Table of Contents

Schedule-at-a-Glance ...... 2 FiO + LS Chairs’ Welcome Letters ...... 3 General Information ...... 5 Conference Materials Access to Technical Digest Papers ...... 6 FiO + LS Conference App ...... 6 Plenary Session/Visionary Speakers ...... 7 Science & Industry Showcase Science & Industry Theater Programming ...... 11 Poster Session and Dynamic E-Posters ...... 11 Participating Companies ...... 12 OSA Member Zone ...... 14 Awards, Honors and Special Recognitions FiO + LS Awards Ceremony & Reception ...... 15 OSA 2018 Awards and Honors ...... 15 APS/DLS 2018 Awards and Honors ...... 20 OSA Foundation 2018 Prizes and Special Recognitions ...... 21 Special Events ...... 23 FiO + LS Committees ...... 27 Explanation of Session Codes ...... 29 FiO + LS Agenda of Sessions ...... 31 FiO + LS Abstracts ...... 35 Key to Authors and Presiders ...... 92

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/DLS thank the following sponsors for their generous support of this meeting:

FiO + LS 2018 • 16–20 September 2018 1

2018FiO Front.indd 1 8/20/18 9:07 AM 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 16 September 17 September 18 September 19 September 20 September

GENERAL

Registration 16:00–19:00 07:00–17:30 07:00–18:00 07:30–18:00 07:30–11:00

Speaker Preparation Room 16:00–19:00 07:00–17:30 07:00–17:30 07:30–17:30 07:30–11:00

Coffee Breaks 10:00–10:30 09:30–10:00 10:00–10:30 10:00–10:30 16:00–16:30 13:30-14:00 13:30-14:00

PROGRAMMING

Technical Sessions 08:00–16:00 15:00–18:15 08:00–18:00 08:00–12:30

Visionary Speakers 08:30–11:15 09:15–10:00 09:15–10:00

LS Symposium on Undergraduate Research 12:00–18:00

Plenary Session 08:00–09:30

Postdeadline Paper Sessions 19:00–21:00

SCIENCE & INDUSTRY SHOWCASE 09:30–15:00 10:00–15:00

Science & Industry Theater Programming, See page 11 10:00–15:00 10:15–15:00 for complete schedule .

Poster Sessions and DynamicE–Posters 10:00–12:00 10:00–12:00 13:00–15:00 13:00–15:00

OIDA VIP Industry Leaders Networking Speed 12:00–13:00 Meeting Lunch

SPECIAL EVENTS

Women of Light, a Special Program for Women in 08:00–16:00 Optics

OSA Technical Group Events 12:30–13:30 16:00–19:00

Meet OSA’s Journal Editors 16:00–17:00

DLS Annual Business Meeting 16:00–17:00

Career Development Programming 16:00–18:30

Unconscious Bias Workshop 18:00–19:00

Awards Ceremony & Reception 18:00–21:00

OSA Annual Business Meeting 17:30–18:15

Conference Reception 18:30–20:30

OSA Family and Friends Tour 10:00–12:00

Meet the Physical Review Journal Editors Reception 15:30–17:00

Capitol Hill Visits 10:00–16:00

2 FiO + LS 2018 • 16–20 September 2018

2018FiO Front.indd 2 8/20/18 9:07 AM Welcome to FiO + LS 2018

Whether you are in an autonomous vehicle looking to avoid collisions with nearby objects or rambling in a won- derland with a virtual reality/augmented vision device, the Frontiers in Optics + Laser Science APS/DLS (FIO + LS) offers something for you . We are pleased to welcome you to Washington, D .C ., the home of The Optical Society and The American Physical Society - Division of Laser Science .

This year’s conference experience continues to be 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 2018 .

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 stunning technology . Our plenary speakers, Heike E . Riel from IBM Research Frontiers Institute will share her research activities in the field of information technology and present the new paradigms of cognitive hardware technologies and quantum computing and Gerard Mourou from École Polytechnique will discuss the development of petawatt laser pulse compression and the generation of a single-cycled X-ray pulse leading to exawatt and zeptosecond science and technology . In addition, seven Visionary Speakers who have been paired with four themes will join to share their visions on the cutting-edge ad- vances in the four dimensions: Automotive, Nanophotonics and Plasmonics, Quantum Technologies, and Virtual Reality and Augmented Vision .

While at FiO + LS, we encourage you to visit the 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 . This year we have added additional programing in the theater . Take the time to learn about new products, find technical and business solu- tions and gain the most up-to-date market perspective of your industry .

Again, we welcome you to FiO + LS 2018 and encourage you to enjoy the dynamic programming incorporated into the next few days ahead .

With best regards, Christoph Harder and Wei Lee

Christoph Harder Wei Lee FiO General Chair FiO General Chair Swissphotonics, Switzerland National Chaio Tung University, Taiwan

FiO + LS 2018 • 16–20 September 2018 3

2018FiO Front.indd 3 8/20/18 9:07 AM Welcome to Laser Science 2018

The leadership of the Division of Laser Science (DLS) of the American Physical Society (APS) is pleased to welcome you to our 34th annual meeting, Laser Science (LS) 2018, in Washington, D .C . We are grateful for the help of our colleagues and technical program organizers, Peter Delfyett and Nathan Newbury, 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 at 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 Monday, which showcases the work of some of our youngest scientists . The Symposium will feature a special poster session to present the work of undergraduate researchers .

The technical sessions for the Laser Science meeting are organized around several broad themes: Quantum Science; Extreme Laser Science; Nanophotonics and Plasmonics; and Precision Spectroscopy .

We welcome you to the Laser Science 2018 Meeting and encourage you to take full advantage of this year’s technical sessions, visionary and plenary talks, as well as the Science & Industry Showcase featuring leading suppliers to the laser science community, Rapid-fire Oral Presentations and Poster Sessions including e-posters .

Enjoy! Peter and Nate

Peter Delfyett Nathan Newbury LS Chair LS Chair University of Central Florida, USA National Institute of Standards & Technology, USA

4 FiO + LS 2018 • 16–20 September 2018

2018FiO Front.indd 4 8/20/18 9:07 AM General Information General Information Registration Special Needs Terrace Level Foyer If you have a disability and require special accommodations to fully participate in this conference, please contact Con- Sunday, 16 September 16:00–19:00 ference Management at the registration desk . Your specific Monday, 17 September 07:00–17:30 needs will be addressed . Tuesday, 18 September 07:00–18:00 Wednesday, 19 September 07:30–18:00 OSA Code of Conduct Thursday, 20 September 07:30–11:00 It is the policy of The Optical Society that all forms of discrimination and harassment, sexual or otherwise, are prohibited in any OSA or OSA-managed events or activities . Speaker Preparation Room All Conference guests, attendees, and exhibitors are subject Albright to OSA’s Code of Conduct policy, the full text of which is available at www .osa org/codeofconduct. . Conference man- Presenters are encouraged to stop by the Speaker Prepara- agement reserves the right to take any and all appropriate tion Room during registration hours to test their presenta- actions to enforce the Code of Conduct, up to and including tions prior to their session . The room will be equipped with ejecting from the Conference individuals who fail to comply laptops, LCD projectors, and screens . with the policy .

Media Room OSA CAM Lounge Convention Office on Concourse Level Boundary A staffed media room is available for credentialed mem- We’re Celebrating All Members (CAM) bers of the media . Badges for pre-registered reporters and with quick interviews that highlight you! reporter registration are in the media room along with media All OSA members are invited to stop by kits, internet connectivity, printers, a quiet work space, and the CAM Lounge to be filmed talking conference information . about what inspired them to pursue their current work, and what excites them Monday, 17 September 12:00–17:00 most about what they do . The collection of these short videos will be featured on Tuesday, 18 September 08:00–17:00 OSA’s website, social media, and at various conferences . Wednesday, 19 September 08:00–17:00 Thursday, 20 September 08:00–12:00 Monday, 17 September 08:00-17:00 Tuesday, 18 September 08:00–17:00 WiFi Access Instructions Wednesday, 19 September 08:00–17:00 To access the complimentary WiFi services during the FiO + LS Conference, please use the following login information . APS Booth SSID: FIOLS2018 Science & Industry Showcase, Booth #205 Password: FIOLS2018 Founded in 1899, the American Physical Society (APS) is a non-profit membership First Aid and Emergency Information organization working to advance and diffuse the knowledge of physics . APS publishes the In the event of an emergency at the Washington Hilton, world’s most widely read physics research and please dial #60 from any courtesy phone . If you happen to review journals: Physical Review Letters, Physical Review X, dial 911 on your own, please call #60 as well to inform the Reviews of Modern Physics, Physical Review A-E, Physical hotel about the emergency . Review Accelerators and Beams, Physical Review Applied, Physical Review Fluids, Physical Review Materials, Physical Lost and Found Review Physics Education Research, and Physics. Please stop by our table near Registration to learn more about the For lost and found please check first at the conference prestigious Physical Review collection and our newest registration desk . Please put your name on all conference journal Physical Review Materials, a new broad-scope materials (including your Conference Program), as they will international journal for the multidisciplinary community only be replaced for a fee . engaged in materials research .

FiO + LS 2018 • 16–20 September 2018 5

2018FiO Front.indd 5 8/20/18 9:07 AM Conference Materials 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 2018 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 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

Conference Materials Conference Exhibit Buyers’ Guide Search for conference presentations by day, topic, speaker After careful consideration, Show Management has decided or program type . Plan your schedule by setting bookmarks to take the FiO + LS Buyers’ Guide GREEN . Attendees will on programs of interest . Technical attendees can access be directed to the Conference App to access exhibiting technical papers within session descriptions . companies’ detailed information . In addition, you’ll find all exhibitors listed on page 12 in this book . Science & Industry Showcase Search for exhibitors or view the complete list . Bookmark Conference Program Update exhibitors as a reminder to stop by their booth . Tap on the map icon within a description, to find their location on the Technical program changes will be communicated in the on- show floor map . site Conference Program Update Sheet distributed with your onsite registration materials . In addition, all updates will be Access Technical Digest Papers made in the FiO + LS conference app . Check daily for new Full technical registrants can navigate directly to the tech- information and/or reference the FiO + LS conference app . nical papers right from the FiO + LS conference app . Locate the session or talk in “Event Schedule” and click on Poster Presentation PDFs the “Download PDF” link that appears in the description . IMPORTANT: You will need to log in with your registration Authors presenting posters have the option to submit the email and password to access the technical papers . Access is PDF of their poster, which will be attached to their papers in limited to Full Conference attendees only . OSA Publishing’s Digital Library . If submitted, poster PDFs will be available about three weeks after the conference end Need assistance? date . While accessing the papers in OSA Publishing’s Digital Contact our support team, available 24 hours a day Monday Library, look for the multimedia symbol . through Friday, and from 09:00 to 21:00 EDT on weekends, at +1 .888 .889 .3069 option 1 .

Join the Social Conversation at FiO + LS! We will be tweeting about program highlights and the latest updates throughout the conference . Fol- low @OpticalSociety on Twitter and tweet about your conference experience using #FIO18 in your tweets . Join the conversation!

6 FiO + LS 2018 • 16–20 September 2018

2018FiO Front.indd 6 8/20/18 9:07 AM Conference Plenary Session Plenary Presentations Tuesday, 18 September, 08:00–09:30 International Ballroom Center Heike E. Riel Gérard Mourou IBM Research Frontiers Institute, École Polytechnique, France Switzerland Chirped Pulse Amplification to ELI and The Future of Computing Beyond Extraordinary enhancements in com- PW laser could be compressed into puting power over the last 50 years high-energy single-cycled laser pulse, have been driven by “smaller & denser” offering a fundamentally new laser-matter resulting in “faster & cheaper” . The interaction ambit, which could become quest for ever-increasing computing the fulcrum of novel scientific and performance continues . This raises the societal applications . Among them, we fundamental question of ‘what is next?’ Today, the most foresee efficient laser electron and ion acceleration, as well exciting new frontiers of information technology are non-von as the generation of a single-cycled X-ray pulse leading to Neumann computing and quantum computing . This talk Exawatt and zeptosecond science and technology . will give an overview of our research activities in the field of About the Speaker: extending the core technology roadmaps and in the new Gérard Mourou, recipient of the 2018 paradigms of cognitive hardware technologies and quantum Arthur L . Schawlow Prize in Laser Science and the 2016 computing . Frederic Ives Medal/Jarus W . Quinn Prize, is Professor Haut-Collége at the École Polytechnique . He is also the About the Speaker: Heike E . Riel is Executive Director A .D . Moore Distinguished University Emeritus Professor of of the IBM Research Frontiers Institute, and Director of the University of Michigan . He received his undergraduate IoT Technology & Solutions, Switzerland . In 2013, Dr . Riel education at the University of Grenoble (1967) and his Ph .D . became an IBM Fellow, achieving the company’s highest from University Paris VI in 1973 . Plenary Session technical distinction, and became a member of the IBM Academy of Technology . Her research interests include He has made numerous contributions to the field of ultra- nanoscale materials and novel device concepts for applica- fast lasers, high-speed electronics, and medicine . His most tions in electronics, optoelectronics, and energy harvesting . important invention, developed with Donna Strickland while Dr . Riel studied physics at the Friedrich-Alexander University at the University of Rochester (N .Y .), is the laser amplifica- of Erlangen-Nuremberg (), and received her Ph .D . tion technique known as Chirped Pulse Amplification (CPA), in 2003 from the University of Bayreuth (Germany) for her a method that is universally used today . CPA’s attosecond work on the optimization of multilayer organic light-emitting pulse generation and compact particle accelerators made devices . After an internship at the Hewlett-Packard Research possible the generation of extremely high laser intensities, Laboratory in Palo Alto, California, she joined IBM Research making a new branch of optics possible . Zurich in 1997, first as a diploma student, then as a Ph .D . In 2005, Prof . Mourou proposed a new infrastructure, student before becoming a Research Staff Member in 2003 . Extreme Light Infrastructure (ELI), which is distributed over From 2008 to 2014, Dr . Riel led the Nanoscale Electronics three pillars located in the Czech Republic, Romania, and Group before moving to the Materials Integration and Na- Hungary . Prof . Mourou also pioneered the field of femto- noscale Devices group . In 2003, Dr . Riel was named as one second ophthalmology that relies on a femtosecond laser of the world’s Top 100 Young Innovators by MIT Technology for precise myopia correction and corneal transplants . Over Review . Since then, she has gone on to receive the Applied a million such procedures are now performed annually . Physics Award from the Swiss Physical Society, and the Swiss Prof . Mourou is member of the U S. . National Academy of Association of Women in Engineering Innovation Award . In Engineering, an OSA Fellow, and a foreign member of the 2015 Dr . Riel was elected to the Swiss Academy of Engineer- Russian Science Academy, the Austrian Sciences Academy, ing Sciences, to the Leopoldina, and to the German National and the Lombardy Academy for Sciences and Letters . He is Academy of Sciences . In 2016 she was awarded an honorary Chevalier de la Légion d’honneur . doctorate from the Faculty of Engineering at Lund University (Sweden) .

FiO + LS 2018 • 16–20 September 2018 7

2018FiO Front.indd 7 8/20/18 9:07 AM Visionary Speakers

Monday, 17 September, 08:30–11:15 tions, coordination with technology provider, suppliers and customer contacts . Teri Odom, Northwestern University, Källhammer started 30 years ago with Machine Vision in USA automotive manufacturing at Borg Warner Corporation in Theme: Nanophotonics and Plasmonics Des Plaines, Illinois . He has also several years of experience with high-speed cameras and data analysis in automotive Peering through the Looking Glass: crash tests . In 1995 he joined Autoliv AB, Sweden — the The Next Frontier in Nano-optics world’s largest supplier of airbag and seat-belt systems — Over the past decade, significant responsible for corporate funded research and development progress in controlling light-matter projects . There he launched active safety in the late 1990s . interactions at the nanoscale has been He is now with Veoneer — the electronics spin-off from achieved . Most of the advances, however, have relied on Autoliv . Källhammer has a PhD in Cognitive Systems from fixed systems limited to as-fabricated nanostructures and the department of Information and Computer Science at singly periodic arrays and simple unit cells . This visionary talk Linköping University, Sweden, an M S. . In E .E . from Duke will discuss how the ability to engineer complex nanopho- University, and a an MS in mechanical engineering from tonics responses—on demand—may address key challenges Luleå Technical University, Sweden . He has co-authored 29 and open unexpected possibilities in nanoscale optics . We articles and conference papers and has 19 patent proposals will highlight new designs in topological photonics, stimu- or granted patents . li-responsive nanostructured substrates for tunable nano-las- ing and reconfigurable lensing, and prospects of multi-peri- Prem Kumar, Northwestern University, odic structured materials . USA About the Speaker: Teri W . Odom is Charles E . and Emma Theme: Quantum Technologies H . Morrison Professor of Chemistry, Professor of Materials Quantum Communication and Net- Science and Engineering, and Associate Director of the working International Institute of Nanotechnology (IIN) at North- western University . She is an expert in designing structured Machines that process quantum infor- nanoscale materials that exhibit extraordinary size and mation are likely to be commercially shape-dependent optical properties . Odom has pioneered a available in the near future . Networking suite of multi-scale nanofabrication tools that have resulted them via quantum communication to achieve a higher level in flat optics that can manipulate light at the nanoscale and of performance is a topic of current interest . In this talk I beat the diffraction limit, -based nanoscale lasers will review the current status and speculate on the future that exhibit tunable color, and hierarchical substrates that possibilities . show controlled wetting and super-hydrophobicity . She has About the Speaker: Prem Kumar is Professor of Information also invented a class of biological nanoconstructs that are Technology in the Robert R . McCormick School of Engineer- facilitating unique insight into nanoparticle-cell interactions ing and Applied Science at Northwestern University . His and that show superior imaging and therapeutic properties primary research focus is on photonic devices and their ap- because of their gold nanostar shape . plications utilizing the principles of nonlinear and quantum optics . In particular: generation, distribution, and ultrafast Jan-Erik Källhammer, Veoneer, Inc., processing of photonic entanglement for applications in Sweden quantum information networks; novel quantum light states Theme: Automotive for precision measurements, imaging, and sensing; and novel optical amplifiers and devices for networked classical From Night Vision to LiDAR: An Auto- optical communications . motive Perspective Earlier this year, Kumar returned to Northwestern after Work is underway to complement camer- Visionary Speakers spending four years at DARPA, where he served as a as and radar with LiDAR in serial automo- Program Manager in the Defense Sciences Office . Prior tive use . There are many considerations to joining DARPA, he served on the National Academies besides technical challenges to be made before LiDAR can Committee that issued the 2012 landmark study: “Optics be launched as a serial product . The talk will draw on experi- and Photonics: Essential Technologies for Our Nation,” ences of taking Night Vision to the automotive market . which spawned the National Photonics Initiative . Kumar is a About the Speaker: Jan-Erik Källhammer has almost 20 Fellow of the OSA, APS, IEEE, IoP (UK), AAAS and SPIE . He years’ experience with automotive active safety develop- has been a Distinguished Lecturer for the IEEE Photonics ment . He was responsible for the inception and develop- Society, Hermann A . Haus Lecturer at MIT, recipient of the ment of a Night Vision Drivers Vision Enhancement based on Quantum Communication Award from Tamagawa University an uncooled long-wave infrared camera . The system is now in Tokyo, Japan, and the Walder Research Excellence Award on the market in Audi, BMW, Cadillac, Mercedes, Peugeot from the Provost’s office at Northwestern University . and some luxury cars . Current works focus on visual en- hancement in darkness and inclement weather (Night Vision, LiDAR, gated imaging) . Key aspects are functional specifica-

8 FiO + LS 2018 • 16–20 September 2018

2018FiO Front.indd 8 8/20/18 9:07 AM Wednesday, 19 September, 09:15–10:00 Thursday, 20 September, 09:15–10:00

Mark Bolas, Microsoft Corp., USA David DeMille, Yale University, USA Theme: Virtual Reality and Augmented Activities Shaping the Wavefront of Vision Nanophotonics Bending Light to Bend Reality Remarkably, certain ultra-precise spectro- scopic measurements are sensitive to the As we dive head-first into the new me- existence of certain new, yet-undiscov- dium of mixed reality, we find that the ered particles whose mass far exceeds ability to bend light is central to the pal- that of the recently discovered Higgs ette of mixed reality systems and content boson . This talk will describe ongoing designers as they bend the reality that is ultimately formed and future examples of such measurements, including the in the user’s mind . This talk will look backward and forward in ACME experiment, a search for the electron’s electric dipole time to explore just how messy that process has been, and moment . how much messier it will become . About the Speaker: David DeMille is a Professor of Physics About the Speaker: Mark Bolas is a researcher exploring at Yale University . DeMille received his PhD from the Uni- perception, agency and intelligence . He is a Professor of versity of California, Berkeley in 1994 and joined the faculty Interactive Media in the USC Interactive Media Division, at Yale in 1998 . He is the recipient of awards including the USC School of Cinematic Arts at the University of Southern Francis M . Pipkin Award of the American Physical Society California, Director of their Interactive Narrative and Immer- (APS) (2006), the Cottrell Scholars Award from Research sive Technologies Lab, Director of Mixed Reality Laboratory Corporation (2000), a Sloan Foundation Fellowship (2000), at USC’s Institute for Creative Technologies, and chairman and a Packard Foundation Fellowship (1999), and he was of Fakespace Labs in Mountain View, California . Bolas is named a Fellow of APS in 2005 . DeMille’s research interests currently on leave from USC, working on the Hololens team span a wide range of topics in atomic, molecular and optical at Microsoft . physics . For example, he and his group have developed In 1988, Bolas co-founded Fakespace Inc . with Ian McDowall pioneering techniques that use polar molecules to enhance and Eric Lorimer to build instrumentation for research labs the sensitivity of precision measurements to fundamental to explore virtual reality . This work resulted in the invention symmetry-violating effects . In parallel, DeMille and his group of display and interaction tools used by many VR research have developed methods for laser cooling and trapping and development centers around the world, including the of diatomic species . They have proposed many potential BOOM (Binocular Omni-Orientation Monitor), the Pinch applications for ultracold molecules, such as for quantum in- glove, the RAVE, the PUSH, and VLIB software . Bolas was formation processing and for next-generation electric dipole awarded the IEEE VGTC Virtual Reality Technical Achieve- moment searches, including a search for the electric dipole ment Award for 2005 in recognition of seminal technical moment of the proton . achievement in virtual and augmented reality . Sir Peter Knight, Kavli Royal Society Mark Brongersma, Stanford University, International Center, UK USA Theme: Quantum Technologies Theme: Nanophotonics and Plasmonics Quantum Technology for a Networked Activities Shaping the Wavefront of World Speakers Visionary Nanophotonics I will describe the worldwide efforts to In the field of nanophotonics we aim to develop quantum technology, exploiting manipulate the flow of light using opti- coherence and superposition . A second cally resonant nanostructures . I will share quantum revolution is emerging with electronic and photon- my personal perspective on a number of exciting recent ic devices that use quantum science, harnessing our ability developments in the field that are transforming the way we to interact with atoms, photons and electrons with exquisite create new optical materials and devices . level of control and with transformative potential for technol- ogy . About the Speaker: Mark Brongersma is a Professor in the Departments of Materials Science and Applied Physics at About the Speaker: Sir Peter Knight is Senior Fellow in Stanford University . He leads a research team of ten students Residence at the Kavli Royal Society International Centre and five postdocs . Their research is directed towards the at Chicheley Hall and a past President of the Institute of development and physical analysis of new materials and Physics and of The Optical Society . Knight retired at the end structures that find use in nanoscale electronic and photonic of September 2010 as Deputy Rector (Research) at Imperial devices . He received a National Science Foundation Career College where he was responsible for the college’s research Award, the Walter J . Gores Award for Excellence in Teach- strategy . He retains his Professorship of Quantum Optics at ing, the International Raymond and Beverly Sackler Prize in Imperial . His research centers on theoretical quantum optics the Physical Sciences (Physics) for his work on plasmonics, and quantum information science . He has a strong interest in and is a Fellow of OSA, SPIE, and APS . Brongersma received fostering multidisciplinary research and set up the Grantham his PhD from the FOM Institute AMOLF in Amsterdam, The Institute for Climate Change and other centers at Imperial Netherlands, in 1998 . From 1998-2001 he was a postdoctor- College London . al research fellow at the California Institute of Technology .

FiO + LS 2018 • 16–20 September 2018 9

2018FiO Front.indd 9 8/20/18 9:07 AM He is a Thomson-ISI “Highly Cited Author” . He was knighted in the Queen’s Birthday Honours List in 2005 for his work in optical physics . Knight was chair of the Defence Scientific Advisory Council at the UK Ministry of Defence until 2010 and was a member of the Science and Technology Facilities Council until 2012 . He continues to be involved in advising government on science issues . Knight was Chief Scientific Advisor at the UK National Physical Laboratory until the end of 2005 and currently chairs their Quantum Metrology Insti- tute . He is also a Board member of the UK National Quan- tum Technology Initiative . He led, with Sir Mark Walport, the Government Office of Science Blackett Report in Quantum Technology in 2016 . He has won a number of prizes and awards including the Thomas Young Medal and the Gla- zebrook Medal of the Institute of Physics, the Royal Medal of the Royal Society, and the Frederic Ives Medal/Jarus W . Quinn Prize of The Optical Society, as well as Honorary Doc- torates from a number of universities including most recently Birmingham . He is currently a member of the Millennium Prize Jury at TAF, Finland . Visionary Speakers

10 FiO + LS 2018 • 16–20 September 2018

2018FiO Front.indd 10 8/20/18 9:07 AM Science & Industry Showcase

Tuesday, 18 September, 09:30–15:00 Rapid Fire Oral Presentations RAPID Wednesday, 19 September, 10:00–15:00 Held in the Theater during the first hour of each poster Columbia, Terrace Level session, a select number of poster presenters offer Rapid-fire The FiO + LS Science & Industry Showcase hosts exhibit- Oral Presentations, which consist of a brief oral presentation ing companies partnered with innovative demonstrations, accompanied by slides . This format enables poster pre- networking events, poster presentations, e-posters and senters to preview key results from their research in brief, Rapid-fire Oral Presentations . Learn about new products, three-minute segments . In the session’s second hour, pre- find technical and business solutions and gain the most up- senters are available for more in-depth discussions adjacent to-date market perspective of your industry . Don’t miss this to their accompanying posters . View the poster sessions in opportunity to visit companies representing a broad range the abstracts for the the symbol indicates Rapid-fire Oral of the best products and applications in the optics and pho- Presentations . tonics industry . There is no charge to attend the Showcase— it is open to all registered attendees! Entrepreneur - That’s French for Crazy Person Poster Sessions & E-Posters E-Poster Tuesday, 18 September, 10:00–12:00, 13:00–15:00 Serial entrepreneur and seasoned executive, Sujatha Ra- Wednesday, 19 September, 10:00–12:00, 13:00–15:00 manujan will share her philosophy on creating a successful start-up with an emphasis on building the right team, under- Attend the Poster Sessions and view more than 500 posters standing your market and ensuring your technology, solution scheduled for presentation . Poster presentations communi- or product gives you an advantage over others . She will cate new research findings in an intimate setting that encour- share information on Luminate (the world’s only accelerator ages lively and detailed discussion between presenters and for optics, photonics, and imaging) and its focus on bringing attendees . visionary entrepreneurs from around the globe together with A select number of presentations will be offered as e-post- OPI pioneers and qualified investors to help start-ups speed ers—which supplements the author’s introduction, motiva- innovation and time to market . She also detail how entre- tion, results and conclusions with digital capabilities that aid preneurs can apply to be a part of Luminate’s next cohort deeper discussion . Look for the symbol to see who will be by Sept . 24 . Sujatha Ramanujan is a Managing Director at presenting e-posters . Luminate Accelerator, USA .

Science & Industry Showcase Theater A Look toward the Future — Remarks from the OSA President Tuesday, 18 September Under the leadership of OSA President Ian Walmsley, the 09:45–10:45 Rapid Fire Oral Presentations 1 Society has engaged in scenario planning that will shape the 10:50–11:40 Entrepreneur - That’s French for Crazy future of the Society . What are the biggest disruptors facing Person The Optical Society in 2030? What are new products and member services that the Society will offer in 2030? OSA is 11:45–12:00 A Look toward the Future — Remarks seeking your input . Join President Walmsley and members from the OSA President of the Board of Directors for an engaging presentation and 12:00–13:00 Job Seeker Tutorial - discussion focused on the professional society of the future . WORKinOPTICS .com 13:00–14:00 Rapid Fire Oral Presentations 2 Job Seeker Tutorial - WORKinOPTICS.com 14:05–15:00 Leveraging LinkedIn – Building Attend this session and learn how to navigate the WORK- Relationships, Attracting Recruiters, inOPTICS career board and maximize your chances of Finding the Best Jobs and Growing Your getting the perfect job . WORKinOPTICS is the global talent Network hub for optics and photonics professionals . Start your search Wednesday, 19 September today . Science & Industry Showcase 10:15–11:15 Rapid Fire Oral Presentations 3 11:15–12:15 Frontiers in Funding 12:20–12:55 Enabling and Entangling: the Tools to Innovate in Quantum Technology 13:00–14:00 Rapid Fire Oral Presentations 4 14:05–15:00 Understanding the National Quantum Initiative

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2018FiO Front.indd 11 8/20/18 9:07 AM Leveraging LinkedIn – Building Demonstration Areas Relationships, Attracting Recruiters, Finding the Best Jobs and Growing Your VR, AR and MR Headsets Demo Network The current and future technologies of VR, AR and MR will be feature during the Virtual Reality and Augmented Vision Networking is the primary way people build relationships Theme sessions . During the Science & Industry Showcase to learn about unadvertised career opportunities, get their attendees can experience this technology hands on by foot in the door at a company, and grow their professional taking part in the VR, AR, MR Demo Area . The following contacts . LinkedIn is a fantastic tool to accomplish all of headsets will be available for attendees to experience . these goals . LinkedIn is, by far, the most popular social me- dia platform used by professionals in the workforce, as well In addition to an invited program of speakers and a visionary as recruiters looking to fill open positions . Learning how to talk, you will find the following headsets for live demonstra- create and present a strong LinkedIn profile is essential for tions in the showcase area: building relationships, developing a professional network, VR headsets: establishing your brand and thought leadership, and finding - Oculus CV1 new career opportunities . As LinkedIn frequently enhances - Oculus Go its platform to offer new features, this workshop will also in- - HTC Vive troduce any new tools and features that will benefit LinkedIn users . The speaker is Josh Henkin, STEM Career Services, AR headsets: USA . - Hololens - Lenovo Frontiers in Funding - Mira Come to the FiO Registration desk to sign up for a 15-min- This program, featuring representatives from funding agen- ute demo slot . cies, will provide attendees with the opportunity to hear about the latest in science funding with a focus on the con- ference themes . Throughout the exhibit attendees will be Vehicle Equipped with Ouster LIDAR Demo able to further explore and discuss opportunities at agency Ouster will host live demonstrations of an OS-1-64 LIDAR alley on the show floor . sensor mounted on a vehicle on the exhibit floor, highlight- ing its panoramic imaging capabilities, high spatial acuity, Enabling and Entangling: the Tools to and small form factor . Ouster is a leading developer of LI- DAR and perception technology for the autonomous vehicle Innovate in Quantum Technology. and robotics sectors . The company’s flagship product, the This presentation will be delivered by Vincent Tagliamonti OS-1-64, provides industry leading performance, scalability, from TOPTICA Photonics . View the Conference App for a reliability, and form factor . Ouster’s corporate headquarters complete description . and manufacturing facility are located in San Francisco . For more information, visit www .ouster .io/ . Understanding the National Quantum 2018 Participating Companies: Initiative (as of 16 August 2018) The U .S . is getting serious about quantum research and American Institute of Physics Booth 313 technology . Several bills have been introduced in Congress www aip. org. to advance this area of research, and two of which would create a large new coordinated federal effort cutting across American Physical Society Booth 205 academia, laboratories, and Industry . Join this session to www aps. .org learn from where this National Quantum Initiative originated, how it would be structured, and how you can get involved to asphericon, Inc . Booth 214 support it . www asphericon-inc. .com Dark Field Technologies Booth 209 OIDA VIP Industry Leaders Speed www darkfield. .com Meetings Lunch Energetiq Technology Booth 305 Wednesday, 19 September, 12:00–13:30 www energetiq. com. Science & Industry Showcase Hamamatsu Corporation Booth 404 This session brings together industry executives to share www hamamatsu. .com their business experience with early career professionals, Inrad Optics Booth 301 recent graduates and students . Learn how they started their www inradoptics. .com careers, lessons learned and how they are using their de- grees in executive positions . Informal networking over lunch Liquid Instruments Booth 219 is followed by a transition to “speed meetings” — brief, www liquidinstruments. .com small-group visits with each executive to discuss industry Luminate Booth 303 trends or career topics . www nextcorps. org. Science & Industry Showcase Sponsored by

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2018FiO Front.indd 12 8/20/18 9:07 AM M Squared Lasers, Ltd . Booth 210 www .m2lasers .com Menlo Systems Booth 309 www .menlosystems com. Newport Corporation Booth 221 www .newport .com NKT Photonics Booth 203 www .nktphotonics .com Optimax Systems, Inc . Booth 201 www .optimaxsi .com OptoSigma Corporation Booth 315 www .optosigma com. OSA Member Zone Booth 213 www .osa .org/membership OSA - The Optical Society Terrace Foyer www .osa .org Ouster, Inc . Booth 200 www .ouster .io PHASICS Corporation Booth 308 www .phasicscorp .com Photonics Media Booth 318 www .photonics com. Santec USA Corporation Booth 311 www .santec .com SPIE Booth 417 www .SPIE .org Springer Booth 419 www .springer .com Synopsys, Inc . Booth 302 www .synopsys com/optical-solutions. Thorlabs Booth 400, Sponsor www .thorlabs com. Tianjin University Booth 304 www .tju .edu .cn WORKinOPTICS Booth 421 www .WORKinOPTICS .com Zygo Corporation Booth 212 www .zygo .com Science & Industry Showcase

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2018FiO Front.indd 13 8/20/18 9:07 AM OSA Member Zone

OSA Member Zone – Booth 213 OSA Publishing (OSAP) provides the largest collection of peer-reviewed optics and photonics content in the world Tuesday, 18 September 09:45-15:00 and hosts more than 370,000 articles from 18 publications, as well as conference papers from more than 775 meetings . Wednesday, 19 September 10:00-15:00 EXCITING NEWS – OSAP has launched a new, inclusive, rapid-publication, Open-Access journal entitled OSA Con- Through its world-renowned publications, meetings and tinuum . OSA Continuum publishes articles that meet OSA’s OSA Member Zone membership programs, OSA provides quality information high standards for technical accuracy, scientific rigor, and and inspiring interactions that power achievements in the presentation quality and without judgment on impact or science of light . More than 21,000 Members, residing in significance . over 100 countries and spanning academic, government and industry, call OSA their professional home . OSA Technical Groups offer members the chance to All members are invited to stop by the OSA Member Zone connect with colleagues in their area of expertise through to meet OSA staff, and learn more about our publications, innovative events and focused networking opportunities . conferences and meetings, and membership for individuals Both in person and online events are planned throughout and companies . Not a member? Definitely stop by and the year . Have an idea for your technical group? Bring it the learn more about OSA! All conference attendees who Zone! Looking to engage with a technical group while at join or renew as an Individual 1-year member will receive FiO? Browse the special events on the conference app for a 50% off the cost of annual dues. list of technical group events or visit www osa. .org/TGevents . Staff and/or volunteer members from the following six division will be in the OSA Member Zone to answer your OSA Member Recognition Events questions, help you increase your engagement or discuss suggestions you have for future programs: Grab It While it’s Cold! Tuesday, 18 September 13:00–15:00 OIDA (OSA Industry Development Associates) helps cor- porations optimize product development resources and re- Ice Cream Social sponsored – grab your favorite ice cream duce time to market by giving professionals access to quality treat, mingle with colleagues and learn more about what information, quality interactions and premium opportunities OSA has planned for 2019 . for collaboration . If You’ve Got the Time, We’ve Got the Beer OSA Advocacy works to promote optics and photonics Wednesday, 19 September 14:00–15:00 globally . One way to ensure this outreach is for OSA mem- Had enough coffee? Swing by the OSA Zone for a cold bers to visit with their elected officials, inform governments beer and snacks . Chat with colleagues, make plans for the about optics and photonics by providing technical insights, evening and discuss how you can get more involved with and reach out to decision makers so they understand OSA programs . why science - and optics in particular - is an integral part of society . OSA’s public policy programs are designed to facilitate this interaction . Stop by to learn about the OSA Congressional Science Policy Fellowships, how you can get involved in OSA’s global advocacy programs, write to your members of U .S . Congress, and more .

OSA Foundation provides training, mentoring, recognitions, scholarships and travel support programs as directed by our donors . We are supporting over 30 scholarships, grants, priz- es, professional development trainings, and summer schools benefitting students and early-career professionals this year . Stop by to learn more about our Career Calibrator and our plans for expanded programming.

OSA Meetings convenes more than 40 events throughout the world annually to provide you with opportunities to advance your scientific ambitions, expand your professional network and influence the future of optics and photonics worldwide . Learn more about the 2019-2020 schedule and discuss how you can participate in your favorite meeting .

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2018FiO Front.indd 14 8/20/18 9:07 AM Awards, Honors and Special Recognitions

FiO + LS Awards Ceremony & Reception OSA Honorary Members Monday, 17 September, 18:00–21:00 The most distinguished of all OSA Member categories, Hon- Carnegie Institute of Science, 1530 P St. NW orary Membership is awarded for unique, seminal contribu- Join us for an evening of celebration as we recognize the tions to the field of optics, and is confirmed by the Awards achievements of award and honor recipients from OSA and Council and OSA Board of Directors . APS Division of Laser Science . This is a great opportunity David J. Wineland, University of to connect with the OSA Board of Directors, honorees and Oregon, USA colleagues . For the most up-to-date information on the cer- emony program, please visit frontiersinoptics .com/awards . Wineland is honored for pioneering ad- vances in laser cooling of ions together Schedule for the Evening with unprecedented control of individ- Awards and Honors Program: 18:00–19:30 ual ions in foundational experiments of Reception: 19:30–21:00 quantum optics and quantum informa- Note: This is a ticketed event. Limited tickets will be avail- tion . able for purchase on-site at the conference registration desk. Doors open at 17:45. Amnon Yariv, California Institute of OSA 2018 Awards and Honors Technology, USA Yariv is honored for pioneering scien- Frederic Ives Medal/Jarus W. Quinn Prize tific and engineering contributions to Rod Alferness, University of 90thAnniversary photonics and quantum electronics that California, Santa Barbara, USA have profoundly impacted lightwave communications, and the field of optics The Ives Medal/Quinn Prize recognizes as a whole . overall distinction in optics and is OSA’s highest award . This year marks the 90th anniversary of the medal’s establishment . It was endowed by OSA charter mem- Esther Hoffman Beller Medal ber Herbert Ives, in honor of his father, Uli Lemmer, Karlsruhe Institute of Technology Anniversary photography pioneer Frederic Ives . A (KIT), Germany 25th subsequent endowment in honor of long- The Beller Medal recognizes outstanding contributions to time OSA Executive Director Jarus Quinn funds the prize . education in optical science and engineering . The 2018 OSA honors Alferness for basic contributions and leadership medal is presented to Lemmer for developing a vision for an in the development of integrated optics, high-speed optical international education program in optics that appreciates modulation and switching, and configurable WDM networks its importance as an enabling technology, and for successful- that have provided significant economic and societal impact . ly establishing the Karlsruhe School of Optics & Photonics . Alferness is the Dean of the College of Engineering at the University of California, Santa Barbara, USA . A member of Max Born Award the National Academy of Engineering and a Fellow of OSA Demetrios Christodoulides, CREOL- The College of Optics and the IEEE Photonics Society, he served as OSA president & Photonics, University of Central Florida, USA in 2008 and as a member of the OSA Board of Directors The Born Award is presented to a person who has made from 2001 to 2003 . He has authored over 100 papers and 5 outstanding contributions to physical optics, theoretical or book chapters and holds 35 patents . His work and research experimental . Christodoulides is recognized for founding has earned him numerous awards throughout his career, and continuing to lead the fields of Parity-Time non-Hermi- including the OSA Robert E . Hopkins Leadership Award in tian Optics and Accelerating Waves, and for groundbreaking 2010, the IEEE Millennium Award and the IEEE Photonics contributions in multiple areas in Physical Optics . Award . Alferness is world-renowned for his work on integrated-optic Stephen D. Fantone Distinguished Service Award devices and optical switching technology and architecture . Bob Jopson, Nokia Bell Labs, USA His research has been central to the development of global The Fantone Award recognizes outstanding service to The fiber optic communications networks . As chief scientist Optical Society . OSA celebrates Jopson for 25 years of at Bell Labs, he was responsible for strategic directions, enthusiastic service, principled leadership, and a tenacious technical excellence and global partnerships . In a prior role, commitment to OSA’s publications, conferences, processes, as senior vice president for research, he had overall respon- and especially its membership . sibility for the company’s global research laboratories . As chief technical officer for Bell Labs’ parent company, Lucent Technologies, Alferness was responsible for transferring the optical technology he and coworkers had invented to the business units .

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2018FiO Front.indd 15 8/20/18 9:07 AM Paul F. Forman Team Engineering Excellence Award microscopy and magnetic resonance spectroscopy/imaging The Adaptive Optics Facility on the VLT at ESO’s Paranal through the development of pulse shaping techniques . Observatory The Forman Team Award recognizes technical achievements David Richardson Medal in optical engineering . The Adaptive Optics Facility on Steven Frisken, Finisar Australia and Cylite, Australia the VLT at ESO’s Paranal Observatory is recognized for The Richardson Medal recognizes significant contributions to quipping one of the 8-m Unit Telescopes at ESO’s Paranal optical engineering, primarily in the commercial and industri- Observatory in Chile with an Adaptive Optics Laser Guide al sector . The 2018 Medal is presented to Frisken for seminal Star Facility, providing exquisite images to the unique 3D contributions as a researcher, inventor, and entrepreneur, to spectrograph MUSE and near-infrared imager HAWK-I . a wide range of photonic technologies which have enabled the growth of the internet, and for inspiring an entrepreneur- Robert E. Hopkins Leadership Award ial culture amongst Australian researchers . Anna Consortini, Università degli Studi di Firenze, Italy The Hopkins Award recognizes significant impact on the Kevin P. Thompson Optical Design global optics and photonics community or on society as a Innovator Award New whole stemming from non-research oriented activities . The Ulrike Fuchs, asphericon GmbH, Germany Award 2018 award is presented to Consortini for outstanding dedi- The Thompson Award recognizes contributions to lens cation to promoting optics at an international level with very design, optical engineering, or metrology at an early career valuable leadership in institutions and scientific societies like stage . The inaugural award is presented to Fuchs for inter- ICO (International Commission for Optics), ICTP, OSA, and linking aspects of optical design, tolerancing, metrology, SIOF . and manufacturing for aspherics to enable their usage as reasonable choice in optical systems . Edwin H. Land Medal Awards and Honors Awards Ann E. Elsner, Indiana University and Aeon Imaging, LLC, OSA Treasurer’s Award USA Naomi Chavez, The Optical Society, USA The Land Medal recognizes pioneering work empowered The Treasurer’s Award recognizes an OSA employee who by scientific research to create inventions, technologies, contributes significantly to organizational excellence, pro- and products . It is co-sponsored by OSA and the Society motes and enacts innovative solutions and/or exemplifies for Imaging Science and Technology . Elsner is honored for inspirational leadership . Naomi Chavez is recognized for contributions to the fields of ophthalmic instrumentation outstanding and innovative leadership, on a continued and and vision science with innovative imaging technologies, sustained basis, of the Optical Society’s meeting and confer- state-of-the-art psychophysical research, and entrepreneurial ence portfolio . ventures . R. W. Wood Prize Emmett N. Leith Medal Christopher Barty, University of California, Irvine, USA Asher Albert Friesem, Weizmann Institute of Science, Israel The Wood Prize recognizes an outstanding discovery, The Leith Medal recognizes seminal contributions to the scientific or technical achievement, or invention in the field field of optical information processing . The 2018 medal is of optics . The 2018 prize is presented to Barty for founda- presented to Friesem for pioneering, seminal and wide rang- tional innovations that have enabled ultrafast and energetic ing contributions to coherent optics, particularly the devel- intense lasers around the world . opments of new techniques and procedures in holographic applications and optical information processing . OSA Awards Presented Elsewhere Adolph Lomb Medal Recipients of these OSA and OSA co-sponsored awards Andrei Faraon, California Institute of Technology, USA were recognized at other conferences this year . The Lomb Medal recognizes noteworthy contributions made to optics at an early career stage . Faraon is recognized for Michael S. Feld Biophotonics Award seminal contributions to on-chip quantum photonic technol- Lihong Wang, California Institute of Technology, USA ogies . The Feld Biophotonics Award recognizes individuals for their innovative and influential contributions to the field C. E. K. Mees Medal of biophotonics, regardless of their career stage . Wang is Stanley Whitcomb, LIGO Laboratory, California Institute of recognized for inventing the world’s fastest two-dimensional Technology, USA receive-only camera and enabling real-time imaging of the The Mees Medal recognizes an original use of optics across fastest phenomena such as light propagation and fluores- multiple fields . The 2018 medal is presented to Whitcomb cence decay . for pioneering interdisciplinary contributions to the develop- ment of LIGO gravitational-wave interferometers . Joseph Fraunhofer Award/Robert M. Burley Prize Bahram Javidi, University of Connecticut, USA William F. Meggers Award The Fraunhofer Award/Burley Prize recognizes significant Warren S. Warren, Duke University, USA research accomplishments in the field of optical engineering . The Meggers Award recognizes outstanding work in spec- Javidi is honored for seminal contributions to passive and troscopy . Warren is recognized for pioneering contributions active multi-dimensional imaging from nano- to micro- and in the fundamental science of optical and spin coherence macro-scales . and their synergistic applications in optical spectroscopy/

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2018FiO Front.indd 16 8/20/18 9:07 AM Joseph W. Goodman Book Writing Award Herbert Walther Award Michael T. Eismann, US Air Force Research Laboratory, USA Gerd Leuchs, Universität Erlangen-Nürnberg & MPI for the The Goodman Award, co-sponsored with SPIE, recognizes Science of Light, Germany authorship of an outstanding book in the field of optics and The Walther Award, co-sponsored with Deutsche Physika- photonics, published in the last six years, that has contrib- lische Gesellschaft (DPG), recognizes distinguished con- uted significantly to research, teaching, or the optics and tributions in quantum optics and atomic physics as well as photonics industry . Eismann is honored as the author of leadership in the international scientific community . Leuchs is Hyperspectral Remote Sensing (SPIE Press, 2002) . honored for pioneering and widespread scientific contribu- tions ranging from ultrasmall focii of light to nonlinear optics, Nick Holonyak Jr. Award squeezed states of light and their application in metrology Dieter Bimberg, Technische Universität Berlin and King and quantum information, as well as for a continuing com- Abdul Aziz University, Germany/ Saudi Arabia mitment to the physics community, quantum optics and his The Holonyak Award recognizes contributions to optics students and team members . based on semiconductor-based devices and optical materi-

als, including basic science and technological applications . OSA Fellows Awards and Honors Bimberg is recognized for fundamental discoveries on 101 OSA Fellow Members were elected in 2018. The growth and physics of semiconductor nanostructures leading recipients listed below are being recognized at FiO. to novel nanophotonic devices for information science and communications . Domenico Bonaccini Calia, European Southern Observatory, Germany Sang Soo Lee Award For fostering the development of Photonics in novel astro- Cheng-Chung Lee, National Central University, Taiwan nomical instrumentation, including the field of Laser Guide The Lee Award, co-sponsored with the Optical Society of Star Adaptive Optics with the invention of narrow-band high Korea, recognizes outstanding leadership in founding or power Raman Fiber Amplifiers growing the optics and photonics community locally . Lee is Heike Ebendorff-Heidpriem, University of Adelaide, honored for guiding, educating, developing and inspiring Australia the optical coating industry in Taiwan for over 30 years and For groundbreaking science contributions to the field of serving as a key figure in its growth and success . optical glasses and fibers Ellis R. Lippincott Award Anne Myers Kelley, University of California, Merced, USA Peter Hamm, Universität Zürich, Switzerland For innovative work in the theory and practice of resonance The Lippincott Award, co-sponsored with the Coblentz Raman and hyper-Raman spectroscopy Society and the Society for Applied Spectroscopy, recog- François Légaré, Institut National de la Recherche nizes contributions to vibrational spectroscopy . Hamm is Scientifique, Centre Énergie, Matériaux, et recognized for seminal contributions to developing multi- Télécommunications, Canada dimensional infrared, Raman and Terahertz spectroscopy For major contributions to ultrafast molecular imaging, to and pioneering studies of protein and hydrogen bonding the development and application of high-power ultrashort dynamics in molecular liquids . infrared lasers including the concept of Frequency domain Optical Parametric Amplification, and the interpretation of Edgar D. Tillyer Award nonlinear optical signals from tissues Martin S. Banks, University of California, Berkeley, USA Innocenzo Pinto, The Tillyer Award recognizes distinguished work in the field University of Sannio, INFN, LVC, and of vision . Banks is honored for applying an innovative and KAGRA, Italy rigorous scientific approach to make significant contributions For fundamental contributions to thermal noise reduction in in the fields of visual development, sensory cue combination the mirror coatings of the LIGO interferometric gravitational and 3D vision . wave detectors, and for original contributions to the science of Electromagnetics Charles Hard Townes Award Gernot Pomrenke, US Air Force Office of Scientific Research Peter Fritschel, Kavli Institute for Astrophysics and Space (AFRL/AFOSR), USA Research, Massachusetts Institute of Technology, USA For outstanding technical leadership in formulating and The Townes Award recognizes contributions to quantum advancing the areas of Optical Materials Characterization, electronics . Fritschel is recognized for advances in quan- Opto-Electronics, Integrated Photonics, Silicon Photonics, tum-limited precision measurement in the Advanced LIGO Nano-photonics, Metamaterials and Plasmonics detectors, leading to the first direct detection of gravitation- Nickolas Vamivakas, University of Rochester, USA al waves . For significant contributions to the fields of solid-state quan- tum optics and nano photonics John Tyndall Award Peter J. Winzer, Nokia Bell Labs, USA The Tyndall Award, co-sponsored with the IEEE/Photonics Society, recognizes contributions to fiber optic technology . Winzer is honored for contributions to understanding and advancing the capacity of coherent optical communication systems including advanced modulation formats and spatial mutiplexing .

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2018FiO Front.indd 17 8/20/18 9:07 AM Congratulations, 2018 OSA Senior Members - OSA Randolph Hall, Conejo Valley Research, USA welcomes the following 169 distinguished individuals to Kiichi Hamamoto, Kyushu University, Japan the rank of Senior Member. For more on Senior Member Young-Geun Han, Hanyang University, China status and how to apply, please visit www.osa.org/ Christoph Hauri, Paul Scherrer Institut, Switzerland seniormember. Joseph Hayward, Juravinski Cancer Centre, Canada Mark Henesian, Lawrence Livermore Lab (retired), USA Esmail Ahouzi, Institut National des Postes et Telecomm, Wei-Da Hu, Chinese Academy of Sciences, China Morocco Zhaoran Huang, Rensselaer Polytechnic Institute, USA Tatiana Alieva, Universidad Complutense de Madrid, Spain Yu-Chueh Hung, National Tsing Hua University, China Rebecca Andersen, The Optical Society, USA Boyd Hunter, Praxis Optics, USA Shamsul Arafin, University of California Santa Barbara, USA Amiel Ishaaya, Ben Gurion University of the Negev, Israel Christos Argyropoulos, University of Nebraska Lincoln, USA Shudong Jiang, Dartmouth College, USA John Arkwright, Flinders University, Australia Alexander Khanikaev, City College of New York, USA Seung-Whan Bahk, University of Rochester, USA Dae Wook Kim, University of Arizona, USA Anirudh Banerjee, Amity University Lucknow, India Toshiaki Koike-Akino, Mitsubishi Electric Research Labs, Santanu Basu, Basu Labs, USA Japan Can Bayram, Univ of Illinois at Urbana-Champaign, USA Tanya Kosc, University of Rochester, USA Matthew Berg, Kansas State University, USA Stephen Kuebler, University of Central Florida, USA David Boertjes, Ciena Corporation, Canada G .V . Pavan Kumar, IISER-Pune, India Nicolas Bonod, CNRS-UPS, France Franko Küppers, TU Darmstadt, Germany Bosanta Boruah, Indian Institute of Technology Guwahati, Brian Lail, Florida Institute of Technology, USA India Geon Joon Lee, Kwangwoon University, South Korea Ozdal Boyraz, University of California Irvine, USA Jiun-Haw Lee, National Taiwan University, Taiwan

Awards and Honors Awards Aidan Brooks, California Institute of Technology, USA Feng Li, The Hong Kong Polytechnic University, Hong Kong David Busch, UT Southwestern Medical Center at Dallas, Yan Li, Peking University, China USA Juhao Li, Peking University, China Vijayan C, Indian Institute of Technology Madras, India Charles Lieber, Harvard University, USA Alejandro Carballar, Universidad de Sevilla, Spain Daniel Litynski, Western Michigan University, USA Swapnajit Chakravarty, Omega Optics, USA Zhixin Liu, University College London, UK Guo-En Chang, National Chung Cheng University, Taiwan Jung-Ping Liu, Feng Chia University, China Ching-Hung Chang, National Chiayi University, Taiwan Yanhua Luo, University of New South Wales, Australia Chih-Hao Chang, North Carolina State University, USA Yiran Ma, Finisar, Australia Yu Chen, University of Maryland at College Park, USA Brian Mangan, OFS Laboratories, USA Francesco Chiadini, Universita degli Studi di Salerno, Italy Onofrio Marago, CNR-IPCF, Italy Ricky Chuang, National Cheng Kung University, Taiwan Alireza Marandi, Stanford University, UK Hsiang-Chen Chui, National Cheng Kung University, Taiwan A . Márquez, Universidad de Alicante, Spain C . Ciminelli, Politecnico di Bari, Italy Maurizio Martino, Universita del Salento, Italy Christophe Codemard, SPI Lasers, UK Goran Mashanovich, University of Southampton, UK John Corless, Verity Instruments, USA Dale McMorrow, US Naval Research Laboratory, USA Razvan Dabu, Institute Nuclear Physics & Engineering, Yobani Mejia-Barbosa, Universidad Nacional de Colombia, Romania Columbia Antonio d’Alessandro, Sapienza University of Rome, Italy Charles Middleton, Harris Corporation, USA Hamed Dalir, Omega Optics, USA Uladzimir Minkovich, Centro de Investigaciones en Optica Kamal Das, Alcon Laboratories, USA AC, Mexico Marcelo Davanco, National Inst. of Standards & Technology, Paolo Minzioni, Universita degli Studi di Pavia, Italy USA Eric Mottay, Amplitude, France Nazif Demoli, Institute of Physics Zagreb, Croatia K .M . Naga Srinivas Nadella, University College London, UK Xinyong Dong, China Jiliang University, China Tamas Nagy, Max Born Institute, Germany Richard Dorshow, MediBeacon, USA Tien Khee Ng, King Abdullah Univ of Science & Tech, Saudi Anthony Durkin, University of California Irvine, USA Arabia Achyut Dutta, Banpil Photonics, USA Mark Niedre, Northeastern University, USA Christoph Englert, US Naval Research Laboratory, USA Gregory Nielson, Nielson Scientific, USA Dirk Englund, Massachusetts Institute of Technology, USA Ampalavanapilla Nirmalathas, University of Melbourne, Oliver Faehnle, FISBA AG, Switzerland Australia Xinyu Fan, Shanghai Jiao Tong University, China Ioan Notingher, University of Nottingham, UK Reza Faraji-Dana, University of Tehran, Iran Tatiana Novikova, Ecole Polytechnique, France Steve Federman, University of Toledo, USA Teri Odom, Northwestern University, USA Ulrike Fuchs, Asphericon GmbH, Germany Zhengbiao Ouyang, Shenzhen University, China Qiaoqiang Gan, State University of New York at Buffalo, USA Megan Paciaroni, Fort Lewis College, USA Jaime Garcia-Ruperez, Universidad Politecnica de Valencia, Mrinmay Pal, Central Glass & Ceramics Res Institute, India Italy Shilong Pan, Nanjing Univ Aeronautics & Astronautics, China Zabih Ghassemlooy, University of Northumbria, UK Konstantin Pavlov, University of New England, USA Ashish Ghunawat, MNIT Jaipur, India Frederick Perry, Boston Electronics Corp., USA Dana Granciu, IOR, Romania Rita Peterson, US Air Force Research Laboratory, USA Mark Guardalben, University of Rochester, USA Peter Pilon, OFS Laboratories, USA

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2018FiO Front.indd 18 8/20/18 9:07 AM Luis Ponce, IPN CICATA ALTAMIRA, Mexico Constantinos Valagiannopoulos, Nazarbayev University, Bryce Richards, Karlsruhe Institute of Technology, Germany Kazakhstan Jorge Ripoll, Universidad Carlos III de Madrid, Spain Stacey Vargas, Virginia Military Institute, USA Eduardo Rosa-Molinar, University of Kansas, USA Philippe Velha, Scuola Sant’Anna, Italy Joachim Sacher, Sacher Lasertechnik GmbH, Germany Deepa Venkitesh, Indian Institute of Technology Madras, Prasant Sahu, IIT Bhubaneswar, India India Massimo Santarsiero, Università degli Studi Roma Tre, Italy Taco Visser, Vrije Universiteit Amsterdam, The Netherlands Mohammad Sayeh, Southern Illinois University Carbondale, Josef Vojtech, CESNET, Prague USA Giovanni Volpe, Goteborgs Universitet, Sweden Christian Schäfer, isarpatent Munich, Germany Matthew Weed, Luminar Technologies, USA Jochen Schroeder, Chalmers Tekniska Hogskola, Sweden Ralf Wehrspohn, Fraunhofer IMWS Halle, Germany Rainer Schuhmann, Berliner Glas KGaA Herbert Kubatz GmH Antoine Weis, Universite de Fribourg, Switzerland &Co., Germany Ian White, University of Maryland at College Park, USA Ranjan Sen, Central Glass & Ceramics Res Institute, India Rengmao Wu, Zhejiang University, China Utkarsh Sharma, Optovue Inc., USA

Haiyun Xia, Univ of Science and Technology of China, China Awards and Honors Gholamreza Shayeganrad, Basel University, Switzerland Sanshui Xiao, DTU Fotonik, The Netherlands Jason Sickler, Torchlight Solutions, USA Huailiang Xu, Jilin University, China Hukum Singh, NorthCap University, India Fei Xu, Nanjing University, China Philip Smith, SEMROCK, USA Changyuan Yu, Hong Kong Polytechnic University, Hong Vincenzo Spagnolo, Politecnico di Bari, Italy Kong Bernhard Stumpf, University of Idaho, USA Shuiqing Yu, University of Arkansas, USA Lan Sun, Raytheon Company, USA Zhiliang Yuan, Toshiba Research Europe Ltd, UK Jun Takeda, Yokohama National University, Japan Jinhui Yuan, Beijing University of Posts and Telecomm, China Herve Tatenguem Fankem, Sacher Lasertechnik GmbH, Robert Zawadzki, University of California Davis, USA Germany Yundong Zhang, Harbin Institute of Technology, China Alison Taylor, The Optical Society, USA Lin Zhang, Aston University, UK Chao Tian, University of Science and Tech. of China, China Luming Zhao, Jiangsu Normal University, China Ion Tiginyanu, Academy of Sciences of Moldova, Moldova Kaiming Zhou, Aston University, UK Atsushi Uchida, Saitama University, Japan Chao Zhou, Lehigh University, USA Kathleen Vaeth, Cornell University, USA Xiushan Zhu, University of Arizona, USA Weiren Zhu, Shanghai Jiao Tong University, China

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2018FiO Front.indd 19 8/20/18 9:07 AM APS/Division of Laser Science 2018 Bin Fang, University of Illinois Urbana-Champaign, USA Manipulation of Photonic Quantum States: From Generation, Awards and Honors Engineering, and Characterization to Storage and Retrieval Pablo Solano, MIT, USA Arthur L. Schawlow Prize in Laser Science Quantum Optics in Optical Nanofibers Gérard Albert Mourou, École Polytechnique, France APS DLS Fellows For fundamental contributions in ultra- Hui Deng, University of Michigan, USA fast, ultrahigh-field laser inventions, such For pioneering contributions to fundamental physics and as chirped pulse amplification, that led to applications of matter-light coupled systems . the new discipline of relativistic optics . Munira Khalil, University of Washington, USA Gérard Mourou is Professor Haut-Collége For probing coherently coupled vibrational and electronic at the École Polytechnique . He is also motion during ultrafast charge transfer processes by using the A .D . Moore Distinguished University a unique combination of infrared, visible, and X-ray experi- Emeritus Professor of the University of ments to provide new insights into this mechanism . Michigan . He received his undergraduate education at the University of Grenoble (1967) and his Ph .D . from Universi- N. Asger Mortensen, University of Southern Denmark, ty Paris VI in 1973 . He has made numerous contributions Denmark to the field of ultrafast lasers, high-speed electronics, and For fundamental explorations of light-matter interactions in medicine . His most important invention, developed with nanostructures at the interface of classical electrodynamics Donna Strickland while at the University of Rochester (N Y. .), and quantum physics .

Awards and Honors Awards is the laser amplification technique known as Chirped Pulse Gunter Steinmeyer, Max Born Institute, Germany Amplification (CPA), universally used today . CPA’s attosecond For outstanding contributions to ultrafast nonlinear optics, pulse generation and compact particle accelerators made in particular for the development of pulse characteriza- possible the generation of extremely high laser intensities, tion techniques, the experimental demonstration of pulse making a new branch of optics possible . In 2005, Prof . Mou- self-compression through laser filamentation, and the inves- rou proposed a new infrastructure, extreme light infrastruc- tigations of higher-order nonlinear susceptibilities and rogue ture (ELI), which is distributed over three pillars located in waves . the Czech Republic, Romania, and Hungary . Prof . Mourou also pioneered the field of femtosecond ophthalmology that Edo Waks, University of Maryland College Park, USA relies on a femtosecond laser for precise myopia correction For significantly advancing the field of quantum photonics and corneal transplants . Over a million such procedures are and for developing new concepts to strongly interact sol- now performed annually . Prof . Mourou is member of the U .S . id-state quantum emitters with nanophotonic components . National Academy of Engineering, an OSA Fellow, and a for- eign member of the Russian Science Academy, the Austrian Sciences Academy, and the Lombardy Academy for Sciences and Letters . He is Chevalier de la Légion d’honneur .

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 on Monday morning . The winner will be announced at the DLS business meeting late Monday afternoon . The following presentations will be given during this special session on Monday at 08:00 . Sara Campbell, Lawrence Berkeley National Laboratory; Univ. of California, Berkeley, USA A Fermi-degenerate 3D Optical Lattice Clock Mark Dong, University of Michigan, USA Quantum-well Diode Lasers for Frequency Comb Generation

20 FiO + LS 2018 • 16–20 September 2018

2018FiO Front.indd 20 8/20/18 9:07 AM OSA Foundation 2018 Prizes and Special OSA Foundation Incubic/Milton Chang Travel Grant Recognitions Funded by an endowment from Milton and Rosalind Chang, this program provides 10 grants of $500 USD each to enable OSA Foundation Boris P. Stoicheff Memorial students who present papers to travel to Frontiers in Optics . Scholarship - Grants are awarded to the presenter and usually the first author of the paper . Established in 2011 by the OSAF and the Canadian Asso- ciation of Physicists Educational Trust Fund (CAPETF), this Past student recipients for this program can be found online program pays tribute to Boris P . Stoicheff, an internationally at osa .org/incubic . renowned laser spectroscopist who also served as Presi- Congratulations to our 2018 Grant Recipients: dent of OSA (1976) and CAP (1983-84) This. $3,000 USD scholarship is awarded annually to a graduate student who Ankan Bag, Max Planck Institute for the Science of Light, has demonstrated both research excellence and significant Friedrich-Alexander-University Erlangen-Nuremberg, service to the optics or physics community . Germany

Avijit Chatterjee, Indian Institute of Science Bangalore, Awards and Honors Past student recipients for this program can be found online India at osa .org/stoicheff . Congratulations to our 2018 scholarship Aysan Bahari, Texas A&M University, USA recipient: Hsuan-Hao Lu, Purdue University, USA Robin Puchert, Universität Regensburg, Germany Jingyang Peng, RMIT University, Australia Liang Xu, Nanjing University, China Luca La Volpe, Laboratoire Kastler Brossel, France OSA Foundation Emil Wolf Outstanding Student Milica Notaros, Massachusetts Institute of Technology, USA Paper Competition Poolad Imany, Purdue University, USA This competition recognizes the innovation, research excel- Shahriar Aghaeimeibodi, University of Maryland, USA lence and presentation abilities of students presenting their work during FiO and honors Emil Wolf for his many contribu- OSA Foundation Jean Bennett Memorial Student tions to science and The Optical Society . One winner is se- Travel Grant lected from each of the seven FiO subcommittees . Winners receive a complimentary OSA three-year student member- Established in 2008, in memory of Jean M . Bennett, a highly ship, an award stipend of $300 USD and an award certificate . decorated research physicist who was recognized for her contributions to the studies of optical surfaces and served Past student recipients for this program can be found online as OSA’s first female president, this $1,000 USD grant is at osa .org/wolf . 2018 recipients will also be announced at awarded to a student presenting their work at FiO . This the FiO + LS Awards Banquet . competition is administered by the OSA Foundation and is made possible through the generous support of Nanoptek Congratulations to our finalists competing at FiO: Corporation, the Pennsylvania State University Department Abhijit Roy, Indian Institute of Technology Kharagpur, India of Physics and individual contributors . Ayan Chattopadhyay, Princeton University, USA Past student recipients for this program can be found online Bingchang Wu, University of Tokyo, Japan at osa .org/bennett . Erwan Lucas, Ecole Polytechnique Fédérale de Lausanne, Switzerland Congratulations to our 2018 grant recipient: James D. Gaynor, University of Washington, USA Jingyi Yang, Baylor University, USA Muhammed Veli, University of California, Los Angeles, USA João Moura, Delft University of Technology, Netherlands Julie Chang, Stanford University, USA OSA Foundation Robert S. Hilbert Memorial Lorenzo De Angelis, Delft University of Technology, Student Travel Grant Netherlands Manoj Kumar Dasa, Technical University of Denmark, Established in 2009 by Optical Research Associates (ORA), Denmark now the Optical Solutions Group at Synopsys, as a memorial Muhammad Faris Shahin Shahidan, University of to ORA’s former President and Chief Executive Officer Rob- Melbourne, Australia ert S . Hilbert, this $1,100 USD grant recognizes the research Muhammed Veli, University of California, Los Angeles, USA excellence of students in the areas of optical engineering, Poliane Aires Teixeira, Federal University of Itajubá, Brazil lens design and illumination design . Robert Pettit, University of Rochester, USA Past student recipients for this program can be found online Thomas Muir Hird, University of Oxford, University College at osa .org/Hilbert . Congratulations to our 2018 grant recip- London, United Kingdom ients: Zhenxu Bai, Macquarie University, Australia Ayan Chattopadhyay, Princeton University, USA Abhijit Roy, Indian Institute of Technology Kharagpur, India Nisha Nisha, Bharati Vidyapeeths College of Engineering, India

To learn more about these programs, attend the FiO + LS Awards Ceremony & Reception on 17 September from 18:00–21:00 . Stop by registration to purchase a ticket .

FiO + LS 2018 • 16–20 September 2018 21

2018FiO Front.indd 21 8/20/18 9:07 AM 2018FiO Front.indd 22 8/20/18 9:07 AM Special Events WiSTEE Connect (Women in Science, OSA Quantum Computing and Technology, Engineering and Communication Technical Group Entrepreneurship) Networking Lunch Sunday, 16 September, 08:00–16:00 Monday, 17 September, 12:30–13:30 OSA Headquarters Fairchild East WiSTEE Connect (Women in Science, Technology, Engineer- Members of the Quantum Computing and Communication ing and Entrepreneurship) is collaborating with the OSA Technical Group are invited to join us for a networking lunch Foundation to organize the 3rd International Symposium, on Monday . The event will provide an opportunity to con- “Global Women of Light” (GWL) . This GWL symposium will nect with fellow attendees who share an interest in this field, focus on Career Strategies for Women in Science, Technol- learn more about this technical group, and provide your in- ogy, Engineering, and Entrepreneurship . Preregistration is put on future technical group activities . An RSVP is required required . for this technical group event; please contact TGactivities@ osa .org to register, pending availability .

Laser Science Symposium on Hosted by: Undergraduate Research Monday, 17 September, 12:00–18:00 OSA Senior Member Workshop International Ballroom East Monday, 17th September, 15:00–17:00 Organizers: Chad Hoyt, Bethel University, USA, and Harold Holmead, Lobby Level Metcalf, Stony Brook University, USA This session focuses on the potential to lead lasting and The Symposium on Undergraduate Research has been a positive change in yourself and the future leaders in op- feature of the annual meeting of the Division of Laser Sci- tics through quality mentoring and sponsorship . With your ence of the American Physical Society (APS-DLS) for sixteen guidance, you can help build and strengthen personal years, and has showcased the research of more than 500 brands, leadership skills and business ethics . If you’re a Special Events students during that time . Students’ presentations often de- senior member and interested in mentoring and sponsorship scribe their work during the previous summer . The NSF has opportunities, join us at this interactive session . During the played a vital role by providing the research opportunities session you will reflect on both the impact and the oppor- for many of the students through its REU programs, as well tunity of having both mentors and sponsors in your life and as by direct support of the event . The symposium has been Evaluate best practices and internal strategies to elevate generously supported by the DLS, OSA, NSF, SPS, and Univ . others while expanding your personal leadership capabilities MD (JQI), along with corporate sponsors Thorlabs, Photon- and Understand and build a business case for mentoring and ics Industries, East Coast Optical Technologies, and Bristol sponsorship in your organization to drive diversity, retention, Instruments . knowledge transfer and engagement . This program is open to Senior Members only . Limited space is available, rsvp to OSA Therapeutic Laser Applications gmontanez@osa .org . Technical Group “Birds of a Feather” DLS Annual Business Meeting Networking Lunch Monday, 17 September, 16:00–17:00 Monday, 17 September, 12:30–13:30 Georgetown West Fairchild West All members and interested parties are invited to attend Join the OSA Therapeutic Laser Applications Technical the annual business meeting of the APS Division of Laser Group for a guided networking session during lunch on Science (DLS) . The DLS officers will report on the activities Monday . In addition to learning more about this technical of the past year and on plans for the future . Questions will group, you will have a chance to connect with your fellow be taken from the floor . This is an opportunity to help define attendees who share an interest in the same topics as you, the operations of the DLS and the Laser Science Conference . such as lasers in ophthalmology, tissue imaging, spectro- In addition, the winner of the Carl E . Anderson Dissertation scopic tools and methods, and light-tissue interactions . An Award will be announced . RSVP is required to attend this event . Please contact tgactivi- ties@osa .org to register, pending availability .

Hosted by:

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2018FiO Front.indd 23 8/20/18 9:07 AM Meet OSA’s Journal Editors Finishing Touches: A Tutorial in Blender for Monday, 17 September, 16:00–17:00 Cover Art and Figures Concourse Foyer Monday, 17 September 16:00–18:00 Join OSA Publishing’s Journal Editors for conversation and Jefferson West refreshments . The Editors welcome your questions, concerns Join the OSA Optical Materials Studies Technical Group for and ideas for any of OSA’s Journals . Topics that can be cov- an opportunity to learn more about putting Blender, a free ered include best practices when submitting a manuscript, graphics software, to use to enhance your papers and pre- elements of a useful manuscript review, criteria editors look sentations . Nathaniel Kinsey of Virginia Commonwealth Uni- for in submitted manuscripts, and the process to propose a versity will take attendees through a live demonstration on Feature Issue topic for publication in an OSA Journal . All are the basics of how to use Blender to create scientific figures welcome to attend . and cover art as well as more advanced topics related to cre- ating images for optics, such as making laser beams, adding focal blur, creating realistic optical materials, and merging real photo images with CGI images . An RSVP is required for OSA Optical Fabrication and Testing this technical group event; please contact TGactivities@osa . Technical Group Knowledge Café org to register, pending availability . Monday, 17 September, 16:00–17:30 International Ballroom West Hosted by: Do you have questions about optical fabrication and optics testing? Join the OSA Optical Fabrication and Testing Tech- Cheeky Scientist Career Development nical Group at our Knowledge Café on Monday afternoon for a drink and a chance to seek out the answers to your Workshops Monday, 17 September, 16:00–18:30 questions in an informal atmosphere . Our knowledgeable “bartenders”, experts in their own fields, will be available Jefferson East to answer your questions and discuss issues related to the Isaiah Hankel from Cheeky Scientist works with hundreds of group’s areas of interest . Please contact TGactivities@osa . graduate students and postdocs daily assisting them in their org to let us know you will be joining us in the café . transition to industry by first showing them how to present themselves as business professionals . These programs will Hosted by: provide you with a strong understanding of what it takes to have a tailored industry resume and how to showcase your OSA Photonic Metamaterials Technical transferrable skills . Group Tutorial on Metalens Design and Session 1: Networking: An Art & Science: 16:00–17:00

Special Events Simulation This section is created based on the networking strategies Monday, 17 September, 16:00–18:00 of some of the most strategic networkers in the world and Lincoln West also goes into the science of building rapport and why this is important for the job seeking professional . While this topic Join the OSA Photonic Metamaterials Technical Group for a tends to be popular, it seems people are still not using it tutorial on metalens design and simulation on Monday after- effectively and thus we have detailed specific action steps noon . This tutorial, aimed at students and new researchers, job seekers can take, and specific scripts to use while net- will focus on hands-on skills . Dr . Wei Ting Chen from Harvard working . University will provide an introduction to metalenses fol- lowed by a tutorial on how to simulate the phase of different Session 2: The Modern Job Search: 17:30–18:30 nanostructures and a real-time simulation demo of metalens- Using online profiles to maximize the effectiveness of the job es . An RSVP is required for this technical group event; please seeking/transition process . Hiring managers use LinkedIn to contact TGactivities@osa .org to register, pending availability . determine whether they will bring in a candidate for an inter- view, this topic will cover all the key elements of the LinkedIn Hosted by: profile and how each section should be used to strategically maximize its impact . In addition, we will show candidates how to use LinkedIn algorithms to support their job search, and sell themselves to perspective employers .

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2018FiO Front.indd 24 8/20/18 9:07 AM Foundational Skills of Professional OSA Polarization Technical Group Rapid- Networking – How First Impressions and Fire Presentations & Networking Event Elevator Pitches Lead to Career Success Monday, 17 September, 18:00–19:00 and Longevity International Ballroom West Monday, 17 September, 16:00–17:00 Join the OSA Polarization Technical Group for a networking Cabinet event on Monday evening that will highlight the research being done in this topic area by students and early career When you enter a new organization and seek to meet new professionals . Our event will be an opportunity to hear people or to build relationships to expand your professional rapid-fire presentations of the work they will present during network, you are inevitably asked: “Tell me a little bit about Frontier in Optics while networking with your colleagues yourself ”. The traditional “elevator pitch”—a 30-60 second over refreshments . Attendees can then visit the presenters’ introduction about oneself—is commonly practiced, mem- posters during the conference poster sessions on Tuesday orized and delivered to initiate this conversation . This initial and Wednesday to learn more about their research and interaction can often determine you value and “likeability” also to cast their vote for the Best Polarization Presentation . that can set you on a path of relationship success, or failure . Please contact TGactivities@osa .org to let us know you will Making a mistake can be costly and difficult to recover from . be joining us for this event . In a very short time, you must be able to quickly establish a relationship with a new person and show them why it’s Hosted by: important to remain connected to you . Once this occurs, this new contact will want to include you in their network and Workshop: Understanding Unconscious help you achieve the outcomes you desire . The speaker is Josh Henkin, STEM Career Services, USA Bias Monday, 17 September, 18:00–19:00 After this workshop, you will be able to: Georgetown East 1 . Understand the criticality of first impressions, “likeability” Research demonstrates that we all have unconscious biases . and the double edged sword of networking These biases can result in best and brightest talent made to 2 . Craft and deliver an elevator pitch that clearly communi- feel unwelcome, invisible, and not important to the success

cates your professional highlights, what you currently do, of the organization . This training, led by Sara Bendoraitis, Special Events why you do it and who it benefits, and what is next for will explore concepts and engage participants to better un- you professionally derstand implicit bias, increase awareness and understand- ing of the impact on organizational culture, and identify ways 3 . Learn how to express yourself authentically to differenti- to promote greater engagement with diversity and inclusion . ate from others with similar training/skills/experiences Hosted by: The Rules of Engagement: Navigating Important Business Relationships Monday, 17 September, 16:00–17:30 OSA Annual Business Meeting Georgetown East Tuesday, 18 September, 17:30–18:15 Kaloroma Important business relationships often are formed and cemented in social settings . Yet, many professionals feel Learn more about OSA and join the OSA Board of Directors uncomfortable in these environments . Working a crowded for the Society’s annual business meeting . An update on the room and managing the more formal dining setting—these Society’s activities will be presented and the results of the and other business entertainment opportunities chal- Board of Directors election will be announced . lenge many professionals, junior and more senior alike . This 90-minute program, led by Mary Crane, is specifically Conference Reception designed to help professionals feel competent and com- Tuesday, 18 September, 18:30–20:30 fortable in any business-social setting . Participants will learn International Ballroom Center ten specific rules for working a reception and ten more rules for managing a business lunch or dinner . To the extent your Dance the night away and enjoy tasty treats with your fellow organization would like, we also cover rules for electronic conference attendees from around the world . The reception communications and personal presentation . is sure to be a high point in a memorable conference week . Sponsored by

FiO + LS 2018 • 16–20 September 2018 25

2018FiO Front.indd 25 8/20/18 9:07 AM NAS Decadal Assessment and Outlook Meet the Physical Review Journal Editors Report on Atomic, Molecular, and Optical Reception Science Wednesday, 19 September, 15:30–17:00 Wednesday, 19 September, 09:05–10:00 Monroe Cabinet The editors of the Physical Review journals invite you to join Join National Academies of Sciences Committee Chairs them for conversation and light refreshments . The editors Jun Ye (JILA) and Nergis Mavalvala (MIT) to hear about and will be available to answer questions, hear your ideas and provide input into their once-a-decade retrospective and discuss any comments about the journals . prospective assessment of the frontiers of AMO research, funding, and workforce . The resulting report will help guide OSA Senior Member Reception federal research directions . Wednesday, 19 September, 17:00–19:00 Holmead, Lobby Level OSA Family and Friends Tour Wednesday, 19 September, 10:00–12:00 Join your colleagues at the first annual Senior Member re- ception . The reception is an RSVP event for Senior Members Tudor Place is a National Historic Landmark nestled in the of OSA to network, enjoy refreshments, food and mingle neighborhood of Georgetown . Completed in 1816, lived in with fellow Senior Members . Each Senior Member can bring by six generations of a single family, and opened to the pub- one guest that can discover the benefits of becoming an lic in 1988, Tudor Place Historic House & Gardens preserves, OSA Senior Member . RSVP to gmontanez@osa .org . interprets, and shares with the public and scholars the rich resources of architecture, history, collections, and archives . OSA Capitol Hill Meetings With an object collection representing every time period of Thursday, 20 September the estate’s occupation since 1805, the estate is a time cap- Senate and House Office Buildings, Washington D.C. sule of culture . Its 15,000-plus objects spans three centuries and include a range of cultural touchstones from Martha and As U S. . Congress determines spending levels in the George Washington’s personal items to Asian and European FY2019 funding legislation, it is important for members decorative arts, musical instruments, garden implements, of U S. . Congress to hear directly from their constituents . weaponry, 20th-century couture, and a 1919 automobile . To facilitate those interactions, OSA will be holding U .S . Capitol Hill meetings to advocate for R&D funding as well as Ground transportation will be provided to and from the other issues such as the National Quantum Initiative . Prior museum . RSVP required to participate . If you RSVP’d for Capitol Hill meetings and have questions, contact Brandy Dillingham at To register, please email Jennifer Mehltretter at jmehltret- bdillingham@osa .org . ter@osa .org Special Events

26 FiO + LS 2018 • 16–20 September 2018

2018FiO Front.indd 26 8/20/18 9:07 AM FiO + LS Committees Thanks to the technical program committee members! Your time and efforts are appreciated!

Frontiers in Optics General Chairs FiO 4A: Fiber Optics and Optical Communications Christoph Harder, Swissphotonics, Switzerland Photonics Wei Lee, National Chaio Tung University, Taiwan Greg Raybon, Nokia Bell Labs, USA, Subcommittee Chair Anjali Agarwal, Vencore Labs, USA Tymon Barwicz, IBM, USA FiO Theme Coordinators Mina Esmaeelpour, Stanford University, USA Takuro Fujii, NTT Device Technology Laboratories, Japan Automotive Lyuba Kuznetsova, San Diego State University, USA Anna Peacock, University of Southampton, United Kingdom Alex Fong, TruTag Technologies, Inc., USA Karsten Rotwitt, DTU Fotonik, Netherlands Sabbir Rangwala, Patience Consulting LLC, USA Alexey Turukhin, TE SubCom, USA Nanophotonics and Plasmonics Thomas Van Vaerenbergh, Hewlett Packard Labs, USA Ortwin Hess, , United Kingdom FiO 4B: Photonic Integrated Devices for Computing, Quantum Technologies Sensing, and Other Applications Paul Barclay, University of Calgary, Canada, Subcommittee Nils Hempler, M Squared Lasers Ltd., United Kingdom Chair Virtual Reality and Augmented Vision Amy C . Foster, John Hopkins University, USA Femius Koenderink, FOM Inst. for Atomic & Molecular Physics, Bernard Kress, Microsoft, USA Netherlands Dangyuan Lei, Hong Kong Polytechnic University, Hong Kong FiO Program Committees Di Liang, Hewlett Packard Enterprise, USA Qiang Lin, University of Rochester, USA FiO 1: Fabrication, Design and Instrumentation Michelle Lynn Povinelli, University of Southern California, USA Byoungho Lee, Seoul National University, Korea, Subcommittee Chair FiO 5: Optics in Biology, Medicine, Vision, and Color Liangcai Cao, Tsinghua University, China David Busch, University of Texas Southwestern, USA, Chau-Jern Cheng, National Taiwan Normal University, Taiwan Subcommittee Chair Jessica DeGroote Nelson, Optimax Systems Inc., USA Joeseph Angelo, NIST, USA Pietro Ferraro, Instituto Nazionale di Ottica, Italy Bernhard Baumann, Medizinische Universität Wien, Austria Groot Gregory, Synopsys, Inc., USA Félix Fanjul-Vélez, University of Cantabria, Spain Yoshio Hayasaki, Utsunomiya University, Japan Delphine Gourdon, University of Ottawa, Canada Joohwan Kim, NVIDIA Corporation, USA Jana Kainerstorfer, Carnegie Mellon University, USA John Koshel, University of Arizona, USA Marina Zannoli, Oculus VR, USA Pascal Picart, LAUM CNRS Université du Maine, France Jamie Leigh Ramsey, RPO, USA FiO 6: Information Acquisition, Processing, and Display Yunlong Sheng, Université Laval, Canada Kenji Yamamoto, National Institute of Information and Simon Thibault, Université Laval, Canada Communications Technology, Japan, Subcommittee Chair Johannes K . Courtial, University of Glasgow, United Kingdom FiO 2: Optical Interactions Nobuyuki Hashimoto, Citizen Watch Co., LTD, Japan Tomasz Kozacki, Politechnika Warszawska, Poland

Halina Rubinsztein-Dunlop, University of Queensland, Australia, Committees Subcommittee Chair Hong-Seok Lee, Samsung Electronics, Korea Gregory J . Gbur, University of North Carolina at Charlotte, USA Ting-Chung Poon, Virginia Tech, USA Igor Jovanovic, University of Michigan, USA Elena Stoykova, Bulgarian Academy of Sciences, Bulgaria Igor Litvinyuk, Griffith University, Australia Qiong-Hua Wang, Sichuan University, China Carlos Lopez-Mariscal, Underwater Photonics, Mexico William Munro, NTT Basic Research Laboratories, Japan Laser Science Chairs Kae Nemoto, National Institute of Informatics, Japan Peter Delfyett, University of Central Florida, USA Takashige Omatsu, Chiba University, Japan Nathan Newbury, National Institute of Standards & Technology, Monika Ritsch-Marte, Innsbruck Medical University, Austria USA FiO 3: Quantum Electronics Antonio Badolato, University of Ottawa, Canada, Subcommittee Laser Science Program Committees Chair Marcelo Davanco, National Institute of Standards and 1. Extreme Laser Science (Wavelength, Power, Time) Technology (NIST), USA David Reis, Stanford University, USA Rosario Fazio, Scuola Normale Superiore, Italy Dario Gerace, Università degli Studi di Pavia, Italy 2. Quantum Science Brian D . Gerardot, Heriot-Watt University, United Kingdom Xiaoqin (Elaine) Li, University of Texas, USA Evelyn L . Hu, Harvard University, USA Katarzyna Matczyszyn, Wroclaw University of Science and 3. Precision Spectroscopy Technology, Poland Hiroyuki Sasada, University of Tokyo, Japan Joyce Poon, University of Toronto, Canada Luca Sapienza, University of Southampton, United Kingdom 4. Novel Lasers, Plasmonics, Nanophotonics Giuseppe Strangi, Case Western Reserve University, USA Pieter Kik, CREOL, USA Richard Warburton, University of Basel, Switzerland

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2018FiO Front.indd 27 8/20/18 9:07 AM NOTES ______

28 FiO + LS 2018 • 16–20 September 2018

2018FiO Front.indd 28 8/20/18 9:07 AM Explanation of Session Codes

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 .

FiO + LS 2018 • 16–20 September 2018 29

2018FiO Front.indd 29 8/20/18 9:07 AM 30 FiO + LS 2018 • 16–20 September 2018

2018FiO Front.indd 30 8/20/18 9:07 AM Agenda of Sessions — Monday, 17 September Agenda of Sessions

International Georgetown Georgetown Jefferson Jefferson Lincoln Ballroom Cabinet West East West East West East 07:00–17:30 Registration, Terrace Level Foyer 08:00–10:00 LM1B • LM1C • Carl 08:30–09:15 FM1A • Quantum E. Anderson Visionary: Science I Division of Jan-Erik Laser Science Kallhammer Dissertation Award 09:00–10:00 FM2A • Presentations Visionary: Teri Odom

10:00–10:30 Coffee Break, Concourse Foyer 10:30–12:30 LM3A • LM3B • FM3C • FM3D • FM3E • FM3F • FM3G • Visionary: Quantum Advanced Novel Devic- LIDAR Ap- Biomedical Frontiers of Prem Kumar Science II Beam es, Manufac- proaches and Optics Nanoplas- (ends at (begins at Shaping and turing and the Demands monics: New 11:15) 11:30) Trapping Testing on Optical Materials – Components Active – Slow Light 12:00–18:00 Laser Science Symposium on Undergraduate Research, International Ballroom East 12:30–14:00 Lunch break on your own 12:30–13:30 OSA Therapeutic Laser Applications Technical Group “Birds of a Feather” Networking Lunch, Fairchild West (advanced registration required) 12:30–13:30 OSA Quantum Computing and Communication Technical Group Networking Lunch, Fairchild East (advanced registration required) 14:00–16:00 LM4A • FM4B • Light FM4C • FM4D • A FM4E • FM4F • Quantum – Matter Imaging Realistic Advanced Complex Science III Interaction and Sensing Assessment Microscopy Nanophoton- (ends at 15:15) Technologies of Optics for ics Self-driving Vehicles (panel) 15:00–17:00 OSA Senior Member Workshop, Holmead, Lobby Level (advanced registration required) 16:00–16:30 Coffee Break, Concourse Foyer 16:00–17:00 Meet OSA’s Journal Editors, Concourse Foyer 16:00–17:00 DLS Annual Business Meeting, Georgetown West 16:00–17:00 Foundational Skills of Professional Networking – How First Impressions and Elevator Pitches Lead to Career Success and Longevity, Cabinet 16:00–17:30 OSA Optical Fabrication and Testing Technical Group Knowledge Café, International Ballroom West 16:00–17:30 The Rules of Engagement: Navigating Important Business Relationships, Georgetown East 16:00–18:00 Finishing Touches: A Tutorial in Blender for Cover Art and Figures, Jefferson West 16:00–18:00 OSA Photonic Metamaterials Technical Group Tutorial on Metalens Design and Simulation, Lincoln West 16:00–18:30 Cheeky Scientist Career Development Workshops, Jefferson East 18:00–19:00 OSA Polarization Technical Group Rapid- Fire Presentations & Networking Event, International Ballroom West 18:00–19:00 Workshop: Understanding Unconscious Bias, Georgetown East 18:00–21:00 Awards Ceremony & Reception, Carnegie Institute of Science, 1530 P St. NW (Separate Ticket Required)

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.

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FiO + LS 2018 • 16–20 September 2018 31

2018FiO Agenda.indd 1 8/19/18 8:22 PM Agenda of Sessions — Tuesday, 18 September

International Jefferson Jefferson Lincoln Cabinet Georgetown Ballroom East West East West

07:00–18:00 Registration, Terrace Level Foyer

08:00–09:30 Plenary Session, International Ballroom Center Agenda of Sessions 09:30–15:00 Science & Industry Showcase, Columbia on the Terrance Level 09:30–10:00 Coffee Break 10:00–12:00 Poster Session I and Dynamic E-Posters 10:00–11:00 Rapid Fire Oral Presentations I, Science & Industry Showcase Theater 10:00–15:00 Vehicle Equipped with Ouster LIDAR Demo, Demo Area 10:00–15:00 VR, AR and MR Headset Demo, Demo Area 10:50–11:40 Entrepreneur - That’s French for Crazy Person, Science & Industry Showcase Theater 11:45–12:00 Remarks from the OSA President, Science & Industry Showcase Theater 12:00–13:00 Job Seeker Tutorial - WORKinOPTICS.com, Science & Industry Showcase Theater 12:00–13:00 Lunch 13:00–15:00 Poster Session II and Dynamic E-Posters 13:00–14:00 Rapid Fire Oral Presentations 2, Science & Industry Showcase Theater 13:30–14:00 Coffee Break 14:05–15:00 Leveraging LinkedIn – Building Relationships, Attracting Recruiters, Finding the the Best Jobs and Growing Your Network, Science & Industry Showcase Theater

15:00–16:30 FTu4A • Applied FTu4B • Short FTu4C • FTu4D • Optical FTu4E • LTu4F • Extreme Nanoplasmonics: Pulse Lasers Terahertz Technologies Integrated Laser Science I Solar – Science for Autonomy Nanophotonic Sensing – in Realistic Devices Communication Weather (panel)

16:45–18:15 FTu5A • FTu5B • FTu5C • Novel FTu5D • Optical FTu5E • LTu5F • Extreme Quantum and Semiconductor Lasers and Technologies Topological Laser Science II Near-Field Lasers and SDM Applications for Autonomy Photonics Nanoplasmonics in Unstructured Environments (panel)

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

18:30–20:30 Conference Reception, International Ballroom

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

32 FiO + LS 2018 • 16–20 September 2018

2018FiO Agenda.indd 2 8/19/18 8:22 PM Agenda of Sessions — Wednesday, 19 September Agenda of Sessions

International Jefferson Jefferson Lincoln Cabinet Georgetown Ballroom East West East West 07:30–18:00 Registration, Terrace Level Foyer 08:00–09:00 FW1A • The FW1B • Novel FW1C • FW1D • Quan- FW1E • LW1F • Coming of Lasers and Nanophotonics I tum Sensing for Nanophotonic Novel Lasers, Age for Smart Photodetectors Industry and sensing and Plasmonics, Glasses, AR and Fundamental optomechanics Nanophotonics I VR Physics I 09:15–10:00 FW2A • NAS Decadal LW2B • Visionary: Mark Assessment and Visionary: Mark Bolas Outlook Brongersma Report on Atomic, Molecular, and Optical Science (starts at 09:05) 10:00–15:00 Science & Industry Showcase, Columbia on the Terrance Level 10:00–10:30 Coffee Break 10:00–12:00 Poster Session III and Dynamic E-Posters 10:15–11:15 Rapid Fire Oral Presentations III, Science & Industry Showcase Theater 10:00–15:00 Vehicle Equipped with Ouster LIDAR Demo, Demo Area 10:00–15:00 VR, AR and MR Headsets Demo, Demo Area 11:15–12:15 Frontiers in Funding, Science & Industry Showcase Theater 12:00–13:00 OIDA VIP Industry Leaders Speed Meetings Lunch 12:00–13:00 Lunch 12:20–12:55 Enabling and Entangling the Tools to Innovate in Quantum Technologies 13:00–15:00 Poster Session IV and Dynamic E-Posters 13:00–14:00 Rapid Fire Oral Presentations IV, Science & Industry Showcase Theater 13:30–14:00 Coffee Break 14:05–15:00 Understanding the National Quantum Initiative, Science & Industry Showcase Theater 10:00–12:00 OSA Members, Family and Friends Tour, Tudor Place 15:00–16:30 FW5A • AR and FW5B • Optical FW5C • FW5D • FW5E • LW5F • VR Ecosystems Communications Quantum Quantum Plasmonic and Novel Lasers, Developments Systems Sensing for Nanophotonic Plasmonics, Industry and Materials Nanophotonics Fundamental II Physics II 15:30–17:00 Meet the Physical Review Journal Editors Reception, Monroe 16:45–18:00 FW6A • FW6B • Novel FW6C • Solid FW6D • FW6E • LW6F • New Optical Optical Fibers State Quantum Quantum Meta- and Novel Lasers, Hardware is and Modulators Optics Computing Nanophotonic Plasmonics, Key to Next with Atoms and Devices for Nanophotonics Generation AR Photons I Imaging and III and MR Applications (ends at 18:45) 17:00–19:00 OSA Senior Member Reception, Holmead, Lobby Level 18:15–19:00 Dinner break on your Own 19:00–21:00 Postdeadline Papers (A complete list of presentations and locations will be in the conference update sheet.)

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.

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FiO + LS 2018 • 16–20 September 2018 33

2018FiO Agenda.indd 3 8/19/18 8:22 PM Agenda of Sessions — Thursday, 20 September

International Jefferson Jefferson Lincoln Cabinet Georgetown Ballroom East West East West 07:30–11:00 Registration, Terrace Level Foyer 08:00–09:00 FTh1A • Vision FTh1B • FTh1C • FTh1D • FTh1E • LTh1F • Comfort as a Quantum Shaping Light Quantum Computational/ Precision Laser Agenda of Sessions Key to AR Mass Information and Design Computing Transformation Spectroscopy Adoption of Quantum with Atoms and Optics and Devices Photons II Optics in Computing 09:00–09:15 Break 09:15–10:00 FTh2A • LTh2B • Visionary: Sir Visionary: David Peter Knight DeMille 10:00–10:30 Coffee Break, Concourse Foyer 10:00–16:00 OSA Capitol Hill Meetings, Senate and House Office Buildings, Washington D.C. 10:30–12:30 FTh3A • AR/ FTh3B • FTh3C • FTh3D • FTh3E • LTh3F • VR Applications Quantum Optical Comb Quantum Information Advances in for Enterprise Electronics Metrology Communications Processing, Molecular and Consumer and the Future Information Spectroscopy Markets Quantum Display and Internet Optical Device

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

34 FiO + LS 2018 • 16–20 September 2018

2018FiO Agenda.indd 4 8/19/18 8:22 PM International Georgetown West Georgetown East Ballroom East FiO LS

08:30–09:15 08:00–10:00 08:00–10:00 FM1A • Visionary: Jan-Erik LM1B • Quantum Science I LM1C • Carl E. Anderson Kallhammer Presider: Evan Meyer-Scott; Universität Division of Laser Science Presider: Sabbir Rangwala; Paderborn, Germany Dissertation Award Patience Consulting LLC, USA Presentations LM1B.1 • 08:00 LM1C.1 • 08:00 Hong-Ou-Mandel Effect Between Single-Photon Source and Thermal Light, Elisha Frequency Comb Generation from Laser 1 2 1 1 2 Siddiqui , Tim Byrnes , Jonathan P. Dowling ; Louisiana State Univ., USA; New York Diodes, Mark Dong1, Herbert G. Winful1, Univ., China. We describe the theory of Hong-Ou-Mandel (HOM) interference, between Steven T. Cundiff1; 1Univ. of Michigan, USA. a single photon source and thermal light and demonstrate the maximum visibility We model and experimentally characterize Monday, 17 Septem attainable for non-ideal single photon resources. frequency combs generated from laser diodes. Their optical and RF spectra are measured LM1B.2 • 08:15 and analyzed. Quantum-Limited Discrimination between Laser Light and Noise, Jonathan Habif1, Saikat Guha2; 1Information Sciences Inst., Univ. of Southern California, USA; 2College of Optical Sciences, Univ. of Arizona, USA. We evaluate quantum limits and structured receiver performance for discriminating between a mode excited in a thermal or a coherent state, and show an interesting inversion in receiver performance going from single-shot to collective measurements. LM1C.2 • 08:30 FM1A.1 • 08:30 VISIONARY LM1B.3 • 08:30 ber Characterizing Photon Statistics in an Unbalanced Beam Splitter, Hamed Pourbey- An Optical Frequency Atomic Clock Based On From Night Vision to LiDAR: An Auto- 2,3 ram1, Cody Bassett1, Arash Mafi1; 1Univ. of New Mexico, USA. A theoretical framework Quantum Matter, Sara L. Campbell , Ross B. motive Perspective, Jan-Erik Kallham- Hutson2,3, G. E. Marti2, Akihisa Goban2, Nelson 1 1 has been developed and examined experimentally for photon statistics in an unbalanced mer ; Autoliv Sverige AB, Sweden. Work 2 2,3 beam splitter. We show that it is possible to determine the photon statistics of a lights D. Oppong , Rees L. McNally , Lindsay Son- is underway to complement cameras and 2,3 2,3 2 source without coincidence counting. derhouse , John M. Robinson , Wei Zhang , radar with LiDAR in serial automotive use. Benjamin J. Bloom2,3, Jun Ye2,3; 2JILA, NIST There are many considerations besides 3 LM1B.4 • 08:45 and Univ. of Colorado, USA; Dept. of Physics, technical challenges to be made before Quantum Enhanced Measurement Using SU(1,1) Interferometer with Dual-beam Univ. of Colorado, USA. We present the first LiDAR can be launched as a serial product. Sensing, 1 1 1 1 1 1,2 atomic clock based on quantum degenerate The talk will draw on experiences of taking Yuhong Liu , Jiamin Li , Liang Cui , Nan Huo , Xiaoying Li , Zheyu Ou ; 1 2 matter, which reaches a record spectroscopic Night Vision to the automotive market. Tianjin Univ., China; Dept. of Physics, Indiana Univ.-Purdue Univ. Indianapolis, USA. Using an SU(1,1) interferometer with dual-beam as the sensing field, we experimentally quality factor of Q = 5.2e15 and can measure demonstrate the sensitivity of phase measurement is 2.4 dB higher than the standard a frequency difference to 3e-19 in 2 hours. quantum limit achieved by directly measuring a probe beam.

LM1B.5 • 09:00 LM1C.3 • 09:00 Observation of One-way Einstein-Podolsky-Rosen Steering, Sabine Wollmann1,2, Travis Coupling Atoms Through An Optical Nano- 09:15–10:00 J. Baker2, Nathan Walk2,3, Adam Bennet2, Nora Tischler2, Howard M. Wiseman2, Geoff J. fiber Waveguide, Pablo Solano1,2; 1Joint Pryde2, Jonathan C. Matthews1; 1Univ. of Bristol, UK; 2Griffith Univ., Australia; 3Dept. of Quantum Inst. and Dept. of Physics, Univ. of FM2A • Visionary: Teri Odom Computer Science, Univ. of Oxford, UK. We prove and experimentally demonstrate that Maryland, USA; 2Dept. of Physics and Research Presider: Ortwin Hess; Imperial EPR-steering can be rigorously asymmetric, unlike Bell tests, by constructing quantum Lab of Electronics, MIT, USA. We present our College, London, UK states which are steerable in one direction, whilst two-way steering is impossible with results on using ultra-high transmission op- arbitrary quantum measurements. tical nanofibers to couple cold atoms to the evanescent field a guided electromagnetic LM1B.6 • 09:15 FM2A.1 • 09:15 VISIONARY mode, and realizing infinite-range atom-atom Generation of Photon-Subtracted Two-Mode Squeezed Vacuum States, Roberto Peering Through the Looking Glass: The interactions mediated by the guided field. d. Leon Montiel1, Omar Magana Loaiza2, Armando Perez Leija3,4, Alfred U’Ren1, Kurt Next Frontier in Nano-Optics, Teri W. Busch3,4, Adriana E. Lita2, Saw W. Nam2, Thomas Gerrits2, Richard Mirin2; 1Instituto de Odom1; 1Northwestern Univ., USA. Over Ciencias Nucleares, Universidad Nacional Autónoma de Mexico, Mexico; 2National the past decade, significant progress in Inst. of Standards and Technology, USA; 3Max-Born-Institut, Germany; 4Inst. für Physik, controlling light-matter interactions at Humboldt-Universität zu Berlin, Germany. We experimentally demonstrate that the the nanoscale has been achieved. Most simultaneous subtraction of photons from a two-mode squeezed vacuum state leads of the advances, however, have relied to the generation of entangled states with increasingly larger average photon number. on fixed systems limited to as-fabricated nanostructures and singly periodic arrays LM1B.7 • 09:30 and simple unit cells. This visionary talk LM1C.4 • 09:30 Tailored photon-pair generation in optical fiber through dual-pump spontaneous will discuss how the ability to engineer Manipulation of Photonic Quantum States: four-wave mixing, Yujie Zhang1, Ryan Spiniolas1, Kai B. Shinbrough1, Fang Bin1, Offir complex nanophotonics responses—on From Generation, Engineering, and Char- Cohen1, Virginia O. Lorenz1; 1Dept. of physics, Univ. of Illinois at Urbana-Champaign, demand—may address key challenges acterization To Storage And Retrieval, Bin USA. We experimentally tailor the joint spectra of photon pairs produced via dual-pump 1 1 and open unexpected possibilities in Fang ; Dept. of Physics, Univ. of Illinois at Ur- spontaneous four-wave mixing, achieving a joint spectral intensity without sidelobes, nanoscale optics. We will highlight new bana-Champgian, USA. We present our work presenting a new route towards generating spectrally uncorrelated photon pairs. designs in topological photonics, stimu- on various critical aspects of manipulation li-responsive nanostructured substrates for of photonic quantum states, including the LM1B.8 • 09:45 tunable nano-lasing and reconfigurable generation of entangled states, engineering Generation of quantum correlated photons in different spatial modes using few- lensing, and prospects of multi-periodic of the spectral correlations of photon-pairs, mode fibers, Cheng Guo1, Jie Su1, Zhenzhen Zhang1, Liang Cui1, Xiaoying Li1; 1Tianjin structured materials. characterization of quantum states and ul- Univ., China. We generate photon pairs at 1550 nm telecom through the intermodal tra-broadband storage.

four-wave mixing between LP01 and LP11 mode in a few-mode fiber. The ratio of coinci- dence to accidental coincidence rates is measured to be 28.

10:00–10:30 Coffee Break, Concourse Foyer

FiO + LS 2018 • 16–20 September 2018 35

FiO Abstracts.indd 1 8/20/18 9:11 AM International Georgetown Georgetown Jefferson Ballroom East West East West LS FiO

10:30–11:15 11:30–12:30 10:30–12:30 10:30–12:30 LM3A • Visionary: Prem Kumar LM3B • Quantum Science II FM3C • Advanced Beam FM3D • Novel Devices, Presider: Peter Delfyett; Presider: Peter Rakich; Yale Shaping and Trapping Manufacturing and Testing. University of Central Florida, University, USA Presider: Carlos Lopez-Mariscal ; Presider: Jamie Ramsey; RPO, USA Underwater Photonics, USA USA

FM3D.1 • 10:30 LM3A.1 • 10:30 VISIONARY FM3C.1 • 10:30 Invited Performance of an Adaptive Optics Quantum Communication and Network- Structured Light-Matter Interactions in System in the Presence of Diffractive 1 1 Nano-Engineered Nonlinear Photonic ing, Prem Kumar ; Northwestern Univ., 1 1 Media, Natalia M. Litchinitser1, Jingbo Grooves, Emily Finan , Tom D. Milster , USA. Machines that process quantum 1 1 1 1 2 Youngsik Kim ; Univ. of Arizona, USA. information are likely to be commercially Sun , Wiktor Walasik , Salih Silahli , Yun 2 1 3 Diffractive phase introduced by light ber available in the near future. Networking Xu , Mikhail Shalaev , Jesse Frantz , Jason 3 4 reflected from grooves on optical stor- them via quantum communication to Myers , Robel Bekele , Jasbinder Sang- 3 5 1 age media might be problematic for AO achieve a higher level of performance is hera , Alexander Tsukernik ; Duke Univ. , 2 correction in high-performance systems. a topic of current interest. In this talk I will USA; Univ. at Buffalo, The State Univ. of 3 Simulations and experiments are present- review the current status and speculate on New York, USA; US Naval Research Lab, 4 ed to examine the performance of AO the future possibilities. USA; Univ. Research Foundation, USA; 5Univ. of Toronto, Canada. We discuss with media samples. theoretical and experimental studies of the nonlinear beam shaping in engineered FM3D.2 • 10:45 nano-colloidal suspensions with negative Three-dimensional Direct Laser Writing polarizability and saturable nonlinearity of Ultra-low Density Neuron-inspired Monday, 17 Septem Monday, 1 and in all-optically reconfigurable chalco- Steiner Tree Structures, Haoyi Yu , 1 1 1 genide glass based metasurfaces. Qiming Zhang , Min Gu ; RMIT Univ., Australia. We fabricate neuron-inspired Steiner tree structures using the three-di- mensional direct laser fabrication method. An ultra-low density three-dimensional Steiner tree structure with the feature size of 1 µm is achieved.

FM3C.2 • 11:00 FM3D.3 • 11:00 Full-Field Optical Coherence Tomogra- Self-imaging of Azimuthal Intensity Pet- phy Using Acousto-Optically Tuned Ex- al Based on Orbital Angular Momentum ternal-Cavity Laser Diode and Wavelet Beams, Jianqi Hu1, Camille-Sophie Bres1, Transform, Takamasa Suzuki1, Gen Suda1, Chen-Bin Huang2; 1École polytechnique Samuel Choi1, Osami Sasaki1; 1Niigata fédérale de Lausanne, Switzerland; Univ., Japan. An acousto-optically tuned 2National Tsing-Hua Univ., Taiwan. We external-cavity laser diode using Littrow demonstrate for the first time azimuthal configuration is proposed. The thickness Talbot effect based on orbital angular distribution of a cover glass was obtained momentum beams. The intensity petal is using this light source with maximum self-imaged in the azimuthal angle. We scanning range of 45 nm and continuous also draw the analogy between azimuthal wavelet transform. and temporal Talbot effect.

FM3C.3 • 11:15 FM3D.4 • 11:15 The zoo of topological singularities Development of Flexible Pad Polishing in 2D random waves: from phase and for Freeform Surface, Vinod Mishra1,2, polarization singularities to polarization Daliramu Burada2, Vinod Karar1, Alakesh 1 vortices, Lorenzo De Angelis , Filippo Manna3, Gufran Khan2; 1Optical Devices 1 1 1 Alpeggiani , L. Kuipers ; Kavli Inst. of and System, CSIR-CSIO, India; 2IDDC, IIT Nanoscience, Delft Univ. of Technology, Delhi, India; 3Mechanical Engineering, Netherlands. With experiments and the- PEC Chandigarh, India. A method for ory, we demonstrate that the correlation polishing of freeform mould is demon- of C points in random light undergoes strated by using flexible pad polishing on dramatic changes when confining waves a diamond turning machine. The results propagation to 2D, concluding a com- show that the presented polishing setup prehensive overview on topological is capable to polish low slope freeform singularities in random light. optics.

LM3B.1 • 11:30 Invited FM3C.4 • 11:30 FM3D.5 • 11:30 Engineering Integrated Sources of En- Measuring Geometric Phase Without In- Describing Mid-Spatial Frequencies tangled Photon Pairs, Evan Meyer-Scott1, terferometry, Rodrigo Gutiérrez-Cuevas1, consistently for Optical Design, Man- Nidhin Prasannan1, Nicola Montaut1, Tanya Malhotra1, Jeremy Hassett1, Mark R. ufacturing and Metrology, Sven Wick- Johannes Tiedau1, Georg Harder1, Linda Dennis2,3, Anthony N. Vamivakas1, Miguel enhagen1, Anna Möhl1, Ulrike Fuchs1; Sansoni1, Harald Herrmann1, Christof A. Alonso1,4; 1Univ. of Rochester, USA; 1Asphericon GmbH, Germany. This paper Eigner1, Raimund Ricken1, Viktor Quir- 2Univ. of Bristol, UK; 3Univ. of Birmingham, is dealing with different specifications and ing1, Tim J. Bartley1, Sonja Barkhofen1, UK; 4Aix Marseille Universite, Centrale tolerancing of Mid-spatial frequency (MSF) Christine Silberhorn1; 1Univ. of Paderborn, Marseille, Institut Fresnel, France. A for aspheric and freeform surfaces. Various Germany. We present progress on our simple, non-interferometric method for models are discussed with respect to suit- optimization of photon pair sources us- measuring geometric phases of struc- ability for optical design, manufacturing, ing waveguides. The sources show high tured-Gaussian beams is presented. By and metrology. heralding efficiency, indistinguishability, studying the intensity distribution of an brightness, and entanglement visibility, occluded beam, the Gouy and Pancharat- and require low pump power. nam-Berry phases can be determined.

36 FiO + LS 2018 • 16–20 September 2018

FiO Abstracts.indd 2 8/20/18 9:11 AM Jefferson Lincoln East West Cabinet FiO

10:30–12:35 10:30–12:30 10:30–12:30 FM3E • LIDAR Approaches and the FM3F • Biomedical Optics FM3G • Frontiers of Nanoplasmonics: New Demands on Optical Components Presider: David Busch; UT Southwestern Materials – Active – Slow Light Presider: Sabbir Rangwala; Patience Medical Center at Dallas, USA Presider: Ortwin Hess; Imperial University, Consulting LLC, USA UK

FM3F.1 • 10:30 Invited FM3G.1 • 10:30 Invited FM3E.1 • 10:30 Invited From Man To Mouse: Translational Studies in Stroke Solids in Ultrafast Strong Laser Fields: Optical Control Think like a Robot, Perceive like a Human, Barry Behnken, Recovery, Adam T. Eggebrecht1, Adam Q. Bauer1; 1Ra- of Electronic State, Mark Stockman1; 1Georgia State AEye, Inc., USA. AEye is an artificial perception pioneer

diology, Washington Univ. in Saint Louis, USA. This joint Univ., USA. When a strong optical field with amplitude Monday, 17 Septem whose multi-sensor iDAR technology brings the power of talk will cover 1) Bedside neuromonitoring with high den- comparable to the internal fields acts on a solid, it creates, agile scanning and edge computing to the LiDAR market, sity DOT during the acute phase of stroke recovery and 2) for a femtosecond duration of the pulse, a new state of changing the way all autonomous vehicles perceive the Understanding and optimizing endogenous mechanisms solid where fundamental properties are modified. environment. of stroke recovery in mouse models of stroke. ber

Invited FM3E.2 • 10:54 FM3F.2 • 11:00 FM3G.2 • 11:00 Invited Geiger-mode LiDAR for Autonomous Vehicles , Mark Evaluation of Oximetry Measurement Accuracy of Nanophotonics with metal nitrides and carbides: Itzler, Argo AI LLC, USA. We describe disruptive automo- Multispectral Photoacoustic Imaging Systems Using from bulk to 2D, Alexandra Boltasseva1; 1Purdue Univ., tive Geiger-mode LiDAR performance essential to future a Dynamically Tunable Blood Flow Phantom, Xuewen USA. We explore emerging materials for nanophotonics, autonomous vehicle navigation enabled by the combination 1 1 1 1 Zhou , William C. Vogt , Rudy Andriani , Keith Wear , plasmonics and optical metasurfaces namely transition of single-photon sensitivity and greater eye-safety at wave- 1 1 1 Brian Garra , Joshua Pfefer ; US Food and Drug Ad- metal nitrides and carbides in their bulk, ultra-thin and lengths beyond 1400 nm. ministration, USA. A blood flow phantom with tunable 2D form known as MXenes for applications in on-chip oxygen saturation (SO ) was developed as an oximetry 2 circuitry, sensing, energy. performance test method for emerging photoacoustic imaging systems. Results highlight the importance of flu-

ence corrections in improving SO2 measurement accuracy.

FM3E.3 • 11:18 Invited FM3F.3 • 11:15 Next Generation Compact LIDAR Systems: Making Every Porcine Tissues Characterization by Diffuse Reflectance Photon Count, Angus Pacala, Ouster, USA. Ouster has Spectroscopy, Felix Fanjul-Velez1, Jose Luis Arce-Diego1; developed the world’s first compact, long range imaging 1Univ. of Cantabria, Spain. Biological tissues characteri- LIDAR employing single photon avalanche diode detectors zation can be made by diffuse reflectance spectroscopy in standard CMOS. This talk will review our approach, some (DRS). Tissue discrimination is critical in surgery. In this unique advantages of the CMOS SPAD architecture, as well work data from porcine tissues are statistically analyzed as future outlook for the technology and challenges still to for estimating discrimination potential. be overcome.

FM3F.4 • 11:30 Invited Pulsed-Laser-Induced Modification of Gold Nanorods: FM3G.3 • 11:30 Damage Thresholds and Impact on Photoacoustic Bose-Einstein Condensation and Ultrafast Lasing in a 1 1 Imaging in Turbid Media, Andrew M. Fales1, William Plasmonic Lattice, Paivi Torma , Tommi Hakala , Antti 1 1 1 Vogt1, Keith Wear1, Ilko Ilev1, Joshua Pfefer1; 1U.S. Food Moilanen , Aaro Väkeväinen , Rui Guo , Jani-Petri Marti- 1 1 1 and Drug Administration, USA. Nanorod reshaping kainen , Konstantinos Daskalakis , Heikki Rekola , Aleksi 1 1 during photoacoustic imaging (PAI) may severely impact Julku ; Aalto Univ., Finland. We demonstrate a Bose-Ein- performance. Nanorod damage thresholds were studied stein condensate (BEC) of surface plasmon polaritons in with electron microscopy and spectrophotometry, and lattice modes of a metal nanoparticle array interacting the effect of laser exposure on PAI was studied in a with molecules. A crossover from BEC to ultrafast lasing turbid phantom. is realized by tailoring the band structure.

FiO + LS 2018 • 16–20 September 2018 37

FiO Abstracts.indd 3 8/20/18 9:11 AM International Georgetown Georgetown Jefferson Ballroom East West East West LS FiO

LM3B • Quantum Science II— FM3C • Advanced Beam FM3D • Novel Devices, Continued Shaping and Trapping— Manufacturing and Testing— Continued—Continued Continued

FM3D.6 • 11:45 FM3C.5 • 11:45 Vibration Testing and Thermal Vacuum Generation of Quantum Airy Photons, Flight Qualification of NASA’s Global Santosh Kumar1, Stephanie Maruca1, Yong Ecosystem Dynamics Investigation Meng Sua1, Yu-Ping Huang1; 1Dept. of (GEDI) Laser Transmitters, Furqan Chira- Physics, Stevens Inst. of Technology, USA. gh3, Donald B. Coyle1, Erich Frese2, Paul Airy beams have been studied for many R. Stysley1; 1NASA Goddard Space Flight exciting applications. Here we extend Center, USA; 2ASRC Federal Space and those studies to the quantum domain Defense, USA; 3Velos LLC, USA. The GEDI ber by creating quantum-correlated photons Mission will employ three lasers systems in Airy spatial modes and explore their developed, built, and tested by NASA potential applications. Goddard Space Flight Center. We discuss the flight level Thermal Vacuum (TVAC) and vibrational qualification testing each unit must pass.

LM3B.2 • 12:00 Invited FM3C.6 • 12:00 FM3D.7 • 12:00 Invited Optical-Fiber Source of Energy-Entan- Huygens Dipole for Nanolocalization, Electrically Tunable Liquid Crystal gled Three-Photon W-State, Virginia O. 1,2 1,2 Monday, 17 Septem Monday, Ankan Bag , Martin Neugebauer , Lenses for Augmented Reality, Yi-Hsin Lorenz1; 1U. Illinois at Urbana-Champaign, 1,2 1,2 Pawel Wozniak , Gerd Leuchs , Peter Lin1; 1National Chiao Tung Univ., Taiwan. USA. We experimentally demonstrate an 1,2 1 Banzer ; Max Planck Inst. for the Sci- We demonstrate an optical-see-through energy-entangled three-photon W-state 2 ence of Light, Germany; Inst. of Optics, system via liquid crystal lenses for aug- source based on spontaneous four-wave Information and Photonics, Dept. of mented reality (AR) in order to solve the mixing in polarization-maintaining optical Physics, Friedrich-Alexander-Univ. Erlan- challenges of vision correction and image fiber. We characterize the source using gen-Nuremberg, Germany. We discuss a registration. The optical zoom function is reduced density-matrix tomography, with- nanolocalization technique with sub-nano- also added in the AR system. out the need for frequency conversion. meter localization resolution based on position dependent transverse Kerker scattering, obtained via interference of tailored electric and magnetic dipole moments.

FM3C.7 • 12:15 Arrays of dark optical traps on a toroidal surface, Jakub Belin1, Vassilis Lembessis2, Andreas Lyras2, Omar Aldossary2,3, Jo- hannes K. Courtial1; 1Univ. of Glasgow, UK; 2Dept. of Physics and Astronomy, College of Science, King Saud Univ., Saudi Arabia; 3The National Center for Applied Physics, KACST, Saudi Arabia. We have theoreti- cally constructed light fields containing arrays of dark optical traps distributed on the surface of a torus. The array di- mensions are not diffraction-limited and their period can be, in principle, deeply sub-wavelength.

12:00–18:00 Laser Science Symposium on Undergraduate Research, International Ballroom East

12:30–14:00 Lunch break on your own

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FM3E • LIDAR Approaches and the FM3F • Biomedical Optics—Continued FM3G • Frontiers of Nanoplasmonics: New Demands on Optical Components— Materials – Active – Slow Light—Continued Continued

FM3F.5 • 11:45 Invited FM3E.4 • 11:42 Supercontinuum Laser for Spectroscopic Photoacous- Integrated Optical Phased Arrays for Solid-State LiDAR, tic Imaging of Lipids in the Extended Near-Infrared Matthew Byrd; Analog Photonics, USA. LiDAR with integrat- Region, Manoj Kumar Dasa1, Christos Markos1, Michael ed optical phased arrays provides an attractive solution to Maria1, Ivan Gonzalo1, Christian Petersen1, Peter Morten the automotive industry by enabling solid-state, small form Moselund2, Ole Bang1,2; 1Technical Univ. of Denmark, factor systems. Here, we review this technology and present Denmark; 2NKT Photonics, Denmark. We demonstrate Monday, 17 Septem beam steering and real-time coherent LiDAR results. a cost-efficient high-power supercontinuum laser source based on a telecom range diode laser system and few meters of a standard optical fiber for spectroscopic photoacoustic imaging of lipids in the extended near-in- frared region.

FM3F.6 • 12:00 Invited FM3G.4 • 12:00 Invited Lowering the Cost and Improving the Usability of Non-Equilibrium Photonics with Self-Adaptive Order, ber Retinal Imaging and Visual Function Assessment, Ann Xiang Zhang1, Chad Ropp1, Nicolas Bachelard1, David E. Elsner1,2, Matthew S. Muller2, Joel Papay1, Bryan P. Barth1, Yuan Wang1; 1UC Berkeley, USA. Structures driven Haggerty1, Thomas J. Gast1,2, Stephen A. Burns1; 1Indiana far from thermodynamic equilibrium can self-organize Univ., USA; 2Aeon Imaging, LLC, USA. Cost, size, and and behave as artificial living matter. We show how such complexity are all barriers to the use of improved optical dynamic order emerges in an array of initially disorganized technology to provide eye care. Resolution, wavelength, photonic resonators, coupled through thermo-optic and computer-assisted detection of imagers can be tar- feedback. geted to the optical signature of biomarkers.

FM3E.5 • 12:06 Invited A vehicle platform perspective on 3D sensing, Matthew Weed, Luminar Technologies, USA. Photons are the currency of LiDAR design, but time is the currency of self-driven vehi- cles. High-resolution, long-range 3D data with low latency gives these vehicles enough time to make safe, informed decisions about their environment.

12:00–18:00 Laser Science Symposium on Undergraduate Research, International Ballroom East

12:30–14:00 Lunch break on your own

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14:00–16:00 14:00–16:00 14:00–16:00 LM4A • Quantum Science III FM4B • Light – Matter Interaction FM4C • Imaging and Sensing Technologies Presider: Peter Rakich; Yale University, USA Presider: To be Determined Presider: Byoungho Lee; Seoul National University, South Korea

LM4A.1 • 14:00 Invited FM4B.1 • 14:00 Invited FM4C.1 • 14:00 Invited 1 Photons Probe Processes in the Brain, Robert R. Alfano ; Motion Rectification and Transport Control in 2D Fundamental Limits in Imaging: A Computational 1 1 CUNY City College, USA. The salient properties of pho- Optical Brownian Ratchets, Karen. Volke-Sepulveda , Imaging Approach, Amit Ashok1; 1Univ. of Arizona, USA. 1 1 tons as they enter and excite quantum processes in brain Alejandro Vasquez Arzola , Mario Villasante-Barahona , While the computational imaging approach has been 2 2 1 tissue: spin and orbital angular momentum, complex wave Petr Jakl , Pavel Zemanek ; Univ Nacional Autonoma de explored and applied to various imaging problems, such 2 front, polarization, classical and quantum entanglement Mexico, Mexico; Inst. of Scientific Instruments of CAS, as compressive imaging, it is has been only shown recently will be presented. Czechia. We create a reconfigurable 2D ratchet formed that it can achieve fundamental limits using rigorous with a static asymmetric potential, based on holographic information-theoretic analysis.

ber optical micromanipulation techniques, and an unbiased driving generating a rocking mechanism. Motion rectifi- cation is obtained along different directions.

LM4A.2 • 14:30 FM4B.2 • 14:30 FM4C.2 • 14:30 Invited Correlation Properties of Photon Pairs Generated near Multi-photon Fabrication of Compact Low-loss Optical Progress on Optical Trap Volumetric Displays, Daniel 1 the Pump in the Normal Group-Velocity-Dispersion Waveguides in Polydimethylsiloxane, Giulia Panusa , Ye Smalley1, Erich Nygaard1, Wesley Rogers1, Kamran 1 1 1 1 1 1 1 Regime, Kyungdeuk Park , Dongjin Lee , Yong Sup Ihn , Pu , Jieping Wang , Christophe Moser , Demetri Psaltis ; Qaderi1; 1Brigham Young Univ., USA. We review the fun- 1 1 1 1 Yoon-Ho Kim , Heedeuk Shin ; POSTECH, South Korea. EPFL, Switzerland. We report the fabrication of compact damentals photophoretic trap displays and discuss the We present photon pairs generated near the pump flexible optical waveguides in polydimethylsiloxane possibility of creating occlusion capable image points. wavelength in the normal GVD regime by spontaneous through multiphoton direct laser writing, for the first time

Monday, 17 Septem Monday, Anisotropic scattering is observed independently in single four-wave mixing. The generated photons have temporal without a photoinitiator. A transmission loss of 0.03 dB/ and double point traps. and spectral correlations and can be exploited as tele- cm was measured in the 650-700 nm band. com-band quantum light sources.

FM4B.3 • 14:45 Invited LM4A.3 • 14:45 Probing lipid membranes with vibrational sum-fre- Quantum Acoustics: Controlling Phonons Using Light quency scattering, Jan Dedic2,1, Halil Okur2, Sylvie and Superconducting Circuits, 1 1 Peter Rakich ; Yale Roke2; 1EPFL Photonics Chapter, Switzerland; 2Lab Univ., USA. We demonstrate powerful new strategies to for Fundamental Biophotonics, EPFL, Switzerland. To control high frequency (10-40GHz) bulk acoustic phonons understand how biological membranes work we must using optomechanical interactions and superconducting study the behavior of their constituent molecules in-situ. circuits. We identify a path towards robust ground-state With vibrational sum-frequency scattering, we now have control in cavity optomechanics and realize complex a non-invasive way of accessing this information. quantum states using circuit QED techniques.

FM4B.4 • 15:00 FM4C.3 • 15:00 Advanced Multiphoton Polymerization Using Tunable Digital Aberration Correction with Single-Pixel Spatial 1 Shaped Laser Wavepackets, MARIA MANOUSIDAKI1,2, Frequency Projection Imaging, Jeffrey J. Field , Jeff 2 1 1 2 Vladimir Y. Fedorov3,4, Dimitrios G. Papazoglou1,2, Maria Squier , Randy Bartels ; Colorado State Univ., USA; Col- Farsari1, Stelios Tzortzakis3,1; 1IESL-FORTH, Greece; orado School of Mines, USA. We show that single-pixel 2Materials Science and Technology Dept., Univ. of Crete, with CHIRPT microscopy encodes optical aberrations in Greece; 3Texas A&M Univ. at Qatar, Qatar; 4Lebedev temporal modulations of fluorescent light emitted from Physical Inst. of the Russian Academy of Sciences, Russia. a specimen. We recover aberrations from several test Tunable abruptly autofocusing ring Airy beams enable objects and remove them digitally after image collection. advanced multiscale photo-polymerization. Scaling down to the paraxial regime, these beams can approach the wavelength limit while presenting a strong enhancement of their focal intensity.

FM4B.5 • 15:15 FM4C.4 • 15:15 Evidence of Magnetic Torque Dynamics in Optical- Towards Scalable Fabrication of Plasmonic Colour via ly-induced Magnetization, Krishnandu Makhal1, Minh Nanoimprint Lithography, Muhammad F. Shahidan1, T. Trinh1, Stephen C. Rand1,2; 1Electrical Engineering Jingchao Song1, Evgeniy Panchenko1, Paul Mulvaney2, and Computer Science, Univ. of Michigan, USA; 2Dept. Timothy James1,3, Ann Roberts1; 1School of Physics, The of Physics, Univ. of Michigan, USA. Rotational assign- Univ. of Melbourne, Australia; 2ARC Centre of Excellence ments and polarization states of inelastic components in Exciton Science, Bio 21 and School of Chemistry, The in the cross-polarized spectrum of light scattered by Univ. of Melbourne, Australia; 3Reserve Bank of Australia, liquid samples of tetrahedral molecules provide direct Australia. We demonstrate the versatility of nanoimprint evidence of a theorized enhancement mechanism for lithography to fabricate scalable ‘plasmonic pixels’ which induced magnetism. producing non-diffractive color. Several designs are pres- ent and the colors produced shows their dependence upon the direction of polarization.

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14:00–16:00 14:00–16:00 14:00–16:00 FM4D • A Realistic Assessment of Optics FM4E • Advanced Microscopy FM4F • Complex Nanophotonics for Self-driving Vehicles Presider: Felix Fanjul Velez; University of Presider: Ortwin Hess; Imperial University, Moderator: Sabbir Rangwala, Patience Cantabria, Spain UK Consulting LLC, USA FM4E.1 • 14:00 Invited FM4F.1 • 14:00 Invited Optical Imaging for Cardiac Ablation, Christine P. Hen- Structuring Light with Metastructures, Nader Engheta1; LIDAR and other ADAS (Advanced Driver Assistance Sys- don1; 1Columbia Univ., USA. I will discuss developments 1Dept. of Electrical and Systems Engineering, Univ. of tems) imaging technologies promise to enable driverless within optical coherence tomography and near infrared Pennsylvania, USA. Sculpting waves with metamaterials cars, with potentially wide-ranging impacts to the vehicle spectroscopy to enable monitoring of cardiac radiofre- may lead to useful functionalities. In this talk, I will present manufacturing industry, vehicle-enabled services such as quency ablation, including extraction information on en- several scenarios in which metastructures and metasur- trucking and taxis, shared transportation and urban planning.

ergy delivery, tissue composition, and fiber orientations. faces can be used as platforms for structured light with Monday, 17 Septem But how close are we to ramping production for actual desired features. vehicle sales? What are the hurdles ahead for LIDAR and other optical systems and components? Where else does optics play a role in autonomous vehicles? What other factors impact the success of these optical technologies, from narrow technical issues to broader issues of regulation, FM4E.2 • 14:30 standards, safety and customer acceptance? This panel of FM4F.2 • 14:30 Invited Fiber-Laser-Based Ultrasound Sensors for Fast-Scan- Topological Photonics in Gyroids: 3D Nano-Printing experts will conduct a lively discussion of these issues on 1 ning in vivo Photoacoustic Microscopy, Long Jin , Yizhi of Weyl Points, Min Gu1, Benjamin P. Cumming1; 1Royal this timely subject. 1 2 1 1 Liang , Lidai Wang , Jinwei Liu ; Inst Photonics Tech, Melbourne Inst. of Technology, Australia. The gyroid is a Jinan Univ, China; 2Dept. of Mechanical and Biomedical

Panelists: useful platform for the study of topological photonics. In ber Engineering, City Univ. of Hong Kong, Hong Kong. We Brandon Collings, Lumentum, USA this talk we demonstrate the creation and characterization present a new fiber-laser-based ultrasound sensor with Kevin Dopart, US Department of Transportation, USA of gyroid Weyl points at optical frequencies using 3D high sensitivity and large field-of-view, based on which Rob Murano, II-VI Inc., USA Nano-Printing and high refractive-index coating. a fast-scanning optical-resolution photoacoustic micro- Martin Zirngibl, Finisar, USA scope was built for in vivo microvascular imaging with a frame rate of 2 Hz.

FM4E.3 • 14:45 Quantification of Staphylococcus aureus on Contact Lenses using Mobile Holographic Imaging of Curved Surfaces and Machine Learning, Muhammed Veli1, Aydogan Ozcan1; 1Electrical and Computer Engineer- ing, Univ. of California, Los Angeles, USA. We present a cost-effective mobile sensor based on 3D imaging of contact lenses and machine learning for quantification of Staphylococcus aureus. Compatible with human tear, this wearable-sensor can detect various pathogens and analytes in tear.

FM4E.4 • 15:00 FM4F.3 • 15:00 Invited Chip-based Total Internal Reflection Fluorescence Next Generation Photonics Based on 2D Materials, 1,3 2 Microscopy, Vishesh Kumar Dubey , Rajwinder Singh , Michal Lipson1; 1Columbia Univ., USA. Two dimensional 1,3 1 3 Azeem Ahmad , Dalip S. Mehta , Balpreet S. Ahluwalia ; materials such as monolayer transition metal dichalco- 1 2 Indian Inst. of Technology Delhi, India; Cell Biology and genides (TMD) are expected to have large changes in 3 Biophysics Unit, EMBL, Germany; Dept. of Physics and their optical sheet conductivity by controlling their carrier Technology, UiT The Arctic Univ. of Norway, Norway. In densities. We demonstrate a platform for waveguide-in- present study we have performed total internal reflection tegrated phase modulators in the nearinfrared regime fluorescence microscopy on optical waveguide chip. This based on Tungsten disulphide (WS2) gating. enables large field of view of imaging with high axial solution and signal to noise ratio with low phototoxicity.

FM4E.5 • 15:15 Holographic Region-of-Interest with Oblique Illumina- tion, Alexander Jügler1, Jan Becker1, Patrick Then1, Rainer Heintzmann1,2; 1Leibniz Inst. of Photonic Technology, Germany; 2Inst. of Physical Chemistry and Abbe Center of Photonics, Friedrich-Schiller-Univ. Jena, Germany. Our programmable holographic microscopy approach allows an adaptive oblique regions-of interest illumination. This reduces phototoxicity and out-of-focus blur and improves potentially Single-Molecule-Localization-Microscopy while easy to integrate.

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LM4A • Quantum Science III—Continued FM4B • Light – Matter Interaction— FM4C • Imaging and Sensing Continued Technologies—Continued

FM4B.6 • 15:30 FM4C.5 • 15:30 Remote Detection Sodium Cell Magnetometry using Incorporating Polarization into Phase Retrieval Meth- Amplitude Modulated Light, Renu Tripathi1, Christiane ods, Scott Paine1, James R. Fienup1; 1Univ. of Rochester, Ebongue1, Lorna Caesar1, Gour S. Pati1, Anthony Yu2, Mi- USA. Traditional wavefront-sensing phase retrieval prob- chael Krainak2; 1Delaware State Univ., USA; 2NASA GSFC, lems often neglect the effects of polarization. In order to USA. We investigated performance of a remote-detection improve simulated point-spread functions, we present sodium cell magnetometer using synchronous optical a method to parameterize and include polarization in pumping. This magnetometer is used to measure ambient phase retrieval models. geomagnetic field with high-sensitivity using backscat- tered resonance fluorescence. ber

FM4B.7 • 15:45 FM4C.6 • 15:45 High Sensitivity CPT and Pulsed CPT based Axial Sensing polarization rotation through scattering Magnetic Field Measurements, Gour S. Pati1, Bruce media, Abhijit Roy1, Rakesh K. Singh2, Maruthi Manoj Barrios1, Robin Depto1, Renu Tripathi1, Anthony Yu2, Mi- Brundavanam1; 1Dept. of Physics, Indian Inst. of Tech- 2 1 2 2 Monday, 17 Septem Monday, chael Krainak ; Delaware State Univ., USA; NASA GSFC, nology Kharagpur, India; Dept. of Physics, Indian Inst. USA. We have demonstrated high-sensitivity axial B-field of Space Science and Technology, India. We present a measurements based on coherent population trapping technique based on an interferometric approach to sense (CPT) and pulsed CPT phenomena. the polarization rotation through scattering media with the help of a known reference speckles, by studying the degree of coherence of the mixed speckles.

15:00–17:00 OSA Senior Member Workshop, Holmead, Lobby Level (advanced registration required)

16:00–16:30 Coffee Break, Concourse Foyer

16:00-17:00 Meet OSA’s Journal Editors, Concourse Foyer

16:00–17:00 DLS Annual Business Meeting, Georgetown West

16:00–17:00 Foundational Skills of Professional Networking – How First Impressions and Elevator Pitches Lead to Career Success and Longevity, Cabinet

16:00–17:30 OSA Optical Fabrication and Testing Technical Group Knowledge Café, International Ballroom West

16:00–17:30 The Rules of Engagement: Navigating Important Business Relationships, Georgetown East

16:00–18:00 Finishing Touches: A Tutorial in Blender for Cover Art and Figures, Jefferson West

16:00–18:00 OSA Photonic Metamaterials Technical Group Tutorial on Metalens Design and Simulation, Lincoln West

16:00–18:30 Cheeky Scientist Career Development Workshops, Jefferson East

18:00–19:00 OSA Polarization Technical Group Rapid- Fire Presentations & Networking Event, Cabinet

18:00–19:00 Workshop: Understanding Unconscious Bias, Georgetown East

18:00–21:00 Awards Ceremony & Reception, Carnegie Institute of Science, 1530 P St. NW (Separate Ticket Required)

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FM4D • A Realistic Assessment of Optics FM4E • Advanced Microscopy—Continued FM4F • Complex Nanophotonics— for Self-driving Vehicles—Continued Continued

FM4E.6 • 15:30 FM4F.4 • 15:30 Invited A Portable Optical Diagnostic System for Malaria Linear Frequency Conversion in a Rapidly Time-variant 2 1 Screening, Dongyu Chen , Samantha E. McBirney , Kris- Metasurface, Bumki Min1; 1Korea Advanced Inst of Sci- 1 3 4 tina Kaypaghian , Alexis Scholtz , Hossein Ameri , Andrea ence & Tech, Korea (the Democratic People’s Republic of). 5 1 M. Armani ; Dept. of Biomedical Engineering, Univ. of The frequencies of electromagnetic waves are converted 2 Southern California, USA; Ming Hsieh Dept. of Electrical as the waves propagate through a temporally varying Engineering-Electrophysics, Univ. of Southern California, medium. Interestingly, this frequency conversion is not 3 USA; Dept. of Biomedical Engineering, Johns Hopkins based on well-known nonlinear processes. Here, we ex- Univ., USA; 4USC Roski Eye Inst., Dept. of Ophthalmology,

plain basic principles of linear frequency conversion and Monday, 17 Septem Keck School of Medicine of the Univ. of Southern Califor- show various interesting properties of rapidly time-variant 5 nia, USA; Mork Family Dept. of Chemical Engineering metadevices. and Materials Science, Univ. of Southern California, USA. We developed a portable optical diagnostic system for rapid malaria screening in low-resource areas. Detection limits well below the clinical relevance are demonstrated using β-hematin in unprocessed, whole rabbit blood.

FM4E.7 • 15:45 cellSTORM − Super-Resolution on a Cellphone, Bene- 1 1 1

dict Diederich , Patrick Then , Alexander Jügler , Ronny ber Förster1, Rainer Heintzmann1,2; 1Leibniz Inst. of Photonic Technology, Germany; 2Inst. of Physical Chemistry and Abbe Center of Photonics, Friedrich-Schiller-Univ. Jena, Germany. We present a way to use smartphones for Single-Molecule-Localization-Microscopy. Using con- sumer-grade smartphone cameras and neural networks instead of scientific-grade cameras we achieved optical resolution below 80 nm.

15:00–17:00 OSA Senior Member Workshop, Holmead, Lobby Level (advanced registration required)

16:00–16:30 Coffee Break, Concourse Foyer

16:00-17:00 Meet OSA’s Journal Editors, Concourse Foyer

16:00–17:00 DLS Annual Business Meeting, Georgetown West

16:00–17:00 Foundational Skills of Professional Networking – How First Impressions and Elevator Pitches Lead to Career Success and Longevity, Cabinet

16:00–17:30 OSA Optical Fabrication and Testing Technical Group Knowledge Café, International Ballroom West

16:00–17:30 The Rules of Engagement: Navigating Important Business Relationships, Georgetown East

16:00–18:00 Finishing Touches: A Tutorial in Blender for Cover Art and Figures, Jefferson West

16:00–18:00 OSA Photonic Metamaterials Technical Group Tutorial on Metalens Design and Simulation, Lincoln West

16:00–18:30 Cheeky Scientist Career Development Workshops, Jefferson East

18:00–19:00 OSA Polarization Technical Group Rapid- Fire Presentations & Networking Event, Cabinet

18:00–19:00 Workshop: Understanding Unconscious Bias, Georgetown East

18:00–21:00 Awards Ceremony & Reception, Carnegie Institute of Science, 1530 P St. NW (Separate Ticket Required)

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08:00–09:30 JTu1A • Plenary Session

JTu1A.1 Plenary The Future of Computing, Heike E. Riel; IBM Research Frontiers Institute, USA. Extraordinary enhancements in computing power over the last 50 years have been driven by “smaller & denser” resulting in “faster & cheaper”. The quest for ever increasing computing performance continues. This raises the fundamental question of what is next? Today the most exciting new frontiers of information technology are non-von Neumann computing and quantum computing. This talk will give an overview of our research activities in the field of extending the core technology roadmaps and in the new paradigms of cognitive hardware technologies and quantum computing.

JTu1A.2 Plenary Chirped Pulse Amplification to ELI and Beyond, Gerard Mourou, École Polytechnique, France. PW laser could be compressed into high-energy single-cycled laser pulse, offering a fundamentally new laser-matter interaction ambit, which could become the fulcrum of novel scientific and societal applications. Among them, we foresee efficient laser electron and ion acceleration, as well as the generation of a single-cycled X-ray pulse leading to Exawatt and zeptosecond science and technology.

09:30–15:00 Science & Industry Showcase Visit page 11 for a complete program schedule.

10:00–11:00 Rapid Fire Oral Presentation I, Science & Industry Theater Presider: David Busch; Univ. Texas Southwestern Medical Center at Dallas, USA Participating posters are noted in the list of poster for session JTu2A with the icon RAPID. Each presenter will have 3 minutes and the order will be determined by poster number.

JOINT FiO + LS

10:00–12:00 JTu2A • Poster Session I and Dynamic E Posters

JTu2A.10 JTu2A.1 E-Poster JTu2A.5 E-Poster Dynamic Ferroelectricity of Trojan Electrons on Mul-

ber Organic Molecular Beam Deposition and In-Situ Poling Diffraction of Laguerre-Gauss Vortex Beams from Sier- tiple Parallel Regular 2-dimensional Lattices, Matt of Dense Supramolecular Assemblies for Second Order pinski Triangles, Sean Nomoto1, Reeta Vyas1, Surendra Kalinski1; 1Utah State Univ., USA. Dynamic ferroelectric Nonlinear Optics, Michael Erickson1, Lauren Dallachiesa1, Singh1; 1Univ. of Arkansas, USA. Fraunhofer diffraction of orders are discovered in a volume filled with a parallel Ivan Biaggio1; 1Lehigh Univ., USA. We demonstrate that Laguerre-Gauss beams from Sierpinski triangle apertures layers of various regular 2-dimensional lattices consisting in-situ poling during organic molecular beam deposition of different iteration orders is studied and its dependence of hydrogen atoms self-consistently supporting Trojan of single-component dense supramolecular assemblies on iteration order, topological charge, and aperture loca- Wave Packet states via the rotating dipole interactions. can be used to obtain a preferential molecular order tion relative to the beam-waist is investigated. and a bulk linear electro-optic effect in the resulting JTu2A.11 organic films. JTu2A.6 E-Poster Study of the generation dynamics in a strict polariza- Towards the Use of Machine Learning in Setups for tion-controlled passively mode-locked Er-fiber laser., JTu2A.2 E-Poster OAM Mode Excitation in Optical Fibers, Antonio 2

Tuesday, 18 Septem Tuesday, Luis Alberto Rodriguez Morales , Hector Santiago-Her- Self-assembling of functionalized micro-optical el- Astorino1, Jesper Glückstad1, Karsten K. Rottwitt1; 1DTU, nandez2, Baldemar Ibarra-Escamilla2, Georgina Beltrán ement driven by pyro-electrohydrodynamic forces, Denmark. Machine Learning algorithms driving spatial Pérez1, Ivan Armas Rivera2, Manuel Durán Sanchéz2, Sara Coppola1, Giuseppe Nasti1, Veronica Vespini1, Pietro light modulators may help achieve higher purity in ex- Yazmin Bracamontes3, Olivier Pottiez3, Marco V. Hernán- Ferraro1; 1Inst. of Applied Sciences and Intell, Italy. We cited orbital angular momentum modes in fibers. Some dez-Arriaga2, Evgeny A. Kuzin2; 1BUAP, Mexico; 2Optics, present a repeatable and accurate method to pattern preparatory steps are investigated to potentially enable INAOE, Mexico; 3Centro de investigaciones en Óptica, fluorescent particles into polymer microlens array and flex- effective Machine Learning in such a configuration. Mexico. We report the relation between the polarization ible elastomeric membranes. This method uses intense state of the pulses propagating in the cavity and the electric field generated by a Periodically Poled Lithium JTu2A.7 E-Poster generation regimes. Rotating the polarization azimuth Niobate (PPLN) in order to direct the self-assembly elec- Coherent Blue Light Driven by a Diode Laser and a gets transition from the generation of noise-like pulses trophoretic and dielectrophoretic forces. High Repetition Rate Pulse Train, Marco P. Moreno1, to soliton molecules Alexandre A. Almeida2, Sandra S. Vianna2; 1Departa- JTu2A.3 E-Poster mento de Física, Universidade Federal de Rondônia, JTu2A.12 3D Fractal Analysis of Optical Images of Retinal Brazil; 2Departamento de Física, Universidade Federal de Magnetically Controllable Random Lasers, Yun-Tzu Amyloid for Staging in Alzheimer’s Disease, Peter A. Pernambuco, Brazil. Using a diode laser and a 1 GHz fem- Hsu1, Yu-Ming Liao1, Cheng-Yen Tsai1, Wei-Cheng Liao1, Neathway1, Tao Jin1, Melanie C. Campbell1,2; 1Physics tosecond pulse train, we investigate the Autler-Townes Wei-Ju Lin1, Shih-Yao Lin1, Cheng-Han Chang1, Golam and Astronomy, Univ. of Waterloo, Canada; 2School splitting and the influence of an electromagnetic induced Haider1, Tzu-Min Sun1, Yang-Fang Chen1; 1National Taiwan of Optometry and Vision Science, Univ. of Waterloo, transparency window in the coherent blue light generated Univ., Taiwan. Controllability is crucial for random lasers. Canada. Fractal dimensions of retinal amyloid deposits in rubidium vapor. Here, magnetically controllable random lasers (MCRLs) were calculated using a 3D box counting method. The are designed, fabricated. The applied magnetic field can maximum and average fractal dimensions were signifi- JTu2A.8 RAPID be used to manipulate the distribution of scatterers, which cantly correlated to the number of deposits (p<0.03 and Generating Broadened UV Pulses for Ultrafast Non- finally determines laser action. p<0.05, respectively). linear Experiments, James D. Gaynor1, Joel Leger1, Munira Khalil1; 1Univ. of Washington, USA. Broadened JTu2A.13 JTu2A.4 E-Poster UV pulses are generated and used in Fourier transform Comparison Between InGaAs SPD and Superconduct- Universal All-Optical Computing Based on Intercon- two-dimensional electronic-vibrational spectroscopy to ing Nanowire Detector Using a Silicon Photon-pair nected Lasers, Tuomo von Lerber2,1, Matti Lassas1, Quang study vibronic couplings in a solar cell sensitizing dye. Source, Woncheol Shin1, Heedeuk Shin1, Kyungdeuk Trung Le2, Franko Küppers2; 1Dept. of Mathematics and Park1, Young-Wook Choi2, Yong-Su kim2; 1Pohang Univ. Statistics, Univ. of Helsinki, Finland; 2Photonics Lab, JTu2A.9 of Science and Technol, South Korea; 2Center for Quan- Technische Universität Darmstadt, Germany. We present Dye-Doped Random Microlasers Fabricated via tum Information, Korea Inst. of Science and Technology, an all-optical computing scheme based on normalization Two-Photon Polymerization, Nathalia B. Tomazio1, Lucas South Korea. Photon-pair generation rate through a operations of injection-locked lasers. We show cascad- F. Sciuti1, Gustavo F. Almeida1, Leonardo De Boni1, Cleber silicon photon-pair source is measured by InGaAs SPD ed operations in cellular automaton by an all-optical R. Mendonca1; 1USP Inst de Fisica de Sao Carlos, Brazil. and superconducting nanowire detector, showing 240 Conway’s Game of Life and simulate 100 generations We demonstrate coherent random lasing in dye-doped times higher coincidence count than InGaAs SPD. A of gaming. microstructures fabricated by two-photon polymerization. high coincidence-to-accidental ratio of 524 is achieved. Randomly distributed irregularities on the microstructure sidewall surfaces act as back-scattering elements, provid- ing feedback for lasing.

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JOINT FiO + LS

JTu2A • Poster Session I and Dynamic E Posters—Continued

JTu2A.14 JTu2A.22 JTu2A.28 Optimized Growth of Titanium Nitride Films using Plas- Localized Electromagnetic Field Enhancement with Withdrawn ma Enhanced Atomic Layer Depostion, Dhruv Fomra1, Patterned Hyperbolic Metamaterials, Jongwoo Hong1, Ray R. Secondo1, Vitaliy Avrutin1, Natalia Izyumskaya1, Chulsoo Choi1, Byoungho Lee1; 1Seoul National Univ., JTu2A.15 1 1 1 Independent phase modulation of two polarization Ümit Özgür , Nathaniel Kinsey ; Virginia Commonwealth South Korea. The electromagnetic field enhancement Univ., USA. We investigate and find that the quality of tita- is a key factor in efficient light-matter interaction due to states with reflection-type metasurface, Jangwoon nium nitride grown at 350°C and 375°C using atomic layer small mode volume and loss. We propose hyperbolic Sung1, Gun-Yeal Lee1, Chulsoo Choi1, Byoungho Lee1; deposition on silicon and sapphire substrates respectively metamaterial cavity for field enhancement by patterning 1Seoul National Univ., South Korea. Taking the advantage are approaching the metallicity of sputtered films. funneled aperture on metal-dielectric layers. of propagation phase with geometric phase, we designed a novel reflection-type metasurface enabling independent JTu2A.23 JTu2A.29 phase control of two polarization states. This method Automatic Surface Defect Detection using Autore- Extended Propagation Distances For Diffraction-Free achieves phase control with the high efficiency up to 95%. gressive Modeling based Fringe Analysis, Dr. Rishikesh Space-Time Light-Sheets, Basanta Bhaduri1, Murat Kulkarni2, Earu Banoth1, Dr. Parama Pal1; 1TCS Research Yessenov1, Ayman Abouraddy1; 1Univ. of Central Florida, JTu2A.16 2 High Peak Intensity and Tunable Range Bessel Beams and Innovation, Tata Consultancy Services, India; Dept. CREOL, USA. We synthesize propagation-invariant space- of Electronics and Electrical Engineering, Indian Inst. of time wave packets in the form of a pulsed light-sheet of Generation and Characterization, A. Srinivasa Rao1, technology Guwahati, India. We propose a novel fringe transverse spatial width 200 mm and spectral bandwidth Goutam K. Samanta1; 1AMOPH, Physical Research Lab, analysis technique based on an autoregressive (AR) of 2 nm, and observe its diffraction-free propagation for India. We report on a novel method to generate high peak modeling of fringe signals for detecting surface defects. a record 6 meters. ∼ intensity, segmented, smooth, zero-order Bessel beams Defects are localized by studying variations in fringe ∼ with tunable range peak position using axicon with hollow frequencies computed using estimated AR coefficients. JTu2A.30∼ Gaussian beam (HGB) as pump mode. Dynamic Footprint Differentiation from Machine 1 1 JTu2A.17 JTu2A.24 Acceleration Effect, Guoyu Yu , Christina Reynolds , KW-level Triple-Cladding Laser Fiber, 1,2 2 1 1 Optical Simulations of Wavefront Aberrations of In- Shuang Liu , Oliver Faehnle , David Walker ; OpTIC Centre, Univ. of 1 1 1 1 1 2 terpenetrating Polymer Network Hydrogel’s Artificial Huan Zhan , Kun Peng , Xiaolong Wang , Li Ni , Juan Yu , Huddersfield, UK; QA/QES & Continuous Improvement, Jianjun Wang1, Feng Jing1, Rihong Zhu2, Aoxiang Lin1; FISBA AG, Switzerland. This paper investigates the differ- Cornea, Chung-Tsung Hsieh1, Jia-Han Li1; 1National Tai- 1Laser Fusion Research Center, China; 2Nanjing Univ. of entiation between machine’s static and dynamic footprint wan Univ., Taiwan. The various structure parameters and Science and Technology, China. We fabricated a kW-level (FP). Results have shown progressing footprint variation materials are chosen for artificial cornea. Our simulation triple-cladding Yb-doped aluminophosphosilicate fiber related to tool’s tilt angle. Tilt angle compensation has Tuesday, 18 Septem results show that increasing the complexity of structures with an added low-refractive-index fluorine-doped silica been applied to offset this effect. and choosing high refractive index material are important cladding. 1.36kW laser output was obtained at 1079.6nm to properties of artificial cornea. with 82.3% slope efficiency and without nonlinear effects. JTu2A.31 JTu2A.18 Linear and nonlinear hyperspectral imaging of nano- and bio- materials in photo-induced force microscopy, Multimode supercontinuum generation in As S chalco- JTu2A.25 2 3 Development of Multi-modal Bacterial Rapid Detec- Eun S. Lee1; 1Korea Research Inst of Standards & Sci, genide photonic crystal fiber, Amani Ben Khalifa1, Rim tion Instrument, Iyll-joon Doh1, Huisung Kim1, Jennifer South Korea. Linear and nonlinear optical responses of Cherif1, Amine Ben Salem1; 1Univ. of carthage, Tunisia. Sturgis2, Valery Patsekin2, J. Paul Robinson2,3, Euiwon nano materials are measured through force detection in The mid-infrared supercontinuum generation spanning Bae1; 1Mechanical Engineering, Purdue Univ., USA; 2Basic photo-induced optical microscopy. The measurement 2 to 4 µm at -40 dB for mode HE11 is obtained in multi-

Medical Sciences, College of Veterinary Medicine, Purdue results of Raman vibrational signal and excited state ber mode As S photonic crystal fiber. Energy transfer occurs 2 3 Univ., USA; 3Weldon School of Biomedical Engineering, absorption of molecular clusters are presented. only with long pulses between modes with comparable Purdue Univ., USA. An instrument providing simultaneous geometries. optical measurement modalities is presented. Integrating JTu2A.32 JTu2A.19 custom confocal module, three laser diodes, and sensors An opposite approach to steam generation using solar power: cooler for more, 1 1 Reflective Liquid Crystal Lenses with Electrically Aniso- into an upright microscope allows measuring multiple Lyu Zhou , Haomin Song , optical characteristics of a bacterial colony. Youhai Liu1, Matthew Singer1, Dengxin Ji1, Nan Zhang1, tropic Wavefront Modulation, Yu-Jen Wang1, Jun-Lin Xie Zeng1, Zongmin Bei1, Zongfu Yu2, Qiaoqiang Gan1; Chen1, Yi-Hsin Lin1; 1Dept. of Photonics, National Chiao JTu2A.26 1State Univ. of New York at Buffalo, USA; 2Electrical and Tung Univ., Taiwan. Reflective lenses are important in Resolution Enhancement for AR/VR Displays Based Computer Engineering, Univ. of Wisconsin Madison, optical design and applications. We investigate reflective on LC Sub-pixel Frame Shift, Kyookeun Lee1, Nikolay USA. We proposed a cold vapor generation beyond the liquid crystal lenses with anisotropic wavefront modu- Muravyev2, Dmitry Piskunov2, Jaeyeol Ryu2, Kyusub input solar energy limit. The vapor was produced at a lation. The impact of this study is to design electrically Kwak1, Myongjo Choi1, James D. Kim1; 1Samsung Re- temperature below that of ambient, resulting in ~2.2 kg tunable devices for adaptive optics. search, South Korea; 2Samsung R&D Inst. Russia, Russia. m-2 h-1 generation rate under one sun. JTu2A.20 We propose a resolution enhancement method for AR/ Revealing of Axial Separation between Diffusers VR displays based on sub-pixel frame shift using a LC JTu2A.33 deflector. Experimental results using Samsung Gear VR Actively mode-locked Yb-doped fiber laser via pump through Lateral Speckle Correlation, Gokul G. Nair1, and Galaxy S8 show that the resolution is doubled and modulation, Zihao Zhao1, Sze Set1, Shinji Yamashita1; Dinesh N. Naik1, Michael L. Jakobsen2, Steen G. Han- the screen door effect is reduced. 1Univ. of Tokyo, Japan. An active mode-locked Yb-doped son2, Rakesh K. Singh1; 1IIST Trivandrum, India; 2Dept. fiber laser via pump modulation is demonstrated. The of Photonics Engineering, Technical Univ. of Denmark, JTu2A.27 mode-locked all-normal-dispersion fiber laser operates Denmark. We experimentally demonstrate that the inten- Effect of Temperature on the Efficiency of Thin-Film in dissipative soliton regime without any spectral filter. sity correlation of speckled speckles before and after the Amorphous Silicon Tandem Heterojunction Solar Cells lateral displacement of the concealed scatterer discloses with AFORS-HET, Muhammad Riaz1, Ahmad S. Azzah- JTu2A.34 the axial separation though speckle size, decorrelation rani1,2, Ahmed C. Kadhim1; 1Florida Inst. of Technology, Pulse Shaping and its Influence on Contrast Enhance- length and speckle gearing. USA; 2Northern Borders Univ., Saudi Arabia. : Simulation ment in Nonlinear Optical Imaging, George O. Dwapan- and design of a-SiC/a-Si(i)/a-Si:H/ and a-SiC/a-Si(i)/a- yin1, Gurthwin Bosman1, Pieter Neethling1, Erich Rohwer1; JTu2A.21 1 Single shot vectorial shearing interferometry tech- SiGe:H solar cells are investigated and optimized. The Laser Research Inst., Dept. of Physics, Stellenbosch Univ., nique for wavefront reconstruction and aberration maximum efficiency is achieved by changing temperature South Africa. The influence of temporal phase control of up to 400K. ultra-broadband femtosecond laser pulses on contrast calculation, Pramod Panchal1, Surya Gautam1, Dinesh enhancement in nonlinear imaging and its application N Naik1, C. S. Narayanamurthy1; 1Physics, IIST, India. We in a custom built multimodal microscope, is presented propose a vectorial sheared interferometry technique in this study. based on two sagnac interferometer to calculate gradient information along two orthogonal directions. We present an approach to reconstruct the wavefront and calculation of wavefront aberration.

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JOINT FiO + LS

JTu2A • Poster Session I and Dynamic E Posters—Continued

JTu2A.35 JTu2A.43 JTu2A.50 RAPID Extreme nonlinear optics under vortex lasers, Chengpu Energetic ultrafast self-similar fiber laser tunable in Plasma Formed by Dual-Filament Interaction, Danielle 1 1 1 Liu ; Shanghai Inst. of Optics and Fine Mechanics, CAS, 1030-1100 nm wavelength range, Chunyang Ma , Reyes1, Jessica Pena1, Matthieu Baudelet1, Shermineh R. 2 2 1 China. As for the interaction of few-cycle vortex laser with Ankita Khanolkar , Andy Chong ; JILIN UNIV., China; Fairchild1, Martin C. Richardson1; 1Univ. of Central Florida, 2 matter, many novel phenomena beyond those occurred in Univ. of Dayton, USA. We report a tunable Yb-doped USA. The filament plasma resulting from the interaction traditional nonlinear optics are disclosed, such as nonliear self-similar fiber laser for 1030-1100 nm by tuning center between two co-propagating beams, separated by 180 vortex precusors, THz necklace beam, and so on. wavelength of a narrow spectral filter. The result shows and 280 µm, was characterized for different energy dis- the self-similar operation is suitable for tunable lasers with tributions – two subcritical beams, one subcritical beam JTu2A.36 short pulse durations. with one filament, and two filaments. Modulation of Third Harmonic Generation Achieved 1 through Ground State Depletion, Szu-Yu Chen , Hao- JTu2A.44 JTu2A.51 1 1 1 1 Hao Wu , Jui-Ting Hung , Jian-Ling Chen ; National Generalized Laguerre-Gauss vortex beams, Alfonso Surface Enhanced Raman Scattering Efficiency of Metal 1 2,3 Central Univ., Taiwan. Third harmonic generation (THG) I. Jaimes-Nájera , Jesús Gómez-Correa , Sabino Coatings on Photochemically Roughened Silicon Sur- 1 1 2 is known being able to be enhanced though real-state Chávez-Cerda ; INAOE, Mexico; Facultad de Ingeniería faces, Tuba Önder1; 1Middle East Technical Univ., Turkey. 3 absorption. Suppressing absorption through ground-state Mecánica y Eléctrica, UANL, Mexico; Unidad Monterrey, The aim is obtaining optimal surface to enhance Raman depletion, the THG intensity can be modulated for the CICESE, Mexico. We present new families of vortex scattering by applying different parameters (power, du- purpose of resolution improvement of THG microscopy. beams with orbital angular momentum establishing a ration). Laser assisted wet etching technique was used to generalization of the Laguerre-Gauss beams in its stan- roughened surface of Si surfaces and they were analyzed JTu2A.37 dard and elegant formulation. Their closed analytical to measure enhancement factors. Beam Riders and Sailcraft Based on Diffractive Light free-space propagation formula is obtained. 1 1 Sails, Grover A. Swartzlander , Ying-Ju Lucy Chu , Prateek JTu2A.52 1 1 R. Srivastava ; Rochester Inst. of Technology, USA. Both JTu2A.45 High harmonic generation in diamond driven by solar and laser driven sailcraft are described whereby Nonuniform Dynamic Bragg Gratings for Laser Pulses intense femtosecond near infrared laser pulse, Boyan 1 1 diffraction, rather than reflection, is used to impart mo- Manipulation, Andrey ILJIN , Svitlana Bugaychuk , Obreshkov1; 1INRNE-BAS, Bulgaria. We present theoret- 1 1 mentum to a sailcraft for in-space propulpsion. Vycheslav Pinchuk ; Inst. of Physics, NAS of Ukraine, ical results on photoionization high-harmonic generation Ukraine. Nonlinear Schrödinger equation describes in bulk diamond induced by intense laser pulse of photon JTu2A.38 effects of wave self-diffraction in an extended dynamic energy 1.55 eV, having a time duration of 15 fs. Laguerre-Gauss Beams with Polarization-OAM En- nonlocal medium. The resulting dynamic grating has a tanglement in a Graded-Index Medium, Nikolai I. soliton-like envelope of modulation depth and provides JTu2A.53 RAPID 1 1 Petrov ; Scientific and Technological Center of Unique energy exchange and laser pulse amplification. Two-qudit deterministic optical quantum logic in a ber Instrumentation of the Russian Academy of Sciences, single photon, Poolad Imany1, Jose A. Jaramillo-Villegas1, Russia. Propagation of linearly and circularly polarized JTu2A.46 Joseph M. Lukens2, Ogaga D. Odele1, Daniel E. Leaird1, vortex light beams in cylindrical graded-index waveguide The Micromaser in a Cross Cavity: A Fidelity Perspec- Minghao Qi1, Andrew M. Weiner1; 1Purdue Univ., USA; 1 taking into account spin-orbit and nonparaxial effects is tive, Julio C. Garcia-Melgarejo , Nestor Lozano-Crisósto- 2Oak Ridge National Lab, USA. We demonstrate deter- 1 1 investigated. Effects of collapse and long-term revival of mo , Ariel Dominguez-Pachecano , J. Sanchez Mon- ministic two-qudit gates using the time and frequency 2 1 wave packets are examined. dragon ; Universidad Autonoma de Coahuila, Mexico; degrees of freedom of a single photon, showing the 2 INAOE, Mexico. We discuss the generation of a Fock potential of our scheme for deterministic quantum com- JTu2A.39 state photon distribution in a perfect cross-cavity. We puting in high-dimensional Hilbert spaces. Collective Three-Photon Blockade In A Cavity QED verify such generation through the numerical computation 1 1 2 System, Chengjie Zhu , Yaping Yang , Girish Agarwal ; of the fidelity in two important cases. JTu2A.54 RAPID 1 2 Tuesday, 18 Septem Tuesday, Tongji Univ., China; Texas A&M Univ., USA. We present Quantum-Limited Electro-Optic Modulator Based a theoretical proposal to realize three-photon blockade JTu2A.47 on Thermal Rydberg Atoms, Kevin C. Cox1, David H. in a coherently-driven, two-qubits cavity QED system. We Analysis of the Twin-soliton Bound States in Passive Mi- Meyer2,1, Zachary A. Castillo2,1, Paul D. Kunz1; 1US Army 1 1 show that the three-photon blockade with two-photon croresonator, Maitrayee Saha , Samudra Roy , Shailendra Research Lab, USA; 2Physics, Univ. of Maryland, College 1 1 bunching can be achieved when two qubits couple the Varshney ; IIT-KGP, India. We numerically study spectral Park, USA. We discuss the standard quantum limit for cavity asymmetrically. characteristics of frequency comb in presence of two electro-optic conversion using a quantum sensor and solitons separated by a delay much greater than their experimentally demonstrate quantum-limited operation JTu2A.40 characteristic width. Nature of interaction potential and using electromagnetically-induced-transparency with Opticaly tunable conductivity of carbon nanotubes in energy signify the stability of bound state. thermal Rydberg atoms. terahertz frequency range, Daniel Gomon1, Sviatoslav 1 1 2 Gusev , Petr Demchenko , Ilya Anoshkin , Dmitry Lyub- JTu2A.48 RAPID JTu2A.55 RAPID 2 1 1 2 chenko , Mikhail Khodzitsky ; ITMO Univ., Russia; KTH Superdiffusive charge screening for phase singulari- The Quest for Nonclassicality using Number-Resolving 1 Royal Inst. of Technology, Sweden. Impact of infrared ties in isotropic random waves, Lorenzo De Angelis , Single-Photon Detectors, Raphael A. Abrahao1,2, Farid 1 1 radiation illumination (980 nm) on the properties of car- L. Kuipers ; Kavli Inst. of Nanoscience, Delft Univ. of Shahandeh2, Geoff Gillett1,2, Martin Ringbauer1,2, Till bon nanotubes (CNT), such as complex conductivity and Technology, Netherlands. We present a quantitative study Weinhold1,2, Marcelo P. Almeida1,2, Timothy C. Ralph2, permittivity, with different geometric parameters in the on the screening among phase singularities in random Andrew G. White1,2; 1Centre for Engineered Quantum frequency range of 0.2-1.0 THz was studied. waves. We prove that the fluctuation of the total topo- Systems, School of Mathematics and Physics, Univ. of 2 〈 2 logical charge Q contained in an area R satisfies ΔQ Queensland, Australia; 2Centre for Quantum Computation 〉 〈 2〉 JTu2A.41 RlogR rather than the ordinary diffusive ΔQ R. and Communication Technology, School of Mathematics Theoretical Approach to Resolution Limit Calculations and Physics, Univ. of Queensland, Australia. The quest ∼ ∼ in Optical Microscopy with the use of Feynman Dia- JTu2A.49 RAPID for nonclassicality is the search for the border between 1 1 grams, Naoki Fukutake ; Nikon Corporation, Japan. By Femtosecond Pulse-Splitting Effect in Second Har- classical and quantum physics. Our work aims to show means of double-sided Feynman diagrams describing monic Generation in the Laue Diffraction Scheme that nonclassical correlations can be observed even in the 1 optical processes, we formulate the calculation rules of From 1D Photonic Crystals, Vladimir B. Novikov , Boris absence of entanglement and quantum discord. the resolution limits for all types of optical microscopy I. Mantsyzov1, Tatiana V. Murzina1; 1M. V. Lomonosov that employ linear, nonlinear, coherent, and incoherent Moscow State Univ., Russia. Phase-matched second har- JTu2A.56 RAPID optical processes. monic generation at temporal laser pulse-splitting effect Enhancing the number of bi-photon orbital angular in one-dimensional photonic crystals under the Bragg momentum modes using asymmetric vortex beam, JTu2A.42 diffraction in the Laue geometry is studied experimentally Jabir M. V.1, Goutam K. Samanta1, Ali Anwar1; 1Physical Stimulated Supercontinuum Generation in CW-pumped and theoretically involving supercomputer resources. Research Lab, India. We report on controlling the bi-pho- 1 2 1 1 Regime, Chao Huang , H. Y. Fu , Qian Li ; Peking Univ., ton OAM eigenmodes in down-conversion process by 2 China; Tsinghua Univ., China. We numerically demon- simply adjusting the asymmetry of the pump vortex beam. strate the significant improvement in spectral bandwidth Calculation of the Schmidt number shows the increase in and coherence of CW pumped supercontinuum genera- the number of OAM eigenmodes. tion stimulated by a weak CW seed.

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JOINT FiO + LS

JTu2A • Poster Session I and Dynamic E Posters—Continued

JTu2A.57 JTu2A.64 JTu2A.70 First-Principles Study of the Optical Properties of AA- Pump-probe Quantum State Tomography and Photon Phase Noise Based Quantum Random Number Genera- Stacked Bilayer Graphene, Jun-Fu Zhang1, Min-Hsueh Statistics in Semiconductor Quantum Dots, Fabian tor Suppressing Classical Noise, Ziyang Chen1, Zhengyu Chiu1, Chang-Tsung Hsieh1, Tony Wen-Hann Sheu1, Boehm1, Nicolai B. Grosse1, Mirco Kolarczik1, Bastian Her- Li1, Yichen Zhang2, Hong Guo1; 1State Key Lab of Ad- Jia-Han Li1; 1National Taiwan Univ., Taiwan. The density zog1, Nina Owschimikow1, Ulrike K. Woggon1; 1Technische vanced Optical Communication Systems and Networks, functional theory is used to study optical properties in Universität Berlin, Germany. Quantum state tomography School of Electronics Engineering and Computer Science, AA-stacked bilayer graphene. The band gap increases as is applied to InGaAs quantum dot-semiconductor optical Center for Quantum Information Technology, Peking the interlayer distance gets smaller. The anisotropic per- amplifiers to reconstruct the Wigner function and photon Univ., China; 2State Key Lab of Information Photonics mittivity of AA-stacked bilayer graphene is demonstrated. statistics for a coherent state interacting with QDs with and Optical Communications, Beijing Univ. of Posts and high time-resolution and in the few-emitter limit. Telecommunications, China. We present a phase-noise- JTu2A.58 based random number generation scheme with a rate Conductive Gap-Plasmon Nanocavity, Seied Ali Sa- JTu2A.65 of 600Mbps without using optical delay line, which can fiabadi Tali1, Wei Zhou1; 1Virginia Tech, USA. We can Quantum holography with twin photons of large spatial remove the classical noise induced by fiber jitter. design and create conductive gap-plasmon nanocavity dimensionality, Fabrice. Devaux1, Alexis Mosset2, Florent structures using vertically stacked nanodisks made of Bassignot3, Eric Lantz1; 1Universite de Franche-Comte, JTu2A.71 metals or conductive oxides, which can simultaneously France; 2FEMTO-ST, France; 3FEMTO Engineering, Stochastic Runge-Kutta Algorithm and Parameter serve as nanoelectrodes and nanoantennas for hybrid France. We report results of quantum holography where Optimization in Optical Simulations Using MATLAB, electrical-optical interface. spatial information stored in phase hologram is restored John R. Thompson1, Hongbo Zhang1; 1Virginia Military by measuring spatial coincidences between two images Inst., USA. An algorithm and MATLAB code for solving JTu2A.59 formed by spatially entangled twin photons of high-di- nonlinear stochastic rate equations are presented and A Comparative Analysis of TM Guided Modes in Silicon mensionality transmitted by the hologram. applied to the problem of parameter optimization using on Insulator (SOI) based Rectangular Optical Wave- high performance computing. guide, Dhananjoy De1, Ritu Raj Singh1, Vishnu Priye1; JTu2A.66 1Indian Insttitute of Technology, Dhanbad, India. In this Experimental Implementation of Directionally-Unbi- JTu2A.72 paper, TM guided modes of SOI based rectangular optical ased Linear-Optical Multiport, Shuto Osawa1, David S. Spatial solitons as fixed points of Fox-Lee integral waveguide of different widths have been investigated. Simon1,2, Alexander V. Sergienko1; 1Boston Univ., USA; equation, Alex Okulov1; 1Russian Academy of Sciences, Conditions for first and higher order modes are analyzed 2Stonehill College, USA. A directionally-unbiased optical Russia. The exactly solvable model of nonlinear eigen- mathematically and justified with the FEM simulation. multiport allows a photon to reverse direction inside and modes of laser cavities in Fox-Lee integral equations exit at any port, including the input port. This multiport form includes correctly boundary conditions. Bright Tuesday, 18 Septem JTu2A.60 could be used as a quantum gate and for efficiently soliton solutions and their instability increments are Example of Guessing Probability on Secret Key by implementing quantum walks. obtained explicitly. Known-Plaintext Attack on Y00 Quantum Stream Cipher, Takehisa Iwakoshi1; 1Tamagawa Univ., Japan. JTu2A.67 JTu2A.73 While Quantum-Key-Distribution is regarded as prom- Multiphoton discrete fractional Fourier operations in Quantum Fractional Fourier Transform, Yesid A. Madrid ising secure communication, security of Y00 protocol H. waveguide beam splitters, Armando P. Leija1,2, Konrad Carrillo2,1, Martha Molina2, Rafael Torres3; 1Grupo de P. Yuen proposed for the affinity to conventional optical Tschernig2, Roberto D. Leon Montiel3, Omar Magana Loai- Ciencias Computacionales, Universidad de Pamplona, communication is not well-understood yet. This study za4, Alexander Szameit5, Kurt Busch1,2; 1Max Born Inst., Colombia; 2Grupo de Óptica Moderna, Física, Univer- gives some insights. Germany; 2Inst. of Physics, Humboldt Univ., Germany; sidad de Pamplona, Colombia; 3Grupo de Óptica y 3 4 5 ICN, UNAM, Mexico; NIST, USA; Inst. of Physics, Univ. Tratamiento de Señales, Escuela de Física, Universidad ber JTu2A.61 of Rostock, Germany. We show that exciting a waveguide Industrial de Santander, Colombia. Our propose consist in Influence of multiple scattering on self-focusing in beam-splitter with N indistinguishable photons, give rise show a new quantum gate that can perform the Fractional nematic liquid crystals, Alessandro Alberucci1, Chan- to lattice-like structures in the photon number space that Fourier Transform defined by Namias as a tool to solve the droth P. Jisha2, Serena Bolis3,4, Jeroen Beeckman4, Stefan are formally equivalent to coupled systems that perform differential equation of the quantum mechanical oscillator, Nolte1,5; 1Friedrich-Schiller-Universitat Jena, Germany; discrete fractional Fourier transforms. which it can satisfy the condition of to be unitary. 2Universidade do Porto, Portugal; 3Universite libre de Bruxelles, Belgium; 4Ghent Univ., Belgium; 5Fraunhofer JTu2A.68 JTu2A.74 RAPID Inst. of Applied Optics and Precision Engineering, Ger- Experimental Implementation of One-Qubit Logic Characterization of Fiber Bragg Gratings in Multicore many. We study the interplay between multiple scattering Gates and Verification Via Quantum State Tomogra- Fibers Using Quantitative Phase Imaging, Yijun Bao1, and self-focusing in Nematic Liquid Crystals (NLCs). At phy, Christian D. Torres Quelal1, Carlos A. Melo1, John Thomas K. Gaylord1; 1Georgia Inst. of Technology, USA. low powers self-focusing increases the coherence, but H. Reina1; 1Physics, Universidad del Valle, Colombia. We A quantitative phase imaging method is applied to for large powers a continuous temporal oscillation is implemented one-qubit quantum gates testing through characterize fiber Bragg gratings in multicore fibers. observed. the production of the polarization set of states, with |Hi Digital image processing techniques are developed to as input. Complementary, we reconstructed the state for overcome the difficulties arising from the short period of JTu2A.62 each output via the quantum-tomography protocol with the fiber Bragg gratings. Thermal Decoherence of the Carrier-Envelope-Offset fidelities over 95%. Frequency in a Kerr-Microresonator Comb, Tara E. JTu2A.75 Drake1, Jordan Stone1,2, Travis C. Briles1,2, Daryl Spencer1, JTu2A.69 Mode-Transition Bragg Gratings with Increased Group Scott B. Papp1,2; 1Time and Frequency Division, NIST, USA; Link between Debye Temperature, Bang Gap Energy, Index for On-Chip Optical Delay Lines, Lingjun Jiang1, 2Physics, Univ. of Colorado, Boulder, USA. We present and Fine Structure Constant, Haowen Xi2, Bruno Ullrich1, Zhaoran R. Huang1; 1Electrical, computer and systems measurements of the carrier-envelope-offset frequency Mithun Bhowmick3; 1Ullrich Photonics LLC, USA; 2Dept. of engineering, Rensselaer Polytechnic Inst., USA. We pro- noise spectrum of a silicon nitride Kerr-microresonator Physics and Astronomy, Bowling Green State Univ., USA; posed and demonstrated mode-transition Bragg gratings comb. Our preliminary observations suggest that thermal 3School of Chemical Sciences, Univ. of Illinois at Urba- for optical delay line applications. It shows a stronger slow decoherence is an important contribution. na-Champaign, USA. The link between the fine structure light effect than conventional apodized Bragg gratings, constant, energy band gap, and Debye temperature of and a maximum group index of 15.8 has been achieved. JTu2A.63 semiconductors is reported. The revealed relation has Withdrawn the potential to be highly influential for the design of JTu2A.76 optoelectronic and photonic devices. Scintillation Index Analysis for a Downlink Satellite Communication Based on the Three-layer Altitude Model for Moderate-to-strong Turbulence, Xin Shan1,2, Yong Ai1, Curtis Menyuk2; 1Electronic Information School, Wuhan Univ., China; 2Computer Science and Electrical Engineering Dept., Univ. of Maryland Baltimore County, USA. Scintillation is analyzed by adopting different wave-structure functions in the three-layer model. Results show that weak-fluctuation theory is limited to smaller zenith angles, and the scintillation index has a larger peak in the focusing regime.

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JTu2A • Poster Session I and Dynamic E Posters—Continued

JTu2A.77 JTu2A.83 JTu2A.90 RAPID Mode-locking Pulse Generation Based on In-fiber Analysis and Optimization of Edge-Filter Interrogation Broadband and Gate-Tunable Conducting Oxide Ep- 1 Acousto-optic Tunable Bandpass Modulator, Andrés Scheme for FBG Sensors, SAI R. EAGALA , Abhinav silon- Near-Zero Perfect Absorber, Long Tao3, Aleksei 1,2 1,2 1 1 1 1 Camarillo-Avilés , Erika N. Hernandez , Miguel Bel- Gautam , Ritu Raj Singh , Amitesh Kumar , Vishnu Priye ; Anopchenko3, Sudip Gurung3, Catherine Arndt3, Jason 1,2 3 1 lo-Jiménez , Manuel Durán-Sánchez , Baldemar Ibar- Indian Inst. of Technology (ISM), India. A technique to Myers2, Howard Lee3,1; 1The Inst. for Quantum Science 3 4 3 1 ra-Escamilla , Olivier Pottiez , Evgeny A. Kuzin ; Univer- interrogate an FBG based on edge-filter detection is pro- and Engineering, Texas A&M Univ., USA; 2US Naval 2 sidad Autonoma de San Luis Potosí, Mexico; Instituto de posed and demonstrated. The interrogation is performed Research Lab, USA; 3Dept. of Physics, Baylor Univ., USA. 3 Investigación en Comunicación Óptica, Mexico; Óptica, along the slope of a filter. The filters used are Trapezoidal, We demonstrate broadband and gate-tunable conduct- Instituto Nacional de Astrofísica, Óptica y Electrónica, Gaussian, Bessel and Butterworth filter. ing oxide epsilon-near-zero perfect absorbers grown by 4 Mexico; Centro de Investigaciones en Óptica, Mexico. atomic layer deposition. Absorption bandwidth (> 90%) An all-fiber acousto-optic tunable bandpass modulator JTu2A.84 of 214 nm for Berreman mode in NIR region is realized. and its application to perform mode-locking operation Simulation of the Brillouin Effect in an Optical Feed- 1 2 is reported. Experimental results demonstrate efficient back, Leidy J. Quintero Rodríguez , Min Won Lee , Ana JTu2A.91 RAPID 1 1 1 spectral filtering to support high intense and ultrashort G. Correa Mena , Ignacio E. Zaldívar Huerta ; INAOE, Random Lasers based on Polymer Membranes with 2 pulse generation. Mexico; Laboratoire de Physique des Lasers, Université Silver Nanoflowers, Junhua Tong1, Tianrui Zhai1; 1College Paris 13, France. Simulations of the dynamical behavior of Applied Sciences, Beijing Univ. of Technology, China. JTu2A.78 of a semiconductor laser subjected to stimulated Brill- Low-threshold random lasing was achieved in a polymer Fast Quasiadiabatic 2×2 Broadband 3-dB Couplers on ouin scattering and conventional optical feedback are membrane with silver nanoflowers. The random laser was 1 1 SOI Strip Waveguides, Zhong-Ying Li , Tung-Ke Huang , presented. It is corroborated that the laser parameters fabricated by attaching the polymer membrane on the 1 1 1 Hung-Ching Chung , Shuo-Yen Tseng ; National Cheng are changed and the BFS is at 11.12GHz. silver nanoflowers. Kung Univ., Taiwan. We propose a short and broadband 2×2 silicon 3-dB coupler optimized by the fast quasiadi- JTu2A.85 JTu2A.92 abatic approach. The designed device is 67.6 μm long Temperature Sensor Based on Fiber-Optic Fabry-Perot Demonstration of a High Q-factor Microring Resonator 1 1 and has a bandwidth of 280 nm for 3±1 dB splitting ratio. Interferometer, Sigifredo Marrujo , Sofia Flores , Miguel Fully Suspended by a Subwavelength Sidewall Grating, 1 2 3 Torres-Cisneros , Daniel López , David Monzón , Daniel Soha E. Yousuf1, Anatol Khilo2, Marcus S. Dahlem1; 1Khalifa 2 1 1 JTu2A.79 May , Iván Hernández ; Guanajuato Univ., Mexico; Univ. of Science and Technology, United Arab Emirates; 2 3 Experimental Supercontinuum Generetion with Centro de Investigaciones en Óptica, Mexico; Centro 2Boston Univ. , USA. A microring resonator fully suspend- Combination of Different Types of Optical Fibers, de Investigaciones en Óptica, Mexico. A fiber optic Fab- ed by a subwavelength sidewall grating is demonstrated, 1 1 Daniel Torres González , Juan Manuel Sierra Hernández , ry-Perot interferometer was fabricated. It was constructed with measured quality factor of 125k around 1550 nm. 1 1 Daniel Jáuregui Vázquez , Julian Moises Estudillo Ayala , by splicing a single mode fiber and a hollow core fiber, The structure is promising for sensing applications, with 1 1 ber Juan Carlos Hernández García , Roberto Rojas-Laguna ; cleaving the last one to a length of 16 µm and filling it with predicted sensitivities up to 1250 nm/RIU. 1Universidad de Guanajuato, Mexico. Supercontinuum polydimethylsiloxane. The sensitivity was 0.61 nm/°C. generation was achieved with numerous setups of optical JTu2A.93 fibers which include SMF-28, high-Numerical Aperture JTu2A.86 RAPID Mid-Infrared Supercontinuum Generation with a and dispersion-shifted fiber. Supercontinuum flatness was Correlating Macroscopic and Microscopic Vibrations Weak CW Trigger, Rongle Huang1, Renlai Zhou2, Qian studied by modifying the configurations and inducing in Silicon Carbide (SiC) Micromechanical Resonators, Li1; 1Peking Univ., China; 2Naval Univ. of Engineering, 1 1 1 1 fiber losses. Yanan Wang , Jaesung Lee , Vivian Zhou , Caleb Main , China. We numerically demonstrate picosecond pulse 1 2 1 1 Christian Zorman , Qiang Lin , Philip Feng ; Electrical pumped mid-infrared supercontinuum generation in 2 JTu2A.80 Engineering, Case Western Reserve Univ., USA; Electrical chalcogenide photonic crystal fibers with a weak CW Micro-Ring Resonator based Digital Photonic Half Engineering, Univ. of Rochester, USA. Device and lattice trigger. An untra-stable and bright supercontinuum with 1 Tuesday, 18 Septem Tuesday, Adder Demonstration, F. K. Law , Mohammad Rakib vibrations in SiC resonators have been comprehensively greatly enhanced coherence is achieved. Uddin1, Nur Musyiirah Masir1; 1Univeristi Teknologi Brunei, studied by laser interferometry and Raman spectroscopy. Brunei Darussalam. This paper presents the design and Bridging macroscopic and microscopic objects via strain JTu2A.94 simulation of a digital photonic half adder with two silicon mediation or phonon coupling will open up opportunities Small-Period Titanium-Diffused Periodically Poled Lith- micro-ring resonators as its base element. Simulation toward quantum applications. ium Niobate Waveguides for Strongly Nondegenerate result with timing diagrams have been shown to justify Quantum Frequency Conversion, John W. Snyder1, the adder function. JTu2A.87 RAPID Alexander V. Sergienko1,2; 1Electrical and Computer En- Efficient second-harmonic generation in sub-micron gineering, Boston Univ., USA; 2Physics, Boston Universiry, 1 1 JTu2A.81 PPLN waveguides, Jiayang Chen , Yong Meng Sua , USA. A Ti-diffused periodically poled Lithium Niobate 1 1 1 1 1 Design of Interaction Gate for high performance Zhaohui Ma , Chao Tang , Zhan Li , Yu-Ping Huang ; Ste- device with ultra-short poling periods has been devel- 2 1 computing structures, Santosh Kumar , Amna Bedi , vens Inst. of Technology, USA. Efficient second-harmonic oped for strongly nondegenerate quantum nonlinear 2 1 2 Nan-Kuang Chen ; DIT Univ., India, India; School of generation (SHG) is demonstrated in sub-micron period- optics. Quantum frequency conversion from 369.5nm to Physics Sciences and Information Technology, Liaocheng ically poled lithium niobate waveguides with normalized 1550nm with a 485nm pump laser is targeted. Univ., China. The present work provides a reversible op- conversion efficiencies over 440% W-1cm-2. tical computation universal signal interaction gate using JTu2A.95 lithium-niobate based Mach-Zehnder interferometer for JTu2A.88 RAPID A Novel Photonic Stampfli Quasicrystal Fiber Based high performance computing structures. The results are Excitation of hybrid epsilon-near-zero/plasmonic D-Glucose Microbiosensor, Aruna Gandhi M S1, Xuanyi verified using beam propagation method. modes in ALD-AZO coated nanoantennae, Subhajit Liu1, Qian Li1; 1Shenzhen Graduate School, Peking 1 1 1 1 Bej , Sudip Gurung , Aleksei Anopchenko , Brian Ko , University, China. The proposed photonic Stampfli qua- 1 1 JTu2A.82 Howard Lee ; Baylor Univ., USA. We study optical sicrystal fiber-based D-glucose Microbiosensor achieves Accurate Optical Vortex Identification in the Presence properties of nanoantennae conformally coated with a maximum sensitivity of 20000 nm/RIU and a resolution of Distortions Using a Shack-Hartmann Sensor, Jaime epsilon-near-zero (ENZ) Al-doped zinc oxide thin films. of 5 × 10-8 RIU in the different concentrations from 50% 1 1 1 A. Anguita , Jaime E. Cisternas , Gustavo L. Funes ; Results show splitting of nanoantenna resonance due to to 60% of the D-glucose solution. 1Universidad de los Andes - Chile, Chile. We present coupling between plasmonic and ENZ modes. and evaluate a robust method to identify orbital angular JTu2A.96 momentum states with a SH sensor for possible use in JTu2A.89 RAPID Tunable Electromagnetically Induced Transparency in free-space optical communication links. Experimental Entanglement Enhancement in Multimode Integrated Ge Sb Te -Based Infrared Metasurfaces, Riad Yahiaoui1, 1 3,2 2 2 5 verification using a 200m-range test bed is presented. Circuits, Zacharie M. Léger , Aharon Brodutch , Amr Joshua Burrow2, Jay Mathews2, Andrew Sarangan2, 1,3 1 Helmy ; The Edward S. Rogers Sr. Dept. of Electrical & Imad Agha2, Thomas A. Searles1; 1Howard Univ., USA; 2 Computer Engineering, Univ. of Toronto, Canada; Dept. 2Dayton Univ., USA. We report the investigation of an 3 of Physics, Univ. of Toronto, Canada; Center for Quantum all-dielectric metasurface (ADM) based on an array of Information and Quantum Control, Univ. of Toronto, Ge2Sb2Te 5 (GST) meta-molecules exhibiting a tunable Canada. Entanglement enhancement through photon electromagnetically induced transparency (EIT) effect in subtraction is studied in the multimode scenario. Optimal the infrared frequency regime. gain regions were identified for bipartite and multipartite measures; positive gains in entanglement were found after losses of 80% for specific bipartite splittings.

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JTu2A • Poster Session I and Dynamic E Posters—Continued JTu2A.97 JTu2A.103 JTu2A.110 Novel refractive index sensor based on hybrid long Sub-wavelength focusing in air using semiconductor Design and Characterization of Nanocavity Photonic range plasmon in H-shaped optical fiber, Nelson Go- based Hyperbolic Metamaterial for infrared imaging, Crystal Lasers, Binte M. Muminur1, Muhammad M. mez-Cardona2,1, Erick Reyes2,1, Rodrigo Acuña2, Pedro Norhan Salama1, Mai Desouky1, Mohamed M. Swillam1; Rahman1; 1Physics, Jahangirnagar Univ., Bangladesh. Torres2; 1Departamento de Electrónica y Telecomunica- 1Physics, American Univ. in Cairo, Egypt. We theoretically Photonic laser sources have great potential in communi- ciones, Instituto Tecnológico Metropolitano, Colombia; demonstrate sub-wavelength focusing in air using doped cation applications. We explore the design, fabrication 2Escuela de Física, Universidad Nacional de Colombia, InAs/intrinsic InAs hyperbolic metamaterial (HMM). and characterization of lasers based on photonic crystal Sede Medellin, Colombia. We propose a novel design for Sub-wavelength focusing in air is achieved in the near nanocavities. We demonstrate CW and ultrashort pulse a refractive index (RI) sensor based on hybrid long-range field at wavelength of 9.31µm with focusing distance of response of photonic lasers. plasmon in H-shaped microstructured optical fiber. Good 1µm with resolution down to 0.13λ. sensitivity, as high as 6.1*103 nm/RIU, can be achieved in JTu2A.111 the proposed structure. JTu2A.104 Standoff microparticles characterization with digital Honeycomb photonic crystal as a zero index meta- holographic Raman spectroscopy, Nava R. Subedi1, JTu2A.98 material, Nishant Shankhwar1, Yogita Kalra1, Ravindra Gombojav O. Ariunbold1, Prakash Adhikari1, Matthew Highly confined light guiding in a dielectric-nanow- K. Sinha1; 1Delhi Technological Univ., India. In this article J. Berg2; 1Mississippi State Univeristy, USA; 2Physics, ire-loaded hybrid Bloch-surface-polariton waveguide, zero index behaviour of honeycomb photonic crystal has Kansas State Univ., USA. A detail standoff interrogation of Weijing Kong1, Yu Sun2, Haiyang Zhang1, Yu Sun1, Shuang been demonstrated. The zero index behaviour arises due microparticles irradiated with a coherent light source will Wang1, Wenhui Zhao1; 1School of Electronic Engineer- to the dirac-like dispersion induced by degeneracy of be discussed. The results suggest that the methodology ing, Tianjin Univ. of Technology and Education, China; modes at the dirac point. could be applied to characterize airborne respirable-sized 2School of Information Science and Technology, Beijing particles in free-flowing aerosol form. Forestry Univ., China. A hybrid dielectric-nanowire load- JTu2A.105 ed Bloch-surface-polariton waveguide is presented and Design and Analysis of Broadband Square Spi- JTu2A.112 investigated. The results reveal the hybrid configuration ral Shaped Nanoantenna, Ritika Ranga1, Nishant Optically induced pure frequency modulation based enables significantly improved mode confinement com- Shankhwar1, Yogita Kalra1; 1Delhi Technological Univ., on a mid-infrared quantum cascade laser, Hai J. Zhou1, bined with low propagation loss. India. In this paper, a broad band square spiral shaped Chen Peng2, Tao Chen2, Biao Wei1; 1ChongqQing Univ., nanoantenna is proposed and analysed by finite element China; 2China Academy of Engineer Physics, China. JTu2A.99 method via COMSOL Multiphysics software. Electric field Purified frequency modulation is demonstrated in a Topologically-protected Edge Modes in Thue-Morse is enhanced in the gap of nanoantenna. middle-infrared quantum cascade laser by illuminating

Photonic Crystals, Mukesh K. Shukla1, Ritwick Das1; its front facet with two optimized near infrared lasers. Tuesday, 18 Septem 1National Institute of Science Education & Research, India. JTu2A.106 It is beneficial in improving signal fidelity for free space We report topologically-protected optical edge modes Disordered coupled photonic crystal slab cavities: optical communication. in Thue-Morse (TM) sequence based distributed-reflector effects on the coupling strength, Juan P. Vasco1, Vin- (DR) with exceptionally high quality-factor. Topological cenzo Savona1; 1Physics, École Polytechnique Fédérale JTu2A.113 features are explored through the phase and surface-po- de Lausanne (EPFL), Switzerland. We study the effects of Near Field Enhancement in a Hollow Flower Shaped laritons in TM-DR lattice. disorder on the coupling strength of coupled photonic Nanoantenna, Parul Goyal1, Nishant Shankhwar1, Yogita crystal slab cavities and establish upper bounds for the Kalra1; 1Delhi Technological Univ., India. In this paper, a JTu2A.100 quantity of disorder in order to the system work into the metallic hollow flower shaped nanoantenna has been Carbon-dots Embedded Glass Based Inverse Micropil- coupling regime. designed to obtain a near field enhancement in the feed

lar Structures by Two-photon Polymerization Process, gap of nanoantenna in the visible vision. The modeling ber Pratyusha Das1, Meher Wan1, Subhrajit Mukherjee1, Samit JTu2A.107 of the nanoantenna has been done using COMSOL K. Ray1,2, Shivakiran Bhaktha B N1; 1Indian Inst. of Tech- Leaky-mode Band Dynamics of Photonic Crystal Slabs, Multiphysics software. nology Kharagpur, India; 2S N Bose National Centre for Sun-Goo Lee1, Robert Magnusson1; 1Univ. of Texas at Basic Sciences, India. A simple fabrication of 2D photonic Arlington, USA. We present analytical and numerical JTu2A.114 crystal with hexagonal lattice system of air-column in a results on the formation of the second (leaky) stop band Optical Biosensor Based on Guided Mode Grating high-dielectric medium based on 3D photolithography of photonic crystal slabs. We show that Bragg processes Coupler, Rukmani Singh1, Ritu Raj Singh1, Vishnu Pri- technique and interaction of quantum emitters embed- generated by spatial Fourier harmonics control the band ye1; 1Indian Institute of Technology, Dhanbad, India. ded in a microcavity is presented. transition dynamics. Demonstration of highly sensitive optical biosensor based on interaction of analyte with guided mode light JTu2A.101 JTu2A.108 in silicon-on-insulator waveguide through grating coupler Inverse Design of Long-range Intensity Correlations Super-Absorbing Metamaterials Using Epsilon-Near-Ze- is proposed. The presented device is compact and high in Scattering Media, Milan Koirala1, Raktim Sarma2, ro Plasma Resonance, Jinnan Chen1, Justin W. Cleary2, sensitive (422nm/RIU). Hui Cao2, Alexey G. Yamilov1; 1Missouri Univ of Science Joshua R. Hendrickson2, Evan M. Smith2,3, Junpeng & Technology, USA; 2Applield Physics, Yale University, Guo1; 1Univ. of Alabama in Huntsville, USA; 2Air Force JTu2A.115 USA. We obtain analytical expression for the long-range Research Lab, USA; 3KBRwyle, USA. Metamaterials of Dual-Functional Integrated Modulator-Detector for spatial intensity correlation in a disordered waveguide epsilon-near-zero (ENZ) and dielectric layer structures are Optical Communication On-Chip, Shuai Sun1, Ruoyu of an arbitrary shape. Inverting this relationship allows a investigated for wideband light absorption in the wave- Zhang1, Jiaxin Peng1, Hamed Dalir2, Tarek El-Ghazawi1, possibility to manipulate wave transport complimentary length range from 1 to 2 micron. Increasing the number Volker J. Sorger1; 1George Washington Univ., USA; 2Ome- to the wavefront shaping. of ENZ-dielectric layers results in wider absorption band. ga Optics, Inc., USA. Here we show a novel integrated broadband hybrid photonic-plasmonic device termed JTu2A.102 JTu2A.109 MODetector featuring dual light modulation and detec- Mid Infra-red Directional Coupler Optical Switch Design of microring resonator sensor for liquid chem- tion, with 10 dB extinction ratio, 0.8 dB insertion loss, Based on Phase Change Material Embedded in Par- ical sensing applications, Amna Bedi1, Sonika Singh1, and 0.7 A/W responsivity. tially Etched SOI Waveguide, Nadir Ali1, Rajesh Kumar1; Santosh Kumar2, Nan-Kuang Chen2; 1Dept. of Electrical 1Indian Inst. of Technology Roorkee, India. An ultra-com- and Electronics & Communication Engineering, DIT Univ., JTu2A.116 pact 1x2 optical coupler switch at wavelength 2.1 µm is India, India; 2School of Physics Sciences and Information Ultrafast sources for optical virtual skin biopsy: a

designed and simulated using Ge2Sb2Te 5 embedded in Technology, Liaocheng Univ., China. A microring reso- fiber-based solution to pulses at 1250 nm, Hsiang-Yu 1,2 1,2 3 1,2 silicon waveguide. The phase alteration of Ge2Sb2Te 5 nator sensor for liquid chemical sensing applications is Chung , Wei Liu , Rüdiger Greinert , Franz Kärtner , results in coupling ratio change from >90% to < 2%. proposed, which is based on the change in optical signal Guoqing Chang1,4; 1DESY, Germany; 2Physics, Universität intensity with refractive index of analytes. The input and Hamburg, Germany; 3Skin Cancer Center Buxtehude, output intensity inside sensor is measured. Germany; 4The Hamburg Centre for Ultrafast Imaging, Universität Hamburg, Germany. We demonstrate a fiber-based ultrafast source generating 450-mW, sub-100- fs pulses centered at 1250 nm by implementing self-phase modulation enabled spectral selection. This source is ideal for harmonic generation microscopy in human skin.

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JTu2A.117 JTu2A.124 JTu2A.131 RAPID Fast Hyperspectral Detection of the Frequency Optimal Plasmonic Nanopillars Array for Light Con- Numerical Modeling of Unit Cell and Field Stop 1 Response of Highly Scattering Tissue using a Femto- finement of Fluorescence Imaging, Soojung Kim , Effects in Apodized Pupil Lyot Coronagraphs, Scott 1 1 1 1 second Pulse with Light Labeling, Patrick A. Stockton , Hyerin Song , Tae Young Kang , Heesang Ahn , Kyujung Will1, James R. Fienup1; 1Univ. of Rochester, USA. We 1 2 1 1 Randy Bartels , Mohammad Torabzadeh , Bruce J. Kim ; Pusan National Univ., South Korea. Vertical SiO2 show that the field diffracted from the apodizing mask 2 1 2 Tromberg ; Colorado State University, USA; Biomedical nanopillars array terminated with Au nanofilms for light of an apodized pupil Lyot coronagraph can be computed Engineering, Univ. of California, USA. We introduce a new localization. Reducing light scattering to enable light exactly, and analyze the effect on instrument performance diffuse optical spectroscopy measuring technique for fast localization in the vicinity of metals. As a result, we could as a function of field stop diameter acquisition of optical properties. We utilize a broad band- confirm reducing light scattering. width femtosecond illumination to simultaneously probe JTu2A.132 the spectral and frequency response of a scattering tissue. JTu2A.125 Sparsity-based One-dimensional Phase Retrieval of Development of Four Channel Based Linear Continuous Non-negative Pulse Trains, Qianqian Su1, JTu2A.118 Stokes-Mueller Polarization Microscope For Tissue Jianfei Hua1; 1Tsinghua Univ., China. Represented by dis- 1 1 Silicon photonics with hybrid integrated 2D MoO3: Characterization, Spandana K. U , Krishna K. Mahato , crete-time signals, continuous non-negative pulse trains 1 1 plasmonic pH driven sensing and reconfigurability, Nirmal Mazumder ; Manipal Academy of Higher Edu- have been successfully reconstructed from under-sampled 1 1 1 Guanghui Ren , Baoyue Zhang , Markus Knoerzer , cation, India. We have developed Stokes-Mueller based measurements of their Fourier amplitude based on as- 1 1 1 Arnan Mitchell , Jianzhen Ou ; Royal Melbourne Inst. polarization imaging technique to extract the quantitative sumptions of sparsity and finite support. of Technology, Australia. A new plasmonic label-free microstructural information of biological sample. optical pH sensing platform is realized by integrating JTu2A.133 + two-dimensional H doped molybdenum oxide on a JTu2A.126 Contour-based depth-of-field extension in multi-focus silicon micro-ring resonator. High Speed, High-Resolution First Surface Defect integral imaging system, Miao Zhang1, Yongri Piao1, Detection for Virtual and Augmented Reality Optics, Chuanzhen Wei1, Rui Xu1; 1Dalian Univ. of Technology, 1 1 JTu2A.119 Timothy A. Potts ; Dark Field Technologies, USA. First China. To solve the limited DoF of integral imaging, the Quantitative Second-harmonic Generation Imaging of surface inspection of uncoated and coated optics is contour-based object extraction and minimum bound- Tissue Damage from Environmental-scanning Electron critical for high volume production of Virtual and Aug- ing box based size correction are developed. Finally, 1 1 Microscopy, Woowon Lee , Kimani C. Toussaint, Jr. ; mented Reality headsets and eyeware. Solid State Laser all-in-focus EIs are obtained by the block-based image 1 Univ. of Illinois, USA. We quantitatively evaluate changes Reflection (SSLR) technology delivers high-speed first fusion method. of collagenous tissue due to beam exposure in an envi- surface inspection. ronmental-scanning electron microscope. Quantitative JTu2A.134 second-harmonic generation microscopy is used to image JTu2A.127 Programmable Multiwavelength Achromatic Focusing ber and assess selected regions before and after exposure. Vibrational Spectroscopic Preliminary Study of Blood Through Scattering Media, Jiannan Wang1, Wei Li1, 1 and Its Components in Mice, Ariunbold Gombojav , Su- Jietao Liu1, Xueying Sun1, Guo Chengfei1, Xiaopeng 1 1 2 JTu2A.120 priya Nagpal , Prakash Adhikari , Enkhsaikhan Purevjav , Shao1; 1XiDian Univ. of China, China. We demonstrate 3 1 2 Development of Medical Diagnostic System using a Lu Lu ; Mississippi State Univ., USA; Pediatrics, Univ. with numerical simulations that multiple scattering can 3 Non-labeled Extraordinary Optical Transmission Bio- of Tennessee Health Science Center, USA; Genetics, be controlled via serial optical transmission matrix and 1 1 1 sensor, Yeji Lee , Hyerin Song , Heesang Ahn , Kyujung Genomics and Informatics, Univ. of Tennessee Health parallel optical transmission matrix to obtain achromatic 1 1 kim ; Pusan National Univ., South Korea. Extraordinary Science Center, USA. Spectroscopic study of blood and 3D focusing at arbitrary position by wavefront shaping. optical transmission sensor with sensitivity of 458.33 nm/ serum of the mice strains produced from progenitors RIU was designed and distinguished the hypoalbumin- C57BL/6J and DBA/2J for identifying biomarkers is JTu2A.135 emia group with a probability of over 98 %. underway. A preliminary study shows that multivariate Surface Normals Correction by Removing Specular Re-

Tuesday, 18 Septem Tuesday, spectral analyses discriminate the mice with their ages. flection for 3D Polarization Imaging, Shengzhi Huang1, JTu2A.121 Fei Liu1, Pingli Han1, Xuan Li1, Xiaopeng Shao1; 1XiDian 1.7-μm gain-switched thulium-doped fiber laser with JTu2A.128 RAPID Univ., China. 3D polarization imaging is challenged by electrically tuning and its application to spectroscopic Imaging Brain Pathology in Alzheimer’s Disease by surface distortion caused by the specular reflection. We 1 1 photoacoustic imaging, Can Li , Jiawei Shi , Cihang Contrast-Enhanced Optical Coherence Tomography, used the dichromatic reflection model to remove the 1 2 2 1 1 1 Kong , Xiaojing Gong , Liang Song , Kenneth K. Wong ; Bernhard Baumann , Antonia Lichtenegger , Pablo Eu- specular reflection and correct surface normals to obtain 1 2 1 1 1 1 Univ. of Hong Kong, Hong Kong; Inst. of Biomedical gui , Martina Muck , Marco Augustin , Thomas Roetzer , accurate 3D image. and Health Engineering, Shenzhen Institutes of Advanced Danielle J. Harper1, Adelheid Woehrer1, Christoph 1 1 Technology, Chinese Academy of Sciences, China. We Hitzenberger ; Medizinische Universität Wien, Austria. JTu2A.136 demonstrate a gain-switched thulium-doped fiber laser We present three approaches for using optical coher- Bit-length vs. dimension: Image formation of ghost with electrically wavelength tuning in the 1.7-μm band. ence tomography (OCT) to visualize neuritic plaques in imaging, Meijing Ke1, Junhui Li1, Guohua Wu1, Bin The achieved stable laser pulses with an energy of 1.6 μJ Alzheimer’s disease based on intrinsic optical properties, Luo1, Dongyue Yang1, Longfei Yin1, Hong Guo2; 1Beijing are exploited to implement spectroscopic photoacoustic namely their birefringence, spectroscopic characteristics Univ of Posts & Telecom, China; 2Peking Univ., China. microscopy of lipid. and scattering profile. Length-variant pooling according to conducted sample number excludes endeavor to expand image dimension JTu2A.122 JTu2A.129 RAPID from image formation process of ghost imaging, leaving Single-shot multiple-color holography of single neuron Spatial resolution of compressive-sensing-based ghost bit-length growth alone. using spatial frequency multiplexing, Behnam Tayebi1, imaging can approach theoretical upper bound, Xieyu 1 1 1 1 1 1 1 1 Yeonwoo Jeong , Jae-Ho Han ; Korea Univ., South Korea. Du , Junhui Li , Guohua Wu , Bin Luo , Dongyue Yang , JTu2A.137 1 2 1 Here, we present a single-shot triple-wavelength holo- Longfei Yin , Hong Guo ; Beijing University of Posts Structural contrast function improves image alignment 2 graphic microscopy technique for high-resolution color & Telecom, China; Peking Univ., China. We present a precision of ghost imaging, Dongchu Han1, Junhui Li1, imaging of the neuronal cells using a monochromatic method for the spatial resolution of ghost imaging to Guohua Wu1, Bin Luo1, Dongyue Yang1, Longfei Yin1, camera. The feasibility of the technique is demonstrated approach its theoretical upper limit based on parameter Hong Guo2; 1Beijing University of Posts & Telecom, by imaging of neuronal cells. optimization of compressive sensing. This method shows China; 2Peking Univ., China. Structural contrast function robustness against additive noise in bucket detector. prevails cross-correlation and mutual information on JTu2A.123 image alignment of ghost imaging, both accuracy (pixel A Report on ISCOSA sponsored 1st International JTu2A.130 RAPID shift) and robustness (error curve kurtosis), especially in Day of Light Event 2018 – Light Enchantment, Sumit Pixel-based Engineering for Suppression of Higher under-sampling condition. Ghosh1,2; 1School of Optics-ISCOSA, India; 2Physics, Orders of Diffraction, Joanna Starobrat1, Jan Bolek1, Andhra Vidyalaya-Osmania Univ., India. Indian Student Michal Makowski1; 1Faculty of Physics, Warsaw Univ. of Chapter of Optical Society of America celebrated the Technology, Poland. For the reduction of higher diffraction 1st International Day of Light 2018 by organizing an orders in computer hologram reconstructions, pixel engi- optics-based event ‘Light Enchantment’ for the un- neering methods are proposed: pixel apodization (phase der-privileged students. A brief report is being presented. and amplitude) and their randomization. The results of simulations and experiments are discussed.

50 FiO + LS 2018 • 16–20 September 2018

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JTu2A • Poster Session I and Dynamic E Posters—Continued JTu2A.138 JTu2A.140 JTu2A.141 Open Source Computational Photonics Toolbox, Alec Raman Spectroscopy as a Tool for Characterisation Stationary Fourier Transform Spectrometer, Erez N. Hammond1, Ryan M. Camacho1; 1Electrical & Computer of Liquid Phase Devices, Benjamin T. Hogan1; 1Univ. of Ribak1; 1Technion Israel Inst. of Technology, Israel. We Engineering, Brigham Young Univ., USA. We present Exeter, UK. In this paper, we demonstrate how Raman developed a non-scanning and extremely stable Fou- an open source and collaborative integrated photonics spectroscopy can be an effective tool for the elucidation rier Transform Infra-red Spectrometer, for detection of simulation environment capable of accurately modeling of the properties of liquid phase devices, looking at signal narrow atmospheric lines. We intend to use it to identify individual components using traditional vectorial meth- enhancement through to beam profiling. and measure molecules in our own atmosphere or in ods and large circuits using linear system theory and remote planets. deep learning.

JTu2A.139 3D Multiple Sclerosis Image Analysis Based on Proba- bilistic Methods for a 4F Array, Eduardo Perez1; 1DICIS, Mexico. This work presents a detection of multiple sclero- sis (MS) knowing is a challenging process, which usually requires several analysis of the imaging over time. All of this to be implemented in a 4F array.

10:00–15:00 Science & Industry Showcase Visit page 11 for a complete program schedule. Tuesday, 18 Septem ber

FiO + LS 2018 • 16–20 September 2018 51

FiO Abstracts.indd 17 8/20/18 9:11 AM Science & Industry Showcase 13:00–14:00 Rapid Fire Oral Presentation II, Science & Industry TheaterJOINT FiO + LS Presider: David Busch; Univ. Texas Southwestern Medical Center at Dallas, USA Participating posters are noted in the list of poster for session JTu3A with the icon RAPID. Each presenter will have 3 minutes and the order will be determined by poster number.

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13:00–15:00 JTu3A • Poster Session II and Dynamic E Posters

JTu3A.1 E-Poster JTu3A.8 RAPID JTu3A.14 Polarization-Filtering Negative Curvature Fibers, Noise tolerant LIDAR via mode selective up-conver- A Metasurface-inspired Focusing Collector for Con- 1 1 2 1 1 sion detection, Yong Meng Sua1, Amin Shahverdi1, Ivan centrated Solar Power Applications, Qing Ding , Chengli Wei , Curtis Menyuk , Jonathan Hu ; Baylor 1 1 1 2 Dickson1, Malvika Garikapati1, Yu-Ping Huang1; 1Stevens Shama Barna , Kyle Jacobs , Aakash Choubal , Glennys Univ., USA; Univ. of Maryland Baltimore County, USA. 1 2 2 3 Inst. of Technology, USA. We study mode selective Mensing , Zhong Zhang , Kaito Yamada , Robert Tirawat , We design a polarization-filtering negative curvature fiber. 3 3 4 up-conversion detection to improve SNR for LIDAR Nicholas Kincaid , Guangdong Zhu , Tim Wendelin , L. The loss ratio between the two polarizations is more than 2 1 1 1 applications. We demonstrate a 41-dB increase in the Jay Guo , Placid Ferreira , Kimani C. Toussaint, Jr. ; Univ 100. This simple design will be useful in hollow-core fiber 2 SNR for single-photon counting compared to that of of Illinois at Urbana-Champaign, USA; Univ. of Michigan, devices that are sensitive to polarization effects. 3 direct detection using a InGaAs single-photon detector. Ann Arbor, USA; National Renewable Energy Lab, USA; 4 JTu3A.2 E-Poster Solar Dynamics, USA. We present a metasurface-inspired Simulation Retrieval of Frequency-Resolved Optical JTu3A.9 RAPID planar focusing collector for concentrated solar power. Gating Traces Using Neural Network, Zhe Guang1,2; Enhanced Light Absorption in Silicon Nanocones Fabrication is achieved using two-photon lithography and 1School of Physics, Georgia Inst. of Technology, USA; for Solar Applications, Sara Al Menabawy1, Joumana subsequent nanoimprint lithography test for scalability. 2School of Computer Science, Georgia Inst. of Technol- El-Rifai1, Mohamed M. Swillam1; 1American Univ. in Cairo, Optical characterization results are reported. ogy, USA. We present a FROG pulse retrieval approach Egypt. In this work, we report a one-step fabrication of JTu3A.15 using neural network and Hermite-Gaussian decomposi- silicon nanocones from amorphous silicon substrates using excimer laser by melting and re-solidifying the Thin Film High Efficiency Epitaxial Lift-Off Solar Cells, tion. It shows retrieval error an order of magnitude better 1 1 1 deposited material. They show broadband absorption Drew Cardwell , Alex Kirk , Martin Drees , Christopher than before. Hermite-Gaussian modes also provide the 1 1 1 1 privilege to retrieve non-Gaussian pulses. enhancement at multiple angles. Stender , Ray Chan , Andree Wibowo , Chris Youtsey , Glen Hillier1, Mark Osowski1, Noren Pan1; 1MicroLink De- JTu3A.3 E-Poster JTu3A.10 RAPID vices Inc., USA. MicroLink Devices has developed flexible, Biomolecule Detection Based on a Liquid Crystal Film Coherence Resonances and Bandgaps in Plasmonic lightweight, high efficiency III-V inverted metamorphic 1 1 1 1 multi-junction epitaxial lift-off solar cells that are attractive

ber Coated on a Single Substrate, Wei Liang Hsu , Chao- Hole Arrays, Matt Smith , Gregory J. Gbur ; Univ. Ping Pai1, Po-Chang Wu1, Mon-Juan Lee2, Wei Lee1; of North Carolina at Charlotte, USA. We theoretically for mobile, terrestrial, airborne, and space applications. 1Inst. of Imaging and Biomedical Photonics, National demonstrate the existence of optical coherence band- JTu3A.16 Chiao Tung Univ., Taiwan; 2Dept. of Bioscience Technol- gaps by simulating plasmonic interaction with a partially Femtosecond Written Silica Waveguides for High ogy, Chang Jung Christian Univ., Taiwan. In comparison coherent field on a subwavelength-thickness gold plate Extinction Polarization Filtering, 1 1 with the conventional approach entailing sandwiched perforated by a linear array of circular holes. Timothy Lee , Qi Sun , Rand Ismaeel1, Marta Castro-Lopez2, Bocheng Cao3, cells for LC-based biosensing, here we demonstrate a 1 1 1 JTu3A.11 Martynas Beresna , Gilberto Brambilla ; Optoelectronics simpler label-free platform—a unique single-substrate 2 Development of an In-situ Metrology Technique for Research Centre, Univ. of Southampton, UK; Huawei technique capable of rapid screening and bioassay of 3 DNA hybridization. Freeform Optics, Daliramu Burada1, Kamal Pant1,2, Technologies Duesseldorf GmbH, Germany; Huawei Vinod Mishra1,3, Bichra Mohamed4, Gufran Khan1, Stefan Technologies Japan KK, Japan. Silica waveguides with po- Tuesday, 18 Septem Tuesday, JTu3A.4 E-Poster Sinzinger4, Chandra Shakher1; 1Indian Inst. of Technology larization-selective transmission were written by femtosec- Non-linear vertical coupling for III-V/SOI interconnects, Delhi, India; 2DRDO, IRDE, India; 3CSIR, CSIO, India; ond laser inscription using linear and circular polarization. Ruth Rubio Noriega1; 1National Inst. for Research and 4Fachgebiet Technische Optik, Technische Universität By tailoring writing parameters, polarization-dependent Training in Telecommunications, Peru. Hybrid III-V/Si Ilmenau, Germany. The paper presents the development losses from 0.5 to 24dB at 1310nm were achieved. devices have been recently exploited for optical inter- of Shack-Hartmann sensor as in-situ metrology technique JTu3A.17 connects applications. In this work, a 0.2dB loss for the that can be integrated to the machining platforms and Polarization-Holographic-Element-Based-Method for S, C and L bands, process tolerant, vertical evanescent helps in the development process of aspheric and Determining the Complex Birefringence Distribution, coupling structure is presented. freeform optics within the required tolerances. Barbara N. Kilosanidze1, George Kakauridze1, Irina 1 1 1 JTu3A.5 E-Poster JTu3A.12 Kobulashvili , Yuri Mshvenieradze ; Lab of Holographic Mode-Selective Image Upconversion, Santosh Kumar1, High-Efficiency Beam Deflection of Visible Light Recording and Processing of Information, Georgian He Zhang1, Stephanie Maruca1, Yu-Ping Huang1; 1Dept. of Based on Dielectric Metasurfaces, Rifat Ahmmed Technical Univ., Georgia. A new method is presented for Physics, Stevens Inst. of Technology, USA. We experimen- Aoni1, Mohsen Rahmani1, Lei Xu2, Khosro Kamali1, Andrei determining the distribution of complex birefringence in tally demonstrate selective frequency up-conversion of Komar1, Jingshi Yan1, Dragomir Neshev1, Andrey Mirosh- different materials based on the polarization-holographic complex spatial modes through a nonlinear crystal, with nichenko2; 1Nonlinear Physics Centre, Research School element when circularly polarized light beam transmitted potential applications in areas of quantum communica- of Physics and Engineering, The Australian National through the sample diffracts on the element tions and pattern recognition. Univ., Australia; 2School of Engineering and Information Technology, Univ. of New South Wales, Australia. We JTu3A.18 1 JTu3A.6 E-Poster experimentally demonstrate a dielectric metasurface for Image rotation with three skew lenses, Jakub Belin , 2 1 2 Rotation of dielectric microspheres trapped near an beam-deflection with off-resonance near-unity transmit- Gergely Ferenczi ; Univ. of Glasgow, UK; Univ. of ultrathin optical fiber, Cindy Liza C. Esporlas1, Georgiy tance in the visible wavelength. By reducing the supercell Strathclyde, UK. We present an image-rotating arrange- Tkachenko1, Aili Maimaiti1, Viet Giang Truong1, Síle Nic length, the beam deflection can switch efficiently and ment of skew lenses. We demonstrate the image-rotating Chormaic1; 1Okinawa Inst. of Science & Technology, Ja- achieved 16.50o. property using ray-tracing simulations. pan. We experimentally investigate the rotational motion JTu3A.19 arising from laser light scattering of dielectric particles JTu3A.13 Superbunching Effect of Light with Digitally Designed Design and Fabrication of Microring Resonator Array trapped near the evanescent field of a water-clad ultra- 1 Wavefront, Lu Zhang1, Yiping Lu1, Liming Li1, Guoquan for mid-IR Filter Applications, Rajat K. Sinha , Meher thin optical fiber with a guided quasi-circularly polarized 1 1 1 1 fundamental mode. Zhang1; 1Nankai Univ., China. Superposition of multiple Wan , Saawan Kumar Bag , Shailendra Varshney ; Indian two-photon paths is introduced with digital wavefront en- Inst. of Technology Kharagpur, India. Mid-IR bandpass JTu3A.7 E-Poster coding technique, resulting in superbunching effect. Ex- filter based on microring resonators 2D array is designed Ultra-Fast Relaxation and Singlet-Triplet Conversion perimentally, we measured a bunching peak of 4.18±0.05 and fabricated. The structure is analyzed using transfer Quantum Yield of Ir Complexes, Salimeh Tofighi1; 1Univ. with the digitally designed wavefront of classical light. matrix-method and simulated using FDTD. The design is of Central Florida, CREOL, USA. The nonlinear-optical fabricated with IP-Dip using two-photon polymerization properties of Iridium complexes including triplet yield process. and excited-state cross-sections was studied by steady- state time-resolved measurements using picosecond and femtosecond excitation at multiple wavelengths.

52 FiO + LS 2018 • 16–20 September 2018

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JOINT FiO + LS

JTu3A • Poster Session II and Dynamic E Posters—Continued

JTu3A.20 JTu3A.27 JTu3A.34 Classification of Propagation-Invariant Space-Time Variation of Refractive indices from twisted dielectric High-repetition-rate Femtosecond-laser Inscription of Wave Packets in Free-Space, Basanta Bhaduri1, Murat media, Dipan Sinha1, Dipti Banerjee2; 1Dept. of Physics, Low-loss Thermally Stable Waveguides in Lithium Nio- Yessenov1, Hasan E. Kondakci1, Ayman Abouraddy1; 1Univ. Univ. Of Calcutta, India; 2Dept. of Physics, Vidyasagar bate, Teerawat Piromjitpong2,1, Mykhaylo Dubov3, Sonia of Central Florida, CREOL, USA. We classify all propaga- College for Women, India. The properties of twisted Boscolo2,1; 1School of Engineering and Applied Science, tion-invariant pulsed beams with respect to their group dielectric matrix has been studied for symmetric and Aston Univ., UK; 2Aston Inst. of Photonic Technologies, velocity, direction of propagation, and spatial-frequency anti-symmetric part. Variation of refractive index with the UK; 3Optoscribe Ltd., UK. Optical-lattice-like WGs were

content. We identify 10 unique classes that we synthesize internal and external birefringence is also been studied. fabricated in z-cut LiNbO3 by HRR pulse laser. Low propa- experimentally using a single optical arrangement. gation loss was observed in both orthogonal polarizations JTu3A.28 in the visible and near-IR spectrum. Single-mode guiding JTu3A.21 Polarization and Coherence in the Hanbury Brown- was maintained after high-temperature annealing. Comparative Characteristics of the Properties of Twiss Effect, Taco D. Visser1, Ari Friberg2, David Kuebel3; Photoanisotropic Materials Composed with Covalent 1Vrije Universiteit Amsterdam, Netherlands; 2Univ. of JTu3A.35 Bond and Electrostatic Interactions, Irakli Chaganava1,2, Eastern Finland, Finland; 3Univ. of Rochester, USA. We Large Scale Optical Comb Frequencies Stabilization by Sakinah M. Alauddin4, Nurul F. Aripin4, Alfonso M. Felipe3, study the correlation of intensity fluctuations in random Using An Intro-cavity Electro-optic Polarization Mod- Irine Kobulashvili1; 1Lab of Holographic Recording and electromagnetic beams, the Hanbury Brown-Twiss effect. ulator, Yanyan Zhang1,2, Pan Zhang1, Lulu Yan1,2, Bingjie Processing of Information, Inst. of Cybernetics of Geor- Not just the state of coherence of the source, but also its Rao1, Xiaofei Zhang1,2, Wenge Guo1, Shougang Zhang1,2, gian Technical Univ., Georgia; 2Georgian State Teaching state of polarization has a strong influence. Haifeng Jiang1,2; 1National Time Sevice Center (China), Univ. of Physical Education and Sport, Georgia; 3Chemical China; 2School of Astronomy and Space Science, Univ. of and Materials Engineering Research Group, Univ. of JTu3A.29 Chinese Academy of Sciences, China. We demonstrate a Aberdeen, King’s College, UK; 4Faculty of Chemical Engi- Turbulence Mitigation using Chaos-modulated Image frequency control approach of a nonlinear-polarization-ro- neering, Univ. of Technology MARA, Malaysia. The paper Propagation along a Slanted Path under Gamma-Gam- tation mode-locked Er:fiber laser by rotating polarization presents the study of the polarization-sensitive materials ma Atmospheric Turbulence, Monish R. Chatterjee1, state with an intro-cavity electro-optic modulator, en- developed by us. It is demonstrated the advantages of Ali A P. Mohamed1; 1Univ. of Dayton, USA. Mitigation of abling a large scale high bandwidth frequency control. these light-recording organic media composed both via distortion under gamma-gamma turbulence is examined covalent bindings and through electrostatic interactions. for propagation along a low-altitude slanted path using JTu3A.36 acousto-optic chaos and the Huffnagel-Valley model. Partially Coherent Vortex Beams in the Atmosphere, Tuesday, 18 Septem JTu3A.22 System performance is measured using bit error rates Gregory J. Gbur1, Charlotte Stahl1; 1Univ of North Carolina Reflection By and Transmission Through an ENZ Inter- and compared with non-chaotic propagation. at Charlotte, USA. We investigate, through simulations, face, Zhangjin Xu1, Henk F. Arnoldus1; 1Dept. of Physics the robustness of vortices in partially coherent beams and Astronomy, Mississippi State Univ., USA. Reflection JTu3A.30 RAPID propagating through atmospheric turbulence. Several and transmission of radiation by an ENZ interface is stud- Quantum Random Number Generator with Program- classes of partially coherent vortex beams are considered. ied. For s polarization, the transmitted magnetic field is mable Probability Distributions, Lac Nguyen1, Yu-Ping circularly polarized. For p polarization, the electric field Huang2, Yong Meng Sua2, Patrick Rehain2; 1Physics, JTu3A.37 is circularly polarized and the magnetic field vanishes. Stevens Inst. of Technology, USA; 2Physics, Stevens Inst. Withdrawn of Technology, USA. We present a method of generat- JTu3A.23 ing quantum random numbers with arbitrarily defined JTu3A.38 ber High-Resolution, In-Situ Defect Detection, Timothy A. probability distributions featuring high dimensionality Measurements of the Nonlinear Refractive Index (n2) 1 1 Potts ; Dark Field Technologies, USA. Defect detection and post-processing free, for significantly improved for Indium Fluoride (InF3) Bulk Glass and Fiber, Anthony of optical glass, during vacuum deposition, has been a Monte-Carlo simulations and data analyses. M. Johnson1, Isaac Basaldua1, Robinson Kuis1, Paul Bur- long-standing industry need. A special Solid State Laser kins1, Zack Jiang2; 1Univ. of Maryland Baltimore County, 2 Reflection (SSLR) technology has been developed which JTu3A.31 USA; Thorlabs, USA. We measured the n2 of InF3 bulk is easily installed and delivers 100% inspection during Withdrawn glass and fiber using the Z-scan and the induced grating

deposition. autocorrelation (IGA), respectively. The n2 value measured

JTu3A.32 for the InF3 fiber is 1.5X that for ZBLAN fiber. JTu3A.24 Demonstration of Ultra-High Time-Bandwidth Prod- Ion Assisted E-beam Deposition of Silicon dioxide Thin uct in a Non-Reciprocal Fiber-Optic System, Davide JTu3A.39 films with Graded Refractive Index, Vemuri Srs Praveen Grassani1, Ivan Cardea1, Simon Fabbri1, Jeremy Upham2, Photonically Tunable MIR Epsilon-Near Zero Modes in Kumar1,2, Mukesh Kumar1, Neelam Kumari1,2, Vinod Karar1, Robert Boyd2, Hatice Altug1, Sebastian Schulz3, Kosmas CdO Thin Films, Elizabeth Radue1, Evan Runnerstrom2, Amit L. Sharma1,2; 1Central Scientific Instruments Organ- Tsakmakidis1, Camille-Sophie Bres1; 1Ecole Polytech- Kyle Kelley3, J. P. Maria2, Patrick Hopkins1,4; 1Mechanical isation, India; 2Optical Devices and Systems, Academy nique Federale de Lausanne, Switzerland; 2Dept. of and Aerospace Engineering, Univ. of Virginia, USA; 2Ma- of Scientific and Innovative Research, India. We report Physics, Univ. of Ottawa, Canada; 3School of Physics and terials Science, Penn State Univ., USA; 3Materials Science, 4 the design and fabrication of SiO2 films using the GLAD Astronomy, Univ. of St Andrews, UK. We demonstrate North Carolina State Univ., USA; Materials Science and technique with different incidence angles from 10° to 80° that a non-reciprocal, time-variant fiber cavity can op- Engineering, Univ. of Virginia, USA. We propose a novel by Ion-Assisted E-beam deposition resulting in the de- erate above the “fundamental” time-bandwidth limit way of tuning plasmonic absorption of light. By photoex- crease of effective film refractive index from 1.46 to 1.38. (TBL) of reciprocal structures by more than two orders citing electrons from platinum to a CdO film, we are able of magnitude. to control of the ENZ resonance frequency of the film. JTu3A.25 Phasing a Segmented Space Telescope, Erez N. Ribak1, JTu3A.33 JTu3A.40 Martin Levine1; 1Technion − Israel Inst. of Technology, Mid-Wave Infrared Nonlinear Optics in Polycrystalline Experimental Research on the KrF Laser Driven Israel. We wish to phase a segmented and sparse tele- Zinc Selenide and Zinc Sulfide, Kevin Werner2, Noah quasi-insentropic compression, Zhao Wang1, Pinliang scope in space, employing only wide-band light from an Talisa2, Brian Wilmer3, Laura Vanderhoef4, Aaron Sch- Zhang2, Bao-xian Tian1, Zhi-xing Gao1, Jing Li1, Feng-Ming extended object. A stochastic search for the sharpest weinsberg1, Christopher Wolfe4, Anthony Valenzuela4, Hu1; 1China Inst. of Atomic Energy, China; 2Beijing Inst. of image lasts up to one day, for a four-segment telescope. Chowdhury Enam2; 1ORISE, USA; 2The Ohio State Univ., Spacecraft Environment Engineering, China. The HEAVEN USA; 3SURVICE Engineering, USA; 4U.S. Army Research I laser is used to direct drive quasi-isentropic compression JTu3A.26 Lab, USA. We investigate the nonlinear optical properties up to 18 GPa in samples of aluminum without temporal Measurement of remote sound based on laser of ZnSe and ZnS using ultrashort mid-wave infrared laser pulse shaped. The monotonically increasing loading with feedback interferometry, Zongren Dai1, Kaiyi Zhu1, pulses. Multiple harmonic generation in both materials rise time is over 16 ns. Yidong Tan1; 1Tsinghua Univ., China. An optical sound was observed, as well as significant spectral modification measurement technology is developed based on mi- of the fundamental pulse. JTu3A.41

crochip Nd:YVO4 laser feedback interferometry. The Withdrawn system can recover the sound signal by measuring the vibration of non-cooperative target, which is located in the sound field.

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JTu3A • Poster Session II and Dynamic E Posters—Continued

JTu3A.42 JTu3A.49 Quadratic Bright Soliton and Cnoidal Wave Frequency Endurance of photon indistinguishability in noisy quan- JTu3A.55 RAPID Combs in Microresonators by Second Harmonic Gen- tum networks, Armando P. Leija1, Diego Guzman-Silva2, Experimental Demonstration of CNOT Gate for 1 eration, Zhen Qi1; 1Univ. of Maryland Baltimore County, Roberto Leon-Montiel3, Markus Graefe4, Matthias Hein- Frequency-Encoded Qubits, Hsuan-Hao Lu , Joseph 2 1 2 USA. We study bright solitons and cnoidal waves in rich5, Hector-Cessa6, Alexander Szameit2, Kurt Busch1; M. Lukens , Poolad Imany , Nicholas A. Peters , Brian P. 2 1 2 1 microresonators with quadratic nonlinearity. In the case 1Max Born Inst., Germany; 2Physics, Univ. of Rostock, Williams , Andrew M. Weiner , Pavel Lougovski ; School of both fundamental frequency and second harmonic Germany; 3ICN, UNAM, Mexico; 4Physics, Univ. of Jena, of Electrical and Computer Engineering, Purdue Univ., 2 in the same dispersion regime, we obtain stable bright Germany; 5Physics, Rostock Univ., Germany; 6Optics, USA; Quantum Information Science Group, Oak Ridge solitons and cnoidal waves. INAOE, Mexico. We show that when indistinguishable National Lab, USA. We demonstrate the first two-photon photons copropagate through quantum networks affect- gate for frequency-bin qubits, using optical pulse shaping JTu3A.43 ed by nondissipative noise, the system always evolves into and electro-optic phase modulation. Our coincidence-ba- Implementation of an Alternative Method for the a steady state in which coherences accounting for particle sis CNOT has a fidelity of 0.9947±0.0008 and shows Detection and Temporal Correlation of Spontaneous indistinguishabilty perpetually prevail. controlled qubit flips in the computational basis. Parametric Down Converted Photons with Single Photon Counters, Francisco Sierra1; 1Universidad del JTu3A.50 JTu3A.56 RAPID Valle, Colombia. We propose an alternative method for Four-wave mixing of 10 µm radiation in quadratic A Single-Pass Quantum Source of Multimode Squeezed 1 1 the detection of SPDC photons and their temporal cor- nonlinear crystals, Jeremy Pigeon2, Sergei Tochitsky1, Eric States of Light, Luca La Volpe , Syamsundar De , 1 1 1 relations. All this doing mainly by photon counters, a BBO Welch1, Ilan Ben-Zvi2, Chan Joshi1; 1Univ. of California - Los Tiphaine Kouadou , Valentina Parigi , Claude Fabre , 1 1 crystal type II, a PBS and taking counts on fundamental Angeles, USA; 2Physics and Astronomy, Stony Brook Univ., Nicolas Treps ; Laboratoire Kastler Brossel, France. We points (Control points). USA. We report measurements of the effective nonlinear present a parametric down-conversion based source refractive index of quadratic nonlinear crystals using four- generating broadband squeezed light in multiple spectral modes. The source will be used to create large-scale JTu3A.44 wave mixing of a dual-frequency CO2 laser pulse. The Progress On Supercontinuum Generation of Highly contribution of second-order processes to the four-wave cluster states, and to perform space-time positioning Nonlinear Fibers at NTSC, Songtao Fan1,2, Pan Zhang1, mixing efficiency is discussed. measurements beyond classical limit. Yanyan Zhang1,2, Lulu Yan1,2, Wenge Guo1, Xiaofei Zhang1,2, Shougang Zhang1,2, Haifeng Jiang1,2; 1National JTu3A.51 JTu3A.57 time service center, China; 2Univ. of Chinese Academy Application of Machine Learning Techniques to Quan- Withdrawn of Sciences, China. We report on supercontinuum gen- tum Optical Problems, Anesan A. Reddy1, Ilya Sinayskiy1, eration in four types of highly-nonlinear-fibers (HNLFs) Francesco Petruccione1,2; 1Chemistry and Physics, Centre JTu3A.58 pumped by 1.56-μm laser solitons. Experimental results for Quantum Technology UKZN, South Africa; 2National 8×8 Programmable Quantum Photonic Processor ber provide guidelines for choosing and using HNLFs for Inst. of Theoretical Physics, South Africa. Researchers Based on Silicon Nitride Waveguides, Caterina Ta- 1 2 2 erbium-fiber-based optical frequency combs. have begun applying Machine Learning Techniques ballione , Tom A. Wolterink , Jasleen Lugani , Andreas 2 2 3 3 (MLT) to difficult problems in physics. E.g., Convolutional Eckstein , Bryn A. Bell , Robert Grootjans , Ilka Visscher , 4 3 3 JTu3A.45 Neural Networks can detect phase transitions in Ising Jelmer J. Renema , Dimitri Geskus , Chris G. Roeloffzen , 2 4 1 Spectron and Dispersive Fourier Transformation: Phase and Bose-Hubbard models. I will report on MLT applied Ian A. Walmsley , Pepijn W. Pinkse , Klaus-J. Boller ; 1 Aspect, Narek Karapetyan1,2, Minas Sukiasyan1,2, Hrach in Quantum Optics. Laser Physics and Nonlinear Optics, Univ. of Twente, 2 Toneyan1,2, Aghavni Kutuzyan1, Levon Mouradian1,2; Netherlands; Ultrafast Quantum Optics and Optical 3 1Dept. of Optics, Yerevan State Univ., Armenia; 2CAN- JTu3A.52 Metrology, Univ. of Oxford, UK; LioniX International, 4 DLE Synchrotron Research Inst., Armenia. The phase Computational Modeling of InGaAs/InP Single Photon Netherlands; Complex Photonic Systems, Univ. of behavior of spectron pulses, shaped in the far zone of Detector for High Sensitive Applications, Ahmed C. Twente, Netherlands. Integrated universal linear optical 1 1 1 Tuesday, 18 Septem Tuesday, dispersion, is discussed in view of dispersive Fourier Kadhim , Ahmad Alalyani , Ahmad S. Azzahrani , Saud networks are essential for the development of quantum transformation, on the basis of our analytical, numerical Alanzi1; 1Florida Inst. of Technology, USA. An approached information processing (QIP). We demonstrate a universal, and experimental studies. to define output current of single photon avalanche reconfigurable, 8×8 photonic processor based on Si3N4 photodiode (SPAD) is introduced using a mathematical waveguides showing a variety of QIP primitives. JTu3A.46 RAPID formula. The mathematical steps and derivations are Synthesis and Analysis of Ultrafast Waveform Gen- shown that the dependency of SPAD on gating signals. JTu3A.59 eration using Coherent Raman Sidebands, Aysan Highly Efficient Nonlinear Integrated Photonics in Bahari1, Alexandra A. Zhdanova1, Mariia Shutova1, Alexei JTu3A.53 Ultracompact Periodically-Poled Lithium Niobate 1 1 Sokolov1; 1Texas A&M Univ., USA. We combine four co- Multi-resonant Optical Nanocavities by Out-of-plane on Silicon, Ashutosh Rao , Kamal Abdelsalam , Tracy 1 1 herent Raman sidebands generated inside diamond with Magnetic Plasmon Hybridization, Seied Ali Safiabadi Sjaardema , Guillermo Camacho-González , Amirmahdi 1 1 1 an OPA-generated beam to create an ultrashort pulse. By Tali1, Wei Zhou1; 1Virginia Tech, USA. In vertically-stacked Honardoost , Sasan Fathpour ; Univ. of Central Florida, using frequency-resolved optical gating (FROG) and inter- double-cavity metal-insulator-metal nanostructures, the CREOL, USA. We present second-harmonic generation, ferometric techniques, we characterize the resultant pulse. strong optical interaction between magnetic plasmon pumped in the telecom wavelengths, with strong non- -1 -2 modes in each of the nanocavities leads to new hybridized linear conversion efficiencies up to 1230 %W cm using JTu3A.47 modes with individually tunable energy levels. ultracompact periodically-poled thin-film lithium niobate Mode-Locked Fiber Laser Pulse Repetition Rate Adjust- waveguides on a silicon chip. ment with Piezoelectric Transducer and Thermoelectric JTu3A.54 Cooler, Alexander I. Donodin1, Vasilii S. Voropaev1, SHG from Nanoparticles of Noncentrosymmetric Ge- JTu3A.60 Vladimir A. Lazarev1, Mikhail Tarabrin1,2, Valeriy Karasik1; ometry, Raksha Singla1, Wolf L. Mochan1; 1Instituto de Experimental Statistical Signature of Many-body 1 1 1Bauman Moscow State Technical Univ., Russia; 2P. N. Leb- Ciencias Físicas, UNAM, Mexico. The effect in the SHG Quantum Interference, Taira Giordani , Fulvio Flamini , 1 1 1 edev Physical Inst. of the Russian Academy of Sciences, from an almost-centrosymmetric nanoparticle is studied Matteo Pompili , Niko Viggianiello , Nicolò Spagnolo , 2,3 2,3 4 Russia. We demonstrate an adjustment of the all-fiber analytically. We obtain its bulk and surface contributions, Andrea Crespi , Roberto Osellame , Nathan Wiebe , 5,6 6 ring femtosecond erbium laser pulse repetition rate using discuss their multipolar character and their spectral res- Mattia Walschaers , Andreas Buchleitner , Fabio Sciar- 1 1 2 piezoelectric transducer and thermoelectric cooler. The onances, and compare them to numerical calculations. rino ; Fisica, Sapienza Università di Roma, Italy; Istituto experimental values are verified with theoretical results. di Fotonica e Nanotecnologie, Consiglio Nazionale delle Ricerche, Italy; 3Fisica, Politecnico di Milano, Italy; 4Sta- JTu3A.48 tion Q Quantum Architectures and Computation Group, 5 Withdrawn Microsoft Research, USA; Laboratoire Kastler Brossel, UPMC-Sorbonne Universités, CNRS, ENS-PSL Research Univ., Collège de France, CNRS, France; 6Physikalisches Institut, Albert-Ludwigs-Universität Freiburg, Germany. Quantum interference is a fundamental ingredient for technologies that can provide a quantum advantage. In this work we investigate a clear signature of its presence in a BosonSampling experiment.

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JTu3A.61 JTu3A.69 RAPID JTu3A.76 Local filtering of polarization entangled photon pairs Polarization diversity phase modulator for measuring Multi-wavelength Fiber Laser Temperature Sensor by the components of a telecom network, Brian T. frequency-bin entanglement of biphoton frequency Based on Modal Fiber Interferometer, Yanelis Lopez 1 1 1 1 Kirby , Dan Jones , Michael Brodsky ; The US Army Re- combs in in a depolarized channel, Oscar Sandoval1, Dieguez1, Julian Moises Estudillo Ayala1, Daniel Jauregui1, search Lab, USA. By treating the polarization dependent Navin B. Lingaraju1, Poolad Imany1, Daniel E. Leaird1, Mi- Luis A. Herrera Piad1, Juan M. Sierra Hernandez1, Diego loss of fiber-optic quantum channels as a local filtering chael Brodsky2, Andrew M. Weiner1; 1Purdue Univ., USA; Garcia-Mina2, Juan C. Hernandez-Garcia1, Abraham operation, we show both theoretically and experimentally 2U.S. Army Research Lab, USA. We report frequency-bin Gatelum Barrios3, Roberto Rojas-Laguna1; 1Universidad de how entanglement can be distilled by properly orienting entanglement measurements of arbitrarily polarized pho- Guanajuato, Mexico; 2Universidad del Centro Ocidente, local filters. ton pairs using a polarization diversity phase modulator, Colombia; 3Universidad Autónoma de Queretaro, Mexico. thereby extending this technique to depolarized channels A fiber optic laser arrangement for temperature sensing JTu3A.62 such as in a practical quantum networking environment. applications is presented. The multi-wavelength spectrum Towards Extending Super-conducting Nanowire Sin- has a SMSR of 40dB and moreover, the temperature gen- gle-photon Detectors into the Infrared Wavelength JTu3A.70 RAPID erated tunable multi-wavelength effect, here, a sensitivity 1 1 1 Range, Paulina S. Kuo , Brian G. Alberding ; NIST, USA. Direct extrusion of suspended-core polymer optical of 20pm/°C is achieved. We characterize the long-wavelength transmission of fibers from 3D printers, Wanvisa Talataisong1, Rand coiled and uncoiled SMF-28 and SM2000 fibers, which Ismaeel1, Martynas Beresna1, Gilberto Brambilla1; 1Op- JTu3A.77 is important for extending the range of super-conducting toelectronics Research Centre, UK. We demonstrate the Vehicular FSO Communication Systems Applying nanowire single-photon detectors (SNSPDs) to infrared single-step manufacturing of a microstructured polymer Real-time Recognition and Tracking, JIANAN ZHANG1, wavelengths beyond 1550 nm. optical fiber (MPOF) by extruding and directly drawing Wentao Xia1, Tim Kane1; 1PENN STATE UNIV., USA. As the polymer from a structured 3D printer nozzle. the field-of-view of an optical receiver decreases, the JTu3A.63 receiver gain increases. By applying real-time recognition Self-referenced continuous-variable quantum key for JTu3A.71 RAPID and tracking, the demonstration of a vehicular free-space 1 distribution over longer optical fiber links, Ming Li , Open Cavity Raman-Erbium Hybrid Random Fiber optical communication system which has a small field-of- 1 1 Milorad Cvijetic ; Univ. of Arizona , USA. We have eval- Laser with Single Arm Pumping Scheme, Nadiah view is presented. uated the impact of phase noise in self-referenced con- Zainol Abidin2, Muhammad Hafiz Abu Bakar2, Nizam tinuous-variable quantum key distribution protocol and Tamchek1, Mohd Adzir Mahdi2; 1Dept. of Physics, Faculty JTu3A.78 confirmed its application over longer optical fiber links. of Science, Universiti Putra Malaysia, Malaysia; 2Wireless Numerical Study of Spatio-Temporal Evolution of Chaotic Effects in the Generation of Broad Spectra, and Photonics Networks Research Centre, Faculty of En- Tuesday, 18 Septem JTu3A.64 gineering, Universiti Putra Malaysia, Malaysia. This paper Jose Ramon Martinez Angulo1, Juan C. Hernandez-Gar- Quantum Phase Transitions in Finite Atomic Ensemble analyzes forward and backward spectral outputs of 80 cia1,2, Jesus P. Lauterio-Cruz1, Julian M. Estudillo-Aya- 1 1 under the EIT Configuration, Raúl A. Robles ; IPT km Raman-erbium hybrid random fiber laser employing la1, Olivier Pottiez3, Jose D. Filoteo-Razo1, Carlos M. Tsing Hua, Taiwan. We study the ground states of finite single arm pumping. Stable laser generation at the output Carrillo-Delgado1, Daniel Jauregui-Vazquez1, Juan M. ensembles of Λ-type three-level atoms interacting with is achieved without resonance within the entire cavity. Sierra-Hernandez1, Roberto Rojas-Laguna1; 1Universidad two electromagnetic fields in the EIT approximation. de Guanajuato, Mexico; 2Catedratico CONACYT, Consejo Critical couplings are revealed for the existence of QPT. JTu3A.72 Nacional de Ciencia y Tecnologia, Mexico; 3Centro de Propagation of a supercontinuum light source in a Investigaciones en Optica (CIO), Mexico. We report the JTu3A.65 novel tellurite hollow core optical fiber, Hoang Tuan implementation of the RK4IP method for studying the Squeezed photons from a single quantum-dot with Tong1, Nobuhiko Nishiharaguchi1, Takenobu Suzuki1, propagation of a hyperbolic secant pulse into 10 km of 1 ber tuneable central frequency, Parvendra Kumar , Agniku- Yasutake Ohishi1; 1Toyota Technological Inst., Japan. standard fiber. The results describe the appearance of 2 1 mar G. Vedeshwar ; Dept. of Physics and Astrophysics, We experimentally demonstrated the fabrication of a chaotic phenomena in the spectral broadening. Univ. of Delhi, India. We theoretically demonstrate the novel tellurite hollow core optical fiber and managed generation of quadrature squeezed photons from a single to propagate a supercontinuum light from 500 to more JTu3A.79 quantum-dot with tuneable central frequency. The effects than 1550 nm in the fiber core by the fundamental mode. Extreme power fluctuations in optical communications, of exciton-phonon coupling on quadrature squeezing are Stanislav Derevyanko1, Alexey Redyuk2,3, Sergey Verge- also investigated. JTu3A.73 les4,5, Sergei Turitsyn6,2; 1Ben Gurion Univ. of the Negev, ITO-based Mach Zehnder Modulator, Rubab Amin1, Ri- Israel; 2Novosibirsk State Univ., Russia; 3Inst. of Computa- JTu3A.66 shi Maiti1, Caitlin Carfano1, Volker J. Sorger1; 1The George tional Technologies, Russia; 4Landau Inst. for Theoretical Design of Switch gate using Mach-Zehnder interfer- Washington Univ., USA. We report the first experimental Physics, Russia; 5Moscow Inst. of Physics and Technology, 2 ometer for quantum communications, Santosh Kumar , Mach Zehnder modulator on SOI-platform with ITO as Russia; 6Aston Inst. of Photonic Technologies, Aston 1 2 1 Amna Bedi , Nan-Kuang Chen ; Dept. of EECE, DIT the active phase-shifting material. Our results show a low Univ., UK. We present an analysis of dangerous symbol Univ., India; 2School of Physics Sciences and Information sequences in CO-OFDM optical transmission systems VπL of 0.52 V-mm with 6 dB insertion loss. Technology, Liaocheng Univ., China. In this paper, a leading to appearance of extreme power fluctuations and design of reversible switch gate using lithium-niobate JTu3A.74 study their influence on system performance in dispersion based Mach-Zehnder interferometer for quantum com- Ultra-flat Optical Frequency Comb Generation Based uncompensated long haul fiber links. munication is proposed. The results are verified using on an Electroabsorption Modulated Laser and Adap- beam propagation method. tive Pulse Shaping, Linnan Li1, Juanjuan Yan1, Jing Chen1; JTu3A.80 1BeiHang Univ., China. A scheme for the generation of One-step waveguide endface dicing approach for Sil- JTu3A.67 ultra-flat optical frequency comb (OFC) is proposed by ica-on-Silicon PIC chip, Xu Liu1, Zhekai Zhang1, Xiaohan A dynamical approach to low-cost shortcut to adiaba- using an Electroabsorption Modulated Laser and adaptive Sun1; 1Southeast Univ. (China), China. The IL of 0.055dB/ 1 1 1 ticity, Hamidreza Ramezani , Fatemeh Mostafavi ; Univ. pulse shaping. An OFC with a 0.5-dB bandwidth of 4nm facet at 1550nm wavelength is achieved for Silica-on-Sil- of Texas, Rio Grande Valley, USA. By introducing a class containing 50 spectral lines is achieved. icon waveguide using Disco ZH05-SD3500-N1-70FF/01 of non-Hermitian Hamiltonians we propose an approach blade with spindle revolution speed, workpiece feed to low-cost shortcut to adiabaticity. Our approach focuses JTu3A.75 speed and cooling water flow velocity of 30000r/min, on dynamical properties of the system and has application Analysis and Elimination of Shrinkage Phenomenon of 1mm/s and 1.2L/min. in STIRAP, tunable mode filtering. Photonic Crystal Fiber during Fusion Splicing, Chunxiao Wu1, Ningfang Song1, Jingming Song1, Jiaqi Liu1, Haowei JTu3A.81 RAPID JTu3A.68 Li1; 1Beihang Univ., China. The impact of shrinkage phe- Optomechanics Outside the Lab: Prototyping and Design and Analysis of a Cross V-shaped Nanoantenna nomenon of photonic crystal fiber during fusion splicing Field-testing a Whispering Gallery Mode Accelerome- 1 1 for Visible Region, Shanu Kumar , Pooja Chauhan , is analyzed. A method based on temperature distribution ter, Ying Lia Li1, Peter F. Barker1; 1UCL, UK. The dispersive 1 1 Ajeet Kumar ; Delhi Technological Univ., India. A cross analysis is proposed to eliminate the detrimental phe- and dissipative optomechanical coupling between a whis- V-shaped nanonoantenna is designed using gold with nomenon. The splice loss and strength are improved. pering gallery mode (WGM) resonance and the motion gap of 10 nm. The scattering cross-section and the Elec- of the WGM cavity is used to measure acceleration. We tric field at the centre is obtained with optical resonant describe the prototype assembly and the results from wavelength of 530 nm in visible range. outdoor field-trials.

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JTu3A.82 RAPID JTu3A.89 JTu3A.97 Superhydrophobic SERS Substrates based on Plas- Novel Mid-Infrared Metamaterial Thermal Emitters for Mid IR absorption using Hyperbolic Silicon tubes, Mai monic Hierarchical Micro-nanostructures, Junyeob Optical Gas Sensing, Yongkang Gong2, Sang Soon Oh2, desouky1, Ahmed Mahmoud1,2, Mohamed M. Swillam1; 1 2 2 1 Song , Weifeng Cheng , Jiangtao Cheng , Wei Zhou ; Diana L Huffaker2, Nigel Copner1; 1Univ. of South Wales, 1Physics, American Univ. in Cairo, Egypt; 2electrical, Amer- 1 2 Electrical Engineering, Virginia Tech, USA; Mechan- UK; 2School of Physics and Astronomy, Cardiff Univ., UK. ican Univ. in Cairo, Egypt. Doped semiconductors have ical Engineering, Virginia Tech, USA. Integration of We demonstrated that metamaterial technology enables been extensively investigated for mid IR metamaterials. multilayered plasmonic nanostructures with hierarchical us to tailor infrared thermal emission and provides a We theoretically demonstrate mid IR absorber using micro-nanopillar arrays can result in a superhydrophobic promising strategy towards novel, cost-effective and Doped Si/Si hyperbolic tubes with broad band absorption surface with high-performance Surface Enhanced Raman highly efficient mid-infrared source for optical gas sensing. reaching 0.95 across the mid-IR range. Spectroscopy (SERS) functionality. JTu3A.90 JTu3A.98 JTu3A.83 RAPID Withdrawn On Red, Stop. Simple Speed and Stop Control for Gallium Indium Phosphide Nanostructures with Sup- Traffic Automation, Forrest F. Jesse1; 1Beijing Xixuan pressed Photoluminescence for Applications in Nonlin- JTu3A.91 Lab, China. A simple design for local signaling in an 1 1 ear Optics, Eleonora De Luca , Dennis Visser , Srinivasan Metamaterial Tunable Notch Filters Operating in Long- intelligent transportation network which endows vehicles 1 1 1 Anand , Marcin Swillo ; KTH Royal Inst. of Technology, wave Infrared, Neelam Gupta1, Mark S. Mirotznik2; 1US with awareness of sub-meter local transportation condi- Sweden. Nanostructured GaInP shows remarkable non- Army Research Lab, USA; 2Dept. of Electrical and Com- tions, and which allows speed control and stop control linear properties. By measuring the SHG before and after puter Engineering, Univ. of Delaware, USA. We describe of vehicles is discussed. stimulating photobleaching, we observed suppressed the design of metamaterial tunable notch filter operating photoluminescence and unchanged nonlinear properties, from 8 to 12 µm based on the guided-mode resonance JTu3A.99 making it suitable for low-noise applications. phenomenon using dielectric materials germanium and Single Spot Focusing with Dielectric based Plasmonic zinc selenide and their characterization using quantum Phase Manipulation, Mayur S. Darak2, Rakesh G. Mote1, JTu3A.84 RAPID cascade lasers. Shobha Shukla3; 1Dept. of Mechanical Engineering, Indian 1 Multifocal Optical Meta-Lenses, Nantakan Wongkasem , Inst. of Technology, Bombay, India; 2Centre for Research 2 1 Patricia Briea ; Univ. of Texas Rio Grande Valley, USA; JTu3A.92 in Nanotechnology and Science (CRNTS), Indian Inst. 2 MetaSolver, USA. Multifocal optical and flat meta-lenses Size dependent optical performance of light trap- of Technology, Bombay, India; 3Dept. of Metallurgical are investigated towards designing an improved multi- ping metallic electrodes, Mengdi Sun1, Pieter G. Kik1,2; Engineering and Materials Science (MEMS), Indian Inst. focal meta-lens with ultra-thin multilayers and flat shape 1CREOL, Univ. of Central Florida, USA; 2Physics Dept., of Technology, Bombay, India. A slit type dielectric based overcoming the background noise occurring from the Univ. of Central Florida, USA. The optical performance phase manipulative plasmonic lens for in-plane focusing physical restriction of multiple focus regions. of light-trapping embedded metal electrodes with widths of linearly polarized light to a single spot is proposed. ber varying from 100-1000nm was investigated. Up to 90% of Focal spot with full-width at half-maximum of 0.28λ0 is JTu3A.85 visible light incident on the metal wire can be trapped, obtained to beat the diffraction limit. Double-sided guided-mode resonance metamaterials, limited by diffraction and plasmon-mediated absorption. Hafez Hemmati1, Robert Magnusson1; 1Univ. of Texas JTu3A.100 at Arlington, USA. We fabricate resonant metamaterial JTu3A.93 Naturally phase matched waveguides and microrings membranes with subwavelength gratings on both sides Optimized Ultrabroadband Absorbing Multilayer Thin on lithium niobate-on-insulator (LNOI), Jiayang Chen1, employing nanoimprint lithography methods. Measured Film Structure, Corey T. Matyas1, Chenglong You1, Yin Yong Meng Sua1, Heng Fan1, Yu-Ping Huang1; 1Stevens spectral response of the resonance membranes is in good Huang2, Jonathan P. Dowling1, Georgios Veronis1; 1Lou- Inst. of Technology, USA. We demonstrate naturally agreement with numerical results. isiana State Univ., USA; 2Central South Univ., China. We phase matched waveguides and microrings on chip design an optimized aperiodic multilayer thin film struc- for second-harmonic generation (SHG) with submicron Tuesday, 18 Septem Tuesday, JTu3A.86 ture with ultrabroadband absorption over a broad angular transverse mode confinement. GaN Distributed Bragg Reflector Cavity for Sensing range. Using a hybrid optimization algorithm, we achieve Applications, Simeng Jia1, Emmanuel L. Boulbar3, Krishna an average 97.9% absorption from 400 nm to 2500 nm. JTu3A.101 RAPID C. Balram1, Jon Pugh1, Tao Wang2, Duncan Allsopp3, Philip Generation of shaped THz beams by nonlinear 3 1 1 2 Shields , Martin Cryan ; Univ. of Bristol, UK; Univ. of Shef- JTu3A.94 metasurfaces, Shay Keren-Zur1,3, Daniel Mittleman2, Tal 3 field, UK; Univ. of Bath, UK. GaN grating couplers and Design and Fabrication of Embedded Nanofences Ellenbogen1,3; 1School of Electrical Engineering, Tel Aviv a distributed Bragg reflector cavity are fabricated using in Racetrack Microring Resonator for Single Gold Univ., Israel; 2School of Engineering, Brown Univ., USA; displacement Talbot lithography on GaN-on-sapphire. Nanoparticle Detection, Saawan Kumar Bag1, Rajat K. 3Center for Light-Matter Interaction, Tel Aviv Univ., Israel. Cavity resonances are simulated and measured for two Sinha1, Meher Wan1, Shailendra Varshney1; 1Indian Inst. of We present functional nonlinear plasmonic metasurfaces devices with Q factors of ~200. Technology Kharagpur, India. Photonic nanofence assist- for generation of shaped broadband THz beams. The ed racetrack microring resonator is proposed, numerically spatial phase of the emitted THz wavefront is tailored by JTu3A.87 analyzed and fabricated. Numerical results shows the the distribution of the meta-atoms orientation to control A Narrowband Photothermoelectric Detector Using device ability to detect single gold nanoparticle which the generation process. Guided-Mode Resonance Filter, Hosein Monshat1, can be a potential platform for biosensing applications. Longju Liu1, Meng Lu1; 1Iowa State Univ., USA. A nar- JTu3A.102 rowband photothermoelectric detector, integrating a JTu3A.95 Multilayer plasmonic structures for ultrasensitive guided-mode resonance (GMR) structure and a metal Fano Resonances Based on Aperture-coupled Square protein probing, Ildar Salakhutdinov1, Bo Shrewsbury1, thermocouple, is demonstrated. The detector utilizes Plasmonic System and its Application in Nanosensor, Nolan Johnston1, Ertan Salik1; 1Physics and Astronomy, the GMR effect to selectively absorb light and generate Yilin Wang1, Li Yu1; 1Beijing Univ. of Posts and Telecom- California State Polytechnic Univ., USA. Multilayer thermoelectric voltage outputs. munications, China. A novel refractive index plasmonic plasmonic structures consisting of alternating layers of nanosensor was proposed with high properties based metal and dielectric create a new type of guiding modes JTu3A.88 on groove and aperture-coupled square resonator. This with very high effective refractive index. We chose a Implementation and Optimization of a Cost-Effective nanosensor with sharp Fano profiles yield an ultra-high biomedical sensing including protein detection as the 2D Haar Transform Network for Image Compression, sensitivity of 1300nm/RIU and a FOM of 9400. main application. Catia Pinho1,2, Tiago Morgado1, Berta Neto1,2, Mario Lima1,2, António Teixeira1,2; 1Instituto de Telecomuni- JTu3A.96 ∼ ∼ JTu3A.103 cações (IT), UA, Portugal; 2Dept. of Electronics, Tele- Absolute Optimization Method of a Vertical Grating Modulation of Electromagnetically Induced Transpar- communications and Informatics (DETI), Univ. of Aveiro, Coupler, Anat Demeter1; 1Tel-Aviv Univ., Israel. Based ency in Toriodal Resonance Terahetz Metasurface, Sirak Portugal. A new cost-effective 2D Haar transform network on S-matrix formalism a method for analyzing and de- M. Mekonen1, Riad Yahiaoui1, Joshua Burrow2, Andrew Sa- for data compression composed by three 2×2 MMI signing vertical grating couplers is presented. Optimal rangan2, Imad Agha3, Jay Mathews2, Thomas A. Searles1; magic-T disposed in a two level signal decomposition efficiency values and corresponding design parameters 1Howard Univ., USA; 2Electro-Optics and Photonics, Univ. architecture is implemented and tested. A model for are provided, including a theoretical return loss limit of Dayton, USA; 3Physics, Univ. of Dayton, USA. We report design optimization is proposed. better than 56dB. modulation of electromagnetically induced transparency in toroidal planar terahertz metamaterials. By breaking symmetry, we demonstrate tunability of EIT while exciting multiple Fano-like resonances with high Q-factor.

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JTu3A.104 JTu3A.110 JTu3A.116 High Sensitivity Vibrational Mode Detection with Dop- Modeling of SPAD Response of Absorbed Near-In- Laguerre-Gaussian Vortex Beam Transmission through 3 3 pler Raman Spectroscopy, David Smith , Jeffrey J. Field , frared Light in a Biological Tissue to Improve Diffuse Mouse Brain Tissue, Sandra Mamani1; 1IUSL at 1 1 3 1 David Winters , Scott Domingue , Jesse Wilson , Daniel Optical Tomography Resolution, Ahmed C. Kadhim , City College, USA. Abstract: Light transmission of 2 3 1 2 1 1 1 Kane , Randy Bartels ; KM Labs, USA; Mesa Photonics, Ahmad Alalyani , Ahmad S. Azzahrani , Muhammad Riaz ; Laguerre-Gaussian (LG) vortex beams in different local re- 3 1 USA; Colorado State Univ., USA. We present Doppler Florida Inst. of Technology, USA. This paper introduces a gions in mouse brain tissue is investigated. Transmittance Raman, a novel detection technique for coherent Raman new mathematical model to determine the single photon is measured in ballistic region with various polarizations scattering that offers improved sensitivity and readily avalanche photodiodes response and the dark count rate states and orbital angular momentums (OAM). detects low frequency modes from 10cm-1 to 1500cm-1 that occupied with the detector output when the photon for use in studying biological systems. is absorbed by the biological tissue. JTu3A.117 Blue and Red Light Emitting Diode (LED) Variation on JTu3A.105 JTu3A.111 Soybean (Glycine Max) Growth, Selvy U. Hepriyadi1, Spectroscopic Imaging of DDS Nano-particle by Polar- Application of heat-sensitive fluorescent dyes to Wilda Prihasty1, Intan D. Kurniawati1, Achmad S. Hidayat1, ization Interferometric Nonlinear Confocal Microscopy, determine the spatial and temporal temperature dis- Iman R. Rosohadi1, Detak Y. Pratama1; 1Institut Teknologi 1 1 1 1 Chikara Egami , Shota Kawasaki ; Shizuoka Univ., Japan. tribution in liquid media, Mykyta O. Redkin , Yakunov Sepuluh Nopember, Indonesia. Soybeans were grown 2 1 1 In this study, we propose a polarization-interferometric V. Andrii , Gaiduk Natalia ; Minor Academy of Science, in uniform boxes and obtained that most optimum 2 nonlinear confocal microscope targeted on Drug Delivery Ukraine; Optics, KNU , Ukraine. For many technologi- soybean plant is using the lighting ratio of the red LEDs System (DDS) spectroscopic imaging. The microscope cal processes,a non-contact measurement of the local 75% and blue 25% as the reference of modern artificial successfully measured microscopic optical anisotropy in temperature is necessary. A pyrometric method doesn’t light for soybean. a single DDS nano-particle. provide the necessary spatial resolution and accuracy. There we used the phenomenon of fluorescence depen- JTu3A.118 RAPID JTu3A.106 dence on temperature. Assessment of basal cell carcinoma from normal human Optical coherence propagation in biological tissues skin tissues using Resonance Raman spectroscopy, Lin with significant scattering by Green’s functions, JTu3A.112 Zhang Chen1, Cheng-hui Liu1, Binlin Wu2; 1The City Col- 1 1 Jose Luis Ganoza-Quintana , Felix Fanjul-Velez , Jose Sensitivity Improvement for a Smartphone-Based lege of New York, USA; 2Southern Connecticut State Univ., 1 1 1 L. Arce-Diego ; Universidad de Cantabria, Spain. Lateral Flow Immunoassay Reader, Lalita Saisina , USA. VRR spectroscopy was used for BCC and normal 2 2 Diagnostic optical techniques employ usually intensity Ratthasart Amarit , Armote Somboonkaew , Oraprapai skin tissues with 532nm excitation. The spectra showed 3 3 1 measurements, disregarding coherence. Scattering Gajanandana , Orawan Himananto , Boonsong Sutapun ; significant changes in collagen, carotenoids and lipids. 1 2 greatly influences propagation. Analyzing coherence Suranaree Univ. of Technology, Thailand; National Elec- These enhanced fingerprints demonstrate a potential use Tuesday, 18 Septem 3 propagation in scattering media by Green’s functions tronics and Computer Technology Center, Thailand; Na- as label-free pathology method. could provide additional contrast. tional Center for Genetic Engineering and Biotechnology, Thailand. We show that manually adjusting the camera’s JTu3A.119 RAPID JTu3A.107 exposure time of a smartphone lateral flow reader to Photonic Resonator Outcoupler Microscopy (PROM) Extracting Fluorescence Efficiency and Emission the highest slope of the nonlinear transfer function can for Quantitative Monitoring of Stem Cell Focal Ad- 1 Spectra of Cervical Tissue, Shih Cheng Tu , Tsan-Hsueh significantly improve the sensitivity of the reader. hesion Area, Yue Zhuo1, Ji Sun Choi1, Thibault Marin2, 1 1 1 Huang , Ting-Wen Yu , Ming-Hwa Hong , Ling-Hong Hojeong Yu1, Brendan A. Harley1, Brian Cunningham1; 2 2 1 1 Wei , Chi-Hau Chen , KUNG-BIN SUNG ; National JTu3A.113 1Univ of Illinois at Urbana-Champaign, USA; 2Univ. of 2 Taiwan Univ., Taiwan; National Taiwan Univ. Hospital, An Accessible Implementation for Synthetic Optical Illinois Research Park, USA. We developed a novel la- 1,2 3 Taiwan. This study aims to extract layer-resolved fluores- Holography (SOH), Arturo Canales , Martin Schnell , bel-free imaging approach, named Photonic Resonator ber 2 1 1 cence efficiency and emission spectral shape of in-vivo Raul I. Hernandez-Aranda , P. Scott Carney ; The Inst. Outcoupler Microscopy (PROM) utilizing the reduction of 2 cervical mucosa tissue by a two-layered fluorescence of Optics, Univ. of Rochester, USA; Photonics and the peak-resonance intensity reflected from a photonic Monte Carlo model. Mathematical Optics Group, Tecnológico de Monterrey, crystal surface. PROM can monitor the variation of focal 3 Mexico; CIC nanoGUNE, Spain. We propose an acces- adhesion areas in live cells dynamically and quantitatively JTu3A.108 sible implementation for synthetic optical holography for extended time. Single Element Detection Phase Contrast Spatial (SOH) in confocal microscopes by using an interferometry Frequency Modulation Imaging, Nathan G. Worts1, objective, and a nano-positioning z-stage, thus providing JTu3A.120 2 2 3 4 Jeff Field , Randy Bartels , Jason Jones , Jeff Broderick , quantitative phase imaging capabilities. Polarization Splitter with TE Homogeneous Media 1 1 2 Jeff Squier ; Colorado School of Mines, USA; Electrical and TM Inhomogeneous Media, Poliane A. Teixeira1, and Computer Engineering, Colorado State Univ., USA; JTu3A.114 Daniely G. Silva1, Lucas H. Gabrielli2, Danilo Spadoti1, 3 4 Moog Inc., USA; Epilog Laser, USA. For the first time, Optical Parametric Amplification of Gated Confocal Mateus Junqueira1; 1Federal Univ. of Itajubá, Brazil; dynamic phase contrast imaging is demonstrated using Reflectance Microscopy Signals in Scattering Media, 2School of Electrical and Computer Engineering, Univ. of 1 1 1 1 1 single element detection, spatial frequency modulated Yi Sun , Haohua Tu , Sixian You , Stephen Boppart ; Univ. Campinas, Brazil. QCTO is employed to develop reflec- imaging (SPIFI). Sub-micron axial resolution is shown. of Illinois , USA. We apply optical parametric amplifica- tionless non-magnetic polarization splitter with uniaxial tion to amplify weak ballistic photons and suppress the properties, where the transformation is applied only in JTu3A.109 multiple-scattering background. The reflectance imaging the TM mode. A low insertion loss and high extinction The Influence of Melanopsin Activation on the signal are amplified with over 50 dB gain. Improvements rate within a broadband are achieved. Cone-mediated Photopic White Noise Electroretino- in imaging depth are demonstrated. gram (wnERG) in Humans, Prakash Adhikari1, Andrew JTu3A.121 1 3 4 2,5 J. Zele , Dingcai Cao , Jan Kremers , Beatrix Feigl ; JTu3A.115 Passive Underwater Polarization Imaging in Neritic 1 School of Optometry and Vision Science & Inst. of Feasibility Study of Spectral Fusing GD-OCM using Area, Yi Wei1, Pingli Han1, Fei Liu1, Kui Yang1, Xinhua 1 Health and Biomedical Innovation, Queensland Univ. FPGA Acquisition Device, Panomsak Meemon , Yuta- Wang2, Xiaopeng Shao1; 1XiDian Univ., China; 2Chang- 2 1 1 1 of Technology (QUT), Australia; School of Biomedical na Lenaphet , Joewono Widjaja ; Suranaree Univ. of chun Inst. of Optics, China. A passive underwater po- Sciences & Inst. of Health and Biomedical Innovation, Technology, Thailand. Gabor-domain optical coherence larization imaging method is proposed to address color 3 Queensland Univ. of Technology (QUT), Australia; Dept. microscopy (GD-OCM) overcomes depth-of-focus limita- cast and degradation of image contrast in neritic area of Ophthalmology and Visual Sciences, Univ. of Illinois at tion by combining multiple images acquired at different imaging. Results demonstrate its contribution to object 4 Chicago, USA; Dept. of Ophthalmology, Univ. Hospital focus positions. Here, an implementation of FPGA-based information restoration in underwater target detection. Erlangen, Germany; 5Queensland Eye Inst., Australia. Gabor fusion to improve processing speed was studied. The white noise ERG (wnERG) measurements using JTu3A.122 silent-substitution methods show melanopsin activation Effective pipeline to suppress coherent noise in digital supresses the human cone wnERG, potentially mediated holograms recorded under visible and infrared laser via retrograde signalling from melanopsin cells to cones light, Vittorio Bianco1, Pasquale Memmolo1, Melania through dopaminergic amacrine cells. Paturzo1, Pietro Ferraro1; 1Consiglio Nazionale delle Ricerche-ISASI, Italy. We introduce an effective pipeline to reconstruct denoised digital holograms from multiple or single shot recordings. This is based on the simulation of noise diversity and a sparsity promoting filtering scheme.

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JTu3A • Poster Session II and Dynamic E Posters—Continued

JTu3A.123 JTu3A.131 JTu3A.138 Parallel GPU Computing in Light Scattering Metrology Graphene and the Control of Liquid Crystal Alignment, Multiphoton processing technologies applied in 1 1 1 of Ultrafast Surface Dynamics, Larry Theran , Armando Benjamin T. Hogan ; Univ. of Exeter, UK. Here, we present laser-based 3D printing, Bogdan S. Calin1, Marian 1 1 1 1 Rúa , Felix Fernández , Sergiy Lysenko ; Univ. of Puerto results on using graphene as electrodes for controlling Zamfirescu1, Irina Paun1, Catalin Luculescu1, Florin Jipa1, Rico, USA. Phase-retrieval algorithms are developed for the orientation of liquid crystal molecules. We examine Stefana Iosub1, Emanuel Axente1, Felix Sima1; 1INFLPR, parallel computing of surface autocorrelation function how graphene can pre-align the molecules as well as be Romania. Micrometer scale 3D printing using various (ACF) and for solving the inverse problem of light scat- used to apply electric field. materials, either through additive or subtractive manufac- tering. A real-time visualization of ACF was achieved for turing, offers a clean, precise and reproducible method transient spectroscopy of materials. JTu3A.132 RAPID of fabricating various passive devices for biomedical Reconstruction of conditions of rays in space using applications. JTu3A.124 a light-field display combined with Retro-Reflector, 1 2 1 Snow Cover Monitoring Algorithm in Northeast China Toru Iwane , Hirotsugu Yamamoto ; Nikon Corporation, JTu3A.139 1 1 2 Using FY-2G Satellite Data, Tong Wu , Lingjia Gu , Ruizhi Japan; Dept. of Optical Engineering, Utsunomiya Univ., Organic Microlasers with Tunable Output, Yongli Yan1; 1 1 1 Ren , Haoyang Fu ; College of Electronic Science and Japan. With reversing a light-field camera system com- 1Chinese Academy of Sciences, China. A supermolecu- Engineering, Jilin Univ., China. The multi-temporal geo- bined with retro-reflector which can be regarded as a time lar inclusion strategy to construct wavelength-tunable stationary satellite FY-2G was used to reduce the cloud reversing device for light, 3D scene can be reconstructed microlasers was developed. Both β-cyclodextrin and interference. The BRDF models were used in angular from light-field data acquired by light-field camera. metal-organic framework materials have been successfully correction. An improved snow monitoring algorithm adopted as matrix to encapsulate various dyes for lasing. combined with geostationary satellite and BRDF model JTu3A.133 Novel 1066nm Nd:GdYTaO laser under indirect and was proposed. 4 JTu3A.140 1 1 1 direct pumping, Xudong Li , Guichuan Xu ; National Relativistic Laser-Plasma Diagnostics with the Third JTu3A.125 Key Lab of Tunable Laser Technology, Harbin Inst. of Harmonic, Matthew Edwards1, Alec R. Griffith1, Tim General Theoretical Analysis of Noise in Single-pixel Technology, China. CW and acousto-optically Q-switched Bennett1, Julia Mikhailova1; 1Princeton Univ., USA. We Imaging, 1 1 1 Robby Stokoe , Patrick Stockton , Ali Pezeshki , operations with a novel Nd:Gd0.69Y0.3TaO 4 mixed crystal experimentally demonstrate the efficient generation 1 1 Randy Bartels ; Colorado State Univ., USA. In single-pixel were demonstrated for the first time under indirect and of second and third harmonic light from a solid-density imaging, every reconstructed pixel includes noise from direct pumping. plasma for relativistic laser intensities and compare the the entire object. We derive a general expression for emission characteristics to simulation and theory. the noise associated with any single-pixel imaging JTu3A.134 technique, enabling development of techniques that Surface Plasmon Polariton Generation in a Sin- JTu3A.141 1,2 account for noise. gle-Walled Carbon Nanotube, Sergey G. Moiseev , Igor Cr:ZnSe laser generation in two longitudinal modes ber 1,3 1 1 Zolotovskii , Yuliya Dadoenkova , Aleksei Kadochkin ; regime with intracavity monoblock Fabry-Perot in- 1 2 JTu3A.126 Ulyanovsk State Univ., Russia; Kotelnikov Inst. of Radio terferometer for methane saturation spectroscopy, Withdrawn Engineering and Electronics of the Russian Academy of Mikhail Tarabrin1,2, Sergey Tomilov1,2, Vladimir Lazarev1, 3 Sciences, Russia; Institute of Nanotechnologies of Micro- Valeriy Karasik1, Alexey Kireev2, Alexander Shelkovnikov2, JTu3A.127 electronics of the Russian Academy of Sciences, Russia. Dmitry Tyurikov2, Mikhail Gubin2,3; 1Bauman Moscow State Classification of Saline-alkaline Soil Using Multispectral Show that high quality of carbon nanotube in surface Technical Univ., Russia; 2P. N. Lebedev Physical Inst. of the 1 1 Remote Sensing Data, Haoyang Fu , Chenglin Sun , plasmon polariton generator as a resonator is achieved Russian Academy of Sciences, Russia; 3National Research 1 1 Lingjia Gu ; Jilin Univ., China. This paper analyzes the due to modulation of the phase velocity of the surface Nuclear Univ. MEPhI, Russia. We reported on the Cr:ZnSe relationship between soil salinity and spectral character- plasmon polariton wave along the nanotube. single crystal laser with intracavity monoblock Fabry-Perot istics. And LANDSAT 5 TM multispectral data is used to interferometer and two Lyot filters for methane saturation Tuesday, 18 Septem Tuesday, classify saline-alkaline soil into three degrees according JTu3A.135 RAPID spectroscopy at 2.36 μm. to salinization ratings. Time Resolved Study of Optical Properties and Microscopic Dynamics During the Drying of TiO2 JTu3A.128 Films by Spectral Diffusing Wave Spectroscopy, Luis Speckle Reduction in Computer-Generated Hologra- F. Rojas-Ochoa1, Damián Jacinto-Méndez1, Angel A. phy with Multi-level Amplitude Encoding, Hang Feng1, Duran-Ledezma1; 1Cinvestav-IPN, Mexico. We present a Weiping Wan1, Qihuang Gong1,2, Yan Li1,2; 1Peking Univ., combined experimental, theoretical and numerical study China; 2Shanxi Univ., China. Speckles often occur in the of photon transport and microscopic dynamics in rigid and

reconstructed image of a phase-only computer-generated drying turbid thin TiO2 films during the full drying process. hologram. Here we present the speckle reduction by en- coding hologram with both the phase and multi-level am- JTu3A.136 plitude, which can be realized by a dielectric metasurface. Study of dual-wavelength quasi-mode-locked regimes in a strict polarization-controlled Er-fiber ring laser, JTu3A.129 Luis Alberto Rodriguez Morales1, Hector Santiago-Her- Image Focus Analysis using Gaussian Windows applied nandez1, Baldemar Ibarra-Escamilla1, Manuel Durán to Fourier Transform Frecuency, Eduardo Perez1; 1DICIS, Sanchéz1, Marco V. Hernández-Arriaga1, Evgeny A. Kuzin1; Mexico. Different analysis techniques have been devel- 1Optics, INAOE, Mexico. We report a dual-wavelength oped to help understand and characterize image analysis quasi mode-locked (DWQML) operation of a strict polar- with focal errors, in this paper we present an implementa- ization-controlled passively mode-locked Er-Fiber laser. tion using Gaussian windows applied to Fourier analysis. The DWQML properties are studied by a birefringent Fiber optical loop mirror (FOLM). JTu3A.130 Multi-resolution Based Cone-beam Computed To- JTu3A.137 mography High Precision Point Cloud Acquisition, Jia Acousto-Optic Filter with Ultra-Narrow Bandwidth, Zheng1, Dinghua Zhang1, Kuidong Huang1, Yuanxi Sun1; Nikolai I. Petrov1, Vladislav I. Pustovoit1; 1Scientific and 1Northwestern Polytechnical Univ., China. We improve Technological Center of Unique Instrumentation of Rus- disconnections in sub-pixels of cone-beam computed sian Academy of Sciences, Russia. Significant increase in tomography (CBCT) slice images. The proposed meth- spectral resolution of acoustooptic filter due to spatial od, which is based on the multi-resolution, can acquire variation of refractive index of medium is shown. Influence more connective sub-pixels and point cloud with higher of light absorption and random variation of dielectric precision. constant on the filter spectrum is investigated.

58 FiO + LS 2018 • 16–20 September 2018

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15:00–16:30 15:00–16:30 15:00–16:30 FTu4A • Applied Nanoplasmonics: Solar – FTu4B • Short Pulse Lasers FTu4C • Terahertz Science Sensing – Communication Presider: Junho Cho; Nokia Bell Labs, USA Jelena Vuckovic; Stanford University, USA Presider: Ortwin Hess; Imperial University, UK

FTu4A.1 • 15:00 Invited FTu4B.1 • 15:00 Invited FTu4C.1 • 15:00 Invited 1 1 Title to be Determined, Harry Atwater ; California Institute Spatiotemporal Mode-Locking in Multimode Fiber Topological Insulator Lasers, Miguel A. Bandres1, of Technology, USA. No abstract available. Lasers, Frank W. Wise1; 1Cornell Univ., USA. Existing Steffen Wittek2, Gal Harari1, Midya Parto2, Jinhan Ren2, mode-locked lasers operate in a single transverse mode. Demetrios N. Christodoulides2, Mordechai Segev1, Locking of multiple transverse and longitudinal modes Mercedeh Khajavikhan2; 1Technion, Israel; 2CREOL, USA. in a laser was recently demonstrated. Implications for We demonstrate a topological insulator laser exhibiting laser science and high-power sources will be discussed. topologically-protected transport. The topological properties give rise to single mode lasing, robustness against defects, and higher slope efficiencies compared to its trivial counterpart.

FTu4A.2 • 15:00 Invited FTu4B.2 • 15:30 FTu4C.2 • 15:30 Solving the Resistive Loss Problem in Optical Antennas, Patterned Graphene on SiN Waveguides with NPR for Withdrawn 1 Eli Yablonovitch1, Sean Hooten1; 1University of California, Fiber Laser Mode-Locking, Goran Kovacevic , Takuma Shirahata1, Bingchang Wu1, Ting-Hui Xiao2, Lei Jin1, Taiki

ber USA. One of the greatest problems in metal optics (of 3 3 2 1 which plasmonics is a subset), is loss and dissipation in the Inoue , Shigeo Maruyama , Zhenzhou Cheng , Sze Set , 1 1 2 metal. The basis of all radio is that antennas can concentrate Shinji Yamashita ; RCAST, Univ. of Tokyo, Japan; Dept. 3 electromagnetic energy within an extremely small volume, of Chemistry, Univ. of Tokyo, Japan; Dept. of Mechanical <10‑15(l)3. Resistive loss limits every application of metals in Engineering, Univ. of Tokyo, Japan. We passively mode optics, particularly in the new concept of “optical antennas”. locked a fiber laser using SiN waveguides covered with Such antennas produce sub-wavelength concentration of graphene of different lengths, and observed two types of optical energy, enabling the antenna-LED (Light Emitting solitons, with single and multiple pulses. Grating couplers Diode), which can be faster than lasers. The tiny optical induce NPR, but graphene triggers mode-locking. antenna vertices experience locally concentrated optical currents which severely increase Ohmic losses. When the FTu4C.3 • 15:45 Tuesday, 18 Septem Tuesday, FTu4B.3 • 15:45 concentrated optical region is smaller than the electron Hybrid mode-locked erbium fiber laser with a 40 GHz Effect of Pulse Duration on the Performance of Sub-Ter- mean-free-path in the metal, surfaces collisions lead to even 1 phase modulator and graphene saturable absorber, awatt Laser Wakefield Acceleration, Chia-Ying Hsieh , further dissipation. On the other hand, dielectric antennas 1 2 1 Eduardo J. Aiub1, Eunezio Thoroh de Souza1, Lucia Saito1; Shih-Hung Chen , Ming-Wei Lin ; Dept. of Physics, Na- have little dissipation, but they do not concentrate electro- 2 1Universidade Presbiteriana Mackenzie, Brazil. We report tional Central Univ., Taiwan; Inst. of Nuclear Engineering magnetic energy nearly as well as metallic antennas. If the a hybrid mode-locked erbium fiber laser operating at and Science, National Tsing Hua Univ., Taiwan. A 3-D metallic optical antenna is supplemented by 10nm dielectric 40 GHz using CVD monolayer graphene on a D-shaped particle-in-cell (PIC) model is developed to investigate the tips at the vertices, they suffer only 2x larger concentration fiber as saturable absorber. As result, we obtain ultrashort effect of pulse duration when 1030-nm lasers are applied volume, but the Ohmic loss problem becomes solved. pulses with temporal width of 1 ps. to drive the sub-terawatt laser wakefield acceleration.

FTu4B.4 • 16:00 FTu4C.4 • 16:00 Pre-chirp Managed Amplification Using Chirped Mir- Multiple Acceleration of High-velocity Flyer Driven rors for Pulse Compression, Huang Hangdong1,2, Yang By Long-pulse KrF Laser, Bao-xian Tian1, Zhao Wang1, Xie1, Hao Teng2, Shaobo Fang2, Hainian Han2, Guoqing Pinliang Zhang2, Zhixing Gao1, Jing Li1, Fengming Hu1; Chang2, Zhiyi Wei2; 1Xi Dian Univ., China; 2Chinese 1Dept. of Nuclear Physics, China Inst. of Atomic Energy, Academy of Sciences, China. We employ high-dispersion China; 2Beijing Inst. of Spacecraft Environment Engineer- chirped mirrors as the pulse compressor and demonstrate ing, China. Planar aluminum flyers are accelerated to more an Yb-fiber pre-chirp managed amplification laser system, than 10 km/s driven by long-pulse laser. Multiple accel- which produces 55 fs pulses with 43 W average power. eration processes were observed by VISAR. However, the flyer is easily broken up for four or more acceleration because of 2-D effects.

FTu4B.5 • 16:15 FTu4C.5 • 16:15 Passive Q-switching Tm-Doped Fiber Laser by Using an EuPRAXIA - a Compact, Cost-Efficient XFEL Source, Alcohol-Based Saturable Absorber, Manuel Duran-San- Maria Katharina Weikum1, Paul A. Walker1, Ralph Ass- chez1, Berenice Posada-Ramirez1, Ricardo Iván Alvarez-Ta- mann1; 1Deutsches Elektronensynchrotron DESY, Germa- mayo2, Baldemar Ibarra-Escamilla1, Jared Alaniz-Baylón1, ny. The EuPRAXIA design study aims to develop a first Miguel Bello-Jiménez3, Patricia Prieto-Cortes2, Evgeny large-scale accelerator and Free-Electron-Laser facility A. Kuzin1; 1INAOE, Mexico; 2Universidad Autonoma based on plasma acceleration technology. We present an de Nuevo Leon, Mexico; 3IICO, UASLP, Mexico. With overview over the status of the project as well as possible the maximum pump power of 1.42 W are obtained user applications. Q-switched pulses with minimum pulse duration of ~1.46 µs and maximum repetition rate of 66.71 kHz, peak power of 634 mW and pulse energy of 0.93 µJ.

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15:00–16:30 15:00–16:30 15:00–16:30 FTu4D • Optical Technologies for FTu4E • Integrated Nanophotonic Devices LTu4F • Extreme Laser Science I Autonomy in Realistic Weather Presider: Mohammad Hafezi, University of Presider: David Reis; Stanford University, Maryland Joint Quantum Institute, USA USA

The general understanding that sensors “work” often FTu4E.1 • 15:00 LTu4F.1 • 15:00 Invited neglects real world conditions outside of laboratories Free-space Communication Links with Transmitting and Boiling the Quantum Vacuum with Extremely Intense or sunny streets. Most tests and demonstrations focus Receiving Integrated Optical Phased Arrays, Matthew Laser Light, Sebastian Meuren1; 1Princeton Univ., USA. on controlled or favorable conditions, leaving out the Byrd1, Christopher V. Poulton1, Murshed Khandaker1, According to our current understanding of quantum harsher realities of real-world operation. Rain, snow, fog, Erman Timurdogan1, Diedrik Vermeulen1, Michael R. electrodynamics (QED) the properties of matter change pollen, dust, and numerous other common obscurants can Watts1; 1Analog Photonics, USA. A lens-free chip-to-chip qualitatively in the presence of ultra-strong electromag- negatively affect a variety of sensing modalities. Sensor free space optical communication link showing data trans- netic fields. The scale at which novel quantum effects are failure can take a variety of forms: graceful degradation mission from a single transmitter to multiple receivers is predicted to occur is called the QED critical or Schwinger with built-in warnings, unknown blind-spots, low signal- demonstrated using steerable integrated silicon photonic field. By colliding highly energetic gamma photons with to-noise ratios (known or unknown), etc. In this session we optical phased arrays at a data rate of 1Gbps. ultra-intense optical laser pulses the strong-field quan- address failure modalities, how improved sensor design tum regime of light-matter interaction is explorable with can improve autonomy estimations, and the optical tech- FTu4E.2 • 15:15 existing technology. In particular, nontrivial properties nologies needed to address common weather conditions. Highly-efficient second-harmonic generation in of the quantum vacuum (vacuum birefringence and semi-nonlinear nanophotonic waveguides, Rui Luo1, dichroism, anomalous dispersion), the production of Panelists: Yang He1, Hanxiao Liang1, Mingxiao Li1, Qiang Lin1; matter from pure light, and laser-induced electron-pos- Chris DeBrunner, Lockheed Martin, USA 1Univ. of Rochester, USA. We report second-harmonic itron recollision processes are now within experimental Paolo Masini, Raytheon Vision Systems, USA generation in semi-nonlinear nanophotonic waveguides reach. After a general introduction into strong-field QED Joseph Minor, U.S. Army, USA composed of titanium oxide and lithium niobate, with recent results related to those phenomena are discussed Colin Reese, U.S. Army Research Laboratory, USA a theoretical normalized conversion efficiency of 2900 and conceptual similarities to analogous phenomena in W-1cm-2, and an experimental efficiency of 650 W-1cm-2. atomic physics are pointed out.

FTu4E.3 • 15:30 LTu4F.2 • 15:30 Invited Probing finite-size effects and disorder in extended Extreme Conditions from Ultra-Intense Femtosecond Tuesday, 18 Septem slow light photonic crystal coupled-cavity waveguides, Laser Pulses Interacting with Aligned Nanostructures, Mohamed S. Mohamed1, Yiming Lai2, Momchil Minkov3, Jorge J. Rocca1, Reed J. Hollinger1, V. N. Shlyaptsev1, Vincenzo Savona1, Antonio Badolato4, Romuald Houdré1; Maria Capeluto1, Alden H. Curtis1, Chase Calvi1, Stephen 1Inst. of Physics, École Polytechnique Fédérale de Laus- Kasdorf1, Vural Kaymak2, Alexander Pukhov2, Yong Wang1, anne, Switzerland; 2The Inst. of Optics, Univ. of Rochester, Shoujun Wang1, Alex Rockwood1; 1Colorado State Univ., USA; 3Ginzton Lab, Stanford Univ., USA; 4Dept. of Physics, USA; 2Heinrich-Heine-Universität, Germany. Irradiation of Univ. of Ottawa, Canada. Slow light properties of Si ordered nanowire arrays with highly relativistic pulses is photonic crystal coupled-cavity waveguides comprising demonstrated to volumetrically heat solid density matter up to 800 cavities are experimentally investigated using to extreme temperatures, resulting in record conversion Fourier-space imaging. The influence of cavity chain into keV photons, high energy ions, & ultrafast neutron length and disorder on slow light transport is elucidated. bursts. ber

FTu4E.4 • 15:45 High-quality two-dimensional lithium niobate photonic crystal slab nanoresonators, Mingxiao Li1, Hanxiao Li- ang1, Rui Luo1, Yang He1, Qiang Lin1; 1Univ. of Rochester, USA. We report a 2D LN PhC slab nanoresonators with high optical Q over 3 hundred thousand. Such a high quality enables us to probe the intriguing anisotropy of nonlinear optical phenomena of LN never reported previously.

FTu4E.5 • 16:00 Invited LTu4F.3 • 16:00 1 Superconducting Nanowire Single-photon Detector A high-energy mid-infrared to THz laser, Yuxi Fu , 1 1 1 Integrated with a Nanophotonic Cavity,Julian Münz- Katsumi Midorikawa , Eiji J. Takahashi ; RIKEN, Japan. berg2, Andreas Vetter2, Wladislaw Hartmann1, Fabian Employing a dual-chirped difference frequency genera- Beutel1, Carsten Rockstuhl2, Wolfram Pernice1;1University tion (DC-DFG) method, we generate a source tunable of Munster, Germany; 2Karlsruhe Institute of Technology, from mid-infrared (3 μm) to THz (15 THz). DC-DFG, which Germany. We present the design and the characterization is an energy scalable approach, enables us to generate of a new generation of on-chip single-photon detectors, few-mJ THz pulses. integrated with a double heterostructure photonic crystal cavity to combine high detection efficiency in the near-in- frared and sub-ns recovery time.

LTu4F.4 • 16:15 Jitter-Induced Max-of-N Fluence Distribution at Na- tional Ignition Facility, Zhi M. Liao1, C W. Carr1, Paul We- gner1; 1Lawrence Livermore National Lab, USA. Measured pointing jitter from NIF is used to simulate the effect of Max-of-N accumulated fluence distribution. The simulate result was able to reproduce the measured Max-of-N effect for different energy and wavelength operations.

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16:45–18:15 16:45–18:15 16:45–18:00 FTu5A • Quantum and Near-Field FTu5B • Semiconductor Lasers and SDM FTu5C • Novel Lasers and Applications Nanoplasmonics Presider: Bob Jopson; Nokia Bell Labs, USA Presider: Kaoru Minoshima; University of Presider: Ortwin Hess; Imperial University, Electro-Communications, Japan UK

FTu5A.1 • 16:45 Invited FTu5B.1 • 16:45 Invited FTu5C.1 • 16:45 Invited Strong Coupling of a Single Quantum Dot to a Plas- Quantum-Inspired Redesign of the Semiconductor Random Lasers for Sensing, Judith M. Dawes1, Wan monic Nanoresonator at Ambient Conditions, Bert Laser for High Coherence , Amnon Yariv1; 1Caltech, USA. Zakiah Wan Ismail1,2, Charlotte Hurot1,3, Corentin Huard1,3, Hecht1; 1Inst. of Physics, Univ. Of Würzburg, Germany. The semiconductor laser (sl) basic architecture reflects Nonthanan Sitpathom1,4; 1MQ Photonics, Dept of Physics We exploit the ultrasmall modal volume of plasmonic the historical need for high gain needed to achieve CW and Astronomy, Macquarie Univ., Australia; 2Universiti slit resonators to achieve broadband strong coupling to operation. This design is antithetical to high coherence Sains Islam Malaysia, Malaysia; 3Ecole Centrale de Lyon, quantum dots at ambient conditions. The slit resonantor i.e. to small Schawlow-Townes (ST) linewidth.Our new France; 4Mahidol Univ., Thailand. We sensitively detect is positioned by means of scanning probe technology design starts with a drastic lowering of the optical modal biomolecules by their effect on gold nanoparticle ag- with respect to the quantum dot. losses which is a prerequisite to the reduction of the gregates in a random laser. The aggregation affects the noisy coherence -lowering spontaneous emission into scattering properties of the laser, enabling us to quanti- the laser mode. New lasers fabricated in our group will tatively measure dopamine to nanomolar concentrations. be described and relevant data shown which include ST linewidths in the single Hz regime Semiconductor lasers with sub hertz ST linewidths are extrapolated.

FTu5A.2 • 17:15 Invited FTu5B.2 • 17:15 FTu5C.2 • 17:15 Giant Nonlinear Response at a Plasmonic Nanofocus Influence of the upper nonlasing state on the route Enhanced THz Emission from Two-Color Femtosecond 1 Drives Efficient Four-wave Mixing Over Micron Length to chaos of InAs/GaAs quantum dot lasers, Heming Laser Filamentation at Low Pressures, Dogeun Jang , 3 1 1,2 1,2 1 1 Scales, Rupert Oulton1, Michael P. Nielsen1, Xingyuan Shi1, Huang , Dejan Arsenijević , Dieter Bimberg , Frederic Yungjun Yoo , Ki-Yong Kim ; Univ. of Maryland at Col- 3,4 1 2 Paul Dichtl1, Stefan A. Maier1; 11Imperial College London, Grillot ; Institut für Festkörperphysik, Technische Univer- lege Park, USA; Thorlabs Imaging Systems, USA. We 2 UK. We report efficient four-wave mixing (FWM) over sität Berlin, Germany; “Bimberg Chinese-German Center report enhanced terahertz (THz) emission from elongated, micron-scale interaction lengths at telecommunications of Green Photonics” of Chinese Academy of Science at two-color-laser filamentation at low gas pressures. This 3 wavelengths on silicon. This was achieved by creating a CIOMP, China; COMELEC, LTCI, Télécom ParisTech, counterintuitive pressure dependence is investigated with 4 giant nonlinear response within an integrated plasmonic gap Université Paris-Saclay, 46 rue Barrault, France; Center experimental and numerical studies. waveguide incorporating a nonlinear polymer. The technique for High Technology Materials, Univ. of New-Mexico, 1313 ber introduces the possibility of compact, broadband, and Goddard SE, USA. This paper investigates the route to efficient frequency mixing integrated with silicon photonics. chaos of a quantum dot laser emitting exclusively on a single lasing state. Results reveal that amplified sponta- neous emission from the upper non-lasing state drastically accelerates the destabilization process.

FTu5A.3 • 17:45 Invited FTu5B.3 • 17:30 Invited FTu5C.3 • 17:30 Plasmonics with Quantum States of Light Towards Laguerre-Gaussian Spatial Mode Sorter, Joel A. Carpen- Coherent Extreme-Ultraviolet Source Applied to Atom 1 Quantum Applications, Sahin Ozdemir1; 1Department of ter1; 1Queensland Univ., Australia. Abstract not available. Probe Tomography, Luis Miaja Avila , Ann N. Chiara- 1 1 1 Engineering Science and Mechanics, Pennsylvania State monti , Paul T. Blanchard , Norman A. Sanford , Henry C. Kapteyn2, Margaret M. Murnane2, David R. Diercks3, Tuesday, 18 Septem Tuesday, University, USA. Plasmonics promise novel properties to 3 1 2 integrated quantum photonics, such as nanoscale footprint Brian P. Gorman ; NIST, USA; JILA, Univ. of Colorado, 3 and strong light-matter interactions. In this talk, I will discuss USA; Colorado School of Mines, USA. We have adapted our studies on probing plasmonic structures using single and an atom probe tomograph (APT) with an extreme ultra- entangled photons and realizing quantum applications such violet (EUV) source. The observations suggest that the as random number generation and entanglement distillation photoionization pathway provided by the EUV light is in plasmonic structures. superior to the thermal mechanism in conventional APT.

FTu5C.4 • 17:45 Measurement of the nonlinear refractive index of air constituents from λ=2.5 μm to λ=10.6 μm, Sina Zahed- pour Anaraki1, Scott W. Hancock1, Fatholah Salehi1, Jared K. Wahlstrand2, Howard Milchberg1; 1Univ. of Maryland at College Park, USA; 2National Inst. of Standards and Technology, USA. We measure the nonlinear refractive indices of major air constituents in the wavelength range of λ=2.5μm-10.6μm extending the range of prior mea- surements [1]. These results are important for the study of intense laser propagation in the atmosphere. FTu5B.4 • 18:00 Mode-Group Selective Air-Clad Photonic Lantern, Neethu Mariam Mathew1, Lars Grüner-Nielsen2, Mario A. Castaneda1, Michael Galili1, Karsten K. Rottwitt1; 1DTU, Denmark; 2Danish Optical Fiber Innovation, Denmark. A new method for fabrication of mode group selective photonic lanterns is experimentally demonstrated. The design is very simple, using only a tapered fiber bundle and an air-cladding. Good mode group selectivity is demonstrated.

18:30–20:30 Conference Reception, International Ballroom

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16:45–18:15 16:45–18:15 16:45–18:15 FTu5D • Optical Technologies for FTu5E • Topological Photonics LTu5F • Extreme Laser Science II Autonomy in Unstructured Environments Presider: Simone Ferrari, University of Presider: Jorge Rocca; Colorado State Münster, Germany University, USA

Typical discussions of autonomy revolve around self-driv- FTu5E.1 • 16:45 Invited LTu5F.1 • 16:45 Invited ing cars on the streets of major metropolitan areas. These Non-Hermitian Photonics: Lasers and Sensors, Merce- Title to be Determined, Agostino Marinelli1; 1SLAC highly structured environments offer standard visual cues, deh Khajavikhan1; 1Univ. of Central Florida, CREOL, USA. National Accelerator Lab, USA. Abstract not available. commonly accepted behavioral protocols, and obstacles Abstract not available. occurring within a standard plane and region. Throughout large parts of the world, it is not unusual to find the local road is dirt track which may have limited variation from the surrounding landscape. Moreover, operation off-road is regularly required by the military, rescue personnel, and aid organizations. For an autonomous system to operate in complex, unstructured environments, the sensors must be able to observe the environment in a new way. This session will address the difficulties facing optical sensors in environments ranging from featureless snow fields to dense jungles. FTu5E.2 • 17:15 Invited LTu5F.2 • 17:15 Panelists: An intense soft X-ray harmonic super-continuum gener- Brendan Byrne, Argo AI, USA Towards Quantum Topological Photonics, Mohammad Hafezi1; 1Joint Quantum Inst., USA. I discuss two recent ated by a three-channel optical waveform synthesizer, Marcus Chevitarese, Raytheon, USA 1 1 1,2 3 application of topological photonics in the quantum Bing Xue , Yuxi Fu , Kotaro Nishimura , Oliver Mucke , Deva Ramanan, Carnegie Mellon University, USA 2 1 1 regime: (1) strong light-matter interaction in topological Akira Suda , Katsumi Midorikawa , Eiji J. Takahashi ; Robert Sadowski, U.S. Army TARDEC, USA 1 2 3 photonic crystals (2) topological quantum source of light RIKEN, Japan; Tokyo Univ. of Science, Japan; Center in silicon ring resonators. for Free-Electron Laser Science, DESY, Germany. We report a soft X-ray super-continuum supporting 200 as

isolated attosecond pulses at 60 eV generated using a Tuesday, 18 Septem TW-scale three-channel optical waveform synthesizer. The continuum soft X-ray pulse energy is beyond 0.2 μJ at the exit of the argon gas.

LTu5F.3 • 17:30 Invited Probing Photoionization Dynamics by High-spec-

tral-resolution Attosecond Spectroscopy, Shiyang ber Zhong1, Marcus Isinger1, Richard Squibb2, David Busto1, Anne Harth1, David Kroon1, Saikat Nandi1, Cord Arnold1, Miguel Miranda1, J. M. Dahlström1,3, Eva Lindroth3, Raimund Feifel2, Mathieu Gisselbrecht1, Anne L’Huillier1; 1Dept. of Physics, Lund Univ., Sweden; 2Dept. of Physics, Gothenburg Univ., Sweden; 3Dept. of Physics, Stockholm Univ., Sweden. Photoionization time delays are measured with two-color (XUV+IR) interferometric technique. The combination of attosecond temporal resolution and FTu5E.3 • 17:45 high spectral resolution from narrowband harmonics Parity-Time (PT) symmetric photonic system based allows the study of ultrafast dynamics in both time and on Parametric Gain, Tong Lin1, Avik Dutt1, Xingchen frequency domain. Ji1, Utsav Dave1, Alexander Gaeta1, Michal Lipson1; 1Co- lumbia Univ., USA. We report the first demonstration of

PT symmetry based on parametric gain, in a single Si3N4 microring. We observe the typical merging of eigenvalue branches as the gain/loss contrast between counterpro- pagating modes is increased.

FTu5E.4 • 18:00 LTu5F.4 • 18:00 Topological Photonics with Bichromatic Photonic Dissipative Soliton Resonance in a Figure-Eight Crystals, Filippo Alpeggiani1, L. Kuipers1; 1TU Delft, Thulium-Doped Fiber Laser, Manuel Duran-Sanchez1, Netherlands. We investigate the spectrum of bichromatic Berenice Posada-Ramirez1, Baldemar Ibarra-Escamilla1, photonic crystals, a novel class of nanostructures which Hector Santiago-Hernandez1, Ricardo Iván Alvarez-Ta- represent a photonic analog of topological insulators. mayo3, Miguel Bello-Jiménez2, Evgeny A. Kuzin1; 1INAOE, Nontrivial topology is illustrated by the formation of Mexico; 2IICO, UASLP, Mexico; 3Universidad Autonoma topologically protected boundary states. de Nuevo Leon, Mexico. We reported dissipative soliton resonance effects passively mode-locked figure-eight thulium doped fiber laser. At maximum pump power was achieved 85.18 ns pulse duration, a pulse energy of 206 nJ, a repetition rate of 1.19 MHz.

18:30–20:30 Conference Reception, International Ballroom

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08:00–09:00 08:00–09:00 08:00–09:00 FW1A • The Coming of Age for Smart FW1B • Novel Lasers and Photodetectors FW1C • Nanophotonics I Glasses, AR and VR Presider: Alexey Turukhin; TE SubCom, USA Presider: Katarzyna Matczyszyn; Wroclaw Presider: Bernard Kress; Microsoft, USA University of Science and Techn., Poland

Introduction to the AR/VR themed days at FIO 2018, FW1B.1 • 08:00 FW1C.1 • 08:00 Invited Bernard Kress; Microsoft, USA. High-Speed Waveguide Integrated Si Photodetector Enabling Next-Generation Optical Microsystems, on SiN-SOI Platform for Short Reach Optical Inter- Gordon A. Keeler1; 1DARPA, USA. Integrated photonics 1 1 1 connect, Avijit Chatterjee , Saumitra S , Sujit K. Sikdar , promises revolutionary solutions for communications, 1 1 Shankar K. Selvaraja ; Indian Inst. of Science Bangalore, sensing, and metrology. This talk describes DARPA India. We demonstrate high-speed Silicon pin photo- efforts to develop technology through investments in detector integrated with SiN waveguide. Optimized components and materials, and highlights programs waveguide-photodetector coupling yields maximum driving innovation. responsivity of 0.44A/W and highest ever bandwidth of 15.5GHz for waveguide integrated Silicon photodetector.

FW1A.1 • 08:10 Invited FW1B.2 • 08:15 User-centered Design of Head Worn Displays, Thad 10-Gb/s Floor-Free Transmission of a Hybrid III-V Starner1; 1School of Interactive Computing, Georgia Inst. on Silicon Distributed Feedback Laser with Optical of Technology, USA. Fashion and head weight are more Feedback, Sandra Gomez1, Heming Huang1, Bewindin important than field-of-view for on-the-go AR displays, Sawadogo1, Frederic Grillot1,2; 1Telecom ParisTech, and displays centered in line-of-sight may be rejected by France; 2Univ. of New Mexico, USA. A 10 Gb/s trans- on-the-go users due to safety perceptions. What other mission by direct modulation of a distributed feedback surprises might user-centered design reveal? semiconductor laser heterogeneously integrated onto silicon is studied with optical feedback. Its impact on the bit error rate and power penalty degradation is analyzed.

FW1A.2 • 08:35 Invited FW1B.3 • 08:30 Invited FW1C.2 • 08:30 Head-Mounted Displays for High Stress Occupations, III-V Membrane Buried Heterostructure Lasers on SiO2/ Multiplexing Soliton-Combs in Optical Microres- 1 2,3 James E. Melzer1; 1Thales Visionix, Inc., USA. Pilots, Si Substrate, Tomonari Sato1; 1NTT Device Technology onators, Erwan Lucas , Grigory Lihachev , Romain 1 2 1 warfighters, first responders and medical personnel must Labs, Japan. A membrane buried heterostructure with a Bouchand , Nikolay Pavlov , Arslan S. Raja , Maxim 1 2,3 1 maintain their situation awareness in times of high stress lateral p-i-n junction on SiO2/Si substrate enables tight Karpov , Michael Gorodetsky , Tobias Kippenberg ; 1 or risk harm to themselves, team members or those in confinement of carriers and photons simultaneously, Ecole Polytechnique Fédérale de Lausanne, Switzerland; 2 3 their care. While we can’t necessarily make them better which enables us to achieve energy-efficient lasers. Russian Quantum Center, Russia; Moscow State Univ., at their job, perhaps we can give them a head-mounted Russia. We simultaneously create stable solitons in up to 3 distinct mode families of a single crystalline MgF (or helmet-mounted) display that can provide cognitively 2 “pre-digested” information in a hands-free and timely microresonator. The resulting Kerr combs have distinct manner that will reduce their workload? What are the repetition rates, are mutually coherent allowing dual or requirements for maintaining situation awareness and future triple comb applications. reducing workload for these important occupations? How do these requirements translate into performance FW1C.3 • 08:45 specifications for the head-mounted display? In-situ Backpropagation in Photonic Neural Networks, 1 1 1 ber Momchil Minkov , Tyler W. Hughes , Yu J. Shi , Ian Wil- liamson1, Shanhui Fan1; 1Stanford Univ., USA. Using the adjoint variable method, we derive an in-situ backpropa- gation procedure for training of photonic neural networks. Our method may also be of interest for experimental sensitivity analysis and optimization of reconfigurable optics platforms. Wednesday, 19 Septem Wednesday, 09:15–10:00 FW2A • Visionary: Mark Bolas

FW2A.1 • 09:15 VISIONARY Bending Light to Bend Reality, Mark Bolas1; 1Microsoft Corp, USA. As we dive head-first into the new medium of mixed reality, we find that the ability to bend light is central to the palette of mixed reality systems and content designers as they bend the reality that is ultimately formed in the user’s mind. This talk will look backwards and for- ward in time to explore just how messy that process has been, and how much messier it will become.

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08:00–09:00 08:00–09:00 08:00–09:00 FW1D • Quantum Sensing for Industry and FW1E • Nanophotonic Sensing and LW1F • Novel Lasers, Plasmonics, Fundamental Physics I Optomechanics Nanophotonics I Presider: To be Determined Presider: Roel G. F. Baets; Ghent University Presider: Maiken Mikkelsen; University of INTEC, Belgium California Berkeley, USA FW1D.1 • 08:00 Invited FW1E.1 • 08:00 LW1F.1 • 08:00 Invited 1 Enabling Technologies for Cold-Matter Based Quan- Robust non-Hermitian sensors, Qi Zhong , Mohammad High Performance Flat Optics, Federico Capasso1, 1 1 1 tum Systems, Evan A. Salim1; 1ColdQuanta Inc., USA. Hosain Teimourpour , Ramy El-Ganainy ; Michigan Wei-Ting Chen1; 1Harvard Univ., USA. The talk will focus Quantum technologies exploit properties of matter to Technological Univ., USA. We introduce a new design on metasurface optics including broadband achromatic manage information, and to measure phenomena in ways concept for non-Hermitian photonic that combine ro- and tunable metalenses, ultracompact spectrometers and that greatly exceed existing capabilities. We present on bustness with sensitivity and demonstrate its utility for polarimeters that match the performance of state-of-the- key technologies to enable quantum information science, sensing applications. art ones and novel endoscopes for lung cancer detection. sensing, and timekeeping.

FW1E.2 • 08:15 Quantum metrology for high-accuracy measurement of refractive index difference in original optical fibers, Florent Mazeas1,2, Romain Dauliat3,4, Djeylan Aktas5, Mattis Reisner1,2, Panagiotis Vergyris1,2, Philippe Roy3,4, Raphael Jamier3,4, Florian Kaiser6,7, Laurent Labonté1,2, Sébastien Tanzilli1,2; 1Université Côte d’Azur, CNRS, France; 2Institut de Physique de Nice, France; 3Université de Limoges , France; 4XLIM, France; 5Univ. of Bristol, UK; 6Univ. of , Germany; 73rd Inst. of Physics, Germany. We report on a quantum-based measurement of index differ- ence in original fibers. With an interferometric setup and a peculiar optical fiber structure, we demonstrate index difference measurements with a precision reaching the 10-5 - 10-6 level.

FW1D.2 • 08:30 Invited FW1E.3 • 08:30 LW1F.2 • 08:30 Invited Quantum Enhanced Metrology with Trapped Ions, Arrays of High Reflectivity SiN Photonic Crystal Mem- Nonreciprocal Photonics, Andrea Alu1; 1Photonics Inita- 1 Dietrich Leibfried1; 1National Inst. of Standards and branes for Cavity Optomechanics, João Moura , Claus tive, CUNY Advanced Science Research Center, USA. We 1,2 1 1 Technology, USA. Laser cooling and quantum logic allows Gärtner , Wouter Haaxman , Richard A. Norte , Simon discuss opportunities to break reciprocity in photonics 1 1 us to prepare atomic and molecular ions into nearly pure Gröblacher ; Kavli Inst. of Nanoscience, Delft Univ. of using mechanical motion, spatio-temporal modulation, 2 quantum states of their internal degrees of freedom and Technology, Netherlands; Vienna Center for Quantum and/or nonlinearities, and their impact in the context of external motion and subsequently interrogate them with Science and Technology (VCQ), Univ. of Vienna, Austria. integrated photonics, slow-light devices, and photonic high metrological precision. We fabricate photonic crystal SiN membranes with re- topological insulators. flectivity > 99.9% at 1550 nm. These form a platform for studying arrays of mechanical oscillators inside optical cavities, which can potentially reach strong single-photon optomechanical coupling.

FW1E.4 • 08:45 Wednesday, 19 Septem Demonstration of a Phonon Laser With a Nanosphere Levitated in an Optical Tweezer, Robert Pettit1, Wen- chao Ge2, Pardeep Kumar2, Danika Luntz-Martin1, Justin Schultz1, Levi Neukirch3, Mishkat Bhattacharya2, Anthony N. Vamivakas1; 1Univ. of Rochester, USA; 2Rochester Inst. of Technology, USA; 3Los Alamos National Lab, USA. A phonon laser based on the center-of-mass oscillations of a silica nanosphere, levitated in an optical tweezer under vacuum, is proposed and developed. The observed dynamics are shown to result from stimulated emission of phonons. ber

09:15–10:00 LW2B • Visionary: Mark Brongersma Presider: Pieter G. Kik; University of Central Florida, USA

LW2B.1 • 09:15 VISIONARY Activities Shaping the Wavefront of Nanophotonics, Mark Brongersma1; 1Stanford Univ., USA. In the field of nanophotonics we aim to manipulate the flow of light using optically resonant nanostructures. I will share my personal perspective on a number of exciting recent developments in the field that are transforming the way we create new optical materials and devices.

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FiO Abstracts.indd 31 8/20/18 9:11 AM Science & Industry Showcase 10:15-11:15 Rapid Fire Oral Presentation III, Science & Industry TheaterJOINT FiO + LS Presider: Wei Lee; National Chiao Tung University, Taiwan Participating posters are noted in the list of poster for session JW3A with the icon RAPID. Each presenter will have 3 minutes and the order will be determined by poster number.

JOINT FiO + LS

10:00–12:00 JW3A • Poster Session III and Dynamic E Posters

JW3A.1 E-Poster JW3A.8 RAPID JW3A.14 Fabrication of active microdisc resonators using solvent Amplitude Shifting Holography, Surya Gautam1, Pramod Scintillation of Gaussian-, multi-Gaussian-, and non- 1 1 immersion imprint lithography, Priyanka Choubey , Panchal1, Dinesh N. Naik1, C. S. Narayanamurthy1, Rakesh uniformly-correlated beams, Milo W. Hyde , Svetlana 1 1 1 2 2 1 Shailendra Varshney , Shivakiran Bhaktha B. N. ; In- K. Singh1; 1Physics, Indian Institute of Space Science Avramov-Zamurovic , Charles Nelson ; Air Force Inst. 2 dian Inst. of Technology Kharagpur, India. We present & Technology, India. Amplitude Shifting Holography of Technology, USA; USA Naval Academy, USA. We fabrication of active microdisc resonators for sensing method for imaging complex value objects is based on compute the mean intensities and scintillation indices platform based on whispering-gallery modes. The arrays the consideration that one point can be taken from the for Gaussian-, multi-Gaussian-, and nonuniformly-cor- of microdisc are fabricated from DCM laser dye-doped object as a reference and by shifting its amplitude to related sources. Under the simulated conditions, we PVA using solvent immersion imprint lithography (SIIL). record the digital hologram. find no significant scintillation improvement over the Gaussian-correlated source. JW3A.2 E-Poster JW3A.9 RAPID Polarization Rotation Utilizing Berry’s Phase in Asym- Fabrication of Black Silicon using Laser Annealing, JW3A.15 1 1 1 Symmetry Aspects of the Cesium D Double Resonance metric Silicon Waveguides, Ryan Patton , Ronald M. Sara Al Menabawy , Joumana El-Rifai , Mohamed M. 2 1 1 1 1 Reano ; Ohio State Univ., USA. We present a method Swillam1; 1American Univ. in Cairo, Egypt. A novel fab- Spectrum, Thomas Marty ; Thomas Marty (private), to achieve polarization rotation in asymmetric silicon rication technique of Silicon nanowires using excimer Switzerland. Dark resonance spectra were recorded with a + waveguides using Berry’s phase. By exploiting periodic laser is developed in this work. Using one-step and easily σ -polarized beam from a laser diode. Longitudinal mag- in-plane and out-of-plane sections, we achieve 90° po- scalable method, array of nanowires with broadband netic fields reveal seven double resonances. In orthogonal larization rotation in the presence of linear birefringence. absorption enhancement are formed without etching magnetic fields fifteen double resonances appear. This the deposited material. indicates strong angular dependence. JW3A.3 Withdrawn JW3A.10 RAPID JW3A.16 High Efficiency Photon Sieves by Laser Direct Writing, Multi-Plane, Learning Algorithm for Focal Volume 1 1 JW3A.4 E-Poster Matthew Julian1, David MacDonnell2, Mool Gupta1; 1Univ. Beam Shaping, Harry Burton , Ashish Bachavala , Chris- 1 1 1 Single-pixel three-dimensional profiling with a du- of Virginia, USA; 2NASA Langley Research Center, USA. topher Debardelaben , Wafa Amir , Thomas A. Planchon ; 1 1 1 1 al-comb fiber laser, Yihong Li , Xin Zhao , Qian Li , Jie We show that photon sieve focusing efficiencies can Delaware State Univ., USA. A Multi-Plane Genetic Algo- 1 1,2 1 Chen , Zheng Zheng ; School of Electronic and Informa- be increased 7-fold. Such sieves can be fabricated via rithm is developed to optimize the focal volume of a laser 2 tion Engineering, Beihang Univ., China; Beijing Advanced standard laser direct writing techniques. By optimizing instead of its focal plane. Using a Spatial Light Modulator, Innovation Center for Big Date-based Precision Medicine, laser parameters, near diffraction limited performance non-diffracting beams are generated to demonstrate the Beihang Univ., China. Using a single-cavity, dual-comb is demonstrated. validity of the approach. fiber laser, single-pixel 3D profiling is demonstrated with a simple and compact setup. Sub-millimeter resolution JW3A.11 JW3A.17 achievable with the dual-comb ranging scheme can be Mode-locking Fiber Laser Using SMS Fiber Structure as Simple Circular Beam Lattices via Phase Modulated 1 1,2 attractive to many applications. a Saturable Absorber, Yunxiu Ma1,2, Xiushan Zhu1, Luyun Bessel Beams, Mariia Shutova , Aleksandr Goltsov , 3 1,2 1 Yang2, Jing Zhang3, Wei Shi4, Nasser Peyghambarian1; Anatoli Morozov , Alexei Sokolov ; Inst. for Quantum JW3A.5 E-Poster 1College of Optical Sciences, Univ. of Arizona, USA; Science and Engineering, Dept. of Physics and Astrono- 2 3 Quasi-monoenergetic Electron Beams from Mid-IR La- 2Wuhan National Lab for Optoelectronics, Huazhong Univ. my, Texas A&M Univ., USA; Baylor Univ., USA; Princeton ser Wakefield Acceleration in the Bubble Regime, An- of Science and Technology, China; 3School of Science, Univ., USA. We tailor Bessel beams generated by an 1 1 1 astasia Korolov , Daniel C. Woodbury , Robert Schwartz , Changchun Univ. of Science and Technology, China; axicon employing phase modulation. Resultant non-dif- 1 1 Howard Milchberg ; Institute for Research in Electronics 4College of Precision Instrument and Optoelectronics fracting circular lattices create stable intensity channels, ber & Applied Physics, USA. We present simulation results Engineering, Tianjin Univ., China. Mode-locking fiber laser which, if modified according to experimental needs, offer of laser plasma wakefield acceleration in the bubble re- by nonlinear Kerr effect of a single-mode-multimode-sin- an ideal instrument for plasma guiding. gime driven by ultrashort mid-infrared laser pulses (30fs, gle-mode (SMS) fiber structure as saturable absorber was 17 2 λ=3.9µm, 3x10 W/cm ). We observe a quasi-monoener- demonstrated. A 13.01 MHz mode-locking Tm3+-doped JW3A.18 getic accelerated electron bunch at ~20MeV. fiber laser operating at 1941.37 nm was obtained. Linearly Polarized Generalized-Gaussian Laser Beams, Jessica P. Conry1; 1Arkansas Tech Univ., USA. Dominant JW3A.6 E-Poster JW3A.12 and cross-polarization intensity profiles of Generalized Enhanced resolution in remote sensing using UV fila- Diffractive Fresnel Lens Fabrication with Femtosecond Gaussian beams are produced of several orders and 1,2 ments with long pulses, Ladan Arissian , Jean Claude Bessel Beam Writing in Silica, Qi Sun1, Timothy Lee1, angle parameter using a spatial light modulator. The 1 1 1 1 Diels , Ali Rastegari , Brian Kamer ; CHTM, Univ. of New Ziqian Ding2, Martynas Beresna1, Gilberto Brambilla1; experimental and theoretical profiles are in agreement. 2 Mexico, USA; Univ. of Ottawa, Canada. We present high 1Optoelectronics Research Centre, Univ. of Southampton, resolution spectroscopy of solid samples from 200ps UV UK; 2Huawei Technologies Co., Ltd., China. A 3-layer JW3A.19 Wednesday, 19 Septem Wednesday, filaments. The temperature gradient on the expanding Fresnel lens with 52% diffraction efficiency was inscribed Performance Evaluation of Infrared Thermographic 1 plume results into self-absorption of the hot plasma by with a femtosecond Bessel beam in silica, with each layer Fever Screening Systems, Pejhman Ghassemi , Joshua 1 1 1 1 the surrounding colder regions improving the resolution. being ~80 μm. An anomalous dispersion property was Pfefer , Jon Casamento , Quanzeng Wang ; Food and characterized with an RGB LED source. Drug Administration, USA. Methods to test stability and JW3A.7 E-Poster uniformity of infrared thermographs were evaluated and Signatures of Coherent Photon Transport in Nanowire JW3A.13 improvements were suggested. The study has provided Waveguides with Coupled Quantum Dots, Chelsea Material Selection for Generalized Achromatic Lenses significant insights toward the design of least burdensome 1 2 2 L. Carlson , Dan Dalacu , Robin L. Williams , Phillip J. Including Conventional, Gradient Index, and Diffractive standardized test methods. 2 1 1 2 Poole , Stephen Hughes ; Queen’s Univ., Canada; Na- Components, Guy Beadie1, Joseph N. Mait2; 1US Naval tional Research Council of Canada, Canada. We present Research Lab, USA; 2US Army Research Lab, USA. Opti- JW3A.20 theory and experiments of coupled quantum dots (QDs) mum material selection is discussed for unconventional A Full-field Heterodyne Interferometer using for Modal 1 1 1 in semiconductor nanowire waveguides. Depending achromatic lenses, including gradient index and diffractive Identification, Zong H. Chen , Wen Xiao , Feng Pan ; 1 upon the two QD spatial separation, we demonstrate optical elements. The approach is based on defining a Beihang Univ., China. In this paper, a full-field heterodyne pronounced spectral shifts, as well as strongly coupled figure of merit, and finding material combinations that interferometer, is proposed for modal identification. The super/sub-radiant states. maximize its value. experiment results show a great agreement with data obtained from theoretical calculation and LDV.

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JOINT FiO + LS

JW3A • Poster Session III and Dynamic E Posters—Continued

JW3A.21 JW3A.29 JW3A.37 Measurement of Centering Errors of Glass Molds and Remote Detection of Radioactive Material using Diffusion of External Magnetic Field into Laser-pro- Casted Lenses for Production of Ophthalmic Lenses, Optically Induced Air Breakdown Ionization, Joshua duced Plasma Plume, Narayan Behera1, Rajesh K. Singh1, Saharat Kaew-aram1, Boonsong Sutapun1; 1Suranaree J. Isaacs1, Phillip Sprangle1; 1Univ. of Maryland, USA. We Ajai Kumar1; 1 Inst. for Plasma Research, HBNI, India. The Univ. of Technology, Thailand. In this work, we discuss model irradiated air to estimate the density of negative diffusive term of the generalized Ohm’s law is calculated the instrument design challenges and preliminary results ions and use a set of coupled rate equations to simulate to understand how magnetic field diffuses into laser-pro- for the development of an apparatus for measurement the subsequent laser-induced avalanche ionization for duced plasma as it is useful to understand confinement of centering error of the assembled glass molds used for detection of radioactive materials remotely. and acceleration of the plasma plume and its dynamics. manufacturing of plastic ophthalmic lenses. JW3A.30 JW3A.38 JW3A.22 Modeling the Formation of Nanometer-Scale High-Den- Single mode fibers for two stage higher-order soliton Non-uniformly correlated partially coherent lasers, sity Electron Bunches in Relativistic Laser-Solid Inter- compression at 2 μm, Fumin Wang1, Zihao Cheng1, Jixiong Pu1, Chengcheng Chang1, Xudong Chen1, Ziyang action: Effects of Numerical Resolution, Nicholas M. Qian Li1; 1PKU Shenzhen graduate school, China. We Chen1; 1Huaqiao Univ., China. We demonstrate a new Fasano1, Matthew Edwards1, Julia Mikhailova1; 1Princeton demonstrate design of single mode fibers for two-stage kind of laser, called as a partially coherent digital laser, Univ., USA. With numerical simulations we demonstrate higher-order soliton compression at 2 μm. A compression producing non-uniformly correlated partially coherent that laser-driven electrons near solid targets bunch factor of 79.9 has been achieved and the pedestal energy light (NUC-PCL) beams by “playing a video” inside the together and travel along a synchrotron-like trajectories. is only 51.54%. cavity directly. The effect of numerical resolution on the formation of these nanoscale bunches is studied. JW3A.39 JW3A.23 Avoiding Parametric Instability in Advanced LIGO, Terra Low-loss BSO photonic waveguides, Florent Behague1, JW3A.31 RAPID C. Hardwick1,2; 1LIGO, USA; 2Physics, Louisiana State Univ., Nadege Courjal1, Florent Bassignot1, Ludovic Gauthi- Frequency Shifting Whispering Gallery Modes With USA. Parametric instability is a three mode optical-me- er-Manuel1, Alexis Caspar1, Venancio Calero Vila1, Fadi Planar Dielectric Substrates, Patrick A. Devane1, Madhuri chanical interaction that, if not controlled, can cause the Baida1; 1femto-st, France. We report for the first time the Kumari1, Luke Trainor1, Harald G. Schwefel1; 1Univ. of high power LIGO arm cavities to lose resonance. We fabrication of low loss ridge-waveguides in Bismuth-Sili- Otago, New Zealand. We assess a proposed method of discuss theory, observation, mitigation and applications con-oxide by optical grade-dicing. This approach promis- dielectric tuning for whispering gallery mode resonators of parametric gain. es to be powerful for compact and highly sensitive E-field using a set up that allows dielectric substrates to move sensors, scintillators and laser applications. into close proximity with a lithium niobate resonator and JW3A.40 RAPID analyse the resulting frequency shifts. Coherent Anti-Stokes Raman Scattering Enhanced by 1 1 JW3A.24 MoS2 Nanoparticles, Anton D. Shutov , Zhenhuan Yi , Design and Fabrication of Germanium-Zinc Sulfide JW3A.32 RAPID Jizhou Wang1, Alexander M. Sinyukov1, Zhe He1, Chenwei Mid-IR Photonic Devices, Daniel Carney1, Robert Mag- Stationary Beam Synthesis From its Coherent Modes, Tang1,2, Jiahao Chen1,2, Zhedong Zhang1, Esther J. Ocola3, nusson1; 1Univ. of Texas at Arlington, USA. The mid-IR Xi Chen1, Jia Li1, Mohammad Hashemi Rafsanjani1, Olga. Jaan Laane3, Alexei V. Sokolov1,4, Dmitri V. Voronine5, from 3 to 13 μm is an established region for scientific Korotkova1; 1Univ. of Miami, USA. We introduce a tech- Marlan O. Scully1,4; 1Inst. for Quantum Science and Engi- and industrial applications and may benefit from the nique for synthesis of stationary beams via superposition neering, Texas A&M Univ., USA; 2School of Science, Xi’an introduction of photonic devices. Methods for the design of coherent modes. Some stationary beams are generated Jiaotong Univ., China; 3Dept. of Chemistry, Texas A&M and fabrication mid-IR devices are demonstrated. from randomized sequences of ten Laguerre-Gaussian Univ., USA; 4Baylor Research Innovative Center, Baylor modes and analyzed on propagation in vacuum and Univ., USA; 5Univ. of South Florida, Dept. of Physics, USA. JW3A.25 atmosphere. We demonstrate the surface enhancement of coherent The Absorbed Energy of Essential Amino Acids by anti-Stokes Raman scattering (CARS) on pyridine-ethanol 1,2 1 Geometric Phase, Dipti Banerjee ; Vidyasagar College JW3A.33 RAPID solution by MoS2 nanoparticles. The time resolved CARS for Women, India; 2ICTP, Italy. Optical activity of essential Modulated Photoluminescence of Germanium via measurements reveal increased dephasing rates of pyri- amino acids is studied experimentally. Rotation of plane Intense Terahertz Pulse Electric Fields, Mary Alvean dine vibrational modes. polarization results in the change of helicity & energy. B. Narreto1, Chenxi Huang1, David N. Purschke1, Frank Variation of absorbed intensity with the geometric phase Hegmann1; 1Univ. of Alberta, Canada. We show a nonlin- JW3A.41 RAPID has been studied for different concentrations. ear effect of intense terahertz pulse electric fields (>200 Continuous-Wave, Singly-Resonant Optical Parametric Wednesday, 19 Septem kV/cm) on the photoluminescence of bulk germanium. Oscillator Source of Vortex Beams Tunable in the Ultra- JW3A.26 Terahertz-pulse-induced direct-gap photoluminescence violet, Varun Sharma1, Goutam K. Samanta1, R.P. Singh1, 2D Material Liquid Crystal Nanocomposites for Opto- quenching is observed. S. C. Kumar2, M. Ebrahim-Zadeh2,3; 1PRL Ahmedabad, In- electronic and Photonic Devices, Benjamin T. Hogan1; dia; 2ICFO-Institut de Ciencies Fotoniques, Mediterranean 1Univ. of Exeter, UK. We synthesise, characterise and JW3A.34 RAPID Technology Park, 08860 Castelldefels, Barcelona, Spain, move toward application of 2D material liquid crystalline Lorenz-Mie Scattering in Terms of Complex Focus Spain; 3Institucio Catalana de Recerca i Estudis Avancats nanocomposites for optoelectronic and photonic devices, Fields, Rodrigo Gutiérrez-Cuevas1, Nicole J. Moore2, (ICREA), Spain. We report a continuous-wave source focussing on those produced using graphene oxide, Miguel A. Alonso1,3; 1Univ. of Rochester, USA; 2Gonzaga of ultraviolet radiation in vortex spatial intensity profile tungsten disulfide and boron nitride. Univ., USA; 3Aix Marseille Universite, Centrale Marseille, tunable across 332-344 nm based on a green-pumped Institut Fresnel, France. An analytic approach to the Mie optical parametric oscillator. JW3A.27 scattering of highly focused fields is presented. By de- Optical 3D μ-Printing of Polymer Whispering-Gal- scribing the incident field in terms of complex focus fields JW3A.42 ber lery-Mode Microcavity Lasers, Xia Ouyang1, Jijun He1, we can model the scattering and trapping properties of Coherent Mid-infrared Supercontinuum Generation A. Ping Zhang1, Hwa-Yaw Tam1; 1Electrical Engineering, fields with many properties of interest. Using All Solid Hybrid Micro-structured Tellurite Fibers, The Hong Kong Polytechnic Univ., Hong Kong. A new Hoa P. Nguyen1, Hoang Tuan Tong1, Than Singh Saini1, optical printing technology for the fabrication of polymer JW3A.35 Luo Xing1, Takenobu Suzuki1, Yasutake Ohishi1; 1Toyota whispering-gallery-mode microcavity lasers is presented. Withdrawn Technological Inst., Japan. We simulate supercontinuum Polymer mushroom-like optical microresonators capped generation using all solid hybrid micro-structured tellurite with a layer of dye-based gain film were shown for WGM JW3A.36 RAPID fibers. By controlling carefully the chromatic dispersion, laser applications. Angle Dependent THz Absorption in Aligned RGO/ a highly coherent and broad SC spectrum (0.78 μm – 4.8 Fe3O4 Nanocomposite, Nikita Porwal1, Shivam V. Raval1, μm) is obtained using a laser pumping at 2 μm. JW3A.28 Tridib Sinha1, Samit K. Ray1,2, Prasanta Kumar Datta1; 1IIT Spectroscopy Analysis for Real Time Application in Kharagpur, India; 2SN Bose National Centre for Basic Oil and Gas Instrumentation, Eduardo Perez1; 1DICIS, Sciences, India. We report a polarizing nature in aligned Mexico. Spectroscopy applied to technical innovation Fe3O4\RGO Nanocomposite of 10 nm size. The DOP continues with the spectrometer, whose provides excel- of the nanocomposite varies from 0.51-0.04 for 0.4-1.6 lent optical design for sharper images and spectra for dra- THz, suggesting a good polarization effect for future matically improved resolution and signal-to-noise ratio. polarizer applications.

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JW3A.43 JW3A.50 JW3A.57 Near-perfect terahertz wave amplitude modulation Image Transmission across a Nonchiral/chiral Boundary Radiative interaction with arbitrary material bodies, 1 1 enabled by impedance matching in VO2 thin films, Based on Dispersive Fresnel Coefficients, Monish R. Yu-Lin Xu ; Univ. of Texas at El Paso/JETS, USA. This work Jiang Li1; 1Inst. of Fluid Physics, CAEP, China. A terahertz Chatterjee1, Rajab Ataai1; 1Univ. of Dayton, USA. Fresnel introduces an effective way to study radiative responses amplitude modulation method with near perfect E-field coefficients for LCP/RCP modes are computed for s-polar- of bulk materials, in which a material body is regarded amplitude modulation depths of 97.6% that is based on ized wave transmission across an achiral/chiral interface. as an array of microscopic particles. Practical examples

impedance matching in VO2 thin films during the thermally 2D image transmission and recovery is examined using include the comparison between theory and experiment. induced insulator-metal transition. dispersive dielectric parameters, PCM encoding and discrete sideband analysis. JW3A.58 JW3A.44 Withdrawn Crumple Nanostructured Graphene for Mechanically JW3A.51 Reconfigurable Plasmonic Resonances, Pilgyu Kang3, Complex Mirror Symmetry in Optics, Li Ge1; 1College JW3A.59 Kyoung-Ho Kim1, Hong-Gyu Park1, SungWoo Nam2; of Staten Island, CUNY, USA. We first show the existence Towards Sub-shot-noise Imaging using Squeezed Light 1Dept. of Physics, Korea Univ., South Korea; 2Dept. of of a novel non-Hermitian symmetry, i.e., complex mirror from Four-Wave Mixing in Rubidium, Rory W. Speirs1, Mechanical Science and Engineering, Univ. of Illinois at symmetry. We then demonstrate a recursive process that Nicholas Brewer1, Meng-Chang Wu1,2, Paul Lett1,3; 1Joint Urbana-Champaign (UIUC), USA; 3Dept. of Mechanical generates high-order non-Hermitian degeneracies based Quantum Inst., Univ. of Maryland, USA; 2Inst. for Physical Engineering, George Mason Univ., USA. We present an on this new symmetry, which can potentially increase Science and Technology, Univ. of Maryland, USA; 3Nation- innovative approach to achieve mechanically reconfigu- the spontaneous emission rate and sensing sensitivity of al Inst. of Standards and Technology, USA. We present rable, strong plasmonic resonances via crumple nano- optical devices by orders of magnitude. progress towards the generation of sub-shot-noise im- structured graphene. The mechanical reconfiguration of ages using two-mode intensity difference squeezed light crumpled graphene enables broadband tunability from JW3A.52 beams produced by four wave mixing in rubidium vapour. mid- to near-infrared. Broadband THz Spectral Characterization with THz Bandpass Filters, Yungjun Yoo1,2, Dogeun Jang1, Malik JW3A.60 JW3A.45 Kimbrue1, Ki-Yong Kim1; 1Univ. of Maryland at College Quantum Frequency Conversion of Ba+ Photons, John Effects of Spatial Confinement on Plasmon Modulated Park, USA; 2Thorlabs Imaging Systems, USA. Metal-mesh M. Hannegan1,2, James Siverns2,1, Qudsia Quraishi3,2; Photoluminescence, Robert D. Lemasters1, Hayk Ha- bandpass THz filters often exhibit undesired transmission 1Physics, Univ. of Maryland, College Park, USA; 2Joint rutyunyan1; 1Emory Univ., USA. Investigating the effects at their block-band frequencies. By solving an inverse Quantum Inst., USA; 3Army Research Lab, USA. Hybrid of spatial confinement of plasmon gap-modes on PL in matrix problem with regularization, we overcome this quantum networks consisting of disparate memories nanometrically precise plasmonic nanostructures. Results limitation and correctly characterize THz radiation from require identical photons for entanglement distribution. show a linearly increasing nonlinear power law for pulsed 1 to 30 THz. Using frequency conversion of either single photons from laser excitation and linear power law for CW excitation. Ba+ or resonant laser light, we generate 780 nm and 1260 JW3A.53 nm light respectively. JW3A.46 Design of Photonic Quasicrystal Mirrors Using Adjoint Laser Cooling of Crystalline Yb: YAG and Yb: KYW, Shape Optimization, Behrooz Semnani1,2; 1Univ. of Wa- JW3A.61 Long Cheng1, Laura Andre1, Stephen C. Rand1,2; 1EECS, terloo, Canada; 2Inst. for quantum computing, Canada. Photon-Phonon Pair Correlations in Sapphire, Kai B. Univ. of Michigan, USA; 2Physics, Univ. of Michigan, USA. This work presents application of the adjoint optimization Shinbrough1, Bin Fang1, Yanting Teng1, Offir Cohen1, Laser cooling of a 3%Yb:YAG crystal by 4K is achieved for inverse construction of qua-sicrystal slab-mirrors. The Virginia O. Lorenz1; 1Univ. of Illinois Urbana-Champaign, under ambient temperature and pressure conditions in topology of the structure is obtained based on band USA. We measure the quantum-state purity of Stokes an open lab environment and laser cooling of 1%Yb:KYW analysis and is adjusted for high performance operation. photons from sapphire, achieving a purity of 1.00±0.03 is reported for the first time. and quantitative agreement with a new theoretical model JW3A.54 of photon-phonon correlations that includes dispersion JW3A.47 Frustrated Tunnel Ionization with Few-cycle Pulses, and finite excitation lifetime. 2 2 2,1 Ultrafast Carrier Dynamics in Self-Assembled La1-xS- Rohan Glover , Dashavir Chetty , Bruno A. deHarak , 1 2 3 4 rxMnO3/SrTiO3 Heterostructures, Joel E. Taylor , Rami Adam J. Palmer , Milad A. Dakka , John L. Holdsworth , JW3A.62 A. Khoury2, Kun Zhao1, Mohammad Saghayezhian1, Louis Igor Litvinyuk2, Andre N. Luiten3, Philip S. Light3, Robert Withdrawn Haber2, Ward Plummer1; 1Dept. of Physics & Astronomy, T. Sang2; 1Physics Dept., Illinois Wesleyan Univ., USA; Louisiana State Univ., USA; 2Dept. of Chemistry, Louisiana 2Centre for Quantum Dynamics, Griffith Univ., Australia; JW3A.63 RAPID ber State Univ., USA. Optically excited carrier dynamics are 3Inst. for Photonics and Advanced Sensing and School Engineering a Noiseless and Broadband Raman Quan-

observed for self-assembled La1-xSrxMnO3/SrTiO3 hetero- of Physical Sciences, The Univ. of Adelaide, Australia; tum Memory for Temporal Mode Manipulation, Thomas structures using pump-probe reflectivity. 4School of Mathematical and Physical Sciences, Univ. M. Hird1,2, Sarah Thomas1,4, Joseph Munns1,4, Oscar Lazo of Newcastle , Australia. We experimentally investigate Arjona1, Shaobo Gao1, Joshua Nunn3, Benjamin Brecht1, JW3A.48 frustrated tunnel ionization with few-cycle pulses. Our Dylan Saunders1, Patrick Ledingham1, Ian A. Walmsley1; Efficient Polarization Modulation by a Phase Change results indicate that frustrated tunnel ionization is more 1Univ. of Oxford, UK; 2Dept. of Physics and Astronomy, Material on Metal, Alain Hache1, Tran Vinh Son1, Truong prevalent with few-cycle pulses and shows qualitative Univ. College London, UK; 3Dept. of Physics, Univ. of Vo-Van2, Phuong Ahn Do1; 1Universite de Moncton, Can- agreement with modelling. Bath, UK; 4Blackett Lab, Imperial College London, UK. ada; 2Physics, Concordia Univ., Canada. The polarization The Raman quantum memory can manipulate temporal state of light interacting with a layer of vanadium dioxide JW3A.55 modes of light - a promising high-dimensional basis for on metals undergoing phase transition is observed to Non-Destructive Heterodyne Measurement of Number quantum information processing. We demonstrate both change due to large variations in the material’s refrac- of Atoms in Cesium-Potassium Mixture, Jakub Dobo- temporal mode manipulation and a novel suppression Wednesday, 19 Septem Wednesday, tive index. sz1; 1Univ. of Warsaw, Poland. We present a setup of a scheme for four-wave mixing noise. heterodyne interferometer for measuring phase shift of JW3A.49 light passing through atomic cloud mixture of cesium and JW3A.64 RAPID

Second Harmonic Generation in CH3NH3PbI3 Thin Films, potassium, to derive the number of atoms in the cloud Twin-beam Intensity-difference Squeezing below 10 Hz Anna A. Popkova1, Vladimir O. Bessonov1, Irina V. Sobole- with atom losses. from Dual-seeded Four-wave Mixing, Meng-Chang Wu1, va1, Mehedhi Hasan2, Dmitry Lyashenko2, Alex Zakhidov2,3, Bonnie Schmittberger1, Nicholas Brewer1, Rory W. Speirs1, Andrey A. Fedyanin1; 1Lomonosov Moscow State Univ., JW3A.56 Paul Lett1; 1Univ. of Maryland, College Park, USA. We have Russia; 2MSEC, Texas State Univ., USA; 3Dept. of Physics, Influence of an acoustic wave on particle trapped obtained bright-beam intensity-difference squeezing Texas State Univ., USA. Second-harmonic generation in in optical tweezers in the air, Gabriela Mach1, Lukasz below 10 Hz via four-wave mixing in a rubidium vapor. 2 1 1 CH3NH3PbI3 perovskite multidomain film is experimentally Golacki , Jan Masajada ; Optics and Photonics, Wroclaw This was accomplished by increasing phase matching studied. The MAPI nonlinear second-order susceptibility Univ. of Science and Technology, Poland; 2Experimental angle and using two seed beams to balance the power. is estimated. Polarization of MAPI SHG signal is observed Physics, Wroclaw Univ. of Science and Technology, Po- and hyper-Rayleigh scattering angle is estimated. land. The phenomena of optical tweezers which causes the trapping is called photophoresis, which occurs to uniform distribution of temperature over the particle surface irradiated by a laser beam.

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JW3A.65 RAPID JW3A.71 JW3A.76 Active Light Emission Control via Tunable Hybrid Ep- Bowtie Plasmonic Nanoantennas with Nanocrystals: Slow Light Generation in Decagonal Liquid Core Pho- 1 1 silon-Near-Zero and Surface-Plasmon-Polariton Mode, Photon Antibunching, Polarization Selectivity and Tun- tonic Crystal Fiber, Rahul Kumar , Pooja Chauhan , Ajeet 1 1 1 1 Aleksei Anopchenko1, Long Tao1, Norbert Danz2, Girish ability, Svetlana G. Lukishova , Jeremy Staffa , Huiqing Kumar ; Delhi Technological Univ., India. Liquid Core PCF 1 1 3 1,2 1 Agarwal3,4, Howard Lee1,3; 1Baylor Univ., USA; 2Fraunhofer Zhu , Kevin Kuyk , Andreas Liapis , Robert Boyd ; Univ. has been designed using carbon-disulphide as core and 2 3 Inst. for Applied Optics and Precision Engineering IOF, of Rochester, USA; Univ. of Ottawa, Canada; Harvard silica as cladding. Confinement loss has been plotted Germany; 3Inst. for Quantum Science and Engineering, Medical School, USA. Photon antibunching was observed and a time delay of 166.70ns is calculated for maximum Texas A&M Univ., USA; 4Biological and Agricultural from NV-nanodiamonds and nanocrystal quantum dots power of 102 mW at 1.55µm. Engineering, Texas A&M Univ., USA. Field-effect tuning within bowtie plasmonic nanoantennas. We also showed of strongly coupled epsilon-near-zero and surface-plas- polarization selectivity of these nanoantennas. Numerical JW3A.77 mon-polariton modes in ITO/oxide/Au heterostructure modeling was carried out for air and liquid crystals. 100-Gb/s Doubly Differential QPSK System with Im- is shown. The tuning enables active control of emissive proved Receiver Sensitivity Using Polarization Switch- 1 1 1 properties of quantum emitters coupled to the hybrid JW3A.72 ing, Tingting Zhang , Christian Sanchez , Andrew Ellis ; 1 polariton mode. Quantum State Engineering Using One-dimensional Aston Univ., UK. 0.7-dB receiver sensitivity improvement Discrete-time Quantum Walks, Luca Innocenti1, Helena at 7% HD-FEC threshold is numerically demonstrated us- 1 2 2 JW3A.66 RAPID Majury , Taira Giordani , Nicolò Spagnolo , Fabio Sciarri- ing polarization switching in 100-Gb/s doubly differential 2,3 1,4 1 1 Mutually unbiased bases for time-bin qudits, Joseph no , Mauro Paternostro , Alessandro Ferraro ; Centre QPSK 80-km SSMF transmission system with simplified M. Lukens1, Nurul T. Islam2, Charles C. Lim3, Daniel J. for Theoretical Atomic, Molecular, and Optical, School receiver-side DSP. Gauthier2; 1Oak Ridge National Lab, USA; 2The Ohio of Mathematics and Physics, Queen’s Univ. Belfast, UK; 2 State Univ., USA; 3National Univ. of Singapore, Singapore. Dipartimento di Fisica, Sapienza Università di Roma, JW3A.78 3 We introduce a method for generation and detection of Italy; Consiglio Nazionale delle Ricerche, Istituto dei Spectra of Raman scattering in Few Mode Fibers, Zhen- 4 1 1 1 1 mutually unbiased bases for time-bin qudits employing sistemi Complessi (CNR-ISC), Italy; Laboratoire Kastler zhen Zhang , Cheng Guo , Liang Cui , Ming Xu , YIchi 2 1 1 2 electro-optic phase modulator -- coded fiber Bragg Brossel, ENS-PSL Research Univ., France. The capability Zhang , Xiaoying Li ; Tianjin Univ., China; Fiberhome grating pairs. Our approach uses one spatial mode and of generating arbitrary quantum states is a fundamental Telecommunication Technologies Co Ltd, China. We can switch rapidly between bases. task in many quantum information areas. Here we propose measure Raman scattering (RS) in polarization maintained a scheme for quantum state engineering that exploits few mode fiber (FMF) and common FMF, respectively, JW3A.67 discrete-time quantum walk in the angular momentum and show vector mode coupling of the degenerate Towards Room-Temperature Single-Photon LEDs by of single-photons. modes affect the dependence of RS on polarization and FRET from Metal Nanoparticles to Exfoliated 2D spatial mode. Crystal Overlayers, Robin Puchert1, Florian Steiner1, JW3A.73 Gerd Plechinger1, Felix Hofmann1, Philipp Nagler1, Fluctuations Statistics in an Erbium Random Fiber JW3A.79 1 1 Alexey Chernikov1, Christian Schüller1, Tobias Korn1, Jan Laser, Bismarck C. Lima , Pablo I. Pincheira , André L. Entanglement Concentration Service for the Quantum 2 1 1 2,1 1 1 Vogelsang1, Sebastian Bange1, John Lupton1; 1Institut Moura , Anderson S. Gomes , Leonardo d. Menezes , Internet, Laszlo Gyongyosi , Sandor Imre ; Budapest 3 1 4 2 für Experimentelle und Angewandte Physik, Universität Ernesto P. Raposo , Cid B. Araújo , Raman Kashyap ; Univ of Techolology & Economic, Hungary; Univ. of 1 Regensburg, Germany. Localized surface-plasmon res- Departamento de Física, Universidade Federal de Per- Southampton, UK. A fundamental concept of the quan- 2 onances enable efficient coupling to proximal resonant nambuco, Brazil; Grupo de Física da Matéria Conden- tum Internet is quantum entanglement. The aim of our dipole transitions. By exploiting energy transfer from sada, NCEx, Campus Arapiraca, Universidade Federal de entanglement concentration service is to provide reliable, 3 metal nanoparticles to monolayers of 2D crystals we point Alagoas, Brazil; Laboratório de Física Teórica e Computa- high-quality entanglement for a dedicated set of quantum a way to generate single photons at room temperature. cional, Departamento de Física, Universidade Federal de nodes in the quantum Internet. Pernambuco, Brazil; 4Fabulas Lab, Dept. of Engineering JW3A.68 Physics, Dept. of Electrical Engineering, Polytechnique JW3A.80 Two-mode intensity squeezing using OAM-carrying Montreal, Canada. The mixed statistical regime of a Unequally Spaced Channel Allocation Algorithm in Hy- pump and probe beams, Nikunj Prajapati1, Nathan Random Fiber Laser is experimentally and theoretically brid DWDM System for Reduction of FWM, Yugnanda 1 1 1 1 Super1, Irina Novikova1; 1Physics, College of William & studied with the framework of the generalized extreme Malhotra , Ashutosh Singhal , Nisha Nisha ; Electronics value and alpha stable distribution statistics. and Communication Engineering, Bharati Vidyapeeth

Mary, USA. We investigate the transfer of optical angular Wednesday, 19 Septem momentum (OAM) and two-mode intensity squeezing in College of Engineering, India. We propose an Unequally the four-wave-mixing process. We could control the OAM JW3A.74 Spaced Channel Allocation Algorithm in a 0.2nm, mixed of the generated stokes field in a wide range maintaining High Dimensional Quantum Key Distribution Based on bit rates, DWDM system, for FWM reduction. Overall per- similar squeezing levels. Coherence Modulation and Orbital Angular Momen- formance in terms of covered optical bandwidth, reduced tum, Paula A. López Higuera2,3, Yezid Torres Moreno2, FWM products and received output power is reported. 1 1 JW3A.69 William T. Rhodes ; Dept. of Computer & Electrical What are the physical processes behind the evolution Engineering and Computer Science, Florida Atlantic Univ., JW3A.81 2 of spatial coherence out of incoherent light and particle USA; Grupo de Óptica y Tratamiento de Señales GOTS, Femtosecond Pulse Propagation through Large Mode beams? Chandra Roychoudhuri1; 1Univ. of Connecticut, Escuela de Física, Universidad Industrial de Santander, Area Tapered Fiber at 1.06 μm Wavelength, Mohd Re- 3 1 1 1 1 USA. This paper raises the fundamental questions to Colombia; Escuela de Ingenierías Eléctrica, Electrónica han , Gyanendra Kumar , Vipul Rastogi , Rajesh Kumar ; 1 explore the possible physical models behind the evolu- y de Telecomunicaciones, Universidad Industrial de IIT ROORKEE, India. We demonstrate femtosecond pulse tion of spatial coherence during the propagation of an Santander, Colombia. A QKD scheme based on coher- propagation through large mode area tapered fiber at ber incoherent EM wave beam or a particle beam. ence modulation of OAM beams, with an orthonormal 1.06 μm wavelength. We obtain compression, soliton like basis of delays τn and charge l is proposed. The mutually propagation and dispersion of ultra-short pulses which JW3A.70 unbiased set uses linear combination of wave trains of can be utilized in medical applications. Room-Temperature Photon-Number-Resolved Detec- OAM beams. tion Using A Two-Mode Squeezer, Elisha Siddiqui1, JW3A.82 Deepti Deepti Vaidyanathan2, Kenji W. Arai4, Ryan T. JW3A.75 Flatness Optimization of Optical Frequency Combs Glasser3, Hwang Lee1, Jonathan P. Dowling1; 1Physics Radiation-reaction electromagnetic fields in metasur- Using an Adapted Differential Evolution Algorithm, 1 1 1 1 and Astronomy, Louisiana State Univ., USA; 2Baton faces, Michele Merano ; Universita degli Studi di Pado- Guilherme F. Pendiuk , Paulo D. Neves , Alexandre D. 1 1 Rouge Magnet High School, USA; 3Dept. of Physics va, Italy. I derive the optical response of a metasurface Pohl ; CPGEI, Universidade Tecnológica Federal do and Engineering Physics, Tulane Univ., New Orleans, starting from the microscopic description. Surprisingly Paraná, Brazil. A Differential Evolution based algorithm LA 70118, USA; 4Reed College, USA. Intensity-intensity the advanced potential solutions of the inhomogeneous is used to identify input driving parameters of a Dual-Par- correlations signal (〈C〉) at the output of a two-mode Maxwell’s equations are necessary to compute the mac- allel Mach-Zehnder Modulator to generate flat Optical squeezing device with N-photon state and coherent light roscopic fields. Frequency Combs. Combs with 7 lines showing flatness as inputs is studied. Photon-number is resolved from the of 0.03 dB can be obtained. jumps in〈C〉vs. N.

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JW3A • Poster Session III and Dynamic E Posters—Continued

JW3A.83 RAPID JW3A.89 JW3A.96 Single Photon Optical Memory With Cavityless VO / ITO Hybrid Plasmonic High Performance Elec- Properties of the Effective Noise for the Nonlinear 2 1 1 1 Fourier Transform-Based Transmission, Maryna Pankra- Levitated Optomechanics, Pardeep Kumar , Mishkat tro-Optical Modulator, Aya Amer , Mohamed Badr , 1 1 1 1 tova1, Anastasiia Vasylchenkova1, Jaroslaw E. Prilepsky1, Bhattacharya ; Rochester Inst. of Technology, USA. We Mohamed M. Swillam ; American Univ. in Cairo, Egypt. Stanislav Derevyanko2; 1Aston Univ., UK; 2Dept. of Elec- investigate a protocol to upload, store and retrieve a A hybrid plasmonic slot waveguide electro-optical mod- single photon quantum state from a mechanical mode in ulator using VO and ITO is proposed. An extinction ratio trical and Computer Engineering, Ben-Gurion Univ. of the 2 Negev, Israel. We investigate the correlation properties cavityless levitated optomechanics. A high fidelity in our (ER) of 6.36 dB and an insertion loss (IL) of 1.13 dB are of optical noise in nonlinear Fourier domain for commu- results indicates efficient photon-phonon-photon transfer. achieved at 1.55 μm wavelength. nication systems using the nonlinear Fourier transform. Effective covariance functions are obtained numerically JW3A.90 JW3A.97 and compared with theoretical predictions. The Super absorbing Ag-Au Metasurfaces for Sur- Graphene-based Slot Waveguide Photodetectors for face-Enhanced Raman Spectroscopy Sensing of Optical Communications, Kazuya Kikunaga1,2, Zhizhen 1 1 1 1 1 1 JW3A.84 Drugs and Chemicals, Lyu Zhou , Nan Zhang , Dengxin Ma , Rishi Maiti , Volker J. Sorger ; George Washington 1 1 1 1 1 2 Analysis of the evolution of the polarization states Ji , Haomin Song , Youhai Liu , Qiaoqiang Gan ; State Univ., USA; National Inst. of Advanced Industrial Sci- of a pumping source on an Erbium doped fiber, Karla Univ. of New York at Buffalo, USA. We proposed a super ence and Technology, Japan. Here we report on a novel E. Contreras-Vallejo1, Julian Moises Estudillo Ayala1, absorbing metasurfaces with hybrid Ag-Au nanostruc- graphene-based plasmonic slot waveguide photodetec- Roberto Rojas-Laguna1, Daniel Jauregui-Vazquez1, tures, which enables efficient light trapping and result in tor. The ultra-narrow 15 nm slot waveguide enables short Juan C. Hernandez-Garcia1, Juan M. Sierra-Hernandez1, enhanced SERS sensing performance. carrier transitions times resulting in a gain-bandwidth 15 Jose D. Filoteo-Razo1, Manuel Toledano-Ayala2, Ramon product 5.3x10 at l = 1.5 µm. Martinez-Angulo1; 1Universidad de Guanajuato, Mexico; JW3A.91 2División de Investigación y Posgrado, Facultad de Inge- Fluorescence Enhancement and Quenching in Tip-En- JW3A.98 hanced Fluorescence Spectroscopy, Justin Isaac1, Investigation of Si N Microring Resonator for niería, Universidad Autónoma de Querétaro, Mexico. An 3 4 1 1 1 analysis of the effects of the evolution of the polarization Huizhong Xu ; San Francisco State Univ., USA. Fluo- Bio-Chemical Sensing Applications, Subrata Das , Sarath 1 1 3 states on an Erbium doped fiber is presented; this it to rescence enhancement and quenching is studied for a C. Samudrala , Kyu Lee , Brett R. Wenner , Jeffery W. 2 2 1 optimize the development tunable fiber laser systems. fluorophore near a metal tip above a glass substrate. Allen , Monica S. Allen , Robert Magnusson , Michael Resonant behavior is observed as a function of tip-sub- Vasilyev1; 1Univ. of Texas at Arlington, USA; 2Air Force 3 JW3A.85 strate distance and displays a strong dependence on Research Lab Munitions Directorate, USA; Air Force Experimental Implementation of High-speed Balanced tip dimensions. Research Lab Sensors Directorate, USA. We design 1 1 and fabricate Si N microring resonator for measuring Homodyne Detector, Xiaoxiong Zhang , Yichen Zhang , 3 4 Bingjie Xu2, Song Yu1, Hong Guo3; 1Beijing Univ. of Posts JW3A.92 refractive index change in aqueous environment. The and Telecommunications, China; 2Inst. of Southwestern Linear Localization of Non-Hermitian Photonic Zero experimentally observed sensitivity >72 nm/RIU indicates 1,2 1,2 1 Communication, China; 3Peking Univ., China. We pres- Modes, Bingkun Qi , Li Ge ; College of Staten Island, its suitability for biochemical sensing applications. 2 ent a high-speed balanced homodyne detector whose CUNY, USA; Graduate Center, CUNY, USA. A non-Hermi- bandwidth is above 900 MHz and quantum to classical tian photonic zero mode can exhibit an unusual behavior JW3A.99 noise ratio reaches 12 dB respectively, which could be at the transition between extended and localized regimes: Equilibrium Temperature of Wideband Perfect Light applied to the high-speed continuous variable quantum it displays a linearly decreasing amplitude spatially in a Absorbers Under Direct Solar Illumination, Jinnan 1 1 1 information. weakly coupled non-Hermitian reservoir. Chen , Junpeng Guo ; Univ. of Alabama in Huntsville, USA. A new method is introduced to calculate equilibrium JW3A.86 JW3A.93 temperature by using dipole antenna model. It is found Simplified PAM4 optical signals combined with spatial- High-speed pulse control and optimization of quantum that the single dielectric layer absorbing structure gives 1 ly multiplexed communication systems, Syed H. Mur- cascade laser using all-optical modulation, Chen Peng , the highest equilibrium temperature of 979 K. 2 1 2 1 1 shid1, Han Wang1, Gregory Lovell1, Abhijit Charavarty1, Ce Haijun Zhou , Tao Chen , Biao Wei , Zeren Li ; Inst. of 2 Su1, Bilas Chowdhury1; 1Florida Inst. of Technology, USA. Fluid Physics, China Academ, China; Chongqing Univ., JW3A.100 Experimental eye diagram of a four-level simplified pulse China. Pulse control and optimization are demonstrated Optical Coupling in Dielectric Resonator Nanoan- 2 amplitude modulation scheme is presented along with in a middle-infrared quantum cascade laser via an all op- tenna, Gilliard N. Malheiros-Silveira , Hugo E. Hernan- 1 1 2 simulated results. The output is then used with two chan- tical approach. It has the potential for application in free dez-Figueroa ; Univ. of Campinas, Brazil; São Paulo space optical communication and high speed frequency State Univ. (Unesp), Brazil. A theoretical study regarding

ber nel SDM system to generate PAM16 efficiency per fiber. modulation spectroscopy. to coupling efficiency between a dielectric resonator JW3A.87 nanoantenna (DRNA) integrated to a metal-dielec- The All Optical Magnetic Recording Head with Near-In- JW3A.94 tric-metal-dielectric nanostrip waveguide (NW), and free frared Enhancement, Zhihao Zeng1, Haiwei Wang1, Octave-spanning Supercontinuum Generation in Na- space is evaluated. 1 Sicong Wang2, Hongyun Li1, Yuhao Zou1, Lanlan Huang1, noscale Lithium Niobate Waveguides, Juanjuan Lu , 1 1 1 1 Yao Xiao1, Changsheng Xie1; 1Huazhong Univ of Science Yuntao Xu , Joshua Surya , Hong Tang ; Yale Univ., USA. JW3A.101 and Technology, China; 2Jinan Univ., China. We present We demonstrate an octave-spanning supercontinuum Plasmonic Blazing of a Wire-Grid Polarizer: How It a fabricated nanograting structured magnetic write head (SC) generation in nanoscale lithium niobate (LN) wave- Improves the Polarimetric Performance, Changhun 1 2 1 1 featuring near-infrared optical enhancement and low guides with anomalous dispersion by a turn-key pulsed Lee , Eunji Sim , Donghyun Kim ; Electrical and Electronic 2 angle sensitivity, suitable for ultrafast magnetic switching, laser at 1560nm, which enables a simple and integrable Engineering, Yonsei Univ., South Korea; Chemistry, Yon- ultrahigh-density magnetic recording. SC source in LN nanophotonic platform. sei Univ., South Korea. We investigate the polarimetric performance of surface plasmon-enhanced blazed wire- Wednesday, 19 Septem Wednesday, JW3A.88 JW3A.95 grid polarizer (WGP) compared with conventional WGP. 1 Acoustical Response Characteristics of an Optome- Dynamic Plasmonic Pixels, Nicholas J. Greybush , Kristin Highest extinction ratio was found to be 15,740 at 800 nm 2 2 3 chanical Accelerometer, Ramgopal Madugani1, Feng M. Charipar , Nicholas Charipar , Jeffrey A. Geldmeier , period which allows easier fabrication of WGPs. 2 2 1 Zhou1, Randall P. Wagner1, Yiliang Bao1, Jason J. Gor- Jawad Naciri , Jake Fontana ; National Research Coun- man1, Thomas W. LeBrun1; 1National Inst. of Standards cil (NRC) Postdoctoral Research Associate, U.S. Naval JW3A.102 2 and Technology, USA. A Fabry-Perot microcavity-based Research Lab, USA; U.S. Naval Research Lab, USA; Topology of High-k States in Quartic Metamaterials, 3 1 1 1 1 accelerometer was tested in an anechoic chamber to American Society for Engineering Education (ASEE) Maxim Durach , Thomas Mulkey , Jimmy Dillies ; Georgia measure the limiting noise for the device operating in air Postdoctoral Fellow, U.S. Naval Research Lab, USA. We Southern Univ., USA. We study the short-wavelength at room temperature. The acoustic response illustrates the demonstrate spectral, spatial, and temporal control of waves in quartic metamaterials. The quartic k-surfaces design requirement for an optical microphone. plasmonically generated color through alignment of feature from 0 to 4 cones, longitudinal polarization and Au nanorods by an applied electric field. Tailoring the perpendicular to k-vectors group velocities, which leads nanorod aspect ratio enables operation across the visible to negative refraction in quartic metamaterials. and near-infrared spectrum.

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FiO Abstracts.indd 36 8/20/18 9:11 AM Science & Industry Showcase

JOINT FiO + LS

JW3A • Poster Session III and Dynamic E Posters—Continued

JW3A.103 JW3A.110 RAPID JW3A.117 Damage Detection in Bridge-Weigh-In-Motion Struc- Calibration and imaging in acoustophoresis platforms Characterization and In Vivo Application of Mobile tures using Fiber Bragg Grating Sensors, Sravanthi by Digital Holography, Teresa Cacace1,2, Pasquale Phones for Near-Infrared Fluorescence Imaging of 1 1 2 1 1 1 Alamandala , Saiprasad R L N , Rathish Kumar P , Ravi Memmolo1, Vittorio Bianco1, Melania Paturzo1, Massimo Tumors, Nitin Suresh , Qinggong Tang , Yi Liu , Joshua 1 1 2 1 1 Kumar M ; Dept. of Physics, National Inst. of Technology Vassalli3, Pietro Ferraro1; 1CNR-ISASI, Italy; 2Univ. of Pfefer , Yu Chen ; Fischell Dept. of Bioengineering, Univ. 2 2 Warangal, India; Dept. of Civil Engineering, National Inst. Campania “L.Vanvitelli”, Italy; 3Istituto di Biofisica-CNR, of Maryland - College Park, USA; Center for Devices and of Technology, India. Fiber Bragg Grating (FBG) based Italy. We demonstrate that ultrasound field calibration and Radiological Health, U.S. Food and Drug Administration, Weigh-In-Motion system is proposed for the study of the imaging are achievable in a vertical resonator using digital USA. To elucidate the performance of near-infrared fluo- health condition of structures. Artificial damage is created holography, showing that it is a flexible tool to assist the rescence imagers for cancer detection and localization, in the system, and the results were compared with those diffusion of acoustophoresis microfluidic devices. we performed imaging of phantoms and a rodent tumor of undamaged. model. Results provide insights into differences between JW3A.111 mobile phone and CCD-based systems. JW3A.104 Imaging of cochlear cells through scattering bone, A 3D Nanostructure based SPR Sensor for Enhance- Marilisa Romito1, Konstantina M. Stankovic2, Demetri JW3A.118 1 1 ment of Sensing Ability, Heesang Ahn , Hyerin Song , Psaltis1; 1Optics, Ecole Polytechnique Federale de Lau- Biomimetic Microvascular Tissue Phantoms Fabricat- 1 1 1 1 1 Kyujung kim , Taeyeon Kim , Yeji Lee ; Pusan National sanne, Switzerland; 2Otolaryngology, Harvard Medical ed with Two-Photon 3D Printing, Hannah Horng , Yi 1 1 2 2 Univ., South Korea. We investigated localized surface plas- School, USA. Intracochlear imaging will be important for Liu , Nitin Suresh , Pejhman Ghassemi , Joshua Pfefer , 1 1 mon resonance sensors based on 3D nanostructures array the assessment of hearing disorders. Currently, cochlear Yu Chen ; Fischell Dept. of Bioengineering, Univ. of 2 patterns. The enhancement of the near-field distribution small size and encasement in bone prevent visualization Maryland at College Park, USA; Center for Devices and on the 3D nanostructure is confirmed with calculation and of intracochlear microanatomy. We report a technique for Radiological Health, Food and Drug Administration, experimental results. imaging cochlear cells through bone. USA. Phantoms that simulate tissue microvasculature may provide tools to facilitate development and assessment of JW3A.105 JW3A.112 biophotonic devices. We evaluate the use of two-photon The Method and Mechanism of Tuning LSPR on The Imaging-Aided Temperature Measurements with a Sin- polymerization-based 3D printing to fabricate phantoms 1 Biased Metallic Nanosphere, Lihui Gong , Xianyang gle Optical Fiber for In-vivo Sensing Applications, Erik with biomimetic micro-channels. 1 1 Lyu ; Research Lab, School of Transportation, Nantong P. Schartner1, Jiawen Li1, Stefan Musolino1, Bryden Quirk1, Univ., China. We propose a method for creating tunable Rodney Kirk1, Robert McLaughlin1, Heike Ebendorff-Hei- JW3A.119 localized surface plasmon resonance (LSPR) by applying depriem1; 1Univ. of Adelaide, Australia. We present a Flexible and Highly EffectiveTrapping Particles of Op- 1 a variable bias to metallic nanospheres. This method combined imaging and physical sensing probe based tical Tweezers in Nonlinear Optical Imaging, Qin Wu , 1 1 1 base on a different extinction equation and has been on optical coherence tomography and up-conversion Hang S. Chang , Feng X. Huang ; School of Science, supported by experiments. fluorescence respectively, integrated into a single optical Hangzhou Dianzi Univ., China. We demonstrate flexible fiber enabling precise locating of the probe for in-vivo and highly-effective single beam trapping particles by JW3A.106 sensing applications. optical tweezers in nonlinear optical imaging system, Hybrid Vanadium Dioxide Plasmonic Electro-Optical achieve a diverse manipulation of the particles, increase Modulator based on Race-Track shaped Resonator, JW3A.113 the imaging depth and contrast of the particles. 1,2 1 Mohamed Abdelatty , Mahmoud M. Elgarf , Mohamed Combination digital breast tomosynthesis and diffuse 1 1 M. Swillam ; Physics, American Univ. in Cairo, Egypt; optical tomography, Duchang Heo1, Kee-Hyun Kim1, JW3A.120 2 Engineering / Basic sciences, The British Univ. in Egypt, Young-Min Bae1, Young-Wook Choi1, Sohail Sabir2, Withdrawn Egypt. An optical modulator based race-track shaped res- Seungryong Cho2, Hak Hee Kim3; 1Korea Electrotech- onator utilizing the phase change properties of Vanadium nology Research Inst., South Korea; 2Korea Advanced JW3A.121 dioxide. An extinction ratio of 8.45 dB and an insertion Inst. of Science and Technology, South Korea; 3Asan Improved Inverse Two- Layered Monte Carlo Fitting loss of 1.85 dB is achieved at the telecommunications Medical Centerv, South Korea. We report a frequency of In-vivo Skin Diffuse Reflectance Spectra, Chiao-Yi 1 1 1 1 wavelength (1.55 μm). domain DOT system with high-speed data acquisition Wang , Ting-Xuan Lin , Kung-Bin Sung ; National Taiwan to improve the diagnostic accuracy of DBT. We test Univ., Taiwan. The objective of this study is to improve the JW3A.107 inverse Monte Carlo fitting method to make the extraction

the basic performance of the DOT system with optical Wednesday, 19 Septem Radius Optimization of SOI based Rectangular Wave- phantom and can obtain DBT/DOT images using blood of optical coefficients more reliable and precise. Some 1 guide Ring Resonator Filter, Ritu Raj Singh , Soumya vessel mimic phantom. non-invasive in-vivo human skin measurements were done Kumari1, Abhinav Gautam1, Vishnu Priye1; 1Indian Institute to validate the proposed approach. of Technology, Dhanbad, India. The SOI ring resonator JW3A.114 as a notch filter is analyzed by varying ring radius and Withdrawn JW3A.122 performance parameters such as FSR, FWHM, finesse Time-resolved diffusion technique to probe pro- 1 1 and Q-factor has been optimized for 220nm silicon height JW3A.115 tein-drug interaction, Masahide Terazima ; Kyoto technology at C-band wavelengths. Large-scale Volumetric Imaging of Insects with Natural Univ., Japan. A time-resolved diffusion method was Color, Ming Lei1; 1Xi’an Inst. of Optics and Precision applied to detections of the protein-protein interaction, JW3A.108 Mech, China. We present a structured illumination-based protein-DNA interaction, and protein-small molecule. A Scalable SERS by Activating “Passive” Hotspots in Mul- approach to get large-scale 3D images with full natural number of examples show that this method is powerful 1 tigap Nanoplasmonic Systems, Junyeob Song , Wonil color, and high spatiotemporal resolution. With this ap- to explore the protein-drug interaction. 1 1 1 ber Nam , Wei Zhou ; Electrical Engineering, Virginia Tech, proach, full-color volumetric images and morphological USA. A partial removal of dielectric materials in nanogaps data of insect samples can be obtained. JW3A.123 can activate “passive” hotspots in multigap nanoplas- Photonic Neural Network Nonlinear Activation Func- monic systems for scalable high-performance Surface JW3A.116 tions by Electrooptic Absorption Modulators, Jonathan 1 1 1 Enhanced Raman Spectroscopy (SERS) applications. Tomographic phase microscopy for label-free imaging K. George , Armin Mehrabian , Rubab Amin , Tarek 1 2 1 1 in biomedicine, Pietro Ferraro1, Francesco Merola1, El-Ghazawi , Paul R. Prucnal , Volker J. Sorger ; George 2 JW3A.109 RAPID Pasquale Memmolo1, Lisa Miccio1, Martina Mugnano1, Washington Univ., USA; Dept. of Electrical Engineering, Boosting Local Field Enhancement by Synergistic Massimiliano Villone2, Pier Luca Maffettone2; 1ISASI-CNR, Princeton Univ., USA. We report on using the transfer func- 1 Nanoantenna-Microcavity Coupling, Qinglan Huang , Italy; 2DICMAPI, Federico II Univ., Italy. Full-tomography tion of electrooptic absorption modulators as nonlinear 1 2 2 Jui-Nung Liu , Keng-Ku Liu , Srikanth Singamaneni , in phase contrast modality of both sick and healthy cells activation functions of photonic neurons and show 95% 1 1 Brian Cunningham ; Dept. of Electrical and Computer flowing in microchannels is demonstrated. The proposed accuracy of MNIST classification inference on an AlexNet Engineering, Dept. of Bioengineering, Univ. of Illinois at method can open the way for real-world biomedical di- in optical artificial neural networks. 2 Urbana-Champaign, USA; Dept. of Mechanical Engi- agnosis by quantitative coherent imaging. Results on Red neering and Materials Science, Inst. of Materials Science Blood Cells (RBC), diatoms and tumor cells are reported. and Engineering, Washington Univ. in St. Louis, USA. We theoretically and experimentally studied a photonic-plas- monic hybrid system integrating the dielectric photonic crystal slab (as a photonic microcavity) and gold nanorod (as a plasmonic nanoantenna) for highly cooperative near- field enhancement.

FiO + LS 2018 • 16–20 September 2018 71

FiO Abstracts.indd 37 8/20/18 9:11 AM Science & Industry Showcase

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JW3A • Poster Session III and Dynamic E Posters—Continued

JW3A.124 JW3A.130 JW3A.136 Achieving Invisibility in the Far Field with a 3D Carpet High-energy 50-attosecond ‘water window’ X-ray Power improvement in a CW THz polariton laser, Cloak Design for Visible Light, Daniely G. Silva1, Poliane driven by a high-energy infrared waveform synthesizer, Yameng Zheng1, Andrew Lee1, Helen Pask1; 1Macquarie A. Teixeira1, Lucas H. Gabrielli2, Mateus A. Junqueira1, Yuxi Fu1, Hua Yuan2, Pengfei Lan2, Katsumi Midorikawa1, Univ., Australia. An enhancement in the performance of Danilo Spadoti1; 1Federal Univ. of Itajubá, Brazil; 2Univ. Eiji J. Takahashi1; 1RIKEN, Japan; 2Huazhong Univ. of an intracavity CW THz polariton laser is reported. THz of Campinas, Brazil. This work presents new results for Science and Technology, China. Combining high-energy output power of up to 23.1 µW was detected at 1.66 THz, a 3D carpet cloak designed with transformation optics infrared laser, which are generated by a dual-chirped frequency tunability across 1.30 - 2.51 THz was achieved. and quasi-conformal mapping. Simulations confirm the optical parametric amplification (DC-OPA) method, and successful operation at optical frequencies for arbitrary an optical waveform synthesizer, strong ‘water window’ JW3A.137 propagation directions, and in far field region. soft X-rays with 50-attosecond pulse duration can be Prepulse-Induced Three-Halves-Harmonic Generation obtained. as a Probe for Relativistic-Laser-Driven High-Density JW3A.125 RAPID Plasmas, Alec R. Griffith1, Matthew Edwards2, Tim Ben- Differential Digital Holography of Distant Objects JW3A.131 nett2, Julia Mikhailova2; 1Astrophysical Sciences, Princeton with the Use of Fiber Optics, Maciek Neneman1, Michal Extraction of Laser Pulses from the Rejection Port of Univ., USA; 2Mechanical and Aerospace Engineering, Dolinski1, Agnieszka Siemion1, Michal Makowski1; 1Warsaw an All-PM Figure-eight Femtosecond Er-doped Fiber Princeton Univ., USA. We examine three-halves-harmonic Univ. of Technology, Poland. A lensless setup capable Laser, Jin-long Peng1; 1Industrial Technology Research generation for femtosecond laser pulses under varying of recording differential holograms over large distance Inst., Taiwan. An all-PM figure-eight femtosecond Er-fiber pulse intensity and contrast. Strong variation in the shape is presented. Reference beam is propagated in optical laser with a rejection port is demonstrated to deliver and relative magnitude of the three-halves harmonic is fiber, allowing compact setup. Advantages of proposed output power of 23 mW. This is the highest output power observed. solution allow detailed surface imaging in orbital devices. ever reported in all-PM Er-fiber lasers based on NOLM/ NALM technique. JW3A.138 JW3A.126 A non-destructive method for measuring the absorp- Optical simulation of curved 2D and 3D spaces, Jakub JW3A.132 tion coefficient of a Yb-doped fiber, Mostafa Pey- Belin1, Dimitris Georgantzis Garcia1, Gregory Chaplain2, Theoretical Analysis of High Efficiency Laser-di- sokhan1, Esmaeil Mobini1, Behnam Abaie1, Arash Mafi1; Tomas Tyc3, Christoph Englert1, Johannes K. Courtial1; ode-pumped Continuous-Wave Hemispherical Short 1Univ. of New Mexico, USA. A non-destructive method 1Univ. of Glasgow, UK; 2Dept. of Mathematics, Imperial Cavity Laser, Fumihiro Sugiki1, Ryo Kobayashi1, Tomoki for measuring the absorption coefficient of the doped college of London, UK; 3Dept. of Theoretical Physics Kanetake1, Naoya Nakajima1, Shunji Kataoka1, Yuu Aoya- optical fiber is presented that is based on tuning the pump and Astrophysics, Masaryk Univ., Czechia. A method for gi2, Kohei Tomizawa2, Masashi Shibata2, Shunya Maeda2, wavelength and measuring the spontaneous emission at the optical simulation of curved spaces using so-called Hiroki Yamakawa2, Sakae Kawato3,4; 1Graduate School of two different locations along the fiber. space-cancelling wedges is presented. We model, Engineering, Univ. of Fukui, Japan; 2School of Engineer- theoretically, devices for optical simulation of two- and ing, Univ. of Fukui, Japan; 3Faculty of Engineering, Univ. three-dimensional curved manifolds. of Fukui, Japan; 4Life Science innovation Center, Univ. of Fukui, Japan. We theoretically analyzed a optical-to-op- JW3A.127 tical conversion efficienciy of a CW hemispherical cavity Improving the quality of ghost imaging system based Yb:YAG laser which pump source is a single-emitter-la- on Wiener Filtering, Dongyue Yang1, Junhui Li2, Chen ser-diode. As a result, the maximum efficiency of 78.6% Chang1, Guohua Wu1, Bin Luo2, Longfei Yin1, Hong Guo3; was obtained by high intensity pumping. 1School of Electronic Engineering, Beijing Univ. of Posts and Telecommunications, China; 2State Key Lab of Ad- JW3A.133 vanced Optical Communication Systems and Networks, PQ:DMNA/PMMA, a new material for recording Beijing Univ. of Posts and Telecommunications, China; volume Bragg grating for laser spectrum narrowing, 3State Key Lab of Advanced Optical Communication Te-Yuan Chung1, Yu-Hua Hsieh1, Yu-Che Hsiao1; 1National Systems and Networks, Peking Univ., China. In ghost Central Univ., Taiwan. PQ:DMNA/PMMA is a photo- imaging with pseudo-thermal light, Wiener filter improves polymer sensitive to red light exposure. Volume Bragg reconstructed image quality with the estimation of point gratings are successfully recorded in PQ:DMNA/PMMA spread function and a noise factor, which is well-fitted as and serve as external mirror of a 638 nm diode laser to proportional relation to noise amplitude in image. achieve single longitudinal mode. ber JW3A.128 JW3A.134 RAPID Optical System for Capturing 3D Images, Nikolai I. Radiation Balanced Ytterbium-doped Silica Dou- Petrov1, Angela Storozheva1, Maxim Khromov1, Yuri ble-Clad Fiber Amplifier, Esmaeil Mobini1, Mostafa Sokolov1; 1Scientific and Technological Center of Unique Peysokhan1, Behnam Abaie1, Arash Mafi1; 1Univ. of New Instrumentation of Russian Academy of Sciences, Russia. Mexico, USA. Heat mitigation by radiative cooling is An optical system for capturing 3D images and a method investigated in a fiber amplifier, where the amplifier tem- for capturing 3D images, in particular, for capturing 3D perature does not change substantially from the ambient, objects in real-time for video-conference and 3D image while amplifying 0.1 W of input signal power to 7.6 W. display using integral imaging technology are proposed. JW3A.135 JW3A.129 Effective Medium Model of Biochar - Iron Ore - Binder Wednesday, 19 Septem Wednesday, Polarization Imaging Through Highly turbid Water, Powders Mixture for Enhanced Reduction of Iron, Leo- Fei Liu1,2, Pingli Han1, Yi Wei1, Guang Zhang2, Dayu Li2, nid Butko1, Anton Anzulevich1, Igor Bychkov1, Svetlana Xiaopeng Shao1; 1Xidian Univ., China; 2Changchun Inst. of Anzulevich1, Zhiwei Peng2; 1Chelyabinsk State Univ., Rus- Optics, China. We present a polarization imaging method sia; 2Central South Univ., China. A model of biochar-iron to image through highly turbid water based on the de- ore-binder powders mixture was studied at microwaves. pendence of light scattering and the optical correlation The effective medium Bruggeman expression was ex- theory. Experiments demonstrate its contribution to make panded for three types of particles. Wave impedance “can’t see” into “can see”. dependency on concentration of iron ore was calculated.

10:15–15:00 Science & Industry Showcase Theater Programming. See page 11 for a complete list of programs.

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FiO Abstracts.indd 38 8/20/18 9:11 AM Science & Industry Showcase 13:00–14:00 Rapid Fire Oral Presentation IV, Science & Industry TheaterJOINT FiO + LS Presider: Wei Lee; National Chiao Tung University, Taiwan Participating posters are noted in the list of poster for session JW4A with the icon RAPID. Each presenter will have 3 minutes and the order will be determined by poster number.

JOINT FiO + LS

13:00–15:00 JW4A • Poster Session IV and Dynamic E Posters

JW4A.1 E-Poster JW4A.7 RAPID JW4A.13 THz Detection with Structured Plasmonic Channel, Incoherent Propagation-Invariant Space-Time Light Laser Temperature Sensor Based on a Core-offset 1 1 1 Sheets Produced from a Broadband Light Emitting Aluminum Coated Mach-Zehnder Interferometer, Kiana Montazeri , Pouya Dianat , Zhihuan Wang , Bah- 1 1 1 1 Diode, Murat Yessenov1, Hasan E. Kondakci1, Monjurul Javier A. Martin Vela , Eloísa Gallegos Arellano , Juan ram Nabet ; Drexel Univ., USA. We are proposing a 1 1 F. Meem2, Rajesh Menon2, Ayman Abouraddy1; 1CRE- M. Sierra Hernandez , Daniel Jauregui Vazquez , Juan C. novel semiconductor based terahertz detector, using 1 1 OL, Univ. of Central Florida, USA; 2Dept. of Electrical Hernandez-Garcia , Julian M. Estudillo-Ayala , Erika Silva the plasma wave propagation in a structured 2DEG by 1 1 1 electrically measuring the voltage across the channel in and Computer Engineering, Univ. of Utah, USA. We Alvarado , Roberto Rojas-Laguna ; Education, Mexico. A room temperature. demonstrate the experimental synthesis of incoherent laser temperature sensor based on a core-offset aluminum broadband diffraction-free space-time beams in the coated Mach-Zehnder interferometer is presented. The JW4A.2 E-Poster form of light sheets from an LED by introducing judicious experimental results shown a temperature sensitivity of All-Dielectric Polarization-Independent Metasurface spatio-temporal spectral correlations. 28 pm/°C and a signal to noise ratio of 45 dB. Using Cross-Shaped Unit cell, Mostafa Abdelsalam1, JW4A.14 Ahmed Mahmoud2, Mohamed M. Swillam1; 1Dept. of JW4A.8 RAPID A Simple and Robust Technique For Full Spatiotem- Physics, American Univ. in Cairo, Egypt; 2Electronics and Experimental Ray Tracing – from simulation to reality, Tobias Binkele1, David Hilbig1, Ufuk Ceyhan2, Gustavo poral Measurement of Ultrafast Laser Pulses, Daniel Communication Engineering Dept., The American Univ. 1 1 2 1 Gutierrez3, Mahmoud Essameldin1, Thomas Henning1, Adams , Henry C. Kapteyn , Seth L. Cousin ; Physics, in Cairo, Egypt. Metasurfaces depend on introducing 2 a phase gradient across the interface. In this paper we Friedrich Fleischmann1; 1Univ. of Applied Sciences Univ. of Colorado, Boulder, USA; KMLabs, USA. We show a novel polarization-independent all-dielectric Bremen, Germany; 2BLF Optik Teknoloji Sanayi A.S., present a straightforward tool for routine evaluation of metasurface, that is CMOS-compatible, showing beam Turkey; 3Cofem S.A., Spain. Ray tracing is mostly known the spatiotemporal field of ultrafast pulses. We combine steering capabilities with efficiency of 89%. from simulation. However, Häusler et al. also proposed white light interferometry with reference-free wave-front- an experimental implementation of ray tracing. We sensing and pulse-measurement in a single-scan to obtain JW4A.3 E-Poster have taken the proposal to real life and covered a lot of 3D pulse profiles. Diagnosis of glioma brain cancer using visible res- applications with it. JW4A.15 onance Raman spectroscopy, Yan Zhou2, Binlin Wu1, 3 2 2 JW4A.9 RAPID Suppression of Back-Side Reflections with Broadband Cheng-hui Liu , Xinguang Yu , Gangge Cheng , Kai 1 1 4 3 5 3 Improved Subaperture Stitching for the Measurement Elastomeric Light Trap, David Miller , Robert R. McLeod ; Wang , Chunyuan Zhang , Lingyan Shi , Robert Alfano ; 1 1Southern Connecticut State Univ., USA; 2Air Force Gen- of Freeform Wavefront, kamal pant1,2, Daliramu Burada1, Univ. of Colorado at Boulder, USA. Using elastomeric eral Hospital, PLA, China; 3City College of New York, Amitava Ghosh2, Gufran Khan1, Chandra Shakher1; 1IDDC, material and a broadband absorber, we detail a method USA; 4Jilin Univ., China; 5Dept. of Chemistry, Columbia IIT, India; 2IRDE, India. This paper presents an improved for broadband suppression of Fresnel reflections from the Univ., USA. Resonance Raman spectroscopy using stitching technique for freeform metrology. The lateral backside of transparent substrates. Applications include 532nm excitation was used to distinguish normal brain misalignments are minimized using modified iterative spectroscopic ellipsometry, holography, and lithography. tissue from different grades of glioma tissues. Principal closest point based registration. The method is applied JW4A.16 component analysis was used to analyze the spectral data to freeform measurement using Shack-Hartmann Sensor. LDLS Powered High Throughput Tunable Light Source, and achieved high accuracy. 1 1 1 JW4A.10 RAPID Xiaohua Ye , Alex Cutler , Qingsong Wang , Tseten 1 1 1 1 JW4A.4 E-Poster Extremely Compact and Broadband Polarization Beam Lungjangwa , Ron Collins , Matt Besen , Huiling Zhu ; 1 Non-Adiabatic Tapered Fibers for the Operation Splitter Enabled by Customized Port Angles, Yannick Energetiq Inc., USA. High throughput tunable light D’Mello1, Eslam El-Fiky1, James Skoric1, Yun Wang1, sources (TLS) using an ultrahigh-brightness Laser-Driven

of a Switchable Multi-Wavelength Thulium-Doped Wednesday, 19 Septem Fiber Laser, Baldemar Ibarra-Escamilla1, Marco V. Amar Kumar1, David Patel1, David V. Plant1; 1McGill Univ., Light Source (LDLS™) are developed for photonic appli- Hernández-Arriaga1, Manuel Durán-Sánchez2, Hector Canada. We demonstrate a compact yet fabrication cations. Measurement results of in-band fluxes and FWHM Santiago-Hernandez1, Evgeny A. Kuzin1; 1INAOE, Mexico; tolerant polarization beam splitter. Customized angles bandwidths, between 400nm and 1100nm, are presented. 2INAOE, CONACyT, Mexico. A switchable multi-wave- at each port facilitate a broadband response over 100 JW4A.17 length thulium-doped fiber laser based on non-adiabatic nm, including 3 dB insertion loss and 11.2 dB extinction Tunable Stacks of Wedged Interferometers for Optical tapered fibers is experimentally demonstrated. The laser ratio in the C-band. Communications and Spectroscopy, Marin Nenchev2, is switched from single to multi-wavelength by curving the 1 2 1 JW4A.11 RAPID Elena Stoykova , Margarita Deneva ; Bulgarian Academy tapers showing high stability output near 2 μm region. 2 A Tunable Low-pass Filter for Femtosecond Lasers of Sciences, Bulgaria; Technical Univ. - Plovdiv Branch, JW4A.5 E-Poster Based on a Passive Cavity, Xiao Xiang1, Feiyan Hou1, Bulgaria. We propose a stack of two Fizeau interferome- Continuous Wave Laser Induced Damage Threshold Dongdong Jiao1, Tao Liu1, Shougang Zhang1, Ruifang ters for selection of a single continuously tunable within of Ge Sb Se at 1.07 microns, John E. McElhenny1; Dong1; 1National Time Service Center, CAS, China. We 10-50 nm resonance with a linewidth of 0.01 nm or less

28 12 60 ber 1US Army Research Lab, USA. The continuous wave report a tunable optical low-pass filter for femtosecond and utilization of such stacks for wavelength-division laser-induced damage threshold of chalcogenide glass, lasers based on a passive cavity. The cutoff frequency multiplexing. Ge Sb Se , is measured for a 5s exposure of 1.07 µm can be tuned by stabilizing the cavity length to different 28 12 60 JW4A.18 light focused to a spot size with 1/e2 diameter of 830 µm, secondary resonance peaks. Anti-Reflecting Surfaces Using Two-layer Motheye following the ISO standards. 1 JW4A.12 Structures for Spinel Ceramic Windows, Chaoran Tu , 1 1 JW4A.6 E-Poster Nonregular Three-Dimensional Polarization States, Curtis Menyuk ; Univ. of Maryland Baltimore County, Engineering the Wavelength and Topological Charge of Jose J. Gil2, Andreas Norrman3, Tero Setälä1, Ari Tapio USA. We design and optimize a two-layer pyramid 1 1 2 motheye structures for long wavelength MgAl O spinel Non-diffracting Beams along their Axis of Propagation, Friberg ; Univ. of Eastern Finland, Finland; Univ. of 2 4 Ahmed Dorrah1, Michel Zamboni-Rached2, Mo Mojahedi1; Zaragoza, Spain; 3Max Planck Inst. for the Science of ceramic windows. We show that a two-layer pyramid 1Dept. of Electrical and Computer Engineering, Univ. of Light, Germany. General three-dimensional (3D) states of motheye structure can achieve average transmission of Toronto, Canada; 2School of Electrical Engineering, Univ. polarization may be classified as regular and nonregular. 98.96% from 0.5 μm to 5 μm. of Campinas, Brazil. We report on class of non-diffracting We consider the concept of nonregularity and assess its beams where the wavelength and topological charge characterization and consequences with applications to (orbital angular momentum) can be controlled along evanescent electromagnetic waves. the beam’s axis, thus addressing challenges in imaging, materials processing, and dense data communications.

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JW4A • Poster Session IV and Dynamic E Posters—Continued

JW4A.19 JW4A.25 RAPID JW4A.32 Photodarkening of kW-level Yb-doped Aluminosilicate Two-Dimensional Reconstruction of The Fly Drosophila Temporal and Polarization Symmetry Breaking in Ring (Al O -SiO ) Fiber, Jiacheng Wu1, Tianhong Qian1, Kaijun Resonators, Francois Copie1, Michael T. Woodley1, 2 3 2 Melanogaster By Holographic Interferometry, Luis A. 1 1 1 1 Shu ; Anhui Univ. of Chinese Medicine, China. We report- Marín1, Evelyn A. Granizo1; 1Optics Lab, ESPOCH, Ecua- Leonardo Del Bino , Jonathan M. Silver , Shuangyou 1 1 1 ed on laser performance of a kW-level 20/400 Yb-doped dor. Using the Matlab software, images obtained from the Zhang , Pascal Del’Haye ; National Physical Lab, UK, aluminosilicate fiber. Laser running of 120 minutes at fly Drosophila melanogaster are shown in a holographic UK. We study the occurrence of two symmetry breaking 1.2kW showed power degradation of 10.6% and slope simulator designed with the objective of processing and processes in ring resonators pumped by short pulses. efficiency degradation of 116%, directly justifying serious reconstructing binary holograms. An unconventional Different scenarios are predicted depending on the input photodarkening effect. system of teaching science. characteristics, including a complex dynamical interplay between the two mechanisms. JW4A.20 JW4A.26 Camera and Inverse Camera System for Free-Space High-Resolution, High Speed Defect Detection of JW4A.33 1,2 Optical Communications, Sajad Saghaye Polkoo , Curved Optics, Timothy A. Potts1; 1Dark Field Technol- Brillouin Comb Generation in a Highly Nonlinear Tel- 1,2 1 1 1 Christopher K. Renshaw ; Univ. of Central Florida, ogies, USA. Automated inspection of curved optics is a lurite Single Mode Fiber, Luo Xing , Hoang Tuan Tong , 2 1 1 1 CREOL, USA; Physics, Univ. of Central Florida, USA. We large industry need. Conventional laser/camera systems Than Singh Saini , Hoa P. Nguyen , Takenobu Suzuki , 1 1 introduce an imaging-based transceiver for FSOC that cannot deliver reliable inspection of curved surfaces. Yasutake Ohishi ; Research Center for Advanced Photon enables precision beam steering over a wide field-of- Solid State Laser Reflection (SSLR) technology solves the Technology, Toyota Technological Inst., Japan. Brillouin regard using low-cost components with no moving parts. problem of curved optics inspection. comb generation in a ring cavity composed of a piece Passive beam steering provides dynamic beam-shaping of tellurite single mode fiber was demonstrated. Cas- and multiplexable communication. JW4A.27 caded stimulated Brillouin Stokes and anti-Stokes lines Multimodal imaging Mueller polarimetric microscope resulted in multi-wavelength Brillouin comb generation JW4A.21 on geometrical analysis of spherical microparticles, bi-directionally. A Fabrication of Nanostructures with a Transmission Thomas Sang Hyuk Yoo1, Andrea Fernández2, Fernando Light and a Plasmonic Field at Different Z-axis Position, Moreno2, Jose Maria Saiz2, Razvigor Ossikovski1, Enric JW4A.34 1 1 1 Taeyeon Kim , Heesang Ahn , Hyerin Song , Jong-ryul Garcia-Caurel1; 1LPICM, Ecole Polytechnique, France; Surface Modification of Additively Manufactured 2 1,3 1 Choi , Kyujung Kim ; Dept. of Cogno-mechatronics 2Dpto. de Física Aplicada, Universidad de Cantabria, Titanium Components via Femtosecond Laser Micro- 2 1 2 1 Engineering, Pusan National Univ., South Korea; Medical Spain. We developed a multimodal imaging polarimetric machining, Nathan G. Worts , Jason Jones , Jeff Squier ; 1 2 Device Development Center, Dagu-Gyeongbuk Medical microscope which images both in Fourier (back-focal) and Colorado School of Mines, USA; Moog Inc., USA. Novel 3 Innovation Foundation (DGMIF), South Korea; Dept. of real planes. We propose an application to study spherical capabilities including surface roughness modification, Optics and Mechatronics Engineering, Pusan National microparticles showing size and shape dependent pola- nanogratings, and micro-cones are achieved through Univ., South Korea. We fabricated two hole-array pattern rimetric properties. post-processing of additively manufactured parts by masks and observed the differences between conven- an amplified femtosecond laser. Applications of these tional photolithography and plasmonic lithography by JW4A.28 surface features are discussed. controlling the gap distance between the mask and the Toward Training a Deep Neural Network to Optimize photoresist. Lens Designs, Geoffroi Côté1, Jean-François Lalonde1, JW4A.35 Simon Thibault1; 1Université Laval, Canada. A deep neural Radiation detection with mid-IR laser breakdown of air, 1 1 1 JW4A.22 network (DNN) is trained in an unsupervised manner, Daniel C. Woodbury , Robert Schwartz , Joshua Isaacs , 1 1 1 Non-scanning three-dimensional measurements us- using RMS spot size, to output optimized lens designs Phillip Sprangle , Howard Milchberg ; Univ. of Maryland ing a chirped frequency comb interferometry with a from provided specifications. at College Park, USA. We demonstrate standoff detection multi-mode fiber bundle, Megumi Uchida1,2, Takashi of radioactive material based on avalanche breakdown 1,2 1,2 1,2 1 Kato , Yurina Tanaka , Kaoru Minoshima ; The Univ. JW4A.29 of irradiated air with mid-IR laser pulses. With radiation 2 of Electro-Communications (UEC), Japan; Japan Science Synchronized Microphone Array for Single-shot Axial present, breakdowns experience a temporal shift in their and Technology Agency (JST), ERATO MINOSHIMA Profiles of Femtosecond Filaments, Ilia Larkin1, Aaron evolution, and can exhibit on-off sensitivity. Intelligent Optical Synthesizer (IOS) Project, Japan. We Schweinsberg2, Anthony Valenzuela3, Howard Milchberg1; developed a non-scanning three-dimensional measure- 1IREAP, Univ. of Maryland, USA; 2Oak Ridge Inst. for JW4A.36 ment method using multi-mode fiber bundle. Based on 3 Coherent Excitation of Phonon Polaritons in BaGa Se Science and Education, USA; US Army Research Lab, 4 7 ultrafast space-time-frequency conversion with the optical by Terahertz Pulses, Bo Wang1, Yiwen E1, Jiyong Yao2,

ber Aberdeen Proving Grounds, USA. A synchronized array 1 1 frequency comb, non-scanning 3D imaging with high of microphones maps, in a single shot, the axial energy Li Wang ; Beijing National Lab for Condensed Matter power efficiency is demonstrated. deposition profile from a femtosecond laser filament as Physics, Inst. of Physics, Univ. of Chinese Academy of 2 a function of perturbations in input laser energy, pulse Sciences, Chinese Academy of Sciences, China; Key Lab JW4A.23 duration, and focusing geometry. of Functional Crystals and Laser Technology, Technical Slit-Width Effects in a Double-Slit Experiment with a Inst. of Physics and Chemistry, Univ. of Chinese Acad- 1 Partially-Coherent Source, Brett J. Pearson , Natalie JW4A.30 emy of Sciences, Chinese Academy of Sciences, China. Ferris1, Ruthie Strauss1, Hongyi Li1, David P. Jackson1; Phonon polaritons are generated in BaGa Se by linear High-sensitive Absorption Measurement in Silica and 4 7 1 Dickinson College, USA. We perform a Young’s dou- Quartz Crystal with Time-resolved Photo-thermal Com- excitation of terahertz pulses, and probed using 800 ble-slit experiment using a partially-coherent light source. mon-path Interferometry, Ksenia V. Vlasova1, Alexandre nm femtosecond laser pulses. The observed phonon As compared to the standard theory, the data agree much Makarov1, Nikolai Andreev1; 1Inst. of Applied Physics polaritons can be perfectly reproduced by a damped more favorably with a calculation that fully accounts for RAS, Russia. The results of measurements of ultra-low harmonic oscillator model. the width of the slits. (~10-7cm-1) absorption of optical radiation (λ=1.07 μm) Wednesday, 19 Septem Wednesday, in synthetic crystalline quartz and in fused quartz by JW4A.37 JW4A.24 time-resolved modification of a Photo-thermal common Third-Order Nonlinear Optical Properties of ALD Fabrication of YAlO :Gd3+ Thin Films for Nanoimaging, Grown TiO Films by Thermally Managed Z-scan Meth- 3 interferometry are presented. 2 Mykyta Kolchiba1, Wataru Inami2, Yoshimasa Kawata2; od, Isaac Basaldua1, Paul Burkins1, Robinson Kuis1, Jaron 1 1 1 1 Graduate School of Science and Technology, Shizuoka JW4A.31 Kropp , Theodosia Gougousi , Anthony M. Johnson ; 2 1 Univ., Japan; Research Inst. of Electronics, Shizuoka Coherent ultra-broadband wave-breaking radiation in a Univ. of Maryland Baltimore County, USA. Thermally 3+ Univ., Japan. We have fabricated YAlO :Gd perovskite 1 1 managed Z-scan performed on ALD grown TiO films 3 laser plasma accelerator, Bo Miao , Linus Feder , Howard 2 -11 -10 2 thin films by RF magnetron sputtering as free-standing 1 1 demonstrated n values of 1.7x10 and 1.94 x10 cm /W Milchberg ; Univ. of Maryland at College Park, USA. Ab- 2 membranes for optical nanoimaging systems. Homoge- stract: Electron self-injection in a laser plasma accelerator for films grown at 100°C and 250°C, respectively – greater neous, robust and bright scintillators emerge a perfect generates an ultra-broadband coherent radiation flash. than 1000X that of other growth methods. candidate in high-resolution imaging. We show that the flash spectrum reveals information on the plasma density and the electron injection process. JW4A.38 Polarization and Entanglement in Mixed Classical States, Asma Al-Qasimi1, Joseph H. Eberly1; 1Univ. of Rochester, USA. The relationship between polarization and entanglement [1] implies classical entanglement places limits on observable coherence properties. Here we study how the coherences affect each other in the case of mixed classical states.

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JW4A • Poster Session IV and Dynamic E Posters—Continued

JW4A.39 JW4A.47 RAPID JW4A.54 Design and Modeling of a Chalcogenide Taper Fiber Development of high-precision mode decomposition Probing Vibration-Cavity Polariton Dynamics via Ultra- 2,1 for High Average Power Supercontinuum Generation, devices for optical vortices, Keisaku Yamane1, Yuho fast Infrared Spectroscopy, Andrea B. Grafton , Adam 1 1 1 1 1 2,1 Than Singh Saini , Hoa P. Nguyen , Hoang Tuan Tong , Watanabe1, Isamu Wakisaka1, Kazuhiko Oka2, Yasunori Dunkelberger , Kenan Fears , Roderick Davidson , Blake 1 1 1 1 1 1 1 Luo Xing , Takenobu Suzuki , Yasutake Ohishi ; Toyota Toda1, Ryuji Morita1; 1Hokkaido Univ., Japan; 2Hirosaki Simpkins , Jeffrey Owrutsky ; U.S. Naval Research Lab, 2 Technological Inst., Japan. Chalcogenide taper-fiber Univ., Japan. New mode decomposition devices for op- USA; National Research Council, USA. Time resolved structure is reported for high-power broadband super- tical vortices were developed. Their performances were IR pump-probe spectroscopy was used to measure the continuum spectrum covering from 1.5–14 µm. The taper experimentally verified and in good agreement with the vibrational dynamics of strong chromophores in optical fiber was pumped with femtosecond laser pulse of an cavities. A fast component in the lifetime of W(CO) corresponding simulations, showing precise spatial-phase 6 average power of 200 mW at 3.5 μm. control based on Pancharatnam-Berry phase. in hexane was observed, but not in the other systems.

JW4A.40 JW4A.48 RAPID JW4A.55 Optical Switching and Thermal Recovery of Vanadium Photokinetic effects in vector Bessel beams, Aaron Self-Compression of Ultrashort Pulses in Hollow Wave- 1 1 1 1 Dioxide, Marc Currie , Virginia Wheeler , Mario Ancona , Yevick1, David G. Grier1; 1New York Univ., USA. Vector Bes- guide for High Harmonic Generation, Qiandong Ran , 1 1 1 2 2 2 2 1 Tatyana Feygelson , Karl Hobart ; US Naval Research Lab, sel Beams are a conical superposition of polarized plane Lifeng Wang , Lu Li , Hao Li , Ying Zhang ; Nanyang 2 USA. Vanadium dioxide films were grown on sapphire waves. The angular spectrum including polarizations is Technological Univ., Singapore; Singapore Inst. of Man- substrates as well as thin diamond membranes. Optical useful for identifying relationships among different polar- ufacturing Technology, Singapore. Self-compression of pump-probe experiments show large optical modulation ization states, and understanding forces on small objects. pulses was observed in gas-filled waveguide. This can in response to moderate optical excitation and follow a be used to enhance High Harmonic Generation (HHG). pure thermal model. JW4A.49 RAPID Here, 2cm hollow waveguide with inner diameter 150μm Ultrafast magnetization dynamics in nanoscale two-di- was used. Bright HHG in water window was produced. JW4A.41 mensional Permalloy annular antidot lattices, Nikita Linear Localization of non-Hermitian Photonic Zero Porwal1, Sucheta Mondal2, Samiran Choudhury2, Anulekha JW4A.56 RAPID 1 1 1 Modes, Li Ge , Bingkun Qi ; College of Staten Island, De2, Jaivardhan Sinha2, Anjan Barman2, Prasanta Kumar Probing Light-Metal Interaction with the Photon-Drag 2 2,1 2 CUNY, USA. A non-Hermitian photonic zero mode can Datta1; 1Indian Inst. of Technology Kharagpur, India; Effect, Jared Strait , Glenn Holland , B. Robert Ilic , Amit 2,1 2,3 2 1 exhibit an unusual behavior at the transition between 22Dept. of Condensed Matter Physics and Material Agrawal , Domenico Pacifici , Henri Lezec ; Maryland 2 extended and localized regimes: it displays a linearly Sciences, S. N. Bose National Centre for Basic Sciences, NanoCenter, Univ. of Maryland, USA; Center for Na- 3 decreasing amplitude in space inside a weakly coupled Block JD, Sector III, Kolkata , India. The static and dynamic noscale Science and Technology, NIST, USA; School of non-Hermitian reservoir. Engineering and Dept. of Physics, Brown Univ., USA. We response of 2-D Ni80Fe20 annular antidot lattices has been investigated with varying bias magnetic field using TR- demonstrate that the sign of the photon-drag effect in JW4A.42 MOKE microscopy. Multiple frequency modes observed smooth metal films conflicts with the prevailing intuitive Dark Soliton and Cnoidal Wave Frequency Combs in in experiment are verified by micromagnetic simulations. model of direct momentum transfer to free electrons, Microresonators by Second Harmonic Generation, establishing the need for a new microscopic model of 1 1 Zhen Qi ; Univ. of Maryland Baltimore County, USA. We JW4A.50 RAPID radiation pressure. study dark solitons and cnoidal waves frequency combs Vector vortex beam from doubly-resonant nanosecond generated by second harmonic generation in microreso- optical parametric oscillator, Varun Sharma1, Goutam JW4A.57 RAPID nators. We obtain stable dark solitons and cnoidal waves K. Samanta1, S. C. Kumar2, A Aadhi1, H. Ye2, M. Ebra- Multiplexing a Cavity-Enhanced Quantum Memory, 1 1 2,1 when fundamental frequency and second harmonic in him-Zadeh2,3; 1PRL Ahmedabad, India; 2ICFO-Institut Paul D. Kunz , Kevin Cox , David Meyer , Zachary A. 2,1 1 2 oppositely dispersive regimes. de Ciencies Fotoniques, The Barcelona Inst. of Science Castillo ; Army Research Labs, USA; Physics, Univ. of and Technology, Spain; 3Institucio Catalana de Recerca i Maryland, USA. We present ongoing work on a multi- JW4A.43 Estudis Avancats (ICREA), Spain. We demonstrate a novel plexed atom-cavity quantum memory with the goal of THz Region Elastic Scattering from a Silica Micro- experimental scheme to generate tunable vector vortex achieving fast entanglement generation - one of the pri- 1 1 sphere, Suat Kurt , Nurperi Yavuz , Syed Sultan Shah beam directly from an optical parametric oscillator (OPO). mary remaining hurdles to a functional quantum repeater. 1 1 1 Bukhari , Ali Serpengüzel ; Koc Univ., Turkey. Using Using a nanosecond doubly-resonant OPO, we produce GLMT, we investigated 0° transmission and 90° elastic JW4A.58 RAPID

vector vortex beam tunable across 964-990 nm. Wednesday, 19 Septem scattering from a silica microsphere. The numerically Entanglement between Topological and Trivial Modes, 1 1 2 observed mode spacing agrees well with the theoretically JW4A.51 Andrea Blanco-Redondo , Bryn A. Bell , Dikla Oren , Ben- 1 2 1 estimated value. Silica microspheres show promise for Propagation of Vortex Pulsed Beams in Free Space, jamin J. Eggleton , Mordechai Segev ; Univ. of Sydney, 2 novel THz applications. Nikolai I. Petrov1; 1Scientific and Technological Center Australia; Technion, Israel. We report the experimental of Unique Instrumentation of Russian Academy of Sci- observation of biphoton entanglement between topo- JW4A.44 ences, Russia. Propagation of spatiotemporal pulses logically and trivially localized modes in a nanophotonic Imaging with Thick Lenses using ABCD Matrices and in free-space taking into account nonparaxial effects is lattice of coupled silicon waveguides. under First-Order Material Dispersion, Monish R. Chat- investigated. Non-invariance of the velocity of spatially 1 1 1 terjee , Salaheddeen Bugoffa ; Univ. of Dayton, USA. localized vortex pulsed beams in vacuum is shown by JW4A.59 RAPID ABCD matrices for a thick lens are applied for imaging a rigorous calculation of the wave equation. Sensitivity-bandwidth Enhancement of Gravitational colored 2D object under first-order material dispersion. Wave Detector Without Using Dispersive Medium, 1 1 1 1 Frequency-dependent dispersion of permittivity is incor- JW4A.52 Minchuan Zhou , Zifan Zhou , Selim M. Shahriar ; North- ber porated in the analysis and results are compared with the Ultrafast Laser Micro-stressing for Correction of Thin western Univ., USA. We show that via small changes in the non-dispersive problem. Fused Silica Optics for Future X-Ray Space Telescopes, parameters of the existing signal-recycled interferometric Heng Zuo1,2, Brandon Chalifoux2, Ralf Heilmann2, Mark gravitational wave detector, it is possible to achieve an JW4A.45 Schattenburg2; 1Dept. of Aeronautics and Astronautics, enhancement on the order of 10 in the sensitivity-band- 1 1 Warped Space-Time Optics, William B. Webb ; Energy MIT, USA; 2MIT Kavli Inst. for Astrophysics Research, width product. Control Engineering, USA. Atoms are structured from USA. We present a novel application of ultrafast laser Loopons; a variety of Photons. Loopon Electrons warp. micromachining for figure correction of future light-weight JW4A.60 Their speed-of-light is warped, producing a transparent high-resolution X-ray mirrors. Preliminary results of local Generation and Storage of Entanglement between 1 material’s Index of Refraction. Photons obliquely entering deformation and stress changes in flat fused silica sub- Two All-Optical Quantum Memories, Fumiya Okamoto , 1 1 1 or leaving bend and change speeds outside the material. strates are demonstrated. Yosuke Hashimoto , Jun-ichi Yoshikawa , Rei Sakakibara , Peter v. Loock2, Akira Furusawa1; 1The Univ. Of Tokyo, 2 JW4A.46 RAPID JW4A.53 Japan; Johannes Gutenberg Univ. Mainz, Germany. We Spatio-temporal observation of the Fermi-Pasta-Ulam Interaction of Laser Beam with Plasmonic Nanoparti- experimentally demonstrate generation and storage of 1 recurrence in optical fibers, Corentin Naveau , Pascal cles, Avesh Kumar1,2; 1Bhim Rao Ambedkar Univ., India; entanglement between two concatenated cavity mem- 1 1 1 Szriftgiser , Alexandre Kudlinski , Matteo Conforti , Ste- 2AMOPH, Physical Research Lab, India. Interaction of ories. The logarithmic negativity is 0.150±0.006 even at 2 1 1 fano Trillo , Arnaud Mussot ; Université de Lille, France; input laser beams with colloidal suspensions of plasmonic 400 ns storage time. 2 Univ. of Ferrara, Italy. We report the spatio-temporal ob- nanoparticles is studied. It results in different types of servation of the Fermi-Pasta-Ulam recurrence via non-de- structures after propagation through a suspension. structive distributed measurements in phase and intensity of main frequency components of the frequency comb.

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JW4A • Poster Session IV and Dynamic E Posters—Continued

JW4A.61 JW4A.68 JW4A.75 Optimized Cooling of Atoms in Optical Lattice for Correlation Properties of Polarization Dynamics in Tunable Stub Plasmonic Structures for Terahertz High Rate Quantum Memory Operation, Michal J. Quantum Dot Lasers with Optical Feedback, Chen Detectors and Sources, Michael Shur1,2, Gregory Aizin3, Piotrowicz2, Thomas G. Akin3, John Reintjes2, Alex Yang1, Salim Ourari1, Hong Lin1; 1Bates College, USA. John Mikalopas3; 1Rensselaer Polytechnic Inst., USA; Kuzmich4, Adam T. Black1, Mark Bashkansky1; 1Optical Dynamics of polarized states are examined for a quan- 2Electronics of the Future, Inc., USA; 3Kingsborough Sciences Division, U.S. Naval Research Lab, USA; 2KeyW tum dot laser subject to polarization-rotated feedback. College, USA. Plasmonic boom terahertz devices could Corporation, USA; 3NRC Postdoctoral Research Associ- Correlations of different polarizations are studied by increase the generated power and detection sensitivity ate, USA; 4Dept. of Physics, Univ. of Michigan, USA. We evaluating cross correlation functions. by orders of magnitude. They require tuning conditions at present an optimized cooling sequence for Rb atoms in a heterodimensional interfaces and slow . These 1D optical lattice for quantum memory experiments. We JW4A.69 requirements are met using plasmonic stubs. show an increase in number of memory write and read Rectangular Core Dispersion Engineered Photonic events per one lattice load. Crystal Fiber for Supercontinuum Generation, Pooja JW4A.76 Chauhan1, Ajeet Kumar1, Yogita Kalra1, Than Singh Saini2; Effective photonic potential for TM waves, Alessandro JW4A.62 1Delhi Technological Univ., India; 2Toyota Technological Alberucci1, Chandroth P. Jisha2, Stefan Nolte1,3; 1Fried- Dual-Seeded Four-Wave Mixing in Portable Quantum Inst., Japan. Design of a rectangular core photonic crystal rich-Schiller-Universitat Jena, Germany; 2Universidade 1 1 3 Light Source, Nicholas Brewer , Meng-Chang Wu , Rory fiber in Ge20Sb15Se64 chalcogenide glass is presented for do Porto, Portugal; Fraunhofer Inst. of Applied Optics W. Speirs1, Paul Lett2; 1Univ. of Maryland, USA; 2National mid-IR. Our simulation results include the study of disper- and Precision Engineering, Germany. We use an effective Inst. of Standards and Technology, USA. The noise sion, nonlinearity and fundamental effective mode area. photonic potential to describe light confinement of TM spectrum of intensity-difference squeezed light exhibits waves in sub-wavelength structures, such as GRIN and slot excess noise at high frequencies when a tapered ampli- JW4A.70 waveguides. The predictions of the model are confirmed fier is used as a pump beam. Our dual-seed technique Blu-ray DVD as SERS substrate for reliable detection by FDTD simulations. corrects this noise. and quantification of urea, Nabadweep Chamuah1, Ankita Saikia1, Pabitra Nath1; 1Tezpur Univ., India. Herein JW4A.77 JW4A.63 development SERS substrate using blu-ray DVD and Aluminum Gallium Arsenide as a High-Reflectivity Coat- Complete characterization of optical multi-tempo- subsequent use for detection of urea is demonstrated. ing Material for Interferometric Gravitational-wave ral-mode quantum states, Kan Takase1, Masanori The substrate yields reproducibility with RSD value of Detectors, Gregory M. Harry1, Steve Penn2, Garrett Okada1, Takahiro Serikawa1, Shuntaro Takeda1,2, Jun-ichi 14.33%. Urea concentration of 0.06µg/dL can be detected Cole3, GariLynn Billingsley4, Matthew Evans5, Geoffrey Yoshikawa1, Akira Furusawa1; 1applied physics, the Univ. reliably with this substrate. Lovelace6; 1American Univ., USA; 2Hobart and William of Tokyo, Japan; 2JST, PRESTO, Japan. We propose and Smith Colleges, USA; 3Crystalline Mirror Solutions, USA; demonstrate a method useful to characterize optical JW4A.71 4LIGO Lab, California Inst. of Technology, USA; 5LIGO multi-temporal-mode Fock states typified by quantum Anderson Localization in Subwavelength Plasmonic Lab, MIT, USA; 6Physics, California State Univ. Fullerton, error correction code states using a simple experimental Structures, Ali Ghoreyshi1, R. H. Victora1; 1Univ. of USA. Substrate-transferred single-crystal semiconductor setup and data analysis procedure. Minnesota, USA. We used the FDTD simulation to study heterostructures are effective as low-thermal-noise optical photon propagation in arrays of plasmonic particles. In coatings for small beams. We discuss progress in devel- JW4A.64 such systems, structural randomness can lead to localiza- oping GaAs/AlGaAs coatings at a size for gravitational Two Opto-Atomic Devices for Classical and Quantum tion of light in the deep subwavelength regime, similar wave detectors such as LIGO. Communication, David H. Meyer1, Kevin C. Cox2, Zach- to Anderson localization of electrons. ary A. Castillo1, Paul D. Kunz2; 1Dept. of Physics, Univ. of JW4A.78 Maryland at College Park, USA; 2U.S. Army Research Lab, JW4A.72 Solitary wave solutions in nonlinear media with quartic USA. We present ongoing developments of two atomic Free-Space Daylight Quantum Key Distribution without and quadratic dispersion—implications for high-power devices to improve optical communication rates in the Source Side Channel Effects, Heasin Ko1, Chun Ju Youn1; lasers, Kevin K. Tam1, Tristram J. Alexander1, Andrea classical and quantum regimes: a Rydberg atomic receiver 1Electronics and Telecommunications Research Inst., Blanco-Redondo1, C. Martijn de Sterke1; 1Univ. of Syd- for classical data and a ring-cavity atomic memory for long South Korea. We study the performance of a free-space ney, Australia. We consider solutions to the nonlinear distance quantum communication. quantum key distribution system operated at the clock Schrödinger equation with quadratic and quartic disper- rate of 400MHz in daylight without source side channel sion, and discover a temporal soliton family that includes JW4A.65 effects. Noise photons from sunlight were effectively recently discovered pure quartic solitons and solitons with

Carrier Dynamics in Monolayer WS2 via Time-Resolved eliminated with filtering techniques. only quadratic dispersion. ber Terahertz Spectroscopy, Jon K. Gustafson1, Michael Hayden1; 1Physics, UMBC, USA. We investigate the ultra- JW4A.73 JW4A.79 fast dynamics of photogenerated charge carriers in the Strong-Coupling Model for Pulsed Light Propagation Electro-Optic Temporal Optical Systems for Spectral 1 two-dimensional material WS2 via time-resolved terahertz and Quantum Kinetics of Electron-Hole Plasmas in Shaping of Quantum Light, Filip Sosnicki , Maciej spectroscopy. We report on the behavior of excitons, Quantum Wire Arrays, Jeremy R. Gulley1, Danhong Galka1,2, Michal Mikolajczyk1, Alex O. Davis3, Valérian trions, and unbound electrons/holes in this material. Huang2; 1Dept. of Physics, Kennesaw State Univ., USA; Thiel3, Brian J. Smith3,4, Michal Karpinski1,3; 1Uniwersytet 2Space Vehicles Directorate, Air Force Research Lab, Warszawski, Poland; 2Cavendish Lab, Univ. of Cambridge, JW4A.66 USA. A quantum-kinetic model is proposed for ultrafast UK; 3Clarendon Lab, Univ. of Oxford, UK; 4Dept. of Physics Reduced Decoherence of Macroscopic States Using carrier-scattering dynamics in quantum wires coupled to and Oregon Center for Optical, Molecular, and Quantum Squeezing and Anti-Squeezing, Richard A. Brewster1, resonant scattering of ultrashort light pulses. The model Science, Univ. of Oregon, USA. We experimentally show James Franson1; 1Univ. of Maryland, Baltimore County, includes effects from transverse, longitudinal, and applied spectral-temporal (ST) modification of single-photon USA. The decoherence of macroscopic quantum states DC fields on the wires. pulses by a system of two electrooptic time lenses. Our Wednesday, 19 Septem Wednesday, due to loss can be reduced by squeezing before trans- work enables ST shaping of quantum light for mode mission, followed by amplification and anti-squeezing to JW4A.74 matching in quantum networks and for quantum infor- restore the original amplitude. This approach does not Probing Dynamics In Quantum Magnetism With mation processing. decrease the data transmission rate. Ultracold Atoms, Araceli Venegas Gomez1, Andrew J. Daley1, Wolfgang Ketterle2; 1Univ. of Strathclyde, UK; JW4A.80 JW4A.67 2MIT, USA. The macroscopic control over cold atoms An Effective Suppression of Relative Intensity Noise Picosecond Pulse Pumped Supercontinuum Genera- in optical lattices offers an excellent platform to study for Fiber-Optic Gyroscopes with Harmonics Demodu- tion in Silicon-on-insulator Waveguide with a Weak the out-of-equilibrium behaviour of strongly correlated lation, Yulin Li1, Fang Ben1, Rongya Luo1, Sheng Deng1, Continuous Wave Trigger, Guangkuo Li1, Qian Li1; systems, such as spin models, which are usually motivated Fangyuan Chen1, Dong He1, Chao Peng1, Zhengbin Li1; 1Peking Univ., China. We investigate the effect of a weak by solid state physics. 1State Key Lab of Advanced Optical Communication continuous-wave trigger on picosecond pulse pumped Systems and Networks, Peking Univ., China. A relative supercontinuum generation in silicon-on-insulator intensity noise suppression method is demonstrated for waveguide. A spectrally broadened and highly coherent interferometric fiber-optic gyroscopes with harmonics supercontinuum is achieved. demodulation by processing the interference and refer- ence signals electronically, which decreases the angular random walk by 40%.

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JW4A.81 JW4A.88 JW4A.96 400 Gbps PM-QPSK Transmission for Metro-DCI Ap- Off-Axis Parabolic Mirrors Based Multiplexer Design Integration of TMDCs Layer on a Silicon Micro-ring plications Employing 20 Gbaud Transmitter, Lakshmi for Spatial Domain Multiplexing, Syed H. Murshid1, Ce Resonator for Photonic Applications, Rishi Maiti1, Rohit Narayanan Venkatasubramani1, Aneesh Sobhanan1, Su1; 1Florida Inst. of Technology, USA. CAD based model Hemnani1, Rubab Amin1, Volker J. Sorger1; 1GEORGE Deepa Venkitesh1, David Koilpillai1; 1INDIAN INST. OF to multiplex the input of MIMO based spatially multi- WASHINGTON UNIV., USA. Here we report on the inte- TECHNOLOGY, MADRAS, India. A PM-QPSK super- plexed optical communications system is presented. The gration of 2D TMDCs materials on Silicon microring to channel transmission is experimentally demonstrated for design uses off the shelf components and allows better tune the rings resonance as a function of coverage length. 400-Gbps data center interconnects, based on 20-GBd coupling effiency and reduces insertion loss. This hybrid platform can be used for versatile photonic transmitter and coherent receiver technology, yielding a device applications. spectral efficiency of 4-b/s/Hz. JW4A.89 RAPID Quantum Measurement of Time Difference in an Un- JW4A.97 JW4A.82 balanced Fiber Mach-Zehnder Interferometer, Yiwei All-dielectric integrated photonic devices based on Impact of Dispersion on the Relative Cross-Talk of Zhai1,2, Runai Quan1,2, Yue Zhang1,2, Tao Liu1,2, Shougang multimode intereference of Bloch surface waves, WDM Channels in Multicore Fiber Systems., Monica Zhang1,2, Ruifang Dong1,2; 1National Time Service Center, Dmitry N. Gulkin1, Kirill Safronov1, Ksenia Abrashitova1,2, Lopez-Coyote1, Ramon Gutierrez-Castrejon1, Daniel E. China; 2Univ. of Chinese Academy of Sciences, China. We Ilya Antropov1, Aleksandr Frolov1, Vladimir O. Bessonov1, Ceballos-Herrera1; 1Inst. of Engineering, Universidad report a novel way for measuring the time difference in an Andrey A. Fedyanin1; 1Lomonosov Moscow State Univ., Nacional Autónoma de México UNAM, Mexico. We unbalanced fiber Mach-Zehnder interferometer based on Russia; 2mmanuel Kant Baltic Federal Univ., Russia. The report a numerical analysis of the group velocity disper- the second-order quantum interference of the frequency multimode intereference of the Bloch surface wave sion impact on the relative inter-core cross-talk among entangled light source. devices in 1D photonic crystal was experimentally and WDM channels in a two-core fiber transmission system numerically studied. Photonics devises based on this by considering simultaneously Four-Wave Mixing and JW4A.90 phenomena were demonstrated. Stimulated Raman Scattering. A Fiber-Pigtailed Hemispherical Fabry-Pérot Microcav- ity for Accelerometry and Sensing, Feng Zhou1; 1NIST, JW4A.98 JW4A.83 USA. A novel hemispherical Fabry-Pérot microcavity with Highly Sensitive Nanogap-Based Surface Plasmon Method for High-Speed Optical Modulator Characteri- high finesse, good optical performance and compact Resonance Biosensing through Light-Matter Colo- zation Using Only DC Measurements, lam Bui1; 1School packaging is developed for potential applications in calization, Changhun Lee1, Eunji Sim2, Donghyun Kim1; of Engineering and Technology, Central Queensland optomechanical accelerometry and precision sensing. 1Electrical and Electronic Engineering, Yonsei Univ., South Univ., Australia. A novel technique to obtain the frequency Korea; 2Chemistry, Yonsei Univ., South Korea. We present response of high-speed optical modulators is presented. JW4A.91 characteristics of surface plasmon resonance biosensing The proposed technique uses only DC measurements Highly Sensitive Plasmonic Metasensor with Wide with nanogap-based light-matter colocalization. Optical which greatly simplify the setup and reduce the time and Detection Range, Rifat Ahmmed Aoni1, Mohsen Rah- signature was shown to increase by nearly 15 times than cost of device characterization. mani1, Lei Xu2, Rajib Ahmed3, Dragomir Neshev1, Andrey conventional detection with high sensitivity at a relatively Miroshnichenko2; 1Nonlinear Physics Centre, Research large gap. JW4A.84 School of Physics and Engineering, Australian National Modal Analysis of Dielectric Chiral Optical Fibers by Univ., Australia; 2School of Engineering and Informa- JW4A.99 Immersed Interface Method, Yusheng Cao1; 1Ningxia tion Technology, Univ. of New South Wales, Australia; Residual Intensity Modulation Analysis of Multifunction Univ., China. We describe a mode solver for dielectric 3Bio-Acoustic MEMS in Medicine (BAMM) Lab, School Integrated Optic Circuit, Jiaqi Liu1, Chunxi Zhang1, chiral optical fibers, with the immersed interface method of Medicine, Stanford Univ., USA. We propose a highly Jingming Song1, Dewei Yang1, Wei Cai1, Chunxiao Wu1; utilized to treat the discontinuity of medium parameters sensitive plasmonic metasensor for the detection of wide 1Beihang Univ., China. The reasons for residual intensity

across the core-cladding interface, which produce a range of analyte refractive index (RI) from 1 to 1.60. The modulation (RIM) in APE LiNbO3 MIOC are theoretical second order accuracy. proposed metasensor shows the average sensitivity of analyzed. The linear and nonlinear part are evaluated 630 nm/RIU with high linearity of 0.9998. quantitatively. The RIM of a high PER MIOC with spatial JW4A.85 filters is tested. FBG Based Optical Surveillance Network for Oil and JW4A.92 Gas Pipelines, Abhinav Gautam1, Ritu Raj Singh1, Amitesh Non-Reciprocal Transport in Floquet Photonic Reso- JW4A.100 Kumar1, Jaisingh Thangaraj1, Vishnu Priye1; 1Indian Inst. nators: High Frequency Expansion, Huanan Li1, Boris Withdrawn Wednesday, 19 Septem of Technology (ISM), India. A FBG based pipeline surveil- Shapiro2, Tsampikos Kottos1; 1Wesleyan Univ., USA; lance architecture is proposed. An array of FBGs, having 2Technion - Israel Inst. of Technology, Israel. We develop JW4A.101 RAPID unique reflection wavelength is used to spot location of a systematic high-frequency expansion of the scattering Fabrication of Nano Arrays on Chromium Coated Op- any pressure or temperature variation, which is smartly matrix of Floquet periodically-driven photonic systems. tical Fibre Tip, Meher Wan1, Saawan Kumar Bag1, Rajat sensed using optical heterodyning technique. The method unveils the critical role of micro-motion for K. Sinha1, Shailendra Varshney1, B. Lahiri1, chacko Jacob1, non-reciprocal transport in such systems. Cheruvu S. Kumar1; 1Indian Inst. of Technology-Kharagpur, JW4A.86 India. We report the creation of chromium-coated optical Observation of Optical Multistability in directional JW4A.93 fiber meta-tip using Focused-Ion-Beam Lithography. A coupler with negative index material channel, Kanaga- Withdrawn 2D nano array is designed and fabricated on standard raj Nithyanandan2,1; 1Universite de Bourgogne, India; optical fiber tip and supports the localized surface plas- 2Laboratoire Interdisciplinaire de Physique, Universite JW4A.94 mon resonance. de Grenoble Alpes, France. We observe mulistability in Photonic Crystals Band Diagrams Computation by ber directional couplers with negative index material channel. Using Extreme Learning Machine, Adriano da Silva JW4A.102 The emergence of multiple stable states is a result of the Ferreira2, Gilliard N. Malheiros-Silveira1, Hugo E. Her- SPR based fiber optic pH sensor using polyaniline as a action of nonlinear saturation and opposite directionality nandez-Figueroa2; 1São Paulo State Univ. (Unesp), Brazil; sensing layer, Vivek Semwal1, Banshi D. Gupta1; 1Indian of phase velocity and energy flow in the ODC. 2DECOM, Univ. of Campinas, Brazil. We modeled Extreme Inst. of Technology, Delhi, India. In the present work, we Learning Machine feed-forward Artificial Neural Network report a surface plasmon resonance based fiber optic pH JW4A.87 for estimating band diagrams of tri-dimensional photonic sensor utilizing polyaniline as a sensing layer. The sensor Tuning of the Free Spectral Range of a Fiber Optic crystals and demonstrated a simple approach for speedy works for the pH range from 3 to 11. Notch Filter Using a Dispersive Link, Luis A. González computations. Mondragón1, Ignacio E. Zaldívar Huerta1, Leidy J. Quin- JW4A.103 tero Rodríguez1, Ana G. Correa Mena1, Jorge Rodríguez JW4A.95 ULI based single-mode multimode single-mode wave- Asomoza2, Alejandro García Juárez3, Ana L. Leal Cruz3; Improved Acetylene-Filled Photonic Bandgap Fiber guide structure as a highly sensitive refractive index 1INAOE, Mexico; 2UDLAP, Mexico; 3Universidad de Sono- Cells Fabricated using a Tapering Method, Sajed sensor: Design and simulation, Parvinder Kaur1, M. R. ra, Mexico. Theoretical and experimentally is demonstrat- Hosseini1, Manasadevi Thirugnanasambandam1, Kushan Shenoy1; 1Dept. of Physics, Indian Inst. of Technology ed that the free spectral range of a fiber optic notch filter Weerasinghe1, Kristan Corwin1, Brian Washburn1; 1Kansas Delhi, India. We propose the design of a highly sensi- can be tuned by adjusting the length of the optical link. State Univ., USA. Gas-filled photonic microcells (PMC) tive refractive index sensor based on ULI single-mode A series of numerical simulations validate this proposal. have been produced by tapering the end of photonic multimode single-mode waveguide structure. The VE bandgap fibers. This method improves cell transmission multimode waveguide sensor has refractive index sen- and reduces etalon-like effect. PMC contamination was sitivity ~ 104 nm/RIU. determined by fitting the measured absorption lines.

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JW4A.104 JW4A.111 JW4A.117 Transmission Control in Photonics Crystal Slab Using Optical Sum Frequency Generation Spectroscopy and High-throughput Light Sheet Tomography Platform Transparent Conductive Oxide, Vishal Vashistha1, An- Microscopy of Starch in Rice Grain as a Function of for Fast Imaging of Whole Mouse Brain, Xiong driy Serebryannikov1, Maciej Krawczyk1; 1Physics, Adam Developing Stage, Akira Matsubara1, Goro Mizutani1, Yang1, Qi Zhang1, Fei Huang1, Longhui Li1, Yongsheng Mickiewicz Univ. in Poznan, Poland. We proposed to Khuat Thi Thu Hien1, Wataru Kouyama1, Sultana Sharmin1, Zhang1, Xiaofeng Cheng1, Shaoqun Zeng1, Xiaohua Lv1; control the propagation of light through PhC slab by Yasunori Nakamura2; 1Japan Adv. Inst. of Sci. and Tech., 1Huazhong Univ. of Science and Technology, China. Here imposing a lossy boundary condition from the direction Japan; 2Akita Prefectural Univ., Japan. The change of we develop a high-throughput light-sheet tomography perpendicular to plane of propagation using transparent the molecular structure of sugar chains in rice seeds at platform (HLTP), by which an aligned three-dimensional conducting oxides. different growth stages after flowering using a confocal image dataset of a whole mouse brain can be obtained sum frequency generation microscope. The starch struc- within 5 hours. JW4A.105 ture in the developing rice endosperm was estimated ITO-Si heterojunction solar cell with nanocrystal line by SFG spectra. JW4A.118 CdTl thin films, Andrii Pocherpailo1, Sergii Kondraten- Enhanced Discrimination of Cervical Cancer by Applica- ko1; 1Taras Shevchenko National Univ., Ukraine. ITO-Si JW4A.112 tion of PCA with SVM on Time-Resolved Fluorescence heterojunction solar cell with nanocrystal line CdTe thin Quantitative Analysis of Glucose Concentration Using Decay, Gyana Sahoo1, Asima Pradhan1,2; 1Physics, Indian films grown by magnetron sputtering is studied. The NIR Spectroscopy, Selvy U. Hepriyadi1, Iwan C. Setiadi1, Inst. of Technology Kanpur, India; 2CELP, Indian Inst. of electrical and optical properties of these solar cell de- Aulia Nasution1; 1Engineering Physics, Institut Teknologi Technology Kanpur, India. Time-resolved fluorescence vices were studied by current–voltage and photovoltage Sepuluh Nopember, Indonesia. The quantitative evalu- decay of normal and abnormal cervical tissue is seen to spectroscopy. ations were carried out using PLS model. The collected display better discrimination on application of PCA, which absorbance data was pre-processed before calibration. captures subtle changes in fluorophore environment and JW4A.106 From the data acquisition, it can be obtained the good the application of SVM quantifies the discrimination. Effects of spectral shift on ultrashort pulse propa- model for predicting glucose concentration. gation in AZO/ZnO multilayered metamaterials at JW4A.119 epsilon-near-zero, Priscilla Kelly1, Lyuba Kuznetsova1; JW4A.113 A White Random Laser, Chia-Tse Tai1, Yu-Ming Liao1, 1San Diego State Univ., USA. Numerical FDTD study of A Custom Multi-Pixel Photodetector Probe and Partial Shu-Wei Chang1, Wei-Cheng Liao1, Shih-Yao Lin1, Wei-Ju ultrashort (100 fs) pulse propagation shows strong pulse Least Squares Regression for the Efficient Identifica- Lin1, Cheng-Han Chang1, Hung-I Lin1, Packiyaraj Perumal1, shaping for central frequencies smaller than the epsi- tion of Optical Tissue Properties, Callie M. Woods1, Golam Haider1, Tai-Yuan Lin1, Yang-Fang Chen1; 1National lon-near-zero (ENZ) point, and soliton-like propagation Ozlem Senlik1, Nan M. Jokerst1; 1Electrical and Computer Taiwan Univ., Taiwan. The hope of next-generation illu- (up to 500 nm) for central frequencies larger than ENZ. Engineering, Duke Univ., USA. Diffuse reflectance spec- minants goes on random laser. Random laser is naturally troscopy performed using a custom photodetector array endowed with two key superiorities, namely, laser-level JW4A.107 combined with partial least squares regression increases intensity and broad-angular emissions, which are mutually Rectangular Waveguide based SOI Toluene Gas Sensor, the accuracy of optical tissue property extraction. Pre- exclusive in common light sources and lasers. 1 1 1 Anumeha Varma , Dhananjoy De , Ritu Raj Singh , Vishnu diction accuracies of 4.15% (us), 9.02% (ua) are reported. Priye1; 1Indian Insttitute of Technology, Dhanbad, India. JW4A.120 The Silicon on insulator (SOI) rectangular waveguide as a JW4A.114 RAPID Lens free microscope with an Arduino monochrome toluene gas sensor is designed. Change in confinement Near-real time evaluation of live and dead bacterial camera module, Camila de Paula D’Almeida1, Patrick factor and sensitivity of the sensor against the low fraction concentration using the optrode – a portable fluo- Oliveira Feitosa1, Sebastião Pratavieira1; 1Instituto de of toluene is reported at 1550nm operating wavelength. rimeter, Fang Ou1, Cushla McGoverin1, Simon Swift2, Física de São Carlos (IFSC), Brazil. Lens free microscope Frédérique Vanholsbeeck1; 1The Dodd-Walls Centre for is an emerging portable and simple image device. In this JW4A.108 Photonic and Quantum Technologies, Dept. of Physics, paper, we present our version of this microscope, which Surface Plasmon Resonance as a biosensing technique The Univ. of Auckland, New Zealand; 2School of Medical make use of an Arduino camera module. for possible development of a point of care diagnostic Sciences, The Univ. of Auckland, New Zealand. We tool., Rudzani Malabi1,2, sello Manoto1, Saturnin Ombin- describe a method to determine live and dead bacterial JW4A.121 daLemboumba1, Patience Mthunzi-Kufa1; 1CSIR National concentration that take advantage of an inexpensive Purity Analysis of Adulterated Vegetable Oils by Ra- Laser Centre, South Africa; 2Physics, UNISA , South fibre-based fluorimeter, the optrode, which can measure man and FTIR Spectroscopy, Shyju Bhaskar1, Spandana Africa. Surface Plasmon Resonance is an optical sensing fluorescence intensity in bacterial solutions in challenging K. U1, Krishna K. Mahato1, Nirmal Mazumder1; 1Manipal technique with the ability to monitor molecular binding in working environments. Academy of Higher Education, India. Raman and Fourier ber real-time for biological and chemical sensing applications. transfer infrared (FTIR) spectroscopy have been used to JW4A.115 compute the purity and investigate the adulteration in JW4A.109 Two-photon fluorescence microscopy and selective edible oils which are commonly used. Instantaneous Quantum Description of Photonic laser ablation through multimode fibers, Eirini Kak- Wavefronts for Phase-Sensitive Amplification, Andre kava1, Donald Conkey1, Damien Loterie1, Christophe JW4A.122 Vatarescu1; 1R&D, Fibre-Optic Transmission of Canberra, Moser1, Demetri Psaltis1; 1Ecole Polytechnique Federale Dual Pulsed Laser Stimulation to the Auditory Nerve Australia. Pure photonic quantum states consist of two de Lausanne, Switzerland. Using wavefront shaping, we in Vivo, Muqun Yang1, Tian Guan1, Yonghong He1; consecutive number states, enabling evaluation of instan- deliver a focus spot through a multimode fiber (MMF) 1Graduate School at Shenzhen, TSINGHUA UNIV., taneous amplitudes and phases of wavefront distributions with a maximum peak power of ~1x1013W/cm2, sufficient China. We demonstrated a system of dual pulsed laser of photons Sub-Poissonian distributions are shaped to perform two-photon fluorescence (TPF) imaging and stimulation could successfully induce auditory response. without the need for quasi-probabilities. laser ablation (LA) of a variety samples. We analyze its characterization and mechanism for future artificial cochlea. Wednesday, 19 Septem Wednesday, JW4A.110 JW4A.116 Optical Responses of Asymmetrical Ag Nano-par- Simultaneous Two-layer Two-photon Imaging with JW4A.123 ticles in Graphene Environment, Shivani Bhardwaj1, Confocal Strategy, Qinglei Hu1, Pei Li1, Yu Wang1, Yumaio Displaying 3D Images on Mobile Phones, Nikolai I. R.P. Sharma1; 1Indian Inst. of Technology, Delhi, India. Xiong1, Xiaohua Lv1, Shaoqun Zeng1; 1Huazhong Univ. of Petrov1, Vladislav G. Nikitin1, Yuri Sokolov1, Maxim Khro- Scattering and absorption efficiencies of the Oblate and Science and Technology, China. To simultaneously record mov1; 1Scientific and Technological Center of Unique ortho-Oblate Ag nano-particles has been calculated by images from two planes at different axial positions, a Instrumentation of Russian Academy of Sciences, Russia. the numerical experiment named as Discrete Dipole Ap- two-photon imaging method was proposed in which Multiview 3D display system consisting of mobile phone proximation (DDA) against the quasi-static approximation signal demultiplexing is implemented using confocal screen and optical screen consisting of microlens array in Graphene environment. strategy. film is designed. 3D image files are created and images are demonstrated on different smartphones with high resolution displays.

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JW4A.124 RAPID JW4A.130 JW4A.138 Automatic snow grain size measurement method Passively Q-switched Laser Performance of Nd :Gd Sub-Rayleigh Limit Localization with a Spatial Mode 0.01 0. 1 1 1 3 based on adaptive minimum circumscribed rectangle, La NbO Mixed Crystal, Haiyue Sun , Yufei Ma , Analyzer, Jeremy Hassett , Tanya Malhorta , Miguel 89 0.1 4 1 1 1 1 2 1 1 2 Alonso1, Robert Boyd1,2, Mohammad Hashemi Rafsanja- Xintong Fan , Lingjia Gu , Ruizhi Ren , Haoyang Fu ; Shoujun Ding , Zhenfang Peng , Ying He , Fang Peng , 1 1 2 1 ni1, Anthony N. Vamivakas1,3; 1Optics, Univ. of Rochester, Jilin Univ., China. Snow grain size affects the brightness Xin Yu , Qingli Zhang ; Harbin Inst. of Technology, 2 USA; 2Physics, Univ. of Ottawa, Canada; 3Physics, Univ. temperature of snow. At present, snow grain size is mainly China; Chinese Academy of Sciences, Hefei , China. of Rochester, USA. A spatial mode analyzer based on a based on manual measurement. In this paper, a method Diode-pumped continue-wave and passively Q-switched of automatic snow grain size measurement is proposed. lasers with novel Nd :Gd La NbO mixed crystals generalized Michelson interferometer is applied to the 0.01 0.89 0.1 4 estimation of sub-Rayleigh limit incoherent point source were demonstrated. The maximum peak power was separations. Proof-of-principle experimental measure- JW4A.131 1.13 kW with the pulse width of 32 ns and the repetition ments of a single shifted source are presented. Three-Dimensional Digital Reconstruction Methodol- rate of 24.5 kHz. ogy Specialized in Human Skulls, Andrés L. González1, 1 1 JW4A.125 RAPID Jaime E. Meneses ; Universidad Industrial de Santander, JW4A.139 Rapid detection of variability and adulteration of diesel Colombia. This paper presents a three-dimensional Quantum-Classical Intersection from Perspective of oils, Boniphace E. Kanyathare1, Buratin Khampirat2, Kai E. reconstruction strategy (3DR) specialized in the digital Spatially-Resolved Intensity Interferometry, Piotr F. We- 1 1 1 1 Peiponen3, Boonsong Sutapun1; 1Electronic Engineering, reconstruction of Human Skulls. The strategy is based grzyn , Lukasz Zinkiewicz , Radek Lapkiewicz ; Faculty of Suranaree Univ. of Technology, Thailand; 2School of Gen- on the fringe projection technique. Physics, Univ. of Warsaw, Poland. We present an extension eral Education, Inst. of Social Technology, Suranaree Univ. to the intensity interferometry, which is an example of the of Technology, Thailand; 3Physics and Mathematics, Univ. JW4A.132 intersection of quantum and classical theory. We believe of Eastern Finland, Finland. Adulteration and smuggling Shadow Detection and Removal from Buildings in UAV that obtained results would contribute to deeper under- 1 1 1 of diesel oils are serious problems. Vis-NIR and PCA Data, Tingting Zhou , Haoyang Fu ; Jilin Univ., China. standing of correspondence between those theories. were applied to study samples from same oil fields and Considering the problem that UAV data is susceptible refinery process. Variability and adulteration were both to shadow interference, shadow detection and removal JW4A.140 detected rapidly. algorithms are used for buildings in UAV data in this paper. Dinamic Laser Speckle applied to the determination of the specific surface area of clays, Ruth D. Mojica 1 2 JW4A.126 JW4A.133 Sepulveda , Mendoza Herrera Luis Joaquin , Bertolini 3 3 1 Weak-measurement-enhanced Metrology in the Low-rank Constrained Image Enhancement For Ghost Guillermo , Cabello Carmen I. , Soria Delia B. , Trivi 1 1 1 2 1 2 Presence of CCD Noise and Saturation, Liang Xu1, Imaging., Tiaohua Li , Bin Luo , Dongchu Han , Junhui Marcelo ; CEQUINOR, Argentina; Centro de Investi- 1 1 1 2 1 3 Zexuan Liu1, Lijian Zhang1; 1Nanjing Univ., China. We Li , Dongyue Yang , Guohua Wu , Hong Guo ; Beijing gaciones Ópticas, Argentina; Centro De Investigacion 2 experimentally demonstrate that the measurement using Univ of Posts & Telecom, China; Peking Univ., China. Y Desarrollo En Ciencias Aplicadas, Argentina. Dynamic weak value amplification offers metrological advantages Low-rank constraint improves image quality of ghost laser speckle (DLS) is proposed as a complementary over the conventional measurement in the presence of imaging, for both correlation and compressive sensing technique to determine the specific surface area of classical noise and detection saturation with a generic approaches.Image by correlation plus low-rank constraint natural and chemically modified bentonite. To verify this scientific CCD. can even surpass that by compressive sensing when approach, we compared DLS technique with the standard under-sampling. physicochemical methods. JW4A.127 Naked-Eye Full-Screen Resolution Stereoscopic Im- JW4A.134 JW4A.141 aging Based on Amplitude-Polarization Imager and Image compression in real-time holographic projection Relativistic Single-Cycle Tunable Infrared Pulses Gen- 1 1 Passive Distant Binocular Filter with Complementary in color, Paula A. Kochanska , Michal Makowski , Izabela erated from a Tailored Plasma Density Structure, Zan 1 1 1 1 1 1 2 Liquid Crystal Layers, Vasily A. Ezhov1, Peter Ivashkin1, Ducin , Karol Kakarenko , Jaroslaw Suszek , Marcin Bie- Nie , Chih-Hao Pai , Jianfei Hua , Chaojie Zhang , Wei 1 1 1 1 3 3,4 2 Alexander Galstian1; 1GPI RAS, Russia. The described da , Adam Kowalczyk ; Faculty of Physics, Warsaw Univ. Lu , Hsu-Hsin Chu , Jyhpyng Wang , Warren Mori , 2 1 2 method of the naked-eye stereoscopic imaging is of Technology, Poland. In the paper we present holo- Chan Joshi ; Tsinghua Univ., China; Univ. of California 3 4 flicker-free at 60 Hz frame rate due to simultaneous re- graphic projection system used in holographic real-time Los Angeles, USA; National Central Univ., Taiwan; Inst. producing both full-screen view images. High separation transmission in color between Poland and Japan. We of Atomic and Molecular Sciences, Academia Sinica, discuss visually-lossless data compression of CGH on the Taiwan. A new scheme capable of generating tunable

contrast is due to complementarity of LC layers of the Wednesday, 19 Septem imager and the filter. fly with client-adjustable compression ratios. relativistically intense, single-cycle pulses in the spectral range of 5-14 μm with a 1.7% conversion efficiency JW4A.128 JW4A.135 through asymmetric self-phase modulation in a tailored Using adaptive window and non-uniform sampling Imaging Through Scattering Layers with Extention of plasma density structure is proposed. model to improve autofocusing performances, Jie Memory Effect Range Driven by Prior Information, 1 1 1 1 Cao1, Yuqing Xiao1, Qun Hao1, Yang Cheng1; 1School Wei Li , Jiannan Wang , Jietao Liu , Xueying Sun , Guo 1 1 1 of Optics and Photonics, Beijing Inst. of Technology, Chengfei , Xiaopeng Shao ; Xidian Univ., China. We China. An adaptive autofocusing method based adaptive demonstrate numerically and experimentally that by sampling window and non-uniform sampling model is exploiting a known object, or even a point as prior in- proposed. Model verification is carried out. The autofocus formation, the speckle correlation imaging method can time under 8× using Laplacian (LAP) autofocus function be used to observe the extended object exceeding the reduces from 1670ms to 1240ms. memory-effect range. ber

JW4A.129 JW4A.136 Large field of view imaging based on compound and Imaging through haze utilizing a multi-aperture coaxial 1 1 1 human hybrid eye using non-uniform curved microlens polarization imager, Xuan Li , Pingli Han , Fei Liu , Yi 1 1 1 array, Yang Cheng1, Jie Cao1, Fanghua Zhang1, Qun Hao1; Wei , Xiaopeng Shao ; Xidian Univ., China. This study 1Beijing Key Lab. for Precision Optoelectronic Measure- focused on a polarization-based dehazing technology ment Instrument and Technology, School of Optics and based on the multi-aperture coaxial polarization imager. Photonics, Beijing Inst. of Technology, China. A large field By solving the image displacement problem accompanied of view (FOV) imaging system based on compound and with the imager, instant polarization dehazing is possible. human hybrid eye using non-uniform curved microlens array is proposed. Model verification is carried out. The JW4A.137 FOV of this system is up to 96°. Intramolecular Charge Transfer Probed by Femto- second Stimulated Raman Spectroscopy, Sebok Lee1, Myungsam Jen1, Kooknam Jeon1, Joonwoo Kim1, Yoon- soo Pang1; 1Gwangju Inst of Science & Technology, South Korea. Distinct Raman spectra of the locally excited and charge transferred conformers of DCM were resolved from femtosecond stimulated Raman measurements and a twisted geometry was proposed for the intramolecular charge transfer state.

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15:00–16:30 15:00–16:30 15:00–16:30 FW5A • AR and VR Ecosystems FW5B • Optical Communications FW5C • Quantum Systems Developments Presider: Greg Raybon; Nokia Bell Labs, Presider: Gordon A. Keeler; DARPA, USA Presider: Jim Melzer; Thales Visionix; USA USA

FW5A.1 • 15:00 Invited FW5B.1 • 15:00 Invited FW5C.1 • 15:00 Invited The Opportunities and Challenges of Creating Artificial Rate-Adaptive Modulation Schemes for High Spectral A Dissipative Phase Transition in a Two-photon-driven Perception Through Augmented and Virtual Reality, Efficiency Optical Communications, Junho Cho1, Sethu- Array of Kerr Resonators, Vincenzo Savona1; 1Ecole Barry Silverstein1; 1Optics and Display, Facebook Reality madhavan Chandrasekhar1, Peter J. Winzer1; 1Nokia Bell Polytechnique Federale de Lausanne, Switzerland. We Labs., USA. Researchers are beginning to create and de- Labs, USA. We review various rate-adaptive modulation show that an array of coupled Kerr resonators, with liver realistic artificial human inputs. These inputs of sight, schemes for optical communications that maximize the two-photon drive and dissipation, behaves as a quantum sound, motion, and touch are being woven together into spectral efficiency for any channel condition, and analyze simulator of the quantum XY spin model with transverse virtual and augmented reality systems than can emulate their benefits and weaknesses. field. We study the associated quantum phase transition convincing human perception. and its universality class.

FW5A.2 • 15:30 Invited FW5B.2 • 15:30 FW5C.2 • 15:30 Smart Glasses and AR Headsets for Enterprise and Ultra-wideband parametric amplification in telecom Implementing Majorana Fermions in a Cold-Atom Consumer Markets, John Haddick1; 1Osterhout Design wavelengths with an optimally mode-matched PPLN Honeycomb Lattice with Textured Pairings, Ruizhi 1 1 1 1 1 Group, USA. Abstract not available. waveguide, Yong Meng Sua , Jia-Yang Chen , Yu-Ping Pan , Charles Clark ; Univ. of Maryland, College Park, Huang1; 1Stevens Inst. of Technology, USA. Ultra-wide- USA. We propose a model to create unpaired Majorana band parametric amplification over 14 THz in the telecom fermions at one edge of a pseudospin-state dependent, band is realized via cascaded nonlinear processes in an time-reversal symmetry noninvariant honeycomb lattice optimally mode-matched PPLN waveguide. With a tai- by generalizing a topologically nontrivial Haldane model lored waveguide cross-section, we observe a maximum and introducing textured pairings. gain of 38.3 dB.

FW5B.3 • 15:45 FW5C.3 • 15:45 Generation of Phase-correlated Parametric Frequency Self-trapping of light via the Pancharatnam-Berry Combs Spaced at 10GHz Based on Injection Locking, phase, Chandroth P. Jisha2, Alessandro Alberucci1, Stefan Jing Chen1, Juanjuan Yan1, Linnan Li1; 1Beihang Univ., Nolte1,3; 1Friedrich-Schiller-Universitat Jena, Germany; China. We demonstrate a phase-correlated parametric 2Universidade do Porto, Portugal; 3Fraunhofer Inst. of frequency comb generator using injection locking. A Applied Optics and Precision Engineering, Germany. We frequency comb spaced at 10GHz is experimentally discover a new type of light self-trapping based upon the generated in a span of 3nm. Pancharatnam-Berry phase. These waves need a rotation of the optical axis dependent on the input light intensity, such as liquid crystals.

FW5B.4 • 16:00 FW5C.4 • 16:00 FW5A.3 • 16:00 Invited Scaling Bandwidths of Optical Frequency Combs Light Superfluidity in Hot Atomic Vapors, Quentin The Age of Light: From an Electronic to a Photonic Generated in Silicon Modulators through Heterodyne Fontaine1, Alberto Bramati1, Quentin Glorieux1, Tom Society, 1,2 1 Tish Shute ; Dir. AR/VR, Huawei, USA, USA; Optical Frequency Locking., Nagarjun KP1, Vikram B.S.1, Bienaimé1; 1Laboratoire Kastler Brossel, France. We 2 Co-Founder, Augmented World Expo & Augmented Roopa Prakash1, Vadivukkarasi Jeyaselvan1, Shankar K. investigate the dispersion relation of small amplitude Reality Org, USA. This talk will look at the transformation Selvaraja1, Supradeepa V.R.1; 1IISc, Bangalore, India. We density waves propagating on top of a photon fluid. We from Electronics to Photonics and the important role demonstrate bandwidth-scaling of frequency combs also present two ongoing experiments to study dispersive AR/VR/MR will play in creating a Photonic Society and ber in silicon charge-injection modulators by linking two shock waves and observe superfluidity of light. a better life for all. 10GHz combs (8 lines) through heterodyne optical fre- quency-locking within 6.6MHz resulting in a broadened comb of 13 lines in a 30dB band.

FW5B.5 • 16:15 FW5C.5 • 16:15 Free-Space Optical Stealth Communication Based Goos-Hänchen shift in a two-dimensional atomic on Wideband Noise, Yang Qi1, Ben Wu1; 1Electrical & crystal, Michele Merano1; 1Universita degli Studi di Computer Engineering, Rowan Univ., USA. We demon- Padova, Italy. It is widely known that the Goos–Hänchen strate a free-space optical (FSO) stealth communication shift in three dimensional materials is proportional to system to protect the privacy of FSO channels. The signal the wavelength of the incident light. In freestanding is hidden in the phase randomness of wideband optical two-dimensional crystals instead, it is proportional to

Wednesday, 19 Septem Wednesday, noise generated by spontaneous emission. their surface susceptibility.

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15:00–16:30 15:00–16:30 15:00–16:30 FW5D • Quantum Sensing for Industry and FW5E • Plasmonic and Nanophotonic LW5F • Novel Lasers, Plasmonics, Fundamental Physics II Materials Nanophotonics II Presider: To be Determined Presider: Mercedeh Khajavikhan; University Presider: Federico Capasso; Harvard of Central Florida, USA University, USA

FW5D.1 • 15:00 Invited FW5E.1 • 15:00 Invited LW5F.1 • 15:00 Invited Commercialization of Quantum Sensing Technologies, The Next Generation of Colloidal Quantum Emitters Infrared Nanophotonics Based on Phonon Polaritons in 1 1 1 1 Nils Hempler ; M Squared Lasers, UK. The presentation for Nanophotonics and Plasmonics, David Norris1; 1ETH Boron Nitride , Rainer Hillenbrand ; Nanogune, Spain. will describe M Squared’s mission to transfer the demon- Zurich, Switzerland. New quantum emitters with improved Thin hexagonal boron nitride layers host ultra-confined strated potential of quantum technologies from lab based properties for nanophotonics will be discussed. Examples and long-lived phonon polaritons, which allow for ma- demonstrator systems to fully engineered products that include lanthanide-doped nanocrystals, semiconductor nipulating mid-infrared light on the nanometer scale. will benefit a wide range of industries. nanoplatelets, and perovskite nanocrystals. We discuss our recent progress including phonon-en- hanced molecular vibrational sensing and hyperbolic metasurfaces.

FW5D.2 • 15:30 Invited FW5E.2 • 15:30 LW5F.2 • 15:30 Invited Time for Quantum Technologies: Optical Clocks for Purcell Enhancement in 1-D ITO-slot Photonic Crystal Resolving Multipolar Transitions and Directional 1 Users, Stephan Ritter1; 1TOPTICA Photonics, Germany. Nanobeam Cavity, Rubab Amin , Mohammad H. Ta- Metasurface Light Emission with Momentum-Resolved 1 1 1 1 1 High-precision clocks are one of the first and most prom- hersima , Zhizhen Ma , Can Suer , Ke Liu , Rishi Maiti , Spectroscopy, Jon Schuller1; 1Univ. of California Santa 1 1 inent examples of quantum technology. Optical clocks Volker J. Sorger ; The George Washington Univ., USA. Barbara, USA. In momentum-resolved spectroscopy, employ narrow-band optical transitions in atoms or ions as We report Si-slot waveguide with active-ITO layer 1D researchers measure or control light’s momentum content. frequency standards, with applications ranging from syn- photonic crystal nanobeam cavity delivering 3.4 nm tun- Using momentum-resolved spectroscopy, we demon- chronization and navigation to the measurement of height ing keeping Q-factor moderately high. The subdiffraction strate multipolar light emission in layered perovskites and 3 differences. As with other quantum technologies, optical limited mode volume (0.1(λ/2n) ) facilitates a high Purcell directional light emission in GaN metasurfaces. clocks have to be brought out of the laboratory and into factor exceeding 4000. the hands of users in order to exploit their full application potential. To this end, a consortium of six companies, FW5E.3 • 15:45 two universities, one research and one federal institute Interactions of Hexagonal Boron Nitride with the have teamed up to realize a robust, long-lasting and Insulator-Metal Phase Transition in Vanadium Dioxide, easy-to-use demonstrator device for an optical single-ion Samuel T. White1, Alireza Fali2, Thomas G. Folland3, Josh- clock. The project, led by TOPTICA Photonics and the ua D. Caldwell3, Yohannes Abate2, Richard F. Haglund1; Physikalisch-Technische Bundesanstalt (PTB) and partially 1Vanderbilt Univ., USA; 2Physics, Univ. of Georgia, USA; funded by the German Federal Ministry of Education and 3Mechanical Engineering, Vanderbilt Univ., USA. Phonon Research, will run for three years. It will on the one hand polaritons in hexagonal boron nitride (hBN) reflect and help to transfer scientific research results into industry and refract at phase domains in underlying vanadium dioxide on the other hand leverage industrial expertise in project (VO2) crystals, a potential reconfigurable metasurface. management, engineering, and system integration. In the Also, hBN slows the VO2 phase transition via thermal talk, we will give an overview of the clock system and ex- or strain effects. plain how the necessary development of key technologies will also benefit other quantum technologies. Related FW5E.4 • 16:00 LW5F.3 • 16:00 Invited developments at TOPTICA will be sketched and we will MIR spin angular momentum detection by a chiral Plasmonic Metasurfaces: Combinatorial Colors and review how this fits into the broader picture of a primarily 1 graphene plasmonic nanostructure, Jingyang Peng , High-Speed Photodetection, Maiken Mikkelsen1; 1Duke quantum-enabling company. 1 1 1 Benjamin P. Cumming , Min Gu ; School of Science, Univ., USA. Plasmonic film-coupled nanocubes are used RMIT Univ., Australia. A graphene-chiral plasmonic to demonstrate large-area perfect absorbers, pixel arrays nanostructure photodetector that can detect MIR spin and ~10,000 combinatorial colors. By integrating a py- Wednesday, 19 Septem angular momentum (SAM) has been designed, modelled roelectric thin-film, we also demonstrate a high-speed, and fabricated. We demonstrate circular dichroism of spectrally-selective thermal photodetector operating at 30% and absorption of 65% at a wavelength of 3.9 µm. room temperature.

FW5E.5 • 16:15

Active photonic integrated circuits combining Si3N4 microresonators with 2D materials for applications in the visible wavelength range, Clément Javerzac-Galy1, Junqiu Liu1, Arslan S. Raja1, Tobias Kippenberg1, Dome- 2 2 2

nico De Fazio , Alisson Cadore , Ioannis Paradeisanos , ber Giancarlo Soavi2, Gang Wang2, Andrea Ferrari2; 1Ecole Polytechnique Federale de Lausanne, Switzerland; 2Cambridge Graphene Centre, Univ. of Cambridge, UK. We present air-cladded silicon nitride microresonators at visible wavelengths compatible with 2D material transfer, fabricated using the photonic Damascene reflow process. Quality factors of 1 million have been measured at 765 nm.

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16:45–18:45 16:45–18:15 16:45–18:15 FW6A • New Optical Hardware is Key to FW6B • Novel Optical Fibers and FW6C • Solid State Quantum Optics Next Generation AR and MR Modulators Presider: Vincenzo Savona; Ecole Presider: Patricia Shute; Huawei, USA Presider: Lyuba Kuznetsova; San Diego Polytechnique Federale de Lausanne, State University; USA Switzerland

FW6A.1 • 16:45 Invited FW6B.1 • 16:45 Invited FW6C.1 • 16:45 Invited Recreating Reality: Enabling Immersive VR/AR Expe- High Performance Chalcogenide Photonic Crystal Deterministic Coupling of Quantum Emitters in 1 1 rience on Mobile Platforms, Behnam Bastani ; Oculus, Fibers Pumped in the Short Wave Infrared, Camille-So- Two-dimensional Materials to Optical Cavities, Stefan 1 1 USA. The talk outlines how a full system integration, from phie Bres ; Ecole Polytechnique Federale de Lausanne, Strauf1; 1Stevens Inst. of Technology, USA. We review our content creation, to transmission to display optics play an Switzerland. We present recent advances in Chalcogenide recent work on deterministic coupling of site controlled important role on delivering an immersive experience in photonic crystal fibers for use in the short wave infrared. quantum emitters in WSe2 to plasmonic nanocavities as head-mounted displays. It highlights the challenges in the Results on fiber quality, nonlinear parametric effects and well as integration schemes for quantum emitters in boron industry especially as customer would like to have a more supercontinuum generation are covered. nitride to metallo dielectric antennas. realistic experience on standalone devices.

FW6A.2 • 17:15 Invited FW6B.2 • 17:15 FW6C.2 • 17:15 Photonic crystal fiber metalensenabled by geometric Charge-Tunable Quantum Dots in Monolayer WSe , Meta-Resonant Waveguide-Gratings - Monochromatic 2 1 1 1 1 1 Diffraction to AR, Guillaume Basset1; 1Resonant Screens, phase optical metasurfaces, Jingyi Yang , Indra Ghimire , Mauro Brotons-Gisbert , Artur Branny , Santosh Kumar , 2 1 1 1 1 1 1 Switzerland. Meta-Resonant Waveguide-Gratings can Pin Chieh Wu , Sudip Gurung , Catherine Arndt , Din Ping Raphael Picard , Raphael Proux , Brian Gerardot ; Her- 2 1,3 1 be engineered to have selective and tunable diffraction, Tsai , Howard Lee ; Dept. of Physics, Baylor Univ., USA; iot-Watt Univ., UK. We demonstrate Coulomb blockade 2Research Center for Applied Sciences, Academia Sinica, in monolayer WSe quantum dots. Further, gate tunable while being manufactured with high throughput meth- 2 3 ods. This enables new optical combiners for AR being Taiwan; The Inst. for Quantum Science and Engineering, hybridization of the localized and continuum of electron affordable, compact and providing a better immersion. Texas A&M Univ., USA. We demonstrate an in-fiber chro- states in a Fermi sea is observed due to strong tunnel matic metalens that can focus light upon exiting the fiber interaction. with numerical-aperture of 0.3714 at wavelength of 1550 nm by integrating geometric phase metasurface on the end-facet of photonic crystal fiber.

FW6B.3 • 17:30 FW6C.3 • 17:30 Virtual Draw of Tubular Hollow-Core Fibers, Gregory T. A Silicon Photonic On-Chip Filter for Quantum Emit- Jasion1, John R. Hayes1, Natalie V. Wheeler1, Yong Chen1, ters, Shahriar Aghaeimeibodi1, Je-Hyung Kim2, Mustafa Thomas D. Bradley1, Reza Sandoghchi1, Marco Petrovich1, Atabey Buyukkaya1, Chang-Min Lee1, Christopher J. Rich- Francesco Poletti1, David Richardson1; 1Optoelectronics ardson3, Richard P. Leavitt3, Edo Waks1,4; 1Electrical and Research Centre, Univ. of Southampton, UK. A numerical Computer Engineeering, Univ. of Maryland, USA; 2Dept. model that accurately predicts the fabricated geometry of of Physics, Ulsan National Inst. of Science and Technology, tubular hollow-core fibers is presented and experimentally South Korea; 3Lab for Physical Sciences, Univ. of Maryland, 4 ber validated. Such a model can be invaluable in driving USA; Joint Quantum Inst., Univ. of Maryland, USA. We design decisions for yield upscaling and loss reduction. demonstrate on chip filtering of single photons using a hybrid integrated device that contains III/V quantum dots and a silicon-on-insulator photonic disk resonator.

FW6A.3 • 17:45 Invited FW6B.4 • 17:45 FW6C.4 • 17:45 Is LCOS the Display of Choice for AR?, Poking Li1; Composite Material Hollow Core Optical Fiber Elec- Enhancing Two-Photon Emission From Epitaxially 1 1 1Himax, Taiwan. Abstract not available. tro-Modulation, Adam Lewis , Francesco De Lucia , Grown Quantum Dot With Nanoantennas, Andrzej Walter Belardi1, Chung-Che Huang1, John R. Hayes1, Gajewski1, Karolina Slowik1, Jakob Straubel2, Carsten Francesco Poletti1, Dan Hewak1, Pier Sazio1; 1Univ. of Rockstuhl2; 1Nicolaus Copernicus Univ., Poland; 2Karlsruhe Southampton, UK. We demonstrate the integration of Inst. of Technology,, Germany. We present the result of the Transition Metal Dichalcogenide (TMDC) materials broad analysis of enhancement and control of emission of

Wednesday, 19 Septem Wednesday, WS2 and MoS2 into hollow core anti-resonant fibers. an entangled two-photon pair from the epitaxially grown We show the potential to use such structures as all fiber quantum dot (InAs/InP) by the mean of nanoantennas. electro-optical modulators.

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16:45–18:15 16:45–18:15 16:45–18:15 FW6D • Quantum Computing with Atoms FW6E • Meta- and Nanophotonic Devices LW6F • Novel Lasers, Plasmonics, and Photons I for Imaging and Applications Nanophotonics III Presider: To be Determined Presider: David Norris; ETH Zurich, Presider: Andrea Alu; University of Texas at Switzerland Austin, USA

FW6D.1 • 16:45 Invited FW6E.1 • 16:45 Invited LW6F.1 • 16:45 Photonic Integrated Circuits for Scalable Quantum Medical Device Applications of Silicon Photonics, Roel Active-Cavity Optomechanics: A Self-Cooling Laser, 1 1 1 Networks, Dirk Englund1; 1MIT, USA. Photonic integrat- G. F. Baets1, Yanlu Li1; 1Ghent Univ., INTEC and IMEC, Bel- John Lawall , Adarsh Ganesan , Justin Foley , Weijian 2 3 1 2 ed circuits (PICs) have become increasingly important gium. Silicon photonics enables compact and cost-effec- Yang , Christopher Chase ; NIST, USA; Electrical and in classical communications applications over the past tive photonic integrated circuits, based on manufacturing Computer Engineering, Univ. of California at Davis, 3 decades, including as transmitters and receivers in in CMOS fabs. It can serve point-of-care medical device USA; Bandwidth 10, Inc., USA. We demonstrate inter- long-haul, metro and datacenter interconnects. Many of applications. Here we focus on multi-beam laser Doppler ferometrically that a laser with a mechanically compliant the same attributes that make PICs attractive for these vibrometry circuits for cardiovascular disease monitoring. output coupler can optically self-cool its fundamental applications — compactness, high bandwidth, and the mechanical mode from room temperature to an effective ability to control large numbers of optical modes with temperature of 30 K. high phase stability — also make them appealing for quantum information processing. The first part of this LW6F.2 • 17:00 talk will review our recent progress in adapting one of the Quantum-Well Diode Lasers for Frequency Comb 1 1 leading PIC architectures—silicon photonics—for various Generation, Mark Dong , Herbert G. Winful , Steven 1 1 quantum secure communications protocols. The second T. Cundiff ; Univ. of Michigan, USA. We experimentally part of the talk will describe how photonic integrated demonstrate single-section InGaAsP/InP quantum-well circuits technology can extend the reach of quantum diode lasers for frequency comb generation at 1.5 µm communications through all-optical and memory-based and 1.3 µm wavelengths. Their optical and RF spectra quantum repeater protocols. are measured and analyzed.

FW6D.2 • 17:15 Invited FW6E.2 • 17:15 LW6F.3 • 17:15 Quantum Control and Metrology with Trapped Ions, Symmetric cladding thin film waveguides – from lossy Low-Threshold Lasing From Monolithic Nanostructured 1 Michael Biercuk1; 1Univ. of Sydney, Australia. In this talk media to disordered metasurfaces, Karsten Pufahl1, D. Porous Silicon Hybrid Microcavities, Giuseppe Barillaro ; 1 we provide an overview of the field of quantum control Boyaciyan2, Jan Heckmann1, Philipp Franz1, Nicolai B. Information Engineering, Univ. of Pisa, Italy. Here we engineering and the tools we have built to enhance the Grosse1, Regine v. Klitzing2, Ulrike K. Woggon1; 1Tech- demonstrate low-threshold lasing from fully-transparent performance of quantum devices for applications in nische Universität Berlin, Germany; 2TU Darmstadt, Ger- nanostructured porous silicon (PSi) monolithic micro- quantum computing and quantum sensing. We introduce many. Symmetric cladding thin film waveguides (SCTW) cavities (MCs) infiltrated with a polyfluorene derivative the concept of the filter function, a simple heuristic tool are investigated with respect to nonlinear response and that supports single-mode blue lasing at 466 nm, with to characterize the decoherence-sensitivity of arbitrary propagation length. Enhancement of both is demonstrat- line width of ~1.3 nm and lasing threshold of 5 nJ (i.e. 2 quantum operations performed on single or multi-qubit ed on thin metal films and functionalized metasurfaces fluence of 15 μJ/cm ). devices. We perform experiments with trapped ions (Au nanoparticles in a polymer brush). to validate the predictive power of the filter functions and demonstrate how they can enable quantum control solutions addressing major challenges in both error FW6E.3 • 17:30 LW6F.4 • 17:30 suppression for quantum computing and narrowband Dynamic Pulse Shaping by Metasurfaces, Shawn Observed Phase-locking Between a Rubidium Raman 1,2 1,2 1,2 2 1,2 detection for quantum sensing. These concepts form Divitt , Wenqi Zhu , Cheng Zhang , Henri Lezec , Laser and its Pump Laser, Nicholas Condon , Devin 1,2 1 1,2 1,2 1 1 the fundamental tools at the heart of our venture-backed Amit Agrawal ; Univ. of Maryland College Park, USA; Hileman , Shih Tseng , Zifan Zhou , Selim M. Shahriar ; 2 1 2 quantum technology startup Q-CTRL. National Inst. of Standards and Technology, USA. Northwestern Univ., USA; Digital Optics Technologies, Metasurfaces offer the ability to shape optical pulses USA. We have observed that the beat-note between a

with unprecedented resolution. Here, we demonstrate rubidium Raman ring laser and its gain pump is much Wednesday, 19 Septem dynamic shaping of <15 femtosecond ultrafast laser narrower than the spectral width of the pump laser itself, pulses using a Taylor series system in conjunction with indicating that they are mutually phase-locked. silicon metasurfaces.

FW6E.4 • 17:45 LW6F.5 • 17:45 A Broadband Achromatic Metalens, Yi-Teng Huang2, Novel free space and fiber laser cavities demonstrating Hsin Yu Kuo1, Pin Chieh Wu2; 1National Taiwan Univ., extreme sensitivities in Intracavity Phase Interferome- Taiwan; 2California Institue of Technology, USA. Metalens try systems, James Hendrie1, Hanieh Afkhamiardakani1, suffers from chromatic aberration issue, which limits its Luke Horstman1, Matthias Lenzner1, Ladan Arissian1, Jean 1 1

applications on color images. Here we demonstrate the Claude Diels ; Univ. of New Mexico, USA. A method to ber first broadband achromatic metalens in visible wave- enhance the sensitivity of sensors based on Intracavity length based on the concept of integrated-resonant unit Phase Interferometry by a factor of up to 10,000 is elements (IRUEs). demonstrated in a free space laser. This technique is then implemented in fiber lasers.

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FW6A • New Optical Hardware is Key to FW6B • Novel Optical Fibers and FW6C • Solid State Quantum Optics— Next Generation AR and MR—Continued Modulators—Continued Continued

FW6B.5 • 18:00 FW6C.5 • 18:00 Integrated Visible-Light Liquid-Crystal Phase Modu- Field Effect Transistors Deploying Anisotropic lator, Milica Notaros1, Manan Raval1, Jelena Notaros1, Two-Dimensional Materials for Light Generation and Michael R. Watts1; 1MIT, USA. An integrated liquid-crys- Detection, Ergun Simsek1, Mengqing Yuan3, Qing H. Liu2; tal phase modulator for applications within the visible 1Electrical Engineering and Computer Science, Exponent, wavelength range is demonstrated. A threshold voltage USA; 2Electrical and Computer Engineering, Duke Univ., of ±1.2V is shown and 24π phase shift is achieved within USA; 3Wave Computation Technologies, USA. Photode- ±2.5V in a 500-μm-long modulator. tector sensitivity and photoluminescence efficiency of ReS2 coated SiO2/Si substrates are studied. For ultra-thin applications, metal nanoparticles embedded in Si yield maximum enhancement.

FW6A.4 • 18:15 Invited Stereo, Parallax, Wavefronts, and Immersion - Where is the Value?, Joel S. Kollin1; 1Microsoft, USA. The dominant display paradigm (smart phones) prioritizes convenience over performance, and wrist- and head-mounted displays have yet to gain traction. How do we ensure that HMD doesn’t follow stereoscopic video into niche markets or irrelevance?

18:15–19:00 Dinner break on your Own

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FW6D • Quantum Computing with Atoms FW6E • Meta- and Nanophotonic Devices LW6F • Novel Lasers, Plasmonics, and Photons—Continued for Imaging and Applications—Continued Nanophotonics III—Continued

FW6E.5 • 18:00 LW6F.6 • 18:00 Dynamic Transmission Control Based on All-Dielec- A Free-space Brillouin Laser Using Diamond, Zhenxu tric Huygens Metasurfaces, Austin A. Howes1, Wenyi Bai1, Robert Williams1, Ondrej Kitzler1, Soumya Sarang1, Wang1, Ivan Kravchenko2, Jason Valentine1; 1Vanderbilt David Spence1, Richard Mildren1; 1MQ Photonics Research Univ., USA; 2Oak Ridge National Lab, USA. Dielectric Centre, Dept. of Physics and Astronomy, Macquarie Univ., metasurfaces exhibit low-loss modes, but their volumetric Australia. Continuous-wave lasing in a free-space crystal field profiles make them difficult to dynamically tune. Brillouin laser is demonstrated using CVD diamond. For a We overcome this issue by coupling resonators to an <111> polarized pump a threshold of 125 W is obtained, epsilon-near-zero mode in a thin film to actively modulate which corresponds to a gain coefficient of 60 cm/GW. transmittance.

18:15–19:00 Dinner break on your Own

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08:00–09:00 08:00–09:00 08:00–09:00 FTh1A • Vision Comfort as a Key to AR FTh1B • Quantum Information FTh1C • Shaping Light and Design of Mass Adoption Presider: Momchil Minkov; Stanford Quantum Devices Presider: Barry Silverstein; Oculus, USA University, USA Presider: Greg Gbur; University of North Carolina at Charlotte, USA

FTh1A.1 • 08:00 Invited FTh1B.1 • 08:00 Invited FTh1C.1 • 08:00 Invited Optimizing Head mounted Light Field Displays for Silicon Photonics for Generating and Manipulating Framework for Complex Quantum State Generation 1 1 1 Quality and Comfort, Hong Hua ; Univ. of Arizona, USA. Entangled Photons, Shayan Mookherjea , Chaoxuan and Coherent Control Based on On-Chip Frequency 1 1 1 In this presentation, we describe a generalized framework Ma , Xiaoxi Wang ; Univ. of California San Diego, USA. Combs, Piotr Roztocki1, Christian Reimer1,3, Stefania to model the image formation process of light-field Review of recent advances, future challenges and the Sciara1,4, Luis Romero Cortés1, Yanbing Zhang1, Benja- display methods and present a systematic method to state-of-the-art in integrated silicon photonics for quan- min Wetzel1,5, Mehedi Islam1, Alfonso Cino4, Sai Chu6, characterize the retinal image and the accommodation tum optical communications and other applications of Brent Little7, David Moss8, Lucia Caspani9, Jose Azaña1, response rendered by a light field display. We further em- heralded single and entangled photons. Michael Kues1,10, Roberto Morandotti1,2; 1INRS-Energie ploy this framework to investigate engineering guidelines Mat & Tele Site Varennes, Canada; 2National Research for designing a 3D light field displays with a balance of Univ. of Information Technologies, Mechanics and Op- quality and view comfort. tics, Russia; 3Harvard Univ., USA; 4Univ. of Palermo, Italy; 5Univ. of Sussex, UK; 6City Univ. of Hong Kong, China; 7Chinese Academy of Science, China; 8Swinburne Univ. of Technology, Australia; 9Univ. of Strathclyde, UK; 10Univ. of Glasgow, UK. Integrated frequency combs introduce a scalable framework for the generation and manipulation of complex quantum states (including multi-photon and high-dimensional states), using only standard silicon chip and fiber telecommunications components. FTh1A.2 • 08:30 Invited FTh1B.2 • 08:30 FTh1C.2 • 08:30 Invited Title to be Determined, Edward Tang1; 1Avegant Cor- High-precision phase noise estimation for continu- Connecting Quantum Systems through Optimized 1 poration, USA. Abstract not available. ous-variable quantum key distribution, Yijia Zhao , Photonics, Jelena Vuckovic1; 1Stanford Univ., USA. 1 1 1 2 Yichen Zhang , Yundi Huang , Song Yu , Hong Guo ; Our inverse design approach offers a powerful tool to 1 2 Beijing Univ of Posts & Telecom, China; Peking Univ., implement classical and quantum photonic circuits with China. We propose a high-precision phase noise estima- superior properties, including robustness to errors in tion for continuous-variable quantum key distribution to fabrication and temperature, compact footprints, novel reduce the phase noise caused by inaccurate estimation. functionalities, and high efficiencies. We illustrate this The phase noise is reduced below 1/10 by using modified with a number of demonstrated devices in silicon and reference data. in diamond.

FTh1B.3 • 08:45 Unsupervised Machine Learning Control of Quantum Gates in Gate-Model Quantum Computers, Laszlo Gyongyosi2,1, Sandor Imre1; 1Budapest Univ of Techololo- gy & Economic, Hungary; 2Univ. of Southampton, UK. The precise and stable working of quantum gates in quantum computers is essential for any quantum computations. We define a machine learning-based framework for the unsupervised control of entangled quantum gates in gate-model quantum computers.

09:00–09:15 Break

09:15–10:00 FTh2A • Visionary: Sir Peter Knight Presider: Kartik Srinivasan; National Inst of Standards & Technology, USA

FTh2A.1 • 09:15 VISIONARY Quantum Technology for a Networked World, Peter L. 1 1

ber Knight ; Kavli Royal Society International Ctr, UK. I will describe the worldwide efforts to develop quantum tech- nology, exploiting coherence and superposition. A sec- ond quantum revolution is emerging with electronic and photonic devices that use quantum science, harnessing our ability to interact with atoms, photons and electrons with exquisite level of control and with transformative potential for technology.

10:00–10:30 Coffee Break, Concourse Foyer Thursday, 20 Septem Thursday,

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08:00–09:00 08:00–09:00 08:00–09:00 FTh1D • Quantum Computing with Atoms FTh1E • Computational/Transformation LTh1F • Precision Laser Spectroscopy and Photons II Optics and Optics in Computing Presider: Konstantin Vodopyanov; University Presider: To be Determined Presider: Simon Horsley; Exeter University, of Central Florida CREOL, USA United Kingdom FTh1D.1 • 08:00 Invited LTh1F.1 • 08:00 Invited FTh1E.1 • 08:00 Invited Quantum computing with Neutral Atoms, David Weiss1; Development of Cryogenic Strontium Optical Lattice Topology and the optical Dirac equation, S. A. R. 1Dept. of Physics, Penn State Univ., USA. I will describe our Clocks and their Applications, Masao Takamoto1, Ichiro Horsley1; 1Univ. of Exeter, UK. Maxwell’s equations can approach to neutral atom quantum computing using a 3D Ushijima2,1, Hidetoshi Katori2,1; 1RIKEN, Japan; 2The Univ. be written as an effective Dirac equation (the ‘optical optical lattice. We have previously demonstrated perfect of Tokyo, Japan. The recent progress of optical lattice Dirac equation’), which can be a useful tool to classify filling of 5x5x2 and 4x4x3 arrays and site-addressed single clocks has improved the accuracies to 10-18, which out- electromagnetic materials. This analogy can be provide qubit gates with 0.997 fidelity and low cross talk. Most performs the realization of the SI second. We will present a new way to relate the integral of the Berry curvature recently, we have achieved lossless state detection with the development of the clocks and their applications in (the Chern number) to the number of interface states. In fidelities exceeding 0.999. geodetic measurements. contrast to the common approach we show that the Chern number can be computed without knowledge of how the FTh1D.2 • 08:30 Invited material parameters depend on frequency. Reconfigurable and Programmable Ion Trap Quantum Computer, David Moehring, Jungsang Kim; IonQ, USA. Trapped atomic ion qubits present a fundamentally scal- able approach to quantum computation. All qubits are identical, and interactions can be faithfully replicated and measured with near-perfect efficiency. Unlike many other approaches to quantum hardware, trapped ion qubits op- erate effectively at room-temperature, and even allow for reconfigurable quantum circuits. This flexibility will likely allow ion trap quantum computers to express the super- FTh1E.2 • 08:30 LTh1F.2 • 08:30 set of all known quantum computation operations, and Optical Convolutional Neural Networks with Opti- Laser system to laser-cool and trap cadmium: towards 1 thus efficiently target any type of application that arises. mized Phase Masks for Image Classification, Julie a cadmium optical lattice clock, Daniel T. Schussheim , Chang1, Vincent Sitzmann1, Gordon Wetzstein1; 1Electrical Kurt Gibble1; 1The Pennsylvania State Univ., USA. We Engineering, Stanford Univ., USA. Convolutional neural use frequency doubling and summing to generate >1 W networks excel in many computer vision applications of 326 nm to laser cool cadmium. Other wavelengths, but exert high computational demands. We propose a 361, 468, and 480 nm, are also generated from the high zero-power optical convolutional layer that can be incor- power fiber amplifier. We developed an FPGA controller porated for increased efficiency and show its potential to automatically lock the system. in simulation.

FTh1E.3 • 08:45 LTh1F.3 • 08:45 Deep Neural Networks for Information Recovery Optimization of acousto-optic frequency combs for Through Multimode Fibers, Eirini Kakkava1, Navid multi-heterodyne spectroscopy, Kanagaraj Nithyanan- 1 1 1 Borhani1, Christophe Moser1, Demetri Psaltis1; 1Ecole dan , Leao Djevarhidjian , Vicente Duran , Come Schné- 1 1 1 Polytechnique Federale de Lausanne, Switzerland. Image belin , Samir Kassi , Guillaume Mejean , Daniele Romani- 1 1 1 classification and reconstruction from the instensity speck- ni , Guillet de Chatellus Hugues ; CNRS / Université le patterns at the distal end of a multimode fiber (MMF) Grenoble Alpes, France. Acousto-optic frequency combs was demonstrated using Deep Neural Networks (DNNs). provide more than 1000 mutually-coherent lines, and are a Handwritten digits were recovered after propagation in valuable tool for multi-heterodyne coherent spectroscopy. 1km long MMF. We present and validate a simple model of acousto-optic frequency combs, and discuss their limitations.

09:00–09:15 Break

09:15–10:00 LTh2B • Visionary: David DeMille Presider: Nathan Newbury; NIST, USA

LTh2B.1 • 09:15 VISIONARY Activities Shaping the Wavefront of Nanophotonics, 1 1 David DeMille ; Yale Univ., USA. Remarkably, certain Thursday, 20 Septem ultra-precise spectroscopic measurements are sensitive to the existence of certain new, yet-undiscovered particles whose mass far exceeds that of the recently discovered Higgs boson. This talk will describe ongoing and future examples of such measurements, including the ACME experiment, a search for the electron’s electric dipole moment. ber 10:00–10:30 Coffee Break, Concourse Foyer

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10:30–12:30 10:30–12:30 10:30–12:30 FTh3A • AR/VR Applications for Enterprise FTh3B • Quantum Electronics FTh3C • Optical Comb Metrology and Consumer Markets Presider: Shayan Mookherjea; University of Presider: Judith Dawes; Macquarie Presider: Hong Hua; University of Arizona, California San Diego, USA University, Australia USA

FTh3A.1 • 10:30 Invited FTh3B.1 • 10:30 Invited FTh3C.1 • 10:30 Invited Waveguide Manufacturing for AR Displays, Past, Quantum-state Generation and Frequency-Domain Spatio-temporal Manipulation of Light Waves by use of Present and Future, Jonathan Waldern1; 1DigiLens, USA. Manipulation using Nanophotonics, Kartik Srinivasan1; Optical Frequency Combs, Kaoru Minoshima1,2, Akifumi Current AR waveguide fabrication processes, including 1NIST, USA. I will review experiments on the generation Asahara1,2; 1Univ. of Electro-Communications, Japan; 2 Surface Relief Gratings (SRG), holographic and cascaded and frequency-domain manipulation of photonic quantum JST ERATO MINOSHIMA Intelligent Optical Synthesizer mirrors, are reviewed. We present DigiLens’s Switchable states using scalable nanophotonic devices, and discuss (IOS), Japan. Relative carrier envelope phase control in Bragg Grating (SBG) based process, a manufacturing their relevance to several applications in photonic quan- the dual-comb was utilized to generate an advanced light method based on classical holographic contact copy, tum information science. source for versatile spatiotemporal phase manipulation. which today is used for both large and small AR displays Optical vortex comb is experimentally demonstrated with including a range of displays suitable for HUD and XR application for optical tweezers. applications.

FTh3A.2 • 11:00 Invited FTh3B.2 • 11:00 FTh3C.2 • 11:00 Augmented Reality Smart Glasses: Disruption or On-demand four-wave mixing parametric processes in Efficient Non-Linear Optical Spectroscopy with Mul- 1 Distraction?, Kayvan Mirza1; 1Optinvent, France. The periodically-tapered waveguides, Mohammed F. Saleh ; tiple High-Frequency Modulated Optical Frequency 1 1 1 destiny of mobile AR has been inextricably linked to the Heriot Watt Univ., UK. I show using Fourier-series analysis Combs, Ayan Chattopadhyay , Alexei Goun , Herschel 1 1 success of Smart Glasses. Although there is some traction how sinusoidally-tapered waveguides can be employed Rabitz ; Princeton Univ., USA. High signal-to-noise de- in the enterprise space, consumer adoption has remained as efficient quasi-phase-matching schemes in third-or- tection of the non-linear polarization is obtained, utilizing elusive. Will the next generation of Smart Glasses be der nonlinear media for on-demand four-wave mixing multiple high-frequency modulated optical frequency more successful than their predecessors in bringing AR parametric processes, such as third-harmonic generation. combs that place the observed polarization in the field- to the masses? free region within comb line structure.

FTh3B.3 • 11:15 FTh3C.3 • 11:15 Complementarity of Vectorial Quantum Light, An- Bridging Telecom Wavelengths to Alkali Atomic Tran- dreas Norrman1, Kasimir Blomstedt2, Tero Setälä2, Gerd sitions with Tunable Kerr Frequency Combs, Su-Peng Leuchs1,3, Ari Tapio Friberg2; 1Max Planck Inst. for the Yu1,2, Travis C. Briles1,2, Gregory T. Moille3, Xiyuan Lu3, Science of Light, Germany; 2Univ. of Eastern Finland, Fin- Scott A. Diddams1,2, Kartik Srinivasan3, Scott B. Papp1,2; land; 3Univ. of Erlangen-Nuremberg, Germany. We study 1Time and Frequency Division, NIST Boulder, USA; 2Dept. partial coherence and polarization in double-pinhole of Physics, Univ. of Colorado, USA; 3Center for Nanoscale interference and establish two general complementarity Science and Technology, NIST Gaithersburg, USA. We relations for genuine vectorial quantum-light fields. The report a silicon-nitride microresonator frequency comb framework uncovers new fundamental aspects of photon platform that provides coverage from the telecom L band wave–particle duality. to the 780 nm range. Arbitrary design and generation of Kerr-soliton combs enables continuous fine-tuning across the entire bandwidth.

FTh3A.3 • 11:30 Invited FTh3B.4 • 11:30 FTh3C.4 • 11:30 Use of AR and smart glasses at Erie Insurance, Brett Increasing Sensitivity of an Atom Interferometer to Progress Towards a Three-Node Free-Space Clock 1 1 McCorkle1; 1Erie Insurance, USA. The insurance industry the Heisenberg Limit using Enhanced Quantum Noise, Network, Paritosh Manurkar , Sarah Stevenson , Isaac 1 1 1 1 2 1 is rooted in legacy technology and business practices. Renpeng Fang , Resham Sarkar , Selim M. Shahriar ; Khader , Jean-Daniel Deschenes , William Swann , Na- 1 1 1 1 Introducing technologies like smart glasses and AR is Northwestern Univ., USA. We show how, by using a than R. Newbury , Laura Sinclair ; NIST Boulder, USA; 2 challenging due to change resistance and technical Schroedinger Cat state, the sensitivity of an atomic in- Octosig Consulting, Canada. We report the latest prog- uncertainty. Using human-focused design in your im- terferometer can be increased, to the Heisenberg limit, ress towards the development of a three-node free-space plementation helps you engage users and increase the while enhancing the quantum noise, thereby suppressing clock network. We will demonstrate clock comparison likelihood of adoption. strongly the effect of excess noise. between two optical nodes via coherent time/frequency transfer through a third node.

FTh3B.5 • 11:45 FTh3C.5 • 11:45 Self-similar Pulse Compression in the Tapered Silicon Towards Isolated Attosecond Pulses at 100 kHz for Waveguide, Jiayao Huang1, Aruna Gandhi M S1, Qian Electron-Ion Coincidence Spectroscopy, Federico J. Li1; 1Peking Univ., China. We demonstrate self-similar Furch1, Tobias Witting1, Felix Schell1, Mikhail Osolodkov1, pulse compression in the tapered silicon waveguide. Claus Peter Schulz1, Marc J. Vrakking1; 1Max Born Inst., The initial 1 ps pulse can be compressed to 76.4 fs, and Germany. We report on the progress towards isolated at- the corresponding peak power is 7.1 times compared tosecond pulses in the extreme ultraviolet at 100 kHz with to the initial pulse. high photon flux. The system will be used in pump-probe experiments detecting electrons and ions in coincidence ber Thursday, 20 Septem Thursday,

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10:30–12:30 10:30–12:30 10:30–12:30 FTh3D • Quantum Communications and FTh3E • Information Processing, LTh3F • Advances in Molecular the Future Quantum Internet Information Display and Optical Device Spectroscopy Presider: To be Determined Presider: Michael Klug; Magic Leap, USA Presider: Nathan Newbury; National Institute of Standards and Technology, USA

FTh3D.1 • 10:30 Invited FTh3E.1 • 10:30 Invited LTh3F.1 • 10:30 Invited Quantum Dot Based Devices for Telecom Wavelength Optics for Wearable Spatial Computing Systems, Optical Pulse Shaping, From Nanoseconds to Fem- 1 1 1 Quantum Networks, Joanna Skiba-Szymanska , Tina Michael Klug ; Magic Leap, USA. Spatial Computing toseconds, And Its Roles in Coherent Molecular 1 2 1 1 Müller , Andrey Krysa , Jan Huwer , Ginny Shooter , requires visual system and wearable display compatibility Spectroscopy and Medical Imaging, Warren S. Warren1; 1 1 2 Mathew Anderson , Martin Felle , Ian Farrer , Richard for accurate perception, user comfort, and effective inter- 1Duke Univ., USA. I will discuss the evolution of pulse 3 1 2 Penty , Richard M. Stevenson , Jon Heffernan , David action. We present optical approaches that balance these shaping and pulse train modulation technologies over 3 1 1 Ritchie , Andrew Shields ; Toshiba Research Europe goals with demands for manufacturability and practicality. many different timescales, with modern applications for 2 3 Ltd., UK; Univ. of Sheffield, UK; Univ. of Cambridge, characterizing materials and diagnosing disease. UK. Quantum networks rely on robust and secure distri- bution of quantum states to share entanglement between connected technologies. We demonstrate quantum dot based devices that use photons as flying qubits within existing fibre optics infrastructure.

FTh3D.2 • 11:00 Invited FTh3E.2 • 11:00 LTh3F.2 • 11:00 Invited Quantum Computation and Quantum Information, Digitally designed HOE lens arrays for large size see- Cavity-enhanced Ultrafast Spectroscopy: Enabling 1 Ian Walmsley1; 1Univ. of Oxford, UK. Hybrid light-matter through head up displays, Jackin Boaz Jessie , Lode Transient Absorption Spectroscopy of Dilute Species 2 1 1 networks offer the promise for delivering robust quantum Jorissen , Ryutaro Oi , Koki Wakunami , Yasuyuki Ichi- in Molecular Beams, Melanie Reber1, Nicholas Cooper1, 1 2 1 1 information processing technologies, from sensor arrays hashi , Philippe Bekaert , Kenji Yamamoto ; National Inst Ramesh Basnet1, Kayla Warren1; 1Univ. of Georgia, USA. 2 to quantum simulators. New sources, circuits, detectors of Information & Comm Tech, Japan; Expertise Center for Coupling ultrafast frequency combs to external en- and memories illustrate progress towards building a Digital Media, Hasselt Univ.-tUL, Belgium. See-through hancement cavities increases the sensitivity of transient resilient, scalable photonic quantum network. head-up 3D display which uses a commercial projector absorption spectroscopy by several orders of magnitude. and holographic lens array is reported. The display system This enables femtosecond transient absorption of dilute is significantly simplified and a 3D scene of size 20cm x species in molecular beams, such as hydrocarbon radicals. 10cm x 5 cm (Depth) is successfully reconstructed.

FTh3E.3 • 11:15 Depth-induced Cellular Automata for Light Field Sa- liency, Yongri Piao1, Xiao Li1, Miao Zhang1; 1Dalian Univ. of Technology, China. A Depth-induced Cellular Automata (DCA) is proposed to optimize light field saliency maps. DCA is robust to challenging scenes because it con- sidered interactions and complementarities of intrinsic structure among the abundant cues on light field.

FTh3D.3 • 11:30 Invited FTh3E.4 • 11:30 LTh3F.3 • 11:30 Invited Quantum Communication Experiments with Tele- Iterative Forward-Backward Algorithm for Optical Massively Parallel Sensing of Trace Molecules with 1 com-band Photonics Technologies, Hiroki Takesue1; Diffraction Tomography, Shengli Fan , Seth D. Smith- Broadband Mid-Infrared Subharmonic Frequency 1 1 1 1 1NTT Basic Research Labs, Japan. We present our effort to Dryden , Guifang Li , Bahaa Saleh ; Univ. of Central Combs, Konstantin L. Vodopyanov1, Andrey Muraviev1, realize basic functions for advanced quantum communica- Florida, CREOL, USA. An iterative forward-backward Viktor O. Smolski3, Zachary E. Loparo2; 1CREOL, College tion systems using telecom-band photonics technologies, algorithm for optical diffraction tomography is proposed of Optics and Photonics, Univ. Cent. Florida, USA; 2Me- including entanglement sources using nano-scale silicon for imaging phase objects with large refractive index chanical and Aerospace Engineering, Univ. Cent. Florida, devices and quantum logic gate for time-bin qubits based contrast. Numerical results demonstrate accurate and USA; 3Mid-Infrared Lasers, IPG Photonics, USA. We use a on electro-optic modulators. robust reconstructions with sub-wavelength resolution. pair of mutually-coherent frequency-divide-by-two OPOs with instantaneous span 3.1-5.5µm to demonstrate fast acquisition of 350,000 mode-resolved spectral data FTh3E.5 • 11:45 points and perform parallel detection in a mixture of 22 Deep Neural Network for Low Light Phase Recovery, molecular species. Alexandre Goy1, Kwabena Arthur1, Shuai Li1, George Barbastathis1,2; 1Mechanical Engineering, MIT, USA; 2Singapore-MIT Alliance for Research and Technology Centre, Singapore. Poisson noise severely impacts imag- ing systems in low light conditions. We demonstrate the use of deep neural networks applied to phase retrieval Thursday, 20 Septem and show successful phase recovery with only 10 photons per detector pixel. ber

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FTh3A • AR/VR Applications for Enterprise FTh3B • Quantum Electronics—Continued FTh3C • Optical Comb Metrology— and Consumer Markets—Continued Continued

FTh3A.4 • 12:00 Invited FTh3B.6 • 12:00 FTh3C.6 • 12:00 AR UI for Lunar and Martian Energy Operations, Simulation of nonlinear photonic crystals by modified Gallium Phosphide Microresonator Frequency Combs, 2,1 2 2 Micah TinklePaugh1; 1EPRI Inst., USA. Astronauts and finite difference frequency domain method, Tamás Dalziel Wilson , Simon Hönl , Katharina Schneider , Miles 1 2 1 1 1 2 1 utility workers need better visual tools than afforded Szarvas , Zsolt Kis ; BME Dept. of Atomic Physics, Anderson , Tobias Kippenberg , Paul Seidler ; Ecole 2 2 by static screens and current interfaces. ‘Holograms’ in Hungary; HAS Wigner Research Center for Physics, Polytechnique Federale de Lausanne, Switzerland; IBM remote terrain, space capsules, control rooms, and storm Hungary. We have worked out a true vectorial numerical Research, Zurich, Switzerland. We demonstrate the first affected environments might make them more effective method for the simulation of second harmonic generation microresonator frequency combs in GaP, a III-V semicon- and efficient. by extending the finite difference frequency domain ductor transparent above 549 nm. High Kerr nonlinearity method. As an application we have simulated an array ( 10-17 m2/W) yields THz combs at 1550 nm with a 3-mW of nonlinear cylinders. power threshold and >100-nm bandwidth. ∼ FTh3B.7 • 12:15 FTh3C.7 • 12:15 Nonlinear optical studies of new bioprobes, Katarzyna Revealing the quantum nature of a free electron in an Matczyszyn1; 1Wroclaw Univ. of Science and Techn., Po- attosecond laser pulse, Ori Reinhardt1, Ido Kaminer1; land. Two-photon fluorescent dyes and bistable molecular 1Technion, Israel. Free electrons interacting with the fre- photoswitches are key components in the ongoing quest quency comb of an attosecond laser pulse follow intricate toward increasingly sophisticated, selective, sensitive, quantum dynamics. We present an analytic treatment of and versatile biological procedures and constitute an the interaction and use it to shape the electron energy ideal mean to manipulate a wide range of bio-events. spectrum. ber Thursday, 20 Septem Thursday,

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FTh3D • Quantum Communications and FTh3E • Information Processing, LTh3F • Advances in Molecular the Future Quantum Internet—Continued Information Display and Optical Device— Spectroscopy—Continued Continued

FTh3E.6 • 12:00 Invited LTh3F.4 • 12:00 Invited FTH3D.4 • 12:00 Electro-Optical Response of Nonconventional Choles- Quantum Key Distribution: From Technology to Probing Soot Formation and Chemical Evolution during teric Liquid Crystal with Refined Uniform Lying Helix 1 1 1 1 Combustion, Hope A. Michelsen ; Combustion Research Real-World Implementation, Bruno Huttner ; ID 1 1 1 Alignment, Yueh-Chern Lin , Po-Chang Wu , Wei Lee ; Facility, Sandia National Labs, USA. Large gaps in the Quantique, Switzerland. The quantum computer is now 1 College of Photonics, National Chiao Tung Univ., Tai- understanding of soot formation during combustion are seen as a credible threat to cybersecurity. Companies wan. We demonstrate a well-aligned and stable uniform world-wide understand that upgrading to quantum-safe predominantly attributable to a limited ability to probe lying helix structure by adding bent-core molecules into relevant particle parameters during formation. This talk security is required. Quantum technologies, and espe- a cholesteric liquid crystal. The frequency-dependent cially quantum key distribution, provide a solution, which will describe approaches to developing appropriate electro-optic response is characterized by flexoelectrici- diagnostics. can be implemented today, and will contribute to a new ty-induced dielectric relaxation. cybersecurity infrastructure. FTh3E.7 • 12:15 Synthesis of Broadband Space-Time Diffraction-Free Wave Packets Using Transmissive Phase Plates, Murat Yessenov1, Hasan E. Kondakci1, Monjurul F. Meem2, Dan- ielle Reyes1, Daniel Thul1, Shermineh R. Fairchild1,3, Martin C. Richardson1, Rajesh Menon2, Ayman Abouraddy1; 1CREOL, Univ. of Central Florida, USA; 2Dept. of Electrical and Computer Engineering, Univ. of Utah, USA; 3Physics and Space Sciences, Florida Inst. of Technology, USA. We demonstrate the synthesis of broadband diffraction-free space-time pulsed light sheets using transmissive phase plates. We produce propagation-invariant wave packets having a bandwidth of 30~nm from a multi-terawatt femtosecond laser. Thursday, 20 Septem ber

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FiO Abstracts.indd 57 8/20/18 9:11 AM Key to Authors and Presiders

A Andrii, Yakunov V.- JTu3A.111 Barna, Shama - JTu3A.14 Aadhi, A - JW4A.50 Anguita, Jaime A.- JTu2A.82 Barrios, Bruce - FM4B.7 Abaie, Behnam - JW3A.134, JW3A.138 Anopchenko, Aleksei - JTu2A.88, JTu2A.90, Bartels, Randy - FM4C.3, JTu2A.117, JTu3A.104, Abate, Yohannes - FW5E.3 JW3A.65 JTu3A.108, JTu3A.125 Abdelatty, Mohamed - JW3A.106 Anoshkin, Ilya - JTu2A.40 Barth, David - FM3G.4 Abdelsalam, Kamal - JTu3A.59 Antropov, Ilya - JW4A.97 Bartley, Tim J.- LM3B.1 Key to Authors Abdelsalam, Mostafa - JW4A.2 Anwar, Ali - JTu2A.56 Basaldua, Isaac - JTu3A.38, JW4A.37 Abouraddy, Ayman - FTh3E.7, JTu2A.29, JTu3A.20, Anzulevich, Anton - JW4A.100 Bashkansky, Mark - JW4A.61 JW4A.7 Aoyagi, Yuu - JW3A.132 Basnet, Ramesh - LTh3F.2 Abrahao, Raphael A.- JTu2A.55 Arai, Kenji W.- JW3A.70 Basset, Guillaume - FW6A.2 Abrashitova, Ksenia - JW4A.97 Araújo, Cid B.- JW3A.73 Bassett, Cody - LM1B.3 Abu Bakar, Muhammad Hafiz - JTu3A.71 Arce-Diego, Jose L.- JTu3A.106 Bassignot, Florent - JTu2A.65, JW3A.23 Acuña, Rodrigo - JTu2A.97 Arce-Diego, Jose Luis - FM3F.3 Baudelet, Matthieu - JTu2A.50 Adams, Daniel - JW4A.14 Aripin, Nurul F.- JTu3A.21 Bauer, Adam Q.- FM3F.1 Adhikari, Prakash - JTu2A.111, JTu2A.127, Arissian, Ladan - JW3A.6, LW6F.5 Baumann, Bernhard - JTu2A.128 JTu3A.109 Ariunbold, Gombojav O.- JTu2A.111 Beadie, Guy - JW3A.13 Afkhamiardakani, Hanieh - LW6F.5 Armani, Andrea M.- FM4E.6 Becker, Jan - FM4E.5 Agarwal, Girish - JTu2A.39, JW3A.65 Armas Rivera, Ivan - JTu2A.11 Bedi, Amna - JTu2A.109, JTu2A.81, JTu3A.66 Agha, Imad - JTu2A.96, JTu3A.103 Arndt, Catherine - FW6B.2, JTu2A.90 Beeckman, Jeroen - JTu2A.61 Aghaeimeibodi, Shahriar - FW6C.3 Arnold, Cord - LTu5F.3 Behague, Florent - JW3A.23 Agrawal, Amit - FW6E.3, JW4A.56 Arnoldus, Henk F.- JTu3A.22 Behera, Narayan - JW3A.37 Ahluwalia, Balpreet S.- FM4E.4 Arsenijević, Dejan - FTu5B.2 Behnken, Barry N.- FM3E.1 Ahmad, Azeem - FM4E.4 Arthur, Kwabena - FTh3E.5 Bei, Zongmin - JTu2A.32 Ahmed, Rajib - JW4A.91 Asahara, Akifumi - FTh3C.1 Bej, Subhajit - JTu2A.88 Ahmmed Aoni, Rifat - JTu3A.12, JW4A.91 Ashok, Amit - FM4C.1 Bekaert, Philippe - FTh3E.2 Ahn, Heesang - JTu2A.120, JTu2A.124, JW3A.104, Assmann, Ralph - FTu4C.5 Bekele, Robel - FM3C.1 JW4A.21 Astorino, Antonio - JTu2A.6 Belardi, Walter - FW6B.4 Ai, Yong - JTu2A.76 Ataai, Rajab - JW3A.50 Belin, Jakub - FM3C.7, JTu3A.18, JW3A.126 Aiub, Eduardo J.- FTu4B.3 Atabey Buyukkaya, Mustafa - FW6C.3 Bell, Bryn A.- JTu3A.58, JW4A.58 Aizin, Gregory - JW4A.75 Atwater, Harry - FTu4A.1 Bello-Jiménez, Miguel - FTu4B.5, JTu2A.77, LTu5F.4 Akin, Thomas G.- JW4A.61 Augustin, Marco - JTu2A.128 Beltrán Pérez, Georgina - JTu2A.11 Aktas, Djeylan - FW1E.2 Avramov-Zamurovic, Svetlana - JW3A.14 Ben Khalifa, Amani - JTu2A.18 Al Menabawy, Sara - JTu3A.9, JW3A.9 Avrutin, Vitaliy - JTu2A.22 Ben Salem, Amine - JTu2A.18 Alalyani, Ahmad - JTu3A.110, JTu3A.52 Axente, Emanuel - JTu3A.138 Ben, Fang - JW4A.80 Alamandala, Sravanthi - JW3A.103 Azaña, Jose - FTh1C.1 Bennet, Adam - LM1B.5 Alaniz-Baylón, Jared - FTu4B.5 Azoury, Doron - JTu3A.48 Bennett, Tim - JTu3A.140, JW3A.137 Alanzi, Saud - JTu3A.52 Azzahrani, Ahmad S.- JTu2A.27, JTu3A.110, Ben-Zvi, Ilan - JTu3A.50 Alauddin, Sakinah M.- JTu3A.21 JTu3A.52 Beresna, Martynas - JTu3A.16, JTu3A.70, JW3A.12 Alberding, Brian G.- JTu3A.62 Berg, Matthew J.- JTu2A.111 Alberucci, Alessandro - FW5C.3, JTu2A.61, B Besen, Matt - JW4A.16 JW4A.76 B.S., Vikram - FW5B.4 Bessonov, Vladimir O.- JW3A.49, JW4A.97 Aldossary, Omar - FM3C.7 Bachavala, Ashish - JW3A.16 Bhaduri, Basanta - JTu2A.29, JTu3A.20 Alexander, Tristram J.- JW4A.78 Bachelard, Nicolas - FM3G.4 Bhaktha B N, Shivakiran - JTu2A.100 Alfano, Robert R.- JW4A.3, LM4A.1 Badolato, Antonio - FTu4E.3 Bhaktha B. N., Shivakiran - JW3A.1 Ali, Nadir - JTu2A.102 Badr, Mohamed - JW3A.96 Bhardwaj, Shivani - JW4A.110 Allen, Monica S.- JW3A.98 Bae, Euiwon - JTu2A.25 Bhaskar, Shyju - JW4A.121 Allsopp, Duncan - JTu3A.86 Bae, Young-Min - JW3A.113 Bhattacharya, Mishkat - FW1E.4, JW3A.89 Almeida, Alexandre A.- JTu2A.7 Baets, Roel G. F.- FW6E.1 Bhowmick, Mithun - JTu2A.69 Almeida, Gustavo F.- JTu2A.9 Bag, Ankan - FM3C.6 Biaggio, Ivan - JTu2A.1 Alonso, Miguel A.- FM3C.4, JW3A.34, JW4A.124 Bag, Saawan Kumar - JTu3A.19 Bianco, Vittorio - JTu3A.122, JW3A.110 Alpeggiani, Filippo - FM3C.3, FTu5E.4 Bahari, Aysan - JTu3A.46 Bieda, Marcin - JW4A.134 Al-Qasimi, Asma - JW4A.38 Bai, Zhenxu - LW6F.6 Bienaimé, Tom - FW5C.4 Altug, Hatice - JTu3A.32 Baida, Fadi - JW3A.23 Biercuk, Michael - FW6D.2 Alu, Andrea - LW1F.2, LW6F Baker, Travis J.- LM1B.5 Billingsley, GariLynn - JW4A.77 Alvarez-Tamayo, Ricardo Iván - FTu4B.5, LTu5F.4 Balram, Krishna C.- JTu3A.86 Bimberg, Dieter - FTu5B.2 Amarit, Ratthasart - JTu3A.112 Bandres, Miguel A.- FTu4C.1 Binkele, Tobias - JW4A.8 Amer, Aya - JW3A.96 Banerjee, Dipti - JTu3A.27, JW3A.25 Black, Adam T.- JW4A.61 Ameri, Hossein - FM4E.6 Bang, Ole - FM3F.5 Blanchard, Paul T.- FTu5C.3 Amin, Rubab - FW5E.2, JTu3A.73, JW3A.123, Bange, Sebastian - JW3A.67 Blanco-Redondo, Andrea - JW4A.58, JW4A.78 JW4A.96 Banoth, Earu - JTu2A.23 Blomstedt, Kasimir - FTh3B.3 Amir, Wafa - JW3A.16 Banzer, Peter - FM3C.6 Boaz Jessie, Jackin - FTh3E.2 Anand, Srinivasan - JTu3A.83 Bao, Yijun - JTu2A.74 Boehm, Fabian - JTu2A.64 Ancona, Mario - JW4A.40 Bao, Yiliang - JW3A.88 Bolas, Mark - FW2A.1 Anderson, Mathew - FTh3D.1 Barbastathis, George - FTh3E.5 Bolek, Jan - JTu2A.130 Anderson, Miles - FTh3C.6 Barillaro, Giuseppe - LW6F.3 Bolis, Serena - JTu2A.61 Andre, Laura - JW3A.46 Barker, Peter F.- JTu3A.81 Boller, Klaus-J. - JTu3A.58 Andreev, Nikolai - JW4A.30 Barkhofen, Sonja - LM3B.1 Boltasseva, Alexandra - FM3G.2 Andriani, Rudy - FM3F.2 Barman, Anjan - JW4A.49 Bondar, Mykhailo V.- JTu3A.7

92 FiO + LS 2018 • 16–20 September 2018

FiO Abstracts.indd 58 8/20/18 9:11 AM Boppart, Stephen - JTu3A.114 Carney, P. Scott - JTu3A.113 Chiu, Min-Hsueh - JTu2A.57 Borhani, Navid - FTh1E.3 Carpenter, Joel A.- FTu5B.3 Cho, Junho - FTu4B, FW5B.1 Cho, Seungryong - JW3A.113 Boscolo, Sonia - JTu3A.34 Carr, C.W.- LTu4F.4 Key to Authors Bosman, Gurthwin - JTu2A.34 Carrillo-Delgado, Carlos M.- JTu3A.78 Choi, Chulsoo - JTu2A.15, JTu2A.28 Bouchand, Romain - FW1C.2 Casamento, Jon - JW3A.19 Choi, Ji Sun - JTu3A.119 Boulbar, Emmanuel L.- JTu3A.86 Caspani, Lucia - FTh1C.1 Choi, Jong-ryul - JW4A.21 Boyaciyan, D - FW6E.2 Caspar, Alexis - JW3A.23 Choi, Myongjo - JTu2A.26 Boyd, Robert - JTu3A.32, JW3A.71, JW4A.124 Castaneda, Mario A.- FTu5B.4 Choi, Samuel - FM3D.3 Bracamontes, Yazmin - JTu2A.11 Castillo, Zachary A.- JTu2A.54, JW4A.57, JW4A.64 Choi, Young-Wook - JTu2A.13, JW3A.113 Bradley, Thomas D.- FW6B.3 Castro-Lopez, Marta - JTu3A.16 Chong, Andy - JTu2A.43 Bramati, Alberto - FW5C.4 Ceballos-Herrera, Daniel E.- JW4A.82 Choubal, Aakash - JTu3A.14 Brambilla, Gilberto - JTu3A.16, JTu3A.70, JW3A.12 Ceyhan, Ufuk - JW4A.8 Choubey, Priyanka - JW3A.1 Branny, Artur - FW6C.2 Chaganava, Irakli - JTu3A.21 Choudhury, Samiran - JW4A.49 Brecht, Benjamin - FTh3D.2, JW3A.63 Chalifoux, Brandon - JW4A.52 Chowdhury, Bilas - JW3A.86 Bres, Camille-Sophie - FM3C.2, FW6B.1, JTu3A.32 Chamuah, Nabadweep - JW4A.70 Christodoulides, Demetrios N. - FTu4C.1 Brewer, Nicholas - JW3A.59, JW3A.64, JW4A.62 Chan, Ray - JTu3A.15 Chrzanowski, Helen - FTh3D.2 Brewster, Richard A.- JW4A.66 Chandrasekhar, Sethumadhavan - FW5B.1 Chu, Hsu-Hsin - JW4A.141 Briea, Patricia - JTu3A.84 Chang, Chen - JW3A.127 Chu, Sai - FTh1C.1 Briles, Travis C.- FTh3C.3, JTu2A.62 Chang, Chengcheng - JW3A.22 Chu, Ying-Ju Lucy - JTu2A.37 Broderick, Jeff - JTu3A.108 Chang, Cheng-Han - JTu2A.12, JW4A.119 Chuang, Yi-Chen - JW3A.131 Brodsky, Michael - JTu3A.61, JTu3A.69 Chang, Guoqing - FTu4B.4, JTu2A.116 Chung, Hsiang-Yu - JTu2A.116 Brodutch, Aharon - JTu2A.89 Chang, Hang S.- JW3A.119 Chung, Hung-Ching - JTu2A.78 Brongersma, Mark - LW2B.1 Chang, Julie - FTh1E.2 Chung, Te-Yuan - JW3A.133 Brotons-Gisbert, Mauro - FW6C.2 Chang, Shu-Wei - JW4A.119 Cino, Alfonso - FTh1C.1 Brundavanam, Maruthi Manoj - FM4C.6 Chaplain, Gregory - JW3A.126 Cisternas, Jaime E.- JTu2A.82 Bruner, Barry - JTu3A.48 Charavarty, Abhijit - JW3A.86 Clark, Charles - FW5C.2 Buchleitner, Andreas - JTu3A.60 Charipar, Kristin M.- JW3A.95 Cleary, Justin W.- JTu2A.108 Bugaychuk, Svitlana - JTu2A.45 Charipar, Nicholas - JW3A.95 Clements, William - FTh3D.2 Bugoffa, Salaheddeen - JW4A.44 Chase, Christopher - LW6F.1 Clergerie, Alex - JTu3A.48 Bui, Lam - JW4A.83 Chatterjee, Avijit - FW1B.1 Cohen, Offir - JW3A.61, LM1B.7 Bukhari, Syed Sultan Shah - JW4A.43 Chatterjee, Monish R.- JTu3A.29, JW3A.50, Cole, Garrett - JW4A.77 Burada, Daliramu - FM3D.4, JTu3A.11, JW4A.9 JW4A.44 Collins, Ron - JW4A.16 Burkins, Paul - JTu3A.38, JW4A.37 Chattopadhyay, Ayan - FTh3C.2 Condon, Nicholas - LW6F.4 Burns, Stephen A.- FM3F.6 Chauhan, Pooja - JTu3A.68, JW3A.76, JW4A.69 Conforti, Matteo - JW4A.46 Burrow, Joshua - JTu2A.96, JTu3A.103 Chávez-Cerda, Sabino - JTu2A.44 Conkey, Donald - JW4A.115 Burton, Harry - JW3A.16 Chen, Chi-Hau - JTu3A.107 Conry, Jessica P.- JW3A.18 Busch, David R.- FM3F, JTu2A.142, JTu3A Chen, Dongyu - FM4E.6 Contreras-Vallejo, Karla E. - JW3A.84 Busch, Kurt - JTu2A.67, JTu3A.49, LM1B.6 Chen, Fangyuan - JW4A.80 Cooper, Nicholas - LTh3F.2 Busto, David - LTu5F.3 Chen, Jiahao - JW3A.40 Copie, Francois - JW4A.32 Butko, Leonid - JW4A.100 Chen, Jian-Ling - JTu2A.36 Copner, Nigel - JTu3A.89 Bychkov, Igor - JW4A.100 Chen, Jiayang - JTu2A.87, JTu3A.100 Coppola, Sara - JTu2A.2 Byrd, Matthew - FM3E.4, FTu4E.1 Chen, Jia-Yang - FW5B.2 Correa Mena, Ana G.- JTu2A.84, JW4A.87 Byrnes, Tim - LM1B.1 Chen, Jie - JW3A.4 Corwin, Kristan - JW4A.95 Chen, Jing - FW5B.3, JTu3A.74 Côté, Geoffroi - JW4A.28 C Chen, Jinnan - JTu2A.108, JW3A.99 Courjal, Nadege - JW3A.23 C. Ralph, Timothy - JTu2A.55 Chen, Jun-Lin - JTu2A.19 Courtial, Johannes K.- FM3C.7, JW3A.126 Cacace, Teresa - JW3A.110 Chen, Nan-Kuang - JTu2A.109, JTu2A.81, JTu3A.66 Cousin, Seth L.- JW4A.14 Cadore, Alisson - FW5E.5 Chen, Shih-Hung - FTu4C.3 Cox, Kevin C.- JTu2A.54, JW4A.57, JW4A.64 Caesar, Lorna - FM4B.6 Chen, Szu-Yu - JTu2A.36 Coyle, Donald B.- FM3D.6 Cai, Wei - JW4A.99 Chen, Tao - JTu2A.112, JW3A.93 Crespi, Andrea - JTu3A.60 Caldwell, Joshua D.- FW5E.3 Chen, Wei-Ting - LW1F.1 Cryan, Martin - JTu3A.86 Calero Vila, Venancio - JW3A.23 Chen, Xi - JW3A.32 Cui, Liang - JW3A.78, LM1B.4, LM1B.8 Calin, Bogdan S.- JTu3A.138 Chen, Xudong - JW3A.22 Cumming, Benjamin P.- FM4F.2, FW5E.4 Calvi, Chase - LTu4F.2 Chen, Yang-Fang - JTu2A.12, JW4A.119 Cundiff, Steven T.- LW6F.2 Camacho, Ryan M.- JTu2A.138 Chen, Yong - FW6B.3 Cunningham, Brian - JTu3A.119, JW3A.109 Camacho-González, Guillermo - JTu3A.59 Chen, Yu - JW3A.117, JW3A.118 Currie, Marc - JW4A.40 Camarillo-Avilés, Andrés - JTu2A.77 Chen, Ziyang - JTu2A.70, JW3A.22 Curtis, Alden H.- LTu4F.2 Campbell, Melanie C.- JTu2A.3 Chen, Zong H.- JW3A.20 Cutler, Alex - JW4A.16 Canales, Arturo - JTu3A.113 Cheng, Gangge - JW4A.3 Cvijetic, Milorad - JTu3A.63 Cao, Bocheng - JTu3A.16 Cheng, Jiangtao - JTu3A.82 Cao, Dingcai - JTu3A.109 Cheng, Long - JW3A.46 D Cao, Hui - JTu2A.101 Cheng, Weifeng - JTu3A.82 da Silva Ferreira, Adriano - JW4A.94 Cao, Jie - JW4A.128, JW4A.129 Cheng, Xiaofeng - JW4A.117 Dadoenkova, Yuliya - JTu3A.134 Cao, Yusheng - JW4A.84 Cheng, Yang - JW4A.128, JW4A.129 Dahlem, Marcus S.- JTu2A.92 Capasso, Federico - LW1F.1, LW5F Cheng, Zhenzhou - FTu4B.2 Dahlström, J. M.- LTu5F.3 Capeluto, Maria - LTu4F.2 Cheng, Zihao - JW3A.38 Dai, Zongren - JTu3A.26 Cardea, Ivan - JTu3A.32 Chengfei, Guo - JTu2A.134, JW4A.135 Dakka, Milad A.- JW3A.54 Cardwell, Drew - JTu3A.15 Cherif, Rim - JTu2A.18 Dalacu, Dan - JW3A.7 Carfano, Caitlin - JTu3A.73 Chernikov, Alexey - JW3A.67 Daley, Andrew J.- JW4A.74 Carlson, Chelsea L.- JW3A.7 Chetty, Dashavir - JW3A.54 Dalir, Hamed - JTu2A.115 Carmen I., Cabello - JW4A.140 Chiaramonti, Ann N.- FTu5C.3 Dallachiesa, Lauren - JTu2A.1 Carney, Daniel - JW3A.24 Chiragh, Furqan - FM3D.6 Danz, Norbert - JW3A.65

FiO + LS 2018 • 16–20 September 2018 93

FiO Abstracts.indd 59 8/20/18 9:11 AM Darak, Mayur S.- JTu3A.99 Ducin, Izabela - JW4A.134 Fedyanin, Andrey A.- JW3A.49, JW4A.97 Das, Pratyusha - JTu2A.100 Dudovich, Nirit - JTu3A.48 Feifel, Raimund - LTu5F.3 Das, Ritwick - JTu2A.99 Dunkelberger, Adam - JW4A.54 Feigl, Beatrix - JTu3A.109 Das, Subrata - JW3A.98 Durach, Maxim - JW3A.102 Felipe, Alfonso M.- JTu3A.21 Dasa, Manoj Kumar - FM3F.5 Durán Sanchéz, Manuel - JTu2A.11, JTu3A.136 Felle, Martin - FTh3D.1 Daskalakis, Konstantinos - FM3G.3 Duran, Vicente - LTh1F.3 Feng, Hang - JTu3A.128 Datta, Prasanta Kumar - JW3A.36, JW4A.49 Duran-Ledezma, Angel A. - JTu3A.135 Feng, Philip - JTu2A.86 Dauliat, Romain - FW1E.2 Duran-Sanchez, Manuel - FTu4B.5, LTu5F.4 Ferenczi, Gergely - JTu3A.18 Dave, Utsav - FTu5E.3 Durán-Sánchez, Manuel - JTu2A.77, JW4A.4 Fernández, Andrea - JW4A.27 Davidson, Roderick - JW4A.54 Dutt, Avik - FTu5E.3 Fernández, Felix - JTu3A.123 Key to Authors Davis, Alex O.- JW4A.79 Dwapanyin, George O.- JTu2A.34 Ferrari, Andrea - FW5E.5 Dawes, Judith M.- FTu5C.1 Ferrari, Simone - FTu4E.5 De Angelis, Lorenzo - FM3C.3, JTu2A.48 E Ferraro, Alessandro - JW3A.72 De Boni, Leonardo - JTu2A.9 E, Yiwen - JW4A.36 Ferraro, Pietro - JTu2A.2, JTu3A.122, JW3A.110, De Fazio, Domenico - FW5E.5 Eagala, Sai R.- JTu2A.83 JW3A.116 De Luca, Eleonora - JTu3A.83 Ebendorff-Heidepriem, Heike - JW3A.112 Ferreira, Placid - JTu3A.14 De Lucia, Francesco - FW6B.4 Eberly, Joseph H. - JW4A.38 Ferris, Natalie - JW4A.23 de Paula D’Almeida, Camila - JW4A.120 Ebongue, Christiane - FM4B.6 Feygelson, Tatyana - JW4A.40 de Sterke, C. Martijn - JW4A.78 Ebrahim-Zadeh, M. - JW3A.41, JW4A.50 Field, Jeff - JTu3A.108 De, Anulekha - JW4A.49 Eckstein, Andreas - FTh3D.2, JTu3A.58 Field, Jeffrey J.- FM4C.3, JTu3A.104 De, Dhananjoy - JTu2A.59, JW4A.107 Edwards, Matthew - JTu3A.140, JW3A.137, Fienup, James R.- FM4C.5, JTu2A.131 De, Syamsundar - JTu3A.56 JW3A.30 Filoteo-Razo, Jose D.- JTu3A.78, JW3A.84 Debardelaben, Christopher - JW3A.16 Egami, Chikara - JTu3A.105 Finan, Emily - FM3D.1 Dedic, Jan - FM4B.3 Eggebrecht, Adam T.- FM3F.1 Flamini, Fulvio - JTu3A.60 Deepti Vaidyanathan, Deepti - JW3A.70 Eggleton, Benjamin J.- JW4A.58 Fleischmann, Friedrich - JW4A.8 deHarak, Bruno A.- JW3A.54 Eigner, Christof - LM3B.1 Flores, Sofia - JTu2A.85 Del Bino, Leonardo - JW4A.32 El-Fiky, Eslam - JW4A.10 Floyd, Thomas F.- JTu2A.142 Delfyett, Peter - LM3A El-Ganainy, Ramy - FW1E.1 Foley, Justin - LW6F.1 Del’Haye, Pascal - JW4A.32 Elgarf, Mahmoud M.- JW3A.106 Folland, Thomas G.- FW5E.3 Delia B., Soria - JW4A.140 El-Ghazawi, Tarek - JTu2A.115, JW3A.123 Fomra, Dhruv - JTu2A.22 Demchenko, Petr - JTu2A.40 Ellenbogen, Tal - JTu3A.101 Fontaine, Quentin - FW5C.4 Demeter, Anat - JTu3A.96 Ellis, Andrew - JW3A.77 Fontana, Jake - JW3A.95 DeMille, David - LTh2B.1 El-Rifai, Joumana - JTu3A.9, JW3A.9 Förster, Ronny - FM4E.7 Deneva, Margarita - JW4A.17 Elsner, Ann E.- FM3F.6 Franson, James - JW4A.66 Deng, Sheng - JW4A.80 Enam, Chowdhury - JTu3A.33 Frantz, Jesse - FM3C.1 Dennis, Mark R.- FM3C.4 Engheta, Nader - FM4F.1 Franz, Philipp - FW6E.2 Depto, Robin - FM4B.7 Englert, Christoph - JW3A.126 Frese, Erich - FM3D.6 Derevyanko, Stanislav - JTu3A.79, JW3A.83 Englund, Dirk .- FW6D.1 Friberg, Ari - JTu3A.28 Deschenes, Jean-Daniel - FTh3C.4 Erickson, Michael - JTu2A.1 Friberg, Ari Tapio - FTh3B.3, JW4A.12 Desouky, Mai - JTu2A.103, JTu3A.97 Esporlas, Cindy Liza C.- JTu3A.6 Frolov, Aleksandr - JW4A.97 Devane, Patrick A.- JW3A.31 Essameldin, Mahmoud - JW4A.8 Fu, H. Y. - JTu2A.42 Devaux, Fabrice - JTu2A.65 Estudillo Ayala, Julian Moises - JTu2A.79, Fu, Haoyang - JTu3A.124, JTu3A.127, JW4A.130, Dianat, Pouya - JW4A.1 JTu3A.76, JW3A.84 JW4A.132 Dichtl, Paul - FTu5A.2 Estudillo-Ayala, Julian M.- JTu3A.78, JW4A.13 Fu, Yuxi - JW3A.130, LTu4F.3, LTu5F.2 Dickson, Ivan - JTu3A.8 Eugui, Pablo - JTu2A.128 Fuchs, Ulrike - FM3D.5 Diddams, Scott A.- FTh3C.3 Evans, Matthew - JW4A.77 Fukutake, Naoki - JTu2A.41 Diederich, Benedict - FM4E.7 Ezhov, Vasily A.- JW4A.127 Funes, Gustavo L.- JTu2A.82 Diels, Jean Claude - JW3A.6, LW6F.5 Furch, Federico J.- FTh3C.5 Diercks, David R.- FTu5C.3 F Furusawa, Akira - JW4A.60, JW4A.63 Dillies, Jimmy - JW3A.102 Fabbri, Simon - JTu3A.32 Ding, Qing - JTu3A.14 Fabre, Baptiste - JTu3A.48 G Ding, Shoujun - JW4A.138 Fabre, Claude - JTu3A.56 Gabrielli, Lucas H.- JTu3A.120, JW3A.124 Ding, Ziqian - JW3A.12 Faehnle, Oliver - JTu2A.30 Gaeta, Alexander - FTu5E.3 Divitt, Shawn - FW6E.3 Fairchild, Shermineh R.- FTh3E.7, JTu2A.50 Gajanandana, Oraprapai - JTu3A.112 Djevarhidjian, Leao - LTh1F.3 Fales, Andrew M.- FM3F.4 Gajewski, Andrzej - FW6C.4 D’Mello, Yannick - JW4A.10 Fali, Alireza - FW5E.3 Galili, Michael - FTu5B.4 Do, Phuong Ahn - JW3A.48 Fan, Heng - JTu3A.100 Galka, Maciej - JW4A.79 Dobosz, Jakub - JW3A.55 Fan, Shanhui - FW1C.3 Gallegos Arellano, Eloísa - JW4A.13 Doh, Iyll-Joon - JTu2A.25 Fan, Shengli - FTh3E.4 Galstian, Alexander - JW4A.127 Dolinski, Michal - JW3A.125 Fan, Songtao - JTu3A.44 Gan, Qiaoqiang - JTu2A.32, JW3A.90 Domingue, Scott - JTu3A.104 Fan, Xintong - JW4A.130 Gandhi, Aruna M.S.- FTh3B.5, JTu2A.95 Dominguez-Pachecano, Ariel - JTu2A.46 Fang, Bin - JW3A.61, LM1B.7 Ganesan, Adarsh - LW6F.1 Dong, Mark - LW6F.2 Fang, Renpeng - FTh3B.4 Ganoza-Quintana, Jose Luis - JTu3A.106 Dong, Ruifang - JW4A.11, JW4A.89 Fang, Shaobo - FTu4B.4 Gao, Feng - JTu2A.142 Donodin, Alexander I.- JTu3A.47 Fanjul-Velez, Felix - FM3F.3, FM4E, JTu3A.106 Gao, Shaobo - JW3A.63 Dorrah, Ahmed - JW4A.6 Farrer, Ian - FTh3D.1 Gao, Zhixing - FTu4C.4 Dowling, Jonathan P.- JTu3A.93, JW3A.70, LM1B.1 Farsari, Maria - FM4B.4 Gao, Zhi-xing - JTu3A.40 Drake, Tara E.- JTu2A.62 Fasano, Nicholas M.- JW3A.30 García Juárez, Alejandro - JW4A.87 Drees, Martin - JTu3A.15 Fathpour, Sasan - JTu3A.59 Garcia-Caurel, Enric - JW4A.27 Du, Xieyu - JTu2A.129 Fears, Kenan - JW4A.54 Garcia-Melgarejo, Julio C.- JTu2A.46 Dubey, Vishesh Kumar - FM4E.4 Feder, Linus - JW4A.31 Garcia-Mina, Diego - JTu3A.76 Dubov, Mykhaylo - JTu3A.34 Fedorov, Vladimir Y.- FM4B.4 Garikapati, Malvika - JTu3A.8

94 FiO + LS 2018 • 16–20 September 2018

FiO Abstracts.indd 60 8/20/18 9:11 AM Garra, Brian - FM3F.2 Guan, Tian - JW4A.122 Heckmann, Jan - FW6E.2 Gärtner, Claus - FW1E.3 Guang, Zhe - JTu3A.2 Heffernan, Jon - FTh3D.1

Gast, Thomas J.- FM3F.6 Gubin, Mikhail - JTu3A.141 Hegmann, Frank - JW3A.33 Key to Authors Gatelum Barrios, Abraham - JTu3A.76 Guha, Saikat - LM1B.2 Heilmann, Ralf - JW4A.52 Gates, James - FTh3D.2 Guillermo, Bertolini - JW4A.140 Heinrich, Matthias - JTu3A.49 Gautam, Abhinav - JTu2A.83, JW3A.107, JW4A.85 Gulkin, Dmitry N.- JW4A.97 Heintzmann, Rainer - FM4E.5, FM4E.7 Gautam, Surya - JTu2A.21, JW3A.8 Gulley, Jeremy R.- JW4A.73 Helmy, Amr - JTu2A.89 Gauthier, Daniel J.- JW3A.66 Guo, Cheng - JW3A.78, LM1B.8 Hemmati, Hafez - JTu3A.85 Gauthier-Manuel, Ludovic - JW3A.23 Guo, Hong - FTh1B.2, JTu2A.129, JTu2A.136, Hemnani, Rohit - JW4A.96 Gaylord, Thomas K.- JTu2A.74 JTu2A.137, JTu2A.70, JW3A.127, JW3A.85, Hempler, Nils - FW5D.1 Gaynor, James D.- JTu2A.8 JW4A.133 Hendon, Christine P.- FM4E.1 Gbur, Gregory J.- FTh1C, JTu3A.10, JTu3A.36 Guo, Junpeng - JTu2A.108, JW3A.99 Hendrickson, Joshua R.- JTu2A.108 Ge, Li - JW3A.51, JW3A.92, JW4A.41 Guo, L. Jay - JTu3A.14 Hendrie, James - LW6F.5 Ge, Wenchao - FW1E.4 Guo, Rui - FM3G.3 Henning, Thomas - JW4A.8 Geldmeier, Jeffrey A.- JW3A.95 Guo, Wenge - JTu3A.35, JTu3A.44 Heo, Duchang - JW3A.113 Georgantzis Garcia, Dimitris - JW3A.126 Gupta, Banshi D.- JW4A.102 Hepriyadi, Selvy U.- JTu3A.117, JW4A.112 George, Jonathan K.- JW3A.123 Gupta, Mool - JW3A.10 Hernández García, Juan Carlos - JTu2A.79 Gerardot, Brian - FW6C.2 Gupta, Neelam - JTu3A.91 Hernandez, Erika N.- JTu2A.77 Gerrits, Thomas - LM1B.6 Gurung, Sudip - FW6B.2, JTu2A.88, JTu2A.90 Hernández, Iván - JTu2A.85 Geskus, Dimitri - JTu3A.58 Gusev, Sviatoslav - JTu2A.40 Hernandez-Aranda, Raul I. - JTu3A.113 Ghassemi, Pejhman - JW3A.118, JW3A.19 Gustafson, Jon K.- JW4A.65 Hernández-Arriaga, Marco V.- JTu2A.11, Ghimire, Indra - FW6B.2 Gutierrez, Gustavo - JW4A.8 JTu3A.136, JW4A.4 Ghoreyshi, Ali - JW4A.71 Gutierrez-Castrejon, Ramon - JW4A.82 Hernandez-Figueroa, Hugo E.- JW3A.100, Ghosh, Amitava - JW4A.9 Gutiérrez-Cuevas, Rodrigo - FM3C.4, JW3A.34 JW4A.94 Ghosh, Sumit - JTu2A.123 Guzman-Silva, Diego - JTu3A.49 Hernandez-Garcia, Juan C.- JTu3A.76, JTu3A.78, Gibble, Kurt - LTh1F.2 Gyongyosi, Laszlo - FTh1B.3, JW3A.79 JW3A.84, JW4A.13 Gil, Jose J.- JW4A.12 Herrera Piad, Luis A. - JTu3A.76 Gillett, Geoff - JTu2A.55 H Herrmann, Harald - LM3B.1 Giordani, Taira - JTu3A.60, JW3A.72 Haaxman, Wouter - FW1E.3 Herzog, Bastian - JTu2A.64 Gisselbrecht, Mathieu - LTu5F.3 Haber, Louis - JW3A.47 Hess, Ortwin - FM2A Glasser, Ryan T.- JW3A.70 Habif, Jonathan - LM1B.2 Hewak, Dan - FW6B.4 Glorieux, Quentin - FW5C.4 Hache, Alain - JW3A.48 Hidayat, Achmad S.- JTu3A.117 Glover, Rohan - JW3A.54 Haddick, John - FW5A.2 Hien, Khuat Thi Thu - JW4A.111 Glückstad, Jesper - JTu2A.6 Hafezi, Mohammad - FTu5E.2 Hilbig, David - JW4A.8 Goh, Chia C.- JTu2A.142 Hagan, David J.- JTu3A.7 Hileman, Devin - LW6F.4 Golacki, Lukasz - JW3A.56 Haggerty, Bryan P.- FM3F.6 Hillenbrand, Rainer - LW5F.1 Goltsov, Aleksandr - JW3A.17 Haglund, Richard F.- FW5E.3 Hillier, Glen - JTu3A.15 Gombojav, Ariunbold - JTu2A.127 Haider, Golam - JTu2A.12, JW4A.119 Himananto, Orawan - JTu3A.112 Gomes, Anderson S.- JW3A.73 Hakala, Tommi - FM3G.3 Hird, Thomas M.- JW3A.63 Gomez, Sandra - FW1B.2 Hammond, Alec - JTu2A.138 Hitzenberger, Christoph - JTu2A.128 Gomez-Cardona, Nelson - JTu2A.97 Han, Dongchu - JTu2A.137, JW4A.133 Hobart, Karl - JW4A.40 Gómez-Correa, Jesús - JTu2A.44 Han, Hainian - FTu4B.4 Hofmann, Felix - JW3A.67 Gomon, Daniel - JTu2A.40 Han, Jae-Ho - JTu2A.122 Hogan, Benjamin T.- JTu2A.140, JTu3A.131, Gong, Lihui - JW3A.105 Han, Pingli - JTu2A.135, JTu3A.121, JW3A.129, JW3A.26 Gong, Qihuang - JTu3A.128 JW4A.136 Holdsworth, John L.- JW3A.54 Gong, Xiaojing - JTu2A.121 Hancock, Scott W.- FTu5C.4 Holland, Glenn - JW4A.56 Gong, Yongkang - JTu3A.89 Hangdong, Huang - FTu4B.4 Hollinger, Reed J.- LTu4F.2 González Mondragón, Luis A.- JW4A.87 Hannegan, John M.- JW3A.60 Honardoost, Amirmahdi - JTu3A.59 González, Andrés L.- JW4A.131 Hanson, Steen G.- JTu2A.20 Hong, Jongwoo - JTu2A.28 Gonzalo, Ivan - FM3F.5 Hao, Qun - JW4A.128, JW4A.129 Hong, Ming-Hwa - JTu3A.107 Gorman, Brian P.- FTu5C.3 Harari, Gal - FTu4C.1 Hönl, Simon - FTh3C.6 Gorman, Jason J.- JW3A.88 Harder, Georg - LM3B.1 Hooten, Sean - FTu4A.3 Gorodetsky, Michael - FW1C.2 Hardwick, Terra C.- JW3A.39 Hopkins, Patrick - JTu3A.39 Gougousi, Theodosia - JW4A.37 Harley, Brendan A.- JTu3A.119 Horng, Hannah - JW3A.118 Goun, Alexei - FTh3C.2 Harper, Danielle J.- JTu2A.128 Horsley, S. A. R. - FTh1E, FTh1E.1 Goy, Alexandre - FTh3E.5 Harry, Gregory M.- JW4A.77 Horstman, Luke - LW6F.5 Goyal, Parul - JTu2A.113 Harth, Anne - LTu5F.3 Hosseini, Sajed - JW4A.95 Graefe, Markus - JTu3A.49 Harutyunyan, Hayk - JW3A.45 Hou, Feiyan - JW4A.11 Grafton, Andrea B.- JW4A.54 Hasan, Mehedhi - JW3A.49 Houdré, Romuald - FTu4E.3 Granizo, Evelyn A.- JW4A.25 Hashemi Rafsanjani, Mohammad - JW3A.32, Howes, Austin A.- FW6E.5 Grassani, Davide - JTu3A.32 JW4A.124 Hsiao, Yu-Che - JW3A.133 Greinert, Rüdiger - JTu2A.116 Hashimoto, Yosuke - JW4A.60 Hsieh, Chang-Tsung - JTu2A.17, JTu2A.57 Greybush, Nicholas J.- JW3A.95 Hassett, Jeremy - FM3C.4, JW4A.124 Hsieh, Chia-Ying - FTu4C.3 Grier, David G.- JW4A.48 Hayden, Michael - JW4A.65 Hsieh, Yu-Hua - JW3A.133 Griffith, Alec R.- JTu3A.140, JW3A.137 Hayes, John R.- FW6B.3, FW6B.4 Hsu, Wei Liang - JTu3A.3 Grillot, Frederic - FTu5B.2, FW1B.2 He, Dong - JW4A.80 Hsu, Yun-Tzu - JTu2A.12 Gröblacher, Simon - FW1E.3 He, Jijun - JW3A.27 Hu, Fengming - FTu4C.4 Grootjans, Robert - JTu3A.58 He, Yang - FTu4E.2, FTu4E.4 Hu, Feng-Ming - JTu3A.40 Grosse, Nicolai B.- FW6E.2, JTu2A.64 He, Ying - JW4A.138 Hu, Jianqi - FM3C.2 Grüner-Nielsen, Lars - FTu5B.4 He, Yonghong - JW4A.122 Hu, Jonathan - JTu3A.1 Gu, Lingjia - JTu3A.124, JTu3A.127, JW4A.130 He, Zhe - JW3A.40 Hu, Qinglei - JW4A.116 Gu, Min - FM3D.2, FM4F.2, FW5E.4 Hecht, Bert - FTu5A.1 Hua, Hong - FTh1A.1

FiO + LS 2018 • 16–20 September 2018 95

FiO Abstracts.indd 61 8/20/18 9:11 AM Hua, Jianfei - JTu2A.132, JW4A.141 Jaramillo-Villegas, Jose A.- JTu2A.53 Kato, Takashi - JW4A.22 Huang, Chao - JTu2A.42 Jasion, Gregory T.- FW6B.3 Katori, Hidetoshi - LTh1F.1 Huang, Chen-Bin - FM3C.2 Jauregui Vazquez, Daniel - JW4A.13 Kaur, Parvinder - JW4A.103 Huang, Chenxi - JW3A.33 Jáuregui Vázquez, Daniel - JTu2A.79 Kawasaki, Shota - JTu3A.105 Huang, Chung-Che - FW6B.4 Jauregui, Daniel - JTu3A.76 Kawata, Yoshimasa - JW4A.24 Huang, Danhong - JW4A.73 Jauregui-Vazquez, Daniel - JTu3A.78, JW3A.84 Kawato, Sakae - JW3A.132 Huang, Fei - JW4A.117 Javerzac-Galy, Clément - FW5E.5 Kaymak, Vural - LTu4F.2 Huang, Feng X.- JW3A.119 Jen, Myungsam - JW4A.137 Kaypaghian, Kristina - FM4E.6 Huang, Heming - FTu5B.2, FW1B.2 Jeon, Kooknam - JW4A.137 Ke, Meijing - JTu2A.136 Huang, Jiayao - FTh3B.5 Jeong, Yeonwoo - JTu2A.122 Keeler, Gordon A.- FW1C.1 Key to Authors Huang, Kuidong - JTu3A.130 Jesse, Forrest F.- JTu3A.98 Kelley, Kyle - JTu3A.39 Huang, Lanlan - JW3A.87 Jeyaselvan, Vadivukkarasi - FW5B.4 Kelly, Priscilla - JW4A.106 Huang, Qinglan - JW3A.109 Ji, Dengxin - JTu2A.32, JW3A.90 Keren-Zur, Shay - JTu3A.101 Huang, Rongle - JTu2A.93 Ji, Xingchen - FTu5E.3 Ketterle, Wolfgang - JW4A.74 Huang, Shengzhi - JTu2A.135 Jia, Simeng - JTu3A.86 Khader, Isaac - FTh3C.4 Huang, Tsan-Hsueh - JTu3A.107 Jiang, Haifeng - JTu3A.35, JTu3A.44 Khajavikhan, Mercedeh - FTu4C.1, FTu5E.1 Huang, Tung-Ke - JTu2A.78 Jiang, Lingjun - JTu2A.75 Khalil, Munira - JTu2A.8 Huang, Yin - JTu3A.93 Jiang, Zack - JTu3A.38 Khampirat, Buratin - JW4A.125 Huang, Yi-Teng - FW6E.4 Jiao, Dongdong - JW4A.11 Khan, Gufran - FM3D.4, JTu3A.11, JW4A.9 Huang, Yundi - FTh1B.2 Jin, Lei - FTu4B.2 Khandaker, Murshed - FTu4E.1 Huang, Yu-Ping - FM3C.5, FW5B.2, JTu2A.87, Jin, Long - FM4E.2 Khanolkar, Ankita - JTu2A.43 JTu3A.100, JTu3A.30, JTu3A.5, JTu3A.8 Jin, Tao - JTu2A.3 Khilo, Anatol - JTu2A.92 Huang, Zhaoran R.- JTu2A.75 Jing, Feng - JTu2A.24 Khodzitsky, Mikhail - JTu2A.40 Huard, Corentin - FTu5C.1 Jipa, Florin - JTu3A.138 Khoury, Rami A.- JW3A.47 Huffaker, Diana L - JTu3A.89 Jisha, Chandroth P.- FW5C.3, JTu2A.61, JW4A.76 Khromov, Maxim - JW3A.128, JW4A.123 Hughes, Stephen - JW3A.7 Johnson, Anthony M.- JTu3A.38, JW4A.37 Kik, Pieter G.- JTu3A.92, LW2B Hughes, Tyler W.- FW1C.3 Johnston, Nolan - JTu3A.102 Kikunaga, Kazuya - JW3A.97 Hugues, Guillet de Chatellus - LTh1F.3 Jokerst, Nan M.- JW4A.113 Kilosanidze, Barbara N.- JTu3A.17 Hung, Jui-Ting - JTu2A.36 Jones, Dan - JTu3A.61 Kim, Donghyun - JW3A.101, JW4A.98 Huo, Nan - LM1B.4 Jones, Jason - JTu3A.108, JW4A.34 Kim, Hak Hee - JW3A.113 Hurot, Charlotte - FTu5C.1 Jopson, Robert - FTu5B Kim, Huisung - JTu2A.25 Huwer, Jan - FTh3D.1 Jorissen, Lode - FTh3E.2 Kim, James D.- JTu2A.26 Hyde, Milo W.- JW3A.14 Joshi, Chan - JTu3A.50, JW4A.141 Kim, Je-Hyung - FW6C.3 Jügler, Alexander - FM4E.5, FM4E.7 Kim, Joonwoo - JW4A.137 I Julian, Matthew - JW3A.10 Kim, Kee-Hyun - JW3A.113 Ibarra-Escamilla, Baldemar - FTu4B.5, JTu2A.11, Julku, Aleksi - FM3G.3 Kim, Ki-Yong - FTu5C.2, JW3A.52 JTu2A.77, JTu3A.136, JW4A.4, LTu5F.4 Junqueira, Mateus A.- JTu3A.120, JW3A.124 Kim, Kyoung-Ho - JW3A.44 Ichihashi, Yasuyuki - FTh3E.2 Kim, Kyujung - JTu2A.120, JTu2A.124, JW3A.104, Ihn, Yong Sup - LM4A.2 K JW4A.21 Ilev, Ilko - FM3F.4 Kaczmarek, Krzysztof - FTh3D.2 Kim, Soojung - JTu2A.124 Ilic, B. Robert - JW4A.56 Kadhim, Ahmed C.- JTu2A.27, JTu3A.110, Kim, Taeyeon - JW3A.104, JW4A.21 Iljin, Andrey - JTu2A.45 JTu3A.52 Kim, Yong-Su - JTu2A.13 Imany, Poolad - JTu2A.53, JTu3A.55, JTu3A.69 Kadochkin, Aleksei - JTu3A.134 Kim, Yoon-Ho - LM4A.2 Imre, Sandor - FTh1B.3, JW3A.79 Kaew-aram, Saharat - JW3A.21 Kim, Youngsik - FM3D.1 Inami, Wataru - JW4A.24 Kaiser, Florian - FW1E.2 Kimbrue, Malik - JW3A.52 Innocenti, Luca - JW3A.72 Kakarenko, Karol - JW4A.134 Kincaid, Nicholas - JTu3A.14 Inoue, Taiki - FTu4B.2 Kakauridze, George - JTu3A.17 Kinsey, Nathaniel - JTu2A.22 Iosub, Stefana - JTu3A.138 Kakkava, Eirini - FTh1E.3, JW4A.115 Kippenberg, Tobias - FTh3C.6, FW1C.2, FW5E.5 Isaac, Justin - JW3A.91 Kalinski, Matt - JTu2A.10 Kirby, Brian T.- JTu3A.61 Isaacs, Joshua J.- JW3A.29, JW4A.35 Kallhammer, Jan-Erik - FM1A.1 Kireev, Alexey - JTu3A.141 Isinger, Marcus - LTu5F.3 Kalra, Yogita - JTu2A.104, JTu2A.105, JTu2A.113, Kirk, Alex - JTu3A.15 Islam, Mehedi - FTh1C.1 JW4A.69 Kirk, Rodney - JW3A.112 Islam, Nurul T.- JW3A.66 Kamali, Khosro - JTu3A.12 Kis, Zsolt - FTh3B.6 Ismaeel, Rand - JTu3A.16, JTu3A.70 Kamer, Brian - JW3A.6 Kitzler, Ondrej - LW6F.6 Itzler, Mark A.- FM3E.2 Kaminer, Ido - FTh3C.7 Klitzing, Regine V.- FW6E.2 Ivashkin, Peter - JW4A.127 Kane, Daniel - JTu3A.104 Klug, Michael - FTh3E, FTh3E.1 Iwakoshi, Takehisa - JTu2A.60 Kane, Tim - JTu3A.77 Kneller, Omer - JTu3A.48 Iwane, Toru - JTu3A.132 Kanetake, Tomoki - JW3A.132 Knight, Peter L.- FTh2A.1 Izyumskaya, Natalia - JTu2A.22 Kang, Pilgyu - JW3A.44 Knoerzer, Markus - JTu2A.118 Kang, Tae Young - JTu2A.124 Ko, Brian - JTu2A.88 J Kanyathare, Boniphace E.- JW4A.125 Ko, Heasin - JW4A.72 Jabir, M. V.- JTu2A.56 Kapteyn, Henry C.- FTu5C.3, JW4A.14 Kobayashi, Ryo - JW3A.132 Jacinto-Méndez, Damián - JTu3A.135 Karapetyan, Narek - JTu3A.45 Kobulashvili, Irina - JTu3A.17 Jackson, David P.- JW4A.23 Karar, Vinod - FM3D.4, JTu3A.24 Kobulashvili, Irine - JTu3A.21 Jacob, Chacko - JW4A.101 Karasik, Valeriy - JTu3A.141, JTu3A.47 Kochanska, Paula A.- JW4A.134 Jacobs, Kyle - JTu3A.14 Karpinski, Michal - JW4A.79 Koilpillai, David - JW4A.81 Jaimes-Nájera, Alfonso I.- JTu2A.44 Karpov, Maxim - FW1C.2 Koirala, Milan - JTu2A.101 Jakl, Petr - FM4B.1 Kärtner, Franz - JTu2A.116 Kolarczik, Mirco - JTu2A.64 Jakobsen, Michael L.- JTu2A.20 Kasdorf, Stephen - LTu4F.2 Kolchiba, Mykyta - JW4A.24 James, Timothy - FM4C.4 Kashyap, Raman - JW3A.73 Kollin, Joel S.- FW6A.4 Jamier, Raphael - FW1E.2 Kassi, Samir - LTh1F.3 Kolthammer, W. Steven - FTh3D.2 Jang, Dogeun - FTu5C.2, JW3A.52 Kataoka, Shunji - JW3A.132 Komar, Andrei - JTu3A.12

96 FiO + LS 2018 • 16–20 September 2018

FiO Abstracts.indd 62 8/20/18 9:11 AM Kondakci, Hasan E.- FTh3E.7, JTu3A.20, JW4A.7 Lapkiewicz, Radek - JW4A.139 Li, Lu - JW4A.55 Kondratenko, Sergii - JW4A.105 Larkin, Ilia - JW4A.29 Li, Ming - JTu3A.63

Kong, Cihang - JTu2A.121 Lassas, Matti - JTu2A.4 Li, Mingxiao - FTu4E.2, FTu4E.4 Key to Authors Kong, Weijing - JTu2A.98 Lauterio-Cruz, Jesus P.- JTu3A.78 Li, Pei - JW4A.116 Korn, Tobias - JW3A.67 Law, F. K. - JTu2A.80 Li, Poking - FW6A.3 Korolov, Anastasia - JW3A.5 Lawall, John - LW6F.1 Li, Qian - FTh3B.5, JTu2A.42, JTu2A.93, JTu2A.95, Korotkova, Olga - JW3A.32 Lazarev, Vladimir A.- JTu3A.141, JTu3A.47 JW3A.38, JW3A.4, JW4A.67 Kottos, Tsampikos - JW4A.92 Lazo Arjona, Oscar - JW3A.63 Li, Shuai - FTh3E.5 Kouadou, Tiphaine - JTu3A.56 Le, Quang Trung - JTu2A.4 Li, Tiaohua - JW4A.133 Kouyama, Wataru - JW4A.111 Leaird, Daniel E.- JTu2A.53, JTu3A.69 Li, Wei - JTu2A.134, JW4A.135 Kovacevic, Goran - FTu4B.2 Leal Cruz, Ana L.- JW4A.87 Li, Xiao - FTh3E.3 Kowalczyk, Adam - JW4A.134 Leavitt, Richard P.- FW6C.3 Li, Xiaoying - JW3A.78, LM1B.4, LM1B.8 Krainak, Michael - FM4B.6, FM4B.7 LeBrun, Thomas W.- JW3A.88 Li, Xuan - JTu2A.135, JW4A.136 Kravchenko, Ivan - FW6E.5 Ledingham, Patrick - FTh3D.2, JW3A.63 Li, Xudong - JTu3A.133 Krawczyk, Maciej - JW4A.104 Lee, Andrew - JW3A.136 Li, Yan - JTu3A.128 Kremers, Jan - JTu3A.109 Lee, Byoungho - FM4C, JTu2A.15, JTu2A.28 Li, Yanlu - FW6E.1 Kress, Bernard - (blank) Lee, Changhun - JW3A.101, JW4A.98 Li, Yihong - JW3A.4 Kroon, David - LTu5F.3 Lee, Chang-Min - FW6C.3 Li, Ying Lia - JTu3A.81 Kropp, Jaron - JW4A.37 Lee, Dongjin - LM4A.2 Li, Yulin - JW4A.80 Krueger, Michael - JTu3A.48 Lee, Eun S.- JTu2A.31 Li, Zeren - JW3A.93 Krysa, Andrey - FTh3D.1 Lee, Gun-Yeal - JTu2A.15 Li, Zhan - JTu2A.87 Kudlinski, Alexandre - JW4A.46 Lee, Howard - FW6B.2, JTu2A.88, JTu2A.90, Li, Zhengbin - JW4A.80 Kuebel, David - JTu3A.28 JW3A.65 Li, Zhengyu - JTu2A.70 Kues, Michael - FTh1C.1 Lee, Hwang - JW3A.70 Li, Zhong-Ying - JTu2A.78 Kuipers, L. - FM3C.3, FTu5E.4, JTu2A.48 Lee, Jaesung - JTu2A.86 Liang, Hanxiao - FTu4E.2, FTu4E.4 Kuis, Robinson - JTu3A.38, JW4A.37 Lee, Kyookeun - JTu2A.26 Liang, Yizhi - FM4E.2 Kulkarni, Dr. Rishikesh - JTu2A.23 Lee, Kyu - JW3A.98 Liao, Wei-Cheng - JTu2A.12, JW4A.119 Kumar Bag, Saawan - JTu3A.94, JW4A.101 Lee, Min Won - JTu2A.84 Liao, Yu-Ming - JTu2A.12, JW4A.119 Kumar, Ajai - JW3A.37 Lee, Mon-Juan - JTu3A.3 Liao, Zhi M.- LTu4F.4 Kumar, Ajeet - JTu3A.68, JW3A.76, JW4A.69 Lee, Sebok - JW4A.137 Liapis, Andreas - JW3A.71 Kumar, Amar - JW4A.10 Lee, Sun-Goo - JTu2A.107 Lichtenegger, Antonia - JTu2A.128 Kumar, Amitesh - JTu2A.83, JW4A.85 Lee, Timothy - JTu3A.16, JW3A.12 Light, Philip S.- JW3A.54 Kumar, Avesh - JW4A.53 Lee, Wei - FTh3E.6, JTu2A, JTu3A.3, JW3A Lihachev, Grigory - FW1C.2 Kumar, Cheruvu S.- JW4A.101 Lee, Woowon - JTu2A.119 Lim, Charles C.- JW3A.66 Kumar, Gyanendra - JW3A.81 Lee, Yeji - JTu2A.120, JW3A.104 Lima, Bismarck C.- JW3A.73 Kumar, M. Ravi - JW3A.103 Leger, Joel - JTu2A.8 Lima, Mario - JTu3A.88 Kumar, Mukesh - JTu3A.24 Léger, Zacharie M.- JTu2A.89 Lin, Aoxiang - JTu2A.24 Kumar, Pardeep - FW1E.4, JW3A.89 Lei, Ming - JW3A.115 Lin, Hong - JW4A.68 Kumar, Parvendra - JTu3A.65 Leibfried, Dietrich - FW1D.2 Lin, Hung-I - JW4A.119 Kumar, Prem - LM3A.1 Leija, Armando P.- JTu2A.67, JTu3A.49 Lin, Ming-Wei - FTu4C.3 Kumar, Rahul - JW3A.76 Lemasters, Robert D.- JW3A.45 Lin, Qiang - FTu4E.2, FTu4E.4, JTu2A.86 Kumar, Rajesh - JTu2A.102, JW3A.81 Lembessis, Vassilis - FM3C.7 Lin, Shih-Yao - JTu2A.12, JW4A.119 Kumar, S. C.- JW3A.41, JW4A.50 Lenaphet, Yutana - JTu3A.115 Lin, Tai-Yuan - JW4A.119 Kumar, Santosh - FM3C.5, FW6C.2, JTu2A.109, Lenzner, Matthias - LW6F.5 Lin, Ting-Xuan - JW3A.121 JTu2A.81, JTu3A.5, JTu3A.66 Leon Montiel, Roberto D.- JTu2A.67, LM1B.6 Lin, Tong - FTu5E.3 Kumar, Shanu - JTu3A.68 Leon-Montiel, Roberto - JTu3A.49 Lin, Wei - JTu2A.142 Kumari, Madhuri - JW3A.31 Lett, Paul - JW3A.59, JW3A.64, JW4A.62 Lin, Wei-Ju - JTu2A.12, JW4A.119 Kumari, Neelam - JTu3A.24 Leuchs, Gerd - FM3C.6, FTh3B.3 Lin, Yi-Hsin - FM3D.7, JTu2A.19 Kumari, Soumya - JW3A.107 Levine, Martin - JTu3A.25 Lin, Yueh-Chern - FTh3E.6 Kunz, Paul D.- JTu2A.54, JW4A.57, JW4A.64 Lewis, Adam - FW6B.4 Lindroth, Eva - LTu5F.3 Kuo, Hsin Yu - FW6E.4 Lezec, Henri - FW6E.3, JW4A.56 Lingaraju, Navin B.- JTu3A.69 Kuo, Paulina S.- JTu3A.62 L’Huillier, Anne - LTu5F.3 Lipson, Michal - FM4F.3, FTu5E.3 Küppers, Franko - JTu2A.4 Li, Can - JTu2A.121 Lita, Adriana E.- LM1B.6 Kurniawati, Intan D.- JTu3A.117 Li, Dayu - JW3A.129 Litchinitser, Natalia M.- FM3C.1 Kurt, Suat - JW4A.43 Li, Guangkuo - JW4A.67 Little, Brent - FTh1C.1 Kutuzyan, Aghavni - JTu3A.45 Li, Guifang - FTh3E.4 Litvinyuk, Igor - JW3A.54 Kuyk, Kevin - JW3A.71 Li, Hao - JW4A.55 Liu, Cheng-hui - JTu3A.118, JW4A.3 Kuzin, Evgeny A.- FTu4B.5, JTu2A.11, JTu2A.77, Li, Haowei - JTu3A.75 Liu, Chengpu - JTu2A.35 JTu3A.136, JW4A.4, LTu5F.4 Li, Hongyi - JW4A.23 Liu, Fei - JTu2A.135, JTu3A.121, JW3A.129, Kuzmich, Alex - JW4A.61 Li, Hongyun - JW3A.87 JW4A.136 Kuznetsova, Lyuba - FW6B, JW4A.106 Li, Huanan - JW4A.92 Liu, Jiaqi - JTu3A.75, JW4A.99 Kwak, Kyusub - JTu2A.26 Li, Jia - JW3A.32 Liu, Jietao - JTu2A.134, JW4A.135 Li, Jia-Han - JTu2A.17, JTu2A.57 Liu, Jinwei - FM4E.2 L Li, Jiamin - LM1B.4 Liu, Jui-Nung - JW3A.109 La Volpe, Luca - JTu3A.56 Li, Jiang - JW3A.43 Liu, Junqiu - FW5E.5 Laane, Jaan - JW3A.40 Li, Jiawen - JW3A.112 Liu, Ke - FW5E.2 Labonté, Laurent - FW1E.2 Li, Jing - FTu4C.4, JTu3A.40 Liu, Keng-Ku - JW3A.109 Lahiri, B. - JW4A.101 Li, Junhui - JTu2A.129, JTu2A.136, JTu2A.137, Liu, Longju - JTu3A.87 Lai, Yiming - FTu4E.3 JW3A.127, JW4A.133 Liu, Qing H.- FW6C.5 Lalonde, Jean-François - JW4A.28 Li, Liming - JTu3A.13 Liu, Shuang - JTu2A.24 Lan, Pengfei - JW3A.130 Li, Linnan - FW5B.3, JTu3A.74 Liu, Tao - JW4A.11, JW4A.89 Lantz, Eric - JTu2A.65 Li, Longhui - JW4A.117 Liu, Wei - JTu2A.116

FiO + LS 2018 • 16–20 September 2018 97

FiO Abstracts.indd 63 8/20/18 9:11 AM Liu, Xu - JTu3A.80 Mait, Joseph N.- JW3A.13 Meyer-Scott, Evan - LM1B, LM3B.1 Liu, Xuanyi - JTu2A.95 Maiti, Rishi - FW5E.2, JTu3A.73, JW3A.97, Miaja Avila, Luis - FTu5C.3 Liu, Yi - JW3A.117, JW3A.118 JW4A.96 Miao, Bo - JW4A.31 Liu, Youhai - JTu2A.32, JW3A.90 Majury, Helena - JW3A.72 Miccio, Lisa - JW3A.116 Liu, Yuhong - LM1B.4 Makarov, Alexandre - JW4A.30 Michelsen, Hope A.- LTh3F.4 Liu, Zexuan - JW4A.126 Makhal, Krishnandu - FM4B.5 Midorikawa, Katsumi - JW3A.130, LTu4F.3, LTu5F.2 Loock, Peter V.- JW4A.60 Makowski, Michal - JTu2A.130, JW3A.125, Mikalopas, John - JW4A.75 Loparo, Zachary E.- LTh3F.3 JW4A.134 Mikhailova, Julia - JTu3A.140, JW3A.137, JW3A.30 Lopez Dieguez, Yanelis - JTu3A.76 Malabi, Rudzani - JW4A.108 Mikkelsen, Maiken H. - LTu5F, LW5F.3 López Higuera, Paula A.- JW3A.74 Malheiros-Silveira, Gilliard N.- JW3A.100, JW4A.94 Mikolajczyk, Michal - JW4A.79 Key to Authors López, Daniel - JTu2A.85 Malhorta, Tanya - JW4A.124 Milchberg, Howard - FTu5C.4, JW3A.5, JW4A.29, Lopez-Coyote, Monica - JW4A.82 Malhotra, Tanya - FM3C.4 JW4A.31, JW4A.35 Lopez-Mariscal, Carlos - FM3C Malhotra, Yugnanda - JW3A.80 Mildren, Richard - LW6F.6 Lorenz, Virginia O.- JW3A.61, LM1B.7, LM3B.2, Mamani, Sandra - JTu3A.116 Miller, David - JW4A.15 LM4A Manna, Alakesh - FM3D.4 Milster, Tom D.- FM3D.1 Loterie, Damien - JW4A.115 Manoto, Sello - JW4A.108 Min, Bumki - FM4F.4 Lougovski, Pavel - JTu3A.55 Manousidaki, Maria - FM4B.4 Minkov, Momchil - FTu4E.3, FW1C.3 Lovelace, Geoffrey - JW4A.77 Mantsyzov, Boris I.- JTu2A.49 Minoshima, Kaoru - FTh3C.1, JW4A.22 Lovell, Gregory - JW3A.86 Manurkar, Paritosh - FTh3C.4 Miranda, Miguel - LTu5F.3 Lozano-Crisóstomo, Nestor - JTu2A.46 Marcelo, Trivi - JW4A.140 Mirin, Richard - LM1B.6 Lu, Hsuan-Hao - JTu3A.55 Maria, J. P. - JTu3A.39 Miroshnichenko, Andrey - JTu3A.12, JW4A.91 Lu, Juanjuan - JW3A.94 Maria, Michael - FM3F.5 Mirotznik, Mark S.- JTu3A.91 Lu, Lu - JTu2A.127 Marín, Luis A.- JW4A.25 Mirza, Kayvan - FTh3A.2 Lu, Meng - JTu3A.87 Marin, Thibault - JTu3A.119 Mishra, Vinod - FM3D.4, JTu3A.11 Lu, Wei - JW4A.141 Marinelli, Agostino - LTu5F.1 Mitchell, Arnan - JTu2A.118 Lu, Xiyuan - FTh3C.3 Markos, Christos - FM3F.5 Mittleman, Daniel - JTu3A.101 Lu, Yiping - JTu3A.13 Marrujo, Sigifredo - JTu2A.85 Mizutani, Goro - JW4A.111 Lucas, Erwan - FW1C.2 Martikainen, Jani-Petri - FM3G.3 Mobini, Esmaeil - JW3A.134, JW3A.138 Luculescu, Catalin - JTu3A.138 Martin Vela, Javier A.- JW4A.13 Mochan, Wolf L.- JTu3A.54 Lugani, Jasleen - JTu3A.58 Martinez Angulo, Jose Ramon - JTu3A.78 Moehring, David - FTh1D.2 Luis Joaquin, Mendoza Herrera - JW4A.140 Martinez-Angulo, Ramon - JW3A.84 Mohamed, Ali A P.- JTu3A.29 Luiten, Andre N.- JW3A.54 Marty, Thomas - JW3A.15 Mohamed, Bichra - JTu3A.11 Lukens, Joseph M.- JTu2A.53, JTu3A.55, JW3A.66 Maruca, Stephanie - FM3C.5, JTu3A.5 Mohamed, Mohamed S.- FTu4E.3 Lukishova, Svetlana G.- JW3A.71 Maruyama, Shigeo - FTu4B.2 Möhl, Anna - FM3D.5 Lungjangwa, Tseten - JW4A.16 Masajada, Jan - JW3A.56 Moilanen, Antti - FM3G.3 Luntz-Martin, Danika - FW1E.4 Masir, Nur Musyiirah - JTu2A.80 Moille, Gregory T.- FTh3C.3 Luo, Bin - JTu2A.129, JTu2A.136, JTu2A.137, Matczyszyn, Katarzyna - FTh3B.7 Moiseev, Sergey G.- JTu3A.134 JW3A.127, JW4A.133 Mathew, Neethu Mariam - FTu5B.4 Mojahedi, Mo - JW4A.6 Luo, Rongya - JW4A.80 Mathews, Jay - JTu2A.96, JTu3A.103 Mojica Sepulveda, Ruth D.- JW4A.140 Luo, Rui - FTu4E.2, FTu4E.4 Matsubara, Akira - JW4A.111 Molina, Martha - JTu2A.73 Lupton, John - JW3A.67 Matthews, Jonathan C.- LM1B.5 Mondal, Sucheta - JW4A.49 Lv, Xiaohua - JW4A.116, JW4A.117 Matyas, Corey T.- JTu3A.93 Monshat, Hosein - JTu3A.87 Lyashenko, Dmitry - JW3A.49 May, Daniel - JTu2A.85 Montaut, Nicola - LM3B.1 Lyras, Andreas - FM3C.7 Mazeas, Florent - FW1E.2 Montazeri, Kiana - JW4A.1 Lysenko, Sergiy - JTu3A.123 Mazumder, Nirmal - JTu2A.125, JW4A.121 Monzón, David - JTu2A.85 Lyu, Xianyang - JW3A.105 McBirney, Samantha E.- FM4E.6 Mookherjea, Shayan - FTh1B.1 Lyubchenko, Dmitry - JTu2A.40 McCorkle, Brett - FTh3A.3 Moore, Nicole J.- JW3A.34 McElhenny, John E.- JW4A.5 Morandotti, Roberto - FTh1C.1 M McGoverin, Cushla - JW4A.114 Moreno, Fernando - JW4A.27 Ma, Chaoxuan - FTh1B.1 McLaughlin, Robert - JW3A.112 Moreno, Marco P.- JTu2A.7 Ma, Chunyang - JTu2A.43 McLeod, Robert R.- JW4A.15 Morgado, Tiago - JTu3A.88 Ma, Yufei - JW4A.138 Meem, Monjurul F.- FTh3E.7, JW4A.7 Mori, Warren - JW4A.141 Ma, Yunxiu - JW3A.11 Meemon, Panomsak - JTu3A.115 Morita, Ryuji - JW4A.47 Ma, Zhaohui - JTu2A.87 Mehrabian, Armin - JW3A.123 Morozov, Anatoli - JW3A.17 Ma, Zhizhen - FW5E.2, JW3A.97 Mehta, Dalip S.- FM4E.4 Moselund, Peter Morten - FM3F.5 MacDonnell, David - JW3A.10 Mejean, Guillaume - LTh1F.3 Moser, Christophe - FM4B.2, FTh1E.3, JW4A.115 Mach, Gabriela - JW3A.56 Mekonen, Sirak M.- JTu3A.103 Moss, David - FTh1C.1 Madrid Carrillo, Yesid A.- JTu2A.73 Melo, Carlos A.- JTu2A.68 Mosset, Alexis - JTu2A.65 Madugani, Ramgopal - JW3A.88 Melzer, James E.- FW1A.2 Mostafavi, Fatemeh - JTu3A.67 Maeda, Shunya - JW3A.132 Memmolo, Pasquale - JTu3A.122, JW3A.110, Mote, Rakesh G.- JTu3A.99 Maffettone, Pier Luca - JW3A.116 JW3A.116 Moura, André L.- JW3A.73 Mafi, Arash - JW3A.134, JW3A.138, LM1B.3 Mendonca, Cleber R.- JTu2A.9 Moura, João - FW1E.3 Magana Loaiza, Omar - JTu2A.67, LM1B.6 Meneses, Jaime E.- JW4A.131 Mouradian, Levon - JTu3A.45 Magnusson, Robert - JTu2A.107, JTu3A.85, Menezes, Leonardo D.- JW3A.73 Mourou, Gerard - (blank) JW3A.24, JW3A.98 Menon, Rajesh - FTh3E.7, JW4A.7 Moya-Cessa, Hector - JTu3A.49 Mahato, Krishna K.- JTu2A.125, JW4A.121 Mensing, Glennys - JTu3A.14 Mshvenieradze, Yuri - JTu3A.17 Mahdi, Mohd Adzir - JTu3A.71 Menyuk, Curtis - JTu2A.76, JTu3A.1, JW4A.18 Mthunzi-Kufa, Patience - JW4A.108 Mahmoud, Ahmed - JTu3A.97, JW4A.2 Merano, Michele - FW5C.5, JW3A.75 Muck, Martina - JTu2A.128 Maier, Stefan - FTu5A.2 Merola, Francesco - JW3A.116 Mucke, Oliver - LTu5F.2 Maimaiti, Aili - JTu3A.6 Meuren, Sebastian - LTu4F.1 Mugnano, Martina - JW3A.116 Main, Caleb - JTu2A.86 Meyer, David - JW4A.57 Mukherjee, Subhrajit - JTu2A.100 Mairesse, Yann - JTu3A.48 Meyer, David H.- JTu2A.54, JW4A.64 Mulkey, Thomas - JW3A.102

98 FiO + LS 2018 • 16–20 September 2018

FiO Abstracts.indd 64 8/20/18 9:11 AM Muller, Matthew S.- FM3F.6 O Pearson, Brett J.- JW4A.23 Müller, Tina - FTh3D.1 Obreshkov, Boyan - JTu2A.52 Peiponen, Kai E.- JW4A.125

Mulvaney, Paul - FM4C.4 Ocola, Esther J.- JW3A.40 Pena, Jessica - JTu2A.50 Key to Authors Muminur, Binte M.- JTu2A.110 Odele, Ogaga D.- JTu2A.53 Pendiuk, Guilherme F.- JW3A.82 Munns, Joseph - FTh3D.2, JW3A.63 Odom, Teri W.- FM2A.1 Peng, Chao - JW4A.80 Muraviev, Andrey - LTh3F.3 O’Donnell, Ryan M.- JTu3A.7 Peng, Chen - JTu2A.112, JW3A.93 Muravyev, Nikolay - JTu2A.26 Oh, Sang Soon - JTu3A.89 Peng, Fang - JW4A.138 Murnane, Margaret M.- FTu5C.3 Ohishi, Yasutake - JTu3A.72, JW3A.42, JW4A.33, Peng, Jiaxin - JTu2A.115 Murshid, Syed H.- JW3A.86, JW4A.88 JW4A.39 Peng, Jingyang - FW5E.4 Murzina, Tatiana V.- JTu2A.49 Oi, Ryutaro - FTh3E.2 Peng, Jin-long - JW3A.131 Musolino, Stefan - JW3A.112 Oka, Kazuhiko - JW4A.47 Peng, Kun - JTu2A.24 Mussot, Arnaud - JW4A.46 Okada, Masanori - JW4A.63 Peng, Zhenfang - JW4A.138 Myers, Jason - FM3C.1, JTu2A.90 Okamoto, Fumiya - JW4A.60 Penn, Steve - JW4A.77 Okulov, Alex - JTu2A.72 Penty, Richard - FTh3D.1 N Okur, Halil - FM4B.3 Perez Leija, Armando - LM1B.6 Nabet, Bahram - JW4A.1 Oliveira Feitosa, Patrick - JW4A.120 Perez, Eduardo - JTu2A.139, JTu3A.129, JW3A.28 Naciri, Jawad - JW3A.95 OmbindaLemboumba, Saturnin - JW4A.108 Perumal, Packiyaraj - JW4A.119 Nagarjun, K.P. - FW5B.4 Önder, Tuba - JTu2A.51 Peters, Nicholas A.- JTu3A.55 Nagler, Philipp - JW3A.67 Oren, Dikla - JW4A.58 Petersen, Christian - FM3F.5 Nagpal, Supriya - JTu2A.127 Osawa, Shuto - JTu2A.66 Petrov, Nikolai I.- JTu2A.38, JTu3A.137, JW3A.128, Naik, Dinesh N.- JTu2A.20, JW3A.8 Osellame, Roberto - JTu3A.60 JW4A.123, JW4A.51 Naik, Dinesh N.- JTu2A.21 Osolodkov, Mikhail - FTh3C.5 Petrovich, Marco - FW6B.3 Nair, Gokul G.- JTu2A.20 Osowski, Mark - JTu3A.15 Petruccione, Francesco - JTu3A.51 Nakajima, Naoya - JW3A.132 Ossikovski, Razvigor - JW4A.27 Pettit, Robert - FW1E.4 Nakamura, Yasunori - JW4A.111 Ou, Fang - JW4A.114 Peyghambarian, Nasser - JW3A.11 Nam, Saw W.- LM1B.6 Ou, Jianzhen - JTu2A.118 Peysokhan, Mostafa - JW3A.134, JW3A.138 Nam, SungWoo - JW3A.44 Ou, Zheyu - LM1B.4 Pezeshki, Ali - JTu3A.125 Nam, Wonil - JW3A.108 Oulton, Rupert - FTu5A.2 Pfefer, Joshua - FM3F.2, FM3F.4, JW3A.117, Nandi, Saikat - LTu5F.3 Ourari, Salim - JW4A.68 JW3A.118, JW3A.19 Narayanamurthy, C S - JTu2A.21, JW3A.8 Ouyang, Xia - JW3A.27 Piao, Yongri - FTh3E.3, JTu2A.133 Narreto, Mary Alvean B.- JW3A.33 Owrutsky, Jeffrey - JW4A.54 Picard, Raphael - FW6C.2 Nasti, Giuseppe - JTu2A.2 Owschimikow, Nina - JTu2A.64 Pigeon, Jeremy - JTu3A.50 Nasution, Aulia - JW4A.112 Ozcan, Aydogan - FM4E.3 Pincheira, Pablo I.- JW3A.73 Natalia, Gaiduk - JTu3A.111 Özgür, Ümit - JTu2A.22 Pinchuk, Vycheslav - JTu2A.45 Nath, Pabitra - JW4A.70 Pinho, Catia - JTu3A.88 Naveau, Corentin - JW4A.46 P Pinkse, Pepijn W.- JTu3A.58 Neathway, Peter A.- JTu2A.3 P, Rathish Kumar - JW3A.103 Piotrowicz, Michal J.- JW4A.61 Neethling, Pieter - JTu2A.34 P. Almeida, Marcelo - JTu2A.55 Piromjitpong, Teerawat - JTu3A.34 Nelson, Charles - JW3A.14 Pacala, Angus - FM3E.3 Piskunov, Dmitry - JTu2A.26 Nenchev, Marin - JW4A.17 Pacifici, Domenico - JW4A.56 Planchon, Thomas A.- JW3A.16 Neneman, Maciek - JW3A.125 Pai, Chao-Ping - JTu3A.3 Plant, David V.- JW4A.10 Neshev, Dragomir - JTu3A.12, JW4A.91 Pai, Chih-Hao - JW4A.141 Plechinger, Gerd - JW3A.67 Neto, Berta - JTu3A.88 Paine, Scott - FM4C.5 Plummer, Ward - JW3A.47 Neugebauer, Martin - FM3C.6 Pal, Dr. Parama - JTu2A.23 Pocherpailo, Andrii - JW4A.105 Neukirch, Levi - FW1E.4 Palmer, Adam J.- JW3A.54 Pohl, Alexandre D.- JW3A.82 Neves, Paulo D.- JW3A.82 Pan, Feng - JW3A.20 Poletti, Francesco - FW6B.3, FW6B.4 Newbury, Nathan R.- FTh3C.4, LTh2B, LTh3F Pan, Noren - JTu3A.15 Pompili, Matteo - JTu3A.60 Nguyen, Hoa P.- JW3A.42, JW4A.33, JW4A.39 Pan, Ruizhi - FW5C.2 Pons, Bernard - JTu3A.48 Nguyen, Lac - JTu3A.30 Panchal, Pramod - JTu2A.21, JW3A.8 Poole, Phillip J.- JW3A.7 Ni, Li - JTu2A.24 Panchenko, Evgeniy - FM4C.4 Popkova, Anna A.- JW3A.49 Nic Chormaic, Síle - JTu3A.6 Pang, Yoonsoo - JW4A.137 Popovitz-Biro, Ronit - FTu5C.5 Nie, Zan - JW4A.141 Pankratova, Maryna - JW3A.83 Porwal, Nikita - JW3A.36, JW4A.49 Nielsen, Michael - FTu5A.2 Pant, Kamal - JTu3A.11, JW4A.9 Posada-Ramirez, Berenice - FTu4B.5, LTu5F.4 Nikitin, Vladislav G.- JW4A.123 Panusa, Giulia - FM4B.2 Pottiez, Olivier - JTu2A.11, JTu2A.77, JTu3A.78 Nisha, Nisha - JW3A.80 Papay, Joel - FM3F.6 Potts, Timothy A.- JTu2A.126, JTu3A.23, JW4A.26 Nishiharaguchi, Nobuhiko - JTu3A.72 Papazoglou, Dimitrios G.- FM4B.4 Poulton, Christopher V.- FTu4E.1 Nishimura, Kotaro - LTu5F.2 Papp, Scott B.- FTh3C.3, JTu2A.62 Pourbeyram, Hamed - LM1B.3 Nithyanandan, Kanagaraj - JW4A.86, LTh1F.3 Paradeisanos, Ioannis - FW5E.5 Pradhan, Asima - JW4A.118 Nolte, Stefan - FW5C.3, JTu2A.61, JW4A.76 Parigi, Valentina - JTu3A.56 Prajapati, Nikunj - JW3A.68 Nomoto, Sean - JTu2A.5 Park, Hong-Gyu - JW3A.44 Prakash, Roopa - FW5B.4 Norris, David - FW5E.1 Park, Kyungdeuk - JTu2A.13, LM4A.2 Prasannan, Nidhin - LM3B.1 Norrman, Andreas - FTh3B.3, JW4A.12 Parto, Midya - FTu4C.1 Pratama, Detak Y.- JTu3A.117 Norte, Richard A. - FW1E.3 Pask, Helen - JW3A.136 Pratavieira, Sebastião - JW4A.120 Notaros, Jelena - FW6B.5 Patel, David - JW4A.10 Prieto-Cortes, Patricia - FTu4B.5 Notaros, Milica - FW6B.5 Paternostro, Mauro - JW3A.72 Prihasty, Wilda - JTu3A.117 Novikov, Vladimir B.- JTu2A.49 Pati, Gour S.- FM4B.6, FM4B.7 Prilepsky, Jaroslaw E.- JW3A.83 Novikova, Irina - JW3A.68 Patsekin, Valery - JTu2A.25 Priye, Vishnu - JTu2A.114, JTu2A.59, JTu2A.83, Nundy, Koushik K.- JW4A.93 Patton, Ryan - JW3A.2 JW3A.107, JW4A.107, JW4A.85 Nunn, Joshua - FTh3D.2, JW3A.63 Paturzo, Melania - JTu3A.122, JW3A.110 Proux, Raphael - FW6C.2 Nygaard, Erich - FM4C.2 Paun, Irina - JTu3A.138 Prucnal, Paul R.- JW3A.123 Pavlov, Nikolay - FW1C.2 Pryde, Geoff J.- LM1B.5

FiO + LS 2018 • 16–20 September 2018 99

FiO Abstracts.indd 65 8/20/18 9:11 AM Psaltis, Demetri - FM4B.2, FTh1E.3, JW3A.111, Ribak, Erez N.- JTu2A.141, JTu3A.25 Sandoval, Oscar - JTu3A.69 JW4A.115 Richardson, Christopher J.- FW6C.3 Sanford, Norman A.- FTu5C.3 Pu, Jixiong - JW3A.22 Richardson, David - FW6B.3 Sang, Robert T.- JW3A.54 Pu, Ye - FM4B.2 Richardson, Martin C.- FTh3E.7, JTu2A.50 Sanghera, Jasbinder - FM3C.1 Puchert, Robin - JW3A.67 Ricken, Raimund - LM3B.1 Sansoni, Linda - LM3B.1 Pufahl, Karsten - FW6E.2 Riel, Heike - Santiago-Hernandez, Hector - JTu2A.11, Pugh, Jon - JTu3A.86 Ringbauer, Martin - JTu2A.55 JTu3A.136, JW4A.4, LTu5F.4 Pukhov, Alexander - LTu4F.2 Ritchie, David - FTh3D.1 Sanyal, Shourjya - JW4A.93 Purevjav, Enkhsaikhan - JTu2A.127 Roberts, Ann - FM4C.4 Sarang, Soumya - LW6F.6 Purschke, David N.- JW3A.33 Robinson, J. Paul - JTu2A.25 Sarangan, Andrew - JTu2A.96, JTu3A.103 Key to Authors Pustovoit, Vladislav I.- JTu3A.137 Robles, Raúl A.- JTu3A.64 Sarkar, Resham - FTh3B.4 Rocca, Jorge J.- LTu4F.2, LTu5F Sarma, Raktim - JTu2A.101 Q Rockstuhl, Carsten - FW6C.4 Sasaki, Osami - FM3D.3 Qaderi, Kamran - FM4C.2 Rockwood, Alex - LTu4F.2 Sato, Tomonari - FW1B.3 Qi, Bingkun - JW3A.92, JW4A.41 Rodríguez Asomoza, Jorge - JW4A.87 Saunders, Dylan - FTh3D.2, JW3A.63 Qi, Minghao - JTu2A.53 Rodriguez Morales, Luis Alberto - JTu2A.11, Savona, Vincenzo - FTu4E.3, FW5C.1, JTu2A.106 Qi, Yang - FW5B.5 JTu3A.136 Savva, Kyriaki - FTu5C.5 Qi, Zhen - JTu3A.42, JW4A.42 Roeloffzen, Chris G.- JTu3A.58 Sawadogo, Bewindin - FW1B.2 Qian, Tianhong - JW4A.19 Roetzer, Thomas - JTu2A.128 Sazio, Pier - FW6B.4 Quan, Runai - JW4A.89 Rogers, Wesley - FM4C.2 Schartner, Erik P.- JW3A.112 Quintero Rodríguez, Leidy J.- JTu2A.84, JW4A.87 Rohwer, Erich - JTu2A.34 Schattenburg, Mark - JW4A.52 Quiring, Viktor - LM3B.1 Rojas-Laguna, Roberto - JTu2A.79, JTu3A.76, Schell, Felix - FTh3C.5 Quirk, Bryden - JW3A.112 JTu3A.78, JW3A.84, JW4A.13 Schmittberger, Bonnie - JW3A.64 Quraishi, Qudsia - JW3A.60 Rojas-Ochoa, Luis F.- JTu3A.135 Schnébelin, Come - LTh1F.3 Roke, Sylvie - FM4B.3 Schneider, Katharina - FTh3C.6 R Romanini, Daniele - LTh1F.3 Schnell, Martin - JTu3A.113 Rabitz, Herschel - FTh3C.2 Romero Cortés, Luis - FTh1C.1 Scholtz, Alexis - FM4E.6 Radue, Elizabeth - JTu3A.39 Romito, Marilisa - JW3A.111 Schüller, Christian - JW3A.67 Rahman, Muhammad M.- JTu2A.110 Ropp, Chad - FM3G.4 Schuller, Jon - LW5F.2 Rahmani, Mohsen - JTu3A.12, JW4A.91 Rosohadi, Iman R.- JTu3A.117 Schultz, Justin - FW1E.4 Raja, Arslan S.- FW1C.2, FW5E.5 Rottwitt, Karsten K.- FTu5B.4, JTu2A.6 Schulz, Claus Peter - FTh3C.5 Rakib Uddin, Mohammad - JTu2A.80 Roy, Abhijit - FM4C.6 Schulz, Sebastian - JTu3A.32 Rakich, Peter - LM3B, LM4A.3 Roy, Philippe - FW1E.2 Schussheim, Daniel T.- LTh1F.2 Ramezani, Hamidreza - JTu3A.67 Roy, Samudra - JTu2A.47 Schwartz, Robert - JW3A.5, JW4A.35 Ramsey, Jamie - FM3D Roychoudhuri, Chandra - JW3A.69 Schwefel, Harald G.- JW3A.31 Ran, Qiandong - JW4A.55 Rozen, Shaked - JTu3A.48 Schweinsberg, Aaron - JTu3A.33, JW4A.29 Rand, Stephen C.- FM4B.5, JW3A.46 Roztocki, Piotr - FTh1C.1 Sciara, Stefania - FTh1C.1 Ranga, Ritika - JTu2A.105 Rúa, Armando - JTu3A.123 Sciarrino, Fabio - JTu3A.60, JW3A.72 Rao, A. Srinivasa - JTu2A.16 Rubio Noriega, Ruth - JTu3A.4 Sciuti, Lucas F.- JTu2A.9 Rao, Ashutosh - JTu3A.59 Runnerstrom, Evan - JTu3A.39 Scully, Marlan O.- JW3A.40 Rao, Bingjie - JTu3A.35 Ryu, Jaeyeol - JTu2A.26 Searles, Thomas A.- JTu2A.96, JTu3A.103 Raposo, Ernesto P.- JW3A.73 Secondo, Ray R.- JTu2A.22 Rastegari, Ali - JW3A.6 S Segev, Mordechai - FTu4C.1, JW4A.58 Rastogi, Vipul - JW3A.81 Saumitra, S. - FW1B.1 Seidler, Paul - FTh3C.6 Raval, Manan - FW6B.5 Sabir, Sohail - JW3A.113 Selvaraja, Shankar K.- FW1B.1, FW5B.4 Raval, Shivam V.- JW3A.36 Safiabadi Tali, Seied Ali - JTu2A.58, JTu3A.53 Semnani, Behrooz - JW3A.53 Ray, Samit K.- JTu2A.100, JW3A.36 Safronov, Kirill - JW4A.97 Semwal, Vivek - JW4A.102 Raybon, Gregory - FW5B Saghaye Polkoo, Sajad - JW4A.20 Senlik, Ozlem - JW4A.113 Reano, Ronald M.- JW3A.2 Saghayezhian, Mohammad - JW3A.47 Serebryannikov, Andriy - JW4A.104 Reber, Melanie - LTh3F.2 Saha, Maitrayee - JTu2A.47 Sergienko, Alexander V.- JTu2A.66, JTu2A.94 Reddy, Anesan A.- JTu3A.51 Sahoo, Gyana - JW4A.118 Serikawa, Takahiro - JW4A.63 Redkin, Mykyta O.- JTu3A.111 Saikia, Ankita - JW4A.70 Serpengüzel, Ali - JW4A.43 Redyuk, Alexey - JTu3A.79 Saini, Than Singh - JW3A.42, JW4A.33, JW4A.39, Set, Sze - FTu4B.2, JTu2A.33 Rehain, Patrick - JTu3A.30 JW4A.69 Setälä, Tero - FTh3B.3, JW4A.12 Rehan, Mohd - JW3A.81 Saiprasad, R. L. N.- JW3A.103 Setiadi, Iwan C.- JW4A.112 Reimer, Christian - FTh1C.1 Saisina, Lalita - JTu3A.112 Shahandeh, Farid - JTu2A.55 Reina, John H.- JTu2A.68 Saito, Lucia - FTu4B.3 Shahidan, Muhammad F.- FM4C.4 Reinhardt, Ori - FTh3C.7 Saiz, Jose Maria - JW4A.27 Shahriar, Selim M.- FTh3B.4, JW4A.59, LW6F.4 Reintjes, John - JW4A.61 Sakakibara, Rei - JW4A.60 Shahverdi, Amin - JTu3A.8 Reis, David - LTu4F Salakhutdinov, Ildar - JTu3A.102 Shakher, Chandra - JTu3A.11, JW4A.9 Reisner, Mattis - FW1E.2 Salama, Norhan - JTu2A.103 Shalaev, Mikhail - FM3C.1 Rekola, Heikki - FM3G.3 Saleh, Bahaa - FTh3E.4 Shan, Xin - JTu2A.76 Ren, Guanghui - JTu2A.118 Saleh, Mohammed F.- FTh3B.2 Shankhwar, Nishant - JTu2A.104, JTu2A.105, Ren, Jinhan - FTu4C.1 Salehi, Fatholah - FTu5C.4 JTu2A.113 Ren, Ruizhi - JTu3A.124, JW4A.130 Salik, Ertan - JTu3A.102 Shao, Xiaopeng - JTu2A.134, JTu2A.135, Renema, Jelmer J.- FTh3D.2, JTu3A.58 Salim, Evan A.- FW1D.1 JTu3A.121, JW3A.129, JW4A.135, JW4A.136 Renshaw, Christopher K.- JW4A.20 Samanta, Goutam K.- JTu2A.16, JTu2A.56, Shapiro, Boris - JW4A.92 Reyes, Danielle - FTh3E.7, JTu2A.50 JW3A.41, JW4A.50 Sharma, Amit L.- JTu3A.24 Reyes, Erick - JTu2A.97 Samudrala, Sarath C.- JW3A.98 Sharma, R.P. - JW4A.110 Reynolds, Christina - JTu2A.30 Sanchez Mondragon, J - JTu2A.46 Sharma, Varun - JW3A.41, JW4A.50 Rhodes, William T.- JW3A.74 Sanchez, Christian - JW3A.77 Sharmin, Sultana - JW4A.111 Riaz, Muhammad - JTu2A.27, JTu3A.110 Sandoghchi, Reza - FW6B.3 Shelkovnikov, Alexander - JTu3A.141

100 FiO + LS 2018 • 16–20 September 2018

FiO Abstracts.indd 66 8/20/18 9:11 AM Shenoy, M. R. - JW4A.103 Smalley, Daniel - FM4C.2 Sukiasyan, Minas - JTu3A.45 Sheu, Tony Wen-Hann - JTu2A.57 Smith, Brian J.- JW4A.79 Sun, Chenglin - JTu3A.127 Sun, Haiyue - JW4A.138 Shi, Jianmin - JTu3A.7 Smith, David - JTu3A.104 Key to Authors Shi, Jiawei - JTu2A.121 Smith, Evan M.- JTu2A.108 Sun, Jingbo - FM3C.1 Shi, Lingyan - JW4A.3 Smith, Matt - JTu3A.10 Sun, Mengdi - JTu3A.92 Shi, Wei - JW3A.11 Smith, Peter - FTh3D.2 Sun, Qi - JTu3A.16, JW3A.12 Shi, Xingyuan - FTu5A.2 Smith-Dryden, Seth D.- FTh3E.4 Sun, Shuai - JTu2A.115 Shi, Yu J.- FW1C.3 Smolski, Viktor O.- LTh3F.3 Sun, Tzu-Min - JTu2A.12 Shibata, Masashi - JW3A.132 Snyder, John W.- JTu2A.94 Sun, Xiaohan - JTu3A.80 Shields, Andrew - FTh3D.1 Soavi, Giancarlo - FW5E.5 Sun, Xueying - JTu2A.134, JW4A.135 Shields, Philip - JTu3A.86 Sobhanan, Aneesh - JW4A.81 Sun, Yi - JTu3A.114 Shin, Heedeuk - JTu2A.13, LM4A.2 Soboleva, Irina V.- JW3A.49 Sun, Yu - JTu2A.98 Shin, Woncheol - JTu2A.13 Sokolov, Alexei - JTu3A.46 Sun, Yuanxi - JTu3A.130 Shinbrough, Kai B.- JW3A.61, LM1B.7 Sokolov, Alexei V.- JW3A.17, JW3A.40 Sung, Jangwoon - JTu2A.15 Shirahata, Takuma - FTu4B.2 Sokolov, Yuri - JW3A.128, JW4A.123 Sung, Kung-Bin - JTu3A.107, JW3A.121 Shlyaptsev, V. N.- LTu4F.2 Somboonkaew, Armote - JTu3A.112 Super, Nathan - JW3A.68 Shooter, Ginny - FTh3D.1 Son, Tran Vinh - JW3A.48 Suresh, Nitin - JW3A.117, JW3A.118 Shrewsbury, Bo - JTu3A.102 Song, Haomin - JTu2A.32, JW3A.90 Surya, Joshua - JW3A.94 Shu, Kaijun - JW4A.19 Song, Hyerin - JTu2A.120, JTu2A.124, JW3A.104, Suszek, Jaroslaw - JW4A.134 Shukla, Mukesh K.- JTu2A.99 JW4A.21 Sutapun, Boonsong - JTu3A.112, JW3A.21, Shukla, Shobha - JTu3A.99 Song, Jingchao - FM4C.4 JW4A.125 Shur, Michael - JW4A.75 Song, Jingming - JTu3A.75, JW4A.99 Suzuki, Takamasa - FM3D.3 Shute, Tish - FW5A.3 Song, Junyeob - JTu3A.82, JW3A.108 Suzuki, Takenobu - JTu3A.72, JW3A.42, JW4A.33, Shutov, Anton D.- JW3A.40 Song, Liang - JTu2A.121 JW4A.39 Shutova, Mariia - JTu3A.46, JW3A.17 Song, Ningfang - JTu3A.75 Swann, William - FTh3C.4 Siddiqui, Elisha - JW3A.70, LM1B.1 Sorger, Volker J.- FW5E.2, JTu2A.115, JTu3A.73, Swartzlander, Grover A.- JTu2A.37 Siemion, Agnieszka - JW3A.125 JW3A.123, JW3A.97, JW4A.96 Swift, Simon - JW4A.114 Sierra Hernandez, Juan M.- JTu3A.76, JW4A.13 Sosnicki, Filip - JW4A.79 Swillam, Mohamed M.- JTu2A.103, JTu3A.9, Sierra Hernández, Juan Manuel - JTu2A.79 Spadoti, Danilo - JTu3A.120, JW3A.124 JTu3A.97, JW3A.106, JW3A.9, JW3A.96, Sierra, Francisco - JTu3A.43 Spagnolo, Nicolò - JTu3A.60, JW3A.72 JW4A.2 Sierra-Hernandez, Juan M.- JTu3A.78, JW3A.84 Speirs, Rory W.- JW3A.59, JW3A.64, JW4A.62 Swillo, Marcin - JTu3A.83 Sikdar, sujit K.- FW1B.1 Spence, David - LW6F.6 Szameit, Alexander - JTu2A.67, JTu3A.49 Silahli, Salih - FM3C.1 Spencer, Daryl - JTu2A.62 Szarvas, Tamás - FTh3B.6 Silberhorn, Christine - LM3B.1 Spiniolas, Ryan - LM1B.7 Szriftgiser, Pascal - JW4A.46 Silva Alvarado, Erika - JW4A.13 Sprangle, Phillip - JW3A.29, JW4A.35 Silva, Daniely G.- JTu3A.120, JW3A.124 Squibb, Richard - LTu5F.3 T Silver, Jonathan M.- JW4A.32 Squier, Jeff - FM4C.3, JTu3A.108, JW4A.34 Taballione, Caterina - JTu3A.58 Silverstein, Barry - FTh3A.1 Srinivasan, Kartik - FTh3B.1, FTh3C.3 Tahersima, Mohammad H.- FW5E.2 Sim, Eunji - JW3A.101, JW4A.98 Srivastava, Prateek R.- JTu2A.37 Tai, Chia-Tse - JW4A.119 Sima, Felix - JTu3A.138 Srs Praveen Kumar, Vemuri - JTu3A.24 Takahashi, Eiji J.- JW3A.130, LTu4F.3, LTu5F.2 Simon, David S.- JTu2A.66 Staffa, Jeremy - JW3A.71 Takamoto, Masao - LTh1F.1 Simpkins, Blake - JW4A.54 Stahl, Charlotte - JTu3A.36 Takase, Kan - JW4A.63 Simsek, Ergun - FW6C.5 Stankovic, Konstantina M.- JW3A.111 Takeda, Shuntaro - JW4A.63 Sinayskiy, Ilya - JTu3A.51 Starner, Thad - FW1A.1 Takesue, Hiroki - FTh3D.3 Sinclair, Laura - FTh3C.4 Starobrat, Joanna - JTu2A.130 Talataisong, Wanvisa - JTu3A.70 Singamaneni, Srikanth - JW3A.109 Steiner, Florian - JW3A.67 Talisa, Noah - JTu3A.33 Singer, Matthew - JTu2A.32 Stender, Christopher - JTu3A.15 Tam, Hwa-Yaw - JW3A.27 Singh, R.P. - JW3A.41 Stevenson, Richard M.- FTh3D.1 Tam, Kevin K.- JW4A.78 Singh, Rajesh K.- JW3A.37 Stevenson, Sarah - FTh3C.4 Tamchek, Nizam - JTu3A.71 Singh, Rajwinder - FM4E.4 Stockman, Mark - FM3G.1 Tan, Yidong - JTu3A.26 Singh, Rakesh K.- FM4C.6, JTu2A.20, JW3A.8 Stockton, Patrick A.- JTu2A.117, JTu3A.125 Tanaka, Yurina - JW4A.22 Singh, Ritu Raj - JTu2A.114, JTu2A.59, JTu2A.83, Stokoe, Robby - JTu3A.125 Tang, Chao - JTu2A.87 JW3A.107, JW4A.107, JW4A.85 Stone, Jordan - JTu2A.62 Tang, Chenwei - JW3A.40 Singh, Rukmani - JTu2A.114 Storozheva, Angela - JW3A.128 Tang, Edward - FTh1A.2 Singh, Sonika - JTu2A.109 Stoykova, Elena - JW4A.17 Tang, Hong - JW3A.94 Singh, Surendra - JTu2A.5 Strait, Jared - JW4A.56 Tang, Qinggong - JW3A.117 Singhal, Ashutosh - JW3A.80 Stratakis, Emmanuel - FTu5C.5 Tanzilli, Sébastien - FW1E.2 Singla, Raksha - JTu3A.54 Straubel, Jakob - FW6C.4 Tao, Long - JTu2A.90, JW3A.65 Sinha, Dipan - JTu3A.27 Strauf, Stefan - FW6C.1 Tarabrin, Mikhail - JTu3A.141, JTu3A.47 Sinha, Jaivardhan - JW4A.49 Strauss, Ruthie - JW4A.23 Tayebi, Behnam - JTu2A.122 Sinha, Rajat K.- JTu3A.19, JTu3A.94, JW4A.101 Sturgis, Jennifer - JTu2A.25 Taylor, Joel E.- JW3A.47 Sinha, Ravindra K.- JTu2A.104 Stysley, Paul R.- FM3D.6 Teimourpour, Mohammad Hosain - FW1E.1 Sinha, Tridib - JW3A.36 Su, Ce - JW3A.86, JW4A.88 Teixeira, António - JTu3A.88 Sinyukov, Alexander M.- JW3A.40 Su, Jie - LM1B.8 Teixeira, Poliane A.- JTu3A.120, JW3A.124 Sinzinger, Stefan - JTu3A.11 Su, Qianqian - JTu2A.132 Teng, Hao - FTu4B.4 Sitpathom, Nonthanan - FTu5C.1 Sua, Yong Meng - FM3C.5, FW5B.2, JTu2A.87, Teng, Yanting - JW3A.61 Sitzmann, Vincent - FTh1E.2 JTu3A.100, JTu3A.30, JTu3A.8 Tenne, Reshef - FTu5C.5 Siverns, James - JW3A.60 Subedi, Nava R.- JTu2A.111 Terazima, Masahide - JW3A.122 Sjaardema, Tracy - JTu3A.59 Suda, Akira - LTu5F.2 Thangaraj, Jaisingh - JW4A.85 Skiba-Szymanska, Joanna - FTh3D.1 Suda, Gen - FM3D.3 Then, Patrick - FM4E.5, FM4E.7 Skoric, James - JW4A.10 Suer, Can - FW5E.2 Theran, Larry - JTu3A.123 Slowik, Karolina - FW6C.4 Sugiki, Fumihiro - JW3A.132 Thibault, Simon - JW4A.28

FiO + LS 2018 • 16–20 September 2018 101

FiO Abstracts.indd 67 8/20/18 9:11 AM Thiel, Valérian - JW4A.79 Vanderhoef, Laura - JTu3A.33 Wang, Jizhou - JW3A.40 Thirugnanasambandam, Manasadevi - JW4A.95 Vanholsbeeck, Frédérique - JW4A.114 Wang, Jyhpyng - JW4A.141 Thomas, Sarah - JW3A.63 Varma, Anumeha - JW4A.107 Wang, Kai - JW4A.3 Thompson, John R.- JTu2A.71 Varshney, Shailendra - JTu2A.47, JTu3A.19, Wang, Li - JW4A.36 Thoroh de Souza, Eunezio - FTu4B.3 JTu3A.94, JW3A.1, JW4A.101 Wang, Lidai - FM4E.2 Thul, Daniel - FTh3E.7 Vasco, Juan P.- JTu2A.106 Wang, Lifeng - JW4A.55 Tian, Bao-xian - FTu4C.4, JTu3A.40 Vashistha, Vishal - JW4A.104 Wang, Qingsong - JW4A.16 Tiedau, Johannes - LM3B.1 Vasilyev, Michael - JW3A.98 Wang, Quanzeng - JW3A.19 Timurdogan, Erman - FTu4E.1 Vasquez Arzola, Alejandro - FM4B.1 Wang, Shoujun - LTu4F.2 TinklePaugh, Micah - FTh3A.4 Vassalli, Massimo - JW3A.110 Wang, Shuang - JTu2A.98 Key to Authors Tirawat, Robert - JTu3A.14 Vasylchenkova, Anastasiia - JW3A.83 Wang, Sicong - JW3A.87 Tischler, Nora - LM1B.5 Vatarescu, Andre - JW4A.109 Wang, Tao - JTu3A.86 Tkachenko, Georgiy - JTu3A.6 Vedeshwar, Agnikumar G.- JTu3A.65 Wang, Wenyi - FW6E.5 Tochitsky, Sergei - JTu3A.50 Veli, Muhammed - FM4E.3 Wang, Xiaolong - JTu2A.24 Toda, Yasunori - JW4A.47 Venegas Gomez, Araceli - JW4A.74 Wang, Xiaoxi - FTh1B.1 Tofighi, Salimeh - JTu3A.7 Venkatasubramani, Lakshmi Narayanan - JW4A.81 Wang, Xinhua - JTu3A.121 Toledano-Ayala, Manuel - JW3A.84 Venkitesh, Deepa - JW4A.81 Wang, Yanan - JTu2A.86 Tomazio, Nathalia B.- JTu2A.9 Vergeles, Sergey - JTu3A.79 Wang, Yilin - JTu3A.95 Tomilov, Sergey - JTu3A.141 Vergyris, Panagiotis - FW1E.2 Wang, Yong - LTu4F.2 Tomizawa, Kohei - JW3A.132 Vermeulen, Diedrik - FTu4E.1 Wang, Yu - JW4A.116 Toneyan, Hrach - JTu3A.45 Veronis, Georgios - JTu3A.93 Wang, Yuan - FM3G.4 Tong, Hoang Tuan - JTu3A.72, JW3A.42, JW4A.33, Vespini, Veronica - JTu2A.2 Wang, Yu-Jen - JTu2A.19 JW4A.39 Vianna, Sandra S.- JTu2A.7 Wang, Yun - JW4A.10 Tong, Junhua - JTu2A.91 Victora, R. H. - JW4A.71 Wang, Zhao - FTu4C.4, JTu3A.40 Torabzadeh, Mohammad - JTu2A.117 Viggianiello, Niko - JTu3A.60 Wang, Zhihuan - JW4A.1 Torma, Paivi - FM3G.3 Villasante-Barahona, Mario - FM4B.1 Warren, Kayla - LTh3F.2 Torres González, Daniel - JTu2A.79 Villone, Massimiliano - JW3A.116 Warren, Warren S.- LTh3F.1 Torres Moreno, Yezid - JW3A.74 Visic, Bojana - FTu5C.5 Washburn, Brian - JW4A.95 Torres Quelal, Christian D.- JTu2A.68 Visscher, Ilka - JTu3A.58 Watanabe, Yuho - JW4A.47 Torres, Pedro - JTu2A.97 Visser, Dennis - JTu3A.83 Watson, Ash - JW4A.93 Torres, Rafael - JTu2A.73 Visser, Taco D.- JTu3A.28 Watts, Michael R.- FTu4E.1, FW6B.5 Torres-Cisneros, Miguel - JTu2A.85 Vlasova, Ksenia V.- JW4A.30 Wear, Keith - FM3F.2, FM3F.4 Toussaint, Jr., Kimani C.- JTu2A.119, JTu3A.14 Vodopyanov, Konstantin L.- LTh1F, LTh3F.3 Webb, William B.- JW4A.45 Trainor, Luke - JW3A.31 Vogelsang, Jan - JW3A.67 Weed, Matthew D.- FM3E.5 Treps, Nicolas - JTu3A.56 Vogt, William - FM3F.4 Weerasinghe, Kushan - JW4A.95 Trillo, Stefano - JW4A.46 Vogt, William C.- FM3F.2 Wegner, Paul - LTu4F.4 Trinh, Minh T.- FM4B.5 Volke-Sepulveda, Karen - FM4B.1 Wegrzyn, Piotr F.- JW4A.139 Tripathi, Renu - FM4B.6, FM4B.7 von Lerber, Tuomo - JTu2A.4 Wei, Biao - JTu2A.112, JW3A.93 Tromberg, Bruce J.- JTu2A.117 Voronine, Dmitri V.- JW3A.40 Wei, Chengli - JTu3A.1 Truong, Viet Giang - JTu3A.6 Voropaev, Vasilii S.- JTu3A.47 Wei, Chuanzhen - JTu2A.133 Tsai, Cheng-Yen - JTu2A.12 Vo-Van, Truong - JW3A.48 Wei, Ling-Hong - JTu3A.107 Tsai, Din Ping - FW6B.2 Vrakking, Marc J.- FTh3C.5 Wei, Yi - JTu3A.121, JW3A.129, JW4A.136 Tsakmakidis, Kosmas - JTu3A.32 Vuckovic, Jelena - FTh1C.2 Wei, Zhiyi - FTu4B.4 Tschernig, Konrad - JTu2A.67 Vyas, Reeta - JTu2A.5 Weikum, Maria Katharina - FTu4C.5 Tseng, Shih - LW6F.4 Weiner, Andrew M.- JTu2A.53, JTu3A.55, JTu3A.69 Tseng, Shuo-Yen - JTu2A.78 W Weinhold, Till - JTu2A.55 Tsukernik, Alexander - FM3C.1 W. Allen, Jeffery - JW3A.98 Weiss, David - FTh1D.1 Tu, Chaoran - JW4A.18 Wagner, Randall P.- JW3A.88 Welch, Eric - JTu3A.50 Tu, Haohua - JTu3A.114 Wahlstrand, Jared K.- FTu5C.4 Wendelin, Tim - JTu3A.14 Tu, Shih Cheng - JTu3A.107 Wakisaka, Isamu - JW4A.47 Wenner, Brett R.- JW3A.98 Turitsyn, Sergei - JTu3A.79 Waks, Edo - FW6C.3 Werner, Kevin - JTu3A.33 Turukhin, Alexey - FW1B Wakunami, Koki - FTh3E.2 Wetzel, Benjamin - FTh1C.1 Tyc, Tomas - JW3A.126 Walasik, Wiktor - FM3C.1 Wetzstein, Gordon - FTh1E.2 Tyurikov, Dmitry - JTu3A.141 Waldern, Jonathan - FW5A.1 Wheeler, Natalie V.- FW6B.3 Tzortzakis, Stelios - FM4B.4 Walk, Nathan - LM1B.5 Wheeler, Virginia - JW4A.40 Walker, David - JTu2A.30 White, Andrew G. - JTu2A.55 U Walker, Paul A.- FTu4C.5 White, Samuel T.- FW5E.3 U, Spandana K.- JTu2A.125, JW4A.121 Walmsley, Ian A.- FTh3D.2, JTu3A.58, JW3A.63 Wibowo, Andree - JTu3A.15 Uchida, Megumi - JW4A.22 Walschaers, Mattia - JTu3A.60 Wickenhagen, Sven - FM3D.5 Ullrich, Bruno - JTu2A.69 Wan Ismail, Wan Zakiah - FTu5C.1 Widjaja, Joewono - JTu3A.115 Upham, Jeremy - JTu3A.32 Wan, Meher - JTu2A.100, JTu3A.19, JTu3A.94, Wiebe, Nathan - JTu3A.60 U’Ren, Alfred - LM1B.6 JW4A.101 Will, Scott - JTu2A.131 Ushijima, Ichiro - LTh1F.1 Wan, Weiping - JTu3A.128 Williams, Brian P.- JTu3A.55 Wang, Bo - JW4A.36 Williams, Robert - LW6F.6 V Wang, Chiao-Yi - JW3A.121 Williams, Robin L.- JW3A.7 V.R., Supradeepa - FW5B.4 Wang, Fumin - JW3A.38 Williamson, Ian - FW1C.3 Väkeväinen, Aaro - FM3G.3 Wang, Gang - FW5E.5 Wilmer, Brian - JTu3A.33 Valentine, Jason - FW6E.5 Wang, Haiwei - JW3A.87 Wilson, Dalziel - FTh3C.6 Valenzuela, Anthony - JTu3A.33, JW4A.29 Wang, Han - JW3A.86 Wilson, Jesse - JTu3A.104 Vamivakas, Anthony N.- FM3C.4, FW1E.4, Wang, Jianjun - JTu2A.24 Winful, Herbert G.- LW6F.2 JW4A.124 Wang, Jiannan - JTu2A.134, JW4A.135 Winters, David - JTu3A.104 Van Stryland, Eric W.- JTu3A.7 Wang, Jieping - FM4B.2 Winzer, Peter J.- FW5B.1

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FiO Abstracts.indd 68 8/20/18 9:11 AM Wise, Frank W.- FTu4B.1 JTu2A.137, JW3A.127, JW4A.133 Zhang, Jianan - JTu3A.77 Wiseman, Howard M.- LM1B.5 Yang, Jingyi - FW6B.2 Zhang, Jing - JW3A.11

Wittek, Steffen - FTu4C.1 Yang, Kui - JTu3A.121 Zhang, Jun-Fu - JTu2A.57 Key to Authors Witting, Tobias - FTh3C.5 Yang, Luyun - JW3A.11 Zhang, Lijian - JW4A.126 Woehrer, Adelheid - JTu2A.128 Yang, Muqun - JW4A.122 Zhang, Lu - JTu3A.13 Woggon, Ulrike K.- FW6E.2, JTu2A.64 Yang, Weijian - LW6F.1 Zhang, Miao - FTh3E.3, JTu2A.133 Wolfe, Christopher - JTu3A.33 Yang, Xiong - JW4A.117 Zhang, Nan - JTu2A.32, JW3A.90 Wollmann, Sabine - LM1B.5 Yang, Yaping - JTu2A.39 Zhang, Pan - JTu3A.35, JTu3A.44 Wolterink, Tom A.- JTu3A.58 Yao, Jiyong - JW4A.36 Zhang, Pinliang - FTu4C.4, JTu3A.40 Wong, Kenneth K.- JTu2A.121 Yariv, Amnon - FTu5B.1 Zhang, Qi - JW4A.117 Wongkasem, Nantakan - JTu3A.84 Yavuz, Nurperi - JW4A.43 Zhang, Qiming - FM3D.2 Woodbury, Daniel C.- JW3A.5, JW4A.35 Ye, H. - JW4A.50 Zhang, Qingli - JW4A.138 Woodley, Michael T.- JW4A.32 Ye, Xiaohua - JW4A.16 Zhang, Ruoyu - JTu2A.115 Woods, Callie M.- JW4A.113 Yessenov, Murat - FTh3E.7, JTu2A.29, JTu3A.20, Zhang, Shougang - JTu3A.35, JTu3A.44, JW4A.11, Worts, Nathan G.- JTu3A.108, JW4A.34 JW4A.7 JW4A.89 Wozniak, Pawel - FM3C.6 Yevick, Aaron - JW4A.48 Zhang, Shuangyou - JW4A.32 Wu, Ben - FW5B.5 Yi, Zhenhuan - JW3A.40 Zhang, Tingting - JW3A.77 Wu, Bingchang - FTu4B.2 Yin, Longfei - JTu2A.129, JTu2A.136, JTu2A.137, Zhang, Xiang - FM3G.4 Wu, Binlin - JTu3A.118, JW4A.3 JW3A.127 Zhang, Xiaofei - JTu3A.35, JTu3A.44 Wu, Chunxiao - JTu3A.75, JW4A.99 Yodh, Arjun - JTu2A.142 Zhang, Xiaoxiong - JW3A.85 Wu, Guohua - JTu2A.129, JTu2A.136, JTu2A.137, Yoo, Thomas Sang Hyuk - JW4A.27 Zhang, Yanbing - FTh1C.1 JW3A.127, JW4A.133 Yoo, Yungjun - FTu5C.2, JW3A.52 Zhang, Yanyan - JTu3A.35, JTu3A.44 Wu, Hao-Hao - JTu2A.36 Yoshikawa, Jun-Ichi - JW4A.60, JW4A.63 Zhang, Yichen - FTh1B.2, JTu2A.70, JW3A.85 Wu, Jiacheng - JW4A.19 You, Chenglong - JTu3A.93 Zhang, YIchi - JW3A.78 Wu, Meng-Chang - JW3A.59, JW3A.64, JW4A.62 You, Sixian - JTu3A.114 Zhang, Ying - JW4A.55 Wu, Pin Chieh - FW6B.2, FW6E.4 Youn, Chun Ju - JW4A.72 Zhang, Yongsheng - JW4A.117 Wu, Po-Chang - FTh3E.6, JTu3A.3 Yousuf, Soha E.- JTu2A.92 Zhang, Yue - JW4A.89 Wu, Qin - JW3A.119 Youtsey, Chris - JTu3A.15 Zhang, Yujie - LM1B.7 Wu, Tong - JTu3A.124 Yu, Anthony - FM4B.6, FM4B.7 Zhang, Zhedong - JW3A.40 Yu, Guoyu - JTu2A.30 Zhang, Zhekai - JTu3A.80 X Yu, Haoyi - FM3D.2 Zhang, Zhenzhen - JW3A.78, LM1B.8 Xi, Haowen - JTu2A.69 Yu, Hojeong - JTu3A.119 Zhang, Zhong - JTu3A.14 Xia, Wentao - JTu3A.77 Yu, Juan - JTu2A.24 Zhao, Kun - JW3A.47 Xiang, Xiao - JW4A.11 Yu, Li - JTu3A.95 Zhao, Wenhui - JTu2A.98 Xiao, Ting-Hui - FTu4B.2 Yu, Song - FTh1B.2, JW3A.85 Zhao, Xin - JW3A.4 Xiao, Wen - JW3A.20 Yu, Su-Peng - FTh3C.3 Zhao, Yijia - FTh1B.2 Xiao, Yao - JW3A.87 Yu, Ting-Wen - JTu3A.107 Zhao, Zihao - JTu2A.33 Xiao, Yuqing - JW4A.128 Yu, Xin - JW4A.138 Zhdanova, Alexandra A.- JTu3A.46 Xie, Changsheng - JW3A.87 Yu, Xinguang - JW4A.3 Zheng, Jia - JTu3A.130 Xie, Yang - FTu4B.4 Yu, Zongfu - JTu2A.32 Zheng, Yameng - JW3A.136 Xing, Luo - JW3A.42, JW4A.33, JW4A.39 Yuan, Hua - JW3A.130 Zheng, Zheng - JW3A.4 Xiong, Yumaio - JW4A.116 Yuan, Mengqing - FW6C.5 Zhong, Qi - FW1E.1 Xu, Bingjie - JW3A.85 Zhong, Shiyang - LTu5F.3 Xu, Guichuan - JTu3A.133 Z Zhou, Feng - JW3A.88, JW4A.90 Xu, Huizhong - JW3A.91 Zahedpour Anaraki, Sina - FTu5C.4 Zhou, Hai J.- JTu2A.112 Xu, Lei - JTu3A.12, JW4A.91 Zainol Abidin, Nadiah - JTu3A.71 Zhou, Haijun - JW3A.93 Xu, Liang - JW4A.126 Zakhidov, Alex - JW3A.49 Zhou, Lyu - JTu2A.32, JW3A.90 Xu, Ming - JW3A.78 Zaldívar Huerta, Ignacio E.- JTu2A.84, JW4A.87 Zhou, Minchuan - JW4A.59 Xu, Rui - JTu2A.133 Zamboni-Rached, Michel - JW4A.6 Zhou, Renlai - JTu2A.93 Xu, Yu-Lin - JW3A.57 Zamfirescu, Marian - JTu3A.138 Zhou, Tingting - JW4A.132 Xu, Yun - FM3C.1 Zele, Andrew J.- JTu3A.109 Zhou, Vivian - JTu2A.86 Xu, Yuntao - JW3A.94 Zemanek, Pavel - FM4B.1 Zhou, Wei - JTu2A.58, JTu3A.53, JTu3A.82, Xu, Zhangjin - JTu3A.22 Zeng, Shaoqun - JW4A.116, JW4A.117 JW3A.108 Xue, Bing - LTu5F.2 Zeng, Xie - JTu2A.32 Zhou, Xuewen - FM3F.2 Zeng, Zhihao - JW3A.87 Zhou, Yan - JW4A.3 Y Zhai, Tianrui - JTu2A.91 Zhou, Zifan - JW4A.59, LW6F.4 Yablonovitch, Eli - FTu4A.3 Zhai, Yiwei - JW4A.89 Zhu, Chengjie - JTu2A.39 Yahiaoui, Riad - JTu2A.96, JTu3A.103 Zhan, Huan - JTu2A.24 Zhu, Guangdong - JTu3A.14 Yamada, Kaito - JTu3A.14 Zhang Chen, Lin - JTu3A.118 Zhu, Huiling - JW4A.16 Yamakawa, Hiroki - JW3A.132 Zhang, A. Ping - JW3A.27 Zhu, Huiqing - JW3A.71 Yamamoto, Hirotsugu - JTu3A.132 Zhang, Baoyue - JTu2A.118 Zhu, Kaiyi - JTu3A.26 Yamamoto, Kenji - FTh3E.2 Zhang, Chaojie - JW4A.141 Zhu, Rihong - JTu2A.24 Yamane, Keisaku - JW4A.47 Zhang, Cheng - FW6E.3 Zhu, Wenqi - FW6E.3 Yamashita, Shinji - FTu4B.2, JTu2A.33 Zhang, Chunxi - JW4A.99 Zhu, Xiushan - JW3A.11 Yamilov, Alexey G.- JTu2A.101 Zhang, Chunyuan - JW4A.3 Zhuo, Yue - JTu3A.119 Yan, Jingshi - JTu3A.12 Zhang, Dinghua - JTu3A.130 Zinkiewicz, Lukasz - JW4A.139 Yan, Juanjuan - FW5B.3, JTu3A.74 Zhang, Fanghua - JW4A.129 Zolotovskii, Igor - JTu3A.134 Yan, Lulu - JTu3A.35, JTu3A.44 Zhang, Guang - JW3A.129 Zorman, Christian - JTu2A.86 Yan, Yongli - JTu3A.139 Zhang, Guoquan - JTu3A.13 Zou, Yuhao - JW3A.87 Yang, Chen - JW4A.68 Zhang, Haiyang - JTu2A.98 Zuo, Heng - JW4A.52 Yang, Dewei - JW4A.99 Zhang, He - JTu3A.5 Yang, Dongyue - JTu2A.129, JTu2A.136, Zhang, Hongbo - JTu2A.71

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