Schedule-at-a-Glance ...... 2 FiO + LS Chairs’ Welcome Letters ...... 3 General Information ...... 5 Sponsoring Society Booths ...... 6 Stay Connected Conference Materials ...... 7 FiO + LS Conference App ...... 7 Plenary Session/Visionary Speakers Plenary Presentations ...... 8 Visionary Speakers ...... 9 Awards, Honors and Special Recognitions OSA 2017 Awards and Honors ...... 12 APS/DLS 2017 Awards and Honors ...... 14 OSA Foundation 2017 Prizes and Special Recognitions ...... 14 Science & Industry Showcase (Poster Sessions, E-Posters, Rapid-fire Oral Presentations, Exhibits) . . . . . 16 FiO 2017 Participating Companies ...... 17 Special Events ...... 18 FiO + LS Committee ...... 21 Explanation of Session Codes ...... 23 FiO + LS Agenda of Sessions ...... 23 FiO + LS Abstracts ...... 28 Key to Authors and Presiders ...... 85

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

OSA and APS thank the following sponsors for their generous support of this meeting:

FiO + LS 2017 • 17–21 September 2017 1 Conference Schedule-at-a-Glance Note: Dates and times are subject to change. Check the conference app for regular updates. All times reflect eastern time zone. Sunday Monday Tuesday Wednesday Thursday 17 September 18 September 19 September 20 September 21 September GENERAL Registration 15:00–18:00 07:00–18:00 07:00–17:30 07:00–17:30 07:30–11:30 Speaker Preparation Room 15:00–18:00 07:00–17:30 07:00–17:30 07:00–17:30 07:30–11:30 WORKinOPTICS .com Kiosks & E-Center 15:00–18:00 07:00–17:30 07:00–17:30 07:00–17:30 07:30–11:30 Coffee Breaks 10:00–10:30 10:00–10:30 15:30–16:00 PROGRAMMING LS Symposium on Undergraduate Research 12:00–18:00 FiO + LS Visionary Speakers 08:00–08:45 08:00–08:45 08:00–08:45 FiO + LS Technical Sessions 09:00–15:30 15:00–18:15 09:00–18:15 09:00–12:30 Joint FiO + LS Plenary Session 08:00–09:30 Postdeadline Paper Sessions 13:30–15:30 SCIENCE & INDUSTRY SHOWCASE Exhibits 09:30–16:00 10:00–15:00 09:30–10:00 10:00–10:30 Coffee Breaks Sponsored by 13:00–13:30 13:00–13:30

Poster Sessions and E-Posters 10:00–12:00 10:00–12:00 13:00–15:00 13:00–15:00 Rapid-fire Oral Presentations 10:00–11:00 10:00–11:00 13:00–14:00 13:00–14:00 Meet OSA’s Journal Editors 11:45–12:45 12:00–13:00 Pizza Lunch Sponsored by OSA Student Chapter Competition 13:00–15:00 Congressional Fellowship Information Session 12:00-13:00 SPECIAL EVENTS Women of Light, a Special Program 09:00–15:00 for Women in Optics Funded by OSA Student Member Party 18:30–20:30 Capitol Hill Visits 09:00–12:00 Challenges and Emerging Opportunities in 12:30–13:30 Molecular Probes and Nanobio-Optics Grant Writing 101 Workshop 12:30–14:00 OSA Nonlinear Optics Technical Group 16:00–17:30 Workshop & Networking Session Unconscious Bias Workshop 16:00–17:30 Evening with the Agencies & Reception 16:00–18:00 FiO + LS Awards Banquet 18:30–21:00 Environmental Sensing Technical Group 16:30–17:00 Networking Event OSA Annual Business Meeting 17:30–18:15 DLS Annual Business Meeting 17:30–18:30 FiO + LS Conference Reception 18:30–20:30 Sponsored by The “Rush Hour”: What Does a Scientist Owe 09:00–10:00 Policymakers? OSA Members, Family and Friends Tour 09:30–12:00 OSA Optical Material Studies Technical Group Special 12:00–13:00 Talk Polarization Optics - Design and Fabrication 12:00–13:00 Trends and Challenges OIDA VIP Industry Leaders 12:00–13:30 Networking Speed Meeting Lunch Sponsored by Meet the APS Journal Editors Reception 15:30–17:00 Pairing Photons to Electrons: An OSA 16:30–17:00 Nanophotonics Technical Group Networking Networking with the OSA Biomedical Optics 18:30–20:00 Technical Groups

2 FiO + LS 2017 • 17–21 September 2017 Welcome to Frontiers in Optics 2017

Whether you are in an autonomous vehicle looking to avoid collisions with nearby objects, or sitting on Earth and trying to detect collisions of black holes in the furthest galaxies, the Frontiers in Optics + Laser Science APS/DLS (FIO + LS) offers something for you . We are pleased to welcome to Washington, D .C ., the home of The Optical Society and The American Physical Society - Division of Laser Science .

This year’s conference introduces a meeting experience that has been thoughtfully revised — taking the best of the past and adding vital, innovative elements . The result is a conference with invaluable opportunities to learn from and meet with your peers and colleagues . On behalf of the FiO Subcommittee Chairs, we would like to thank our colleagues from the Division of Laser Science (DLS) of the American Physical Society (APS) for assisting in cultivating joint topics and sessions that will greatly enhance the experience of the attendees at FiO + LS 2017 .

The world-class technical program features more than 75 invited speakers, 200 contributed talks and almost 500 poster presentations by celebrated members of the community describing some of the most exciting advances in their fields .

As technology advances at an ever-increasing pace, the potential applications for optics continue to grow and bring us closer to the edge of amazing discovery and automation . Our plenary speakers, Jason Eichenholz, CTO and Founder of Luminar, will discuss LIDAR and technologies driving the emerging autonomous vehicle industry . Laura Cadonati, LIGO Scientific Collaboration will share recent discoveries in gravitational wave science . Add nine Visionary Speakers who address cutting-edge research on topics from nanophotonics to optics in computing; and a special advocacy presentation from former U .S . Congressman and current CEO of AAAS, Rush Holt .

We will toast the achievements of OSA and APS Division of Laser Science award and honor recipients at the inaugural FiO + LS Awards Banquet on Monday night . Those to be recognized include Margaret Murnane, University of Colorado at Boulder, USA, 2017 winner of OSA’s highest honor, the 2017 OSA Frederic Ives Medal / Jarus W . Quinn Prize and John C . Mather, NASA’s Goddard Space Flight Center, USA, OSA 2017 Honorary Member . The OSA awards program spans all areas of optics and photonics, as well as contributions made through service, education and leadership . Nominations for 2018 are due 1 October 2017, so there is still time to recognize the achievements of your colleagues . Visit www .osa .org/awards for details .

While at FiO + LS, we encourage you to visit the new Science & Industry Showcase . The FiO exhibition transforms into The Science & Industry Showcase – in which exhibiting companies are partnered with innovative demonstrations, networking events, poster presentations, e-posters and rapid-fire oral presentations . Take the time to learn about new products, find technical and business solutions and gain the most up-to-date market perspective of your industry .

Again, we welcome you to FiO + LS 2017 and encourage you to enjoy the dynamic programming incorporated into the next few days ahead .

With best regards, Steve & Susana

Steve Cundiff Susana Marcos FiO Chair FiO Chair University of Michigan, USA Consejo Sup Investigaciones Cientificas, Spain

FiO + LS 2017 • 17–21 September 2017 3 Welcome to Laser Science 2017

The leadership of the Division of Laser Science (DLS) of the American Physical Society (APS) is pleased to welcome you to our 33rd annual meeting, Laser Science (LS) 2017, in Washington, D .C . We are grateful for the help of our colleagues and technical program organizers, Josh Vura-Weis and Hui Cao in organizing a broad range of topics in physics and chemistry . This year’s program includes many of the areas at the forefront of laser science that are customarily found at the annual DLS meeting . We have collaborated with our colleagues in The Optical Society to coordinate schedules to encourage your intellectual wanderings between DLS and OSA sessions .

In addition to an outstanding technical program with over 50 Laser Science presentations, there are many exciting special Visionary Speakers and events scheduled for the meeting this year . Special attention is appropriate for the Symposium on Undergraduate Research on Sunday, 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 Science meeting are organized around several broad themes: High Harmonic Generation: Time, Energy and Complexity; Frontiers in X-ray Laser Spectroscopy; Plasmonics and Nanophotonics; and Novel Lasers .

Celebrate the achievements of award and honor recipients from OSA and APS Division of Laser Science and connect with colleagues at the inaugural FiO + LS Awards Banquet on Monday night . Those to be recognized include Louis F . DiMauro, The Ohio State University, USA, 2017 winner of the Arthur L . Schawlow Prize in Laser Science .

The DLS Business meeting will be held Tuesday, 19 September from 17:30–18:30 .

We welcome you to the Laser Science 2017 Meeting and encourage you to take full advantage of this year’s technical sessions, visionary and plenary talks, as well as the new Science & Industry Showcase featuring leading suppliers to the laser science community, Rapid-fire Oral Presentations and Poster Sessions including e-posters .

Enjoy!

Mark G . Raizen Roseanne J . Sension LS Chair LS Chair University of Texas at Austin, USA University of Michigan, USA

4 FiO + LS 2017 • 17–21 September 2017 General Information General Information WiFi Access Instructions Lost and Found To access the complimentary WiFi services during the FiO + For lost and found please check first at the conference LS Conference, use the following information to log in . registration counter in the Concourse Foyer . Please put your name on all conference materials (including your Conference SSID: FiO2017 Program), as they will only be replaced for a fee . Password: opticsindc17

Registration Special Needs Concourse Foyer If you have a disability and require special accommodations in order to fully participate in this conference, please contact Sunday, 17 September 15:00–18:00 Conference Management at the registration desk . Your specific needs will be addressed . Monday, 18 September 07:00–18:00 Tuesday, 19 September 07:00–17:30 First Aid and Emergency Information Wednesday, 20 September 07:30–17:30 In the event of an emergency at the Washington Hilton, Thursday, 21 September 07:30–11:30 please dial #60 from any courtesy phone . If you happen to dial 911 on your own, please call #60 as well to inform the hotel about the emergency . Speaker Preparation Room Albright Room, Terrace Level General InformationNearest Hospital, Fire Station & Police Station Speakers and presenters are encouraged to stop by the George Washington University Hospital Speaker Preparation Room during registration hours (listed 900 23rd Street, NW above) to test their presentations prior to their session . The Washington, DC 20037 room will be equipped with laptops, LCD projectors and +1 .202 .715 .4000 screens . DC Fire Department Engine 9 1617 U Street, NW Media Room Washington, DC 20009 Boundary Room, Terrace Level +1 .202 .673 .3209 A staffed media room is available for credentialed mem- DC Metropolitan Third District Police Station bers of the media . Badges for pre-registered reporters and 1620 V Street, NW reporter registration are in the media room along with media Washington, DC 20009 kits, internet connectivity, printer, quiet work space and con- +1 .202 .673 .6815 ference information . E-Center Monday, 18 September 12:00–17:00 Concourse Foyer Tuesday, 19 September 08:00–17:00 The E-Center, offering free internet connectivity, will be open Wednesday, 20 September 08:00–17:00 Monday through Thursday during registration hours . Thursday, 21 September 08:00–12:00 WORKinOPTICS.com Kiosk Concourse Foyer Business Center FedEx Office, Terrace Level WORKinOPTICS .com provides a state-of-the-art platform to efficiently connect employers and job seekers within the The Washington Hilton’s in-house Business Center, operated optics and photonics community . by FedEx, offers one-stop shopping for all of your business needs . The FedEx Office is open Monday - Friday, 07:00– Your next job opportunity or new hire is just a click away. 19:00, Saturday 09:00–15:00, closed on Sundays . Guests • Post your resume at no charge to reach top of the Washington Hilton have extended access with their employers . guest room key to self-service computer stations available 24 hours a day, 7 days a week . • OSA Industry Development Associates (OIDA) Members receive 20 free job postings .

FiO + LS 2017 • 17–21 September 2017 5 Sponsoring Society Booths OSA Advocacy Booth Concourse Foyer Concourse Foyer Sunday, 17 September 15:00–18:00 Visit the OSA Advocacy Booth to learn more about how you can get involved in OSA’s advocacy programs, talk directly Monday, 18 September 08:00–18:00 with a member of the OSA Government Relations Team, and Tuesday, 19 September 08:00–17:30 have the opportunity to write your members of Congress Wednesday, 20 September 08:00–17:30 about research and development funding . Thursday, 21 September 08:00–11:30

General Information OSA Member Lounge Concourse Foyer Founded in 1899, the American Physical Society (APS) is a non-profit membership OSA Members are invited to take a organization working to advance and diffuse brief respite from the meeting at the the knowledge of physics . APS publishes the Member Lounge . Whether it’s to plan world’s most widely read physics research and your schedule, join or renew your membership, or print your review journals: Physical Review Letters, Physical Review X, boarding pass, the lounge offers comfortable seating and an Reviews of Modern Physics, Physical Review A-E, Physical opportunity to network with your fellow attendees . Review Accelerators and Beams, Physical Review Applied, Conference attendees who join or renew as an Individual Physical Review Fluids, Physical Review Materials, Physical 1-year member will receive 50% off the cost of annual dues . Review Physics Education Research, and Physics. Please stop by our table near Registration to learn more about the prestigious Physical Review collection and our newest Sunday, 17 September 15:00–18:00 journal Physical Review Materials, a new broad-scope Monday, 18 September 08:00–18:00 international journal for the multidisciplinary community Tuesday, 19 September 08:00–17:30 engaged in materials research . Wednesday, 20 September 08:00–17:30 Through world-renowned publica- Thursday, 21 September 08:00–11:30 tions, meetings and membership programs, OSA provides quality information and inspiring interactions that power achieve- OSA Technical Groups Booth ments in the science of light . More than 20,000 OSA International Terrace, Terrace Level Members, residing in over 100 countries and spanning academic, government and industry, call OSA their profes- Connect with your OSA community sional home . Stop by to meet OSA staff, and learn more during FiO by visiting us at the about our publications, conferences and meetings and OSA Technical Groups Booth, membership for individuals and companies . Conference located in the International Terrace . OSA Technical Groups attendees who join or renew as an Individual 1-year member offer members the chance to connect with colleagues in will receive 50 percent off the cost of annual dues . their area of expertise through innovative events and focused networking opportunities . Stop by the booth for a chance to meet your technical group leaders and find out OSA CAM Lounge more about all of the OSA Technical Group events happen- Concourse Foyer ing this week . CAM (Centennial Authentic Moments) is an ongoing program of collecting scientific selfies where members talk about what it means to be an OSA Member, who/what inspired them to get into optics and what excites them about their current work in three minutes or less . The collection of these short videos will be featured on OSA’s website, social media and various conferences .

Monday, 18 September 08:00-17:00 Tuesday, 19 September 08:00–17:00 Wednesday, 20 September 08:00–17:00

6 FiO + LS 2017 • 17–21 September 2017 Stay Connected Access Technical Digest Papers FiO + LS Conference App Technical attendees have FREE continuous online access to Manage your conference experience by downloading the the FiO + LS 2017 technical digest including Postdeadline FiO + LS Conference App to your smartphone or tablet . papers . These 1 or 2-page summaries of invited and accept- Download the app one of three ways: ed contributed papers can be downloaded individually or by downloading daily zip. files . ( .zip files are available for 60 1 . Visit www .frontiersinoptics .com/app days .) 2 . Search for ‘OSA Events’ in the app store 1 . Visit the conference website at http://www .frontiersinoptics com. 3 . Scan the QR code below 2 . Select the “Access Digest Papers” link on the right side of the web page Stay Connected 3 . Log in using your email address and password used for registration . Access is limited to Full Technical Attendees only . If you need assistance with your login information, please use the “forgot password” utility or “Contact Help” link . Schedule Search for conference presentations by day, topic, speaker Conference Program Update or program type . Plan your schedule by setting bookmarks on programs of interest . Technical attendees can access Technical program changes will be communicated in the technical papers within session descriptions . onsite Conference Program Update Sheet distributed with your onsite registration materials . In addition, all updates Science & Industry Showcase will be made in the FiO + LS conference app . We encourage Search for exhibitors or view the complete list . Bookmark you to review them carefully to stay informed on changes to exhibitors as a reminder to stop by their booth . Tap on the the program . map icon within a description, and you’ll find their location Onsite program changes will be posted on an update board on the show floor map . located at the registration desk . Check daily for new infor- Access Technical Digest Papers mation and/or reference the FiO + LS conference app . Full technical registrants can navigate directly to the technical papers right from the FiO + LS conference app . Poster Presentation PDFs Locate the session or talk in “Event Schedule” and click on Authors presenting posters have the option to submit the the “Download PDF” link that appears in the description . PDF of their poster, which will be attached to their papers in IMPORTANT: You will need to log in with your registration OSA Publishing’s Digital Library . If submitted, poster PDFs email and password to access the technical papers . Access is will be available about three weeks after the conference end limited to Full Conference attendees only . date . While accessing the papers in OSA Publishing’s Digital Need assistance? Library, look for the multimedia symbol (above) . Contact our support team, available 24 hours a day Monday through Friday, and from 09:00 to 21:00 EDT on weekends, Exhibit Buyers’ Guide at +1 .888 .889 .3069 option 1 . The Exhibit Buyers’ Guide is composed of descriptions and contact information for exhibiting companies at this year’s conference, and Science & Industry Showcase activities . Guides will be provided to every FiO + LS attendee as part of registration . All exhibitor information changes will be communicated in the FiO + LS conference app . We encourage you to review the conference app carefully to stay informed of changes to the guide .

Join the Social Conversation at FiO + LS 2017! We will be tweeting about program highlights and the latest updates throughout the conference using Twitter . Follow @Opticalsociety on Twitter and tweet about your conference experience using #FIO17 in your tweets . Stop by the OSA booth for more details . Join the conversation .

FiO + LS 2017 • 17–21 September 2017 7 Conference Plenary Session Plenary Presentations Tuesday, 19 September, 08:00–09:30 International Ballroom Center, Terrace Level Jason Eichenholz Laura Cadonati Luminar Technologies, USA Georgia Institute of Technology, USA Building the Vision for Autonomous LIGO, Virgo, and the Dawn of a New Mobility Era in Gravitational Wave Astronomy Autonomous mobility is the disruptive Gravitational waves, ripples in the fabric technology of our era, and at its core are of space-time produced by catastrophic optical sensing challenges . Join OSA Fel- astrophysical events, are arguably the low and Co-Founder of Luminar, Jason most elusive prediction of Einstein’s Eichenholz, in an exploration of the past, theory of General Relativity, so feeble present, and future of mobility as seen through the eyes of a that Einstein himself thought their detection was impossible . laser physicist . Nevertheless, one hundred years later, the Laser Interferom- eter Gravitational-wave Observatory (LIGO) has announced About the Speaker: Jason Eichenholz is a serial entrepre- the observation of gravitational waves produced by the neur and pioneer in laser, optics and photonics product collision of two black holes . This groundbreaking discovery development and commercialization . Over the past 25 years, marks the opening of a new window on the Universe and he led the development of hundreds of millions of dollars of a new era of gravitational wave astrophysics, where grav- new photonics products . itational waves provide new insights into black holes and Before joining Luminar as CTO and co-founder, Eichenholz neutron stars, and may even reveal new objects . was the CEO and founder of Open Photonics, an open As LIGO and its sister project Virgo wrap up their latest data innovation company dedicated to the commercialization of acquisition run, plans are progressing towards a network of optics and photonics technologies . Prior to that, he served ground based detectors that will be tuning in the gravita- as the Divisional Technology Director at Halma PLC . In that tional wave signatures traveling to us from billion light years role he was responsible for supporting innovation, technolo- away . I will present the current status of the detectors, recent gy and strategic development for the Photonics and Health results, their implications for gravitational wave astronomy Optics Divisions . Before joining Halma, he was the CTO and and the outlook for future generations of gravitational wave Board Member of Ocean Optics Inc . as well as the Director detectors . of Strategic Marketing at Newport/Spectra-Physics .

Plenary Session About the Speaker: Laura Cadonati is a gravitational wave Eichenholz is a fellow of The Optical Society (OSA) and SPIE . astrophysicist, member of the Center for Relativistic Astro- He has served as the principal investigator for Air Force and physics at Georgia Tech . She has been a widely-recognized DARPA funded research and development programs and leader in the LIGO Scientific Collaboration in the years holds 10 U .S . patents on new types of solid-state lasers, dis- preparing for and including the discovery of gravitational plays and photonic devices . Eichenholz has a MS and PhD in waves, the most elusive prediction of Einstein’s theory of Optical Science and Engineering from CREOL – The College General Relativity . Cadonati’s research focuses on the de- of Optics and Photonics at the University of Central Florida tection, characterization and astrophysical interpretation of and a BS in Physics from Rensselaer Polytechnic Institute . short-duration gravitational wave signals that are produced by cataclysmic astrophysical events such as the collisions of black holes or core collapse supernovae . She received her undergraduate degree in Italy, with a Laurea in Physics at the University of Milano, and a PhD in Physics from Princeton University . She is a Fellow of the American Physical Society and past-chair for the Division of Gravity of the American Physical Society . She is deputy spokesperson for the LIGO Scientific Collaboration and was awarded an NSF Career Award .

8 FiO + LS 2017 • 17–21 September 2017 Visionary Speakers

Monday, 18 September, 08:00–08:45 of new technologies—such as micro fabricated ion traps, optical micro-electromechanical systems, advanced single Majed Chergui photon detectors, compact cryogenics and vacuum technol- Ecole Polytechnique Fédérale de Laus- ogies—toward a functional integration of quantum informa- anne, Switzerland tion processing systems . Theme: Laser Science Frontiers in X-ray Laser Spectroscopy Scott McEldowney Opportunities with Novel Ultrafast Oculus Research, USA Deep-UV to X-ray Tools Theme: Virtual Reality and Augmented Novel methods and instrumentation from Vision the X-ray to the deep-ultraviolet range have emerged in recent years that offer unique opportunities Building the Vision for Autonomous to probe a wide variety of systems, with elemental-selectiv- Mobility ity, structural sensitivity and high temporal resolution in the About the Speaker: Scott McEldowney femtosecond regime . After briefly introducing these meth- is lead optics researcher for Oculus Re- ods, we will give examples relevant to future electronic and search in Redmond, Washington, USA . He leads a multidis- structural dynamics of chemical and biological systems and ciplinary team of researchers conducting advanced research of solid materials . in near-eye display and advanced imaging systems . Prior to About the Speaker: Majed Chergui is Professor at the Ecole that, McEldowney was a Principal Optical Engineer for Mic- Polytechnique Fédérale de Lausanne (EPFL), Switzerland . He rosoft incubating new hardware technologies that included is known for developing novel ultrafast spectroscopic meth- the development of the Hololens and Kinect . He holds a MS ods . In particular, he pioneered ultrafast X-ray spectroscopy degree in Mechanical Engineering and a PhD in Optical Sci- and more recently, 2-dimensional deep-UV spectroscopy . ences from the College of Optical Sciences at the University With these tools and others, he has solved several problems of Arizona . in chemistry, physics and biology . He is also the founding editor-in-chief of “Structural Dynamics” (AIP Publishing) . In Wednesday, 20 September, 08:00–08:45 recent years, he received the Earle K . Plyler Prize for Mo- lecular Spectroscopy & Dynamics of the American Physical Evelyn Hu Society and the Edward Stern Award of the International Harvard University, USA X-ray Absorption Society . Theme: Nanophotonics and Plasmonics Nanophotonic Systems: Active Fabrics Jungsang Kim of Light Duke University, USA Profound advances in controlling material Theme: Optics in Computing structures and quality at the nanoscale has resulted in our enhanced ability to Quantum Computing using Trapped modulate, store, amplify and transmit Speakers Visionary Atomic Ions photonic information within ever-smaller “footprints .” The Quantum computers are capable of engineering of materials at the nanoscale has given rise to solving some computational problems an abundance of optical metamaterials and metasurfaces that are believed to be intractable using with extraordinary, heterogeneous photonic properties by conventional computers . Recent progress design, such as “near-zero index” materials and “flat” lenses in the development of high quality quantum bits and their and photonic controllers . The integration of heterogeneous successful manipulation have led to significant confidence photonic materials and components produces photonic net- that a moderate scale quantum computers can be construct- works and systems that can be regarded as seamless “fab- ed on leading physical platforms such as trapped ions and rics” of light, fabrics that may embody sensing, computation superconducting circuits . In this presentation, I will discuss and information transfer in new compact forms . Moreover, the prospect of constructing a scalable quantum processor current research in optomechanics indicates the possibility using trapped ions and progress made to date, leveraging of efficient transduction of photon and phonon energies state-of-the-art technical progress leveraging micro-fabri- (mechanical vibrations and heat), forming fabrics that are cated ion traps, optical micro machines, advanced optical not only compact and multi-functional, but also efficient . modulators and laser systems . Concurrently, a variety of two-dimensional materials such as graphene and transition metal dichalcogenides have also About the Speaker: Jungsang Kim leads the Multifunctional emerged as exceptional photonic, as well as electronic ma- Integrated Systems Technology group at Duke University . His terials . These materials have the promise of being naturally main area of current research is quantum information scienc- interwoven into emerging fabrics of light, with easy integra- es, where his group uses trapped atomic ions and a range tion onto electronic circuits . The promise of these fabrics of of photonics technologies in an effort to construct scalable light lies in “smart textiles” for individuals that could sense, quantum information processors and quantum communi- analyze, compute and communicate information about the cation networks . His research focuses on the introduction

FiO + LS 2017 • 17–21 September 2017 9 environment as well as harvest the energy that would power discuss two lines of research in this area that may allow us those functions . Moreover, these smart fabrics could be in- to overcome quantum and thermal limits on today’s best tegrated pervasively, atop vehicles, infrastructures (bridges, precision measurements . First, I will discuss using collective buildings), as well as natural objects to harvest energy, carry measurements to break through the standard quantum limit, out complex sensing and analysis of the local environment . a fundamental quantum fuzziness of any measurement using independent atoms . The collective measurement projects a About the Speaker: Evelyn Hu received a PhD and MA laser-cooled ensemble of rubidium atoms into an entangled degrees in Physics from Columbia University and a BA in state in which atoms conspire to partially cancel one anoth- Physics from Barnard College . Prior to her appointment at er’s quantum noise such that we can directly observe up to Harvard, she was Scientific Co-director, California Nanosys- 18 dB of phase resolution beyond the standard quantum tems Institute, and a Professor in the Departments of Electri- limit . Next, I will discuss our work to break through long- cal and Computer Engineering and Materials at the Univer- standing thermal limitations on laser linewidth by utilizing a sity of California, Santa Barbara . Previously, she worked at novel gain medium: the 1 millihertz linewidth optical transi- AT&T Bell Laboratories . tion in laser-cooled strontium atoms . I will describe our first observation of pulsed lasing and measurements that indicate that this type of laser could be more than 100,000 times less Wilhelm Kaenders sensitive to both the technical and thermal brownian motion TOPTICA Photonics AG, Germany of the cavity mirrors that limit today’s best stable lasers . We Quantum Physics: Science, Technology, also observe that the cavity can create long range spin-ex- but also Business and Politics?! change interactions between the strontium atoms, perhaps useful one day for both creating entanglement between the The quantum character of the physical atoms and creating a many-body energy gap to protect the world today is not only a tested scientific atomic coherence against dephasing . These are just two reality but it provides also an increasingly examples of answering a question that will be answered in interesting playfield for new technology many diverse and hopefully surprising ways in the next de- development . Many countries have cade: for precisely measuring our universe, what are things started national programs, often driven we can do with many quantum objects that we fundamental- by strategic and defense/security interest to identify and ly cannot do with just one? progress into quantum technology applications . The open skies-policy of fundamental research has been the key for About the Speaker: James Thompson’s laboratory at JILA success of the field and provides opportunities for existing and the University of Colorado focuses on trying to advance and new businesses, but there are political challenges at the the frontiers of fundamental measurement science using horizon, in particular for small companies . many-body systems where interactions and entanglement enable the breaking of thermal and quantum limits . He About the Speaker: Being infected by Cold Atom Physics as attended Florida State University, earning a BA and MS a PhD student at the Institute of Quantum Optics in Han- in Physics, and received his PhD in Physics in 2003 from nover, and being part of the technology of Hänsch’s group the Massachusetts Institute of Technology (MIT), where he at the Max-Planck-Institute in Garching, Wilhelm Kaenders also did his post doctoral work . He has received the 2004 started a successful business activity with tunable diode American Physical Society’s DAMOP thesis award and the laser technology . “Frequency Division” in the early days and Department of Commerce Bronze medal . His work includes “Frequency Combing” today have started the Passion of the most precise direct test to date of Einstein’s relationship Precision and are still the driving force in TOPTICA’s extend- E=mc2, the most precise mass comparisons ever performed, ed scientific product range on its way to mature markets . lasers using millihertz linewidth atomic transitions, narrow As cofounder of TOPTICA, he serves together with Thomas bandwidth entangled photons, and the achievement of 18 Weber as “Vorstand” . dB of observed spin-squeezing .

James K. Thompson University of Colorado at Boulder JILA, Thursday, 21 September, 08:00–08:45 USA Michael Godwin Visionary Speakers Theme: Laser Science Novel Lasers OSRAM Opto Semiconductors, USA Breaking Quantum and Thermal Limits: Theme: Automotive Things we can do with many quantum Digital Lighting Trends in Automotive objects that we cannot do with just Applications: Bits, Bytes and Photons one Novel methods and instrumentation During the twentieth century, the field from the X-ray to the deep-ultraviolet of laser and atomic science learned to master the quantum range have emerged in recent years that states of individual atoms and ions, enabling quantum-based offer unique opportunities to probe a precision sensors of time, acceleration, and gravity, as well wide variety of systems, with elemental-selectivity, structural as new probes of the fundamental nature of our universe . sensitivity and high temporal resolution in the femtosecond A new frontier is to move beyond the current single-atom regime . After briefly introducing these methods, we will paradigm of precision measurement, and now learn to give examples relevant to future electronic and structural harness interactions and correlations between many atoms dynamics of chemical and biological systems and of solid for realizing even more precise probes of nature . I will materials .

10 FiO + LS 2017 • 17–21 September 2017 About the Speaker: Michael S . Godwin is Director of Auto- Marc Taubenblatt motive LED Marketing with OSRAM Opto Semiconductors . IBM, USA He focuses on the automotive interior market globally and exterior market in North America . Prior to this position, God- Theme: Optics in Computing win has held positions in Interior Marketing in Regensburg, Optical Interconnects in Large Scale Germany, and Business Development, General Marketing Computing Systems...What’s Next? Manager and Product Marketing Manager in Michigan . All good exponentials must come to an Godwin joined OSRAM Opto Semiconductors in 1999 and end . but. we find new ways to continue assisted in establishing marketing and application teams in progress . When processor clock speeds the automotive and multi market industries . Through efforts could not be further increased due to chip power limitations, with his team, OSRAM was awarded the Automotive News we continued performance progress with multiple cores per PACE award (2002); Finalist distinction for industry 1st white chip, and now with accelerator chips, and all along scaling lighting on the Lincoln Navigator/Aviator (2006); PACE data centers and HPC systems to ever larger numbers of winner for Color on Demand (2011); Audi A8 winner OSTAR components . Optical interconnects have played a pivotal Headlamp and Audi A7 OSLON Black Flat Multichip product role in providing the interconnection bandwidth to allow family (2015) . scaling these systems, with per channel data rates increasing He previously held positions in sales management, man- from hundreds of Mb/s to many 10’s Gb/s . in the last few ufacturing and quality management with leading lighting, decades . Off-switch chip bandwidth will soon exceed 10 electrical interconnect and automotive sensor companies . Tb/s . Before long, electrical links will begin to reach practical per channel limits, and switch chip power will limit off-chip Godwin received his BS in Materials Science and Metallur- bandwidth . Tighter integration of optics with switch and gical Engineering from Michigan Technological University in compute chips, optical switching and advanced modulation 1987 . formats are a few examples where optics can offer potential paths forward, though not without pitfalls . What’s next for optical interconnects? Vladimir M. Shalaev About the Speaker: Marc Taubenblatt is currently Senior Purdue University and Birck Nanotech- Manager, Optical Communications and High Speed Test, at nology Center, USA IBM’s T .J . Watson Research Center, focusing on optical inter- Theme: Laser Science Plasmonics and connects and high speed electrical packaging for computer Nanophotonics systems and data centers, test and innovative diagnostic techniques for high performance computer chips and ther- Plasmonic Metamaterials Reimagined mal solutions for HPC and Data Center systems . He has had The fields of nanophotonics, plasmonics responsibility for coordinating the IBM Research WW optical and optical metamaterials have enabled interconnect strategy for the past 17 years . In addition, he unprecedented ways to control the flow currently manages a government sponsored research pro- light at both the micro- and nanometer length scales, un- gram on advanced computing technology . Taubenblatt has folding new optical phenomena, with a potential to reshape served on the IBM Research technical strategy staff, where the existing optical technologies and create new ones . In he co-led the Global Technology Outlook, an IBM Research this presentation, emerging plasmonic, metamaterial and Division wide effort in forecasting future technology trends . metasurfaces concepts as well as material platforms will be Before that, he managed the IBM Research Microelectronics discussed with the focus on practical photonic technologies Manufacturing Research Program, a cross-research R&D pro- Speakers Visionary for communication, quantum optics, bio-medical and energy gram in collaboration with IBM’s microelectronics division, applications . focusing on projects directly influencing semiconductor fabrication cost and efficiencies . About the Speaker: Vladimir M . Shalaev, Scientific Director for Nanophotonics at Birck Nanotechnology Center and Taubenblatt received a BS degree in Electrical Engineering Distinguished Professor of Electrical and Computer Engi- from Princeton University and MS and PhD degrees in Elec- neering at Purdue University, specializes in nanophotonics, trical Engineering from Stanford University . He has been at plasmonics and optical metamaterials . He has received IBM Research for over 31 years and is also a member of the several awards for his research in the field of nanophotonics IBM Academy of Technology and a Principal Research Staff and metamaterials, including the Max Born Award from The Member . Optical Society for his pioneering contributions to the field of optical metamaterials, the Willis E . Lamb Award for Laser Science and Quantum Optics, the Rolf Landauer medal of the ETOPIM (Electrical, Transport and Optical Properties of Inhomogeneous Media) International Association, the UNE- SCO Medal for the development of nanosciences and nanotechnologies, OSA and SPIE Goodman Book Writing Award, and the IEEE Photonics Society William Streifer Scientific Achievement Award . He is a Fellow of the IEEE, APS, SPIE, MRS and OSA . Shalaev has authored three books, 30 invited book chapters and over 500 research publications .

FiO + LS 2017 • 17–21 September 2017 11 Awards, Honors and Special Recognitions

FiO + LS Awards Banquet OSA Honorary Member Monday, 18 September John C. Mather, NASA’s Goddard Space Reception: 18:30 Flight Center, USA Program: 19:00–21:00 International Ballroom Center, Terrace Level The Optical Society’s Honorary Member- ship is the Society’s most distinguished Join your colleagues and the OSA Board of Directors at the membership status and is confirmed by inaugural FiO + LS Awards Banquet . Celebrate the achieve- the OSA Board of Directors . John C . ments of award and honor recipients from OSA and APS Mather was elected in 2016 for his con- Division of Laser Science and connect with colleagues . tribution to NASA’s Cosmic Background For the most up-to-date information on the banquet pro- Explorer (COBE) project which measured gram, please visit frontiersinoptics .com/awardsbanquet . the cosmic background radiation and its anisotropy with amazing precision from 50 to 600 GHz . This Note: This is a ticketed event. Limited tickets will be avail- is regarded as the starting point of cosmology as a precision able for purchase on-site at FiO registration up until 12:00 science . on Monday, 18 September. Esther Hoffman Beller Medal OSA 2017 Awards and Honors Martijn de Sterke, University of Sydney, Australia The Beller Medal recognizes outstanding contributions to Frederic Ives Medal/Jarus W. Quinn Prize optical science and engineering education . OSA recognizes Martijn de Sterke for far-reaching contributions to optics Margaret Murnane, University of and photonics education in Australia and the world through Colorado at Boulder, USA exceptional dedication to classroom teaching, outstanding PhD student advising and a sustained commitment to out- The Ives Medal/Quinn Prize recognizes reach activities . overall distinction in optics and is OSA’s highest award . OSA honors Margaret Murnane for pioneering and sustained Michael S. Feld Biophotonics Award contributions to ultrafast science ranging Paras N. Prasad, State University of New York at Buffalo, from femtosecond lasers to soft x-ray USA high-harmonic generation to attosecond The Feld Biophotonics Award recognizes individuals for their studies of atoms, molecules and surfaces . innovative and influential contributions to the field of biophotonics, regardless of their career stage . OSA recognizes Margaret Murnane is a Fellow of JILA and a faculty member Paras N . Prasad for pioneering research in biophotonics, in Physics at the University of Colorado . She runs a trans-dis- particularly in application of nonlinear optical and multipho- ciplinary research group with her husband, Henry Kapteyn . ton processes, and for promoting biophotonics and educat- She received her B .S and M S. . degrees from University ing future researchers through his seminal monographs and College Cork, Ireland, and her Ph .D . from UC Berkeley . She reviews . joined the faculty at Washington State University in 1990 . In 1996, she moved to the University of Michigan, and in Paul F. Forman Team Engineering Excellence Award 1999 to the University of Colorado . Henry and Margaret also Guide Star Alliance, representing TOPTICA Photonics AG, co-founded KMLabs, the first laser company to commercially Germany and MPB Communications, Inc., Canada offer 10fs Ti:sapphire lasers as well as coherent high harmon- The Forman Team Engineering Excellence Award recog- ic systems . nizes team technical achievements in optical engineering . Her research revolutionized ultrafast laser and x-ray science . OSA recognizes Guide Star Alliance for the development With her husband and their students, she first designed of the first high-power, fully remote-controlled, turn-key lasers that operated at the fundamental limits of stability and sodium guide star laser system with optimized photon return pulse duration . Murnane then developed a new understand- enabling next-generation adaptive optics under the extreme ing of extreme nonlinear optics, making it possible to effi- conditions of telescope sites . ciently upshift femtosecond lasers into the x-ray region via high-order harmonic generation (HHG) . By producing spa- Joseph Fraunhofer Award/Robert M. Burley Prize tially and temporally coherent beams that are fast enough to Yeshaiahu (Shaya) Fainman, University of California San capture all motion in our natural world relevant to function, Diego, USA HHG is impacting quantum materials, molecular, nano and The Fraunhofer Award/Burley Prize recognizes significant imaging science worldwide . research accomplishments in the field of optical engineering . OSA presents this award to Yeshaiahu (Shaya) Fainman for pioneering, seminal and wide ranging contributions to nanoscale engineering linear and nonlinear optical materials and devices for optical information processing systems . Awards and Honors Awards

12 FiO + LS 2017 • 17–21 September 2017 Edwin Land Medal OSA Fellows Alan C. Bovik, The University of Texas at Austin, USA Brian E. Applegate, Texas A&M University, USA The Land Medal recognizes pioneering work empowered For significant contributions to development of novel multi- by scientific research to create inventions, technologies, modal molecular and functional optical imaging approaches and products . It is co-sponsored by OSA and the Society and innovations in 3-D cochlear optical vibrometry, and for for Imaging Science and Technology . Alan Bocik is honored service to the optics community . for substantially shaping the direction and advancement of modern perceptual image quality computation, and for Roel G. F. Baets, Ghent University – IMEC, Belgium energetically engaging industry to transform his ideas into For major contributions to silicon photonics and service to global practice . the photonics community . John J. Degnan, Sigma Space Corp, USA Emmett N. Leith Medal For leadership in the advancement of laser technology and Jumpei Tsujiuchi, Japan its applications in satellite and precision interplanetary dis- The Leith Medal recognizes seminal contributions to the tance ranging, 3D imaging and atmospheric lidar, free space field of optical information processing . OSA honors Jumpei optical communication and medical instrumentation . Tsujiuchi for early pioneering work in optical information processing, holography and optical metrology, including the David W. Hahn, University of Florida, USA first demonstration of coherent optical processing for image For pioneering contributions to the analysis of aerosol par- restoration . ticles, including single particle analysis, using laser-induced breakdown spectroscopy while also advancing the funda- Adolph Lomb Medal mental understanding of plasma-analyte interactions . Dirk Robert Englund, Massachusetts Institute of N. Asger Mortensen, University of Southern Denmark, Technology, USA Denmark The Lomb Medal recognizes noteworthy contributions made For pioneering contributions to the field of photonic crystal to optics at an early career stage . Dirk Robert Englund is fibers and the theory of nonlocal phenomena in nanoplas- receiving this medal for pioneering contributions to scalable monics . solid-state quantum memories in nitrogen-vacancy diamond, high-dimensional quantum key distribution, and photonic Zhe-Yu Jeff Ou, Indiana University-Purdue University India- integrated circuits for quantum communication and compu- napolis, USA tation . For pioneering work in multi-photon interference, quantum entanglement of continuous variables, and narrow-band C. E. K. Mees Medal two-photon sources of light, for the work on precision phase Ming C. Wu, University of California, Berkeley, USA measurement in quantum metrology, and quantum amplifi- The Mees Medal recognizes an original use of optics across cation . different fields . OSA recognizes Ming C . Wu for the in- Keith D. Paulsen, Dartmouth College, USA vention of optoelectronic tweezers that enable massively For applications of diffuse optical tomography reconstruc- parallel manipulation of individual biological cells controlled tion methods and surgical guidance with stereovision and by digital optical projectors . fluorescence . Tomasz S. Tkaczyk, Rice University, USA William F. Meggers Award For development of cost effective technologies in optics, Shaul Mukamel, University of California Irvine, USA opto-mechanics, electronics, and materials to engineer novel The Meggers Award recognizes outstanding work in spec- imaging instruments, multi-dimensional snapshot imaging troscopy . Mukamel is being recognized for developing the modalities, and systems for early detection and treatment of theoretical framework of coherent multidimensional spec- cancer . troscopy for electronic excitations in the optical regime and proposing extensions to the x-ray spectral regime . Rashid Zia, Brown University, USA For seminal contributions to the field of nanophotonics, OSA Treasurer’s Award including pioneering work on surface plasmon waveguides, Scott Dineen, The Optical Society, USA optical-frequency magnetic dipole transitions, and energy- The OSA Treasurer’s Award recognizes an OSA employee momentum spectroscopy . who contributes significantly to organizational excellence, promotes and enacts innovative solutions and/or exemplifies inspirational leadership . Awards and Honors

FiO + LS 2017 • 17–21 September 2017 13 APS/Division of Laser Science Vivishek Sudhir, Ecole Polytechnique Federale De Laus- anne, Switzerland 2017 Awards and Honors Quantum Limits on Measurement and Control of a Me- chanical Oscillator Arthur L. Schawlow Prize in Laser Science Shuo Sun, University of Maryland, College Park, USA Louis F. DiMauro, The Ohio State Nanophotonic Spin-photon Quantum Transistor University, USA For groundbreaking work in several areas OSA Foundation 2017 Prizes and Special of high field and ultrafast optical science, Recognitions from high harmonic generation and free electron lasers to attosecond science . OSA Foundation Grant Recipients Louis F . DiMauro, Ph .D ., is professor of physics and the Edward and Sylvia The OSA Foundation would like to congratulate our FiO Hagenlocker Chair at The Ohio State grant recipients . Through the following programs we have University (Columbus) . He received his been able to provide nearly 20 grants, scholarships and B A. . in 1975 from Hunter College, the City University of prizes to help students attending FiO . New York, and his Ph .D . from the University of Connecticut You can help to inspire and support the next generation (Storrs) in 1980 and was a postdoctoral fellow at the State of science and engineering innovators by making a dona- University of New York, Stony Brook, before arriving at tion to the OSA Foundation . All donations are matched AT&T Bell Laboratories near Summit, New Jersey, in 1981 . 100% by The Optical Society—so your gift has twice the DiMauro joined the staff at Brookhaven National Laborato- impact . To learn more and to make a donation online, visit ry in Upton, New York, in 1988 rising to the rank of senior www .osa .org/foundation, or stop by the OSA booth . scientist . In 2004 he joined the faculty at OSU, the same year he was awarded the Brookhaven National Laboratory/ OSA Foundation Boris P. Stoicheff Memorial Brookhaven Science Associates Science & Technology Prize, the 2012 OSU Distinguished Scholar Award, and the 2013 Scholarship Optical Society (OSA) Meggers Prize . DiMauro is a fellow of 2017 Recipient: Ali K. Jahromi, University of Central the American Physical Society, The Optical Society (OSA), Florida, USA and the American Association for the Advancement of Sci- ence . He has served on numerous national and international Established in 2011 by the OSAF and the Canadian Asso- committees, government panels, served as the 2010 APS ciation of Physicists Educational Trust Fund (CAPETF), this Division of Atomic, Molecular and Optical Physics chair and program pays tribute to Boris P . Stoicheff, an internationally vice-chair of the National Academy of Sciences Committee renowned laser spectroscopist who also served as Presi- on Atomic, Molecular and Optical Sciences . His research dent of OSA (1976) and CAP (1983-84) .This $3,000 USD interest is in experimental ultra-fast and strong-field phys- scholarship is awarded annually to a graduate student who ics . In 1993, DiMauro and his collaborators introduced the has demonstrated both research excellence and significant widely accepted semiclassical model in strong-field physics . service to the optics or physics community . His current work is focused on the generation, measurement, Past student recipients for this program can be found online and application of attosecond X-ray pulses, and the study of at osa .org/stoicheff . 2017 recipient will also be announced at fundamental scaling of strong field physics . the FiO + LS Awards Banquet . Carl E. Anderson Division of Laser Science Dissertation Award The Carl E . Anderson Award for Outstanding Doctoral Dissertation in Laser Science was established in 2013 by the American Physical Society (APS) Division of Laser Science (DLS) . Its purpose is to recognize doctoral research in the Laser Science area and to encourage effective written and oral presentation of research results . The award consists of $1,000 USD and a certificate citing the contribution made by the recipient . The finalists will present their work at a special session of the Laser Science conference . The winner will be announced at the DLS business meeting Tuesday . The following presentations will be given during this special session: Tal Galfsky, The City University of New York CUNY Graduate Center, USA Control of Light-matter Interaction Using Photonic Hyper- crystals

Awards and Honors Awards Dennis Gardner, University of Colorado Boulder, USA First Demonstration of Sub-Wavelength Imaging at Short Wavelengths

14 FiO + LS 2017 • 17–21 September 2017 OSA Foundation Emil Wolf Outstanding Student Shun Fujii, Keio University, Japan Paper Competition Gun-Yeal Lee, Seoul National University, Republic of Korea M.V Jabir, Physical Research Laboratory, India This competition recognizes the innovation, research excel- Ezgi Sahin, Singapore University of Technology and Design, lence and presentation abilities of students presenting their Singapore work during FiO and honors Emil Wolf for his many contribu- Maria Solyanik, George Washington University, USA tions to science and The Optical Society . One winner is se- Nathália B. Tomazio, University of Sao Paulo/Sao Carlos lected from each of the seven FiO subcommittees . Winners Institute of Physics, Brazil receive a complimentary OSA three-year student member- Yunyi Yang, Centre for Micro-Photonics/Swinburne ship, an award stipend of $300 USD and an award certificate . University of Technology, Australia Past student recipients for this program can be found online Han Zhang, University of Texas at Arlington, USA at osa .org/wolf . 2017 recipients will also be announced at the FiO + LS Awards Banquet . OSA Foundation Jean Bennett Memorial Student Travel Grant Congratulations to our finalists competing at FiO: 2017 Recipient: Aonan Zhang, Nanjing University, China FiO 1: Fabrication, Design and Instrumentation Gun-Yeal Lee, Seoul National University, Republic of Korea Established in 2008, in memory of Jean M . Bennett, a highly David Miller, University of Colorado at Boulder, USA decorated research physicist who was recognized for her Haoyi Yu, RMIT University, Australia contributions to the studies of optical surfaces and served as OSA’s first female president, this $1,000 USD grant is FiO 2: Optical Interactions awarded to a student presenting their work at FiO . This Lorenzo De Angelis, Delft University of Technology, competition is administered by the OSA Foundation and is Netherlands made possible through the generous support of Nanoptek Rodrigo Gutiérrez-Cuevas, University of Rochester, USA Corporation, the Pennsylvania State University Department Fatholah Salehi, University of Maryland, USA of Physics and individual contributors . FiO 3: Quantum Electronics Past student recipients for this program can be found online Anand Bahl, University of Arizona, USA at osa .org/bennett . 2017 recipient will also be announced at Jeremy Pigeon, UCLA, USA the FiO + LS Awards Banquet . Yu Shiozawa, The University of Tokyo, Japan FiO 4: Photonics OSA Student Chapter & Local Section Ali Kazemi Jahromi, University of Central Florida, CREOL, USA Excellence Prize Alexander Lind, National Institute of Standards and OSA annually recognizes chapters and sections for excel- Technology, University of Colorado Boulder, USA lence supporting their local communities and their members . Kai Wang, Friedrich-Schiller-Universität Jena, The Australian Winners will be announced at FiO + LS . National University, Australia Finalists will compete for top honors in two categories: FiO 5: Biomedical Optics Joana Paiva, INESC TEC - INESC Technology and Science, Sciences Faculty of University of Porto, Portugal Community/Youth Education Outreach Seth Smith-Dryden, University of Central Florida, USA This category is for chapters and sections who have made Florian Stroehl, University of Cambridge, United Kingdom a difference in their local communities . These are chapters/ FiO 6: Information Acquisition, Processing and Display sections who visit schools and science fairs, create their own Yijun Bao, Georgia Institute of Technology, USA outreach kits as well as using the the Optics Suitcase in order Mahed Batarseh, University of Central Florida, USA to teach youth about the science of light . Zhean Shen, CREOL, USA Professional Development FiO 7: Vision and Color No finalists from FiO 7 The Professional Development category is for chapters/ sections that are well-oiled machines . These are chapters/ OSA Foundation Incubic/Milton Chang Travel Grant sections that hold technical conferences and lecture series with the polish of many professional conferences as well Funded by an endowment from Milton and Rosalind Chang, as chapters/sections who are able to guarantee a special this program provides 10 grants of $500 USD each to enable experience for members and support diversity and inclusion students who present papers to travel to Frontiers in Optics . within both the chapter/section and the optics and photon- Awards and Honors Grants are awarded to the presenter and usually the first ics community . author of the paper . Past student recipients for this program can be found online at osa .org/incubic . 2017 recipients will also be announced at the FiO + LS Awards Banquet . Travel Grant Recipients: Yijun Bao, Georgia Institute of Technology, USA Joshua A. Burrow, University of Dayton, USA

FiO + LS 2017 • 17–21 September 2017 15 Science & Industry Showcase

Tuesday, 19 September, 09:30–16:00 Meet OSA’s Journal Editors Wednesday, 20 September, 10:00–15:00 Tuesday, 19 September, 11:45–12:45 Columbia, Terrace Level Science Showcase Theater Come celebrate the anniversaries of Optics Letters and The FiO exhibition transforms into The Science & Industry Optics Express at the OSA Journals lunchtime reception . Showcase – in which exhibiting companies are partnered Enjoy complimentary pizza, cake and refreshments while with innovative demonstrations, networking events, poster conversing with OSA Publishing’s Editors-in-Chief, Deputy

Science & Industry Showcase presentations, e-posters and Rapid-fire Oral Presentations . Editors and Associate Editors . Bring your questions about Learn about new products, find technical and business submitting manuscripts, ideas for Feature Issues or other solutions and gain the most up-to-date market perspective questions and concerns about the journals . of your industry . Don’t miss this opportunity to visit companies representing a broad range of the best products and applications in the optics and photonics industry . There is no Pizza Lunch charge to attend the Showcase—it’s open to all registered Tuesday, 19 September, 12:00–13:00 attendees! Join your colleagues for a FREE pizza lunch . This is a great opportunity to meet the exhibitors and OSA Journal Editors . Beyond R2D2: Advances in Robotics Booth #119 Sponsored by The Laboratory for Computational Sensing and Robotics (LCSR) at the Johns Hopkins University will showcase cutting-edge research projects in Medical Robotics . The LCSR OSA Student Chapter Competition exhibition will include live demonstrations of surgical robots Tuesday, 19 September, 13:00–15:00 for eye surgery . It will also highlight other robotic work that Each year OSA student members are invited to participate include Extreme Environments Robotics, Human-Machine in a unique competition that tests their skills in the field . This Systems for Manufacturing, BioRobotics and more . See year students have been challenged to develop a hands on these demonstrations at Booth #119 during Showcase hours . outreach activity for K-12 youth education . The goal is to engage children in the optics and photonics field through a Poster Sessions & E-Posters variety of hands on activities . Tuesday, 19 September, 10:00–12:00, 13:00–15:00 Wednesday, 20 September, 10:00–12:00, 13:00–15:00 Congressional Fellowship Information Attend the Poster Sessions and view more than 500 posters Session scheduled for presentation . Poster presentations communi- Wednesday, 20 September, 12:00–13:00 cate new research findings in an intimate setting that encour- Science Showcase Theater ages lively and detailed discussion between presenters and attendees . Learn more about the Congressional Science Policy Fellow- ships from a past Congressional Fellow . The Congressional A select number of presentations will be offered as e-post- Science Policy Fellowships provide a unique opportunity for ers—which supplements the author’s introduction, motiva- PhD scientists and engineers to spend one year working for tion, results and conclusions with digital capabilities that aid a U .S . member of Congress or Congressional committee deeper discussion . Look for the symbol to see who E-Poster to learn about the policy making process while also bring- will be presenting e-posters . ing their scientific backgrounds and perspectives to the Congressional office . OSA cosponsors two Congressional Rapid-fire Oral Presentations Fellows per year . This information session will feature a past Science Showcase Theater Congressional Fellow who will discuss the fellowship experience, how it has had an impact on their career, why scientists Held in the Science Showcase Theater during the first hour and engineers should consider applying for the fellowship, of each poster session, a select number of poster presenters and answer questions from interested attendees . To learn offer Rapid-fire Oral Presentations, which consist of a brief more about the fellowships or the applications process, visit oral presentation accompanied by slides . This format en- www .osa .org/congressionalfellowships . ables poster presenters to preview key results from their research in brief, five-minute segments . In the session’s second hour, presenters are available for more in-depth discussions adjacent to their accompanying posters . The RAPID symbol indicates Rapid-fire Oral Presentations . See the abstracts for a detailed schedule .

16 FiO + LS 2017 • 17–21 September 2017 FiO 2017 Participating Companies: Science & Industry Showcase (as of 8/20/17) Booth Number Booth Number Accumold 219 NKT Photonics 203 American Association for the Advancement Ophir-Spiricon, LLC 310 of Science Sponsor Optimax Systems, Inc . 201 Asphericon 215 OSA Industry Development Associates (OIDA) Sponsor Association for Research in Vision and Ophthalmology 212 OSA Publishing Sponsor Bruker Nano Surfaces Division 204 Photonic Cleaning Technologies 314 De Gruyter 221 Photonics Media/Laurin Publishing 118, Publication Bin Energetiq Technology, Inc . 315 Physics Today 213, Publication Bin General Photonics Corp . 318 piezosystem jena, Inc . 303 High Tech Rochester Luminate Accelerator 304 SPIE: The International Society for Optics Imagine Optic/Axiom Optics 205 and Photonics 114 Inrad Optics 312 Springer Nature 302 IOP Publishing Ltd . 305 Synopsys, Inc . 409, Sponsor Liquid Instruments 115 OSA – The Optical Society 419 Material Research Society (MRS) Publication Bin Thorlabs 107 Menlo Systems, Inc . 112 Vermont Photonics Inc . 208 Microtech Instruments, Inc . 120 WORKinOPTICS 304 MKS (Newport Corp) 125 Wuhan National Lab for Optoelectronics 300 National Institute of Standards and Technology (NIST), Zygo Corporation 214 Center for Nanoscale Science &Technology 313

FiO + LS 2017 • 17–21 September 2017 17 Special Events Women of Light, a Special Program for Capitol Hill Visits Women in Optics hosted by WiSTEE Monday, 18 September, 09:00–12:00 Connect Senate and House Office Buildings, Washington D.C. Sunday, 17 September, 09:00–15:00 As Congress determines spending levels in the FY 2018 OSA Headquarters, 2010 Massachusetts Ave., NW, Budget, it is important for members of Congress to hear Washington, D.C. directly from their constituents about the importance of research and development funding . To facilitate those interac- The overall goal of the “Global Women of Light” Sympo- tions, OSA will be holding U .S . Capitol Hill visits to advocate sium is to shine light on women’s careers in science, tech- for R&D funding . Prior RSVP was required to participate . If nology, engineering, mathematics and entrepreneurship; you RSVP’d for Capitol Hill visits and have questions, contact recruit women across career ranks and disciplines; and build Brandy Dillingham at bdillingham@osa .org . a sustainable community of women in both academia and industry from which career growth, mobility and leadership opportunities may be sought . Grant Writing 101 Workshop Monday, 18 September, 12:30–14:00 WiSTEE Connect is an organization that serves to connect Fairchild Room, Terrace Level female students, faculty members, scientists, and engineers in Science, Technology, Engineering and Entrepreneurship Join the leaders of the OSA Tissue Imaging and Spectros copy Technical Group, Paul Campagnola and Kyle Quinn, for Special Events (STEE) from universities, government labs and private companies . The vision of WiSTEE Connect is to promote women a workshop aimed at helping young investigators develop leadership in STEE and assist women involved in these areas competitive grant proposals . Best practices and tips for to gain regional and/or global connections and recognition . writing strong grant proposals will be shared with workshop This organization helps to bridge the gap between science attendees . An RSVP is required for this workshop as lunch and entrepreneurship while providing a forum through which will be provided . Contact TGactivities@osa .org to register, women in these fields may learn, connect and lead . pending availability .

Funded by Sponsored by

Laser Science Symposium on Challenges and Emerging Opportunities in Undergraduate Research Molecular Probes and Nanobio-Optics Sunday, 17 September, 12:00–18:00 Monday, 18 September, 12:30-13:30 Jefferson East, Concourse Level Georgetown East, Concourse Level Organizers: Chad Hoyt, Bethel University, USA, and Harold Join the OSA Molecular Probes and Nanobio-Optics Tech- Metcalf, Stony Brook University, USA nical Group for a panel discussion exploring challenges and emerging opportunities in molecular probes and nano- The Symposium on Undergraduate Research has been a fea- bio-optics . Short presentations from our featured panelists ture of the annual meeting of the Division of Laser Science will be followed by a moderated question and answer of the American Physical Society (APS-DLS) for sixteen years, session, helping facilitate the exchange of information with and has showcased the research work of more than 500 our community . An RSVP is required for this technical group students during that time . Students’ presentations often de- event as lunch will be provided . Contact TGactivities@osa . scribe their work during the previous summer . The NSF has org to register, pending availability . played a vital role by providing the research opportunities for many of the students through its REU programs, as well as by direct support of the event . The symposium has been Sponsored by generously supported by the DLS, OSA, NSF, SPS, and Univ . MD (JQI), along with corporate sponsors Thorlabs, Photon- OSA Nonlinear Optics Technical Group ics Industries, East Coast Optical Technologies, and Bristol Workshop & Networking Session Instruments . Monday, 18 September, 16:00-17:30 Georgetown West, Concourse Level OSA Student Member Party Sunday, 17 September, 18:30–20:30 This special workshop will bring together researchers The Brixton, 901 U. St. NW Washington, DC interested in the area of nonlinear optics for a discussion on new and emerging topics in the field . Immediately OSA Student Members who are student full technical reg- following the presentations from the workshop’s featured istrants of FiO + LS are invited to attend the OSA Student speakers, attendees are invited to join the OSA Nonlinear Member Party . This party will celebrate the next generation Optics Technical Group for a small reception where they of leaders in the optics and photonics community with food, can network with colleagues over refreshments . Contact drinks and entertainment . TGactivities@osa .org to register, pending availability .

Sponsored by

20 FiO + LS 2017 • 17–21 September 2017 FiO + LS Committee Thanks to the technical program committee members! Your time and efforts are appreciated!

Frontiers in Optics General Chairs FiO 4: Photonics Steve Cundiff, University of Michigan, USA Greg Raybon, Nokia/Alcatel-Lucent, USA, Subcommittee Susana Marcos, Consejo Sup Investigaciones Cientificas, Chair Spain Paul Barclay, University of Calgary, Canada, Subcommittee Chair FiO Theme Coordinators Tymon Barwicz, IBM, USA Mina Esmaeelpour, Stanford University, USA Automotive Lara Garrett, TEsubcom, USA Alex Bowers, Schepens Eye Research Institute, USA Roger Helkey, University of California Santa Barbara, USA Ruben Mohedano, LPI Europe, Spain Femius Koenderink, AMOIF, Netherlands Chris Trowbridge, Argo, USA Dangyuan Lei, Hong Kong Polytechnique Montreal, Canada Qiang Lin, University of Rochester, USA Nanophotonics and Plasmonics Michelle Povinelli, University of Southern California, USA Dirk Englund, MIT, USA FiO 5: Biomedical Optics Optics in Computing David Busch, University of Pennsylvania, Children’s Hospital Katharine Shmidtke, Facebook, USA of Philadelphia, USA, Subcommittee Chair Caroline Boudoux, Wellman Center for Photomedicine, Virtual Reality and Augmented Vision Canada Bernard Kress, Microsoft, Inc., USA Félix Fanjul-Vélez, Universidad de Cantabria, Spain FiO 6: Information Acquisition, Processing and Display FiO Program Committees Wei Lee, National Chiao Tung University, Taiwan, Subcommittee Chair FiO 1: Fabrication, Design and Instrumentation Johannes Courtial, University of Glasgow, UK Byoungho Lee, Seoul National University, Korea, Ben Gallant, Daydream Virtual Reality Group, Google Inc., Committees Subcommittee Chair USA Jessica DeGroote Nelson, Optimax Systems, Inc., USA Hong Hua, University of Arizona, USA Pietro Ferraro, Inst. of Applied Sciences and Intelligent Bahram Javidi, University of Connecticut, USA System - CNR, Italy Amy Oldenburg, University of North Carolina at Chapel Hill, Groot Gregory, Synopsys, Inc., USA USA Yoshio Hayasaki, Utsunomiya University, Japan Anne Sentenac, Fresnel Institute, France Joohwan Kim, NVIDIA Corporation, USA Kenji Yamamoto, National Institute of Information and John Koshel, University of Arizona, USA Communications Technology, Japan Pascal Picart, Laboratoire d’Acoustique de l’Universite du Maine, France FiO 7: Vision and Color Jamie Leigh Ramsey, Rochester Precision Optics, USA Gabriel Diaz, Rochester Institute of Technology, USA, Yunlong Sheng, Université Laval, Canada Subcommittee Chair Simon Thibault, Université Laval, Canada Jeff Mulligan, NASA Ames Research Group, USA Changhe Zhou, Shanghai Inst. of Optics and Fine Mechanics, Marina Zanolli, Oculus Research, USA China FiO 2: Optical Interactions Laser Science Chairs Kishan Dholakia, University of St. Andrews, UK, Mark G . Raizen, University of Texas at Austin, USA Subcommittee Chair Roseanne J . Sension, University of Michigan, USA Greg Gbur, University of North Carolina at Charlotte, USA Carlos Lopez-Mariscal, Underwater Photonics, Mexico Laser Science Program Committees Takashige Omatsu, Chiba University, Japan Halina Rubensztein-Dunlop, University of Queensland, 1. High-harmonic Generation: Time, Energy, and Australia Complexity Donna Strickland, University of Waterloo, Canada Josh Vura-Weis, University of Illinois-Urbana Champaigne, USA, Organizer FiO 3: Quantum Electronics Dan Gauthier, The Ohio State University, USA, 2. Frontiers in X-ray Laser Spectroscopy Subcommittee Chair Roseanne J . Sension, University of Michigan, USA Paul M . Alsing, Air Force Research Laboratory, Rome, Italy 3. Plasmonics and Nanophotonics Antonio Badalato, University of Ottawa, Canada Serge Massar, Universite Libre de Bruxelles, Belgium Mark G . Raizen, University of Texas at Austin, USA Christine Silberhorn, Universitat Pderhorn, Germany 4. Novel Lasers Brian Smith, University of Oregon, USA Hui Cao, Yale University, USA, Organizer Michael Vasilyev, University of Texas at Arlington, USA

FiO + LS 2017 • 17–21 September 2017 21 22 FiO + LS 2017 • 17–21 September 2017 Explanation of Session Codes Agenda of Sessions

FTu1A.4

Session Designation (alphabetically)

Meeting Name Number F = Frontier in Optics (FiO) Series Number (presentation L = Laser Science (LS) 1 = First Series of Sessions order within J = Joint 2 = Second Series of Sessions the session)

Day of the Week M = Monday Tu = Tuesday W = Wednesday Th = Thursday

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, Wednesday = W, Thursday = Th). The third element indicates the session series in that day (for instance, 1 would denote the first parallel sessions in that day). Each day begins with the letter A in the fourth element and continues alphabetically through a series of parallel sessions. The lettering then restarts with each new series. The number on the end of the code (separated from the session code with a period) signals the position of the talk within the session (first, second, third, etc.). For example, a presentation coded FW2A.1 indicates that this paper is part of the FiO + LS Meeting and is being presented on Wednesday (W) in the second series of sessions (2), and is the first parallel session (A) in that series and the first paper (1) presented in that session.

Agenda of Sessions — Sunday, 17 September

15:00–18:00 Registration, Concourse Foyer

07:00–17:00 OSA Student Chapter Leadership Conference (Invitation Only), International Ballroom East, Concourse Level

09:00–15:00 Women of Light: A Special Program for Women in Optics, OSA Headquarters, 2010 Massachusetts Ave., NW

12:00–18:00 Laser Science Symposium on Undergraduate Research, Jefferson East, Concourse Level

18:30–20:30 OSA Student Member Party, The Brixton, 901 U Street, NW

All locations listed are in the Washington Hilton unless otherwise noted. Locations may change, please check the conference app and update sheet for the latest scheduling updates.

Key to Shading Frontiers in Optics Laser Science Joint

FiO + LS 2017 • 17–21 September 2017 23 Agenda of Sessions — Monday, 18 September

International International Georgetown Georgetown Jefferson Jefferson Ballroom West Ballroom East West East West East 07:00–18:00 Registration, Concourse Foyer 08:00–08:45 FM1A • FM1B • LM1C • Visionary Visionary Visionary Agenda of Sessions Speaker: Speaker: Scott Speaker: Majed Jungsang Kim McEldowney Chergui 08:45–09:00 Break 09:00–12:00 Capitol Hill Visits, Senate and House Office Buildings, Washington D.C. 09:00–10:00 FM2A • FM2B • FM2C • Optical FM2D • FM2E • LM2F • Modulators and Advances with Systems for Quantum Quantum Frontiers in Resonators Pulsed Laser Automotive Measurement Absorbers and X-ray Laser Sources Applications and Emitters Spectroscopy Communication 10:00–10:30 Coffee Break, International Terrace, Terrace Level 10:30–12:30 FM3A • Silicon FM3B • FM3C • FM3D • FM3E • LM3F • Carl Photonics I Trapping and Computational/ Nanophotonics I Quantum E. Anderson Advanced Beam Transformation Memories and Outstanding Shaping Optics and Interfaces Dissertation Optics in Award in Laser Computing Science 12:30–13:30 Lunch Break (on your own) 12:30–13:30 Challenges and Emerging Opportunities in Molecular Probes and Nanobio-Optics, Georgetown East, Concourse Level 12:30–14:00 Grant Writing 101 Workshop, Fairchild Room, Terrace Level 13:30–15:30 FM4A • FM4B • Studies FM4C • General FM4D • FM4E • High- LM4F • X-Ray Plamonics and with Complex Information Biomedical Dimension Science With Metamaterials Media, Imaging Acquisition, Optics in Quantum Table Top and and Light Processing and Scattering Systems and XFEL Lasers Display Media Simulation 15:30–16:00 Coffee Break, International Terrace, Terrace Level 16:00–17:30 Workshop: Understanding Unconscious Bias, Georgetown East, Concourse Level 16:00–17:30 OSA Nonlinear Optics Technical Group Workshop & Networking Session, Georgetown West, Concourse Level 16:00–18:00 Evening with the Agencies & Reception, Jefferson West, Concourse Level 18:30–21:00 FiO + LS Awards Banquet, International Ballroom Center, Terrace Level

All locations listed are in the Washington Hilton unless otherwise noted. Locations may change, please check the conference app and update sheet for the latest scheduling updates.

Key to Shading Frontiers in Optics Laser Science Joint

24 FiO + LS 2017 • 17–21 September 2017 Agenda of Sessions — Tuesday, 19 September Agenda of Sessions

International International Georgetown Georgetown Jefferson Jefferson Ballroom West Ballroom East West East West East 07:00–17:30 Registration, Concourse Foyer

08:00–09:30 JTu1A • Joint Plenary Session, International Ballroom Center, Terrace Level

09:30–10:00 Exhibits and Coffee Break, Science & Industry Showcase, Columbia, Terrace Level

10:00–12:00 JTu2A • Science & Industry Showcase Exhibits, Poster Session & E-Posters Rapid-Fire Oral Presentations I in Theater Columbia, Terrace Level

11:45–12:45 Meet OSA’s Journal Editors, Science Showcase Theater, Columbia, Terrace Level

12:00–13:00 Pizza Lunch, Science & Industry Showcase, Columbia, Terrace Level

13:00–13:30 Coffee Break, Science & Industry Showcase, Columbia, Terrace Level

13:00–15:00 JTu3A • Science & Industry Showcase Exhibits, Poster Session & E-Posters Rapid-Fire Oral Presentations II in Theater Columbia, Terrace Level

15:00–16:30 FTu4A • FTu4B • FTu4C • Display FTu4D • Novel FTu4E • LTu4F • High Integrated Advanced Technology Phenomena Quantum Harmonic Optics Spectroscopy for VR/AR in Photonic Electronics in Sources and and New Applications Devices the Automotive Applications Approaches Sector

16:30–16:45 Break

16:30–17:00 Environmental Sensing Technical Group Networking Event, OSA Technical Group Booth, International Terrace, Terrace Level

16:45–18:15 FTu5A • Pulse FTu5B • FTu5C • Real- FTu5D • FTu5E • LTu5F • and Comb Advanced time Optical Nanophotonic Quantum Applications of Sources Imaging and Guidance of Systems Measurement Ultrafast X-rays Interactions Cancer Therapy and Sensors with Materials

17:30–18:15 OSA Annual Business Meeting, Kalorama, Lobby Level

17:30–18:30 APS Division of Laser Science Annual Business Meeting, Holmead East, Lobby Level

18:30–20:30 FiO + LS Conference Reception, International Ballroom Center, Terrace Level

All locations listed are in the Washington Hilton unless otherwise noted. Locations may change, please check the conference app and update sheet for the latest scheduling updates.

Key to Shading Frontiers in Optics Laser Science Joint

FiO + LS 2017 • 17–21 September 2017 25 Agenda of Sessions — Wednesday, 20 September

International International Georgetown Georgetown Jefferson Jefferson Ballroom West Ballroom East West East West East 07:30–17:30 Registration, Concourse Foyer 08:00–08:45 FW1A • FW1B • LW1C • Visionary Visionary Visionary

Agenda of Sessions Speaker: Evelyn Speaker: Speaker: James Hu Wilhelm K.Thompson Kaenders 08:45–09:00 Break 09:00–10:00 FW2A • FW2B • FW2C • Optics FW2D • The FW2E • LW2F • Quantum Trapping and in Computing “Rush Hour”: Precision Nanophotonics Communications Shaping of Light and Imaging Science Policy Measurement II talk by Rush Using Holt Laser-atom Interactions 10:00–10:30 Coffee Break, Science & Industry Showcase, Columbia, Terrace Level 10:00–12:00 JW3A • Science & Industry Showcase Exhibits, Poster Session & E-Posters Rapid-Fire Oral Presentations III in Theater Columbia, Terrace Level 12:00–13:00 Lunch Break (on your own) 12:00–13:00 Congressional Fellowship Program Information Session, Science Showcase Theater, Columbia, Terrace Level 12:00–13:00 OSA Optical Material Studies Technical Group Special Talk, Georgetown West, Concourse Level 12:00–13:00 Polarization Optics - Design and Fabrication Trends and Challenges, Georgetown East, Concourse Level 12:00–13:30 OIDA VIP Industry Leaders Speed Meetings Lunch, Kalorama, Lobby Level 13:00–13:30 Coffee Break, Science & Industry Showcase, Columbia, Terrace Level 13:00–15:00 JW4A • Science & Industry Showcase Exhibits, Poster Session & E-Posters Rapid-Fire Oral Presentations IV in Theater Columbia, Terrace Level 15:00–16:30 FW5A • Silicon FW5B • FW5C • Optical FW5D • FW5E • LW5F • High- Photonics II Shaping, Phase, Systems for Advanced Quantum harmonic and Microscopy VR/AR Microscopy and Nonlinear Generation: Imaging Optics and Time, Energy, Nanophotonics and Complexity 15:30–17:00 Meet the APS Journal Editors Reception, International Terrace, Terrace Level 16:30–17:00 Pairing Photons to Electrons: An OSA Nanophotonics Technical Group Networking, OSA Technical Group Booth, International Terrace, Terrace Level 16:45–18:15 FW6A • Optical FW6B • Novel FW6C • FW6D • Super- FW6E • LW6F • Novel Fibers and Studies of Nanophotonics resolution Quantum Lasers I Transmission Waveguides Devices and and Extreme Electronics and Atomic Instrumentation Microscopy of Ultrafast Interactions Signals and Atmospheric Propagation 18:30–20:00 Networking with the OSA Biomedical Optics Technical Groups, OSA Headquarters, 2010 Massachusetts Ave., NW

All locations listed are in the Washington Hilton unless otherwise noted. Locations may change, please check the conference app and update sheet for the latest scheduling updates.

Key to Shading Frontiers in Optics Laser Science Joint

26 FiO + LS 2017 • 17–21 September 2017 Agenda of Sessions — Thursday, 21 September Agenda of Sessions

International International Georgetown Georgetown Jefferson Jefferson Ballroom West Ballroom East West East West East 07:30–11:30 Registration, Concourse Foyer

08:00–08:45 FTh1A • FTh1B • LTh1C • Visionary Visionary Visionary Speaker: Marc Speaker: Speaker: Taubenblatt Michael Godwin Vladimir M. Shalaev

08:45–09:00 Break

09:00–10:00 FTh2A • FTh2B • High FTh2C • Optical FTh2D • FTh2E • Optics LTh2F • Tailoring Harmonics Coherence Fabrication for in Computing Plasmonics Light with and Novel Tomography Nanophotonics Nanophotonic Photomemission in Biomedical Structures Optics

10:00–10:30 Coffee Break, International Terrace, Terrace Level

10:30–12:30 FTh3A • FTh3B • FTh3C • Vision FTh3D • FTh3E • LTh3F • Nanophotonics Optomechanics and Color Instrumentation Quantum Plasmonics and for Computing and Sensors for Optical Simulation, Lasing and Sensing Devices and Communication Systems and Entanglement

12:30–13:30 Lunch Break (on your own)

13:30–15:30 FTh4A • FTh4B • LTh4C • Novel Postdeadline Postdeadline Lasers III Papers Papers

All locations listed are in the Washington Hilton unless otherwise noted. Locations may change, please check the conference app and update sheet for the latest scheduling updates.

Key to Shading Frontiers in Optics Laser Science Joint

FiO + LS 2017 • 17–21 September 2017 27 International Ballroom West International Ballroom East Georgetown West

FiO

07:00–18:00 Registration, Concourse Foyer

08:00–08:45 FM1A • Visionary Speaker: Jungsang Kim, International Ballroom West FM1B • Visionary Speaker: Scott McEldowney, International Ballroom East LM1C • Visionary Speaker: Majed Chergui, Jefferson East

08:45–09:00 Break

09:00–12:00 Capitol Hill Visits, Senate and House Office Buildings, Washington D.C. ber

09:00–10:00 09:00–10:00 09:00–10:00 FM2A • Modulators and Resonators FM2B • Advances with Pulsed Laser FM2C • Optical Systems for Automotive Sources Applications Presider: Tyler Neely; The University of Presider: Byoungho Lee; Seoul National Queensland, Australia University, South Korea

FM2A.1 • 09:00 FM2B.1 • 09:00 FM2C.1 • 09:00 Invited Monday, 18 Septem Monday, Electro-Optic Switching and Regenerative Oscillation of Laser wakefield acceleration with mid-IR laser pulses, The Photonics Supply Chain for Autonomous Vehicles 1 1 2 a Localized Gap Plasmomechanical Resonator, Brian J. Daniel C. Woodbury , Linus Feder , Valentina Shumakova , - Technology, Tools and Talent, Ira Moskowitz1; 1The 1 1 1 2 1 1 Roxworthy , Vladimir Aksyuk ; Center for Nanoscale Sciene Claudia Gollner , Bo Miao , Robert Schwartz , Andrius Innovation Inst. at the MassTech Collaborative, USA. This 2,3 2,3 1 1 and Technology, National Inst. of Standards and Technology, Baltuška , Audrius Pugzlys , Howard Milchberg ; Univ. of presentation will explore the opportunities as well as the 2 USA. We present a plasmomechanical system comprising Maryland at College Park, USA; Vienna Univ. of Technology, challenges of the photonics supply chain for self-driving 3 localized gap-plasmon resonators embedded into tunable Austria; Center for Physical Sciences & Technology, Lithua- cars, emphasizing the most essential technologies that will nanomechanical devices. We show low-voltage tuning of lo- nia. We present the first results from laser plasma wakefield be required such as photonic integrated LIDAR circuits. calized plasmons and observe plasmon-driven regenerative acceleration driven by ultrashort mid-infrared laser pulses mechanical oscillations. (100fs, λ=3.9μm). The onset of relativistic self-focusing and electron acceleration scale with critical laser power and target width.

FM2A.2 • 09:15 FM2B.2 • 09:15 Graphene electro-absorption optical modulator design MeV electron acceleration at 1 kHz with <10 mJ Laser onto a D-shaped optical fiber, Maria Cecília S. Araújo1, Pulses, Fatholah Salehi1, Andy Goers1, George Hine1, Linus Rafael E. De Oliveira1, Lucia A. Saito1; 1Mackenzie Presby- Feder1, Donghoon Kuk1, Bo Miao1, Daniel C. Woodbury1, Ki- terian Univ., Brazil. We present the design of a graphene Yong Kim1, Howard Milchberg1; 1Univ. of Maryland, USA. We

electro-optical modulator with a dielectric layer of Al2O3 built demonstrate laser driven acceleration of electrons to MeV onto a D-shaped optical fiber. The all-fiber optical modulator scale energies at 1 kHz repetition rate using few mJ pulse

is optimized by controlling the dielectric thickness, achieving energies focused on near critical density He and H2 gas jets. ~1GHz bandwidths.

FM2A.3 • 09:30 FM2B.3 • 09:30 FM2C.2 • 09:30 Invited Sub-wavelength Plasmonic Graphene-based Slot Temperature determination in a supersonic gas jet from Flat-panel See-through Display for Augmented Reality 1 Electro-optic Modulator, Zhizhen Ma , Mohammad H. self-absorption free excitation spectra of carbon monox- Using Symmetric Integral Imaging System, Yasuhiro 1 1 1 1 1 1 1 Tahersima , Rubab Amin , Sikandar Khan , Volker J. Sorger ; ide, Andre de Bruyn , Christin Steenkamp , Erich G. Rohwer , Takaki1; 1Tokyo Univ of Agriculture and Technology, Japan. 1 1 1 George Washington Univ., USA. We proposed a novel Anton Du Plessis ; Univ. of Stellenbosch, South Africa. In this Optical see-through 3D displays having a flat-panel shape structure for plasmonic graphene modulator. Extinction study the effect of self-absorption on rotational excitation have been developed, which can be used for future smart ratio (ER) larger than 1 dB/um is shown using single layer spectra in the VUV region and the role that self-absorption phones and tablets. The symmetric integral imaging system graphene. Also, by engineering more layers of graphene, plays in determining the rotational temperature of a super- is employed. Produced 3D images can occlude real scenes. an even higher ER is demonstrated. sonic gas jet is reported.

FM2A.4 • 09:45 FM2B.4 • 09:45 Sub 1-Volt Graphene-based Plasmonic Electroabsorp- Commissioning experiments of VEGA-2 at Centro de La- tion Modulator on Silicon, Sikandar Khan1, Zhizhen Ma1, seres Pulsados (CLPU), M Huault2, G Zeraouli2, J G. Ajates2, Joohyeon Jeon2, Cheol J. Lee2, Volker J. Sorger1; 1George J Apinaniz2, E Garcia2, I Hernandez2, S Malko2, C Mendez2, J Washington Univ., USA; 2Dept. of Micro/Nano Systems, A. Perez2, J D. Pisonero2, C Salgado2, X Vaisseau2, O Varela2, Korea Univ., South Korea. We experimentally show a sub-volt Giancarlo Gatti2, Luca Volpe2, Luis Roso2, Robert Fedoseje- graphene-based hybrid plasmonic waveguide-integrated vs4, A Longman4, Ronnie Shepherd3, Wendell T. Hill1; 1Univ. electro-absorption modulator showing an extinction ratio of Maryland at College Park, USA; 2CLPU, Spain; 3LLNL, (0.25 dB/μm) compact footprint (5 μm2) enabled by improved USA; 4Univ. of Alberta, Canada. The results of commissioning both electrostatics and mode overlap factor. experiments -- betatron radiation and protons acceleration from gaseous and solid targets -- at the petawatt user facility, Centro de Laseres Pulsados in Salamanca, Spain, are reviewed along with facility capabilities.

10:00–10:30 Coffee Break, International Terrace, Terrace Level

28 FiO + LS 2017 • 17–21 September 2017 Georgetown East Jefferson West Jefferson East

FiO LS

07:00–18:00 Registration, Concourse Foyer

08:45–09:00 Break

09:00–12:00 Capitol Hill Visits, Senate and House Office Buildings, Washington D.C. Monday, 18 Septem

09:00–10:00 09:00–10:00 09:00–10:00 FM2D • Quantum Measurement and FM2E • Quantum Absorbers and Emitters LM2F • Frontiers in X-ray Laser Communication Presider: Amy Helmy; University of Toronto, Spectroscopy Presider: Bonnie Schmittberger; University Canada Presider: Philippe Wernet; Helmholtz- of Maryland, USA Zentrum Berlin, Germany ber

FM2D.1 • 09:00 FM2E.1 • 09:00 LM2F.1 • 09:00 Invited Experimental contextuality of quantum and classical Combined Atomic Force Microscopy and Photolumines- Finding Intersections Between Electronic Excited States 1 1 2 systems, Aonan Zhang , Lijian Zhang , Brian J. Smith ; cence Imaging to Increase the Yield of Quantum Dot with Ultrafast X-ray Scattering and Spectroscopy, Kelly 1 1,2 2 3 National Lab of Solid State Microstructures and College Photonic Devices, Luca Sapienza , Jin Liu , Jin Dong Song , Gaffney2,1, Kasper Kjaer3; 1Stanford Univ., USA; 2SSRL and 4 4 5 of Engineering and Applied Sciences, Nanjing Univ., Stefan Falt , Werner Wegscheider , Antonio Badolato , Kartik PULSE Inst., SLAC National Accelerator Lab, USA; 3Centre 2 2 1 2 China; Dept. of Physics and Oregon Center for Optical, Srinivasan ; Univ. of Southampton, UK; National Inst. of for Molecular Movies, Dept. of Physics, Technical Univ. 3 Molecular, and Quantum Science, Univ. of Oregon, USA. Standards and Technology, USA; Center for Opto-Electronic of Denmark, Denmark. We use ultrafast x-ray emission 4 Contextuality of quantum and classical systems is examined. Materials and Devices Research,, KIST, South Korea; ETH, spectroscopy and x-ray scattering to study spin crossover 5 Differing definitions of events result in a range of violations of Switzerland; Dept. of Physics, Univ. of Ottawa, Ottawa, , 2+ in [Fe(bipyridine)3] . These measurements enable the pro- non-contextual hidden-variable models. This highlights clas- Canada. We present a combined optical and AFM charac- jection of intersections between ligand field excited states sical-correlation resources and the quantum-classical divide. terization technique that determines whether single InAs/ onto the Fe-ligand bond length coordinate. GaAs quantum dots appear in proximity to topographic surface features that can be detrimental to quantum photonic device performance.

FM2D.2 • 09:15 FM2E.2 • 09:15 Experimental demonstration of loop state-prepara- Metallic Nano-Rings for Free-Space Extraction of Light tion-and-measurement tomography, Mark Beck1, Aidan from Single Quantum Dots, Oliver Trojak1, Jin Dong Song2, F. McCormick1, Steven J. van Enk2; 1Whitman College, Luca Sapienza1; 1Univ. of Southampton, UK; 2Korea Inst. of USA; 2Univ of Oregon, USA. We demonstrate, using qubits Science and Technology, South Korea. We show 25× en- encoded in the polarization of heralded individual photons, hancements of the free-space collection of light from single that loop state-preparation-and-measurement tomography In/As quantum dots, via metallic nano-rings deposited on the is capable of detecting correlated errors between the prepa- sample surface. Such a lensing effect is broadband, scalable ration and the measurement of a quantum system. and compatible with any substrate/emitter.

FM2D.3 • 09:30 FM2E.3 • 09:30 Invited LM2F.2 • 09:30 Weather-proof Quantum Communications, Yong Meng Single Photon Absorption by Single Photosynthetic Light Polarized XANES Elucidate Femtosecond Bond Elonga- 1 1 1 1 1 1 1 Sua , Heng Fan , Amin Shahverdi , jiayang chen , Rainer Harvesting Systems, Birgitta Whaley1; 1Univ. of California tion, Nicholas A. Miller , Roseanne J. Sension ; Univ. of 1 1 1 Martini , Yuping Huang ; Stevens Inst. of Technology, Berkeley, USA. I present a unified theoretical analysis of Michigan, USA. Ultrafast x-ray spectroscopy characterizes the USA. We identify a weather-proof channel for quantum quantum dynamics of single photon absorption and sub- excited state structural relaxation in vitamin B12. Polarized communications using 3950 nm photons, and report on sequent excitonic energy transfer in photosynthetic light XANES separates in-plane and out-of-plane contributions. their generation and detection via parametric conversion harvesting complexes with implications for spatio-temporal These contributions show discrete relaxation of axial, then with coincidence to accidental ratio of 54±7 and spectral dynamics of absorption from sunlight. equatorial ligands. brightness of 4.4x102 pair/s/nm/mW.

FM2D.4 • 09:45 LM2F.3 • 09:45 Phase sensing with a truncated SU(1,1) interferometer, X-Ray Amplification by Stimulated Brillouin Scattering, Prasoon Gupta1, Brian E. Anderson1, Bonnie L. Schmitt- Matthew Edwards1, Julia M. Mikhailova1, Nathaniel J. Fisch1; berger1, Travis Horrom1, Carla Hermann-Avigliano1, Kevin 1Princeton Univ., USA. Parametric amplification using stimu- Jones2, Paul D. Lett1,3; 1Univ. of Maryland, College Park, lated Raman or Brillouin scattering in plasma may generate USA; 2Williams College, USA; 3National Inst. of Standards extraordinarily intense x-ray pulses. Particle-in-cell simula- and Technology, USA. We present an SU(1,1) interferometer tions suggest that ion-based Brillouin amplification provides variation by replacing the second nonlinear interaction with efficient x-ray amplification. the homodyne detection and demonstrate an improvement in phase sensitivity over the standard quantum limit.

10:00–10:30 Coffee Break, International Terrace, Terrace Level

FiO + LS 2017 • 17–21 September 2017 29 International Ballroom West International Ballroom East Georgetown West

FiO

10:30–12:30 10:30–12:30 10:30–12:30 FM3A • Silicon Photonics I FM3B • Trapping and Advanced Beam FM3C • Computational/Transformation Presider: Volker Soger; George Washington Shaping Optics and Optics in Computing University, USA Presider: Benjamin Perez-Garcia; Presider: Johannes Courtial; University of Underwater Photonics, Mexico Glasgow, UK

FM3A.1 • 10:30 Invited FM3B.1 • 10:30 Invited FM3C.1 • 10:30 Invited Progress on Multilayer Silicon Nitride-on-Silicon Integrat- Exploring Exotic Polarization Topologies in Complex 3D Computational Optical Imaging for 3D Capture and Dis- ed Photonic Platforms, Joyce K. Poon1; 1Univ. of Toronto, Electromagnetic Fields, Peter Banzer1; 1Max-Planck-Inst play Devices, Ginni Grover1; 1Intel Labs, USA. Computational Canada. This talk presents my group’s progress in multilayer Physik des Lichts, Germany. If electromagnetic fields are optical systems allow novel architectures for capturing real silicon nitride-on-silicon integrated photonic platforms. spatially confined, exotic polarization phenomena and to- world in multiple dimensions and showing it on displays These platforms are useful for the implementation of very pologies can be observed. Here, we discuss the appearance which enable 3D perception. In this talk, I explore integral large-scale, three-dimensional silicon photonic circuits. and experimental study of optical polarization Möbius strips displays, issues of human perception and capture methods. ber and ribbons at the nanoscale. Monday, 18 Septem Monday,

FM3A.2 • 11:00 FM3B.2 • 11:00 FM3C.2 • 11:00 Connecting Visible and Telecommunications Wavelengths Direct observation of optical trapping of a single quantum A Composite Algorithm for Optimized Baseline Correc- with Silicon Nitride Nanophotonics, Xiyuan Lu1, Qing Li1, dot with an all-silicon nanoantenna, Zhe Xu1, Wuzhou tion in Raman Spectroscopy, Andrew Huzortey1, Benjamin Daron Westly1, Kartik Srinivasan1; 1NIST, USA. We report Song1,2, Kenneth B. Crozier1,3; 1School of Physics, Univ. of Anderson1, Alfred Owusu1; 1Univ. of Cape Coast, Ghana. We a nanophotonic device connecting visible and telecom Melbourne, Australia; 2School of Materials Science and propose a novel algorithm for the pretreatment and recovery wavelengths through degenerate four-wave mixing in Engineering, Huazhong Univ. of Science and Technology, of Raman signals from fluorescence contaminated spectra. the silicon nitride platform. This device is promising for China; 3Dept. of Electrical and Electronic Engineering, Univ. This algorithm combines the 2nd derivative and iterative extending classical/quantum nanophotonic applications to of Melbourne, Australia. Silicon nanoantennas are used smoothening routines for optimized baseline estimation new spectral bands. to trap individual streptavidin-coated CdSe/ZnS quantum and correction dots (QDs) with minimal thermal effects. Using fluorescence microscopy, we track the position and light emission from optically-trapped QDs as a function of time.

FM3A.3 • 11:15 FM3B.3 • 11:15 FM3C.3 • 11:15 Fully-Differential, Hybrid, Multi-channel 4x25Gbps Direct Lasing with Propagation Invariant Shaped Beams, Nir . Iterative tomographic deconvolution phase microscopy, Direction Receiver in 0.25µm BiCMOS SiGe Technology, Davidson1, Ronen Chriki1, Slava Smartsev1, Gilad Barach1, Yijun Bao1, Thomas K. Gaylord1; 1Georgia Inst. of Technology, Sergiy Gudyriev1, J. Christoph Scheytt1, Christian Kress1, Lei Chene Tradonsky1, Asher Friesem1; 1Weizmann Inst. of USA. The existing refractive index imaging method, tomo- Yan 2, Christian Meuer2, Lars Zimmermann3; 1Heinz Nixdorf Science, Israel. Propagation invariant shaped beams are graphic deconvolution phase microscopy, is improved by Inst., Germany; 2Sicoya Gmbh, Germany; 3IHP Microelec- generated in a modified degenerate cavity laser. Such a applying an iterative optimization algorithm. The required tronics, Germany. A hybrid multi-channel receiver featuring cavity allows direct access to both the x-space and k-space number of illumination angles is greatly reduced, while the fully-differential transimpedance input stages for 25Gbps components, thereby enabling control of the propagation accuracy remains high. data rate per channel is presented along with measurement properties of shaped beams. results. OMA of -16dBm at a BER of 10-4 is estimated at the photodiode for all channels.

FM3A.4 • 11:30 FM3B.4 • 11:30 FM3C.4 • 11:30 On-chip large dispersion using cladding-modulated Bragg Determining Topological Charge of an LG beam using a Spatiotemporal Holography Using Flutter Shutter Cam- gratings, Ezgi Sahin1,2, Kelvin J. Ooi1, Ching Eng Png2, Dawn wedged optical flat, Behzad Khajavi1,2, Enrique J. Galvez2; era, Muralidhar Madabhushi Balaji1, Prasanna Rangarajan1, T. H. Tan1; 1Photonics Devices and Systems Group, Engineer- 1Physics and Astronomy, Florida Atlantic Univ., USA; 2Physics Indranil Sinharoy1, Duncan MacFarlane1, Marc Christensen1; ing Product Development, Singapore Univ. of Technology and Astronomy, Colgate Univ., USA. We present a method to 1Southern Methodist Univ., USA. A spatiotemporal approach and Design, Singapore; 2Dept. of Electronics and Photonics, determine the magnitude and sign of the topological charge for recovering holograms is proposed in this paper. Flut- Inst. of High Performance Computing, A*Star , Singapore. of an optical beam carrying orbital angular momentum using ter-shutter camera is used for temporal demodulation. The A cladding-modulated Bragg grating is realized for creating a wedged optical flat and two confocal lenses. proposed method needs lesser measurements than phase ultra-large dispersion. Normal dispersion as large as -11.5 shifting interferometry to extract the hologram. ps/nm is demonstrated on a silicon chip. Devices possess absolute group delay dispersion × bandwidth product up to 218 ps.

30 FiO + LS 2017 • 17–21 September 2017 Georgetown East Jefferson West Jefferson East

FiO LS

10:30–12:30 10:30–12:30 10:30–12:30 FM3D • Nanophotonics I FM3E • Quantum Memories and Interfaces LM3F • Carl E. Anderson Dissertation Presider: Shu-Wei Huang; University of Presider: Mark Beck; Whitman College, USA Award in Laser Science California, Los Angeles, USA Presider: Kristan Corwin; Kansas State University, USA

FM3D.1 • 10:30 FM3E.1 • 10:30 Invited LM3F.1 • 10:30 Invited Highly sensitive biomolecular detection using compact Multidimensional Tomography of Photon-pair Sources Control of Light-matter Interaction Using Photonic Hy- 1 high-Q silicon spiral resonators, Ahmad Usman , Razi Using Stimulated Emission, Virginia O. Lorenz1; 1Physics, percrystals, Tal Galfsky1,2, Zheng Sun1,2, Jie Gu1,2, Nicholas 1 1 1 1 Dehghannasiri , Ali Eftekhar , Ali Adibi ; Georgia Inst. of Univ. of Illinois at Urbana-Champaign, USA. The efficient Proscia1,2, Evgenii E. Narimanov3, Vinod M. Menon1,2; 1City Technology, USA. We present highly sensitive and compact characterization of photonic quantum sources enables Univ. of New York, USA; 2Physics, CUNY Graduate Center, label-free biosensors employing spiral resonators on SOI 3 precise source engineering for quantum information ap- USA; Electrical and Computer Engineering, Purdue Univ., Monday, 18 Septem with high-Q TM modes providing high-sensitivity and large plications. I present our demonstrations of the stimulated USA. We demonstrate broadband enhancement of light sensing area. The sensor performance is characterized using emission tomography technique to efficiently characterize emission from quantum dots, single photon emitters and avidin-biotin surface chemistries. sources in multiple degrees of freedom. 2D semiconductors using photonic hypercrystals (PHC). Both out-coupling and spontaneous emission rate are increased from the different emitters.

FM3D.2 • 10:45 Dual-band focusing metasurfaces based on stacked graphene ribbons, Wei Ma1, Zhong Huang1,2, Xiaokang 1 2 1 1

Bai , Peng Zhan , Yongmin Liu ; Northeastern Univ., USA; ber 2Nanjing Univ., China. We theoretically demonstrated focusing reflective metasurfaces based on stacked graphene ribbons. The dual-band performance originates from the weak inter-layer coupling, where the focusing effect can be independently tuned for two target wavelengths

FM3D.3 • 11:00 FM3E.2 • 11:00 LM3F.2 • 11:00 Invited Electrically controlled reconfigurable metadevice em- A Noiseless Quantum Optical Memory at Room Tem- Quantum Limits on Measurement and Control of a Me- 1 1 1 ploying nanostructured vanadium dioxide, Zhihua Zhu , perature, Krzysztof T. Kaczmarek , Patrick M. Ledingham , chanical Oscillator, Vivishek Sudhir1; 1Ecole Polytechnique 2 1 1 1 1 1,5 Phil Evans , Richard Haglund , Jason Valentine ; Vanderbilt Benjamin Brecht , Sarah E. Thomas , Guillaume S. Thek- Federale De Lausanne, Switzerland. The motion of a macro- 2 3 1 1,5 Univ., USA; Oak Ridge National Lab, USA. We demonstrate kadath , Oscar Lazo-Arjona , Joseph H. Munns , Eilon scopic mechanical oscillator – a glass nanostring – has been a near infrared metadevice modulator using VO nanostruc- Poem4, Amir Feizpour1, Dylan J. Saunders1, Joshua Nunn2, 2 measured, using a cavity-enhanced optical interferometer, 1 1 2 tures. This device shows a modulation depth up to 33%, Ian A. Walmsley ; Univ. of Oxford, UK; Univ. of Bath, UK; with a sensitivity that is 40 dB below that at the standard 3 4 wavelength shift of 360 nm, and 1.27 ms recovery time Univ. of Ottawa, Canada; Weizmann Inst. of Science, Israel; quantum limit, forming the most precise measurement of the when VO undergoes semiconductor-to-metal phase change. 5Imperial College London, UK. We demonstrate a noise-free, 2 zero-point motion of a mechanical oscillator yet. room-temperature quantum memory for broadband light. We store heralded single photons with a bandwidth of 1GHz and retrieve them with a heralded g2(0)=0.028(9), which is the lowest value measured so far.

FM3D.4 • 11:15 FM3E.3 • 11:15 Negative index in a dispersive chiral material with first-or- Demonstration of Real-Time Quantum Non-Demolition der sideband dispersion under dielectric losses, Monish R. Interaction, Yu Shiozawa1, Shota Yokoyama2, Toshiyuki Kaji1, Chatterjee1, Salah G. Bugoffa1; 1Univ. of Dayton, USA. Recent Ryosuke Nakamura1, Warit Asavanant1, Kenzo Makino1, Taka- work on conductively lossy dispersive chiral materials showed hiro Serikawa1, Shigenari Suzuki1, Jun-ichi Yoshikawa1,3, Akira NIM behavior and spiral spatial polarization. We introduce Furusawa1; 1The Univ. of Tokyo, Japan; 2Univ. of New South dielectric losses to explore NIM characteristics to determine Wales, Australia; 3Quantum-Phase Electronics Center, The negative index sidebands under realistic dielectric losses. Univ. of Tokyo, Japan. We experimentally demonstrate real-time quantum non-demolition (QND) interaction between optical quantum states in terms of satisfying the criteria for QND measurement and generating quantum entanglement.

FM3D.5 • 11:30 FM3E.4 • 11:30 LM3F.3 • 11:30 Invited Nanophotonic Devices for Three-Dimensional Control of Temporal and Spectral Manipulations of Correlated Nanophotonic Spin-photon Quantum Transistor, Shuo 1 2 1,2 Optical Beams, Stephen M. Kuebler , Rashi Sharma , Jenne- Photons using a Time-Lens, Sunil Mittal , Venkata Vikram Sun1, Hyochul Kim1; 1Inst. for Research in Electronics and 1 3 3 1,2 1 3 fir L. Digaum , Noel Martinez , Cesar L. Valle , Raymond C. Orre , Alessandro Restelli , Reza Salem , Elizabeth A. Applied Physics, Univ. of Maryland, College Park, USA. We 3 1 2 4,1 1,2 1 Rumpf ; CREOL, Univ. of Central Florida, USA; Chemistry, Goldschmidt , Mohammad Hafezi ; Joint Quantum demonstrate an optical transistor operating at the most 3 2 Univ. of Central Florida, USA; EM Lab, College of Engineer- Inst., Univ. of Maryland at College Park, USA; Dept. of fundamental quantum limit, where a single spin controls ing, Univ. of Texas-El Paso, USA. Spatially-variant photonic Electrical and Computer Engineering and IREAP, Univ. of the polarization of a single photon, and reversibly a single 3 4 crystals (SVPCs) are new nanophotonic devices that control Maryland, College Park, USA; PicoLuz, LLC, USA; U. S. photon flips the orientation of the spin. the propagation of optical beams in three dimensions. This Army Research Lab, USA. We use a time-lens to magnify work reports the fabrication and characterization of the first the two-photon wavefunction associated with time-bin en- SVPC that operate at 1550 nm. tangled photons and measure their joint-temporal intensity with a resolution far exceeding the limitations imposed by detector timing jitter.

FiO + LS 2017 • 17–21 September 2017 31 International Ballroom West International Ballroom East Georgetown West

FiO

FM3A • Silicon Photonics I—Continued FM3B • Trapping and Advanced Beam FM3C • Computational/Transformation Shaping—Continued Optics and Optics in Computing— Continued

FM3A.5 • 11:45 FM3B.5 • 11:45 FM3C.5 • 11:45 Nanosecond polarization modulation in phase transition The dating game at dimension zero: creation and anni- Frequency Modulated Continuous Wave Compressive material thin films, Alain Hache1, Jean-Francois Bisson1, Tran hilation of phase singularities in optical random waves, Depth Mapping, Daniel Lum1, John Howell1; 1Univ. of Vinh Son1, Truong Vo-Van2; 1Universite de Moncton, Canada; Lorenzo De Angelis1,2, Filippo Alpeggiani1,2, Andrea Di Rochester, USA. We present an achitecture for converting 2Physics, Concordia Univ., Canada. Thin layers (50-150 nm) Falco3, Kobus Kuipers1,2; 1Kavli Inst. of Nanoscience, Delft a frequency modulated continuous wave LiDAR into a of vanadium dioxide are shown to modulate polarization of Univ. of Technology, Netherlands; 2Center for Nanopho- compressing sensing depth mapping device. Our protocol incident light when a phase transition is induced by laser tonics, AMOLF, Netherlands; 3SUPA, School of Physics and requires only two compressed sensing image reconstructions pulses. High modulation amplitudes through polarizers are Astronomy, Univ. of St Andrews, UK. Phase singularities can to extract depth maps. obtained at nanosecond time scales. be created and annihilated, but always in pairs. With optical near-field measurements, we track singularities in random ber waves as a function of wavelength, and discover correlations between creation and annihilation events.

FM3A.6 • 12:00 Invited FM3B.6 • 12:00 FM3C.6 • 12:00 1 How Monolithic Photonic Integration Can Help to Over- Spatiotemporal Optical Vortices, Nihal Jhajj , George Deep Learning, Dynamic Sampling and Smart Energy-dis- 1 1 1 1 1 2 come Frontiers in Optics., Sven Otte1; 1Sicoya GmBH, Ger- Hine , Ilia Larkin , Eric Rosenthal , Sina Zahedpour , Jared persive Spectroscopy, Yan Zhang , Dilshan Godaliyadda , 2 1 1 1 3 2 many. The era of exponential data growth just started which Wahlstrand , Howard Milchberg ; Univ. of Maryland at Nicola Ferrier , Emine Gulsoy , Charles Bouman , Charudatta 2 1 1 2 generates technical and business requirements for optical College Park, USA; NIST, USA. Nonlinearly propagating Phatak ; Argonne National Lab, USA; Purdue Univ., USA; 3 component vendors. Here we are presenting monolithically beams undergoing optical collapse are shown to universally Northwestern Univ., USA. A convolutional neural network Monday, 18 Septem Monday, integrated Silicon Photonic engines that help to overcome self-generate a new type of optical vortex: the spatiotem- (CNN) classifier is trained using simulated energy-dispersive these frontiers. poral optical vortex (STOV). Beams with STOVs have orbital spectroscopy data. The CNN incorporated within a dynamic angular momentum transverse to propagation. sampling method is to reduce radiation exposure and data acquisition time for elemental mapping.

FM3B.7 • 12:15 FM3C.7 • 12:15 Photonic topologically protected bulk propagation, Monte Carlo Simulation of Coherence Propagation Eran Lustig1, Steffen Weimann2, Yonatan Plotnik1, Miguel through Scattering Media, Zhean Shen1, Sergey Sukhov1, Bandres1, Yaakov Lumer3, Alexander Szameit2, Mordechai Aristide Dogariu1; 1CREOL, USA. Traditional Monte Carlo Segev1; 1Technion, Israel; 2Univ. of Rostock, Germany; 3Univ. (MC) technique of photon transport in random medium of Pennsylvania, USA. We present photonic topological insu- is able to describe only single point properties. Here we lators displaying topologically protected bulk propagation, propose the method of extending MC to simulate two-point robust to large-scale defects. These topological insulators property, spatial coherence. are described in synthetic dimensions and open the door for shaping topological propagation.

12:30–13:30 Lunch Break (on your own)

12:30–13:30 Challenges and Emerging Opportunities in Molecular Probes and Nanobio-Optics, Georgetown East, Concourse Level

12:30–14:00 Grant Writing 101 Workshop, Fairchild Room, Terrace Level

Join the conversation. Follow @Opticalsociety on Twitter. Use hashtag #FIO17

32 FiO + LS 2017 • 17–21 September 2017 Georgetown East Jefferson West Jefferson East

FiO LS

FM3D • Nanophotonics I—Continued FM3E • Quantum Memories and LM3F • Carl E. Anderson Dissertation Interfaces—Continued Award in Laser Science—Continued

FM3D.6 • 11:45 FM3E.5 • 11:45 Broadband graphene oxide anti-reflection coating on Scalable Ion-Photon Quantum Interface based on In- silicon nanostructures, Yunyi Yang1, Han Lin1, Baohua tegrated Diffractive Mirrors, Steven Connell1, Mojtaba Jia1, Yinan Zhang2, Minghui Hong3; 1Swinburne Univ. of Ghadimi1, Valdis Blums1, Benjamin G. Norton1, Paul Fisher1, Technology, Australia; 2Jinan Univ., China; 3National Univ. Jason M. Amini2, Curtis Volin2, CS Pai2, Dave Kielpinski1, of Singapore, Singapore. We show the ultra-thin graphene Mirko Lobino1,3, Erik W. Streed1,4; 1Griffith Univ., Australia; oxide films are conformably coated on silicon nanowires 2Georgia Tech Research Inst., USA; 3Queensland Micro and through a layer-by-layer method. The coating can achieve Nanotechnology Centre, Griffith Univ., Australia; 4Inst. for up to 20% reduction in the overall reflection with a broad- Glycomics, Griffith Univ., Australia. We demonstrate the Monday, 18 Septem band wavelength. viability of diffractive mirrors monolithically integrated with a microfabricated ion trap for quantum networking and an ion-fibre coupling of 4.1(6)% giving an 8.6x increase in entanglement rates from previous state-of-the-art.

FM3D.7 • 12:00 FM3E.6 • 12:00 Invited LM3F.4 • 12:00 Invited Imaging of acoustic pressure field in opto-mechano-flu- Ion-photon Interfaces for Quantum Networks, Tracy First Demonstration of Sub-Wavelength Imaging at Short idic resonators with a single particle probe, Jeewon Northup1; 1Univ. of Innsbruck, Austria. I will discuss the Wavelengths, Dennis F. Gardner1, Elisabeth R. Shanblatt1, 1 1 1 1 Suh , Kewen Han , Gaurav Bahl ; Mechanical Science and cavity-mediated transfer of quantum information between Michael Tanksalvala1, Xiaoshi Zhang2, Benjamin R. Galloway1, Engineering, Univ. of Illinois at Urbana-Champai, USA. We ions and photons, with the goal of linking distant qubits in Christina L. Porter1, Robert Karl1, Charles Bevis1, Bosheng ber present a technique for mapping the acoustic pressure a quantum network, focusing on multi-ion encodings and Zhang1, Matthew H. Seaberg1, Giulia F. Mancini1, Daniel E. fields within microfluidic optomechanical resonators using adiabatic passage along channels. Adams1, Henry C. Kapteyn1,2, Margaret M. Murnane1,2; 1Univ. a single particle probe. These mappings help improve the of Colorado Boulder, USA; 2KM Labs, USA. Combining table- detection capabilities of high-throughput opto-mecha- top 13.5nm HHG EUV with novel ptychography algorithms, no-fluidic sensors. we demonstrate diffraction-limit high-NA and subwavelength resolution imaging at EUV wavelengths for the first time, a FM3D.8 • 12:15 record resolution for full-field light-based microscopy. Dielectric veins type photonic crystal as a zero-index-metamaterial, Nishant Shankhwar1, Yogita Kalra1, Ravin- dra K. Sinha2; 1Delhi Technological Univ., India; 2 CSIR-Central Scientific Instruments Organisation (CSIO), India. In this paper we present a dielectric veins type two dimensional photonic crystal which acts as a zero-index-material. The underlying principles is the existence of a Dirac cone at the center of the Brillouin zone

12:30–13:30 Lunch Break (on your own)

12:30–13:30 Challenges and Emerging Opportunities in Molecular Probes and Nanobio-Optics, Georgetown East, Concourse Level

12:30–14:00 Grant Writing 101 Workshop, Fairchild Room, Terrace Level

FiO + LS 2017 • 17–21 September 2017 33 International Ballroom West International Ballroom East Georgetown West

FiO

13:30–15:30 13:30–15:30 13:30–15:30 FM4A • Plamonics and Metamaterials FM4B • Studies with Complex Media, FM4C • General Information Acquisition, Presider: Hanjo Rhee; Sicoya, Germany Imaging and Light Processing and Display Presider: Frederique Vanholsbeeck; Presider: Wei Lee; Taiwan University, Taiwan University of Auckland, New Zealand

FM4A.1 • 13:30 Invited FM4B.1 • 13:30 Invited FM4C.1 • 13:30 Invited All-dielectric Nanophotonics and Metasurfaces Govern 3D Computational Microscopy in Scattering Media, Laura Non-contact Scanning Diffuse Correlation Tomography by Mie Resonances, Yuri S. Kivshar1; 1Nonlinear Physics Waller1; 1Univ. of California Berkeley, USA. We describe new for Blood Flow Monitoring During Bone Healing, Regine Center, RSPE, The Australian National Univ., Australia. We computational methods for 3D microscopy in scattering me- Choe1; 1Univ. of Rochester, USA. Vascularization is a key step demonstrate that Mie resonances can play a crucial role in dia: single-shot 3D fluorescence imaging and detection-side in bone healing, but is seldom measured due to technical all-dielectric meta-optics enhancing many optical effects aperture coding of angle (Fourier) space for capturing 4D difficulties. We demonstrate the capabilities of diffuse cor- near magnetic dipole resonances and driving new physical phase-space (e.g. light field) datasets. relation tomography to monitor spatiotemporal blood flow ber effects due to electric and magnetic multipolar interference. changes associated with bone healing. Monday, 18 Septem Monday,

FM4A.2 • 14:00 FM4B.2 • 14:00 FM4C.2 • 14:00 Brewster Plasmons: The Antiresonant Plasmonic Degrees Noise reduction in Brillouin microscopy via spectral Single Chip LIDAR with Discrete Beam Steering by Digital of Freedom, Gilad Rosenblatt1, Boris Simkhovich2, Guy coronagraphy, Eitan Edrei1, Malte C. Gather2, Giuliano Micromirror Device, Braden Smith1, Brandon Hellman1, Bartal1,2, Meir Orenstein1; 1Dept. of Electrical Engineering, Scarcelli1; 1Bioengineering, Univ. of Maryland, USA; 2Univ. Adley Gin1, Alonzo Espinoza1, Yuzuru Takashima1; 1The Univ. Technion - Israel Inst. of Technology, Israel; 2The Russell of St Andrews, UK. We have adapted the design of coro- of Arizona, USA. MEMS-based beam steering by Digital Berrie Nanotechnology Inst., Technion - Israel Inst. of Tech- nagraphs used for exosolar planet imaging to the spectral Micromirror Device illuminated by pulsed laser enables nology, Israel. We experimentally and theoretically prove the domain for high extinction Brillouin spectroscopy. Our design single-chip LIDAR. We demonstrate 48° field of view, 3.4k existence of a new class of plasmonic modes, distinct from enables spectral mapping near reflecting interfaces and points/sec scan rate, and <1cm accuracy for 1.2 m distance surface plasmons, we call Brewster plasmons. We measure within scattering samples. across five steering angles. dispersion and demonstrate far-field coupling to both surface and Brewster plasmons.

FM4A.3 • 14:15 FM4B.3 • 14:15 FM4C.3 • 14:15 Dual-width Plasmonic Nanogap Gratings electrodes Imaging a Mask Object Embedded in Thick Tissue Using Polarization Splitter Design with Quasi-Conformal Trans- for GaAs Metal-Semiconductor-Metal Photodetectors Speckle Intensity Correlations Over Object Position, formation Optics, Poliane A. Teixeira1, Daniely Silva1, Lucas Enhancement, Ahmad A. Darweesh1, Stephen Bauman1, Qiaoen Luo1, Kevin J. Webb1; 1Purdue Univ., USA. Spatial Gabrielli2, Mateus Junqueira1, Danilo Spadoti1; 1Federal zach Brawley1, Joseph Herzog1; 1Univ. of Arkansas, USA. A speckle intensity correlation measurements in relation to Univ. of Itajubá, Brazil; 2School of Electrical and Computer dual-width plasmonic nanograting structure with a 5 nm gap object position are used to image a moving mask embedded Engineering, Univ. of Campinas, Brazil. TO is used to develop has been designed and simulated. Optical enhancement was between tissue-mimicking phantoms, demonstrating the 2D polarization beam splitter. A quasi-conformal mapping is calculated for the application of improving the performance practicality of this approach for imaging in heavy scatter. applied, resulting in a medium with inhomogeneous uniaxial of metal-semiconductor-metal photodetectors. (MSM-PDs) permittivity and without magnetic response. This splitter is broadband and has modal preservation.

FM4A.4 • 14:30 FM4B.4 • 14:30 FM4C.4 • 14:30 Invited Full-color imaging with PSF-engineered metasurfaces and Non-Hermitian invisibility based on constant-intensity High Resolution Imaging with a Moving Coded Aperture, 1 1 2 computational reconstruction, Shane A. Colburn , Alan waves, Andre Brandstotter , Konstantinos Makris , Stefan Abhijit Mahalanobis1; 1Lockheed Martin Corporation, USA. 1 1 1 1 1 Zhan , Arka Majumdar ; Univ. of Washington, USA. We build Rotter ; Inst. for Theoretical Physics, Vienna Univ. of Tech- It is well known that a translating mask can optically encode 2 a full-color imaging system comprising a single metasurface nology, Austria; Physics Dept., Univ. of Crete, Greece. We low resolution measurements from which higher resolution by designing a wavelength-invariant point spread function demonstrate the possibility of scattering media that are images can be computationally reconstructed. across the whole visible band combined with post-capture unidirectional invisible and are not necessarily parity-time deconvolution with a single linear filter. symmetric. The required gain-loss distribution is related to the phase of the corresponding constant-intensity scattering state.

34 FiO + LS 2017 • 17–21 September 2017 Georgetown East Jefferson West Jefferson East

FiO LS

13:30–15:30 13:30–15:30 13:30–15:30 FM4D • Biomedical Optics in Scattering FM4E • High-Dimension Quantum Systems LM4F • X-Ray Science with Table Top and Media and Simulation XFEL Lasers Presider: David Busch; Children’s Hospital of Presider: Valerian Thiel; University of Oxford, Presider: Kyung-Han Hong; Massachusetts Philadelphia, USA UK Institute of Technology, USA

FM4D.1 • 13:30 FM4E.1 • 13:30 Invited LM4F.1 • 13:30 Invited Evaluation of Out-of-Plane Sensitivity and Artifacts in Quantum State Engineering on Chip, Amr S. Helmy1; 1ECE, Chemical and Bio-chemical X-ray Spectroscopy at Current 1 1 Photoacoustic Imaging, William C. Vogt , Congxian Jia , Univ. of Toronto, Canada. Dispersion in integrated optics and Future X-ray Lasers, Philippe Wernet1; 1Helmholtz-Ze- 1 1 1 1 Keith A. Wear , Brian S. Garra , T. Joshua Pfefer ; US Food enable quantum devices with versatile attributes. Dispersion ntrum Berlin, Germany. It is demonstrated how x-ray laser and Drug Administration, USA. Photoacoustic Imaging (PAI) unlocks novel capabilities including in-situ control over spectroscopy with femtosecond x-ray pulses offers unique systems are rapidly emerging biomedical diagnostic devices. spectral/polarization entanglement, tunable time-ordering, insight into photochemical dynamics and bio-chemical Monday, 18 Septem We investigated PAI out-of-plane artifacts using biorealistic and entanglement-sensitive coincidence. processes with the ability to probe the valence electronic tissue phantoms, which can support device optimization, structure at atomic length and time scales. clinical translation, and inter-comparison.

FM4D.2 • 13:45 Localization of Arteries Using Diffuse Light for Assisting Surgery, Brian Bentz1, Timothy Wu2, Vaibhav Gaind3, Kevin J. Webb1; 1Purdue Univ., USA; 2 Private Practice in Periodontol- ogy, USA; 3KLA-Tencor, USA. We present an approach for the localization of arteries in the roof of the mouth that has the potential to reduce complications during oral surgery. The ber method is demonstrated using a printed tissue-simulating mouth phantom.

FM4D.3 • 14:00 FM4E.2 • 14:00 LM4F.2 • 14:00 Intraoperative Monitoring of Spinal Cord Blood Flow, Finding excited states of physical Hamiltonians on a silicon Carrier- and Element-Specific Femtosecond XUV Transient David R. Busch1, Wei Lin2, Alisa Cutrone3, Brandon J. Ko- quantum photonic device, Raffaele Santagati1, Jianwei Absorption of Hybrid Lead Halide Perovskites, Ming-Fu varovic2, Jakub Tatka4, Arjun G. Yodh1, James Barsi4, Thomas Wang1, Antonio Gentile1, Stefano Paesani1, Nathan Wiebe2, Lin1, Max Verkamp1, Joshua Leveillee2, Elizabeth Ryland1, F. Floyd3,2; 1Physics and Astronomy, Univ. of Pennsylvania, Jarrod McClean3, Damien Bonneau1, Joshua Silverstone1, Kristin Benke1, Kaili Zhang1, Andre Schleife2, Josh Vura-Weis1; USA; 2Biomedical Engineering, Stony Brook Univ., USA; Sam Morley-Short1, Peter Shadbolt1, David Tew4, Xiao-Qi 1Dept. of Chemistry, UIUC, USA; 2Dept. of Materials Science 3Anesthesiology, Stony Brook Univ., USA; 4Orthopedics, Zou5, Jeremy O’Brien1, Mark Thompson1; 1Quantum Engi- and Engineering, Univ. of Illinois at Urbana-Champaign, Stony Brook Univ., USA. Spinal cord ischemia is commonly neering Technology Labs, Univ. of Bristol, UK; 2Quantum USA. XUV transient absorption spectroscopy is used to associated with both trauma and surgery. We demonstrate Architectures and Computation Group, Microsoft Research, measure carrier dynamics in hybrid lead halide perovskites. a catheter-based optical tool to continuously monitor USA; 3Computational Research Division, Lawrence Berkeley Distinct signals are observed for photoinduced electrons and spinal cord blood flow intraoperatively in a ovine model National Lab,, USA; 4School of Chemistry, Univ. of Bristol, UK; holes, allowing the dynamics of each carrier to be tracked of spinal surgery. 5State Key Lab of Optoelectronic Materials and Technologies independently. and School of Physics, Sun Yat-sen Univ., China. We introduce the concept of eigenstate-witness to implement a new protocol for finding excited-states of physical Hamiltonians. We experimentally demonstrate it on a silicon quantum photonic device embedding arbitrary controlled unitary operations.

FM4D.4 • 14:15 Invited FM4E.3 • 14:15 LM4F.3 • 14:15 Functional NIRS for attention monitoring, Angela Harriv- Boltzmann sampling for an XY model using a non-de- High Harmonic Generation in Acetone for Time-Resolved 1 el1; 1Crew Systems and Aviation Operations Branch, NASA generate optical parametric oscillator network, Yutaka Spectroscopy Applications, Phillip D. Keathley , Guillaume 1,2 2 3,4 1,2 1 1 1,3 Langley Research Center, USA. We applied functional Near Takeda , Shuhei Tamate , Yoshihisa Yamamoto , Hiroki Laurent , Sergio Carbajo , Jeffrey Moses , Franz Kaertner ; 5 5 1,2 1 1 2 Infrared Spectroscopy and adaptive noise filtering to quantify Takesue , Takahiro Inagaki , Shoko Utsunomiya ; Dept. of Massachussetts Inst. of Technology, USA; Physics, Au- 3 brain activity in attentional networks. We then employed pat- Physics, Faculty of Science, Tokyo Univ. of Science, Japan; burn, USA; Center for Free Electron Laser Science, DESY, 2 3 tern classification toward real-time monitoring of attentional National Inst. of Informatics, Japan; ImPACT Program, Germany. High harmonic generation in acetone was used 4 performance during operational tasks. Japan Science and Technology Agency, Japan; E. L. to generate EUV harmonics spanning 10-30 eV. A flux of Ginzton Lab, Stanford Univ., USA; 5NTT Basic Research 1.5x106 ph/pulse/harmonic was measured near 17 eV, and Labs, NTT Corporation, Japan. We built a non-degenerate polarization gating was used to generate an isolated 2.6 fs optical parametric oscillator (NOPO) network to simulate pulse spanning 16-18 eV. a one-dimensional XY model in thermal equilibrium. We experimentally found that the effective temperature can be controlled via an external noise injection.

FM4E.4 • 14:30 Invited LM4F.4 • 14:30 Invited Exploring Many-Body Dynamics on a Programmable 50 Ultrafast X-ray Studies of Chemical and Interfacial Dynam- Atom Quantum Simulator, Mikhail Lukin1; 1Harvard Univ., ics, Oliver Gessner1; 1Lawrence Berkeley National Lab, USA. USA. We will describe recent experiments aimed at exploring Ring-opening dynamics in heterocyclic aromatic molecules dynamics of strongly interacting many-body systems on a and charge-transfer dynamics at molecule-semiconductor programmable quantum simulator. interfaces are studied by femtosecond and picosecond time-resolved inner-shell spectroscopy techniques.

FiO + LS 2017 • 17–21 September 2017 35 International Ballroom West International Ballroom East Georgetown West

FiO

FM4A • Plamonics and Metamaterials— FM4B • Studies with Complex Media, FM4C • General Information Acquisition, Continued Imaging and Light—Continued Processing and Display—Continued

FM4A.5 • 14:45 FM4B.5 • 14:45 Optimization of Nonlinear Optical Processes in Arrays of Universality of Stochastic Interactions Between Laser Metallic Nanocavities, Yael Blechman1, Euclides Almeida1, Beams, Amir Sagiv1, Adi Ditkowski1, Gadi Fibich1; 1Tel Aviv Basudeb Sain1, Yehiam Prior1; 1Dept. of Chemical Physics, Univ., Israel. We show that laser beams lose their initial Weizmann Insitute of Science, Israel. We challenge the phase in nonlinear propagation. Therefore, prediction and conventional wisdom that enhancement of nonlinear optical control of long-range interactions between beams become processes in plasmonic nanomaterials can be fully predicted impossible. The statistics of these chaotic interactions, are by their linear properties. universal and computable.

FM4A.6 • 15:00 FM4B.6 • 15:00 FM4C.5 • 15:00 Wave-guiding and Cavity Engineering in Core-shell Elegant Laguerre-Gaussian beams as structured wave- Lensless Object Detection and Positioning via Coher- 1 1 2 ber Nanowires with Two Dimensional Electron Gas Plasmons, fields: light on self-healing, Alfonso I. Jaimes-Nájera , Jorge ence Measurement, Hasan E. Kondakci , Andre Beckus , Kiana Montazeri1, Zhihuan Wang1, Bahram Nabet1; 1Drexel A. Ugalde-Ontiveros1, Songjie Luo2, Jixiong Pu2, Sabino Ahmed El-Halawany1, Nafiseh Mohammadian1, George Univ., USA. Effect of confined electron gas plasmons on Chávez-Cerda1; 1INAOE, Mexico; 2College of Information Atia2, Ayman Abouraddy1; 1CREOL, Univ. of Central Florida, waveguiding and optical resonance properties of core- Science and Engineering, Huaqiao Univ., China. We demon- USA; 2Electrical and Computer Engineering, Univ. of Central shell nanowires are analyzed, showing how the cavity can strate that elegant Laguerre-Gaussian beams belong to the Florida, USA. We measure the complex-coherence function be engineered for specific resonance wavelengths such as families of structured wavefields. As such, they also have the of incoherent light scattered by a one-dimensional object 830 or 1550 nm. self-healing property that is explained on physical grounds in various configurations and determine the axial and trans- as traveling waves that superposed conform these beams. verse position of the object and its size by examining only the coherence function.

FM4A.7 • 15:15 FM4B.7 • 15:15 FM4C.6 • 15:15 Monday, 18 Septem Monday, Periodic Black Phosphorene Nanoribbons Infrared Edge Wigner Distribution Function of Airy Beam, Fengfei Wang1, Scene Reconstruction via Two-dimensional Complex Plasmon Enhanced Absorbance, Desalegn T. Debu1, David Singh1, Ping Yu1, Guohai Situ2; 1Univ. of Missouri, USA; Coherency Imaging, Ahmed Elhalawany1, Andre Beckus1, Stephen J. Bauman1, Joseph B. Herzog1; 1Univ. of Arkan- 2Shanghai Inst. of Optics and Fine Mechanics, China. We Hasan E. Kondakci1, Nafiseh Mohammadian1, George sas, USA. This work demonstrates enhanced infrared light studied Wigner distribution function for finite-energy Airy Atia1, Ayman Abouraddy1; 1Univ. of Central Florida, USA. absorption due to edge confined strong plasmon enhance- beam in theory and experiment, and proposed that with The location of 1D objects is determined by numerically ment in anisotropic black phosphorene nanoribbons. The a large truncating factor, Airy beam can be simplified for backpropagating the experimentally measured spatial absorption spectra peak position of nanoribbon is tunable optical imaging based on phase-space method. coherence function. Partial coherent light and dynamical in a wide infrared wavelength range. double slits generated by digital light processor are used in coherence measurement.

15:30–16:00 Coffee Break, International Terrace, Terrace Level

16:00–17:30 Workshop: Understanding Unconscious Bias, Georgetown East, Concourse Level

16:00–17:30 OSA Nonlinear Optics Technical Group Workshop & Networking Session, Georgetown West, Concourse Level

16:00–18:00 Evening with the Agencies & Reception, Jefferson West, Concourse Level

18:30–21:00 FiO + LS Awards Banquet, International Ballroom Center, Terrace Level

36 FiO + LS 2017 • 17–21 September 2017 Georgetown East Jefferson West Jefferson East

FiO LS

FM4D • Biomedical Optics in Scattering FM4E • High-Dimension Quantum Systems LM4F • X-Ray Science with Table Top and Media—Continued and Simulation—Continued XFEL Lasers—Continued

FM4D.5 • 14:45 Invited Towards Standardization of Clinical Biophotonic Device Technologies, T. Joshua Pfefer1; 1FDA Ctr Devices & Radio- logical Health, USA. Standardized test methods are commonly used to facilitate development and clinical translation of medical imaging systems. Currently, efforts are underway in Biophotonics to establish consensus guidelines and develop objective, quantitative tests based on innovative phantoms.

FM4E.5 • 15:00 LM4F.5 • 15:00 Monday, 18 Septem Two-Photon Joint Spectral Wave Function Measurement Holographic generation of high-harmonic vortex beams, via Electro-Optic Spectral Shearing Interferometry, Alex Fanqi Kong1,2, Chumei Zhang1,2, Frédéric Bouchard1, Zheng- O. Davis1, Valérian Thiel1, Brian J. Smith1,2; 1Oxford Univ. yan Li1,2, Graham Brown1,2, Donghyuk Ko1,2, Thomas Ham- , UK; 2Univ. of Oregon, USA. We present a technique to mond1,2, Ladan Arissian2, Robert Boyd1,3, Ebrahim Karimi1, completely characterize the joint spectral-temporal wave Paul Corkum1,2; 1Univ. of Ottawa, Canada; 2National Research function of a photon pair at 830 nm center wavelength using Council of Canada , Canada; 3Univ. of Rochester, USA. We spectral-shearing interferometry. Our fully self-referencing introduce a holographic method to manipulate the wavefront method applies spectral shear using an EOM. structures of extreme ultraviolet (XUV) beams. Based on this concept, we generate optical vortices with controllable orbital angular momentum (OAM) on high-order harmonics. ber

FM4D.6 • 15:15 FM4E.6 • 15:15 LM4F.6 • 15:15 Polymer Metamaterial Fabrics for Personal Radiative Full mode reconstruction of optical twin beams via An Instrument for Time-Resolved Photoelectron Spec- Thermal Management, Seyed Hadi Zandavi1, Yi Huang1, photon-number-resolved measurement, Elizabeth Gold- troscopy at 87 MHz, Christopher Corder1, Peng Zhao1, George Ni1, Richard Pang2, Richard M. Osgood III2, Preet schmidt1,2, Ivan Burenkov2,3, Ankita Sharma3, Thomas Gerrits3, Xinlong Li1, Matthew D. Kershis1, Amanda R. Muraca1, Kamal3, Amit Jain3, Gang Chen1, Svetlana V. Boriskina1; 1MIT, Georg Harder4, Tim Bartley4, Christine Silberhorn4, Sergey Michael G. White1, Thomas K. Allison1; 1Stony Brook Univ., USA; 2US Army Natick Soldier Research, Development, and Polyakov3; 1US Army Research Lab, USA; 2Joint Quantum USA. We describe an instrument for high-repetition rate Engineering Center, USA; 3Shingora Textiles Limited, India. Inst., USA; 3National Inst. of Standards and Technology, time-resolved XUV photoelectron spectroscopy, based on We report on the design, fabrication and characterization of USA; 4Univ. of Paderborn, Germany. We present a method cavity-enhanced high-order harmonic generation. This sys- flexible polymer metamaterial fabrics that provide passive ra- to reconstruct the mode structure of multimode conjugated tem enables ultrafast surface photoemission studies without diative cooling or heating by utilizing optical resonant effects optical fields using an experimentally measured joint pho- space-charge constraints. in polymer microfibers with tailored sizes and composition. ton-number probability distribution and demonstrate a reconstruction of a bright parametric down-conversion source.

15:30–16:00 Coffee Break, International Terrace, Terrace Level

16:00–17:30 Workshop: Understanding Unconscious Bias, Georgetown East, Concourse Level

16:00–17:30 OSA Nonlinear Optics Technical Group Workshop & Networking Session, Georgetown West, Concourse Level

16:00–18:00 Evening with the Agencies & Reception, Jefferson West, Concourse Level

18:30–21:00 FiO + LS Awards Banquet, International Ballroom Center, Terrace Level

FiO + LS 2017 • 17–21 September 2017 37 07:00–17:30 Registration, Concourse Foyer

08:00–09:30 JTu1A • Joint Plenary Session, International Ballroom Center, Terrace Level

09:30–10:00 Exhibits and Coffee Break, Science & Industry Showcase, Columbia, Terrace Level

10:00–12:00 JTu2A • Science & Industry Showcase Exhibits, Poster Session & E-Posters Rapid-Fire Oral Presentations I in Theater Columbia, Terrace Level

Science Showcase Theater

JOINT FiO + LS

10:00–11:00 JTu2A • Rapid-Fire Oral Presentations I

JTu2A.11 • 10:00 RAPID JTu2A.68 • 10:20 RAPID JTu2A.84 • 10:35 RAPID Phosphor Screens for Laser Projection Systems, Taka- 2D Computational Modeling of Optical Trapping Mechanical properties of cellular nucleus characterized masa Kohmoto1, Masamichi Ohta1, Ichiro Fujieda1, Wataru Effects on Malaria-infected Red Blood Cells, Joana S. by Brillouin flow cytometry, Jitao Zhang1, Xuefei Nou1, Watanabe1; 1Ritsumeikan Univ., Japan. High-resolution Paiva1,2, Rita S. R. Ribeiro1,2, Pedro A. S. Jorge1,2, Carla C. Hanyoup Kim2, Giuliano Scarcelli1; 1Univ. of Maryland at images can be displayed on a phosphor screen by pro- Rosa1,2, A. Guerreiro1,2, Joao P. S. Cunha1,3; 1INESC TEC College Park, USA; 2Canon U.S. Life Sciences, Inc., USA. jecting laser light. The screen can be made transparent - INESC Technology and Science, Portugal; 2Astronomy We developed a label-free flow cytometry platform to and might be applicable for a head-up display and a and Physics Dept., Sciences Faculty of Univ. of Porto, characterize the nuclear mechanics based on Brillouin volumetric 3d display. Portugal; 3Dept. of Electrical and Computer Engineer- microscopy, which is an all-optical technique so that can

ber ing, Faculty of Engineering of Univ. of Porto, Portugal. measure the stiffness of the nucleus in a non-contact, JTu2A.12 • 10:05 RAPID A computational method for optical fiber trapping of non-invasive manner. Novel Hard Mask Fabrication Method for Hybrid healthy and Malaria-infected blood cells characterization Plasmonic Waveguide and Metasurfaces, Sajid Choud- is proposed. A trapping force relation with the infection JTu2A.91 • 10:40 RAPID hury1, Volodymyr Zenin2, Soham Saha1, Vladimir Shalaev1, stage was found, which could trigger the development Utilizing Machine Learning for Smart Starting Guesses Sergey I. Bozhevolnyi2, Alexandra Boltasseva1; 1Purdue of a diagnostic sensor. for Phase Retrieval, Scott Paine1, James Fienup1; 1Univ. Univ., USA; 2Univ. of Southern Denmark, Denmark. A of Rochester, USA. Traditional wavefront-sensing phase hybrid plasmonic waveguide fabrication technique has JTu2A.71 • 10:25 RAPID retrieval problems with large amounts of wavefront error been developed and waveguides have been demonstrat- Laser Induced Fluorescence in combination with often do not converge without a good starting point. We ed. The developed technique can create similar hybrid Multivariate analysis classifies anti-malarial herbal use machine learning in an attempt to produce better waveguide structures and metasurfaces with transition plants, Charles L. Amuah1; 1Univ. of Cape Coast, Ghana. starting guesses for these problems. Tuesday, 19 Septem Tuesday, metal nitrides and epitaxial silver. Laser-induced fluorescence in combination with multivariate analysis as a simple, rapid and non-destructive JTu2A.92 • 10:45 RAPID JTu2A.25 • 10:10 RAPID method for classifying anti-malarial herbal plants is Building Scalable Integrated Silicon Photonics Reser- 1 Switchable quarter wave plate using Ge2Sb2Te 5 meta- presented. A suitable alternative method that enhances voirs for Signal Processing, Andrew Katumba , Matthias surface, Chul Soo Choi1, Jeong-geun Yun1, Gun-yeal Lee1, safety and objectivity. Freiberger2, Jelle Heyvaert1, Joni Dambre2, Peter Bienst- Sun-je Kim1, Byoungho . Lee1; 1Seoul national Univ., South man1; 1Dept. of Information Technology, Gent Univ. - imec, RAPID 2 Korea. Ge2Sb2Te 5 (GST) is in the spotlight as an ingredient JTu2A.72 • 10:30 Belgium; Dept. of Electronics and Information Systems, of metasurface to achieve active feature. Here, we pro- Characterization and discrimination of basal cell carci- Gent Univ., Belgium. Photonic reservoir computing is a pose a novel method for active switching of polarization noma and normal human skin tissues using resonance novel bio-inspired paradigm for signal processing. We via the metasruface composed of GST nanorods. Raman spectroscopy, Cheng-hui Liu1, Binlin Wu3, Susie discuss how it can be scaled up by injecting multiple Boydston-White2, Hugh Beckman1, Vidyasagar Sriramo- copies of the input and by using multi-mode rather than JTu2A.60 • 10:15 RAPID ju1, Laura Sordillo1, Chunyuan Zhang1, Jason Smith3, single-mode components. Guided-Mode Resonance Biosensors: Quantifying the Lin Zhang1, Lingyan Shi4, Robert R. Alfano1; 1CUNY Binding of Neuropeptide Y to its Antibody, Kyu J. Lee1, City College, USA; 2CUNY, USA; 3Southern Connecticut JTu2A.105 • 10:50 RAPID Robert Magnusson1, Brett R. Wenner2, Jeffery Allen2, State Univ., USA; 4Columbia Univ., USA. Resonance Automatic calibration of Projector and DDHOE based Monica S. Allen2; 1Univ. of Texas at Arlington , USA; 2Air Raman spectroscopy is used for rapid detection of skin IP displays, Jackin Boaz Jessie1, Lode Jorissen2, Ryutaro Force Research Lab, USA. We apply the guided-mode BCC cancer. The cross-validated classification accuracy Oi1, Koki Wakunami1, Yasuyuki ichihashi1, Makoto Okui1, resonance sensor principle to record peptide binding is achieved to be as high as 98% using nonnegative Philippe Bekaert2, Kenji Yamamoto1; 1National Inst. dynamics. In particular, we conveniently and expeditiously matrix factorization along with support vector machine of Communications Tec, Japan; 2Expertise Center for quantify anti-NPY binding to NeutrAvidin and then NPY statistical method. Digital Media, Hasselt Univ.-tUL, Belgium. A calibration binding to anti-NPY. technique for integral photography(IP) based 3D display that uses a commercial projector and digitally designed holographic optical element (DDHOE), is reported. This method requires less number of input images for calibration.

38 FiO + LS 2017 • 17–21 September 2017 Science & Industry Showcase

JOINT FiO + LS

10:00–12:00 JTu2A • Joint Poster Session I

JTu2A.1 E-Poster JTu2A.8 E-Poster JTu2A.15 Angle-Resolved Measurement of Photoluminescence Computational ghost imaging under Gaussian distrib- Research of Solid-state Laser Based on Pre-polymerization PMMA Polymer Doped with Laser Dye, Spectra for Illumination and Display Applications, uted sparse speckles, Yong Yue1, Bin Luo2, Junhui Li3, Zhigang 1,2 1,2 1,2 1,2 Masamichi Ohta1, Ichiro Fujieda1; 1Ritsumeikan Univ., Dongyue Yang1, Guohua Wu1, Longfei Yin1, Hong Guo3; Zhou , Rongwei Fan , Zhaodong Chen , Xinrui Xu , 1,2 1,2 1 Japan. Photoluminescence spectra from a laser-driven 1School of Electronic Engineering, Beijing Univ. of Posts Tao Jia , Deying Chen ; Inst. of Optical-Electronics, 2 phosphor layer vary with the emission angle. This phe- and Telecommunications, China; 2State Key Lab of Infor- National Key Lab of Tunable Lasers, China; Harbin Inst. nomenon is attributed to uneven absorption of the laser mation Photonics and Optical Communications, Beijing of Technology, China. light and self-absorption of the emitted photons within Univ. of Posts and Telecommunications, China; 3School This article gave a brief research about solid-state dye the phosphor layer. of Electronics Engineering and Computer Science, Pe- laser based on PMMA polymer doped with different king Univ., China. Computational ghost imaging under laser dye through pre-polymerization method, and JTu2A.2 E-Poster Gaussian distribution sparse speckles (GSGI) with spatial showed good fluorescence and laser characteristics in Holographic Microscope Slide for Single Beam Off-Axis light modulator(SLM) is proposed and demonstrated. At a experimental research. Digital Holography Microscopy, Biagio Mandracchia1, price of more measurements, GSGI outperformances its Vittorio Bianco1, Melania Paturzo1, Pietro Ferraro1; 1Inst. counterpart under traditional random speckles. JTu2A.16 Two-photon absorption lithography for nanofabrica- for Applied Sciences and Intelligent Systems, Italian tion of 3D X-Ray compound refractive lenses, National Research Council, Italy. We designed, realized, JTu2A.9 E-Poster Ksenia 4 1,4 4 and tested a pocket module that allows performing Normally Transparent Liquid-Crystal Smart Glass for Abrashitova , Alexandr Petrov , Vladimir Bessonov , 4 4 1 off-axis Digital Holography microscopy with no need for Augmented Reality Head-Up Displays, Chun-Wei Kokareva Natalia , Kirill Safronov , Alexandr Barannikov , 1 1 1 an interferometer setup. To this purpose, a commercial Chen1, Tsung-Jui Ho1, Iam Choon Khoo1; 1Pennsylvania Petr Ershov , Nataliya Klimova , Ivan Lyatun , Vyacheslav 2 1 3 plastic chip is engineered for the scope. State Univ., USA. We report a translucency-tunable cho- Yunkin , Maxim Polikarpov , Irina Snigireva , Andrey Fed- 4 1 1 lesteric liquid crystal window, of which the transparent yanin , Anatoly Snigirev ; Immanuel Kant Baltic Federal 2 JTu2A.3 E-Poster state is the only stable state upon removal of electric Univ., Russia; Inst. of Microelectronics Technology RAS, 3 3-D Printed Spatial Domain Multiplexer, Syed H. fields. The relaxation from the scattering to clear state Russia; European Synchrotron Radiation Facility, France; 4 Murshid1, Nasir Hariri1, Greg Lovell1, Engine Eyceyurt1, takes only 100’s ms. Lomonosov Moscow State Univ., Russia. The present Rayan Enaya1; 1Florida Inst. of Technology, USA. This work proves that X-Ray compound refractive nano-lens paper presents the capability of using a 3D printing JTu2A.10 can be produced through two-photon polymerization technology in manufacturing a platform that will improve Identification of optimum transforms for evaluating lithography. It was tested successfully at the X-ray micro- Tuesday, 19 Septem fixation and stability which provide more control over the perceptual image quality scores using objective met- focus Lab source and a focal spot of 5 μm was measured. current SDM system. rics, Quanzeng Wang1, Nitin Suresh1; 1Food and Drug Administration, USA. Regression models for conversion JTu2A.17 Surface-energy-driven growth and optical modulation JTu2A.4 E-Poster of objective quality metrics to perceptual scores are of ZnO hexagonal microtube optical cavities, Deep learning on OCT images of skin cancer, Dmi- identified. These models depend on the distortion type Hongxing 1 1 try Raupov1, Oleg Myakinin1, Ivan Bratchenko1, Valery present in the image, and an ensemble of metrics is best Dong ; Shanghai Inst. of Optics and Fine Mechanics, Zakharov1; 1Samara National Research Univ. , Russia. A suited for overall evaluation. China. A distinct “split and recoalescence” growth mech- deep learning with neural nets for diagnostics of skin anism of tubular ZnO micro/nanostructures is observed. tumors on OCT images is investigated. The convolu- JTu2A.11 Optical resonant modes of such microtube optical cavities tional neural network is used to solve the task of tumor Phosphor Screens for Laser Projection Systems, Taka- were directly observed experimentally. recognition. masa Kohmoto1, Masamichi Ohta1, Ichiro Fujieda1, Wataru ber Watanabe1; 1Ritsumeikan Univ., Japan. High-resolution JTu2A.18 Integrated Gradient-Index Planar Optofluidic Polymer JTu2A.5 E-Poster images can be displayed on a phosphor screen by pro- Waveguide, 1 1 Transmission of Polarization-Entangled Photons jecting laser light. The screen can be made transparent Juan E. Villegas , Mutasem A. ODEH , 1 1 Through Brain Tissue, Enrique J. Galvez1,2, Behzad Khaja- and might be applicable for a head-up display and a Marcus S. Dahlem ; Masdar Inst., United Arab Emirates. vi1,3, Lingyan Shi4,2, Jhonny Castrillon1,5, Robert R. Alfano2; volumetric 3d display. We propose a microfluidic channel with a rectangular 1Colgate Univ., USA; 2Physics, City College of New York, cross-section, built on a polydimethylsiloxane substrate USA; 3Physics and Astronomy, Florida Atlantic Univ., USA; JTu2A.12 that also acts as a waveguide through a controlled gra- 4Chemistry, Columbia Univ., USA; 5Fisica, Universidad de Novel Hard Mask Fabrication Method for Hybrid dient refractive index profile, fabricated by a modified Antioquia, Colombia. We characterize the entanglement Plasmonic Waveguide and Metasurfaces, Sajid Choud- soft-lithography technique. after one of two polarization-entangled photons travels hury1, Volodymyr Zenin2, Soham Saha1, Vladimir Shalaev1, through a soft-matter scattering medium: brain tissue. Sergey I. Bozhevolnyi2, Alexandra Boltasseva1; 1Purdue JTu2A.19 2-Beam action spectroscopies: A new class of methods We consider tissue samples of distinct thickness, water Univ., USA; 2Univ. of Southern Denmark, Denmark. A for the measurement of the effective order of nonlinear content, type, and healthy or affected by disease. hybrid plasmonic waveguide fabrication technique has absorption, 1 1 been developed and waveguides have been demonstrat- Nikos Liaros , Zuleykhan Tomova , Sandra 1 1 1 JTu2A.6 E-Poster ed. The developed technique can create similar hybrid A. Gutierrez Razo , Samuel R. Cohen , John T. Fourkas ; 1 Design of a Steerable, Configurable Detection, waveguide structures and metasurfaces with transition Chemistry and Biochemistry, Univ. of Maryland at Col- Adaptive Optics Scanning Laser Ophthalmoscope metal nitrides and epitaxial silver. lege Park, USA. We introduce a new class of methods, with Integrated Fixation and Stimulation, Stephen A. based on excitation with two independent beams, for Burns1, Alberto de Castro1,2, Lucie Sawides1,2, Ting Luo1, JTu2A.13 determining the order of effective nonlinearity in different Kaitlyn Sapoznik1; 1Indiana Univ., USA; 2Physics, Univ. of Analysis of Double Slot Hybrid Plasmonic Ring Reso- materials. We discuss representative examples of 2-beam Murcia, Spain. We present an AOSLO with steering that nator with different dielectric materials in Nanoslots, action spectroscopies and their applications allows imaging 30 degrees, with minimal distortion. A Lokendra Singh1, Santosh Kumar1; 1DIT Univ., India, spatial light modulator in the confocal plane provides India. This paper presents the analysis of double slot JTu2A.20 Fabrication of Anti-reflection Microstructures on ZnSe detection specificty. An integrated display subsystem hybrid plasmonic ring resonator structure by varying the Single Crystal by Using Femtosecond Laser Pulses, allows measuring functional responses. dielectric materials in ring nanoslots using finite element 1,2 1 method (FEM). It enhances the sensitivity of the refrac- Mikhail K. Tarabrin , Andrey Bushunov , Vladimir A. 1 1 2 JTu2A.7 E-Poster tive-index sensor. Lazarev , Valerii E. Karasik , Vladimir I. Kozlovsky , Dmi- 2 2,3 2 Exploiting Speckle Decorrelation Rate To Decouple triy Sviridov , Yuriy Korostelin , Mikhail P. Frolov , Yan 2 1 Singly Scattered Light Reflected from A Scattering JTu2A.14 K. Skasyrsky ; Bauman Moscow State Technical Univ., 2 Surface, Aparna Viswanath1, Prasanna Rangarajan1, In- Photonic Bandgap Effect in Mie Scattering of Bragg Russia; P. N. Lebedev Physical Inst. of the Russian Acad- 3 dranil Sinharoy1, Muralidhar M. Balaji1, Marc Christensen1, Fibers, Zeba Naqvi1, Tsing-Hua Her1; 1Univ of North emy of Sciences, Russia; Moscow Inst. of Physics and Duncan MacFarlane1; 1Southern Methodist Univ., USA. Carolina at Charlotte, USA. Anomalous suppression and Technology, Russia. We report the demonstration of zinc Angular dependence of surface/sub-surface scattering enhancement in scattering of optical fibers coated with selenide single crystal reflectivity reduction in a spectral from rough reflecting sample is examined, as evidenced Bragg layers is observed. A scattering angle diagram is range of 3.5 to 15 µm up to 3% by using femtosecond in objective speckle patterns acquired at standoff, to introduced to explain the anomalous features and are laser pulses for microstructure formation without any decouple the single and multiply-scattered light using attributed to photonic bandgap of Bragg layers. etching technique. Principal-Component -Analysis.

FiO + LS 2017 • 17–21 September 2017 39 Science & Industry Showcase

JOINT FiO + LS

JTu2A • Joint Poster Session I—Continued

JTu2A.21 JTu2A.29 JTu2A.37 Real Time Sulfur Particles Analysis in Diesel Using Fiber optical current sensor based on tapered Ter- Efficient 1550 nm Diffractive Log-Polar Element Based Instrumentation Methods based on Spectrometry, fenol-D composite, Suha Lasassmeh1, Edward Lynch1, Orbital Angular Momentum Mode-division Multiplex- Eduardo Perez1,2; 1DICIS, Mexico; 2Electronics, Univ. of Chiu T. Law1; 1Univ. of Wisconsin Milwaukee, USA. This ing, Wenzhe Li1, Keith Miller1, Indumathi Srimathi1, Yuan Guanajuato, Mexico. Sulfur contamination has been a paper presents an optical current sensor which is based Li1, Kaitlyn Morgan1, Eric G. Johnson1; 1Clemson Univ., problem since the begging in oil refinery methods. This on introducing non-uniform period onto a fiber Bragg USA. Diffractive log-polar orbital angular momentum paper proposes the application of a monochromatic Grating (FBG) by embedded it in a magnetostrictive elements have been designed and fabricated for 1550 wavelength fluorescence (MWDXRF) technique to identify composite with tapering shape. nm. Mode-division multiplexing has been experimentally and reduce the sulfur particles contained in Diesel. demonstrated. The power efficiency of the two log-polar JTu2A.30 elements are 84% and 81%, respectively. JTu2A.22 Automated phase-shifting in a cube beam splitter Flexible Tunable Liquid Crystal Platform in Terahertz interferometer, Uriel Rivera-Ortega1; 1Strategic Planning JTu2A.38 Region, Abubaker M. Tareki1, Robert G. Lindquist1, Emin and Technology Management, Universidad Popular Random Micro-Lens Arrays: Effects of Coherence and Gulduren1; 1Univ. of Alabama in Huntsville, USA. We Autónoma del Estado de Puebla, Mexico. It is presented Polarization, Nikolai I. Petrov1, Galina N. Petrova1; 1Sci- investigated an engineered flexible material platform to a low-cost and fully automated process for phase-shifting entific Research Center of Unique Instrumentation of the actively modulate terahertz waves in phase and ampli- interferometry by continuously changing the input voltage Russian Academy of Sciences, Russia. Influence of light tude using stratified layers of patterned gold, Teflon and of a laser diode under the scheme of a common-path coherence on the intensity distribution of diffracted beam liquid crystals. Both simulation and experimental results cube beam splitter interferometer by random microlens arrays is investigated. Significant will be provided. influence of wave-front curvature and polarization of inci- JTu2A.31 dent beam on the reflectance and transmittance is shown. JTu2A.23 Optical Cloaking Using Afocal System, Pavan D. Va- Applications of Software Defined Radio to heterodyne dapalli1, Sourabh Roy1; 1Dept. of Physics, National Inst. JTu2A.39 optoelectronics, Lucas M. Riobo1,2, Francisco E. Veiras1,2, of Technology Warangal, India. Using paraxial approx- Non-destructive optical loss characterization using María T. Garea1, Patricio A. Sorichetti1; 1Universidad imations an optical cloaking device is designed and is designed scattering features, David Lombardo1, Imad de Buenos Aires , Argentina; 2CONICET, Argentina. simulated using CODE – V. The aberrations in the system Agha1, Andrew Sarangan1; 1Univ. of Dayton, USA. We de- This paper describes a real time detection system for are within allowed limits. MTF of the device is more than velop and demonstrate a new, non-destructive technique heterodyne optoelectronics using a Software Defined 50% at 30 cycles/mm of spatial frequency. for measuring optical material losses. This technique Radio (SDR) receiver. The performance of the system is takes advantage of induced scattering by designed demonstrated in an application on displacement mea- JTu2A.32 photoresist features to measure the optical power in thin suring interferometry (DMI). Detection of damage in Oil and Gas Pipelines using film waveguides. ber FBG Sensor, Vaishali Kothari1, Santosh Kumar1; 1DIT Univ., JTu2A.24 India, India. The idea of a Fiber Bragg grating (FBG) sen- JTu2A.40 Holistic Performance-Cost Metric for Post Moore Era, sor has been proposed for detecting damage in pipeline Generation of vector Bessel beams by using phase el- Shuai Sun1, Vikram Narayana1, Armin Mehrabian1, Ruoyu structure based on acoustic emission and their output has ements based on the Jacobi-Anger expansion, Gabriel Zhang1, Tarek EI-Ghazawi1, Volker J. Sorger1; 1George been simulated using MATLAB. Mellado-Villaseñor1, Dilia Aguirre-Olivas2, Ulises Ruiz1, Washington Univ., USA. Here we demonstrated the first Victor Arrizón1; 1Óptica, Instituto Nacional de Astrofísica, holistic metric which includes all critical performance and JTu2A.33 Óptica y Electrónica, Mexico; 2Instituto de Fisiología Celu- cost variables that accurately evaluates the overall abilities Suppressing 1.06-mm spontaneous emission of Neo- lar-Neurociencias, Universidad Nacional Autónoma de of post Moore’s law computing machines and matches dymium by using a tellurite all-solid photonic bandgap México, Mexico. We generate vector Bessel beams (VBBs) with all historical data. fiber, Hoang Tuan Tong1, Demichi Daisuke1, Takenobu of arbitrary order by using a diffraction phase element. 1 1 1

Tuesday, 19 Septem Tuesday, Suzuki , Yasutake Ohishi ; Toyota Technological Inst., The phase transmittance of this element is based on the JTu2A.25 Japan. We demonstrate a suppression of the 1.06-µm Jacobi-Anger identity. Results of the VBB generation are 4 4 Switchable quarter wave plate using Ge2Sb2Te 5 meta- emission which corresponds to the F3/2→ I11/2 transition shown through numerical simulations. surface, Chul Soo Choi1, Jeong-geun Yun1, Gun-yeal Lee1, of Nd3+ ion doped in a tellurite all-solid photonic bandgap Sun-je Kim1, Byoungho . Lee1; 1Seoul national Univ., South fiber by employing the light-guiding properties of its JTu2A.41

Korea. Ge2Sb2Te 5 (GST) is in the spotlight as an ingredient photonic bandgap structure. Holographic Screens with Controlled Scattering Indi- of metasurface to achieve active feature. Here, we pro- catrix, Nikolai I. Petrov1; 1Scientific Research Center of pose a novel method for active switching of polarization JTu2A.34 Unique Instrumentation of the Russian Academy of Sci- via the metasruface composed of GST nanorods. Color Beam Combiners and Splitters, Nikolai I. Petrov1, ences, Russia. Optical layers with controllable scattering Maxim Khromov1, Angela Storozheva1, Yuri Sokolov1; 1Sci- indicatrices are considered. The influence of light source JTu2A.26 entific Research Center of Unique Instrumentation of the coherence, roughness height and correlation length of the Greatly extended depth of field for microscopic Russian Academy of Sciences, Russia. Beam combiners surface roughness on the scattering angle is investigated. imaging, Zengzhuo Li1, Guoqiang Li1; 1The Ohio State and splitters based on the frustrated total internal reflec- Univ., USA. Based on wavefront-coding technique, a tion, diffraction and refraction effects of light beams are JTu2A.42 custom transmissive phase plate can extend the depth considered. New high efficiency prismatic beam combiner Telescope windows: development of a novel pixellated of field (DoF) of a microscope by more than 13 times consisting of uniform material is proposed. optical system, Cyril Bourgenot2, Johannes K. Courtial1, with diffraction-limited resolution in comparison with the Euan Cowie1, John Girkin2, Gordon Love2, David Rob- conventional microscope. JTu2A.35 ertson2, Laura Young2; 1Univ. of Glasgow, UK; 2Dept. of Super-Resolution Imaging in Optical Waveguide, Physics, Durham Univ., UK. We describe progress towards JTu2A.27 Nikolai I. Petrov1; 1Scientific Research Center of Unique building arrays of small telescopes called telescope Design of reversible TR gate using pockel’s effect in Instrumentation of the Russian Academy of Sciences, windows. The telescopes act as pixels of a light-ray-di- lithium -niobate based Mach-Zehnder interferometers, Russia. Remote focusing of light via mode interference rection-changing window. Applications include improved Chanderkanta Chauhan1, Santosh Kumar1; 1DIT Univ., in optical waveguide is demonstrated using exact solu- medical low-vision aids. India, India. In this paper, design of reversible TR gate tions. The possibility of super-resolution image transfer using lithium- niobate based Mach-Zehnder interferom- through the graded-index optical waveguide due to the JTu2A.43 eter is proposed. The results are verified using beam large-scale revival effect is shown. Wavefront analysis of Aberrated Laguerre-Gaussian propagation method and MATLAB simulations. Beam , Chittur S. Narayanamurthy1; 1Indian Inst. of Space JTu2A.36 Sci & Tech, India. Wavefront analysis of an aberrated JTu2A.28 Fiber-based Optical Thermocouples for In-Situ Tem- Laguerre-Gaussian beam generated using LC-SLM and af- Optical flat comb source generation based on a perature Sensing in Extreme Environments, Benjamin ter passing through a Pseudo Random Phase Plate(PRPP) cascade of two stage mach-zehnder modulator, Abir R. Anderson1, Steven Livers1, Ray Gunawidjaja1, Hergen is carried out using Shack Hartmann wavefront sensor and Hraghi1; 1Engring School of Communication of Tunis, Tu- Eilers1; 1Washington State Univ., USA. We develop an Zernike polynomials. nisia. A novel technique to generate an optical flat comb optical thermocouple for use in extreme environments source is presented experimentally demonstrated. the by depositing a Dy:YAG film on a sapphire fiber using transmission of 137.5Gbps(11*11.5Gbps) QPSK-OFDM- pulsed laser deposition. Temperature sensing is achieved UDWDM signal is experimentally illustratted over 25km by way of two-color photoluminescence thermometry. and 100km SSMF link using direct detection.

40 FiO + LS 2017 • 17–21 September 2017 Science & Industry Showcase

JOINT FiO + LS

JTu2A • Joint Poster Session I—Continued

JTu2A.44 JTu2A.52 JTu2A.59 Description of Pairs of Skew Lenses as a Single Lens, Catching Robot Hand System in Dynamic Depth Vari- Fiber Bragg Grating based Temperature Sensor for Jakub Bělín1, Stephen Oxburgh1, Tomáš Tyc2, Johannes ation with a Rotating Variable Focusing Unit, Kenichi Biomedical applications, Vaishali Kothari1, Amna Bedi1, K. Courtial1; 1Univ. of Glasgow, UK; 2Inst. of Theoretical Murakami2, Lihui Wang2, Tomohiko Hayakawa2, Taku Se- Santosh Kumar1; 1DIT Univ., India, India. In this paper, Physics and Astrophysics, Masaryk Univ., Czech Republic. noo1, Masatoshi Ishikawa2,1; 1Dept. of Information Physics measurement of temperature for biomedical instruments We describe pairs of skew ideal thin lenses as a single thin and Computing, Univ. of Tokyo, Japan; 2Dept. of Creative like medical drugs, heat liquids or to clean medical equip- lens with non-coinciding, non-parallel, principal planes. Informatics, Univ. of Tokyo, Japan. We proposed a catch- ment using Fiber Bragg grating (FBG) sensors has been This description facilitates the understanding of structures ing robot hand system that extended the focal length of given. The results have been simulated using MATLAB. of skew lenses such as the ideal-lens cloak. the original optics unit by adding rotating adjustment transparent plates, and succeeded the catching task with JTu2A.60 JTu2A.45 the adaptive optics in dynamic scene. Guided-Mode Resonance Biosensors: Quantifying the Ideal-Lens Cloak and Omnidirectional Lens, Johannes Binding of Neuropeptide Y to its Antibody, Kyu J. Lee1, K. Courtial1, Tomáš Tyc2, Jakub Bělín1, Stephen Oxburgh1, JTu2A.53 Robert Magnusson1, Brett R. Wenner2, Jeffery Allen2, Euan Cowie1, Chris D. White3; 1Univ. of Glasgow, UK; 2Inst. Calculation of the impulse response of PIN and MUTC Monica S. Allen2; 1Univ. of Texas at Arlington , USA; 2Air of Theoretical Physics and Astrophysics, Masaryk Univ., photodetectors using the drift-diffusion equations, Force Research Lab, USA. We apply the guided-mode Czech Republic; 3Centre for Research in String Theory, Seyed Ehsan Jamali Mahabadi1, Curtis R. Menyuk1; 1Univ. resonance sensor principle to record peptide binding Queen Mary Univ. of London, UK. We present a structure of Maryland, Baltimore County, USA. We calculate the dynamics. In particular, we conveniently and expeditiously of ideal thin lenses that acts as an omnidirectional trans- impulse response of high-current PIN and MUTC pho- quantify anti-NPY binding to NeutrAvidin and then NPY formation-optics cloak and an omnidirectional lens. We todetectors using the drift-diffusion equations, avoiding binding to anti-NPY. present the design principles, and discuss experimental computationally-expensive Monte Carlo simulations. realisability and potential applications. We calculate the shot noise limit and cut-off frequency JTu2A.61 of the devices. Photo-bio modulatory response of platelets to low JTu2A.46 power laser - A pilot study, Bharath Rathnakar1, Namita Beam Quality Deterioration Due to Angular Dispersion JTu2A.54 Bhyravbhatla1, Subhash Chandra1, Bola Sadashiva Satish of Optical Elements, Sergiy Mokhov1; 1Univ. of Central Parametric Studies on Wide Field of View Imaging Rao1, Krishna Kishore Mahato1; 1Manipal Univ., India. Florida, CREOL, USA. The deterioration of M2 from Systems with Curved Image Sensors, Gil Ju Lee1, Young Platelets isolated were treated with varying fluences (0.5, unity due to angular dispersion for non-monochromatic Min Song1; 1GIST, South Korea. We present simple optical 1 and 2 J/cm2) of low power laser (830 nm). Mitochondrial Gaussian beam is found analytically. It depends on beam systems composed of curved image sensors and different membrane potential (MMP) of platelets were assessed size and meansquare variation of optical element angular lens geometries reducing the complexity of the optical through flow cytometry using Tetramethylrhodamine, Tuesday, 19 Septem dispersion averaged with beam spectral distribution. system while capturing optical performances such as Methyl Ester (TMRM). wide field of view. JTu2A.47 JTu2A.62

Electronic frequency divider as a tool for phase/fre- JTu2A.55 Nonlinear Photoacoustic Studies of Cu2O nanoparticles quency noise analysis, Dipenkumar Barot1, Lingze Duan1; Optical Fiber Loops and Helices: Tools for Integrated for Photonic and Biomedical Applications, Vijayaku- 1Univ. of Alabama in Huntsville, USA. We demonstrate Photonic Devices Characterization and Microfluidic mar Sadasivan Nair1, Chandra S. Yelleswarapu1; 1Univ. 1 1 experimentally that the electronic frequency divider can Manipulations, Yundong Ren ; Worcester Polytechnic of Massachusetts Boston, USA. We synthesized Cu2O be used as a simple tool for measuring phase/frequency Inst., USA. We fabricated two special geometry tapered nanoparticles and performed structural, nonlinear optical modulation noise in the beat note and also provide fibers, tapered fiber loops and helices. And demonstrated characterization. Grain size of the nanoparticles was found

theoretical explanation for that. their applications in nanophotonics and microfluidics. to be 21 nm with a band gap of 2.32eV. Z-scan studies ber depicts reverse saturable absorption type behavior. JTu2A.48 JTu2A.56 Detecting of spectrometric information in a diffraction Nanocomposites of plasmon nanoparticles with dyes JTu2A.63 grating spectral device, Artur Paraskun1, Vasily Kazakov1, and biological objects, Valentyn Smyntyna1, Valentyna Styryl BODIPY Derivatives as Contrast Agents for Oleg Moskaletz1; 1St. Petersburg State Univ. of Aerospace Skobeeva2, Nikolay Malushin2, Vladimir Tkachenko2, In Vivo Photoacoustic Imaging, Maryam Hatamimos- Instrumentation, Russia. The detecting process of spec- Vadim Ulyanov3, Mariya Makarova3; 1Dept. of Physics, lehabadi1, Stephanie Bellinger1, Jonathan Rochford1, trometric information via CCD structures in diffraction Odessa National I. I. Mechnikov Univ., Ukraine; 2Research Chandra S. Yelleswarapu1; 1Univ. of Massachusetts Boston, spectral device is considered. Mathematical relationships Inst. of Physics, Odessa National I. I. Mechnikov Univ., USA. We report synthesis and characterization of BODIPY between photocurrent in each element of CCD and inci- Ukraine; 3Odessa National Medical Univ., Ukraine. The inspired molecular systems as photoacoustic contrast dent spectrum of optical radiation is obtained. optical properties of heterogeneous systems, including agents. Chemical modification of pristine BODIPY Ag nanoparticles and dye were studied. The effect of provided amplified photoacoustic response in the NIR JTu2A.49 Ag nanoparticles influence on molecular structuring of biologically transparent region. Exploring Lens Geometry for Superlensing in an Elec- methylene blue dye and on luminescence of dye, on trostatic Pendry Lens, Elizabeth Keys1, Sergei Mistyuk1, immunomodulating blood cells. JTu2A.64 Christopher Keys1, Gary Shoemaker1; 1California State Design of a Spectrometer for Frequency Domain Univ., Sacramento, USA. In superlensing, the methods of JTu2A.57 Optical Coherence Tomography Working at 1325 nm, manufacturing complicated lens designs can be cost-pro- Extreme light confinement based on plasmonic Athira G1, Naren Mekala1, Nitin Chandrachoodan1, hibitive. Motivated by unpublished results in 2007, a nanopost arrays for super-localization microscopy, Ashish Mishra1, Anil Prabhakar1, Shanti Bhattacharya1; changeable electrostatic Pendry lens was designed and HK Lee1, Donghyun Kim1; 1Yonsei Univ., South Korea. 1indian Inst. of Technology Madras, India. For an FDOCT the effects of geometry are being pursued. Near-field distribution produced by plasmonic nanopost system imaging depth, axial resolution and sensitivity arrays was measured and compared with finite difference roll-off depend on the characteristics of its detector JTu2A.50 time domain simulations. The possibility of plasmonic which is a spectrometer. Optical and electronic design Chebyshev Freeform Microlens Array Homogenizer nanopost arrays for applications in super-localization considerations of a spectrometer for a 1325nm FDOCT for Excimer Laser Beam Shaping, Yuhua Jin1, Ali Has- microscopy was explored. system are presented. san1, Yijian Jiang1; 1Beijing Univ. of Technology, China. A novel design technique of microlens beam homogenizer JTu2A.58 JTu2A.65 for excimer lasers is presented. As a new approach by Long Range Capturing and Delivery of Water Dis- Diethyl Ether Sensor using Double Nanoslot Hybrid applying Chebyshev freeform surface microlens array, the persed Nanoparticles for High Resolution Detection, Plasmonic Waveguide, Lokendra Singh1, Amna Bedi1, homogenizer can yield superior beam shaping results than Francesco Tantussi1, Gabriele Messina1, Laura Lovato1, Santosh Kumar1; 1DIT Univ., India, India. The diethyl ether conventional method. Rosario Capozza1, Michele Dipalo1, Francesco De Ange- can be easily detected using double nanoslot hybrid lis1; 1Istituto Italiano di Tecnologia, Italy. The generation plasmonic waveguide based sensor. The sensitivity can JTu2A.51 and the following collapse of a gas bubble in water is a be achieved up to 27.67π (nm/RIU) at the wavelength U Shaped Fiber-Optic pH Sensor Using Sol-gel Coating highly efficient technique for capturing, trapping and de- of 1550nm. Over TiO2, Akhilesh K. Pathak1, Vinod k. Singh1; 1IIT(ISM), livering water dispersed nanoscale elements in a specific India. A wide range U shaped fiber optic pH sensor uti- area of a substrate. lizing titanium dioxide (TiO2) layer with sol-gel coating, has been fabricated and demonstrated in this paper. A high sensitivity of 0.37 dBm/pH is observed with fast response time of 14s.

FiO + LS 2017 • 17–21 September 2017 41 Science & Industry Showcase

JOINT FiO + LS

JTu2A • Joint Poster Session I—Continued

JTu2A.66 JTu2A.73 JTu2A.80 Optical Properties Distribution in Nanobiophotonics Multimodal Method of Virtual Biopsy for Skin Cancer Three-Stage Blood Plasma Photodynamic Drug Deliv- Theranostic Applications, Felix Fanjul-Velez1, Jose L. Diagnosis, Oleg Myakinin1, Ivan Bratchenko1, Valery ery & Activation Device, Abdullah J. Zakariya1; 1Ministry Arce-Diego1; 1Universidad de Cantabria, Spain. Theranos- Zakharov1; 1Samara National Research Univ., Russia. In of Interior Kuwait, Kuwait. A three stage integrated optical tic biomedical optical techniques can add nanoparticles to this paper we present a multimodal method of virtual microfluidic drug delivery and activation device consists increase contrast in diagnosis, or to potentiate treatment (optical) biopsy for the diagnosis of skin oncological of a monolithic selectively intermixed QW LED structure effect. Specific optical properties of the nanoparticles neoplasms. The results of diagnostic accuracy (75%-95%), emitting three wavelengths of 805nm, 787nm and 772nm involved may greatly influence the efficiency of these applications as well as further directions of the method to allow a single step photodynamic operation. techniques. development are shown. JTu2A.81 JTu2A.67 JTu2A.74 2D Fourier Fractal Analysis of Skin Tumor with Spectral An Isogeometric solution to the forward problem of Multiple analyze on 3D-OCT images of skin cancer, Domain Optical Coherence Tomography, Wei Gao1, Jing Optical Tomographic reconstruction, Vahid Bateni1, Dmitry Raupov1, Oleg Myakinin1, Ivan Bratchenko1, Julia Jin1, Dmitry Raupov2, Oleg Myakinin2, Yulia Khristoforo- Robert West1; 1Virginia Tech, USA. Optical tomography Khristoforova1, Valery Zakharov1, Alexander Khramov1; va2, Ivan Bratchenko2, Valery Zakharov2; 1Ningbo Univ. (OT) is a powerful tool for diagnosis. We applied Isogeo- 1Samara National Research Univ., Russia. A computer of Technology, China; 2Dept. of Laser and Biotechnical metric Analysis (IGA), a novel numerical method, to the method for diagnostics of skin tumors on OCT images System, Samara National Research Univ. , Russia. The 2D forward problem. IGA shows more accurate and efficient based on textural, morphological, geometrical, spectral Fourier fractal analysis (FFA) was utilized in OCT images results compared to Finite Element Method. and other features is proposed. The method is designed for automatically categorizing the basal cell carcinomas, for 2D and 3D images. melanomas and pigment nevi. JTu2A.68 2D Computational Modeling of Optical Trapping JTu2A.75 JTu2A.82 Effects on Malaria-infected Red Blood Cells, Joana S. Performance Testing of a Mobile-Phone-Based Quantitative X-ray ultra-small angle scattering retrieval Paiva1,2, Rita S. R. Ribeiro1,2, Pedro A. S. Jorge1,2, Carla C. Near-Infrared Fluorescence Imaging System, Pejhman with structured illumination for microvessel character- Rosa1,2, A. Guerreiro1,2, Joao P. S. Cunha1,3; 1INESC TEC Ghassemi1, Bohan Wang2, Jianting Wang1, Quanzeng ization, ziling wu1, Yunhui Zhu1, Xiaolong Li1; 1Electrical - INESC Technology and Science, Portugal; 2Astronomy Wang1, Yu Chen2, T. Joshua Pfefer1; 1US Food and Drug and Computer Engineering, Virginia Tech, USA. A struc- and Physics Dept., Univ. of Porto, Portugal; 3Dept. of Elec- Administration, USA; 2Univ. of Maryland , USA. This tured illumination based X-ray ultra-small angle scattering trical and Computer Engineering, Univ. of Porto, Portugal. study explores the potential for fluorescence imaging imaging resolves the orientation-dependent differential A computational method for optical fiber trapping of with an NIR-enabled mobile phone. Measurements of cross-section from a single shot, enabling texture analysis healthy and Malaria-infected blood cells characterization tissue phantoms and an ex vivo rodent model provide for microvessels with a large field of view. is proposed. A trapping force relation with the infection quantitative and qualitative insights into performance ber stage was found, which could trigger the development relative to a CCD system. JTu2A.83 of a diagnostic sensor. Computational Analysis of Swallowing Mechanics in an JTu2A.76 Aging Rodent Model, Heidi Kletzien1, Nadine P. Connor1; JTu2A.69 Optimization for measurement of diffusion correlation 1Univ. of Wisconsin - Madison, USA. Novel methodology Design Considerations in Decreasing the Cost of Adap- spectroscopy: experiment study, Zeren Li1, Detian was developed to computationally analyze swallowing tive Optics Retinal Imaging, Ann E. Elsner1,2, Matthew Wang1, Liguo Zhu1, Peng Gao1, Qixian Peng1, Jianheng mechanics in a rodent model using multivariate mor- S. Muller2, Joel A. Papay1, Edmund Arthur1, Stephen A. Zhao1; 1China Academy of Engineering Physics, China. We phometric analysis of skeletal and muscular landmarks Burns1; 1Indiana Univ., USA; 2Aeon Imaging, USA. Cost, present how the optical intensity and optode’s separation during vidofluoroscopy. With aging, biomechanics of the size, and complexity inhibit the use of adaptive optics affect the DCS measurement. swallow are altered. retinal imaging. Designing an imager with only sufficient

Tuesday, 19 Septem Tuesday, resolution for key features provides visualization and JTu2A.77 JTu2A.84 quantification of biomarkers not seen with wide field Skin Redox Potential Inspection Based on Ubiquinone Mechanical properties of cellular nucleus characterized techniques. Using Multispectral and Fluorescence Analysis, Elvira by Brillouin flow cytometry, Jitao Zhang1, Xuefei Nou1, O. Timofeeva1, Elena Gorbunova1, Aleksandr Chertov1; Hanyoup Kim2, Giuliano Scarcelli1; 1Univ. of Maryland at JTu2A.70 1ITMO Univ., Russia. This research is dedicated to College Park, USA; 2Canon U.S. Life Sciences, Inc., USA. PPPIX-based Photodynamic Therapy Monitoring by investigate optical properties of ubuquinone and find We developed a label-free flow cytometry platform to Fluorescence Patterns, Felix Fanjul-Velez1, José Luis the way to apply the results to clinical diagnostics of the characterize the nuclear mechanics based on Brillouin Arce-Diego1; 1Univ. of Cantabria, Spain. Photodynamic redox potential. microscopy, which is an all-optical technique so that can Therapy provides highly specific tumor destruction. measure the stiffness of the nucleus in a non-contact, Treatment efficiency depends on the photodynamic JTu2A.78 non-invasive manner. process. Fluorescence patterns emitted by the photo- Optical characterization of polymeric nanocapsules sensitizer contribute to treatment dosimetry guidelines interaction with the cell membrane and in vivo JTu2A.85 and recurrence avoidance. analysis, Yana V. Tarakanchikova1,2, Tatyana Avsievich1, Non-scanning gonioreflectometer for rapid multi-an- Evgeny Zherebtsov3,1, Seppo Vainio1, Igor Meglinski1, gle spectrum measurement, Szu-Yu Chen1, Hong Ling JTu2A.71 Alexey Popov1; 1Oulu Univ., Finland; 2Remotely Controlled Chen1; 1National Central Univ., Taiwan. A non-scanning Laser Induced Fluorescence in combination with Theranostics Systems, Saratov State Utiversity, Russia; measuring system for multi-angle spectrum was intro- Multivariate analysis classifies anti-malarial herbal 3Aston Inst. of Photonic Technologies, Aston Univ., UK. duced to fit for rapid dynamics measurement. Using plants, Charles L. Amuah1; 1Univ. of Cape Coast, Ghana. Polymeric nanocapsules was studied with respect to an objective to transform the angular information into Laser-induced fluorescence in combination with multi- intracellular drug delivery applications. In this paper, we spatial domain, spectra within -60o~60o can be measured variate analysis as a simple, rapid and non-destructive review diffraction phase microscopy (DPM), an effective with one snap. method for classifying anti-malarial herbal plants is quantitative phase microscopy tool which was used for presented. A suitable alternative method that enhances determination cells structure. JTu2A.86 safety and objectivity. Exceptional Point Engineered Multifunctional Glass JTu2A.79 Slide for Microscopic Thermal Mapping, Han Zhao1, JTu2A.72 Fiber-shifting endomicroscopy for enhanced resolution Zhaowei Chen2, Ruogang Zhao2, Liang Feng1; 1Dept. Characterization and discrimination of basal cell carci- imaging, Khushi Vyas1, Michael Hughes1,2, Guang-Zhong of Electrical Engineering, SUNY Buffalo, USA; 2Dept. noma and normal human skin tissues using resonance Yang1; 1Imperial College London, UK; 2Univ. of Kent, of Biomedical Engineering, SUNY Buffalo, USA. We Raman spectroscopy, Cheng-hui Liu1, Binlin Wu3, Susie UK. We introduce a miniaturized two-axis, fiber-shifting demonstrate a thermal sensitive glass slide with en- Boydston-White2, Hugh Beckman1, Vidyasagar Sriramo- endomicroscope in which a super-resolution image is hanced sensitivity by exploiting an optical exceptional ju1, Laura Sordillo1, Chunyuan Zhang1, Jason Smith3, restored from multiple pixelation limited images by scan- point. The devised glass slide expands its functionality Lin Zhang1, Lingyan Shi4, Robert R. Alfano1; 1CUNY ning the fiber-bundle behind a fixed micro-lens, giving a to cost-efficient thermal mapping under a conventional City College, USA; 2CUNY, USA; 3Southern Connecticut 2-fold resolution improvement. microscope system. State Univ., USA; 4Columbia Univ., USA. Resonance Raman spectroscopy is used for rapid detection of skin BCC cancer. The cross-validated classification accuracy is achieved to be as high as 98% using nonnegative matrix factorization along with support vector machine statistical method.

42 FiO + LS 2017 • 17–21 September 2017 Science & Industry Showcase

JOINT FiO + LS

JTu2A • Joint Poster Session I—Continued

JTu2A.87 JTu2A.94 JTu2A.101 Real-time confocal fluorescence lifetime imaging Volumetric Light-field Encryption at the Microscopic Active underwater polarization imaging technology, microscopy (FLIM) based on the analog mean-delay Scale, Changliang Guo1, Haoyu Li1, Inbarasan Muniraj2, Kui Yang1, Pingli Han1, Fei Liu1, XiaoPeng Shao1; 1Xidian (AMD) method, Young Jae Won1, Seungrag Lee1; Bryce Schroeder1, John Sheridan2, Shu Jia1; 1Stony Brook Univ., China. This study attempts to recover high-quality 1Osong Medical Innovation Foundation, South Korea. Univ., USA; 2School of Electrical, Electronic Engineering, underwater images through the PSF of degraded images We demonstrated GPU accelerated real-time confocal Univ. College Dublin, Ireland. A light-field based method and the polarimetric technology. This experiment employs fluorescence lifetime imaging microscopy (FLIM) based allowing the optical encryption of three-dimensional (3D) extracted slant-edge to estimate the PSF and then the on the analog mean-delay (AMD) method. The frame volumetric information at the microscopic scale is report- recovery of image is achievable. rate of our system was demonstrated to be 13 fps for a ed, in which it paves the way for biomedical applications 200 × 200 pixel image. in processing and securing data. JTu2A.102 FRFT-based method for estimating parameters of opti- JTu2A.88 JTu2A.95 cal fiber connectors, Ming-Feng Lu1, Jinmin J. Wu1, Kun Second-Harmonic Generation Microscopy Imaging of PSF Engineering for Sensor Protection, Jacob H. Xiong1, Zhen Guo1, Jian Xu1, Chenchen Ji1, Feng Zhang1, Corneal Superstructure, Chen Y. Dong1; 1National Taiwan Wirth1, Abbie Watnik2, Grover Swartzlander1; 1Rochester Ran Tao1, Zhi-Chun Zhao1; 1Beijing Inst. of Technology, Univ., Taiwan. Optical clarity and mechanical strength are Inst. of Technology, USA; 2Naval Research Lab, USA. An China. This paper proposes a fractional Fourier method properties of cornea that are dictated by the collagen imaging system is designed to protect sensors from laser to analyze a single closed interferogram of the connector superstructure. We used second hamronic generation radiation. A Spatial Light Modulator is used to engineer a end-face. When shadowed or discontinuous areas exist, microscopy to characterize and study chicken cornea new point spread function with low peak intensity while higher accuracy is obtained in comparison with 5-step model in thee-dimensions. sharp images are recovered in post-processing. phase shifting interferometry.

JTu2A.89 JTu2A.96 JTu2A.103 Label-free cell membrane detection by Raman spec- Multiple-image Authentication based on Random High space-bandwidth product compressive lensless troscopy using biocompatible gold nanostructure Sparse Encoding of Optical Discrete Cosine Transform, holography with efficient block-wise model, Hua microscale arrays on a ferroelectric template, Rusul M. Ayman Alfalou1, Qu Wang1, Christian Brosseau1; 1IS- Zhang1, Liangcai Cao1, Wenhui Zhang1, Hao Zhang1, Al-Shammari1,2, Nebras Alattar1, Michele Manzo3, Katia EN-Brest, France. In our proposal, a synthetic ciphertext Guofan Jin1; 1Tsinghua Univ., China. The applications of Gallo3, Brian Rodriguez1,2, James Ricejam1,2; 1School of is constructed and the security level of this scheme is compressive holography are limited by its long processing Physics, Univ. college Dublin, Ireland; 2Conway Inst. of improved greatly because the decryption result gener- time due to huge global searching space. A block-wise Biomolecular and Biomedical Research, Univ. college ated from correct decryption keys is a noise-like image model is developed with multiple sub-holograms to 3 Dublin, Ireland; Applied Physics, KTH, Sweden. A without plaintext visually revealed. reduce reconstructed time by fifty times. Tuesday, 19 Septem biocompatible ferroelectric template, patterned with gold nanoparticles by photodeposition, is used here JTu2A.97 JTu2A.104 to enable SERS monitoring of the cell membrane of Augmented Reality Based Real-Time Data Visualiza- Vehicle Extraction from UAV Data, Tingting Zhou1, osteoblast-like cells. tion Concept for Ultra-Efficient Car Prototype, Peter Lingjia Gu1, Ruizhi Ren1, Qiong Cao1; 1Jilin Univ., China. Wozniak1,2, Oliver Vauderwange1,2, Nicolas Javahiraly2, For the purpose of vehicles dynamic management of the JTu2A.90 Dan Curticapean1; 1Offenburg Univ., Germany; 2Univ. of parking lot, a color image segmentation algorithm is used Seeing Through Fog: Polarized Monte Carlo Light Strasbourg / ICube, France. For an ultra-efficient car-en- to extract static vehicles and a Gaussian mixture model Propagation through Turbid Atmosphere, Brett H. gineering project, we aim to utilize AR technology for the is used to extract dynamic vehicles. Hokr1, Jonathan Farmer2, Christopher Persons3, Robert driver and engineering team. A real-time monitoring of 2 2 3 4 1

DeSilva , James Kirkland , Greg Finney , Kirk Fuller ; US the car’s operational parameters is crucial for best possible JTu2A.105 ber Army Space and Missile Defense Comman, USA; 2Eikon fuel efficiency and overall performance. Automatic calibration of Projector and DDHOE based Research, Inc., USA; 3Ierus Technologies, Inc., USA; 4Earth IP displays, Jackin Boaz Jessie1, Lode Jorissen2, Ryutaro System Science Center, Univ. of Alabama in Huntsville, JTu2A.98 Oi1, Koki Wakunami1, Yasuyuki ichihashi1, Makoto Okui1, USA. The ability to see through turbid media has many Calibration between a 3D camera and an aerial screen Philippe Bekaert2, Kenji Yamamoto1; 1National Inst. applications ranging from driving in fog to imaging the without relative change of object size, Shusei Ito2, Nao of Communications Tec, Japan; 2Expertise Center for brain. Here we develop a Monte Carlo light transport Kurokawa2, Hirotsugu Yamamoto2,1; 1JST, ACCEL, Japan; Digital Media, Hasselt Univ.-tUL, Belgium. A calibration simulation capable of simulating polarized light transport 2Utsunomiya Univ., Japan. The purpose of this paper is technique for integral photography(IP) based 3D display through fog. to propose a calibration method of a 3D camera and an that uses a commercial projector and digitally designed aerial information screen. Our proposed method features holographic optical element (DDHOE), is reported. JTu2A.91 direct input in the real space and a short calibration time. This method requires less number of input images for Utilizing Machine Learning for Smart Starting Guesses calibration. for Phase Retrieval, Scott Paine1, James Fienup1; 1Univ. JTu2A.99

of Rochester, USA. Traditional wavefront-sensing phase Radiation Modes of Surface Plasmons in SnO2 Thin JTu2A.106 retrieval problems with large amounts of wavefront error Films, Viktor S. Grinevych1, L. M. Filevska1, Valentyn Smyn- Babinet Principle for Partially Coherent Fields, Mahed often do not converge without a good starting point. We tyna1, S. P. Rudenko2, M. A. Stetsenko2, L. S. Maksimenko2, Batarseh1, Sergey Sukhov1, Roxana Rezvani Naraghi1,2, use machine learning in an attempt to produce better Boris Serdega2; 1Odessa National I.I.Mechnikov Univ., Heath E. Gemar1, Alexandru Tamasan3, Aristide Dogariu1; starting guesses for these problems. Ukraine; 2V.E.Lashkarev Inst. of Semiconductor Physics, 1CREOL, The College of Optics and Photonics, Univ. of National Academy of Sciences of Ukraine, Ukraine. SP Central Florida, USA; 2Dept. of Physics, Univ. of Central JTu2A.92 radiation modes, responsible for structure-dependent Florida, USA; 3Dept. of Mathematics, Univ. of Central

Building Scalable Integrated Silicon Photonics Reser- energy loss, are studied by MPS in SnO2 films depending Florida, USA. Babinet theorem (BT) in an electromagnetic voirs for Signal Processing, Andrew Katumba1, Matthias on production technology. Amplitude decrease r(l) is diffraction theory relates single-point quantities, intensi- Freiberger2, Jelle Heyvaert1, Joni Dambre2, Peter Bienst- associated with precursor concentration increase in films ties or field amplitudes, generated by complementary man1; 1Dept. of Information Technology, Gent Univ. - imec, production initial solution. sources. We demonstrated BT for two-point quantity, the Belgium; 2Dept. of Electronics and Information Systems, spatial coherence function of the field. Gent Univ., Belgium. Photonic reservoir computing is a JTu2A.100 novel bio-inspired paradigm for signal processing. We Digital image encryption using chaotic logistic map- JTu2A.107 discuss how it can be scaled up by injecting multiple ping, Francisca A. Canales1, Roman Hurtado Perez1, Mar- Integral Imaging Multi-View 3D Display, Nikolai I. copies of the input and by using multi-mode rather than tin Hernandez-Romo1; 1Optica, Universidad Politécnica de Petrov1, Yuri Sokolov1, Maxim Khromov1, Angela Storozhe- single-mode components. Tulancingo, Mexico. The protection against unauthorized va1; 1Scientific Research Center of Unique Instrumentation access is essential. The proposed method of digital proof the Russian Academy of Sciences, Russia. Multiview 3D JTu2A.93 cessing of encrypted images decreases the correlation display system consisting of the modules of capturing Single pixel non-imaging object saliency detection by between adjacent pixels, increasing entropy, using secret three-dimensional objects, image processing and display means of Fourier spectrum acquisition, Hui C. Chen1, key and chaotic encryption. screen is developed. Multi-projector system with four Jian H. Shi1, Xia l. Liu1, Gui H. Zeng1; 1Shanghai Jiao Tong projectors is designed and 3D images on 30-inch screen Univ., China. We propose and experimentally demon- are demonstrated. strate object saliency detection by means of Fourier spectrum acquisition can realize single pixel non-imaging object saliency detection. This technique can be applied to saliency detection and recognition of image.

FiO + LS 2017 • 17–21 September 2017 43 Science & Industry Showcase

JOINT FiO + LS

JTu2A • Joint Poster Session I—Continued

JTu2A.108 JTu2A.112 JTu2A.116 UMapβ: A Semi-automatic Image Analysis Assistant Statistics of Wave inside Random Media with Lévy Peripheral Monochromatic Aberrations in Young Adult Bridging the Gap between Experimentalists and Image Disorder, Xujun Ma1, Victor Gopar2, Azriel Genack1; Caucasian and East Asians, Uchechukwu L. Osuagwu1, Analysis Specialists, Jeffrey La1, Briana Mason1, Tiffany 1CUNY Graduate Center and Queens College, USA; Noel A. Brennan2, Marwan Suheimat1, David A. Atchi- Donaldson1, Chandra S. Yelleswarapu1; 1Univ. of Massa- 2Departamento de Fisica Teorica and BIFI, Universidad de son1; 1Optometry & Vision Science, Queensland Univ. of chusetts Boston, USA. Quantitative biological analysis Zaragoza, Spain. We explored the anomalous localization Technology, Australia; 2Johnson & Johnson Vision Care, traditionally relies on labor intensive manual methods of waves inside random media with Lévy disorder. The Inc., Jacksonville, FL, USA. We determined variations in and newer fully automated methods are often inflexible average of intensity and its logarithm exhibit a power peripheral aberration across the visual field. Caucasians and unfeasible to implement. We propose UMapβ, our law fall-off, which implies that the LDOS falls within the and East Asians had similar relative peripheral myopia semi-automated graphical user interface, as a solution. medium. but vertical coma and spherical aberration coefficients were more negative in Caucasians than in East Asians. JTu2A.109 JTu2A.113 Phase modulation based optical asymmetric image Reducing Cybersickness: The Role of Wearing Comfort JTu2A.117 encryption, Areeba Fatima1, Naveen K. Nishchal1; 1Indi- and Ease of Use, Kai Israel1, Christopher Zerres1, Dieter Fine Tuning of Reflective Colors by Introducing Po- an Inst. of Technology, Patna, India. This work proposes K. Tscheulin2; 1Dept. of Media and Information, Univ. of rosity in Ultra-thin Lossy Films, Youngjin Yoo1, Young an optical asymmetric cryptosystem. Information of the Applied Sciences Offenburg, Germany; 2Dept. of Business Min Song1; 1Gwangju Inst. of Science and Technology, input image is encoded in the phase of the circular Administration, Univ. of Freiburg, Germany. The paper South Korea. We demonstrate a fine tuning of reflective

components of an optical beam. Simulation results have focuses on how wearing comfort and ease of use of colors by porosity (Pr) in ultra-thin lossy films by oblique

been produced to substantiate the proposed scheme. smartphone-based headmounted displays can minimize angle deposition (OAD). The effect of Pr with an optical the occurrence of cybersickness. resonance-shift is shown by calculation and experimental JTu2A.110 results. Building detection from high-resolution remotely JTu2A.114 sensed images, Qiong Cao1, Lingjia Gu1, Ruizhi Ren1; 1Ji- Integrating Technology to Supplement Classroom JTu2A.118 lin Univ., China. The commercial high-resolution satellite Teaching of Optics, Sumit Ghosh1; 1School of Optics, Ultra-large Mode Field Diameter of Outer Fibers of images became available, which provides more potential India. A teaching-learning process which concentrates Rod Photoreceptor Cells, Ziming Meng1, Anhui Liang1; for automatic and accurate building detection. So Build- on a collaborative methodology with simultaneous 1Guangdong Univ. of Technology, China. In this paper, ing extraction currently is important in the application of integration of technology has been developed to teach we theoretically calculate the MFD of outer fibers of rod remote sensing imagery. the basic principles of optics to students hailing from photoreceptor cells. under-privileged schools. JTu2A.111 ber Fast Implementation of Fractional Fourier Analysis of JTu2A.115 Quadratic Phase Interferogram, Feng Zhang1, Ming- New Perspectives in Color Vision using Spectroscopy Feng Lu1, Zhi-hai Zhuo2, Jinmin J. Wu1, Cui-ling Qi1; and Nanotechnology: Application to Media Photonics, 1Beijing Inst. of Technology, China; 2Beijing Information Oliver Vauderwange1,2, Peter Wozniak1,2, Nicolas Javahi- Science and Technology Univ., China. An image block raly2, Dan Curticapean1; 1Offenburg Univ., Germany; 2Univ. linear superpose method is proposed for fast implementa- of Strasbourg / ICube, France. This paper summarizes tion of Fractional Fourier analysis of quadratic phase inter- the basic ideas of the actual research work, based on the ferogram, its performance, verifying the feasibility of the question, how quantum dots changes the possibilities method, is assessed by analyzing Newton’s rings images. of color rendering, with the focus on the human visual perception. Tuesday, 19 Septem Tuesday,

11:45–12:45 Meet OSA’s Journal Editors, Science Showcase Theater, Columbia, Terrace Level

12:00–13:00 Pizza Lunch, Science & Industry Showcase, Columbia, Terrace Level

13:00–13:30 Coffee Break, Science & Industry Showcase, Columbia, Terrace Level

Join the conversation. Follow @Opticalsociety on Twitter. Use hashtag #FIO17

44 FiO + LS 2017 • 17–21 September 2017 13:00–15:00 JTu3A • Science & Industry Showcase Exhibits, Poster Session & E-Posters Rapid-Fire Oral Presentations II in Theater Columbia, Terrace Level

Science Showcase Theater

JOINT FiO + LS

13:00–14:00 JTu3A • Rapid-Fire Oral Presentations II

JTu3A.12 • 13:00 RAPID JTu3A.75 • 13:20 RAPID JTu3A.104 • 13:40 RAPID Temporal measurement of the wave-breaking flash in Tunable Cavity Fiber-Optic Fabry-Perot Magnetometer Gain-Clamping for an Externally-Incident Field Passing a laser plasma accelerator, Bo Miao1, Jared Wahlstrand1, Based on Fiber-Cantilever Beam-Deflection, Somarpita through a Laser Cavity, Ali Kazemi Jahromi1, Alexander Linus Feder1, Andy Goers1, George Hine1, Fatholah Pradhan1, Samik Saha1, Partha Roy Chaudhuri1; 1Indian Cerjan2, A. Douglas Stone3, Ayman Abouraddy1; 1Univ. of Salehi1, Daniel C. Woodbury1, Howard Milchberg1; 1Inst. Inst. of Technology Kharagpur, India. We devised a Central Florida, CREOL, USA; 2Applied Physics, Stanford for Research in Electronics and Applied Physics, Univ. of tunable cavity fiber Fabry-Perot magnetometer using Univ., USA; 3Applied Physics, Yale Univ., USA. Behavior of Maryland, College Park, USA. Wave-breaking injection of deflection of cobalt-doped nickel ferrite coated optical a self-oscillating cavity probed with an externally incident electrons in a laser plasma accelerator generates intense fiber cantilever. Sensitivity is improved by introducing a field has been the subject of controversy for decades. We broadband (Δλ≈300 nm) radiation flash. We study its silver coated fiber-mirror in the developed configuration. address this issue by designing an experiment, and verify spectral coherence and measure its pulse length (~50 fs) it with state-state ab-initio laser theory. with single-shot supercontinuum spectral interferometry. JTu3A.81 • 13:25 RAPID Diffusive Dynamics and Signature of Phase Singularities JTu3A.105 • 13:45 RAPID RAPID JTu3A.35 • 13:05 in Gain/Loss Assisted Disordered Optical Waveguide Efficient Lasing on Alkali Atomic D2 Lines Utilizing Enhanced optical nonlinearities in ultra-silicon-rich Lattices, Somnath Ghosh1, Ravi K Varshney3, Bishnu P. Spin-Polarized Alkali Vapor, Andrey Mironov1, J. G. photonic crystal waveguides, Ezgi Sahin1,3, Kelvin J. Pal2; 1Indian Inst. of Technology Jodhpur, India; 2MEC Eden1; 1Univ of Illinois at Urbana-Champaign, USA. We Ooi1, George F. R. Chen1, Doris K. T. Ng2, Ching Eng Hyderbad, India; 3Indian Inst. of Technology Delhi, India. report a novel method for significantly improving the ef- Png3, Dawn T. H. Tan1; 1Photonics Devices and Systems Co-existence and interplay between mesoscopic light ficiency of alkali atomic lasers. By pumping alkali-rare gas Group, Engineering Product Development, Singapore dynamics with singular optics in spatially disordered atomic pairs with a circularly polarized optical field, an in- 2 Univ. of Technology and Design, Singapore; Data Stor- waveguide lattices is reported. Disorder induced singular crease in the efficiency of >50% has been demonstrated. Tuesday, 19 Septem age Inst., A*STAR, Singapore; 3Dept. of Electronics and behavior and diffusive wave propagation are quantita- Photonics, Inst. of High Performance Computing, A*STAR, tively analyzed. JTu3A.113 • 13:50 RAPID Singapore. Photonic crystal waveguides (PhCWs) are Studies on nonlocal plasmonic resonances: analyt- realized on ultra-silicon-rich nitride platform which pos- JTu3A.85 • 13:30 RAPID ical and numerical approaches, Milan Burda1, Pavel sesses negligible nonlinear losses. An effective nonlinear Generation of optical vector beams using a single Kwiecien1, Ivan Richter1, Jan Fiala1; 1Czech Technical parameter of 1.97×104(Wm)-1 is estimated from self-phase spatial light modulator, Benjamin Perez-Garcia1, Carlos Univ. in Prague, Czech Republic. Both (quasi)analytical modulation on PhCW of length 96.6 µm. Lopez-Mariscal2, Raul I. Hernandez-Aranda1, Julio C. and numerical approaches describing the complexity of Gutiérrez-Vega1; 1Tecnologico de Monterrey, Mexico; nonlocal interactions at nanoscaled plasmonic structures JTu3A.42 • 13:10 RAPID 2Underwater Photonics, Mexico. We present an optical are investigated, in comparison with the standard linear Velocity-selective Saturated Spectroscopy with a Train scheme to produce vector beams. Our realization features response approximation. ber of Ultra-short Pulses and a Diode Laser, Alexis Carlos G. control over the local polarization state of the transverse Wong1, Alexandre Almeida1, Natalia R. de Melo2, Sandra coordinates. As an example, we investigate the genera- S. Vianna1; 1UFPE, Brazil; 2Escola politécnica, UPE, Brazil. tion of cylindrical vector vortex beams. A mode-locked 1 GHz femtosecond laser together with a diode laser is used to perform coherent spectroscopy of JTu3A.100 • 13:35 RAPID the D2 rubidium line. The results are well described using Three waveguide direction coupler based polarization the Bloch equations in the frequency domain picture. splitter under stimulated Raman adiabatic passage, Pragati Aashna1; 1Indian Inst. of Technology, Delhi, India. JTu3A.61 • 13:15 RAPID We propose the design of a polarization splitter based on Nonlinear Optical Properties of Chalcogenopy- stimulated Raman adiabatic passage (STIRAP) mechanism rylium-Terminated Heptamethine Dyes in Multiple in a three waveguide directional coupler. Polymer Hosts, Taylor G. Allen1, Yulia Getmanenko1,2, Hyeongue Kim1, Joel M. Hales1, Bhupinder Sandhu2, Marina S. Fonari2, Kyrill Y. Suponitsky2,3, Yadong Zhang1, Jonathan D. Matichak1, Victor N. Khrustalev2,4, Tatiana Timofeeva2, Stephen Barlow1, San-Hui Chi1, Joseph W. Perry1, Seth Marder1; 1Georgia Inst. of Technology, USA; 2Biology and Chemistry, New Mexico Highlands Univ., USA; 3A. N. Nesmeyanov Inst. of Organoelement Com- pounds, Russian Academy of Sciences, Russia; 4Peoples’ Friendship Univ. of Russia, Russia. Z-scan and linear loss measurements on polymethine-polymer blends with varied chalcogens and hosts confirm polymethine aggre- gation as the primary interaction influencing solid-state NLO properties for ultrafast all-optical signal-processing.

FiO + LS 2017 • 17–21 September 2017 45 Science & Industry Showcase

JOINT FiO + LS

13:00–15:00 JTu3A • Joint Poster Session II

JTu3A.1 E-Poster JTu3A.7 E-Poster JTu3A.14 Laser driven droplets generation and their optical Diffractals from regular polygon Sierpinski gaskets, Dark Solitons and Cnoidal Waves in Microresonators with Normal Dispersion, 1 delivery using a tapered hollow optical fiber for liquids Sean M. Nomoto1, Reeta Vyas1, Surendra Singh1; 1Univ. Zhen Qi , Giuseppe D’Aguan- 2 1 1 with a wide range of refractive indices, Hyeonwoo Lee1, of Arkansas, USA. Fraunhofer diffraction of a collimated no , Curtis Menyuk ; Univ. of Maryland Baltimore County, 2 Jinwon Yoo1, Jihyun Hwang1, Wonhyoung Ryu2, Kyung- Gaussian beam by fractal screens with regular polygon USA; Univ. of Texas at Austin, USA. We study dark solitons hwan Oh1; 1Inst. of Physics and Applied Physics, Yonsei Sierpinski gaskets up to fifth iteration was studied ex- and cnoidal waves in microresonators with normal disper- Univ., South Korea; 2Dept. of Mechanical Engineering, perimentally for 3–9 sided polygons and compared to sion. In the lossless case, we obtain analytical expressions Yonsei Univ., South Korea. Liquids of a wide range of theoretical results. for solitons and cnoidal waves. When loss is present, we refractive indices were atomized by a guided IR laser discuss accessibility of cnoidal waves. along a tapered hollow optical fiber with a nanometer JTu3A.8 E-Poster hole. Liquid droplet delivery by the light field was also Laser cooling investigation of a single-mode Yb- JTu3A.15 All-Fiber Passively Mode-Locked Ring Laser Based on experimentally investigated. doped ZBLAN optical fiber, Esmaeil Mobini1, Mostafa Normal Dispersion Active Tm-Doped Fiber, Peysokhan1, Behnam Abaie1, Arash Mafi1; 1Univ. of New Vasilii S. 1 1,2 1 JTu3A.2 E-Poster Mexico, USA. A theoretical study on laser cooling of a Voropaev , Alexander Donodin , Vladimir A. Lazarev , 1,2 1 Test Methods for Assessing Plasmonic Nanoparticle single-mode Yb3+:ZBLAN fiber is presented. Strategies Mikhail K. Tarabrin , Valerii E. Karasik , Alexander A. 3 1 Photodamage: Spectral Evaluation of Nanosphere to maximize the cooling efficiency are highlighted. The Krylov ; Science and Education Center for Photonics Reshaping, Andrew M. Fales1, William C. Vogt1, T. cooling scales quadratically with the core and inversely and IR-Technology, Bauman Moscow State Technical 2 Joshua Pfefer1, Ilko Ilev1; 1CDRH, FDA, USA. There is a with the cladding radius Univ., Russia; Frequency Standards Lab, P.~N.~Lebedev current lack of standardized test methods for evaluating Physical Inst. of the Russian Academy of Sciences, Russia; 3 pulsed laser-nanoparticle interaction damage thresholds. JTu3A.9 E-Poster Fiber Optics Research Center of the Russian Academy Photothermally-induced reshaping of 20-100 nm diam- Dynamic control of laser-induced flow-focused of Sciences, Russia. We demonstrate the generation of eter gold nanospheres was characterized, and damage microjets., Jan Krizek1, Paul Delrot1, Christophe Moser1; stable 210 fs pulses with 26 nm spectral width at a central thresholds determined. 1École Polytechnique Fédérale de Lausanne, Switzerland. wavelength of 1940 nm with 150 mW average output Laser-based actuation of liquid microjet relies on precise power and 11 MHz repetition rate. JTu3A.3 E-Poster localisation of the optical focus with respect to the liquid/ Growth and characterization of niobate laser crystals, air meniscus. We show the meniscus position control by JTu3A.16 High Harmonics Source for Probing Ultrafast Optical Shoujun Ding1,2; 1USTC, China; 2Chinese Academy of synchronisation of laser pulses with a dynamic settling Demagnetization in Multilayer Films, Sciences, China. In this work, the growth and characteri- of its position. Katherine K. 1 1 2 zation of a series of Nd-doped niobate laser crystals have Légaré , Vincent Cardin , Tadas Balciunas , François ber 1 1 2 been reviewed, including Nd:YNbO , Nd:GdNbO and JTu3A.10 E-Poster Légaré ; INRS, Centre EMT, Canada; Inst. of Photonics, 4 4 Vienna Univ. of Technology, Austria. We generate har- Nd:GdYNbO4. The excellent laser properties make them Reconfiguring structured light beams using nonlinear to be used in many fields. metasurfaces, Yun Xu1, Jingbo Sun1, Jesse Frantz2, monics in neon, reaching the cobalt M-edge absorption Mikhail Shalaev1, Jason D. Myers2, Robel Y. Bekele4, resonance. A pump-probe scheme then allows us to JTu3A.4 E-Poster Alexander Tsukernik3, Jasbinder S. Sanghera2, Natalia retrieve demagnetization curves by observing resonant Axial plane optical microscopy for particle manipula- M. Litchinitser1; 1Univ. at Buffalo SUNY, USA; 2US Naval X-ray magnetic scattering on a multilayer cobalt/plati- tion with Weber accelerating beams, Sha An1,2, Tong Research Lab, USA; 3Univ. of Toronto, Canada; 4Univ. num sample. Peng1, Guoxia Han1, Zhangxiang Huang1, Meirong Wang3, Research Foundation, USA. We show a nonlinear meta- Baoli Yao1, Peng Zhang1; 1State Key Lab of Transient surface made of nanostructured chalcogenide glass. We JTu3A.17 Low-power consumption dual-comb spectroscopy Optics and Photonics, Xi’an Inst. of Optics and Preci- combined on- and off-resonance nanostructures to realize

Tuesday, 19 Septem Tuesday, based on a battery-powered, free-running dual-comb sion Mechanics of Chinese Academy Sciences, China; reconfigurable structured light that switches between Her- laser system, 1 1 1 2Univ. of Chinese Academy Sciences, China; 3School of mit-Gaussian and vortex shape depending on its intensity. Jie Chen , Siyao Yin , Xin Zhao , Ruliu 1 1 1 1,2 Science, Northwestern Polytechnical Univ., China. We Wang , Yingling Pan , Jiansheng Liu , Zheng Zheng ; 1 directly observe the optical particle manipulation with JTu3A.11 School of Electronic and Information Engineering, Bei- 2 Weber accelerating beams by the axial plane optical Atmospheric Propagation Model and affecting on laser hang Univ. , China; Collaborative Innovation Center of microscopy (APOM). Optically trapped particles moving beam propagation via Free Space, Hussein T. Khamees1; Geospatial Technology, China. Dual-comb spectroscopy along parabolic trajectories are successfully monitored 1Electronic and Communication Engineering, Cankaya is demonstrated with an energy-efficient free-running by the APOM. Univ., Turkey. In this article, a laser source (He-Ne) laser fiber laser and the amplifiers. Avoiding feedback control with maximum output power ( 2.95 mW) was used to electronics, the dual-comb source consumes only a few JTu3A.5 E-Poster study and analyze laser beam when the laser propagates watts and runs on a mobile power pack for cell phones. Measurement of Kerr Coefficient in Large Bandgap through the atmosphere. Atmosphere layer, also the spot Solids at Mid-IR Wavelengths, Sina Zahedpour Anaraki1, diameter of the laser beam can be measured. JTu3A.18 Generation of circularly polarized high-order harmonics Jared K. Wahlstrand2, Howard Milchberg1; 1Univ. of Mary- in solids driven by single-color infrared pulses, land at College Park, USA; 2National Inst. of Standards JTu3A.12 Nicolai 1,2 1 1,2 and Technology , USA. We measure the Kerr coefficients Temporal measurement of the wave-breaking flash in Klemke , Giuseppe Di Sciacca , Yudong Yang , Giulio 1,2 1,2 for widely used solids in mid-IR applications. To our a laser plasma accelerator, Bo Miao1, Jared Wahlstrand1, M. Rossi , Roland E. Mainz , Nicolas Tancogne-De- 3,4 3,4 1,2 1,5 knowledge, this is the first direct absolute measurement Linus Feder1, Andy Goers1, George Hine1, Fatholah jean , Angel Rubio , Franz X. Kärtner , Oliver Mücke ; 1 for pump wavelengths longer than 800 nm. We observed Salehi1, Daniel C. Woodbury1, Howard Milchberg1; 1Inst. Center for Free-Electron Laser Science CFEL, Deutsches 2 insignificant dispersion in the measured n values. for Research in Electronics and Applied Physics, Univ. of Elektronen-Synchrotron DESY, Germany; Physics Dept., 2 3 Maryland, College Park, USA. Wave-breaking injection of Univ. of Hamburg, Germany; Max Planck Inst. for the 4 JTu3A.6 E-Poster electrons in a laser plasma accelerator generates intense Structure and Dynamics of Matter, Germany; European Pulse Train Generation in Fiber Lasers with Tunable broadband (Δ ≈300 nm) radiation flash. We study its Theoretical Spectroscopy Facility (ETSF), Germany; λ 5 Repetition Rate, Dmitry Korobko1, Andrei Fotiadi1,2, spectral coherence and measure its pulse length (~50 fs) The Hamburg Center for Ultrafast Imaging, Germany. Sergey G. Moiseev1, Igor O. Zolotovskii1; 1Ulyanovsk State with single-shot supercontinuum spectral interferometry. Intraband and interband dynamics generating high-order Univ, Russia; 2Univ. of Mons, Belgium. Simple approach harmonics in solids exhibit qualitatively different respons- was applied to analyze behavior of the harmonically JTu3A.13 es to driver-pulse ellipticity. TDDFT simulations and mode-locked fiber laser with adjustable Mach-Zehnder Analysis of Modulation Instability in Free-carrier experiments demonstrate circularly polarized harmonics interferometer. The model describes key features of the Driven Microring Resonator Based Kerr Frequency from single-color pulses. laser outputs at different repetition rates tuned over a Comb, Raktim Haldar1, Arkadev Roy1, Partha Mondal1, whole GHz range. Vishwatosh Mishra1, Shailendra K. Varshney1; 1Indian Inst. JTu3A.19 Rapid Frequency Comb Spectroscopy from 4.4 μm to of Technology Kharagpur, India. Analytical and numerical 4.7 μm using a Virtually Imaged Phased Array, studies on the dynamics of modulation-instability and Adam 1 1 Kerr-comb in free-carrier driven microring resonators are J. Fleisher ; NIST, USA. Rapid, precise, and sensitive multiplexed measurements of N O were performed us- reported through Lugiato-Lefever equation in presence 2 of multi-photon, free-carrier absorptions and dispersions. ing a mid-infrared frequency comb and virtually imaged phased array spectrometer. Multiplexed images covering >35 cm-1 were recorded in 500 μs.

46 FiO + LS 2017 • 17–21 September 2017 Science & Industry Showcase

JOINT FiO + LS

JTu3A • Joint Poster Session II—Continued

JTu3A.20 JTu3A.27 JTu3A.33

Broadband Cavity-enhanced Precision Molecular Detection of Janus Au-SiO2 Nanoparticles with a Optical and electrical control of valley polarized exci- Spectroscopy using Electro-optic Frequency Combs, Photothermal Technique, Maryam Zahedian1, Yan Yu1, ton polaritons in 2D materials, Zheng Sun1, Biswanath Adam J. Fleisher1, David Long1, Joseph Hodges1; 1NIST, Bogdan Dragnea1; 1Indiana Univ. Bloomington, USA. In Chakraborty2, Jie Gu1, Vinod M. Menon1; 1City Univ. of USA. We extend the tunable bandwidth of electro-optic this study, we explore the optical properties of Janus New York, USA; 2City College of New York, USA. We

frequency comb spectroscopy to >2 THz around λ = Au-SiO2 Nanoparticles that consist of silica deposited report the observation of optical and electrical-control 1.6 μm using an external cavity diode laser and report on a partial surface of Au nanospheres with the aid of of microcavity polaritons in 2D WS2 embedded in mi-

precision spectroscopy of CO2, H2O, and N2O. photothermal microscopy. crocavity. Optical control of polariton states show their distinct valley origin and the electrical control shows the JTu3A.21 JTu3A.28 spectral tuning. Topological properties of graphene on a nanowire Laser Induced Fluorescence Spectroscopy in Dyspro- superlattice subjected to ultrafast circular pulses, sium Atomic Vapor, Jhonatha Ricardo2,1, Jonas Jakutis JTu3A.34 Hamed Koochaki Kelardeh1,2, Vadym Apalkov1,2, Mark Neto2, José W. Neri2, Patricia Bueno2,1, Marcelo G. De- The effect of Laser Induced Periodic Surface Structures Stockman1,2; 1Georgia State Univ., USA; 2Center for stro2; 1Instituto Tecnológico da Aeronáutica ITA, Brazil; on Wear and Friction Coefficient, Hasnaa Meliani2,1, Nano-Optics, USA. We manifest the topological nature 2Photonics, Instituto de Estudos Avançados, Brazil. This Mohamed Assoul2, Michaël Fontaine3, Guy Monteil3, of graphene without a magnetic field. Graphene under paper presents the observation of the isotopes 162Dy, Vahan Malkhasyan1; 1Femto-st, France; 2Univ. Bourgogne a few-cycle circularly polarized optical field and coupled 163Dy and 164Dy of the dysprosium optical transition Franche-Comté, France; 3ENSMM, France. The influence to a nanowire superlattice allows for observing the Berry 0→16717.79 cm-1 .The high-resolution spectra were ob- of laser surface texturing on tribological properties of phase in the excitation distribution. tained through the laser induced fluorescence technique stainless steel was studied. Linear Reciprocating Tri- in atomic vapor. bometer (LRT) was used to observe evolution of friction JTu3A.22 coefficient and wear versus number of cycles performed. Synchronous All-Optical Buffer-cum-Logic Gates In JTu3A.29 Dual-Pump Kerr Microring Resonators, Arkadev Roy1, Observation of Third Harmonic Enhancement Due to JTu3A.35 Raktim Haldar1, Shailendra K. Varshney1; 1Indian Inst. Tunneling at a Metal-Insulator-Metal Junction, Mallik Enhanced optical nonlinearities in ultra-silicon-rich of Technology Kharagpur, India. We report robust and Mohd Raihan Hussain1, Zhengning Gao2, Domenico de photonic crystal waveguides, Ezgi Sahin1,3, Kelvin J. synchronous all-optical buffer in dual-pumped microring Ceglia3, Maria Vinceti4, Andrew Sarangan1, Imad Agha1, Ooi1, George F. R. Chen1, Doris K. T. Ng2, Ching Eng resonators by leveraging temporal cavity solitons. The Michael Scalora5, Parag Banergee2,6, Joseph W. Haus1; Png3, Dawn T. H. Tan1; 1Photonics Devices and Systems proposed scheme can also be employed to carryout 1Dept. of Electro-Optics and Photonics, Univ. of Dayton, Group, Engineering Product Development, Singapore Tuesday, 19 Septem logical operations. USA; 2Inst. of Materials Science and Engineering, Wash- Univ. of Technology and Design, Singapore; 2Data Stor- ington Univ., USA; 3AEgis Technologies Group Inc., USA; age Inst., A*STAR, Singapore; 3Dept. of Electronics and JTu3A.23 4Dept. of Information Engineering, Univ. of Brescia, Italy; Photonics, Inst. of High Performance Computing, A*STAR, Topological phase transitions in the photonic spin Hall 5Charles M. Bowden Research Lab, US Army AMRDEC, Singapore. Photonic crystal waveguides (PhCWs) are effect, Wilton Kort-Kamp1; 1Los Alamos National Lab, USA; 6Dept. of Mechanical Engineering & Materials realized on ultra-silicon-rich nitride platform which pos- USA. We unveil topological phase transitions in the spin Science, Washington Univ., USA. We experimentally ob- sesses negligible nonlinear losses. An effective nonlinear Hall effect of light in the graphene family materials and served an enhancement of the third harmonic (TH) signal parameter of 1.97×104(Wm)-1 is estimated from self-phase show that spinoptics provides a unprecedented pathway at Au/Al2O3/Au interfaces. The TH signal behavior with modulation on PhCW of length 96.6 µm. to investigate spintronics and valleytronics in two-dimen- surface coverage qualitatively resembles the quantum

sional semiconductors. tunneling predictions. JTu3A.36 ber Strong-Field Ionization Modified by Optical and JTu3A.24 JTu3A.30 Quantum Interferences, David B. Foote1, Yingda Implications of Self-Steepening on Temporal Tweezing Enhancement of Electromagnetically-Induced Focusing Lin1, Kevin Lehr1, Zhenqian Jian1, Wendell T. Hill1, Jean of Light in Optical Buffer Applications, Arkadev Roy1, by a Microwave Field, Onkar N. Verma1, Sourabh Roy1; Marcel N. Djiokap2, Liang-Wen Pi2, Anthony F. Starace2; Raktim Haldar1, Shailendra K. Varshney1; 1Indian Inst. of 1Dept. of Physics, National Inst. of Technology Warangal, 1Univ. of Maryland, USA; 2Univ. of Nebraska, USA. We Technology Kharagpur, India. We numerically explore India. We have theoretically studied the effect of a mi- measure Xe+ and electron yields after ionization from the impact of self-steepening on temporal tweezing of crowave field on electromagnetically-induced focusing of twin-peaked pulses. The ionization spectra show periodic light while manipulating temporal cavity solitons. Differ- a weak probe beam due to spatial variations of control modulation indicating interference. Small features of the ences observed in transient and steady state behavior beam in an electromagnetically-induced transparency pulse substantially change the optical interference and establishes the importance of self-steeping in this regard. medium. ion/electron yields.

JTu3A.25 JTu3A.31 JTu3A.37 Light Emission Enhancement of 2D Materials in Mid-Infrared Pump-Probe Measurements of Carrier Withdrawn. Monomer vs. Dimer Nanoantennae, Mohammad H. Dynamics in Black Phosphorus, Yigit Aytac1, Martin Tahersima1, Muhammad Danang Birowosuto2, Zhizhen Mittendorff1, Thomas E. Murphy1; 1Univ. of Maryland, USA. JTu3A.38 Ma1, William C. Coley3, Michael Valentin3, Sahar Naghibi Time-resolved transmission measurements are employed Inherent Limitations in Mid-Wave and Long-Wave-IR Alvillar3, Cesare Soci2, Ludwig Bartels3, Volker J. Sorger1; to probe the carrier dynamics in black phosphorus. Mea- Upconversion Detector, Ajanta Barh1, Yu-Pei Tseng1, 1The George Washington Univ., USA; 2Nanyang Techno- surements at mid-IR wavelengths near the bandgap show Christian Pedersen1, Peter Tidemand-Lichtenberg1; logical Univ., Singapore; 3Univ. of California Riverside, saturable absorption attributed to Pauli blocking and a 1Technical Univ. of Denmark (DTU), Denmark. Inherent USA. We show that the emission enhancement from a fluence-dependent recombination. limitations in terms of optical losses, selection of nonlinear TMD emitter- monomer antenna cavity system rivals that crystal(s), detection efficiency and pumping conditions of dimers at much reduced lithographic effort. JTu3A.32 in mid-wave (3-5 µm) and long-wave (8-12 µm) infrared Application of adiabatic following to three specific frequency upconversion modules are investigated in JTu3A.26 three-sate quantum system, Wei Huang1, Bruce Shore2, this paper. High-NA Aberration-Corrected Raman Analysis of Andon Rangelov3, Elica Kyoseva2; 1Singapore Univ. of Femtosecond Bessel Beam Modification in Diamond, Technology and D, Singapore; 2retire, USA; 3Sofia Univ., Brian K. Canfield1, Lloyd M. Davis1; 1Univ. of Tennessee James Bourchier, Bulgaria. We propose an adiabatic Space Inst., USA. We report femtosecond Bessel beam following for a Vee, a Ladder and a Lambda quantum laser processing of diamond with high-NA aberration-cor- system. We illustrate different possibilities for population rected Raman analysis in order to create improved arrays transfer in these multi-level quantum systems. of micron diameter columnar graphitized electrodes for use in advanced high-energy particle detectors.

FiO + LS 2017 • 17–21 September 2017 47 Science & Industry Showcase

JOINT FiO + LS

JTu3A • Joint Poster Session II—Continued

JTu3A.39 JTu3A.46 JTu3A.53 Bragg-induced Rabi Oscillations in Periodic Photonic Low Jitter Measurement of Laser Linewidth using Polarization Properties of White-Light Continuum due

Structures With $\mathcal{PT}$ Symmetry, Paulo A. Brillouin Induced Self-Heterodyne Method., Arpita to a Single Femtosecond Filament in YVO4 Crystal, Brandão1, Solange B. Cavalcanti1; 1Instituto de Física, Sinha Roy1; 1IIT Kanpur, India. We mathematically analyse Chinmoy Biswas1, Maruthi M. Brundavanam1; 1Indian Inst. Universidade Federal de Alagoas, Brazil. We study optical and experimentally measure the linewidth of a DFB laser of Technology Kharagpur, India. Polarization properties Rabi-like oscillations between a pair of resonant Bragg using Brillouin induced self-heterodyne method. We show of white-light continuum due to a single femtosecond

modes in a linear $\mathcal{PT}$ symmetric periodic that Brillouin induced self-heterodyne method reduces filament inside a YVO4 crystal are investigated at different photonic structure by analytically solving the paraxial the jitter effect as compared to self-heterodyne method. input laser powers. The results show the depolarization wave equation. of the white-light continuum at high powers. JTu3A.47 JTu3A.40 Ultrafast carrier dynamics in wide bandgap semi- JTu3A.54 Aberrated Soliton Forming at Femtosecond Pulse conductor materials, Roderick B. Davidson2, Adam D. Conical third-harmonic generation in a 2D periodical- Propagation in Cubic Nonlinear Medium with Inho- Dunkelberger1, Ioannis Chatzakis2, Brad Pate1, Joshua ly-poled crystal, XinYuan Fang1, Yong Zhang1; 1Nanjing mogeneous Refraction Index, V. A. Trofimov1, Alexei Caldwell1, Jeffrey Owrutsky1; 1Naval Research Lab, USA; Univ., China. We have experimentally demonstrated A. Kalinovich1, Irina G. Zakharova1; 1M. V. Lomonosov 2 National Research Council, USA. Free-carrier relaxation conical third-harmonic generation in a two dimensional

Moscow State Univ., Russia. We demonstrate a possibility dynamics in several unique wide bandgap materials is periodically poled LiTaO3 crystal, which was attributed to of the formation of a new soliton type, named as chirped characterized by pump-probe spectroscopy. Lifetimes cascaded quasi-phase-matching processes assisted by or aberrated soliton. Such solitons arise at optical pulse are observed from ten to hundreds of picoseconds in scattering fundamental waves in the crystal. propagation in a nonlinear layered structure situated in aluminum nitride, polymorphic diamond, and hexagonal a cubic nonlinear medium. boron nitride. JTu3A.55 Chemical vapor sensing in photonic crystal slabs, JTu3A.41 JTu3A.48 Yonghao Liu1, Priyanka Biswas1, Weidong Zhou1, Yuze Femtosecond Laser-induced Dual Periodic Structures X-ray Photoelectron Spectroscopy Analysis of Surface Sun1; 1Univ. of Texas at Arlington, USA. We report here on Ni, Hyun Uk Lim1,4, Jeongjin Kang1, Chunlei Guo2,3, Segregation in Bimetallic Nanoalloy, Justyna Piwowar1, chemical vapor sensing in free-space coupled defect-free Taek Yong Hwang1; 1Molds & Dies R&D group, Korea Inst. Adam Lewera1; 1Faculty of Chemistry, Univ. of Warsaw, photonic crystal slabs. It shows a quality factor of 6,890 of Industrial Technology, South Korea; 2The Inst. of Optics, Poland. The surface composition of a heterogeneous and a sensitivity of 1.76x10-2 pm/ppm for hexane, with a Univ. of Rochester, USA; 3The Guo China-US Photonics catalyst determines its properties. This presentation will detection limit of 57 ppm. Lab, Changchun Inst. of Optics, Fine Mechanics, and demonstrate that X-ray Photoelectron Spectroscopy Physics, China; 4Mechanical Engineering, Dankook Univ., innovative analysis in an efficient way of studying surface JTu3A.56 South Korea. Under femtosecond laser pulse irradiation segregation. Nonlinear Pulse Compressor on Silicon Slot Hybrid ber at off normal incidence, we create nanostructure-covered Optical Waveguide, Nishit Malviya1, Vishnu Priye1; 1IIT laser-induced dual periodic surface structures on Ni. JTu3A.49 (ISM) Dhanbad, India. Theoretical investigation of pulse Mechanisms of the structure formation will be discussed Metal-enhanced lasing from zinc-doped GaAs nanow- compression in slot optical waveguide based on non- in this work. ires, Fatemesadat Mohammadi1, Mykhaylo Lysevych2, linear organic material PTS is presented. Results depict Hoe Tan2, Chennupati Jagadish2, Hans Peter Wagner1; compression of pulse from 1ps to 0.59ps in propagation JTu3A.42 1Dept. of Physics, Univ. of Cincinnati, USA; 2Dept. of range of 20 cm at 1550 nm Velocity-selective Saturated Spectroscopy with a Train Electronic Materials Engineering, Research school of of Ultra-short Pulses and a Diode Laser, Alexis Carlos G. Physics and Engineering, Australia. We observe enhanced JTu3A.57 Wong1, Alexandre Almeida1, Natalia R. de Melo2, Sandra optically excited lasing and decreased lasing threshold A Dynamical Perspective on Noise in Passively Mod- S. Vianna1; 1UFPE, Brazil; 2Escola politécnica, UPE, Brazil. in Zn doped GaAs laid on gold and silver films. The en- elocked Lasers, Curtis Menyuk1, Shaokang Wang1, Thom- 1 1

Tuesday, 19 Septem Tuesday, A mode-locked 1 GHz femtosecond laser together with a hancement is attributed to energy transfer between the as Carruthers ; Univ. of Maryland, Baltimore County, USA. diode laser is used to perform coherent spectroscopy of stimulated emission in the NWs and surface plasmons We show how to use dynamical methods to calculate the

the D2 rubidium line. The results are well described using in the metal. impact of noise on the timing jitter and power spectral the Bloch equations in the frequency domain picture. density of passively modelocked lasers without using JTu3A.50 computationally expensive Monte Carlo simulations. JTu3A.43 Significant Enhancement of Magneto-Optical Rotation Preliminary Investigation On Selective Laser Melting in a Low-Light Resonant Tripod System, Eric Y. Zhu1, JTu3A.58 Of 17-4PH Steel Using High laser Powers Of up to Feng Zhou1, Edward W. Hagley2, Lu Deng1; 1Quantum Realization of S-type and N-type Hysteresis Loops at 1500W, Nkutwane Washington Makoana1,2, Heinrich Measurement Division, National Inst. of Standards and Femtosecond Laser Pulse Action in Semiconductor, V. Moller1, Danie Louw1, Igor Yadroitsev2; 1Council for Sci- Technology, USA; 2Sensor Science Division, National Inst. A. Trofimov1, Mariya M. Loginova1, Vladimir A. Egoren- entific and Industrial Research, South Africa; 2Mechanical of Standards and Technology, USA. The magneto-optical kov1; 1M. V. Lomonosov Moscow State Univ., Russia. Using Engineering, Central Univ. of Technology, South Africa. rotation experienced by a resonant probe field in an am- computer simulation, we showed a possibility of simulta- High laser powers of up to 1500W were used to additively bient-temperature atomic vapor is enhanced more than neous existence of S- type and N-type hysteresis loops manufacture 17-4PH samples. Porosity was measured ten-fold when a secondary low-intensity optical field is at femtosecond pulse interaction with a semiconductor. using the image analysis technique, and all samples are introduced, forming an atomic tripod system. fairly dense with a maximum of 0.42 percent porosity. JTu3A.59 JTu3A.51 Nonlinear self-channeling of laser pulses through JTu3A.44 Linear and Nonlinear Optical Properties of Organic distributed atmospheric turbulence, Michael H. Helle1, Liquid Crystal Elastomers (LCEs) Dynamics in Response Cavity Polaritons in the Ultrastrong Regime, Bin Liu1, Gregory DiComo1, John Palastro1, Joseph Penano1, to Visible Light Illumination, Vahideh Abdolazimi1, Adam Michael Crescimanno2, Kenneth Singer1; 1Case Western Jennifer Elle2, Andreas Schmitt-Sody2; 1Naval Research Fontecchio2,3; 1Electrical and Computer Engineering, Reserve Univ., USA; 2Youngstown State Univ., USA. Lab, USA; 2U.S. Air Force Research Lab, USA. We present Drexel Univ., USA; 2Vice Dean, Graduate College, Drexel We demonstrate coupling between two ultrastrong experimental evidence of a new propagation paradigm Univ., USA; 3Professor of Electrical and Computer Engi- exciton-photon coupled low-Q organic microcavities where a laser pulse, near the self-focusing power of air neering, Drexel Univ., USA. Liquid crystal elastomers are at room temperature. We also experimentally observe with a spot size smaller than the coherence diameter of elastic materials that deform by illumination. The LCE cavity-polariton enhanced third harmonic generation in turbulence, self-channels over hundreds of meters. film dynamics under different visible light frequencies single exciton-photon coupled microcavities. is simulated. The results illustrate rapid deformations at higher frequencies with greater resultant forces. JTu3A.52 Analytical Expression for Z-scan Curves in Solely JTu3A.45 Refractive Nonlocal Thick Media, Roman Torres1, M. Bound Electron Nonlinearity Beyond the Ionization Maribel Méndez Otero1, M. Luis Arroyo Carrasco1, E. Threshold, Jared K. Wahlstrand1,2, Sina Zahedpour2, Reynoso Lara1, M. David Iturbe Castillo2; 1BUAP, Mexico; Howard Milchberg2; 1NIST, USA; 2Univ. of Maryland, USA. 2Optics, INAOE, Mexico. Z-scan curves in thick nonlinear We measure the residual bound electron nonlinear po- nonlocal media are analytically calculated by considering larizability well above the ionization threshold in a range the sample as a stack of thin slices without coupling of of gases, and find that it scales approximately linearly nonlinearities between them. Obtained results are com- with laser intensity. pared with previously reported in literature.

48 FiO + LS 2017 • 17–21 September 2017 Science & Industry Showcase

JOINT FiO + LS

JTu3A • Joint Poster Session II—Continued

JTu3A.60 JTu3A.66 JTu3A.73 Experimental Study on the Relationship Between Frequency downshifting of perturbed dissipative Withdrawn. the Polarizability and Non-Linear Refractive Index in solitons: A variational approach, Ambaresh Sahoo1, Hydrocarbons, Sebastian Vergara Palacio1, Carlos A. Samudra Roy1, Govind P. Agrawal2; 1Indian Inst. of JTu3A.74 Rodriguez Ortiz2,1, Raul E. Jimenez Mejia1, Rodrigo Acu- Technology Kharagpur, India; 2The Inst. of Optics, Univ. Broadband pulse generation from a low-power, na Herrera1, Carlos Andres Alvarez Ocampo1,2; 1Escuela of Rochester, USA. We develop a variational approach carbon-nanotube mode-locked fiber laser, Ting Li1, de Fisica, Universidad Nacional de Colombia-Medellin, to study the Raman-induced frequency downshift of Guoqing Hu1, Jie Chen1, Zhi Qiao1, Xin Zhao1, Zheng Colombia; 2Ciencias Basicas, Universidad de Medellin, dissipative solitons whose evolution is governed by a Zheng1,2; 1School of Electronic and Information Engi- Colombia. Theoretical and experimental characterization complex Ginzburg-Landau equation. We derive a set of neering, Beihang Univ. , China; 2Collaborative Innovation of non-linear refractive index of Hydrocarbons dyes is coupled differential equations that explain the dynamics. Center of Geospatial Technology, China. Using a simple presented by using the free electron model. An empirical dispersion-managed ring cavity, 48-nm wide pulses linear relationship between nonlinear and linear refractive JTu3A.67 are generated at a low intra-cavity pulse energy of 23 index was found. High Order Harmonic Generation in ZnSe Driven by 3 picojoules under small normal dispersion, facilitated by μm Parametric Laser Source at High Repetition Rate, a polarization spectral filtering mechanism. JTu3A.61 Giedre M. Archipovaite1, Stéphane Petit1, Jean-Christo- Nonlinear Optical Properties of Chalcogenopy- phe Delagnes1, Eric Cormier1; 1CELIA, France. We present JTu3A.75 rylium-Terminated Heptamethine Dyes in Multiple an ultrashort high-power 3μm laser source based on Tunable Cavity Fiber-Optic Fabry-Perot Magnetometer Polymer Hosts, Taylor G. Allen1, Yulia Getmanenko1,2, optical parametric amplification. The source provides a Based on Fiber-Cantilever Beam-Deflection, Somarpita Hyeongue Kim1, Joel M. Hales1, Bhupinder Sandhu2, promising tool for strong field experiments in solids and Pradhan1, Samik Saha1, Partha Roy Chaudhuri1; 1Indian Marina S. Fonari2, Kyrill Y. Suponitsky2,3, Yadong Zhang1, high-order harmonics have been generated in ZnSe. Inst. of Technology Kharagpur, India. We devised a Jonathan D. Matichak1, Victor N. Khrustalev2,4, Tatiana tunable cavity fiber Fabry-Perot magnetometer using Timofeeva2, Stephen Barlow1, San-Hui Chi1, Joseph W. JTu3A.68 deflection of cobalt-doped nickel ferrite coated optical Perry1, Seth Marder1; 1Georgia Inst. of Technology, USA; Highly Sensitive Ammonia Gas Detection with a Silica fiber cantilever. Sensitivity is improved by introducing a 2Biology and Chemistry, New Mexico Highlands Univ., Toroid Microcavity Packaged in a Box, Taku Okamura1, silver coated fiber-mirror in the developed configuration USA; 3A. N. Nesmeyanov Inst. of Organoelement Com- Misako Kobayashi1, Shun Fujii1, Takasumi Tanabe1; 1Keio pounds, Russian Academy of Sciences, Russia; 4Peoples’ Univ., Japan. We demonstrate highly sensitive and prac- JTu3A.76

Friendship Univ. of Russia, Russia. Z-scan and linear loss tical ammonia gas (NH3) detection with a packaged silica Coherent Combination and Self-similar Compression measurements on polymethine-polymer blends with toroid microcavity. We report our experimental results and of Two RC Pulses with Different Pulse Widths, Ziyun 1 1 1 1 varied chalcogens and hosts confirm polymethine aggre- achieve a detection sensitivity of 0.43 nm/ppm. Jian , Guangkuo Li , Qian Li ; Peking Univ., China. Two Tuesday, 19 Septem gation as the primary interaction influencing solid-state raised cosine pulses with different initial pulse widths NLO properties for ultrafast all-optical signal-processing. JTu3A.69 firstly coalesce into a single pulse and then experience Narrowband Tunable Thz Generation in Orientation self-similar compression. JTu3A.62 Patterned Gallium Phosphide, Patrick Tekavec1, Vladimir Simple Diagnostics of Femtosecond Pulses by the Use Kozlov1, Peter Schunemann2; 1Microtech Instruments, JTu3A.77 of Nanosecond Oscilloscope, Karapet Manukyan1, Minas USA; 2BAE Systems, USA. We demonstrate tunable, The Impact of Laser Beam Polarization on Small-Scale Sukiasyan1,2, Hrach Toneyan1,2, Aram Zeytunyan3, Levon narrowband THz generation by optical rectification of Self-Focusing in Isotropic Crystals, Anton Kochetkov1, Mouradian1,2; 1Yerevan State Univ., Armenia; 2CANDLE a femtosecond pulse in orientation patterned Gallium Vlad Ginzburg1, Maryana Kuz’mina1, Efim Khazanov1; Synchrotron Research Inst., Armenia; 3Technology and Phosphide. Center frequencies from 0.9 – 3.8 THz with 1IAP RAS, Russia. Direct measurements of spatial noise

Applications Center, Newport Corporation, USA. We de- average power up to 15 μW were obtained. gain in a wave propagating in [001]-orientated BaF2 were ber termine the duration of femtosecond pulses by coupling performed. Significant dependence of gain on the angle them into a passive fiber, generating the nanosecond JTu3A.70 between the radiation polarization and the crystallograph- duration nonlinear-dispersive similaritons and recording Spectral Broadening of a High Average Power Yb:K- ic axis predicted earlier was demonstrated. them by an oscilloscope. This diagnostics has real-time GW Laser, John E. Beetar1, Shima Gholam-Mirzaei1, performance. Sean Buczek1, Steven Solis1, Michael Chini1; 1UCF, USA. JTu3A.78 Broadening and compression efficiency of high average Time-Evolving Single-Shot Imaging of Laser-Produced JTu3A.63 power NIR pulses from a Yb:KGW laser amplifier, under- Plasmas by Spatial Division, Sarang Yeola1, Donghoon Withdrawn. going self-phase modulation in a series of thin fused silica Kuk1, Ki-Yong Kim1; 1Univ. of Maryland at College plates, is investigated through spatial characterization of Park, USA. We have developed an ultrafast single-shot JTu3A.64 spectrum and power. pump-probe technique which uses spatially- and tem- Airy Wavepackets Accelerating Only in the Spatio-Tem- porally-separated multiple probe pulses to capture four poral Domain, Hasan E. Kondakci1, Ayman Abouraddy1; JTu3A.71 frames of laser-induced plasmas at ~10 trillion frames 1CREOL, Univ. of Central Florida, USA. We experimentally Efficient Production of Picosecond 9-11 µm Pulses by per second (fps). demonstrate Airy wavepackets accelerating only in the Parametric Three Wave Mixing in GaSe, Eric C. Welch1, spatio-temporal domain of the localized pulse produced Sergei Tochitsky1, Chandrashekhar Joshi1; 1Electrical JTu3A.79 via a two-dimensional pulse shaper. When observed with Engineering, UCLA, USA. Generation of picosecond, Interband absorption of topologically structured pho- a slow detector, the Airy wavepacket does not accelerate. 5 µJ, 10 µm pulses by parametric three wave mixing in ton beams by semiconducting quantum dots, Maria GaSe is demonstrated. Two new methods are explored Solyanik1, Andrei Afanasev1; 1The George Washington JTu3A.65 in which the nonlinear interaction is seeded by either the Univ., USA. Interaction of topological photon beams Single-shot, Axially Resolved Measurements of Fem- signal or idler waves. with semiconducting quantum dots is described in QED tosecond Filament Energy Deposition over 10 Meter formalism. Absorption rates are calculated, and distinctive Scales, Ilia Larkin1, Eric Rosenthal1, Nihal Jhajj1, Howard JTu3A.72 features arising due to the wavefront topology, such as Milchberg1; 1Univ. of Maryland, USA. The axial energy Geometric parametric instability of femtosecond modified selection rules, are discussed. deposition profile of an extended femtosecond filament pulses in graded-index multimode fiber, Uğur Tegin1,2, is captured in a single shot over a >10 m propagation Bülend Ortaç1,2; 1Inst. of Materials Science and Nano- JTu3A.80 distance by an array of synchronized microphones. technology, Bilkent Universitesi, Turkey; 2National Nan- Withdrawn. otechnology Research Center, Bilkent Univ., Turkey. We experimentally study the spatio-temporal femtosecond JTu3A.81 pulse evolution in graded-index multimode fiber at nor- Diffusive Dynamics and Signature of Phase Singularities mal dispersion regime. We report the first demonstration in Gain/Loss Assisted Disordered Optical Waveguide of geometric parametric instability with ultrashort pulses Lattices, Somnath Ghosh1, Ravi K Varshney3, Bishnu P. in the literature. Pal2; 1Indian Inst. of Technology Jodhpur, India; 2MEC Hyderbad, India; 3Indian Inst. of Technology Delhi, India. Co-existence and interplay between mesoscopic light dynamics with singular optics in spatially disordered waveguide lattices is reported. Disorder induced singular behavior and diffusive wave propagation are quantitatively analyzed.

FiO + LS 2017 • 17–21 September 2017 49 Science & Industry Showcase

JOINT FiO + LS

JTu3A • Joint Poster Session II—Continued

JTu3A.82 JTu3A.89 JTu3A.95 Evolution of an Optical Vortex on the Morphology Superfluidicity in an Optical Lattice with a PT Sym- Radiation Pressure on a Transmissive Diffraction Grat- Sphere by Control of Fractional Charge of the Dislo- metric Defect, Lingxuan Zhang1,2, Wenfu Zhang2, Li ing, Ying-Ju Chu1, Grover A. Swartzlander1; 1Rochester cation, Satyajit Maji1, Maruthi M. Brundavanam1; 1Indian Ge1; 1College of Staten Island, CUNY, USA; 2Xi’an Inst. Inst. of Technology, USA. Diffraction films afford advantag- Inst. of Technology Kharagpur, India. Evolution of the of Optics and Precision Mechanics, China. We consider es over reflective films for applications like solar sailing. morphology parameters associated with the anisotropic a nonlinear waveguide array with a PT symmetric defect Our torsion pendulum demonstrated radiation pressure vortex phases of generated non-canonical optical vor- at the center of a parabolic potential. The oscillations of on a thin transmissive Littrow grating. A significant tan- tices is demonstrated in experiment and simulation by a coherent state persist without dissipation, if its velocity gential force was observed. changing fractional charge of the dislocation and input is below a critical value. beam curvature. JTu3A.96 JTu3A.90 Nonlinear Interaction of Ultrafast Hollow Gaussian JTu3A.83 Evolutionary Optimization of Nondiffracting Helicon Beams, Amrit Chaitanya1, Apurv Chaitanya Nellikka2, J Optimization of a Birefringent Mask for Generating Beams, Bryce Schroeder1, Zhen H. Zhu1, Changliang Banerji2, Goutam K Samanta2; 1Pondicherry Univ., India; Optical Bottle Fields, Anthony Vella2, Hippolyte Dour- Guo1, Shu Jia1; 1Stony Brook Univ., SUNY, USA. We op- 2Physical Research Lab, India. We report on frequen- dent1, Lukas Novotny1, Miguel A. Alonso2; 1Photonics timized helicon-like beams in a high resolution imaging cy-doubling of ultrafast hollow Gaussian beam (HGB) Lab, ETH Zürich, Switzerland; 2The Inst. of Optics, Univ. sytem with an evolutionary algorithm, achieving a tight in the green with HGB order as high as six and power of Rochester, USA. We optimize the spatial variation of a intensity profile while largely maintaining self-rotation and >250 mW. We observed doubling of the order of HGB birefringent mask, placed in a high-NA focusing system, nondiffraction. The method promises wide applicability in frequency-doubling process. to generate a bottle field with minimal volume. The in beam design. optimal birefringence distribution is nearly identical to a JTu3A.97 stress-engineered optical element. JTu3A.91 Withdrawn. Polarization Singularities due to Unfolding of Frac- JTu3A.84 tional Vortex Beams in a Birefringent Crystal, Aswini JTu3A.98 Confined bases: from paraxial to electromagnetic, K. Pattanayak1, Satyajit Maji1, Maruthi M. Brundavanam1; Frequency shift in three-photon resonant four-wave Rodrigo Gutiérrez-Cuevas1, Miguel A. Alonso1; 1Univ. 1Indian Inst. Of Technology Kharagpur, India. The evo- mixing due atom-field interaction, Natalia R. de Melo1, of Rochester, USA. We present novel discrete bases for lution of polarization singularities due to unfolding of Sandra S. Vianna2; 1Universidade de Pernambuco, Bra- optical fields with the distinct property of being confined. optical vortex beams with topological charges varying zil; 2Departamento de Física, Universidade Federal de This delivers interesting properties like order-independent from 0 to 1 in fractional steps is investigated at the output Pernambuco, Brazil. We investigate Frequency shift in fits and simple description of fields with varying degrees of a birefringent crystal. three-photon resonant four-wave mixing in rubidium of focusing. vapor. The results are consistent with theoretical model ber JTu3A.92 based on semiclassical Maxwell-Bloch equations con- JTu3A.85 Effect of Astigmatism on Intensity Speckle Pattern, sidering the generated radiation field self-consistently. Generation of optical vector beams using a single Abhijit Roy1, Maruthi M. Brundavanam1; 1Indian Inst. of spatial light modulator, Benjamin Perez-Garcia1, Carlos Technology Kharagpur, India. Effect of astigmatism on JTu3A.99 Lopez-Mariscal2, Raul I. Hernandez-Aranda1, Julio C. intensity speckle pattern, generated using a ground glass Influence of silver concentration on the locality of Gutiérrez-Vega1; 1Tecnologico de Monterrey, Mexico; plate, is investigated experimentally exploiting angular nonlinear response in colloidal Ag nanocubes, Emma V. 2Underwater Photonics, Mexico. We present an optical memory effect for different amounts of astigmatism intro- García Ramírez1, Daysi Ramírez Martínez1, Sergio sabinas scheme to produce vector beams. Our realization features duced by rotating a lens at different angles. Hernandez1, Gabriela Díaz Guerrero1, Alejandro Reyes control over the local polarization state of the transverse esqueda1; 1Univ Nacional Autonoma de Mexico, Mexico. coordinates. As an example, we investigate the genera- JTu3A.93 Colloidal Ag nanocubes systems with particle sizes of 99

Tuesday, 19 Septem Tuesday, tion of cylindrical vector vortex beams. A Second Harmonic Technique to Determine Metal-In- and 215 nm and different volume fraction were analyzed duced-Gap-State Density, Mallik Mohd Raihan Hussain1, by Z-scan technique. Changes in the spatial nonlocality JTu3A.86 Zhengning Gao2, Domenico de Ceglia3, Maria Vinceti4, of their third order nonlinear response were observed. Transformation of Complex Spatial Coherence Function Andrew Sarangan1, Imad Agha1, Michael Scalora5, Parag in Reflection from Random Media, Mahed Batarseh1, Banergee2,6, Joseph W. Haus1; 1Dept. of Electro-Optics JTu3A.100 Zhean Shen1, Roxana Rezvani Naraghi1,2, Heath E. Ge- and Photonics, Univ. of Dayton, USA; 2Inst. of Materials Three waveguide direction coupler based polarization mar1, Sergey Sukhov1, Aristide Dogariu1; 1CREOL, The Science and Engineering, Washington Univ., USA; 3AEgis splitter under stimulated Raman adiabatic passage, College of Optics and Photonics, Univ. of Central Florida, Technologies Group Inc., USA; 4Dept. of Information En- Pragati Aashna1; 1Indian Inst. of Technology, Delhi, India. USA; 2Dept. of Physics, Univ. of Central Florida, USA. gineering, Univ. of Brescia, Italy; 5Charles M. Bowden Re- We propose the design of a polarization splitter based on We investigate both experimentally and numerically the search Lab, US Army AMRDEC, USA; 6Dept. of Mechanical stimulated Raman adiabatic passage (STIRAP) mechanism transformation of the spatial coherence function (SCF) Engineering & Materials Science, Washington Univ., USA. in a three waveguide directional coupler. reflected from media with both surface and volume We experimentally determine the metal-induced-gap-

scattering, and demonstrate the conditions for the SCF state (MIGS) density at Au/Al2O3 interfaces by applying JTu3A.101 survivability during scattering. a sensitive second harmonic generation (SHG) technique. Analysis of Markovian modes and their applications on 1 We measure SHG efficiencies at these interfaces for Al2O3 holography, Carina Gutiérrez Ojeda , Patricia Martinez JTu3A.87 films of nanometer thickness. Vara2, Gabriel Martinez Niconoff1; 1Instituto Nacional de 2 Azimuthal asymmetry in HE1,X modes analyzed, Antonio Astrofísica Óptica, Mexico; Engineering, BUAP, Mexico. Astorino1, Mario A. Usuga Castaneda1, Stine M. Israelsen1, JTu3A.94 We have numerically generated Markovian optical fields Jesper Lægsgaard1, Karsten Rottwitt1; 1DTU, Denmark. An Appropriate field of illumination size for reflective of variable amplitude. By using such fields we describe the analytical study of higher-order modes in step-index fibers ghost imaging concerning image quality, Lichen Zhang1, recording holographic and reconstruction processes. The has been conducted with the aim of justifying the circular Bin Luo2, Guohua Wu1, Junhui Li3, Dongyue Yang1, Long- model is generalized to a set of holographic structures. asymmetry experimentally observed in the intensity of fei Yin1, Hong Guo3; 1School of Electronic Engineering, higher-order Bessel-like modes. Beijing Univ. of Posts and Telecommunications, China; 2State Key Lab of Information Photonics and Optical JTu3A.88 Communications, Beijing Univ. of Posts and Telecommu- White light beam shaping by volume holographic nications, China; 3School of Electronics Engineering and element, Sunil Vyas1, Po-Hao Wang1, Yuan Luo1; 1Na- Computer Science, Peking Univ., China. For reflective tional Taiwan Univ., Taiwan. Utilizing angle-wavelength ghost imaging, illumination field with the same size of coupling degeneracy of volume holograms, we experi- the object provides the best image quality. Among other mentally demonstrate the generation of white light beam assessments, contrast-to-noise ratio (CNR) reflects the size shapes corresponding to three different types of beams: effect best, and is more vulnerable to noise. Laguerre-Gaussian, Bessel-Gaussian and Airy-Gaussian beams.

50 FiO + LS 2017 • 17–21 September 2017 Science & Industry Showcase

JOINT FiO + LS

JTu3A • Joint Poster Session II—Continued

JTu3A.102 JTu3A.109 JTu3A.115

Efficient Relativistic High-Order Harmonic Generation Research on LD Pumped Nd:GdYTaO4 Quasi-three-lev- Tamm plasmon polaritons in aperiodic metal depos- with Waveform-Engineered Driving Pulses, Matthew el 928 nm Laser, Wentao Wu1, XuDong Li1, Renpeng ited Bragg reflectors, Mukesh K. Shukla1, Ritwick Das1; Edwards1, Julia M. Mikhailova1; 1Princeton Univ., USA. Yan 1, Yufei Ma1, Fang Peng2, Qingli Zhang2, Renqin Dou2, 1National Inst of Sci Education & Res., India. We present Multi-color synthesized waveforms generate relativistic Jing Gao3; 1National Key Lab of Tunable Laser Technol- existence of Tamm-plasmon-polariton (TPP) modes high-order harmonics with far higher efficiencies than ogy, Harbin Inst. of Technology, China; 2The Key Lab of in one-dimensional quasi-crystals and deterministic single-color driving pulses. Particle-in-cell simulations Photonic Devices and Materials, Anhui Inst. of Optics aperiodic structures for normal incidence of broadband suggest an optimal waveform, providing an efficiency and Fine Mechanics, China; 3Jiangsu Key Lab of Medical light. They exhibit similar propagation characteristics as limit on the process. Optics, Suzhou Inst. of Biomedical Engineering and conventional TPP modes. Technology, China. We demonstrated a diode-pumped

JTu3A.103 Nd:Gd0.69Y0.3TaO 4 quasi-three-level 928 nm laser. Output JTu3A.116 Simultaneous emission of noise-like pulse and solitons power of 87 mW at 928 nm was obtained in quasi-contin- Dynamic Ferroelectricity of Trojan Electrons on Hexag- from a fiber laser, Yazmin E. Bracamontes-Rodriguez1, Ol- uous-wave operation under 808 nm laser diode pumping. onal Face-Centered 3-Triangular Lattice, Matt . Kalinski1; ivier Pottiez1, Hugo Ibarra1, J. P. Lauterio-Cruz1, Baldemar 1Utah State Univ., USA. We discover several types of Ibarra-Escamilla2, Evgeny Kuzin2; 1División de Fotónica, JTu3A.110 the dynamic ferroelectric orders on the regular lattice Centro de Investigaciones en Óptica, Mexico; 2Óptica, Spectroscopy of Metastable Xenon Atoms in High consisting of three triangular lattices forming Hexagonal INAOE, Mexico. Pressure Plasma Discharges, Carl R. Sanderson1, Face-Centered Lattice on which hydrogen atoms with Passively mode-locked fiber lasers (PML-FLs) are versatile Amanda Clark2, Ian Gabalski2, Paul J. Moran3, Eric Guild4, coherently phase moving Trojan wavepackets are placed. sources for generating a broad variety of pulses. This Jiande Han5, Michael Heaven5, Brett Hokr2; 1Systems work presents a PML-FL in an unusual hybrid regime, with Management and Production Center, Univ. of Alabama JTu3A.117 simultaneous emission of NLP and solitons at different in Huntsville, USA; 2High Energy Laser Division, US Army Spectroscopic & electrical investigations on Yb3+/Er3+ 3 wavelengths. SMDC/ARSTRAT, USA; Laser Technology Branch, Air co-doped Ba0.5Ca0.5ZrO3 ceramics for application in Force Research Lab, USA; 4Leidos Inc., USA; 5Dept. of sensing devices, PRASENJIT PRASAD SUKUL1, Kaushal JTu3A.104 Chemistry, Emory Univ., USA. Tunable diode laser ab- Kumar1; 1Applied Physics, Indian Inst. of Technology(ISM), 3+ 3+ Gain-Clamping for an Externally-Incident Field Passing sorption spectroscopy measurements of the metastable India. Yb /Er codoped Ba0.5Ca0.5ZrO3 ceramics at dif- through a Laser Cavity, Ali Kazemi Jahromi1, Alexander xenon population densities and spectral line broadening ferent sintering temperature through solid state reaction Cerjan2, A. Douglas Stone3, Ayman Abouraddy1; 1Univ. of of the 904.545 nm transition in three high pressure plasma route are prepared and photoluminescence properties of Central Florida, CREOL, USA; 2Applied Physics, Stanford discharges are presented. the ceramic were investigated. 3 Univ., USA; Applied Physics, Yale Univ., USA. Behavior of Tuesday, 19 Septem a self-oscillating cavity probed with an externally incident JTu3A.111 JTu3A.118 field has been the subject of controversy for decades. We Variation in polarization profiles of Ince-Gaussian Fluorescence Quantum Yield Measurements in Silver address this issue by designing an experiment, and verify beams with eccentricity, Sean M. Nomoto1, Reeta Vyas1, Nanoparticle-Rhodamine B Systems by Thermal Lens it with state-state ab-initio laser theory. Surendra Singh1; 1Univ. of Arkansas, USA. Polarization Spectroscopy, Luis Rodriguez1, Marco Ferreira1, Vincent intensity profiles for dominant and cross components of Piscitelli1; 1Universidad Central de Venezuela, Venezuela, JTu3A.105 Ince-Gaussian beams for orders up to p = 5 and eccentric- Bolivarian Republic of. We studied the changes induced

Efficient Lasing on Alkali Atomic D2 Lines Utilizing ities 0.01, 0.2, 1.0, and 2.0 were observed. Experimental by silver nanoparticles, generated by laser ablation, in the Spin-Polarized Alkali Vapor, Andrey Mironov1, J. G. results agree with the theory. quantum yield of Rhodamine B. The silver nanoparticles Eden1; 1Univ of Illinois at Urbana-Champaign, USA. We quenched the fluorescence of the Rhodamine B and

report a novel method for significantly improving the ef- JTu3A.112 depended on both concentrations. ber ficiency of alkali atomic lasers. By pumping alkali-rare gas Study on Features of a Diode-Pumped Alkali Laser: atomic pairs with a circularly polarized optical field, an in- Temperature 3D-Distribution, Thermally-Induced crease in the efficiency of >50% has been demonstrated. Lens, and Ionization Processes, Guofei An1, You Wang1, Juhong Han1, Wei Zhang1, He Cai1, Shunyan Wang1, JTu3A.106 Kepeng Rong1, Hang Yu1, Hongyuan Wang1; 1Southwest Minimizing heat generation by radiative cooling in a Inst. of Technical Physics, China. We develop a 3D-model Ytterbium-doped silica fiber laser, Mostafa Peysokhan1, to evaluate the kinetic processes and thermal features of Arash Mafi1; 1Univ. of New Mexico, USA. We study thermal a cesium-vapor laser. The 3D temperature distribution, management and radiative cooling in a Ytterbium-doped effective focal length of a thermally-induced lens, and the silica fiber laser and design a specific fiber laser that influence of ionization processes are analyzed. minimizes the thermal load while maintaining an efficient power operation. JTu3A.113 Studies on nonlocal plasmonic resonances: analyt- JTu3A.107 ical and numerical approaches, Milan Burda1, Pavel Theoretical Investigation of Blue-laser-diode-pumped Kwiecien1, Ivan Richter1, Jan Fiala1; 1Czech Technical High Efficiency CW Ti:sapphire Laser by High Intensity Univ. in Prague, Czech Republic. Both (quasi)analytical Pumping, Tomoki Kanetake1; 1Fukui Univ., Japan. The and numerical approaches describing the complexity of efficiency of a blue laser-diode-pumped CW Ti:sapphire nonlocal interactions at nanoscaled plasmonic structures laser was investigated theoretically. The maximum are investigated, in comparison with the standard linear optical-to-optical conversion efficiency was obtained to response approximation. be 20.4% at a pump power of 14W, with a high cavity loss of 20%. JTu3A.114 Vortex-antivortex wavefunction for superfluids in JTu3A.108 exciton-polariton laser, Alex Okulov1; 1Russian Acad- Theoretical Analysis of Efficiency in a Mode-locked emy of Sciences , Russia. It is shown that interaction of Laser with an Intra-Cavity Highly Nonlinear Medium, exciton-polariton superfluid with structured light in laser Naoya Nakajima1; 1Fukui Univ., Japan. We analyzed the microcavity leads to spontaneous formation of vortex-an- optical-to-optical conversion efficiency of a mode-locked tivortex quantum states laser with an intra-cavity highly-nonlinear medium. Effi- ciency reduction was caused when the output spectrum are wider than the gain spectrum edge.

FiO + LS 2017 • 17–21 September 2017 51 International Ballroom West International Ballroom East Georgetown West

FiO

15:00–16:30 15:00–16:30 15:00–16:30 FTu4A • Integrated Optics FTu4B • Advanced Spectroscopy and New FTu4C • Display Technology for VR/AR Presider: Roger Helke; University of Approaches Applications California, Santa Barbara, USA Presider: Takashige Omatsu; Chiba Presider: Hong Hua; The University of University, Japan Arizona, USA

FTu4A.1 • 15:00 Invited FTu4B.1 • 15:00 Invited FTu4C.1 • 15:00 Invited Arbitrary and Self-configuring Optics – New Oppor- Chemical Sensing From 3–13 µm Using Femtosecond Op- Next Challenge for Augmented Reality as a Smart Display tunities for Integrated Photonics, David A. B. Miller1; tical Parametric Oscillators, Derryck T. Reid1; 1Heriot-Watt Technology, Hirokazu Kato1; 1Nara Inst. of Science and 1Stanford Univ., USA. Recent understanding shows how to Univ., UK. Fourier-transform and dual-comb spectroscopy Technology, Japan. Since the concept of Augmented Reality make universal linear components, beyond conventional using MgO:PPLN and OPGaP femtosecond optical para- was proposed in the 1990’s, that technology has evolved to optics. Fundamental consequences include new radiation metric oscillators is described in a variety of embodiments reach a practical level. I will present its brief history and the laws. Practical integrated Mach-Zehnder meshes can be including stand-off identification of liquids and aerosols, and challenges for further development in the future. self-configured for arbitrary linear functions. precision spectroscopy of gases.

FTu4A.2 • 15:30 FTu4B.2 • 15:30 FTu4C.2 • 15:30 Invited Lasing and Steering an integrated Vortex Laser, Babak Deep UV pulse shaping at 207 nm through Fourier-do- Head-mounted Holographic Display with Correct 1 1 1 1 Bahari , Felipe Valini , Thomas Lepetit , Ricardo Tellez-Li- main frequency upconversion, Philippe Lassonde , Bruno Depth-focusing for AR, Yuji Sakamoto1; 1Hokkaido Univ., 1 1 1 1 2 1 3 mon , Junhee Park , Ashok Kodigala , Yeshaiahu Fainman , E. Schmidt , Guilmot Ernotte , Matteo Clerici , Roberto Japan. A compact and lightweight head-mounted holo- 1 1 1 1 1 1 Boubacar Kante ; Univ. of California San Diego, USA. We Morandotti , Heide Ibrahim , François Légaré ; INRS-emt, graphic display based on computer-generated hologram 2 3 ber demonstrated theoretically and experimentally a Bound Canada; Few-cycle inc., Canada; School of Engineering, for AR was developed. It shows 3D images at correct State in the Continuum Surface Emitting Laser that operates Univ. of Glascow, UK. We demonstrate controlled amplitude depth-focusing without fatigue by the depth difference with at room temperature and it can steer the beam with an angle and phase transfer of an ultrashort laser pulse through the gazing object. depending on the topology of structure. second-harmonic generation in the frequency domain. Sequential conversion allowed pulse shaping down to the deep UV at 207 nm.

FTu4A.3 • 15:45 FTu4B.3 • 15:45 Graphene oxide integrated on-chip tunable waveguide Pulsed Light Sheets with Arbitrary Beam Profiles via polarizer, Subhabrata Ghosh1, Debabrata Mandal1, Am- Correlated Spatio-Temporal Spectrum, Hasan E. Kondakci1, reesh Chandra1, Shivakiran Bhaktha B. N.1; 1Indian Inst. of Ayman Abouraddy1; 1CREOL, Univ. of Central Florida, USA. Tuesday, 19 Septem Tuesday, Technology Kharagpur, India. We demonstrate tunable TE We experimentally demonstrate diffraction-free pulsed

pass polarizer in graphene oxide (GO) coated SiO2-HfO2 light sheets with arbitrary spatial profile at the pulse center channel waveguides fabricated by UV-photolithography. by introducing tight correlations between the spatial and The tunability has been achieved by reduction of GO by temporal degrees of freedom in hyperbolic form. controlled IR irradiation.

FTu4A.4 • 16:00 FTu4B.4 • 16:00 FTu4C.3 • 16:00 Flexible Visible Photonic Crystal Laser Cavity, Jie Zhou1,2, Advanced microscopy techniques for revealing molecular Multi-SLM Holographic 3D Display of Real-world Holo- Taojie Zhou2, Jiagen Li2, Kebo He2, Qian Li1, Zhaoyu Zhang2; structure of starch granules, Nirmal Mazumder1, Suchitta graphic Data with Numerical Data Adaptation, Weronika 1Peking Univ., China; 2Chinese Univ. of Hong Kong, China. Umashankar1, Bharath Ratnakar1, Krishna Kishore Mahato1, Zaperty1, Piotr L. Makowski1, Tomasz Kozacki1; 1Warsaw The authors propose a L3 defect photonic crystal nano- Fu-Jen Kao2; 1Dept. of Biophysics, School of Life Sciences, Univ. of Technology, Poland. We present color holographic laser embedded in flexible medium for nanoscale strain Manipal Univ., India; 2Inst. of Biophotonics, National Yang imaging system, which data capture and reconstruction pro- detections. A theoretical optical strain sensitivity of ~4.5 Ming Univ. , Taiwan. The molecular structure (crystalline and cesses are characterized by different parameters. Necessary nm or 3 nm per ε (1% strain) in the x-direction or y-direction amorphous components) of potato starch was characterized holographic content adaptation is performed numerically on is predicted. using second harmonic generation (SHG) and coherent the Fourier hologram basis. anti-Stoke Raman scattering (CARS) microscopy as well as scanning electron microscope (SEM).

FTu4A.5 • 16:15 FTu4B.5 • 16:15 FTu4C.4 • 16:15 Distributed Brillouin Scattering Measurement with Efficient visible frequency microcomb generation with Digital Degenerate Cavity Laser, Nir . Davidson1, Chene Sub-mm Spatial Resolution, Atiyeh Zarifi1,2, Birgit Stiller1,2, 22% conversion efficiency, Xiang Guo1, Chang-ling Zou1, Tradonsky1, Ronen Chriki1, Gilad Barach1, Vishwa Pal1, Asher Moritz Merklein1,2, Khu Vu3, Stephen J. Madden3, Benjamin Hojoong Jung1, Zheng Gong1, Alexander Bruch1, Liang Friesem1; 1Weizmann Inst. of Science, Israel. A novel digital J. Eggleton1,2; 1Univ. of Sydney, Australia; 2Australian Inst. Jiang1, Hong X. Tang1; 1Yale Univ., USA. We demonstrate an degenerate cavity laser allows computer controlled gener- for Nanoscale Science and Technology (AINST), Australia; efficient visible frequency comb generation process in the ation of arbitrary output intensity distributions, propagation 3CUDOS, Laser Physics Centre, Australian National Univ., aluminum nitride microring resonator. Up to 22% conversion invariance of the output distribution, and rapid all-optical Australia. We report a highly localized SBS response with efficiency from infrared pump to the visible comb is realized. solution of inverse scattering problems. 780 μm spatial resolution in an As2S3 photonic integrated waveguide. This approach is used to characterize the waveguide based on its acousto-optic properties.

16:30-17:00 Environmental Sensing Technical Group Networking Event, OSA Technical Group Booth, International Terrace, Terrace Level

52 FiO + LS 2017 • 17–21 September 2017 Georgetown East Jefferson West Jefferson East

FiO LS

15:00–16:30 15:00–16:30 15:00–16:30 FTu4D • Novel Phenomena in Photonic FTu4E • Quantum Electronics in LTu4F • High Harmonic Sources and Devices Automotive Sector Applications Presider: Thomas Gerrits; National Institute Presider: Robert Baker; The Ohio State of Standards & Technology, USA University, USA

FTu4D.1 • 15:00 Invited FTu4E.1 • 15:00 LTu4F.1 • 15:00 Invited Ultra-sensitive Fiber Sensors using Structural Slow Light, 1060 nm HCG MEMS-VCSEL with 73 nm Tuning Range, New Generation Attosecond X-ray Light Sources, Zenghu 1 1 1 Michel Digonnet1; 1Stanford Univ., USA. Slow-light fiber Kevin T. Cook , Pengfei Qiao , Connie J. Chang-Hasnain ; Chang1; 1CREOL and Physics, Univ. of Central Florida, USA. 1 Bragg gratings exhibit very narrow resonances that can be Electrical Engineering and Computer Sciences, Univ. of Isolated X-ray pulses as short as 53 as with photon energy used to fabricate sensors with unprecedented resolutions. California, Berkeley, USA. We present a MEMS-actuated, reaching the carbon K-edge were generated by sub-cycle Their principles of operation and properties will be illustrated high-contrast grating VCSEL operating at 1060 nm with a gating. The X-ray sources is driven by a carrier-envelope with strain, temperature, and acoustic sensors. 73 nm tuning range. The tuning range ratio (Δλ/λ) of 6.9% phase stable laser centered at 1.7 mm. is the highest for an electrically pumped laser, to the best of our knowledge.

FTu4E.2 • 15:15 Toward a Multi-Species Gas Sensor on a Chip, Afshin Shamsshooli1, Chen Zhang1, Yonghao Liu1, Prithviraj Palit1, Yuze A. Sun1, Michael Vasilyev1; 1Univ. of Texas at Arlington, USA. We demonstrate on-chip implementation of an optically accessible gas expansion chamber for a gas sensing system combining micro-gas-chromatography with optical spectroscopy. Acetylene traces are reliably detected in a 1-cm-long chamber.

FTu4D.2 • 15:30 FTu4E.3 • 15:30 Invited LTu4F.2 • 15:30 Material Loss Omits Nonlinearity in Optically Thick Ma- Laser-based measurements of combustion engines– inside High-harmonic generation in solids using a mid-infrared 1 1 1 1 terials, Boris Simkhovich , Guy Bartal ; Technion, Israel. We and outside., Paul Ewart1, Ben Williams1; 1Univ. of Oxford, sub-cycle pulse synthesizer, Kyung-Han Hong , Zhou 2 1,3 2 1 show that Kerr-like nonlinearities may be omitted in lossy op- UK. The development of linear and non-linear optical tech- Wang , Tobias Kroh , Hyunwook Park , Krogen Peter , Tuesday, 19 Septem 1 2 1,3 1 tically thick materials, resulting in underestimated Nonlinear niques for high precision measurements of combustion in Houkun Linag , Louis DiMauro , Franz X. Kärtner ; MIT, 2 3 effects. This indicates that Nonlinear characterization should internal combustion engines is described for applications USA; Physics, Ohio State Univ., USA; CFEL, DESY, Germa- be obtained in thin samples to avoid masking of the effect. in design of future fuels, increased engine efficiency and ny. We generate high harmonics in Si using a mid-infrared th reduced emissions. (2.5-9.0 µm) pulse synthesizer. Even and odd harmonics (19 order) with few-cycle pulses and near-continuous spectra with sub-cycle pulses, indicating an isolated harmonic emission, are observed.

FTu4D.3 • 15:45 LTu4F.3 • 15:45 Invited A new path to speckle by randomizing a vortex lattice,

Attosecond Dynamics without Dipole Approximation, ber 1 1 Argelia Balbuena Ortega , Santiago Lopez Huidobro , Ursula Keller1; 1ETH Zurich, Switzerland. To honor Louis Di- 1 1 Freddy Jackson Poveda Cuevas , Laura Perez Garcia , Jorge Mauro’s 2017 APS Schawlow Prize we will review our recent 1 1 Amin Seman Harutinian , Alejandro Vasquez Arzola , Karen work on ionization and rescattering in strong mid-infrared 1 1 Volke Sepulveda ; UNAM, Mexico. In this work, we intend laser fields in the non-dipole regime over the full range of to establish a connection between the propagation of arrays polarization ellipticity. of vortices, either ordered or random, and the emergence of speckle patterns. Experimental results are presented and compared with numerical simulations.

FTu4D.4 • 16:00 FTu4E.4 • 16:00 Invited Self-Seeded Mid-Infrared Generation in Periodically-Poled Automotive LiDAR: Challenges and Opportunities, Lute 1,2 Lithium Niobate Waveguides, Alexander Lind , Abijith Maleki1,2; 1OEwaves Inc, USA; 2Strobe, Inc., USA. LiDAR is 1 1 1 S. Kowligy , Daniel D. Hickstein , David Carlson , Nima being used for development of autonomous vehicles. The 1 1 1 1 Nader , Henry Timmers , Erin Lamb , Gabe Ycas , Scott current technology, however, does not meet the required 1 1,2 1 Papp , Scott Diddams ; National Inst. of Standards and performance for full autonomous operation. In this paper 2 Technology, USA; Physics, Univ. of Colorado Boulder, USA. a demonstrated approach achieving this objective will be We demonstrate a mid-infrared source, tunable from 4–5 μm, discussed. via cascaded χ(2) supercontinuum generation and subsequent difference frequency generation (DFG) within a single lithium niobate waveguide.

FTu4D.5 • 16:15 LTu4F.4 • 16:15 Optical Isolation with Nonlinear Topological Photonics, Electronic structure and ultrafast charge carrier dynamics Xin Zhou1, You Wang1, Daniel Leykam1, Yidong Chong1; of Zn clusters supported on a Si(100) surface, Mihai E. 1Nanyang Technological Univ., Singapore. We present a Vaida1, Brett M. Marsh2, Bethany Lamoureux2, Stephen Le- theoretical study of optical isolation based on self-induced one4,3; 1Dept. of Physics, Univ. of Central Florida, USA; 2Dept. topological photonic edge states, occurring in nonlinear to- of Chemistry, Univ. of California, USA; 3Lawrence Berkeley pological photonic structures such as 1D and 2D waveguide National Lab, USA; 4Dept.s of Chemistry and Physics, Univ. arrays and coupled-ring lattices. of California, USA. Femtosecond XUV photoemission spectroscopy is employed to monitor the non-metal to metal transition in Zn clusters grown on p-Si(100) as well as the ultrafast charge migration, trapping, and recombination at the surface.

16:30-17:00 Environmental Sensing Technical Group Networking Event, OSA Technical Group Booth, International Terrace, Terrace Level

FiO + LS 2017 • 17–21 September 2017 53 International Ballroom West International Ballroom East Georgetown West

FiO

16:45–18:15 16:45–18:15 16:45–18:15 FTu5A • Pulse and Comb Sources FTu5B • Advanced Imaging and FTu5C • Real-time Optical Guidance of Interactions with Materials Cancer Therapy Presider: Sile Nic Chormaic; Okinawa Presider: David Busch; University of Institute of Science & Technology, Japan Pennsylvania Children’s Hospital of Philadelphia, USA

FTu5A.1 • 16:45 Invited FTu5B.1 • 16:45 Invited FTu5C.1 • 16:45 Invited Soliton Microcomb Physics and Applications, Kerry Vahala1; Dispersion mapping for tissue differentiation in optical Real-time quantitative optical imaging for surgery, Syl- 1Caltech, USA. The physics of dissipative Kerr solitons in coherence tomography, Frederique Vanholsbeeck1,2; 1Univ. vain Gioux1,2, Joseph Angelo3; 1Universite de Strasbourg, high-Q micro cavities is reviewed including discussion of of Auckland, New Zealand; 2Dodd-Walls centre for photonics France; 2Harvard Medical School, USA; 3National Inst. of Raman effects and counter-propagating soliton behavior. and quantum technologies, New Zealand. We compare the Standards and Technology, USA. There currently exist no techniques such as fractional Fourier transform or multiband tools to effectively assist healthcare professionals during OCT we have used to map chromatic dispersion in tissues surgery. In this presentation we will review our efforts to using OCT dataset. provide real-time, wide-field & quantitative optical imaging for surgical applications.

FTu5A.2 • 17:15 FTu5B.2 • 17:15 FTu5C.2 • 17:15 Soliton Mitosis Across a Zero-Nonlinearity Wavelength in Systematic Refractive Index Control in DNA Solid Thin Fast Multispectral Fluorescence Lifetime Rigid Endoscope Photonic Crystal Fibers, Francisco Rodrigo Arteaga Sierra1, Films by DNA-Denaturation Process, Hayong H. Jeong1, for Screening of Skin Lesions, Ramon G. Rosa1, Sebastião Aku Antikainen1, Govind P. Agrawal1; 1Univ. of Rochester, Bjorn Paulson1, Seongjin Hong1, Seunguk Cheon1, Kyung- Pratavieira1, Javier Jo2, Cristina Kurachi1; 1Sao Carlos Inst. Mexico. We show numerically the splitting of a single fun- hwan Oh1; 1Dept. of Physics in Yonsei Univ., South Korea. of Physics, Univ. of Sao Paulo, Brazil; 2Dept. of Biomedical damental soliton into two copropagating solitons across Denaturation process to unchain double-strand (ds) DNAs Engineering, Texas A&M Univ., USA. The development of a the zero-nonlinearity wavelength through femtosecond into single-strand (ss) DNAs was experimentally found to fast multispectral fluorescence lifetime rigid endoscope for pumping of a photonic crystal fiber with frequency-depen- systematically control the refractive index of spin-coated in vivo imaging is reported. Our preliminary results show dent nonlinearity. DNA thin solid films. the potential to identify precisely the borders of human skin lesions.

FTu5A.3 • 17:30 FTu5B.3 • 17:30 FTu5C.3 • 17:30

ber Multispectral optical frequency comb based on microre- Two-Photon Polymerization of Biocompatible Hydro- Quantitative characterization for identification of brain sonator Faraday instability, Shu-Wei Huang1, Abhinav K. gels, Haibo Ding1,2, Qiming Zhang1, Zhongze Gu2, Min cancer surgical margin using resonance Raman spec- Vinod1, Jinghui Yang1, Mingbin Yu2, Dim-Lee Kwong2, Chee Gu1; 1School of Science, RMIT Univ., Australia; 2School troscopy, Yan Zhou2, Cheng-hui Liu1, Binlin Wu3, Xinguang Wei Wong1; 1Univ. of California Los Angeles, USA; 2Inst. of of Biological and Medical Engineering, Southeast Univ., Yu4, Gangge Cheng2, Chunyuan Zhang1, Robert R. Alfano1; Microelectronics, Singapore. We demonstrate a new type China. We demonstrate a common UV photoinitiator with 1CUNY City College, USA; 2Air Force General Hospital, of microresonator frequency comb where the momentum a two-photon absorption cross-section of 4.5 GM in the China; 3Southern Connecticut State Univ., USA; 4PLA General conservation law is fulfilled by azimuthal modulation of the wavelength of 535 nm. Three-dimensional microstructured Hospital, China. A new criterion was developed to charac- waveguide dispersion. The concept expands the parametric scaffolds could be achieved with two-photon polymerization terize brain tissue using resonance Raman spectroscopy, range in which Kerr comb is obtained. of biocompatible hydrogels. by which, negative margins of cancer can be differentiated from normal tissues. This method may help a surgeon better decide surgical margins. Tuesday, 19 Septem Tuesday,

FTu5A.4 • 17:45 FTu5B.4 • 17:45 FTu5C.4 • 17:45 Stability Evaluation of Passively Q-switched Erbium Visible spectrum luminescence of nanolayered erbium In Vivo Diagnostics of Malignant and Benign Tumors with 1 1 Doped Fiber Laser based on Double and Multi-Walled doped ZnO and TiO2, Arslan Anjum , Elangovan Elam- Low-Cost Raman Spectrometer, Julia Khristoforova , Ivan Carbon Nanotubes, A. Hadi Al-Janabi1, Dunya Z. Mo- urugu1, Jaime P. Viegas1; 1ECE - Masdar Inst., Khalifa Univ., Bratchenko1, Dmitry Artemyev1, Oleg Myakinin1, Alexandr hammed1; 1Inst. of Laser for Postgraduate Studies, Iraq. United Arab Emirates. Visible luminescence of erbium doped Moryatov2, Oleg Kaganov2, Sergey Kozlov2, Valery Zakharov1; 1 2 The stability of Q-switched erbium-doped fiber laser using ZnO / TiO2 thin films deposited by magnetron sputtering Samara Univ., Russia; Samara State Medical Univ., Russia. A double and multi -walled carbon nanotubes (DWCNTs and is presented. Through adjustment of deposition rates and method for malignant skin tumors diagnostics based on the MWCNTs) saturable absorbers (SAs) has been investigated. layer thickness, doping concentration can be tailored with combination of Raman spectroscopy and autofluorescence DWCNTs SA showed better stability than MWCNTs SA at observable effect on photoluminescence. analysis is proposed. Multivariate analysis of spectral data the proposed concentration. demonstrated 98.4% accuracy of malignant and benign tumors classification.

FTu5A.5 • 18:00 FTu5B.5 • 18:00 FTu5C.5 • 18:00

Greatly Enhanced Absorption in Weakly-Doped Fibers Two-Photon Absorption Spectroscopy in Cuins2 (Cis) Second-harmonic Patterned Polarization-Analyzed Re- through Coherent Perfect Absorption, Ali Kazemi Jahromi1, Quantum Dots For Bio-Imaging, Gabriel Nagamine1, Hunt- flection Confocal Microscopy of Collagen, Chukwuemeka Ayman Abouraddy1; 1Univ. of Central Florida, CREOL, USA. er McDaniel2, Carlos Henrique Brito Cruz1, Lázaro Padilha1; Okoro1, Kimani Toussaint1; 1Univ. of Illinois Urbana-Cham- We experimentally show that coherent perfect absorption is 1UNICAMP, Brazil; 2UbiQD, USA. We study two-photon paign, USA. Polarization analysis of images obtained by

achievable in a few-centimeter-long moderately-doped fiber, absorption in CuInS2 quantum dots. We show that the combining confocal microscopy with a second-harmonic and prove the CPA is best configuration to get a uniform maximum two-photon absorption cross-section strongly de- mask permits traditional polarimetric metrics to be adapted absorption per unit length of the absorbing medium. pendents on quantum-confinement, and that the material is to collagen imaging. This approach applies to any nonlinear a promising candidate as label for multi-photon bio-imaging. scattering imaging technique.

16:30–16:45 Break

17:30–18:15 OSA Annual Business Meeting, Kalorama, Lobby Level

17:30–18:30 APS Division of Laser Science Annual Business Meeting, Holmead East, Lobby Level

18:30–20:30 FiO + LS Conference Reception, International Ballroom Center, Terrace Level

54 FiO + LS 2017 • 17–21 September 2017 Georgetown East Jefferson West Jefferson East

FiO LS

16:45–18:15 16:45–18:15 16:45–18:15 FTu5D • Nanophotonic Systems FTu5E • Quantum Measurement and LTu5F • Applications of Ultrafast X-rays Presider: Yoshio Hayasaki; Utsunomiya Sensors Presider: Mihai Vaida; University of Central University, Japan Presider: Lute Maleki; OEwaves Inc, USA Florida, USA

FTu5D.1 • 16:45 Invited FTu5E.1 • 16:45 Invited LTu5F.1 • 16:45 Invited 3D Nanophotonic Systems for Biosensing and Inte- New detectors and advanced electronics for quan- Probing Electron Delocalization with Femtosecond X-ray grated Photonics, Euan McLeod1; 1Univ. of Arizona, USA. tum-based technologies, Rik van Gorsel1; 1Boston Elec- Spectroscopy, Munira Khalil1; 1Univ. of Washington, USA. Three-dimensional nanophotonic systems assembled from tronics Corp., USA. No Abstract Provided Uisng femtosecond X-ray spectroscopy and multidimen- soft materials such as liquids, polymers, and colloids can sional vibrational-electronic spectroscopies we will probe enable sensitive and high-throughput biosensing, as well the electronic delocalization and vibronic coupling in a as compact and efficient integrated photonics components. mixed valence transition metal complex dissolved in water.

FTu5D.2 • 17:15 FTu5E.2 • 17:15 LTu5F.2 • 17:15 Three-dimensional Direct Laser Writing of Neuron-in- Quantum Metrology in the Joint Measurement of Multiple Nonlinear optical signals and spectroscopy with quantum spired Structures, Haoyi Yu1, Qiming Zhang 1, Zengji Yue Parameters Encoded in Non-Commuting Observables light and in microcavitites, Shaul Mukamel1, Konstantin 1, Min Gu1; 1RMIT Univ., Australia. We propose the use of with SU(1,1) Interferometer, Yuhong Liu1, Jiamin Li1, Dorfman1, Markus Kowalewski1, Kochise Bennett1, Frank three-dimensional direct laser writing to create neuron-in- Xiaoying Li1, Zhe-Yu . Ou2, Syed M. Assad3; 1Tianjin Univ., Schlawin1; 1Univ. of California Irvine, USA. Nonlinear optical spired structures. The experimental realization of neuron-in- China; 2Indiana Univ.-Purdue Univ. Indianapolis, USA; 3The signals induced by quantized light fields and entangled spired structures 10 times smaller than biological neurons is Australian National Univ., Australia. Joint measurement photon pairs are presented. Different signals, and photon achieved using two-photon direct laser writing. of phase and amplitude modulations on a probe field is counting setups are discussed and illustrated for molecular performed with an SU(1,1) interferometer. Signal-to-noise model systems. ratios in the joint measurement simultaneously beat the classical limit by 1dB. Tuesday, 19 Septem FTu5D.3 • 17:30 FTu5E.3 • 17:30 LTu5F.3 • 17:30 Invited Concave Grating Enabled Compact Mid-IR Upconversion Quantum position measurement of a shadow: beating the Femtosecond Time-resolved X-ray Absorption Spectros- 1 1 1 1 Spectrometer, Ajanta Barh , Peter Tidemand-Lichtenberg , classical limit, Ermes Toninelli , Matthew P. Edgar , Paul-An- copy of Liquids Using the SPring-8 Angstrom Compact 1 1 1 1 1 Christian Pedersen ; Technical Univ. of Denmark (DTU), toine Moreau , Graham M. Gibson , Giles D. Hammond , Free-Electron Laser (SACLA, Kazuhiko Misawa1,2; 1Dept of 1 1 Denmark. The paper demonstrates a wide-band (3.6 – 4.8 Miles J. Padgett ; School of Physics & Astronomy, Univ. of Applied Physics, Tokyo Univ of Agriculture and Technology, µm) compact mid-infrared grating spectrometer combining Glasgow, UK. The precision with which the position of a shad- Japan; 2Inst. of Global Innovation Research, Tokyo Univ of a nonlinear frequency upconversion process and a flat-field ow can be measured is classically limited by shot-noise. We Agriculture and Technology, Japan. We present time-re- aberration corrected concave grating with overall system achieve sub-shot-noise position sensitivity by jointly detect- solved X-ray absorption spectroscopy of ammonium iron(III) dimension of 25cm×50cm. ing correlated photons with a simple split-detector scheme. oxalate trihydrate and anatase TiO2 nanoparticles in aqueous

solutions using an X-ray free electron laser in combination ber with a synchronized ultraviolet femtosecond laser.

FTu5D.4 • 17:45 FTu5E.4 • 17:45 Invited Low loss 19-cell hollow core photonic bandgap fiber High-efficiency Superconducting Detectors and Their as transmission medium for mode division multiplexed Applications in Quantum Optics, Thomas Gerrits1; 1NIST, 1 1 system, Olena Muliar , Mario Usuga Castaneda , Karsten USA. High efficiency single-photon detection resides at the 1 1 1 Rottwitt , Jesper Lægsgaard ; Technical Univ. of Denmark, heart of many quantum information applications. Our efforts Denmark. We investigated and simulated the modal content towards high efficiency, fast single photon detectors, and of 19-cell hollow core photonic bandgap fiber (19-cell HC their range of applications and impacts in quantum optics PBGF) with anti-resonant elements and low loss region for will be discussed. the fundamental mode around 1550nm.

FTu5D.5 • 18:00 LTu5F.4 • 18:00 Broadband metasurface for chiral phase control, Gun-Yeal Achieving Surface Sensitivity in Ultrafast XUV Spec- 1 1 1 1 Lee , Jangwoon Sung , Byoungho . Lee ; Seoul National troscopy: M2,3-edge Reflection-Absorption of Transition Univ., South Korea. We report a novel metasurface that Metal Oxides, Robert Baker1, Anthony Cirri1, Jakub Husek1, controls the spatial phase distributions of light and switches Somnath Biswas1; 1Chemistry & Biochemistry, The Ohio State them by using chirality of incident light, which can be applied Univ., USA. We have developed near grazing angle XUV to chiral imaging and chiral control of optical beams. reflection-absorption (RA) spectroscopy to study ultrafast carrier dynamics at surfaces and provide a general method for interpreting XUV RA spectra that quantitatively accounts for surface morphology.

16:30–16:45 Break

17:30–18:15 OSA Annual Business Meeting, Kalorama, Lobby Level

17:30–18:30 APS Division of Laser Science Annual Business Meeting, Holmead East, Lobby Level

18:30–20:30 FiO + LS Conference Reception, International Ballroom Center, Terrace Level

FiO + LS 2017 • 17–21 September 2017 55 International Ballroom West International Ballroom East Georgetown West

FiO

07:30–17:30 Registration, Concourse Foyer

08:00–08:45 FW1A • Visionary Speaker: Evelyn Hu, International Ballroom West FW1B • Visionary Speaker: Wilhelm Kaenders, International Ballroom East LW1C • Visionary Speaker: James K. Thompson, Jefferson East

08:45–09:00 Break

09:00–10:00 09:00–10:00 09:00–10:00 FW2A • Quantum Communications FW2B • Trapping and Shaping of Light FW2C • Optics in Computing and Imaging Presider: Carlos Lopez-Mariscal; Underwater Presider: Jae-Hyeung Park; Inha Univ., South Photonics, Mexico Korea

FW2A.1 • 09:00 FW2B.1 • 09:00 FW2C.1 • 09:00 Invited Simultaneous high-contrast switching and high-efficiency Nonlinearity-induced spectral lattice with optically tun- Deep Learning Optical Devices and Architectures, Kelvin 1 1 2 routing for spontaneous emission, He Hao , Juanjuan able long-range complex hopping, Bryn Bell , Kai Wang , H. Wagner1; 1Univ. of Colorado Boulder, USA. A rectifying 1 1 2 1 2 2 Ren , Xue k. Duan , Iam Choon Khoo , Guowei Lu , Ying Alexander S. Solntsev , Dragomir N. Neshev , Andrey A. linear unit implemented as a bidiectional switch along with 1 1 1 2 2 1 1 Gu , Qihuang Gong ; Peking Univ., China; Pennsylvania Sukhorukov , Benjamin Eggleton ; Centre for Ultrahigh convolutional layers using lenslet arrays and thick Fourier state Univ., USA. We theoretically demonstrated a high Bandwidth Devices for Optical Systems (CUDOS), School of holograms allows the implemention of Deep Neural Net- 2 contrast switching of spontaneous emissionas well as high Physics, Univ. of Sydney, Australia; Nonlinear Physics Centre, works in a self-aligning multilayer optical neural network. efficient routing photons enabled by liquid crystal tuned Research School of Physics and Engineering, The Australian gap surface plasmons. National Univ., Australia. We suggest and realize quantum walks on a spectral photonic lattice with optically tunable long-range and complex hopping facilitated by nonlinear interactions, enabling asymmetric frequency shaping and Talbot effect with arbitrary periodicity.

FW2A.2 • 09:15 FW2B.2 • 09:15 Lattice Dislocation in a Photonic Weak Topological Insu- Direct generation of tunable optical vortex dipole beams lator with a Synthetic Frequency Dimension, Qian Lin1, using a Gaussian beam pumped optical parametric oscil- Xiaoqi Sun1, Meng Xiao1, Shanhui Fan1; 1Stanford Univ., lator, Varun Sharma1,2, Aadhi A1, Goutam K Samanta1; 1PRL USA. We propose realization of photonic 3D topological Ahmedabad, India; 2Physics, IIT Gandhinagar, India. We insulator in a 2D ring array with a synthetic dimension, and report on tunable optical vortex dipole source based on an show that with dynamic modulating we can create a screw optical parametric oscillator (OPO) pumped with Gaussian dislocation that supports protected one-way state localized beam. Pumped in the green, the source produces vortex on the dislocation. dipole tunable across the wavelength range 968-1181 nm.

FW2A.3 • 09:30 Invited FW2B.3 • 09:30 Invited FW2C.2 • 09:30 New Color Centers in Diamond for Long Distance Quan- Advanced Optical Trapping of Ultracold Atoms for Study- Fused phase image obtained from frequency comb pro- 1 tum Communication, Nathalie de Leon1; 1Princeton Univ., ing Superfluid Transport and Turbulence, Tyler W. Neely1,2, filometer and optical interferometer, Yoshio Hayasaki , 1 1 USA. We have developed new methods to stabilize SiV0 in Guillaume Gauthier1,2, Stuart Szgeti1,2, Thomas Bell1,2, Mark Quang D. Pham ; Utsunomiya Univ., Japan. Phase images ber diamond, and observe T approaching 1 minute at 4K, and Baker1, Matthew J. Davis1, Halina . Rubinsztein-Dunlop1,2; obtained in the radio frequency and optical frequency rang- 1 5 >90% of its emission into its zero phonon line, making it a 1Univ. of Queensland, Australia; 2ARC Centre of Excellence es, whose difference was about 4 x 10 , were combined on promising single atom quantum memory. for Engineered Quantum Systems, Univ. of Queensland, the basis of a pattern matching method. Australia. We utilise direct-imaging of a digital micromirror device to create binary and optimised optical potentials for the trapping and manipulation of atomic Bose-Einstein FW2C.3 • 09:45 condensates. Studies of a superfluid circuit and quantum Quantitative Phase Imaging by Evanescent Wave Micros- 1 1 1 turbulence are described. copy, biagio mandracchia , Melania Paturzo , Pietro Ferraro ; 1Inst. for Applied Sciences and Intelligent Systems, Italian National Research Council, Italy. Here we show the versatility of Digital Holography Microscopy for the development of innovative systems for quantitative phase imaging of Total

Wednesday, 20 Septem Wednesday, Internal Reflection.

10:00–10:30 Coffee Break, Science & Industry Showcase, Columbia, Terrace Level

10:00–12:00 JW3A • Science & Industry Showcase Exhibits, Poster Session & E-Posters Rapid-Fire Oral Presentations III in Theater Columbia, Terrace Level

56 FiO + LS 2017 • 17–21 September 2017 Georgetown East Jefferson West Jefferson East

FiO LS

07:30–17:30 Registration, Concourse Foyer

08:45–09:00 Break

09:00–10:00 09:00–10:00 09:00–10:00 FW2D • Advocacy Session FW2E • Precision Measurement Using LW2F • Nanophotonics II Science Policy talk by Rush Holt, CEO of Laser-Atom Interactions Presider: Gary Wiederrecht; Argonne AAAS and former U.S. member of Congress Presider: Virginia Lorenz; University of National Lab, USA Illinois, USA

At a time when there are widespread concerns about the FW2E.1 • 09:00 LW2F.1 • 09:00 Invited place of science in our society and government, we should Sub-nano-Tesla, Shield-less, Field Compensation-Free Plasmon-empowered Single-photon Sources, Sergey consider: What is the obligation of a scientist, engineer, Optical Wave Mixing Magnetometry for Bio-magnetism, I. Bozhevolnyi1; 1Univ. of Southern Denmark, Denmark. 1 2 1,3 1 or technologist to policymakers? Sometimes, we simply Lu Deng , Yvonne L. Li , Feng Zhou , Eric Y. Zhu , Edward Coupling of quantum emitters to localized and propagating 1 1 2 disparage the ill-founded pronouncements of politicians, W. Hagley ; NIST, USA; Dept. of Medical Oncology, surface plasmons is considered from the viewpoint of en- decisions producing inadequate funding for research, or Dana-Farber Cancer Inst., Harvard Medical School, USA; hancing spontaneous emission rates, revealing advantages 3 regulations hampering research, when instead we might ask Dept. of Physics, Huazhong Univ. of Science and Technol- of plasmon-based configurations as compared to purely what we can do to help avoid such short-sighted actions. ogy, China. We report an optical wave-mixing-enhanced dielectric structures. Zeeman-coherence atomic magnetometry scheme that results in sub-nT magnetic field detection at human-body temperatures without magnetic field shielding, zero-field compensation, or RF-modulation spectroscopy.

FW2E.2 • 09:15 Multiaxis, Single-Laser Atom Interferometer for Inertial Sensing, Xuejian Wu1, Jordan Dudley1, Fei Zi1,2, Holger Müller1; 1Univ. of California, Berkeley, USA; 2Zhejiang Univ., China. We demonstrate a multiaxis atom interferometer based on a pyramidal magneto-optical trap and one diode laser. Being simple and capable of multiaxis operation, our atomic sensor opens up applications in geodesy, geology, or inertial navigation.

FW2E.3 • 09:30 Invited LW2F.2 • 09:30 Precision Inertial Measurements with Cold Atom Interfer- High-repetition-rate, Nanosecond, Self-Q-switched ometers, Remi Geiger1, Bess Fang1, Denis Savoie1, Matteo Cr,Nd:YAG Microchip Laser for Stable Vortex Beam, Jun Wednesday, 20 Septem Altorio1, Nicolas Mielec1, almazbek imanaliev1, romain karch- Dong1, Hongsen He1; 1Xiamen Univ., China. Stable vortex er1, Carlos Garrido Alzar1, Sébastien Merlet1, Franck Pereira beams have been generated in a self-Q-switched Cr,Nd:YAG Dos Santos1, Arnaud Landragin1; 1LNE-SYRTE, Observatoire microchip laser with the pulse width of 8.5 ns and repetition de Paris, PSL Research Univ., CNRS, Sorbonne Universités, rate of 113 kHz. The lasing threshold for optical vortex is UPMC Univ. Paris 06, France. This talk will describe the prin- just 1.2 W. ciple of cold atom interferometers and review some recent results in the field of precision inertial measurements. It will LW2F.3 • 09:45 present different applications in basic science and related Optically indcued alignement of gold nanorods and to industrial developments. dichroism in plasmonic nanosuspesnions, Pepito Bustos Alvaro1, Trevor Kelly1, Yu-xuan Ren1, HUIZHONG Xu1, Zhigang Chen1,2; 1San Francisco State Univ., USA; 2Nankai

Univ, China. We demonstrate soliton-mediated, polariza- ber tion-dependent alignment of gold nanorods in colloidal suspensions. We discuss orientation-enhanced dichroism due to disorder-to-order transition of nanorods resulting from the torque exerted by soliton beam.

10:00–10:30 Coffee Break, Science & Industry Showcase, Columbia, Terrace Level

10:00–12:00 JW3A • Science & Industry Showcase Exhibits, Poster Session & E-Posters Rapid-Fire Oral Presentations III in Theater Columbia, Terrace Level

FiO + LS 2017 • 17–21 September 2017 57 10:00–12:00 JW3A • Science & Industry Showcase Exhibits, Poster Session & E-Posters Rapid-Fire Oral Presentations III in Theater Columbia, Terrace Level

Science Showcase Theater JOINT FiO + LS

10:00–11:00 JW3A • Rapid-Fire Oral Presentations III

JW3A.19 • 10:00 RAPID JW3A.35 • 10:15 RAPID JW3A.77 • 10:30 RAPID Nonlinear Coupled Mode Equations for Kerr Comb Influence of Counterpropagating Light on Phase Plasmonic Filter Arrays for Infrared Spectral Recon- Generation in Coupled Microcavity System, Shun Fujii1, Matching in Second Harmonic Generation, Amy L. Ly- struction, Benjamin Craig1, Kenneth B. Crozier1; 1Univ. of Yusuke Okabe1, Takumi Kato1, Ryo Suzuki1, Atsuhiro Hori1, tle1, Thomas Lehman-Borer1, Etienne Gagnon1; 1Franklin Melbourne, Australia. We experimentally demonstrate an Takasumi Tanabe1; 1Keio Univ., Japan. We performed a & Marshall College, USA. Experimental and numerical array of plasmonic infrared transmission filters. We show, rigorous numerical simulation of Kerr comb generation results verify the influence of counterpropagating light on by simulations that include noise, reconstruction of the with nonlinear coupled mode equations including mode phase matching of SHG, enhancing conversion efficiency spectra of infared light sources from measurements of coupling between two different mode families. The by up to 20%, toward understanding and implementation the energy transmitted through each filter. calculated results agree well with experimental results. of an all-optical method for quasi-phase matching. JW3A.80 • 10:35 RAPID JW3A.20 • 10:05 RAPID JW3A.75 • 10:20 RAPID Planar Optics with High Numerical Apertures at Controllable photon quantum state generation in Differential Polarisation-sensitive Photodetectors Visible Wavelengths, Wei-Ting Chen1, Alexander Zhu1, multimode optical fibers, Hamed Pourbeyram1, Arash Design Utilising Plasmonic Metasurfaces, Evgeniy Mohammadreza Khorasaninejad1, Zhujun Shi1, Federico Mafi1; 1Univ. of New Mexico, USA. We present the multi- Panchenko1, Jasper J. Cadusch1, Timothy D. James1, Capasso1; 1Harvard Univ., USA. We report high numerical mode optical fiber as a robust and practical platform to Lukas Wesemann1, Ann Roberts1; 1The Univ. of Mel- aperture planar optics using metasurfaces. Meta-axicons manipulate and control the quantum state of light using bourne, Australia. We propose and demonstrate a CMOS and immersion meta-lenses with numerical apertures various linear and nonlinear mechanisms. compatible plasmonic antenna-based differential photo- up to 1.1 are demonstrated; they can generate wave- detector. Our design permits using differential detection length-independent Bessel beams and diffraction-limited JW3A.34 • 10:10 RAPID techniques in telecommunication systems potentially focal spots. Temporal Amplitude & Phase: Algorithmic Recon- significantly increasing the data transmission rate. struction via Time-domain Interferometry (TeAPARTI), Joseph H. Munns2,1, Sang Park1, Benjamin Brecht1, Ian JW3A.76 • 10:25 RAPID A. Walmsley1; 1Univ. of Oxford, UK; 2Imperial College Bio-sensing with asymmetric THz metasurfaces, Joshua London, UK. We introduce a novel protocol for the Burrow1, Thomas Searles2, Imad Agha1,3, Jay Mathews3,1; complex characterisation of nanosecond duration pulses 1Electro-Optics and Photonics, Univ. of Dayton, USA; -- TeAPARTI -- and apply it to different test pulses. In all 2Physics & Astronomy, Howard Univ., USA; 3Physics, Univ. cases, the reconstructed intensity and phase profiles of Dayton, USA. We demonstrate an asymmetric 4-gap agree very well with the target pulses. square ring resonator terahertz (THz) metasurface as an ultra-sensitive biological sensor. Polarization-insensitive modes due to asymmetry exhibit low minimal detectable concentration of bovine serum albumin. ber Wednesday, 20 Septem Wednesday,

58 FiO + LS 2017 • 17–21 September 2017 Science & Industry Showcase

JOINT FiO + LS

10:00–12:00 JW3A • Joint Poster Session III

JW3A.1 E-Poster JW3A.9 E-Poster JW3A.14 Colossal Bunching in Nanodiamond Cathodolumines- Broadband Near Infrared Supercontinuum for Z-Scan Adjoint Optimization for Automated Metasurface Mir- ror Design, 1 2 cence, Matthew A. Feldman1,2, Roderick Davidson1,2, Nonlinear Spectrometer, Natalia Múnera2,1, Peng Jason Herrmann , Turner Silverthorne , Alex- 3 2 1 Jordan Hachtel1,2, Eugene Dumitrescu2, Raphael Poos- Zhao2, Rodrigo Acuna Herrera1, David J. Hagan2, Eric W. ander Y. Piggott , Michal Bajcsy ; Physics Dept., Harvard 2 3 er2, Anming Hu3, Denzel Bridges3, Phil Evans2, Richard Van Stryland2; 1Escuela de Fisica, Universidad Nacional Univ., USA; IQC, Univ. of Waterloo, Canada; Ginzton Haglund1, Benjamin Lawrie2; 1Dept. of Physics and As- de Colombia Medellin, Colombia; 2CREOL, Univ. Of Lab, Stanford Univ., USA. We apply adjoint optimization tronomy, Vanderbilt Univ., USA; 2Oak Ridge National Lab, Central Florida, USA. High-spectral-irradiance infrared to automate the design of high-reflectivity metasurface USA; 3Dept. of Mechanical, Aerospace and Biomedical supercontinuum with fundamental gaussian spatial profile mirrors for gaussian beams. Adjoint techniques reduce Engineering, Univ. of Tennessee, USA. Photon bunching was generated in Krypton gases. We demonstrate its requisite computation time and power, as well as the need with g(2)(0)>30 was observed in cathodoluminescence usefulness for Z-scan nonlinear spectroscopy in the 800- for a known starting structure. from nanodiamond particles coupled to Ag surface-plas- 1600nm spectral range using GaAs and CS2. mon polaritons. Comparisons with the photon bunching JW3A.15 One Dimensional Atom Microscopy Via Surface Plas- of diamond nanoparticles point to Ag-plasmon-mediated JW3A.10 E-Poster mon Polariton, 1 1 decoherence processes. Plasmonic sensing beyond the shot noise limit, Ashok Syed A. Shah , Sana Ullah , Muhammad 1 1 1 1 Kumar1, Mohammadjavad Dowran1, Benjamin Lawrie2, Idrees , Bakht A. Bacha , Arif Ullah ; Dept. of Physics, JW3A.2 E-Poster Raphael Pooser2, Alberto Marino1; 1Univ. of Oklahoma, Univ. of Malakand, Pakistan. We demonstrate the possi- Photonic transport in disordered multiqubit non-chiral USA; 2Oak Ridge National Lab, USA. We demonstrate a bility for atom localization via surface plasmon polariton. waveguide QED., Imran M. Mirza1; 1Univ. of Michigan sensitivity enhancement of plasmonic sensors by a factor A single and double localized peaks are observed in the , USA. We study photon transport in one-dimensional of 1.6 beyond the shot noise limit using quantum states absorption/dispersion spectrums of surface plasmon waveguide side coupled to a position disordered mul- of light. Our results show the potential to enhance the polariton. tiqubit array. Particularly, we show how emitter-waveguide sensitivity of real-life devices. coupling influences the formation of localized photonic JW3A.16 The entangled quantum photons generation in whis- states under varying disorder strength. JW3A.4 Spectrally Multiplexed Upconversion Single-Photon pering gallery mode resonator of silica microsphere, 2,1 1 JW3A.3 E-Poster Detection with C-band Pump and Signal Wavelengths, Jingming Cao ; Univ. of Erlangen-Nuremberg, Germa- 2 Quantum tomography with all-dielectric metasurfaces, Michael L. Silver1, Vesselin Velev1, Carsten Langrock2, Mar- ny; The school of Advanced Optics and Technology, Kai Wang1, Sergey S. Kruk1, Lei Xu1,2, Matthew Parry1, tin Fejer2, Prem Kumar1, Gregory Kanter1; 1Northwestern Germany. The modeled and fabricated apparatus to gen- Hung-Pin Chung1,3, James Titchener1, Ivan Kravchenko4, Univ., USA; 2Stanford Univ., USA. We demonstrate low erate the nonclassic light source of entangled quantum Yen-Hung Chen3, Alexander S. Solntsev1, Yuri S. Kivshar1, noise, spectrally multiplexed, upconversion single-photon photons in the normal dispersion regime by the enhanced Dragomir N. Neshev1, Andrey A. Sukhorukov1; 1Nonlinear detection using a waveguide with multiple phase-match- higher quality factor in waveguide of silica microsphere Physics Centre, Research School of Physics and Engineer- ing peaks. Two signal wavelengths are upconverted using in modern optics applications. ing, The Australian National Univ., Australia; 2The MOE two distinct pump wavelengths, all in the 1550-nm band. Key Lab of Weak Light Nonlinear Photonics, School of JW3A.17 Nondegenerate Two Photon Carrier Generation in Physics and TEDA Applied Physics Inst., Nankai Univ., JW3A.8 Multiple Quantum Well for the C-Band Telecommuni- China; 3Dept. of Optics and Photonics, National Central Strong suppression of forward or backward Mie cation, 1,2 Univ., Taiwan; 4Center for Nanophase Materials Sciences, scattering by using partial coherence, Taco D. Visser1, Carlos Andres Alvarez Ocampo , Rodrigo Acuna 1 1 Oak Ridge National Lab, USA. We suggest and realize yangyundou wang2, Hugo Schouten1; 1Vrije Universiteit, Herrera ; Escuela de Fisica, Universidad Nacional de 2 experimentally dielectric metasurfaces with high trans- Amsterdam, Netherlands; 2NPU, China. The intensity of Colombia-Medellin, Colombia; Ciencias Basicas, Univer- mission efficiency for quantum multi-photon tomography, forward- or backward Mie scattering can be suppressed sidad de Medellin, Colombia. We study numerically the allowing for full reconstruction of pure or mixed quantum several orders of magnitude by tuning the coherence Two Photon Carrier Generation in Multiple Quantum Well made of Al Ga As for the c-band telecommunication via polarization states across a broad bandwidth. length of a J_0 Bessel correlated field. x 1-x Nondegenerate Two Photon Absorption. We show how JW3A.5 E-Poster JW3A.11 the mole fraction x and probe wavelength are important.

Frequency comb manipulation by photonic gauge Large Purcell Enhancement with Efficient One-di- Wednesday, 20 Septem potentials, Chengzhi Qin1, Bing Wang1, Peixiang Lu1; mensional Collection via Coupled Nanowire-nanorod JW3A.18 A Quantum Opto-plasmonic Capacitor for Low-power 1Huazhong Univ of Science and Technology, China. We System, Xue k. Duan1, Juanjuan Ren1, Fan Zhang1, He High-speed Information Processing, 2 experimentally demonstrate photonic gauge potential in Hao1, Guowei Lu1,2, Ying Gu1,2, Qihuang Gong1,2; 1State Pouya Dianat , 1 1 2 frequency dimension based on electro-optic phase mod- Key Lab for Mesoscopic Physics, Collaborative Innovation Bahram Nabet ; Drexel Univ., USA; Electrical Engineer- ulators. The gauge potentials can be used to manipulate Center of Quantum Matter, Dept. of Physics, Peking ing and Computer Sciences, Northwestern Univ., USA. frequency comb evolution, leading to spectral shift and Univ., China; 2Collaborative Innovation Center of Extreme A quantum plasmonic photodetector is described with bandwidth expansion. Optics, Shanxi Univ., China. Spontaneous emission is integrated low-power logic operations of ~9aJ/bit and enhanced by thousands of times based on excitation of unbounded by transport limitations. This is achieved by JW3A.6 E-Poster gap surface plasmons in the coupled system. More than optoelectrical exploitation of quantum-exclusive energies Ultrafast Insulator-Metal Transition in Strained Vanadi- 50% of emitted photons are guided along one dimension of interacting 2D hole plasma. um Dioxide Films, Ryan J. Suess1, Nicholas S. Bingham2, in subwavelength scale. 3 3 3 JW3A.19

Kristin Charipar , Heungsoo Kim , Scott Mathews , Alber- ber Nonlinear Coupled Mode Equations for Kerr Comb to Pique3, Nicholas Charipar3; 1Nova Research, Inc., U.S. JW3A.12 Generation in Coupled Microcavity System, 1 Naval Research Lab, USA; 2National Research Council Current gain compression in strain-balanced SiGeSn/ Shun Fujii , 1 1 1 1 Research Associate, U.S. Naval Research Lab, USA; 3U.S. GeSn based transistor laser, Ravi Ranjan1; 1Electronics Yusuke Okabe , Takumi Kato , Ryo Suzuki , Atsuhiro Hori , Takasumi Tanabe1; 1Keio Univ., Japan. We performed a Naval Research Lab, USA. Strained VO2 films are charac- Engineering, Indian Inst. of Technology (Indian School terized by optoelectronic autocorrelation measurements of Mines), India. We present the design of SiGeSn/GeSn rigorous numerical simulation of Kerr comb generation that reveal a material response of 400 fs. This suggests the based transistor laser. Collector current density as a func- with nonlinear coupled mode equations including mode coupling between two different mode families. The insulator-metal transition in strained VO2 can be activated tion of collector-emitter voltage for different injected base by electronic, rather than thermal, means. current density in common-emitter mode is calculated to calculated results agree well with experimental results. show the current gain compression. JW3A.7 E-Poster JW3A.20 Single Peaked Optical Ramsey Interference with JW3A.13 Controllable photon quantum state generation in multimode optical fibers, 1 Repeated Query Interrogation, Zachary Warren1, Renu Single photon generation at 785nm in CMOS compat- Hamed Pourbeyram , Arash 1 1 Tripathi1, Gour S. Pati1; 1Delaware State Univ., USA. In this ible photonic devices, Robert Cernansky1, Francesco Mafi ; Univ. of New Mexico, USA. We present the multi- paper, we have proposed a repeated query technique Martini1, Alberto Politi1; 1Univ. of Southampton, UK. mode optical fiber as a robust and practical platform to as a new interrogation method for acquiring Ramsey Single photon sources are crucial components for any manipulate and control the quantum state of light using interference fringes with enhanced central fringe and future quantum photonic technology. We demonstrate various linear and nonlinear mechanisms. suppressed side fringes. generation of non-classical states of light for quantum computation using CMOS compatible PECVD SiN ring resonator at near-visible wavelengths.

FiO + LS 2017 • 17–21 September 2017 59 Science & Industry Showcase

JOINT FiO + LS

JW3A • Joint Poster Session III—Continued

JW3A.21 JW3A.28 JW3A.36 Generation of near-infrared correlated photon pairs Investigations of Nonlinear Optical Properties of Improving the Detection of Squeezed Light in the Pres- in a long optical nano-fibers, Jin-Hun Kim1, Yong Sup Diamond Nanoparticles using Z-scan Technique, Renu ence of Loss, Tian Li1, Brian E. Anderson1, Travis Horrom1, Ihn1, Heedeuk Shin1, Yoon-Ho Kim1; 1physics, POSTECH, Tripathi1, Michael J. Williams1, gour s. pati1; 1Delaware Bonnie L. Schmittberger1, Kevin Jones2, Paul D. Lett1,3; South Korea. We report generation of frequency-nonde- State Univ., USA. We present results from investigations 1Univ. of Maryland at College Park, USA; 2Williams Col- generate correlated photon pairs in an 8 cm-long optical of third-order nonlinear optical properties of diamond lege, USA; 3Quantum Measurement Division, NIST, USA. nano-fiber. The coincidence-to-accidental ratio bigger nanoparticles suspended in dimethylformamide (DMF) Squeezed light has many applications, but its quantum than 400 has been achieved at a very low average pump solvent using the single-beam Z-scan technique at advantages disappear quickly with increasing loss. Here power of 50 µW. 1064 nm. we show that a four-wave-mixing-based phase-sensitive amplifier can be used to preserve squeezing even in the JW3A.22 JW3A.29 presence of substantial loss. Evanescent field controlled entanglement modulation Withdrawn. in a plasmonic nanoparticle-emitters hybrid system, JW3A.37 Fan Zhang1, Xue k. Duan1, Juanjuan Ren1, zhao chen1, Ying JW3A.30 Dynamics of Quantum Dot Lasers Subject to Polariza- Gu1,2, Qihuang Gong1,2; 1State Key Lab for Mesoscopic Spatially Dependent Replica Symmetry Breaking in an tion-Rotated Feedback, Salim Ourari1, Tianyao Huang1, Physics, Collaborative Innovation Center of Quantum Optofluidic Random Laser, Anirban Sarkar1, Jonathan Hong Lin1; 1Bates College, USA. Polarization-rotated Matter, School of Physics, Peking Univ., China; 2Collabo- Andreasen2, Shivakiran Bhaktha B. N.1; 1Indian Inst. of optical feedback stimulates orthogonal polarization in a rative Innovation Center of Extreme optics, Shanxi Univ., Technology Kharagpur, India; 2Georgia Tech Research quantum dot laser. The frequency of feedback dynamics China. We theoretically demonstrate the evanescent-field Inst., USA. We study replica symmetry breaking (RSB) in an is decreased by a factor of 2 when the polarization of controlled entanglement modulation in a dielectric optofluidic random laser. Using a pump-probe technique feedback is rotated by a large angle. nanowire, emitters and Ag nanoparticle hybrid system. recently developed to map the lasing modes results in Modulation range of 0-0.75 has been achieved by varying RSB only at the edges of the pumped region. JW3A.38 incident field amplitude and detunings. Limints on conditional photon statistics manipulation JW3A.31 via interference of weak lasers, Kang-Hee Hong1, JW3A.23 Four-Wave Mixing in Potassium Vapor, Ryan T. Glasser1, Jisung Jung2, Young-Wook Cho2, Sang-Wook Han2, High Efficient Grating Couplers and an Effective Nano- Jon D. Swaim1; 1Tulane Univ., USA. We demonstrate Sung Moon2, Kyunghwan Oh3, Yong-Su Kim2, Yoon-Ho fabrication Method for High Performance Plasmonic the generation of bright, squeezed twin beams via a Kim1; 1Pohang Univ of Sci & Tech (POSTECH), South Waveguides, Zahraa Al-Baiaty1,2, Benjamin P. Cumming2, four-wave mixing process in warm potassium vapor, in Korea; 2Center for Quantum Information, Korea Inst. of Xiaosong Gan1, Min Gu2; 1Swinburne Univ., Australia; which strong asymmetric absorption is present between Science and Technology (KIST), South Korea; 3Dept. of 2RMIT Univ., Australia. We developing efficient and high the two modes. Physics, Yonsei Univ., South Korea. We report theoretical performance nanoplasmonic waveguides. Our results analysis on the limits of manipulating conditional photon show enhancement in the intensity and propagation dis- JW3A.32 statistics via interference of weak lasers. We demonstrate tance of the propagating plasmons by introducing an op- Hybrid photon model bridges classical and quantum explicitly that photon anti-bunching cannot be obtained timized grating coupler utilizing efficient nanofabrication. optics, Chandra Roychoudhuri1,2; 1Univ. of Connecticut, in such a scheme. USA; 2Femto Macro Continuum, USA. Photons are transient QM energy packets at emission that evolve as JW3A.39 JW3A.24 Huygens wave-packets. We use the quantum cup postu- Dynamic Characteristics of VCSELs with Combined Optical Greatly enhanced strong photon-exciton coupling in late, along with known interferometric and spectrometric Injection and Feedback, Niccolo Bigagli1, Aashu Jha1, Hong two dimensional evanescent-vacuum, Juanjuan Ren1, data to resolve the currently perceived contradictions. Lin1; 1Bates College, USA. We explore dynamics of a VCSEL He Hao1, Xue k. Duan1, Fan Zhang1, Tiancai zhang2, Ying with simultaneous optical injection and feedback. Broadband Gu1, Qihuang Gong1; 1Peking Univ., China; 2Shanxi Univ., JW3A.33 dynamics is achieved for combination of feedback of differ- China. Taking the two dimensional evanescent vacuum as Size-scale analysis of spin detection sensitivity in ent polarizations and parallel injection. electromagnetic background, we theoretically investigate miniature vapor cells, Ricardo Jimenez-Martinez1; 1ICFO- the enhanced strong photon-exciton coupling, where the Inst. of Photonic Sciences, Spain. I describe a size-scale JW3A.40 coupling coefficients with silver plate can be 7.6 times analysis of spin-detection sensitivity in miniature, i.e. Von Neumann Entropy in a Cross Cavity, Julio Cesar larger than that without plate. microfabricated, vapor cells and discuss tools and tech- Garcia Melgarejo2, Nestor Lozano-Crisostomo2, Rodolfo niques that can be deployed to enhance it. Mena-Montes2, Edgar S. Arroyo-Rivera1, J. Javier San- ber JW3A.25 chez-Mondragon1; 1Inst Nac Astrofisica Optica Electron- Study of GeSn Strain Compensated Quantum Well as JW3A.34 ica, Mexico; 2Facultad de Ingenieria Mecanica y Electrica, EAM, Prakash Pareek1, Ravi Ranjan1, Mukul K. Das1; 1Indi- Temporal Amplitude & Phase: Algorithmic Recon- Universidad Autonoma de Coahuila, Mexico. We discuss an Inst. of Technology (indian School of Mines) Dhanbad, struction via Time-domain Interferometry (TeAPARTI), the entropy between a two-level atom and a cross-cavity India. Study of Stark effect in strain compensated GeSn Joseph H. Munns2,1, Sang Park1, Benjamin Brecht1, Ian resulting in an extended lifetime of the entanglement. quantum well is done by calculating field dependent A. Walmsley1; 1Univ. of Oxford, UK; 2Imperial College absorption considering excitonic effect. A significant London, UK. We introduce a novel protocol for the JW3A.41 change in refractive index is determined which confirmed complex characterisation of nanosecond duration pulses Waiting time distributions for the first photodetection its potentiality as modulator. -- TeAPARTI -- and apply it to different test pulses. In all for classical and quantum light sources, Reeta Vyas1, cases, the reconstructed intensity and phase profiles Surendra Singh1; 1Univ. of Arkansas, USA. Waiting time JW3A.26 agree very well with the target pulses. probabilities for detecting the first photon, starting Modeling of Dark Count Rate of InGaAs/InP Single Pho- at an arbitrary instant, from stationary quantum and Wednesday, 20 Septem Wednesday, ton Avalanche Photodiode Gated with Soliton Signal, JW3A.35 classical light sources, and information they contain are Ahmed C. Kadhim1, Susan Earles1, Ahmad S. Azzahrani1, Influence of Counterpropagating Light on Phase discussed and analytic expressions for several sources Muhammad Riaz1, Mano R. Pakalapati1; 1Electrical and Matching in Second Harmonic Generation, Amy L. Ly- are presented. Computer Engineering, Florida Inst. of Technology, USA. tle1, Thomas Lehman-Borer1, Etienne Gagnon1; 1Franklin Dark count rate (DCR) of InGaAs/InP SPAD is modeled & Marshall College, USA. Experimental and numerical JW3A.42 using soliton gating signal and compared to experimen- results verify the influence of counterpropagating light on Coherence in the Jaynes-Cumming Model, Julio Cesar tal counts of sinusoidal gating. Simulation results show phase matching of SHG, enhancing conversion efficiency Garcia Melgarejo2, J. Javier Sanchez-Mondragon1, Nestor that soliton has fewer effects of excess voltage on DCR. by up to 20%, toward understanding and implementation Lozano-Crisostomo2, Edgar S. Arroyo-Rivera1, Daniel A. of an all-optical method for quasi-phase matching. May-Arrioja3, D E. Ceballos-Herrera4, Miguel Torres-Cis- JW3A.27 neros5; 1Inst Nac Astrofisica Optica Electronica, Mexico; Soliton Pulse Gated InGaAs/InP Avalanche Photodiode 2FIME, Universidad Autonoma de Coahuila, Mexico; for Low Dark Count Rate Single Photon Detection, 3Centro de Investigaciones en Optica, Mexico; 4UNAM, Ahmed C. Kadhim1, Susan Earles1, Muhammad Riaz1, Mexico; 5Universidad de Guanajuato, Mexico. We present Ahmad S. Azzahrani1, Mano R. Pakalapati1; 1Florida Inst. a realistic way to explore the Coherence of the quantum of Technology , USA. A mathematical model for dark field through the analysis of the JCM in a cross-cavity. We count rate of soliton pulse gated InGaAs/InP SPAD is also explore the dipole and photon number coherence. developed. The results are compared with experimental counts of Gaussian gating. Simulation results show that Soliton gating width reduced the DCR.

60 FiO + LS 2017 • 17–21 September 2017 Science & Industry Showcase

JOINT FiO + LS

JW3A • Joint Poster Session III—Continued

JW3A.43 JW3A.50 JW3A.57 Dynamical Aspects of Lasing Inside Microcavities High-Q Optical Cavities at Visible Wavelengths in Emission and lasing properties of CdS nanoribbons Without Resorting to the Concept of Density of Photonic Crystals in the Anderson-localized regime, modulated by strain-engineering, Liaoxin Sun1, Qi Modes, Tracy Robertson1, Serge Gauvin1; 1Physique et Tom Crane1, Oliver Trojak1, Luca Sapienza1; 1Univ. of Wang1, Fangfang Sun1, Bo Zhang1, Xuechu Shen1, Wei astronomie, Université de Moncton, Canada. Optical Southampton, UK. We demonstrate Anderson localization Lu1; 1Shanghai Inst. of Technical Physics, China. The confinement allows manipulation of spontaneous emis- of visible light in silicon nitride photonic crystals. We periodic buckling of CdS nanoribbons is fabricated sion. Density of modes is used to account for this effect. measure optical resonances by disorder-induced light and the strain-modulated exciton and exciton-phonon However, another interpretation based on modulation of localization showing quality factors of ≈ 10000 that exceed coupling are clearly observed in PL mapping. Moreover, vacuum field fluctuations leads to a new description of engineered 2D photonic crystal cavities. the strain-dominated mode selection in multi-mode laser thresholdless lasers. is presented. JW3A.51 JW3A.44 Bloch-surface-polariton based hybrid waveguide for JW3A.58 Unidirectional Scattering by All-dielectric Cuboidal low loss light propagation at the subwavelength scale, Flexible Hybrid Microdisk Cavity for Lasing, Jie Zhou1,2, Nanoparticle, Richa Mantri1, Reena Dalal1, Ajeet Ku- Weijing Kong1, Yuhang Wan2, Xiaochang Ni1, Wenhui Taojie Zhou2, Jiagen Li2, Kebo He2, Zhaoyu Zhang2; 1Pe- mar1; 1Delhi Technological Univ., India. In this paper, we Zhao1, Zheng Zheng2; 1School of Electronic Engineering, king Univ., China; 2Chinese Univ. of Hong Kong, China. report unidirectional scattering by all dielectric cuboidal Tianjin Univ. of Technology and Education , China; 2School The authors propose a hybrid microdisk cavity embedded nanoparticle. The variation in scattering cross section, of Electronic and Information Engineering, Beihang Univ. in flexible medium for lasing applications. The 2-µm-di- far field and directivity are studied when material of the , China. A novel hybrid Bloch surface polariton waveguide ameter microdisk features a lasing threshold of 1.2 µW cuboid is changed from Silicon (Si) to Germanium (Ge). by integrating a periodic multilayer structure with metallic and lasing wavelength of ~680 nm with a linewidth of 0.3 nanowire is proposed and investigated. The results reveal nm at room temperature. JW3A.45 a deep-subwavelength mode confinement with reason- Surface Plasmon Polariton Amplification in a Single able propagation distance. JW3A.59 Carbon Nanotube by Direct Electric Current, Sergey G. Modification of Charge Carrier Mobility by Strong Moiseev1, Aleksei S. Kadochkin1, Yuliya S. Dadoenkova1, JW3A.52 Light-Matter Coupling in Organic and Inorganic Semi- Igor O. Zolotovskii1; 1Ulyanovsk State Univ, Russia. A Disorder-Induced Light Confinement in Photonic conductors, Henry Fernandez1, Saverio Russo1, William mechanism of amplification of surface plasmon polaritons Crystals as a Platform for Efficient Optical Sensing, Barnes1; 1Dept. of Physics and Astronomy, Univ. of Exeter, due to the transfer of electromagnetic energy from a drift Oliver Trojak1, Tom Crane1, Luca Sapienza1; 1Univ. of UK. Strong light-matter coupling is anticipated to modify current into a terahertz surface wave propagating along Southampton, UK. We demonstrate optical sensing with the electronic properties of semiconductor materials. We the single-walled carbon nanotube is proposed. disorder-induced confined light on silicon nitride photonic discuss an experiment suited to study the charge mobility crystal waveguides. For a refractive index change of of semiconductors where exciton modes are coupled to JW3A.46 ≈0.38, we measure 14 nm wavelength shifts of an optical tuneable microcavity modes. High-Mobility Transparent Conducting Oxides for resonance 0.4 nm broad. Compact Epsilon-Near-Zero Silicon Integrated Optical JW3A.60 Modulators, Michael G. Wood1, Salvatore Campione1, JW3A.53 Two-dimensional Phononic Crystal Design with Large Darwin Serkland1, S Parameswaran1, Jon Ihlefeld1, Ting Electrically Pumped Spaser Based on Semiconductor Band Gaps, Shuo Li1, Yangfan Li2, Fei Meng2, Han Lin1, Luk1, Joel R. Wendt1, Kent Geib1, Gordon Keeler1; Film with Graphene Nanosheet, Sergey G. Moiseev1, Xiaodong Huang2, Baohua Jia1; 1Centre for Micro-Pho- 1Sandia National Labs, USA. We study the role of carrier Yuliya S. Dadoenkova1, Igor O. Zolotovskii1; 1Ulyanovsk tonics, Swinburne Univ. of Technology, Australia; 2Faculty mobility in transparent conducting oxides integrated into State Univ, Russia. A model of slow surface plasmon of Science, Engineering and Technology, Swinburne Univ. epsilon-near-zero modulators. High-mobility materials in- polariton distributed feedback laser (spaser) based on of Technology, Australia. We present unit-cell designs cluding CdO enable sub-micron length electroabsorption semiconductor film with pump by drift current in graphene for 2D phononic crystals formed by solid-solid materials modulators through >4dB/µm extinction ratios. is proposed. with large phononic band gaps for (1) out-of-plane, (2) in-plane, and (3) combined out- and in-plane elastic waves JW3A.47 JW3A.54 propagation, based on Voronoi diagram. The cutoff and critical power of Modulation Instability Extreme Twists of Light in Photonic Crystal Wave- (MI) gain in Silicon-on-insulator (SOI) Nanowaveguides , guides, Isabelle Palstra1, Dolfine Kosters2, Filippo JW3A.61 Deepa Chaturvedi1, Ajit Kumar1; 1Indian Inst. of Technolo- Alpeggiani2, Kobus Kuipers2; 1Center for Nanophotonics, Experimental demonstration of coherent light emission Wednesday, 20 Septem gy, Delhi, India. We have studied the effect of free-carriers AMOLF, Netherlands; 2Dept. of Quantum Nanoscience, by a metallic optofluidic cavity exploiting continuous (FC) on MI gain in SOI nanowaveguides. The MI analysis Kavli Inst. of Nanoscience, Netherlands. We demonstrate pump, Hailang Dai1, Xianfeng Chen1; 1Shanghai Jiaotong is carried out in the nanowaveguides with anomalous that superchiral near fields, fields that are essentially more Univ., China. Ultralow-threshold continuous wave micro- and normal group velocity dispersion (GVD) parameters. twisted than circularly polarized light, exist above conven- fluidic dye laser based on hollow-core metal-cladding tional silicon photonic crystal waveguides. We envision optical waveguide.For Methylene blue with concentration JW3A.48 using these fields to accurately sense chiral molecules. of 2.57*10-13 mol/ml, can be observed with the launched Cascaded Floquet Resonators as Dual-Carrier Optical pump threshold bolew 2.1 μW/cm2 lasing. Circulators, Ian Williamson1, Zheng Wang1; 1The Univ. of JW3A.55 Texas at Austin, USA. Floquet resonances arising in tem- Defect States Emerging from a non-Hermitian Flat JW3A.62 porally modulated resonators exhibit highly nonreciprocal Band of Photonic Zero Modes, Bingkun Qi1,2, Li Ge1,2; Ge-ZnS Mid-IR Wideband Resonant Reflectors, Dan- responses when coupled to external photonic structures. 1College of Staten Island, CUNY, USA; 2Physics, The iel J. Carney1, Robert Magnusson1; 1Univ. of Texas at We demonstrate a circulator response to a dual-carrier Graduate Center, CUNY, USA. We report the emergence Arlington, USA. We provide design and fabrication of ber input compatible with on-chip photonic systems. of a defect state in a photonic flat band with non-Her- robust GMR devices operating in the 3-15 µm spectral mitian particle-hole symmetry. It can be viewed as an range. Optimized reflectors are designed with inverse JW3A.49 unconventional alignment of a pseudo-spin in a complex numerical methods. Preliminary experimental spectra Impact of Fourth-order dispersion (FOD) parameter magnetic field. agree qualitatively with theory. on Modulation Instability (MI) in Silicon-On-Insulator (SOI) Nanowaveguides , Deepa Chaturvedi1, Ajit Kumar1; JW3A.56 JW3A.63 1Indian Inst. of Technology, Delhi, India. We have studied Trapezoidal Sub-wavelength Grating Micro-Ring Robustness of single mode PT lasers, Mohammad the MI gain due to second-order dispersion (SOD) and Resonator with High Quality Factor, Elnaz Akbari1; Hosain Teimourpour2, Ramy El-Ganainy2,1; 1Michigan FOD parameters in SOI nanowaveguides and discussed 1Electrical, GWU, USA. We report the trapezoidal structure Technological Univ. , USA; 2Dept. of Physics and Henes the impact of FOD parameter on the MI gain spectra subwavelengeth grating waveguide micro ring resonator Center for Quantum Phenomena, Michigan Technological existing due to SOD parameter. with high quality factors 10474 for 3.1μm radius. Trape- Univ., USA. We investigate the robustness of single lon- zoidal shape can significantly reduce the bend loss and gitudinal mode operation in PT symmetric lasers against therefore increase the quality factors. instabilities triggered by spectral hole burning effects. Results, supported by numerically integrating the rate equations and linear stability analysis.

FiO + LS 2017 • 17–21 September 2017 61 Science & Industry Showcase

JOINT FiO + LS

JW3A • Joint Poster Session III—Continued

JW3A.64 JW3A.71 JW3A.78 Mode selectivity in PT symmetric lasers, Mohammad Raman Comb Formation in Silica Rod Microresonator, Broadband polarization-independent selective absorb- Hosain Teimourpour1, Ramy El-Ganainy1; 1Dept. of Physics Ryo Suzuki1, Akihiro Kubota1, Shun Fujii1, Atsuhiro Hori1, er enabling large angle acceptance, Xu Han1,2, Kebo and Henes Center for Quantum Phenomena, Michigan Takumi Kato1, Takasumi Tanabe1; 1Keio Univ., Japan. We He2, Zhaoyu Zhang2; 1School of Electronic and Computer Technological Univ., USA. We introduce a general scheme report smooth Raman comb generation with a linewidth Engineering, Shenzhen Graduate School, Peking Univ., for controlling mode selectivity in PT symmetric lasers via of a few kHz despite a complex Raman gain. The center China; 2School of Science and Engineering, Chinese inhomogeneous loss engineering. wavelength was controlled depending on the pump Univ. of Hong Kong, Shenzhen, China. A broadband detuning. polarization-insensitive selective solar absorber is shown JW3A.65 to have beyond 90% absorptance from 0.5μm to 1.75μm Non-Hermitian Particle-Hole Symmetry and its Impli- JW3A.72 and predicted absorptance below 12.6% from 2.5μm to cations in Photonic Systems, Li Ge1,2; 1College of Staten Third Order Nonlinear Properties of GeSbS Chalco- 4μm, while showing large angle acceptance. Island, CUNY, USA; 2Graduate Center, CUNY, USA. I genide Waveguides, Samuel F. Serna Otálvaro1,4, Hong- will discuss how particle-hole symmetry, a fermionic tao Lin2, Carlos Alonso-Ramos1, Anupama Yadav3, Xavier JW3A.79 symmetry in condensed matter systems, can be realized Le Roux1, Kathleen Richardson3, Eric Cassan1, Nicolas Magneto-optical waveguiding InSb-based structures in non-Hermitian photonics. It leads to many interesting Dubreuil4, Juejun Hu2, Laurent Vivien1; 1C2N, Universite with nonreciprocal properties, Pavel Kwiecien1, Ivan phenomena, including symmetry-protected flat bands de Paris-Sud XI, France; 2MIT, USA; 3Univ. of Central Flor- Richter1, Vladimir Kuzmiak2, Jiri Čtyroký2; 1Dept. of Phys- and single-mode lasers. ida, USA; 4Laboratoire Charles Fabry, Institut d’Optique ical Electronics, Czech Technical Univ. in Prague, Faculty Graduate School, France. We report the characterization of Nuclear Sciences and Physical Engineering, Czech JW3A.66 of highly nonlinear GeSbS chalcogenide glass integrated Republic; 2Inst. of Photonics and Electronics of the Czech Directional Forward Scattering by Linear Chain of waveguides. Linear and nonlinear measurements were Academy of Sciences, Czech Republic. We have studied Cylindrical Nanoparticles, Sonam Dogra1, Reena Dalal1, performed in the telecom window, illustrating the poten- theoretically surface magnetoplasmons in several types Ajeet Kumar1; 1Delhi Technological Univ., India. Highly tial of As-free chalcogenides for photonics applications. of THz guiding structures, based on a combination of directional forward scattering in the chain of cylindrical InSb, dielectric, and metal parts, both in planar and more Silicon nanoparticles has been reported. There is an JW3A.73 general configurations, under the external magnetic field. enhancement of directivity when the size of the chain Parity-Time Symmetric Adiabatic Elimination, Mojgan has been increased along the direction of propagation Dehghani1, Hamidreza Ramezani1; 1Physics and Astron- JW3A.80 of electric field. omy, Univ. of Texas Rio Grande Valley, USA. We investi- Planar Optics with High Numerical Apertures at gate the influence of parity-time symmetry on adiabatic Visible Wavelengths, Wei-Ting Chen1, Alexander Zhu1, JW3A.67 elimination in coupled waveguides. We show that while Mohammadreza Khorasaninejad1, Zhujun Shi1, Federico Fano resonant all-dielectric core-shell nanoparticles, adiabatic elimination is not affected in the symmetric Capasso1; 1Harvard Univ., USA. We report high numerical Reena Dalal1, Nishant Shankhwar1, Yogita Kalra1, Ajeet phase, in the broken phase it does not hold. aperture planar optics using metasurfaces. Meta-axicons Kumar1, Ravindra K. Sinha2; 1Applied Physics, Delhi and immersion meta-lenses with numerical apertures Technological Univ., India; 2Central Scientific Instruments JW3A.74 up to 1.1 are demonstrated; they can generate wave-

Organisation, India. We report directional Fano resonance Temperature Dependence of Nanoscale Si3N4 Tuning length-independent Bessel beams and diffraction-limited 1 in the core-shell (Silicon-MgOTiO2) nanoparticle in the Fork Cavity Optomechanical Transducers, Rui Zhang , focal spots. visible region. Interference of resonant magnetic dipole Yundong Ren1, Marcelo Davanço2, Vladimir Aksyuk2, and broad electric dipole result in asymmetric profile of Kartik Srinivasan2, Yuxiang Liu1; 1Worcester Polytechnic JW3A.81 Fano resonance. Inst., USA; 2Center for Nanoscale Science and Technol- Hyperstructured Illumination with Metamaterial ogy, National Inst. of Standards and Technology, USA. Disorder, Emroz Khan1, Evgenii E. Narimanov1; 1School JW3A.68 We investigate the temperature dependence of doubly of Electrical and Computer Engineering and Birck Nan-

Design of a High-Q Resonant Raman Amplifier, Ren-Jie clamped Si3N4 tuning fork cavity optomechanical trans- otechnology Center, Purdue Univ., USA. Hyperstructured Chen1, Yeong H. Ko1, Jae W. Yoon2, Robert Magnusson1; ducers. The temperature-induced mechanical resonance illumination, a super-resolution scheme based on struc- 1Univ. of Texas at Arlington , USA; 2Hanyang Univ., shift was experimentally measured and investigated by tured illumination in hyperbolic media, must account for South Korea. We analyze silicon-based resonant Raman both numerical and analytical modeling. material disorder. We show that even with no informa- amplifiers. We provide an initial design study based on tion on disorder, the method allows for accurate image nanopatterned c-Si films. By spectral and angular tuning, JW3A.75 reconstruction. two resonant lines exhibit the proper spectral Raman Differential Polarisation-sensitive Photodetectors ber separation for silicon. Design Utilising Plasmonic Metasurfaces, Evgeniy JW3A.82 Panchenko1, Jasper J. Cadusch1, Timothy D. James1, Organic Adhesion Layer for an Increased Wave- JW3A.69 Lukas Wesemann1, Ann Roberts1; 1The Univ. of Mel- guide-Excited Surface-Enhanced Raman Signal, Nina Optomechanical Pressure and Temperature Sensing, bourne, Australia. We propose and demonstrate a CMOS Turk1, Pieter Wuytens1, Ali Raza1, Andre Skirtach2, Roel Robinjeet Singh1, Stephen Eckel2, James Fedchak2, Thom- compatible plasmonic antenna-based differential photo- Baets1; 1Ghent Univ. - imec, Belgium; 2Ghent Univ., Bel- as Purdy2; 1JQI/NIST, USA; 2National Inst. of Standards detector. Our design permits using differential detection gium. By replacing the titanium adhesion layer with 3-mer- and Technology, USA. We analyze the dynamics of various techniques in telecommunication systems potentially captopropyltrimethoxysilane we show a 3-fold increase of eigenmodes of a high stress $Si_3N_4$ nanomechanical significantly increasing the data transmission rate. the collected signal in on-chip Surface Enhanced Raman membrane resonator. This work explores applications of Spectroscopy using nanoplasmonic antennas integrated optomechanical systems for pressure and temperature JW3A.76 on a nanophotonic waveguide. metrology. Bio-sensing with asymmetric THz metasurfaces, Joshua Burrow1, Thomas Searles2, Imad Agha1,3, Jay Mathews3,1; JW3A.83 Wednesday, 20 Septem Wednesday, JW3A.70 1Electro-Optics and Photonics, Univ. of Dayton, USA; Non-Linear Plasmonic Oscillations of Laser Pulse Irradi- Design and Fabrication of SU-8 Polymer Based Pho- 2Physics & Astronomy, Howard Univ., USA; 3Physics, Univ. ated Fullerene, Uday Chakravarty1, Deepa Chaturvedi2; tonic Crystal Waveguide, Swagata Samanta1, Pallab of Dayton, USA. We demonstrate an asymmetric 4-gap 1RRCAT, India; 2Physics, IIT Delhi, India. Intense laser Banerji2, Pranabendu Ganguly1; 1Advanced Technol- square ring resonator terahertz (THz) metasurface as an energy coupling in fullerene is analytically modeled ogy Development Centre, Indian Inst. of Technology ultra-sensitive biological sensor. Polarization-insensitive by considering fullerene as a laser driven non linear Kharagpur, India; 2Materials Science Centre, Indian Inst. modes due to asymmetry exhibit low minimal detectable plasmonic oscillator. Efficient collisionless absorption of Technology Kharagpur, India. We make use of optical concentration of bovine serum albumin. is estimated depending upon the laser parameters and lithography along with focused ion beam milling to fab- fullerene geometry. ricate our designed photonic crystal waveguide; milling JW3A.77 depth of 220nm is obtained with an ion dose of 10K, rms Plasmonic Filter Arrays for Infrared Spectral Recon- JW3A.84 roughness being 33.1nm. struction, Benjamin Craig1, Kenneth B. Crozier1; 1Univ. of Numerical Computation of Surface Plasmon Polariton Melbourne, Australia. We experimentally demonstrate an Propagation and Dispersion in the Presence of Non- array of plasmonic infrared transmission filters. We show, locality, Hao Yang1, Xiang Meng1, Shuhao Wu1, Jerry I. by simulations that include noise, reconstruction of the Dadap1, Richard M. Osgood1; 1Columbia Univ., USA. We spectra of infared light sources from measurements of develop a surface-hydrodynamic numerical model for the energy transmitted through each filter. studying the impact of nonlocality on propagating surface plasmon polaritons in metallic nanostructures, resulting in a larger (~2×) SPP wavelength compared to the local case at plasma resonance.

62 FiO + LS 2017 • 17–21 September 2017 Science & Industry Showcase

JOINT FiO + LS

JW3A • Joint Poster Session III—Continued

JW3A.85 JW3A.91 JW3A.97 Broadband unidirectional reflectionless aperiodic Full Gamut of Structural Colors in All-Dielectric Mes- Confining Low Energy Light with Tapered Conical multilayer structure, Chenglong You1, Corey T. Matyas2, oporous Network Metamaterials, Yoichiro Tsurimaki1, Plasmonic Nanowires, Kiana Montazeri1, Zhihuan Wang1, Yin Huang3,4, Jonathan Dowling1, Georgios Veronis2,5; Alejandra Ruiz de Clavijo2, Olga Caballero2, George Bahram Nabet1; 1Drexel Univ., USA. We show tapered 1Dept. of Physics and Astronomy, Louisiana State Univ. Ni1, Gang Chen1, Marisol Martin Gonzalez2, Svetlana V. conical nanowires modified to have embedded two-di- , USA; 2School of Electrical Engineering and Computer Boriskina1; 1MIT, USA; 2Instituto de Microelectrónica de mensional electron gas plasmons enhance low-energy, Science, Louisiana State Univ., USA; 3School of Physics Madrid, Spain. We engineer and demonstrate a full gamut long-wavelength light confinement at the tip of the and Electronics, Central South Univ., China; 4Key Lab of of structural colors in network metamaterials fabricated formed resonant optical cavity, making them useful for Optoelectronic Devices and Systems of Ministry of Edu- by the electrodeposition method. The macroscopic-size optoelectronic devices. cation and Guangdong Province, Shenzhen Univ., China; mesoporous structures are candidates for sensing, secu- 5Center for Computation and Technology, Louisiana rity, and color rendering applications. JW3A.98 State Univ., USA. We design non-parity-time-symmetric Achieving arbitrary control over pairs of polarization multilayer structures, one of which consists of alternating JW3A.92 states using complex birefringent meta-materials, silicon and silica layers, while the other one includes a Giant higher-order multipoles enable strong intrinsic Alexander Cerjan1, Shanhui Fan1; 1Stanford Univ., USA. gain material. Our structures can achieve broadband chirality in planar nanostructures, Alexander Y. Zhu1, We demonstrate a specific class of meta-material, termed unidirectional reflectionlessness. Wei-Ting Chen1, Aun Zaidi1, Yao-Wei Huang1, Moham- complex birefringent meta-materials, are able to produce madreza Khorasaninejad1, Vyshakh Sanjeev1, Cheng-Wei two orthogonally polarized states from two non-orthog- JW3A.86 Qiu2, Federico Capasso1; 1Harvard Univ., USA; 2National onal initial states, realizing arbitrary control over pairs of Studies of Optical and Magnetic responses of iron Univ. of Singapore, Singapore. We demonstrate near-unity polarization states. Nanoparticles obtained by femtosecond laser abla- circular dichroism and polarization rotation exceeding tion, David Muñeton1, Jesica M. Santillán1, Daniel C. 100,000°/mm in planar dielectric nanostructures at visible JW3A.99 Schinca1, Lucía B. Scaffardi1; 1Centro de Investigaciones wavelengths. Such strong intrinsic chiral behavior is due to On the Coupling Efficiency of Tamm Plasmon Polar- Opticas, Argentina. Optical and magnetic responses the excitation of giant higher-order multipoles. itons, Samir Kumar1, Mukesh K. Shukla1, Ritwick Das1; of Fe colloids produced by fs-pulsed laser ablation in 1School of Physical Sciences, National Inst. of Science water and ethanol are studied. An absorption band in JW3A.93 Education and Research, HBNI, India. A novel design UV-region is measured; heterogeneous composition and Control of Valley Polarization in 2D Transition Metal technique based on structural parameters is proposed superparamagnetic state of the nanoparticles are proved. Dichalcogenides by all Dielectric Metasurface, Sriram for the efficient coupling of light to Tamm plasmon-po- Guddala1, Rezlind Bushati1, Jie Gu1,2, Zheng Sun1,2, Mat- laritons (TPPs). Optimization of the structure is essential JW3A.87 thew Weiner1, Alexander Khanikaev1, Vinod M. Menon1,2; to completely utilize the field enhancement due to TPPs. Cylindrical, High-Q Surface Plasmon Cavities for Las- 1Physics, City college of New York, USA; 2Physics, The ing and Sensing in the Visible Range, Shawn Divitt1,2, Graduate Center of the City Univ. of New York, USA. We JW3A.100 Jared Strait2, Wenqi Zhu1,2, Cheng Zhang1,2, Henri Lezec2, demonstrate control of valley polarization through the Unidirectional Excitation of Radiative-Loss-Free Amit Agrawal1,2; 1Univ. of Maryland, USA; 2National Inst. coupling of 2D materials with chiral metasurface. The Surface Plasmon Polaritons in Parity-Time Symmetric of Standards and Technology, USA. We discuss recent modified density of states in the metasurface resulting Systems, Zhong Huang1,2; 1Northeastern Univ., USA; efforts in realizing an optical resonator consisting of a in preferential emission with specific helicity 2School of Physics and National Lab of Solid State metal-coated dielectric cylinder that supports whisper- Microstructures, Nanjing Univ., China. We investigate ing-gallery-type surface plasmon polaritons capable of ex- JW3A.94 unidirectionally surface plasmon polaritons at flat metal hibiting high quality factors in the visible frequency range. Effect of Silver Nano-Protrusions on Field Enhance- dielectric interface with parity time symmetric modulation. ment in Tip-enhanced Raman Spectroscopy, Justin We show that the SPPs life time and propagation distance JW3A.88 Isaac1, Bin Zhang2, Lina Ramanauskaite3, Valentinas can be significantly improved. Inverse scattering method to design or determine Snitka3, Huizhong Xu1; 1Dept. of Physics & Astronomy, properties of metamaterials, Nitish Chandra1; 1Univ of San Francisco State Univ., USA; 2Inst. of Modern Physics, JW3A.101 North Carolina Charlotte, USA. Inverse scattering meth- Fudan Univ., China; 3Research Center for Microsystems Optical effects in magnetoplasmonic crystals with ods can be used to design/determine the permittivity and and Nanotechnology, Kaunas Univ. of Technology, Lithua- burried gold grating, Alexander Chekhov1, Pavel permeability of meta-atoms, metamaterials or general nia. The field enhancement in a gap-mode tip-enhanced Naydenov3, Alexander Stognij2, Tatiana Murzina1; 1M. V. structures from the scattered field. These methods can Raman spectroscopy (TERS) setup with hemispherical Lomonosov Moscow State Univ., Russia; 2Scientific-Practi- Wednesday, 20 Septem be improved by using Green’s functions and potentials. nano-protrusions on the substrate is studied numerically cal Materials Research Centre of NAS of Belarus, Belarus; and is found to display a resonant behavior as a function 3Moscow Technological Univ. (MIREA), Russia. We present JW3A.89 of the protrusion radius. a study of magnetoplasmonic crystals with a gold grating Exceptional Points in Passive Plasmonic Nanostruc- in bismuth iron garnet surrounding. Experimental results tures, Ashok Kodigala1, Thomas Lepetit1, Boubacar JW3A.95 for the first time evidence the excitation of long-range Kante1; 1Univ. of California, San Diego, USA. We present Plasmonic Coupling in Metal Nanocavities, Basudeb surface plasmon polariton mode in a magnetic material. evidence of the existence of exceptional points (EPs) in Sain1, Roy Kaner1, Yaara Bondy 1, Yehiam Prior1; 1Dept. three-dimensional plasmonic nanostructures. The systems of Chemical Physics, Weizmann Inst. of Science, Israel. JW3A.102 are composed of coupled plasmonic nanoresonators and Optical Fabry-Perot like modes, situated diagonally Dispersion-tailored Metasurfaces and Meta-lenses, can be judiciously driven to EP by controlling symme- as a function the gap, are observed in transmission Wei-Ting Chen1, Vyshakh Sanjeev1,2, Alexander Zhu1, try-compatible modes. through pairs of coupled nanocavities in gold film, while Zhujun Shi1, Mohammadreza Khorasaninejad1, Federi- plasmonic wakes are observed from a linear array of co Capasso1; 1Harvard Univ., USA; 2Univ. of Waterloo, ber JW3A.90 individual cavities. Canada. We report dispersion-tailored metasurfaces in Complete absorption of broadband, unpolarized light the visible, including an achromatic meta-lens capable in a deep-subwavelength graphene metamaterial, C. JW3A.96 of keeping a constant focal length within a continuous Martijn de Sterke1, Han Lin2, Bjorn Sturmberg1, Xiaorui Implications of Active Material and Optical Mode on bandwidth. The dispersion of meta-lenses can also be Zheng2, Yunyi Yang2, Teck K. Chong3, Baohua Jia2; 1Univ. of Nanoscale Electro-Optic Modulation, Rubab Amin1, tailored with tunable Abbe numbers. Sydney , Australia; 2Swinburne Univ. of Technology, Aus- Can Suer1, Zhizhen Ma1, Ibrahim Sarpkaya1, Jacob B. tralia; 3Australian National Univ., Australia. We report total Khurgin2, Ritesh Agarwal3, Volker J. Sorger1; 1The George JW3A.103 absorption of unpolarized, wide bandwidth (800-1550 Washington Univ., USA; 2Johns Hopkins Univ., USA; 3Univ. Intra-cavity Spin Controlled Geometric Phase Metasur- nm) light in 90 nm thick graphene-based metamaterial. of Pennsylvania, USA. Motivated by index-tuning-to- face, Nir . Davidson1, Ronen Chriki1, Elhanan Maguid2, Grooves in the metamaterial couple incoming light into loss tradeoff dictated by fundamental Kramers-Kronig Chene Tradonsky1, Vladimir Kleiner2, Asher Friesem1, Erez the absorber’s guided modes. Fabrication is low-cost relations, we demonstrate a comprehensive analysis for Hasman2; 1Weizmann Inst. of Science, Israel; 2Technion, and scalable. high-performance compact on-chip electro-optic mod- Israel. Geometric phase metasurface elements were in- ulators for a set of active materials and optical modes. corporated into laser cavities, to generate unique output beams. These include, coherent and partially coherent vortex beams, multiple harmonic vortex beams, and vectorial vortices.

FiO + LS 2017 • 17–21 September 2017 63 Science & Industry Showcase

JOINT FiO + LS

JW3A • Joint Poster Session III—Continued

JW3A.104 JW3A.111 JW3A.118 Nanoimprinted Resonant Filters Made with Or- Plasmonically tailored nanotraps for neutral atoms A Fully Automated Dual-Probe Scanning Near-Field ganic-Inorganic Nanocomposites, Hafez Hemmati1, based on periodic ring nanocavities, Zhao Chen1, Qi Optical Microscopy Technique, Najmeh Abbasirad1; Robert Magnusson1; 1Univ. of Texas at Arlington, USA. Zhang1, Fan Zhang1, Ying Gu1, Qihuang Gong1; 1Peking 1Inst. of Applied Physics, Abbe Center of Photonics, Guided-mode resonance devices are fabricated by Univ., China. We have theoretically demonstrated the Friedrich Schiller Univ. Jena, Germany. An automated, nanoimprint lithography applied to a nanocomposite atom trapping based on periodic ring nanocavities by robust dual-probe scanning near-field optical micro- containing silicon nanoparticles in a polymer host. Optical circular blue-detuned light. A three-dimensional trapping scope is demonstrated by measuring surface plasmon transmission spectra of the experimental and simulated potential are achieved with ultra-low optical power, scat- polaritons. To measure the probe-probe crosstalk, the devices are in good agreement. tering rate and large trapping lifetime. collision prevention implements two probes oscillating at different frequencies. JW3A.105 JW3A.112 Ghost Resonance in Optical Scattering, Sanjay Deb- Carcinogenic Chromium (VI) sensing using fiber Bragg JW3A.119 nath1, Evgenii E. Narimanov1; 1Purdue Univ., USA. We grating based on swelling of stimulus responsive Surface-Plasmon-Polariton Laser with Narrow Line- demonstrate the presence of ghost resonance in optical hydrogel, Pabbisetti Vayu Nandana Kishore1; 1National width and Low Threshold, Wenqi Zhu1, Cheng Zhang1, scattering from dielectric particles. Inst of Technology, Warangal, India. This Paper proposes Ting Xu1, Amit Agrawal1, Henri Lezec1; 1NIST, USA. We a Chemo-mechanical-optical approach of sensing the demonstrate a surface-plasmon-polariton laser with nar- JW3A.106 Chromium (VI) metal ion. Transducing property of both row linewidth and low threshold based on a low-loss open Nonlinear saturations effects in non-Hermitian scat- FBG and hydrogels is utilized for sensing. Traces of Cr (VI) cavity resonator that leverages grating-coupled SPPs to tering systems, Oksana Shramkova1, Konstantinos even in the orders of 10ppb can be sensed by the method. pump the lasing SPPs with improved spatial overlap and Makris2, Giorgos Tsironis2, Demetrios Christodoulides3; minimum perturbation. 1Research & Innovation, Technicolor R&D France, France; JW3A.113 2Univ. of Crete, Greece; 3Univ. of Central Florida, USA. Novel applications of hyperlens, Jingbo Sun1, Tianboyu JW3A.120 The nonlinear scattering properties of non-Hermitian Xu1, Natalia M. Litchinitser1; 1State Univ. of New York at Disordered Nanoantennas: A New Paradigm in dispersive system with saturable gain/loss are examined. Buffalo, USA. By exploiting strongly anisotropic optical Space-Division Multiplexing, Mohammad Haghtalab1, It is shown that the non-reciprocal response of nonlinear properties of engineered nanostructures, we proposed Safieddin Safavi-Naeini1; 1Univ. of Waterloo, Canada. medium depends on gain/absorption coefficient and total and demonstrated several hyperlens-based devices that A novel approach for information multiplexing is intro- thickness of the bilayer. integrate super resolution properties into the practical duced. The degrees of freedom provided by disordered applications. structures can be employed for realizing information JW3A.107 processing devices. Disordered highly coupled nanoan- Excitation of Surface Plasmons in Subwavelength Grat- JW3A.114 tennas are investigated for this purpose. ings, Nikolai I. Petrov1, Viktor Danilov1, Vladimir Popov2, Plasmonic Resonance of Trapezoidal Nanograting Boris Usievich3; 1Scientific Research Center of Unique Shined with Normal Incident Light, Kang Tae-young1, JW3A.121 Instrumentation of the Russian Academy of Sciences, Dong-Myeong Shin1, Kyujung Kim1, Hyerin Song1; 1Pusan Fresnel Coefficients for Electromagnetic Propagation Russia; 2Moscow State Univ., Russia; 3General Physics Inst. National Univ., South Korea. The plasmon polaritons of across a Non-Chiral and Chiral Dispersive Interface with of the Russian Academy of Sciences, Russia. The results the structure can be quantitatively controlled by the Negative Index, Monish R. Chatterjee1, Rajab Y. Ataai1; of computer calculations and measurements of subwave- geometries. also showed a correlation between the 1Univ. of Dayton, USA. Fresnel coefficients are found for length diffraction gratings in the visible spectral range are enhancements in electric field intensity and the nanostruc- a non-chiral/chiral (first-order) dispersive interface with presented. It is shown that the plasmon resonance via a ture geometry under the normal incident light. permittivity, permeability and chirality parameters func- grating coupling occurs at the determined conditions. tions of sideband frequency en route to possible negative JW3A.115 index behavior in the second medium. JW3A.108 Large-scale Day-time Radiative Cooling Metafilm, Yao Integrated zero-index supercouplers, Daryl Vulis1, Zhai1, Yaoguang Ma1, Sabrina David3, Dongliang Zhao1, JW3A.122 Philip Camayd-Munoz1, Yang Li1, Orad Reshef1, Marko Runnan Lou1, Chuanwei Wu1, Gang Tan2, Ronggui Yang1, Room-temperature quantum emitter arrays in hex- Loncar1, Eric Mazur1; 1Harvard Univ., USA. Zero-index Xiaobo Yin1,3; 1Dept. of Mechanical Engineering, Univ. of agonal boron nitride, Nicholas Proscia1,2, Zav Shotan1, supercoupling offers a mechanism through which light is Colorado Boulder, USA; 2Dept. of Civil and Architectural Harishankar Jayakumar1, Prithvi Reddy3, Marcus Doherty3, confined to sub-diffraction scales and coupling between Engineering, Univ. of Wyoming, USA; 3Materials Science Audrius Alkauskas4, Carlos Meriles1,2, Vinod Menon1,2; disparate modes is achieved. We consider this phenom- and Engineering Program, Univ. of Colorado, USA. We 1CUNY City College of New York, USA; 2Physics, Graduate ber ena in an integrated metamaterial toward experimental demonstrate a large-scale day-time radiative cooling Center Cuny, USA; 3Physics and Engineering, Australian demonstration. metafilm that is fabricated by a roll-to-roll process. The National Univ., Australia; 4Center for Physical Sciences metafilm has demonstrated 93 W/m2 cooling power at and Technology, Lithuania. We demonstrate deterministic JW3A.109 noon-time, which is a performance promising for large- formation of quantum emitter arrays in hexagonal Boron Active beam steering based on reconfigurable phase- scale cooling applications. Nitride (hBN) at room temperature. The emitters are change metasurface, Ren Jie Lin1, Cheng Hung Chu2, Yu localized around the location of high strain provided by Han Chen1, Ting-Yu Chen1, Wei-Yi Tsai1, Din Ping Tsai2,1; JW3A.116 the nanopillar substrate. 1National Taiwan Univ., Taiwan; 2Research Center for Uniaxially Stretched Flexible Surface Plasmon Res- Applied Sciences, Academia Sinica, Taiwan. We present onance Film for Versatile Surface Enhanced Raman the tunable optical response of phase change material Scattering Diagnostics, Kaichen Xu1,2, Rong Ji2, Minghui 1 1 2 Ge2Sb2Te 5, which can be used to metasurfaces with varied Hong ; National Univ. of Singapore, Singapore; Data functionalities. The research is promising to apply to the Storage Inst., (A*STAR), Singapore. A flexible SERS film is Wednesday, 20 Septem Wednesday, area of the metadevice. demonstrated via irreversibly and longitudinally stretching metal deposited poly(ε-caprolactone) film. The stretched JW3A.110 surface plasmon resonance film exhibits ~10 times signal Versatile Polarization Generation by using Aluminum enhancement compared to unstretched composite film. Plasmonic Metasurface, Mu Ku Chen1, Pin Chieh Wu1,2, Wei-Yi Tsai1, Hsiang-Chu Wang2, Jia-Wern Chen1, Chun JW3A.117 Yen Liao1, Cheng Hung Chu1,2, Greg Sun3, Din Ping Effective Permittivity and Permeability of Metamaterial Tsai1,2; 1Dept. of Physics, National Taiwan Univ., Taiwan; from Rectilinear Thin Wires Array, L. N. Butko2, A. P. An- 2Research Center for Applied Sciences, Academia Sinica, zulevich2, D. A. Pavlov2, Sergey G. Moiseev1; 1Ulyanovsk Taiwan; 3Dept. of Engineering, Univ. of Massachusetts State Univ, Russia; 2Chelyabinsk State Univ, Russia. The Boston, USA. We demonstrate a reflective metasurface effective permittivity and permeability of the composite polarization generator (MPG) capable of producing light structure consisting of rectilinear thin wires array forming beams of any polarizations all from a linearly polarized a 2D square lattice within the non-conductive host media light source with a single optically thin chip. are theoretically investigated.

64 FiO + LS 2017 • 17–21 September 2017 12:00–13:00 Lunch Break (on your own)

12:00–13:00 Congressional Fellowship Program Information Session, Science Showcase Theater, Columbia, Terrace Level

12:00–13:00 OSA Optical Material Studies Technical Group Special Talk, Georgetown West, Concourse Level

12:00–13:00 Polarization Optics - Design and Fabrication Trends and Challenges, Georgetown East, Concourse Level

12:00–13:30 OIDA VIP Industry Leaders Speed Meetings Lunch, Kalorama, Lobby Level

13:00–13:30 Coffee Break, Science & Industry Showcase, Columbia, Terrace Level

13:00–15:00 JW4A • Science & Industry Showcase Exhibits, Poster Session & E-Posters Rapid-Fire Oral Presentations IV in Theater Columbia, Terrace Level

Science Showcase Theater JOINT FiO + LS

13:00–14:00 JW4A • Rapid-Fire Oral Presentations IV

JW4A.12 • 13:00 RAPID JW4A.23 • 13:20 RAPID JW4A.56 • 13:40 RAPID Interaction-free All-optical Modulation on Chip, Jiayang Electro-optic frequency beamsplitter for quantum Analysis of Stimulated Raman Scattering and Four- Chen1, Yong Meng Sua1, Zi-Tong Zhao1, Mo Li1, Yuping networking applications, Hsuan-Hao Lu1, Joseph M. Wave Mixing Effects on Crosstalk of Multicore Fibers, Huang1; 1Stevens Inst. of Technology, USA. We report Lukens2, Nicholas A. Peters2, Ogaga Odele1, Andrew Daniel Ceballos2, Ramon Gutierrez-Castrejon2, J. Javier the observation of quantum Zeno blockade on chip, M. Weiner1, Pavel Lougovski2; 1Purdue Univ., USA; 2Oak Sanchez-Mondragon1; 1INAOE, Mexico; 2Instituto de where a lightwave is modulated by another in a distinct Ridge National Lab, USA. We implement a frequency Ingenieria, Universidad Nacional Autonoma de Mexico ``interaction-free’’ manner. For quantum applications, we beamsplitter for spectrally encoded photons, based (UNAM), Mexico. We report a numerical analysis of also verify its operations on single photons. on electro-optic modulation and Fourier-transform inter-core crosstalk in multicore fibers (MCFs) based on pulse shaping. The ultrahigh fidelity, bandwidth, and a dual-core-fiber model that includes Stimulated Raman JW4A.14 • 13:05 RAPID dense mode packing offer new potential for quantum Scattering (SRS) and Four Wave Mixing (FWM) nonlinear- Generation of Qudits Using Four Photons and a interconnects. ities in the presence of random perturbations. Single Degree of Freedom, José Ferraz1,2, Pierre L. de Assis2,3, Marcos A. Carvalho2,4, Sebastião de Pádua2; JW4A.24 • 13:25 RAPID JW4A.66 • 13:45 RAPID 1Departamento de Física, Universidade Federal Rural New Coherence Theorem, Xiao-Feng Qian1, S Kizhak- Near-field absorption imaging by two color Raman de Pernambuco, Brazil; 2Departamento de Física, Uni- kumpurath Manikandan1, A Al Qasimi1, Nickolas Vami- nano-light source, Ryo Kato1, Yuika Saito2, Takayuki Wednesday, 20 Septem versidade Federal de Minas Gerais, Brazil; 3Instituto vakas1, Joseph Eberly1; 1Univ. of Rochester, USA. A new Umakoshi1, Prabhat Verma1; 1Osaka Univ., Japan; 2Ga- de Física, Universidade Estadual de Campinas, Brazil; identity for optical coherence is derived. It generalizes kusyuin Univ., Japan. We demonstrate new nano-imaging 4Departamento de Física, Instituto Federal do Norte de the notion of polarization so that it is applicable in more technique for intrinsic absorption properties of materials Minas Gerais, Brazil. We present the controlled generation than one way to any optical beam with multiple degrees using near-field scanning optical microscopy. Raman of two copies of two-qudit states using four photons of freedom. scattering from the apex of a silicon nano-tip was used as and a single degree of freedom, transverse momentum. probe light for nano-scale absorption analysis. It’s experimentally and theoretically shown that both JW4A.29 • 13:30 RAPID highly-entangled and separable states were generated. Generation of hybrid entangled two photon state using JW4A.76 • 13:50 RAPID classical non-separable state of the pump beam, Jabir Nonlinear Optical Properties of Hoplia coerulea, JW4A.15 • 13:10 RAPID M. V.1, Apurv Chaitanya Nellikka1, Goutam K Samanta1; Charlotte Verstraete1, Sébastien R. Mouchet2, Stijn Van Linear optical computing of matrix permanent via ther- 1Physical Research Lab, India. We report on transfer of Cleuvenbergen1, Peter Vukusic2, Branko Kolaric3, Thierry 1 1 1 1 2 mal light boson sampling, Yosep Kim , Kang-Hee Hong , classical non-separable state in down-conversion pro- Verbiest ; Chemistry, KU Leuven, Belgium; School of ber Joonsuk Huh2, Yoon-Ho Kim1; 1Dept. of Physics, Pohang cess to generate twin photons entangled in both OAM Physics, Univ. of Exeter, UK; 3Physics, Univ. of Mons, Univ. of Science and Technology (POSTECH), South and polarization degree of freedom. Measurement on Belgium. H. coerulea’s elytra show a strong two-photon Korea; 2Dept. of Chemistry, Sungkyunkwan Univ., South entanglement witness operator showed that the state fluorescence signal, which depends on the presence of Korea. We show linear optical calculation of permanent is entangled. water in the photonic structure. A polarization-dependent of Hermitian positive semidefinite matrices via thermal Third Harmonic Generation signal was detected as well light boson sampling. The experimental results are in JW4A.40 • 13:35 RAPID and thoroughly investigated. good agreement with the calculation and are compared Raman spectroscopy study of Hydrogen Plasma Treat- RAPID with the Gaussian sampling results. ment effect on a single layer Graphene/MoS2 hybrid JW4A.77 • 13:55 structure, Anishkumar Soman1, Jianping Shi2, Ugochukwu Fabrication and Characterization of an All-solid Dou- JW4A.16 • 13:15 RAPID Nsofor1,3, Steve Hegedus1,3, Yanfeng Zhang2, Robert ble-clad Tellurite Photonic Bandgap Fiber, Tonglei Temporal-mode selection with a Raman quantum mem- Burke4, Tingyi Gu1; 1Univ. of Delaware, USA; 2Peking Cheng1, Shunta Tanaka1, Tong Hoang Tuan1, Takenobu ory, Joseph H. Munns1,3, Sarah E. Thomas1,3, Krzysztof T. Univ., China; 3Inst. of Energy Conversion, USA; 4US Army Suzuki1, Yasutake Ohishi1; 1ofmlab, Japan. An all-solid Kaczmarek1, Patrick M. Ledingham1, Dylan J. Saunders1, Research Lab, USA. In this study we report the effect of double-clad tellurite photonic bandgap fiber is fabricated 2 1 1 1 Joshua Nunn , Benjamin Brecht , Ian A. Walmsley ; Univ. hydrogen plasma treatment on Graphene/ MoS2 hybrid based on three glasses. Photonic bandgap properties are of Oxford, UK; 2Univ. of Bath, UK; 3Imperial College heterostructures using Raman spectroscopy. The effect calculated by the plane wave expansion method, and London, UK. We demonstrate temporal-mode-selective of plasma voltage on the defects has been investigated the results agree well with the measured transmission storage and retrieval of weak coherent pulses in a Raman on graphene, MoS2 and the hybrid structure. spectrum. quantum memory in warm atomic Caesium vapour with a switching fidelity of 86.5%. This paves the way to scalable photonic quantum networks.

FiO + LS 2017 • 17–21 September 2017 65 Science & Industry Showcase

JOINT FiO + LS

13:00–15:00 JW4A • Joint Poster Session IV

JW4A.1 E-Poster JW4A.7 E-Poster JW4A.14 Chaos-Based Mitigation of Image Distortion under Scalar and Vector Vortex Modes through SLM-based Generation of Qudits Using Four Photons and a Single Degree of Freedom, 1,2 Anisoplanatic Electromagnetic Signal Propagation Kolmogorov Turbulence, Mitchell A. Cox1, Andrew José Ferraz , Pierre L. 2,3 2,4 2 through Turbulence, Monish R. Chatterjee1, Ali Mo- Forbes1; 1Univ. of the Witwatersrand, South Africa. Both de Assis , Marcos A. Carvalho , Sebastião de Pádua ; 1 hamed1; 1Univ. of Dayton, USA. Electromagnetic (EM) scalar and vector vortex modes are often used as trans- Departamento de Física, Universidade Federal Rural 2 propagation across a slanted anisoplanatic turbulent path mission bases for mode division multiplexing. We demon- de Pernambuco, Brazil; Departamento de Física, Uni- 3 is examined for EM carrier-embedded information and an strate theoretically and experimentally that the crosstalk versidade Federal de Minas Gerais, Brazil; Instituto image-bearing transparency through optical lensing, and within either mode set due to turbulence is the same. de Física, Universidade Estadual de Campinas, Brazil; 4 distortion mitigation using a chaotic carrier is examined. Departamento de Física, Instituto Federal do Norte de JW4A.8 E-Poster Minas Gerais, Brazil. We present the controlled generation JW4A.2 E-Poster Experimental Investigation of Cascaded Raman and In- of two copies of two-qudit states using four photons Deterministic spectral tuning of InAs quantum dots in termodal Nonlinear Interaction Based Supercontinuum and a single degree of freedom, transverse momentum. photonic crystal membrane diodes with laser anneal- Generation in Corning® LEAF® Fiber, Partha Mondal1, It’s experimentally and theoretically shown that both ing, Joel Q. Grim1, Allan S. Bracker1, Sam G. Carter1, Mijin Nitin Bhatia1, Vishwatosh Mishra1, Raktim Haldar1, Shailen- highly-entangled and separable states were generated. Kim2, Helen H. Parks3, Bumsu Lee4, Brennan Pursely4, dra K. Varshney1; 1Indian Inst. of Technology Kharagpur, Michael Yakes1, Dan Gammon1; 1U.S. Naval Research India. We demonstrate spectral broadening based on JW4A.15 Linear optical computing of matrix permanent via ther- Lab, USA; 2Sotera Defense Solutions, USA; 3ASEE cascaded Raman and intermodal nonlinear interaction mal light boson sampling, 1 1 research associate residing at the U.S. Naval Research in Corning®LEAF® fiber pumped by a picosecond laser Yosep Kim , Kang-Hee Hong , 2 1 1 Lab, USA; 4NRC research associate residing at the U.S. source. The effect of fiber length and pump power over Joonsuk Huh , Yoon-Ho Kim ; Dept. of Physics, Pohang Naval Research Lab, USA. The spectral inhomogeneity of spectral broadening are also investigated. Univ. of Science and Technology (POSTECH), South 2 semiconductor quantum dots (QDs) is a major challenge Korea; Dept. of Chemistry, Sungkyunkwan Univ., South preventing the development of scalable QD quantum JW4A.9 E-Poster Korea. We show linear optical calculation of permanent networks. Using laser annealing, three QDs are tuned into Bent Negative Curvature Fibers Using Circular or El- of Hermitian positive semidefinite matrices via thermal resonance, paving the way for on-chip quantum networks. liptical Cladding Tubes, Chengli Wei1, Curtis Menyuk2, light boson sampling. The experimental results are in Jonathan Hu1; 1Electrical and Computer Enginnering, good agreement with the calculation and are compared JW4A.3 E-Poster Baylor Univ., USA; 2Computer Science and Electrical with the Gaussian sampling results. A monolithic, doubly-resonant parametric down-con- Engineering, Univ. of Maryland Baltimore County, USA. version source for Caesium Raman memories, Benjamin We study nondegenerate modes in bent negative cur- JW4A.16 Temporal-mode selection with a Raman quantum mem- Brecht1, Oscar Lazo-Arjona1, Krzysztof T. Kaczmarek1, vature fibers. Fibers with circular tubes perform better ory, 1,3 1,3 Thomas Parker1, Raimund Ricken2, Viktor Quiring2, Chris- than fibers with elliptical tubes when the bend radius is Joseph H. Munns , Sarah E. Thomas , Krzysztof T. 1 1 1 tof Eigner2, Kai Hong Luo2, Harald Herrmann2, Christine less than 12 cm. Kaczmarek , Patrick M. Ledingham , Dylan J. Saunders , 2 1 1 1 Silberhorn2, Ian A. Walmsley1; 1Univ. of Oxford, UK; 2Univ. Joshua Nunn , Benjamin Brecht , Ian A. Walmsley ; Univ. 2 3 of Paderborn, Germany. We demonstrate a simple, JW4A.79 E-Poster of Oxford, UK; Univ. of Bath, UK; Imperial College bright, resonant parametric down-conversion source Terahertz detection mechanisms in black phosphorus, London, UK. We demonstrate temporal-mode-selective generating spectrally single-mode photons at 852.4nm Martin Mittendorff1, Ryan J. Suess1, Edward Leong1, storage and retrieval of weak coherent pulses in a Raman and 1601nm. Bandwidths of around 250MHz make the Andrei Sushkov1, H. Dennis Drew1, Thomas E. Murphy1; quantum memory in warm atomic Caesium vapour with a photons compatible with cavity Raman memories in warm 1Univ. of Maryland, USA. We present three THz detection switching fidelity of 86.5%. This paves the way to scalable Caesium vapour. mechanisms in black phosphorus: bolometric detection, photonic quantum networks. photothermoelectric detection, and photoconductive JW4A.4 E-Poster sampling of THz fields. Photothermal detection exhibits JW4A.17 Pursuing many-body dynamics of NV centers in dia- Near-field frequency-to-time mapping for arbitrary an internal responsivity of 44V/W and 20ps response time. mond, 1 1 2 shaping of biphoton correlations, Hsuan-Hao Lu1,2, Demitry Farufnik , Yahel Horowicz , Nir Alfasi , 2 2 1 Ogaga Odele1,2, Daniel E. Leaird1,2, Andrew M. Weiner1,2; JW4A.10 Sergai Masis , Yaron Kauffmann , Elad Farchi , Yoav 1 1 1 1 1School of Electrical and Computer Engineering, Purdue Withdrawn. Romach , Eyal Buks , Nir Bar-Gill ; Hebrew Univ. of Jeru- 2 Univ., USA; 2Purdue Quantum Center, USA. We demon- salem, Israel; Technion, Israel Inst. of Technology, Israel. ber strate a shaper-assisted near-field frequency-to-time JW4A.11 We study the interactions of optically addressable spin mapping technique using biphotons. By pre-modifying Investigation of two-pulse photon echo in acety- ensembles (NV centers) in diamond through optimized the two-photon spectral amplitude and phase, arbitrary lene-filled photonic-crystal fiber at 1530nm, Nayeli electron irradiation, confocal microscopy, and dynamical temporal correlations can be achieved with dispersion in Casillas-Rodríguez1, Manuel Ocegueda2, Eliseo Hernán- decoupling sequences, to reach the dipolar NV-NV inter- the near-field region. dez-Hernández1, Serguei Stepanov1; 1CICESE, Mexico; action-dominated regime. 2UABC, Mexico. Two-pulse photon echo in acety- JW4A.5 E-Poster lene-filled HC-PCF at 1530.37nm is reported. Initial JW4A.18 Experimental Test for the Finite-TimeWave Function Programmable unitary transformation of spectro-tem- transverse relaxation time T ≈11 ns, determined by the 2 Collapse, 1 2 poral modes, Valérian Thiel2, Alex O. Davis2, Peru molecule flight-time across fiber mode diameter, de- José Ferraz , Raoni S. Moreira , Alyson J. 2 2 2 D’Ornellas2, Nicolas Treps1, Brian J. Smith2; 1Laboratoire creased to 7ns at acetylene pressure 0.6Torr. Carvalho , Fernando R. Parisio , Lucio H. Acioli , Daniel 2 1 Kastler Brossel, France; 2Univ. of Oxford, Clarendon Lab, Felinto ; Departamento de Física, Universidade Federal 2 Univ. of Oxford, UK. We present simulations of ultrafast JW4A.12 Rural de Pernambuco, Brazil; Departamento de Física, Universidade Federal de Pernambuco, Brazil. An experi- Wednesday, 20 Septem Wednesday, temporal pulse shaping with a fiber-coupled EOM and Interaction-free All-optical Modulation on Chip, Jiayang fiber Bragg grating. The scheme can be used to realize Chen1, Yong Meng Sua1, Zi-Tong zhao1, Mo Li1, Yuping mental test for the wave function collapse is realized. The unitary transformations of pulse modes allowing lossless Huang1; 1Stevens Inst. of Technology, USA. We report experimental results reaffirms the epistemic interpretation manipulation of a multimode quantum state. the observation of quantum Zeno blockade on chip, for the state vector and opposes the ontic view. where a lightwave is modulated by another in a distinct JW4A.6 E-Poster ``interaction-free’’ manner. For quantum applications, we JW4A.19 Extreme Phase-Amplification under Direct Detection Near-infrared photon-pair generation by intermodal also verify its operations on single photons. of Atomic States for Heisenberg Limited Sensitivity four-wave mixing in a few-mode fiber, Erik N. Chris- in an Atomic Interferometer Employing Schroedinger tensen1, Søren M. Friis1, Jacob G. Koefoed1, Mario Usuga JW4A.13 Cat States, 1 1 Castaneda1, Karsten Rottwitt1; 1DTU Fotonik, Denmark. Intensity correlations of twisted photons generated Renpeng Fang , Resham Sarkar , Selim M. 1 1 We demonstrate a photon-pair source based on inter- by spontaneous parametric down-conversion, NIJIL Shahriar ; Northwestern Univ., USA. We show that for modal four-wave mixing in a few-mode fiber generating LAL C. K.1,2, Ali Anwar1, Chithrabhanu Perumangatt1, R an N-particle atom interferometer, an N-fold reduction 1 1 2 in fringe-width due to phase amplification can be photons at 965 nm and 1187 nm in the LP01 and LP02 P Singh ; Physical Research Lab, India; Physics, Indian modes, respectively, with a coincidence-to-accidental Inst. of Technology, India. We generate heralded single achieved via direct detection of atomic states, employing ratio of 12. photons carrying orbital angular momentum (OAM) by Schroedinger Cat states, yielding Heisenberg limited spontaneous parametric down-conversion (SPDC). We sensitivity study the influence of orbital angular momentum of the photon on the second-order optical coherence.

66 FiO + LS 2017 • 17–21 September 2017 Science & Industry Showcase

JOINT FiO + LS

JW4A • Joint Poster Session IV—Continued

JW4A.20 JW4A.27 JW4A.34 Competition between Incoherent Pumping and Losses Selective Detection of Picosecond Overlapping Quan- Information Capacities of LTI Quantum Bosonic Chan- in a System of Two Interacting Qubits, Julian C. Triana1, tum Modes, Amin Shahverdi1, Yong Meng Sua1, Yu-Ping nels, Jacob M. Leamer1, Chenglong You2, Bhaskar Roy Karen M. Fonseca Romero1; 1Universidad Nacional de Huang1; 1Stevens Inst. of Technology, USA. We demon- Bardhan3; 1Physics, Grove City College, USA; 2Physics, Colombia, Colombia. We consider a model of two qubits. strate selective frequency conversion of single photons in Hearne Inst. for Theoretical Physics and Louisiana State We calculate and compare two quantifiers of non-classical overlapping quantum modes of picosecond waveforms, Univ., USA; 3Physics, State Univ. of New York Geneseo, correlations: the quantum discord and the entanglement achieving a detection signal-to-noise well exceeding the USA. We investigate various information capacities of of formation, in the steady state. theoretical limit of the optimal time-frequency filtering. linear time invariant quantum bosonic channels representing amplification and attenuation in optical fiber JW4A.21 JW4A.28 communications. We compare these capacities with those Detecting nonlocal correlated errors: Bob gets caught Cavity QED based Sequential Atom Entangler for of optical coherent detection. faking a Bell-inequality violation, Meghan Feldman1, Heisenberg-Limited Atom Interferometry, Sylvester Gabe Juul1, Steven J. van Enk2, Mark Beck1; 1Whitman Amoah1; 1Western Illinois Univ., USA. We propose a cavity JW4A.35 College, USA; 2Univ. of Oregon, USA. We demonstrate QED based sequential N-atom GHZ state generator. As Periodic suppression and enhancement of spontaneous that loop state-preparation-and-measurement tomogra- GHZ states can be easily converted to path-entangled two-photon emission via interference, Dong-Gil Im1, phy is capable of detecting nonlocal correlated errors by N00N states, this would open new pathways for Heisen- Yosep Kim1, Yoon-Ho Kim1; 1Dept. of Physics, POSTECH, catching Bob as he tries to fake a Bell-inequality violation berg-limited atom interferometry. South Korea. An effective periodic boundary condition while using nonlocal knowledge of Alice’s measurement can be introduced to spontaneous parametric down-con- settings. JW4A.29 version by using a continuous-wave multi-mode pump. Generation of hybrid entangled two photon state using We show this effect can result in periodic suppression JW4A.22 classical non-separable state of the pump beam, Jabir and enhancement of spontaneous two-photon emission. Generation of Multi-mode NOON States with Three M. V.1, Apurv Chaitanya Nellikka1, Goutam K Samanta1; Photons Using Linear Optics, Lu Zhang1, Kam Wai 1Physical Research Lab, India. We report on transfer of JW4A.36 Clifford Chan1; 1Univ. of Oklahoma, USA. We propose a classical non-separable state in down-conversion pro- High Speed Information Reconciliation for Long Dis- setup to generate multi-mode NOON states with N=3 cess to generate twin photons entangled in both OAM tance Continuous-variable Quantum Key Distribution using single photons, coherent states, and single-photon and polarization degree of freedom. Measurement on System, Xiangyu Wang1, Yichen Zhang1, Song Yu1, Hong detectors, which has great importance in simultaneous entanglement witness operator showed that the state Guo2; 1Beijing Univ of Posts & Telecom, China; 2Peking multi-phase estimation with higher efficiency than indi- is entangled. Univ., China. We report the experiment realization of high vidual estimation. speed information reconciliation for continuous-variable JW4A.30 quantum key distribution system with multi-edge LDPC JW4A.23 Robust, bright entangled photon source based on codes based on graphic processing unit where the aver- Electro-optic frequency beamsplitter for quantum type-0, non-collinear phase matching in periodically age speed is up to 30.39 Mb/s. networking applications, Hsuan-Hao Lu1, Joseph M. poled crystal, Jabir M. V.1, Goutam K Samanta1; 1Physical Lukens2, Nicholas A. Peters2, Ogaga Odele1, Andrew Research Lab, India. We demonstrate a novel source JW4A.37 M. Weiner1, Pavel Lougovski2; 1Purdue Univ., USA; 2Oak of high-brightness polarization entangled photons at Joint Characterization of Two Single Photon Detectors Ridge National Lab, USA. We implement a frequency room temperature. Using non-collinear phase-matching with a Fiber-based Source of Entangled Photon Pairs, beamsplitter for spectrally encoded photons, based of PPKTP crystal we generate entangled state with Daniel E. Jones1, Brian T. Kirby1, Michael Brodsky1; 1U.S. on electro-optic modulation and Fourier-transform 18.76kHz/mW/nm number of photon pairs, with fidelity Army Research Lab, USA. By simultaneously measuring pulse shaping. The ultrahigh fidelity, bandwidth, and ~0.975. individual and coincidence counts of two single photon dense mode packing offer new potential for quantum detectors connected to an entangled photon pair source, interconnects. JW4A.31 we extract the detector efficiencies, the average number Optimizing Coincidence Measurementsof Entangled of generated pairs, and the Raman noise floor. JW4A.24 Photons, Matthew Reichert1, Hugo Defienne1, Jason W. New Coherence Theorem, Xiao-Feng Qian1, S Kizhak- Fleischer1; 1Princeton Univ., USA. We present the general JW4A.38 Wednesday, 20 Septem kumpurath Manikandan1, A Al Qasimi1, Nickolas Vami- SNR of coincidence measurements of joint probability of Recovery of distributed quantum information in vakas1, Joseph Eberly1; 1Univ. of Rochester, USA. A new entangled-photon-pairs. Experiments with an EMCCD quantum networks, Ankur Raina1, Priya Nadkarni1, identity for optical coherence is derived. It generalizes camera show excellent agreement for count rates up to Shayan G. Srinivasa1; 1Electronic Systems Engineering, the notion of polarization so that it is applicable in more saturation, and an optimum based on electronic noise. Indian Inst. of Science, India. We use quantum networks than one way to any optical beam with multiple degrees to store quantum information in a distributed setting. of freedom. JW4A.32 We propose recovery methods to restore the stored Withdrawn. quantum information in the event of failure of any of the JW4A.25 nodes of the network. A low-power, electrically-controllable alkali source for JW4A.33 cold-atom microsystems, Songbai Kang1, Russell Mott2, Composable Security Analysis for Continuous-Variable JW4A.39 Kevin Gilmore1,3, Logan Sorenson2, Mattew Rakher2, Eliz- Measurement-Device-Independent Quantum Key Entanglement enabled synthetic aperture in decoher- abeth A. Donley1, John . Kitching1, Christopher Roper2; Distribution, Song Yu1, Zhengyu Li2, Yichen Zhang1, ing environments, Siddhartha Santra1, Brian T. Kirby1, ber 1NIST, USA; 2HRL , USA; 3physics Dept., Univ. of Colora- Hong Guo2; 1Beijing Univ of Posts & Telecom, China; Vladimir S. Malinovsky1, Michael Brodsky1; 1Army Re- do Boulder, USA. We develop a low-power, solid-state 2Peking Univ., China. We report the composable security search Lab, USA. We propose a protocol for synthesizing electrochemical alkali source. Vapor-phase sinking and analysis for continuous-variable measurement-device-in- large apertures in interferometry using imperfectly entan- sourcing of Rb atoms have been demonstrated with just dependent quantum key distribution protocol, in which gled quantum states shared between remote telescopes. 5 V opposite-polarity voltages. The device is of consid- detection is conducted by an untrusted third party and The protocol is feasible in any environment and provides erable interest for cold-atom microsystems. naturally defend all detector side channels. high-resolution images of distant sources.

JW4A.26 JW4A.40 Generation of frequency-bin entangled narrowband Raman spectroscopy study of Hydrogen Plasma Treat- 1 biphotons and their Bell test, Xianxin Guo , Yefeng ment effect on a single layer Graphene/MoS2 hybrid Mei1, shengwang Du1; 1Physics, the Hong Kong Univ. structure, Anishkumar Soman1, Jianping Shi2, Ugochukwu of Science and Technology, Hong Kong. We report the Nsofor1,3, Steve Hegedus1,3, Yanfeng Zhang2, Robert generation of frequency-bin entangled narrowband Burke4, Tingyi Gu1; 1Univ. of Delaware, USA; 2Peking biphotons from spontaneous four-wave mixing (SFWM). Univ., China; 3Inst. of Energy Conversion, USA; 4US Army Making use of time-resolved detection, we observe Research Lab, USA. In this study we report the effect of

violation of the CHSH Bell inequality and confirm the hydrogen plasma treatment on Graphene/ MoS2 hybrid genuine entanglement. heterostructures using Raman spectroscopy. The effect of plasma voltage on the defects has been investigated

on graphene, MoS2 and the hybrid structure.

FiO + LS 2017 • 17–21 September 2017 67 Science & Industry Showcase

JOINT FiO + LS

JW4A • Joint Poster Session IV—Continued JW4A.41 JW4A.48 JW4A.55 All-Silicon Directional Coupler Electro-Optic Modulator Design of a Novel Polarization-Independent Power Hybrid Photonic-Plasmonic Directional Coupler En- Utilizing Transparent Conducting Oxides, Mohamed Splitter Using Coupled Silicon Rib Waveguides, Swaga- abled Optical Transceiver, Shuai Sun1, Ruoyu Zhang1, Badr1, Mohamed Abdelatty1,2, Mohamed A. Swillam1; ta Samanta1, Pallab Banerji2, Pranabendu Ganguly1; 1Ad- Jiaxin Peng1, Vikram Narayana1, Tarek EI-Ghazawi1, Volker 1Physics, American Univ. in Cairo, Egypt; 2Basic Sciences, vanced Technology Development Centre, Indian Inst. of J. Sorger1; 1George Washington Univ., USA. We proposed The British Univ. in Egypt, Egypt. An all-silicon elec- Technology Kharagpur, India; 2Materials Science Centre, a novel device structure termed Mo-detector for on-chip tro-optic modulator based on a transparent conducting Indian Inst. of Technology Kharagpur, India. Design of signal modulation and detection. With 180um2 footprint, oxide-integrated directional coupler is proposed. An a three-coupled silicon rib waveguide based polariza- 37.4 fJ/bit energy efficiency and 167 GHz operating extinction ratio (ER) of 8.45 dB and an insertion loss (IL) tion-independent power splitter is presented taking into speed, Mo-detector has a great potential in inter-chip of 0.75 dB are achieved at 1.55 μm wavelength. account excess loss in coupled region and total bending communication. loss for double arc S-bends at the output. JW4A.42 JW4A.56 Germanium metal-semiconductor-metal photode- JW4A.49 Analysis of Stimulated Raman Scattering and Four- tectors grown on Silicon using low temperature A Full Three-Dimensional Isotropic Carpet Cloak Wave Mixing Effects on Crosstalk of Multicore Fibers, RF-PECVD, Ghada Dushaq1, Ammar Nayfeh1, Mahmoud Designed by Transformation Optics, Daniely G. Silva1, Daniel Ceballos2, Ramon Gutierrez-Castrejon2, J. Javier Rasras1; 1Masdar Inst., United Arab Emirates. This paper Poliane A. Teixeira1, Lucas Gabrielli2, Mateus Junqueira1, Sanchez-Mondragon1; 1INAOE, Mexico; 2Instituto de presents a direct growth of germanium on silicon using Danilo Spadoti1; 1Federal Univ. of Itajubá, Brazil; 2Univ. of Ingenieria, Universidad Nacional Autonoma de Mexico, standard RF-PECVD process at substrate temperature of Campinas, Brazil. This work presents a 3D isotropic carpet Mexico. We report a numerical analysis of inter-core cross- 500C. Ge Metal-Semiconductor-Metal photodetectors cloak designed via transformation optics. A quasi-confor- talk in multicore fibers (MCFs) based on a dual-core-fiber (MSM) are fabricated and characterized based on this mal mapping was obtained using numerical optimization. model that includes Stimulated Raman Scattering (SRS) low temperature growth. Simulations demonstrate the invisibility effect for arbitrary and Four Wave Mixing (FWM) nonlinearities in the pres- directions of incident waves. ence of random perturbations. JW4A.43 Hybrid Plasmonic Electro-Optical Directional Coupler JW4A.50 JW4A.57 Based Modulator Based on Electrically Tuning the Research on cavity solitons in Kerr combs with pump Reconfigurable All-Photonic Inter-Rack Interconnect for ITO’s Properties, Mohamed Abdelatty1,2, Mohamed M. feedback for flat broadband multi-wavelength source, Data-Centers, Priyankar Roychowdhury1, Ahmed Louri1; Badr1, Mohamed A. Swillam1; 1American Univ. in Cairo, Shaowu Chen1, Xun Lei1; 1Inst. of Semiconductors, CAS, 1The George Washington Univ., USA. In this paper, we Egypt; 2Basic Sciences Dept., Faculty of Engineering, China. We propose a Kerr comb generation scheme with have proposed a reconfigurable optical interconnect The British Univ. in Egypt, Egypt. An optical directional pump feedback loop. Simulations show that the scheme that can provide Tera bits per second throughput with coupler (ODC) based on two silicon-on-insulator wave- can enhance the nonlinear energy conversion efficiency micro second network latency to handle increasing ma- guides separated by a hybrid plasmonic waveguide is of comb and reduce the pump power level by about 32%. chine-to-machine traffic in data-centers. studied. An extinction ratio of 5.275 dB is achieved at the telecommunications wavelength (1.55 μm). JW4A.51 JW4A.58 Hyperdoped Silicon Characterization and Photode- Design of Elliptical Ring Core Fiber with support JW4A.44 tectors, Yining Liu1; 1Univ. of Dayton, USA. Hyperdoped of four LP modes in SDM applications, Vigneswaran U-Bend Silicon Waveguide Interconnect for 3-D Multi- silicon is a promising material for infrared detection via in- Dhasarathan1, Manirajan Senthil2; 1Electronics and Com- layer Photonics Integrated Circuit, Vishnu Priye1, Vikash termediate band absorption. In this work, enhancement of munication, Sri Krishna College of Inst. of Technology, Kumar1; 1Indian Inst. of Technology (ISM), Dhanbad, IR absorption of hyperdoped silicon is demonstrated and India; 2Annna Univ., India. We propose a novel fiber India. Critical physical and geometrical parameters of methods for fabrication of Ohmic contacts are explored. used for space division multiplexing (SDM) system which the proposed U-bend silicon waveguide interconnect has elliptical ring core with dual cladding on the silica are ascertained for its application in multi-layered hybrid JW4A.52 background. 3-D Photonics Integrated circuits. A possible fabrication Simulation of an Improved Beam Combiner Module methodology is also discussed. (BCM) for Spatial Domain Multiplexing (SDM), Syed JW4A.59 H. Murshid1, Ce Su1; 1Florida Inst. of Technology, USA. Experimental verification of two spatially multiplexed JW4A.45 Spatial Domain Multiplexing (SDM) is a MIMO archi- 10Gbps channels in single core multimode fibers for A Core-Shell Nanowire Platform for Silicon Photonics, tecture that can significantly increase the bandwidth of data center applications, Syed H. Murshid1, Bilas Chow- Zhihuan Wang1, Pouya Dianat5, Kiana Montazeri1, Baris optical fiber. A stable multiplexer is crucial for SDM. This dhury1, Engine Eyceyurt1, Saud Alanzi1; 1Florida Inst. of Taskin1, Marc Currie2, Paola Prete3, Nico Lovergine4, paper presents a simulation for an improved multiplexer Technology, USA. This presents experimental validation of ber Bahram Nabet1; 1Drexel Univ., USA; 2Optical Sciences for SDM. spatially multiplexed optical communication architecture Division, Naval Research Lab, USA; 3IMM-CNR, Inst. by supporting two 9.95–11 Gbps, C-band channels of for Microelectronics and Microsystems, Italy; 4Dept. of JW4A.53 exactly the same wavelength in a single core multimode Innovation Engineering, Univ. of Salento, Italy; 5Center Waveguide Superstructure Bragg Grating based fiber to double the LAN channel capacity. for Quantum Devices, Northwestern Univ., USA. Core- Multiparametric Sensor for Pressure and Accelera- shell nanowires are versatile optoelectronic devices that tion Measurement, Chandrika T. Nataraj1, Shafeek A. JW4A.60 can serve as light emitters, detectors and modulators. Samad1, Srinivas Talabatula1, Gopalakrishna Hegde1, Designing the Coupling Ratios in a Binary Driven Here we offer a high-performance low-cost platform for Gurusiddappa R. Prashanth2; 1Indian Inst. of Science, 64-QAM Transmitter, Naji Albakay1; 1Univ. of Nebras- heterogeneous photonic integrated circuits on silicon India; 2National Inst. of Technology, Goa, India. We report ka-Lincoln, USA. This paper describes the design for the based on such nanowire. here superstructure Bragg grating based multiparametric coupling ratios of the optical couplers in a binary driven sensor using micro-machined diaphragm and cantilever 64-QAM transmitter. The design considers the optical JW4A.46 beam. Coupled mode theory has been used to design insertion loss in order to generate a proper 64-QAM Wednesday, 20 Septem Wednesday, On-chip Integrated All-Optical Fast Fourier Transform: and analyze the shift in wavelength due to applied pres- symbol constellation. Design and Analysis, Hani Nejadriahi1, Volker J. Sorger1; sure and acceleration. 1George Washington Univ., USA. We report the design of JW4A.61 an all-optical fast Fourier transform (FFT) on a silicon-pho- JW4A.54 Amplitude Equalization Analysis of Optical Frequen- tonics on-chip platform, show the phase-, amplitude-, FDTD with an off-diagonal permittivity tensor compo- cy Combs Generated by Dual Drive Mach-Zehnder and delay sensitivity of the transfer function, and a delay nent to study the magneto-optical effect in a slow light Modulator for High Capacity Optical Transmissions, performance of 20 Tbps. waveguide, Naotaka Kamioka1, Tomohiro Tetsumoto1, Leonid A. Huancachoque1, Aldario C. Bordonalli1; 1Dept. Takasumi Tanabe1; 1Keio Univ., Japan. We develop and of Communications, Univ. of Campinas, Brazil. An am- JW4A.47 calculate the impact of the slow light effect on a mag- plitude equalization analysis of optical frequency comb Experimental Study of Integrated Cascade Silicon neto-optical isolator in a photonic crystal waveguide. generation by a dual-drive Mach-Zehnder modulator is Bragg Gratings for Optical Delay Lines, Lingjun Jiang1, We obtained an eight times larger isolation ratio in the presented. The resulting algorithm allowed lower than Zuoxi Li1, Stephen Anderson1, Weimin Zhou2, Zhaoran R. slow light regime. 0.01 comb intensity standard deviation via modulating Huang1; 1Electrical, Computer and Systems Engineering, signal amplitude control. Rensselaer Polytechnic Inst., USA; 2Sensors &Electron Devices Directorate, US Army Research Lab, USA. We demonstrated cascade integrated silicon Bragg gratings for optical delay line applications. A maximum group index of 8.3 has been achieved. Long delay time is also enabled by cascading the gratings in dense integration.

68 FiO + LS 2017 • 17–21 September 2017 Science & Industry Showcase

JOINT FiO + LS

JW4A • Joint Poster Session IV—Continued JW4A.62 JW4A.69 JW4A.76 Propagation Model for Spatially Multiplexed MIMO SPR Based Fiber Optic Quercetin Biosensor Utilizing Nonlinear Optical Properties of Hoplia coerulea, Optical Channels Combining Electromagnetic Wave rGO: PPy: Chitosan Nanocomposite Network, Ravi Charlotte Verstraete1, Sébastien R. Mouchet2, Stijn Van and Modified Laguerre-Gaussian Beams, Syed H. Kant1, Banshi D. Gupta1; 1Indian Inst. of Technology, Cleuvenbergen1, Peter Vukusic2, Branko Kolaric3, Thierry Murshid1, Bilas Chowdhury1, Greg Lovell1, Ibrahim Barka1; Delhi, India. Synthesis of nanocomposite network of rGO: Verbiest1; 1Chemistry, KU Leuven, Belgium; 2School of 1Florida Inst. of Technology, USA. : A model characterizing PPy: Chitosan and its application for quercetin detection Physics, Univ. of Exeter, UK; 3Physics, Univ. of Mons, spatially multiplexed (SDM) based optical channels, utiliz- utilizing fiber optic SPR is presented. The sensor is load- Belgium. H. coerulea’s elytra show a strong two-photon ing the modified LG beam equations is presented. This ed with myriad advantages with an operating range of fluorescence signal, which depends on the presence of model allows for determination of independent modes 0.001-10 µM. water in the photonic structure. A polarization-dependent of the SDM system architecture. Third Harmonic Generation signal was detected as well JW4A.70 and thoroughly investigated. JW4A.63 Temperature Sensor Based on two twin biconical-taper Investigation of under/over sampling impact on the fiber fabricated with Standard Fiber, Julian Moises JW4A.77 modulation format identification for high speed optical Estudillo Ayala1, Emmanuel A. Hernández-Robles1, Juan Fabrication and Characterization of an All-solid Dou- networks, Latifa Guesmi1; 1Sup’Com, Tunisia. Sampling M. Sierra Hernandez1, Roberto Rojas-Laguna1, Daniel ble-clad Tellurite Photonic Bandgap Fiber, Tonglei rate impact to the formats recognition is investigated in Jauregui-Vazquez1, Yanelis Lopez-Dieguez1, Javier A. Cheng1, Shunta Tanaka1, Tong Hoang Tuan1, Takenobu this paper. We report a novel method using pattern-rec- Martin Vela1, Juan C. Hernandez-Garcia1; 1Universidad Suzuki1, Yasutake Ohishi1; 1ofmlab, Japan. An all-solid ognition algorithm trained by amplitude histograms. De Guanajuato, Mexico. A temperature sensor based on double-clad tellurite photonic bandgap fiber is fabricated Results show high recognition probabilities at increased a Mach-Zehnder interferometer is proposed. In the SMF- based on three glasses. Photonic bandgap properties are sampling frequencies. 28 fiber the Mach- Zehnder interferometer is fabricated calculated by the plane wave expansion method, and with two concatenated tapers, with a waist diameter of the results agree well with the measured transmission JW4A.64 25 ~ 40 µm. spectrum. Characterizing Large-Scale Production Reliability for 100G Optical Interconnect in Facebook Data Centers, JW4A.71 JW4A.78 Abhijit Chakravarty1, Srinivasan Giridharan1, Matt Kelly1, CW Triggering in CW Pumped Supercontinuum Gener- Independent-Tunable Dual-wavelength Thulium-Doped Ashwin Poojary1, Vincent Zeng1; 1Facebook Inc., USA. ation, Cai Wen1, Peng Lu1, H.Y. Fu2, Qian Li1; 1Peking Univ. Fiber Laser Based on an In-Fiber Interferometers Array, Facebook is deploying cost effective 100G CWDM4 Shenzhen Graduate School, China; 2Tsinghua-Berkeley Marco V. Hernández-Arriaga1, Baldemar Ibarra-Escamilla1, transceivers in data centers. This paper describes the Shenzhen Inst., China. We investigate the influence of Manuel Durán-Sánchez2, Hector Santiago-Hernandez1, post production performance monitoring system which the CW trigger’s intensity on CW pumped SC generation Evgeny Kuzin1; 1INAOE, Mexico; 2CONACyT, Mexico. is being implemented to identify optical interconnect and a moderate intensity of the CW trigger is further A tunable dual-wavelength ring cavity Tm-doped fiber early failure modes. suggested. laser is presented. This configuration based on tapered

fibers enables independent-tunable laser peaks (λ1, λ2) JW4A.65 JW4A.72 from 1844.6 to 1835.1 nm and from 1930.3 to 1934.3 100Gb/s CWDM4 Optical Interconnect at Facebook Tunable dual-wavelength thulium-doped fiber laser in nm, respectively. Data Centers for Bandwidth Enhancement, Abhijit the range from 2067 to 2073.5 nm, Manuel Duran-San- Chakravarty1, Katharine Schmidtke1, Vincent Zeng1, chez1, Ricardo Ivan Alvarez Tamayo2, B. Posada-Ramirez1, JW4A.80 Srinivasan Giridharan1, Cathie Deal1, Reza Niazmand1; Baldemar Ibarra-Escamilla1, Evgeny Kuzin1, Miguel Vicen- Geometrical Volume-Nonlinear Optical Property Rela- 1Facebook Inc, USA. Facebook has developed 100G te Andres3; 1INAOE, Mexico; 2Universidad Autónoma de tionship of Carbon Nanotubes, Vijayakumar Sadasivan data centers from the ground-up by fine tuning optical Nuevo Leon, Mexico; 3Universidad de Valencia, Spain. A Nair1, Chandra S. Yelleswarapu1; 1Univ. of Massachusetts technologies, optimizing link-budget, limiting operating tunable dual-wavelength lineal cavity Tm-doped fiber Boston, USA. We studied the influence of geometrical temperatures and ultimately improving manufacturabil- laser is presented. The generation of the laser lines is volume on nonlinear absorption and scattering properties ity. 100G-CWDM4 is an effective technology to enable based on the use of cascaded fiber Bragg gratings and of carbon nanotube (CNT) suspensions. Results show connectivity over duplex single-mode fiber. a Hi-Bi fiber optic loop mirror. an inverse relationship attributing to the generation of nonlinear laser induced scattering sites. JW4A.66 JW4A.73 Near-field absorption imaging by two color Raman Results for the Measured Field of View for an Omni- JW4A.81 Wednesday, 20 Septem nano-light source, Ryo Kato1, Yuika Saito2, Takayuki directional Free Space Optical Receiver Architecture, Yb-Doped Fluorosilicate Optical Fiber Development Umakoshi1, Prabhat Verma1; 1Osaka Univ., Japan; 2Ga- Syed H. Murshid1, Bilas Chowdhury1, Michael Finch1, Greg For Laser Cooling and Radiation Balancing Applica- kusyuin Univ., Japan. We demonstrate new nano-imaging Lovell1, Charles Curt1; 1Florida Inst. of Technology, USA. tions, Peter D. Dragic1, Maxime Cavillon2, Andrey Miron- technique for intrinsic absorption properties of materials Free space optical communication provides fiber optic ov1, courtney kucera2, Thomas Hawkins2, J. G. Eden1, using near-field scanning optical microscopy. Raman bandwidths in a wireless environment. A fiber bundle John Ballato2; 1Univ of Illinois at Urbana-Champaign, scattering from the apex of a silicon nano-tip was used as employed as an omni-directional O-FSO receiver will be USA; 2Clemson Univ., USA. With F content greater than probe light for nano-scale absorption analysis. experimentally studied and normalized received optical about 5at%, Yb-doped fluorosilicate fibers exhibit the power patterns will be presented. short average emission wavelengths and long lifetimes JW4A.67 characteristic of the fluoride glasses used in cooling Fiber Cantilever Based Acoustic Sensor, Sumit Dass1, JW4A.74 applications. Evidence of cooling behavior is presented. Suman halder1, Jitendra Sharma1, Rajan Jha1; 1Indian Intermodal Suppression of Spectral Broadening in Inst of Technology, Bhubaneswar, India. A low-cost high Normal Dispersion Few-Mode Fibers, Shaival Buch1, JW4A.82 ber sensitivity SMF micro tip in cantilever configuration based Govind P. Agrawal1; 1Univ. of Rochester, USA. We observe Analysis of Long Period Fiber Gratings Sensor Systems acoustic sensor is demonstrated. For cantilever length of and investigate suppression of spectral broadening in for Aircraft Wing Drag Optimization, Alex A. Kazemi1; 11.2 mm, sensor shows a linear response in frequency the fundamental mode of a few-mode fiber owing to 1MC 0L73, The Boeing Compnay, USA. In this paper we range of 100 - 600 Hz. intermodal nonlinear effects caused by the presence of focus on the testing and aviation requirements for LPFG energy in the higher-order mode. sensors. We discuss drag analsysie optimization and JW4A.68 the bases of aviation standards for fiber optic sensor Refractive index liquid sensing based on bound states JW4A.75 measurements, and the quantities that are measured. in photonic crystal slabs, Yonghao Liu1, Deyin Zhao1, Formation of Optical Trajectories in the Photopolymer Weidong Zhou1, Yuze Sun1; 1Univ. of Texas at Arlington, Material during Self-Written Waveguides Process, USA. We theoretically investigate the bound states in Ra’ed Malallah1,2, Derek Cassidy 1, Inbarasan Muniraj free-space coupled defect-free photonic crystal slabs at 1, Liang Zhao 1, John Sheridan1; 1Univ. College Dublin, discrete vector k points for refractive index sensing to Ireland; 2Physics, Univ. of Basrah, Iraq. During the SWWs achieve low detection limit. process, the optical waveguide trajectories formed in an AA/PVA a photopolymer material photosensitive at 532 nm are examined. The largest index changes taking place at any time during the exposure are present.

FiO + LS 2017 • 17–21 September 2017 69 Science & Industry Showcase

JOINT FiO + LS

JW4A • Joint Poster Session IV—Continued JW4A.83 JW4A.89 JW4A.96 Transport Quantities in Random 1D System, Yiming Stability of a Fiber Optical Parametric Oscillator With Spatial coherence of localized modes in an Anderson Huang1,2, Xujun Ma1,2, Xiaojun Cheng1,2, Cassandra and Without a Seed Signal, Ioannis Begleris1, Peter localizing optical fiber, Behnam Abaie1, Thomas Haw- Imperato1, YUHAO KANG1,2, Azriel Genack1, Victor Horak1; 1Univerity of Southampton, UK. We present a nu- kins2, John Ballato2, Arash Mafi1; 1Univ. of New Mexico, Gopar1,3, Miztli Yepez4, Pier Mello5; 1Physics, Queens merical model of a unidirectional fiber optical parametric USA; 2Clemson Univ., USA. Exciting a localized beam in College, CUNY, USA; 2Physics, The Graduate Center, oscillator. Power fluctuations between signal round-trips an Anderson localizing fiber results in a high degree of USA; 3Universidad de Zaragoza, Spain; 4Departamento are investigated and found to be significant. Finally, the output spatial coherence. The fringe patterns resemble de Física, Universidad Autónoma Metropolitana-Iztapa- option of seeding the signal wave is discussed. those from singlemode fibers, indicating that a single lapa, Mexico; 5Instituto of Física, Universidad Nacional localized mode is predominantly excited. Autónoma de México, Mexico. We find the statistics of the JW4A.90 logarithm of energy density inside random 1D system with Laser Linewidth and the Thermal Grating Generation of JW4A.97 and without a reflector using random matrix theory and TMI in kW-class Fiber Amplifiers, Marc D. Mermelstein1; Langevin Approach Analysis of the Frequency Noise in microwave experiments. The results extend and correct 1MDM Optics, LLC, USA. Abstract: The laser linewidth Quantum Cascade Lasers, Xing-Guang Wang1, Cheng the single-parameter scaling hypothesis. dependence to TMI generated by a thermal grating (TG) Wang1; 1ShanghaiTech Univ., China. This work investigates is examined. Laser linewidths comparable to the thermal the frequency noise of quantum cascade lasers using the JW4A.84 relaxation time are required for TMI generation. This result Langevin approach. It is found that the frequency noise Low-loss photonic Nulling Interferometer in the conflicts with experimental demonstrations. spectrum exhibits a broad peak, and the intrinsic linewidth Mid-Infrared for Astronomical Applications, Thomas deviates from the Schawlow-Townes limit. Gretzinger1,2, Simon Gross1,2, Alexander Arriola1,2, Peter JW4A.91 Tuthill3, Michael Withford1,2; 1Centre for Ultrahigh band- Two-Photon Circular-Linear Dichroism on a Binaph- JW4A.98 width Devices for Optical Systems (CUDOS), Australia; talene-based Polymer, Jessica -. Dipold1, Guy Koeckel- Laser Line Selection from a Broadband Erbium Doped 2Physics and Astronomy, MQ Photonics Research Centre, berghs3, Marcelo G. Vivas2, Leonardo De Boni1, Cleber Fiber Ring Laser Using a Versatile Intra-Cavity Filter, Macquarie Univ., Australia; 3Sydney Inst. for Astronomy, R. Mendonça1; 1Instituto de Física de São Carlos, Brazil; Suchita Yadav2, Vijaya R2,1; 1Centre for Lasers and Pho- School of Physics, The Univ. of Sydney, Australia. We 2Instituto de Ciência e Tecnologia, Universidade Federal tonics, Indian Inst. of Technology Kanpur, India; 2Dept. report the fabrication of a photonic Nulling Interferom- de Alfenas, Brazil; 3Lab of Macromolecular and Physical of Physics, Indian Inst. of Technology Kanpur, India. The eter in Gallium Lanthanum Sulphide operating at 4 µm. Organic Chemistry, Katholieke Universiteit Leuven, possibility of selecting multiple spectrally narrow laser The device has low propagion loss waveguides of 0.22 Belgium. Two-photon absorption cross-section and cir- lines of width up to 0.08nm is demonstrated using a Mach- ± 0.02 dB/cm, which is sufficient enough to perform cular-linear dichroism spectra of a polymer was studied Zehnder interferometer-based filter inside the cavity of a on-sky experiments. for different polarization.The studies show that there are broadband erbium doped fiber ring laser. 2 possible final states for the two-photon transition, with JW4A.85 largest cross-section of 584 GM. JW4A.99 Fiber Bragg Strain Sensor Calibration System Based Non-permanent graded-index waveguide-inscription on Mechanical Nanomotion Transducer, Vladimir A. JW4A.92 in bulk chalcogenides., Nicholas Nye1, Soroush Shaba- Lazarev1, Mikhail K. Tarabrin1,2, Valerii E. Karasik1; 1Science Investigation of an optimal coupling condition with hang1, Christos Markos1,2, Demetrios Christodoulides1, and Education Center for Photonics and IR-Technology, a nanobeam cavity made of low refractive index Ayman Abouraddy1; 1Univ. of Central Florida, CREOL, Bauman Moscow State Technical Univ., Russia; 2Frequency material, Tomohiro Tetsumoto1, Hajime Kumazaki1, USA; 2DTU Fotonik, Denmark. Conventional wave- Standards Lab, P. N. Lebedev Physical Inst. of the Russian Kentaro Furusawa2, Norihiko Sekine2, Takasumi Tanabe1; guide-writing techniques in bulk chalcogenides rely Academy of Sciences, Russia. FBG strain sensor fabrica- 1Keio Univ., Japan; 2National Inst. of Information and on permanent photo-structural changes,which lead tion processes can lead to nonlinear behavior that affects Communications Technology, Japan. We investigated to ridge-like guiding channels. Here, we demonstrate the accuracy of measurements. We present a calibration an optimized coupling condition in a side-coupled cav- non-permanent opto-thermally induced graded-index

technique for FBG sensors. The performance of FBG sen- ity system consisting of a silica nanobeam cavity and a waveguides in As2Se3 glass. sor was investigated, and calibration curve is presented. nanofiber. We achieved a high coupling efficiency of 89% with a loaded Q of over 104. JW4A.100 JW4A.86 Writing 2nd Order Reflective Volume Bragg Grating in Nonlinear Optical Characterization of Gorilla® Glass JW4A.93 PQ:PMMA, Te-yuan Chung1, Yu-Hua Hsieh1, Wan-Ting Waveguides, Franciele Henrique1, Gustavo F. Almeida1, Bi-tapered fiber sensor using a supercontinuum light Hsu1, Bao-Jen Shih1, Shiuan-Huei Lin2; 1National Central Jonathas P. Siqueira1, Renato J. Martins1, Cleber R. Men- source, Diego Garcia Mina1, Andy Chong1, Ankita Univ., Taiwan; 2National Chiao Tung unversity, Taiwan. A donça1; 1São Carlos Inst. of Physics, Univ. of São Paulo, Khanolkar1, Karolyn Hansen1, Joseph W. Haus1; 1Univ. of thorough study on the rate equations of recording PQ:P- ber Brazil. We performed Dispersive-scan measurements in Dayton, USA. We developed a bi-tapered optical fiber MMA volume Bragg grating is performed. Base on the waveguides produced in Gorilla® Glass to determine and studied its transmission properties using a sub-micron rate equations, 2nd order grating recording in PQ:PMMA the nonlinear refractive index of the compression layer. wavelength, fiber-based, supercontinuum light source. is confirmed by the experiment. Our results indicate that its value is close to the one for We successfully tested the sensitivity of our fiber sensor fused silica. with aqueous solutions. JW4A.101 Effects of Fog in Free-Space Optics Communication JW4A.87 JW4A.94 System, Indira Marília A. Almeida2,1, Eduardo J. Aiub1, Generation of flat supercontinuum spectrum pumped Waveguide Grating Couplers in Overlaid Chips: Lucia A. Saito1, Jose J. Ribeiro2; 1Mackenzie Presbyterian by amplified noise-like pulses from a figure-eight fiber Efficiency Optimization and Angular Misalignment Univ., Brazil; 2Instituto Nacional de Telecomunicações laser, Erika N. Hernandez1, Miguel Ángel Bello Jiménez1, Simulation, Congshan Wan1, Muhannad S. Bakir1, Thomas (INATEL), Brazil. We demonstrated experimental results Olivier Pottiez2, Baldemar Ibarra-Escamilla3, Rosa E. K. Gaylord1; 1Georgia Inst. of Technology, USA. Applying of fog effects in Free Space Optics system in visible and López-Estopier1,4, Manuel Duran-Sanchez3,4, Evgeny reflectors adds 30%~40% to the diffraction efficiencies near-infrared for different relative humidity. Ultrashort Wednesday, 20 Septem Wednesday, Kuzin3; 1Instituto de Investigación en Comunicación Óp- of binary waveguide gratings. The greatest angular pulses and eye diagram analysis indicate acceptable tica,Universidad Autónoma de San Luis Potosí, Mexico; misalignment sensitivity occurs for rotations about the transmission requirements at 90% RH. 2CIO, Mexico; 3INAOE, Mexico; 4Consejo Nacional de grating groove axis and rotation should be limited to ±3°. Ciencia y Tecnología (CONACYT), Mexico. A figure-eight JW4A.102 fiber laser and their application for supercontinuum gen- JW4A.95 Multimode Interference based All-Fiber Selective eration in the anomalous dispersion regime is presented. Effect of Linear Coupling on Nonlinear Phase Noise Mode Launcher for Few Mode Fiber Applications, Flat uniformity of around 3-dB in the range from 1261 to in Two-Core Fibers, Nestor Lozano-Crisostomo1, Julio Nitin Bhatia1, Shailendra K. Varshney1; 1Indian Inst. of 2261 nm is achieved. C. Garcia-Melgarejo1, Jose E. Rocha Medina1, Alfonso Technology Kharagpur, India. We demonstrate an all-fiber J. Salas-Sanchez4, Daniel A. May-Arrioja2, J. Javier San- multimode interference device for achieving controlled JW4A.88 chez-Mondragon3; 1Facultad de Ingenieria Mecanica y and repeatable mode launching condition in a few mode Objective-lens-free Fiber based Position Detection Electrica, Universidad Autonoma de Coahuila, Mexico; fiber. The device is easy to design, quick to customize, with Nanometer Resolution in a Fiber Optical Trapping 2Centro de Investigaciones en Óptica, Mexico; 3Depar- and require bare minimum equipments for fabrication. System, Chaoyang Ti1, Yao Shen1, Minh-Tri Ho Thanh1, tamento de Optica, Instituto Nacional de Astrofisica, Qi Wen1, Yuxiang Liu1; 1Worcester Polytechnic Inst., Optica y Electronica, Mexico; 4Universidad Autonoma de USA. We develop an objective-lens-free fiber optical Sinaloa, Mexico. Considering the elementary two-core trapping system for applying force and sensing particle fiber (TCF) switching process, we describe how the linear motion with nanometer resolution. We used this system coupling in a TCF affects the nonlinear phase noise of to measure cellular response to external mechanical initial amplified pulses. stimuli in real time.

70 FiO + LS 2017 • 17–21 September 2017 Science & Industry Showcase

JOINT FiO + LS

JW4A • Joint Poster Session IV—Continued JW4A.103 JW4A.111 JW4A.117 Modulation Instability in the Weak Dispersion Regime Optical rouge wave generation in dielectrics with GaSb-core Optical Fibers, Seunghan Song1, Noel of Dispersion Oscillating Fiber-ring Cavity, Francois correlated fluctuations of refractive index, Mostafa Healy3, Ulf Österberg1, Michael Fokine2, Trygve Sørgård1, Copie2, Matteo Conforti2, Alexandre Kudlinski2, Stefano Peysokhan1, Esmaeil Mobini1, John Keeney1, Arash Anna Peacock4, Ursula J. Gibson1,2; 1Norges Teknisk Trillo1, Arnaud Mussot2; 1Dept. of Engineering, Univ. of Mafi1; 1Univ. of New Mexico, USA. We study rouge wave Naturvitenskapelige Univ, Norway; 2Dept. of Applied Ferrara, Italy; 2Physique des Lasers Atomes et Molécules generation for the propagation of light in a dielectric with Physics, KTH Royal Inst. of Technology, Sweden; 3Newcas- (PhLAM), Univ. of Lille, France. We investigate modulation correlated fluctuations of its refractive index and observe tle Univ., UK; 4Univ. of Southampton, UK. This paper re- instability in a dispersion modulated passive fiber-ring that with increasing the correlation length, the probability ports recent results on the formation of GaSb-core fibers, cavity with very a low local dispersion. In this configu- of rouge wave generation increases. formed by molten-core drawing. Purity, crystallographic ration, an unprecedented number of spectral sidelobes results and preliminary photoluminescence data are are observed, related to Faraday parametric resonances. JW4A.112 provided for both the as-drawn and laser annealed fibers. Application of Bessel-Gaussian Beams to Model JW4A.104 Spatial Domain Multiplexing, Syed H. Murshid1, Greg JW4A.118 Fabrication of Fiber Based Inline Micro Air Cavities Lovell1; 1Florida Inst. of Technology, USA. Presented is a Effect of two-photon absorption on cavity soliton: with Tunable Geometrical Parameters, Jitendra N. basic mathematical model for single core spatial domain stability and perturbation analysis, Ambaresh Sahoo1, Dash1, Rajan Jha1; 1IIT bhubaneswar, India. We report a multiplexing (SDM) utilizing Bessel-Gaussian Beams. This Samudra Roy1; 1Indian Inst. of Technology Kharagpur, novel procedure to fabricate fiber based inline micro air model will theoretically allow accurate modeling of SDM India. We study the stability criteria and propagation cavities with tunable geometrical parameters over a wide to allow more optimal use in optical fiber communication dynamics of cavity soliton under two-photon absorption range by tuning the length of hollow core photonic crystal systems. by solving Lugiato-Lefever equation numerically. A fiber and splicing parameters. semi-analytical variational technique is further adopted JW4A.113 to explain the complete dynamics. JW4A.105 Edge states between photonic topological insulator Application of optical analog of two-photon Rabi domains emulating Quantum Spin Hall and Quantum JW4A.119 oscillations in polarization splitter, Pragati Aashna1, K Valley Hall effects, Yuhao Kang1,2, Xiaojun Cheng1,2, Nonreciprocal modal conversion via strongly coupled Thyagarajan1; 1Indian Inst. of Technology, Delhi, India. Xiang Ni3,2, Alexander Khanikaev3,2, Azriel Genack1,2; nonlinear dynamics in multimode fibers, Hamed We report the design of a polarization splitter based 1Queens College, CUNY, USA; 2The Graduate Center of Pourbeyram1, Arash Mafi1; 1Univ. of New Mexico, USA. on two-photon Rabi oscillations in a three waveguide the City Univ. of New York, USA; 3The City College of the Strong coupling between a phase-matched parametric directional coupler. We show the practical feasibility of City Univ. of New York, USA. We observe edge states be- process and a nonlinear mode coupling results in a the device by carrying out simulations in lithium niobate tween domains of photonic systems emulating quantum non-reciprocal mode conversion in a multimode fiber. waveguides. valley-Hall and spin-Hall states by measuring transmission The novel experimental features can be used for greater spectra. The robustness of photonic transport along the modal control in fibers. JW4A.106 edge is tested by measuring group velocity. Optical Temperature Sensing in NaYSiO4:Er3+/Yb3+ JW4A.120 Upconvesion Phosphors, Xiaojie Xue1, Tonglei Cheng1, JW4A.114 Nanostructural-Core Photonic Crystal Fiber with Very Takenobu Suzuki1, Yasutake Ohishi1; 1Toyota Techno- Conservation of Topological Charge During Diffraction Low Negative Dispersion for Nonlinear Applications, logical Inst., Japan. Er3+/Yb3+ co-doped NaYSiO4 Through a Triangular Aperture, José Carlos A. Rocha1, Pooja Chauhan1, Ajeet Kumar1, Than Singh Saini2, Yogita upconversion phosphors were successfully synthesized João Paulo Amaral1, Alcenísio José Jesus Silva1, Eduardo Kalra1; 1Delhi Technological Univ., India; 2Advanced for optical temperature sensing. The sensitivity of this Jorge Silva Fonseca1; 1Universidade Federal de Alagoas, Materials and Sensors Division, CSIR-Central Scientific sensor was about 0.0047 K−1 at 573 K. Brazil. We break the symmetry of non-generic singularities Instruments Organization, Sector-30C, Chandigarh, India. in Laguerre-Gauss fields by diffraction through a triangular We have designed a nanostructural–core photonic crystal JW4A.107 aperture and studied their propagation. Conservation of fiber in pure silica glass. The reported structure has a very An Efficient Spatial Domain Optical De-Multiplexer topological charges is also observed. low and flat dispersion of -0.07 ps/nm.Km and very high Design, Syed H. Murshid1, Engine Eyceyurt1; 1Florida Inst. nonlinear coefficient of 64.57 W-1Km-1 at zero dispersion of Technology, USA. An efficient optical based spatial do- JW4A.115 wavelength. main de-multiplexer design is presented and simulation Multi-pulse dynamics in a full polarization-controlled results of the demodulation in CODE V are given. The passively mode-locked Er-Fiber laser, HECTOR SANTI- JW4A.121 Wednesday, 20 Septem system is designed to minimize the light power loss in AGO-HERNANDEZ1, Yazmin E. Bracamontes-Rodríguez4, On possibility of substance absorption lines identifi- de-multiplexer part. Baldemar Ibarra-Escamilla1, Manuel Durán-Sánchez2,1, G. cation at the THz pulse frequency up-conversion, V. A. Beltrán-Pérez3, Olivier Pottiez4, Ivan Armas-Rivera3, Luis A. Trofimov1, Dmitry Y. Zagursky1, Irina Zakharova1; 1M. V. JW4A.108 Rodríguez-Morales1, Marco Hernández-Arriaga1, Evgeny Lomonosov Moscow State Univ., Russia. Using computer Control of Optical Rogue Waves in CW Pumped Su- Kuzin1; 1Óptica, Instituto Nacional de Astrofísica, Óptica simulation we demonstrate a transform of substance percontinuum With a Weak Femtosecond Pulse Seed, y Electrónica, Mexico; 2Consejo Nacional de Ciencia y absorption properties due to SHG of few-cycle THz pulse peng lu1, Qian Li1; 1Peking Univ., China. We numerically Tecnología, Mexico; 3Benemérita Universidad Autónoma that transmits through the substance. demonstrate the improvement of spectrum bandwidth de Puebla, Mexico; 4Centro de Investigaciones en Optica, and pulse-to-pulse stability of continuous wave pumped Mexico. We report the experimental study of multi-pulse JW4A.122 supercontinuum generation by applying a weak coherent dynamics in a passively mode locked-fiber laser with total Effects of Fluctuations of Pulse Duration and Peak femtosecond pulse seed. control of polarization finding the condition to generate Power on the Coherence Properties of Supercontinuum reproducible noise-like pulse, soliton molecules, bound Spectra, Lai Liu1, Kenshiro Nagasaka1, Takenobu Suzuki1, JW4A.109 solitons and single soliton. Yasutake Ohishi1; 1Toyota Technological Inst., Japan. The ber Energy Density Distributions in the Interior of Random effects of fluctuations of pulse duration and peak power and Periodic Samples, Xiaojun Cheng1,2, Yuhao Kang1,2, JW4A.116 on the coherence properties of supercontinuum spectra Yiming Huang1,2, Azriel Genack1,2; 1CUNY Queens Col- Unique propagation characteristics of Airy pulsen in fibers with all-normal dispersion have been numeri- lege, USA; 2Graduate Center, City Univ. of New York, USA. under cubic phase modulation in linear regime, Aritra cally investigated by solving the generalized nonlinear We find the average of the logarithm of the energy density Banerjee1, Samudra Roy1; 1IIT Kharagpur, India. We theo- Schrödinger equation. decays linearly inside samples with different degrees of retically demonstrate that temporal flipping and distortion structural correlation. The fall-off rate initially decreases of a propagating truncated airy pulse under third order JW4A.123 and then increases slightly with increasing disorder. dispersion can be prevented by cubic phase modulation Optical Bistability in dual core directional coupler with (CMP). The shape preservation of pulse under CPM is negative index material channel, Kanagaraj Nithyanan- JW4A.110 confirmed numerically. dan1; 1Dept. de Physique, Universite de Bourgogne, Simulation of multi-wavelength SDM systems with France. We observe that the oppositely directed coupler OAM using ZEMAX and MATLAB, Syed H. Murshid1, possesses Bistability. This property arises due to effective Bilas Chowdhury1, Han Wang1; 1Florida Inst. of Technol- feedback mechanism as a result of opposite directionality ogy, USA. Experimental analysis of spatial multiplexed of the phase velocity and energy flow in the negative systems has shown independence of both wavelength index materials. division and orbital angular momentum multiplexing. In order to validate this a simulated analysis is performed on the system and presented.

FiO + LS 2017 • 17–21 September 2017 71 International Ballroom West International Ballroom East Georgetown West

FiO

15:00–16:30 15:00–16:30 15:00–16:30 FW5A • Silicon Photonics II FW5B • Shaping, Phase and Microscopy FW5C • Optical Systems for VA/AR Presider: Oleg Sinkin; Subcom, USA Presider: Laura Waller; University of Presider: Groot Gregory; Synopsys, Inc, USA California Berkeley, USA

FW5A.1 • 15:00 Invited FW5B.1 • 15:00 Invited FW5C.1 • 15:00 Invited Amorphous silicon photonics for nonlinear and quantum Structural microscopy via engineered scattered light, Advances in Computational Display for Virtual & Aug- interactions, Amy C. Foster1; 1Johns Hopkins Univ., USA. Hilton B. de Aguiar1, Sylvain Gigan3, Sophie Brasselet2; mented Reality, Kaan Aksit1; 1NVIDIA Corporation, USA. Hydrogenated amorphous silicon (a-Si:H) is a promising 1Département de Physique, Ecole Normale Supérieure/Paris, Computational displays” for virtual and augmented reality CMOS-compatible material for nonlinear integrated pho- France; 2Institut Fresnel, France; 3Laboratoire Kastler-Brossel, co-design the optics, display, and rendering algorithm for the tonics due to its high nonlinearity and compatibility with France. Scattered light has always been seen as a nuisance human visual system, achieving new tradeoffs in size, focus 3D integration. Recent progress in a-Si:H for nonlinear and in high resolution structural microscopy. We will review our cues, and resolution. I describe challenges, opportunities, quantum applications will be discussed. recent efforts on using wavefront shaping to control complex and several prototypes. light in order to enable molecular-level structural microscopy.

FW5A.2 • 15:30 FW5B.2 • 15:30 FW5C.2 • 15:30 Invited 1 Photonic Crystal with Buried Heterostructure Platform for Customizing Speckle Statistics, Nicholas Bender , Hasan Toward occlusion-capable optical see-through head- 1 1 2 1 1 2 Laser Devices Directly Bonded to Si, Aurimas Sakanas , Yi Yilmaz , Yaron Bromberg , Hui Cao ; Yale Univ., USA; The mounted displays, Hong Hua1; 1The Univ. of Arizona, USA. 1 1 1 1 Yu , Elizaveta Semenova , Luisa Ottaviano , Hitesh K. Sahoo , Racah Inst. of Physics, The Hebrew Univ. of Jerusalem, Isra- Most of the state-of-the-art optical see-though head-mount- 1 1 1 Jesper Mørk , Kresten Yvind ; Technical Univ. of Denmark, el. We develop a general method for customizing speckle ed displays (OST-HMD) lack the ability to occlude bright Denmark. In pursuit of fabricating compact and efficient light statistics. Using a phase-only spatial light modulator we real-world view with the virtual objects. In this paper, we sources for optical interconnects on Si, our directly bonded experimentally generate speckle patterns with arbitrari- will present the development of an occlusion-capable OST- InP buried heterostructure photonic crystal membrane lasers ly-tailored intensity probability-distributions, over a finite HMD prototype. benefit from the separation between active and passive intensity range. material regions.

FW5A.3 • 15:45 FW5B.3 • 15:45 Lens-Free Chip-to-Chip Free-Space Laser Communica- Achieving the gauge potential in a synthetic space using tion Link with a Silicon Photonics Optical Phased Array, coherent Raman sideband generation, Luqi Yuan1, Da-wei Christopher V. Poulton1, Diedrik Vermeulen1, Ehsan Hossei- Wang2, Shanhui Fan1; 1Dept. of Electrical Engineering and ni1, Erman Timurdogan1, Zhan Su1, Ben Moss1, Michael R. Ginzton Lab, Stanford Univ., USA; 2Dept. of Physics & Astron- Watts1; 1Analog Photonics, USA. We demonstrate a record omy and Inst. for Quantum Science and Engineering, Texas free-space 50m laser communication link between a silicon A&M Univ., USA. We study nontrivial topological effect in photonics optical phased array and an avalanche photode- the Raman sideband generation process, where probe field ber tector at 100Mbps. This lens-free technology opens the door shows features of one-way transport and Landau levels. Our to compact low-cost long-distance optical links. proposal provides a unique connection between topological photonics and nonlinear optics.

FW5A.4 • 16:00 FW5B.4 • 16:00 FW5C.3 • 16:00 Invited Characterization of a Coherent-Perfect-Absorption-based Surface Plasmons Carry a Pancharatnam-Berry Phase, Taco Waveguide-type See-through 3D Head-mounted Dis- 1 1 2 2 2 DPSK Demodulator for Si Photonics, Asif Ahmed , Hao D. Visser , Ari Friberg , Salman Daniel , Toni Saastamoinen , plays Without Accommodation Vergence Mismatch, 1 2 3 5 2 2 1 Yang , Brian Souhan , Zhao Wang , Christopher Evans , Joel Kimmo Saastamoinen , Ismo Vartiainen ; Vrije Universiteit, Jae-Hyeung Park1; 1Inha Univ., South Korea. We introduce 5 1 3 2 M. Hensley , Jerry I. Dadap , Andrew P. Knights , Richard Amsterdam, Netherlands; Univ. of Eastern Finland, Finland. holographic and Maxwellian head mounted displays to avoid 4 1 1 2 Grote , Richard M. Osgood ; Columbia Univ., USA; USA We show that when Surface Plasmon Polaritons are manipu- vergence-accommodation conflict in augmented reality ap- 3 4 Military Academy, USA; McMaster Univ., Canada; Univ. of lated and then converted to light, the light acquires not just plications. Principles and our recent implementation results 5 Pennsylvania, USA; Physical Sciences Inc, USA. We char- a dynamic phase, but also a geometric Pancharatnam-Berry using waveguide configuration are presented. Wednesday, 20 Septem Wednesday, acterize a novel DPSK demodulator for Si photonics using phase that is associated with polarization changes. coherent perfect absorption in ring resonator. The fabricated devices are matched with design parameters by measuring transmission spectra in the C-band of telecommunication wavelength.

FW5A.5 • 16:15 FW5B.5 • 16:15 15:30–17:00 Meet the APS Journal A hybrid silicon-phosphorene nanolaser, Chad A. Husko1, Plasma Q-Plate for Intense Laser Beam Shaping, Kenan Editors Reception, International Terrace, Joohoon Kang2, Joshua Wood2, Gregory moille3, Zheng Qu1, Qing Jia1, Nathaniel J. Fisch1; 1Princeton Univ., USA. Han3, David Gosztola1, Xuedan Ma1, Sylvain Combrie4, Alfre- A q-plate for manipulating wavefronts of high-intensity Terrace Level do De Rossi4, Mark Hersam2, Xavier Checoury3, Jeff Guest1; laser beams is proposed in a magnetized plasma. Using 1Argonne National Lab, USA; 2Northwestern Univ., USA; particle-in-cell simulations, we demonstrate that light with 3Centre de Nanosciences et de Nanotechnologies, France; orbital angular momentum above ionization intensity can 16:30–17:00 Pairing Photons to 4Thales Research and Technology, France. We show evidence be generated. Electrons: An OSA Nanophotonics of lasing from a hybrid nanostructure composed of a silicon optical resonator and a two-dimensional phosphorene film. Technical Group Networking, The ~1555 nm emission wavelength opens possibilities for OSA Technical Group Booth, International optically-active devices for integrated silicon photonics. Terrace, Terrace Level

72 FiO + LS 2017 • 17–21 September 2017 Georgetown East Jefferson West Jefferson East

FiO LS

15:00–16:30 15:00–16:30 15:00–16:30 FW5D • Advanced Microscopy and FW5E • Quantum Nonlinear Optics and LW5F • High-harmonic Generation: Time, Imaging Nanophotonics Energy, and Complexity Presider: Francisco Robles; Georgia Institute Presider: Nir Davidson; Weizmann Institute Presider: Josh Vura-Weis; Department of of Technology, USA of Science, Israel Chemistry, UIUC, USA

FW5D.1 • 15:00 FW5E.1 • 15:00 Invited LW5F.1 • 15:00 Invited Compact Module for High-Throughput Label-Free Im- Nonreciprocal on the Nanoscale: Nonlinear Generation Attosecond Charge-transfer Dynamics in Condensed Mat- 1 aging with Custom Field of View, biagio mandracchia , via Multipole Interference, Ekaterina Poutrina1,2, Augustine ter, Martin Schultze1; 1Max Planck Institut fuer Quantenoptik, 1 2,1 1 Vittorio Bianco , Zhe Wang , Melania Paturzo , Pietro Urbas1; 1Air Force Research Lab, USA; 2UES, Inc., USA. We Germany. Electronic population transfer in band-gap ma- 1 1 Ferraro ; Inst. for Applied Sciences and Intelligent Systems, demonstrate that nonreciprocal directionality of nonlinear terials is the basis of modern electronics. Now attosecond 2 Italian National Research Council, Italy; College of Applied generation is inherent to the nonlinear multipolar response of spectroscopy allows us to track this process in real time and Sciences, Beijing Univ. of Technology, China. We designed nanostructures. Similarly, nonlinear multipole interference al- explore possible routes towards light-frequency opto-elec- a LoC with embedded optofluidic holographic microscopy lows directionally selective inhibition of a nonlinear process. tronic signal processing. capabilities. Object flow allows unlimited FoV microscopy of samples in a liquid volume. High-throughput counting and 3D tracking of RBCs is demonstrated.

FW5D.2 • 15:15 Holographic 3D Microscopy of Optically Cleared Tissue, Yibo Zhang1, Yoonjung Shin1, Kevin Sung1, Sam Yang1, Harrison Chen1, Hongda Wang1, Da Teng1, Yair Rivenson1, Rajan Kulkarni1, Aydogan Ozcan1; 1UCLA, USA. Using on-chip holographic microscopy and a simplified CLARITY method with colorimetric staining, we present 3D imaging of optically cleared mouse brain tissue over a large volume of ~5.2 mm × 3.9 mm × 0.2 mm.

FW5D.3 • 15:30 FW5E.2 • 15:30 Invited LW5F.2 • 15:30 Spectral and lifetime measurements of endogenous Propagation and Scaling of Pure Quartic Solitons, C. High Peak Power and Repetition Rate Laser Systems with 1 fluorescence using endoscopic and benchtop microscope Martijn de Sterke1, Gordon H. Li1, Chih Wei Lo1, Alessio Ste- Thin Disk Ti:Sa Amplifiers , Vladimir V. Chvykov , Roland 2 2 1 1 1 configuration, ali ibrahim , Hussein Mehidine , Fanny Pou- fani1, Andrea Blanco Redondo1; 1Univ. of Sydney , Australia. Nagymihaly , Huabao Cao , Mihkail Kalashnikov , Karoly 2 3 3 3 1 1 lon , Johan Pallud , Pascale varlet , Bertrand Devaux , Darine Through numerical simulations and analytical developments Osvay ; ELI-HU Non-Profit Ltd., Hungary. Resuts of the 1 1 Abi Haidar ; Laboratoire IMNC/ Université Paris diderot, we show the propagation behaviour, stability, and energy proof-of-principal experiments with two types thin disc water 2 3 France; Laboratoire IMNC, France; Hopital Sainte Anne, scaling of the recently discovered pure quartic solitons, cooled Ti:Sa amplifiers will be presented. Scaling simulations France. We study the spectral and fluorescence lifetime of indicating excellent potential for pure-quartic solitons in based on experimental results demonstrate feasibility of endogenous fluorescence of tumoral and healthy human ultrafast lasers. hundreds Hz sub-PW Ti:Sa laser systems. tissues. Measurements were taken using endoscope and classical microscopy.

FW5D.4 • 15:45 LW5F.3 • 15:45 Invited Time-Gated Optical Diffraction Tomography, Seth D. Electron Motion Induced by HHG and Strong Fields, 1 1 1 1 Smith-Dryden , Shengli Fan , Guifang Li , Bahaa Saleh ; Philip H. Bucksbaum1; 1Stanford Univ., USA. We present 1 CREOL, Univ. of Central Florida, USA. Optical diffraction time-resolved X-ray absorption spectroscopy of ammonium tomography algorithms typically assume weak scattering, iron(III) oxalate trihydrate and anatase TiO₂ and are therefore not applicable to multiple-scattering

nanoparticles in aqueous solutions using an X-ray free Wednesday, 20 Septem objects. A time-gating approach extending the validity of electron laser in combination with a synchronized ultraviolet these algorithms is proposed and numerically demonstrated. femtosecond laser.

FW5D.5 • 16:00 FW5E.3 • 16:00 Invited Crimp Analysis of Connective Tissue Using Quantitative AlGaAs photonic devices for quantum information, Gi- 1 Second-harmonic Generation Microscopy , Woowon Lee , orgio Maltese1, Jonathan Belhassen1, Saverio Francesconi1, 1 1 1 Hafizur Rahman , Mariana E. Kersh , Kimani C. Toussaint ; Aristide Lemaître2, Florent Baboux1, Maria Amanti1, Sara 1 Univ. of Illinois, Urbana-Champaign, USA. We assess the Ducci1; 1Université Paris Diderot, France; 2Centre de Nano- capacity for second-harmonic generation (SHG) microscopy sciences et de Nanotechnologies, France. We present our ber by quantitatively characterizing collagen fiber crimp pattern last achievements on AlGaAs photonic devices emitting in the posterior cruciate ligament (PCL) and disclosing the non-classical states of light at room temperature. Different 3D structure in PCL and porcine tendon. device designs can be adopted to engineer the generated quantum state depending on the target application.

FW5D.6 • 16:15 15:30–17:00 Meet the APS Journal LW5F.4 • 16:15 Background Removal in Pump-Probe Microscopy, Subir Editors Reception, International Terrace, Multi-port Intra-Cavity High Harmonic Generation in a Das1, Bo-Wei Ho1, Fu-Jen Kao1; 1Inst. of Biophotonics, Yb:YAG Thin Disk Mode-Locked Oscillator with MHz National Yang-Ming Univ., Taiwan. We have established Terrace Level Repetition Rate, Natsuki Kanda1,2, Tomohiro Imahoko3, Koji a pump-probe microscopy with lock-in amplifier for the Yoshida3, A. Amani Eilanlou1, Yasuo Nabekawa1, Tetsumi detection of spontaneous loss and stimulated gain into a Sumiyoshi3, Makoto Kuwata-Gonokami4,5, Katsumi Midorika- single configuration. 16:30–17:00 Pairing Photons to wa1,4; 1RIKEN center for Advanced Photonics, RIKEN, Japan; Electrons: An OSA Nanophotonics 2Photon Science Center, The Univ. of Tokyo, Japan; 3Cyber Laser Inc., Japan; 4Inst. for Photon Science and Technology, Technical Group Networking, The Univ. of Tokyo, Japan; 5Dept. of Physics, The Univ. of OSA Technical Group Booth, International Tokyo, Japan. We demonstrated intra-cavity high harmonic Terrace, Terrace Level generation (HHG) in a Yb:YAG thin disk mode-locked oscillator with a repetition rate of 3MHz. Two HHG ports are simultaneously operated in a single mode-locked oscillator.

FiO + LS 2017 • 17–21 September 2017 73 International Ballroom West International Ballroom East Georgetown West

FiO

16:45–18:15 16:45–18:15 16:45–18:15 FW6A • Optical Fibers and Transmission FW6B • Novel Studies of Waveguides, FW6E • Nanophotonics Devices and Presider: Greg Raybon; Nokia/Bell Labs, Lasers and Atomic Interactions Instrumentation USA Presider: Junsuk Rho; POSTECH, South Korea

FW6A.1 • 16:45 Invited FW6B.1 • 16:45 Invited FW6E.1 • 16:45 Invited High-Capacity Undersea Transmission, Oleg V. Sinkin1, Higher Order Modes of Ultrathin Optical Fibers for Semiconductor Nanolasers Based on 2D Monolayer Gain Alexey Turukhin1, Jin-Xing Cai1, Hussam Batshon1, Matthew Particle Manipulation, Cindy Esporlas1, Aili Maimaiti1, Viet Media Integrated with Silicon Waveguides, Cun-Zheng Mazurzcyk1, Ding Wang1, Milen Paskov1, Carl Davidson1, G. Truong1, Sile Nic Chormaic1; 1Okinawa Inst of Science Ning2,1; 1Arizona State Univ., USA; 2Electronic Engineer- Greg Wolter1, William Patterson1, Pat Corbett1, Tim & Technology, Japan. We exploit some of the properties ing, Tsinghua Univ., China. We review recent progress in Hammon1, Maxim Bolshtyansky1, Dmitri Foursa1, Alexei of the first group of higher order ultrathin optical fiber studying 2D monolayer transition metal dichalcogenides Pilipetskii1; 1TE SubCom, USA. We discuss technologies that modes for particle manipulation. This allows us to exploit as gain materials to be integrated with various micro and enable high-capacity and power-efficient undersea transmis- features such as negative torque and spin-orbital angular nano-cavities for the realization of low energy lasers including sion. We review recent long-haul transmission experiments momentum transfer. room-temperature operation. using conventional single mode fibers and multicore fibers for space division multiplexing.

FW6A.2 • 17:15 FW6B.2 • 17:15 FW6E.2 • 17:15 Ultra-broadband mode conversion with length-apodized Comparison Among Microchannels Fabricated by Nano, Performance analysis of surface plasmon resonance long-period grating on polymer waveguide, Wen Wang1, Pico and Femtosecond-Laser Technologies for Microflu- sensors in the spectral mode: polarimetric vs. intensity. JieYun Wu1, Kaixin Chen1, Wei Jin2, Kin Seng Chiang2; 1Univ idic Applications, María Aymerich López1, María Teresa What is better? and under which conditions?, Ibrahim of Science and Tech of China, China; 2Electronic Engineering, Flores-Arias1, Carlos Molpeceres2, David Canteli2, Javier Watad1, Ibrahim S. Abdulhalim1; 1Ben-Gurion Univ., Israel. City Univ. of Hong kong, Hong Kong. We design and fab- Rodriguez Vazquez de Aldana3; 1USC, Spain; 2UPM, Spain; Recently we have proposed a new spectropolarimetric ricate a length-apodized long-period grating on a polymer 3USAL, Spain. Microchannels fabrication by laser direct method to extract the phase information in surface plasmon

waveguide for ultra-broadbandLP01-LP11b mode conversion. writing over soda-lime glass is presented. Three different resonance sensors. Here, we present a detailed study of the The fabricated device provides a mode-conversion efficiency laser in the IR are employed working on different temporal technique together with comparison to the conventional higher than 99% over a bandwidth of ~150 nm. regimes. Differences among them are evaluated in terms of intensity measurement. their topological surfaces.

FW6A.3 • 17:30 FW6B.3 • 17:30 FW6E.3 • 17:30 Multicore Optical Fibre Components Fabricated Using a Observation of New Mechanism for Slowing Femtosec- Fabrication and Performance Analysis of Mach-Zehnder Femtosecond Laser Direct Writing, Andrei Donko1, Yong- ond Pulses by Liquid-Crystalline Chiral Photonic Crystals, Interferometer Coupled Polymer Microring Resonator min Jung1, Yun Wang1, John Hayes1, Shaif Alam1, Gilberto Chun-Wei Chen1, Xuexue Guo1, Xingjie Ni1, Iam Choon with Microfluidic Channel for Refractive-Index Sensing, Brambilla1, David Richardson1, Martynas Beresna1; 1Univ. Khoo1; 1Pennsylvania State Univ., USA. Studies with ultrafast Saawan Kumar Bag1, Raktim Haldar1, Meher Wan1, Shailendra of Southampton, UK. We report the fabrication of optical laser pulses in cholesteric liquid crystalline photonic crystal K. Varshney1; 1Indian Inst. of Technology Kharagpur, India. components in multicore fibers based on femtosecond laser have revealed a new and more effective mechanism than Mach-Zehnder interferometer coupled polymer microring direct writing, including core selective writing of fibre Bragg bandedge dispersion for slowing light when the laser wave- resonator possessing microfluidic channel is proposed, gratings and optical attenuator for channel equalization. length is located within the photonic bandgap. numerically studied and fabricated for refractive-index sensing applications. Numerical results suggest an improved sensitivity of 202nm/RIU.

FW6A.4 • 17:45 FW6B.4 • 17:45 FW6E.4 • 17:45 Impact of Intercore Cross-talk of a 7-core EDFA in a Intrinsic Optical Bistability in a Rydberg Ensemble, Natalia Single-Process Fabrication Technique for Multi-Level Pho- Photonic Beamformer System, Vanessa C. Duarte1, R. de Melo1, Christopher G. Wade2, Nikola Sibalic2, Jorge tonic Structures, Mutasem A. ODEH1, Marcus S. Dahlem1; 1,2 1 1 2 2 2 1 1

ber Rogério N. Nogueira , Miguel V. Drummond ; Instituto M. Kondo , Charles S. Adams , Kevin J. Weatherill ; Uni- Electrical and Computer Engineering, Masdar Inst., Khalifa de Telecomunicações, Portugal; 2Watgrid, Lda, Portugal. In versidade de Pernambuco, Brazil; 2Joint Quantum Centre Univ. of Science and Technology, United Arab Emirates. We this paper we present a numerical assessment of intercore (JQC) Durham Newcastle, Dept. of Physics, Durham Univ., propose an alignment-free fabrication process to realize cross-talk coming from a 7-core multi-core EDFA when used UK. We investigate intrinsic optical bistability and hysteresis two-level photonic structures using a bilayer resist. The high in a photonic beamforming system. It was observed that in diluted cesium vapor as function of different parameters. contrast of the resist is preserved, and the technique can the distribution increases as path lengths get increasingly The results are consistent with theoretical model based therefore be used in integrated nanophotonics. mismatched. on the semiclassical Maxwell-Bloch equations adding interaction effects.

FW6A.5 • 18:00 FW6B.5 • 18:00 FW6E.5 • 18:00 Optical phase response to thermal strain in a multi-layered Elimination of Spatial Hole Burning in Microlasers, Zhifeng Two-photon fabrication of type I optical Weyl points in hollow-core photonic crystal fiber, Seth Meiselman1, Geof- Zhang1, Pei Miao1, Jingbo Sun1, Stefano Longhi2, Natalia M. photonic crystals, Elena Goi1,2, Zengji Yue1, Benjamin P. frey Cranch2; 1Sotera Defense Solutions, Inc., USA; 2Optical Litchinitser1, Liang Feng1; 1SUNY Buffalo, USA; 2Dipartimento Cumming1,2, Min Gu1,2; 1RMIT, Australia; 2Centre for Ultrahigh Wednesday, 20 Septem Wednesday, Sciences Division, Naval Research Lab, USA. Measurements di Fisica, Politecnico di Milano and Istituto di Fotonica e Bandwidth Devices for Optical Systems (CUDOS), Australia. of thermal phase sensitivity in hollow core photonic crystal Nanotecnologie del Consiglio Nazionale delle Ricerche, Italy. High refractive-index gyroid photonic crystals with broken and kagome type fibers are presented, resolving a discrep- By tailoring the complex index modulations at an exceptional inversion symmetry exhibit two pairs of Type I Weyl points. ancy in previously reported results. We extend an existing point, we demonstrate a microring laser without spatial hole We realize micron-scale structures exhibiting Weyl points derivation to include kagome lattice photonic crystal fiber. burning effect and producing a robust single-mode emission by means of laser direct writing and high refractive-index with enhanced laser slop efficiency and stability. coating.

18:30-20:00 Networking with the OSA Biomedical Optics Technical Groups, OSA Headquarters, 2010 Massachusetts Ave., NW

74 FiO + LS 2017 • 17–21 September 2017 Georgetown East Jefferson West Jefferson East

FiO LS

16:45–18:15 16:45–18:15 16:45–18:15 FW6D • Super-resolution and Extreme FW6E • Quantum Electronics of Ultrafast LW6F • Novel Lasers I Microscopy Signals and Atmospheric Propagation Presider: Ursula Keller; ETH Zurich, Presider: Felix Fanjul-Velez; University of Presider: Brian Smith; University of Oregon Switzerland Cantabria, Spain USA

FW6D.1 • 16:45 Invited FW6E.1 • 16:45 Invited LW6F.1 • 16:45 Invited Nanoscale phase imaging of live cells, Adam Wax1; 1Duke Attosecond Sampling of Arbitrary Optical Waveforms, Advances in Microscale Parity-time-symmetric Lasers, Univ., USA. Quantitative phase imaging uses interferome- Adam S. Wyatt1,2, Tobias Witting4,3, Andrea Schiavi2, Davide Mercedeh Khajavikhan1; 1Univ. of Central Florida, CREOL, try to obtain nanoscale information on live cells. Here we Fabris4, Paloma Matia-Hernando4, Ian Walmsley2, Jon Maran- USA. Microscale semiconductor lasers are an indispensable describe its use for disease diagnosis and analysis of cell gos4, John Tisch4; 1STFC Central Laser Facility, UK; 2Physics, part of integrated photonic circuits. In this paper, we review biomechanical properties. Univ. of Oxford, UK; 3Max Born Inst. for Nonlinear Optics some of the efforts in our group towards the realization of and Short Pulse Spectroscopy, Germany; 4Physics, Imperial such sources using the concept of parity-time-symmetry. College, UK. An interferometric measurement of the real electric field of arbitrary optical waveforms with attosecond resolution via high harmonic generation is experimentally demonstrated and the linearity and temporal/spectral response is numerically analysed.

FW6D.2 • 17:15 Invited FW6E.2 • 17:15 LW6F.2 • 17:15 Ultraviolet Hyperspectral Interferometric Microscopy, Theory-experiment comparison of a quantum based Hybrid Microlaser Resonators Stabilized by Spherical 1 Francisco E. Robles1; 1Georgia Inst. of Technology, USA. We light-matter interaction model for optical filamentation, Waveguides or Unicellular Organisms, Jose A. Rivera , 1 1 2,3 1 1 1 present ultraviolet hyperspectral interferometric microscopy, Anand Bahl , Miroslav Kolesik , Jared Wahlstrand , Howard Thomas Galvin , J. G. Eden ; UIUC, USA. Micro-refractive 3 1 a method that provides molecular information based on Milchberg ; College of Optical Sciences, Univ. of Arizona, element stabilized lasers afford the opportunity to synthesize 2 absorption and dispersion properties of biological samples, USA; Engineering Physics Division, National Inst.s of Stan- composite beam wave-fronts in the far-field. We achieve 3 with subcellular resolution, in the ultraviolet region of the dards, USA; Inst. for Research and Applied Physics, Univ. of lasing from open and closed resonator topologies based spectrum. Maryland, USA. We present an extensive, experiment-theory on either spherical waveguides or unicellular organisms. comparison of the Metastable Electronic State Approach to describe light-matter interaction in nonlinear optics. Excellent agreement validates the method for large-scale space-time resolved simulations.

FW6E.3 • 17:30 LW6F.3 • 17:30 Invited Measurements of the nonlinear refractive index of noble Simulating Spins with Coupled Lasers, Nir . Davidson1; gases and major air constituents at 10 µm using four-wave 1Weizmann Inst. of Science, Israel. We present a system 1 1 1 mixing, Jeremy Pigeon , Sergei Tochitsky , Eric C. Welch , of coupled lasers used for simulating XY spins and finding 1 1 Chandrashekhar Joshi ; UCLA, USA. We report measure- their ground state. ments of the nonlinear refractive index of air, N2, O2, Kr, and Xe at a wavelength near 10 µm by four-wave mixing of an

intense, 200 ps, CO2 laser beat-wave.

FW6D.3 • 17:45 FW6E.4 • 17:45 Invited High-Resolution Light-Field Microscopy, Haoyu Li1, Chan- Creating and dissipating clouds in the atmosphere with Wednesday, 20 Septem 1 1 1 gliang Guo , Shu Jia ; Stony Brook Univ., USA. We report a ultrashort lasers, Jean Pierre Wolf1; 1Universite de Geneve, high-resolution light-field microscopy (LFM) system using a Switzerland. Ultrashort intense lasers are able to efficiently focused optical design. The system has been characterized condensate water vapor in air into droplets, even without both numerically and experimentally. 3D volumetric imaging ionization (mid-IR sub-TW lasers). In addition, existing drop- of cellular structures has been demonstrated. lets can be expelled from the beam to transmit information through fogs.

FW6D.4 • 18:00 LW6F.4 • 18:00 Increasing Acquisition Speeds in Structured Illumination Demonstration of a Self-Stabilized Highly Subluminal ber Microscopy and its Limits, Florian Stroehl1, Clemens F. Laser with a Factor of 400 Suppression in Sensitivity to Kaminski1; 1Univ. of Cambridge, UK. We present a framework Fluctuations, Joshua Yablon1, Zifan Zhou1, Nicholas Con- for structured illumination microscopy (SIM) reconstructions don1,2, Devin Hileman1,2, Shih Tseng1,2, Selim M. Shahriar1; that enables superresolution from 3 raw frames. This pushes 1Northwestern Univ., USA; 2Digital Optics Technologies, SIM’s speed to its boundaries but also defines a limit beyond USA. We demonstrate a self-stabilized, highly-subluminal which deconvolution microscopy is superior. laser in which frequency shift due to cavity length change is suppressed by a factor of the group-index, with a value as high as ~400, with applications in precision metrology.

18:30-20:00 Networking with the OSA Biomedical Optics Technical Groups, OSA Headquarters, 2010 Massachusetts Ave., NW

FiO + LS 2017 • 17–21 September 2017 75 International Ballroom West International Ballroom East Georgetown West

FiO

07:30–11:30 Registration, Concourse Foyer

08:00–08:45 FTh1A • Visionary Speaker: Marc Taubenblatt, International Ballroom West FTh1B • Visionary Speaker: Michael Godwin, International Ballroom East LTh1C • Visionary Speaker: Vladimir M. Shalaev, Jefferson East

08:45–09:00 Break

09:00–10:00 09:00–10:00 09:00–10:00 FTh2A • Tailoring Light with FTh2B • High Harmonics and Novel FTh2C • Optical Coherence Tomography in Naonophotonic Structures Photomemission Biomedical Optics Presider: Aristeidis Karalis; Massachusetts Presider: Christian Reimer; INRS-EMT, Presider: Felix Fanjul-Velez; University of Institute of Technology, USA Canada Cantabria, Spain

FTh2A.1 • 09:00 FTh2B.1 • 09:00 FTh2C.1 • 09:00 Invited 1 Non-Hermiticity Induced Flat Bands, Hamidreza Ramezani ; High Harmonic Generation (HHG) inside a Modelocked Optical Coherence Tomography in Ophthalmology: 1 1 1 Univ. of Texas,Rio Grande Valley, USA. We demonstrate Thin-Disk Laser, Maxim S. Gaponenko , François Labaye , Current Applications and Future Directions, Danuta M. 1 1 1 generation of a robust entire flat band at the exceptional Valentin Wittwer , Clément Paradis , Norbert Modsching , Sampson1,2, Avenell L. Chew1,2, David Alonso-Caneiro3, 1 2 2 point of a PT symmetric lattice. The obtained flat band is Loïc Merceron , Andreas Diebold , Florian Emaury , Ivan Peijun Gong1, Karol Karnowski1, David A. Mackey1,2, Fred 2 1 3 embedded in between dispersive bands and can be con- Graumann , Christopher R. Phillips , Clara J. Saraceno , K. Chen1,2; 1Univ. of Western Australia, Australia; 2Lions Eye 4,5 2 1 sidered as BIC [1]. Christian Kränkel , Ursula Keller , Thomas Südmeyer ; Inst., Australia; 3Queensland Univ. of Technology,, Australia. 1 2 Univ. of Neuchatel, Switzerland; ETH Zurich, Switzer- Optical coherence tomography (OCT) has been the most 3 4 land; Ruhr-Universität Bochum, Germany; Institut für revolutionary diagnostic tool in eye care over the past 5 Laser-Physik, Universität Hamburg, Germany; Center for 20 years. This paper reviews the current status and future Laser Materials, Leibniz Inst. for Crystal Growth, Germany. directions of OCT in ophthalmic application. We demonstrate a compact coherent XUV source based on intracavity high harmonic generation inside a modelocked thin-disk laser, generating photons with energy up to 20.4 eV (17th harmonics) at a repetition rate of 17.4 MHz.

FTh2A.2 • 09:15 FTh2B.2 • 09:15 Chiral Photonic Limiters Utilizing Topologically Protected Tailoring Semiconductors for High Harmonic Generation, Defect States, Ulrich Kuhl3, Fabrice Mortessagne3, Eleana Marco Taucer1, Murat Sivis1,2, Kyle Johnston1, Giulio Vampa1, Makri1, Ilya Vitebskiy2, Tsampikos Kottos1; 1Wesleyan Univ., André Staudte1, Andrei Naumov1, David Villeneuve1, Claus USA; 2Sensors Directorate, Air Force Research Lab, USA; Ropers2, Paul Corkum1; 1National Research Council of 3Institut de Physique de Nice, Université Côte d’Azur, France. Canada, Canada; 24th Physical Inst., Univ. of Goettingen, We propose the design of waveguide limiters based on Germany. We demonstrate new possibilities to tailor high resonances via a topologically protected mode supported harmonic emission in semiconductors using nanofabrication. by coupled microwave resonator arrays. The operational Morphology and local composition can each localize and principle is demonstrated by theoretical analysis and scat- enhance emission, which can be used to realize new high tering measurements. harmonic devices.

FTh2A.3 • 09:30 FTh2B.3 • 09:30 FTh2C.2 • 09:30 Measuring the complex weak value of photon wavefunc- (Angle Resolved) Photoemission Spectroscopy Utilizing Active Microrheology of Hydrogels Based on Oscillations tions beyond weak interaction regime, Kai Wang1,2, Steffen Attosecond Pulse Trains in Argon and Tungsten, Stephan Induced by Optical Radiation Pressure, Nichaluk Leartpra- Weimann1,3, Tim Richardt1, Felix Zimmermann1, Alexander S. Heinrich2,1, Alexander Guggenmos2,1, Fabian Apfelbeck2, pun1, Rishyashring R. Iyer1, Steven G. Adie1; 1Cornell Univ., Solntsev2, Stefan Nolte1, Andrey A. Sukhorukov2, Alexander Michael Stanislawski2, Jürgen Schmidt2, Ulf Kleineberg2,1; USA. Using phase-sensitive OCT, we detect sub-nanometer Szameit1,3; 1Inst. of Applied Physics, Abbe Center of Photon- 1Max-Planck-Institut für Quantenoptik, Germany; 2Fakultät für bead oscillation induced by radiation pressure from a ics, Friedrich-Schiller-Universität Jena, Germany; 2Nonlinear Physik, Ludwig-Maximilians-Universität München, Germany. low-NA beam in agar hydrogels. Our method may enable Physics Centre, Research School of Physics and Engineering, We report on experiments with attosecond pulse trains that characterization of microscale viscoelastic properties, with The Australian National Univ., Australia; 3Inst. for Physics, are focused on gas and solid state targets. Using the RAB- applications in cell mechanics. Rostock Universität, Germany. We measure the complex BITT-technique the emitted photoelectrons reveal informa-

ber weak value beyond the weak interaction regime between tion about the pulse train itself and the system under study. the measurement apparatus and the measured photon wavefunction based on the direct measurement scheme. Thursday, 21 Septem Thursday,

76 FiO + LS 2017 • 17–21 September 2017 Georgetown East Jefferson West Jefferson East

FiO LS

07:30–11:30 Registration, Concourse Foyer

08:45–09:00 Break

09:00–10:00 09:00–10:00 09:00–10:00 FTh2D • Fabrication for Nanophotonics FTh2E • Optics in Computing LTh2F • Plasmonics Presider: Euan McLeod; University of Presider: Alexander Sergienko; Boston Presider: Ursula Keller; ETH Zurich, Arizona, USA University, USA Switzerland

FTh2D.1 • 09:00 Invited FTh2E.1 • 09:00 LTh2F.1 • 09:00 Invited Realization of 3D Metamaterial and Plasmonic Devices at High Speed Self-testing Quantum Random Number Quantifying Optical Coherence Modulation with Plasmon- 1,2 Optical Frequencies, Junsuk Rho1; 1POSTECH, South Korea. Generation Without Detection Loophole, Yang Liu , Xiao ic Interferometry, Domenico Pacifici1; 1Brown Univ., USA. 1,2 1,2 4 3 I will discuss recent development of fabrication for three-di- Yuan , Ming-Han Li , Weijun Zhang , Qi Zhao , Jiaqiang Plasmonic interferometry can be employed to measure and 5 1,2 1,2 1,2 4 mensional metamaterials based on two different approaches. Zhong , Yuan Cao , Yu-Huai Li , Luo-Kan Chen , Hao Li , modulate the spectral degree of coherence of light. This 3 1,2 1,2 The examples include 3D chiral metamaterials (at terahertz Tianyi Peng , Yu-Ao Chen , Cheng-Zhi Peng , Sheng-Cai technique lends itself as a new tool to design multifunc- 5 4 4 3 1,2 and infrared) and self-assembled 3D chiral materials. Shi , Zhen Wang , Lixing You , Xiongfeng Ma , Jingyun Fan , tional optical elements beyond conventional refractive- and 1,2 1,2 1 Qiang Zhang , Jian-Wei Pan ; Shanghai Branch, National diffractive-based photonics. Lab for Physical Sciences at Microscale, Univ. of Science and Tech. of China, China; 2Shanghai Branch, CAS Center for Excellence and Synergetic Innovation Center in Quantum Information and Quantum Physics, Univ. of Science and Tech of China, China; 3Center for Quantum Information, Inst. for Interdisciplinary Information Sciences, Tsinghua Univ., Chi- na; 4State Key Lab of Functional Materials for Informatics, Shanghai Inst. of Microsystem and Information Tech, Chinese Academy of Sciences, China; 5Purple Mountain Observatory and Key Lab of Radio Astronomy, Chinese Academy of Sci- ences, China. We experimentally demonstrate a self-testing quantum random number generation based on an detection-loophole free Bell test with entangled photons. We achieve a final random bit rate of 114 bits/s, with a failure probability less than 10^-5.

FTh2E.2 • 09:15 All Optical Rapid Solver of the Inverse Scattering Prob- lem, Nir . Davidson1, Chene Tradonsky1, Ronen Chriki1, Vishwa Pal1, Asher Friesem1; 1Weizmann Inst. of Science, Israel. An all-optical approach for very rapidly solving inverse scattering problems by means of novel computer controlled digital degenerate cavity laser is presented, along with supporting simulated and experimental results.

FTh2D.2 • 09:30 FTh2E.3 • 09:30 Invited LTh2F.2 • 09:30 Electro-Optically Sampled Time Response of Core-Shell Photonic Networks for Neuromorphic Computing, Daniel Robust enhancement of random laser action assisted 2 3 3 1 1 Nanowires, Marc Currie , Anna Persano , Adriano Taurino , Brunner1, Ingo Fischer2, Maxime Jacquot1, Laurent Larger1; by hyperbolic metamaterials, Hung-I Lin , Yu-Ming Liao , 3 3 3 1 1 1 Fabio Quaranta , Adriano Cola , Paola Prete , Nico Lov- 1CNRS - FEMTO-ST, France; 2IFISC, UIB-CSIC, Spain. We kun-ching Shen , Yang-Fang Chen ; National Taiwan Univ., 4 5 1 1 ergine , Pouya Dianat , Zhihuan Wang , Bahram Nabet ; introduce a novel scheme for optically coupling photonic Taiwan. We use hyperbolic metamaterials to strongly en- 1 2 Drexel Univ., USA; Optical Sciences Division, Naval Re- emitters. Our network of 1600 nonlinear oscillators raises hance random laser action and reduce lasing threshold. The 3 search Lab, USA; IMM-CNR, Inst. for Microelectronics and current limits by orders of magnitude.We implement neu- excited high-k modes can increase the possibility of forming 4 Microsystems, Italy; Dept. of Innovation Engineering, Univ. romorphic computing in our photonic network and predict closed loop paths and decrease the energy consumption of 5 of Salento, Italy; Northwestern Univ., Center for Quantum a chaotic timeseries. photon propagation. Thursday, 21 Septem Devices, USA. We present time response measurements of single GaAs/AlGaAs core-shell nanowire using high-resolution electro-optic sampling technique. These nanowires show high quantum efficiency and a response speed faster than comparable devices in bulk. ber

FiO + LS 2017 • 17–21 September 2017 77 International Ballroom West International Ballroom East Georgetown West

FiO

FTh2A • Tailoring Light with FTh2B • High Harmonics and Novel FTh2C • Optical Coherence Tomography in Naonophotonic Structures—Continued Photomemission—Continued Biomedical Optics—Continued

FTh2A.4 • 09:45 FTh2B.4 • 09:45 FTh2C.3 • 09:45 Unidirectional Localized Modes, Hamidreza Ramezani1, Frequency comb generation in continuously pumped op- A Hand-Held Optical Coherence Tomography and Pankaj Jha2, Yuan Wang2, Xiang Zhang2; 1Univ. of Texas,Rio tical parametric oscillator, maria parisi1, Iolanda Ricciardi1, Vibrometry Device for Human Inner Ear Imaging with Grande Valley, USA; 2Mechanical Engineering, Univ. of Francois Leo2, Tobias Hansson3, Miro Erkintalo4, Pasquale Subnanometer Sensitivity to Vibration, Wihan Kim1, California Berkeley, USA. we demonstrate the generation of Maddaloni1, Paolo De Natale5, Stefan Wabnitz6,1, Maurizio Sangmin Kim1, John Oghalai2, Brian E. Applegate1; 1Dept. unidirectional localized mode in a spatiotemporally modulat- De Rosa1, simona mosca; 1CNR-INO, Istituto Nazionale di of Biomedical Engineering, Texas A&M Univ., USA; 2Dept. ed photonic lattice containing a static defect. Our proposal Ottica, Italy; 2OPERA-photonics, Université Libre de Brux- of Otolaryngology-Head and Neck Surgery, Stanford Univ., might help the design for devices such as non-reciprocal elles, Belgium; 3INRS-EMT, Canada; 4The Dodd-Walls Centre USA. We are developing endoscopic OCT to visualize the sensors, and unidirectional lasers. for Photonic and Quantum Technologies, Dept. of Physics, morphology and functional vibratory response of the human The Univ. of Auckland, New Zealand; 5CNR-INO, Istituto inner ear through the round window. Preliminary results show Nazionale di Ottica, Italy; 6Dipartimento di Ingegneria dell’In- good image quality with 41±21 pm sensitivity on piezo formazione, Università di Brescia, Italy. We demonstrate and element while hand-held. theoretically explain optical frequency comb generation in a cw-pumped, doubly resonant optical parametric oscillator. Numerical simulations are in pretty good agreement with the observed comb patterns.

10:00–10:30 Coffee Break, International Terrace, Terrace Level

NOTES ______

ber ______

Thursday, 21 Septem Thursday, ______

78 FiO + LS 2017 • 17–21 September 2017 Georgetown East Jefferson West Jefferson East

FiO LS

FTh2D • Fabrication for Nanophotonics— FTh2E • Optics in Computing—Continued LTh2F • Plasmonics—Continued Continued

FTh2D.3 • 09:45 LTh2F.3 • 09:45 Omniresonant Absorption in a One-Dimensional Cavity Refractive Index Sensing With 1D Photonic Crystal, Samir Containing Monolayer Graphene, Ali Kazemi Jahromi1, Kumar1, Ritwick Das1; 1School of Physical Sciences, National Massimo Villinger1, Ahmed Elhalawany1, Soroush Shabaha- Inst. of Science Education and Research, HBNI, India. A ng1, H. E. Kondakci1, Ayman Abouraddy1; 1Univ. of Central refractive index sensor is proposed based on the cavity Florida, CREOL, USA. Coherent perfect absorbers are mode formed in a thin analyte layer sandwiched between deemed to exhibit total absorption only at discrete wave- multilayers of SiO2/Ta2O5, and a metal film. This study opens lengths. By pre-conditioning wavelength-angle relation of up alternatives to the SPR based biochemical sensors. an incoming beam, we demonstrate a resonant absorption in continuously broadband range of wavelengths.

10:00–10:30 Coffee Break, International Terrace, Terrace Level

NOTES ______Thursday, 21 Septem ______

______ber ______

FiO + LS 2017 • 17–21 September 2017 79 International Ballroom West International Ballroom East Georgetown West

FiO

10:30–12:30 10:30–12:30 10:30–12:30 FTh3A • Nanophotonics for Computing FTh3B • Optomechanics and Sensors FTh3C • Vision and Color and Sensing Presider: Gabriel Diaz; Rochester Institution of Technology, USA

FTh3A.1 • 10:30 Invited FTh3B.1 • 10:30 FTh3C.1 • 10:30 Invited Silicon Photonics, Thomas van Vaerenbergh1; 1Hewlett Inertial Injection Locking in an Electro-optomechanical Visual and Multi-modal In-vehicle Collision Warnings, 1 1 Packard, USA. Abstract not provided. System, Christiaan Bekker , Christopher Baker , Rachpon Carryl Baldwin1; 1George Mason Univ., USA. In-vehicle for- 1 1 1 Kalra , Warwick P. Bowen ; School of Mathematics and ward collision warnings can be presented in visual, auditory Physics, The Univ. of Queensland, Australia. Electro-optome- or tactile modalities. Unimodal and bimodal warning combi- chanical systems are a platform for exploring rich physics nations were compared. Audiovisual and visuotactile FCWs such as frequency conversion and synchronization. Here hold promise for improving traffic safety. we demonstrate the first case of inertial injection locking in a radiation pressure driven electro-optomechanical system.

FTh3B.2 • 10:45 Magnetometry via spin-mechanical coupling in levitated optomechanics, Pardeep Kumar1, Mishkatul Bhattacha- rya1; 1Rochester Inst. of Technology, USA. We investigate magnetometry with a levitated nanodiamond. Our results indicate that high magnetic field gradient sensitivity (50 µTm- 1Hz-1/2) can be achieved by interrogating the nanodiamond position or spin.

FTh3A.2 • 11:00 FTh3B.3 • 11:00 FTh3C.2 • 11:00 Invited Organically modified microresonators for high efficiency Optomechanical cooling without added damping, Seung- Perceptual considerations for building a foveated display 2 2,1 1 2 2,3 1 1 microlasers , Xiaoqin Shen , Rigoberto C. Beltran , Vinh hwi Kim , Xunnong Xu , Jacob Taylor , Gaurav Bahl ; Univ. for VR/AR, Joohwan Kim1, David Luebke1; 1NVIDIA Cor- 2 2 2 1 2 Diep , Soheil Soltani , Andrea Armani ; Universidad de of Illinois at Urbana-Champaign, USA; Univ. of Maryland, poration, USA. Foveated display is a promising paradigm 2 3 Guanajuato, Mexico; Univ. of Southern California , USA. USA; National Inst. of Standards and Technology, USA. for achieving the challenging requirements of immersive We report a strategy to excite specific frequency conversion We demonstrate optomechanical cooling without added and comfortable VR/AR experiences. In this talk, a set of processes by organically modified microresonators with a damping in a whispering gallery mode resonator by means perceptual considerations for building a foveated display monolayer of small molecules. Frequency comb generation of disorder-induced scattering. The phenomenon results will be reviewed. and Raman lasing are selectively activated and enhanced from a reduction of thermal loading so that it eventually up to three orders. induces chirality of phonons.

FTh3A.3 • 11:15 FTh3B.4 • 11:15 Low-threshold Rhodamine B doped microlasers fabricat- Ergoregion in Metamaterials Mimicking a Kerr Spacetime, ed via two-photon polymerization, Nathalia B. Tomazio1, Danilo Pires1, Paulo A. Brandão2, José C. Rocha1; 1GON, Leonardo De Boni1, Cleber R. Mendonça1; 1USP Inst de Brazil; 2Instituto de Física, Brazil. We design metamaterials Fisica de Sao Carlos, Brazil. We present dye whispering which simulate an ergoregion that is, in the context of gen- gallery mode (WGM) microlasers fabricated via two-photon eral relativity, a region surrounding rotating black holes in polymerization. Threshold pump energies as low as 13 nJ which all particles must rotate in the same sense as the hole. with slope efficiency of 30% were obtained for free space pulsed excitation at 532 nm.

FTh3A.4 • 11:30 FTh3B.5 • 11:30 FTh3C.3 • 11:30 Invited Improvement of sensing performance of ITO grating Polarization-independent, Narrowband Transmission The Potential for Improving Impaired Vision with Aug- assisted SPR sensor using ITO-metal configuration, Ashish Filter Using Symmetry-protected Bound States in the mented Reality, Emily Cooper1; 1Dartmouth College, USA. 1 1 1 1 1 Bijalwan , Vipul Rastogi ; Physics, Indian Inst. of Technology Continuum, Justin M. Foley , Yichen Shuai , Navin Lingara- I will present work assessing whether current-generation 1 1 1 Roorkee, India. We propose an ITO grating and metallic ju , John Lawall ; Physical Measurement Lab, National Inst. augmented reality systems can be used to improve the (Au or Ag or Al) film based SPR sensor. Here, we report a of Standards and Technology, USA. We compututationally functional vision of people with low vision or blindness. comparative study of conventional ITO grating and proposed and experimentally demonstrate a narrowband, polariza- ITO grating-metallic film based sensors using RCWA. tion-independent transmission filter using a subwavelength, 2D photonic crystal slab that operates through coupling to symmetry-protected bound states in the continuum.

FTh3A.5 • 11:45 FTh3B.6 • 11:45 Thermally-Tunable-Silicon-Ring-Resonator-Based High- Mid IR focusing in Doped-Semiconductor Hyperbolic Speed Optical Sensor Interrogator for Impact Monitoring, Metamateial, Mai desouky1, Ahmed Mahmoud1, Mohamed Hyun-Tae Kim1, Miao Yu1; 1Univ. of Maryland at College A. Swillam1; 1Physics, American Univ. in Cairo, Egypt. Doped ber Park, USA. We demonstrate dynamic strain measurement semiconductors with plasmonic resonance in the mid IR have using a high-speed (100 kHz) optical sensor interrogator been realized for mid IR Metamaterials. We theoretically with a thermally tunable silicon ring resonator. Resonance demonstrate sub-wavelength focusing at 7.32 µm using frequencies of the aluminum cantilever under impact loading doped InAs/InAs Hyperbolic Metamaterial with focusing were measured up to 7.36 kHz. resolution of 0.128λ. Thursday, 21 Septem Thursday,

80 FiO + LS 2017 • 17–21 September 2017 Georgetown East Jefferson West Jefferson East

FiO LS

10:30–12:30 10:30–12:30 10:30–12:30 FTh3D • Instrumentation for Optical FTh3E • Quantum Simulation, LTh3F • Plasmonics and Lasing Devices and Systems Communication and Entanglement Presider: Domenico Pacifici; Brown Presider: Junsuk Rho; Seoul National University , USA University, South Korea

FTh3D.1 • 10:30 Invited FTh3E.1 • 10:30 Invited LTh3F.1 • 10:30 Invited How Freeform Optics Induced Optical Aberrations Mat- Quantum Simulation of Complex Hamiltonians with Broadband Hot Electron Creation and Ultrafast Optical ter, Jannick P. Rolland1, Aaron Bauer1; 1Univ. of Rochester, Directionally Unbiased Linear-Optical Multiports, Alexan- Responses in Nanoscale Gap Plasmon Metasurfaces, Gary USA. Aberration theory and optical design walk hand-in- der V. Sergienko1, David S. Simon2,1, Shuto Osawa1, Casey Wiederrecht1; 1Argonne National Lab, USA. Ultrafast photo- hand, whether it is human or computer driven. We shall take Fitzpatrick1; 1Boston Univ., USA; 2Stonehill College, USA. excitation of plasmonic nanostructures can produce highly a peek at the aberrations of freeform optics and their impact The directionally unbiased optical multiport is introduced, energetic “nonthermal” electrons. We report on the unusual on design strategies – is the past obsolete? in which photons may reflect back out the input direction. ability of gap plasmon metasurfaces to produce nonthermal Quantum walks on arrays of such multiports allow the electrons at high efficiency over broad spectral ranges. simulation of a range of complex quantum Hamiltonians.

FTh3D.2 • 11:00 FTh3E.2 • 11:00 LTh3F.2 • 11:00 Efficient Measurement of Nonstationary Complex Integrated generation of high-dimensional entangled Formation of Spatial Solitons in a Colloid of Biosyn- Coherence Functions, Heath E. Gemar1, Roxana Rezvani photon states and their coherent control, Christian Re- thesized Gold Nanoparticles, Argelia Balbuena Ortega1, Naraghi1, Mahed Batarseh1, Andre Beckus1, George Atia1, imer1, Michael Kues1, Piotr Roztocki1, Luis Romero Cortes1, Martha Yadira Salazar Romero1, Valentin López Gayaou2, Sergey Sukhov1, Aristide Dogariu1; 1Univ. of Central Florida, Stefania Sciara1, Benjamin Wetzel1, Yanbing Zhang1, Alfonso Alejandro Vasquez Arzola1, Karen Volke Sepulveda1; 1UNAM, USA. We demonstrate an accurate, two-step procedure for Cino2, Sai Chu3, Brent Little4, David Moss5, Lucia Caspani6, Mexico; 2CIBA-IPN, Mexico. The nonlinear optical properties measuring the full complex coherence function. The mea- Jose Azana1, Roberto Morandotti1; 1INRS-EMT, Canada; of gold nanoparticles were investigated. As a result of the surement relies on a wavefront shearing interferometer that 2Univ. of Palermo, Italy; 3City Univ. of Hong Kong, China; characterization, samples with the higher nonlinear optical permits characterizing nonstationary fields over an extended 4Xi’an Inst. of Optics and Precision Mechanics of CAS, response were selected, to demonstrate the formation of angular domain. China; 5Swinburne Univ. of Technology, Australia; 6Univ. of bright spatial solitons propagating 10mm. Strathclyde, UK. We demonstrate the generation of high-dimensional entangled photon pairs with a Hilbert-space dimensionality larger than 100 from an on-chip nonlinear microcavity, and introduce a coherent control scheme using standard telecommunications components.

FTh3D.3 • 11:15 FTh3E.3 • 11:15 LTh3F.3 • 11:15 Automated Multiple Target Superresolution Imaging, Frequency-bin entangled qutrits in an on-chip microres- Stretchable random lasers with tunable coherent loops, Farzin Farzam1, Keith A. Lidke1; 1Univ. of New Mexico, USA. onator, Poolad Imany1, Jose A. Jaramillo-Villegas1, Ogaga Shih-Yao Lin1, Tzu-Min Sun1, Cih-Su Wang1, Chi-Shiun Liao1, Single molecule superresolution of multiple targets is chal- Odele1, kyunghun han1, minghao Qi1, Daniel E. Leaird1, Packiyaraj Perumal1, Chia-Wei Chiang1, Yang-Fang Chen1; lenging due to limited availabe dyes with right photophysical Andrew M. Weiner1; 1Electrical and Computer Engineering, 1National Taiwan Univ., Taiwan. We have successfully demon- properties and emission path differential aberrations. We Purdue Univ., USA. We demonstrate three-dimensional fre- strated a stretchable random laser with tunable coherent present an automated high-throughput microscope to quency-bin entanglement using three contiguous frequency loops based on ZnO nanobrushes deposited on PDMS overcome challenges. mode pairs from a quantum frequency comb generated in elastomer substrate. The number of laser modes increases an integrated optical microresonator. with increasing external strain applied on the substrate.

FTh3D.4 • 11:30 FTh3E.4 • 11:30 LTh3F.4 • 11:30 Invited Withdrawn. Quantum fingerprinting without a shared phase refer- Solid-state quantum optics with atomically thin semi- 1 1 1 ence, Michal Lipka , Michal Jachura , Marcin Jarzyna , Kon- conductors, Nickolas Vamivakas1; 1Univ. of Rochester, USA. 1 1 rad Banaszek ; Univeristy of Warsaw, Poland. We present a Excitons and trions in transition metal dichalcogenides are quantum fingerprinting protocol relying on two-photon inter- providing new opportunities for solid-state quantum optics. ference which does not require phase stabilization between In this talk I will describe recent work on both quantum dots the parties. Application of non-classical single photon states and cavity polaritons in these materials. enhances its performance even for high transmission loss.

FTh3D.5 • 11:45 FTh3E.5 • 11:45 Sub-Diffraction Feature Size in Conventional I-Line Pho- Entanglement Detection of a Mixed State without Coin- toresists, David Miller1, Adam Jones2, Robert R. McLeod1; cidence Measurement, Mayukh Lahiri1, Gabriela B. Lemos2, Thursday, 21 Septem 1Univ. of Colorado at Boulder, USA; 2Sandia National Labs, Armin Hochrainer1, Anton Zeilinger1,2; 1VCQ, Faculty of USA. Applying a technique from super-resolution micros- Physics, Univ. of Vienna, Austria; 2Inst. for Quantum Optics copy to photolithography, we achieve feature sizes below and Quantum Information, Vienna, Austria. We consider two the diffraction limit. Using conventional i-line photoresists spatially separated identical bi-photon sources each of which exposed with near UV, we demonstrate individual feature can produce a polarization entangled mixed state. We show sizes below 100 nm. that it is possible to determine whether the state is entangled without any coincidence measurement. ber

FiO + LS 2017 • 17–21 September 2017 81 International Ballroom West International Ballroom East Georgetown West

FiO

FTh3A • Nanophotonics for Computing FTh3B • Optomechanics and Sensors— FTh3C • Vision and Color—Continued and Sensing—Continued Continued

FTh3A.6 • 12:00 FTh3B.7 • 12:00 FTh3C.4 • 12:00 (Recorded) Fiber optic biosensor for the detection of Bovine Serum Acousto-Optic Filter with Metamaterial Inclusions, Ni- Spectral Considerations for Transportation Lighting Albumin using Graphene Oxide , Jeeban Nayak1, Rajan kolai I. Petrov1, Vladislav I. Pustovoit2; 1Scientific Research Systems, John D. Bullough1; 1Rensselaer Polytechnic Inst., Jha1; 1Indian Inst of Technology, Bhubaneswar, India. Fiber Center of Unique Instrumentation of the Russian Academy USA. Transportation lighting specifications using photopic optic biosensor using Graphene Oxide (GO) decorated gold of Sciences, Russia. The problem of Bragg diffraction of photometry are poorly correlated with many relevant visual nanoparticles (AuNPs) has been reported. GO is immobilized light in the Fabry-Perot resonator formed by two dynamic responses such as peripheral detection, brightness percep- on AuNPs coated fiber probe. The interaction of GO with acousto-optic mirrors is considered. Significant increase in tion and discomfort glare. Potential impacts on specifications BSA reduces the absorbance peak at resonance wavelength. spectral resolution due to the spatial variation of the medium are discussed. properties is shown.

FTh3A.7 • 12:15 FTh3B.8 • 12:15 FTh3C.5 • 12:15 Compact Automotive Optical Current Sensor Based on Transparent conducting electrodes for efficient near-field Improved method to simulate the halos induced by simul- Evanescent-Wave Scattering by Ferromagnetic Particles, thermophotovoltaics, Aristeidis Karalis1, John D. Joan- taneous vision, Guillermo Perez1, Henk Weeber1, Patricia Binghui LI1, Hau Ping Chan1, Kazi T. Ahmmed1, Zhe Huang1; nopoulos1; 1MIT, USA. Doped semiconductors, conducting Piers1; 1Jonhson & Johnson Vision, Netherlands. Halos may 1City Univ. of HONG KONG, Hong Kong. A compact opti- oxides and graphene are compared as transparent front be noticed by patients implanted with intraocular lenses. cal sensor is proposed for automotive current monitoring. electrodes for resonant near-field thin-film TPV cells, with An improved method has been developed to simulate the Dynamic sensitivity of 0.0357 dB/mA is achieved with good resulting efficiencies up to 54% at 2100K thermal-emitter perception of halos that solves inaccuracies and mimics the linearity. Multiple sensor outputs can be transmitted through temperature and >20W/cm2 load power-density. characteristic veiling effect induced by this phenomenon. a single fiber by wavelength-division-multiplex scheme.

12:30–13:30 Lunch Break (on your own)

Join the conversation. Follow @Opticalsociety on Twitter. Use hashtag #FIO17 ber Thursday, 21 Septem Thursday,

82 FiO + LS 2017 • 17–21 September 2017 Georgetown East Jefferson West Jefferson East

FiO LS

FTh3D • Instrumentation for Optical FTh3E • Quantum Simulation, LTh3F • Plasmonics and Lasing—Continued Devices and Systems—Continued Communication and Entanglement— Continued

FTh3D.6 • 12:00 FTh3E.6 • 12:00 LTh3F.5 • 12:00 Rapid Single-Exposure Fabrication of 2D and 3D Cus- The Quantum Entanglement of Measurement, Shota Yo- Lasing from Bound States in the Continuum, Ashok Kodi- tom-Modified Interference Patterns by Pattern-Inte- koyama1,2, Nicola D. Pozza1,2, Takahiro Serikawa1,3, Katanya gala1, Thomas Lepetit1, Qing Gu1, Babak Bahari1, Yeshaiahu grated Interference Lithography, Shruthi Kumara Vadivel1, B. Kuntz1,4, Trevor A. Wheatley1,2, Daoyi Dong1, Elanor H. Fainman1, Boubacar Kante1; 1Univ. of California, San Diego, Matthieu C. Leibovici1, Thomas K. Gaylord1; 1Georgia Inst. Huntington1,5, Hidehiro Yonezawa1,2; 1School of Engineering USA. We have designed a high quality factor cavity that is of Technology, USA. The Pattern-Integrated Interference and Information Technology, The Univ. of New South Wales, based on a bound state in the continuum and harnessed its Lithography (PIIL) exposure system is analyzed. Experimental Australia; 2Centre for Quantum Computation and Commu- properties to demonstrate a novel type of surface emitting results of custom-modified interference patterns show good nication Technology, Australian Research Council, Australia; laser operating at room temperature. agreement with simulations, thus validating the modeling 3Dept. of Applied Physics, School of Engineering, The Univ. and fabrication methods employed. of Tokyo, Japan; 4Inst. for Quantum Computing, Univ. of Waterloo, Canada; 5Research School of Engineering, College of Engineering and Computer Science, Australian National Univ., Australia. We demonstrate two-mode detector tomography on a detector consisting of two superconducting nanowire single photon detectors. The entangling properties of the detector is verified through a new entanglement measure of a multi-mode detection.

FTh3D.7 • 12:15 FTh3E.7 • 12:15 LTh3F.6 • 12:15 Polarization and phase shifting interferometry, Sergej Towards practical characterization of quantum systems Experimental and theoretical study of single-mode 1018 Rothau1, Klaus Mantel2, Norbert Lindlein1; 1Inst. of Optics, with quantum Hamiltonian learning, Raffaele Santagati3, nm ytterbium-doped fiber laser with 100 W output power, Information, and Photonics, Friedrich-Alexander-Univ. Jianwei Wang3, Stefano Paesani3, Sebastian Knauer3, Anto- Jian H. Lin1, Wei-Ting Lin1, Chiang-Hsin Lin1, Wei-Lin Chen1, Erlangen-Nuremberg, Germany; 2Max Planck Inst. for the nio Gentile3, Nathan Wiebe1, Matteo Petruzzella2, Jeremy Wen-Cheng Huang1, Po-Tse Tai1; 1Materials & Electro-Optics Science of Light, Germany. The theory and experimental O’Brien3, John Rarity3, Anthony Laing3, Mark Thompson3; Research Division, National Chung-Shan Inst. of Science and results of a novel interferometric approach for simultaneous 1Quantum Architectures and Computation Group, Micro- Technology, Taiwan. This work theoretically and experimen- characterization of the optical elements with respect to their soft Research, Microsoft, USA; 2Dept. of Applied Physics, tally demonstrates one hundred-watt and near single-mode impact on the polarization and the phase of an incoming Eindhoven Univ. of Technology, Netherlands; 3Quantum En- of the 1018 nm ytterbium-doped fiber laser (YDFL). Amplified light wave are presented. gineering Technology Labs, H. H. Wills Physics Lab and Dept. spontaneous emission effect in YDFL can be suppressed, of Electrical and Electronic Engineering, Univ. of Bristol, which agrees with the simulations. UK. Here we show the first experimental implementation of quantum Hamiltonian Learning, where a silicon-on-insulator quantum photonic simulator is used to learn the dynamics of an electron-spin in an NV center in diamond.

12:30–13:30 Lunch Break (on your own) Thursday, 21 Septem ber

FiO + LS 2017 • 17–21 September 2017 83 Georgetown East Jefferson West Jefferson East

FiO LS

13:30–15:30 13:30–15:30 15:00–17:00 FTh4A • Postdeadline Papers FTh4B • Postdeadline Papers LTh4F • Novel Lasers III Presider: Mark Raizen; University of Texas at Austin, USA

LTh4F.1 • 15:00 Invited See Update Sheet for list of Post-Deadline Papers Random Lasers in the Mid-infrared and Terahertz, Qijie Wang1, Yongquan Zeng1; 1Nanyang Technological Univ., Singapore. Random lasers were demonstrated in the mid-infrared and terahertz regimes in quantum cascade lasers with electrical pumping. Air-holes, dielectric pillars and metallic pillars were employed as efficient scatters to achieve multi-mode lasing.

LTh4F.2 • 15:30 Spatiotemporal Characterization of Ultrashort Pulses from the near- to mid-IR, Sina Zahedpour Anaraki1, Jared K. Wahlstrand2; 1Univ. of Maryland at College Park, USA; 2National Inst. of Standards and Technology, USA. We use 2D spectral interferometry to characterize the full spatiotemporal profile of laser pulses. An intense pump imprints upon a weak broadband visible probe its spatial and temporal profile, which can be recovered using silicon based detectors.

LTh4F.3 • 15:45 Multiple-Beam Generation from a Single-Cavity Titani- um-Sapphire Thin-Disk Laser, Austin W. Steinforth1, José A. Rivera1, J. G. Eden1; 1Univ. of Illinois, USA. We demonstrate

a laser array generated by a Ti:Al2O3 thin disk inside a Fabry-Pérot resonator stabilized by microlenses. More than 1,000 beams were produced from a single cavity.

LTh4F.4 • 16:00 Invited Dual-comb Spectroscopy with One Unstabilized Semi- conductor Laser, Ursula Keller1; 1ETH Zurich, Switzerland. We present dual-comb spectroscopy on water vapor with a free-running modelocked semiconductor laser. The simple and compact laser emits simultaneously two gigahertz pulse trains with slightly different pulse repetition rates from a single cavity.

LTh4F.5 • 16:30 Directional random lasing mediated by transverse Ander- son localization, Behnam Abaie1, Thomas Hawkins2, John Ballato2, Arash Mafi1; 1Univ. of New Mexico, USA; 2Clemson Univ., USA. Anderson localized modes of a dye-filled disordered optical fiber are exploited for directional random lasing. Strong transverse localization reduces the spatial overlap of the lasing modes and results in a spectrally stable random laser emission.

LTh4F.6 • 16:45 Optofluidic droplet lasers on polycarbonate chip, Han Zhang1, Yuze Sun1; 1Univ. of Texas at Arlington, USA. We demonstrated optofluidic droplet lasers using micro-nozzle structures. Easy fabrication, reproducible generation and manipulation of microdroplets provide a promising platform to achieve integrated laser system on chip. ber Thursday, 21 Septem Thursday,

84 FiO + LS 2017 • 17–21 September 2017 Key to Authors and Presiders Key to Authors

A An, Guofei - JTu3A.112 Banergee, Parag - JTu3A.29, JTu3A.93 A, Aadhi - FW2B.2 An, Sha - JTu3A.4 Banerjee, Aritra - JW4A.116 Aashna, Pragati - JTu3A.100, JW4A.105, JTu3A.8, Anderson, Benjamin R. - FM3C.2, JTu2A.36, Banerji, J - JTu3A.96 JW4A.96, LTh4F.5 JTu2A.71 Banerji, Pallab - JW3A.70, JW4A.48 Abbasirad, Najmeh - JW3A.118 Anderson, Brian E. - FM2D.4, JW3A.36 Banzer, Peter - FM3B.1 Abdelatty, Mohamed - JW4A.41, JW4A.43 Anderson, Stephen - JW4A.47 Bao, Yijun - FM3C.3 Abdolazimi, Vahideh - JTu3A.44 Andreasen, Jonathan - JW3A.30 Barach, Gilad - FM3B.3, FTu4C.4 Abi Haidar, Darine - FW5D.3 Andres, Miguel Vicente - JW4A.72 Barannikov, Alexandr - JTu2A.16 Abouraddy, Ayman - FM4C.5, FM4C.6, FTh2D.3, Angelo, Joseph - FTu5C.1 Bar-Gill, Nir - JW4A.17 FTu4B.3, FTu5A.5, JTu3A.104, JTu3A.64, Anjum, Arslan - FTu5B.4 Barh, Ajanta - FTu5D.3, JTu3A.38 JW4A.99 Antikainen, Aku - FTu5A.2 Barka, Ibrahim - JW4A.62 Abrashitova, Ksenia - JTu2A.16 Anwar, Ali - JW4A.13 Barlow, Stephen - JTu3A.61 Acioli, Lucio H. - JW4A.18 Anzulevich, A.P. - JW3A.117 Barnes, William - JW3A.59 Acuna Herrera, Rodrigo - JTu3A.60, JW3A.17, Apalkov, Vadym - JTu3A.21 Barot, Dipenkumar - JTu2A.47 JW3A.9 Apfelbeck, Fabian - FTh2B.3 Barsi, James - FM4D.3 Adams, Charles S. - FW6B.4 Apinaniz, J - FM2B.4 Bartal, Guy - FM4A.2, FTu4D.2 Adams, Daniel E. - LM3F.4 Applegate, Brian E. - FTh2C.3 Bartels, Ludwig - JTu3A.25 Adibi, Ali - FM3D.1 Araújo, Maria Cecília S. - FM2A.2 Bartley, Tim - FM4E.6 Adie, Steven G. - FTh2C.2 Arce-Diego, Jose L. - JTu2A.66 Batarseh, Mahed - FTh3D.2, JTu2A.106, JTu3A.86 Afanasev, Andrei - JTu3A.79 Arce-Diego, José Luis - JTu2A.70 Bateni, Vahid - JTu2A.67 Agarwal, Girish S. - JTu3A.37 Archipovaite, Giedre M. - JTu3A.67 Batshon, Hussam - FW6A.1 Agarwal, Ritesh - JW3A.96 Arissian, Ladan - LM4F.5 Bauer, Aaron - FTh3D.1 Agha, Imad - JTu2A.39, JTu3A.29, JTu3A.93, Armani, Andrea - FTh3A.2 Bauman, Stephen - FM4A.3 JW3A.76 Armas-Rivera, Ivan - JW4A.115 Bauman, Stephen J. - FM4A.7 Agrawal, Amit - JW3A.119, JW3A.87 Arriola, Alexander - JW4A.84 Beck, Mark - FM2D.2, FM3E, JW4A.21 Agrawal, Govind P. - FTu5A.2, JTu3A.66, JW4A.74 Arrizón, Victor - JTu2A.40 Beckman, Hugh - JTu2A.72 Aguirre-Olivas, Dilia - JTu2A.40 Arroyo Carrasco, M.Luis - JTu3A.52 Beckus, Andre - FM4C.5, FM4C.6, FTh3D.2 Ahmed, Asif - FW5A.4 Arroyo-Rivera, Edgar S. - JW3A.40, JW3A.42 Bedi, Amna - JTu2A.59, JTu2A.65 Ahmmed, Kazi T. - FTh3A.7 Arteaga Sierra, Francisco Rodrigo - FTu5A.2 Beetar, John E. - JTu3A.70 Aiub, Eduardo J. - JW4A.101 Artemyev, Dmitry - FTu5C.4 Begleris, Ioannis - JW4A.89 Ajates, J G. - FM2B.4 Arthur, Edmund - JTu2A.69 Bekaert, Philippe - JTu2A.105 Akbari, Elnaz - JW3A.56 Asavanant, Warit - FM3E.3 Bekele, Robel Y. - JTu3A.10 Aksyuk, Vladimir - FM2A.1, JW3A.74 Assad, Syed M. - FTu5E.2 Bekker, Christiaan - FTh3B.1 Al Qasimi, A - JW4A.24 Assoul, Mohamed - JTu3A.34 Belhassen, Jonathan - FW5E.3 Alam, Shaif - FW6A.3 Astorino, Antonio - JTu3A.87 Bělín, Jakub - JTu2A.44, JTu2A.45 Alanzi, Saud - JW4A.59 Ataai, Rajab Y. - JW3A.121 Bell, Bryn - FW2B.1 Alattar, Nebras - JTu2A.89 Atchison, David A. - JTu2A.116 Bell, Thomas - FW2B.3 Al-Baiaty, Zahraa - JW3A.23 Atia, George - FM4C.5, FM4C.6, FTh3D.2 Bellinger, Stephanie - JTu2A.63 Albakay, Naji - JW4A.60 Avsievich, Tatyana - JTu2A.78 Bello Jiménez, Miguel Ángel - JW4A.87 Alfalou, Ayman - JTu2A.96 Aymerich López, María - FW6B.2 Beltran, Rigoberto C. - FTh3A.2 Alfano, Robert R. - FTu5C.3, JTu2A.5, JTu2A.72 Aytac, Yigit - JTu3A.31 Beltrán-Pérez, G. - JW4A.115 Alfasi, Nir - JW4A.17 Azana, Jose - FTh3E.2 Bender, Nicholas - FW5B.2 Al-Janabi, A.Hadi - FTu5A.4 Azzahrani, Ahmad S. - JW3A.26, JW3A.27 Benke, Kristin - LM4F.2 Alkauskas, Audrius - JW3A.122 Bennett, Kochise - LTu5F.2 Allen, Jeffery - JTu2A.60 B Bentz, Brian - FM4D.2 Allen, Monica S. - JTu2A.60 Baboux, Florent - FW5E.3 Beresna, Martynas - FW6A.3 Allen, Taylor G. - JTu3A.61 Bacha, Bakht A. - JW3A.15 Bessonov, Vladimir - JTu2A.16 Allison, Thomas K. - LM4F.6 Badolato, Antonio - FM2E.1 Bevis, Charles - LM3F.4 Almeida, Alexandre - JTu3A.42 Badr, Mohamed M. - JW4A.41, JW4A.43 Bhaktha B.N., Shivakiran - FTu4A.3, JW3A.30 Almeida, Euclides - FM4A.5 Baets, Roel - JW3A.82 Bhatia, Nitin - JW4A.102, JW4A.8 Almeida, Gustavo F. - JW4A.86 Bahari, Babak - FTu4A.2, LTh3F.5 Bhattacharya, Mishkatul - FTh3B.2 Almeida, Indira Marília A. - JW4A.101 Bahl, Anand - FW6E.2 Bhattacharya, Shanti - JTu2A.64 Alonso, Miguel A. - JTu3A.83, JTu3A.84 Bahl, Gaurav - FM3D.7, FTh3B.3 Bhyravbhatla, Namita - JTu2A.61 Alonso-Caneiro, David - FTh2C.1 Bai, Xiaokang - FM3D.2 Bianco, Vittorio - FW5D.1, JTu2A.2 Alonso-Ramos, Carlos - JW3A.72 Bajcsy, Michal - JW3A.14 Bienstman, Peter - JTu2A.92 Alpeggiani, Filippo - FM3B.5, JW3A.54 Baker, Christopher - FTh3B.1 Bigagli, Niccolo - JW3A.39 Al-Shammari, Rusul M. - JTu2A.89 Baker, Mark - FW2B.3 Bijalwan, Ashish - FTh3A.4 Altorio, Matteo - FW2E.3 Baker, Robert - FTh2B, LTu4F, LTu5F.4 Bingham, Nicholas S. - JW3A.6 Alvarez Ocampo, Carlos Andres - JTu3A.60, Bakir, Muhannad S. - JW4A.94 Birowosuto, Muhammad Danang - JTu3A.25 JW3A.17 Balaji, Muralidhar M. - JTu2A.7 Bisson, Jean-Francois - FM3A.5 Alvarez Tamayo, Ricardo Ivan - JW4A.72 Balbuena Ortega, Argelia - FTu4D.3, LTh3F.2 Biswas, Chinmoy - JTu3A.53 Alvaro, Pepito Bustos - LW2F.3 Balciunas, Tadas - JTu3A.16 Biswas, Priyanka - JTu3A.55 Amanti, Maria - FW5E.3 Baldwin, Carryl - FTh3C.1 Biswas, Somnath - LTu5F.4 Amaral, João Paulo - JW4A.114 Ballato, John - JW4A.81, JW4A.96, LTh4F.5 Blanco Redondo, Andrea - FW5E.2 Amin, Rubab - FM2A.3, JW3A.96 Baltuška, Andrius - FM2B.1 Blechman, Yael - FM4A.5 Amini, Jason M. - FM3E.5 Banaszek, Konrad - FTh3E.4 Blums, Valdis - FM3E.5 Amoah, Sylvester - JW4A.28 Bandres, Miguel - FM3B.7 Boaz Jessie, Jackin - JTu2A.105|JTu2A.105 Amuah, Charles L. - JTu2A.71

FiO + LS 2017 • 17–21 September 2017 85 Bolshtyansky, Maxim - FW6A.1 Capozza, Rosario - JTu2A.58 Chen, Zhigang - LW2F.3 Boltasseva, Alexandra - JTu2A.12 Carbajo, Sergio - LM4F.3 Cheng, Gangge - FTu5C.3 Bondy , Yaara - JW3A.95 Cardin, Vincent - JTu3A.16 Cheng, Tonglei - JW4A.106, JW4A.77 Bonneau, Damien - FM4E.2 Carlson, David - FTu4D.4 Cheng, Xiaojun - JW4A.109, JW4A.113, JW4A.83 Bordonalli, Aldario C. - JW4A.61 Carney, Daniel J. - JW3A.62 Cheon, Seunguk - FTu5B.2 Boriskina, Svetlana V. - FM4D.6, JW3A.91 Carruthers, Thomas - JTu3A.57 Chertov, Aleksandr - JTu2A.77 Bouchard, Frédéric - LM4F.5 Carter, Sam G. - JW4A.2 Chew, Avenell L. - FTh2C.1 Bouman, Charles - FM3C.6 Carvalho, Alyson J. - JW4A.18 Chi, San-Hui - JTu3A.61 Bourgenot, Cyril - JTu2A.42 Carvalho, Marcos A. - JW4A.14 Chiang, Chia-Wei - LTh3F.3 Bowen, Warwick P. - FTh3B.1 Casillas-Rodríguez, Nayeli - JW4A.11 Chiang, Kin Seng - FW6A.2 Key to Authors Boyd, Robert - LM4F.5 Caspani, Lucia - FTh3E.2 Chini, Michael - JTu3A.70 Boydston-White, Susie - JTu2A.72 Cassan, Eric - JW3A.72 Cho, Young-Wook - JW3A.38 Bozhevolnyi, Sergey I. - JTu2A.12, LW2F.1 Cassidy, Derek - JW4A.75 Choe, Regine - FM4C.1 Bracamontes-Rodriguez, Yazmin E. - JTu3A.103 Castrillon, Jhonny - JTu2A.5 Choi, Chul Soo - JTu2A.25 Bracamontes-Rodríguez, Yazmin E. - JW4A.115 Cavalcanti, Solange B. - JTu3A.39 Chong, Andy - JW4A.93 Bracker, Allan S. - JW4A.2 Cavillon, Maxime - JW4A.81 Chong, Teck K. - JW3A.90 Brambilla, Gilberto - FW6A.3 Ceballos, Daniel - JW4A.56 Chong, Yidong - FTu4D.5 Brandão, Paulo A. - FTh3B.4, JTu3A.39 Ceballos-Herrera, D E. - JW3A.42 Choudhury, Sajid - JTu2A.12 Brandstotter, Andre - FM4B.4 Cerjan, Alexander - JTu3A.104, JW3A.98 Chowdhury, Bilas - JW4A.110, JW4A.59, JW4A.62, Brasselet, Sophie - FW5B.1 Cernansky, Robert - JW3A.13 JW4A.73 Bratchenko, Ivan - FTu5C.4, JTu2A.4, JTu2A.73, Chaitanya, Amrit - JTu3A.96 Chriki, Ronen - FM3B.3, FTh2E.2, FTu4C.4, JTu2A.74, JTu2A.81 Chakraborty, Biswanath - JTu3A.33 JW3A.103 Brawley, Zach - FM4A.3 Chakravarty, Abhijit - JW4A.64, JW4A.65 Christensen, Erik N. - JW4A.6 Brecht, Benjamin - FM3E.2, JW3A.34, JW4A.16, Chakravarty, Uday - JW3A.83 Christensen, Marc - FM3C.4, JTu2A.7 JW4A.3 Chan, Hau Ping - FTh3A.7 Christodoulides, Demetrios\ - JW3A.106, JW4A.99 Brennan, Noel A. - JTu2A.116 Chan, Kam Wai Clifford - JW4A.22 Chu, Cheng Hung - JW3A.109 Bridges, Denzel - JW3A.1 Chandra, Amreesh - FTu4A.3 Chu, Cheng Hung - JW3A.110 Brito Cruz, Carlos Henrique - FTu5B.5 Chandra, Nitish - JW3A.88 Chu, Ken - FW6D.1 Brodsky, Michael - JW4A.37, JW4A.39 Chandra, Subhash - JTu2A.61 Chu, Sai - FTh3E.2 Bromberg, Yaron - FW5B.2 Chandrachoodan, Nitin - JTu2A.64 Chu, Ying-Ju - JTu3A.95 Brosseau, Christian - JTu2A.96 Chang, Zenghu - LTu4F.1 Chung, Hung-Pin - JW3A.3 Brown, Graham - LM4F.5 Chang-Hasnain, Connie J. - FTu4E.1 Chung, Te-yuan - JW4A.100 Bruch, Alexander - FTu4B.5 Charipar, Kristin - JW3A.6 Chvykov, Vladimir V. - LW5F.2 Brundavanam, Maruthi M. - JTu3A.53, JTu3A.82, Charipar, Nicholas - JW3A.6 Cino, Alfonso - FTh3E.2 JTu3A.91, JTu3A.92 Chatterjee, Monish R. - FM3D.4, JW3A.121, Cirri, Anthony - LTu5F.4 Brunner, Daniel - FTh2E.3 JW4A.1 Clark, Amanda - JTu3A.110 Buch, Shaival - JW4A.74 Chaturvedi, Deepa - JW3A.47, JW3A.49, JW3A.83 Clerici, Matteo - FTu4B.2 Bucksbaum, Philip H. - LW5F.3 Chatzakis, Ioannis - JTu3A.47 Cohen, Samuel R. - JTu2A.19 Buczek, Sean - JTu3A.70 Chauhan, Chanderkanta - JTu2A.27 Cola, Adriano - FTh2D.2 Bueno, Patricia - JTu3A.28 Chauhan, Pooja - JW4A.120 Colburn, Shane A. - FM4A.4 Bugoffa, Salah G. - FM3D.4 Chávez-Cerda, Sabino - FM4B.6 Coley, William C. - JTu3A.25 Buks, Eyal - JW4A.17 Checoury, Xavier - FW5A.5 Combrie, Sylvain - FW5A.5 Bullough, John D. - FTh3C.4 Chekhov, Alexander - JW3A.101 Condon, Nicholas - LW6F.4 Burda, Milan - JTu3A.113 Chen, Chun-Wei - FW6B.3, JTu2A.9 Conforti, Matteo - JW4A.103 Burenkov, Ivan - FM4E.6 Chen, Deying - JTu2A.15 Connell, Steven - FM3E.5 Burke, Robert - JW4A.40 Chen, Fred K. - FTh2C.1 Connor, Nadine P. - JTu2A.83 Burns, Stephen A. - JTu2A.6, JTu2A.69 Chen, Gang - FM4D.6, JW3A.91 Cook, Kevin T. - FTu4E.1 Burrow, Joshua - JW3A.76 Chen, George F.R. - JTu3A.35 Cooper, Emily - FTh3C.3 Busch, David R. - FM4D, FM4D.3, FTu5C Chen, Harrison - FW5D.2 Copie, Francois - JW4A.103 Bushati, Rezlind - JW3A.93 Chen, Hong Ling - JTu2A.85 Corbett, Pat - FW6A.1 Bushunov, Andrey - JTu2A.20 Chen, Hui C. - JTu2A.93 Corder, Christopher - LM4F.6 Butko, L.N. - JW3A.117 Chen, Jia-Wern - JW3A.110 Corkum, Paul - FTh2B.2, LM4F.5 Chen, jiayang - FM2D.3, JW4A.12 Cormier, Eric - JTu3A.67 C Chen, Jie - JTu3A.17, JTu3A.74 Corwin, Kristan - LM3F C.K., Nijil Lal - JW4A.13 Chen, Kaixin - FW6A.2 Courtial, Johannes K. - FM3C, JTu2A.42, JTu2A.44, Caballero, Olga - JW3A.91 Chen, Luo-Kan - FTh2E.1 JTu2A.45 Cadusch, Jasper J. - JW3A.75 Chen, Mu Ku - JW3A.110 Cowie, Euan - JTu2A.42, JTu2A.45 Cai, He - JTu3A.112 Chen, Ren-Jie - JW3A.68 Cox, Mitchell A. - JW4A.7 Cai, Jin-Xing - FW6A.1 Chen, Shaowu - JW4A.50 Craig, Benjamin - JW3A.77 Caldwell, Joshua - JTu3A.47 Chen, Szu-Yu - JTu2A.85 Cranch, Geoffrey - FW6A.5 Camayd-Munoz, Philip - JW3A.108 Chen, Ting-Yu - JW3A.109 Crane, Tom - JW3A.50, JW3A.52 Campione, Salvatore - JW3A.46 Chen, Wei-Lin - LTh3F.6 Crescimanno, Michael - JTu3A.51 Canales, Francisca A. - JTu2A.100 Chen, Wei-Ting - JW3A.102, JW3A.80, JW3A.92 Crozier, Kenneth B. - FM3B.2, JW3A.77 Canfield, Brian K. - JTu3A.26 Chen, Xianfeng - JW3A.61 Čtyroký, Jiri - JW3A.79 Canteli, David - FW6B.2 Chen, Yang-Fang - LTh2F.2, LTh3F.3 Cumming, Benjamin P. - FW6C.5, JW3A.23 Cao, Huabao - LW5F.2 Chen, Yen-Hung - JW3A.3 Cunha, Joao P.S. - JTu2A.68 Cao, Hui - FW5B.2 Chen, Yu - JTu2A.75 Currie, Marc - FTh2D.2, JW4A.45 Cao, Jingming - JW3A.16 Chen, Yu Han - JW3A.109 Curt, Charles - JW4A.73 Cao, Liangcai - JTu2A.103 Chen, Yu-Ao - FTh2E.1 Curticapean, Dan - JTu2A.115, JTu2A.97 CAO, QIONG - JTu2A.104, JTu2A.110 Chen, zhao - JW3A.111, JW3A.22 Cutrone, Alisa - FM4D.3 Cao, Yuan - FTh2E.1 Chen, Zhaodong - JTu2A.15 Capasso, Federico - JW3A.102, JW3A.80, JW3A.92 Chen, Zhaowei - JTu2A.86

86 FiO + LS 2017 • 17–21 September 2017 D Dipold, Jessica -. - JW4A.91 Evans, Christopher - FW5A.4 Dadap, Jerry I. - FW5A.4, JW3A.84 Ditkowski, Adi - FM4B.5 Evans, Phil - FM3D.3, JW3A.1

Dadoenkova, Yuliya S. - JW3A.45, JW3A.53 Divitt, Shawn - JW3A.87 Ewart, Paul - FTu4E.3 Key to Authors D’Aguanno, Giuseppe - JTu3A.14 Djiokap, Jean Marcel N. - JTu3A.36 Eyceyurt, Engine - JTu2A.3, JW4A.107, JW4A.59 Dahlem, Marcus S. - FW6C.4, JTu2A.18 Dogariu, Aristide - FM3C.7, FTh3D.2, JTu2A.106, Dai, Hailang - JW3A.61 JTu3A.86 F Daisuke, Demichi - JTu2A.33 Dogra, Sonam - JW3A.66 Fabris, Davide - FW6E.1 Dalal, Reena - JW3A.44, JW3A.66, JW3A.67 Doherty, Marcus - JW3A.122 Fainman, Yeshaiahu - FTu4A.2, LTh3F.5 Dambre, Joni - JTu2A.92 Donaldson, Tiffany - JTu2A.108 Fales, Andrew M. - JTu3A.2 Daniel, Salman - FW5B.4 Dong, Chen Y. - JTu2A.88 Falt, Stefan - FM2E.1 Danilov, Viktor - JW3A.107 Dong, Daoyi - FTh3E.6 Fan, Heng - FM2D.3 Darweesh, Ahmad A. - FM4A.3 Dong, Hongxing - JTu2A.17 Fan, Jingyun - FTh2E.1 Das, Mukul K. - JW3A.25 Dong, Jun - LW2F.2 Fan, Rongwei - JTu2A.15 Das, Ritwick - JTu3A.115, JW3A.99, LTh2F.3 Donko, Andrei - FW6A.3 Fan, Shanhui - FW2A.2, FW5B.3, JW3A.98 Das, Subir - FW5D.6 Donley, Elizabeth A. - JW4A.25 Fan, Shengli - FW5D.4 Dash, Jitendra N. - JW4A.104 Donodin, Alexander - JTu3A.15 Fang, Bess - FW2E.3 Dass, Sumit - JW4A.67 Dorfman, Konstantin - LTu5F.2 Fang, Renpeng - JW4A.19 Davanço, Marcelo - JW3A.74 D’Ornellas, Peru - JW4A.5 Fang, XinYuan - JTu3A.54 David, Sabrina - JW3A.115 Dou, Renqin - JTu3A.109 Fanjul-Velez, Felix - FTh2C, FW6D, JTu2A.66, Davidson, Carl - FW6A.1 Douglas Stone, A. - JTu3A.104 JTu2A.70 Davidson, Nir - FM3B.3, FTh2E.2, FTu4C.4, FW5E, Dourdent, Hippolyte - JTu3A.83 Farchi, Elad - JW4A.17 JW3A.103, LW6F.3 Dowling, Jonathan - JW3A.85 Farmer, Jonathan - JTu2A.90 Davidson, Roderick B. - JTu3A.47, JW3A.1 Dowran, Mohammadjavad - JW3A.10 Farufnik, Demitry - JW4A.17 Davis, Alex O. - FM4E.5, JW4A.5 Dragic, Peter D. - JW4A.81 Farzam, Farzin - FTh3D.3 Davis, Lloyd M. - JTu3A.26 Dragnea, Bogdan - JTu3A.27 Fatima, Areeba - JTu2A.109 Davis, Matthew J. - FW2B.3 Drew, H.Dennis - JW4A.79 Fedchak, James - JW3A.69 de Aguiar, Hilton B. - FW5B.1 Drummond, Miguel V. - FW6A.4 Feder, Linus - FM2B.1, FM2B.2, JTu3A.12 De Angelis, Francesco - JTu2A.58 Du Plessis, Anton - FM2B.3 Fedosejevs, Robert - FM2B.4 De Angelis, Lorenzo - FM3B.5 Du, Shengwang - JW4A.26 Fedyanin, Andrey - JTu2A.16 de Assis, Pierre L. - JW4A.14 Duan, Lingze - JTu2A.47 Feizpour, Amir - FM3E.2 De Boni, Leonardo - FTh3A.3, JW4A.91 Duan, Xue K. - FW2A.1, JW3A.11, JW3A.22, Fejer, Martin - JW3A.4 de Bruyn, Andre - FM2B.3 JW3A.24 Feldman, Matthew A. - JW3A.1 de Castro, Alberto - JTu2A.6 Duarte, Vanessa C. - FW6A.4 Feldman, Meghan - JW4A.21 de Ceglia, Domenico - JTu3A.29, JTu3A.93 Dubreuil, Nicolas - JW3A.72 Felinto, Daniel - JW4A.18 de Clavijo, Alejandra Ruiz - JW3A.91 Ducci, Sara - FW5E.3 Feng, Liang - FW6B.5, JTu2A.86 de Leon, Nathalie - FW2A.3 Dudley, Jordan - FW2E.2 Fernandez, Henry - JW3A.59 de Melo, Natalia R. - FW6B.4, JTu3A.42, JTu3A.98 Dumitrescu, Eugene - JW3A.1 Ferraro, Pietro - FW2C.3, FW5D.1, JTu2A.2 De Natale, Paolo - FTh2B.4 Dunkelberger, Adam D. - JTu3A.47 Ferraz, José - JW4A.14, JW4A.18 De Oliveira, Rafael E. - FM2A.2 Duran-Sanchez, Manuel - JW4A.72, JW4A.87 Ferreira, Marco - JTu3A.118 de Pádua, Sebastião - JW4A.14 Durán-Sánchez, Manuel - JW4A.115, JW4A.78 Ferrier, Nicola - FM3C.6 De Rosa, Maurizio - FTh2B.4 Dushaq, Ghada - JW4A.42 Fiala, Jan - JTu3A.113 De Rossi, Alfredo - FW5A.5 Fibich, Gadi - FM4B.5 de Sterke, C.Martijn - FW5E.2, JW3A.90 E Fienup, James - JTu2A.91 Deal, Cathie - JW4A.65 Earles, Susan - JW3A.26, JW3A.27 Filevska, L.M. - JTu2A.99 Debnath, Sanjay - JW3A.105 Eberly, Joseph - JW4A.24 Finch, Michael - JW4A.73 Debu, Desalegn T. - FM4A.7 Eckel, Stephen - JW3A.69 Finney, Greg - JTu2A.90 Defienne, Hugo - JW4A.31 Eden, J.G. - JTu3A.105, JW4A.81, LTh4F.3, LW6F.2 Fisch, Nathaniel J. - FW5B.5, LM2F.3 Dehghani, Mojgan - JW3A.73 Edgar, Matthew P. - FTu5E.3 Fischer, Ingo - FTh2E.3 Dehghannasiri, Razi - FM3D.1 Edrei, Eitan - FM4B.2 Fisher, Paul - FM3E.5 Delagnes, Jean-Christophe - JTu3A.67 Edwards, Matthew - JTu3A.102, LM2F.3 Fitzpatrick, Casey - FTh3E.1 Delrot, Paul - JTu3A.9 Eftekhar, Ali - FM3D.1 Fleischer, Jason W. - JW4A.31 Deng, Lu - FW2E.1, JTu3A.50 Eggleton, Benjamin J. - FTu4A.5, FW2B.1 Fleisher, Adam J. - JTu3A.19, JTu3A.20 DeSilva, Robert - JTu2A.90 Egorenkov, Vladimir A. - JTu3A.58 Flores-Arias, María Teresa - FW6B.2 Desouky, Mai - FTh3B.6 EI-Ghazawi, Tarek - JTu2A.24, JW4A.55 Floyd, Thomas F. - FM4D.3 Destro, Marcelo G. - JTu3A.28 Eigner, Christof - JW4A.3 Fokine, Michael - JW4A.117 Devaux, Bertrand - FW5D.3 Eilanlou, A.Amani - LW5F.4 Foley, Justin M. - FTh3B.5 Dhasarathan, Vigneswaran - JW4A.58 Eilers, Hergen - JTu2A.36 Fonari, Marina S. - JTu3A.61 Di Falco, Andrea - FM3B.5 Eisert, Jessie - FTh3C.1 Fonseca Romero, Karen M. - JW4A.20 Di Sciacca, Giuseppe - JTu3A.18 Elamurugu, Elangovan - FTu5B.4 Fontaine, Michaël - JTu3A.34 Dianat, Pouya - FTh2D.2, JW3A.18, JW4A.45 El-Ganainy, Ramy - JW3A.63, JW3A.64 Fontecchio, Adam - JTu3A.44 Diaz, Gabriel - FTh3C Elhalawany, Ahmed - FM4C.6, FTh2D.3 Foote, David B. - JTu3A.36 DiComo, Gregory - JTu3A.59 El-Halawany, Ahmed - FM4C.5 Forbes, Andrew - JW4A.7 Diddams, Scott - FTu4D.4 Elle, Jennifer - JTu3A.59 Foster, Amy C. - FW5A.1 Diebold, Andreas - FTh2B.1 Elsner, Ann E. - JTu2A.69 Fotiadi, Andrei - JTu3A.6 Diep, Vinh - FTh3A.2 Emaury, Florian - FTh2B.1 Fourkas, John T. - JTu2A.19 Digaum, Jennefir L. - FM3D.5 Enaya, Rayan - JTu2A.3 Foursa, Dmitri - FW6A.1 Digonnet, Michel - FTh3A.1 Erkintalo, Miro - FTh2B.4 Francesconi, Saverio - FW5E.3 DiMauro, Louis - LTu4F.2 Ernotte, Guilmot - FTu4B.2 Frantz, Jesse - JTu3A.10 ding, haibo - FTu5B.3 Ershov, Petr - JTu2A.16 Freiberger, Matthias - JTu2A.92 Ding, Shoujun - JTu3A.3 Espinoza, Alonzo - FM4C.2 Friberg, Ari - FW5B.4 Dipalo, Michele - JTu2A.58 Esporlas, Cindy - FW6B.1 Friesem, Asher - FM3B.3, FTh2E.2, FTu4C.4, Estudillo Ayala, Julian Moises - JW4A.70 JW3A.103

FiO + LS 2017 • 17–21 September 2017 87 Friis, Søren M. - JW4A.6 Goldschmidt, Elizabeth A. - FM3E.4, FM4E.6 Han, Sang-Wook - JW3A.38 Frolov, Mikhail P. - JTu2A.20 Gollner, Claudia - FM2B.1 Han, Xu - JW3A.78 Fu, H.Y. - JW4A.71 Gong, Peijun - FTh2C.1 Han, Zheng - FW5A.5 Fujieda, Ichiro - JTu2A.1, JTu2A.11|JTu2A.11 Gong, Qihuang - FW2A.1, JW3A.11, JW3A.111, Hansen, Karolyn - JW4A.93 Fujii, Shun - JTu3A.68, JW3A.19, JW3A.71 JW3A.22, JW3A.24 Hansson, Tobias - FTh2B.4 Fuller, Kirk - JTu2A.90 Gong, Zheng - FTu4B.5 Hao, He - FW2A.1, JW3A.11, JW3A.24 Furusawa, Akira - FM3E.3 Gopar, Victor - JTu2A.112, JW4A.83 Harder, Georg - FM4E.6 Furusawa, Kentaro - JW4A.92 Gorbunova, Elena - JTu2A.77 Hariri, Nasir - JTu2A.3 Gosztola, David - FW5A.5 Harrivel, Angela - FM4D.4 G Graumann, Ivan - FTh2B.1 Hasman, Erez - JW3A.103 Key to Authors G, ATHIRA - JTu2A.64 Gregory, Groot - FW5C Hassan, Ali - JTu2A.50 Gabalski, Ian - JTu3A.110 Gretzinger, Thomas - JW4A.84 Hatamimoslehabadi, Maryam - JTu2A.63 Gabrielli, Lucas - FM4C.3, JW4A.49 Grim, Joel Q. - JW4A.2 Haus, Joseph W. - JTu3A.29, JTu3A.93, JW4A.93 Gaffney, Kelly - LM2F.1 Grinevych, Viktor S. - JTu2A.99 Hawkins, Thomas - JW4A.81, JW4A.96, LTh4F.5 Gagnon, Etienne - JW3A.35 Gross, Simon - JW4A.84 Hayakawa, Tomohiko - JTu2A.52 Gaind, Vaibhav - FM4D.2 Grote, Richard - FW5A.4 Hayasaki, Yoshio - FTu5D, FW2C.2 Galfsky, Tal - LM3F.1 Grover, Ginni - FM3C.1 Hayes, John - FW6A.3 Gallo, Katia - JTu2A.89 Gu, Jie - JTu3A.33, JW3A.93, LM3F.1 He, Hongsen - LW2F.2 Galloway, Benjamin R. - LM3F.4 Gu, Lingjia - JTu2A.104, JTu2A.110 He, Kebo - FTu4A.4, JW3A.58, JW3A.78 Galvez, Enrique J. - FM3B.4, JTu2A.5 Gu, Min - FTu5B.3, FTu5D.2, FW6C.5, JW3A.23 Healy, Noel - JW4A.117 Galvin, Thomas - LW6F.2 Gu, Qing - LTh3F.5 Heaven, Michael - JTu3A.110 Gammon, Dan - JW4A.2 Gu, Tingyi - JW4A.40 Hegde, Gopalakrishna - JW4A.53 Gan, Xiaosong - JW3A.23 Gu, Ying - FW2A.1, JW3A.11, JW3A.111, JW3A.22, Hegedus, Steve - JW4A.40 Ganguly, Pranabendu - JW3A.70, JW4A.48 JW3A.24 Heinrich, Stephan - FTh2B.3 Gao, Jing - JTu3A.109 Gu, Zhongze - FTu5B.3 Helle, Michael H. - JTu3A.59 Gao, Peng - JTu2A.76 Guddala, Sriram - JW3A.93 Hellman, Brandon - FM4C.2 Gao, Wei - JTu2A.81 Gudyriev, Sergiy - FM3A.3 Helmy, Amr S. - FM2E, FM4E.1 Gao, Zhengning - JTu3A.29, JTu3A.93 Guerreiro, A. - JTu2A.68 Hemmati, Hafez - JW3A.104 Gaponenko, Maxim S. - FTh2B.1 Guesmi, Latifa - JW4A.63 Henrique, Franciele - JW4A.86 Garcia Melgarejo, Julio Cesar - JW3A.40, JW3A.42 Guest, Jeff - FW5A.5 Hensley, Joel M. - FW5A.4 Garcia Mina, Diego - JW4A.93 Guggenmos, Alexander - FTh2B.3 Her, Tsing-Hua - JTu2A.14 García Ramírez, Emma V. - JTu3A.97 Guild, Eric - JTu3A.110 Hermann-Avigliano, Carla - FM2D.4 Garcia, E - FM2B.4 Gulduren, Emin - JTu2A.22 Hernandez, Erika N. - JW4A.87 Garcia-Melgarejo, Julio C. - JW4A.95 Gulsoy, Emine - FM3C.6 Hernandez, I - FM2B.4 Gardner, Dennis F. - LM3F.4 Gunawidjaja, Ray - JTu2A.36 Hernandez-Aranda, Raul I. - JTu3A.85 Garea, María T. - JTu2A.23 Guo, Changliang - FW6D.3, JTu2A.94, JTu3A.90 Hernández-Arriaga, Marco V. - JW4A.115, JW4A.78 Garra, Brian S. - FM4D.1 Guo, Chunlei - JTu3A.41 Hernandez-Garcia, Juan C. - JW4A.70 Garrido Alzar, Carlos - FW2E.3 Guo, Hong - JTu2A.8, JTu3A.94, JW4A.33, Hernández-Hernández, Eliseo - JW4A.11 Gather, Malte C. - FM4B.2 JW4A.36 Hernández-Robles, Emmanuel A. - JW4A.70 Gatti, Giancarlo - FM2B.4 Guo, Xiang - FTu4B.5 Hernandez-Romo, Martin - JTu2A.100 Gauthier, Guillaume - FW2B.3 Guo, Xianxin - JW4A.26 Herrmann, Harald - JW4A.3 Gauvin, Serge - JW3A.43 Guo, Xuexue - FW6B.3 Herrmann, Jason - JW3A.14 Gaylord, Thomas K. - FM3C.3, FTh3D.6, JW4A.94 Guo, Zhen - JTu2A.102 Hersam, Mark - FW5A.5 Ge, Li - JTu3A.89, JW3A.55, JW3A.65 Gupta, Banshi D. - JW4A.69 Herzog, Joseph - FM4A.3 Geib, Kent - JW3A.46 Gupta, Prasoon - FM2D.4 Herzog, Joseph B. - FM4A.7 Geiger, Remi - FW2E.3 Gutiérrez Ojeda, Carina - JTu3A.101 Heyvaert, Jelle - JTu2A.92 Gemar, Heath E. - FTh3D.2, JTu2A.106, JTu3A.86 Gutierrez Razo, Sandra A. - JTu2A.19 Hickstein, Daniel D. - FTu4D.4 Genack, Azriel - JTu2A.112, JW4A.109, JW4A.113, Gutierrez-Castrejon, Ramon - JW4A.56 Hileman, Devin - LW6F.4 JW4A.83 Gutiérrez-Cuevas, Rodrigo - JTu3A.84 Hill, Wendell T. - FM2B.4, JTu3A.36 Gentile, Antonio - FM4E.2, FTh3E.7 Gutiérrez-Vega, Julio C. - JTu3A.85 Hine, George - FM2B.2, FM3B.6, JTu3A.12 Gerrits, Thomas - FM4E.6, FTu4E, FTu5E.4 Ho Thanh, Minh-Tri - JW4A.88 Gessner, Oliver - LM4F.4 H Ho, Bo-Wei - FW5D.6 Getmanenko, Yulia - JTu3A.61 Hache, Alain - FM3A.5 Ho, Tsung-Jui - JTu2A.9 Ghadimi, Mojtaba - FM3E.5 Hachtel, Jordan - JW3A.1 Hochrainer, Armin - FTh3E.5 Ghassemi, pejhman - JTu2A.75 Hafezi, Mohammad - FM3E.4 Hodges, Joseph - JTu3A.20 Gholam-Mirzaei, Shima - JTu3A.70 Hagan, David J. - JW3A.9 Hokr, Brett H. - JTu2A.90, JTu3A.110 Ghosh, Somnath - JTu3A.81 Haghtalab, Mohammad - JW3A.120 Hong, Kang-Hee - JW3A.38, JW4A.15 Ghosh, Subhabrata - FTu4A.3 Hagley, Edward W. - FW2E.1, JTu3A.50 Hong, Kyung-Han - LM4F, LTu4F.2 Ghosh, Sumit - JTu2A.114 Haglund, Richard - FM3D.3, JW3A.1 Hong, Minghui - FM3D.6, JW3A.116 Gibson, Graham M. - FTu5E.3 Haldar, Raktim - FW6C.3, JTu3A.13, JTu3A.22, hong, Seongjin - FTu5B.2 Gibson, Ursula J. - JW4A.117 JTu3A.24, JW4A.8 Horak, Peter - JW4A.89 Gigan, Sylvain - FW5B.1 halder, Suman - JW4A.67 Hori, Atsuhiro - JW3A.19, JW3A.71 Gilmore, Kevin - JW4A.25 Hales, Joel M. - JTu3A.61 Horowicz, Yahel - JW4A.17 Gin, Adley - FM4C.2 Hammon, Tim - FW6A.1 Horrom, Travis - FM2D.4, JW3A.36 Ginzburg, Vlad - JTu3A.77 Hammond, Giles D. - FTu5E.3 Hosseini, Ehsan - FW5A.3 Gioux, Sylvain - FTu5C.1 Hammond, Thomas - LM4F.5 Howell, John - FM3C.5 Giridharan, Srinivasan - JW4A.64, JW4A.65 Han, Guoxia - JTu3A.4 Hraghi, Abir - JTu2A.28 Girkin, John - JTu2A.42 Han, Jiande - JTu3A.110 Hsieh, Yu-Hua - JW4A.100 Glasser, Ryan T. - JW3A.31 Han, Juhong - JTu3A.112 Hsu, Wan-Ting - JW4A.100 Godaliyadda, Dilshan - FM3C.6 Han, Kewen - FM3D.7 Hu, Anming - JW3A.1 Goers, Andy - FM2B.2, JTu3A.12 Han, kyunghun - FTh3E.3 Hu, Guoqing - JTu3A.74 Goi, Elena - FW6C.5 Han, Pingli - JTu2A.101 Hu, Jonathan - JW4A.9

88 FiO + LS 2017 • 17–21 September 2017 Hu, Juejun - JW3A.72 Jha, Aashu - JW3A.39 Kato, Hirokazu - FTu4C.1 Hua, Hong - FTu4C, FW5C.2 Jha, Pankaj - FTh1A.4 Kato, Ryo - JW4A.66

Huancachoque, Leonid A. - JW4A.61 Jha, Rajan - FTh3A.6, JW4A.104, JW4A.67 Kato, Takumi - JW3A.19, JW3A.71 Key to Authors Huang, Shu-Wei - FM3D, FTu5A.3 Jhajj, Nihal - FM3B.6, JTu3A.65 Katumba, Andrew - JTu2A.92 Huang, Tianyao - JW3A.37 Ji, Chenchen - JTu2A.102 Kauffmann, Yaron - JW4A.17 huang, wei - JTu3A.32 Ji, Rong - JW3A.116 Kazakov, Vasily - JTu2A.48 Huang, Wen-Cheng - LTh3F.6 Jia, Baohua - FM3D.6, JW3A.60, JW3A.90 Kazemi Jahromi, Ali - FTh2D.3, FTu5A.5, JTu3A.104 Huang, Xiaodong - JW3A.60 Jia, Congxian - FM4D.1 Kazemi, Alex A. - JW4A.82 Huang, Yao-Wei - JW3A.92 Jia, Qing - FW5B.5 Keathley, Phillip D. - LM4F.3 Huang, Yi - FM4D.6 Jia, Shu - FW6D.3, JTu2A.94, JTu3A.90 Keeler, Gordon - JW3A.46 Huang, Yiming - JW4A.109, JW4A.83 Jia, Tao - JTu2A.15 Keeney, John - JW4A.111 Huang, Yin - JW3A.85 Jian, Zhenqian - JTu3A.36 Keller, Ursula - FTh2B.1, LTh2F, LTh4F.4, LTu4F.3, Huang, Yuping - FM2D.3, JW4A.12 Jian, Ziyun - JTu3A.76 LW6F Huang, Yu-Ping - JW4A.27 Jiang, Liang - FTu4B.5 Kelly, Matt - JW4A.64 Huang, Zhangxiang - JTu3A.4 Jiang, Lingjun - JW4A.47 Kelly, Trevor - LW2F.3 Huang, Zhaoran R. - JW4A.47 Jiang, Yijian - JTu2A.50 Kersh, Mariana E. - FW5D.5 Huang, Zhe - FTh3A.7 Jimenez Mejia, Raul E. - JTu3A.60 Kershis, Matthew D. - LM4F.6 Huang, Zhong - FM3D.2, JW3A.100 Jin, Guofan - JTu2A.103 Keys, Christopher - JTu2A.49 Huault, M - FM2B.4 Jin, Jing - JTu2A.81 Keys, Elizabeth - JTu2A.49 Hughes, Michael - JTu2A.79 Jin, Wei - FW6A.2 Khajavi, Behzad - FM3B.4, JTu2A.5 Huh, Joonsuk - JW4A.15 Jin, Yuhua - JTu2A.50 Khajavikhan, Mercedeh - LW6F.1 Huntington, Elanor H. - FTh3E.6 Jo, Javier - FTu5C.2 Khalil, Munira - LTu5F.1 HURTADO PEREZ, ROMAN - JTu2A.100 Joannopoulos, John D. - FTh3B.8 Khamees, Hussein T. - JTu3A.11 Husek, Jakub - LTu5F.4 Johnson, Eric G. - JTu2A.37 Khan, Emroz - JW3A.81 Husko, Chad A. - FW5A.5 Johnston, Kyle - FTh2B.2 Khan, Sikandar - FM2A.3, FM2A.4 Hussain, Mallik Mohd Raihan - JTu3A.29, JTu3A.93 Jones, Adam - FTh3D.5 Khanikaev, Alexander - JW3A.93, JW4A.113 Huzortey, Andrew - FM3C.2 Jones, Daniel E. - JW4A.37 Khanolkar, Ankita - JW4A.93 Hwang, Jihyun - JTu3A.1 Jones, Kevin - FM2D.4, JW3A.36 Khazanov, Efim - JTu3A.77 Hwang, Taek Yong - JTu3A.41 Jorge, Pedro A.S. - JTu2A.68 Khoo, Iam Choon - FW2A.1, FW6B.3, JTu2A.9 Jorissen, Lode - JTu2A.105|JTu2A.105 Khorasaninejad, Mohammadreza - JW3A.102, I Joshi, Chandrashekhar - FW6E.3, JTu3A.71 JW3A.80, JW3A.92 Ibarra, Hugo - JTu3A.103 Jung, Hojoong - FTu4B.5 Khramov, Alexander - JTu2A.74 Ibarra-Escamilla, Baldemar - JTu3A.103, JW4A.115, Jung, Jisung - JW3A.38 Khristoforova, Julia - FTu5C.4, JTu2A.74 JW4A.72, JW4A.78, JW4A.87 Jung, Yongmin - FW6A.3 Khristoforova, Yulia - JTu2A.81 Ibrahim, Ali - FW5D.3 Junqueira, Mateus - FM4C.3, JW4A.49 Khromov, Maxim - JTu2A.107, JTu2A.34 Ibrahim, Heide - FTu4B.2 Juul, Gabe - JW4A.21 Khrustalev, Victor N. - JTu3A.61 Ichihashi, Yasuyuki - JTu2A.105|JTu2A.105 Khurgin, Jacob B. - JW3A.96 Idrees, Muhammad - JW3A.15 K Kielpinski, Dave - FM3E.5 Ihlefeld, Jon - JW3A.46 Kaczmarek, Krzysztof T. - FM3E.2, JW4A.16, Kim, Donghyun - JTu2A.57 Ihn, Yong Sup - JW3A.21 JW4A.3 Kim, Hanyoup - JTu2A.84 Ilev, Ilko - JTu3A.2 Kadhim, Ahmed C. - JW3A.26, JW3A.27 Kim, Heungsoo - JW3A.6 Im, Dong-Gil - JW4A.35 Kadochkin, Aleksei S. - JW3A.45 Kim, Hyeongue - JTu3A.61 Imahoko, Tomohiro - LW5F.4 Kaertner, Franz - LM4F.3 Kim, Hyochul - LM3F.3 Imanaliev, almazbek - FW2E.3 Kaganov, Oleg - FTu5C.4 Kim, Hyun-Tae - FTh3A.5 Imany, Poolad - FTh3E.3 Kaji, Toshiyuki - FM3E.3 Kim, Jin-Hun - JW3A.21 Imperato, Cassandra - JW4A.83 Kalashnikov, Mihkail - LW5F.2 Kim, Joohwan - FTh3C.2, FTh3D Inagaki, Takahiro - FM4E.3 Kalinovich, Alexei A. - JTu3A.40 Kim, Ki-Yong - FM2B.2, JTu3A.78 Isaac, Justin - JW3A.94 Kalinski, Matt - JTu3A.116 Kim, Kyujung - JW3A.114 Ishikawa, Masatoshi - JTu2A.52 Kalra, Rachpon - FTh3B.1 Kim, Mijin - JW4A.2 Israel, Kai - JTu2A.113 Kalra, Yogita - FM3D.8, JW3A.67, JW4A.120 Kim, Sangmin - FTh2C.3 Israelsen, Stine M. - JTu3A.87 Kamal, Preet - FM4D.6 Kim, Seunghwi - FTh3B.3 Ito, Shusei - JTu2A.98 Kaminski, Clemens F. - FW6D.4 Kim, Sun-je - JTu2A.25 Iturbe Castillo, M.David - JTu3A.52 Kamioka, Naotaka - JW4A.54 Kim, Wihan - FTh2C.3 Iyer, Rishyashring R. - FTh2C.2 Kanda, Natsuki - LW5F.4 Kim, Yong-Su - JW3A.38 Kaner, Roy - JW3A.95 Kim, Yoon-Ho - JW3A.21, JW3A.38, JW4A.15, J Kanetake, Tomoki - JTu3A.107 JW4A.35 Jachura, Michal - FTh3E.4 Kang, Jeongjin - JTu3A.41 Kim, Yosep - JW4A.15, JW4A.35 Jacquot, Maxime - FTh2E.3 Kang, Joohoon - FW5A.5 Kirby, Brian T. - JW4A.37, JW4A.39 Jagadish, Chennupati - JTu3A.49 Kang, songbai - JW4A.25 Kirkland, James - JTu2A.90 Jaimes-Nájera, Alfonso I. - FM4B.6 Kang, Yuhao - JW4A.109, JW4A.113, JW4A.83 Kitching, John - JW4A.25 Jain, Amit - FM4D.6 Kant, Ravi - JW4A.69 Kivishar, Yuri - FTh3A Jakutis Neto, Jonas - JTu3A.28 Kante, Boubacar - FTu4A.2, JW3A.89, LTh3F.5 Kivshar, Yuri S. - FM4A.1, JW3A.3 Jamali Mahabadi, Seyed Ehsan - JTu2A.53 Kanter, Gregory - JW3A.4 Kizhakkumpurath Manikandan, S - JW4A.24 James, Timothy D. - JW3A.75 Kao, Fu-Jen - FTu4B.4, FW5D.6 kjaer, kasper - LM2F.1 Jaramillo-Villegas, Jose A. - FTh3E.3 Kapteyn, Henry C. - LM3F.4 Kleineberg, Ulf - FTh2B.3 Jarzyna, Marcin - FTh3E.4 Karalis, Aristeidis - FTh1A, FTh3B.8 Kleiner, Vladimir - JW3A.103 Jauregui-Vazquez, Daniel - JW4A.70 Karasik, Valerii E. - JTu2A.20, JTu3A.15, JW4A.85 Klemke, Nicolai - JTu3A.18 Javahiraly, Nicolas - JTu2A.115, JTu2A.97 Karcher, Romain - FW2E.3 Kletzien, Heidi - JTu2A.83 Jayakumar, Harishankar - JW3A.122 Karimi, Ebrahim - LM4F.5 Klimova, Nataliya - JTu2A.16 Jeon, Joohyeon - FM2A.4 Karl, Robert - LM3F.4 Knauer, Sebastian - FTh3E.7 Jeong, hayong H. - FTu5B.2 Karnowski, Karol - FTh2C.1 Knights, Andrew P. - FW5A.4 Jesus Silva, Alcenísio José - JW4A.114 Kärtner, Franz X. - JTu3A.18, LTu4F.2 Ko, Donghyuk - LM4F.5

FiO + LS 2017 • 17–21 September 2017 89 Ko, Yeong H. - JW3A.68 L Li, Wenzhe - JTu2A.37 Kobayashi, Misako - JTu3A.68 La, Jeffrey - JTu2A.108 Li, Xiaolong - JTu2A.82 Kochetkov, Anton - JTu3A.77 Labaye, François - FTh2B.1 Li, Xiaoying - FTu5E.2 Kodigala, Ashok - FTu4A.2, JW3A.89, LTh3F.5 Lægsgaard, Jesper - FTu5D.4, JTu3A.87 Li, Xinlong - LM4F.6 Koeckelberghs, Guy - JW4A.91 Lahiri, Mayukh - FTh3E.5 Li, XuDong - JTu3A.109 Koefoed, Jacob G. - JW4A.6 Laing, Anthony - FTh3E.7 Li, Yang - JW3A.108 Kohmoto, Takamasa - JTu2A.11|JTu2A.11 Lamb, Erin - FTu4D.4 Li, Yangfan - JW3A.60 Kolaric, Branko - JW4A.76 Lamoureux, Bethany - LTu4F.4 Li, Yuan - JTu2A.37 Kolesik, Miroslav - FW6E.2 Landragin, Arnaud - FW2E.3 Li, Yu-Huai - FTh2E.1 Kondakci, H.E. - FTh2D.3 Langrock, Carsten - JW3A.4 Li, Yvonne L. - FW2E.1 Key to Authors Kondakci, Hasan E. - FM4C.5, FM4C.6, FTu4B.3, Larger, Laurent - FTh2E.3 Li, Zengzhuo - JTu2A.26 JTu3A.64 Larkin, Ilia - FM3B.6, JTu3A.65 Li, Zeren - JTu2A.76 Kondo, Jorge M. - FW6B.4 Lasassmeh, Suha - JTu2A.29 Li, Zhengyan - LM4F.5 Kong, Fanqi - LM4F.5 Lassonde, Philippe - FTu4B.2 Li, Zhengyu - JW4A.33 Kong, Weijing - JW3A.51 Laurent, Guillaume - LM4F.3 Li, Zuoxi - JW4A.47 Koochaki Kelardeh, Hamed - JTu3A.21 Lauterio-Cruz, J.P. - JTu3A.103 Liang, Anhui - JTu2A.118 Korobko, Dmitry - JTu3A.6 Law, Chiu T. - JTu2A.29 Liao, Chi-Shiun - LTh3F.3 Korostelin, Yuriy - JTu2A.20 Lawall, John - FTh3B.5 Liao, Chun Yen - JW3A.110 Kort-Kamp, Wilton - JTu3A.23 Lawrie, Benjamin - JW3A.1, JW3A.10 Liao, Yu-Ming - LTh2F.2 Kosters, Dolfine - JW3A.54 Lazarev, Vladimir A. - JTu2A.20, JTu3A.15, JW4A.85 Liaros, Nikos - JTu2A.19 Kothari, Vaishali - JTu2A.59 Lazo-Arjona, Oscar - FM3E.2, JW4A.3 Lidke, Keith A. - FTh3D.3 Kothari, Vaishali - JTu2A.32 Le Roux, Xavier - JW3A.72 Lim, Hyun Uk - JTu3A.41 Kottos, Tsampikos - FTh1A.2 Leaird, Daniel E. - FTh3E.3, JW4A.4 Lin, Chiang-Hsin - LTh3F.6 Kovarovic, Brandon J. - FM4D.3 Leamer, Jacob M. - JW4A.34 Lin, Han - FM3D.6, JW3A.60, JW3A.90 Kowalewski, Markus - LTu5F.2 Leartprapun, Nichaluk - FTh2C.2 Lin, Hong - JW3A.37, JW3A.39 Kowligy, Abijith S. - FTu4D.4 Ledingham, Patrick M. - FM3E.2, JW4A.16 Lin, Hongtao - JW3A.72 Kozacki, Tomasz - FTu4C.3 Lee, Bumsu - JW4A.2 Lin, Hung-I - LTh2F.2 Kozlov, Sergey - FTu5C.4 Lee, Byoungho - FM2C, FTu5D.5, JTu2A.25 Lin, Jian H. - LTh3F.6 Kozlov, Vladimir - JTu3A.69 Lee, Cheol J. - FM2A.4 Lin, Ming-Fu - LM4F.2 Kozlovsky, Vladimir I. - JTu2A.20 Lee, Gil Ju - JTu2A.54 Lin, Qian - FW2A.2 Kränkel, Christian - FTh2B.1 Lee, Gun-Yeal - FTu5D.5, JTu2A.25 Lin, Ren Jie - JW3A.109 Kravchenko, Ivan - JW3A.3 Lee, HK - JTu2A.57 Lin, Shih-Yao - LTh3F.3 Kress, Christian - FM3A.3 Lee, Hyeonwoo - JTu3A.1 Lin, Shiuan-Huei - JW4A.100 Krizek, Jan - JTu3A.9 Lee, Kyu J. - JTu2A.60 Lin, Wei - FM4D.3 Kroh, Tobias - LTu4F.2 Lee, Seungrag - JTu2A.87 Lin, Wei-Ting - LTh3F.6 Kruk, Sergey S. - JW3A.3 Lee, Wei - FM4C Lin, Yingda - JTu3A.36 Krylov, Alexander A. - JTu3A.15 Lee, Woowon - FW5D.5 Linag, Houkun - LTu4F.2 Kubota, Akihiro - JW3A.71 Légaré, François - FTu4B.2, JTu3A.16 Lind, Alexander - FTu4D.4 Kucera, Courtney - JW4A.81 Légaré, Katherine K. - JTu3A.16 Lindlein, Norbert - FTh3D.7 Kudlinski, Alexandre - JW4A.103 Lehman-Borer, Thomas - JW3A.35 Lindquist, Robert G. - JTu2A.22 Kuebler, Stephen M. - FM3D.5 Lehr, Kevin - JTu3A.36 Lingaraju, Navin - FTh3B.5 Kues, Michael - FTh3E.2 Lei, Xun - JW4A.50 Lipka, Michal - FTh3E.4 Kuhl, Ulrich - FTh1A.2 Leibovici, Matthieu C. - FTh3D.6 Litchinitser, Natalia M. - FW6B.5, JTu3A.10, Kuipers, Kobus - FM3B.5, JW3A.54 Lemaître, Aristide - FW5E.3 JW3A.113 Kuk, Donghoon - FM2B.2, JTu3A.78 Lemos, Gabriela B. - FTh3E.5 Little, Brent - FTh3E.2 Kulkarni, Rajan - FW5D.2 Leo, Francois - FTh2B.4 Liu, Bin - JTu3A.51 Kumar Bag, Saawan - FW6C.3 Leone, Stephen - LTu4F.4 Liu, Cheng-hui - FTu5C.3, JTu2A.72 Kumar, Ajeet - JW3A.44, JW3A.66, JW3A.67, Leong, Edward - JW4A.79 Liu, Fei - JTu2A.101 JW4A.120 Lepetit, Thomas - FTu4A.2, JW3A.89, LTh3F.5 Liu, Jiansheng - JTu3A.17 Kumar, Ajit - JW3A.47, JW3A.49 Lett, Paul D. - FM2D.4, JW3A.36 Liu, Jin - FM2E.1 Kumar, Ashok - JW3A.10 Leveillee, Joshua - LM4F.2 Liu, lai - JW4A.122 Kumar, Kaushal - JTu3A.117 Lewera, Adam - JTu3A.48 Liu, Xia L. - JTu2A.93 Kumar, Pardeep - FTh3B.2 Lewis, Bridget - FTh3C.1 Liu, Yang - FTh2E.1 Kumar, Prem - JW3A.4 Leykam, Daniel - FTu4D.5 Liu, Yining - JW4A.51 Kumar, Samir - JW3A.99, LTh2F.3 Lezec, Henri - JW3A.119, JW3A.87 Liu, Yonghao - FTu4E.2, JTu3A.55, JW4A.68 Kumar, Santosh - JTu2A.13, JTu2A.27, JTu2A.32, LI, Binghui - FTh3A.7 Liu, Yongmin - FM3D.2 JTu2A.59, JTu2A.65 Li, Gordon H. - FW5E.2 Liu, Yuhong - FTu5E.2 Kumar, Vikash - JW4A.44 Li, Guangkuo - JTu3A.76 Liu, Yuxiang - JW3A.74, JW4A.88 Kumara Vadivel, Shruthi - FTh3D.6 Li, Guifang - FW5D.4 Livers, Steven - JTu2A.36 Kumazaki, Hajime - JW4A.92 Li, Guoqiang - JTu2A.26 Lo, Chih Wei - FW5E.2 Kuntz, Katanya B. - FTh3E.6 Li, Hao - FTh2E.1 Lobino, Mirko - FM3E.5 Kurachi, Cristina - FTu5C.2 Li, Haoyu - FW6D.3, JTu2A.94 Loginova, Mariya M. - JTu3A.58 Kurokawa, Nao - JTu2A.98 Li, Jiagen - FTu4A.4, JW3A.58 Lombardo, David - JTu2A.39 Kuwata-Gonokami, Makoto - LW5F.4 Li, Jiamin - FTu5E.2 Loncar, Marko - JW3A.108 Kuzin, Evgeny - JTu3A.103, JW4A.115, JW4A.72, Li, Junhui - JTu2A.8, JTu3A.94 Long, David - JTu3A.20 JW4A.78, JW4A.87 Li, Ming-Han - FTh2E.1 Longhi, Stefano - FW6B.5 Kuzmiak, Vladimir - JW3A.79 Li, Mo - JW4A.12 Longman, A - FM2B.4 Kuz’mina, Maryana - JTu3A.77 Li, Qian - FTu4A.4, JTu3A.76, JW4A.108, JW4A.71 López Gayaou, Valentin - LTh3F.2 Kwiecien, Pavel - JTu3A.113 Li, Qing - FM3A.2 Lopez Huidobro, Santiago - FTu4D.3 Kwiecien, Pavel - JW3A.79 Li, Shuo - JW3A.60 Lopez-Dieguez, Yanelis - JW4A.70 Kwong, Dim-Lee - FTu5A.3 Li, Tian - JW3A.36 López-Estopier, Rosa E. - JW4A.87 Kyoseva, Elica - JTu3A.32 Li, Ting - JTu3A.74 Lopez-Mariscal, Carlos - FM3B, FW2B, JTu3A.85

90 FiO + LS 2017 • 17–21 September 2017 Lorenz, Virginia O. - FM3E.1, FW2E Maleki, Lute - FTu4E.4, FTu5E Miao, Bo - FM2B.1, FM2B.2, JTu3A.12 Lou, Runnan - JW3A.115 Malinovsky, Vladimir S. - JW4A.39 Miao, Pei - FW6B.5 Midorikawa, Katsumi - LW5F.4 Lougovski, Pavel - JW4A.23 Malkhasyan, Vahan - JTu3A.34 Key to Authors Louri, Ahmed - JW4A.57 Malko, S - FM2B.4 Mielec, Nicolas - FW2E.3 Louw, Danie - JTu3A.43 Maltese, Giorgio - FW5E.3 Mikhailova, Julia M. - JTu3A.102, LM2F.3 Lovato, Laura - JTu2A.58 Malushin, Nikolay - JTu2A.56 Milchberg, Howard - FM2B.1, FM2B.2, FM3B.6, Love, Gordon - JTu2A.42 Malviya, Nishit - JTu3A.56 FW6E.2, JTu3A.12, JTu3A.45, JTu3A.5, Lovell, Greg - JTu2A.3, JW4A.112, JW4A.62, Mancini, Giulia F. - LM3F.4 JTu3A.65 JW4A.73 Mandal, Debabrata - FTu4A.3 Miller, David - FTh3D.5 Lovergine, Nico - FTh2D.2, JW4A.45 Mandracchia, biagio - FW2C.3, FW5D.1, JTu2A.2 Miller, David A.B. - FTu4A.1 Lozano-Crisostomo, Nestor - JW3A.40, JW3A.42, Mantel, Klaus - FTh3D.7 Miller, Keith - JTu2A.37 JW4A.95 Mantri, Richa - JW3A.44 Miller, Nicholas A. - LM2F.2 Lu, Guowei - FW2A.1, JW3A.11 Manukyan, Karapet - JTu3A.62 Mironov, A.E. - JTu3A.105 Lu, Hsuan-Hao - JW4A.23, JW4A.4 Manzo, Michele - JTu2A.89 Mironov, Andrey - JTu3A.105, JW4A.81 Lu, Ming-Feng - JTu2A.102, JTu2A.111 Marangos, Jon - FW6E.1 Mirza, Imran M. - JW3A.2 Lu, Peixiang - JW3A.5 Marder, Seth - JTu3A.61 Misawa, Kazuhiko - LTu5F.3 lu, peng - JW4A.108, JW4A.71 Marino, Alberto - JW3A.10 Mishra, Ashish - JTu2A.64 Lu, Wei - JW3A.57 Markos, Christos - JW4A.99 Mishra, Vishwatosh - JTu3A.13, JW4A.8 Lu, Xiyuan - FM3A.2 Marsh, Brett M. - LTu4F.4 Mistyuk, Sergei - JTu2A.49 Luebke, David - FTh3C.2, FW5C.1 Martin Gonzalez, Marisol - JW3A.91 Mittal, Sunil - FM3E.4 Luk, Ting - JW3A.46 Martin Vela, Javier A. - JW4A.70 Mittendorff, Martin - JTu3A.31, JW4A.79 Lukens, Joseph M. - JW4A.23 Martinez Niconoff, Gabriel - JTu3A.101 Mobini, Esmaeil - JTu3A.8, JW4A.111 Lukin, Mikhail - FM4E.4 Martinez Vara, Patricia - JTu3A.101 Modsching, Norbert - FTh2B.1 Lum, Daniel - FM3C.5 Martinez, Noel - FM3D.5 Mohamed, Ali - JW4A.1 Lumer, Yaakov - FM3B.7 Martini, Francesco - JW3A.13 Mohammadi, Fatemesadat - JTu3A.49 Luo, Bin - JTu2A.8, JTu3A.94 Martini, Rainer - FM2D.3 Mohammadian, Nafiseh - FM4C.5, FM4C.6 Luo, Kai Hong - JW4A.3 Martins, Renato J. - JW4A.86 Mohammed, Dunya Z. - FTu5A.4 Luo, Qiaoen - FM4B.3 Masis, Sergai - JW4A.17 Moille, Gregory - FW5A.5 Luo, Songjie - FM4B.6 Mason, Briana - JTu2A.108 Moiseev, Sergey G. - JTu3A.6, JW3A.117, Luo, Ting - JTu2A.6 Mathews, Jay - JW3A.76 JW3A.45, JW3A.53 Luo, Yuan - JTu3A.88 Mathews, Scott - JW3A.6 Mokhov, Sergiy - JTu2A.46 Lustig, Eran - FM3B.7 Matia-Hernando, Paloma - FW6E.1 Moller, Heinrich - JTu3A.43 Lyatun, Ivan - JTu2A.16 Matichak, Jonathan D. - JTu3A.61 Molpeceres, Carlos - FW6B.2 Lynch, Edward - JTu2A.29 Matyas, Corey T. - JW3A.85 Mondal, Partha - JTu3A.13, JW4A.8 Lysevych, Mykhaylo - JTu3A.49 May-Arrioja, Daniel A. - JW3A.42, JW4A.95 Montazeri, Kiana - FM4A.6, JW3A.97, JW4A.45 Lytle, Amy L. - JW3A.35 Mazumder, Nirmal - FTu4B.4 Monteil, Guy - JTu3A.34 Mazur, Eric - JW3A.108 Moon, Sung - JW3A.38 M Mazurzcyk, Matthew - FW6A.1 Moran, Paul J. - JTu3A.110 M.V., Jabir - JW4A.29, JW4A.30 McClean, Jarrod - FM4E.2 Morandotti, Roberto - FTh3E.2, FTu4B.2 Ma, Wei - FM3D.2 McCormick, Aidan F. - FM2D.2 Moreau, Paul-Antoine - FTu5E.3 Ma, Xiongfeng - FTh2E.1 McDaniel, Hunter - FTu5B.5 Moreira, Raoni S. - JW4A.18 Ma, Xuedan - FW5A.5 McLeod, Euan - FTh2D, FTu5D.1 Morgan, Kaitlyn - JTu2A.37 Ma, Xujun - JTu2A.112, JW4A.83 McLeod, Robert R. - FTh3D.5 Mørk, Jesper - FW5A.2 Ma, Yaoguang - JW3A.115 Mcnee, Ian - JTu3A.69 Morley-Short, Sam - FM4E.2 Ma, Yufei - JTu3A.109 Meglinski, Igor - JTu2A.78 Mortessagne, Fabrice - FTh1A.2 Ma, Zhizhen - FM2A.3, FM2A.4, JTu3A.25, Mehidine, Hussein - FW5D.3 Moryatov, Alexandr - FTu5C.4 JW3A.96 Mehrabian, Armin - JTu2A.24 mosca, simona - FTh2B.4 MacFarlane, Duncan - FM3C.4, JTu2A.7 Mei, Yefeng - JW4A.26 Moser, Christophe - JTu3A.9 Mackey, David A. - FTh2C.1 Meiselman, Seth - FW6A.5 Moses, Jeffrey - LM4F.3 Madabhushi Balaji, Muralidhar - FM3C.4 Mekala, Naren - JTu2A.64 Moskaletz, Oleg - JTu2A.48 Maddaloni, Pasquale - FTh2B.4 Meliani, Hasnaa - JTu3A.34 Moskowitz, Ira - FM2C.1 Madden, Stephen J. - FTu4A.5 Mellado-Villaseñor, Gabriel - JTu2A.40 Moss, Ben - FW5A.3 Mafi, Arash - JTu3A.106, JTu3A.8, JW3A.20, Mello, Pier - JW4A.83 Moss, David - FTh3E.2 JW4A.111, JW4A.119, JW4A.96, LTh4F.5 Mena-Montes, Rodolfo - JW3A.40 Mott, Russell - JW4A.25 Magnusson, Robert - JTu2A.60, JW3A.104, Méndez Otero, M.Maribel - JTu3A.52 Mouchet, Sébastien R. - JW4A.76 JW3A.62, JW3A.68 Mendez, C - FM2B.4 Mouradian, Levon - JTu3A.62 Maguid, Elhanan - JW3A.103 Mendonça, Cleber R. - FTh3A.3, JW4A.86, Mücke, Oliver - JTu3A.18 Mahalanobis, Abhijit - FM4C.4 JW4A.91 Mukamel, Shaul - LTu5F.2 Mahato, Krishna Kishore - FTu4B.4, JTu2A.61 Meng, Fei - JW3A.60 Muliar, Olena - FTu5D.4 Mahmoud, Ahmed - FTh3B.6 Meng, Xiang - JW3A.84 Müller, Holger - FW2E.2 Maimaiti, Aili - FW6B.1 Meng, Ziming - JTu2A.118 Muller, Matthew S. - JTu2A.69 Mainz, Roland E. - JTu3A.18 Menon, Vinod M. - JTu3A.33, JW3A.122, JW3A.93, Múnera, Natalia - JW3A.9 Maji, Satyajit - JTu3A.82, JTu3A.91 LM3F.1 Muñeton, David - JW3A.86 Majumdar, Arka - FM4A.4 Menyuk, Curtis R. - JTu2A.53, JTu3A.14, JTu3A.57, Muniraj, Inbarasan - JW4A.75 Makarova, Mariya - JTu2A.56 JW4A.9 Muniraj, Inbarasan - JTu2A.94 Makino, Kenzo - FM3E.3 Merceron, Loïc - FTh2B.1 Munns, Joseph H. - FM3E.2, JW3A.34, JW4A.16 Makoana, Nkutwane Washington - JTu3A.43 Meriles, Carlos - JW3A.122 Muraca, Amanda R. - LM4F.6 Makowski, Piotr L. - FTu4C.3 Merklein, Moritz - FTu4A.5 Murakami, Kenichi - JTu2A.52 Makri, Eleana - FTh1A.2 Merlet, Sébastien - FW2E.3 Murnane, Margaret M. - LM3F.4 Makris, Konstantinos - FM4B.4, JW3A.106 Mermelstein, Marc D. - JW4A.90 Murphy, Thomas E. - JTu3A.31, JW4A.79 Maksimenko, L.S. - JTu2A.99 Messina, Gabriele - JTu2A.58 Malallah, Ra’ed - JW4A.75 Meuer, Christian - FM3A.3

FiO + LS 2017 • 17–21 September 2017 91 Murshid, Syed H. - JTu2A.3, JW4A.107, JW4A.110, Okui, Makoto - JTu2A.105|JTu2A.105 Peng, Tianyi - FTh2E.1 JW4A.112, JW4A.52, JW4A.59, JW4A.62, Okulov, Alex - JTu3A.114 Peng, Tong - JTu3A.4 JW4A.73 Omatsu, Takashige - FTu4B Pereira Dos Santos, Franck - FW2E.3 Murzina, Tatiana - JW3A.101 Ooi, Kelvin J. - FM3A.4, JTu3A.35 Perez Garcia, Laura - FTu4D.3 Mussot, Arnaud - JW4A.103 Orenstein, Meir - FM4A.2 Perez, Eduardo - JTu2A.21 Myakinin, Oleg - FTu5C.4, JTu2A.4, JTu2A.73, Orre, Venkata Vikram - FM3E.4 Perez, Guillermo - FTh3C.5 JTu2A.74, JTu2A.81 Ortaç, Bülend - JTu3A.72 Perez, J A. - FM2B.4 Myers, Jason D. - JTu3A.10 Osawa, Shuto - FTh3E.1 Perez-Garcia, Benjamin - JTu3A.85 Osgood III, Richard M. - FM4D.6 Perry, Joseph W. - JTu3A.61 N Osgood, Richard M. - FW5A.4, JW3A.84 Persano, Anna - FTh2D.2 Key to Authors Nabekawa, Yasuo - LW5F.4 Österberg, Ulf - JW4A.117 Persons, Christopher - JTu2A.90 Nabet, Bahram - FM4A.6, FTh2D.2, JW3A.18, Osuagwu, Uchechukwu L. - JTu2A.116 Perumal, Packiyaraj - LTh3F.3 JW3A.97, JW4A.45 Osvay, Karoly - LW5F.2 Perumangatt, Chithrabhanu - JW4A.13 Nader, Nima - FTu4D.4 Ottaviano, Luisa - FW5A.2 Peter, Krogen - LTu4F.2 Nadkarni, Priya - JW4A.38 Otte, Sven - FM3A.6 Peters, Nicholas A. - JW4A.23 Nagamine, Gabriel - FTu5B.5 Ou, Zhe-Yu - FTu5E.2 Petit, Stéphane - JTu3A.67 Nagasaka, Kenshiro - JW4A.122 Ourari, Salim - JW3A.37 Petrov, Alexandr - JTu2A.16 Naghibi Alvillar, Sahar - JTu3A.25 Owrutsky, Jeffrey - JTu3A.47 Petrov, Nikolai I. - FTh3B.7, JTu2A.107, JTu2A.34, Nagymihaly, Roland - LW5F.2 Owusu, Alfred - FM3C.2 JTu2A.35, JTu2A.38, JTu2A.41, JW3A.107 Nakajima, Naoya - JTu3A.108 Oxburgh, Stephen - JTu2A.44, JTu2A.45 Petrova, Galina N. - JTu2A.38 Nakamura, Ryosuke - FM3E.3 Ozcan, Aydogan - FW5D.2 Petruzzella, Matteo - FTh3E.7 Naqvi, Zeba - JTu2A.14 Peysokhan, Mostafa - JTu3A.106, JTu3A.8, Narayana, Vikram - JTu2A.24, JW4A.55 P JW4A.111 Narayanamurthy, Chittur S. - JTu2A.43 Pacifici, Domenico - LTh2F.1, LTh3F Pfefer, T.Joshua - FM4D.1, FM4D.5, JTu2A.75, Narimanov, Evgenii E. - JW3A.105, JW3A.81, Padgett, Miles J. - FTu5E.3 JTu3A.2 LM3F.1 Padilha, Lázaro - FTu5B.5 Pham, Quang D. - FW2C.2 Natalia, Kokareva - JTu2A.16 Paesani, Stefano - FM4E.2, FTh3E.7 Phatak, Charudatta - FM3C.6 Nataraj, Chandrika T. - JW4A.53 Pai, CS - FM3E.5 Phillips, Christopher R. - FTh2B.1 Naumov, Andrei - FTh2B.2 Paine, Scott - JTu2A.91 Pi, Liang-Wen - JTu3A.36 Nayak, Jeeban - FTh3A.6 Paiva, Joana S. - JTu2A.68 Piers, Patricia - FTh3C.5 Naydenov, Pavel - JW3A.101 Pakalapati, Mano R. - JW3A.26, JW3A.27 Pigeon, Jeremy - FW6E.3 Nayfeh, Ammar - JW4A.42 Pal, Bishnu P. - JTu3A.81 Piggott, Alexander Y. - JW3A.14 Neely, Tyler W. - FW2B.3 Pal, Vishwa - FTh2E.2, FTu4C.4 Pilipetskii, Alexei - FW6A.1 Nejadriahi, Hani - JW4A.46 Palastro, John - JTu3A.59 Pique, Alberto - JW3A.6 Nellikka, Apurv Chaitanya - JTu3A.96, JW4A.29 Palit, Prithviraj - FTu4E.2 Pires, Danilo - FTh3B.4 Neri, José W. - JTu3A.28 Pallud, Johan - FW5D.3 Piscitelli, Vincent - JTu3A.118 Neshev, Dragomir N. - FW2B.1, JW3A.3 Palstra, Isabelle - JW3A.54 Pisonero, J D. - FM2B.4 Ng, Doris K.T. - JTu3A.35 Pan, Jian-Wei - FTh2E.1 Piwowar, Justyna - JTu3A.48 Ni, George - FM4D.6, JW3A.91 Pan, Yingling - JTu3A.17 Plotnik, Yonatan - FM3B.7 Ni, Xiang - JW4A.113 Panchenko, Evgeniy - JW3A.75 Png, Ching Eng - FM3A.4, JTu3A.35 Ni, Xiaochang - JW3A.51 Pang, Richard - FM4D.6 Poem, Eilon - FM3E.2 Ni, Xingjie - FW6B.3 Papay, Joel A. - JTu2A.69 Polikarpov, Maxim - JTu2A.16 Niazmand, Reza - JW4A.65 Papp, Scott - FTu4D.4 Politi, Alberto - JW3A.13 Nic Chormaic, Sile - FTu5B, FW6B.1 Paradis, Clément - FTh2B.1 Polyakov, Sergey - FM4E.6 Ning, Cun-Zheng - FW6C.1 Parameswaran, S - JW3A.46 Poojary, Ashwin - JW4A.64 Nishchal, Naveen K. - JTu2A.109 Paraskun, Artur - JTu2A.48 Poon, Joyce K. - FM3A.1 Nithyanandan, Kanagaraj - JW4A.123 Pareek, Prakash - JW3A.25 Pooser, Raphael - JW3A.1, JW3A.10 Nogueira, Rogério N. - FW6A.4 parisi, maria - FTh2B.4 Popov, Alexey - JTu2A.78 Nolte, Stefan - FTh1A.3 Parisio, Fernando R. - JW4A.18 Popov, Vladimir - JW3A.107 Nomoto, Sean M. - JTu3A.111, JTu3A.7 Park, Hyunwook - LTu4F.2 Porter, Christina L. - LM3F.4 Northup, Tracy - FM3E.6 Park, Jae-Hyeung - FW2C, FW5C.3 Posada-Ramirez, B. - JW4A.72 Norton, Benjamin G. - FM3E.5 Park, Junhee - FTu4A.2 Pottiez, Olivier - JTu3A.103, JW4A.115, JW4A.87 Nou, Xuefei - JTu2A.84 Park, Sang - JW3A.34 Poulon, Fanny - FW5D.3 Novotny, Lukas - JTu3A.83 Parker, Thomas - JW4A.3 Poulton, Christopher V. - FW5A.3 Nsofor, Ugochukwu - JW4A.40 Parks, Helen H. - JW4A.2 Pourbeyram, Hamed - JW3A.20, JW4A.119 Nunn, Joshua - FM3E.2, JW4A.16 Parry, Matthew - JW3A.3 Poutrina, Ekaterina - FW5E.1 Nye, Nicholas - JW4A.99 Paskov, Milen - FW6A.1 Poveda Cuevas, Freddy Jackson - FTu4D.3 Pate, Brad - JTu3A.47 Pozza, Nicola D. - FTh3E.6 O Pathak, Akhilesh K. - JTu2A.51 Prabhakar, Anil - JTu2A.64 O’Brien, Jeremy - FM4E.2, FTh3E.7 Pati, gour S. - JW3A.28, JW3A.7 Pradhan, Somarpita - JTu3A.75 Ocegueda, Manuel - JW4A.11 Pattanayak, Aswini K. - JTu3A.91 Prashanth, Gurusiddappa R. - JW4A.53 ODEH, Mutasem A. - FW6C.4, JTu2A.18 Patterson, William - FW6A.1 Pratavieira, Sebastião - FTu5C.2 Odele, Ogaga - FTh3E.3, JW4A.23, JW4A.4 Paturzo, Melania - FW2C.3, FW5D.1, JTu2A.2 Prete, Paola - FTh2D.2, JW4A.45 Oghalai, John - FTh2C.3 Paulson, Bjorn - FTu5B.2 Prior, Yehiam - FM4A.5, JW3A.95 Oh, Kyunghwan - FTu5B.2, JTu3A.1, JW3A.38 Pavlov, D.A. - JW3A.117 Priye, Vishnu - JTu3A.56, JW4A.44 Ohishi, Yasutake - JTu2A.33, JW4A.106, JW4A.122, Peacock, Anna - JW4A.117 Proscia, Nicholas - JW3A.122, LM3F.1 JW4A.77 Pedersen, Christian - FTu5D.3, JTu3A.38 Pu, Jixiong - FM4B.6 Ohta, Masamichi - JTu2A.1, JTu2A.11|JTu2A.11 Penano, Joseph - JTu3A.59 Pugzlys, Audrius - FM2B.1 Oi, Ryutaro - JTu2A.105|JTu2A.105 Peng, Cheng-Zhi - FTh2E.1 Purdy, Thomas - JW3A.69 Okabe, Yusuke - JW3A.19 Peng, Fang - JTu3A.109 Pursely, Brennan - JW4A.2 Okamura, Taku - JTu3A.68 Peng, Jiaxin - JW4A.55 Pustovoit, Vladislav I. - FTh3B.7 Okoro, Chukwuemeka - FTu5C.5 Peng, Qixian - JTu2A.76

92 FiO + LS 2017 • 17–21 September 2017 Q Robertson, Tracy - JW3A.43 Samad, Shafeek A. - JW4A.53 Qi, Bingkun - JW3A.55 Robles, Francisco E. - FW5D, FW6D.2 Samanta, Goutam K - FW2B.2, JTu3A.96, JW4A.29,

Qi, Cui-ling - JTu2A.111 Rocha Medina, Jose E. - JW4A.95 JW4A.30 Key to Authors Qi, minghao - FTh3E.3 Rocha, José C. - FTh3B.4 Samanta, Swagata - JW3A.70, JW4A.48 Qi, Zhen - JTu3A.14 Rocha, José Carlos A. - JW4A.114 Sampson, Danuta M. - FTh2C.1 Qian, Xiao-Feng - JW4A.24 Rochford, Jonathan - JTu2A.63 Sanchez-Mondragon, J.Javier - JW3A.40, JW3A.42, Qiao, Pengfei - FTu4E.1 Rodriguez Ortiz, Carlos A. - JTu3A.60 JW4A.56, JW4A.95 Qiao, Zhi - JTu3A.74 Rodriguez Vazquez de Aldana, Javier - FW6B.2 Sanderson, Carl R. - JTu3A.110 Qin, Chengzhi - JW3A.5 Rodriguez, Brian - JTu2A.89 Sandhu, Bhupinder - JTu3A.61 Qiu, Cheng-Wei - JW3A.92 Rodriguez, Luis - JTu3A.118 Sanghera, Jasbinder S. - JTu3A.10 Qu, Kenan - FW5B.5 Rodríguez-Morales, Luis A. - JW4A.115 Sanjeev, Vyshakh - JW3A.102, JW3A.92 Quaranta, Fabio - FTh2D.2 Rohwer, Erich G. - FM2B.3 Santagati, Raffaele - FM4E.2, FTh3E.7 Quiring, Viktor - JW4A.3 Rojas-Laguna, Roberto - JW4A.70 SANTIAGO-HERNANDEZ, HECTOR - JW4A.115, Rolland, Jannick P. - FTh3D.1 JW4A.78 R Romach, Yoav - JW4A.17 Santillán, Jesica M. - JW3A.86 R, Vijaya - JW4A.98 Romero Cortes, Luis - FTh3E.2 Santra, Siddhartha - JW4A.39 Rahman, Hafizur - FW5D.5 Rong, Kepeng - JTu3A.112 Sapienza, Luca - FM2E.1, FM2E.2, JW3A.50, Raina, Ankur - JW4A.38 Roper, Christopher - JW4A.25 JW3A.52 Raizen, Mark - LTh4F Ropers, Claus - FTh2B.2 Sapoznik, Kaitlyn - JTu2A.6 Rakher, Mattew - JW4A.25 Rosa, Carla C. - JTu2A.68 Saraceno, Clara J. - FTh2B.1 Ramanauskaite, Lina - JW3A.94 Rosa, Ramon G. - FTu5C.2 Sarangan, Andrew - JTu2A.39, JTu3A.29, JTu3A.93 Ramezani, Hamidreza - FTh1A.1, FTh1A.4, Rosenblatt, Gilad - FM4A.2 Sarkar, Anirban - JW3A.30 JW3A.73 Rosenthal, Eric - FM3B.6, JTu3A.65 Sarkar, Resham - JW4A.19 Ramírez Martínez, Daysi - JTu3A.97 Roso, Luis - FM2B.4 Sarpkaya, Ibrahim - JW3A.96 Rangarajan, Prasanna - FM3C.4, JTu2A.7 Rossi, Giulio M. - JTu3A.18 Saunders, Dylan J. - FM3E.2, JW4A.16 Rangelov, Andon - JTu3A.32 Rothau, Sergej - FTh3D.7 Savoie, Denis - FW2E.3 Ranjan, Ravi - JW3A.25 Rotter, Stefan - FM4B.4 Sawides, Lucie - JTu2A.6 Rao, Bola Sadashiva Satish - JTu2A.61 Rottwitt, Karsten - FTu5D.4, JTu3A.87, JW4A.6 Scaffardi, Lucía B. - JW3A.86 Rarity, John - FTh3E.7 Roxworthy, Brian J. - FM2A.1 Scalora, Michael - JTu3A.29, JTu3A.93 Rasras, Mahmoud - JW4A.42 Roy Bardhan, Bhaskar - JW4A.34 Scarcelli, Giuliano - JTu2A.84 Rastogi, Vipul - FTh3A.4 Roy Chaudhuri, Partha - JTu3A.75 Scarcelli, Giuliano - FM4B.2 Rathnakar, Bharath - JTu2A.61 Roy, Abhijit - JTu3A.92 Scheytt, J.Christoph - FM3A.3 Rathnaker, Bharath - FTu4B.4 Roy, Arkadev - JTu3A.13, JTu3A.22, JTu3A.24 Schiavi, Andrea - FW6E.1 Raupov, Dmitry - JTu2A.4, JTu2A.74, JTu2A.81 Roy, Samudra - JTu3A.66, JW4A.116, JW4A.118 Schinca, Daniel C. - JW3A.86 Raybon, Gregory - FW6A Roy, Sourabh - JTu2A.31, JTu3A.30 Schlawin, Frank - LTu5F.2 Raza, Ali - JW3A.82 Roychoudhuri, Chandra - JW3A.32 Schleife, Andre - LM4F.2 Reddy, Prithvi - JW3A.122 ROYCHOWDHURY, PRIYANKAR - JW4A.57 Schmidt, Bruno E. - FTu4B.2 Reichert, Matthew - JW4A.31 Roztocki, Piotr - FTh3E.2 Schmidt, Jürgen - FTh2B.3 Reid, Derryck T. - FTu4B.1 Rubinsztein-Dunlop, Halina - FW2B.3 Schmidtke, Katharine - JW4A.65 Reimer, Christian - FTh3E.2 Rubio, Angel - JTu3A.18 Schmittberger, Bonnie L. - FM2D, FM2D.4, Ren, Juanjuan - FW2A.1, JW3A.11, JW3A.22, Rudenko, S.P. - JTu2A.99 JW3A.36 JW3A.24 Ruiz, Ulises - JTu2A.40 Schmitt-Sody, Andreas - JTu3A.59 Ren, Ruizhi - JTu2A.104, JTu2A.110 Rumpf, Raymond C. - FM3D.5 Schouten, Hugo - JW3A.8 REN, YAN - JW4A.10 Russo, Saverio - JW3A.59 Schroeder, Bryce - JTu2A.94, JTu3A.90 Ren, Yundong - JTu2A.55, JW3A.74 Ryland, Elizabeth - LM4F.2 Schultze, Martin - LW5F.1 Ren, Yu-xuan - LW2F.3 Ryu, Wonhyoung - JTu3A.1 Schunemann, Peter - JTu3A.69 Reshef, Orad - JW3A.108 Schwartz, Robert - FM2B.1 Restelli, Alessandro - FM3E.4 S Schwartz, Sylvian - FM4E.4 Reyes esqueda, Alejandro - JTu3A.97 S.Abdulhalim, Ibrahim - FW6C.2 Sciara, Stefania - FTh3E.2 Reynoso Lara, E. - JTu3A.52 Saastamoinen, Kimmo - FW5B.4 Seaberg, Matthew H. - LM3F.4 Rezvani Naraghi, Roxana - FTh3D.2, JTu2A.106, Saastamoinen, Toni - FW5B.4 Searles, Thomas - JW3A.76 JTu3A.86 Sadasivan Nair, Vijayakumar - JTu2A.62, JW4A.80 Segev, Mordechai - FM3B.7 Rhee, Hanjo - FM3A.6 Safavi-Naeini, Safieddin - JW3A.120 Sekine, Norihiko - JW4A.92 Rho, Junsuk - FTh2D.1, FW6C Safronov, Kirill - JTu2A.16 Seman Harutinian, Jorge Amin - FTu4D.3 Riaz, Muhammad - JW3A.26, JW3A.27 Sagiv, Amir - FM4B.5 Semenova, Elizaveta - FW5A.2 Ribeiro, Jose J. - JW4A.101 Saha, Samik - JTu3A.75 Senoo, Taku - JTu2A.52 Ribeiro, Rita S.R. - JTu2A.68 Saha, Soham - JTu2A.12 Sension, Roseanne J. - LM2F.2 Ricardo, Jhonatha - JTu3A.28 Sahin, Ezgi - FM3A.4, JTu3A.35 senthil, manirajan - JW4A.58 Ricciardi, Iolanda - FTh2B.4 Sahoo, Ambaresh - JTu3A.66, JW4A.118 Serdega, Boris - JTu2A.99 Ricejam, James - JTu2A.89 Sahoo, Hitesh K. - FW5A.2 Sergienko, Alexander V. - FTh2E, FTh3E.1 Richardson, David - FW6A.3 Sain, Basudeb - FM4A.5, JW3A.95 Serikawa, Takahiro - FM3E.3, FTh3E.6 Richardson, Kathleen - JW3A.72 Saini, Than Singh - JW4A.120 Serkland, Darwin - JW3A.46 Richardt, Tim - FTh1A.3 Saito, Lucia A. - FM2A.2, JW4A.101 Serna Otálvaro, Samuel F. - JW3A.72 Richter, Ivan - JTu3A.113, JW3A.79 Saito, Yuika - JW4A.66 Shabahang, Soroush - FTh2D.3, JW4A.99 Ricken, Raimund - JW4A.3 Sakamoto, Yuji - FTu4C.2 Shadbolt, Peter - FM4E.2 Riobo, Lucas M. - JTu2A.23 Sakanas, Aurimas - FW5A.2 Shah, Syed A. - JW3A.15 Rivenson, Yair - FW5D.2 Salas-Sanchez, Alfonso J. - JW4A.95 Shahriar, Selim M. - JW4A.19, LW6F.4 Rivera, Jose A. - LW6F.2 Salazar Romero, Martha Yadira - LTh3F.2 Shahverdi, Amin - FM2D.3, JW4A.27 Rivera, José A. - LTh4F.3 Saleh, Bahaa - FW5D.4 Shalaev, Mikhail - JTu3A.10 Rivera-Ortega, Uriel - JTu2A.30 Salehi, Fatholah - FM2B.2, JTu3A.12 Shalaev, Vladimir - JTu2A.12 Roberts, Ann - JW3A.75 Salem, Reza - FM3E.4 Shamsshooli, Afshin - FTu4E.2 Robertson, David - JTu2A.42 Salgado, C - FM2B.4 Shanblatt, Elisabeth R. - LM3F.4

FiO + LS 2017 • 17–21 September 2017 93 Shankhwar, Nishant - FM3D.8, JW3A.67 Soltani, Soheil - FTh3A.2 Suzuki, Takenobu - JTu2A.33, JW4A.106, Shao, XiaoPeng - JTu2A.101 Solyanik, Maria - JTu3A.79 JW4A.122, JW4A.77 Sharma, Ankita - FM4E.6 Soman, Anishkumar - JW4A.40 Sviridov, Dmitriy - JTu2A.20 Sharma, Jitendra - JW4A.67 Son, Tran Vinh - FM3A.5 Swaim, Jon D. - JW3A.31 Sharma, Rashi - FM3D.5 Song, Hyerin - JW3A.114 Swartzlander, Grover A. - JTu2A.95, JTu3A.95 Sharma, Varun - FW2B.2 Song, Jin Dong - FM2E.1, FM2E.2 Swillam, Mohamed A. - FTh3B.6, JW4A.41, Shen, kun-ching - LTh2F.2 Song, Seunghan - JW4A.117 JW4A.43 Shen, Xiaoqin - FTh3A.2 Song, Wuzhou - FM3B.2 Szameit, Alexander - FM3B.7, FTh1A.3 Shen, Xuechu - JW3A.57 Song, Young Min - JTu2A.117, JTu2A.54 Szgeti, Stuart - FW2B.3 Shen, Yao - JW4A.88 Sordillo, Laura - JTu2A.72 Key to Authors Shen, Zhean - FM3C.7, JTu3A.86 Sorenson, Logan - JW4A.25 T Shepherd, Ronnie - FM2B.4 Sørgård, Trygve - JW4A.117 Tae-young, Kang - JW3A.114 Sheridan, John - JTu2A.94 Sorger, Volker J. - FM2A.3, FM2A.4, FM3A, Tahersima, Mohammad H. - FM2A.3, JTu3A.25 Sheridan, John - JW4A.75 JTu2A.24, JTu3A.25, JW3A.96, JW4A.46, Tai, Po-Tse - LTh3F.6 Shi, Jian H. - JTu2A.93 JW4A.55 Takaki, Yasuhiro - FM2C.2 Shi, Jianping - JW4A.40 Sorichetti, Patricio A. - JTu2A.23 Takashima, Yuzuru - FM4C.2 Shi, Lingyan - JTu2A.5, JTu2A.72 Souhan, Brian - FW5A.4 Takeda, Yutaka - FM4E.3 Shi, Sheng-Cai - FTh2E.1 Spadoti, Danilo - FM4C.3, JW4A.49 Takesue, Hiroki - FM4E.3 Shi, Zhujun - JW3A.102, JW3A.80 Srimathi, Indumathi - JTu2A.37 Talabatula, Srinivas - JW4A.53 Shih, Bao-Jen - JW4A.100 Srinivasa, Shayan G. - JW4A.38 Tamasan, Alexandru - JTu2A.106 Shin, Dong-Myeong - JW3A.114 Srinivasan, Kartik - FM2E.1, FM3A.2, JW3A.74 Tamate, Shuhei - FM4E.3 Shin, Heedeuk - JW3A.21 Sriramoju, Vidyasagar - JTu2A.72 Tan, Dawn T.H. - FM3A.4, JTu3A.35 Shin, Yoonjung - FW5D.2 Stanislawski, Michael - FTh2B.3 Tan, Gang - JW3A.115 Shiozawa, Yu - FM3E.3 Starace, Anthony F. - JTu3A.36 Tan, Hoe - JTu3A.49 Shoemaker, Gary - JTu2A.49 Staudte, André - FTh2B.2 Tanabe, Takasumi - JTu3A.68, JW3A.19, JW3A.71, Shore, Bruce - JTu3A.32 Steenkamp, Christin - FM2B.3 JW4A.54, JW4A.92 Shotan, Zav - JW3A.122 Stefani, Alessio - FW5E.2 Tanaka, Shunta - JW4A.77 Shramkova, Oksana - JW3A.106 Steinforth, A. - JTu3A.105 Tancogne-Dejean, Nicolas - JTu3A.18 Shuai, Yichen - FTh3B.5 Steinforth, Austin W. - LTh4F.3 Tang, Hong X. - FTu4B.5 Shukla, Mukesh K. - JTu3A.115, JW3A.99 Stepanov, Serguei - JW4A.11 Tanksalvala, Michael - LM3F.4 Shumakova, Valentina - FM2B.1 Stetsenko, M.A. - JTu2A.99 Tantussi, Francesco - JTu2A.58 Sibalic, Nikola - FW6B.4 Stiller, Birgit - FTu4A.5 Tao, Ran - JTu2A.102 Sierra Hernandez, Juan M. - JW4A.70 Stockman, Mark - JTu3A.21 Tarabrin, Mikhail K. - JTu2A.20, JTu3A.15, JW4A.85 Silberhorn, Christine - FM4E.6, JW4A.3 Stognij, Alexander - JW3A.101 Tarakanchikova, Yana V. - JTu2A.78 Silva Fonseca, Eduardo Jorge - JW4A.114 Storozheva, Angela - JTu2A.107, JTu2A.34 Tareki, Abubaker M. - JTu2A.22 Silva, Daniely G. - FM4C.3, JW4A.49 Strait, Jared - JW3A.87 Taskin, Baris - JW4A.45 Silver, Michael L. - JW3A.4 Streed, Erik W. - FM3E.5 Tatka, Jakub - FM4D.3 Silverstone, Joshua - FM4E.2 Stroehl, Florian - FW6D.4 Taucer, Marco - FTh2B.2 Silverthorne, Turner - JW3A.14 Sturmberg, Bjorn - JW3A.90 Taurino, Adriano - FTh2D.2 Simkhovich, Boris - FM4A.2, FTu4D.2 Su, Ce - JW4A.52 Taylor, Jacob - FTh3B.3 Simon, David S. - FTh3E.1 Su, Zhan - FW5A.3 Tegin, Uğur - JTu3A.72 Singer, Kenneth - JTu3A.51 Sua, Yong Meng - FM2D.3, JW4A.12, JW4A.27 Teimourpour, Mohammad Hosain - JW3A.63, Singh, David - FM4B.7 Sudhir, Vivishek - LM3F.2 JW3A.64 Singh, Lokendra - JTu2A.13, JTu2A.27, JTu2A.32, Südmeyer, Thomas - FTh2B.1 Teixeira, Poliane A. - FM4C.3, JW4A.49 JTu2A.59, JTu2A.65 Suer, Can - JW3A.96 Tekavec, Patrick - JTu3A.69 Singh, R P - JW4A.13 Suess, Ryan J. - JW3A.6, JW4A.79 Tellez-Limon, Ricardo - FTu4A.2 Singh, Robinjeet - JW3A.69 Suh, Jeewon - FM3D.7 Teng, Da - FW5D.2 Singh, Surendra - JTu3A.111, JTu3A.7, JW3A.41 Suheimat, Marwan - JTu2A.116 Tetsumoto, Tomohiro - JW4A.54, JW4A.92 Singh, Vinod K. - JTu2A.51 Sukhorukov, Andrey A. - FTh1A.3, FW2B.1, JW3A.3 Tew, David - FM4E.2 Sinha Roy, Arpita - JTu3A.46 Sukhov, Sergey - FM3C.7, FTh3D.2, JTu2A.106, Thekkadath, Guillaume S. - FM3E.2 Sinha, Ravindra K. - FM3D.8, JW3A.67 JTu3A.86 Thiel, Valérian - FM4E, FM4E.5, JW4A.5 Sinharoy, Indranil - FM3C.4, JTu2A.7 Sukiasyan, Minas - JTu3A.62 Thomas, Sarah E. - FM3E.2, JW4A.16 Sinkin, Oleg V. - FW5A, FW6A.1 SUKUL, PRASENJIT PRASAD - JTu3A.117 Thompson, Mark - FM4E.2, FTh3E.7 Siqueira, Jonathas P. - JW4A.86 Sumiyoshi, Tetsumi - LW5F.4 Thyagarajan, K - JW4A.105 Situ, Guohai - FM4B.7 Sun, Fangfang - JW3A.57 Ti, Chaoyang - JW4A.88 Sivis, Murat - FTh2B.2 Sun, Greg - JW3A.110 Tidemand-Lichtenberg, Peter - FTu5D.3, JTu3A.38 Skasyrsky, Yan K. - JTu2A.20 Sun, Jingbo - FW6B.5, JTu3A.10, JW3A.113 Timmers, Henry - FTu4D.4 Skirtach, Andre - JW3A.82 Sun, Liaoxin - JW3A.57 Timofeeva, Elvira O. - JTu2A.77 Skobeeva, Valentyna - JTu2A.56 SUN, SHUAI - JTu2A.24, JW4A.55 Timofeeva, Tatiana - JTu3A.61 Smartsev, Slava - FM3B.3 Sun, Shuo - LM3F.3 Timurdogan, Erman - FW5A.3 Smith, Braden - FM4C.2 Sun, Tzu-Min - LTh3F.3 Tisch, John - FW6E.1 Smith, Brian J. - FM2D.1, FM4E.5, FW6E, JW4A.5 Sun, Xiaoqi - FW2A.2 Titchener, James - JW3A.3 Smith, Jason - JTu2A.72 Sun, Yuze - JW4A.68, LTh4F.6 Tkachenko, Vladimir - JTu2A.56 Smith-Dryden, Seth D. - FW5D.4 Sun, Yuze A. - FTu4E.2, JTu3A.55 Tochitsky, Sergei - FW6E.3, JTu3A.71 Smyntyna, Valentyn - JTu2A.56, JTu2A.99 Sun, Zheng - JTu3A.33, JW3A.93, LM3F.1 Tomazio, Nathalia B. - FTh3A.3 Snigirev, Anatoly - JTu2A.16 Sung, Jangwoon - FTu5D.5 Tomova, Zuleykhan - JTu2A.19 Snigireva, Irina - JTu2A.16 Sung, Kevin - FW5D.2 Toneyan, Hrach - JTu3A.62 Snitka, Valentinas - JW3A.94 Suponitsky, Kyrill Y. - JTu3A.61 Tong, Hoang Tuan - JTu2A.33 Soci, Cesare - JTu3A.25 Suresh, Nitin - JTu2A.10 Toninelli, Ermes - FTu5E.3 Sokolov, Yuri - JTu2A.107, JTu2A.34 Sushkov, Andrei - JW4A.79 Torres, Roman - JTu3A.52 Solis, Steven - JTu3A.70 Suzuki, Ryo - JW3A.19, JW3A.71 Torres-Cisneros, Miguel - JW3A.42 Solntsev, Alexander S. - FTh1A.3, FW2B.1, JW3A.3 Suzuki, Shigenari - FM3E.3 Toussaint, Kimani C. - FTu5C.5, FW5D.5

94 FiO + LS 2017 • 17–21 September 2017 Tradonsky, Chene - FM3B.3, FTh2E.2, FTu4C.4, Vergara Palacio, Sebastian - JTu3A.60 Wang, Shunyan - JTu3A.112 JW3A.103 Verkamp, Max - LM4F.2 Wang, Wen - FW6A.2

Treps, Nicolas - JW4A.5 Verma, Onkar N. - JTu3A.30 Wang, Xiangyu - JW4A.36 Key to Authors Triana, Julian C. - JW4A.20 Verma, Prabhat - JW4A.66 Wang, Xing-Guang - JW4A.97 Trillo, Stefano - JW4A.103 Vermeulen, Diedrik - FW5A.3 Wang, yangyundou - JW3A.8 Tripathi, Renu - JW3A.28, JW3A.7 Veronis, Georgios - JW3A.85 Wang, You - FTu4D.5, JTu3A.112 Trofimov, V.A. - JTu3A.40, JTu3A.58, JW4A.121 Verstraete, Charlotte - JW4A.76 Wang, Yuan - FTh1A.4 Trojak, Oliver - FM2E.2, JW3A.50, JW3A.52 Vianna, Sandra S. - JTu3A.42, JTu3A.98 Wang, Yun - FW6A.3 Truong, Viet G. - FW6B.1 Viegas, Jaime P. - FTu5B.4 Wang, Zhao - FW5A.4 Tsai, Din Ping - JW3A.109 Vigueras-Santiago, Enrique - JTu3A.97 Wang, Zhe - FW5D.1 Tsai, Din Ping - JW3A.110 Villegas, Juan E. - JTu2A.18 Wang, Zhen - FTh2E.1 Tsai, Wei-Yi - JW3A.109 Villeneuve, David - FTh2B.2 Wang, Zheng - JW3A.48 Tsai, Wei-Yi - JW3A.110 Villinger, Massimo - FTh2D.3 Wang, Zhihuan - FM4A.6, FTh2D.2, JW3A.97, Tscheulin, Dieter K. - JTu2A.113 Vinceti, Maria - JTu3A.29, JTu3A.93 JW4A.45 Tseng, Shih - LW6F.4 Vinod, Abhinav K. - FTu5A.3 Wang, Zhou - LTu4F.2 Tseng, Yu-Pei - JTu3A.38 Visser, Taco D. - FW5B.4, JW3A.8 Warren, Zachary - JW3A.7 Tsironis, Giorgos - JW3A.106 Viswanath, Aparna - JTu2A.7 Watad, Ibrahim - FW6C.2 Tsukernik, Alexander - JTu3A.10 Vitebskiy, Ilya - FTh1A.2 Watanabe, Wataru - JTu2A.11|JTu2A.11 Tsurimaki, Yoichiro - JW3A.91 Vivas, Marcelo G. - JW4A.91 Watnik, Abbie - JTu2A.95 Tuan, Tong Hoang - JW4A.77 Vivien, Laurent - JW3A.72 Watts, Michael R. - FTh3B, FW5A.3 Turk, Nina - JW3A.82 Vogt, William C. - FM4D.1, JTu3A.2 Wax, Adam - FW6D.1 Turukhin, Alexey - FW6A.1 Volin, Curtis - FM3E.5 Wear, Keith A. - FM4D.1 Tuthill, Peter - JW4A.84 Volke Sepulveda, Karen - FTu4D.3, LTh3F.2 Weatherill, Kevin J. - FW6B.4 Tyc, Tomáš - JTu2A.44, JTu2A.45 Volpe, Luca - FM2B.4 Webb, Kevin J. - FM4B.3, FM4D.2 Voropaev, Vasilii S. - JTu3A.15 Weeber, Henk - FTh3C.5 U Vo-Van, Truong - FM3A.5 Wegscheider, werner - FM2E.1 Ugalde-Ontiveros, Jorge A. - FM4B.6 Vu, Khu - FTu4A.5 Wei, Chengli - JW4A.9 Ullah, Arif - JW3A.15 Vukusic, Peter - JW4A.76 Weimann, Steffen - FM3B.7, FTh1A.3 Ullah, Sana - JW3A.15 Vulis, Daryl - JW3A.108 Weiner, Andrew M. - FTh3E.3, JW4A.23, JW4A.4 Ulyanov, Vadim - JTu2A.56 Vura-Weis, Josh - LM4F.2, LW5F Weiner, Matthew - JW3A.93 Umakoshi, Takayuki - JW4A.66 Vyas, Khushi - JTu2A.79 Welch, Eric C. - FW6E.3, JTu3A.71 Umashankar, Suchitta - FTu4B.4 Vyas, Reeta - JTu3A.111, JTu3A.7, JW3A.41 Wen, Cai - JW4A.71 Urbas, Augustine - FW5E.1 Vyas, Sunil - JTu3A.88 Wen, Qi - JW4A.88 Usievich, Boris - JW3A.107 Wendt, Joel R. - JW3A.46 Usman, Ahmad - FM3D.1 W Wenner, Brett R. - JTu2A.60 Usuga Castaneda, Mario A. - FTu5D.4, JTu3A.87, Wabnitz, Stefan - FTh2B.4 Wernet, Philippe - LM2F, LM4F.1 JW4A.6 Wade, Christopher G. - FW6B.4 Wesemann, Lukas - JW3A.75 Utsunomiya, Shoko - FM4E.3 Wagner, Hans Peter - JTu3A.49 West, Robert - JTu2A.67 Wagner, Kelvin H. - FW2C.1 Westly, Daron - FM3A.2 V Wahlstrand, Jared K. - FM3B.6, FW6E.2, JTu3A.12, Wetzel, Benjamin - FTh3E.2 VADAPALLI, PAVAN D. - JTu2A.31 JTu3A.45, JTu3A.5, LTh4F.2 Whaley, Birgitta - FM2E.3 Vahala, Kerry - FTu5A.1 Wakunami, Koki - JTu2A.105 Wheatley, Trevor A. - FTh3E.6 Vaida, Mihai - LTu5F Waller, Laura - FM4B.1, FW5B White, Chris D. - JTu2A.45 Vaida, Mihai E. - LTu4F.4 Walmsley, Ian A. - FM3E.2, FW6E.1, JW3A.34, White, Michael G. - LM4F.6 Vainio, Seppo - JTu2A.78 JW4A.16, JW4A.3 Wiebe, Nathan - FM4E.2, FTh3E.7 Vaisseau, X - FM2B.4 Wan, Congshan - JW4A.94 Wiederrecht, Gary - LTh3F.1, LW2F Valentin, Michael - JTu3A.25 WAN, MEHER - FW6C.3 Williams, Ben - FTu4E.3 Valentine, Jason - FM3D.3 Wan, Yuhang - JW3A.51 Williams, Michael J. - JW3A.28 Valini, Felipe - FTu4A.2 Wang, Bing - JW3A.5 Williamson, Ian - JW3A.48 Valle, Cesar L. - FM3D.5 Wang, Bohan - JTu2A.75 Wirth, Jacob H. - JTu2A.95 Vamivakas, Nickolas - JW4A.24, LTh3F.4 Wang, Cheng - JW4A.97 Withford, Michael - JW4A.84 Vampa, Giulio - FTh2B.2 Wang, Cih-Su - LTh3F.3 Witting, Tobias - FW6E.1 Van Cleuvenbergen, Stijn - JW4A.76 Wang, Da-wei - FW5B.3 Wittwer, Valentin - FTh2B.1 van Enk, Steven J. - FM2D.2, JW4A.21 Wang, Detian - JTu2A.76 Wolf, Jean Pierre - FW6E.4 van Gorsel, Rik - FTu5E.1 Wang, Ding - FW6A.1 Wolter, Greg - FW6A.1 Van Stryland, Eric W. - JW3A.9 Wang, Fengfei - FM4B.7 Won, Young jae - JTu2A.87 van Vaerenbergh, Thomas - FTu4D.1 Wang, Han - JW4A.110 Wong, Alexis Carlos G. - JTu3A.42 Vanholsbeeck, Frederique - FM4B, FTu5B.1 Wang, Hongda - FW5D.2 Wong, Chee Wei - FTu5A.3 Varela, O - FM2B.4 Wang, Hongyuan - JTu3A.112 Wood, Joshua - FW5A.5 Varlet, Pascale - FW5D.3 Wang, Hsiang-Chu - JW3A.110 Wood, Michael G. - JW3A.46 Varshney, Ravi K - JTu3A.81 Wang, Jianting - JTu2A.75 Woodbury, Daniel C. - FM2B.1, FM2B.2, JTu3A.12 Varshney, Shailendra K. - FW6C.3, JTu3A.13, Wang, Jianwei - FM4E.2, FTh3E.7 Wozniak, Peter - JTu2A.115, JTu2A.97 JTu3A.22, JTu3A.24, JW4A.102, JW4A.8 Wang, Kai - FTh1A.3, FW2B.1, JW3A.3 Wu, Binlin - FTu5C.3, JTu2A.72 Vartiainen, Ismo - FW5B.4 Wang, Lihui - JTu2A.52 Wu, Chuanwei - JW3A.115 Vasilyev, Michael - FTu4E.2 Wang, Meirong - JTu3A.4 Wu, Guohua - JTu2A.8, JTu3A.94 Vasquez Arzola, Alejandro - FTu4D.3, LTh3F.2 Wang, Po-Hao - JTu3A.88 Wu, JieYun - FW6A.2 Vauderwange, Oliver - JTu2A.115, JTu2A.97 Wang, Qi - JW3A.57 Wu, jinmin J. - JTu2A.102, JTu2A.111 Vayu Nandana Kishore, Pabbisetti - JW3A.112 Wang, Qijie - LTh4F.1 Wu, Pin Chieh - JW3A.110 Veiras, Francisco E. - JTu2A.23 Wang, Qu - JTu2A.96 Wu, Shuhao - JW3A.84 Velev, Vesselin - JW3A.4 Wang, Quanzeng - JTu2A.10, JTu2A.75 Wu, Timothy - FM4D.2 Vella, Anthony - JTu3A.83 Wang, Ruliu - JTu3A.17 Wu, Wentao - JTu3A.109 Verbiest, Thierry - JW4A.76 Wang, Shaokang - JTu3A.57 Wu, Xuejian - FW2E.2

FiO + LS 2017 • 17–21 September 2017 95 Wu, ziling - JTu2A.82 Yue, Zengji - FTu5D.2 Zhang, Yichen - JW4A.33, JW4A.36 Wuytens, Pieter - JW3A.82 Yue, Yong - JTu2A.8 Zhang, yinan - FM3D.6 Wyatt, Adam S. - FW6E.1 Yue, Zengji - FW6C.5 Zhang, Yong - JTu3A.54 Yun, Jeong-geun - JTu2A.25 Zhang, Zhaoyu - FTu4A.4, JW3A.58, JW3A.78 X Yunkin, Vyacheslav - JTu2A.16 Zhang, Zhifeng - FW6B.5 Xiao, Meng - FW2A.2 Yvind, Kresten - FW5A.2 Zhao, Liang - JW4A.75 Xiong, Kun - JTu2A.102 Zhao, Deyin - JW4A.68 Xu, Huizhong - JW3A.94, LW2F.3 Z Zhao, Dongliang - JW3A.115 Xu, Jian - JTu2A.102 Zagursky, Dmitry Y. - JW4A.121 Zhao, Han - JTu2A.86 Xu, Kaichen - JW3A.116 Zahedian, Maryam - JTu3A.27 Zhao, Jianheng - JTu2A.76 Key to Authors Xu, Lei - JW3A.3 Zahedpour Anaraki, Sina - JTu3A.5, LTh4F.2 Zhao, Peng - JW3A.9, LM4F.6 Xu, Tianboyu - JW3A.113 Zahedpour, Sina - FM3B.6, JTu3A.45 Zhao, Qi - FTh2E.1 Xu, Ting - JW3A.119 Zaidi, Aun - JW3A.92 Zhao, Ruogang - JTu2A.86 Xu, Xinrui - JTu2A.15 Zakariya, Abdullah J. - JTu2A.80 Zhao, Wenhui - JW3A.51 Xu, Xunnong - FTh3B.3 Zakharov, Valery - FTu5C.4, JTu2A.4, JTu2A.73, Zhao, Xin - JTu3A.17, JTu3A.74 Xu, Yun - JTu3A.10 JTu2A.74, JTu2A.81 Zhao, Zhi-Chun - JTu2A.102 Xu, Zhe - FM3B.2 Zakharova, Irina G. - JTu3A.40, JW4A.121 Zhao, Zi-Tong - JW4A.12 Xue, Xiaojie - JW4A.106 Zandavi, Seyed Hadi - FM4D.6 Zheng, Xiaorui - JW3A.90 Zaperty, Weronika - FTu4C.3 Zheng, Zheng - JTu3A.17, JTu3A.74, JW3A.51 Y Zarifi, Atiyeh - FTu4A.5 Zherebtsov, Evgeny - JTu2A.78 Yablon, Joshua - LW6F.4 Zeilinger, Anton - FTh3E.5 Zhong, Jiaqiang - FTh2E.1 Yadav, Anupama - JW3A.72 Zeng, Gui H. - JTu2A.93 Zhou, Feng - FW2E.1, JTu3A.50 Yadav, Suchita - JW4A.98 Zeng, Vincent - JW4A.64, JW4A.65 Zhou, Jie - FTu4A.4, JW3A.58 Yadroitsev, Igor - JTu3A.43 Zeng, Yongquan - LTh4F.1 Zhou, Taojie - FTu4A.4, JW3A.58 Yakes, Michael - JW4A.2 Zenin, Volodymyr - JTu2A.12 Zhou, Tingting - JTu2A.104 Yamamoto, Hirotsugu - JTu2A.98 Zeraouli, G - FM2B.4 Zhou, Weidong - JTu3A.55, JW4A.68 Yamamoto, Kenji - JTu2A.105|JTu2A.105 Zerres, Christopher - JTu2A.113 Zhou, Weimin - JW4A.47 Yamamoto, Yoshihisa - FM4E.3 Zeytunyan, Aram - JTu3A.62 Zhou, Xin - FTu4D.5 Yan, Lei - FM3A.3 Zhai, Yao - JW3A.115 Zhou, Yan - FTu5C.3 Yan, Renpeng - JTu3A.109 Zhan, Alan - FM4A.4 Zhou, Zhigang - JTu2A.15 Yang, Dongyue - JTu2A.8, JTu3A.94 Zhan, peng - FM3D.2 Zhou, Zifan - LW6F.4 Yang, Guang-Zhong - JTu2A.79 Zhang, Qiming - FTu5D.2 Zhu, Alexander Y. - JW3A.102, JW3A.80, JW3A.92 Yang, Hao - FW5A.4, JW3A.84 Zhang, Aonan - FM2D.1 Zhu, Chengjie - JTu3A.37 Yang, Jinghui - FTu5A.3 Zhang, Bin - JW3A.94 Zhu, Eric Y. - JTu3A.50 Yang, kui - JTu2A.101 Zhang, Bo - JW3A.57 Zhu, Eric Y. - FW2E.1 Yang, Ronggui - JW3A.115 Zhang, Bosheng - LM3F.4 Zhu, Liguo - JTu2A.76 Yang, Sam - FW5D.2 Zhang, Chen - FTu4E.2 Zhu, Wenqi - JW3A.119, JW3A.87 Yang, Yaping - JTu3A.37 Zhang, Cheng - JW3A.119, JW3A.87 Zhu, Yunhui - JTu2A.82 Yang, Yudong - JTu3A.18 Zhang, Chumei - LM4F.5 Zhu, Zhen H. - JTu3A.90 Yang, Yunyi - FM3D.6, JW3A.90 Zhang, Chunyuan - FTu5C.3, JTu2A.72 Zhu, Zhihua - FM3D.3 Yao, Baoli - JTu3A.4 Zhang, Fan - JW3A.11, JW3A.111, JW3A.22, Zhuo, Zhi-hai - JTu2A.111 Ycas, Gabe - FTu4D.4 JW3A.24 Zi, Fei - FW2E.2 Yelleswarapu, Chandra S. - JTu2A.108, JTu2A.62, Zhang, Feng - JTu2A.102, JTu2A.111 Zimmermann, Felix - FTh1A.3 JTu2A.63, JW4A.80 Zhang, Han - LTh4F.6 Zimmermann, Lars - FM3A.3 Yeola, Sarang - JTu3A.78 Zhang, Hao - JTu2A.103 Zolotovskii, Igor O. - JTu3A.6, JW3A.45, JW3A.53 Yepez, Miztli - JW4A.83 Zhang, Hua - JTu2A.103 Zou, Chang-ling - FTu4B.5 Yilmaz, Hasan - FW5B.2 Zhang, Jitao - JTu2A.84 Zou, Xiao-Qi - FM4E.2 Yin, Longfei - JTu2A.8, JTu3A.94 Zhang, Kaili - LM4F.2 Yin, Siyao - JTu3A.17 Zhang, Lichen - JTu3A.94 Yin, Xiaobo - JW3A.115 Zhang, Lijian - FM2D.1 Yodh, Arjun G. - FM4D.3 Zhang, Lin - JTu2A.72 Yokoyama, Shota - FM3E.3, FTh3E.6 Zhang, Lingxuan - JTu3A.89 Yonezawa, Hidehiro - FTh3E.6 Zhang, Lu - JW4A.22 Yoo, Jinwon - JTu3A.1 Zhang, Peng - JTu3A.4 Yoo, Youngjin - JTu2A.117 Zhang, Qi - JW3A.111 Yoon, Jae W. - JW3A.68 Zhang, Qiang - FTh2E.1 Yoshida, Koji - LW5F.4 Zhang, Qiming - FTu5B.3 Yoshikawa, Jun-ichi - FM3E.3 Zhang, Qingli - JTu3A.109 You, Chenglong - JW3A.85, JW4A.34 Zhang, Rui - JW3A.74 You, Lixing - FTh2E.1 Zhang, Ruoyu - JTu2A.24, JW4A.55 Young, Laura - JTu2A.42 Zhang, Tiancai - JW3A.24 Yu, Hang - JTu3A.112 Zhang, Wei - JTu3A.112 Yu, Haoyi - FTu5D.2 Zhang, Weijun - FTh2E.1 Yu, Miao - FTh3A.5 Zhang, Wenfu - JTu3A.89 Yu, Mingbin - FTu5A.3 Zhang, Wenhui - JTu2A.103 Yu, Ping - FM4B.7 Zhang, Xiang - FTh1A.4 Yu, Song - JW4A.33, JW4A.36 Zhang, Xiaoshi - LM3F.4 Yu, Xinguang - FTu5C.3 Zhang, Yadong - JTu3A.61 Yu, Yan - JTu3A.27 Zhang, Yan - FM3C.6 Yu, Yi - FW5A.2 Zhang, Yanbing - FTh3E.2 Yuan, Luqi - FW5B.3 Zhang, Yanfeng - JW4A.40 Yuan, Xiao - FTh2E.1 Zhang, Yibo - FW5D.2

96 FiO + LS 2017 • 17–21 September 2017

Table of Contents