric Oscillators, Yoshihisa Yamamoto, Japan 15:00–15:30 ...... page 100 Science and Technology Agency, Stanford Univ., USA, Friday, 09:00–09:30 . . page 113 Invited Speakers LTh5H.4 • Topological Theory of Disallowed Couplings, Bo Zhen, , MIT, USA, Thursday, 18:00–18:30 ...... page 109 FTh4I.3 • Motion, Early Vision, and the Plenoptic Function, Edward Adelson, Massachusetts Inst. of Technology, USA, Thursday, 15:00–15:30 ...... page 101 Symposia FW3D.1 • Long Range Light Matter Interactions at Hyperbolic Meta Surface, Girish Agarwal, Oklahoma State Univ., USA, Wednesday, 13:00–13:30 . . . . . page 64 Technical Sessions FTh5A.3 • Mid-Infrared Sources for Ultra-Broadband Cavity Enhanced FTu1A • Symposium on 100 Years of Optical Design, Fabrication, Testing, Spectroscopy, Caroline Amiot, Tampere Univ. of Technology, Institut FEMTO-ST, and Instrumentation - A Historical Look Back I, Tuesday, 08:00–10:00 . . . . page 36 Finland, Thursday, 17:30–18:00 ...... page 106 FTu2A • Symposium on 100 Years of Optical Design, Fabrication, Testing, FF1E.2 • Silicon Photonics Platforms: to standardize or to diversify?, Roel G. and Instrumentation - A Historical Look Back II, Tuesday, 10:30–12:00 . . . . page 42 Baets, Ghent Univ., IMEC, Belgium, Friday, 08:30–09:00 ...... page 111 FTu3A • Symposium on 100 Years of Optical Design, Fabrication, Testing, and Instrumentation - A Historical Look Back III, Tuesday, 13:30–14:30 . . . . page 46

FiO/LS 2016 • 16–21 October 2016 139 FTu3B.4 • Back to the Future - Why Boring Old Materials and Designs are the FTu2B.1 • Recent Development in Optical Fibers for High Capacity Transmission Answer to Next Generation Optical Fibers, John Ballato, Clemson Univ., USA, Systems, Ming-Jun Li, Corning Incorporated, USA, Tuesday, 10:30–11:00 . . . page 42 Tuesday, 15:00–15:30 ...... page 48 FF1E.1 • AIM Photonics – Manufacturing Challenges for Photonic Integrated FF1E.4 • Manufacturing Silicon Photonics for High-performance Datacom Circuits, Michael Liehr, AIM Photonics, SUNY Polytechnic Inst., USA, Friday, Systems, Keren Bergman, Columbia Univ., USA, Friday, 09:30–10:00 . . . . . page 115 08:00–08:30 ...... page 111 FTh5A.1 • All-fiber Sources Operating in the Mid-infrared, Martin Bernier, FTu1B.3 • Bell Lab’s Seminal Testing of Optical Fiber Systems: Past, Present Université Laval, Canada, Thursday, 16:30–17:00 ...... page 104 and Future, John MacChesney, John B. MacChesney Optical Materials, USA, FTu1A.3 • Precision Optics and Metrology at Tropel, John Bruning, Corning, Tuesday, 09:00–09:30 ...... page 38 Subject Index USA, Tuesday, 09:00–09:30 ...... page 38 FW2G.2 • Thirty-Five Years of Liquid Crystal Research at LLE: From Laser FW2D.1 • Control of Optical Intensity Distribution inside a Disordered Fusion to Electronic Paper, Kenneth Marshall, Univ. of Rochester, USA, Waveguide, Hui Cao, Yale Univ., USA, Wednesday, 10:30–10:30 ...... page 58 Wednesday, 11:00–11:30 ...... page 61 FF3E.1 • Silicon Photonics: Applications and High Volume Manufacturing FF1E.3 • Providing Silicon-Photonic Transceivers with an Efficient Laser Platform, Peter de Dobbelaere, Luxtera, USA, Friday, 13:30–14:00 . . . . . page 121 Source: Where does “III-V/Silicon Heterogeneous Integration” Stand?, Sylvie FF5E.2 • Multiplexing of Integrated Single Photon Sources, Benjamin Menezo, CEA-LETI, France, Friday, 09:00–09:30 ...... page 113 Eggleton, Univ. of Sydney, Australia, Friday, 16:30–17:00 ...... page 127 FW2D.3 • Open Channels in Scattering Media: See the Light Inside, Allard FF5E.1 • Quantum Information Processing Using Programmable Silicon Mosk, Universiteit Utrecht, Netherlands, Wednesday, 11:00–11:30 ...... page 62 Photonic Integrated Circuits, Dirk Englund, Massachusetts Inst. of Technology, FF4A.1 • Title to be Announced, Jeremy O’Brien, Univ. of Bristol, Friday, USA, Friday, 16:00–16:30 ...... page 127 14:30–15:00 ...... page 123 FTu1B.1 • The Birth of Optical Fiber Communications, Richard Epworth, FF3E.2 • Development of Integrated Photonic Packaging Standards and Retired, UK, Tuesday, 08:00–08:30 ...... page 36 Foundry Capabilities, Peter O’Brien, Tyndall National Inst., Ireland, Friday, FW2D.2 • Wave Control and Holography with Time Transformations, Mathias 14:00–14:30 ...... page 121 Fink, Ecole Sup Physique Chimie Industrielles, France, Wednesday, FTh4I.2 • Visual Sensitivity and Object Recognition, Denis Pelli, New York 10:30–11:00 ...... page 60 Univ., USA, Thursday, 14:30–15:00 ...... page 99 FTu3B.3 • Realizing a Moore’s Law for Fibers, Yoel Fink, Massachusetts Inst. of FTu3B.2 • Transmitting Beyond The Fictitious Nonlinear Capacity Limit, Technology, USA, Tuesday, 14:30–15:00 ...... page 48 Stojan Radic, Univ. of California San Diego, USA, Tuesday, 14:00–14:30 . . . . page 46 FTu1B.4 • Origins of the Erbium-Doped Fiber Amplifier, Randy Giles, Nokia Bell FTu3B.1 • Recent Advances in Microstructured Optical Fibers and their Labs, USA, Tuesday, 09:30–10:00 ...... page 40 Applications, David Richardson, Univ. of Southampton, UK, Tuesday, FTu1A.4 • Optics Goes to the Movies, John Greivenkamp, Univ. of Arizona, USA, 13:30–14:00 ...... page 46 Tuesday, 09:30–10:00 ...... page 40 FW2G.1 • Optical Glass Science – The How and Why We Got Here, Kathleen FTu2B.2 • Advances in Ultra-low Loss Silica Fibers, Takemi Hasegawa, Sumitomo Richardson, Univ. of Central Florida, CREOL, USA, Wednesday, 10:30–11:00 . . page 59 Electric Industries Ltd, Japan, Tuesday, 11:00–11:30 ...... page 42 FTh4A.2 • Generation and Applications of High Average Power Mid-IR FTu1A.1 • Optical Designs of NASA Telescopes, Joseph Howard, NASA Goddard Supercontinuum in Chalcogenide Fibres, Christian Rosenberg Petersen, DTU Space Flight Center, USA, Tuesday, 08:00–08:30 ...... page 36 Fotonik, Technical Univ. of Denmark, Denmark, Thursday, 14:30–15:00 . . . . . page 98 FTh5A.2 • Power Scaling Concepts for Mid-infrared Fibre Lasers Using Fluoride FTh4A.4 • Mid-Infrared Photonics in Healthcare, Angela Seddon, Univ. of Glass, Stuart Jackson, Macquarie Univ., Australia, Thursday, 17:00–17:30 . . . page 104 Nottingham, UK, Thursday, 15:30–16:00 ...... page 102 FTu1B.2 • Glass and Light: Enabling the Information Age, Donald Keck, FTu2A.2 • History of the Center for Optics Manufacturing, John Schoen, Consultant, USA, Tuesday, 08:30–09:00 ...... page 36 Univ. of Rochester, USA, Tuesday, 11:00–11:30 ...... page 42 FTh5A.4 • Mid-IR Ultrafast Fibre Laser Sources, Khanh Kieu, Univ. of Arizona, FTh4A.1 • Highly Nonlinear Fibre for Applications in the Mid-IR, Brandon USA, Thursday, 18:00–18:30 ...... page 108 Shaw, US Naval Research Laboratory, USA, Thursday, 14:00–14:30 ...... page 98 FTu2A.1 • 30 years of mirror making at the Richard F. Caris Mirror Lab, Dae FW3G.2 • Materials Development in Magnetorheological Finishing: The Wook Kim, Univ. of Arizona, USA, Tuesday, 10:30–11:00 ...... page 42 Work of Dr. Stephen Jacobs, Aric Shorey, Corning Incorporated, USA, Wednesday, 13:30–14:00 ...... page 67 FW3G.1 • Nanomechanics in Optical Manufacturing, John Lambropoulos, Univ. of Rochester, USA, Wednesday, 13:00–13:30 ...... page 65

140 FiO/LS 2016 • 16–21 October 2016 FF4A.2 • Quantum Information with Photon Temporal Modes, Christine Silberhorn, Universitaet Paderborn, Germany, Friday, 15:00–15:30 ...... page 125 FTu2A.3 • APOMA: Past & Present, James Sydor, Sydor Optics Inc, Sydor Subject Index Technologies, USA, Tuesday, 11:30–12:00 ...... page 44 FTu2B.3 • High-Capacity Optical Communications – Can we Guess the Future from the Past?, Robert Tkach, Nokia Bell Labs, USA, Tuesday, 11:30–12:00 . . page 44 FW3D.2 • Cellulose Bio-inspired Hierarchical Structures, Silvia Vignolini, Cambridge Univ., UK, Wednesday, 13:30–14:00 ...... page 66 FF5E.3 • Quantum Nanophotonics: From Inverse Design to Implementations, Jelena Vuckovic, Stanford Univ., USA, Friday, 17:00–17:30 ...... page 129 FTh4I.4 • Fourier, Gabor, Reichardt, Hilbert: Guides on the Path to a Model of Human Motion Perception, Andrew Watson, NASA Ames Research Center, USA, Thursday, 15:30–16:00 ...... page 103 FTu3A.2 • Title to be Announced, Edward White, CDGM Glass Company USA, Tuesday, 14:00–14:30 ...... page 46 FTu3A.1 • History of Optics Manufacturing in Rochester, New York, Robert Wiederhold, Optimax Systems Inc, USA, Tuesday, 13:30–14:00 ...... page 46 FTh4I.1 • Emerging Ocular Applications of Wavefront Correction, David Williams, Univ. of Rochester, USA, Thursday, 14:00–14:30 ...... page 99 FTu1A.2 • Short History of Interferometric Optical Metrology, James Wyant, Univ. of Arizona, Coll of Opt Sciences, USA, Tuesday, 08:30–09:00 ...... page 36

FiO/LS 2016 • 16–21 October 2016 141 Key to Authors and Presiders

A Al Menabawy, Sara - JW4A.135 Amphawan, Angela - JTh2A.33, Atature, Mete - LTu3H.4 Bankapur, Aseefhali - JW4A.113 Aadhi, A. - JW4A.8 Alam, M. Zahirul - FTu1G.4 JW4A.33 Atia, George - FF3G.2 Banker, Jash - FF3C.7 Aalto, Antti - FTh5A.3 Alam, Mahbub - FF5C.2 Amra, Claude - FF3G.3, FW5G.3, Atkin, Joanna M. - LF2D, LTu5H.2 Bao, Changjing - FTh4E.3, FTh5G.2 Abaie, Behnam - JTh2A.122, Alanzi, Saud - JW4A.20, JW4A.22, JW4A.59 Austin, D.R. - LTu2E.2 Bao, Chengying - JW4A.150 JTh2A.196 JW4A.23, JW4A.24 Anderson, Benjamin R. - FF5B.4, Autebert, Claire - FTh4F.4 Bao, Xiaoyi - JW4A.14 Abdollahi, Pedram - JTh2A.76 Alarcon, Aixa - FW2A.2 JTh2A.86, JTh2A.90, JTh2A.95, Avendaño-Alejo, Maximino - Bao, Yijun - JW4A.67 Abdolvand, Amir - JTh2A.135 Alayo, Marco I. - JTh2A.156 LF2D.7 JTh2A.28 Barberis Blostein, Pablo - LW5I.4 Abdul Khudus, M.I.M. - FTu1I.1 Albakay, Naji A. - JW4A.2 Anderson, Brian - FW5B.1, FW5B.5 Avendaño-Alejo, Maximino - Barbier, Margaux - FTh5C.6 Abeywickrema, Ujitha - FF5B.1, Alber, Lucas - FF5D.2 Anderson, Matthw - JTh2A.198 JTh2A.74, JW4A.60 Barcelata-Pinzón, Antonio - JTh2A.37 JW4A.86 Alberucci, Alessandro - FF3H.3, Anderson, Stephen - FTu1D.5, Avetisyan, Vardan - JW4A.44 Bares, Amanda - FTh5D.5 Abouraddy, Ayman - FF1H.2, FF3G.2, JW4A.10, JW4A.12 JTh2A.171 Awaji, Yoshinari - FTh4E.5 Bareza, Nestor Jr. - JW4A.103 FF5G.2, FW5H.8, JW4A.100, Aldridge, Leland - LF2G.7 Andersson-Engels, Stefan - JW4A.118 Awan, Kashif M. -JTh2A.179, Barkur, Surekha - JW4A.113 JW4A.101, JW4A.181 Alejandre, Nicolas - FW3A.2 Andreasen, Jonathan - JW4A.179 JW4A.64 Barman, Biplob - JTh2A.115 Abramochkin, Eugeny - FF5G.4 Alfano, Robert - LTu2H Andreeva, Vera A. -JTh2A.96 Ayubi, Gastón - JW4A.53 Barnett, Stephen - FTh5C.5 Abramski, Krzysztof - JTh2A.105 Algadey, Tarig - JW4A.70 Andresen, Esben R. - FF1A.5 Ayzatskiy, Mykola I. - FW2E.2 Barredo, Daniel - LTu1E.4 Adam, Thomas - FTu2D.5 Alibart, Olivier - FTu3G.3, FW3B.3 Anguita, Jaime A. - FTh5E.4 Azbite, Solveyga - JW4A.89 Barrera, John Fredy - FW2A.4, Adamson, Robert - FW5C.3 Alieva, Tatiana - FF5G.4, JTh2A.108 Ankonina, Guy - FTu2G.2 Azoury, Doron - FTu5C.2 JTh2A.182, JW4A.45 Adelson, Edward H. - FTh4I.3 Alishahi, Fatemeh - FTh5G.2 Antikainen, Aku J. - FTu1I.3, FTu1I.6 Azzam, Shaimaa - JW4A.132 Bartal, Guy - FTu2G.2 Adhikari, Sushovit - JTh2A.29 Allison, Kyle - JW4A.55 Apalkov, Vadym - JTh2A.103 Bartels, Randy - FTh4C.7, FTu2F.2, Key To Authors Key To Adibi, Ali - JTh2A.99 Allman, Michael - FW2B.5 Apolinario, Ulices F. -JTh2A.25 B JTh2A.57, JW4A.121 Aeschlimann, Martin - LF3I.1 Almaiman, Ahmed - FTh4E.3, Apurv Chaitanya, N. - JTh2A.18 Babich, Danylo - JW4A.39 Barton, John B. - FF1A.4 Aflakian, Nafiseh - JW4A.42 FTh5G.2 Aquila, Andy - LF2G, LTu5F.4 Babin, Sergey A. - FTu2I.6, FW5B.2 Barwicz, Tymon - FF5F.3, FTu1D.2, Aftab, Maham - FW5G.4 Almanee, Mohammad - JTh2A.41 Araiza Sixtos, Fernando Arturo - Babinsk, Adam - FF5B.8 FTu2D.2 Agarwal, Anjali - FTu5I.4 Almehmadi, Fares S. - FF3H.6 JW4A.60 Backhaus, Carsten - FW3H.2 Barz, Stefanie - FTu5G.2 Agarwal, Anuradha M. - JTh2A.163 Almeida, Raybel - JW4A.192 Araujo, Luis E. -JTh2A.25 Badolato, Antonio - FF5F.7 Bassett, Lee C. -JTh2A.175 Agarwal, Girish - FW3D.1 Alonso, Miguel A. - FF1A.5, FF3A.7, Arce-Diego, Jose L. -JTh2A.136, Bae, Euiwon - JTh2A.64 Bastille, Isle M. -JTh2A.183 Agnew, Megan - JW4A.43 FF3C.5, FF3G.1, FF3G.4, FF5G, JW4A.119 Baets, Roel G. F. - FF1E.2 Basurto-Pensado, Miguel - JW4A.40 Agrawal, Govind P. - FF3H.1, FF3H.2, FW3H.3, JTh2A.17, JW4A.49 Archer, Justice - JW4A.68 Bagge, Patrick - FTu1F.2 Batista, Rebeca J. - LF2D.3 FTu1I.3, FTu1I.6, JTh2A.47, Alonso-Sanz, Jose Ramon - FW3A.1 Arie, Ady - FTu3D.3, JW4A.41 Baghdady, Joshua - FTh4E.2, FTh4E.4 Bauman, Stephen - JTh2A.123 LTu2H.1 Alpeggiani, Filippo - FF3H.8, Armas-Rivera, Ivan - JTh2A.41 Bagnell, Kristina - JW4A.84 Baumbauer, Carol L. -JW4A.145 Aguilar, Gabriel - FTh4F.1 JW4A.57, JW4A.82 Arnold, C. L. - LTu1E.2 Bahari, Babak - LTu1H.5 Bayer, Mustafa Mert - JTh2A.180 Ahmad, Harith B. - JW4A.29 Alperin, Samuel - JW4A.87 Arnold, Nikita - JW4A.132 Baiz, Carlos - LTu5H.4 Bayer, Tim - LF2D.2 Ahmad, Raja - FTh4A.3 Alsing, Paul - FTh5G.6, FTu3G.4, Arriaga Hernández, Jesús A. Bajcsy, Michal - FTu5G.5, JW4A.7 Beach, Kory - JTh2A.111 Ahmed, Asif - FTu2D.4 LW2I.1 -JTh2A.66 Baker, Chams - JW4A.14 Beach, Raymond J. - LF2G.8 Ahn, Heesang - JW4A.141 Altmann, Robert K. - FTu5C.6 Arroyo Rivera, Edgar Samuel - Bakir, Muhannad S. -JW4A.127 Beadie, Guy - FW3H.4 Aissati, Sara - FW2A.3 Alu, Andrea - LF2E.3 JTh2A.22, JTh2A.5 Ballato, John - FTu2I, FTu2I.1, Beams, Ryan - FTu3F.7, LF2D.5 Aizpurua, Javier - FW3E.3 Alvarado Méndez, Edgar - JW4A.85 Arteaga Sierra, Francisco Rodrigo - FTu3B.4 Beaucamp, Anthony - FW5G.2 Ajayan, Pulickel M. - JTh2A.99, Álvarez-Tamayo, Ricardo Iván – FTu1I.3, FTu1I.6 Balogh, E. - LTu1E.2 Beels, Marten - JW4A.158, JW4A.160 JW4A.192 JTh2A.37, JTh2A.41 Artusio-Glimpse, Alexandra B. - Banaszek, Konrad - FF3C.2 Bekenstein, Rivka - LF5I.3 Akondi, Vyas - FW2A.3, FW3A.1 Alves, Guilherme A. - JW4A.107 FF3H.4 Bance, Manohar - FW5C.3 Bekesi, Nandor - FW3A.2 Aksoylar, Aydan - FW5H.2 Alves, Sarah I. - JTh2A.132 Arzani, Francesco - FTh4F.3 Bandres, Miguel - FTu3G.1, LF5I.3 Belardi, Walter - FTu2I.3 Aksun, M. Irsadi - JW4A.147 Amaral, Anderson M. - JW4A.184 Asgari, Pegah - JTh2A.1, JTh2A.76 Banerjee, Chitram - FF5D.7, JW4A.16 Bellaiche, Laurent - JW4A.195 Aksyuk, Vladimir - FTu3D.5 Amaya, Dafne - JW4A.75 Ashrafi, Solyman - FW5D.5 Banerjee, Partha P. - FF5B.1, JW4A.86 Beltran-Perez, Georgina - JTh2A.41 Aktas, Djeylan - JW4A.27 Ambichl, Phillip - JTh2A.4 Aspden, Reuben - JW4A.166 Banerjee, Sudeep - FTu1C.2, FTu1C.3, Ben Salem, Amine - JW4A.28 Al Graiti, Saif A. - FTu3I.5 Ambrosi, Christina - FF3A.3 Aspelmeyer, Markus - FF3D.1 JW4A.97 Benabid, Fetah - FTu1I.5 Al Maruf, Rubayet - FTu5G.5 Amiot, Caroline G. - FTh5A.3 Assanto, Gaetano - FF3H.3, JW4A.10, Banerji, Jay - FTh5B.5 Benalcazar, Wladimir - LTh5H.1 JW4A.12

142 FiO/LS 2016 • 16–21 October 2016 Benedetti, Carlo - FTu1C.1, FTu1C.5 Boudet, Antoine - FTh4D.5 Bulgakova, Nadezhda - JTh2A.113 Chan, Kam Wai C. - FTh5C.7, Chen, Ting-Wei - JTh2A.31 Bentley, Julie - FTu4A, FTu5A Boudoux, Caroline - FW5C.5 Burgess, Carrie - FTu2G.5 JW4A.194, JW4A.35 Chen, Ting-Yu - JTh2A.143 Ben-yakar, Adela - FF1A.2 Boukenter, Aziz - FW2F.1 Bustard, Philip J. - JW4A.14 Chandrasekara, Rakhitha - FTh4F.5 Chen, Wei-Ting - FTh5B.6, Beresna, Martynas - FTu1I.1 Bouwmans, Géraud - FF1A.5 Byard, Courtney - FTu2F.4 Chang, Chih-Hung - JW4A.137 JTh2A.143, JW4A.63, JW4A.65 Bergman, Keren - FF1E.4, JW4A.149 Boyd, Robert W. - FF1D.1, FF5C.6, Chang, Ki Soo - JW4A.52 Chen, Xi - JTh2A.145 Berini, Pierre - LTh5I.2 FF5D.4, FTh5B.7, FTu1G.4, C Chang, Shih-hui G. -JTh2A.165 Chen, Xiangcai - JW4A.188, Berlarge, Caroline - FF3A.4 FTu3D.4, FW2E.5, JTh2A.14, Cadier, Benoit - FW2F.1 Chang, Zenghu - FTu5C.1 JW4A.199 Bernier, Martin - FTh5A.1, FTu1I.2 JW4A.4, JW4A.64, LF2D.6, Cai, Yangjian - FF5G.1, JW4A.72 Chantasri, Areeya - FTu2G.4 Chen, Xikun - FF5H.3 Betzold, Amber - FTu5A.4 LTu1E.3 Campbell, E. C. - FF5A.4 Chaparala, Suman - JW4A.73 Chen, Xin - FTu2C.5 Beugnot, Jean-Charles - FTu5I.2 Boyer, Nicolas - FTu1D.2 Campbell, Melanie C. - FTh5D.4 Chapman, Robert - LW2I.3 Chen, Yi-Hsi - LF2G.5 Bezryadina, Anna - JW4A.114 Bozhevolnyi, Sergey - FF1G.5 Campos, Joaquin - JTh2A.184 Charlton, Phillip - FW5G.2 Chen, Ying Y. - FW3C.3 Bhaktha B. N., Shivakiran - Brabec, Thomas - LF2H.1 Canavesi, Cristina - FW2C.1, Chatterjee, Monish R. - FF3H.6, Chen, Yujie - JTh2A.92, JW4A.19 JTh2A.155, JW4A.179 Bracamontes-Rodríguez, Yazmin - JTh2A.140 JW4A.70, JW4A.73, JW4A.90 Chen, Yulu - FTu1F.2 Bharadwaj, Divya - JW4A.3 JTh2A.41 Cançado, Luiz Gustavo - FF5B.3, Chau, Fook Siong - FTu3D.6 Chen, Yu-Wen - FW3C.4 Bhattacharya, Mishkatual - JW4A.164 Bradley, Jonathan D. - FTu2D.5 FTu3F.7 Chaudhry, Muhammad Rehan - Chen, Zhanghai - LF2D.4 Key To Authors Bhattacharya, Pallab K. - LTu1H.2 Brahms, C. - LTu2E.2 Canovas, Carmen - FW2A.2 JTh2A.180 Chen, Zhigang - FTu3I.1, JW4A.114 Biaggio, Ivan - JW4A.158, JW4A.160 Brambilla, Gilberto - FTu1I.1, FTu5I, Cao, Hui - FTu2G.1, FW2D.1, Chauhan, Chanderkanta - JW4A.33 Chen, Ziyang - JTh2A.23, JW4A.110 Biancalana, Fabio - FTu3G.6 FTu5I.5 JTh2A.190, LTu1H.1, LTu1H.4 Chavez-Cerda, Sabino - JW4A.91 Cheney, Alec - FTu1F.6 Bianco, Giuseppe - FTh4F.2 Brand, Matthew - FW5H.2 Cao, Wei - LTu5F.2 Chekhova, Maria V. - LW5I.5 Cheng, Cliff - FTh4F.5 Bien, Harold - FF3A.3 Brandstotter, Andre - JTh2A.4 Cao, Yinwen - FTh4E.3, FTh5G.2 Chemnitz, Mario - FW3E.4 Cheng, Risheng - FTh5G.4 Bigelow, Nicholas P. - FW2E.3 Brasselet, Sophie - FF3A.7 Capasso, Federico - FTh5B.6, Chen, Jia-Wern - JTh2A.143 Cheng, Szu-Cheng - JTh2A.31 Bikorimana, Simeon - JTh2A.189 Brecht, Benjamin - FTu5G.2 JW4A.63, JW4A.65 Chen, Bin - JTh2A.127 Cheng, Tonglei - JTh2A.100, Bilenca, Alberto - JTh2A.133 Bres, Camille-Sophie - FTu5D.3 Cardenas, Jaime - FTu1F Chen, Borui - FTu1F.6 JTh2A.38, JW4A.188, JW4A.199 Billat, Adrien - FTu5D.3 Bretenaker, Fabien - FF5D.7, JW4A.16 Carletti, Luca - FF1C.5 Chen, Changqing - FF5H.2 Cheng, Xiaojun - JTh2A.19, Billet, Cyril - FTu3I.4 Brewster, Richard A. - FF3C.4 Carlson, Nathan John - FF1D.3 Chen, Chien-Chih - FW3C.4 JW4A.185 Bingham, Robert - FW5E.5 Brion, Etienne - FF5D.7 Carmichael, Howard - LW5I.4 Chen, Ching-Nien - JTh2A.187 Cheng, Xinru - JW4A.14 Birchall, Patrick - JTh2A.30 Bristow, Alan D. - FTu3F.3 Carney, P. Scott - FW2C.4, JTh2A.78, Chen, Christine P. -JW4A.149 Cheng, Yu-Hsiang - LF2G.6 Birech, Zephania - FF5A.5 Brizuela, F. - LTu1E.2 JW4A.117 Chen, Chun-Hu - JW4A.156 Cheng, Yu-Ting - JTh2A.183 Biswas, Abhijit - JTh2A.51 Brock, Christian - FW5G.6 Carr, Adra - LF3I.1 Chen, Cong - LF3I.1 Chenglong, Hao - LF2G.4 Biswas, Piyali - JTh2A.51 Brodbeck, Sebastian - LF2F.2 Carrée, Jean-Yves - FTu1I.2 Chen, Gang - FW2E.2, JW4A.157 Cherif, Rim - JW4A.28 Bittner, Stefan - JTh2A.190, LTu1H.4 Brodsky, Michael - JTh2A.15 Carreño, Marcelo N. -JTh2A.156 Chen, George F. R. - JTh2A.163, Chidangil, Santhosh - JW4A.113 Bo, Fang - JTh2A.166 Bromage, Jake - FTu2C, FW5E Carreño, Sandra - FTu2G.3 FTh4G.5 Chiles, Jeff - FW5D.2 Boardman, Allan - JW4A.10 Bromberg, Yaron - FW2D.1, FW3F.2 Cartwright, Alexander - FTu1F.6 Chen, Hongyi - JTh2A.93, JTh2A.94, Chin, See Leang - JTh2A.96 Boccuzzi, Krysta - FW5B.6 Brons, Jonathan - FTu3C.1 Carver, Gary E. - FF1A.4 JW4A.173 Cho, Jeongsik - FW3B.1 Boes, Andreas - FTu2C.5, FTu5G.4, Brooks, Daniel R. - FTh4H.4 Caspani, Lucia - FW3F.2 Chen, Hui - JTh2A.92, JW4A.19 Choe, Regine - FW3C.2 LW2I.3 Browaeys, Antoine - LTu1E.4 Cassarly, William J. - FTu4A.1 Chen, Jiajie - FW2C.5 Choi, Heejoo - FW5G.4 Boisvert, Jean-Sébastien - JTh2A.80 Brown, Jeremy - FW5C.3 Cassidy, Derek - JTh2A.146 Chen, Jie - JTh2A.112 Choi, Ju Won - FTh4G.5, JTh2A.163 Bokiniec, Phillip - JTh2A.181 Brown, Thomas G. - FF1A.5, FF3A.7, Castillejo, Marta - JW4A.83 Chen, Jin-Hui - JTh2A.46 Choi, Young-Hwan - JTh2A.13 Bolcar, Matthew R. - FF1G.4 FF3G.4, JW4A.48, JW4A.49 Castillo-Santiago, Gabriel - JTh2A.74 Chen, Kevin - LTh5H.1 Chon, Kwon Su - JW4A.58 Bondar, Mykhailo - JW4A.183 Bruce, Robert L. - FF5F.3 Castro, Jose - FTu5A.5 Chen, Kuang E. - FTh5D.5 Chong, Xinyuan - JW4A.137 Bongiovanni, Domenico - FTu3I.1 Bruner, Barry D. - FTu5C.2, LF3I Cavalcante, Guilherme - JW4A.20 Chen, Li - JW4A.188, JW4A.199 Choudhary, Saumya - FTu3D.4 Booth, Martin J. - FF1G, FW2H.4 Bruning, John H. - FTu1A.3 Cerjan, Alexander - FF1F.2 Chen, Mingzhou - FF5A.4, FTh5E.2, Chowdhury, Bilas - JW4A.20, Boppart, Stephen - JW4A.117 Brytavskyi, Ievgen - JTh2A.91 Ceurvorst, Luke - FW5E.5 JW4A.198 JW4A.22, JW4A.23, JW4A.24 Borghesi, Marco - FF3F.5 Buccheri, Fabrizio - FF3F.3 Chafer, Matthieu - FTu1I.5 Chen, Mu Ku - JTh2A.143 Chrapkiewicz, Radoslaw - FF3C.2, Borghuis, Bart - FTh5D.2 Buch, Shaival - JTh2A.47 Chaganava, Irakli - FF3G.7 Chen, Po-Jui - FTu3F.8 FW3F.3 Boriskin, Victor N. - FW2E.2 Buchnev, Oleksandr - JW4A.12 Chakraborty, Chitraleema - FF5F.7, Chen, Qian - JW4A.166 Christensen, Marc P. - FTh4C, Boriskina, Svetlana V. - FW2E.2, Buckley, Charlotte - FF3A.4 LF2F.1, JW4A.136 Chen, Qiushu - JTh2A.130 FTh5C.1 JW4A.157 Buercklin, Sam - FW2C.4 Chalich, Yamn - FF3C.7 Chen, Shouyuan - FTu1C.2, FTu1C.3, Christodoulides, Demetrios - FF3H.5, Borodinova, Tatiana - JW4A.88 Buettner, Lars - FF1G.3, FW2H.1 Chaloupka, Jan L. -JTh2A.198, JW4A.97 FTu2I.2, JTh2A.141, JTh2A.81, Bouchard, Frederic - FF5D.4 Bulanov, Stepan - FTu1C.1 LF2D.8 Chen, Szu-Yu - JW4A.111 JW4A.100, JW4A.181, JW4A.196

FiO/LS 2016 • 16–21 October 2016 143 Chrzanowski, Helen M. - FF1C.4, D Denisultanov, Alaudi - JW4A.89 Douglass, Glen - FW3H.5 Elías, Ana Laura - JTh2A.79 FTu5G.2 Dabrowski, Michal - FW3F.3 Dequal, Daniele - FTh4F.2 Dovgiy, Alexander A. -JTh2A.141 Ellis, Ian - JW4A.112 Chu, Kang-Yu - FW3C.3 Dadap, Jerry I. - FTu2D.4 Derkachov, Gennadiy - JW4A.68 Dowling, Jonathan - JTh2A.29, Ellis, Jonathan D. - FTh4H.4 Chu, Sai T. - FW3F.2, JTh2A.192, Dadashzadeh, Neda - FTu1I.5 Desforges, Jean - JTh2A.107 JTh2A.30, JW4A.163 Elsner, Ann E. - FTh5D, FW2H.5, JW4A.152 D’Addario, Anthony J. - FTu2G.5, Deshpande, Rucha A. - FF1G.5 Downes, James Downes - FTu3G.3 FW5A.3 Chu, Yu-Jung - JTh2A.56 JW4A.66 Devlin, Rober - FTh5B.6, JW4A.63, Dreissen, Laura S. - FTu5C.6 Emmerich, Sebastian - LF3I.1 Chui, Hsiang-Chen - LF2G.5 Dadgostar, Shabnam - FF5F.6 JW4A.65 Driscoll, Kristina - JW4A.136 Emptage, Laura - FTh5D.4 Chung, Roger - JTh2A.181 Dahal, Pabitra - JTh2A.173, JTh2A.63 Devries, David - FTh5D.4 Drobyshev, Roman V. - FTu2I.6 Enami, Yasufumi - JTh2A.147 Chung, Te-Yuan - JTh2A.187 Dailey, James M. - FTu5I.4 Dhara, Sajal - LF2F.1 Du, Jinjin - JTh2A.34 Enaya, Rayan - JW4A.20 Ciappina, M.F. - JW4A.104 Dajani, Iyad - FW5B, FW5B.1, Dholakia, Kishan - FF5A.4, FTh4C.4, Ducci, Sara - FTh4F.4 Engelmann, Sebastian - FF5F.3, Cisternas, Jaime E. - FTh5E.4 FW5B.3, FW5B.4, FW5B.5 FTh5E.2, JW4A.198 Dudek, Michal - JTh2A.40 FTu1D.2 Clark, Christopher A. - FW5A.3 Daniels, Joost – Ftu1C.1, FTu1C.5 Di Falco, Andrea - FF3H.8, JW4A.82 Dudley, Angela - FF5H.5 England, Duncan G. - JW4A.14 Clark, John I. -JTh2A.124 Darga, Donald - JW4A.117 Di Pasquale, Fabrizio - FF3B.2 Dudley, John M. - FTh4A.3, FTh5C.6, Englund, Dirk - FF5E.1, FTh5G.6, Clark, Thomas W. -JW4A.80 Darudi, Ahmad - JTh2A.1, JTh2A.76 Diamanti, Eleni - FTh4F.4 FTu3I.1, FTu3I.4 FW5D.3 Clemens, James - LW5I.4 Darweesh, Ahmad A. -JTh2A.123 Dias, Frederic - FTu3I.4 Dudovich, Nirit - FTu5C.2, LF2D.2 Entcheva, Emilia - FF3A.3 Cogliati, Andrea - FW2C.1 Das, Ritwick - JTh2A.110 Díaz Guerrero , Gabriela - JW4A.99 Dufour, Adrien - FTh4F.3 Entwisle, Blake - JTh2A.181 Cohen, Lear - JTh2A.133 Daud, Nurul Ashikin B. - FTu2D.3 Dichiara, Anthony - FTu2C.4 Duma, Virgil- Florin - JTh2A.129 Epworth, Richard - FTu1B.1 Cohen, Lior - FF1D.5 D’auria, Virginia - FW3B.3 Dickensheets, David L. -JW4A.145 Durak, Kadir - FF5C.3, FTu2F.6 Erhard, Manuel - FW3F.1 Cohen, Moshe-Ishay - LF5I.3 Davanco, Marcelo - LW5I.2 Diddams, Scott - FTh5G.3, Durán, Vicente D. -JW4A.93 Erickson, David - JW4A.108 Coleman, Rhima - JTh2A.130 Davison, Ian - FF3A.1 JTh2A.114, JTh2A.85 Duran-Sanchez, Manuel - JTh2A.37, Erickson, Michael - JW4A.158, Combrié, Sylvain - FF1F.1 Davydov, Albert - FTu3F.7 Diez-Y-Riega, Helena - FF5B.4 JTh2A.41 JW4A.160 Compertore, David C. - FW2H.3 Dawson, Martin - FTh4D.5 Dimauro, Louis F. - LF2H.3 Dushaq, Ghada - FTu3F.2 Esarey, Eric E. - FTu1C.1, FTu1C.5

Key To Authors Key To Conry, Jessica P. -JTh2A.62 de Angelis, Costantino - FF1C.5 Ding, Xiaoming - JTh2A.73 Dusheyko, Mykhaylo - JW4A.88 Esaulkov, Mikhail N. - JTh2A.96 Constant, Colin - JW4A.120 de Angelis, Lorenzo - FF3H.8, Dinkelaker, Aline N. - FF1H.1 Dutta, Ishir - JTh2A.111 Escobedo-Alatorre, Jesús - JW4A.40 Conti, Claudio - FTu3G.6 JW4A.82 Diouf, Mbaye - JW4A.28 Dwivedi, Ranjeet - JTh2A.168 Estudillo Ayala, Julian Moises - Coolbaugh, Douglas - FTu2D.5 de Araújo, Cid B. - FTu2G.3, FTu3F.5, Dipold, Jessica -. - LF2D.3 JTh2A.32 Coppens, Zachary - JW4A.151 JW4A.184 Dirmeier, Thomas - FF3D.3 E Evans, Alan - FTu1B, FTu2B, FTu3B Corkum, Paul - FTu5C.3, FW5E.3, de Boni, Leonardo - LF2D.3 Dkhil, Brahim - JW4A.195 Eberly, Joseph H. - FF3C.5, FF5C.7, Evans, Richard - FF5B.5 LTh5I.2 de Dobbelaere, Peter - FF3E.1 Doerschuk, Peter C. - FTh5D.5 JTh2A.17 Evlashin, Stanislav - JW4A.155 Cornejo Rodriguez, Alejandro - de La Hoz, Andres - FW3A.2 Dogariu, Aristide - FF5B.3, JW4A.120, Eckstein, Andreas - FTu5G.2 Eyler, Edward E. - LF2G.7 JTh2A.66 de Leon, Israel - FTu1G.4, FTu3D.4, JW4A.6 Eden, James G. - FF1H.3, FF1H.4, Ezquerra, Tiberio A. -JW4A.83 Corwin, Kristan L. - FTu1I.5, LTu1E FW2E.5 Doh, Iyll-joon K. -JTh2A.64 JTh2A.12, JW4A.54 Cote, Daniel C. - FF3A, FTh4D.3 de Lima Moura, Andre - FTu2G.3 Dolgaleva, Ksenia - JTh2A.179, Edgar, Matthew - FF1D.2, FTh5C.5 F Cotrufo, Michele - FTu3D.7 de Lucia, Francesco - FTu1I.1, FTu2I.3 JW4A.64 Eftekhar, Ali - JTh2A.99 Fabre, Claude - FTh4F.3 Couairon, A. - LTu1E.2 de Miranda, Igor P. - FTu3F.5 Donaldson, William R. - FF3H.1 Eggebrecht, Adam T. - FW3C.1 Fainman, Yeshaiahu - FW5D.1, Coudert-Alteirac, H. - LTu1E.2 de Rossi, Alfredo - FF1F.1 Dong, Chunhua - LF2E.1 Eggleton, Benjamin J. - FF5E.2, LTu1H.5 Coulon, Pierre Eugène - JW4A.178 de Rossi, Wagner - FTu2C.2 Dong, Hongxing - LF2D.4 FTh4G.3 Falcao- Filho, Edilson L. - FTu3F.5, Coulter, Tabitha - LF2E.6 de Sterke, C. Martijn - FTu3D.8 Dong, Jingyuan - FTh5D.5 Eguchi, Ryutaro - JTh2A.148 JW4A.184 Courrol, Lilia C. -JTh2A.132 Debord, Benoit - FTu1I.5 Dong, Liang - FW5B.3, FW5B.4 Eich, Steffen - LF3I.1 Fält, Stefan - FF5F.7 Couture, Charles-Andre - FW5E.3 Debuisschert, Thierry - FF1F.1 Donley, Elizabeth A. - FTh5F.4 Eikema, Kjeld S. - FTu5C.6 Fan, Shanhui - FF1F.2, LTh5H.2 Crozier, Kenneth - FW2C.5 Decamp, Matthew F. - FTu2C.4 Dorn, Ralf - FW5G.6 Eilers, Hergen - FF5B.4, JTh2A.86, Fan, Tianren - JTh2A.99 Cruz, Flavio - JTh2A.85 Delfyett, Peter - FTh5G.7, JW4A.84 Dorney, Kevin M. - LF2D.8 JTh2A.90 Fan, Xudong - JTh2A.130 Cruz-Hernandez, Jean C. -JTh2A.183 Dell’anna, Luca - JTh2A.89 Dorrah, Ahmed - FF5H.8, JW4A.193 Eisenberg, Hagai - FF1D.5 Fang, Renpeng - JTh2A.16 Curtis, Jeremy - JTh2A.115, Dellis, Argyrios - FTh5F.4 Dorrer, Christophe - FF3G.5, FTu3F, El Shamy, Raghi - JTh2A.169 Fang, Yunsheng - JW4A.129 JTh2A.197 Dellith, Jan - FW3E.4 FW5H.5 Elamurugu, Elangovan - JTh2A.173 Fanjul-Vélez, Félix - JTh2A.136, Cusano, Andrea - FF3B.1 Demetris, Geddis - JTh2A.170 Dorronsoro, Carlos - FW2A.3, Eldar, Yonina C. - LF2D.2 JW4A.119 Cutter, Kurt - LF2G.8 Demmler, Stefan - FW5E.1 FW3A.1, FW3A.2 Eldridge, William J. - FF3A.6, Fanto, Michael L. - FF5F.5, FTh5G.6, Cvarch, Ben - FTu2G.5 Demos, Stavros G. - LW3I.3 Dorsinville, Roger - JTh2A.189 JTh2A.126 FTu3G.4, FW5D, LW2I.1 Czarske, Jürgen - FF1G.3, FW2H.1 Deng, Hui - LF2F.2, LF5I Dos Santos, Denise V. - FW3A.3 El-ganainy, Ramy - FTu2D.4, Farrell, Joshua - FW5C.3 Deng, Lu - JTh2A.9, LF2E.7 Dostovalov, Alexander V. - FW5B.2 JW4A.186 Farriss, Wesley - FF1G.2, FF5G.2

144 FiO/LS 2016 • 16–21 October 2016 Faryadras, Sanaz - JTh2A.160 Fonseca, Ruben D. - LF2D.3 Gan, Qiaoqiang - FTu1F.6, JTh2A.79, Giles, Randy - FTu1B.4 Griffith, Austin - FTu5D.2 Fasciszewski, A. - JW4A.161 Forbes, Andrew - FF5H.5, FTh4B.5 JW4A.135, JW4A.30 Giner, Lambert - FF1C.6, FF1D.3, Grigutis, Robertas - FTu2C.1 Fatemi, Fredrik K. - FTu3I.6, LTu1E.4, Förster, Ronny - FTh4C.3 Gan, Zongsong - FF5B.5 FF3C.7, FW2H.2, JW4A.14 Grimau Puigibert, Marcel Li - FTh4F.1 LW5I.4 Fortier, Paul - FTu1D.2 Gandara-Montano, Gustavo A. - Giovannini, Daniel - FW2B.3 Gross, Simon - FW3H.5, JTh2A.181 Fathpour, Sasan - FTh5G, FTh5G.7, Fortin, Vincent - FTu1I.2 FTh4H.4 Girard, Sylvain - FW2F.1 Grote, Richard R. -JTh2A.175 FTu2D, FW5D.2 Foster, Mark A. - FTh4G.1 Gao, Boshen - JW4A.64 Girkin, John M. - FF3A.4 Grover, Jeffrey - JTh2A.159 Fattahi, Hanieh - FF3C.1 Fotiadi, Andrei A. - FTu2I.6 Gao, Feng - JW4A.192 Gisin, Nicolas - JW4A.27 Grulkowski, Ireneusz - FTh4H.1 Fedorov, Sergey - FF3D.6 Fouda, Mohammad - FF1B.2 Gao, Lu - JTh2A.14 Glover, Brian - JW4A.153 Gruzdev, Vitaly - JTh2A.113 Fedorov, Vyacheslav I. -JTh2A.125 Fowler, Bert - JW4A.142 Gao, Weiqing - JW4A.188, JW4A.199 Glushchenko, Anatoliy - FF5B.6 Grzeszczyk, Magdalena - FF5B.8 Fedrici, Bruno - FW3B.3, JW4A.27 Franke, Jörg - FW3H.2 Garbovskiy, Yuriy - FF5B.6 Gnilitskyi, Iaroslav - JTh2A.113, Gu, Guancheng - FW5B.3 Fegadolli, William - FTh4G.4 Franke-Arnold, Sonja - FTh5B.3, Garcell, Erik M. - FTu5B.2 JW4A.88 Gu, Kebin - JTh2A.151 Fei, Teng - JTh2A.54 JW4A.80 Garcia Melgarejo, Julio Cesar - Godin, Thomas - FTh4A.3 Gu, Min - FF5B.5, FTu3F.1, FTu5A.3, Feizpour, Amir - FTu5G.2 Franson, James D. - FF3C.4, FF5D.5, JTh2A.21, JTh2A.22, JTh2A.5, Goette, Joerg B. - FTh5B.3 FTu5B.5, JTh2A.145, JTh2A.149 Fejer, Martin M. -JW4A.174 JW4A.171 JW4A.18 Golasa, Katarzyna - FF5B.8 Gu, Qing - LTu1H.5 Feng, Liang - FF5F, FTh4G.4, Fraser, Scott - FTu5B.4 García Ramírez, Emma V. -JW4A.102, Goldfarb, Fabienne - FF5D.7, Gu, Ying - JTh2A.93, JTh2A.94, Key To Authors JTh2A.81 Frederick, Connor - FTh5G.3 JW4A.99 JW4A.16 JW4A.173 Fenton, Eliot - FTu3I.6 Fredin, Leis - JW4A.142 Garcia, Carlos - JTh2A.115 Golding, Terry - JW4A.142 Guang, Zhe - FW5E.2 Ferrari, José A. - JW4A.53 Freeman, Mark - FF3F.2 Gartman, Alexandra - JW4A.155 Goldstein, Adam - JW4A.190 Guarepi, V. - JW4A.161 Ferrero, Alejandro - JTh2A.184 Fregin, Bob - FW2H.1 Gautam, Rekha - JW4A.114 Goldstein, Lee E. -JTh2A.124 Gubin, Mikhail A. -JW4A.180 Ferretti, Hugo M. - FTu2F.1 Freisem, Lars - FF3D.5 Gauthier, D. J. - LTu1E.3 Golovin, Grigory - FTu1C.2, FTu1C.3, Guiomar, Fernando - FTh4E, FTh4E.1 Ferreyrol, Franck - FF1C.3 French, David A. -JTh2A.123 Gauthier, Jean-Christophe - FTu1I.2 JW4A.97 Gunawidjaja, Ray - FF5B.4, JTh2A.86, Fetcho, Joseph R. -JTh2A.183 Friberg, Ari Tapio - FF5H.1, FTh5C.6, Gauvin, Serge - JTh2A.107 Gomes, Anderson - FTu2G.3 JTh2A.90 Fewo, Serge - FTu2G.3 JTh2A.152 Gaylord, Thomas K. - FTu1F.4, Gomez, Jorge - JW4A.75 Guo, Chunlei - FTu5B.2 Fickler, Robert - FF5C.6, FF5D.4, Frostig, Hadas - LF2D.2 FTu2I.4, JW4A.127, JW4A.67 Gomez-Carbonnel, Carme - FTh4F.4 Guo, Guang-Can - LF2E.1 FTh5B.7, FW3F.1, JW4A.4 Fruhling, Colton - FTu1C.2, JW4A.97 Gbur, Gregory J. - FF5H, FTh4B.2, Gong, Qihuang - JTh2A.93, Guo, Hairun - FTu5D.3 Fiddy, Michael A. - FTu1F.3 Fu, Kai-Mei - FF5F.6 FTh4B.4, FTh5B, JW4A.197 JTh2A.94, JW4A.173 Guo, Hong - JTh2A.116, JTh2A.23 Fidler, Ashley - LTu5F.2 Fu, Ling - JTh2A.185 Ge, Li - FTh4G.4, JTh2A.81, Gong, Yongji - JW4A.192 Guo, Junpeng - JW4A.162 Field, Jeffrey J. - FTh4C.7, FTu2F.2, Fu, Walter P. - FW5E.4 JW4A.186 Gonsalves, Anthony J. - FTu1C.1, Guo, Lina - JW4A.72 JTh2A.57, JW4A.121 Fu, Wei - LF2E.1 Ge, Wenchao - JW4A.164 FTu1C.5 Guo, Wei - FF5F.5, FTu1D, FW5C.4 Fienup, James R. - FF1G.2, FF1G.4, Fujii, Shun - FTh5G.5, JTh2A.150 Gearhart, Sara M. - FTh4H.4 Goodfellow, Kenneth M. - FF5F.7, Guo, Xiang - FTh4G.2, FTh5G.4, FF5G.2, FTu2F.3, FW5H.4 Funes, Gustavo L. - FTh5E.4 Geddes, Cameron G. - FTu1C.1, JW4A.136, LF2F.1 JTh2A.114 Filoteo Razo, Jose David - JTh2A.32 Funkenbusch, Paul D. - FTh4H.4 FTu1C.5 Gopinath, Juliet T. - FTh5B.2, Gupta, Banshi D. -JTh2A.44, Finger, Martin A. - LW5I.5 Furusawa, Akira - FTu2G, FTu3G.2 Genack, Azriel - FTu2G.2 JW4A.87 JTh2A.52, JTh2A.53 Fink, Mathias - FW2D.2 Gentile , Antonio Andreas - FTu3G.5 Gorodetsky, Michael L. - FTu5D.5 Gutiérrez-Cuevas, Rodrigo - FF5C.7 Fink, Yoel - FTu3B.3 G Genty, Goëry - FTh5A.3, FTh5C.6, Goswami, Debabrata - JTh2A.117 Guzun, Dorel - JW4A.175 Fiore, Andrea - FTu3D.7, FTu5G.3 Gaarde, Mette - LF2H.2 FTu3I.4 Goto, Takahiro - FTu5C.5 Gvishi, Raz - JW4A.41 Fironova, Nadezhda - JW4A.69 Gaeta, Alexander L. - FTu5D.2, Georgakoudi, Irene - FF1A, FF5A.2 Gotoh, Hideki - FTu5C.5 Fischer, Martin - FF5D.2 LW2I.2, LW5I Germer, Thomas - JW4A.48 Gould, Michael - FF5F.6 H Fisher, Paul - FTu5G.4 Gain, Philippe - JTh2A.140 Gérôme , Frédéric - FTu1I.5 Goulielmakis, Eleftherios - LF2H, Haapamaki, Christopher - FTu5G.5 Fitzpatrick, Casey A. - FF5D.3 Galica, Scott E. - LF2G.7 Gerrits, Thomas - FW2B.5 LTh5I.1 Haberko, Jakub - FF3G.6 Flayac, Hugo - LF2F.4 Galili, Michael - FTh4E.6 Gese, Natalie J. - FF5B.4 Graham, Trent - FTu2F.4, FW2B.2 Hach, Edwin - LW2I.1 Fleischer, Jason W. -JW4A.11 Gallais, Laurent - FTu2C.1 Ghadimi, Amir - FF3D.6 Gramegna, Marco - FW3F.4 Haden, Daniel - FTu1C.2, JW4A.97 Flores, Angel - FW5B.1, FW5B.5 Galtarossa, Andrea - FTu5I.1 Ghamsari, Benhood G. - LTh5I.2 Granados, Fermin S. -JTh2A.66 Hädrich, Steffen - FW5E.1 Flores, Raquel - FTu2I.5, JTh2A.63 Galtier, Sandrine - FTu5C.6 Ghosh, Rupamanjari - JW4A.16 Granados-Baez, Marissa - FW2H.2 Hafezi, Mohammad - LF5I.4, LTh5H Florez, Jefferson - FF1D.3 Galvez, Enrique J. - FTh5B.4, Ghosh, Somnath - JTh2A.51 Grassani, Davide - FTu5D.3 Hagan, David - JTh2A.26, JW4A.183 Flórez, Jefferson - JW4A.14 FTu2G.5, JTh2A.111, JW4A.66 Ghosh, Subhabrata - JTh2A.155 Graves, Logan - FW5G.4 Hagley, E.W. - JTh2A.9, LF2E.7 Flynn, Richard A. - FW3H.4 Galvin, Tom - JW4A.54 Ghosh, Sumit - JTh2A.82, JW4A.105 Green, William M. - FTu2D.2 Haglund, Richard - JTh2A.197 Fokine, Michael - FTu2I.1 Galvis, Jorge - JTh2A.48 Gibson, Graham - FF1D.2, FTh5C.5 Gregg, Patrick - FW2B.4 Haiqing, Li - JTh2A.35 Foltynowicz, Aleksandra - FTu5C.4 Gambra, Enrique - FW2A.3, FW3A.1 Gibson, Ursula J. - FTu2I.1 Greivenkamp, John - FTu1A.4 Haldar, Raktim - JTh2A.50 Fondakowski, Michael - JW4A.116 Gan, Choon H. -JTh2A.75 Giese, Enno - FF5C.6 Grieve, James - FF5C.3, FTh4F.5 Hall, Kimberley - FTu3F.3

FiO/LS 2016 • 16–21 October 2016 145 Hallman, Mark - JW4A.55 Herzog, Joseph B. -JTh2A.123 Hu, Fangyao - FF5A.1 Isik, Okan - FW5B.7 Jingming, Song - FF1B.3, FW2F.3 Hammond, T. J. - FTu1C.4, FW5E.3, Heuer, Axel - LF2G.3 Hu, Guoqing - JTh2A.112, JW4A.31 Ismaeel, Rand - FTu1I.1 Jinyan, Li - JTh2A.35 LTh5I.2 Heyl, Christoph - LTu1E.2 Hu, Hao - FTh4E.6 Isotalo, Tero - JW4A.178 Joannopoulos, John - FF1F.3, Han, Kyunghun - FW5F.5 Hickman, Garrett - FF5D.5, JW4A.171 Hu, Juejun - FF5F.2 Istrati, Daniel - FF1D.5 LTh5H.4 Han, Sangyoon - FTu1D.6 Hickstein, Daniel D. - LF2D.8 Hu, Linxi - FF5H.3 Ito, Tomoyoshi - JTh2A.68 Johansson, Alexandra C. - FTu5C.4 Han, Xiaobo - JTh2A.24 Higbee, Oliver - JTh2A.75 Hu, Sofia H. -JTh2A.183 Iturbe-Castillo, Marcelo D. -JW4A.91 John, Jem Teresa - JTh2A.67 Han, Zhaohong - JTh2A.163 Hill, Alexander - FW2B.2 Hu, Xian - JW4A.175 Iwamoto , Naotaka - JTh2A.164 Johnson, A.S. - LTu2E.2 Handerek, Vincent - FF3B.5 Hill, John - FTu2A.1 Hu, Yi - FTu3I.1 Iwaszczuk, Krzysztof - FF3F.2 Johnson, Eric G. - FF5G.5, FTh4E.2, Hansen, Azure - FW2E.3 Hillenbrand, Rainer - FW2C.4, Huang, Chia-Wei - JW4A.156 FTh4E.4, JTh2A.193 Hao, He - JTh2A.93, JTh2A.94, FW3E.3, JTh2A.78 Huang, Huiling - JW4A.110 J Johnson, Michael A. - LF2G.8 JW4A.173 Hillman, Elizabeth - FTh4D Huang, Jinxin - JTh2A.129, Jachura, Michal - FF1D.4, FF3C.2 Johnson, Steven G. - FF1F.3, LTu1H.3 Hao, Zhenzhong - JTh2A.166 Hilton, David J. -JTh2A.115, JTh2A.138 Jackson, Stuart D. - FTh5A.2 Johnsson, P. - LTu1E.2 Harari, Gal - LF5I.3 JTh2A.197 Huang, Jui-ChieCh - LF2E.8 Jacquard, Clément - FTh4F.3 Johnston, Kyle - FTu5C.3 Hariri, Ali - JW4A.62 Hindman, Holly B. -JTh2A.138, Huang, Po-Jung - FW3C.4 Jahromi, Ali - FF3G.2 Joly, Nicolas - FW5F.4, LW5I.5 Harris, Nicholas - FW5D.3 JTh2A.140 Huang, Sheng - LTh5H.1 Jaimes-Najera, Alfonso - JW4A.91 Jones, Daniel E. - FF5D.5 Hase, Eiji - JTh2A.128 Hine, Allison - JTh2A.62 Huang, Shu-Wei - FTh4G.7 Jain, Vijay - FF5B.2 Jones, Jason S. - FF3A.2 Hasegawa, Takemi - FTu2B.2 Hiraki, Tatsurou - FW5F.3 Huang, Tianyao - JW4A.168 Jakubczyk, Daniel - JW4A.68 Jones, Joshua A. - FTu2G.5, Hashemi Rafsanjani, Seyed Hirayama, Ryuji - JTh2A.68 Huang, Yao-Wei - JTh2A.143 Jakutis Neto, Jonas - JTh2A.109 JTh2A.111, JW4A.66 Mohammad - JTh2A.14 Hitachi, Kenichi - FTu5C.5 Huang, Yi - JW4A.157 James, Daniel F. - FF3D.4, JTh2A.20, Jones, Maxwell - FTu2I.1, FW5B.3 Hashimoto, Kenichi - JTh2A.42 Ho, Joseph - FF1C.3 Huang, Yizhong - FF5F.2 JW4A.182 Jordan, Andrew - FTu2F.4, FTu2G.4 Hassan, Absar U. -JW4A.100 Ho, Xuan Long - FTu3F.8 Huang, Zhaoran R. - FTu1D.5, Jamison, Keith - JW4A.142 Jost, Aurélie - FTh4C.3 Hatakeyama, Taiki - FF5H.7 Hochrainer, Armin - FF3C.6 JTh2A.171 Janeiro, Ricardo - FTu2I.5, JTh2A.63 Jufas, Nicholas - FW5C.3

Key To Authors Key To Hatami, Fariba - FF5F.6 Hoffman, James - FF3F.2 Huang, Zixin - LW2I.3 Janisch, Corey - JTh2A.79 Juffmann, Thomas - FF5C.5 Haufe, Daniel - FF1G.3 Hoffman, Jonathan E. - LTu1E.4 Huber, Marcus - FW3F.1 Janta-Polczynski, Alexander - FTu1D.2 Jun, Hojoong - FTh4G.2 Haus, Joseph - JTh2A.41 Höfling, Sven - FW5D.4, LF2F.2 Hudgings, Janice A. -JW4A.55 Jaramillo-Villegas, Jose A. - FW5F.5, Jung, Daehwan - JTh2A.190 Hausmann, Katharina - FW5B.7 Hohne, Andrew - JW4A.145 Hughes, Taylor - LTh5H.1 JW4A.174, JW4A.150 Jung, Hojoong - FTh5G.4, JTh2A.114 Hawkins, Thomas - FTu2I.1, FW5B.3 Holleman, Joshua - JTh2A.115 Huillier, A. L. - LTu1E.2 Jarosch, S. - LTu2E.2 Jung, Youngkee - JTh2A.64 Hawley, Ryan D. - FTh5B.3 Holmes, Rebecca M. - FW3A.4 Hummon, Matthew T. - FTh5F.4 Jaroszewicz, Zbigniew - FW2A.4, Hay, Darrick - FTu1F.2, JTh2A.172 Holtkamp, David B. -JW4A.153 Hung, Yung-Jr - JW4A.156 JTh2A.182 K Hayashi, Tetsuya - FTh5E.3, FTu2B.2 Honardoost, Amirmahdi - FTh5G.7 Hunter, David G. -JTh2A.124 Jarrahi, Mona - FTh4G.7 Kabakova, Irina - FTh4G.3 Hayes, Adam - FW2C.1 Hong, Peilong - JW4A.74 Hunter, Jennifer J. - FTh4H.3 Jauregui Vazquez, Daniel - JTh2A.32 Kablukov, Sergey I. - FTu2I.6, FW5B.2 Haylock, Ben - FTu5G.4 Horak, Peter - FTu1I.1 Hupfer, Robert J. -JTh2A.135 Javerzac-Galy, Clément - FTu5D.5 Kadhim, Ahmed - JW4A.23 He, Guangqiang - FF5H.3 Hori, Atsuhiro - FTh5G.5 Huttner, Ulrich - LTh5I.3 Jayaseelan, Maitreyi - FW2E.3 Kaiser, Florian - FW3B.3 He, Jing - FTu1I.1 Horne, Christopher K. -JTh2A.43 Huxlin, Krystel R. - FTh4H.4 Jelic, Vedran - FF3F.2 Kakarenko, Karol - FW2A.4, He, Lixin - FTu3C.2 Hornig, Graham - FF3F.2 Huy, Kien Phan - FTu5I.2 Jen, Alex - JTh2A.147 JTh2A.182 He, Ruiqing - JW4A.166 Horton, Matthew - FF3C.7 Huzortey, Andrew - JTh2A.95 Jeong, Gyu-Jae - JW4A.143 Kakauridze, George - FF3G.7, He, Zhiguo - JTh2A.140 Howard, Joseph M. - FTu1A.1, FW5H Hwang, Seonhee - JW4A.141 Jha, Pankaj K. - FF5C.4, FTu1G.3 JTh2A.77 Head, Stephen - FF3G.4 Howell, John - FF1D.6, FF3H.2, Jhajj, Nihal - FTh4B.3 Kakue, Takashi - JTh2A.68 Hegmann, Frank - FF3F.2 FW5F.6, FW2B.5 I Ji, Dengxin - FTu1F.6, JTh2A.79, Kalichevsky-dong, Monica - FW5B.3 Heintzmann, Rainer - FTh4C.3 Howland, Gregory A. - FTh5G.6, Iacchetta, Alexander S. - FF1G.4 JW4A.30 Kalinski, Matt - JW4A.187 Henao, Rodrigo - FW2A.4, JTh2A.182 LW2I.1 Ibarra-Escamilla, Baldemar - Jia, Baohua - FTu5B.4 Kalish, Irina - FTu3F.7 Henderson, Rashaunda - JW4A.42 Hradil, Zdenek - FF3D.3 JTh2A.37, JTh2A.41 Jian, Ziyun - JW4A.26 Kalra, Yogita - JW4A.154, JW4A.92 Hendon, Christine P. - FW3C, FW5C.2 Hsiao, Yu-Cheng - LF2E.8 Ibsen, Morten - FTh4A, FTh5A, FW2F Jiang, Lingjun - FTu1D.5, JTh2A.171 Kaluzny, Bartlomiej - FTh4H.1 Herman, Matthew A. - FTh5C.4 Hsieh, Yu-Hua - JTh2A.187 Igarashi, Koji - FTh5E.3 Jiang, Suhua - JW4A.30 Kam, Ivan - JTh2A.109 Hermosa, Nathaniel - JW4A.103 Hsu, Chia Wei - FF1F.3, LTh5H.4 Ilday, Fatih Ömer - FTu1I.4, FW5B.7 Jiang, Xuefeng - FF5C.8 Kaminer, Ido - LF2E.5 Hernandez Garcia , Juan C. -JTh2A.32 Hsu, Wei-Chun - JW4A.157 Imamura, Katsunori - FTh4E.5 Jimenez, Ralph - LTu5H.3 Kamlapurkar, Swetha - FF5F.3, Hernandez, Margarita - JW4A.83 Hsu, Wei- Lun - JTh2A.143 Imany, Poolad - FW5F.5, JW4A.174 Jin, Jing - FW2F.2, FW2F.3, JTh2A.54 FTu1D.2 Herring, Cyrus - FF1H.4 Hsueh, Yu-Chun - JW4A.15 Inaba, Takahiro - JTh2A.148 Jin, Tao - FTh5D.4 Kamp, Martin - LF2F.2 Herzig Sheinfux, Hanan H. - FTu2G.2, Htoon, Han - LTu3H.3 Inoue, Shuichiro - JTh2A.7 Jing, Jietai - FF5H.3 Kang, Songbai - FTh5F.4 FTu3G.1 Hu, Bin - JW4A.129 Ishizawa, Atsushi - FTu5C.5 Jinggang, Peng - JTh2A.35 Kang, Tae Young - JW4A.141

146 FiO/LS 2016 • 16–21 October 2016 Kanhirodan, Rajan - JTh2A.67 Kieu, Khanh - FTh5A.4, FW5B.4 Kolwas, Krystyna - JW4A.68 Kumar, Arun - JTh2A.168, JW4A.130 Lazarev, Vladimir A. -JW4A.180 Kanta, Chander - JTh2A.33 Kildishev, Alexander - JW4A.132 Kolwas, Maciej - JW4A.68 Kumar, Ashok - JTh2A.2 Leach, Jonathan - JW4A.43 Kante, Boubacar - LTu1H.5 Kilosanidze, Barbara N. - FF3G.7, Kondakci, Hasan Esat - FW5H.8, Kumar, Prem - FW3B.2 Leaird, Daniel E. - FW5F.5, JW4A.150, Kanter, Gregory S. - FW3B.2 JTh2A.77 JW4A.101, FF3G.2, JW4A.181 Kumar, Santosh - JTh2A.33, JW4A.33 JW4A.174 Kanukuntla, Pallav - JTh2A.170 Kim, Bong-jun - JTh2A.70 Kondratenko, Serhiy - JTh2A.158 Kumar, Vikash - JTh2A.178 Leake, Gerard - FTu2D.5 Kao, Fu J. - FW2C.3 Kim, D. - JTh2A.103 Kong, Fanting - FW5B.3 Kumara Vadivel, Shruthi - FTu1F.4 Leary, Cody C. - FW2B.4 Kapteyn, Henry C. - LF2D.8, LF3I.1 Kim, Dae Wook - FTu2A.1, FTu3A, Kong, Kenny - JW4A.112 Kumari, Babita - JW4A.148 Lecaplain, Caroline - FTu5D.5 Karaiskaj, Denis - JTh2A.115, FW5G.4 Kong, Xianming - JTh2A.127 Kunkel, Mint - FW3H.5 Ledingham, Patrick - FTu5G.2 JTh2A.197 Kim, Daesuk - JW4A.51 König, Jörg - FW2H.1 Kuppusamy, Porsezian - JW4A.169, Ledoux, Danielle M. -JTh2A.124 Kardas, Tomasz M. - FTu3C.2 Kim, Donghyun - JW4A.123 Kordts, Arne - FTh4E.3, FTh5G.2 JW4A.46 Leduff, Paul - JTh2A.127 Karim, Akib - LW2I.3 Kim, Jeongmin - FTu1G.3 Kosareva, Olga G. - JTh2A.96 Kurmulis, Sarah - FTu2F.5 Lee, Byoungho - JTh2A.154, Karimi, Ebrahim - FF5D.4, FW2H.2 Kim, Joonsoo - JTh2A.154, Kosc, Tanya Z. - FW2G.3 Kuti, Ayodeji - JTh2A.170 JTh2A.162, JW4A.125 Karkus, Peter - FW3F.6 JTh2A.162, JW4A.125 Kostuk, Raymond K. - FTu5A.5 Kutuzyan, Aghavni - JW4A.44 Lee, Chi-Sen - FF5F.5, FW5C.4 Karpinski, Michal - FF1D.4 Kim, Ki-Joong - JW4A.137 Kota, Akash - JW4A.86 Kuzin, Evgeny - JTh2A.37, JTh2A.41 Lee, Gun-Yeal - JTh2A.154 Karpinski, Pawel - FTu2C.5 Kim, Kyujung - JW4A.141 Kotkov, Artem - JW4A.94 Kuzyk, Mark G. - LF2D.7 Lee, Kyookeun - JTh2A.154 Key To Authors Karpov, Maxim - FTh4E.3, FTh5G.2 Kim, Ryoung-han - FTu1F.2 Koukourakis, Nektarios - FF1G.3, Kwak, Sean - FW3B.1 Lee, Marianne - FF5A.1 Kasevich, Mark A. - FF5C.5 Kim, Seonghoon - LF2F.2 FW2H.1 Kwiat, Paul - FTu2F.4, FW2B.2, Lee, Minjoo Larry - JTh2A.190 Kashyap, Raman - FTu5I.3, JTh2A.80 Kim, Shin Ho - JTh2A.70 Koulouklidis, Anastasios D. -JTh2A.98 FW3A.4 Lee, Seunghun - JW4A.141 Kasim, Muhammad - FW5E.5 Kim, Sun-je - JW4A.125 Kovacs, K. - LTu1E.2 Kwon, Ojoon - JTh2A.103 Lee, Sung-nam - JW4A.143 Kasture, Sachin - FTu5G.4 Kim, Young H. - FTu1D.5, JTh2A.171 Kovalev, Valeri I. - FF1H.7 Kwong, Dim- Lee - FTh4G.7 Lee, Wei - LF2E.8 Kasumie, Sho - FF5C.8 Kimerling, Lionel C. - JTh2A.163 Kovalova, Marianna - JTh2A.158 Lee, Wonju - JW4A.123 Katayama, Tetsuo - LTu5F.3 Kinnischtzke, Laura - FF5F.7 Kracht, Dietmar - FTu1I.4, FW5B.7 L Lee, Yohan - JTh2A.162 Kato, Takumi - FTh5G.5, JTh2A.150 Kippenberg, Tobias J. - FF3D.6, Krajewska, Aleksandra - JTh2A.105 La Gala, Giada - FF3D.5 Leemans, Wim - FTu1C.1, FTu1C.5 Kauranen, Martti - JW4A.178 FTh4E.3, FTh5G.2, FTu3G, Krasnokutska, Inna - LW2I.3 Labate, Giuseppe - JTh2A.83 Légaré, François - FW5E.3 Kawato, Sakae - JTh2A.194 FTu5D.3, FTu5D.5, FW5F.2 Krauss, Todd - JW4A.136 Labonté, Laurent - FW3B.3 Leger, James R. - FW3H.5 Kazakov, Vasily - JW4A.69 Kira, Mackillo - LTh5I.3 Krausz, Ferenc - FF3C.1, FTu3C.1 Laborde, Margarite L. -JTh2A.30 Lehoucq, Gaelle - FF1F.1 Kazemi Jahromi, Ali - FF1H.2, Kirby, Brian T. -JTh2A.15 Kravchenko, Ivan - JW4A.151 Labuhn, Henning - LTu1E.4 Lei, Liao - JTh2A.35 JW4A.100, JW4A.101 Kireev, Alexey N. -JW4A.180 Kravets, Nina - JW4A.12 Lafave, Timothy - FW5D.5, JW4A.42 Lei, Ming - FF3A.5 Keck, Donald B. - FTu1B.2 Kislov, Anatoly - FTh4C.2 Krenn, Mario - FW3F.1 Lagoudakis, Konstantinos - FF5E.3 Leibovici, Matthieu - FTu1F.4 Keeler, Ethan - JW4A.145 Kiss, Zelma H. - FTh4D.4 Kress, Bernard - FTu5A.1 Lahaye, Thierry - LTu1E.4 Leijssen, Rick - FF3D.5 Keil, Robert - JW4A.181 Kitching, John - FTh5F.4 Krishna, C. Hari - JW4A.36, JW4A.98 Lahiri, Mayukh - FF3C.6 Leisawitz, David T. - FF1G.4 Keller, Mark - LF3I.1 Kivshar, Yuri S. - FF1C.5 Krishna, Sanjay - FTu5D.4 Lai, Kueifu - LTh5H.3 Lemaître, Aristide - FTh4F.4 Kelly, Brian - FTu2C.4 Klamkin, Jonathan - FF5F.1 Krishnappa, Arjun - FF5B.1 Lai, Yi-Ming - FF5F.7 Lemieux, Samuel - FF5C.6 Kelly, Joseph - FTh4E.4 Klas, Robert - FW5E.1 Krolikowski, Wieslaw Z. - FTu2C.5 Lambin Iezzi, Victor - FTu5I.3, Lemos, Gabriela - FF3C.6 Kendrick, Richard - FF1G.6 Klaus, Werner - FTh4E.5 Kröll, Stefan - JW4A.118 JTh2A.80 Lencina, Alberto - JW4A.75 Kenyon, Andrew - FF1H.1 Klee, Anthony - JW4A.84 Krueger, Michael - FTu5C.2 Lambropoulos, John C. - FW3G.1 Lendel, Vasyl - JTh2A.158 Khajavi, Behzad - FTh5B.4, JTh2A.111 Klimas, Aleks - FF3A.3 Krutzik, Markus - FF1H.1 Lamrini, Samir - FW5B.7 Lenzini, Francesco - FTu5G.4 Khakimov, Roman I. - FF3H.7 Klopfer, Brannon B - FF5C.5 Krylyuk, Sergiy - FTu3F.7 Lamstein, Joshua - JW4A.114 Leo, Giuseppe - FF1C.5 Khamedi, Ramin - JTh2A.76 Knarr, Samuel H. - FW5F.6 Kryuchkov, Nikita P. - FTh4C.2 Lan, Pengfei - FTu2C.3, FTu3C.2 Leonardo, Midolo - FTu3D.7, FTu5G.3 Khan, Adnan - FTu3I.6 Knitter, Sebastian - LTu1H.4 Kubarych, Kevin - LTu5H Langrock, Carsten - JW4A.174 Leone, Stephen R. - LTu5F.2 Khan, Imran - FF3D.3 Knox, Wayne H. - FTh4H.4 Kubota, Akihiro - FTh5G.5 Lapkiewicz, Radek - FF3C.6 Lepetit, Thomas - LTu1H.5 Khanikaev, Alexander B. - FW3E.3, Knudde, Nicolas - JW4A.159 Kuchik, Igor - JW4A.165 Larina, Irina - FW5C.1 Lepine, Thierry - JTh2A.140 LF5I.2 Kobayashi, Ryo - JTh2A.7 Kudlinski, Alexandre - FTu5I.2 Larkin, Ilia - FTh4B.3 Lequime, Michel - FW5G.3 Khater, Marwan - FTu2D.2 Kobulashvili, Irina - JTh2A.77 Kudryavtseva, Anna - JTh2A.3 Larson, Walker D. - FF3G.2, FF5D.6 Leszczynski, Adam - FF5C.1 Khaw, Ian - FTu1F.2 Koch, Stephan W. - LTh5I.3 Kudyshev, Zhaxylyk - JW4A.132 Laude, Jean-Pierre - JTh2A.84 Leuchs, Gerd - FF3D.3, FF5D.2, Khodabakhsh, Amir - FTu5C.4 Kociak, Mathieu - JW4A.178 Kues, Michael - FTu3I.1, FW3F.2, Laude, Vincent - FTu5I.2 FTu1G, FW5F.4 Khodzitsky, Mikhail - JW4A.89 Kodigala, Ashok - LTu1H.5 JTh2A.192, JW4A.152 Lauterio Cruz, Jesus Pablo - JTh2A.32 Leuthold, Juerg - FTu3D, FW3E.1 Khoo, Iam C. -JTh2A.93, JTh2A.94 Kolodziejczyk, Andrzej - FW2A.4, Kuipers, Kobus - JW4A.57 Lavery, M. P. - LTu1E.3 Levchuk, Artem - JW4A.39 Khorasaninejad, Mohammadreza - JTh2A.182 Kuipers, L. - FF3H.8, JW4A.82 Lawrie, Benjamin - LF2E.6 Lewalle, Philippe - FTu2G.4 FTh5B.6, JW4A.63, JW4A.65 Kolthammer, Steve - FTu5G.2 Kujawinska, Malgorzata - JTh2A.40 Layden, Emily M. - LF2E.6 Li, Martin - FF5A.1

FiO/LS 2016 • 16–21 October 2016 147 Li, Dan - FTu5B.5 Linfield, Edmund - FTu5G.3 Lopez-Mariscal, Carlos - FTh4B MacChesney, John - FTu1B.3 Marin, Yisbel - FF3B.2 Li, Erwen - JW4A.137 Ling, Alexander - FF5C.3, FTh4F.5, Loranger, Sébastien - FTu5I.3, MacDougall, Dan - FW5C.3 Marinins, Alleksandrs - FTu3F.6, Li, Guangyuan - FTu3D.8 FTu2F.6 JTh2A.80 MacFarlane, Duncan - FW5D.5, JW4A.159 Li, Hao - LF2G.4 Linn, Garrison - JTh2A.115 Lorenzo, Simon - JW4A.163 JW4A.42 Marino, Alberto - JTh2A.2 Li, Haoyu - FTu5B.6, JTh2A.146 Lipson, Michal - FTu1D.1, FTu5D.2 Lougovski, Pavel - FTh5F.5 Machado, Leandro M. - FTu2C.2 Markevicius, Gediminas - FF5B.4 Li, Hebin - JW4A.192 Lisicka-Skrek, Ewa - LTh5I.2 Louisy, M. - LTu1E.2 Machekhin, Yuri P. - FW2E.2 Marozas, Brendan - JW4A.142 Li, Jiantong - FTu3F.6 Litchinitser, Natalia M. - FTh4B.1, Lovell, Gregory L. -JTh2A.72, Maczynska, Ewa - FTh4H.1 Marquardt, Christoph - FF3C, FF3D.3, Li, Junhui - JTh2A.116 FTh4F, FTh5F.1, FTu3C.3 JW4A.23, JW4A.24 Madamopoulos, Nicholas - JTh2A.189 FTh5F.2, FW5F.4 Li, Junying - FF5F.2 Little, Bethany J. - FF3H.2 Lovell, Jonathan L. - FF1A.1, FF5A Madden, Stephen - FTh4G.3 Marrucci, Lorenzo - FF3H.3 Li, Lan - FF5F.2 Little, Brent - FW3F.2, JTh2A.192, Lowder, Tyson L. - FW5E.4 Madonna, Megan C. - FF5A.1 Marshall, Kenneth L. - FW2G.2 Li, Liming - JW4A.74 JW4A.152 Lozano-Crisostomo, Nestor - Mafi, Arash - JTh2A.122, JTh2A.196, Marshall, Kevin A. - FF3D.4 Li, Ming-jun - FTu2B.1 Liu, Cheng - FTu1C.2, FTu1C.3, JTh2A.21, JW4A.18 JW4A.32 Marsili, Francesco - FTh4F.1 Li, Nanxi - FTu2D.5 JW4A.97 Lu, Ling - LTh5H.4 Magana Loaiza, Omar S. - FW2E.5, Mart, Cody - FW5B.4 Li, Qian - JW4A.25, JW4A.26 Liu, Cong - FTh5G.2 Lu, Ming- Feng - JW4A.37 JW4A.64, LTu1E.3 Martin, Anthony - JW4A.27 Li, Qing - LW5I.2 Liu, Dongmei - FF5G.6 Lu, Peixiang - FTu2C.3, FTu3C.2, Magden, Emir Salih - FTu2D.5 Martin, Aude - FF1F.1 Li, Ruxin - JTh2A.96 Liu, Haichun - JW4A.118 JTh2A.24 Mahato, K.K. - FW2C.3 Martin, Graham - JW4A.167 Li, Wei - FF1B.3, FW2F.2 Liu, Huiqing - JW4A.115 Lu, Qijing - JW4A.146 Maia, Lauro - FTu3F.5 Martin, Hubert M. - FTu2A.1 Li, Weile - FF1B.3 Liu, Jiansheng - JTh2A.112 Lu, Tsung-Ju J. - FTh5G.6 Mait, Joseph N. - FW3H.4 Martin, Lane - FF3G.2 Li, Wenzhe - FF5G.5, FTh4E.2, Liu, Juan - FTu5A.3 Lu, Wei - FF5H.2, JW4A.26 Majewska, Anna - FTh5D.3 Martin, Yves - FF5F.3, FTu2D.2 FTh4E.4, JTh2A.193 Liu, Kang - FF3F.3, JTh2A.98 Lu, Yan-Qing - FTu3I.3, JTh2A.174 Maji, Partha - JTh2A.110 Martinez Alvarez, Nuria - LF2G.2 Li, Xue - JW4A.188, JW4A.199 Liu, Ke - FTu3D.1 Lu, Zhaolin - FTu3D.2, JTh2A.144, Majumdar, Arka - FTu3D.1 Martínez Martínez, Ricardo - Li, Yang - FTu3C.2 Liu, Lai - JTh2A.38, JTh2A.39 JTh2A.161, JTh2A.177 Makarov, Vladimir A. - JTh2A.96 JTh2A.21, JTh2A.5

Key To Authors Key To Li, Yuan - FF5G.5, JTh2A.193 Liu, Lin - FF5G.1, JTh2A.65, JW4A.72 Luceri, Vincenza - FTh4F.2 Maker, Gareth - FTh4C.4 Martinez, Amy F. - FF5A.1 Li, Yuanxin - JTh2A.10 Liu, Liying - JW4A.146 Lugani, Jasleen - FF5D.7, JW4A.16 Mäkitalo, Jouni - JW4A.178 Martinez, Julian - FF1D.6 Li, Yuhang - JW4A.21 Liu, Sheng - JW4A.146 Luk, Ting S. - JW4A.162 Makris, Konstantinos G. - FF3H.5, Martinez-Enriquez, Eduardo - Li, Yunqi - FF3G.5 Liu, Weitao - FF1D.6, JW4A.56 Lukens, Joseph M. - FTh5F.5, JTh2A.4, JTh2A.81 FW3A.2, FW5A.4 Li, Zhengyu - JTh2A.23 Liu, Xianlong - JW4A.72 JW4A.174, LF2E.6 Maksimchuk, Nataliya - JW4A.88 Martinez- Felipe, Alfonso - FF3G.7 Li, Zhihong - JW4A.115 Liu, Xiaoli - JW4A.61 Lukishova, Svetlana G. - LF2D.6 Malallah, Ra’ed A. - FTu5B.6, Martini, Francesco - FTh4G.6 Liang, Ya-Ching - JW4A.156 Liu, Ya - FTu5I.6 Lum, Daniel - FW2B.5, FW5F.6 JTh2A.146 Masajada, Jan - JW4A.77 Lianhe, Lianhe - FTu5G.3 Liu, Yang - LF2D.4 Lumer, Yaakov - FTu2G.2, FTu3G.1, Malcolm, Graeme - FTh4C.4 Maser, Daniel - JTh2A.85 Liao, Bolin - JW4A.157 Liu, Yi N. -JTh2A.153 LF5I.3 Malhotra, Tanya - FF1G.2, FF3G.2, Masih, Vandana - JW4A.79 Liao, Chun Yen - JTh2A.143 Liu, Yongmin - JTh2A.176 Lundeen, Jeff S. - FF1C.6, FF1D.3, FF5G.2 Masoller, Cristina - LF2G.2 Liao, Peicheng - FTh4E.3, FTh5G.2 Liu, Yuehan - JW4A.19 FF3C.7, FW2H.2, JW4A.14 Malik, Mehul - FW3F.1, LTu1E.3 Matekovits, Ladislau - JTh2A.83 Liapis, Andreas - LF2D.6 Liu, Yunqi - JW4A.34 Lunghi, Tommaso - FTu3G.3 Malinowski, Marcin - FTh5G.7 Mathias, Stefan - LF3I.1 Liehr, Michael - FF1E.1 Liu, Zhanwei - FTu2I.2 Luo, Bin - JTh2A.116, JTh2A.23 Malushin, Nikolay - JTh2A.91 Mathieson, Keith - FTh4D.5 Lightman, Shlomi - JW4A.41 Liu, Zhiwen - JTh2A.79 Luo, Jingdong - JTh2A.147 Malviya, Nishit - JTh2A.178 Matsuda, Nobuyuki - FW3F.6 Lima, Ivan T. -JW4A.116 Liukaityte, Simona - FW5G.3 Luo, Qiaoen - JW4A.13 Mamykin, Sergiy - JW4A.88 Matsumoto, Morio - JTh2A.38 Limpert, Jens - FW5E.1 Liverman, Spencer T. -JTh2A.56 Luo, Wei - FTu3I.3, JTh2A.174 Man, Mengren - JW4A.5 Matsuo, Shinji - FW5F.3 Lin, Hai - JW4A.50 Lloyd, Seth - FW2B.5 Luo, Wenyong - FF1B.3, FW2F.2 Mancuso, Christopher A. - LF2D.8 Matyba, Piotr - LF3I.1 Lin, Han - FTu5B.4 Lobach, Ivan A. - FTu2I.6 Lupo, Cosmo - FW2B.5 Mann, Vidhi - FF5B.7 Mavrikakis, Manos - LF3I.1 Lin, Hong - JW4A.168 Lobino, Mirko - FTu5G.4 Lustig, Eran - LF5I.3 Manthapuram, Vamsi - FTh5C.7 May Arrioja, Daniel Alberto - Lin, Hongtao - FF5F.2 Lobov, Gleb - FTu3F.6 Lutkenhaus, Norbert - FTh5F.3 Manzoor, Shamaila - JTh2A.25 JTh2A.22, JW4A.18 Lin, Qiang - LF2F.3 Locknar, Sarah A. - FF1A.4 Lvyun, Yang - JTh2A.35 Mao, Hann-Shin - FTu1C.1 Maydykovskiy, Anton - JW4A.155 Lin, Tong - FTu3D.6 Loether, Aaron - FTu2C.4 Lyon, Gholson - FF3A.3 Marangos, Jonathan P. - FTu3C.1, Maynard, Marie-Aude - FF5D.7, Lin, Wei-Chen - LF2G.5 Loncar, Marko - FF1F.4 Lysak, Tatiana - JW4A.170, JW4A.94 LTu2E.2, LTu5F JW4A.16 Lin, Yi- Ling - FW3C.3 Lonergan, Jason - FF5F.2 Marciante, John R. - FW5B.6 Maywar, Drew N. - FTu3I.5 Lin, Yu-Ting - LF2E.8 Loomis, Brianna - FF3A.6 M Marcos, Susana - FTh4I, FW2A.3, Mazilu, Michael - FF5A.4, FTh4C.4, Lin, Zhiyuan - JTh2A.191 Loosen, Florian - FW3H.2 M. V., Jabir - FTh5B.5, JTh2A.18, FW3A.1, FW3A.2, FW5A.4 FTh5E.2, JW4A.198 Lin, Zhong - JTh2A.79 Lopéz, Roberto - JW4A.102 JW4A.8 Marcus, Michael A. - FW2C, FW5G.5 Mazumder, Nirmal - FW2C.3 Lindlein, Norbert - FW3H.2 López-Galmiche, Gisela - JW4A.40 Ma, Tsuhsuan - LTh5H.3 Mardani, Davood - FF3G.2 Mazur, Eric - FTu5B.1

148 FiO/LS 2016 • 16–21 October 2016 Mazur, Yuriy I. -JW4A.175 Milne, Christopher J. - LF3I.4, LTu2E Morissette, Jean- Francois - FTu1D.2 Nakamura, Fumi - JW4A.144 Nishikawa, Tadashi - FTu5C.5 Mcclintock, Luke M. -JTh2A.197 Milojkovic, Predrag - FW3H.4 Moroz, Alexander - JTh2A.141 Nakamura, Kei - FTu1C.1, FTu1C.5 Nishimura, Nozomi - FF3A.2, Mccomb, Timothy S. - FW5E.4 Minaeva, Olga V. -JTh2A.124 Morris, Michael - FTu5A.4 Nakayama, Hirotaka - JTh2A.68 JTh2A.183 Mcdonald, Ch. - LF2H.1 Minamikawa, Takeo - JTh2A.128 Morris, Peter A. -JW4A.166 Nam, Sae Woo - FTh4F.1, FW2B.5 Nithyanandan, Kanagaraj - JW4A.169, Mcevoy, Niall - JTh2A.10 Mira-Agudelo, Alejandro - FW2A.4, Mosk, Allard P. - FF1F.1, FW2D.3 Namba, Yoshiharu - FW5G.2, JW4A.46 McFadden, Clare - FF3A.4 JTh2A.182 Moskaletz, Oleg - JW4A.69 JW4A.58 Noda, Susumu - LF1I.2, LF2F McFadden, Sally A. - FW5A.2, Miranda, M. - LTu1E.2 Moss, David J. - FW3F.2, JTh2A.192, Namekata, Naoto - JTh2A.7 Nogajewski, Karol - FF5B.8 FW5A.4 Mirhosseini, Mohammad - FW2E.5, JW4A.152 Nannipieri, Tiziano - FF3B.2 Noh, Jiho - LTh5H.1 McGill, Stephen - JTh2A.115 JTh2A.14, LTu1E.3 Mossad, Hany - JTh2A.169 Narayanamurthy, Chittur S. - FW5H.7 Nomoto, Sean M. -JW4A.190 McIntyre, Brian - FW2E.5 Miri, Mohammad A. - LF2E.3 Motes, Keith R. -JTh2A.30 Narhi, Mikko - FTu3I.4 Noor, M. Sohail - FTh4D.4 McKay, Christopher - JTh2A.127 Mironov, Andrey - JTh2A.12 Moulder, Todd - JTh2A.30 Narimanov, Evgenii E. - FTu1G.2 Norreys, Peter A. - FW5E.5 McLeod, Euan - FTh4C.1 Miroshnichenko, Andrey E. Mouradian, Levon - JW4A.44 Nash, Geoff R. -JTh2A.75 Norrman, Andreas - FF5H.1, McMackin, Lenore - FTh5C.4 -JTh2A.141 Mousavi, Monirehalsadat - JW4A.118 Nasiriavanaki, Mohammadreza - JTh2A.152 McMullan, Simon - JTh2A.181 Mirshafieyan, Seyed Sadreddin - Mrejen, Michael - FTu1G.3 JW4A.62 North, Thibault - FTu5D.3 McReynolds, Naomi - FF5A.4 JW4A.162 Mueller, Christian R. - FF3D.3 Natarajan, Arun - JTh2A.56 Notingher, Ioan - JW4A.112 Key To Authors Meany, Thomas - FTu3G.3 Mirza, Imran M. - FW3F.5 Muhonen, Juha - FF3D.5 Naumov, Andrei - FTu5C.3, LTh5I.2 Nouri, Mehdi - FW5D.5 Medicus, Kate - FTu2A Miseikis, L. - LTu2E.2 Mukherji, Soumyo - FF3B.4 Navarro-Gonzalez, Rafael - JTh2A.127 Novotny, Lukas - FF5B.2, FTu2F.5 Meemon, Panomsak - JW4A.106 Mishra, Ishan - JW4A.63, JW4A.65 Mulhollan, Zachary - FW5H.5 Nawarathna, Dharmakeerthi - Nowierski, Samantha - FW3B.2 Mejía, Hans A. -JW4A.184 Mishra, Vishwatosh - FTu3I.2, Muller, Matthew S. - FW2H.5 JW4A.116 Numata, Hidetoshi - FTu1D.2 Mejooli, Menansili A. - FTh5D.5 JTh2A.50 Müller, Walter - FTh4C.3 Nawrot, Michal - FF3G.6 Nunley, Hayden - JTh2A.2 Melninkaitis, Andrius - FTu2C.1 Mitchell, Arnan - FTu2C.5, FTu5G.4 Mullins, John - FF3A.4 Nayfeh, Ammar - FTu3F.2 Nunn, Joshua - FTu5G.2 Melo, Emerson G. -JTh2A.156 Mitetelo, Nikolai - JW4A.155 Mun, Sang-Eun - JTh2A.154 Neal, Daniel - FW3A Nunnenkamp, Andreas - FF3D.6 Mendonça, Cleber R. - LF2D.3 Mittal, Sunil - LF5I.4 Munday, Jeremy N. -JTh2A.159 Nellikka, Apurv Chaitanya - FTh5B.5, Mendoza-Hernández, Job - JW4A.91 Mittelberger, Daniel E. - FTu1C.1 Muniraj, Inbarasan - FTu5B.6, JW4A.8 O Menezo, Sylvie - FF1E.3 Miyamoto, Shuji - JTh2A.128 JTh2A.146 Neshev, Dragomir N. - FF1C.5 O, Kenneth K. -JW4A.42 Meng, Xiang - FTu2D.4 Mobini, Esmaeil - JTh2A.196 Munro, William J. - FW3F.6 Ness, Sallyanne L. -JTh2A.183 O’Sullivan, M. N. - LTu1E.3 Meng, Xiangyue - FW2C.5 Mohajerin-Ariaei, Amirhossein - Muramatsu, Kyosuke - JW4A.144 Neto, Antonio M. -JTh2A.132 O’Beirne, Aidan - JTh2A.115, Menyuk, Curtis R. -JW4A.189 FTh4E.3, FTh5G.2 Murari, Kartikeya - FTh4D.4 Neukirch, Levi - JW4A.153 JTh2A.197 Merano, Michele - JTh2A.11, Mohamed, Ali - JW4A.90 Murnane, Margaret M. - LF2D.8, Neuman, Tomas - FW3E.3 Oblak, Daniel - FTh4F.1 JTh2A.89, JW4A.128, JW4A.131 Mohammad, Abu B. -JW4A.29 LF3I.1 Neumann, Jörg - FTu1I.4, FW5B.7 O’Brien, Jeremy L. - FF4A.1, FTu1D.3, Merklein, Moritz - FTh4G.3 Moille, Gregory - FF1F.1 Murphree, Joseph D. - FW2E.3 Neumark, Daniel M. - LTu5F.2 FTu3G.5 Merolla, Jean-Marc - FTu3I.4 Mojahedi, Mo - FF5H.8, JW4A.193 Murphy, Helen - FF5A.1 Neveu, Pascal - FF5D.7, JW4A.16 O’Brien, Kevin P. - FF5H.7 Mertens, Lena - JW4A.43 Molander, William - LF2G.8 Murshid, Syed H. -JTh2A.72, Newburgh, G. A. - FW5B.6 O’Brien, Peter A. - FF3E.2 Mertz, Jerome - FW5C Molina, Alejandro - JTh2A.48 JW4A.20, JW4A.22, JW4A.23, Newman, Jason A. -JW4A.13 Ochiai, Tetsuyuki - FF3C.3 Mertz, Jerome C. - FF3A.1 Momgaudis, Balys - FTu2C.1 JW4A.24 Neyra, E. - JW4A.104 Odele, Ogaga D. - FW5F.5, Messias, Djalmir N. -JW4A.107 Moncaster, Juliet A. -JTh2A.124 Musial, Marta E. -JTh2A.186 Ng, D. K. T. - FTh4G.5 JW4A.174 Metzger, Nikolaus K. - FTh4C.4 Mondal, Dipankar - JTh2A.117 Musslimani, Ziad - JTh2A.4 Ng, Daniel - JW4A.120 O’Donnell, Ryan - JW4A.183 Metzler, Rebecca A. - FTu2G.5 Monro, Tanya M. - FF5H.4 Mutti Od Phd, Donald O. - FW5A.1 Ngah, Lutfi A. - FW3B.3 Oh, Dong Yoon - FTh5G.3 Meunier, Vincent - LF2F.1 Montazeri, Kiana - JTh2A.6 Mutugala, Udara - FTh4G.3 Nguyen, Lim - JW4A.2 Oh, Jaewon - FTh5B.6, JW4A.63, Michalko, Aaron - FW5H.4 Monte, Adamo F. -JW4A.107 Nguyen, Peter - FF3F.2 JW4A.65 Michinel, Humberto - FW2E.4 Moon, Benjamin - JW4A.145 N Nguyen, Thinh - JTh2A.56 Oh, Yougjin - JW4A.123 Mihaylova, Dilyana - LF2D.6 Moradi, Ali-Reza - JTh2A.76 Nabeshima, Camila T. -JTh2A.132 Ni, Chenquan - JW4A.188, JW4A.199 Ohishi, Yasutake - JTh2A.100, Milchberg, Howard - FTh4B.3, LF2G.6 Morandotti, Roberto - FTu3I.1, Nabet, Bahram - JTh2A.6 Nic Chormaic, Sile - FF5C.8, JTh2A.38, JTh2A.39, JTh2A.42, Milione, Giovanni - LW3I.2 FTu3I.4, FW3F.2, JTh2A.192, Nacke, Codey - FF1D.3 JTh2A.34 JW4A.188, JW4A.199 Miller, Bill - FTh4C.4 JW4A.152 Naderi, Nader N. - FW5B.1, FW5B.5 Niebuhr, Mario - LF2G.3 Ohodnicki, Paul - JW4A.137 Miller, David - FTu1D.3 Moreno, Pablo - JW4A.83 Nagasaka, Kenshiro - JTh2A.39, Nieddu, Thomas - JTh2A.34 Oi, Daniel - FTh4F.5 Miller, Keith - FF5G.5, FTh4E.2, Moresco, Michele - FTu2D.5 JTh2A.42 Niederriter, Robert - FTh5B.2, Okabe, Yusuke - FTh5G.5, JTh2A.150 FTh4E.4, JTh2A.193 Morgan, Kaitlyn S. - FTh4E.2, FTh4E.4 Nagashima, Takuji - FTh5E.3 JW4A.87 Okawachi, Yoshitomo - FTu5D.2 Miller, Nicholas A. - LF2D.1 Morioka, Motoki - JTh2A.195 Nah, Jae-Woong - FF5F.3 Niemi, Tapio - JW4A.178 Okulov, Alex - JTh2A.188 Miller, Owen - FF1F.3, LF2E, LTh5I.4 Morioka, Toshio - FTh4E.6 Nakagawa, Wataru - JW4A.145 Nishi, Hidetaka - FW3F.6 Okuno, Yudai - FW5D.6

FiO/LS 2016 • 16–21 October 2016 149 Oliver, James - JW4A.48 Pannian, Jisha C. - FF3H.3, JW4A.10, Peuntinger, Christian - FF3D.3 Priyantha, Weerasinghe - JW4A.142 Rangarajan, Prasanna - FTh5C.1 Olivieri, Anthony - LTh5I.2 JW4A.12 Pfeiffer, Martin Hubert Peter - Priye, Vishnu - JTh2A.178 Rao, Ashutosh - FTh5G.7 O’Loughlin, Trevor A. -JW4A.142 Panov, Nikolay A. - JTh2A.96 FTh4E.3, FTh5G.2, FTu5D.3 Prokopeva, Ludmila - JW4A.132 Raposo, Ernesto - FTu2G.3 Olson, Jonathan P. -JTh2A.30 Papa, Jonathan - FW5H.3 Pfund, Johannes - FW5G.6 Pronin, Oleg - FTu3C.1 Rasras, Mahmoud - FTu3F.2 Omatsu, Takashige - FTh5B.1 Papaioannou, Maria - FF5G.7 Phillips, David B. - FTh5C.5 Pryde, Geoff J. - FF1C.3, FF1C.4 Rastogi, Vipul - FF5B.7 Omidi, Parsa - JW4A.62 Papazoglou, Dimitrios G. -JTh2A.98 Pi, Shaohua - JW4A.30 Przewolka, Aleksandra - JTh2A.105 Ratan, Naren - FW5E.5 Ooi, Kelvin J. A. - FTh4G.5 Papp, Scott - JTh2A.114 Piccardi, Armando - JW4A.12 Pu, Jixiong - JW4A.110 Rathje, Christopher - FF3F.2 Ooka, Yuta - FTu2D.3 Parappurath, Nikhil - JW4A.57 Piccirillo, Bruno - FF3H.3 Pu, Minhao - FTh4E.6 Rattan, Anurag - FW2C.5 Oppeneer, Peter M. - LF3I.1 Paredes, Angel - FW2E.4 Piché, Michel - FF5G.3 Pulford, Benjamin - FW5B.3, FW5B.4 Ravets, Sylvain - LTu1E.4 Orazi, Leonardo - JTh2A.113, Parigi, Valentina - FTh4F.3 Pidishety, Shankar - FTu3I, FTu5I.5 Punjabi, Nirmal S. - FF3B.4 Ravizza, Frank - LF2G.8 JW4A.88 Park, Han Sang - JTh2A.126 Piecuch, Martin - LF3I.1 Purnawirman, Purnawirman - FTu2D.5 Rawlinson, Willa - JW4A.191 Orcutt, Jason S. - FTu2D.2 Park, Hyunwook - LF2H.3 Piers, Patricia - FW2A.2 Pütz, Gilles - JW4A.27 Raymer, Michael G. - FW2B.4, LF2E.4 Orenstein, Gal - FTu5C.2 Park, Sung-Jin - FF1H.4 Pilnyak, Yehuda - FF1D.5 Rebollar, Esther - JW4A.83 Orieux, Adeline - FTh4F.4 Parker, Kevin - JTh2A.131 Pimenta, Hudson - JTh2A.20 Q Rechtsman, Mikael C. - FTu3G.1, Oriol, Luis - FF3G.7 Parniak, Michal - FF5C.1, FW3F.3 Pincheira, Pablo I. - FTu2G.3 Qazi, Hummad - JW4A.29 LTh5H.1 Orozco, Luis A. - FTu3I.6, JTh2A.159, Parsons, Joshua - FW5B.3 Piñol, Milagros - FF3G.7 Qi, Minghao - FW5F.5, JW4A.150 Redding, Brandon - JTh2A.190 LTu1E.4, LW5I.4 Pascual, Daniel - FW2A.3, FW3A.1, Pittman, Todd B. - FF5D.5, JW4A.171 Qi, Zhengqing - FTu1F.2 Reddy, Dileep V. - FW2B.4, LF2E.4 Orre, Venkata Vikram - LF5I.4 FW3A.2 Plansinis, Brent - FF3H.1, FF3H.2 Qian, Xiao- Feng - FF3C.5, JTh2A.17 Reed, Graham T. - FTu5D.1 Osgood, Richard M. - FTu2D.4, Pasternak, Iwona - JTh2A.105 Plociniczak, Lukasz - JW4A.77 Qiang, Xiaogang - FTu1D.3 Reena, Reena - JW4A.154 JW4A.149 Paszkiewicz, Sandra - JW4A.83 Plotnik, Yonatan - FTu3G.1, LF5I.3 Qiao, Jie - FTu3C, FTu5B, FTu5B.3, Regan, Brian - FTu2G.5 Östling, Michael - FTu3F.6 Patel, Raj - FF1C.3 Plum, Eric - FF5G.7 FW5H.5 Rehacek, Jaroslav - FF3D.3 Otange, Ben O. - FF5A.5 Patterson, Burkley - FTu3I.6, Pobiedina, Valentina - JW4A.39 Qiao, Yucheng - JTh2A.23 Reichert, Matthew - JTh2A.26,

Key To Authors Key To Oton, Claudio - FF3B.2 JTh2A.159, LW5I.4 Poddubny, Alexander - FF1C.5, Qiu, Chengwei - LF2G.4 JW4A.11 Ottenhues, Christoph - FW5B.7 Pavone, Francesco S. - FTh4D.1 FTu5G.4 Qiu, Jianjun - FW2C.3 Reimer, Christian - FF3F, FW3F.2, Ouerdane, Youcef - FW2F.1 Pedatzur, Oren - FTu5C.2 Poletti, Francesco - FTu2I.3 Qiu, Ling - FTu5B.5 JTh2A.192, JW4A.152 Ourari, Salim - JW4A.168 Pelli, Denis G. - FTh4I.2 Politi, Alberto - FTh4G.6 Quesada, Nicolas - JW4A.182 Reimers, Jacob - FW5H.1 Ouzounov, Dimitre G. -JTh2A.183 Pelliccia, Daniele - FTh5C.2 Pomerantz, Michael - JTh2A.69 Reinoso, Jose - LF2G.2 Owusu, Alfred - JTh2A.95 Pender, Mitchell A. - FTh5D.5 Pongchalee, Pornthep - JW4A.106 R Reis, Arnaldo F. -JW4A.107 Oxenløwe, Leif Katsuo - FTh4E.6 Peng, Bo - FTu1D.2, FTu2D.2 Ponomarenko, Sergey - FF5H.1 Ra, Young-sik - FTh4F.3 Reis, David A. - LF2H.4, LTh5I Oyugi, Julius O. - FF5A.5 Peng, Junzheng - JW4A.61 Poon, Andrew W. - FF1F, FTu2D.1 Rabiei, Payam - FTh5G.7 Rekas, Marek T. - FW2A.4 Oza, Neal N. - FW3B.2 Peng, Xiang - JTh2A.23, JW4A.61 Pooser, Raphael - LF2E.6 Radhakrishnan, Aiswaryah - FW3A.1 Remer, Itay - JTh2A.133 Peng, Xiaopeng - FTh5C.3 Popiolek-Masajada, Agnieszka - Radic, Stojan - FTu3B.2 Ren, Haoran - JTh2A.149 P Percino Zacarias, Elizabeth - JTh2A.66 JW4A.77 Radwell, Neal - FTh5B.3, JW4A.80 Ren, Juanjuan - JTh2A.93, JTh2A.94 Padgett, Miles J. FTh5C.5, FW5F, Percino, Maria Elizabeth - JTh2A.59 Popov, Sergei - FTu3F.6, JW4A.159 Rae, Philip J. -JW4A.153 Ren, Y. - JTh2A.9 JW4A.43, FF1D.2, FW2B.3, Pereira, Dionísio - FTu2I.5, JTh2A.173 Popovic, Milos - LW5I.1 Raghuwanshi, Sanjeev K. -JTh2A.36 Renema, Jelmer - FTu5G.2 JW4A.166, JW4A.4, LTu1E.3 Perez-Hernandez, J.A. - JW4A.104 Pors, Anders - FF1G.5 Raikin, Jared - JTh2A.183 Renganathan, Abhishek - FW2C.5 Paesani, Stefano - FTu1D.3, FTu3G.5 Perez- Leija, Armando - JW4A.181 Pottiez, Olivier - JTh2A.32, JTh2A.41 Rakha, Emad - JW4A.112 Reno, John - JTh2A.115 Paganin, David M. - FTh5C.2 Perez-Merino, Pablo - FW5A.4 Poulain, Marcel - FTu1I.2 Ralph, Timothy C. - FF1C.2, FF1C.3 Restuccia, Sara - FW2B.3 Pagliano, Francesco - FTu5G.3 Perez-Roldan, Maria Jesus - FW2C.4 Poulain, Samuel - FTu1I.2 Ramachandran, Siddharth - FTu5I.5, Retzker, Alex - FF1D.5 Paillard, Charles - JW4A.195 Perlstein, Joshua - FW5H.8 Pourbeyram Kaleibar, Hamed - FW2B.4 Revuelta, Luis - FW5A.4 Paine, Scott - FTu2F.3 Pertot, Yoann - LTu2E.1 JW4A.32 Ramaiah-badarla, Venkata - FTu5C.4 Reyes Esqueda, Jorge Alejandro - Pal, Bishnu P. - JTh2A.51, JW4A.148 Peruzzo, Alberto - LW2I.3 Pourvais, Yousef - JTh2A.1, JTh2A.76 Raman, Aaswath - FF1F.2 JW4A.102, JW4A.99 Palashov, Oleg - JTh2A.87 Petek, Hrvoje - LTu5H.1 Poutrina, Ekaterina - FTu5G.6 Ramanujam, Nirmala - FF5A.1 Rezvani Naraghi, Roxana - FF5B.3, Palastro, John - LF2G.6 Petelczyc, Krzysztof - FW2A.4, Powis, Simon J. - FF5A.4 Ramezani, Hamidreza - LF2E.2 JW4A.6 Palmieri, Luca - FTu5I.1, JW4A.17 JTh2A.182 Preble, Stefan F. - FF1E, FF3E, FF4A, Ramírez Flores, José Alfredo - Rhodes, Michelle - FW5E.2 Palodiya, Vikram - JTh2A.36 Peters, Achim - FF1H.1 FF5E, FF5F.5, FTh4G, FTh5G.6, JTh2A.21, JTh2A.5 Rhodes, William T. -JW4A.96 Palomba, Stefano - FTu3D.8 Peters, Nicholas - LF2E.6 FTu3G.4, FTu5D, FW5C.4, LW2I.1 Ramírez Martínez, Daysi - JW4A.102, Ricciardi, Armando - FF1B, FF3B.1 Pan, Lillyan D. -JTh2A.183 Petrenko, Sasha - FW2D.1 Presti, D. - JW4A.161 JW4A.99 Rice, Perry - LW5I.4 Pan, Yingling - FTu5I.6, JW4A.31 Petruzzella, Maurangelo - FTu3D.7, Price, Patrick - JTh2A.86, JTh2A.90 Ramos, Carlos - FF5F.2 Richardson, David - FTu3B.1 Panneton, Denis - FF5G.3 FTu5G.3 Prince, Kevin - LTu2E.3 Rand, Stephen - FF3F.4

150 FiO/LS 2016 • 16–21 October 2016 Richardson, Kathleen A. - FF5F.2, Roztocki, Piotr - FW3F.2, JTh2A.192, Santhanam, Anand - FW2C.1 Seibel, Eric - FF1A.3 Shi, Zhimin - FTu1F.2, JTh2A.172, FW2G.1, JTh2A.163 JW4A.152 Santos, Jose Luis - FF1B.1, FF3B Seidel, Marcus - FTu3C.1 LTu1E.3 Rider, Sebastien - FF3A.4 Ruane, Garreth - JW4A.1 Sarangi, Srikant - JTh2A.124 Seller, Paul - FTu1C.3 Shibata, Hiroyuki - FW5F.3 Riesen, Nicolas N. - FF5H.4 Rudawski, P. - LTu1E.2 Sarkar, Anirban - JW4A.179 Selyem, Adam - JW4A.80 Shibutani, Hideaki - FW5D.6 Rigneault, Hervé - FF1A.5 Rudolph, Terry - FTu1D.3 Sarkar, Resham - JTh2A.16 Semenov, Alexander - FW2E.2 Shih, Jyun- Fu - JW4A.156 Rippe, Lars - JW4A.118 Rueda, Edgar - JW4A.75 Sarma, R. - FW2D.1 Senellart, Pascale - LW2I.4 Shimizu, Kaoru - FW3F.6 Ritsch-Marte, Monika A. - FW2E.1 Ruesink, Freek - LF2E.3 Sarriugarte, Paulo - FW2C.4, FW3E.3 Sengupta, Amartya - JW4A.9 Shimobaba, Tomoyoshi - JTh2A.68 Ritt, Michael - JTh2A.130 Runyon, Matthew T. - FW2H.2 Sato, Toru - JTh2A.194 Sension, Roseanne J. - LF2D.1 Shipilo, Daniil E. - JTh2A.96 Rivera, Jose A. - FF1H.3, JW4A.54 Russell, Philip S. -JTh2A.135, LW5I.5 Saunders, Dylan - FTu5G.2 Seo, Giwan - JTh2A.70 Shipp, Dustin W. -JW4A.112 Rivera, Nicholas - LF2E.5 Russo, Juan - FTu5A.5 Savich, Gregory - JW4A.142 Seok, Tae Joon - FTu1D.6 Shirai, Tomohiro - FTh4C.6 Rizza, Giancarlo - JW4A.178 Rutkowski, Lucile - FTu5C.4 Savona, Vincenzo - LF2F.4 Sephton, Bereneice C. - FF5H.5, Shiraki, Atsushi - JTh2A.68 Robin, Thierry - FW2F.1 Ryczkowski, Piotr - FTh5A.3, FTh5C.6 Sawado, Yoshinori - FW5D.6 FTh4B.5 Shivanand, Shivanand - FF5B, FW2E Rochette, Martin - FTh4A.3 Ryu, Guen-Hwan - JTh2A.13 Sayinc, Hakan S. - FTu1I.4, FW5B.7 Septriani, Brigitta - FF5C.3 Shkurinov, Aleksander P. - JTh2A.96 Rodenburg, Brandon - FW2E.5, Ryu, Han-Youl - JTh2A.13 Sazio, Pier J. A. - FTu1I.1, FTu2I.3 Sergienko, Alexander V. - FF1D, Shorey, Aric B. - FW3G.2 JW4A.164, LTu1E.3 Schaeffel, Frank - FW5A FF5D.3 Shramkova, Oksana V. - FF3H.5 Key To Authors Rodrigo, Jose A. - FF5G.4, JTh2A.108 S Schaffer, Chris B. - FTh5D.5, Serpengüzel, Ali - JTh2A.180 Shrivastav, Anand M. -JTh2A.44, Rodriguez Beltran, Rene I. -JW4A.83 S. Magaña- Loaiza, Omar - JTh2A.14 JTh2A.183 Serrano, Alejandra - JTh2A.198 JTh2A.52, JTh2A.53 Roelkens, Gunther - FF5F.4 Saaltink, Rebecca - FF1C.6 Scharf, Robert - FTh4D.5 Setälä, Tero - JTh2A.152 Shukla, Mukesh K. -JTh2A.110 Rogers, Edward T F - FF5G.7 Sabinas Hernandez, Sergio - JW4A.99 Schein, Perry - JW4A.108 Severiano Carrillo, Israel - JW4A.85 Shvedov, Vlad - FTu2C.5 Rogers, John R. - FW3H.1 Sacher, Wesley D. - FTu2D.2 Scherer, Axel - FTh4G.4 Shabahang, Soroush - FF3G.2, Shvets, Gennady - FW3E.3, LTh5H.3 Rohde, Peter P. -JTh2A.30 Sadeq, Zaheen S. - FF5H.6 Scheuer, Jacob - FF1B.2 FW5H.8, JW4A.101 Shy, Jow-Tsong - LF2G.5 Rojas Laguna, Roberto - JTh2A.32 Sadler, James - FW5E.5 Schiavon, Matteo - FTh4F.2 Shadbolt, Pete - FTu1D.3 Siadat Mousavi, Saba - LTh5I.2 Rolland, Jannick P. - FTu1A, Saeidi, Shayan - JTh2A.179 Schiemangk, Max - FF1H.1 Shafeeque Ali, A.K. - JW4A.169 Siahmakoun, Azad - JTh2A.160 FW2C.1, FW5H.1, FW5H.3, Safari, Akbar - JW4A.4 Schiesser, Eric M. - FW5H.3 Shahoie, Hiva - FW5D.5 Šiaulys, Nerijus - FTu2C.1 FW5H.6, JTh2A.129, JTh2A.131, Safavi-Naeini, Amir - FF1F.5 Schilling, Ryan - FF3D.6 Shahriar, Selim - FF1B.2, FF1H.8, Siddaramaiah, Manjunath - FW2C.3 JTh2A.138, JTh2A.140, JTh2A.69, Saha, Nabarun - JW4A.130 Schipf, David R. - FF1G.7 JTh2A.102, JTh2A.16 Sidor, Daniel - JW4A.142 JW4A.106 Sahota, Jaspreet - JW4A.182 Schkolnik, Vladimir - FF1H.1 Shalaev, Mikhail - FTh4B.1 Sidorov, Pavel - JW4A.165 Rolland-Thompson, Kevin - FW2C.1 Sai Shankar, Madhuvarasu - JW4A.36 Schlotter, William F. - LF3I.3 Shankhwar, Nishant - JW4A.92 Siemens, Mark - FTh5B.2, JW4A.87 Rollinger, Markus - LF3I.1 Sakai, Shigeaki - JTh2A.164 Schmidgall, Emma - FF5F.6 Sharma, Katelynn - FF3G, JW4A.48, Siemers, Troy J. -JW4A.167 Rolston, Steve L. - FTu3I.6, Sakaidani, Takahide - JTh2A.7 Schmidt, Bruno - FW5E.3 JW4A.49 Silahli, Salih - FTh5F.1 JTh2A.159, LTu1E.4, LW5I.4 Salamo, Gregory J. -JW4A.175 Schmidt, Markus - FW3E.4 Sharum, Haille - FF3F.2 Silberhorn, Christine - FF4A.2 Rook, Caitlin A. -JTh2A.124 Salandrino, Alessandro - FF5H.7 Schneeloch, James - FW5F.6 Shaw, Brandon - FTh4A.1 Silva, Andréa - FTu2G.3 Rop, Ronald - FF5A.5 Salazar-Bloise, Félix - FF5B.3 Schneider, Christian - LF2F.2 Shaw, Brian H. - FTu1C.5 Silva, Daniel L. - LF2D.3 Ropers, Claus - FTu5C.3 Saleh, Bahaa E. - FF5D.6, FW2C.2, Schnell, Martin - FW2C.4, FW3E.3, Shaw, Matthew - FTh4F.1 Silva, Flávia R. -JTh2A.132 Roques-Carmes, C. - JW4A.63 JW4A.181 JTh2A.78 Sheets, Donal - LF2G.7 Simas, Alfredo M. - LF2D.3 Rorrer, Gregory - JTh2A.127 Saleh, Mohammed F. - FTu3G.6 Schoen, John M. - FTu2A.2 Shelkovnikov, Alexander S. Simon, David S. - FF5D.3 Ros, Francesco Da - FTh4E.6 Sales, Tasso R. - FTu5A.4 Schotland, John C. - FW3F.5 -JW4A.180 Simon, Jonathan - LF5I.1 Rosenberg Petersen, Christian - Samad, Ricardo E. - FTu2C.2, Schroder, Tim - LTu3H.1 Shen, Xuechu - FF5H.2 Simon, Peter - FW5G.2 FTh4A.2 JTh2A.132 Schroeder, Carl B. - FTu1C.1, FTu1C.5 Shen, Yichen - FTu1F.5, FW5D.3, LF1I Simone, Birindelli - FTu5G.3 Rosenberg, Jessie C. - FTu2D.2 Samano Aguilar, Luis F. -JTh2A.32 Schuck, Carsten - FTh5G.4 Shen, Zhen - LF2E.1 Sincich, Lawrence - FTh5D.1 Rosenthal, Eric - FTh4B.3 Samanta, Goutam K. - FTh5B.5, Schuetz, Hendrik - FF3D.6 Sheng, Yan - FTu2C.5 Sinclair, Laura - FTu5C Roslaniec, Zbigniew - JW4A.83 JTh2A.18, JW4A.8 Schultz, Justin T. - FW2E.3 Sheridan, John T. - FTu5B.6, Singh, Gurpreet - FTu2D.5 Roso, L. - JW4A.104 Sanchez Mondragon, Javier - Schulz, Sebastian A. - FTu1G.4, JTh2A.146 Singh, Satya P. - FTu3I.2, JTh2A.50 Rostovtsev, Yuri - FTu1G.3 JTh2A.21, JTh2A.22, JTh2A.5, FTu3D.4, JW4A.64 Shi, Jianmin - JW4A.183 Singh, Surendra - JW4A.190, Rothhardt, Jan - FW5E.1 JW4A.18, JW4A.40 Sciarrino, Fabio - FF1C.1, FW3F Shi, Kaifeng - FTu3D.2, JTh2A.144, JW4A.195 Rotter, Mark - LF2G.8 Sánchez-Soto, Luis L. - FF3D.3 Seddon, Angela - FTh4A.4 JTh2A.161, JTh2A.177 Sinha, Ravindra K. -JW4A.154, Rotter, Stefan - JTh2A.4 Santagati, Raffaele - FTu1D.3, Sedlmeir, Florian - FW5F.4 Shi, Lingyan - LTu2H.2, LW3I JW4A.92 Rowland, Kenneth - FW5B.5 FTu3G.5 Segev, Mordechai - FTu2G.2, Shi, Wenjing - FTu3C.2 Sinha, Uttam - FF5B.1 Roxworthy, Brian J. - FTu3D.5 Santagiustina, Marco - JW4A.17 FTu3G.1, LF5I.3, LTh5H.4 Shi, Yun-chao - FTu3I.3 Sipe, John E. - FF5H.6, FTu3D.4, Roy, Sourabh - JW4A.98 Santamato, Enrico - FF3H.3 JW4A.140

FiO/LS 2016 • 16–21 October 2016 151 Sirbu, Lilian - JTh2A.179 Spalding, Gabriel - FF1D.2 Sun, Liaoxin - FF5H.2 Tankam, Patrice - FW2C.1, Tison, Christopher C. - FTh5G.6, Sirutkaitis, Valdas - FTu2C.1 Spano, Samantha - FTu2G.5 Sun, Ming-jie - FF1D.2, FTh5C.5 JTh2A.129, JTh2A.140 FTu3G.4, LW2I.1 Sit, Alicia - FW2H.2 Spesyvtsev, Roman - FTh4C.4 Sun, Qi - FTu1I.1 Tanzilli, Sébastien - FTu3G.3, FW3B.3, Titchener, James - FTu5G.4 Sivankutty, Siddharth - FF1A.5 Squier, Jeff - JTh2A.57 Sun, Shuai - FTu3D.1 JW4A.27 Tittel, Wolfgang - FTh4F.1 Sivaramakrishnan, Sivaraj - JTh2A.130 Squire, Kenneth - JTh2A.127 Sun, Xiaohang - JW4A.11 Tao, Ran - JW4A.37 Titze, Michael - JW4A.192 Sivis, Murat - FTu5C.3 Srimathi, Indumathi R. - FTh4E.2, Suratwala, Tayyab I. - FW5G.1 Tao, Zhensheng - LF3I.1 Tkach, Robert - FTu2B.3 Skobeeva, Valentyna - JTh2A.91 FTh4E.4 Sussman, Benjamin J. - JW4A.14 Taru, Toshiki - FTh5E.3 Tkachenko, Georgiy - JW4A.198 Slablab, Abdallah - JW4A.178 Srinivasan, Balaji - FTu5I.5 Suzuki, Ryo - JTh2A.150 Taucer, Marco - FTu5C.3, FW5E.3 To, Dong B. -JW4A.138 Slavik, Radan - FTh4G.3 Srinivasan, Kartik - LW5I.2 Suzuki, Takenobu - JTh2A.100, Taylor, J. R. - LW3I.1 Toenger, Shanti - FTu3I.4 Slussarenko, Sergei - FF1C.4, FF3H.3 Srivastava, Anchal - JW4A.79 JTh2A.38, JTh2A.39, JTh2A.42, Taylor, Jonathan - FF3A.4, FTh5C.5 Tofighi, Salimeh - JW4A.183 Smalakys, Linas - FTu2C.1 Srivathsan, Bharath - FF5D.2 JW4A.188, JW4A.199 Taylor, Lauren - FTu5B.3 Toivonen, Juha - FTh5A.3 Small, David M. - FF3A.2 Stahl, Charlotte - FTh4B.4 Svyakhovskiy, Sergey - JW4A.155 Tchahame, Joel Cabrel - FTu5I.2 Tokumoto, Takahisa - JTh2A.115 Smid, Jason - JW4A.117 Staudte, Andre - FTu5C.3, LTh5I.2 Swanson, Kelly K. - FTu1C.5 Tchakui, Murielle Vanessa - Toliver, Paul - FTu5I.4 Smith, A. Matthew - FTh5G.6 Steel, Michael - FTu3G.3 Swartzlander, Grover A. - FF1H.5, JTh2A.118, JTh2A.119 Tomasin, Marco - FTh4F.2 Smith, Bradley - FF3F.4 Steelman, Zachary A. -JTh2A.126 FF3H.4, FTh5C.3, JW4A.1 Tcherniega, Nikolay V. -JTh2A.3 Tomomatsu, Yasunori - FW5D.6 Smith, Brian J. - FF1D.4, FTu5G.2 Steidle, Jeffrey A. - FF5F.5, FTh5G.6, Swiecicki, Sylvia D. - FTu3D.4 Tebbenjohanns, Felix - FF5B.2 Toneyan, Hrach - JW4A.44 Smith, Christopher - JW4A.48 FTu3G.4, LW2I.1 Swiecicki, Sylvia D. -JW4A.140 Tegegne, Newayemedhin A. Tong, Hoang Tuan - JTh2A.38, Smith, Earl - FW2A.1 Steinberg, Aephraim M. - FTu2F.1 Swillam, Mohamed - JTh2A.169, -JTh2A.88 JTh2A.39, JTh2A.42 Smith, Matt - JW4A.197 Steinke, Michael - FW5B.7 JW4A.135 Teh, Daniel - JW4A.117 Tong, Jonathan - FW2E.2, JW4A.157 Smith, Roger - FW2B.4 Steinke, Sven - FTu1C.1, FTu1C.5 Sydor, James M. - FTu2A.3 Teleanu, Elena L. - JW4A.93 Tong, Limin - JW4A.126 Smyntyna, Valentyn - JTh2A.91 Steinwandt, Rainer - FW2B, FW2B.1 Sylvestre, Thibaut - FTh4A.3, FTu3I.4, Teo, Yong Siah - FF3D.3 Toprak, Muhammet - FTu3F.6 Snetkov, Ilya - JTh2A.87 Stepanenko, Yuriy - FTu3C.2 FTu5I.2 Terazima, Masahide - JW4A.124 Torchia, Gustavo - JW4A.104,

Key To Authors Key To Sobon, Grzegorz - JTh2A.105 Stephen, Burns A. - FW5A.3 Szameit, Alexander - FTu3G.1, Terrones, Mauricio - JTh2A.79 JW4A.161 Soderberg, Kathy-Anne - FTh5G.6 Stevenson, Marquette A. -JW4A.145 JTh2A.141, JW4A.181 Tetikol, Huseyin S. -JW4A.147 Torres Cisneros, Miguel - JTh2A.22, Sogawa, Tetsuomi - FTu5C.5 Stiller, Birgit - FTh4G.3 Szczepanek, Jan - FTu3C.2 Tetsumoto, Tomohiro - FTu2D.3 JW4A.18 Sohn, Byoung-uk - JTh2A.163 Stockman, Mark - JTh2A.103 Szilvási, Tibor - LF3I.1 Tew, David - FTu3G.5 Torres, Pedro - JTh2A.48 Sokolenko, Bohdan V. -JTh2A.104 Stockton, Patrick A. - FTu2F.2 Szymczyk, Anna - JW4A.83 Tezuka, Hiroshige - JTh2A.38 Torres-Carvalho, Mariana - FF3A.4 Solano, Pablo - FTu3I.6, JTh2A.159, Stone, A. - LTh5H.4 Tham, Weng-Kian - FTu2F.1 Torres-Company, Víctor - JW4A.93 LW5I.4 Stone, Nicholas - FF5A.3 T Thekkadath, Guillaume S. - FF3C.7 Torroba, Roberto - JW4A.45 Soljacic, Marin - FF1F.3, FTu1F.5, St-Onge, Guillaume - FF5G.3 Tadesse, Getnet - FW5E.1 Thekkekara, Litty - FTu5B.5 Tosa, V. - LTu1E.2 FW5D.3, LF1I.1, LF2E.5, LTh5H.4 Stranick, Stephan J. - FTu3F.7, LF2D.5 Taghinejad, Hossein - JTh2A.99 Thew, Rob - JW4A.27 Toth, Csaba - FTu1C.1 Soller, Brian - FF1B.4 Strupinski, Wlodek - JTh2A.105 Tainter, Amy M. -JW4A.153 Thibault, Simon - FF5G.3, FTu2F Toussaint, Kimani C. - FW3E.2 Solntsev, Alexander S. - FF1C.5, Stuber, C.S. - LTu2E.2 Taira, Yoichi - FTu1D.2 Thire, Nicolas - FW5E.3 Trabold, Barbara M. -JTh2A.135 FTu5G.4 Studer, Nick M. -JTh2A.30 Takenobu, Shotaro - FTu1D.2 Thirugnanasambandam, Manasa - Trapateau, Julien - FTh4F.4 Soma, Daiki - FTh5E.3 Su, Lijuan - JTh2A.73 Takesue, Hiroki - FW3F.6 FTu1I.5 Trebino, Rick - FW5E.2 Son, Taehwang - JW4A.123 Su, Ya - JW4A.115 Talukder, Javed Rouf - FTh5G.7 Thomay, Tim - FTu1F.6 Trejo Durán, Monica - JW4A.85 Sondermann, Markus - FF5D.2 Subhash, Hrebesh - FW3A.2 Tambasco, Jean- Luc - LW2I.3 Thompson, John R. -JW4A.167 Treps, Nicolas - FF3D, FTh4F.3 Song, Haomin - FTu1F.6, JTh2A.79, Sudhir, Vivishek - FF3D.6 Tamura, Yoshiaki - FTh5E.3, FTu2B.2 Thompson, Kevin P. - FW5H.1, Trichili, Abderrahmen - JW4A.17, JW4A.30 Sugaya, Kiminobu - JW4A.120 Tan, Cheng-zn - JW4A.111 FW5H.3, JTh2A.69 JW4A.28 Song, Hyerin - JW4A.141 Sugizaki, Ryuichi - FTh4E.5 Tan, Dawn T. H. - FTh4G.5, JTh2A.163 Thompson, Mark G. - FTu1D.3, Trillo, Stefano - FTu3I.1 Song, Jingming - FW2F.2 Sugunan, Abhilash - FTu3F.6 Tan, Yue Chuan - FTh4F.5 FTu3G.5, LW5I.3 Trines, Raoul M. - FW5E.5 Song, Ningfang - FW2F.2, FW2F.3 Sukhorukov, Andrey A. - FF1C.5, Tanabe, Takasumi - FTh5G.5, Thumm, Uwe - LF3I.1 Trofimov, V. A. -JW4A.165, JW4A.170, Sonnleitner, Matthias - JW4A.43 FTu5G.4, JTh2A.141 FTu2D.3, JTh2A.150 Thuret, Gilles - JTh2A.140 JW4A.94 Soomro, Shoaib R. - FTu5A.2 Sukhov, Sergey - JW4A.6 Tanaka, Shunta - JTh2A.42 Thurman, Samuel T. - FF1G.6 Trumper, Isaac - FW5G.4 Soorat, Ram - JW4A.16 Sukiasyan, Minas - JW4A.44 Tang, Hong - FTh4G.2, FTh5G.4, Thyagarajan, Krishna - JW4A.3 Tsai, Din Ping - JTh2A.143 Sorger, Volker J. - FTu3D.1, FW3E Sultan Shah Bukhari, Syed - FTu5G.1, JTh2A.114 Thylen, Lars - FTu3F.6 Tsakmakidis, Kosmas - FF5C.4 Soriano, Gabriel - FF3G.3, JW4A.59 JTh2A.180 Tang, Suning - JTh2A.127 Tian, Feng - FTu3D.6 Tschernajew, Maxim - FW5E.1 Sotor, Jaroslaw Z. -JTh2A.105 Sun, Greg - JTh2A.143 Tang, Yuxing - FW5E.4 Tienvieri, Clair - FW5G Tseng, Sheng-hao - FW3C.3, FW3C.4 Souhan, Brian - JW4A.149 Sun, Jingbo - FTh4B.1, FTh5F.1 Tang, Zhongkan - FTh4F.5 Tilley, Steven - FTh5D.5 Tsironis, Giorgos P. - FF3H.5 Sowers, Kelly - JW4A.136 Sun, Lei - FTu1F.2 Tang, Zong Sheng - FTu2F.6 Tsuchizawa, Tai - FW3F.6, FW5F.3

152 FiO/LS 2016 • 16–21 October 2016 Tsuda, Hiroyuki - FW5D.6, JTh2A.148, Varshney, Shailendra K. - FTu3I.2, W Ware, Morgan E. -JW4A.175 Williams, John - FF3A.3 JTh2A.164, JW4A.144 JTh2A.50 Wabnitz, Stefano - FTu3I.1 Warrick, Erika R. - LTu5F.2 Willner, Alan - FTh4E.3, FTh5G.2 Tsur, Yuval - FTu3D.3 Vasu, Ram M. -JTh2A.67 Wada, Naoya - FTh4E.5 Washburn, Brian - FTu1I.5 Wilmer, Brian L. - FTu3F.3 Tsurimaki, Yoichiro - FW2E.2 Vay, Jean- Luc - FTu1C.1 Waduge, Pradeep - JW4A.136 Wasilewski, Wojciech - FF3C.2, Wilson, Dalziel - FF3D.6 Tsuritani, Takehiro - FTh5E.3 Vayu Nandana Kishore, Pabbisetti - Wague, Ahmadou - JW4A.28 FF5C.1, FW3F.3 Wilson, Matthew - FTu1C.3 Tu, Junjie - JW4A.38 JW4A.36 Wahlstrand, Jared K. - FTh4B.3, Wasylczyk, Piotr - FF3G.6 Wirth, Jacob H. - FF3H.4, JW4A.1 Tuniz, Alessandro - FW3E.4 Veale, Matthew - FTu1C.3 LF2G.6 Watnik, Abbie - JW4A.1 Wise, Frank W. - FTu2I.2, FW5E.4, Tünnermann, Andreas - FW5E.1 Vedovato, Francesco - FTh4F.2 Wakayama, Yuta - FTh5E.3 Watson, Andrew B. - FTh4I.4 JW4A.196 Tupa, Dale - JW4A.153 Velasco-Ocana, Miriam - FW5A.4 Walasik, Wiktor - FTh5F.1, FTu3C.3 Watts, Michael - FTu2D.5 Withford, Michael - FTu3G.3, FW3H.5, Turquet, Léo - JW4A.178 Velez, Alejandro - JW4A.45 Wallraff, Andreas - FF5D.1 Wax, Adam - FF3A.6, JTh2A.126 JTh2A.181 Tyurikov, Dmitry A. -JW4A.180 Vella, Anthony - FF3G.4 Walmsley, Ian A. - FTu5G.2 Webb, Kevin J. -JW4A.13, JW4A.15, Wojtkowski, Maciej - FTh4H.1 Tzeng, Shih-Yu - FW3C.3 Velmanickam, Logeeshan - JW4A.116 Walther, Andreas - JW4A.118 JW4A.5 Wolf, Alexey A. - FW5B.2 Tzortzakis, Stelios - JTh2A.98 Verdon, Rachel - FF3A.4 Wan, Congshan - JW4A.127 Webber, Daniel - FTu3F.3 Wollmann, Sabine - FF1C.4 Vergeles, Klara - JTh2A.91 Wan, Lipeng - JW4A.110 Weber, Markus - FF5D.2 Won, Jungeun - JTh2A.129 U Vergyris, Panagiotis - FTu3G.3 Wang, Alan X. -JTh2A.127, JTh2A.56, Weber, Timothy - FF3A.1 Wong, Chee Wei - FTh4G.7 Key To Authors Ugalde-Ontiveros, Jorge A. -JW4A.91 Verhagen, Ewold - FF3D.5, JW4A.57, JW4A.137 Weeber, Henk - FW2A.2 Wood, D.A. - LTu2E.2 Ummy, Muhammad A. -JTh2A.189 LF2E.3 Wang, Fei - JW4A.72 Weerasinghe, Kushan - FTu1I.5 Wood, Obert - FTu1F.2 Umstadter, Donald P. - FTu1C.2, Verma, Pramode K. -JW4A.194, Wang, Feng - FTu3C.2 Wegscheider, Werner - FF5F.7 Woon, Wei Yen - FTu3F.8 FTu1C.3, JW4A.97 JW4A.35 Wang, Jianwei - FTu1D.3, FTu3G.5 Wei, Cai - FF1B.3, FW2F.2, FW2F.3 Wosinski, Lech - FTu3F.6 Unger, Blair - FW3H Verma, Varun - FTh4F.1, FW2B.5 Wang, Jiawei - FTu2D.1 Wei, Changjiang - JW4A.115 Wozniak, Kaitlin T. - FTh4H.4 Unnithan, Ranjith Rajasekharan - Veronis, Georgios - JW4A.163 Wang, Jie - JTh2A.166 Weidlich, Stefan - FW3E.4 Wozniak, Mariusz P. -JW4A.68 FW2C.5 Victora, Michelle M. - FW3A.4 Wang, Jun - JTh2A.10 Weiner, Andrew M. - FW5F.5, Wright, Logan G. - FTu2I.2, JW4A.196 Unruh, Karl - FTu2C.4 Videla, F. - JW4A.104 Wang, Kai - JTh2A.24 JW4A.150, JW4A.174 Wu, Biming - JTh2A.130 Upham, Jeremy - FTu1G.4, FTu3D.4, Viegas, Jaime P. - FTu1D.4, FTu2I.5, Wang, Lijun - JW4A.21 Weir, Nicholas - FW5C.4 Wu, Chihhui - FTu1G.3 JW4A.64 JTh2A.173, JTh2A.63 Wang, Lirong - JW4A.71 Wen, Cai - JW4A.25 Wu, Chong-jia - JW4A.156 Urbas, Augustine - FTu5G.6 Vieira, Nilson D. - FTu2C.2 Wang, Pengfei - FTu2I.4 Wen, Jianxiang - JW4A.34 Wu, Dingxin - JTh2A.157 Urey, Hakan - FTu5A.2 Vignolini, Silvia - FW3D.2 Wang, Qi - FF5H.2 Wen, Ke - JW4A.38 Wu, Guohua - JTh2A.116 Usha, Sruthi P. -JTh2A.44, JTh2A.52, Vigueras-Santiago, Enrique - Wang, Qiwei - JTh2A.56 Wen, Yuanhui - JTh2A.92, JW4A.19 Wu, Jenny - JW4A.152 JTh2A.53 JW4A.102 Wang, Ranxio Frances - FW3A.4 Wen, Zhengqiang - JW4A.188, Wu, Jin-Min - JW4A.37 Villa, Matteo - FTu5G.4 Wang, Ruliu - JTh2A.112, JW4A.31 JW4A.199 Wu, Ming C. - FTu1D.6 V Villas-Bôas, José Maria - JW4A.107 Wang, Ruoyu - FW2C.5 Weng, Frank J. -JTh2A.124 Wu, Pengfei - JTh2A.171 Vahala, Kerry J. - FTh5G.1, FTh5G.3 Villeneuve, David - FTu5C.3, LTh5I.2 Wang, Shaokang - JW4A.189 Wernsing, Keith - JW4A.121 Wu, Pin Chieh - JTh2A.143 Valente, Denise - FF1G.5 Villinger, Massimo L. - FW5H.8 Wang, Tianyu - JTh2A.183 Weston, Morgan M. - FF1C.4 Wu, Sheldon S. - LF2G.8 Valente, João - FF5G.7 Villoresi, Paolo - FF5D, FTh4F.2, Wang, Tie-Jun - JTh2A.96 Weston, Tyler - FTh5C.4 Wu, Shuhao - JTh2A.157 Valentine, Jason - JW4A.151 FTh5F Wang, Tingyun - JW4A.34 Wetzel, Benjamin - FTu1I, FTu3I.1, Wu, Xiang - JW4A.146 Valivarthi, Raju - FTh4F.1 Vinas, Maria - FW2A.3 Wang, Wei-Chih - FF1G.7, JTh2A.151 FTu3I.4, FW3F.2, JTh2A.192, Wu, Yiyang - FF3A.3 Vallée, Réal - FTu1I.2 Vitullo, Dashiell L. - FW2B.4 Wang, Xiaolei - JTh2A.166 JW4A.152 Wu, Yuanpeng - JW4A.129 Vallone, Giuseppe - FTh4F.2 Vivien, Laurent - FF5F.2 Wang, Yongtian - FTu5A.3 Wheeler, Duncan C. - FTu1F.5 Wurth, Wilfried - LF3I.2 Vamivakas, Nickolas - FF1G.2, Viza, Gerardo - FF1D.6 Wang, Yuan - FF5C.4, FF5H.7, Whitaker, John - FF3F.4 Wyant, James C. - FTu1A.2 FF3G.2, FF5C, FF5F.7, FF5G.2, Vlasov, Yurii A. - FF5F.3, FTu2D.2 FTu1G.3, LF2E.2 White, Andrew G. - FF1C, FF3D.2 JW4A.136, LF2F.1, LTu3H Vogl, Ulrich - FF3D.3, FW5F.4 Wang, Yun - FTu1I.1 White, Edward - FTu3A.2 X Vampa, Giulio - FTu5C.3, FW5E.3, Vohnsen, Brian - FF1G.5, FW3A.3 Wang, Zhaorong - LF2F.2 White, Jonathon David - FTu3F.8 Xiao, Hai - FF3B.3 LTh5I.2, LTu1E.1 Vora, Patrick - FTu3F.7 Wang, Zhihuan - JTh2A.6 Whiteaker, Kevin L. - FW5H.1 Xie, Guodong - FTh5G.2 van der Mooren, Marrie H. - FW2A.2 Vorndran, Shelby - FTu5A.5 Wang, Zhuo - FTu2C.3 Wicker, Kai - FTh4C.3 Xie, Zhijian - JTh2A.43 van Otten, Frank W. M. - FTu3D.7 Voss, Paul L. - FF5C.2 Wang, Zhuoran - JTh2A.191 Wicks, Gary - JW4A.142 Xin, Chenguang - JW4A.126 van Stryland, Eric - JTh2A.26, Vu, Khu - FTh4G.3 Wang, Zihao - FF5F.5, FTu3G.4, Widjaja, Joewono - JW4A.106 Xing, Peng - FTu1D.4 JW4A.183 Vuckovic, Jelena - FF5E.3 FW5C.4 Wiebe, Nathan - FTu3G.5 Xu, Chris - JTh2A.183 van Tilborg, Jeoren - FTu1C.5 Vura-weis, Josh - LTu5F.1 Wanunu, Meni - JW4A.136 Wiederhold, Robert - FTu3A.1 Xu, Di - FW5H.6 Varju, K. - LTu1E.2 Vyas, Reeta - JW4A.190, JW4A.191, Ward, Benjamin - FW5B.4 Wilkes, Callum M. - FTu1D.3 Xu, Fei - FTu3I.3, JTh2A.174, Varshney, Ravi K. -JW4A.148 JW4A.195 Ward, Jonathan - FF5C.8 Williams, David R. - FTh4I.1, FW2A JTh2A.46

FiO/LS 2016 • 16–21 October 2016 153 Xu, Jingjun - JTh2A.166 Ycas, Gabriel - FTh5G.3, JTh2A.85 Zamboni-rached, Michel - FF5H.8, Zhang, Yan- Lei - LF2E.1 Zhu, Huiqing - LF2D.6 Xu, Lei - FF1C.5, JW4A.146 Ye, P. - LTu2E.2 JW4A.193 Zhang, Ying - LF2G.4 Zhu, Ji - JW4A.25 Xu, Linhua - FF5C.8 Ye, Ren - JTh2A.101 Zaquine, Isabelle - FTh4F.4 Zhang, Young - JW4A.152 Zhu, Jun - JTh2A.69 Xu, Qiang - JW4A.188, JW4A.199 Ye, Yuqian - JTh2A.172 Zayats, Anatoly - FTu5G Zhang, Yujing - JW4A.137 Zhu, Na - JTh2A.114 Xu, Wenjing - FTu3I.7 Yeh, Chia-Hua - JW4A.111 Zayats, Anatoly - FTu1G.1 Zhang, Zhifeng - FTh4G.4 Zhu, Xiaosong - FTu3C.2 Xu, Xiaobin - FW2F.3 Yehui, Liu - JTh2A.35 Zaytsev, Kirill - FTh4C.2 Zhang, Zuchen - JTh2A.54 Zhu, Zimu - JW4A.196 Xu, Yang - JW4A.117 Yen, Tzu-Hsiang - JW4A.156 Zeilinger, Anton - FF3C.6, FW3F.1 Zhao, Baozhen - FTu1C.2, FTu1C.3, Zinkiewicz, Lukasz J. - FF3G.6 Xu, Yun - FTh5F.1 Yeremyan, Arsham - JW4A.44 Zeitler, Jochen - FW3H.2 JW4A.97 Zinkiewicz, Malgorzata M. - FF5B.8 Xu, Yunlu - JTh2A.159 Yibo, Wang - JTh2A.35 Zeldovich, Boris Y. - FW2C.2 Zhao, Dongxing - JW4A.173 Ziyadi, Morteza - FTh4E.3, FTh5G.2 Xu, Zhongyang - JW4A.21 Yilmaz, Saniye S. - FW5B.7 Zemskov, Konstantin I. -JTh2A.3 Zhao, Guangming - FF5C.8 Zlobina, Ekaterina A. - FW5B.2 Xuan, Yi - FW5F.5, JW4A.150 Yilmaz, Sinem - FTu1I.4 Zeng, Guang - FW5A.2 Zhao, Han - FTh4G.4 Zobenica, Zarko - FTu3D.7, FTu5G.3 Xue, Gaolei - FTu3F.1, FTu5A.3 Yin, Longfei - JTh2A.116 Zeng, Shaoqun - FTh4D.2 Zhao, J.P. - JTh2A.14 Zou, Chang- Ling - FTh4G.2, Xue, Xiaojie - JTh2A.100, JTh2A.38, Yin, Peichuan - JTh2A.144, Zeng, Xie - JW4A.30 Zhao, Nan - FW5H.6, JTh2A.69 FTh5G.4, LF2E.1 JW4A.188, JW4A.199 JTh2A.161, JTh2A.177 Zeosky, Jonathan J. -JTh2A.111 Zhao, Peng - JTh2A.26, JW4A.183 Zribi, Olena - FF5B.6 Xue, Xiaoxiao - FW5F.5 Yonezawa, Kazuhiro - FTh5E.3 Zerrad, Myriam - FF3G.3, FW5G.3, Zhao, X. - JTh2A.9 Zuegel, Jonathan D. - FW2G, FW3G, Yoo, Choong-shik - JW4A.9 JW4A.59 Zhao, Xin - FTu5I.6, JTh2A.112, JW4A.48 Y Yoon, Taehyun - JW4A.7 Zghal, Mourad - JW4A.17, JW4A.28 JW4A.31 Zulkifli, Mohd Z. -JW4A.29 Yabashi, Makina - LTu5F.3 Yoon, Taerim - JW4A.141 Zhai, Chunyang - FTu3C.2 Zhao, Yanli - JW4A.38 Zusin, Dmitriy - LF3I.1 Yabe, Takashi - LF1I.4 Yoshimura, Anthony - LF2F.1 Zhang, Bo - FF5H.2, LF2F.2 Zhao, Yichen - FTu3F.6 Zvietcovich, Jose F. -JTh2A.131 Yablon, Joshua - JTh2A.102 Yoshizawa, Katsumi - FW5D.6 Zhang, Chenyi - JW4A.34 Zhao, Yunhe - JW4A.34 Zysk, Adam - JW4A.117 Yablonovitch, Eli - FW5F.1, LF2E.2 You, Chenglong - JW4A.163 Zhang, Chunxi - FW2F.2, FW2F.3, Zheleznyak, Len A. - FTh4H.4 Yakovlev, Alexey - JTh2A.87 You, Jong-Bum - JTh2A.70 JTh2A.54 Zheludev, Nikolay I. - FF5G.7,

Key To Authors Key To Yakovlev, Egor - FTh4C.2 You, Wenjing - LF3I.1 Zhang, Deming - FTu5A.5 FTu1F.1, FTu1G.5 Yakunov, Andrey - JW4A.39 Young, Laura - FF3A.4 Zhang, Fan - JW4A.173 Zhen, Bo - FF1F.3, LTh5H.4, LTu1H Yamada, Koji - FW3F.6 Young, Michael D. -JTh2A.57 Zhang, Feng - JW4A.37 Zheng, Xiaorui - FTu5B.4 Yamamoto, Hirotsugu - JTh2A.128 Yu, Changyuan - LF2G.4 Zhang, Guoquan - JTh2A.166, Zheng, Zheng - FTu5I.6, JTh2A.112, Yamamoto, Tsuyoshi - FW5F.3 Yu, Chung - JTh2A.43 JW4A.74 JW4A.31 Yamamoto, Yoshihisa - LF1I.3 Yu, Jiaka - FTh4G.4 Zhang, Haibo - JTh2A.101 Zhigilei, Leonid V. - FF3F.1 Yamamoto, Yoshinori - FTu2B.2 Yu, Jiayi - FF5G.1, JW4A.47 Zhang, Jinwei - FTu3C.1 Zhou, Chanjing - JTh2A.79 Yamilov, Alexey - FW2D.1 Yu, Jinzhu - FF3A.3 Zhang, Jun - FTu1C.2, FTu1C.3, Zhou, Chi - FTu1F.6 Yan, Min - FTu3F.6 Yu, Kyoungsik - JTh2A.70 JW4A.97 Zhou, F - LF2E.7 Yan, Wenchao - FTu1C.2, JW4A.97 Yu, Linhui - FTh4D.4 Zhang, Lin - FTh4E.3, FTh5G.2 Zhou, Guangya - FTu3D.6 Yan, Yan - FTh5G.2 Yu, Mengjie - FTu5D.2 Zhang, Long - LF2D.4 Zhou, Hengyun - FF1F.3, LTh5H.4 Yang, Daquan - JW4A.134 Yu, Mingbin - FTh4G.7 Zhang, Lu - FTh5C.7, JW4A.194, Zhou, Jun - JTh2A.101, JW4A.129 Yang, Dongyue - JTh2A.116 Yu, Siyuan - JTh2A.92, JW4A.19 JW4A.35 Zhou, Minchuan - FF1B.2, FF1H.8, Yang, Jinghui - FTh4G.7 Yu, Xia - LF2G.4 Zhang, Meng - FTu5I.6, JW4A.31 JTh2A.16 Yang, Ki Youl - FTh5G.3 Yu, Yingjie - JW4A.61 Zhang, Nan - FTu1F.6, JW4A.30 Zhou, Qiang - FTh4F.1 Yang, Lan - FF5C.8 Yuan, Guohui - JTh2A.191 Zhang, Ping - FTu1C.2, FTu1C.3, Zhou, Weimin - FTu1D.5, JTh2A.171 Yang, Naixin - JW4A.42 Yuan, Lei - FF3B.3 JW4A.97 Zhou, Xiang - FTh5E.1 Yang, Qing - JW4A.129 Yuan, Yan - JTh2A.73 Zhang, Qi - FF3B.3 Zhou, Xiaoqi - FTu1D.3 Yang, Rouhui - FF3A.1 Yuan, Zhijun - JTh2A.101 Zhang, Qiming - FTu5A.3 Zhou, Yiyu - JTh2A.14 Yang, Shang-Hua - FTh4G.7 Yue, Zengji - FTu3F.1 Zhang, Qingbin - FTu3C.2 Zhou, Zifan - FF1B.2, FF1H.8, Yang, Yong - FF5C.8 Yun, Jeong-geun - JW4A.125 Zhang, Saifeng - JTh2A.10 JTh2A.102 Yang, Yunyi - FTu5B.4 Yun, Seok-Hyun A. - FTh4H, FTh4H.2 Zhang, Tianlei - JTh2A.112 Zhu, Alexander - JW4A.63 Yao, Jianing - FW5H.6, JTh2A.131 Yurchenko, Stanislav - FTh4C.2 Zhang, Wen Qi - FF5H.4 Zhu, Alexander Y. - FTh5B.6, JW4A.65 Yao, Kan - JTh2A.176 Yvind, Kresten - FTh4E.6 Zhang, Xiang - FF5C.4, FF5H.7, Zhu, Benyuan - FTh5E, FTh5E.5 Yao, Ruizhe - FW5C.4 FTu1G.3, LF2E.2 Zhu, Bowen - JTh2A.166 Yao, X. Steve - JW4A.115 Z Zhang, Xi-Cheng - FF3F.3, JTh2A.98 Zhu, Caigang - FF5A.1 Yasui, Takeshi - JTh2A.128 Zahedpour, Sina - FTh4B.3, LF2G.6 Zhang, Xingwang - FTu3D.6 Zhu, Chengrui - FF5H.3 Yates, Dennis - FW5H.1 Zaidi, Aun - FTh5B.6 Zhang, Yanfeng - JTh2A.92, JW4A.19 Zhu, Guoxuan - JTh2A.92, JW4A.19

154 FiO/LS 2016 • 16–21 October 2016