Frontiers in Optics 2009/Laser Science XXV Featuring leaders of optics and photonics, including two Nobel Laureates, FiO/LS 2009 drew together industry luminaries from around the globe. Sessions on 3-D display, supercomputing and imaging at the nanoscale were the talk of the conference, and advances in these areas generated buzz throughout the event. Green energy was also a central theme, with discussions of how to make integrated photonic circuits more environmentally friendly and the popular solar car races demonstrating solar-powered miniature cars for a captive audience. Attended by more than 1,500 of the field’s leaders and with more than 40 companies participating in the exhibition, and more than 1,000 presentations, FiO 2009 provided the latest technical advances, networking opportunities and so much more. We look forward to seeing you next year at FiO 2010 in Rochester, NY from October 24–28.
Watch 2009 FiO Chairs Discuss This Year's Conference Highlights
Video Topics: Overview of FiO 2009 Collocated Topical Meetings The Future of 3-D Display—Special Symposium Gravitational Wave Interferometry from Earth and Space—Special Symposium Optics for Imaging at the Nanoscale and Beyond—Special Symposium Phase Space Optical System Theory for the 21st Century—Special Symposium Short Courses Hot Topics in Optical Design and Instrumentation Hot Topics in Optics in Information Sciences Hot Topics in Photonics Hot Topics in Optics in Biology in Medicine Unveiling a Supermassive Black Hole at the Center of Our Galaxy—Plenary Session View the chairs discussing highlights of FiO 2009 / Fall Optics & Photonics Congress – Lahsen Assoufid, Greg Quarles, and Markus Testorf.
The 2009 Technical Program Features: Six special symposia 10 Tutorials Plenary session held by two of the industry’s finest scientists; Andrea M. Ghez and Janos Kirz Ives Medal Lecture: Reobert Byer, Stanford University, USA Schawlow Prize Lecture: Robert Field, MIT, USA Three Short Courses
Collocated with the Fall OSA Optics & Photonics Congress: Advances in Optical Materials (AIOM) Adaptive Optics: Methods, Analysis and Applications (AO) Computational Optical Sensing and Imaging (COSI) Femtosecond Laser Microfabrication (LM) Signal Recovery and Synthesis (SRS) About FiO/LS FiO/LS Pre-Conference Schedule The Optical Society (OSA) The APS Division of Laser Science (DLS) Future Dates Join your colleagues in San Jose, CA, USA, for a variety of themes, topics, and invited speakers at the Frontiers in Optics (FiO) 2009/Laser Science (LS) XXV conference. These meetings focus on timely topics in optical science and engineering and provide a place for members to exchange ideas and to expand their network of colleagues in both academia and industry.
FiO/LS Pre-Conference Schedule February 19, 2009 Call for Papers Submission Site Opens for FiO/LS 2009 May 26, 2009, 12:00 p.m. noon EDT (16.00 FiO/LS Papers Submission Deadline GMT) June 2009 Registration and Housing Open Authors of submitted papers are notified of July 2009 acceptance/rejection August 2009 FiO/LS 2008 Conference Program Available Online September 11, 2009 Housing Deadline September 16, 2009 Pre-registration deadline September 21, 2009 Post deadline Paper Submission Deadline October 2, 2009 Authors of post deadline papers are notified of acceptance/rejection October 11-15, 2009 FiO/LS held at the San Jose Fairmont & St. Claire Hotel
The Optical Society (OSA) FiO 2009—the 93rd OSA Annual Meeting—and LS XXV unite the OSA and American Physical Society (APS) communities for five days of quality, cutting-edge presentations, fascinating invited speakers and a variety of special events. The FiO 2009 conference will also offer a number of Short Courses designed to increase participants’ knowledge of a specific subject while offering the experience of insightful teachers. An exhibit floor featuring leading optics companies will further enhance the meeting.
The APS Division of Laser Science (DLS) The LS XXV meeting serves as the annual meeting of the American Physical Society (APS) of its Division of Laser Science (DLS) and provides an important forum for presenting the latest work on laser applications and development, spanning a broad range of topics in physics, biology and chemistry. In collaboration with our colleagues at OSA, DLS will provide thorough coverage of mutually interesting topics in a number of joint sessions. Session schedules are coordinated to encourage your intellectual wanderings among DLS, OSA and joint sessions. Be prepared to engage in outstanding technical programs, exciting special symposia and networking events scheduled for this year's annual meeting.
Future Dates Year Dates Location
2010 October 24–28 Rochester, NY 2011 October 16-20 San Jose, CA 2012 October 14–18 Rochester, NY 2013 October 6–10 Orlando, FL
Plenary Session and Awards Ceremony The FiO 2009/LS XXV Plenary Session and Awards Ceremony is on Monday, October 12. Plenary Session Awards Ceremony
Plenary Session
Unveiling a Supermassive Black Hole at the X-Ray Microscopy Center of Our Galaxy Janos Kirz Andrea M. Ghez Advanced Light Source, Lawrence Berkeley Univ. of California at Los Angeles, USA Natl. Lab, USA
View presentation (PDF) View presentation (PDF) Ghez Video Part 1 Kirz Video Part 1 Ghez Video Part 2 Kirz Video Part 2 Ghez Video Part 3 Kirz Video Part 3 Kirz Video Part 4 Abstract: More than a quarter century ago, it was Kirz Video Part 5 suggested that galaxies such as our own Milky Way may harbor massive, though possibly Abstract: X-rays penetrate objects opaque to dormant, central black holes. Definitive proof, for electrons and visible light. X-ray spectra near or against, the existence of a massive central black absorption edges reveal the local chemical hole lies in the assessment of the distribution of environment. Linear and circular dichroism matter in the center of the Galaxy. The motion of provide contrast in magnetic materials. the stars in the vicinity of a black hole offers a way Advances in X-ray optics, as well as lensless to determine this distribution. Based on 10 years imaging methods, provide high spatial of high resolution imaging, Dr. Ghez's team has resolution. X-ray free-electon lasers coming on moved the case for a supermassive black hole at line may open the door to sub-nm resolution the Galactic Center from a possibility to a imaging of macromolecules. certainty. Additionally, spectroscopy has revealed that the stars orbiting in such close proximity are Biography: Janos Kirz received his Ph.D. in apparently massive and young; the origin of these physics from the University of California, stars is difficult to explain, given the strong tidal Berkeley, in 1963. He spent most of his forces, and may provide key insight into the professional life at Stony Brook University, growth of the central black hole. where he is currently Distinguished Professor Emeritus. His interest in X-ray microscopy dates Biography: Andrea M. Ghez, professor of physics to a stay at Oxford University in 1972–1973. and astronomy, is one of the world’s leading During the past 5 years he has been at the experts in observational astrophysics, whose work Advanced Light Source, Lawrence Berkeley sheds light on how our Milky Way Galaxy, Sun Laboratory, where he served as Acting Director and Earth came to be. (2004–2006) and is currently Scientific Advisor.
Working in the field of high resolution imaging, Professor Ghez has used the Keck telescopes to demonstrate the existence of a supermassive black hole at the center of our galaxy, with a mass 4 million times that of our sun. She has also discovered that most, if not all, stars shortly after birth have companion stars and that in most cases the separations of these companions pairs are smaller than the size of our solar system. For her research at Keck, Professor Ghez was named in Discover Magazine's 20th anniversary issue (2000) as one of the top 20 scientists in the country under 40, who ―have demonstrated once-in-a-generation insight‖ and ―will likely change our fundamental understanding of the world and our place in it.‖ Her work at the center of our Galaxy was also selected by the journal Science as one of the top 10 science results for 2002.
A member of the University of California at Los Angeles (UCLA) faculty since 1994, Professor Ghez also serves as a member of the Institute of Geophysics and Planetary Physics. She received a B.S. from MIT in 1987 and a Ph.D. in physics from Caltech in 1992. Before coming to UCLA, she was a Hubble Postdoctoral Research Fellow at University of Arizona's Steward Observatory. Her honors and awards include a MacArthur Fellowship (2008), Aaronson Award from the University of Arizona (2006), election to the National Academy of Sciences (2004) and the American Academy of Arts & Sciences (2004), the Sackler Prize from Tel Aviv University (2004), the Maria Goeppert-Mayer Award from the American Physical Society (1999), the Newton Lacy Pierce Prize from the American Astronomical Society (1998), Sloan Fellowship (1996), and a Packard Fellowship (1996).
Professor Ghez has served on numerous national committees and boards. Currently, her service work includes membership on the National Research Council’s Board on Physics and Astronomy and the Thirty-Meter-Telescope’s Science Advisory Committee.
Awards Addresses
Robert L. Byer Robert W. Field Stanford Univ., USA MIT, USA 2009 Frederic Ives Medal/Jarus W. Quinn 2009 Arthur L. Schawlow Prize in Laser Science Endowment Recipient Recipient
View presentation (PDF) View presentation (PDF)
Ives Medal Lecture: Surfing Lightwaves; Schawlow Prize Lecture: Acetylene: Just Large meeting the challenges of the 21st Century Enough
Abstract: In the fifty years since the Abstract: What can acetylene (H-C≡C-H) do demonstration of the laser, coherent light has that a diatomic molecule cannot? It can undergo changed the way we work, communicate and play. bond-breaking isomerization. The minimum The generation and control of light is critical for energy isomerization path from acetylene to meeting important challenges of the 21st century vinylidene is a very large-amplitude local-bend. from fundamental science to the generation of How are large-amplitude motions encoded in a energy. spectrum? At high vibrational excitation, anharmonic interactions between vibrational Biography: Robert L. Byer has conducted normal-modes become very strong and all of the research and taught classes on lasers and nonlinear textbook energy level patterns, upon which optics at Stanford University since 1969. He has assignments are based, are shattered. Most made extraordinary contributions to laser science vibrational eigenstates are complex, one might and technology including the demonstration of the even say ―ergodic,‖ mixtures of many normal- first tunable visible parametric oscillator, the mode basis-states. However, large-amplitude- development of the Q-switched unstable resonator motion states comprise a tiny fraction of all Nd:YAG laser, remote sensing using tunable eigenstates. How does one gain access to these infrared sources, and precision spectroscopy using rare large-amplitude states? How does one Coherent Anti Stokes Raman Scattering (CARS). distinguish a large-amplitude state from an Byer’s ongoing research includes development of ergodic state in a spectrum? How does one use nonlinear optical materials and laser diode pumped large-amplitude states to map the chemically solid-state laser sources for applications to interesting isomerization path on the S0 potential gravitational wave detection and to laser particle energy surface? Access is provided by a ―local- acceleration. bender pluck‖ state, which exploits anharmonic interactions on the S1 potential energy surface to Currently the William R. Kenan Jr. Professor of escape Franck-Condon restrictions in the S →S Applied Physics, Byer has served as vice provost 1 0 and dean of research at Stanford as well as chair of Stimulated Emission Pumping (SEP) spectrum. the Department of Applied Physics, director of the A relatively low trans-cis isomerization barrier Edward L. Ginzton Laboratory, and Director of the on S1 provides spectroscopic access to Hansen Experimental Physics Laboratory. He is a eigenstates proximal to a high barrier on S0. founding member of the California Council on Electronic properties (such as the electric dipole Science and Technology and served as chair from transition moment) serve as embedded reporters 1995–1999. He has been a member of the National on the existence and extent of large-amplitude Ignition Facility since 2000 and was a member of motions. However, electronic properties give rise the Air Force Scientific Advisory Board from to minuscule level splittings. How does one 2002–2006. He has served as president of both combine a survey over a wide spectral region in OSA and IEEE LEOS. search of rare large-amplitude local-bender states yet simultaneously achieve the extremely high Byer has published more than 500 papers and resolution necessary to read what the embedded holds 50 patents in the fields of lasers and reporter has written? Brooks Pate (University of nonlinear optics. He is a fellow of OSA, IEEE, Virginia) has developed ―Chirped Pulse APS, AAAS, and LEOS, and is a member of the Microwave Spectroscopy (CPMW),‖ which National Academy of Engineering and the combines the previously unimaginable National Academy of Science. combination of survey (10GHz), high-resolution (100kHz), and accurate relative-intensity (1 part in 104) capabilities. The CPMW scheme is perfectly suited to 20 Hz repetition rate pulsed supersonic jet molecular beams and Q-switched Nd:YAG pumped pulsed tunable lasers, upon which most small-molecule spectroscopists depend.
This research has been supported by the Department of Energy (Grant: DE- FG0287ER13671).
Biography: Robert W. Field majored in chemistry at Amherst College (AB thesis with Cooper H. Langford, 1965). He became a physical chemist in the research group of William Klemperer at Harvard University, where he discovered his affinity for multiple resonance spectroscopies and spectroscopic perturbations (PhD, 1972). As a post-doc with Herbert P. Broida and David O. Harris at University of California at Santa Barbara (1971–1974) he performed the first microwave-optical and optical-optical double resonance studies of diatomic molecules using tunable lasers and showed how to extract global insights into the electronic structure of the alkaline earth monoxides from the systematic study of spectroscopic perturbations. At MIT (Assistant Professor 1974, Associate Professor 1978, Professor 1982, Haslam and Dewey Professor 1999) his students and post-docs have continued to develop new laser spectroscopic techniques (most notably Stimulated Emission Pumping) with a goal of uncovering and exploiting unconventional patterns that encode the mechanisms of far-from-equilibrium molecular dynamics, particularly Intramolecular Vibrational Redistribution, Doorway-Mediated Intersystem Crossing, and energy exchange between a Rydberg electron and a molecular ion-core. He is a Fellow of the American Physical Society (APS), The Optical Society (OSA), the American Academy of Arts and Sciences, and the American Association for the Advancement of Science. He has received the Broida (1980) and Plyler (1988) Prizes of the APS, the Lippincott (1990) and Meggers (1996) Awards of the OSA, and the Bomem-Michelson Award of the Coblentz Society. His favorite molecules have been CO, CaF, and acetylene. His book (co- authored with Helene Lefebvre-Brion, 2004), ―The Spectra and Dynamics of Diatomic Molecules,‖ is the user’s guide for both theorists and experimentalists.
Invited Speakers Frontiers in Optics Invited Speakers Laser Science Invited Speakers
FiO 1: Optical Design and Instrumentation NOTE: Roger Angel is unable to attend FiO 2009; Greg P. Smestad (Solar Energy Materials and Solar Cells, and Sol Ideas Technology Development, USA) will give the keynote talk.
1.1: Novel Optical Architectures in Emerging Technologies (Joint with FiO 7) Invited Speakers:
FWR1, Biomolecular Sensing with Ultrafine Optical Fibers and Plasmonic Nanostructures, Donald J. Sirbuly¹, Sarah Baker², Sanja Zlatanovic³, Jason Steiner¹, Sadik Esener¹,³; ¹NanoEngineering Dept., Univ. of California at San Diego, USA, ²Physical and Life Sciences Directorate, Lawrence Livermore Natl. Lab, USA, ³Electrical and Computer Engineering, Univ. of California at San Diego, USA
FWR2, Advances in Microendoscope Design and Application, Arthur Gmitro, Houssine Makhlouf, Andrew Rouse; Univ. of Arizona, USA
FWX1, Miniaturization of Adaptive Optics Scanning Laser Ophthalmoscope Austin Roorda¹, David Merino¹, Kaccie Y. Li¹, Yuhua Zhang²; ¹Univ. of California at Berkeley, USA, ²Univ. of Alabama, Birmingham, USA
1.2: Novel Optical Architectures Using Free-Form Surfaces Tutorial Speaker:
FThN1, Fabrication and Testing of Large Free-Form Surfaces, James Burge; Univ. of Arizona, USA
Invited Speakers:
FThH1, Can You Make/Measure this Asphere for Me? Greg Forbes; QED Technologies Inc., USA
FThN2, Application of Radial Basis Functions to the Design of a Freeform Single Element See-through Head-Worn Display, Ozan Cakmakci¹, Jannick Rolland²; ¹Optical Res. Associates, USA, ²Inst. of Optics, Univ. of Rochester, USA
1.3: Optics for Renewable Energy Keynote Speaker:
FMB1, Optics of Solar Cells, Greg P. Smestad¹,²; ¹Solar Energy Materials and Solar Cells, USA, ²Sol Ideas Technology Development, USA
Invited Speaker:
FMB2, Solar Production of Fuels, Anastasios Melis; Univ. of California at Berkeley, USA
1.4: Polarization and Birefringence in Optical Design Invited Speakers:
FThF1, Photoaligned Liquid Crystal Polymers for Space Variant Polarization Control, Scott McEldowney¹, David M. Shemo², Russell A. Chipman³; ¹Microsoft Corp., USA, ²JDS Uniphase, USA, ³Univ. of Arizona, USA
FThF2, Optical Imaging Instrumentation with Spatially Engineered Polarization, Qiwen Zhan; Univ. of Dayton, USA
FThL1, Polarization Aberration Functions in Three Dimensions, Russell Chipman; Univ. of Arizona, USA
1.6: Diffractive and Holographic Optics FTuH1, Dynamic Holograms, Guoqiang Li; Univ. of Missouri at St. Louis, USA
FTuO1, Applications and Engineering of Three-Dimensional Optics, Eric Johnson¹, Pradeep Srinivasan¹, Menelaos Poutous¹, Zachary Roth¹, Raymond Rumpf²; ¹Univ. of North Carolina at Charlotte, USA, ²Prime Res. LC, USA
FTuV1, Role of Surface Plasmon Polariton in the Diffraction of a Metal Nano-Slit, Yann Gravel, Yunlong Sheng; Univ. Laval, Canada
FThB3, Live Cell Imaging with Field-Based 3-D Microscopy, Michael Feld, Wonshik Choi; MIT, USA
View Computational Optical Sensing and Imaging (COSI) invited speakers.
4.3: Computational Imaging and Photography (Joint with FiO 4)
Symposium: The Future of 3-D Display: The Market Place and the Technology
Symposium: Optics for Imaging at the Nanoscale and Beyond
FiO 2: Optical Sciences
2.1: Extreme Light Sources (Joint with FiO 6) Tutorial Speaker:
FMI1, High Peak Power Laser Technologies: New Directions, Christopher Barty; Lawrence Livermore Natl. Lab, USA
Invited Speakers:
FMI2, The Extreme Light Infrastructure Project, Jean-Paul Chambaret; Lab. d'Optique Appliquée, France
FMI3, An Overview of the Activities of the UK’s High Power Laser Programme, John Collier¹,²; ¹Central Laser Facility, Science and Technology Facilities Council (STFC), Rutherford Appleton Lab, UK, ²Dept. of Physics, Swansea Univ., UK
FTuK1, Status of the National Ignition Facility, Peter (Jeff) Wisoff; Lawrence Livermore Natl. Lab, USA
FTuK2, The Texas Petawatt Laser, Todd Ditmire; Univ. of Texas at Austin, USA
2.2: Short Wavelength—Generation and Applications Tutorial Speaker:
FTuS1, EUV Lithography–The Next Generation of Computer Chip Manufacture, Martin Richardson; CREOL, The College of Optics and Photonics, Univ. of Central Florida, USA
Invited Speakers:
FTuS3, High Brightness Plasma-Based Soft X-Ray Lasers and Applications, James Dunn; Lawrence Livermore Natl. Lab, USA FTuZ1, Coherent X-Rays from Ultrafast Lasers, and Applications—Attosecond Science Meets Nonlinear Optics, Henry C. Kapteyn, Margaret M. Murnane; JILA, Univ. of Colorado at Boulder, USA
FTuZ2, Nanoscale Microscopy with Table-Top Extreme Ultraviolet Lasers, C. S. Menoni¹, F. Brizuela¹, C. Brewer¹, Y. Wang¹, F. Pedaci¹, B. M. Luther¹, W. Chao¹,², E. H. Anderson¹,², D. T. Attwood¹,², A. V. Vinogradov³, I. A. Artioukov³, A. G. Ponomareko4, V. V. Kondratenko4, M. C. Marconi¹, J. J. Rocca¹,4; ¹Colorado State Univ., USA, ²Lawrence Berkeley Natl. Lab, Univ. of California, USA, ³P. N. Lebedev Physical Inst., Russian Acad. of Sciences, Russian Federation, 4Technical Univ., Ukraine
FTuZ3, Extreme High Harmonics from Relativistically Oscillating Surfaces, Matt Zepf; Queen's Univ. Belfast, Ireland
2.3: Biomedical Applications of Ultrafast Optics (Joint with FiO 3 and 7) Invited Speakers:
FWA1, Nanosurgery with Femtosecond Lasers, Eric Mazur; Harvard Univ., USA
FWA2, Improvements in Two-Photon Fluorescence Microscopy, Kengyeh K. Chu, Tom Bifano, Jerome Mertz; Boston Univ., USA
FWA3, Tissue Imaging with Shaped Femtosecond Laser Pulses, Warren S. Warren; Duke Univ., USA
Symposium: Gravitational Wave Interferometry from Earth and Space (Joint with Laser Science)
FiO 3: Optics in Biology and Medicine
Watch Adam Wax, Subcommittee Member, discuss what’s hot in Optics in Biology and Medicine.
3.1: Optics in Interventional Medicine FThP1, Photodynamic Therapy: A Bridge between Technology and Medicine, Tayyaba Hasan; Massachusetts General Hospital, USA
FThP4, User-Friendly, Open-Source Computational Tools for Biophotonics, Vasan Venugoplan; Univ. of California at Irvine, USA
3.2: Optical Trapping and Micromanipulation Invited Speakers:
FWM1, Optical Trapping and Manipulation Using Microfabricated Optical Tweezers Based on Diffractive Optics and Surface Plasmons, Ken Crozier; Harvard Univ., USA
FWS1, High-Resolution, High-Stability, High-Frequency Optical Tweezers Methods with a Simple Video Camera, Wesley Wong; Rowland Inst., Harvard Univ., USA
FWS4, Optical Phase Conjugation for Tissue Turbidity Suppression, Changhuei Yang; Caltech, USA
FWY1, Multimode Light in Action, Roberta Zambrini; IFISC (UIB-CSIC), Univ. Illes Balears, Spain
3.3: Optical Biosensing Invited Speakers:
FTuY3, Designing Interfaces for Optical Biosensors, Ashutosh Chilkoti; Duke Univ., USA
3.4: Tissue Imaging and Spectroscopy Invited Speakers:
FME1, Imaging Metal Nanoparticle Distribution within Tumors, J. Park¹, P. Puvanakrishnan¹, P. Diagaradjane², J. A. Schwartz³, J. D. Payne³, A. K. Dunn¹, S. Krishnan², J. W. Tunnell¹; ¹Univ. of Texas at Austin, USA, ²Radiation Oncology, MD Anderson Cancer Ctr., USA, ³Nanospectra Biosciences Inc., USA
3.5: Microscopy and OCT Invited Speakers:
FMK1, Nonlinear Coherent Imaging of Nanostructures and Single Molecules, Eric Potma; Univ. of California at Irvine, USA
FThV1, Advances in High-Speed Imaging by Objective-Coupled Planar Illumination Microscopy, Timothy Holy; Washington Univ. in St. Louis, USA FThV6, Title to Be Announced, Max Diem; Northeastern Univ., USA
3.6: Molecular Imaging and Nanomedicine Invited Speakers:
FTuL1, Molecular Probes for Microendoscopy, Chris Contag; Stanford Univ. School of Medicine, USA
FTuL4, Biomimetic Strategies for Modification of Surfaces with Passivating and Targeting Moieties, Phillip B. Messersmith; Northwestern Univ., USA
2.3: Biomedical Applications of Ultrafast Optics (Joint with FiO 2 and 7)
7.1: Molecular Imaging in the Eye (Joint with FiO 7)
FiO 4: Optics in Information Science
4.1: Optical Information Processing and Transport in the Age of Nanophotonics and Metamaterials Invited Speakers:
FWB1, Optofluidic Nano-Plasmonics for Biochemical Sensing, Yeshaiahu Fainman, Lin Pang, Boris Slutsky, Joanna Ptasinski; Univ. of California at San Diego, USA
4.2: Optical Signals and System in Four Dimensions Invited Speakers:
FTuU3, Title to Be Announced, Aristide Dogariu; CREOL & FPCE, Univ. of Central Florida, USA
FThR2, Multi-Channel Incoherent Digital Holography, Joseph Rosen, Barak Katz; Ben Gurion Univ. of the Negev, Israel
4.3: Computational Imaging and Photography (Joint with FiO 1) Invited Speakers:
FThR1, Emerging Integrated Computational Imaging Systems, Nicholas George, Wanli Chi; Univ. of Rochester, USA
FThX1, 4-D Frequency Analysis of Computational Cameras for Depth of Field Extension, Anat Levin; Weizmann Inst. of Science, Israel
FThX2, Optimization and Application of Hybrid Optical-Digital Imaging Systems, Andrew Harvey, Mads Demenikov, Gonzalo D. Muyo, Tom Vettenburg; Heriot-Watt Univ., UK
View Computational Optical Sensing and Imaging (COSI) invited speakers.
4.4: Wavefront Design for Information Transport and Sensing Invited Speakers:
FTuG1, Modulation of Polarization Properties of Beams for Laser Communications and LIDAR Systems Operating in Random Media, Olga Korotkova; Univ. of Miami, USA
FTuG2, Vectographic Computer-Generated Optical Elements, Grover Swartzlander; Ctr. for Imaging Science, Rochester Inst. of Technology, USA
FTuU1, SLM Microscopy: Wavefront Shaping for Microscopy with Spatial Light Modulators, Monica Ritsch-Marte; Innsbruck Medical Univ., Austria
FTuU2, Optimal Transmission of Light through Disordered Materials, Allard Mosk; Univ. of Twente, Netherlands
Symposium: Phase Space Optics—Optical System Theory for the 21st Century
FiO 5: Photonics
5.1: Novel Fiber and Integrated-Optical Devices Invited Speakers:
FTuD1, Novel Fiber Lasers with Advanced Glasses and Fiber Designs, Axel Schülzgen; Univ. of Arizona, USA
FTuP3, Principal Modes in Graded-Index Multimode Fibers, Mahdieh Shemirani, Joseph Kahn; Stanford Univ., USA
FWE1, Multimaterial Fiber Devices and Systems, Ofer Shapira; MIT, USA
FWF1, Why Use Photonic Crystal Fibers for Sensing? Jonathan Knight; Univ. of Bath, UK
FWG4, Fiber Optic Sensors Based On Surface Plasmon Resonance, Banshi D. Gupta; Indian Inst. of Technology, India
5.2: Photonic Devices for Sensing Applications Invited Speakers:
FTuE3, Advances in Chemical and Biological Sensing Using Emerging Soft Glass Optical Fibers, Yinlan Ruan, Heike Ebendorff-Heidepriem, Afshar V. Shahraam, Stephen Warren-Smith, Tanya Monro; Univ. of Adelaide, Australia
FWG1, Optical Manipulation using Silicon Nanophotonics, David Erickson; Cornell Univ., USA
FWT1, Plasmonics on Optical Fibers: New Tools for Biochemical Sensing, Jacques Albert, Maria Derosa, Anatoli Ianoul, Yanina Shevchenko, Alexander Beliaev, David A. D. Blair, Nur Ahamad; Carleton Univ., Canada
5.3: All-Optical Signal Processing Devices and Applications Invited Speakers:
FTuI1, Polychromatic High Speed Sampling, Stojan Radic; Univ. of California San Diego, USA
FTuI4, Advances in High-Confinement Fibers, Msaaki Hirano; Sumitomo Electric Industries, Ltd., Japan
FTuW1, All-Optical Header Processing Using Semiconductor Optical Amplifiers, Roderick P. Webb¹, X. Yang², R. J. Manning¹, G. D. Maxwell³, A. J. Poustie³, S. Lardenois³, D. Cotter¹; ¹Tyndall Natl. Inst., Univ. College Cork, Ireland, ²School of Electrical Engineering, Bangor Univ., UK, ³CIP Technologies, UK
FWK1, Nonlinear Optics on a Chip: Breaking the Terabit per Second Barrier, Benjamin J. Eggleton; Univ. of Sydney, Australia
5.4: Optical Communication Invited Speakers:
FMD1, Bi-Directional Multi-Service 60-GHz MM-Wave Radio-over-Fiber Network Interoperable with Multi-Gigabit Wireless Transceiver for Very High Throughput Inbuilding HD Video and Data Delivery, Gee-Kung Chang, Arshad Chowdhury, Hung- Chang Chien; Georgia Tech, USA
FTuC1, Next-Generation Optical Access Networks, Leonid Kazovsky¹, Shing-Wa Wong¹, She-Hwa Yen¹, Shinji Yamashita¹; ¹Stanford Univ., USA, ¹Fujitsu Labs Ltd., Japan
FTuC2, Agile WDM Layer for FlexSelectTM Metro Optical Network, Shan Zhong, Jean-Luc Archambault, Loudon Blair; Ciena Corp., USA
FTuP1, Extended Reach Passive Optical Networks, Chang-Hee Lee; KAIST, Republic of Korea
5.5: Silicon Photonics Invited Speakers:
FML1, Deterministic Aperiodic Structures for Nanoplasmonics, Luca Dal Negro; Boston Univ., USA
FML6, Erbium Doped Silicon Photonic Crystals for Light Sources and Amplifiers, Jelena Vučković¹, Maria Makarova¹, Yiyang Gong¹, Selcuk Yerçi², Rui Li², Luca Dal Negro²; ¹Dept. of Electrical Engineering and Ginzton Lab, Stanford Univ., USA, ²Dept. of Electrical and Computer Engineering, Boston Univ., USA
FWN1, Photonic Signal Processing in CMOS-Compatible Silicon, Mahmoud S. Rasras; Bell Labs, Alcatel Lucent, USA
FWN3, Cascaded Silicon Raman Laser Using Tunable Ring Resonator, Haisheng Rong¹, Omri Raday², Mario Paniccia¹; ¹Intel Corp., USA, ²Intel Corp., Israel
FWZ1, Green Integrated Photonics, Sasan Fathpour; CREOL, The College of Optics and Photonics, Univ. of Central Florida, USA
5.6: Design and Fabrication of Plasmonic Devices and Metamaterials (Joint with FiO 6) Invited Speakers:
FMA1, About Energy, Linear Momentum and Mass Transfer by Electromagnetic Wave in Negative Refraction Media, Victor Veselago; Moscow Inst. of Physics and Technology, Russian Federation
FMH1, Three-Dimensional Metallic Metamaterials: Coupling Matters, Harald Giessen; Univ. of Stuttgart, Germany
FTuB1, Active Terahertz Metamaterials, Hou-Tong Chen; Los Alamos Natl. Lab, USA
FTuN1, Optical Metamaterials, Xiang Zhang; Univ. of California at Berkeley, USA
FWC3, Terahertz Electromagnetic Phenomena near Metallic Nanogap Structures, D. S. Kim¹, M. A. Seo¹, H. R. Park¹, J. S. Kyoung¹, S. M. Koo¹, N. K. Park¹, O. K. Suwal², S. S. Choi²; ¹Seoul Natl. Univ., Republic of Korea, ²Sun Moon Univ., Republic of Korea
FWP1, Ultrafast Optical Nonlinearities in Hybrid Metal-J-Aggregate Nanostructures, Christoph Lienau; Carl von Ossietzky Univ., Germany
FWP4, Tailoring Polarization States of Visible Light through Metallic Nanostructures, J.-Y. Laluet, E. Laux, E. Lombard, A. Drezet, C. Genet, Thomas W. Ebbesen; Univ. de Strasbourg and CNRS, France
View Advances in Optical Materials (AIOM) invited speakers.
FiO 6: Quantum Electronics
6.1: High-Power Continuous-Wave and Fiber Lasers Invited Speakers:
FThD1, High Power CW and Pulsed Fiber Lasers with Double Cladding Fiber Made in China, Qihong Lou, Jun Zhou, Bin He, Songtao Du; Shanghai Inst. of Optics and Fine Mechanics, China
FThD2, 100-kW Coherently Combined Nd:YAG MOPA Laser Array, Stuart J. McNaught, Charles P. Asman, Hagop Injeyan, Andrew Jankevics, Adam M. F. Johnson, Gina C. Jones, Hiroshi Komine, Jason Machan, Jay Marmo, Michael McClellan, Randy Simpson, Jeff Sollee, Marcy M. Valley, Mark Weber, S. Benjamin Weiss; Northrop Grumman Aerospace Systems, USA
FThD5, Spatial Filtering Properties of Large-Mode-Area Fibers with Confined Gain Dopants, John R. Marciante; Univ. of Rochester, USA
FThJ1, Title to Be Announced, Valentin Gapontsev; IPG Photonics Corp., USA
FThJ4, High-Power Fiber Lasers and Amplifiers, Andreas Tünnermann¹,², Thomas Schreiber¹,², Jens Limpert¹,²; ¹Friedrich-Schiller Univ. Jena, Germany, ²Fraunhofer Inst. for Applied Optics and Precision Engineering, Germany
6.2: Microcavity Devices Invited Speakers:
FThC1, Crystalline Whispering Gallery Mode Resonators: Recent Advances and Future Trends, Lute Maleki, Andrey B. Matsko, Anatoliy A. Savchenkov, Vladimir S. Ilchenko, David Seidel; OEwaves, Inc., USA
FThC4, Applications of High-Q Optical Microresonators in Communication, Mani Hossein-Zadeh; Ctr. for High Technology Materials, Univ. of New Mexico, USA
FThO3, Simultaneous Oscillation of Wavelength-Tunable Singlemode Lasers Using Er:ZBLALiP Whispering Gallery Mode Resonator, Patrice Féron¹, Lei Xiao¹,², Stéphane Trébaol¹, Yannick Dumeige¹, Yann G. Boucher¹, ZhiPing Cai², Michel Mortier³; ¹Univ. de Rennes 1, France, ²Xiamen Univ., China, ³Lab de Chimie Appliqúee de l'Etat Solide-LCAES, CNRS-UMR, France
FThU3, Quantum Computing with Rydberg Atoms in Cavities, M. Everitt, J. Dunningham, B. T. H. Varcoe; Univ. of Leeds, UK
6.3: Nonlinear Statistical Optics Invited Speakers:
FTuR1, Freak Ocean Waves in One and Two Dimensions, Peter Janssen, Jean-Raymond Bidlot; European Ctr. for Medium-Range Weather Forecasts, UK
FTuR2, Rogue Waves in Optics, J. M. Dudley¹, G. Genty², F. Dias³; ¹Univ. of Franche- Comté, France, ²Tampere Univ. of Technology, Finland, ³Ctr. de Mathématiques et de Leurs Applications, École Normale Supérieure de Cachan, France
FTuR3, Methods for Simulating Rare Events in Optical Systems, Gino Biondini¹, Richard O. Moore²; ¹SUNY Buffalo, USA, ²New Jersey Inst. of Technology, USA FWD1, Thermodynamic Approach of Statistical Nonlinear Optics, B. Kibler¹, B. Barviau¹, S. Coen², J. Fleischer³, A. Kudlinski4, P. Aschieri5, G. Millot¹, A. Picozzi¹; ¹Univ. de Bourgogne, France, ²Univ. of Auckland, New Zealand, ³Princeton Univ., USA, 4Univ. de Lille, France, 5Univ. de Nice Sophia Antipolis, France
FWD4, Gravity-Like Effects on Light and Fiber Supercontinuum, Dmitry Skryabin; Univ. of Bath, UK
6.4: Quantum Optics in Waveguides Invited Speakers:
FMG1, Quantum Information Science with Photons on a Chip, Alberto Peruzzo, Alberto Politi, Jonathan C. F. Matthews, Anthony Laing, Pruet Kalasuwan, Xiao-Qi Zhou, Maria Rodas, Martin J. Cryan, John G. Rarity, Andre Stefanov, Siyuan Yu, Mark G. Thompson, Jeremy O’Brien; Univ. of Bristol, UK
FMG4, Quantum Optics in Waveguide Lattices, Yaron Bromberg¹, Yoav Lahini¹, Roberto Morandotti², Yaron Silberberg¹; ¹Weizmann Inst. of Science, Israel, ²INRS, Canada
FWJ3, Photon Pair Generation in Birefringent Fiber: A Route to Better Photons, Jeff S. Lundeen¹, Offir Cohen², Pierre Mahou², Brian J. Smith², Ian A. Walmsley²; ¹Inst. for Natl. Measurement Standards, Natl. Res. Council Canada, Canada, ²Clarendon Lab, Univ. of Oxford, UK
FWJ5, Quantum Logic Gates with Fiber-Generated Entanglement in the Telecommunications Band, Prem Kumar, Monika Patel, Milja Medic, Matthew A. Hall, Joseph B. Altepeter; Northwestern Univ., USA
6.5: Entanglement Generation and Measurement Tutorial Speaker:
JTuB1, Efficient Algorithms for Quantum State and Process Tomography, Andrew Doherty; Univ. of Queensland, Australia
Invited Speakers:
JMA1, Synthesizing Arbitrary Photon States in a Superconducting Resonator: The Quantum Digital to Analog Converter, John Martinis, Max Hofheinz, H. Wang, M. Ansmann, Radoslaw C. Bialczak, Erik Lucero, M. Neeley, A. D. O’Connell, D. Sank, J. Wenner, A. N. Cleland; Univ. of California at Santa Barbara, USA
JWD1, Strong Interactions of Single Atoms and Photons with Toroidal Micro- Resonators, H. Jeff Kimble; Caltech, USA.
JWD6, Measurement-Based Entanglement and Quantum Information Processing with Remote Ions, Peter Maunz, Steven Olmschenk, David Hayes, Dzmitry N. Matsukevich, Christopher Monroe; Joint Quantum Inst., Univ. of Maryland and NIST, USA
JWE1, Hyperentangled Photons for Communication and Metrology, Paul Kwiat¹, Julio Barreiro¹,²; ¹Univ. of Illinois at Urbana-Champaign, USA, ²Univ. Innsbruck, Austria
JWE4, Quantum Field State Control and Measurement in a Cavity, J. M. Raimond, S. Deléglise, C. Sayrin, X. Zhou, I. Dotsenko, S, Gleyzes, M. Brune, S. Haroche; École Normale Supérieure, France
6.6: Anderson Localization of Classical and Quantum Waves Invited Speakers:
FMC1, Multiple Scattering of Light in Atomic Gases: From Levy Flights to Random Lasers, Robin Kaiser; Univ. de Nice Sophia-Antipolis, France
FMC4, Photons, Dust and Honey Bees, Pierre Barthelemy, Jacopo Bertolotti, Diederik S. Wiersma; European Lab for Non Linear Spectroscopy, Univ. of Florence, Italy
FTuJ1, Probing Localization in Absorbing Systems via Loschmidt Echos, Tsampikos Kottos¹,²; ¹Wesleyan Univ., USA, ²Max-Planck-Inst., Germany
FTuJ4, Quantum Optics of Random Media, Sergey E. Skipetrov; CNRS, Univ. Joseph Fourier, France
2.1: Extreme Light Sources (Joint with FiO 2)
5.6: Design and Fabrication of Plasmonic Devices and Metamaterials (Joint with FiO 5)
FiO 7: Vision and Color
7.1: Molecular Imaging in the Eye (Joint with FiO 3) Tutorial Speaker:
FThQ1, Molecular Imaging in the Eye, Frederick Fitzke; Univ. College London, UK Invited Speakers:
FThQ3, In vivo Cellular Imaging of the Rodent Retina, Jason Porter; Univ. of Houston, USA
FThQ4, Molecular Imaging with OCT, Joseph Izatt; Dept. of Biomedical Engineering, Duke Univ., USA
View Adaptive Optics: Methods, Analysis and Applications (AO) invited speakers.
7.2: Advances in Adaptive Optics Imaging of the Living Retina Invited Speakers:
JWB3, Adaptive Optics Psychophysics, Heidi Hofer; Univ. of Houston, USA
JWF1, Adaptive Optics Instrumentation, Stephen A. Burns¹, Zhangyi Zhong¹, Weiyao Zou¹, Cong Deng¹, Daniel Ferguson², Xiaofeng Qi¹; ¹Indiana Univ., USA, ²Physical Sciences Inc., USA
JWF3, Adaptive Optics-OCT Imaging of the Retina, Donald T. Miller; Indiana Univ., USA
View Adaptive Optics: Methods, Analysis and Applications (AO) invited speakers.
7.3: Light in the Eye Tutorial Speaker:
FTuQ1, Light and Eye Safety, David Sliney; Consulting Medical Physicist, USA
Invited Speakers:
FTuQ2, Unexpected Retinal Damage below the ANSI Standard, Jennifer Hunter¹, Jessica I. W. Morgan², William H. Merigan¹, David R. Williams¹; ¹Univ. of Rochester, USA, ²Univ. of Pennsylvania, USA
FTuQ3, Light Exposure and the Retina, Jacque Duncan; Univ. of California at San Francisco, USA 1.1: Novel Optical Architectures in Emerging Technologies (Joint with FiO 1)
2.3: Biomedical Applications of Ultrafast Optics (Joint with FiO 2 and 3)
LS 1: Optical Probes of Molecular Chirality and Supramolecular Chiral Assemblies Invited Speakers:
LSMB1, Probing Molecular Chirality by Conventional and Fluorescence Detected Electronic Circular Dichroism, Nina Berova; Columbia Univ., USA
LSMB2, Optical Activity at Interfaces, Peer Fischer; Rowland Inst. at Harvard, Harvard Univ., USA
LSMB3, Intrinsic Chiroptical Response and Its Mediation by Extrinsic Perturbations, Patrick H. Vaccaro; Yale Univ., USA
LSMB4, Circularly Polarized Luminescence from Single Chiral Molecules, Michael D. Barnes, Ruthanne Hassey-Paradise, D. Venkataraman; Univ. of Massachusetts, Amherst, USA
LSMF1, Chiroptical Imaging of Crystals by Mueller Matrix Microscopy, John Freudenthal¹,², Erica Gunn², Bart Kahr¹,²; ¹New York Univ., USA, ²Univ. of Washington, USA
LSMF2, Second-Order Nonlinear Optical Imaging of Chiral Crystals, Ellen Gualtieri, Victoria Hall, Sarah Harden, David Kissick, Ronald Wampler, Debbie Wanapun, Garth J. Simpson; Purdue Univ., USA
LSMF3, Structural Origin of Circularly Polarized Iridescence in Jeweled Beetles, Mohan Srinivasarao; Georgia Tech, USA
LS 2: Single-Molecule Biophysics Invited Speakers:
LSWA1, Single-Molecule Biophysical Imaging, Superresolution, and Trapping, W. E. Moerner; Stanford Univ., USA
LSWA2, Optical Nanoscopy: FPALM Breaks the Diffraction Limit, Samuel Hess; Univ. of Maine, USA LSWD1, Real-Time 3-D Single-Particle Tracking Spectroscopy for Cellular Dynamics, Haw Yang; Princeton Univ., USA
LSWD4, Tracking Fluorescence Correlation Spectroscopy of Individual Biomolecules, Kevin McHale¹,², Andrew Berglund³, Ke Zhang¹, Charles Limouse¹, Chandra Raman¹,4, Hideo Mabuchi¹; ¹Stanford Univ., USA, ²Lab of Chemical Physics, NIDDK, NIH, USA, ³CNST Nanofabrication Res. Group, NIST, USA, 4Georgia Tech, USA
LSWD5, Local Structural Flexibility of Nucleic Acid Probed by a Wide Field Single Molecule FRET Imaging Technique, Tae-Hee Lee; Pennsylvania State Univ., USA
LSThB1, Investigating Amyloid Nucleation and Growth Using Single Molecule Fluorescence Microscopy, Keith Berland, David G. Lynn, Yan Liang; Emory Univ., USA
LSThB2, 3-D Localization in Fluorescence Photoactivation Localization Microscopy and Particle Tracking, Joerg Bewersdorf¹,², Michael J. Mlodzianoski¹,², Stefanie E. K. Kirschbaum²,³,4,5, Manuel F. Juette¹,²,4,5; ¹Yale Univ. School of Medicine, USA, ²Inst. for Molecular Biophysics, The Jackson Lab, USA, ³Dept. of Physics and Astronomy, Univ. of Maine, USA, 4Dept. of Biophysical Chemistry, Univ. of Heidelberg, Germany, 5Dept. of New Materials and Biosystems, Max Planck Inst. for Metals Res., Germany
LSThB3, Single Molecule Imaging of Axonal Transport in Live Neurons, Harsha V. Mudrakola, Chengbiao Wu, Kai Zhang, Bianxiao Cui; Stanford Univ., USA
LSThB4, Probing Cellular Events with Single Quantum Dot Imaging, Maxime Dahan; Lab Kastler Brossel, École Normale Supérieure, France
LSThD1, Imaging Gene Transcription, Christopher J. Fecko; Univ. of North Carolina at Chapel Hill, USA
LSThD2, Total Internal Reflection with Fluorescence Correlation Spectroscopy, Nancy Thompson; Univ. of North Carolina at Chapel Hill, USA
LSThD3, DNA Repair Protein Dynamics through Single-Molecule Fluorescence, Keith R. Weninger¹, Lauryn E. Sass², Vanessa C. DeRocco², Trevor Anderson¹, Dorothy A. Erie²; ¹North Carolina State Univ., USA, ²Univ. of North Carolina at Chapel Hill, USA
LSThF1, Non-Scanning Two-Photon Microscopy for Imaging in Live Cells, Christine Payne; Georgia Tech, USA
LSThF2, Tracking Single Quantum Dots in Three Dimensions: Following Cell Receptor Traffic and Membrane Topology, Nathan P. Wells¹, Diane S. Lidke², M. Lisa Phipps¹, Peter M. Goodwin¹, Bridget S. Wilson², James Werner¹; ¹Los Alamos Natl. Lab, USA, ²Univ. of New Mexico, USA
LSThF3, Dissecting the Molecular Mechanism of Kinesin with Single Molecule Imaging, Ahmet Yildiz; Univ. of California at Berkeley, USA LS 3: Micro- and Nanofluidic Systems Invited Speakers:
LSMC1, Applications of Silicon Photonic Technology for Clinical Diagnostics and Highly Multiplexed Biomolecular Detection, Adam L. Washburn, Abraham J. Qavi, Matthew S. Luchansky, Ji-Yeon Byeon, Ryan C. Bailey; Univ. of Illinois at Urbana- Champaign, USA
LSMC2, Ion Conductance Microscopy of Nanometer Pores, Lane A. Baker; Indiana Univ., USA
LSMC4, Massively Parallel Opto/Electric Manipulation of Colloidal Particles, Steve Wereley; Purdue Univ., USA
LSMG1, Optical and Microfluidic Techniques for Cellular Analysis, Daniel T. Chiu; Univ. of Washington, USA
LSMG2, Optical Microcavities: Label-Free Detection down to Single Virus Particles, Frank Vollmer¹, Stephen Arnold²; ¹Rowland Inst., Harvard Univ., USA, ²Polytechnic Inst., New York Univ., USA
LSMG4, Ultrafast Laser Nanomachining of Analytical and Diagnostic Biomedical Devices, Alan J. Hunt; Univ. of Michigan, USA
LSMG5, Optical and Electrical Characterization of Fluid Transport in Nanoscale Channels, Stephen C. Jacobson, John M. Perry, Kaimeng Zhou; Indiana Univ., USA
LSTuF1, Single Molecule Tracking as a Probe of Free Volume Transitions in Stimulus- Responsive Polymers—Do Single Molecules Behave Like Caribou? Lindsay C. C. Elliott¹, Paul Bohn²; ¹Univ. of Illinois at Urbana-Champaign, USA, ²Univ. of Notre Dame, USA
LSTuF4, Micro- and Nanofluidics for Single Biomolecule Analysis, Yoshinobu Baba; Nagoya Univ., Japan
LS 4: Second-Order Nonlinear Optics Invited Speakers:
LSWB1, Sum Frequency Generation (SFG) Vibrational Spectroscopy and Its Application in Surface Science and Catalysis, Gabor A. Somorjai, George J. Holinga; Univ. of California at Berkeley, USA
LSWB2, Nonlinear Optical Studies of Conjugated Polymer Films and Interfaces, Ian M. Craig, Benjamin J. Schwartz; Univ. of California at Los Angeles, USA LSWB5, Resonant UV SHG Studies of Ion Adsorption at Aqueous Interfaces, Richard J. Saykally¹,²; ¹Univ. of California at Berkeley, USA, ²Lawrence Berkeley Natl. Lab, USA
LSWE1, Nonlinear Optics in Metamaterials, David Cho¹, Wei Wu², Feng Wang¹, Xiang Zhang³, Yuen-Ron Shen¹; ¹Physics Dept., Univ. of California at Berkeley, USA, ²Quantum Science Res., Hewlett-Packard Labs, USA, ³Dept. of Mechanical Engineering, Univ. of California at Berkeley, USA
LSWE2, New Perspectives in Vibrational Sum-Frequency Spectroscopy, John T. Fourkas; Univ. of Maryland at College Park, USA
LSWE3, Polarization-Rotation and Two-Dimensional IR-Visible Sum Frequency Generation Spectroscopy for Surface Analysis, Keng C. Chou; Univ. of British Columbia, USA
LSWH1, Imaging Nonlinear Optical Stokes Ellipsometry for Thin Film and Microparticle Characterization, Garth J. Simpson; Purdue Univ., USA
LSWH2, Electronically Resonant Hyper-Raman Scattering in Solution, Anne M. Kelley; Univ. of California at Merced, USA
LSWH3, Title to Be Announced, Steven Baldelli; Univ. of Houston, USA
LSWK1, Vibrationally-Electronically Doubly-Resonant Sum-Frequency Generation Spectroscopy of Molecular Thin Films, Taka-aki Ishibashi; Hiroshima Univ., Japan
LSWK2, Measurement of Surface Chirality with Nonlinear Spectroscopy: A Quantitative Approach, Yan-yan Xu, Feng Wei, Yuan Guo, Hongfei Wang; Inst. of Chemistry, Chinese Acad. of Sciences, China
LS 5: Cavity Optomechanics Invited Speakers:
LSTuB1, Cavity Optomechanics with Ions, K. Vahala¹, M. Herrmann², S. Knünz², V. Batteiger², G. Saathoff², T. W. Hänsch², Th Udem²; ¹Caltech, USA, ²Max-Planck-Inst. für Quantenoptik, Germany
LSTuB2, Preparation and Detection of a Mechanical Resonator Near the Ground State of Motion, Keith Schwab; Cornell Univ., USA
LSTuB5, Cooling Acoustic Oscillators with Electromagnetic Parametric Transducers and Prospects of Measuring below the Standard Quantum Limit of Displacement, Michael Tobar; Univ. of Western Australia, Australia
LSTuE1, Control and Sensing of Ultracold Atoms and Molecules by Nanomechanical Cantilevers, Pierre Meystre; Univ. of Arizona, USA LSTuE2, Optomechanics of Phononic-Photonic Crystal Defect Cavities, Matt Eichenfield, Jasper Chan, Ryan M. Camacho, Kerry J. Vahala, Oskar J. Painter; Caltech, USA
LSTuE3, Sensing Nanomechanical Motion with a Shot-Noise Limited Microwave Cavity Interferometer, Konrad W. Lehnert, John D. Teufel, Tobias Donner, Jennifer W. Harlow, Manuel A. Castellanos-Betran; JILA, NIST, Univ. of Colorado, USA
LSTuH1, Demonstration of Micromechanics in the Strong Coupling Regime, Simon Groeblacher, Klemens Hammerer, Michael Vanner, Markus Aspelmeyer; IQOQI, Austrian Acad. of Sciences, Austria
LSTuH2, Measurement of Attractive and Repulsive Casimir Forces and Applications to Nanomechanics, Jeremy Munday¹, Federico Capasso²; ¹Thomas J. Watson Labs of Applied Physics, Caltech, USA, ²Harvard Univ., USA
LSTuH3, Exploring the Quantum Limit in Gravitational Wave Detection, Nergis Mavalvala; MIT, USA
LSTuH4, Silicon Optomechanics, Hong X. Tang; Yale Univ., USA
LSTuK1, Optomechanical Correlations between Light and Mirrors, A. Heidmann, P. Verlot, A. Tavernarakis, C. Molinelli, A. Kuhn, T. Briant, P.-f. Cohadon; Lab Kastler Brossel, École Normale Supérieure, Univ. Pierre et Marie Curie, CNRS, France
LSTuK2, Resolved-Sideband Laser Cooling and Measurement of a Micromechanical Oscillator Close to the Quantum Limit, Tobias J. Kippenberg¹,²; ¹Swiss Federal Inst. of Technology Lausanne (EFPL), Switzerland, ²Max Planck Inst. of Quantum Optics, Germany
LS 6: Optoelectronic Materials Characterization Invited Speakers:
LSTuD1, Strong Coupling of Propagating Laser Light to Single Emitters: From Absorption to Stimulated Emission, Vahid Sandoghdar; ETH Zurich, Switzerland
LSTuD2, Single Quantum Dots for Probing Local Environments, Haw Yang; Princeton Univ., USA
LSTuG1, Using Fluorescence Microscopy of Oligomer Aggregates to Understand the Properties of Conjugated Polymers Used in Photovoltaic Devices, Linda Peteanu¹, Gizelle A. Sherwood¹, Kelly Zewe¹, Jurjen Wildeman², James H. Werner³, Andrew P. Shreve³; ¹Carnegie Mellon Univ., USA, ²Zernike Inst. for Advanced Materials, Univ. of Groningen, Netherlands, ³Ctr. for Integrated Nanotechnologies, Los Alamos Natl. Labs, USA LSTuG7, New Aspects of Nanocrystal Lasing, Victor I. Klimov; Los Alamos Natl. Lab, USA
LSTuJ1, Quantum Dots, Experiments, Theory, Predictions, Tests and Unknowns, Rudolph A. Marcus; Caltech, USA
LSTuJ4, Non-Blinking Semiconductor Nanocrystals, Xiaoyong Wang¹, Xiaofan Ren², Keith Kahen², Megan A. Hahn¹, Manju Rajeswaran², Sara Maccagnano-Zacher³, John Silcox³, George E. Cragg4, Alexander L. Efros4, Todd Krauss¹,5; ¹Univ. of Rochester, USA, ²Eastman Kodak Co., USA, ³Cornell Univ., USA, 4NRL, USA, 5Inst. of Optics, Univ. of Rochester, USA
LSWG1, Ultrafast Photoemission Electron Microscopy: Imaging Nonlinear Plasmonic Phenomena on the Femto/Nano Scale, Hrvoje Petek; Univ. of Pittsburgh, USA
LSWG2, New Interface-Selective Electronic Spectroscopy and its Extension to Femtosecond Time-Resolved Measurements, Tahei Tahara; RIKEN, Japan
LSWG5, Ultrafast Hybrid Plasmonics: New Routes to Nanoscale Imaging and Energy Propagation, Gary Wiederrecht; Argonne Natl. Lab, USA
LSWJ2, Ultrafast Laser-Induced Magnetization Dynamics, Bert Koopmans; Eindhoven Univ. of Technology, Netherlands
LSWJ4, Dynamic Signatures of Exciton-Plasmon Interactions in Hybrid Semiconductor-Metal Nanostructures, Marc Achermann; Univ. of Massachusetts at Amherst, USA
LSWJ5, One-Dimensional Exciton Dynamics in Carbon Nanotubes, Tobias Hertel, Zipeng Zhu, Dominik Stich, Jared Crochet; Univ. of Wurzburg, Germany
LS 7: Ultrafast X-Ray Science Invited Speakers:
LSMD1, Title to Be Announced, Jerome Hastings; Stanford Linear Accelerator Ctr., Stanford Univ., USA
LSMD2, The X-Ray Pump-Probe Instrument at LCLS, David Fritz; SLAC Natl. Accelerator Lab, Stanford Univ., USA
LSMD3, Watching Atoms Move: Using X-Ray Diffraction to Observe Structural Dynamics in Crystals on Fundamental Time Scales, Steven L. Johnson; Paul Scherrer Inst., Switzerland
LSMD4, Time-Resolved X-Ray Solution Scattering Reveals Solution-Phase Structural Dynamics, Harry Ihee; KAIST, Republic of Korea
LSMH1, Ultrafast X-Ray Physics with the X-Ray Split and Delay Unit at FLASH, F. Sorgenfrei, W. F. Schlotter, M. Nagasono, M. Beye, T. Beeck, W. Wurth, A. Föhlisch; Inst. für Experimentalphysik, Univ. Hamburg and Ctr. for Free-Electron Laser Science, Germany
LSMH2, Magnetization Dynamics on the Nanoscale, Yves Acremann; PULSE Inst., Stanford Linear Accelerator Ctr., USA
LSMH3, Ultrafast Electron and Spin Dynamics in Complex Materials, Hermann A. Dürr; Helmholtz Zentrum Berlin, BESSY II, Germany
LSTuC1, Sub-Picosecond Intersystem Crossings and Structural Dynamics: Combined Ultrafast Optical and X-Ray Absorption Studies, Majed Chergui; Lab of Ultrafast Spectroscopy, École Polytechnique Fédérale de Lausanne, Switzerland
LSTuC2, Structural Tracking of Chemical Reactions in Solution by Time-Resolved X- Ray Scattering, Martin Meedom Nielsen; Nano-Science Ctr., Univ. of Copenhagen, Denmark
LSTuC3, Ultrafast Photochemical Dynamics in Solution, Munira Khalil; Univ. of Washington, USA
LSTuC4, Ultrafast Soft X-Ray Spectroscopy of Spin-Crossover Dynamics in Solvated Transition-Metal Complexes, Nils Huse¹, Ha Na Cho¹,², Tae-Kyu Kim², Lindsey Jamula³, James McCusker³, Robert Schoenlein4,¹; ¹Chemical Sciences Div., Lawrence Berkeley Natl. Lab, USA, ²Pusan Natl. Univ., Republic of Korea, ³Michigan State Univ., USA, 4Advanced Light Source, Lawrence Berkeley Natl. Lab, USA
LS 8: Multidimensional Spectroscopy Invited Speakers:
LSWC1, Investigating the Major Light Harvesting Complex of Photosystem II with 2- D Electronic Spectroscopy, G. S. Schlau-Cohen, T. R. Calhoun, N. S. Ginsberg, G. R. Fleming; Univ. of California at Berkeley, USA
LSWC2, Coherence in Electronic Energy Transfer: The Intermediate Coupling Regime, Gregory D. Scholes, Elisabetta Collini; Univ. of Toronto, Canada
LSWC3, Optical Two-Dimensional Fourier Transform Spectroscopy of Semiconductors, S. T. Cundiff, A. D. Bristow, D. Karaiskaj, X. Dai; JILA, NIST, Univ. of Colorado, USA
LSWC4, Exciton Relaxation and Energy Transfer Dynamics in Size Selected Polythiophenes, Andrew T. Healy, Nathan P. Wells, Bryan W. Boudouris, Marc A. Hillmyer, David A. Blank; Univ. of Minnesota, USA
LSWF1, Water and Hydrogen-Bond Dynamics in Aqueous Solutions, Damien Laage¹, Guillaume Stirnemann¹, Fabio Sterpone¹, James T. Hynes¹,²; ¹École Normale Supérieure, France, ²Univ. of Colorado, USA
LSWF2, Watching Ultrafast Molecular Dynamics: 2-D IR Chemical Exchange Spectroscopy, Michael D. Fayer; Stanford Univ., USA
LSWF3, Ultrafast Dynamics of Hydrogen Bond Exchange in Aqueous Ionic Solutions, Sungnam Park¹,², Michael Odelius³, Kelly J. Gaffney²; ¹Korea Univ., Republic of Korea, ²Stanford Univ., USA, ³Stockholm Univ., Sweden
LSWI1, Femtosecond Vibrational Optical Activity and IR Photon Echo Studies of Small Organic Molecules, MinHaeng Cho; Korea Univ., Republic of Korea
LSWI2, Correlating Energy Transport Time on a Molecular Level with Distance Using Relaxation-Assisted 2DIR, Igor V. Rubtsov¹, Valeriy M. Kasyanenko¹, Zhiwei Lin¹, Christopher S. Keating¹, Grigory I. Rubtsov², James P. Donahue¹; ¹Tulane Univ., USA, ²Inst. for Nuclear Res., Russian Federation
LS 9: Coherent X-Ray Imaging Invited Speakers:
LSThA1, What Kind of Data Do We Expect in Single-Molecule Imaging Experiments and How Do We Process It? Veit Elser, Duane Ne-Te Loh; Cornell Univ., USA
LSThA2, The Coherent X-Ray Imaging Instrument at LCLS, Sébastien Boutet; SLAC Natl. Accelerator Lab, Stanford Univ., USA
LSThA3, Femtosecond Dynamic Diffraction Imaging with Free Electron Lasers: X- Ray Snapshots of Ultra-Fast Nanoscale Phenomena, Anton Barty¹, Henry N. Chapman², Michael J. Bogan¹, Sébastien Boutet¹,³,4, Matthias Frank¹, Stefan P. Hau-Riege¹, Stefano Marchesini¹,5, Bruce W. Woods¹, Saša Bajt¹, W. Henry Benner¹, Richard A. London¹, Elke Plönjes6, Marion Kuhlmann6, Rolf Treusch6, Stefan Düsterer6, Thomas Tschentscher6, Jochen R. Schneider6, Eberhard Spiller7, Thomas Möller8, Christoph Bostedt8, Matthias Hoener8, David A. Shapiro5, Keith O. Hodgson³, David van der Spoel4, Magnus Bergh4, Carl Caleman4, Gösta Huldt4, Bianca Iwan4, M. Marvin Seibert4, Filipe R. N. C. Maia4, Abraham Szöke¹,4, Nicusor Timneanu4, Janos Hajdu³,4; ¹Lawrence Livermore Natl. Lab, USA, ²Ctr. for Free Electron Laser Science, Univ. Hamburg, Germany, ³Stanford Synchrotron Radiation Lab, Stanford Linear Accelerator Ctr., USA, 4Uppsala Univ., Sweden, 5Univ. of California at Davis, USA, 6Deutsches Elektronen-Synchrotron, DESY, Germany, 7Spiller X-Ray Optics, USA, 8Inst. für Atomare Physik, Technische Univ. Berlin, Germany LSThA4, Title to Be Announced, Stefan Hau-Riege; Lawerence Livermore Natl. Lab, USA
LSThE1, Ankylography: Three-Dimensional Structure Determination from a Single View, Jianwei Miao; Univ. of California at Los Angeles, USA
LSThE2, Imaging of Domain Structures by Coherent X-Ray Diffraction, Ian Robinson; Univ. College London, UK
LS 10: X-Ray Photon Correlation Spectroscopy Invited Speakers:
LSThC1, The X-Ray Photon Correlation Spectroscopy Instrument at LCLS, Aymeric Robert; Linac Coherent Light Source, SLAC Natl. Accelerator Lab, Stanford Univ., USA
LSThC2, Title to Be Announced, Simon Mochrie; Yale Univ., USA
LSThC3, Using X-Ray Correlation Spectroscopy to Test Dynamical Scaling, Mark Sutton; McGill Univ., Canada
LS 11: High Field Dynamics Invited Speakers:
LSTuI1, Fast Electron Migration in Finite Systems under Attosecond and XFEL Light Pulses, Jan-Michael Rost, Ulf Saalmann, Ionut Georgescu, Christian Gnodtke, Alexey Mikaberidze; Max-Planck-Inst. for the Physics of Complex Systems, Germany
LSTuI2, Strong-Field Atomic Physics in the X-Ray Regime, Louis DiMauro; Ohio State Univ., USA
LSTuI3, Probing Coupled Electronic and Nuclear Dynamics Using Coherent Electrons and X-Rays, Wen Li¹, Xibin Zhou¹, Robynne Lock¹, Serguei Patchkovskii², Albert Stolow², Etienne Gagnon¹, Arvinder Sandhu¹, Robin Santra³, Phay Ho³, Vandana Sharma¹, Craig W. Hogle¹, Predrag Ranitovic4, C. Lewis Cocke4, Margaret Murnane¹, Henry C. Kapteyn¹; ¹JILA, Univ. of Colorado at Boulder, USA, ²Natl. Res. Council Canada, Canada, ³Argonne Natl. Lab, USA, 4Kansas State Univ., USA
LSTuL1, First Science with the LCLS X-Ray Free Electron Laser, John D. Bozek; SLAC Natl. Accelerator Lab, Stanford Univ., USA
LSTuL3, X-Ray Probing of High Field Ionization in the Attosecond Limit, Stephen R. Leone; Lawrence Berkeley Natl. Lab, Univ. of California at Berkeley, USA LSTuL4, Ptychographic Imaging in Materials and Life Sciences, Andreas Menzel¹, Cameron M. Kewish¹, Pierre Thibault¹, Martin Dierolf², Franz Pfeiffer², Oliver Bunk¹; ¹Paul Scherrer Inst., Switzerland, ²Technische Univ. München, Germany
Special Symposia at Frontiers in Optics 2009/Laser Science XXV
The Future of 3-D Display: The Marketplace and the Technology Symposium organizer: Hong Hua; Univ. of Arizona, USA 3-D displays have become substantially critical for many applications, including medical and scientific visualization, flight simulation and training, engineering design, and entertainment. One example is the reviving enthusiasm in 3-D cinema. A recent animated film, ―Beowulf‖, was shown in 3-D in many theaters around the world and generated millions of dollars in box office revenue. There is also increasing interest in developing 3-D home entertainment systems. On the technology side, many of the traditional displays methods, such as 3-D projection See Lahsen Assoufid, FiO Program Chair, discuss highlights of the symposium. systems and head mounted displays, have been making steady improvements, and several different new display concepts and technologies have emerged. This symposium aims at bringing together researchers who are involved in 3-D display technologies, a range of applications, and research vis-à- vis human factor. Keynote Speaker FTuA1, 3-D Entertainment: A Revolution that has Already Started, Rod Archer; RealD Inc., USA Tutorial Speaker FTuA2, What Should We Know about Human Depth Perception in Constructing 3-D Displays? Martin Banks; Univ. of California at Berkeley, USA Invited Speakers FTuF1, Three-Dimensional Sensing, Visualization, and Display by Integral Imaging, Bahram Javidi¹, Manuel Martinez-Corral², Adrian Stern³, Edward Watson4; ¹Univ. of Connecticut, USA, ²Univ. of Valencia, Spain, ³Ben Gurion Univ. of the Negev, Israel, 4AFRL, USA FTuF2, Development of Integral Images, Pingfan Wu, Douglas S. Dunn, Robert L. Smithson, Steven J. Rhyner; 3M Corp., USA FTuF3, Problems in Physically Based Simulations of Real-World Environments, Donald P. Greenberg; Program of Computer Graphics, Cornell Univ., USA FTuM1, Accommodation Responses to Stereoscopic Images, Kazuhiko Ukai; Waseda Univ., Japan FTuM2, A Novel 3-D Display that Presents Nearly Correct Focus Cues, Martin S. Banks¹, Gordon D. Love², David M. Hoffman¹, Philip J. W. Hands², Andrew K. Kirby²; ¹Univ. of California at Berkeley, USA, ²Durham Univ., UK FTuM3, Volumetric True 3-D Display Using Multi-Focal Scanned Light, Brian Schowengerdt; Univ. of Washington, USA FTuM4, 3-D TV Based on Integral Method Using Extremely High-Resolution Video System, Masahiro Kawakita, Jun Arai, Fumio Okano; NHK Science & Technical Res. Labs, Japan FTuT1, Large Area 3-D Updateable Holographic Displays Using Photorefractive Polymers, Nasser Peyghambarian; Univ. of Arizona, USA FTuT2, Progress in Volumetric Three-Dimensional Displays and Their Applications, Gregg E. Favalora; Actuality Systems Inc., USA FTuT3, The Coming Generation of Head Worn Displays, Kevin Thompson¹, James P. McGuire¹, Ozan Cakmakci¹, Jannick P. Rolland²; ¹Optical Res. Associates, USA, ²Inst. of Optics, Univ. of Rochester, USA
Gravitational Wave Interferometry from Earth and Space Symposium organizer: Michael Barnes¹, David Reitze²; ¹Univ. of Massachusetts Amherst, USA, ²Univ. of Florida, USA Within the past 10 years, kilometer-scale terrestrial gravitational wave detectors have been built to search for gravitational waves emitted from cataclysmic astrophysical sources such as colliding black holes and the Big Bang. In order to detect gravitational waves, surface-based interferometers have been developed with unprecedented sensitivities, approaching 10-19 m/s. Plans are underway to develop space-based See Tom Carruthers, FiO Program Chair, discuss highlights of the symposium. gravitational wave detectors that will open up a whole new window on the universe. Large-scale underground optical and atom interferometers are in the planning phases. This symposium will cover the emerging field of gravitational wave astronomy with an emphasis on the central role lasers and optical technologies play in the operation of gravitational wave detectors. Tutorial Speaker JMB1, Gravitational Wave Interferometry, Peter Fritschel; MIT, USA Invited Speakers JMB2, LISA: Detecting Gravitational Waves from Space, Jeffrey Livas; NASA Goddard Space Flight Ctr., USA JMB4, The Virgo Gravitational Wave Detector, François Bondu; Univ. de Rennes 1, France JTuA1, Next Generation Interferometers for Gravitational Wave Astronomy, Rana Adhikari; Caltech, USA JTuA3, GEO600 and Directions in Optics Related Research for Interferometric Gravitational Wave Detector, Sheila Rowan; Univ. of Glasgow, UK JTuA5, Japanese Gravitational Wave Detectors: LCGT and DECIGO, Seiji Kawamura, LCGT Collaboration, DECIGO Working Group; Natl. Astronomical Observatory of Japan, Japan
Laser Science Symposium on Undergraduate Research Symposium organizer: Harold Metcalf; Stony Brook Univ., USA This special DLS annual symposium is rapidly becoming one of the most successful DLS traditions (this year's is the ninth of a series that began at the Long Beach meeting in 2001). During the past several years the number of undergraduates presenting papers has grown from only 10 to nearly 40, and the talks have been of outstanding quality, some absolutely stellar. Last year's posters were outstanding as well, and generated a great deal of lively interest and on-the-spot discussion. This year's symposium will consist of afternoon poster and oral sessions. The event provides an opportunity for some of the student members of our community, who are already among the finest young scientists to be found anywhere, to present their work before an audience of their peers as well as the larger optics community. All are invited and encouraged to attend the sessions. View the Complete Program
Optics for Imaging at the Nanoscale and Beyond Symposium organizers: Lahsen Assoufid, Ian McNulty, Christian Schroer, Valeriy Yashchuk; Argonne Natl. Lab, USA Powerful and exciting new tools have enabled imaging with light at unprecedented resolution reaching well into the nanoscale, from the visible to the x-ray region. This symposium brings the latest optical methods for nanoscale imaging across a broad spectral range to the fore. Rapidly developing techniques are covered including single-molecule fluorescence and coherent diffractive imaging, and novel optical elements such as 4-PI lenses, Fresnel zone plates, and singular optics. Researchers in fundamental as well as applied and industrial See Lahsen Assoufid, FiO Program Chair, discuss highlights of the symposium. fields will find this symposium to address a wide range of topics relevant to imaging with light at the nanoscale. Tutorial Speaker FThA1, Introduction to Diffraction Limited X-Ray Optics, David Attwood; Lawrence Berkeley Natl. Lab, USA Invited Speakers FThA3, Singular and Other Novel X-Ray Diffractive Optics, Anne Sakdinawat; Lawrence Berkeley Natl. Lab, Univ. of California at Berkeley, USA FThA4, Laboratory X-Ray Micro- and Nano-Imaging, Hans M. Hertz, M. Bertilson, E. Chubarova, O. Hemberg, O. v Hofsten, A. Holmberg, M. Lindblom, U. Lundström, D. Nilsson, M. Otendal, J. Reinspach, P. Skoglund, P. Takman, T. Tuohimaa, U. Vogt; Royal Inst. of Technology, Sweden FThG1, X-Ray Nano-Tomography at HZB, Gerd Schneider¹, Peter Guttmann¹, Stefan Heim¹, Waltraud Müller², Jim McNally²; ¹Helmholtz-Zentrum Berlin für Materialien und Energie GmbH, Elektronenspeicherring BESSY II, Germany, ²Lab of Receptor Biology and Gene Expression, Natl. Cancer Inst., Natl. Inst. of Health, USA FThG2, X-Ray Refractive Optics for Nanofocusing, Anatoly Snigirev; European Synchrotron Radiation Facility, France FThG3, 10nm-Level Focusing of Hard X-Rays by KB Mirrors, Kazuto Yamauchi; Osaka Univ., Japan FThM1, Intracellular Nanoscale Imaging with Fluorescence Photoactivation Localization Microscopy, Samuel Hess; Univ. of Maine, USA FThM2, Nanoscale X-Ray Focusing with Reflective Optics, Gene E. Ice¹, Jonathan Z. Tischler¹, Jae-Young Choi², Wenjun Liu³, Ali Khounsary³, Lahsen Assoufid³, Deming Shu³, Chian Liu³; ¹Oak Ridge Natl. Lab, USA, ²Pohang Accelerator Lab, Republic of Korea, ³Advanced Photon Source, Argonne Natl. Lab, USA FThM3, Fabrication of Freeform Mirrors: Metrology and Figuring, Helge Thiess, H. Lasser; Carl Zeiss Laser Optics GmbH, Germany FThM4, The Hard X-Ray Nanoprobe Beamline at Argonne National Laboratory, Jörg Maser, Martin V. Holt, Robert P. Winarski, Volker Rose, Gregory Brian Stephenson, Peter Fuesz; Argonne Natl. Lab, USA FThT1, Multi-Modal Scanning X-Ray Microscopy, Andreas Menzel¹, Pierre Thibault¹, Martin Dierolf¹,², Cameron M. Kewish¹, Franz Pfeiffer,; ¹Paul Scherrer Inst., Switzerland, ²Ecole Polytechnique Fédérale de Lausanne, Switzerland FThT3, Future Developments for Hard X-Ray Zone Plates, Wenbing Yun; XRADIA Inc., USA
OSA Topical Meeting Highlights Symposium organizer: Michael Duncan, NRL, USA OSA offers a wide variety of topical meetings where cutting-edge research is presented. In an effort to bring some of the outstanding presentations that are given at these meetings to a broader audience, the committee has chosen, for the fourth year in a row, to offer a special session devoted to important papers from many of the topical meetings. One select presentation from each of a number of topical meetings held in 2009 (or late 2008) will be highlighted so that FiO attendees may see the type of exciting research being reported. The papers in this special session have been chosen by topical meeting attendees and by the topical meeting chairs. Invited Speakers Nonlinear Optics, 2009 FWO1, Active Terahertz Metamaterials, Hou-Tong Chen, John F. O'Hara, Abul K. Azad, Antoinette J. Taylor; Los Alamos Natl. Lab, USA Integrated Photonics and Nanophotonics Research and Applications, 2009 FWO2, Photonics in Supercomputing: The Road to Exascale, Jeffrey Kash; IBM Res., USA Optical Trapping Applications, 2009 FWO3, Optical Manipulation of Femtoliter Aqueous Droplets for Nanochemistry Applications, Ana Jofre, Ben Faulk, Jason Case; Univ. of North Carolina at Charlotte, USA Advanced Solid-State Photonics, 2009 FWO4, Fourier Domain Mode Locking (FDML): A New Laser Operating Regime and Applications for Biomedical Imaging, Profilometry, Ranging and Sensing, Robert Huber; Ludwig- Maximilians-Univ. München, Germany Digital Holography and Three-Dimensional Imaging, 2009 FWV1, Deflectometry Challenges Interferometry: 3-D-Metrology from Nanometer to Meter, Gerd Häusler¹,², M. C. Knauer¹, C. Faber¹, C. Richter¹, S. Peterhänsel¹, C. Kranitzky¹, K. Veit²; ¹Univ. of Erlangen-Nuremberg, Germany, ²3D-Shape GmbH, Germany Slow and Fast Light, 2009 FWV2, Manipulating Slow Light by Ultrahigh-Q Nanocavities and Their Coupled Arrays, Masaya Notomi, T. Tanabe, E. Kuramochi, H. Taniyama; NTT Basic Res. Labs, Japan Novel Techniques in Microscopy, 2009 FWV3, Wide Field, Minimally Invasive OCT: Recent Advances and Clinical Implications, Ben Vakoc, Brett E. Bouma; Massachusetts General Hospital, USA
Phase Space Optics—Optical System Theory for the 21st Century Symposium organizer: Markus Testorf; Dartmouth College, USA This special symposium is aimed at promoting phase space optics, i.e. optical system theory in terms of the Wigner distribution function and related joint signal transformations. In recent years phase space optics has expanded its scope significantly, and it is recognized as an important complement to standard Fourier optics. Important applications that have benefited from phase space concepts include phase retrieval, computational imaging with extended focal depth, and generalized sampling strategies. The special symposium will feature invited presentations given by experts representing the Watch Markus Testorf, Subcommittee Chair and Symposium Organizer, discuss highlights cutting edge of research in this area. of the symposium.
Tutorial Speaker FWQ1, Wigner Distribution, Partial Coherence, and Phase Space Optics, Martin J. Bastiaans; Dept. of Electrical Engineering, Eidhoven Univ. of Technology, Netherlands Invited Speakers FWQ2, The Connection between Rays and Waves, Miguel A. Alonso; Inst. of Optics, Univ. of Rochester, USA FWQ3, Novel Optical Devices for Extended Field of View, Jorge Ojeda-Castañeda; Univ. of Guanajuato, Mexico FWW1, Wigner Cross-Terms in Sampled and Other Periodic Signals, William T. Rhodes¹, John J. Healy², John T. Sheridan²; ¹Florida Atlantic Univ., USA, ²Univ. College Dublin, Ireland FWW2, The Radon-Wigner Transform and Its Application to First-Order Optical Systems, Genaro Saavedra, Walter D. Furlan; Univ. de València, Spain FWW3, Design of Rotating Beams, Tatiana Alieva¹, Eugeny Abramochkin²; ¹Univ. Complutense de Madrid, Spain, ²PN Lebedev Physical Inst., Samara Branch, Russian Federation Short Courses
Short Courses are designed to increase your knowledge of a specific subject while offering you the experience of experts in industry and academia. Top-quality instructors stay current on the subject matter required to advance your research and career goals. An added benefit of attending a Short Course is the availability of continuing education units (CEUs).
Continuing Education Units (CEUs) Demonstrate your commitment to continuing education and advancement in the optical field by earning continuing education units (CEUs). The CEU is a nationally recognized unit of measure for continuing education and training programs that meet established criteria. Certificates awarding CEUs are presented to all individuals who complete a Short Course, CEU form and course evaluation. Forms will be available on-site and certificates will be mailed to participants.
Registration Each Short Course requires a separate fee. Paid registration includes admission to the course and one copy of the Short Course Notes. Advance registration is advisable. The number of seats in each course is limited, and on-site registration is not guaranteed. Free Offer to Student Members. The FiO sponsoring organizations will offer student members of APS or OSA limited free Short Course registration. Free student member course registration will begin immediately after the pre-registration deadline of September 16, 2009. There will not be free student registration for sold-out courses, and on-site registration is not guaranteed. Register early to guarantee your seat at a Short Course.
Schedule For course descriptions, select the course number.
Sunday, October 11, 2009, 9:00 a.m. - 12:30 p.m. SC235 Nanophotonics: Materials, Fabrication and Characterization, Joseph W. Haus, Andrew Sarangan, Qiwen Zhan; Univ. of Dayton, USA SC324 Plasmonics, Stefan Maier; Experimental Solid State Group, Dept. of Physics, Imperial College London, UK CANCELLED NEW! SC326 Patent Fundamentals, Mohammed N. Islam; Optics and Photonics and Solid State Electronics Lab, Dept. of Electrical Engineering and Computer Science, Univ. of Michigan, USA
Schedule Sunday, October 11, 2009, 1:30 p.m. - 5:00 p.m. SC274 Polarization Engineering, Russell Chipman; Univ. of Arizona, USA CANCELLED SC322 Silicon Nanophotonics, Jelena Vuckovic; Edward L. Ginzton Lab, Stanford Univ., USA CANCELLED NEW! SC340 Tissue Optics and Optical Coherence Tomography, Kirill Larin¹, Valery V. Tuchin²; ¹Univ. of Houston, USA, ²Saratov State Univ., Russian Federation
2009 Exhibitor & Sponsor List Click here for the 2008 Exhibitor List. 2009 Exhibitor List (as of October 5, 2009) ALPAO American Elements American Institute of Physics American Physical Society (APS) Amplitude Laser, Inc. Chroma Technology Corp. Coherent, Inc. Del Mar Photonics Elsevier Fianium Ltd. Femtolasers, Inc. Gooch & Housego Imagine Optic IOP Publishing Ltd. JK Consulting LaserFest Laser Focus World Laser Quantum MPF Products, Inc. Nature Publishing Group Onyx Optics, Inc. OPN OP-TEC Optikos Corporation Optimax Systems, Inc. The Optical Society (OSA) OSA Corporate Membership OSA Foundation OSA - Interactive Science Publishing Photonics Media/Laurin Publishing Physics Today PolarOnyx, Inc. Swamp Optics, LLC Taylor & Francis Thorlabs University of Arizona, College of Optical Sciences University of Central Florida University of Rochester Wiley-Blackwell Zygo Corporation
Special Events
OSA Young Professionals Networking Event with Corporate Members Tuesday, October 13, 8:00 a.m.–9:30 a.m. Courtyard Atrium, Sainte Claire Hotel This invitation-only event puts Young Professionals in contact with highly successful OSA members who will share practical career advice. If you are an OSA member who has graduated within the last 3 years, contact KiKi L’Italien at [email protected] to determine whether space is still available. Young Professionals Bloggers Watch for OSA’s own Young Professional Bloggers who will be reporting on events and their own experiences at FiO! Links to their posts will be shared via the Conference Twitter stream #FiO or posts on the OSA.org homepage.
OSA Division and Technical Group Meetings Network with peers, meet group leaders, and get involved in planning future group activities by attending technical group and/or division meetings during FiO. The division meetings will encompass the technical groups affiliated with the division. Should you have any suggestions for any of the technical group activities, contact the respective technical group chair with your input. Please check back regularly for more information. If you are interested in organizing an activity at FiO for your respective technical group, please contact your group chair or Naomi Chávez at [email protected].
Imaging Sensing and Pattern Recognition Technical Group Meeting Wednesday, October 14, 4:00 p.m.–5:00 p.m., Cupertino Room, Fairmont Hotel Join the OSA Imaging Sensing and Pattern Recognition Technical Group for an informal discussion of results presented at the COSI and SRS topical meetings and at FiO. Light refreshments will be served.
What’s Hot in Optics Today? Sunday, October 11, 2009, 4:00 p.m.–6:00 p.m. Regency Ballroom, Fairmont Hotel What’s hot in optics today? Find out what scientific and technical advances are being made over the entire field of optics. The division Chairs of OSA’s technical groups will be presenting recent advancements in their respective technical areas. The overviews highlight recent developments in optics and are designed to be informative and accessible even to the nontechnical attendee. Please check back regularly for more information.
1st International OSA Student Chapter Solar Car Competition Preliminary races: Sunday, October 11, 4:00 p.m.–7:00 p.m. Final races: Tuesday, October 13, 12:00 p.m.–2:00 p.m. Imperial Ballroom, Fairmont Hotel OSA Student Chapters compete to build their own solar cars and race them. The chapters will work to optimize light capturing efficiency, and demonstrate sustainability and aesthetic appeal. OSA families and guests are welcome to attend! Please note: children 12 and under must be accompanied by an adult and strollers are not permitted.
Welcome Reception Sunday, October 11, 2009, 6:00 p.m.–7:30 p.m. Ballroom, Sainte Claire Hotel Free to all Technical Conference Attendees: Get the FiO 2009/LS XXV meeting off to a great start by attending the welcome reception! Meet with colleagues from around the world and enjoy light hors d’oeuvres.
OSA Spouse, Family and Friends Events Fairmont San Jose Hotel Monday, October 12, 8:30 a.m.–10:00 a.m. Hospitality Suite – stop by to get information on what to see and do in San Jose. Download the flyer. Tuesday, October 13, 9:00 a.m.–5:00 p.m. Bus trip to Monterey – space is limited, so sign up at the OSA Membership Booth by 5:00 PM on Monday, October 12. Download the flyer.
Plenary Session and Awards Presentation Monday, October 12, 2009, 8:00 a.m.–12:00 p.m. Regency Ballroom, Fairmont Hotel The 2009 Joint FiO/LS Awards Ceremony and Plenary Session will feature two world-renowned speakers. See the plenary page for detailed descriptions of the speakers and their presentations.
OSA Fellow Member Lunch Tuesday, October 13, 2009, 12:00 p.m.–1:30 p.m. (Sponsored by the OSA Foundation) Silicon Valley Capital Club 50 W San Fernando, Suite 1700 San Jose, California 95113 Tel.: +1 408.971.9300 In September, invitations will be sent out to Fellow Emeritus and Honorary Members. Please email [email protected] by October 2, 2009 to reserve your place.
Meet the Editors of the APS Journals Tuesday, October 13, 2009, 3:30 p.m.–5:30 p.m. Bamboo Lounge, Fairmont Hotel The Editors of the APS journals cordially invite you to join them for conversation and refreshments. Your questions, criticisms, compliments, and suggestions about the journals are welcome. We hope you will be able to join us.
Minorities and Women in OSA (MWOSA) Tea Tuesday, October 13, 2009, 4:30 p.m.–5:30 p.m. Sainte Claire Room, Sainte Claire Hotel Dr. Linda M. Garverick (leadership consultant, process facilitator, and executive coach) is the featured speaker for this free event. Dr. Garverick’s presentation will be―From Objectivity to Conscious Subjectivity: Understanding Unconscious Bias to Create Fair Evaluation & Promotion Practices.‖ Everyone is welcome to attend; refreshments will be served! There is limited space for this event. Please RSVP to [email protected] by October 2, 2009.
Division of Laser Science Annual Business Meeting Tuesday, October 13, 2009, 6:00 p.m.–7:00 p.m. California Room, Fairmont Hotel All members and interested parties are invited to attend the annual business meeting of the Division of Laser Science (DLS). The DLS officers will report on the activities of the past year and on plans for the future. Questions will be taken from the floor. This is your opportunity to help define the operations of the DLS and the LS Conference.
OSA’s Annual Business Meeting Tuesday, October 13, 2009, 6:00 p.m.–7:00 p.m. Piedmont Room, Fairmont Hotel Learn more about OSA and join the OSA Board of Directors for the Society’s annual business meeting. The 2008 activity reports will be presented and the results of the Board of Directors election will be announced. To view the slate of candidates, go to http://www.osa.org/aboutosa/leadership/electionprocess/default.aspx. Agenda I. Welcome 2009 OSA President, Thomas Baer II. 2008 Activity Reports from Society Representatives Chair, Meetings Council: Edward Watson Chair, Board of Meetings: David Fittinghoff Chair, Member and Education Services Council: Irene Georgakoudi Chair, Corporate Associates Committee: Paul Crosby Chair, Public Policy Committee: Alex Fong Chair, International Council: Satoshi Kawata Chair, Board of Editors: Tony Heinz Chair, Publications Council: Govind Agrawal Chair, OSA Foundation: G. Michael Morris
Treasurer: Stephen Fantone III. 2009 Election Results 2009 OSA President, Thomas Baer 2010 Vice President and Directors at Large
OSA Member Reception Tuesday, October 13, 2009, 7:00 p.m.–8:30 p.m. Ballroom, Sainte Claire Hotel (Free Event for all OSA Members) Join OSA President Tom Baer for a special reception in honor of OSA members. This free event is an OSA Annual Meeting tradition and is a great opportunity to meet friends and have a relaxing good time. Beverages and delicious appetizers will be served. Please bring your conference registration badge or OSA member ID number.
Laser Science Banquet Tuesday, October 13, 2009, 7:00 p.m.–10:00 p.m. Gordon Biersch 33 East San Fernando Street San Jose, California 95113 Tel.: +1 408.294.6785 Join your colleagues for the annual LS Banquet. Tickets are required for this event and can be purchased during registration for US $50. There is a limited quantity of tickets and tickets must be purchased by 12:00 p.m. on Monday, October 12.
Export Regulation Fundamentals for the Optics and Photonics Industry Wednesday, October 14, 2009, 9:00 a.m.–12:00 p.m. Sainte Claire Room, Sainte Claire Hotel (Presented by the OSA Corporate Associates) With the global nature of business, it is a necessity for every company employee involved in non-U.S. transactions to fully understand the regulations surrounding export controls. This course will provide the foundation by covering need-to-know information about International Traffic in Arms Regulations (ITAR), Export Administration Regulations (EAR) and your compliance, data management, and licensing responsibilities. Registration required. Employees of OSA Corporate Associates receive a special registration rate.
Joint FiO/LS Poster Session Wednesday, October 14, 2009, 12:00 p.m.–1:30 p.m. Imperial Ballroom, Fairmont Hotel Poster presentations offer an effective way to communicate new research findings and provide an opportunity for lively and detailed discussion between presenters and interested viewers. Please stop by the Regency Ballroom to enjoy the poster session.
FiO Postdeadline Papers Wednesday, October 14, 2009, 6:30 p.m.–8:00 p.m. Empire, Crystal, and Gold Rooms, Fairmont Hotel The FiO 2009 Technical Program Committee accepted a limited number of postdeadline papers for presentation. The purpose of postdeadline sessions is to give participants the opportunity to hear new and significant material in rapidly advancing areas. Only those papers judged to be truly excellent and compelling in their timeliness were accepted. More information, including the schedule and locations, will be posted in the weeks preceding the conference. View Postdeadline Abstracts
2009 OSA Science Educators Day Thursday, October 15, 2009, 5:30 p.m.–8:00 p.m. McCaw Hall, Frances C. Arrillaga Alumni Center, Stanford Univ. 326 Galvez St Stanford, California 94305 Tel.: +1 650.723.2021 Sponsored by The Optical Society and the Stanford Student Chapter, Science Educators’ Day (EDAY) provides middle and high school science teachers with a wide variety of optics-focused lesson plans and classroom demonstration guides. EDAY attendees receive materials that can be used in middle and high school classrooms. The event includes: Approximately 20 stations with educators demonstrating and discussing hands-on materials for teaching optics to secondary school students Gift bags containing demonstration aids and lesson plans for the first 100 registrants Additional optics materials available as door prizes A buffet dinner allowing you to mingle with fellow teachers and conference attendees Questions? Email [email protected]. Space will be limited! Register by Friday, October 2, 2009!
Agenda of Sessions 33 October 11–15, 2009 Fall OSA Optics & Photonics Congress & Photonics OSA Optics Fall • (on your own) Lunch your (on Break Market Street Foyer, Fairmont Hotel Fairmont Foyer, Street Market Registration, registration at provided will be Short Courses, Locations registration at provided will be Locations Short Courses, Ballroom, Sainte Claire Hotel Claire Sainte Ballroom, Reception, FiO/LS Welcome Regency Ballroom, Fairmont Hotel Fairmont Ballroom, Regency Today? What's Hot in Optics Joint Dept. of Electrical Engineering and Computer Science, Univ. of Michigan, USA Michigan, of Univ. Science, Computer and Engineering Electrical of Dept. USA Arizona, of Univ. Chipman; Engineering, Russell SC274: Polarization Plaza Ballroom, Crowne Plaza Hotel Plaza Crowne Chapter LeadershipOSA Student Ballroom, Plaza Meeting, Jelena Vučković; Edward L. Ginzton Lab, Stanford Univ., USA Univ., Stanford Lab, Ginzton L. Edward Vučković; Jelena SC322: Silicon Nanophotonics, Mohammed N. Islam; Optics and Photonics and Solid State Electronics Lab, Lab, Electronics State Solid and Photonics and Optics N. Islam; Mohammed Fundamentals, SC326: Patent FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Mini-Car Preliminary International OSA Student Chapter Solar Races, Imperial Stefan Maier; Experimental Solid State Group, Dept. of Physics, Imperial College London, UK London, College Imperial Physics, of Dept. Group, State Solid Experimental Maier; Stefan SC324: Plasmonics, st 1 Sunday, October 11 October Sunday, — Laser Science Joseph W. Haus, Andrew Sarangan, Qiwen Zhan; Univ. of Dayton, USA Dayton, of Univ. Zhan; Qiwen Sarangan, Andrew Haus, W. Joseph and Characterization, Fabrication Materials, SC235: Nanophotonics: Kirill Larin¹, Valery V. Tuchin²; ¹Univ. of Houston, USA, ²Saratov State Univ., Russian Federation Russian Univ., State USA, ²Saratov Houston, of ¹Univ. Tuchin²; V. Valery Larin¹, Kirill SC340: Tissue Optics and Optical Coherence Tomography,
in Optics Frontiers
6:00 p.m.–7:30 p.m. 6:00 p.m.–7:30 4:00 p.m.–6:00 p.m. 4:00 p.m.–6:00 p.m. 4:00 p.m.–7:00 1:30 p.m.–5:00 p.m. 1:30 p.m.–5:00 12:30 p.m.–1:30 p.m. 12:30 p.m.–1:30 7:00 a.m.–6:00 p.m. 7:00 a.m.–6:00 p.m. 9:00 a.m.–12:30 7:00 a.m.–3:00 p.m. 7:00 a.m.–3:00
Key to Shading Key Agenda of Sessions of Agenda Agenda of Sessions 34 Key toShading Agenda ofSessions 10:00 a.m.–10:30a.m. 8:00 a.m.–12:00p.m. 6:30 p.m.–8:30 p.m. 3:30 p.m.–4:00 p.m. 7:00 a.m.–6:00p.m. 4:00 p.m.–6:00 p.m. 1:30 p.m.–3:30 p.m. 12:00 p.m.–2:00 p.m. 12:00 p.m.–1:30 p.m. Frontiers inOptics in Waveguides I FMG: QuantumOptics (Joint FiO/LS) Measurement I Generation and Entanglement JMA: Empire Science Laser OSA StudentMemberReception, O’Flaherty’s Irish Pub, 25N.Pedro Street, San Jose, California 95110,Phone: 408.947.8007 —Monday, October12 LSMA: Laser ScienceSymposiumonUndergraduateResearch Posters, Cupertino Laser LSMA: Room, Fairmont Hotel FiO/LS/AO/AIOM/COSI/LM/SRS 2009 (ends at 5:45p.m.) FMH: MetamaterialsII MetamaterialsI FMA: 2009 Joint FiO/LS Awards Ceremony and Plenary Session,Regency Ballroom,2009 JointFiO/LSAwardsCeremonyandPlenary Fairmont Hotel Crystal Coffee Break,Regency and Imperial Ballroom Foyer, Fairmont Hotel Coffee Break,Regency and Imperial Ballroom Foyer, Fairmont Hotel Joint Registration, Market Street Foyer, Fairmont Hotel (Joint FiO/LS) I Interferometers JMB: GravitationalWave Renewable Energy FMB: Opticsfor Lunch Break(on yourLunch own) • Fall OSAOptics &Photonics Congress Gold October 11–15,2009 (ends at 5:45p.m.) Technology I FMI: HighPeak Power Laser I FMC: AndersonLocalization Valley Sensors FMJ: IntegratedOptical FMD: RFPhotonics California FMK: MicroscopyandOCTI and Spectroscopy Imaging FME: Tissue Glen Ellen FML: SiliconPhotonicsI Solitons andBeams FMF: SpatialNonlinearities: OSA StudentMemberReception, O’Flaherty’s Irish Pub, 25N.Pedro Street, San Jose, California 95110,Phone: 408.947.8007 Atherton LSMA: Laser ScienceSymposiumonUndergraduateResearch Posters, Cupertino Laser LSMA: Room, Fairmont Hotel 2009 Joint FiO/LS Awards Ceremony and Plenary Session,Regency Ballroom,2009 JointFiO/LSAwardsCeremonyandPlenary Fairmont Hotel Coffee Break,Regency and Imperial Ballroom Foyer, Fairmont Hotel Coffee Break,Regency and Imperial Ballroom Foyer, Fairmont Hotel (ends at 5:30p.m.) Chiroptical SpectroscopyII LSMF: Advancesin Chiroptical SpectroscopyI LSMB: Advancesin Sacramento Registration, Market Street Foyer, Fairmont Hotel Lunch Break(on yourLunch own) (ends at 6:15p.m.) Nanofluidics II LSMG: Micro-and (ends at 3:15p.m.) Nanofluidics I LSMC: Micro-and Piedmont (ends at 5:45p.m.) Science II LSMH: UltrafastX-Ray Science I LSMD: UltrafastX-Ray Hillsborough (4:30 p.m.–6:30 p.m.) Undergraduate Research II Symposium on Science LSMI: Laser (2:00 p.m.–4:00 p.m.) Undergraduate Research I Symposium on Science LSME: Laser Fairfield Agenda of Sessions 35 Fairfield LSME: Laser Science Symposium on I Undergraduate Research p.m.) (2:00 p.m.–4:00 LSMI: Laser Science Symposium on II Undergraduate Research p.m.) (4:30 p.m.–6:30 Hillsborough LSMD: Ultrafast X-Ray LSMD: Ultrafast X-Ray Science I LSMH: Ultrafast X-Ray Science II 5:45 p.m.) at (ends October 11–15, 2009 Piedmont • LSMC: Micro- and Nanofluidics I 3:15 p.m.) at (ends LSMG: Micro- and Nanofluidics II 6:15 p.m.) at (ends (on your own) Lunch your (on Break Market Street Foyer, Fairmont Hotel Fairmont Foyer, Street Market Registration, Sacramento LSMB: Advances in I Chiroptical Spectroscopy Advances in LSMF: Chiroptical Spectroscopy II 5:30 p.m.) at (ends Regency and Imperial Ballroom Foyer, Fairmont Hotel Fairmont Foyer, Ballroom Imperial and Coffee Break, Regency Regency and Imperial Ballroom Foyer, Fairmont Hotel Fairmont Foyer, Ballroom Imperial and Coffee Break, Regency FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Regency Ballroom, Fairmont Hotel Fairmont and Plenary FiO/LS Awards Ceremony 2009 Joint Ballroom, Session, Regency Cupertino Room, Fairmont Hotel Fairmont Room, LSMA: Laser Cupertino Posters, Research Science Symposium on Undergraduate Atherton O’Flaherty’s Irish Pub, 25 N. Pedro Street, San Jose, California 95110, Phone: 408.947.8007 95110, Phone: California Jose, San Street, 25 N. Pedro Pub, Irish O’Flaherty’s OSA Student Member Reception, FMF: Spatial Nonlinearities: Spatial Nonlinearities: FMF: Solitons and Beams I FML: Silicon Photonics Glen Ellen FME: Tissue Imaging and Spectroscopy OCT I FMK: Microscopy and California FMD: RF Photonics FMJ: Integrated Optical Sensors Valley FMC: Anderson Localization I Laser Power FMI: High Peak I Technology 5:45 p.m.) at (ends Gold (on your own) Lunch your (on Break FMB: Optics for Energy Renewable JMB: Gravitational Wave Interferometers I (Joint FiO/LS) Market Street Foyer, Fairmont Hotel Fairmont Foyer, Street Market Registration, Regency and Imperial Ballroom Foyer, Fairmont Hotel Fairmont Foyer, Ballroom Imperial and Coffee Break, Regency Regency and Imperial Ballroom Foyer, Fairmont Hotel Fairmont Foyer, Ballroom Imperial and Coffee Break, Regency Crystal Regency Ballroom, Fairmont Hotel Fairmont and Plenary FiO/LS Awards Ceremony 2009 Joint Ballroom, Session, Regency FMA: I Metamaterials FMH: Metamaterials II 5:45 p.m.) at (ends Cupertino Room, Fairmont Hotel Fairmont Room, LSMA: Laser Cupertino Posters, Research Science Symposium on Undergraduate O’Flaherty’s Irish Pub, 25 N. Pedro Street, San Jose, California 95110, Phone: 408.947.8007 95110, Phone: California Jose, San Street, 25 N. Pedro Pub, Irish O’Flaherty’s OSA Student Member Reception, Empire JMA: Entanglement Generation and Measurement I (Joint FiO/LS) FMG: Quantum Optics I in Waveguides 6:30 p.m.–8:30 p.m. 6:30 p.m.–8:30 7:00 a.m.–6:00 p.m. 7:00 a.m.–6:00 p.m. 8:00 a.m.–12:00 10:00 a.m.–10:30 a.m. p.m. 12:00 p.m.–1:30 p.m. 12:00 p.m.–2:00 p.m. 1:30 p.m.–3:30 p.m. 3:30 p.m.–4:00 p.m. 4:00 p.m.–6:00 Agenda of Sessions 36 Key toShading Agenda ofSessions 4:00 p.m.–5:30 p.m. 3:30 p.m.–5:30 p.m. 12:00 p.m.–1:30 p.m. 7:00 p.m.–10:00 p.m. 7:00 p.m.–8:30 p.m. 6:00 p.m.–7:30 p.m. 6:00 p.m.–7:00 p.m. 6:00 p.m.–7:00 p.m. 4:30 p.m.–5:30 p.m. 3:30 p.m.–4:00 p.m. 1:30 p.m.–3:30 p.m. 12:00 p.m.–1:30 p.m. 12:00 p.m.–2:00 p.m. 10:00 a.m.–10:30a.m. 9:00 a.m.–12:00p.m. 12:00 p.m.–1:30 p.m. 10:30 a.m.–12:00p.m. 10:00 a.m.–4:00p.m. 8:00 a.m.–9:30a.m. 8:00 a.m.–10:00a.m. 7:00 a.m.–5:30p.m. Frontiers in Optics Frontiers II and Research Display Technologies FTuT: Emerging3-D (ends at 3:00p.m.) Frontiers I and Research Display Technologies Emerging3-D FTuM: Displays Visualization and FTuF: 3-DCapturing, (ends at 9:30a.m.) Marketplace Entertainment inthe 3-D FTuA: Empire Science Laser OSA Fellow Silicon MemberLunch, Valley Capital Club, 50W. San Fernando, Suite 1700,San Jose, California 95113,Phone: 408.971.9300 Student Programming:Painless Publishing,SciencePolicy andOSATravelingLecturer, Regency Ballroom II,Fairmont Hotel —Tuesday, October13 Sensing II Transport and Design forInformation WavefrontFTuU: Materials andCloaking NegativeIndexFTuN: (ends at 11:45a.m.) Transport andSensingI Design forInformation WavefrontFTuG: Resonators Emitters and Plasmonic FTuB: OSA Young ProfessionalsNetworkingEventwithCorporateMembers,Courtyard Atrium, Sainte Claire Hotel JTuC: JointAO/COSI/LM/SRS Welcome Reception andPoster Session,Regency Ballroom, Fairmont Hotel Laser ScienceBanquet, Gordon Biersch,Laser 33 East San Fernando Street, San Jose, California, Phone: 408.294.6785 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 1 st InternationalOSAStudentChapterSolarMini-CarFinalRaces,Imperial Ballroom, Fairmont Hotel Crystal Minorities andWomen inOSA(MWOSA)Tea, Sainte Claire Room, Sainte Claire Hotel Meet theEditorsofAPSJournals,Bamboo Lounge, Fairmont Hotel DLS AnnualBusinessMeeting, California Room, Fairmont Hotel OSA AnnualBusinessMeeting,Piedmont Room, Fairmont Hotel Joint Coffee Break/Exhibits,Imperial Ballroom, Fairmont Hotel Emerging Technologies FTuV: Metamaterialsin Holographic OpticsII Diffractiveand FTuO: Holographic OpticsI Diffractiveand FTuH: (ends at 10:15a.m.) (Joint FiO/LS) Wave II Interferometers JTuA: Gravitational OSA MemberReception, Ballroom, Sainte Claire Hotel Exhibit Only Time, ImperialExhibit OnlyTime, Ballroom, Fairmont Hotel Exhibit HallOpen,Imperial Ballroom, Fairmont Hotel Coffee Break,Imperial Ballroom, Fairmont Hotel Registration, Market Street Foyer, Fairmont Hotel Gold Lunch Break(on yourLunch own) • Fall OSAOptics &Photonics Congress October 11–15,2009 Signal ProcessingII FTuW: All-Optical FTuP: OpticalAccess FTuP: Signal ProcessingI All-Optical FTuI: (ends at 10:15a.m.) Communication Optical FTuC: Valley Periodic Structures NovelOpticsof FTuX: FTuQ: LightintheEye FTuQ: Localization II Localization Anderson FTuJ: Devices I NovelFiber FTuD: California (ends at 5:45p.m.) Biosensing FTuY: Optical Related Phenomena RogueFTuR: Waves and Laser TechnologyLaser II HighPeakFTuK: Power (Joint FiO/LS) Measurement II Generation and JTuB: Entanglement Glen Ellen and Microscopy Spectroscopy Applications II: Generation and Wavelength Short FTuZ: (ends at 3:15p.m.) EUV toX-Rays Applications I:From Generation and Wavelength Short FTuS: Nanomedicine Imaging and Molecular FTuL: Optics Sensors Fiber FTuE: Atherton Nanostructures II Dots and of Quantum LSTuJ: Photophysics (ends at 3:45p.m.) Characterization Materials Optoelectronic LSTuG: Nanostructures I Quantum Dotsand Photophysics of LSTuD: Science Laser LSTuA: General Sacramento OSA Fellow Silicon MemberLunch, Valley Capital Club, 50W. San Fernando, Suite 1700,San Jose, California 95113,Phone: 408.971.9300 Student Programming:Painless Publishing,SciencePolicy andOSATravelingLecturer, Regency Ballroom II,Fairmont Hotel OSA Young ProfessionalsNetworkingEventwithCorporateMembers,Courtyard Atrium, Sainte Claire Hotel JTuC: JointAO/COSI/LM/SRS Welcome Reception andPoster Session,Regency Ballroom, Fairmont Hotel Laser ScienceBanquet, Gordon Biersch,Laser 33 East San Fernando Street, San Jose, California, Phone: 408.294.6785 1 st InternationalOSAStudentChapterSolarMini-CarFinalRaces,Imperial Ballroom, Fairmont Hotel (ends at 5:15p.m.) Optomechanics IV LSTuK: Cavity Optomechanics III LSTuH: Cavity Optomechanics II LSTuE: Cavity Optomechanics I LSTuB: Cavity Piedmont Minorities andWomen inOSA(MWOSA)Tea, Sainte Claire Room, Sainte Claire Hotel Meet theEditorsofAPSJournals,Bamboo Lounge, Fairmont Hotel DLS AnnualBusinessMeeting, California Room, Fairmont Hotel OSA AnnualBusinessMeeting,Piedmont Room, Fairmont Hotel Coffee Break/Exhibits,Imperial Ballroom, Fairmont Hotel OSA MemberReception, Ballroom, Sainte Claire Hotel Exhibit Only Time, ImperialExhibit OnlyTime, Ballroom, Fairmont Hotel Exhibit HallOpen,Imperial Ballroom, Fairmont Hotel Coffee Break,Imperial Ballroom, Fairmont Hotel Registration, Market Street Foyer, Fairmont Hotel (ends at 5:45p.m.) Dynamics II LSTuL: HighField Dynamics I LSTuI: HighField Nanofluidics III LSTuF: Micro-and X-Ray ScienceIII LSTuC: Ultrafast Hillsborough Lunch Break(on yourLunch own) Calibration I Spread Function Imaging andPoint AOTuC: HighContrast (ends at 3:10p.m.) (ends at 5:20p.m.) Modeling I Simulation and AOTuD: System Sensing I AOTuB: Wavefront (ends at 9:50a.m.) Optics SystemsI AOTuA: Adaptive Fairfield
Laser Systems Laser with Femtosecond of Waveguides LMTuC: Fabrication (ends at 6:00p.m.) Micromachining Femtosecond Laser Panel Discussionon Processing and LMTuD: Surface Femtosecond Lasers Micromachining with Dimensional LMTuB: Three- with Materials Interactions Laser of Femtosecond Fundamentals LMTuA: Belvedere on Imaging CTuC: Constraints (ends at 5:45p.m.) and PSFDesign CTuD: 3-DImaging Representations CTuB: LightField Sensing Compressive Imaging and CTuA: Computational Club Regent Imaging STuC: Atmospheric (ends at 5:15p.m.) Methods Phase-Space Frequency and STuD: Time- Scattering STuB: Inverse Compressed Data from Limitedand STuA: Imaging Cupertino Agenda of Sessions 37 SRS Cupertino STuD: Time- STuD: and Frequency Phase-Space Methods 5:15 p.m.) at (ends STuA: Imaging STuA: and from Limited Data Compressed Inverse STuB: Scattering STuC: Atmospheric Atmospheric STuC: Imaging COSI Club Regent CTuD: 3-D Imaging CTuD: and PSF Design 5:45 p.m.) at (ends CTuA: Computational Computational CTuA: Imaging and Compressive Sensing Light Field CTuB: Representations CTuC: Constraints CTuC: on Imaging LM Belvedere LMTuD: Surface LMTuD: Processing and Discussion on Panel LaserFemtosecond Micromachining 6:00 p.m.) at (ends LMTuA: LMTuA: Fundamentals of Femtosecond LaserInteractions with Materials Three- LMTuB: Dimensional Micromachining with Lasers Femtosecond LMTuC: Fabrication Fabrication LMTuC: of Waveguides with Femtosecond Laser Systems Fall OSA Optics & Photonics Congress & Photonics OSA Optics Fall
October 11–15, 2009 AO • Fairfield AOTuD: System AOTuD: Simulation and Modeling I 5:20 p.m.) at (ends AOTuA: Adaptive AOTuA: I Optics Systems 9:50 a.m.) at (ends Wavefront AOTuB: Sensing I (ends at 3:10 p.m.) at (ends AOTuC: High Contrast AOTuC: Imaging and Point Spread Function Calibration I
(on your own) Lunch your Break (on Hillsborough LSTuI: High Field LSTuI: Dynamics I High Field LSTuL: Dynamics II 5:45 p.m.) at (ends LSTuC: Ultrafast Ultrafast LSTuC: Science III X-Ray Micro- and LSTuF: Nanofluidics III Market Street Foyer, Fairmont Hotel Fairmont Foyer, Street Market Registration, Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Coffee Break, Imperial Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Exhibit Hall Open, Imperial Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Exhibit Only Time, Imperial Ballroom, Sainte Claire Hotel Claire Sainte Ballroom, OSA Member Reception, Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Coffee Break/Exhibits, Imperial Piedmont Room, Fairmont Hotel Fairmont Room, OSA Annual Business Meeting, Piedmont California Room, Fairmont Hotel Fairmont Room, DLS Annual Business Meeting, California Bamboo Lounge, Fairmont Hotel Fairmont Lounge, Meet the Editors of the APS Journals, Bamboo FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Sainte Claire Room, Sainte Claire Hotel Claire Sainte Room, Claire Sainte in OSA (MWOSA) Tea, Minorities and Women Piedmont LSTuK: Cavity LSTuK: Optomechanics IV 5:15 p.m.) at (ends LSTuH: Cavity LSTuH: Optomechanics III LSTuB: Cavity Cavity LSTuB: I Optomechanics Cavity LSTuE: Optomechanics II Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Mini-Car Final Races, Imperial International OSA Student Chapter Solar st 1 Gordon Biersch, 33 East San Fernando Street, San Jose, California, Phone: 408.294.6785 Phone: California, Jose, San Street, Fernando San 33 East Laser Biersch, Science Banquet, Gordon Regency Ballroom, Fairmont Hotel Fairmont Ballroom, Session, Regency and Poster Reception Joint AO/COSI/LM/SRS Welcome JTuC: Courtyard Atrium, Sainte Claire Hotel Claire Sainte Atrium, Corporate Members, Courtyard Professionals Networking Event with OSA Young Regency Ballroom II, Fairmont Hotel II, Fairmont Ballroom Regency and OSA Traveling Lecturer, Science Policy Publishing, Painless Student Programming: Silicon Valley Capital Club, 50 W. San Fernando, Suite 1700, San Jose, California 95113, Phone: 408.971.9300 95113, Phone: California Jose, 1700, San Suite Fernando, San 50 W. Club, Capital Valley Member Lunch, Silicon OSA Fellow Sacramento LSTuG: LSTuG: Optoelectronic Materials Characterization 3:45 p.m.) at (ends Photophysics LSTuJ: of Quantum Dots and Nanostructures II LSTuA: General LSTuA: LaserScience LSTuD: Photophysics of Quantum Dots and Nanostructures I Atherton FTuS: Short Wavelength Generation and Applications I: From EUV to X-Rays 3:15 p.m.) at (ends FTuZ: Short Wavelength Generation and Applications II: Spectroscopy and Microscopy FTuE:Fiber Optics Sensors FTuL: Molecular Imaging and Nanomedicine Glen Ellen FTuR: Rogue Waves and Waves FTuR: Rogue Phenomena Related Optical FTuY: Biosensing 5:45 p.m.) at (ends JTuB: Entanglement Entanglement JTuB: and Generation II Measurement (Joint FiO/LS) Power FTuK: High Peak II Laser Technology California FTuQ: Eye Light in the FTuX: of Novel Optics Structures Periodic FTuD:Novel Fiber Devices I FTuJ: Anderson Localization II Valley FTuP: Optical Access All-Optical FTuW: Signal Processing II FTuC:Optical Communication 10:15 a.m.) at (ends FTuI: All-Optical Signal Processing I (on your own) Lunch your Break (on Gold Market Street Foyer, Fairmont Hotel Fairmont Foyer, Street Market Registration, Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Coffee Break, Imperial Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Exhibit Hall Open, Imperial Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Exhibit Only Time, Imperial Ballroom, Sainte Claire Hotel Claire Sainte Ballroom, OSA Member Reception, FTuO: and Diffractive Holographic Optics II Metamaterials in FTuV: Emerging Technologies JTuA: Gravitational JTuA: Interferometers II Wave (Joint FiO/LS) 10:15 a.m.) at (ends FTuH: Diffractive and Holographic Optics I Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Coffee Break/Exhibits, Imperial Piedmont Room, Fairmont Hotel Fairmont Room, OSA Annual Business Meeting, Piedmont California Room, Fairmont Hotel Fairmont Room, DLS Annual Business Meeting, California Bamboo Lounge, Fairmont Hotel Fairmont Lounge, Meet the Editors of the APS Journals, Bamboo Sainte Claire Room, Sainte Claire Hotel Claire Sainte Room, Claire Sainte in OSA (MWOSA) Tea, Minorities and Women Crystal Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Mini-Car Final Races, Imperial International OSA Student Chapter Solar st 1 Gordon Biersch, 33 East San Fernando Street, San Jose, California, Phone: 408.294.6785 Phone: California, Jose, San Street, Fernando San 33 East Laser Biersch, Science Banquet, Gordon Regency Ballroom, Fairmont Hotel Fairmont Ballroom, Session, Regency and Poster Reception Joint AO/COSI/LM/SRS Welcome JTuC: Courtyard Atrium, Sainte Claire Hotel Claire Sainte Atrium, Corporate Members, Courtyard Professionals Networking Event with OSA Young FTuN: Negative Index FTuN: Negative Index Materials and Cloaking FTuU: Wavefront Design for Information Transport and Sensing II FTuB:Plasmonic Emitters and Resonators FTuG: Wavefront Design for Information I Transport and Sensing 11:45 a.m.) at (ends Regency Ballroom II, Fairmont Hotel II, Fairmont Ballroom Regency and OSA Traveling Lecturer, Science Policy Publishing, Painless Student Programming: Silicon Valley Capital Club, 50 W. San Fernando, Suite 1700, San Jose, California 95113, Phone: 408.971.9300 95113, Phone: California Jose, 1700, San Suite Fernando, San 50 W. Club, Capital Valley Member Lunch, Silicon OSA Fellow Empire FTuM:3-D Emerging Display Technologies and Research I Frontiers 3:00 p.m.) at (ends Emerging 3-D FTuT: Display Technologies and Research II Frontiers FTuA: 3-D in the Entertainment Marketplace 9:30 a.m.) at (ends 3-D Capturing, FTuF: and Visualization Displays 1:30 p.m.–3:30 p.m. 1:30 p.m.–3:30 p.m. 3:30 p.m.–4:00 p.m. 3:30 p.m.–5:30 p.m. 4:00 p.m.–5:30 p.m. 4:30 p.m.–5:30 p.m. 6:00 p.m.–7:00 p.m. 6:00 p.m.–7:00 p.m. 6:00 p.m.–7:30 p.m. 7:00 p.m.–8:30 p.m. 7:00 p.m.–10:00 7:00 a.m.–5:30 p.m. 7:00 a.m.–5:30 a.m. 8:00 a.m.–10:00 8:00 a.m.–9:30 a.m. 9:00 a.m.–12:00 p.m. 10:00 a.m.–10:30 a.m. 10:00 a.m.–4:00 p.m. 10:30 a.m.–12:00 p.m. p.m. 12:00 p.m.–1:30 p.m. 12:00 p.m.–2:00 p.m. 12:00 p.m.–1:30 p.m. 12:00 p.m.–1:30 Agenda of Sessions 38 Key toShading Agenda ofSessions 6:30 p.m.–8:00 p.m. 4:00 p.m.–5:30 p.m. 6:30 p.m.–8:00 p.m. 3:30 p.m.–4:00 p.m. 1:30 p.m.–3:30 p.m. 12:00 p.m.–1:30 p.m. 12:00 p.m.–1:30 p.m. 10:30 a.m.–12:00p.m. 10:00 a.m.–4:00p.m. 10:00 a.m.–10:30a.m. 9:00 a.m.–12:00p.m. 8:00 a.m.–10:00a.m. 7:30 a.m.–5:30p.m. Frontiers inOptics Fundamental OpticsII FWU: Coherenceand (Joint FiO/LS) Measurement III Generation and JWD: Entanglement (ends at 12:15p.m.) Fundamental OpticsI FWH: Coherenceand Ultrafast Lasers Applications of FWA: Biomedical Empire Science Laser FiO Postdeadline Paper Sessions,Seethe Postdeadline Papers Book in your registration bag for times exact and locations Export Regulation Fundamentals fortheOpticsandPhotonics Industry, Sainte Claire Room, Sainte Claire Hotel —Wednesday, October14 Meeting HighlightsII FWV: OSA Topical Meeting HighlightsI FWO: OSATopical Information Sciences FWI: Opticsin and Metamaterials Age ofNanophotonics and Transportinthe Information Processing FWB: Optical FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Crystal JWC: JointFiO/LSPoster Session,Imperial Ballroom, Fairmont Hotel Joint AIOM Welcome Reception, Regency Ballroom I,Fairmont Hotel Coffee Break/Exhibits,Imperial Ballroom, Fairmont Hotel (ends at 6:00p.m.) (Joint FiO/LS) Measurement IV Generation and JWE: Entanglement FWP: MetamaterialsIII (ends at 12:15p.m.) Waveguides II FWJ: QuantumOpticsin Structured Surface Transmission and FWC: Extraordinary Exhibit HallOpen,Imperial Ballroom, Fairmont Hotel Coffee Break,Imperial Ballroom, Fairmont Hotel Registration, Market Street Foyer, Fairmont Hotel Gold Lunch Break(on yourLunch own) • Fall OSA Optics &Photonics Congress October 11–15,2009 (ends at 3:15p.m.) I Century the 21 for System Theory Optics—Optical FWW: PhaseSpace Theory forthe Theory Optics—Optical System FWQ: PhaseSpace Signal ProcessingIII FWK: All-Optical Phenomena and OtherNonlinear FWD: Turbulence st Century II Century Valley 21st
Technologies II in Emerging Architectures FWX: NovelOptical Technologies I in Emerging Architectures FWR: NovelOptical Communication Devices FWL: Optical (ends at 9:45a.m.) Devices II FWE: NovelFiber California Micromanipulation III Trapping and FWY: Optical Micromanipulation II Trapping and FWS: Optical (ends at 11:45a.m.) Micromanipulation I Trapping and FWM: Optical (ends at 9:45a.m.) Devices FWF: PhotonicBandgap Glen Ellen Photonics III FWZ: Silicon (ends at 3:15p.m.) Sensors FWT: Plasmonic Photonics II FWN: Silicon Sensing Devices FWG: Photonic Atherton (ends at 6:15p.m.) Spectroscopy II LSWJ: Ultrafast Spectroscopy I LSWG: Ultrafast Biophysics II Molecule LSWD: Single- Biophysics I Molecule LSWA: Single- Sacramento FiO Postdeadline Paper Sessions,Seethe Postdeadline Papers Book in your registration bag for times exact and locations Export Regulation Fundamentals fortheOpticsandPhotonics Industry, Sainte Claire Room, Sainte Claire Hotel (ends at 5:45p.m.) Optics IV Order Nonlinear LSWK: Second- (ends at 3:15p.m.) Optics III Order Nonlinear LSWH: Second- Nonlinear OpticsII LSWE: Second-Order Nonlinear OpticsI LSWB: Second-Order Piedmont JWC: JointFiO/LSPoster Session,Imperial Ballroom, Fairmont Hotel AIOM Welcome Reception, Regency Ballroom I,Fairmont Hotel Coffee Break/Exhibits,Imperial Ballroom, Fairmont Hotel Exhibit HallOpen,Imperial Ballroom, Fairmont Hotel Coffee Break,Imperial Ballroom, Fairmont Hotel Registration, Market Street Foyer, Fairmont Hotel (ends at 3:00p.m.) Spectroscopy III Multidimensional LSWI: Spectroscopy II Multidimensional LSWF: Spectroscopy I Multidimensional LSWC: Hillsborough Lunch Break(on yourLunch own) (Joint AO/FiO) Living Retina II Imaging ofthe Adaptive Optics JWF: Advancesin Architecture Algorithms and AOWB: Control (ends at 11:50a.m.) Calibration II Spread Function and Point Contrast Imaging AOWA: High Fairfield Ceramics AWD: Optical (ends at 9:45a.m.) Materials AWA: Semiconductor (ends at 3:15p.m.) AWC: OxideCrystals (ends at 11:45a.m.) Interactions AWB: Laser-Material Belvedere Session AO/COSI/SRS JWA: Joint (ends at 3:15p.m.) Systems CWB: MultiAperture Imaging Sensing and CWA: Polarization Club Regent (ends at 3:15p.m.) Retrieval Methods SWA: Phase (Joint AO/FiO) Living Retina I Imaging ofthe Adaptive Optics JWB: Advancesin Cupertino Agenda of Sessions 39 SRS Cupertino JWB: Advances in Adaptive Optics Imaging of the I Living Retina (Joint AO/FiO) SWA: Phase SWA: Methods Retrieval 3:15 p.m.) at (ends COSI Club Regent CWA: Polarization Polarization CWA: Sensing and Imaging CWB: Multi Aperture Systems 3:15 p.m.) at (ends JWA: Joint JWA: AO/COSI/SRS Session AIOM Belvedere AWB: Laser-MaterialAWB: Interactions 11:45 a.m.) at (ends AWC: Oxide Crystals AWC: 3:15 p.m.) at (ends AWA: Semiconductor AWA: Materials 9:45 a.m.) at (ends AWD: Optical AWD: Ceramics Fall OSA Optics & Photonics Congress & Photonics OSA Optics Fall October 11–15, 2009 AO • Fairfield AOWA: High High AOWA: Contrast Imaging and Point Spread Function Calibration II 11:50 a.m.) at (ends AOWB: Control Algorithms and Architecture JWF: Advances in JWF: Adaptive Optics Imaging of the II Living Retina (Joint AO/FiO)
(on your own) Lunch your Break (on Hillsborough LSWC: Multidimensional I Spectroscopy LSWF: Multidimensional Spectroscopy II LSWI: Multidimensional Spectroscopy III 3:00 p.m.) at (ends Market Street Foyer, Fairmont Hotel Fairmont Foyer, Street Market Registration, Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Coffee Break, Imperial Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Exhibit Hall Open, Imperial Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Coffee Break/Exhibits, Imperial Regency Ballroom I, Fairmont Hotel I, Fairmont Ballroom Regency Reception, AIOM Welcome Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Session, Imperial JWC: Joint FiO/LS Poster FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Piedmont LSWB: Second-Order Second-Order LSWB: I Nonlinear Optics Second-Order LSWE: Nonlinear Optics II LSWH: Second- Order Nonlinear Optics III 3:15 p.m.) at (ends LSWK: Second- Order Nonlinear Optics IV 5:45 p.m.) at (ends Sainte Claire Room, Sainte Claire Hotel Claire Sainte Room, Claire Sainte and Photonics Industry, for the Optics Fundamentals Export Regulation See the Postdeadline Papers Book in your registration bag for exact times and locations and exact times for bag registration your in Book Papers Postdeadline Sessions, See the Paper FiO Postdeadline Sacramento LSWA: Single- LSWA: Molecule I Biophysics LSWD: Single- Molecule Biophysics II LSWG: Ultrafast Spectroscopy I LSWJ: Ultrafast Spectroscopy II 6:15 p.m.) at (ends Atherton FWG: Photonic FWG: Photonic Sensing Devices FWN: Silicon Photonics II FWT: Plasmonic FWT: Sensors 3:15 p.m.) at (ends FWZ: Silicon Photonics III Glen Ellen FWF: Photonic Bandgap Photonic FWF: Devices 9:45 a.m.) at (ends FWM: Optical Trapping and Micromanipulation I 11:45 a.m.) at (ends FWS: Optical Trapping and Micromanipulation II FWY: Optical FWY: Trapping and Micromanipulation III California FWE: Novel Fiber FWE: Novel Devices II 9:45 a.m.) at (ends FWL: Optical Devices Communication FWR: Novel Optical Architectures in Emerging I Technologies FWX: Novel Optical Architectures in Emerging II Technologies
21st Valley Century II st FWQ: Phase Space Optics—Optical System Theory for the Phase Space FWW: Optics—Optical System Theory for the 21 FWD: Turbulence FWD: Turbulence Nonlinear and Other Phenomena FWK: All-Optical Signal Processing III Century I 3:15 p.m.) at (ends (on your own) Lunch your Break (on Gold Market Street Foyer, Fairmont Hotel Fairmont Foyer, Street Market Registration, Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Coffee Break, Imperial Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Exhibit Hall Open, Imperial FWP: Metamaterials III JWE: Entanglement Generation and Measurement IV (Joint FiO/LS) 6:00 p.m.) at (ends FWC: Extraordinary and Transmission SurfaceStructured in FWJ: Quantum Optics II Waveguides 12:15 p.m.) at (ends Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Coffee Break/Exhibits, Imperial Regency Ballroom I, Fairmont Hotel I, Fairmont Ballroom Regency Reception, AIOM Welcome Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Session, Imperial JWC: Joint FiO/LS Poster Crystal FWO: OSA Topical FWO: OSA Topical Meeting Highlights I OSA Topical FWV: Meeting Highlights II FWB: Optical FWB: Optical Processing Information in the and Transport Age of Nanophotonics and Metamaterials FWI: Optics in Information Sciences Sainte Claire Room, Sainte Claire Hotel Claire Sainte Room, Claire Sainte and Photonics Industry, for the Optics Fundamentals Export Regulation See the Postdeadline Papers Book in your registration bag for exact times and locations and exact times for bag registration your in Book Papers Postdeadline Sessions, See the Paper FiO Postdeadline Empire JWD: Entanglement Generation and Measurement III (Joint FiO/LS) FWU: Coherence and Optics II Fundamental FWA: Biomedical FWA: of Applications Ultrafast Lasers FWH: Coherence and Optics I Fundamental 12:15 p.m.) at (ends 1:30 p.m.–3:30 p.m. 1:30 p.m.–3:30 p.m. 3:30 p.m.–4:00 p.m. 4:00 p.m.–5:30 p.m. 6:30 p.m.–8:00 p.m. 6:30 p.m.–8:00 7:30 a.m.–5:30 p.m. 7:30 a.m.–5:30 a.m. 8:00 a.m.–10:00 9:00 a.m.–12:00 p.m. 10:00 a.m.–10:30 a.m. 10:00 a.m.–4:00 p.m. 10:30 a.m.–12:00 p.m. p.m. 12:00 p.m.–1:30 p.m. 12:00 p.m.–1:30 Agenda of Sessions 40 Key toShading Agenda ofSessions 1:30 p.m.–3:30 p.m. 8:00 a.m.–10:00a.m. 5:30 p.m.–8:00 p.m. 3:30 p.m.–4:00 p.m. 12:00 p.m.–1:30 p.m. 10:00 a.m.–10:30a.m. 7:30 a.m.–5:00p.m. 4:00 p.m.–6:00 p.m. 10:30 a.m.–12:00 p.m. Frontiers inOptics (ends at 2:45p.m.) LSThE: X-Ray ImagingII X-RayLSThA: ImagingI (ends at 5:45p.m.) Properties ofMaterials OpticalNonlinear FThS: Correlation Spectroscopy LSThC: X-Ray Photon Science Educators'Day, McCaw Hall, Frances C.Arrillaga Alumni Center, Stanford Univ., 326Galvez Street, Stanford, California 94305,Phone: 650.723.2021 Empire Science Laser —Thursday, October15 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 and InstrumentsI NanoscaleMethods FThM: NanofocusingOpticsI FThA: (ends at 5:15p.m.) and InstrumentsII NanoscaleMethods FThT: NanofocusingOpticsII FThG: Crystal Coffee Break,Regency and Imperial Ballroom Foyer, Fairmont Hotel Coffee Break,Regency and Imperial Ballroom Foyer, Fairmont Hotel Joint Registration, Market Street Foyer, Fairmont Hotel and AlignmentII Design, Characterization Freeform OpticalSurfaces: Asphericand FThN: Holographic OpticsIII Diffractiveand FThB: (ends at 11:45a.m.) Alignment I Characterization and Design, Optical Surfaces: AsphericandFreeform FThH: Lunch Break(on yourLunch own) • Fall OSAOptics &Photonics Congress Gold October 11–15,2009 FThO: Micro-CavityDevicesII FThO: Micro-CavityDevicesI FThC: Optical Phenomena NovelNonlinear FThI: Devices III Micro-Cavity FThU: Valley Interventional Medicine Interventional Opticsin FThP: I Fiber Lasers High-Power FThD: Fiber Lasers II Fiber Lasers High-Power FThJ: California Imaging intheEye Molecular FThQ: IntegratedOptics FThE: FThK: Optoelectronics FThK: FThV: MicroscopyandOCTII Glen Ellen Science Educators’Day, McCaw Hall, Frances C.Arrillaga Alumni Center, Stanford Univ., 326Galvez Street, Stanford, California 94305,Phone: 650.723.2021 (ends at 3:00p.m.) Biophysics V LSThF: Single-Molecule Biophysics III LSThB: Single-Molecule Biophysics IV LSThD: Single-Molecule (ends at 5:45p.m.) Waveguides andDevices Plasmonic FThW: Atherton Coffee Break,Regency and Imperial Ballroom Foyer, Fairmont Hotel Coffee Break,Regency and Imperial Ballroom Foyer, Fairmont Hotel Imaging andPhotographyI Computational FThR: Optical DesignI and Birefringencein PolarizationFThF: (ends at 11:45a.m.) Design II Birefringence inOptical Polarization and FThL: Imaging andPhotographyII Computational FThX: Sacramento Registration, Market Street Foyer, Fairmont Hotel Lunch Break(on yourLunch own) (ends at 3:10p.m.) Sensing II AOThC: Wavefront (ends at 9:40a.m.) Systems II AdaptiveOptics AOThA: (ends at 11:30a.m.) and ModelingII AOThB: SystemSimulation (ends at 5:30p.m.) Correction Technology AOThD: Wavefront Fairfield (ends at 3:15p.m.) Properties AThC: GlassSynthesisand (ends at 9:30a.m.) Materials AThA: Nanostructured of Nanophotonics AThB: Applications AThD: OpticalFibers Belvedere (ends at 3:00p.m.) Spectroscopy Complex Mediaand CThC: Imagingthrough Concepts NewImaging CThA: (ends at 12:15p.m.) Methods CThB: PupilEncoding (4:00 p.m.–5:00 p.m.) Discussion CThD: COSIPanel Club Regent Agenda of Sessions 41 COSI Club Regent CThD: COSI Panel CThD: COSI Panel Discussion p.m.) (4:00 p.m.–5:00 CThA: New Imaging Concepts CThB: Pupil Encoding Methods 12:15 p.m.) at (ends CThC: Imaging through Media and Complex Spectroscopy 3:00 p.m.) at (ends AIOM Belvedere AThD: Optical Fibers AThD: AThA: Nanostructured Nanostructured AThA: Materials 9:30 a.m.) at (ends Applications AThB: of Nanophotonics and Glass Synthesis AThC: Properties 3:15 p.m.) at (ends Fall OSA Optics & Photonics Congress & Photonics OSA Optics Fall AO October 11–15, 2009 Fairfield • AOThD: Wavefront AOThD: Wavefront Correction Technology 5:30 p.m.) at (ends AOThA: Adaptive Optics Systems II 9:40 a.m.) at (ends AOThB: System Simulation and Modeling II 11:30 a.m.) at (ends AOThC: Wavefront Sensing II 3:10 p.m.) at (ends
(on your own) Lunch your (on Break Market Street Foyer, Fairmont Hotel Fairmont Foyer, Street Market Registration, Sacramento FThX: Computational Imaging and Photography II FThF: Polarization FThF:Polarization in and Birefringence Optical Design I FThL: and Polarization Birefringence in Optical Design II 11:45 a.m.) at (ends FThR: Computational I Imaging and Photography Regency and Imperial Ballroom Foyer, Fairmont Hotel Fairmont Foyer, Ballroom Imperial and Coffee Break, Regency Hotel Fairmont Foyer, Ballroom Imperial and Coffee Break, Regency FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Atherton FThW: Plasmonic and Devices Waveguides 5:45 p.m.) at (ends LSThB: Single-Molecule LSThB: Single-Molecule III Biophysics LSThD: Single-Molecule Biophysics IV Single-Molecule LSThF: Biophysics V 3:00 p.m.) at (ends McCaw Hall, Frances C. Arrillaga Alumni Center, Stanford Univ., 326 Galvez Street, Stanford, California 94305, Phone: 650.723.2021 94305, Phone: California Stanford, Street, Galvez 326 Univ., Stanford Center, Alumni C. Arrillaga Frances Hall, McCaw Science Educators’ Day, Glen Ellen FThV: Microscopy and OCT II FThE: Optics Integrated FThK: Optoelectronics FThQ: Molecular Imaging in the Eye California FThD: High-Power Fiber Lasers I FThJ: High-Power Fiber Lasers II FThP: Optics in Interventional Medicine Valley FThU: Micro-Cavity Devices III FThC: Devices I Micro-Cavity FThI: Novel Nonlinear Optical Phenomena FThO: Micro-Cavity Devices II Gold (on your own) Lunch your (on Break FThB: and Diffractive Optics III Holographic FThH: Aspheric and Freeform Optical Surfaces: Design, Characterization and Alignment I 11:45 a.m.) at (ends FThN: Aspheric and Optical Surfaces:Freeform Design, Characterization and Alignment II Market Street Foyer, Fairmont Hotel Fairmont Foyer, Street Market Registration, Regency and Imperial Ballroom Foyer, Fairmont Hotel Fairmont Foyer, Ballroom Imperial and Coffee Break, Regency Hotel Fairmont Foyer, Ballroom Imperial and Coffee Break, Regency Crystal FThT: Nanoscale Methods and Instruments II 5:15 p.m.) at (ends FThA:Optics I Nanofocusing FThG: Nanofocusing Optics II FThM: Nanoscale Methods and Instruments I Empire McCaw Hall, Frances C. Arrillaga Alumni Center, Stanford Univ., 326 Galvez Street, Stanford, California 94305, Phone: 650.723.2021 94305, Phone: California Stanford, Street, Galvez 326 Univ., Stanford Center, Alumni C. Arrillaga Frances Hall, McCaw Science Educators' Day, FThS: Optical Nonlinear Properties of Materials 5:45 p.m.) at (ends LSThA: X-Ray Imaging I LSThA: X-Ray Photon LSThC: X-Ray Correlation Spectroscopy Imaging II LSThE: X-Ray 2:45 p.m.) at (ends 3:30 p.m.–4:00 p.m. 3:30 p.m.–4:00 p.m. 4:00 p.m.–6:00 p.m. 5:30 p.m.–8:00 7:30 a.m.–5:00 p.m. 7:30 a.m.–5:00 a.m. 8:00 a.m.–10:00 10:00 a.m.–10:30 a.m. p.m. a.m.–12:00 10:30 p.m. 12:00 p.m.–1:30 p.m. 1:30 p.m.–3:30 FiO/LS/Fall Congress Key to Authors and Presiders (Bold denotes presider or presenting author. Presentation numbers are listed in alphabetical order.)
Abate, Adam R.—FTuY2 Alipour, Payam—FWZ2 Artal, Pablo—LSWB4 Banks, Martin—FTuA2, FTuM2, FTuF Benson, Oliver—FWE4 Abell, Josh—FMH4 Aller-Carpentier, Emmanuel—AOTuC2 Artar, Alp—FMA4 Barbastathis, George—CThA3, CTuD4, Beresnev, A.—JWA4 Abi-Salloum, T. Y.—LSTuA2 Allman, Brendan—JWB5 Artioukov, I. A.—FTuZ2 FME7, FThB1, FThR3, JWC24 Bergh, Magnus—LSThA3 Abolghasem, Payam—LSWH4 Allsop, T.—LMTuC6 Aschenbach, Konley—JWA4 Barbieri, M.—JWD3 Berglund, Andrew—LSWD4
Key to Authors Key Abramochkin, Eugeny—FWW3 Almeida, Euclides C. L.—AThC5 Aschieri, P.—FWD1 Barbosa, L. C.—FWF2 Berkner, Kathrin—CTuC6 Accardi, Anthony—CTuB5 Almeida, M. P.—JWD3 Ashok, M.—LSTuG6 Barclay, Paul E.—FThU1, FWJ4, LSTuD3 Berkovitch, Nikolai—FMH3 Achermann, Marc—LSWG, LSWJ4 Alonso, Benjamin—JWC10, LSWB4 Askari, Murtaza—FWF6 Barea, Luis A. M.—FThO7 Berland, Keith—LSThB1, LSThF Ackerman, John R.—CThC2 Alonso, Miguel A.—FWH1, FWQ2, FWW Aslanov, Emil—JWC8 Barnakov, Yu. A.—FTuN5 Berova, Nina—LSMB1 Acremann, Yves—LSMH2 Alrubaiee, Mohammad—JTuC10 Asman, Charles P.—FThD2 Barnes, Michael D.—LSMB4, LSMF, Bertilson, M—FThA4 Adam, Vojtĕch—JWC19 Altepeter, Joseph B.—FWJ5 Asobe, Masaki—JWE2 LSTuA, LSTuJ, LSTuJ2, LSTuJ3 Bertolotti, Jacopo—FMC4 Adams, Daniel E.—FWH7 Altug, Hatice—FMA4, FWP6 Aspelmeyer, Markus—LSTuH1 Barnett, Stephen—CTuC2, JTuB4, JWD4 Bewersdorf, Joerg—LSThB2, LSThD Adato, Ronen—FWP6 Alù, Andrea—FMH6 Aspuru-Guzik, A.—JWD3 Baronavski, Andrew—JWC28 Beye, M.—LSMH1 Adhikari, Rana—JMB, JTuA1, JWC20 Amann, Markus C.—FTuW2 Assoufid, Lahsen—FThG, FThM2 Barreiro, Julio—JWE1 Bhakta, Aditya—JWC24 Adibi, Ali—FTuB7, FWF6, FWZ2 Ambekar Ramachandra Rao, Raghu— Athale, Ravindra Anant—CThD, CWB Barros, Gemima—FThS1 Bhakta, Vikrant R.—CThB4, CTuC4, Adkins, Sean—AOTuB1 FMK7 Attwood, David—FTuZ2, FThA1, FThT Barsi, Christopher—FMF1, FThX4 CWB5 Adler, Werner—FThP2 Amitay, Zohar—LSTuG4 Aubailly, Mathieu—CThC3 Bartal, Guy—FTuB2, FTuN2 Bhaktha, Shivakiran N. B.—AThC3 Agarwal, Anu—AThC4 Ammons, Mark—AOTuA4 Audebert, Patrick—FMI2 Barthélémy, Alain—FWI5 Bhattacharya, Dipten—AWA4 Agarwal, Girish S.—FMG5, FWI6, JWD2, Ams, M.—LMTuC1 Aviña-Cervantes, Juan G.—JWC67 Barthelemy, Pierre—FMC4 Bhola, Bipin—FTuB4 LSTuB4, LSTuK3 An, S.—FWE2 Avlasevich, Yuri—FMH2 Bartoli, Filbert—FTuY5 Bialczak, Radoslaw C.—JMA1 Ageev, Eugene—AThB4 Andegeko, Yair—FMF7 Ayala, Oscar D.—FThP6 Barton, Jennifer K.—FME7 Biamonte, J. D.—JWD3 Aggarwal, Ishwar—AThD2 Andersen, David A.—AOThB1 Azad, Abul K.—FWO1 Barty, Anton—LSThA3 Bidlot, Jean-Raymond—FTuR1 Agranov, Gennadiy—CThB6 Andersen, David R.—AOThA4 Azevedo, Antonio—FWT3 Barty, Christopher—FMI1 Bifano, Thomas—AOThD1, FWA2 Agrawal, Govind P.—FML4, FWU1 Anderson, E. H.—FTuZ2 Barviau, B.—FWD1 Bijlani, Bhavin J.—LSWH4 Aguilar-Soto, Jose G.—FTuE1 Anderson, Monte D.—JWC21 Baba, Yoshinobu—LSTuF4 Basden, Alastair G.—AOTuD4, AOTuA5 Biondini, Gino—FTuR3 Aguilera-Gómez, Eduardo—JWC67 Anderson, Matt E.—FThB7 Badieirostami, Majid—CThA4, CTuD1 Bastiaans, Martin J.—FWQ1 Bird, Mark—FTuQ4 Ahamad, Nur—FWT1 Anderson, Ryan—FMJ2 Bae, Hee-Kyoung—FMJ6 Bastin, Thierry—JWD2 Biswas, Prasanta K.—AWA4 Ahmed, Iftikhar—FThO4 Anderson, Troy—AThC4 Bae, In-Ho—JWC11 Basurto-Pensado, Miguel A.—FTuE1 Biswas, Roshni—FTuE5 Ahmed, Nisar—FTuC3 Anderson, Trevor—LSThD3 Bae, Janghwan—CWA1 Batteiger, V—LSTuB1 Biswas, Raka—JWC50 Ahn, Yeong-Hwan—FWC1 Anguita, Jaime A.—FTuC5 Bagheri, Saeed—CTuC5 Baum, Peter—LSWJ1 Bizheva, Kostadinka—FTuQ4 Ahn, Yeonghwan—FWP Ansmann, M.—JMA1 Bagnato, V. S.—JTuC20 Beausoleil, Raymond G.—FThE2, FThU1, Black, Kvar C. L.—JWC76 Aiello, A.—FMF5 Antonio-Lopez, Jose E.—FTuD6 Baig, Mirza I.—FTuC7 FWJ4, FWZ5, LSTuD3 Blain, Celia—AOThD4 Aitchison, J. S.—FThW1, FThW3, Apiratikul, Paveen—FTuI2 Bailey, Ryan C.—LSMC1, LSMG Beckley, Amber M.—FThL2 Blair, David A. D.—FWT1 FThW7, LMTuC5 Applegate, Brian E.—FThV4 Bajt, Saša—LSThA3 Beclin, Franck—AThC3 Blair, John—FTuN4 Akbulut, Mehmetcan—FMD5, FWL1 Arabi, Hesam—FWE2 Baker, Henry—JWC34 Bedggood, Phillip—JWB5 Blair, Loudon—FTuC2 Akozbek, Neset—FThW2 Arai, Alan—LMTuDP Baker, Katherine A.—FThP3 Beeck, T.—LSMH1 Blake, Peter—FThN Al-Qasimi, Asma—FWU5 Arai, Jun—FTuF3 Baker, Lane A.—LSMC2 Begue, Nathan J.—LSWH1 Bland-Hawthorn, Joss—FTuD2 Al-Zayed, Ayman S.—FTuW5 Arain, Muzammil A.—FThS, JTuA4 Baker, Sarah—FWR1 Bekker, Alexander—FWD5 Blank, David A.—LSWC4, LSWI Albert, Jacques—FWG, FWT1 Archambault, Jean-Luc—FTuC2 Balakrishnan, Subramanian—JWC31 Beliaev, Alexander—FWT1 Blinov, Boris B.—JTuB5, JTuB6 Albuquerque, Eudenilson L.—FTuX4 Archer, Rod—FTuA1 Balasubramanian, T.—LSTuG6 Bellec, Matthieu—AWB3 Bliokh, Konstantin Yu—FWP3 Aleksoff, Carl C.—FThO5 Arjmand, Arghavan—LSWH4 Baldelli, Steven—LSWH3 Bello-Jiménez, Miguel A.—FThD4 Bliokh, Yuri P.—FWP3 Alencar, Marcio A. R.—AThA3 Arnold, Stephen—LSMG2 Balla, Naveen K.—LSWK5 Benner, W. H.—LSThA3 Bliss, David—AWA1 Alibart, Olivier—FWJ2 Arnoldus, Henk F.—FMF3 Balle, S.—LSTuI4 Bennink, Ryan S.—JMA4, JMA7 Bloemer, Mark J.—FThW2, FWC6 Alic, Nikola—FML2, FTuD2, FWK2, FWL Arrizón, Victor—JWC2 Banaee, Mohamad G.—FWT2, FWT5 Bennion, Ian—JTuC19, LMTuA6, Blum, Christian—FWS6 Alieva, Tatiana—FWW3, STuD2, STuD3 Arroyo Carrasco, M. L.—JWC59 Bang, Ole—FTuD4 LMTuC6 Bobier, William R.—JWC81
152 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 • October 11–15, 2009 Boccaletti, Anthony—AOTuC3 Brown, Thomas G.—FThL2, FThL3 Castellanos-Betran, Manuel A.—LSTuE3 Chen, Zhigang—FThI3, FTuV5, FTuX2, Chumanov, George—FMH4 Bockenhauer, Samuel—JWC16, LSTuF3 Brune, M.—JWE4 Castro, Jose—FMB3 JWC29 Chun, Mark—AOThA3 Bogan, Michael J.—LSThA3 Brunner, Robert—AThB3 Cavalcanti, Eric G.—LSTuA4 Chen, Ziyang—FThX6 Chung, Chia-Chao—JWC82 Key to Authors Bohn, Paul—LSTuF, LSTuF1 Bryant, George—AWA1 Cavalcanti, Gustavo O.—FWT3 Cheng, Yang-Chun—FTuS2 Chung, Samuel—FWA1 Bokoch, Michael—JWC16 Buchhave, Preben—FThR6 Cavillac, Patrick—FMI2 Cheng, Yih-Shyang—JWC5 Chuntonov, Lev—LSTuG4 Bolognini, Néstor—JWC83 Bueno, Juan M.—LSWB4 Ceballos, Daniel E.—FWP3 Chergui, Majed—LSTuC1 Cingolani, Roberto—FThO1, LMTuB2 Bondar’, Anatolii M.—FThS6 Bun, Philippe—FThB4 Celestre, Richard—FThT2 Chériaux, Gilles—FMI2 Cirino, Giuseppe A.—JWC4 Bondu, François—JMB4 Bunghardt, Kaitlin—FTuQ4 Cerdán, Luis—LSWG4 Cherri, Abdallah K.—FTuW5 Cleland, A. N.—JMA1 Bones, Phil—STuA3, STuD Bunk, Oliver—FThT1, LSTuL4 Cerrina, Franco—FTuS2 Cherroret, Nicolas—FMC5 Cloutier, Sylvain G.—AWA5 Booth, Martin J.—AOThC3, AOWA2 Burch, J.—CThA1 Cerullo, G.—LMTuC3 Chettiar, Uday K.—FTuN3, FTuN7 Cocke, C. L.—LSTuI3 Bordonalli, Aldário C.—FTuC4, FWF2 Burge, James H.—FThH3, FThN1 Cesa, Yanina—FWS6 Chi, Wanli—FThR1, FThR5 Coen, S.—FWD1 Born, Erik G.—JWC33 Burke, Daniel—AOTuC5 Cescato, Lucila H.—JWC4 Chia, Thomas—FWA4 Cohadon, P.-F.—LSTuK1 Borondics, Ferenc—LSWJ3 Burns, Stephen A.—FThQ2, JWB, JWF1 Cha, Myoungsik—FTuO3, JWC11 Chien, Fan-Ching—JWC69, JWC72 Cohen, Adam—FWM2 Borra, Ermanno F.—JWF2 Buse, Karsten—AWC2 Chabanov, Andrey A.—FMC5, FTuJ Chien, Hung-Chang—FMD1 Cohen, Offir—FWJ3 Borrego Varillas, Rocío—JWC10, LSWB4 Busoni, Lorenzo—AOTuA3 Chakravarty, Abhijit—FTuP5, JWC50 Chiesa, Sabine—JTuC6 Cojocaru, Crina M.—FThI1, FTuS4 Bostedt, Christoph—LSThA3 Butler, Anthony—STuA3 Chamanzar, Maysamreza—FTuB7 Chilkoti, Ashutosh—FTuY3 Collier, John—FMI3 Botten, Lindsay C.—FWF5 Butler, Alex C.—JWC14 Chambaret, Jean Paul—FMI2 Chillcce, E. F.—FWF2 Collini, Elisabetta—LSWC2 Bouazaoui, Mohamed—AThC3 Butterley, Timothy—AOTuD4, AOTuA5 Chan, James—FWS2 Chipman, Russell A.—FThF1, FThF, Conan, Jean-Marc—AOThA2, AOWB1, Boucher, Yann G.—FThO3 Byeon, Ji-Yeon—LSMC1 Chan, Jasper—LSTuE2 FThL1, SC274 AOWB4 Boudouris, Bryan W.—LSWC4 Byer, Robert L.—AWC3 Chan, Sze-Chun—FMD3 Chipouline, Arkadi—FMA3, FThC3, Conan, Rodolphe—AOThD4, AOTuB2 Bouma, Brett. E—FWV3 Chan, Wai L.—STuA4 FThC6 Cone, Michael T.—FWR5 Bourguignon, Bernard— JTuC16 Cai, Wei—JTuC10 Chang, Gee-Kung—FMD1, FTuC Chiragh, Furqan L.—FThK1 Conley, Nicholas R.—CTuD1, LSWD2 Bourhis, Kevin—AWB3 Cai, ZhiPing—FThO3 Chang, Yu-Hsiu—JWC1 Chiu, Daniel T.—LSMG1 Contag, Chris—FTuL1 Boutet, Sébastien—LSThA2, LSThA3, Cakmakci, Ozan—FThN2, FTuT3 Chang, Z.-C.—FWC2 Cho, David—LSWE1 Cookson, Christopher J.—FTuQ4 LSThC Calef, Brandoch—STuC1, STuC5 Chang-Hasnain, Connie J.—FThU5, Cho, Hyung Uk—FThK2 Cooper, M. L.—FML2 Bowlan, Pamela R.—FTuO5, SWA6 Caleman, Carl—LSThA3 FTuW2, FWL3 Cho, Ha Na—LSTuC4 Coppey-Moisan, Maité—FThB4 Boyd, Robert W.—FMA2, JWD4 Calhoun, T. R.—LSWC1 Chao, W.—FTuZ2 Cho, Hyoung J.—FTuE1 Coppinger, Matthew—AWA5 Boyraz, Ozdal—FTuE Calmano, Thomas—LMTuC2 Chao, Yu-Faye—FThL4 Cho, MinHaeng—LSWI1 Corbett, Brian—FThJ3 Bozek, John D.—LSTuL1 Calvo, María L.—STuD3 Chapman, Henry N.—LSThA3 Choi, Hee Joo—JWC11 Corkum, P. B.—LMTuA1 Brady, David J.—CThA5, CThA6, CThD, Camacho, Ryan M.—LSTuE2 Charan, Shobhit—JWC69 Choi, Hyunyong—LSWJ3 Cornia, Alberto—AOTuC3 CTuA3, CTuA6, CTuD, CWB2, Cámara, Alejandro—STuD3 Charters, Robbie—FThE5 Choi, Jae-Young—FThM2 Correia, Carlos—AOWB1, AOWB4 CWB4 Campbell, Melanie C.—FTuQ, FTuQ4, Chaturvedi, Pratik—AThA5 Choi, Jiyeon—AWB3 Costa, M. M.—JTuC20 Braga, R. L.—FWF2 JWF2 Chaudhuri, Anabil—FTuC6, FTuP Choi, Kerkil—CThA5, CThA6, CTuA6 Costela, Angel—LSWG4 Bragheri, F.—LSTuI4 Camposeo, Andrea—FThO1, LMTuB2 Chavez Boggio, Jose M.—FML2, FTuD2, Choi, Ki-Man—FTuP2 Costille, Anne—AOThA2 Bratkovski, Alex—FWC5 Canfield, Brian K.—FWM4 FWE Choi, S. S.—FWC3 Cotter, D.—FTuW1 Bres, Camille-Sophie—FWK2 Canioni, Lionel—AWB3 Chemla, Fanny—AOTuA5 Choi, Tae-Il—JTuC13 Coutts, David W.—JWC14 Bretschneider, Mario—AThB3 Cao, Donna—CThB6 Chen, Baosuan—FThX6 Choi, Wonshik—FThB3 Coyle, Kevin—CTuB4 Brewer, C.—FTuZ2 Cao, Shaochun—FTuW4 Chen, Bin—FTuE4 Chou, Keng Chang—LSWE3, LSWK Cragg, George E.—LSTuJ4 Briant, T.—LSTuK1 Capasso, Federico—LSTuH2 Chen, Chia-Chu—FWG3 Chowdhury, Arshad—FMD1 Craig, D. Q. M.—FMK2 Bristow, A. D.—LSWC3 Capoen, Bruno—AThC3 Chen, Chia-Hsu—JWC1, JWC82 Christensen, Marc P.—CTuB4, CTuC4, Craig, Ian M.—LSWB2 Brito, Jose M.—JWC63 Carbillet, Marcel—AOTuC3 Chen, Hou-Tong—FMA, FTuB1, FWO1 CWB5, FThE6 Creeden, Daniel C.—AWA2 Brizuela, F.—FTuZ2 Cardinal, Thierry—AWB3 Chen, Mingzhou—AOThA1 Christodoulides, Demetrios N.—FMC2, Cristiani, I.—LSTuI4 Bromberg, Yaron—FMC2, FMG4, FThX3, Carhart, Gary W.—CThC3, JWA4 Chen, Nanguang—FThR4 FMF4, LSMC3 Crochet, Jared—LSWJ5 FWD3 Carlie, Nathan—AThC4 Chen, Peilin—JWC69, JWC72 Christou, Julian—AOTuC1, AOTuC2, Crognale, Claudio—JWC48 Brooks, Aidan F.—JWC20 Carmon, Tal—FThO5 Chen, Qian—JTuC11 AOWA4, JWA Crozier, Kenneth B.—FThB2, FTuH3, Brousseau, Denis—JWF2 Carney, P. S.—FWH3 Chen, Xi—CThB6, FTuB4 Chu, Kaiqin—FThR5 FTuV2, FTuY2, FWM1, FWT2, Brow, Richard K.—LMTuB4 Carr, Stephen—FWI2 Chen, Xuxing—FWK5 Chu, Kengyeh K.—FWA2 FWT5, FWY Brown, Dean P.—FThL3 Case, Jason—FWO3 Chen, Yuchuan—AOThC2 Chu, Yizhuo—FWT5 Cryan, Martin J.—FMG1 Brown, Jacob E.—JWC84 Cassarly, William J.—FThN5 Chubarova, E.—FThA4 Cui, Bianxiao—LSThB3
FiO/LS/AO/AIOM/COSI/LM/SRS 2009 • October 11–15, 2009 153 Cui, Cuicui—FMD3 Deng, Wu—JTuC5 Doris, Ng—FWN2 Ebisawa, Satoshi—JWC49, JWC52 Faulk, Ben—FWO3 Cui, Meng—FWS4 de Oliveira, Júlio C R. F.—FTuC4 Dorrer, Christophe—STuD1 Efros, Alexander L.—LSTuJ4 Favalora, Gregg E.—FTuT2 Cundiff, S. T.—LSWC3 D’Orazio, Antonella—FWC6 Dorronsoro, Carlos—JWB4 Eftekhar, Ali Asghar—FWZ2 Fayer, Michael D.—LSWF2 Currie, Marc—FThS3 Dereniak, Eustace L.—FThF4 Dossou, Kokou B.—FWF5 Egamov, Shukhrat—FWB3 Faylienejad, Azadeh—JWC79 Cusnir, Nicolas—FThB7 Derickson, Dennis J.—FMJ5 Dotsenko, I.—JWE4 Egger, Robert—FTuV5, FTuX2 Fecko, Christopher J.—LSThB, LSThD1 DeRocco, Vanessa C.—LSThD3 Douglas, Nick—FWM2 Eggleton, Benjamin J.—FTuD4, FTuR5, Fei, Yiyan—FTuY4 d’Aguanno, Giuseppe—FTuS4 Derosa, Maria—FWT1 Douglas, Scott C.—CTuB4, CWB5 FWK1 Fejer, Martin M.—AWA, AWC2, AWC3, da Costa, José A. P.—FTuX4 Desai, Narayana Rao—JTuC17 Douglass, Kyle M.—CWA5 Eichenfield, Matt—LSTuE2 FThS7 Dahan, Maxime—LSThB4 DeSoto, Michael G.—JWC75 Douillet, Denis—FMI2 El-Emawy, Mohamed A.—FMB4, FMB5 Feld, Michael—FThB3
Key to Authors Key Dai, Lun—FTuB2 de Sterke, C. Martijn—FTuD4, FTuR5, Douplik, Alexandre—FThP2 El-Ganainy, Ramy—LSMC3 Ferguson, Daniel—JWF1 Dai, Wanjun—JTuC5 FWF5 Dowling, Jonathan P.—LSTuA3 El-Hanany, Uri—LSTuG4 Fernandes, Gustavo—FWZ4 Dai, X.—LSWC3 Deutsch, Bradley—FTuL2 Drachev, Vladimir—FTuN3 Ellerbroek, Brent L.—AOThB1, AOThC1, Fernandes, Luís A.—LMTuC5 Dainty, Christopher—AOThA1, AOTuC5, Devaney, Nicholas—AOTuC5 Drake, Tyler K.—JWC75 AOTuD2, AOWB3 Fernandez-Cull, Christy—CTuA3 JTuC6, JWA1 DeVree, Brian—JWC16 Drapeau, Julie—JWF2 Elliott, Lindsay C. C.—LSTuF1 Fernando, Harendra N. J.—FThJ3, FThK6 Dal Negro, Luca—FML1, FML6, FTuB3, Dexheimer, Susan L.—LSTuG3, LSTuG5 Drezet, A.—FWP4 Ellis, Jeremy—CWA5 Féron, Patrice—FThO3 FWN Deych, Lev—FThC3, FThC6, LSTuA5 Drobizhev, Mikhail—JTuC14 Elser, Veit—LSThA1, LSThE Ferrando, Albert—FWH4, FWP3 Dam-Hansen, Carsten—JWC3 Di Benedetto, Francesca—FThO1 Drummond, Jack D.—AOWA4 Elshaari, Ali W.—FML3, FThU4 Ferrari, Maurizio—AThC3 Danielyan, Hakob—LSWK4 Di Giansante, Antonella—JWC48 Drummond, Peter D.—LSTuA4 Elsner, Ann E.—FME5, FThQ2 Ferreira, Mário F.—FThI5 Danner, Aaron J.—FTuN6 Diagaradjane, P.—FME1 Du, Songtao—FThD1 Emmert, L.—FThS7 Fessler, Jeffrey A.—CWA2 Dantus, Marcos—FMF7, LMTuA4, LSWI3 Dianov, Evgeny M.—AThD5 Duane, Peter—FTuV2 Emrick, Todd S.—LSTuJ2, LSTuJ3 Fettig, Doug—CThB6 Das, Bhargab—JWC6 Dias, F.—FTuR2 Dubov, Mykhaylo—LMTuA6, LMTuC6 Engheta, Nader—FMA7, FMH6, FTuN7 Fiala, Jan—FWC7 Das, Nilanjana—AWA4 Dickinson, Mary E.—FThV2 Dubra, Alfredo—JWF4 English, Alex—FWC2 Fiala, Pavel—AThA2, FWS3, JWC7 Das, Sumanta—FMG5, FWI6 Dickson, Colin—AOTuA5 Dudley, Angela—FThB6 Englund, Dirk—LSTuD4 Fiddy, Michael A.—CThD, CTuA, CTuB2 Davanco, Marcelo I.—FMG2 Diem, Max—FThV6 Dudley, J. M.—FTuR2 Eom, Tae Bong—JWC11 Fienup, James R.—FThX5, LSThE3, Davila-Rodriguez, Josue—FMD2, FMD5 Dierolf, Martin—FThT1, LSTuL4 Dufour, Pascal—JWC73 Erickson, David—FWG1 STuC6, SWA2 Davis, Andrew—AOThD2 Dietrich, Matthew R.—JTuB5, JTuB6 Dumeige, Yannick—FThO3 Erie, Dorothy A.—LSThD3 Figueira, David S. L.—FThO7 Davis, Brynmor J.—FWH3 Dillon, Daren—JTuC3 Dumelow, Thomas—FTuX4 Erramilli, Shyamsunder—FWP6 Finer, Neil—FThP3 Davis, J. P.—LSTuA2, LSTuI5 Dillon, Keith J.—JTuC7 Duncan, D.—LSTuI5 Erzgräber, Hartmut—FThO6 Fischer, Baruch—FWD5 Davis, Lloyd M.—FWM4 Dimakis, Emmanouil—FMH4 Duncan, Jacque—FTuQ3 Esener, Sadik—FWR1 Fischer, Michael—AOThA4 Davis, Matthew J.—FWM3 DiMaria, Jeff—FMA5 Duncan, Michael—FWO, FWV Esposito, Simone—AOTuA3 Fischer, Peer—LSMB2 Dazzi, A.—FMK2 DiMauro, Louis—LSTuI2 Dunlop, Colin—AOTuA5 Essaian, Stepan—LSWK4 Fitzke, Frederick—FThQ1 de Araújo, Cid B.—AThC5, FThS1 Dinakarababu, Dineshbabu V.—CThC5 Dunn, Andrew K.—FME1, FME2, FTuY Evans, Philip—JMA4 Fleck, Andre—JWC81 de Araujo, Renato—JWC43 Ding, Yiwu—FTuY1 Dunn, Douglas S.—FTuF2 Everitt, M.—FThU3 Fleet, Erin F.—CThC2 Deasy, Kieran—FMG3 Dinu, Raluca—FThE3 Dunn, James—FTuS3 Fleischer, Jason W.—FMF1, FMF4, FMF6, de Ceglia, Domenico—FThW2, FWC6 Dipper, Nigel—AOTuA5 Dunningham, J.—FThU3 Faber, C.—FWV1 FThX4, FTuR4, FWD1, FWD2, DECIGO Working Group —JTuA5 Ditmire, Todd—FTuK2 Dupont, Jairton—AThA3 Fabian, Rotermund—FWC1 FWD6, FWU Deepak, Kallepalli L. N.—JTuC17 Divliansky, I. B.—FML2 Durand, Fredo—CTuB1 Fainman, Yeshaiahu— AThA, AThB1, Fleming, G. R.—LSWC1 Dégardin, Annick F.—FTuO6 Dixon, P. Ben—FMF8 Durfee, Charles G.—FWH7 FWB1, JTuC7 Fletcher, Luke B.—LMTuB4, LMTuC4 De Gracia, Pablo—JWB4 Djordjevic, Ivan B.—FTuP4 Dürr, Hermann A.—LSMH3 Falk, Matthias—AWC2 Flores-Rosas, Ariel—FThD4 Dekany, Richard—AOWB Doerschuk, Peter—STuB3, STuB4 Dussauze, Marc—AWB3 Fam, Adly T.—FTuE5 Föhlisch, A.—LSMH1 Dekker, P.—LMTuC1 Dogariu, Aristide—CThB, CThC1, Düsterer, Stefan—LSThA3 Fan, Shanhui—FMH2 Fontana, Eduardo—FWT3 De Koninck, Yves—JWC73 CThD, CWA1, CWA4, CWA5, CWA6, Dvoyrin, Vladislav—JTuC19 Fang, Nicholas X.—AThA5, FWB6 Forbes, Andrew—FThB6 de la Cruz Gutierrez, Manuel—JTuB2 FTuU3, FWY4 Dylov, Dmitry V.—FMF1, FTuR4, FWD2, Fannjiang, Albert—STuA5 Forbes, Greg—FThH1 Deléglise, S.—JWE4 Doherty, Andrew—JTuB1 FWD6 Faraon, Andrei—FWB5, LSTuD4 Ford, Joseph E.—FThP3, FWG2 Delestre, Aurelien—AWB3 Dominguez-Caballero, Jose A.—FThB1 Dynes, James F.—JWE2 Fargin, Evelyne—AWB3 Foster, Mark A.—FTuW3 Delfyett Jr., Peter J.—FMD2, FMD5, Donahue, James P.—LSWI2 Fathi, Mohammad—FWG5 Fourkas, John T.—LSWE2 FWL1, FWL2, FWX4 Donati, Silvano—FWG5 Early, Kevin T.—LSTuG, LSTuJ2, LSTuJ3 Fathpour, Sasan—FML, FWZ1 Fournet, Dominique—FMI2 Demenikov, Mads—FThX2 Dong, Zhaogang—FWP5 Ebbesen, Thomas W.—FWP4 Fattal, David—FWJ4, FWT6 Fournier, Florian R.—FThN5 Deng, Cong—JWF1 Donner, Tobias—LSTuE3 Ebendorff-Heidepriem, Heike—FTuE3 Fauchet, Philippe M.—FML4 Frandsen, Lars H.—FThE1
154 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 • October 11–15, 2009 Frank, Matthias—LSThA3 Garuccio, Augusto—FWI4 Goggin, M. E.—JWD3 Gunaratne, Tissa C.—LMTuA4 Hata, Masato—FWN4 Franke-Arnold, Sonja—CTuC2, JTuB4, Gat, Omri—FWD5 Goldberg, Kenneth—FThT2 Gündogan, Mustafa—FThU6 Hau-Riege, Stefan P.—LSThA3, LSThA4 JWD4 Gaume, Romain—AWD3 Goldring, Damian—FMJ8 Gunn, Erica—LSMF1 Haubrich, David—FWX3 Key to Authors Fraser, Donald—STuC7 Gavel, Donald T.—AOTuA4, AOWA, Goldsmith, Randall H.—LSWA4 Guo, Chunlei—JTuC18 Haus, Joseph W.—FThD4, SC235 Frateschi, Newton C.—FThO7 AOWB5 Gómez, Luis A.—FThS1 Guo, Hong—FWL4 Häusler, Gerd—FWV1 Frattin, Dan—CTuB4 Gayen, Swapan K.—JTuC10 Gómez-Vieyra, Armando—JWF4 Guo, Peng—FTuW2, FWL3 Hawkins, Aaron R.—FMJ7 Frawley, Mary—FMG3 Gaylord, Thomas K.—FMJ4, FTuE7, Gomila, D.—FThI6 Guo, Yuan—LSWK2 Hayasaki, Yoshio—LMTuA2 Frede, Maik—JTuA2 FTuX5, FWP2 Gong, Wei—FThR4 Gupta, Anurag—FWR6 Hayat, Alex—FMG6, FMH3 Freudenthal, John—LSMF1 Gbur, Greg—FTuG, FTuG3, FWC4, SWA1 Gong, Yiyang—FML6, FTuB3 Gupta, Banshi D.—FWG4, FWT Hayee, M. I.—FTuC3 Frick, Ross—AOThB2 Gehm, Michael E.—CThC5, FWX2 Gonzalez, Leonel—AWA3 Gustafson, Scott B.—FME4 Hayes, David—JWD6 Fritschel, Peter—JMB1 Gelsinger, Paul J.—FME7 Goodman, Doug S.—JMA7 Gustafsson, Mats—LSWA5 He, Bin—FThD1 Fritz, David—LSMD2, LSMH Genack, Azriel—FTuJ2, FTuJ3 Goodwin, Peter M.—LSThF2 Guttmann, Peter—FThG1 He, Qiong Y.—LSTuA4 Fry, Edward S.—FWR5, FWX3 Gendron, Eric—AOTuA5 Gorshkov, Alexey V.—FThS2 Guzman, Dani—AOTuA5 He, Weiji—JTuC11 Frydman, Judith—FWM2 Genet, C.—FWP4 Gösele, Ulrich—AThB3 Guzman-Sepulveda, Jose R.—JWC41 He, Xehua—FWI4 Ftaclas, Christ—AOThA3 Geng, Deli—AOTuA5 Gowing, Laura—FTuQ4 He, Zhusong—FWL6 Fu, Kai-Mei C.—FThU1, FWJ4, LSTuD3 Genty, G.—FTuR2 Goy, Alexandre S.—CThA2 Haack, Karl—CTuB4 Healy, Andrew T.—LSWC4 Fu, Xuelei—FMD3 George, Brandon—FMJ5 Grace, Edward J.—FThE8, FThI2, FWE3 Haefner, David P.—CThC1, CWA1, Healy, John J.—FWW1 Fuerbach, A.—LMTuC1 George, Nicholas—FThR1, FThR5 Granzow, Nicolai—AThD3 CWA6, FWY4 Heckel, John—FMH4 Fuesz, Peter—FThM4 Georges, Patrick—FMI2 Gratadour, Damien—AOTuA5 Hagan, David J.—FThS5, LSTuG2 Heckenberg, Norman R.—FWM3 Fujii, Keita—CWB1 Georgescu, Ionut—LSTuI1 Gravel, Yann—FTuV1 Hageman, Nicholas—JTuC9 Heidmann, A.—LSTuK1 Fujiwara, Masahide—FMD4 Georgiev, Todor G.—CTuB3, STuA6 Gravelle, Bob—CThB6 Hagen, Nathan—CWB4 Heim, Stefan—FThG1 Fukunaga, Yukihiro—JWC74 Gerke, Timothy D.—LMTuB3 Green, Lekara—JWC13 Haggerty, Bryan P.—FThQ2 Helgert, Michael—AThB3 Fukushima, Seiji—FThE4 Gerlein, Felipe—AWA5 Greenfield, Elad—LSMC3 Hahn, Megan A.—LSTuJ4 Helmerson, Kristian—FWS5, JWC60 Fung, Kin Hung—AThA5 Gertsvolf, M.—LMTuA1 Gregor, Markus—FWE4 Hajdu, Janos—LSThA3 Helmy, Amr S.—LSWH4 Furlan, Walter D.—FWW2 Gerwe, David—STuC1 Grenier, Jason R.—LMTuC5 Haji-Saeed, Bahareh—AOThD2, FTuH5, Hemberg, O.—FThA4 Fürstenberg, Alexandre—JWC16, LSTuF3 Ghadarghadr, Shabnam—FTuV4 Grice, Warren P.—JMA4, JMA7, JTuB3, FWI1 Henderson, Marcus H.—JWC75 Fusco, Thierry—AOThA2, AOTuA5, Ghosh, Sankalpa—FWJ2 JWE Halas, Naomi—JWC60 Henry, David—AOTuA5 AOTuC3 Gibson, Stuart J.—STuB5 Grier, David—FWY2 Hall, Matthew A.—FWJ5 Henson, John—FMA5, FMH4 Giessen, Harald—FMH1, FTuB Grinvald, Eran—FMK3 Hall, Victoria—LSMF2 Herbster, Adolfo F.—FTuC4 Gabrielyan, Gevorg—LSWK4 Gill, John—CTuB4 Grobnic, Dan—FTuD7, FTuE2 Hammerer, Klemens—LSTuH1 Herman, Peter R.— LMTuC5 Gaeta, Alexander L.—FTuW3, FWK Gilles, Luc—AOWB3 Groeblacher, Simon—LSTuH1 Hamner, C. R.—LSTuG5 Hernandez, Maritza—JWE6 Gaffney, Kelly J.—LSTuD, LSWF3 Gillet, Jeremie—JWD2 Groff, Tyler D.—AOWA1 Han, Junbo—LSWH4 Hernandez-Romano, Ivan—FTuD6, Gagnon, Etienne—LSTuI3 Gillett, G. G.—JWD3 Grojo, D.—LMTuA1 Han, Ting—FThE5 JWC41 Gaind, Vaibhav—FTuL3 Gilman, Samuel—FTuJ3 Grosberg, Alexander—FWY2 Hands, Philip J. W.—FTuM2 Herriot, Glen—AOThB1, JTuC2 Galeano Zea, July A.—JWC70 Gineste, Jean-Michel—FWY5 Gross, Michel—FThB4 Hänsch, T. W.—LSTuB1 Herrmann, Daniel—FTuK3 Galembeck, André—FThS1 Ginsberg, N. S.—LSWC1 Gu, Claire—FTuE4 Hao, Feng—FTuB6 Herrmann, M.—LSTuB1 Galiová, Michaela—JTuC12, JWC18, Ginzburg, Pavel—FMH3 Gu, Guohua—JTuC11 Harada, Ken-Ichi—JWE2 Hertel, Tobias—LSWJ5 JWC19 Ginzburg, Vladislav—LSWK3 Gu, Tingyi—AThB5 Harden, Sarah—LSMF2 Hertz, Hans M.—FThA4 Gambra, Enrique—JWB4 Girkin, John—LSMG3 Gu, Tingyi— FMB4 , FMB5 Harding, Philip J.—FWF4 Hess, Samuel—FThM1, LSWA2 Gan, Choon How—FWC4 Giuliani, G.—LSTuI4 Gu, Yalong—FTuG3 Harlow, Jennifer W.—LSTuE3 Hester, Brooke C.—JWC60 Gan, Xuetao—JWC32 Give’on, Amir—AOWA3 Gualda, Emilio J.—LSWB4 Haroche, S.—JWE4 Hickmann, Jandir M.—AThA3 Gangopadhyay, Palash—AThB2 Gladden, Chris W.—FTuB2 Gualtieri, Ellen—LSMF2 Harris, S. E.—JMA2 Hickson, Paul—AOTuA2 Gao, Y.—LMTuD2 Gladysz, Szymon—AOTuC1, AOTuC2, Guan, Weihua—FThJ2 Harrison, Mark—AOTuA5, JTuC4 Hill, G. A.—FMK2 Gapontsev, Valentin—FThJ1 AOTuC5 Guehr, Markus—LSTuI, LSTuL Hart, Michael Lloyd—AOTuA3, AOTuD Hill, Jarvis W.—JWC68 García, Olga—LSWG4 Glebov, Leonid—FMF2, FWX5 Guesalaga, Andres—AOTuA5 Harvey, Andrew—FThX2 Hillmyer, Marc A.—LSWC4 García-Casillas, Daniel—JWC36 Glenn, Solomon S.—FWI2 Guha, Shekhar—AWA3 Harwell, Jennifer—FME7 Hirakawa, Yasuyuki—JWC74 García March, M A.—FThI6 Gleyzes, S.—JWE4 Guintrand, Cyril L.—FTuI3 Hasan, Tayyaba—FThP1 Hirano, Msaaki—FTuI4 Garcia-March, Miguel-Angel—FWH4 Gmitro, Arthur—FWR2, FWX Guizar-Sicairos, Manuel—LSThE3 Hassey-Paradise, Ruthanne—LSMB4 Ho, Phay—LSTuI3 García-Moreno, Inmaculada—LSWG4 Gnodtke, Christian—LSTuI1 Guizard, Stéphane—LMTuA5 Hastings, Jerome—LSMD1
FiO/LS/AO/AIOM/COSI/LM/SRS 2009 • October 11–15, 2009 155 Ho, Seng-Tiong—FThC5, FThE3, FThK3, Hunt, Alan J.—LSMG4 Jha, Anand—JWD4 Kamada, Hidehiko—JWE2 Khounsary, Ali—FThM2 FThK4, FThK5, FThO4, FTuB4, Hunter, Jennifer—FTuQ2 Ji, Young Bin—JWC26 Kanaev, Andrey V.—CThC2 Khoury, Jed—AOThD2, FTuH5, FWI1 FWN2, JWC53 Huse, Nils—LSTuC4 Jia, Shu—FMF4, FMF6 Kanai, Yoshikazu—JWC22 Kibler, B.—FWD1 Hodgson, Keith O.—LSThA3 Hutsel, Michael R.—FTuE7 Jian, Fan—FTuS2 Kandel, Mikhail—FTuE5 Kierstead, John—AOThD2, FTuH5, FWI1 Hoener, Matthias—LSThA3 Hvam, Jørn M.—FThE1 Jiang, Chun—AThB5 Kandpal, Hem C.—JWC27 Kilby, Gregory—JWC58 Hofer, Heidi—JWB3 Hwang, Taek Yong—JTuC18 Jiang, Shibin—FTuD5 Kang, Inuk—FMD6, FTuW Kildishev, Alexander—FTuN3 Hoffman, David M.—FTuM2 Hynes, James T.—LSWF1 Jiang, Xuejun—JTuC5 Kang, Yeon Sook—FTuO3 Kim, Byoung Joo—FTuO3 Hoffman, Galen B.—FThE7 Jiang, Yan—FWM2, LSWA4 Kanický, Viktor—JWC18, JWC19 Kim, Dong Jun—FMH5 Hoffnagle, John A.—FThH2 Ianoul, Anatoli—FWT1 Jin, Dan—FThE3 Kanseri, Bhaskar—JWC27 Kim, Donghyun—FMH5
Key to Authors Key Hofheinz, Max—JMA1 Ibarra-Escamilla, Baldemar—FThD4 Jin, Xiaomin—JTuC9 Kapale, Kishore T.— JWC25, JWC84, Kim, Dai-Sik—FTuN, FWC1 Hofmann, Werner—FTuW2 Ibarra-Manzano, Oscar G.—JWC67 Jing, Feng—FTuK4, JTuC5 LSTuA3 Kim, Dae-Chan—JTuC13 Hofmeister, William H.—FWM4 Ibrahim, Hany L.—FWU6 Jing, Gaoshan—FTuY5 Kapteyn, Henry C.—FTuS, FTuZ1, Kim, D. S.—FWC3 Hofsten, O. v—FThA4 Ice, Gene E.—FThM, FThM2 Jingjing, Shi—JWC15 LSTuI3 Kim, Gun-Duk—FMJ6 Hoghooghi, Nazanin—FMD5, FWL1 Ignatovich, Filipp—FTuL2 Jobling, Scott M.—FThN4 Kapur, Pawan—FThN3, FWG6 Kim, Hyunmin—FMK1 Hogle, Craig W.—LSTuI3 Ihee, Harry—LSMD4, LSTuC Jofre, Ana—FWO3 Karadag, Yasin—FThU7 Kim, Hyochul—FWB5 Holá, Markéta—JTuC12 Iijima, Takahiro—JWC22 Johnson, Adam M. F.—FThD2 Karagodsky, Vadim—FThU5 Kim, Jungsang—FWR4 Holinga, George J.—LSWB1 Ikeda, Kazuhiro—AThB1 Johnson, Eric—FTuO1 Karaiskaj, D.—LSWC3 Kim, Kyujung—FMH5 Holmberg, A.—FThA4 Ikesue, Akio—AWD2 Johnson, Luke C.—AOTuA4, AOWB5 Karamehmedović, Emir—FThR6 Kim, Kyu Hyun—JWC75 Holt, Martin V.—FThM4 Ilchenko, Vladimir S.—FThC1 Johnson, Robert—AOTuA1 Karlsson, Magnuss—FTuD2 Kim, Seunghyun—FMJ2 Holy, Timothy—FThV1, JWC71 Imai, Masaaki—FTuC7 Johnson, Steven L.—LSMD3 Karp, Jason H.—FWG2 Kim, Sang Hoon—JWC26 Honjo, Toshimori—JWE2 Ingold, Kirk—JWC58 Johnston, Keith P.—FThP6 Kasdin, N. Jeremy—AOWA1 Kim, Seyoon—JWC54 Horisaki, Ryoichi—CThA5, CThA6, Injeyan, Hagop—FThD2 Jones, Gina C.—FThD2 Käsebier, Thomas—FThC3, FThC6 Kim, Sangin—JWC57 CWB1 Isaka, Mitsuhiro—LMTuA2 Joo, Yang—JWC44 Kash, Jeffrey—FWO2 Kim, Taehyun—FWR4 Horng, Ji-Bin—JWC1 Ishibashi, Taka-aki—LSWK1 Jordan, Andrew N.—FMF8 Kassal, I.—JWD3 Kim, Tae-Kyu—LSTuC4 Hossein-Zadeh, Mani—FThC4, FThU, Islam, Mohammed N.—SC326 Joseph, Joby—JWC6 Kasyanenko, Valeriy M.—LSWI2 Kimble, H. Jeff—JWD1 LSTuB3 Isoyan, Artak—FTuS2 Joseph, Shiju—FWY5 Kato, Koichi—FThE4 Kimerling, Lionel—AThC4 Howell, John C.—FMF8 Iturbe Castillo, Marcelo D.—JWC59 Joud, Fadwa—FThB4 Katz, Barak—FThR2 Kimori, Spencer—JWC34 Hrdlička, Aleš—JWC18 Ivers, Kevin M.—JTuC1 Jovanovic, N.—LMTuC1 Katz, David F.—JWC75 King, Jason K.—FWM4 Hsiao, Hsien-kai—FMJ1 Iwan, Bianca—LSThA3 Ju, Jung Jin—JWC11 Katz, Ori—FMK3, FThX3 King, Newton—JWC13 Hsu, Keng H.—AThA5 Izatt, Joseph—FThQ4 Judge, Alexander C.—FTuD4, FTuR5 Kaul, Rakesh—JWC12 Kinkhabwala, Anika A.—FMH2 Hu, Dongxia—JTuC5 Juette, Manuel F.—LSThB2 Kawakita, Masahiro—FTuF3 Kinowski, Christophe—AThC3 Hu, Honghua—LSTuG2 Jack, Barry—CTuC2, JTuB4, JWD4 Jundt, Dieter H.—AWC2, AWC4 Kawamura, Seiji—JTuA5 Kinto Ramírez, Héctor—JWC55 Hu, Juejun—AThC4 Jackson, Kate—AOTuB2 Jung, Sang-Chul—JTuC13 Kawate, Adin—JWC28 Kippenberg, Tobias J.—LSTuK2 Hu, Pin-Hao—JTuC8, JWC1 Jacobson, Stephen C.—LSMC, LSMG5 Juodawlkis, Paul W.—FWL2 Kazansky, Peter—AWB4 Kir’yanov, Alexander V.—FTuD3 Hu, Yi—FThI3 Jacques, Steven L.—FME4 Juodkazis, Saulius—LMTuB1 Kazmi, S. M . Shams—FME2 Kiraz, Alper—FThU6, FThU7 Hua, Hong—FTuA Jagtap, Vishal S.—FTuO6 Kazovsky, Leonid—FMD, FTuC1 Kirby, Andrew K.—FTuM2 Huang, Juanfeng—JTuC11 Jain, S. C.—FWG6 Kachkovski, Alexei D.—LSTuG2 Kearney, David—AOThB2 Kirk, Jay—FThE6 Huang, Simon—JWC29 James, Daniel F. V.—FWU5 Kagawa, Keiichiro—CWB1 Keating, Christopher S.—LSWI2 Kirschbaum, Stefanie E. K.—LSThB2 Huang, Sumei—LSTuB4, LSTuK3 Jamula, Lindsey—LSTuC4 Kahen, Keith—LSTuJ4 Kellerer, Aglae—AOTuA5 Kishore, Rani—JWC60 Huang, Xiaojun—FTuK4, JTuC5 Jana, Sunirmal—AWA4 Kahn, Joseph—FTuP3 Kelley, Anne M.—LSWE, LSWH2 Kisilak, Marsha L.—FTuQ4 Huang, Yingyan—FThC5, FThE3, FThK3, Jankevics, Andrew—AOThC4, FThD2 Kahr, Bart—LSMB, LSMF1 Kelly, Kevin—CThC6, CTuA5, FWB Kissick, David—LSMF2 FThK5, FThO4, FTuB4, FWN2, Janssen, Peter—FMG, FTuR1, FWD Kaindl, Robert A.—LSWJ3 Kewish, Cameron M.—FThT1, LSTuL4 Kitur, J. K.—FTuB5 JWC53 Javaloyes, J.—LSTuI4 Kaiser, Jozef—JTuC12, JWC18, JWC19 Khajavikhan, Mercedeh—FThD3 Kivshar, Yuri S.—FThI1 Huber, Günter—LMTuC2 Javidi, Bahram—FTuF1, FTuM Kaiser, Robin—FMC1 Khaled, Elsayed Esam M.—FWU6 Kizek, René—JWC19 Huber, Robert—FWO4 Jen, Alex—FThE3 Kajiyama, Maria Claudia C.—AWC2 Khalil, Munira—LSTuC3, LSWC, LSWF Kjoller, K.—FMK2 Hubert, Zoltan—AOTuA5 Jeon, Tae-In—JWC26 Kakur, Pawan—FTuE6 Khaydarov, John—LSWK4 Klapp, Iftach—CWB3, STuA7 Hughes, William L.—FWC2 Jesacher, Alexander—AOThC3 Kalasuwan, Pruet—FMG1 Khazanov, Efim—LSWK3 Kley, Ernst-Bernhard—FThC3, FThC6 Huldt, Gösta—LSThA3 Jessup, Malcolm—JWC13 Kalinowski, Ksawery—FThI1 Khilo, N.—FThB6 Klimentov, Sergey M.—FTuD3 Humble, Travis—JMA4 Jevsevar, Kristen L.—JWC68 Kalinski, Matt K.—LSTuL2 Khoo, Eng-Huat—FThO4 Klimov, Victor I.—LSTuG7
156 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 • October 11–15, 2009 Kluzik, Raphael—JTuA2 Kudlinski, A.—FWD1 Lancry, Matthieu—AWB2, AWB4, Leniec, Monika—FThB5 Lin, Chien-I—FWP2 Knauer, M. C.—FWV1 Kuhlicke, Alexander—FWE4 JTuC16, LMTuA5 Leon, Erich De—FME7 Lin, Hong—JWC33 Knez, Mato—AThB3 Kuhlmann, Marion—LSThA3 Landers, Frank—AOThC4 Leone, Stephen R.—LSTuL3 Lin, Kung-Hsuan—JWC82 Key to Authors Knight, Jonathan—AThC, AThD1, FTuD, Kuhlmey, Boris T.—FTuD4, FTuR5 Landry, James P.—FTuY4 Le Roux, Brice—AOTuB3 Lin, Po-Heng—JWC82 FWF1 Kuhn, A.—LSTuK1 Langrock, Carsten—AWC2 Lester, Luke F.—FMB4, FMB5, FThK1, Lin, Shie-Hen—JWC5 Knoernschild, Caleb—FWR4 Kularatne, Sumith A.—FTuL3 Langston, Peter—FThS7 LSTuA7 Lin, Yu-Ting—AWB1 Knowlton, William B.—FWC2 Kulcsár, Caroline—AOThA2, AOWB1, Lanyon, B. P.—JWD3 Levene, Michael J.—FThP5, FTuL, Lin, Yang-Cheng—JWC1 Knünz, S—LSTuB1 AOWB4 Lanzara, Alessandra—LSWJ3 FTuY6, FWA4, FWA5 Lin, Ziliang—JWE5 Ko, Nak-Hoon—JTuC13 Kulhandjian, H.—FTuE5 Lardenois, S.—FTuW1 Levi, A. F. J.—LSTuA6 Lin, Zhiwei—LSWI2 Kobilka, Brian K.—JWC16 Kulikov, Kirill—JWC65 Lardière, Olivier—AOTuB2 Levin, Anat—FThR, FThX1 Lindblom, M.—FThA4 Koch, Karl W.—FWF3 Kumar, Anil—AThA5 Larin, Kirill—FThV2, SC340 Levin, Carly—JWC60 Linzon, Yoav—FThF6 Kohlgraf-Owens, Dana C.—CThC1 Kumar, Amrinder—FThN3 Larina, Irina V.—FThV2 Levina, Larissa—FThS5 Lipovskii, Andrey A.—AThC5 Kohlgraf-Owens, Thomas—CWA4, Kumar, Arun—FThW6, JWC40 Lasser, H.—FThM3 Levitt, Jonathan M.—FMK3 Lipson, Michal—FTuW3, FWY3 CWA5 Kumar, Prem—FMG, FWJ5, LSWB3 Latas, Sofia C. V.—FThI5 Levoy, Marc—JWA3 Liška, Miroslav—JWC18, JWC19 Kohli, Meenakshi—JWC25 Kumar, Ranjeet—JWC62 Laux, E.—FWP4 Levy, Ronen—FMJ8 Litchinitser, Natalia M.—FTuE5 Kolehmainen, Ville P.—STuA2 Kumar, T. K. S.—JWC66 Lawall, John R.—FWI2 Lew, Matthew—CThA4, CTuD1 Little, D. J.—LMTuC1 Kolis, Joseph W.—AWC1 Kumaran, Raveen—AWC5 LCGT Collaboration—JTuA5 Lewis, Steffan A. E.—FWE3 Littlejohn, David—LSMG3 Kolodzey, James—AWA5 Kumaran Nair Valsala Devi, Adarsh— Leach, Jonathan—CTuC2, JTuB4, JWD4 Li, Chun-Fang—FTuX3, FWH5 Litvinov, Rudol’ph—AThB4 Komarala, Vamsi K.—FWB7 LSTuG4 Le Blanc, Catherine—FMI2 Li, Chaohong—JTuC1 Liu, Boyang—FThE3, FThK3, FThO4 Komatsu, Shinichi—JWC49, JWC52 Kundu, Susmita—AWA4 Leblond, Herve—FThI4 Li, Er-Ping—FThO4 Liu, Chian—FThM2 Komine, Hiroshi—FThD2 Kuo, Bill Ping Piu—FWK2 Lederer, Falk—FMA3 Li, Guoqiang—FTuH1, FTuO Liu, Chongyang—FWN2 Kondratenko, V. V.—FTuZ2 Kupke, Renate—AOTuA4 Lee, Byoung-Su—FWE5 Li, H.—FTuN5 Liu, Chien-Sheng—JWC82 Koo, S. M.—FWC3 Kuramochi, E.—FWV2 Lee, Byoungho—JWC54 Li, Hongpu—FWK5 Liu, Huikan—FMA6 Koopmans, Bert—LSWJ2 Kuranov, Roman—FThP6 Lee, Chee Wei—FThK3 Li, Jieda—FThE6 Liu, Jun—FThE3 Korkiakoski, Visa—AOTuD1 Kurdyukov, Vladimir V.—LSTuG2 Lee, Chang-Hee—FTuP1, FTuP2 Li, Jensen—FTuN2 Liu, Ling—JWA4 Korotkova, Olga—FTuG1, FTuG3, FTuU Kurz, Nathan—JTuB5, JTuB6 Lee, Dongjoo—JWC17 Li, Jingjing—FWC5, FWT6 Liu, Na—LSWD2 Korth, William Z.—JTuA4 Kuzin, Evgeny A.—FThD4 Lee, El-Hang—JTuC13 Li, Kaccie Y.—FWX1 Liu, Rui—FWS2 Koshel, R. John—FWR Kuzucu, Onur—FTuW3 Lee, Eui Su—JWC26 Li, Qin—JWC15 Liu, Shuangqiang—FWL6 Kost, Alan—FMB Kwiat, Paul G.—FThN4, JMA3, JTuB, Lee, Hak-Soon—FMJ6 Li, Rui—FML6 Liu, Sheng—JWC32 Kostuk, Raymond K.—FMB3, FME7 JWE1 Lee, Hong-Shik—FWE5 Li, Wei—AWC5 Liu, Wenjun—FThM2 Kottos, Tsampikos—FMC, FTuJ1 Kwiecien, Pavel—FTuO7 Lee, Hsiao-lu D.—CTuD1, LSWD2 Li, Wen—LSTuI3 Liu, Weiming—FTuX3 Kovanis, Vassilios—LSTuA7 Kwon, Min-Suk—FThW4 Lee, Joyce—FMF4 Li, Xin—FMF3 Liu, Xue—FThV3, FTuH2 Kracht, Dietmar—JTuA2 Kyoung, J. S.—FWC3 Lee, Jin-Hyoung—FTuN4 Li, Xiangyu—FThO4 Liu, Zhijun—FWZ4 Krajcarová, Lucie—JTuC12, JWC19 Lee, Jeunghoon—FWC2 Li, Yan—FThK1 Liu, Zhongqiang—JWC76 Kranitzky, C.—FWV1 Laage, Damien—LSWF1 Lee, Jonathan Y.—FML4 Li, Zhiyong—FWT6 Lo, Victor L.—STuB2 Krapf, Diego—JWC68, LSWD3 Lahini, Yoav—FMC2, FMG4, FWD3 Lee, Kyu Jin—JWC44, JWC56, JWC57 Liang, Yan—LSThB1 Lock, Robynne—LSTuI3 Krauskopf, Bernd—FThO6 Lahiri, Mayukh—FWH2, FWU4 Lee, Marissa K.—LSWD2 Liapis, Andreas C.—FMA2 Loh, Ter-Hoe—JWC53 Krauss, Todd—LSTuJ4 Lai, Changyi—AThC2 Lee, Sang Shin—FMD7 Lidke, Diane S.—LSThF2 Lõhmus, Madis—FTuO5 Krausz, Ferenc—FTuK3 Lai, Yicheng—FThK3, FThK5 Lee, Sang-Shin—FMJ6, FWE5 Lienau, Christoph—FMH, FWP1 Lombard, E.—FWP4 Kreisler, Alain J.—FTuO6 Laing, Anthony—FMG1 Lee, Soonil—FWC1 Lifshitz, Efrat—LSMC3 London, Richard A.—LSThA3 Kretzschmar, Ilona—AThA4 Lakshminarayanan, Vasudevan—JWC79, Lee, Seung Gol—JTuC13 LiKamWa, Patrick—FTuE1 Longmore, Andy—AOTuA5 Krishnamurthy, Subramanian—LSWB3 JWC81 Lee, Wan-Gyu—FMJ6 Lim, Boo-Taek—FMJ6 Loomis, Nick—FThB1 Krishnamurthy, Vivek—FThC5 Laluet, J.-Y.—FWP4 Lee, Yoo Seung—FMD7 Lim, Hwan Hong—FTuO3, JWC11 Looze, Douglas P.—AOThB3 Krishnan, S.—FME1 Lam, Edmund Y.—STuA4 Lee, Yoon-Suk—JTuC13 Lim, Sehoon—CThA6 Lopez-Cortes, Daniel—JWC41 Krol, Denise M.—LMTuB4, LMTuC4 Lam, Kit S.—FTuY4 Leger, James R.—CThA1, FThD3 Lim, Yongjun—JWC54 López-Mariscal, Carlos—FWM, FWS5 Krolikowski, Wieslaw—FThI1 Lambert, Andrew J.—STuB, STuC2, Lehnert, Konrad W.—LSTuE3 Lima, Francinete—FTuX4 Lopez-Santiago, Alejandra—AThB2 Krous, Erik—FThS7 STuC4, STuC7 Leigh, Matthew A.—JWC28 Limouse, Charles—LSWD4 Lord, Samuel J.—CTuD1, LSWD2 Kuang, Wan—FMJ, FWC2 Lamhot, Yuval—LSMC3 LeLouarn, Miska—AOThB, AOTuD3 Limpert, Jens—FThJ4 Lou, Cibo—FThI3 Kubala, Kenny—CWA Lan, Tzu-Hsiang—FWT4 Lencina, Alberto—JWC83 Lin, Chang-Yi—FThK1 Lou, Qihong—FThD1
FiO/LS/AO/AIOM/COSI/LM/SRS 2009 • October 11–15, 2009 157 Louradour, Frederic—FWI5 Mahou, Pierre—FWJ3 Mathieu, François—FMI2 Méndez Otero, Maribel M.—JWC59 Mochi, Iacopo—FThT2 Louri, Ahmed—FWL5 Maia, Filipe R. N. C.—LSThA3 Matsko, Andrey B.—FThC1 Mendlovic, David—CWB3, STuA7 Mochrie, Simon—LSThC2 Love, Gordon D.—FTuM2 Maier, Stefan A.—FTuB6, SC324 Matson, Charles L.—SWA Menezes, Leonardo de S.—AThC5 Moerner, W. E.—CThA4, CTuD1, FMH2, Low, Philip S.—FTuL3 Maikisch, Jonathan S.—FMJ4 Matsukevich, Dzmitry N.—JWD6 Menon, Rajesh—FThA2 FWM2, JWC16, LSTuF3, LSWA1, Lozhkarev, Vladimir—LSWK3 Maire, Jérôme—AOTuC4 Matthews, Dennis—FWS2 Menon, Vinod M.—AThA4 LSWA4, LSWD2 Lozovoy, Vadim V.—FMF7, LMTuA4, Mait, Joseph N.—CThA, CTuA3 Matthews, Jonathan C. F..—FMG1 Menoni, Carmen S.—FThS7, FTuS2, Mohnkern, Lee—AWA2 LSWI3 Majumdar, Arka—FWB5, LSTuD4 Maunz, Peter—JWD6 FTuZ2 Mohseni, M.—JWD3 Lu, Y. F.—LMTuD2 Makarov, Nikolay S.—JTuC14 Maurya, Mahendra K.—JWC45 Menzel, Andreas—FThT1, LSTuL4 Mokhov, Sergiy V.—FMF2, FWX5 Lucero, Erik—JMA1 Makarova, Maria—FML6 Mavalvala, Nergis—LSTuB, LSTuH3 Menzel, Christoph—FMA3 Molinelli, C.—LSTuK1
Key to Authors Key Luchansky, Matthew S.—LSMC1 Makhlouf, Houssine—FWR2 Max, Claire E.—AOTuA4 Merano, M.—FMF5 Möller, Thomas—LSThA3 Luckasevic, Kelly M.—JWC76 Malacara-Hernández, Daniel—JWF4 Maxwell, G. D.—FTuW1 Merigan, William H.—FTuQ2 Momeni, Babak—FTuB7, FWZ2 Lugani, Jasleen—FWJ2 Maleki, Lute—FThC1 May-Arrioja, Daniel A.—FTuD6, FTuD6, Merino, David—FWX1, JWB2 Monken, Carlos H.—JMA6 Lukofsky, David—FThS3 Malina, Radomír—JTuC12, JWC18 FTuE1, JWC41 Mertz, Jerome—FWA2 Monnier, John D.—FMJ1 Lumeau, Julien—FMF2 Malomed, Boris A.—FThF6 Maylin, Matthew I. S.—STuB5 Messersmith, Phillip B.—FTuL4, JWC76 Monro, Tanya—FTuE3 Lumsdaine, Andrew—CTuB3, STuA6 Mance, Jason—LSTuG3 Mazur, Eric—AWB1, FWA1, LMTuA, Mestre, Michael—FThU6, FThU7 Monroe, Christopher—JWD6 Lundeen, Jeffrey S.—FWJ3 Mandridis, Dimitrios—FMD2, FWL1, LMTuDP Metcalfe, Michael B.—FWI2 Montera, Dennis—AOTuA1 Luna, Carlos E.—STuC1 FWL2, FWX4 McCarthy, Nathalie—JTuC15, JWC73 Metha, Andrew B.—JWB5 Mookherjea, S.—FML2 Lundström, U.—FThA4 Mangalaraja, R. V.—LSTuG6 McClellan, Michael—FThD2 Meunier, Jean-Pierre—JWC40 Moon, Han Seb—JWC11 Luo, Jingdong—FThE3 Manning, R. J.—FTuW1 McCusker, James—LSTuC4 Meystre, Pierre—LSTuE1, LSTuH Moon, Jin-Young—FWC1 Luo, Juntao—FTuY4 Mansano, Ronaldo D.—JWC4 McCusker, Kevin T.—JMA3 Mezentsev, Vladimir—JTuC19, LMTuA6, Moore, Nicole J.—FWH1 Luo, Xuan—CTuC3 Manson, Neil B.—LSTuD3 McDowell, Emily—FWS4 LMTuC6 Moore, Richard O.—FTuR3 Luo, Yuan—FME7 Manuel, Anastacia M.—FThH3 McEldowney, Scott—FThF1, FThL Mezosi, G.—LSTuI4 Morandotti, Roberto—FMC2, FMG4, Lurçon, Jean-Marie—AOThD3 Marc, Sorel—FMC2 McFarlane, Michelle—JWC78 Miao, Jianwei—LSThE1 FThF6, FWD3 Luther, B. M.—FTuZ2 Marchesini, Stefano—LSThA3 McGuire, James P.—FTuT3 Michalache, Dumitru—FThI4 Moreno, M.—FThI6 Luther-Davies, Barry—FThE5 Marciante, John R.—FThD5, FThJ2, McHale, Kevin—LSWD4 Migacz, Justin—FWR4 Morgan, Jessica I. W.—FTuQ2 Luzinov, Igor—AThC4 FTuD5 McInerney, John G.—FThJ3, FThK6 Mihailov, Stephen—FTuD7, FTuE2 Morin, Pierre—AOThD3 Lynch, Candace—AWA1, AWD Marconi, Mario C.—FTuS2, FTuZ2 McKinney, Wayne R.—FThT2 Mikaberidze, Alexey—LSTuI1 Moritz, Tobias—FWS2 Lynn, David G.—LSThB1 Marcos, Susana—JWB4 McKinstrie, Colin J.—FTuR Mikhnov, Sergej—AThB4 Moro, Slaven—FTuD2 Marcus, Rudolph A.—LSTuJ1 McMillan, James F.—FML5 Milanfar, Peyman—JWA2 Morris, Tim—AOTuA5, JTuC4 Ma, Guohong—FTuX3 Marega Jr, Euclydes—JWC4 McMillen, Colin D.—AWC1 Milián, Carles—FWP3 Morrison, Gregory—FThT2 Ma, Hyungjin—FWB6 Marin, Emmanuel—JWC40 McNally, Jim—FThG1 Millane, Rick P.—STuB2, STuC Morrissey, F. X.—LSTuG3 Ma, Jing—FThF5 Markosyan, A.—FThS7 McNaught, Stuart J.—FThD2, FThJ Miller, Darren—FThF4 Morrissey, Michael J.—FMG3, FThC2 Ma, Lijun—JMA5 Marks, Daniel L.—CThA5, CThA6, McNeil, Michael R.—JWC68 Miller, David A. B.—CTuC1 Morse, Theodore F.—AThD4 Ma, Li L.—FThP6 CTuA6 McNulty, Ian—FThA Miller, Donald T.—AOThA, JWF3 Mortier, Michel—FThO3 Ma, Ren-Min—FTuB2 Marks, Tobin J.—FThE3 McPhedran, Ross C.—FWF5 Millot, G.—FWD1 Mosallaei, Hossein—FTuV3, FTuV4 Mabuchi, Hideo—LSWD4 Marmo, Jay—FThD2 Measor, Philip—FMJ7 Milner, Thomas E.—FThP6 Moses, Edward I.—FTuK1 Maccagnano-Zacher, Sara—LSTuJ4 Marques, Paulo V. S.—LMTuC5 Medic, Milja—FWJ5 Milojkovic, Predrag—CTuB4 Moshchalkov, Victor—FTuB6 MacFarlane, Duncan—FWR3, JWC9 Marshall, G. D.—LMTuC1 Meech, S. R.—FMK2 Min, Changjun—FThW5 Mosk, Allard P.—FTuU2, FWF4, FWS6 Machan, Jason—FThD2 Marteaud, Michel—AOTuA5 Meehan, Alaster J.—JWB5 Mironov, Sergey—LSWK3 Mouillet, David—AOTuC3 Mackey, Ruth—AOTuB4 Martin, Michael C.—LSWJ3 Mehta, Dalip S.—JWC62 Misawa, Hiroaki—LMTuB1 Moulton, Peter—AWB Madden, Steve—FThE5 Martín, Virginia—LSWG4 Mehta, Gaurav—FTuE5 Mishra, Vinod—FThN3 Mouradian, Levon—FWI5 Madec, Pierre-Yves—AOTuD3 Martinez, Patrice—AOTuC2 Mehta, Monal R.—FMK7 Mishra, Vandana—FWG6 Mourou, Gérard—FMI2 Mafi, Arash—FThW, FWF3, JWC38 Martinez-Corral, Manuel—FTuF1 Mehta, Shalin B.—FMK6, SWA4 Misra, Kamakhya P.—AWA6 Moustakas, Theodore D.—FMH4 Mägi, Eric C.—FTuD4, FTuR5 Martínez-Niconoff, Gabriel—JWC2 Meiselman, Seth—LSTuA2 Mitchell, M.—LMTuD2 Mozharov, Sergey—LSMG3 Magnusson, Robert—FTuH4, FTuY1, Martinez Vazquez, R.—LMTuC3 Mel’nikov, Igor V.—FThI4, FTuD3 Mitra, Anirban—FTuL2 Mudrakola, Harsha V.—LSThB3 FWI3, JWC44, JWC56, JWC57 Martini, Giuseppe—FWG5 Mele, Elisa—FThO1 Mitra, Arnab—JWC30 Mueller, Guido—JMB3, JTuA4 Mahalanobis, Abhijit—CWA5 Martinis, John—JMA1 Melis, Anastasios—FMB2 Mittleman, Daniel M.—STuA4 Mugnier, Laurent—AOTuC3 Mahjouri-Samani, M.—LMTuD2 Masajada, Jan—FThB5 Mencer, Oskar—AOThB2 Miyoshi, Norio—JWC74 Mukhamedgalieva, Anel F.—FThS6 Mahler, Tom—FMC6 Maser, Jörg—FThM4 Méndez, Cruz—JWC10, LSWB4 Mlodzianoski, Michael J.—LSThB2 Mukherjee, Jayanta—FThJ3
158 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 • October 11–15, 2009 Mullen, Klaus—FMH2 Nguyen, Dat—FWX4 Ohnuki, Masayuki—FThF4 Parekh, Devang—FTuW2, FWL3 Peyghambarian, Nasser—AThB2, FTuT1 Muller, Matthew S.—FME5, FThQ2 Nic Chormaic, Sile—FMG3, FThC2 Ohta, Jun—FMD4 Park, Doo-Jae—FWC1 Pfeiffer, Franz—FThT1, LSTuL4 Müller, Waltraud—FThG1 Nichols, Geoffrey—STuC4 Ojeda-Castañeda, Jorge—FWQ3 Park, H. R.—FWC3 Pfrommer, Thomas—AOTuA2 Key to Authors Mulvihill, Alex—JWC46 Nicolodelli, Gustavo—JTuC20 Oka, Kazuhiko—FThF4 Park, J.—FME1 Phillips, Brian S.—FMJ7 Mun, Sil-Gu—FTuP2 Nielsen, Martin M.—LSTuC2 Okano, Fumio—FTuF3 Park, Jongchul—FTuJ3 Phillips, Chris R.—AWC2 Munday, Jeremy—LSTuH2 Niinimäki, Kati—STuA2 Okawachi, Yoshitomo—FTuW3 Park, Junghyun—JWC54 Phillips, Nathaniel B.—FThI, FThS2 Muradoglu, Metin—FThU7 Nilsson, D.—FThA4 Okhrimchuk, Andrey G.—JTuC19, Park, J. S.—FML2 Phipps, M. Lisa—LSThF2 Murakami, Yoshihisa—JWC22 Nilsson, Josefin—JWC78 LMTuA6 Park, N. K.—FWC3 Piché, Michel—JTuC15 Murnane, Margaret M.—FTuZ1, LSTuI3 Ning, Yongqiang—JWC15 Oliveira, Juliano R. F.—FTuC4 Park, Se-Geun—JTuC13 Picozzi, A.—FWD1 Murphy, Thomas E.—FTuI2 Nishida, Yoshiki—JWE2 Oliveira, Luciane F.—AThA3 Park, Sungnam—LSWF3 Piestun, Rafael—CThD, CTuD1, CTuD2, Murphy, Timothy O.—JWC28 Nishii, Junji—AThC1 Oliveira, Sergio C.—FWT3 Park, Won—FTuN4 CTuD3, FMK5, JWA, LMTuB3 Murshid, Syed H.—FTuP5, JWC50, Nitkowski, Arthur—FWY3 Oliveira, Tâmara R.—FThS1 Parra, Sonia—FWA5 Piksarv, Peeter—FTuO5 LSTuF2 Nkenke, Emeka—FThP2 Olmschenk, Steven—JWD6 Parthasarathy, Ashwin—FME2 Pinkse, Pepijn W. H.—FWF4 Musser, Joseph A.—FWR5, FWX3 Noad, Julian—FTuW4 Olson, Eben—FTuY6 Patchkovskii, Serguei—LSTuI3 Piracha, Mohammad Umar—FWX4 Muyo, Gonzalo D.—FThX2 Noda, Toshihiko—FMD4 Olvera-Santamaría, Miguel A.—JWC2 Pate, Dinesh—FThS7 Pires, Henrique D. L.—JMA6 Myers, Richard M.—AOTuA, AOTuA5, Noek, Rachel—FWR4 Orenstein, Meir—FMG6, FMH3, JWD5 Patel, Darayas N.—JWC13 Pisignano, Dario—FThO1, LMTuB2 AOTuD4, JTuC4 Noginov, M. A.—FTuB5, FTuN5 Orszag, Miguel—JWE6 Patel, Monika—FWJ5 Plant, Jason J.—FWL2 Myneni, Vimeetha—CThC4 Noh, Jong Wook—FMJ2 Orth, Antony—FTuH3 Pauca, Paul—CThB2 Plascencia-Mora, Hector—JWC67 Myslivets, Evgeny—FWK2 Nootz, Gero—FThS5 Osellame, R.—LMTuC3 Paufique, Jerome—AOTuD3 Platonenko, Victor T.—LSMH4 Nordin, Gregory P.—FMJ2 Ostendorf, Andreas—LMTuD, LMTuDP Paul, Thomas—FMA3 Plönjes, Elke—LSThA3 Naderi, Nader A.—LSTuA7 Nordlander, Peter—FTuB6 Österberg, Ulf—FThS3 Pavani, Sri Rama Prasanna—CTuD1, Pochet, Michael C.—LSTuA7 Naderian, Azadeh—JWF2 Nordon, Alison—LSMG3 Ostrovsky, Andrey S.—JWC2 CTuD2, FMK5 Podolskiy, V. A.—FTuB5 Nadler, Brett R.—FWG2 Norfolk, Andrew W.—FThI2 Ostrowsky, Dan—FWJ2 Payne, Ben—FMC3, FMC6 Pogorelsky, Igor—LSMH4 Nagasono, M.—LSMH1 Northcott, Malcolm—AOThD O’Sullivan, Joseph A.—CThB5 Payne, Christine—LSThF1, LSWA Politi, Alberto—FMG1 Najdek, David—FWS3 Norton, Andrew—JTuC3 Otendal, M—FThA4 Payne, J. D.—FME1 Pollak, Thomas M.—AWA2, AWA3 Nalawade, Sandipan—JWC37 Norwood, Robert A.—AThB2 Ou, Fang—FThE3, FThO4 Peceli, Davorin—LSTuG2 Polo, Marco—LMTuB2 Narasimhan, Srinivasa—CTuD5 Notomi, Masaya—FWV2 Ou, Haiyan—FThE1 Pedaci, F.—FTuZ2 Polyanskiy, Mikhail N.—LSMH4 Narducci, Francesco A.—LSTuA1, Novikova, Irina—FThS2 Oulton, Rupert F.—FTuB2 Pedersen, Christian—FThR6 Pomeranz, Leonard A.—AWA3 LSTuA2, LSTuI5 Novotný, Filip—AThA2 Ozdur, Ibrahim—FMD5, FWL1, FWL2, Peetrig, Benno L.—FThQ2 Ponomareko, A. G.—FTuZ2 Narimanov, E. E.—FTuN5 Novotný, Jan—JTuC12, JWC18 FWX4 Peña, Abe—FMC5 Ponticorvo, Adrien—FME2 Nataraj, Latha—AWA5 Novotný, Karel—JTuC12, JWC18, JWC19 Ozharar, Sarper—FWL1, FWX4 Penson, Shawn—AWC5 Porter, Jason—FThQ3, JTuC1 Natarajan, S. R.—LMTuC6 Novotny, Lukas—FTuL2 Perry, John M.—LSMG5 Potma, Eric Olaf—FMK1 Nath, Asish Kumar—JWC12 Nugent, Keith A.—JWB5 Padgett, Miles—CTuC2, JTuB4, JWD4 Perry, Susan—FTuY5 Pottiez, Olivier—FThD4 Ne-Te Loh, Duane—LSThA1 Numata, Hidetoshi—JWC39 Padhy, Bibhuti Bhushan—JWC37 Persano, Luana—FThO1 Poulin, Jean Claude—AWB2 Neeley, M.—JMA1 Nuñez Quintero, Jesus A.—JWC42 Padilha, Lazaro A.—FThS5, LSTuG2 Pertsch, Thomas—FMA3, FThC3, FThC6 Poumellec, Bertrand—AWB2, AWB4, Neifeld, Mark Allen—CThD, CTuA2, Nuzzo, Valeria—FWA1 Padmore, Howard A.—FThT2 Peruzzo, Alberto—FMG1 JTuC16, LMTuA5 CTuC Nývlt, Martin—FWS3, JWC64 Pagliara, Stefano—FThO1 Pervak, Vladimir—FTuK3 Poustie, A. J.—FTuW1 Nemet, Greg—LSWK4 Paiella, Roberto—FMA5, FMH4 Pestov, Dmitry—FMF7, LSWI3 Poutous, Menelaos—FTuO1 Nemirovsky, Yoni—LSMC3 O, Beom-Hoan—JTuC13 Paillard, Jean Luc—FMI2 Peteanu, Linda—LSTuG1 Povinelli, Michelle—FThF5 Neshev, Dragomir N.—FThI1 O’Brien, Jeremy—FMG1 Painter, Oskar J.—LSTuE2 Petek, Hrvoje—LSWG1, LSWJ Powell, B. J.—JWD3 Neto, Luiz G.—JWC4 O’Connell, A. D.—JMA1 Palombo, Nola J.—JWC33 Peterhänsel, S.—FWV1 Poyneer, Lisa—AOTuB, AOTuC4, Neumann, Joerg—JTuA2 O’Connor, Shane—FMJ5 Palomino Ovando, Martha Alicia—JWC55 Petermann, Klaus—LMTuC2 AOWB2, JTuC3 Neves, Antonio A. R.—LMTuB2 Odelius, Michael—LSWF3 Pan, Xiaochuan—STuA1 Petersen, Paul Michael—JWC3 Pozzi, Francesca—FMC2 Nevet, Amir—FMG6, FMH3 Odoi, Michael Y.—LSTuJ2, LSTuJ3 Pandiyan, Krishnamoorthy—FTuO3 Petit, Cyril—AOThA2, AOWB1 Prasad, Sudhakar—CTuC3 Newhouse, Rebecca—FTuE4 Oh, K—FWE2 Pang, Lin—FWB1 Petit, Laeticia—AThC4 Prasada Rao, T—LSWG3 Newport, David—FWY5 Oh, Se Baek—CTuD4 Paniccia, Mario—FWN3, FWZ Petrig, Benno L.—FME5 Prater, C.—FMK2 Ng, Keh-Ting—JWC53 Oh, Sang-Min—FTuP2 Panoiu, Nicolae C.—FML5 Petroff, Pierre—FWB5 Preble, Stefan F.—FML3, FThU4 Ng, Wei-Ren—FWX2 O’Hara, John F.—FWO1 Pant, Ravi—FTuD4, FTuR5 Petrov, Nikolai I.—JWC8 Preston, Alix—JMB3 Nguyen, D—FThS7 O’Hara, Ken—LSTuA8 Paranjape, Amit S.—FThP6 Petschulat, Jörg—FMA3 Preza, Chrysanthe—CThB5, CThC4
FiO/LS/AO/AIOM/COSI/LM/SRS 2009 • October 11–15, 2009 159 Prieto, Camilo—JWC10 Rath, Shyama—JWC27 FThN5, FTuT3 Sampson, Philip C.—FWM4 Schmitt, Robert—FTuO4 Proška, Jan—AThA2 Rativa, Diego—JWC43, JWC77 Romero, Carolina—LSWB4 Samuel, Reichel—LSWD2 Schmitz, Holger—LMTuA6 Procházka, David—JTuC12, JWC18 Ravi, Koustuban—FThK5 Romero, Jacquiline—CTuC2, JTuB4, San Román, Julio—JWC10 Schneeberger, Timothy—AOTuA1 Przhonska, Olga V.—LSTuG2 Rawal, Swati—FTuX6 JWD4 Sánchez Sánchez, Mauro—JWC47 Schneider, Gerd—FThG1 Psaltis, Demitri—CThA2 Raynaud, Henri-François—AOThA2, Rong, Haisheng—FWN3 Sanchez-Mondragon, Jose J.—FTuD6, Schneider, Jochen R.—LSThA3 Ptasinski, Joanna—FWB1 AOWB1, AOWB4 Roorda, Austin—FThQ, FWX1, JWB2 JWC41 Schneider, Vitor M.—AThC2 Pu, Jixiong—FThX6 Rayner, D. M.—LMTuA1 Roppo, Vito—FThI1, FThW2, FTuS4 Sanchez-Mondragón, Javier J.—JWC67 Schnelle, Sebastian K.—FWM3 Pu, Minhao—FThE1 Reading, M. M.—FMK2 Rose, Volker—FThM4 Sandhu, Arvinder—LSTuI3 Schoeck, Matthias—AOThB1 Pueyo, Laurent—AOWA1 Reano, Ronald M.—FThE7 Rosen, Joseph—FThR2, FThX Sandoghdar, Vahid—LSTuD1 Schoenlein, Robert—LSTuC4
Key to Authors Key Puncken, Oliver—JTuA2 Rebane, Aleksander—JTuC14 Rosenblum, Serge—JWD5 Sandoz, Patrick—JWC70 Scholes, Gregory D.—LSWC2 Purohit, Gagandeep—JWC37 Reichman, Wilbur—LMTuC4 Roso, Luis—JWC10, LSWB4 Sank, D.—JMA1 Schonbrun, Ethan F.—FThB2, FTuH3, Puvanakrishnan, P.—FME1 Reid, Margaret D.—LSTuA4 Rossi, Vincent M.—FME4 Sankaranarayanan, Ramasubramanian— FTuY2 Reinspach, J.—FThA4 Rost, Jan-Michael—LSTuI1 JWC31 Schoonover, Robert W.—FWH3, FWH6 Qavi, Abraham J.—LSMC1 Reis, David A.—LSMD Roth, Zachary—FTuO1 Santhosh Kumar, M C.—LSWG3 Schotland, John—STuB1 Qi, Xiaofeng—JWF1 Reitze, David H.—FTuK, JTuA, JTuA4 Rotschild, Carmel—LSMC3 Santori, Charles—FThU1, FWJ4, LSTuD3 Schouten, Hugo F.—FWU2 Queener, Hope—JTuC1 Rekawa, Senajith B.—FThT2 Rouse, Andrew—FWR2 Santos, Cassio E. A.—AThA3 Schowengerdt, Brian—FTuM3, FTuT Quimby, Richard S.—AThD4 Ren, Xiaofan—LSTuJ4 Rousset, Gérard—AOTuA5, AOTuC3 Santra, Robin—LSTuI3 Schreiber, Thomas—FThJ4 Quinlan, Franklyn—FMD2, FWL1 Resch, Kevin J.—JWD Roussev, Rostislav V.—AWC3 Saraf, Meirav—LSMC3 Schulz, Timothy J.—CWA3 Quirin, Sean—CTuD3 Rey, Gilles—FMI2 Route, Roger K.—AWC2, AWC3, FThS7 Sarangan, Andrew—SC235 Schülzgen, Axel—FTuD1 Rha, Jungtae—JWF Rowan, Sheila—JTuA3 Sarepaka, Rama Gopal V.—FThN3 Schunemann, Peter G.—AWA2, AWA3, Rabien, Sebastian—AOTuA3 Rhee, Seuk-Joo—FTuN4 Roy Choudhury, Kaushik—LSTuA6 Sargent, Edward H.—FThS5 AWC Raday, Omri—FWN3 Rhodes, William T.—FWW1 Royon, Arnaud—AWB3 Sarkisov, Sergey—JWC13 Schwab, Keith—LSTuB2 Radic, Stojan—FML2, FTuD2, FTuI1, Rhyner, Steven J.—FTuF2 Ruan, Yinlan—FTuE3 Sasagawa, Kiyotaka—FMD4 Schwartz, Benjamin J.—LSWB2, LSWH FWK2 Ribak, Erez N.—AOThC5, AOTuB4 Rubinsztein-Dunlop, Halina—FWM3 Sass, Lauryn E.—LSThD3 Schwartz, J. A.—FME1 Rahman, Saad A.—AOThC3 Rice, J. H.—FMK2 Rubtsov, Grigory I.—LSWI2 Sastikumar, Dillibabu—JWC12 Schwefel, Harald G. L.—FThO2 Rai, Amit—FMG5 Rich, Wade—FThP3 Rubtsov, Igor V.—LSWI2 Sastre, Roberto—LSWG4 Schwesyg, Judith R.—AWC2 Raimond, J. M.—JWE4 Richardson, Kathleen—AThC4, AThD Rudolph, W—FThS7 Sato, Shinya—FTuC7 Scire, A.—LSTuI4 Raineri, Fabrice—FTuS4 Richardson, Martin—AThC4, AWB3, Rumpf, Raymond—FTuO1 Sauvage, Jean-François—AOTuC3 Scribner, Dean A.—CThC2 Raj, Rama—FTuS4 FTuS1, FTuZ Ruschin, Shlomo—FMJ8 Savchenkov, Anatoliy A.—FThC1 Seaman, Aden—FTuQ4 Rajalingam, Dakshinamurthy—JWC66 Richter, C.—FWV1 Russell, Laura—FMG3, FThC2 Sawides, Lucie—JWB4 Sears, Christopher—FTuK3 Rajan, Dinesh—CTuB4 Richter, Ivan—AThA2, FTuO7, FWC7 Russell, Philip S. J.—AThD3 Saykally, Richard J.—LSWB5 Segev, Mordechai—LSMC3, LSTuG4 Rajarajan, Petchimuthu—JWC12 Rickenstorff-Parrao, Carolina—JWC2 Rutkowska, Katarzyna A.—FThF6 Sayrin, C.—JWE4 Seibert, M. M.—LSThA3 Rajeev, P. P.—LMTuA1 Ritcey, Anna M.—JWF2 Ryan, Andrew T.—JMA7 Scalora, Michael—FThW2, FTuS4, FWC6 Seidel, David—FThC1 Rajeswaran, Manju—LSTuJ4 Ritsch-Marte, Monika—CTuC2, FTuU1, Schaake, Jason—JMA4 Seidelin, Jeppe D.—FThR6 Rakich, Andrew—FThH4 FWI Saalmann, Ulf—LSTuI1 Schaeffel, Frank—JWC80 Sendowski, Jacob—FWK3 Ram, Dole—FThN3 Rivenson, Yair—CTuA4 Saari, Peeter—FTuO5 Schaffer, Chris—LMTuB, LMTuDP Sensarn, S.—JMA2 Ramadan, Tarek A.—FWZ3 Rivera, Jose G.—JWC76 Saathoff, G.—LSTuB1 Scheeren, Carla W.—AThA3 Sension, Roseanne J.—LSWI4 Raman, Chandra—LSWD4 Robbe-Cristini, Odile—AThC3 Saavedra, Carlos—JWC63 Scherman, Michael S.—JWC68 Senz, Stephan—AThB3 Ramírez Martínez, Daysi—JWC59 Robert, Aymeric—LSThA, LSThC1 Saavedra, Genaro—FWW2 Scherz, Andreas—LSThE3 Seo, JaeTae—FWB4 Ramos Mendieta, Felipe—JWC55 Robinson, Dirk—CThB3, CTuC6 Saillard, Marc—STuD4 Scheuer, Jacob—FMJ3 Seo, M. A.—FWC3 Ramos-Gonzales, R. E.—FWF2 Robinson, Ian—LSThE2 Sakata, Hironobu—FThS4 Schlau-Cohen, G. S.—LSWC1 Shaddock, Daniel—JMB2 Ramponi, R.—LMTuC3 Robinson, Michael D.—CThB4 Sakdinawat, Anne—FThA3 Schlotter, W. F.—LSMH1 Shaffner, Thomas—JWC34 Randone, Enrico—FWG5 Rocca, Jorge J.—FTuS2, FTuZ2 Saleh, Bahaa E. A.—FWJ1 Schmid, Karl—FTuK3 Shah, Jay D.—LMTuA4 Rangarajan, Prasanna V.—CTuC4 Rockstuhl, Carsten—FMA3 Saleh, Mohammed F.—FWJ1 Schmid, Tobias—FThH4 Shah Hosseini, Ehsan—FWZ2 Ranitovic, Predrag—LSTuI3 Rodas, Maria—FMG1 Salem, Mohamed F.—FWU1 Schmidt, Carsten—FThC3, FThC6 Shaheen, Nicholas J.—FME6 Rao, Devulapalli V.—FThF3, FThV5 Rodrigo, José A.—STuD2, STuD3 Salem, Reza—FTuW3 Schmidt, Holger—FMJ7 Shahraam, Afshar V.—FTuE3 Rarity, John G.—FMG1 Rodriguez, Vincent—AWB3 Salit, Kenneth—LSWB3 Schmidt, Michael—FThP2 Shahriar, Selim M.—FThV3, FTuH2, Raskar, Ramesh—CTuA1, CTuB Rogers, Lachlan J.—LSTuD3 Salit, Mary—JTuA6, LSWB3 Schmidt, Markus A.—AThD3 JTuA6, LSWB3 Rasras, Mahmoud S.—FWN1 Rolland, Jannick P.—FThH4, FThN2, Saltiel, Solomon—FThI1 Schmidt, Regine—FMG3 Shainline, Jeffrey M.—FWZ4
160 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 • October 11–15, 2009 Shakher, Chandra—JWC62 Siebenmorgen, Jörg—LMTuC2 Soma, Venugopal Rao—JTuC17 Stoian, Razvan—LMTuA3 Tamkun, Michael M.—LSWD3 Shalaev, Vladimir—FTuN3 Siegel, David A.—LSWJ3 Somayaji, Manjunath—CWB5 Stolow, Albert—LSTuI3 Tamma, Vincenzo—FWI4 Shanthi, Michael S. L.—LSTuG6 Siemers, Troy J.—JWC34 Somorjai, Gabor A.—LSWB1 Stork, David G.—CThB1, CThB3 Tamma, Venkata A.—FTuN4 Key to Authors Shapira, Ofer—FTuX, FWE1 Silberberg, Yaron—FMC2, FMG4, FMK3, Song, Hahn Young—JWC56, JWC57 Stroebele, Stefan—AOTuD3 Tan, Dawn—AThB1 Shapiro, David A.—LSThA3 FThX3, FWD3 Song, Jung Hun—AThA4 Stürwald, Stephan—FTuO4 Tanabe, Setsuhisa—AWD1 Shapiro, Jeffrey H.—JWE3 Silcox, John—LSTuJ4 Song, Seok—JWC44, JWC56 Subramaniam, Vinod—FWS6 Tanabe, T.—FWV2 Sharma, Ginni—CTuD2 Siltanen, Samuli—STuA2 Sonnefraud, Yannick—FTuB6 Suck, Sarah—FThB4 Tanaka, Daiki—FWN4 Sharma, Pallavi—JWC66 Simmonds, Richard D.—AOWA2 Sooryakumar, R—FThE7 Suda, Ryosuke—FThF4 Tanaka, Kazuki—FTuE4 Sharma, Vandana—LSTuI3 Simpson, Garth J.—LSMF2, LSWB, Sooudi, Ehsan—FThK6 Sudeep, Pallikkara K.—LSTuJ2, LSTuJ3 Tananaev, Georgy—JWC8 Sharpe, Andrew W.—JWE2 LSWH1 Sorel, M.—LSTuI4 Sukhov, Sergey—CThC1, CWA1, CWA6, Tang, Hong X.—LSTuH4, LSTuK Shay, Lisa—JWC58 Simpson, Randy—FThD2 Sorgenfrei, F.—LSMH1 FWY4 Tang, Kuo-Chun—LSWI4 Shchegrov, Andrei—LSWK4 Singh, Amandeep—FThN3 Sorger, Volker J.—FTuB2 Sukhovatkin, Vladimir—FThS5 Tang, Lingling—FThU2 Shcherbakov, Alexandre S.—JWC47 Singh, Ganga Sharan—FThN3 Spanner, M.—LMTuA1 Sullivan, Amy C.—FThE Tang, Sing Hai—FTuX3 Shealy, David L.—FThH2 Singh, Kehar—JWC6 Spears, Kenneth G.—LSWI4 Summers, Christopher J.—FTuN4 Tang, Xiao—JMA5 Shemirani, Mahdieh—FTuP3 Singh, Nahar—FTuE6, FWG6 Spence, David J.—JWC14 Sun, Bo—FWY2 Tangermann-Gerk, Katja—FThP2 Shemo, David M.—FThF1 Singh, Narendra—JWC69 Spencer, John S.—JWC68 Sun, Can—FTuR4, FWD2, FWD6 Tanida, Jun—CWB1 Shen, Yuen-Ron—LSWE1 Singh, Surendra—JWC30, JWC66 Spiller, Eberhard—LSThA3 Sun, Lei—FTuD5 Taniyama, H.—FWV2 Sheng, Yunlong—FThB, FTuV1 Sinha, Kanupriya—FWJ2 Spinhirne, James—AOTuA1 Sun, Ting—CThC6, CTuA5 Tanner, David B.—JTuA4 Shenoy, M. R.—FTuE6, FWG6 Sinha, Ravindra K.—FTuX6 Spivey, Christopher—AOThC2 Sun, Xiankai—FTuX1 Tanzilli, Sebastian—FWJ2 Sheppard, Colin J. R.—FMK6, FThR4, Sinquin, Jean-Christophe—AOThD3 Sprenger, Benjamin—FThO2 Sun, Yung-Shin—FTuY4 Tassev, Vladimir—AWA1 LSWK5, SWA4 Sirbuly, Donald J.—FWR1 Squier, Jeff A.—FWH7 Sunahara, Roger K.—JWC16 Tatic-Lucic, Svetlana—FTuY5 Sher, Meng-Ju—AWB1 Siviloglou, Georgios A.—FMF4 Sredar, Nripun—JTuC1 Sussman, Dafna—FTuQ4 Tautz, Raphael—FTuK3 Sheridan, John T.—FWW1 Škereň, Marek—FWS3, JWC64 Srinivasan, Kartik—FMG2 Sustersic, Nathan—AWA5 Tavella, Franz—FTuK3 Sherwood, Gizelle A.—LSTuG1 Skipetrov, Sergey E.—FMC5, FTuJ4 Srinivasan, Pradeep—FTuO1 Sutton, Mark—LSThC3 Tavernarakis, A.—LSTuK1 Shestakov, Alexander—JTuC19 Skoglund, P.—FThA4 Srinivasarao, Mohan—LSMF3 Suwal, O. K.—FWC3 Taylor, Antoinette J.—FWO1 Shestov, Sergei—AThB4 Skryabin, Dmitry—FWD4 Sriram, Vinay B.—AOThB2 Suyama, Kengo—JWC52 Taylor, Douglas—FWS2 Shevchenko, Yanina—FTuV, FWT1 Slattery, Oliver—JMA5 Srivastava, Atul—AWA6 Svoboda, Jakub—JWC7 Tebaldi, Myrian—JWC83 Shi, Chao—FTuE4 Sliney, David—FTuQ1 Srivastava, Anchal—AWA6 Swaha Krishnamoorthy, Harish N.— Teich, Malvin C.—FWJ1 Shi, Jielong—FTuX3 Slominsky, Yurii L.—LSTuG2 Srivastava, Triranjita—FThW6 AThA4 Terry, Neil—FME6 Shi, Zhimin—FMA2, FWC Slutsky, Boris—FWB1 Staforelli, Juan P.—JWC63 Swartzlander, Jr., Grover A.—FTuG2 Terry, Nathan B.—LSTuA7 Shields, Andrew J.—JWE2 Small, Eran—FWD3 Staliunas, Kestutis—FThI1 Swedov, Igor M.—FThS6 Tessier, Gilles—FThB4 Shih, Min-Hsiung—FWC2 Smelser, Christopher W.—FTuD7, FTuE2 Starkey, Jean—JTuC14 Szameit, Alexander—LSMC3 Tessieres, Régis—FThH3 Shih, Yanhua—FWI4 Smestad, Greg. P.—FMB1 Starling, David J.—FMF8 Szeghalmi, Adriana—AThB3 Testorf, Markus— CTuB2, FWQ, STuA, Shinn, M.—FThS7 Smirnov, Vadim—FMF2, FWX5 Stay, Justin L.—FTuX5 Szöke, Abraham—LSThA3 STuD4 Shivanand,—FMA6 Smith, Brian J.—FWJ3 Stefanov, Andre—FMG1 Teufel, John D.—LSTuE3 Shokooh-Saremi, Mehrdad—FTuH4, Smith, Barbara S.—JWC68 Steier, William H.—FMD7 Tabernero, Juan—JWC80 Thakur, Harneet—JWC37 FWI3 Smithson, Robert L.—FTuF2 Steinberg, Ben Z.—FMJ3 Tabibi, Bagher—FWB4 Thanthvari, Sulakshana—LSTuA3 Sholokhov, Evgeny—JTuC19 Smulakovsky, Vladimir—FWD5 Steiner, Jason—FWR1 Tadanaga, Osamu—JWE2 Thapa, Damber—JWC81 Shostka, Nataliya V.—JWC61 Snigirev, Anatoly—FThG2 Steinvurzel, Paul—FTuY2 Tahara, Tahei—LSWG2 Thériault, Gabrielle—JWC73 Shostka, Vladimir I.—JWC61 So, Peter T. C.—LSWK5 Stelzle, Florian—FThP2 Tahtali, Murat—STuC2 Thibault, Pierre—FThT1, LSTuL4 Shreve, Andrew P.—LSTuG1 Sobhani, Heidar—FTuB6 Stepanov, Serguei—JWC36, JWC42 Taira, Yoichi—JWC39 Thibault, Simon—JWF2 Shu, Deming—FThM2 Soghomonyan, Suren—LSWK4 Stephenson, Gregory B.—FThM4 Takahashi, Hiroshi—FThE4 Thibos, Larry N.—JWB1 Shu, Gang—JTuB5, JTuB6 Soh, Yeng Chai—FWP5 Stern, Adrian—CTuA4, FTuF1 Takesue, Hiroki—JWE2 Thiess, Helge—FThM3 Shubochkin, Roman L.—AThD4 Sokolov, Alexei V.—FMK4 Sterpone, Fabio—LSWF1 Takeyama, Norihide—JWC22 Thirion, Nadege—STuD4 Shukla, R. K.—AWA6 Sola, Íñigo—JWC10 Stich, Dominik—LSWJ5 Takita, Akihiro—LMTuA2 Thomas, Jayan—AThB2 Shvedov, Vladlen G.—JWC61 Solís, Irais V.—JWC67 Stintz, Andreas—FMB4, FMB5 Takman, P.—FThA4 Thompson, John R.—JWC34 Shwartz, Sharon—LSTuG4 Sollee, Jeff—FThD2 Stirnemann, Guillaume—LSWF1 Talbot, Gordon—AOTuA5 Thompson, Kevin P.—FThH4, FTuT3 Si, Ke—FThR4 Solomon, Christopher J.—STuB5 Stites, Ronald W.—LSTuA8 Talla Mbe, J. H.—JWC23 Thompson, Michael A.—CThA4, CTuD1, Siahmakoun, Azad—JWC46 Soltani, Mohammad—FTuB7 Stöhr, Joachim—LSThE3 Talmi, Amos—AOThC5 LSWD2
FiO/LS/AO/AIOM/COSI/LM/SRS 2009 • October 11–15, 2009 161 Thompson, Mark G.—FMG1 Tuohimaa, T.—FThA4 Venkataraman, D.—LSMB4 Wang, Jian—FThE2 Wei, Xin—JWB1 Thompson, Nancy—LSThD2 Turaga, Diwakar—FThV1, JWC71 Venugopalan, Vasan—FThP4, FThV Wang, Jing—FTuJ2 Wei, Yongqiang—FWN2 Thurman, Samuel T.—STuC3 Turner-Foster, Amy C.—FTuW3 Vera, Alice—AWA2 Wang, Kang—STuB3 Weigel, Aubrey V.—JWC68, LSWD3 Thyagarajan, Krishna—FTuE6, FWJ2, Turrell, Sylvia—AThC3 Vera, Esteban—JWC63 Wang, Lianqi—AOTuD2 Weill, Rafi—FWD5 FWG6 Twieg, Robert J.—LSWD2 Veraksa, Alexey—FThV5 Wang, Lijun—JWC15 Weiss, S. B.—FThD2 Thylen, Lars—FWC5 Tyler, Glenn—AOThD4 Véran, Jean-Pierre—AOThA4, AOTuC, Wang, L. J.—FThO2 Weitz, David A.—FTuY2 Tian, Lei—CThA3, FThB1 AOTuC4, AOWB2, JTuC2 Wang, Qi—FTuX3 Wells, Nathan P.—LSThF2 Tian, Zhenhua—JWC15 Udem, Th—LSTuB1 Verdonck, Patrick—JWC4 Wang, Qian—FThK4, FThO4, FWN2, Wells, Nathan P.—LSWC4 Tidemand-Lichtenberg, Peter L.—FThR6 Ukai, Kazuhiko—FTuM1 Verellen, Niels—FTuB6 JWC53 Wen, Zhiying—STuC7
Key to Authors Key Tiedje, Thomas—AWC5 ul Hoda, Faisal—FTuC7 Verevkin, Aleksandr—FTuE5 Wang, Quan—JWC16 Weninger, Keith R.—LSThD3 Tien, Chung-Hao—FWT4 Urbanek, Karel—AWC3 Vérinaud, Christophe—AOTuD1 Wang, Quan—LSTuF3 Wenner, J.—JMA1 Timneanu, Nicusor—LSThA3 Urbanski, Lukasz—FTuS2 Verlot, P.—LSTuK1 Wang, Shih-Yuan—FWC5 Wereley, Steve—LSMC4 Tippie, Abbie E.—STuC6 U’Ren, Alfred B.—FWJ Veronis, Georgios—FThW5 Wang, Tianyi—FThP6 Werner, James H.—LSThF2, LSTuG1 Tischler, Jonathan Z.—FThM2 Ussery, Daryl—JWC44, JWC56 Veselago, Victor—FMA1 Wang, Ting—FTuP4 Weßels, Peter—JTuA2 Tiwari, Umesh K.—FTuE6, FWG6 Utzinger, Urs—FME Vettenburg, Tom—FThX2 Wang, Wei—CWA3 Westall, Carol A.—JWC78 Tobar, Michael—LSTuB5 Vidal, Fabrice—AOTuA5 Wang, Wenjie—FThI1 Weyrauch, Thomas—JWA4 Todd, Stephen—AOTuA5 Vaccaro, Kenneth—AOThD2 Vijande, Javier—FWH4 Wang, Xi—FMK4 Whelan, Maurice—FWY5 Tokuda, Takashi—FMD4 Vaccaro, Patrick H.—LSMB3 Vilaseca, Ramon—FThI1, FTuS4 Wang, Xiao—FTuK4 Whitaker, John F.—FWG3 Tolmachov, Alexei I.—LSTuG2 Vafadar, Bahereh—STuA3 Vincenti, Maria Antonietta—FThW2, Wang, Xiaosheng—FTuV5 White, Andrew G.—JWD3 Toma, Cristian—CWA5 Vahala, Kerry J.—LSTuB1, LSTuB3, FWC6 Wang, Xin—FWI3 White, G. R.—LSTuI5 Tomes, Matthew—FThO5 LSTuE, LSTuE2 Vinogradov, A. V.—FTuZ2 Wang, Xiaosheng—JWC29 White, Madeline C.—JWC33 Torgersen, Todd—CThB2 Vakoc, Ben—FWV3 Visser, Taco D.—FWH6, FWU2 Wang, Xiaoyong—LSTuJ4 White, Tom P.—FWF5 Torres, Richard—FThP5, FTuY6 Valente, Marty—FThH Vodopyanov, Konstantin—FMK2 Wang, Yiliang—FThE3 Whitfield, J. D.—JWD3 Torres, Sergio—JWC63 Valentine, Jason—FTuN2 Vogel, Curtis R.—AOThD4 Wang, Yu—FTuY5 Wiberg, Andreas O. J.—FWK2 Torres-Cisneros, Miguel—JWC41, JWC67 Valenzuela, John R.—CWA2 Vogt, U.—FThA4 Wang, Y.—FTuZ2 Wiberg, Donald M.—AOWB5 Toth, Csaba—FWA Valley, Marcy M.—FThD2 Vohnsen, Brian—JWC43, JWC77 Wang, Yadong—FWN2 Wieczorek, Sebastian—FThO6 Toulouse, Jean—FTuI3 Valley, Michael T.—CThC3 Vollmer, Frank—LSMG2 Wang, Yung-Hsing—JWC1 Wiederrecht, Gary—LSWG5 Toussaint, Jr., Kimani C.—FMK7, FWB2 Vallini, Felipe—FThO7 Vorobyev, A. Y.—JTuC18 Wang, Ye—LSWB3 Wiersma, Diederik S.—FMC4 Tran, Van T. T.—AThC3 Valtna-Lukner, Heli—FTuO5 Vorontsov, Mikhail—AOThC, CThC3, Ward, Jonathan M.—FThC2 Wikner, David A.—CTuA3 Travouillon, Tony—AOThB1 Vance, Calvin—JWC13 JWA4 Warnasooriya, Nilanthi—FThB4 Wildeman, Jurjen—LSTuG1 Trébaol, Stéphane—FThO3 van den Broek, Johanna M.—FWS6 Vos, Willem L.—FWF4, FWS6 Warren, Warren S.—FWA3 Wildey, Chester—FWR3, JWC9 Trebino, Rick—FTuO5, JWC17, SWA6 van der Gracht, Joseph—CThC, CThB2 Voss, Paul—JMA Warren-Smith, Stephen—FTuE3 Willems, Phil—AOThA5 Tremblay, Eric J.—FWG2 van der Spoel, David—LSThA3 Vučković, Jelena—FML6, FTuB3, FWB5, Warwick, Tony—FThT2 Williams, Charles—FMD2 Treusch, Rolf—LSThA3 van Dijk, Thomas—FWU2 JWE5, LSTuD4, SC322 Washburn, Adam L.—LSMC1 Williams, David R.—FTuQ2, JWF4 Tripathi, Santosh—FWB2 Van Dorpe, Pol—FTuB6 Vyas, Reeta—JWC30 Watkins, Amy—FMG3 Williams, Stanley—FWC5 Tripathi, Saurabh M.—JWC40 van Exter, Martin P.—FMF5, JMA6 Watson, Edward—FTuF1 Willner, Alan E.—FThE2, FWK3, FWZ5 Trita, A.—LSTuI4 van Marcos, Dam —AOWB2 Wachulak, Przemyslaw W.—FTuS2 Watts, Richard—STuA3 Wilson, Bridget S.—LSThF2 Trull, Jose F.—FThI1, FTuS4 van Ooijen, Erik D.—FWM3 Wagadarikar, Ashwin A.—CTuA6 Wawro, Debra—FTuY1 Wilson, Tony—AOThC3, AOWA2 Tsai, Hsiu-Ming—FThL4 Van Stryland, Eric W.—FMF, FThS5, Wahhaj, Zahed—AOThA3 Wax, Adam—FME6, FMK, JWC75 Winarski, Robert P.—FThM4 Tsai, Meng-Che—JTuC8, JWC1 LSTuG2 Wakaki, Moriaki—FThS4, JWC22 Webb, Kevin J.—FMA6, FTuL3 Winick, Kim A.—FMJ1 Tsai, Tsung-Han—FThL4 VanNasdale, Dean A.—FME5, FThQ2 Waller, Laura—CThA3, FThR3 Webb, Roderick P.—FTuI, FTuW1 Winkelmann, Lutz—JTuA2 Tschentscher, Thomas—LSThA3 Vanner, Michael—LSTuH1 Walmsley, Ian A.—FWJ3, JTuB2 Weber, Mark—FThD2 Winkler, Mark—AWB1 Tseng, Shih—FThV3, FTuH2 Varcoe, Benjamin—FThU3 Wampler, Ronald—LSMF2 Weber, Ryan—LSWD2 Wirth, Allan—AOThC4 Tsuda, Hiroyuki—FThE4, FWN4 Varela, Oscar—JWC10 Wan, Wenjie—FMF1 Webster, Scott—FThS5, LSTuG2 Witcher, Jonathan—LMTuB4, LMTuC4 Tu, Yanfei—FWK4 Vasilyeu, Ruslan—FThB6 Wanapun, Debbie—LSMF2 Webster, Scott E.—AWC5 Withford, M. J.—LMTuC1 Tuchin, Valery V.—SC340 Vázquez de Aldana, Javier R.—LSWB4 Wang, Feiling—AOThC2 Weegink, Kristian—FWM3 Woafo, P.—JWC23 Tunnell, J. W.—FME1 Veisz, Laszlo—FTuK3 Wang, Feng—LSWE1 Wei, Feng—LSWK2 Wober, Munib—FTuV2 Tünnermann, Andreas—FMA3, FThC3, Veit, K.—FWV1 Wang, H.—JMA1 Wei, Jean—AWA3 Woerdman, J. P. (Han)—FMF5 FThC6, FThJ4 Veltkamp, Christian—JTuA2 Wang, Hongfei—LSWK2 Wei, Wei—FWL4
162 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 • October 11–15, 2009 Wolf, Emil—FTuO2, FWH2, FWU3, Xu, Jimmy—FWZ4 Yerçi, Selçuk —FML6, FTuB3 Zawilski, Kevin T.—AWA3 Zhao, Yue—FMJ7 FWU4 Xu, Lina—CThC6 Yesayan, Garegin—FWI5 Zdyrko, Bogdan—AThC4 Zheng, Yili—STuB4 Wondraczek, Lothar—AThD3 Xu, Lei—FTuP4 Yi, Fei—FThE3, FThK Zeldovich, Boris Y.—FMF2, FWH, FWX5 Zhong, Guixiong—AOThC2 Key to Authors Wong, Chee Wei—FML5 Xu, Min—JTuC10 Yi, Jong Chang—FThK2 Zeng, Xiaoming—FTuK4 Zhong, Shan—FTuC2 Wong, Shing-Wa—FTuC1 Xu, Michelle Y.—FThW1, FThW3, Yildiz, Ahmet—LSThF3, LSWD Zentgraf, Thomas—FTuB2, FTuN2 Zhong, Zhangyi—JWF1 Wong, Wesley—FWS1 FThW7 Yilmaz, Tolga—FWX4 Zepf, Matt—FTuZ3 Zhou, Jun—FThD1 Woods, Bruce W.—LSThA3 Xu, Ningning—FWB7 Yin, G. Y.—JMA2 Zewe, Kelly—LSTuG1 Zhou, Kainan—FTuK4, JTuC5 Woods, Charles—AOThD2, FTuH5, FWI1 Xu, Yan-yan—LSWK2 Yin, Lianghong—FML4 Zeytunyan, Aram—FWI5 Zhou, Kaimeng—LSMG5 Wornell, Gregory—CTuB5 Xu, Zhimin—STuA4 Yokoyama, Eisuke—FThS4 Zgu, G.—FTuN5 Zhou, Shuyun—LSWJ3 Woznica-Raulin, Katarzyna—AThC3 Yoon, Yeo-Taek—FWE5 Zhai, Zhaohui—FWK4 Zhou, Wei—FThE7 Wright, Tom—JWC78 Yadav, Ram A.—JWC45 Yorulmaz, Saime C.—FThU6, FThU7 Zhan, Qiwen—FThF2, SC235 Zhou, Wei—JTuC5 Wu, Binlin—JTuC10 Yadav, Tarun K.—JWC45 Yoshie, Tomoyuki—FThO, FThU2 Zhang, Deming—FMB3 Zhou, Xiao-Qi—FMG1 Wu, Benny—LSThE3 Yakimenko, Vitaly—LSMH4 Young, Michael E.—FMA7 Zhang, Guoquan—FWK4 Zhou, X.—JWE4 Wu, Bing—STuA3 Yamashita, Shinji—FTuC1 Younger, Eddy—AOTuA5 Zhang, Heyi—FWI4 Zhou, Xibin—LSTuI3 Wu, Chengbiao—LSThB3 Yamauchi, Kazuto—FThG3 Yu, Haiwu—FTuK4 Zhang, Jin—FTuE4 Zhou, Y. S.—LMTuD2 Wu, Hao—FWL6 Yamilov, Alexey G.—FMC3, FMC6 Yu, Siyuan—FMG1 Zhang, Jing—FWE6, JWC35 Zhu, Diling—LSThE3 Wu, Jing—FTuV3 Yang, Changhuei—FWS4 Yu, William—FWB4 Zhang, Kun—JTuC5 Zhu, Qihua—FTuK4 Wu, Pingfan—FTuF2 Yang, Haw—LSTuD2, LSWD1 Yu, Xudong—JWC35 Zhang, Kai—LSThB3 Zhu, Qibiao—FTuX3 Wu, Qiaofeng—FThV4 Yang, J.—FThI3 Yu, Zongfu—FMH2 Zhang, Ke—LSWD4 Zhu, Qihua—JTuC5 Wu, Qi—FTuN4 Yang, Kai—FMB4, FMB5 Yuan, Ping—FWE6 Zhang, Lei—CThB2 Zhu, Xiangdong—FTuY4 Wu, Wei—LSWE1 Yang, Qiguang—FWB4 Yuan, Sheng—FThT2 Zhang, Lin—FThE2, FWZ5 Zhu, Xin—LMTuA4 Wu, Xiaoxia—FWK3 Yang, Tianhe—FThO5 Yuan, Zhiliang—JWE2 Zhang, Mathew—FThE5 Zhu, Yizheng—FME6 Wu, Ziran—FWX2 Yang, Weijia—AWB4, JTuC16 Yue, Yang—FThE2, FWZ5 Zhang, Peng—FThI3, FTuE1, FTuX2, Zhu, Zipeng—LSWJ5 Wurth, W.—LSMH1 Yang, Weijian—FTuW2 Yum, Honam—JTuA6 FTuV5, FWF, JWC32 Zielinski, Thomas P.—SWA2 Yang, Wei J.—FWL3 Yun, Wenbing—FThT3 Zhang, Sheng—FTuJ3 Zinter, Joseph P.—FWA5 Xiao, Fajun—FTuV5 Yang, X.—FTuW1 Yuna, Ping—FWL6 Zhang, Xiang—AThA1, FTuB2, FTuN1, Zlatanovic, Sanja—FML2, FWR1 Xiao, Lei—FThO3 Yanik, Ahmet Ali—FMA4, FWP6 Yurke, Bernard—FWC2 FTuN2 Zolotoyabko, Emil—LSTuG4 Xiao, Min—FWB7, JWC35 Yao, Xiao Jie—JWC16 Yvind, Kresten—FThE1 Zhang, Xuenan—FWE6 Zorba, Vassilia—LMTuD1 Xiao, Shumin—FTuN3 Yapp, Cal—AWA1 Zhang, Xiang—FWL5, LSWE1 Zou, Weiyao—JWF1 Xiao-Li, Yinying—FThE2, FWZ5 Yariv, Amnon—FTuX1, FWK3 Zacarés, Mario—FWH4, FWP3 Zhang, Yanpeng—FWB7 Zuegel, Jonathan D.—FTuD5 Xie, Xudong—FTuK4, JTuC5 Yashchuk, Valeriy V.—FThT2 Zadok, Avi—FWK3 Zhang, Yundong—FWE6, FWL6 Zuo, Yanlei—FTuK4 Xin, Hao—FWX2 Ye, Winnie N.—FTuV2 Zagrebin, Leonid—AThB4 Zhang, Ying—FWP5 Xin, Yongchun—FThK1 Yeaton-Massey, David—JWC20 Zaïr, Amelle—JWC10 Zhang, Yuhua—FWX1 Xiong, W.—LMTuD2 Yegnanarayanan, Siva—FTuB7 Zaitsev, Oleg—LSTuA5 Zhang, Yan—JWC15 Xu, J.—FThI3 Yeh, Alvin T.—FThV4 Zam, Azhar—FThP2 Zhao, Jing—AOThC2 Xu, Jun—FWB6 Yelleswarapu, Chandra S.—FThF3, FThV5 Zambon, Veronique—JTuC15 Zhao, Jianlin—FThI3, FTuV5, JWC32 Xu, Jingjun—FWK4 Yen, She-Hwa—FTuC1 Zambrini, Roberta—FThI6, FWY1 Zhao, Junpu—JTuC5
FiO/LS/AO/AIOM/COSI/LM/SRS 2009 • October 11–15, 2009 163 Key to Authors and Presiders (Bold denotes Presider or Presenting Author)
Adam, Roman—PDPA1 Holzlohner, Dmitry—AOThB3P Oulton, Rupert F.—PDPB7 Adamo, Giorgio—PDPB1 Holzlohner, Ronald—AOThB3P, PDPA4 Aeschlimann, Martin—PDPA1 Hoover, Erich—PDPC7 Papp, Scott B.—PDPA7 Afek, Itai—PDPA9 Horstmeyer, R W.—CWB6P Park, Jung S.—PDPB3 Almeida, Euclides—PDPC5 Hu, Juejun—PDPC6 Passmore, Brandon—PDPB8 Alonso, Miguel A.—PDPC4 Huang, Chung‐Che—PDPB1 Peter, Diethard—AOThA6P Ambar, Oron—PDPA9 Petruccelli, Jonathan C.—PDPC4 Amberg, Philip—PDPB5 Ippen, Erich P.—PDPB4 Pinckney, Nathaniel—PDPB5 Angot, Ludovic J.—CThC7P Pinguet, Thierry—PDPB5 Arie, Ady—PDPA5 Jacob, Zubin—PDPB6 Politi, Alberto—PDPA6 Assoufid, Lahsen—PDPB Jia, Yaoshun—PDPB2 Porat, Gil—PDPA5 Athale, R A.—CWB, CWB6P Jimenez, Ralph—PDPC7 Johnson, Anthony—PDPA3 Quarles,Gregory—PDPC Bartal, Guy—PDPB7 Quirrenbach, Andreas—AOThA6P Beausoleil, Raymond G.—PDPC3 Kapteyn, Henry C.—PDPA1 Bonaccini Calia, Domenico—AOThB3P, Kimble, H. Jeff—PDPA7 Radic, Stojan—PDPB3 PDPA4 Kimerling, Lionel C.—PDPC6 Raj, Kannan—PDPB5 Bravo‐Abad, Jorge—PDPB4 Kintaka, Kenji—AThA6P Reagan, Brendan A.—PDPA2 Brener, Igal—PDPB8 Knight,Jonathan—AThC Reese, Colin—CWB6P Budker, Dmitry—AOThB3P Knight, Kenton—PDPB1 Richardson, Kathleen—AWA Krishnamoorthy, Ashok V.—PDPB5 Rocca, Jorge J.—PDPA2 Carruthers, Tom—PDPA Kubacki, Ronald M.—AWA7P Rochester, Simon—AOThB3P Chang, Chuan‐Chung—CThC7P Kuis, Robinson—PDPA3 Chao, Yu‐Faye—PDPC1 Kupp, E R.—AWC6P Sabbagh Alvani, Ali A.—AThC6P Chavez‐Boggio, Jose M.—PDPB3 Sacilotti, Marco—PDPC5 Chen, Po‐Chang—CThC7P Lalanne, Elaine—PDPA3 Salimi, Reza—AThC6P Chichester, Justin—PDPC7 La‐O‐Vorakiat, Chan—PDPA1 Sameie, Hassan—AThC6P Choi, Kyung S.—PDPA7 LeLouarn, Miska—AOThB Sámson, Zsolt L.—PDPB1 Crozier, Kenneth—PDPC6, PDPC8 Lexau, Jon—PDPB5 Sarabi, Ali A.—AThC6P Cui, Xiaoqiang—AThA6P Li, Guoliang—PDPB5 Schneider, Claus M.—PDPA1 Cunningham, John E.—PDPB5 Li, Jingjing—PDPC3 Schwab, Christian—AOThA6P Curtis, Alden H.—PDPA2 Li, Kuan‐Yi—PDPC1 Shaner, Eric—PDPB8 Lin, Shiyun—PDPC6, PDPC8 Shaw, Justin M.—PDPA1 Dai, Lun—PDPB7 Liu, Sheng—PDPA3 Shi, Jing—PDPB5 De Angelis, Francesco—PDPB1 Lougovski, Pavel—PDPA7 Schunemann, Peter G.—AWC Deng, Hui—PDPA7 Lumsdaine, Andrew—SWA7P Siemens, Mark E.—PDPA1 Di Fabrizio, Enzo—PDPB1 Luo, Ying—PDPB5 Silberberg, Yaron—PDPA9 Divliansky, Ivan B.—PDPB3 Luther, Bradley M.—PDPA2 Silva, T. J.—PDPA1 Dubinskii, Mark—AWC6P Smolyaninov, Igor—PDPB6 Ma, Ren‐Min—PDPB7 Soljačić, Marin—PDPB4 Eggleton, Charles D.—PDPC7 MacDonald, Kevin F.—PDPB1 Sorger, Volker J.—PDPB7 Euliss, Gary—CWB6P Marr, David W. M.—PDPC7 Squier, Jeff—PDPC7 Mathias, Stefan—PDPA1 Sraj, Ihab—PDPC7 Fainman, Shaya Y.—AThA Matson, Charles L.—SWA Stack, R A.—CWB6P Fattal, David—PDPC3 Matthews, Jonathan C. F.—PDPA6 Sundheimer, Michael—PDPC5 Feng, Yan—PDPA4 Meehan, Shaun P.—PDPA2 Fischer, Peer—PDPC2 Mekis, Attila—PDPB5 Tahriri, Mohammadreza—AThC6P Fratz, Markus—PDPC2 Merkle, Larry D.—AWC6P Tawa, Keiko—AThA6P Furch, Federico J.—PDPA2 Messing, Gary L.—AWC6P Taylor, Luke R.—PDPA4 Miao, Xiaoyu—PDPB8 Ter‐Gabrielyan, Nikolay—AWC6P Gässler, Wolfgang—AOThA6P Miller, Donald T.—AOThA Thacker, Hiren—PDPB5 Gayer, Ofer—PDPA5 Mookherjea, Shayan—PDPB3 Tsai, Hsiu‐Ming—PDPC1 Georgiev, Todor G.—SWA7P Moro, Slaven—PDPB3 Giel, Dominik M.—PDPC2 Morrison, R L.—CWB6P UʹRen, Alfred B.—PDPA8 Gin, Aaron—PDPB8 Mota, Claudia B.—PDPC5 Gladden, Chris—PDPB7 Moztarzadeh, Fathollah—AThC6P Van der Gracht,Joe—CThC Goban, Akihisa—PDPA7 Murnane, Margaret M.—PDPA1 van Enk, Steven J.—PDPA7 Goma, Sergio—SWA7P Vangala, Shivashankar—PDPB8 Goodhue, William—PDPB8 Narimanov, Evgenii—PDPB6 Grychtol, Patrik—PDPA1 Necioglu, B F.—CWB6P Xu, Yong—PDPB2 Nembach, Hans—PDPA1 Hackenberg, Wolfgang—AOThB3P, Nishii, Junji—AThA6P Zentgraf, Thomas—PDPB7 PDPA4 Nunes, Frederico D.—PDPC5 Zhang, Xiang—PDPB7 Hewak, Dan W.—PDPB1 Zheludev, Nikolay I.—PDPB1 Higbie, James M.—AOThB3P OʹBrien, Jeremy L.—PDPA6 Zheng, Xuezhe—PDPB5 Ho, Ron—PDPB5 OʹDonnell, Kevin A.—PDPA8 Zlatanovic, Sanja—PDPB3 Monday, October 12 44 ies of decay. their by mapping out the Wigner function, and show mov- superconducting qubit. We analyze a variety of states Q high- a coupling by synthesized USA. Barbara,Santa atCaliforniaUniv. Cleland;of N. A. Lucero, M. Neeley, A. D. ErikO’Connell, Bialczak, C. RadoslawD.Ansmann, Wang, Sank,M. H. J. Wenner, Converter, Analog to Digital Quantum The Resonator: conducting Super a in States Photon Arbitrary Synthesizing second photon. the of modulation by enhanced or negated be may correlation,frequency-domainby pair, measured as temporalmodulation of one photon of an entangled experimentally describe a new quantum effect We where Univ.,USA. Stanford Harris; E. S. Yin,Y. G. Biphotons, of Modulation Nonlocal JMA2 •2:00p.m. JMA1 •1:30p.m. Presider Paul Voss; Georgia Tech, USA, and MeasurementI JMA •EntanglementGeneration 1:30 p.m.–3:30p.m. Arbitrary microwave photon states have been been have statesphoton microwave Arbitrary JOINT FiO/LS Empire 12:00 p.m.–2:00p.m. John Martinis, Max Hofheinz, Hofheinz, Max Martinis, John Invited resonator to a to resonator S. Sensarn, Sensarn, S. - LSMA: Laser ScienceSymposiumonUndergraduateResearch Posters, Cupertino Laser LSMA: Room, Fairmont Hotel (Seethe Program in your registration bag.) 8:00 a.m.–12:00p.m. index of refraction, is discussed. negative with medium a in particular in medium, momentum of the photon, propagating in a refractive Technology, Russian Federation. Media, fer by Electromagnetic Wave in Negative Refraction About Energy, Linear Momentum and Mass Trans- FMA1 •1:30p.m. Lab, USA,Presider Hou-Tong Chen; Los Alamos Natl. FMA •MetamaterialsI 1:30 p.m.–3:30p.m. greatly modified. also is phenomenon tunneling Brewster the while modes, optical TM bounded support can media dielectric different two between sandwiched film nanocompositeepsilon-near-zero anisotropic an that calculation mode and reflectance in both show W. Inst.Univ.Boyd;Optics, of We Rochester,of USA. Films Zero Epsilon-near- Anisotropic on Modes Optical FMA2 •2:00p.m. Victor Veselago; Moscow Inst. of Physics andPhysicsVictor Veselago; of Inst. Moscow , Zhimin Shi, Andreas C. Liapis, Robert Liapis, C. Andreas Shi, Zhimin 10:00 a.m.–10:30a.m. Crystal Invited FiO/LS/AO/AIOM/COSI/LM/SRS 2009 The question of linear 2009 Joint FiO/LS Awards Ceremony and Plenary Session,Regency Ballroom,2009 JointFiO/LSAwardsCeremonyandPlenary Fairmont Hotel 12:00 p.m.–1:30p.m. Optics of Solar Cells, version efficiency while reducing while version $/Wp the efficiency cost. within the solar cell itself can maximize its solar con- will be reviewed. Likewise, we present how the optics tor and non-concentrator photovoltaic module optics Development, USA. Key advances in solar concentra - FMB1 •1:30p.m. ics of Cells”. Solar 2002, SPIE published his tutorial book “Optoelectron- thin films researcher, electrochemist and professor. In photovoltaic specialist, design optics engineer,LED careerincludes roles growth asan Czochralski III-V University.His Stanford from Science Materials in degree Masters his and Lausanne in Technologyof InstituteFederalSwiss the from Chemistry Physical nativeof SanJose, Dr. Smestadreceived Ph.D.his in to specialize in photovoltaics, optics and solar cells. A Technology Development, a consultancy he founded ment of Energy. He is principal and owner of Sol Ideas U.S.for grants,the andmissionPIER/EISG - Depart He is currently a reviewer for California Energy - Com journal. peer-reviewed international an Cells, Solar sociate Editor for Elsevier’s Solar Energy Materials and materials. For most of that time, he has as served As - as a scientist and engineer in the field of solar energy Greg P. Smestad, Ph.D., has over 20 years of experience Presider Alan Kost; Univ. of Arizona, USA, Energy FMB •OpticsforRenewable 1:30 p.m.–3:30p.m. Materials and Solar Cells, USA; Coffee Break,Regency and Imperial Ballroom Foyer, Fairmont Hotel Greg P. Smestad Greg Gold Lunch Break(on yourLunch own) Keynote 2 Sol Ideas Technology • 1,2 ; 1 Solar Energy Energy Solar October 11–15,2009 FiO lasing with cold atoms. random and photons of flights Levy subradiance, Dicke and localization Anderson between interplay Welight. the ofstudy properties coherenttransport study to system quantum interesting as emerged Sophia-Antipolis,France.Nice de Flights to Levy Random Lasers, Multiple Scattering of Light in Atomic Gases: From USA, Presider Tsampikos Kottos; Wesleyan Univ., I FMC •AndersonLocalization 1:30 p.m.–3:30p.m. 4 Science, Israel, Christodoulides FMC1 •1:30p.m. intensity correlations. these on nonlinearity of effect the measureWe localization. Anderson exhibiting media disordered dimensional one in light for correlations intensity study experimentally We USA. Florida, Central Pozzi Lattices Photonic Disordered in Correlations Intensity FMC2 •2:00p.m. CREOL, College of Optics and Photonics, Univ.ofPhotonics, and Optics of College CREOL, 2 , Sorel MarcSorel , , ov Lahini Yoav 2 4 Univ. of Glasgow, UK, , Yaron Silberberg 2 , Roberto MorandottiRoberto , Valley 1 , YaronBromberg, Invited 1 ; Robin Kaiser; Univ.
1 Cold atoms have atoms Cold Weizmann Inst. of 3 INRS, Canada, 3 1 , Demetrios , , Francesca , transceiver at mobile the end-terminals. wirelesssingle-chip and head-end conversion the at all-optical using delivery data and video definition access supporting multi-gigabit uncompressed high- optical-wireless 60-GHz with network over-fiber radio- in-buildingbi-directional a time, first the for Tech,USA. Georgia Chien; Chang Delivery, Data and Video HD In-building Throughput Multi-GigabitWirelessTransceiver Very forHigh with Interoperable Network Radio-over-Fiber MM-Wave60-GHz Multi-Service Bi-Directional FMD1 •1:30p.m. USA, Presider Leonid Kazovsky; Stanford Univ., FMD •RFPhotonics 1:30 p.m.–3:30p.m. reduction is observed. mode noise spur suppression by 11 dB, and linewidth presented. Optical supermode suppression, RF super is GHz 10.24 at operating stabilization, feedback term long with oscillator optoelectronic coupled injection-locked optically based, semiconductor A of Optics and Photonics, Univ. of Central Florida, USA. Dimitrios Mandridis, Peter J. Delfyett; CREOL, College Williams, Franklyn Quinlan, Josue Davila-Rodriguez, tor with Long-Term Feedback Stabilization, Injection Coupled Optoelectronic - Locked Oscilla FMD2 •2:00p.m. Gee-Kung Chang, Arshad Chowdhury, Hung- California Invited Wedemonstrate, Charles Charles -
Monday, October 12 45
David Abstract Abstract Jerome Jerome Hastings; SLAC Invited Invited Hillsborough 1:30 p.m.–3:30 p.m. Science I LSMD • Ultrafast X-Ray Michigan, of A. Reis; Univ. David USA, Presider LSMD2 • 2:00 p.m. LSMD1 • 1:30 p.m. The X-Ray Pump-Probe Instrument at LCLS, at Instrument Pump-Probe X-Ray The USA. Univ., Stanford Lab, Accelerator Natl. SLAC Fritz; the be will (XPP) instrument Pump-Probe X-ray The first hard X-ray experimental station to operate at the LCLS in the fall of 2010. The design, status and will XPP be of presented. capabilities Title Title to Be Announced, USA. Univ., Stanford Lab, Accelerator Natl. available. not - Scanning ion Adam L. Washburn,
Invited Invited LS Piedmont 1:30 p.m.–3:15 p.m. I LSMC • Micro- and Nanofluidics Univ., Indiana Jacobson; Stephen USA, Presider LSMC1 • 1:30 p.m. LSMC2 • 2:00 p.m. Ion Conductance Microscopy of Nanometer Pores, Pores, Nanometer of Microscopy Conductance Ion Lane A. Baker; Indiana USA. Univ., conductance microscopy was used to interrogate pores nanometer-scale from emanating currents ion of a polymer activity membrane. Transport of - indi vidual was pores images ion measured from current and corresponding topographic images recorded simultaneously. Applications Applications of Silicon Photonic Technology for Clinical Diagnostics and Highly Multiplexed Biomolecular Detection, Abraham J. Qavi, Matthew S. Ji-Yeon Luchansky, Byeon, Ryan C. Bailey; of Univ. Illinois at Urbana- Champaign, USA. Silicon photonic structures are incredibly responsive to binding-induced changes the surrounding environment index refractive the in device. We are developing microring resonator ar and label-free, sensitive, for platform robust a as rays detection. biomolecular highly multiplexed
LSME: Laser I, Science Symposium on Undergraduate Research October 11–15, 2009 Polarimetry Polarimetry
• Fairfield Room, Fairmont Hotel (See the Program in your registration bag.) registration your in Program (See the Hotel Fairmont Room, Fairfield Peer Fischer; Rowland Rowland Fischer; Peer Invited Invited (on your own) Lunch your (on Break 2:00 p.m.–4:00 p.m. Sacramento Nina Nina Berova; Columbia USA. Univ., Regency and Imperial Ballroom Foyer, Fairmont Hotel Fairmont Foyer, Ballroom Imperial and Regency Coffee Break, LSMB1 • 1:30 p.m. 1:30 p.m.–3:30 p.m. LSMB • Advances in Chiroptical Spectroscopy I USA, Univ., York New Bart Kahr; Presider LSMB2 • 2:00 p.m. We discuss recent results on molecular We probing and porphyrins, sensitive CD by chirality supramolecular metalloporphyrins and other fluorescent reporter groups where for the chiroptical analysis a - conven tional CD and ellipsoidal mirror FDCD detectors employed. were Probing Probing Molecular Chirality by Conventional and Fluorescence Detected Electronic Circular Dichroism, Interfaces, at Activity Optical Inst. at Harvard, Harvard USA. Univ., requires long path-lengths. we Here consider chiro- optical phenomena that arise at an interface and volumes. microfluidic of analysis the allow therefore New effects due to the addition of a magnetic field also described.are - Opti 12:00 p.m.–1:30 p.m. 2 Sergiy Sergiy Wenjie , , Vadim 1 Regency Ballroom, Fairmont Hotel Fairmont and Plenary FiO/LS Awards Ceremony 2009 Joint Ballroom, Session, Regency FiO/LS/AO/AIOM/COSI/LM/SRS 2009 CREOL, College of Optics Optics of College CREOL, 1 , Julien Lumeau ; 1 1 - Mis Arnoldus; F. Henk Li, Xin 10:00 a.m.–10:30 a.m. 10:00 a.m.–10:30 Atherton , Leonid Glebov , Boris Zeldovich Boris , 1 2 and Photonics, Univ. of Florida, Central and USA, Univ. Photonics, FMF2 • 1:45 p.m. Moiré Filter in Volume Bragg Grating Mokhov Eric W. Van Stryland; CREOL, CREOL, Stryland; Van W. Eric Photonics, and Optics of College USA, Florida, Central of Univ. Presider 1:30 p.m.–3:30 p.m. FMF • Spatial Nonlinearities: Solitons and Beams FMF1 • 1:30 p.m. Edge, Straight a from Diffraction Nonlinear Wan, Dmitry V. Dylov, Christopher Barsi, Jason W. Fleischer; Princeton USA. Univ., We experimentally - me a in edge straight a from diffraction demonstrate dium with self-focusing Theoretically, nonlinearity. spatially-dispersive a as flow optical the interpret we pressure. negative with wave shock We propose narrow-band moiré filter in filter moiré narrow-band propose We USA. Grate, transverse via tunable be can It grating. Bragg volume nm 1550 at Filter fibers. in absent freedom of degrees was 95% transmission and pm 50 of bandwidth with demonstrated. FMF3 • 2:00 p.m. - Emit Radiation Atomic of Field near the in Vortices , Interface an near ted for pattern flow energy The USA. Univ., State sissippi exhibits interface an near atom an by emitted radiation field. near the in vortices and singularities numerous nanoscale dimension. of are vortices optical The Smirnov 8:00 a.m.–12:00 p.m. 8:00 a.m.–12:00 Cupertino Room, Fairmont Hotel (See the Program in your registration bag.) registration your in Program (See the Hotel Fairmont Room, LSMA: Laser Cupertino Posters, Research Science Symposium on Undergraduate FiO , S. 1 Metal Metal in vivo , P. - , Diagarad P. 1 , A. K. Dunn 3 We present a new Univ. of Univ. Texas at Austin, 1 Invited ; 1 , J. D. Payne 12:00 p.m.–2:00 p.m. 3 Ashwin Parthasarathy, Adrien Ashwin Parthasarathy, Glen Ellen Glen , P. , Puvanakrishnan P. 1 Nanospectra Biosciences Inc., USA. Inc., Biosciences Nanospectra 3 J. J. Park , J. Tunnell W. 2 Radiation Radiation Oncology, MD Anderson Cancer that are unaffected by the presence of static 2 , J. A. Schwartz 2 1:30 p.m.–3:30 p.m. FME • Tissue Imaging and Spectroscopy Ctr., USA, Ctr., Krishnan USA, FME1 • 1:30 p.m. Urs Utzinger; Univ. of Arizona, Arizona, of Univ. Utzinger; Urs USA, Presider jane targeting targeting kinetics of metal nanoparticles (rods and shells) using multiphoton narrowband microscopy, DOS. and imaging, nanoparticles constitute multifunctional nanovectors nanovectors multifunctional constitute nanoparticles for the combined targeting, imaging, and - treat ment of solid tumors. We demonstrate the Imaging Imaging Metal Nanoparticle Tumor Targeting Kinetics, FME2 • 2:00 p.m. Quantitative Cerebral Blood Flow Measurement through Thinned Skull with Multi Exposure Speckle , Imaging Multi-Exposure Speckle Imaging instrument and a flow of times correlation predict to model speckle new in vivo intact/thinned skull. an as such scatterers Ponticorvo, S. Ponticorvo, M . Shams Kazmi, Andrew K. Dunn; of Univ. Texas at Austin, USA. Monday, October 12 46 pump input scheme. pulsed with rate repetition GHz over at observed temperaturecoincidenceis and Optimal achieved is single dual-element PPKTP waveguide is investigated. a on down-conversion and doubling frequency Tang; NIST, USA. A compact scheme for high-speed Carlos H. MonkenH. Carlos Lab, Leiden Univ., Netherlands, various several-photon states. photonsadd deterministically producingmode, toa pseudo- can we times, several downconversion downconversion.attemptingparametric taneousBy producingmulti-photon states using repeated spon - Illinois, USA. We discuss a novel method of efficiently neering, - Engi State Quantum Optical High-Efficiency JMA3 •2:15p.m. Repetition Rate Repetition GHz over atWaveguide PPKTP Dual-Element Single a by Generation Pair Photon Correlated JMA5 •2:45p.m. ment in Two-PhotonStates, in ment Direct Measurement of Transverse Mode Entangle- JMA6 •3:00p.m. minimize spectral and spatial entanglement.minimize spectral to as so chosen are mode spatial pump and length, poled KTP at 1552 nm. The pump bandwidth, crystal based on collinear down-conversion in periodically- sourcephoton entangled an We describe Lab,USA. Grice, Travis Humble, Jason Schaake; Oak Ridge Natl. Entanglement Spectral Minimum and Emission Mode Single for Optimized Source Photon Entangled Bright JMA4 •2:30p.m. classical coherence theory. in decomposition coherent-mode the and position exploiting a connection between the Schmidt decom- by statestwo-photon entangled spatially of number Schmidt the measure to method new a implement Brazil. Gerais, Minas de Federal and MeasurementI—Continued JMA •EntanglementGeneration JOINT FiO/LS Kevin T.Kevin McCusker, Kwiat;PaulG. Univ. of , PhilipEvans,Ryan Bennink,Warren , 1,2 Oliver Slattery, Lijun Ma, Xiao Ma, LijunSlattery, Oliver , MartinP., Exter van Empire Henrique D. L. Pires L. D.Henrique 2 Dept. de Física, Univ. We introduce and introduceWe 1 ; 1 Huygens 1 , small absorptionsmall losses. while still maintaining large field enhancements and fectively blue-shifted by increasing the particle height two-dimensional silver nanoparticle arrays can be ef- of resonances plasmonic collective the that show investigations theoretical and Experimental USA. Univ.,Paiella;BostonRoberto DiMaria, Jeff Henson, Control, Height Nanoparticle via Arrays al Tunable Plasmonic Resonances in Two-Dimension- FMA5 •2:45p.m. material parameters inapplications. convenienta allowsof impact evaluate meansthe to slab is supported by a finite element simulation. This anisotropic uniaxially a sourceimagethrough line a for solution analytic An Univ.,USA. Webb;Purdue Continued FMA •MetamaterialsI— beyond the electric dipole.beyond electric the multipoles order higher considering by response parameters and inherently induces nonlinear optical proach allows us to determine effective metamaterial nances occurring in meta-atoms is presented. The ap - reso- plasmonic of reinterpretation multipole The FalkFriedrich-Schiller-Univ.Lederer; Jena, Germany. Paul, Thomas Rockstuhl,Carsten Menzel,Christoph Pertsch, Tünnermann,ThomasAndreas Chipouline, Material Optical Interaction Nonlinear and Linear Effective towards tigation Inves Mesoscopic A Metamaterials: Multipole FMA3 •2:15p.m. index changes. refractive to sensitive highly are and enhancements field large show resonances cavity These onstrated. by two physically separated plasmonic layers is dem- Fabry-Perot cavities in 3-D plasmonic crystals created Univ., USA. Extraordinary light transmission through , tals - Crys Plasmonic 3-D Fabry-Perotin Nanocavities FMA4 •2:30p.m. Anisotropic Slab Anisotropic Uniaxially a for ApproximateGreen’sFunction FMA6 •3:00p.m. Alp Artar, Ahmet Ali Yanik, Hatice Altug; Boston , Huikan Liu, Shivanand, Kevin J. Kevin Shivanand,Liu, Huikan Crystal FiO/LS/AO/AIOM/COSI/LM/SRS 2009 , Jörg Petschulat, Arkadi John John - Projected evaluated. yield systemis also energy concentrators.planar holographic two-dimensional to applied is method The verified. experimentally and presented is applications energy solar for tors concentra- ratio concentration low holographic for model A USA. Arizona, Univ.of Zhang; Deming Concentrators Solar Ratio Concentration Low Holographic FMB3 •2:45p.m. confers light-driven specific biofuels production. metabolic transformation technologies in microalgae in microalgal photosynthesis. Further, application of lization to improve solar energy conversion efficiency the optical properties of sunlight absorption and uti - California at Berkeley, USA. Solar Production of Fuels, ences factor inideality behavior with voltage. promising for concentration due to significant differ are cells QD that show results The cells. solar (QD) InAs/GaAsquantumdotof characteristics response ofNew Mexico, WeUSA. andreportI-V the spectral Luke F. Lester; Ctr. for High TechnologyEl-Emawy,AndreasMohamedStintz,Ting-yiA. Gu, Materials, Univ. Applications, Concentration for Cells Solar Dot Quantum InAs/InGaAs GaAs-Based FMB4 •3:00p.m. FMB2 •2:15p.m. Energy—Continued FMB •OpticsforRenewable , Raymond K. Kostuk, Jose Castro, Castro, Jose Kostuk, K. Raymond Gold Invited Research aims to engineer Anastasios Melis; Univ. of • Kai Yang, Kai October 11–15,2009 FiO - flight andflight hence super diffusion. Levy a exhibit photons which in reported is glass Levy called material optical new a transport, Light Spectroscopy,LinearItaly.NonFlorence,Univ. forof Jacopo Bertolotti, Diederik S. Wiersma; European Lab Bees, Honey and Photons, Dust exciting pulse, t. an from time delay of power third a as increase and nonuniversalfluctuationsconductancearedynamic sample-to-samplethat show we measurements, microwave pulsed and calculations diagrammatic UsingFourier,France.Univ. Joseph Condensés, Sergey E. SkipetrovE. Sergey vative Random , Media Classification of Regimes of Wave in Non-Conser FMC3 •2:15p.m. different regimes inwave transport. explore the parameter space of the system and identify we gain, or absorption with media random in cable applilocalization Anderson- of criterion a of search In Technology,USA. and Science Univ.of Missouri AbePeña Nonuniversal Dynamic Conductance Fluctuations, FMC5 •3:00p.m. USA, FMC4 •2:30p.m. Continued I— FMC •AndersonLocalization 2 Lab de Physique et Modélisation des Milieux desModélisation et Physique de Lab 1 , Andrey, ChabanovA. 2 ; 1 Valley Univ. of Texas at San Antonio,San TexasUniv.at of Ben Payne, Alexey G. Yamilov; Invited 1 , Nicolas, Cherroret Pierre Barthelemy,Pierre 2 - , frequency intofrequency modulator. the RF input the of quadruple is spacing frequency The waveguide. niobate lithium poled periodically a and modulator optical sideband single a using by Two-tone photonic signal generation is demonstrated Jun Ohta; Nara Inst. of Science and Technology, Japan. Masahide Fujiwara, Toshihiko Noda, Takashi Tokuda, by Optical Frequency Doubling, Quadruple Frequency Photonic Signal Generation FMD4 •2:30p.m. demonstration is presented. experimental first the and proposed is bandwidth multi-gigahertz and range dynamic free spurious infinite potential a with modulator interferometric Central Florida, USA. A purely linear resonant cavity Univ.ofPhotonics, and Optics of College CREOL, Jr.;Delfyett J. MehmetcanPeterAkbulut, Rodriguez, Davila- JosueOzdur, IbrahimHoghooghi, Nazanin Resonant Cavity Linear Interferometric Modulator, FMD5 •2:45p.m. spectrally-complex pulses. show accurate and stable retrieval is feasible even forWe noise. of presence the in strength modulation temporal the of function a as gratings temporal sinusoidal using characterization pulse of accuracy Kang; Bell Labs, Alcatel Lucent, USA.We analyze the TemporalUsingSinusoidalization Gratings , Accuracy and Stability of Optical Pulse Character FMD6 •3:00p.m. using a2.5-Gbps-grade laser. demonstrated experimentally is subcarrier 16-GHz a to data (RoF) radio-over-fiber of Up-conversion mixer. frequency microwave a as applied is bility insta - under laser semiconductor injected optically An China. Kong, Hong Univ.of City Engineering, Electronic of Dept. Chan; Sze-Chun Cui, Cuicui Fu, , Laser Semiconductor Injected Optically an Using Mixing Frequency Microwave Photonic FMD3 •2:15p.m. FMD •RFPhotonics—Continued California Kiyotaka Sasagawa, Xuelei Inuk Inuk - Monday, October 12 47 Harry Harry Ihee; Steven Steven L. Johnson; Paul Femtosecond Femtosecond pulses of Invited Invited - solu X-ray Time-resolved Hillsborough LSMD • Ultrafast X-Ray X-Ray LSMD • Ultrafast Science I—Continued LSMD3 • 2:30 p.m. LSMD4 • 3:00 p.m. Time-Resolved X-Ray Solution Scattering Reveals Scattering X-Ray Time-Resolved Solution Solution-Phase Structural Dynamics, Korea. of Republic KAIST, struc- direct provides (liquidography) scattering tion tural information generally difficult to extract from ultrafast optical spectroscopy such as molecu- theall of temporal angles and lengths bond of progression intermediates. short-lived specieslar including Watching Atoms Watching Move: Using X-Ray Diffraction to Observe Structural Dynamics in Crystals on Fundamental Time Scales, Scherrer Inst., Switzerland. X-rays generated at a synchrotron offer significant opportunities to study the structural evolution of crystals on fundamental time scales. Here I - pres ent some examples of novel dynamics revealed by probes. X-ray , Ramy , Ramy 1 , Meirav 2 - Green Elad , , Alexander 1 Invited , Mordechai Segev , Mordechai 1 , Yuval , Lamhot Yuval 1 LS Steve Wereley; Purdue Univ., - Technol of Inst. Technion-Israel 1 ; 1 Piedmont , Demetrios N. Christodoulides CREOL, CREOL, College of Optics and Photonics, 2 2 , Yoni Nemirovsky , Yoni 1 We have We recently developed a novel colloidal , Efrat Lifshitz Efrat , 1 , , Carmel Rotschild 1 LSMC • Micro- and LSMC • Micro- I—Continued Nanofluidics LSMC4 • 2:45 p.m. Univ. of Univ. Central Florida, USA. We experimentally controls: optofluidic nonlinear dynamic demonstrate a introduces fluid and light between action symbiotic new class of high-level, entirely optofluidic devices, revealing a self-pulsating light-fluid oscillator and traits. universal with dynamics chaotic ogy, Israel, Israel, ogy, Saraf El-Ganainy field LSMC3 • 2:30 p.m. - Nonlin Symbiotic Optofluidics: Dynamic Complex Chaos, and Self-pulsation, Controls, ear USA. particle manipulation technique that we call Rapid Electrokinetic (REP) Patterning capable of - dynami small as 50 nm. as colloids cally manipulating Massively Massively Parallel Opto/Electric Manipulation of Colloidal Particles, Szameit LSME: Laser I, Science Symposium on Undergraduate Research October 11–15, 2009 • Fairfield Room, Fairmont Hotel (See the Program in your registration bag.) registration your in Program (See the Hotel Fairmont Room, Fairfield Patrick H. Vaccaro; Yale Yale Vaccaro; H. Patrick Invited Invited We describe recent experi - describerecent We Michael Michael D. Barnes, Ruthanne 2:00 p.m.–4:00 p.m. Sacramento The The technique of Cavity Ring-Down
LSMB • Advances in Chiroptical in Chiroptical LSMB • Advances I—Continued Spectroscopy LSMB4 • 3:00 p.m. LSMB3 • 2:30 p.m. Intrinsic Intrinsic Chiroptical Response and Its Mediation Perturbations, Extrinsic by USA. Univ., Polarimetry (CRDP) will be discussed, with special nonresonant of elucidation towards directed emphasis and resonant chiroptical properties under rarified conditions, as well as attendant implications for measurements. condensed-phase canonical Circularly Polarized Luminescence from Single Chiral Molecules, of Univ. Hassey-Paradise, D. - Mas Venkataraman; USA. Amherst, sachusetts from luminescence polarized circularly probing ments single chiral molecules in polymer-supported thin films. Correlation with dissymmetry parameter distributions previously observed in fluorescence discussed. is excitation , , ; 2 1 We , Jason W. , Fleischer Jason W. 1 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 CREOL, College of Optics and and Optics of College CREOL, 2 , Demetrios N. Christodoulides N. Demetrios , 2 , Joyce Lee 1 Atherton Shu Jia, Jason W. Shu Fleischer; Jia, Jason Princeton W. Shu Jia Princeton Univ., USA, Univ., Princeton FMF • Spatial Nonlinearities: FMF • Spatial Beams—Continued Solitons and FMF7 • 3:00 p.m. nm) (~100 Broadband of Compensation Dispersion Laser Pulses for Nonlinear Optical Microscopy Dmitry Pestov, Yair Andegeko, Vadim V. Lozovoy, Marcos Dantus; Michigan State USA. Univ., compensate high-order dispersion of laser laser- pulses a of plane focal the at bandwidth ~100-nm with scanning two-photon microscope. Phase distortion correction accounts for significant increase of two- harmonic second and fluorescence excitation photon signal. generation FMF5 • 2:30 p.m. van Beam, Light a of P. Reflection M. Nonspecular Observing Aiello, A. Merano, M. Woerdman, (Han) P. J. Exter; Leiden, Univ. Netherlands. We present here the first experimental demonstration of angularly nonspecular reflection of a light beam by a the if correction diffractive a planar to due occurs it mirror; 100%. reflectivity below is mirror FMF6 • 2:45 p.m. Nonlinear Light Propagation in - Fractal Wave guide , Arrays USA. Univ., We study nonlinear beam propagation in a fractal waveguide array, created by optically- inducing nested periodic arrays in a self-defocusing photorefractive crystal. Nonlinear mode coupling and energy transport between the folded bands is demonstrated. FMF4 • 2:15 p.m. Nonlinear Airy Beams in Unbiased - Photorefrac tive , Media We experi- USA. Florida, We of Central Univ. Photonics, a of propagation the study theoretically and mentally Airy photorefractive truncated unbiased beaman in crystal. For extraordinary polarization, a solitary- two-wave and diffusion charge between balance wave beam diffraction. suppresses mixing 1 Georgios A. Siviloglou A. Georgios , 4 FiO Univ. of Univ. 2 Matthew , Nicholas J. Oregon State State Oregon 1 2 , Scott B. Gustafson B. Scott , 1,2,3 Duke Univ., Duke USA, Univ., , Yizheng Zhu 1 1 ; 1 Pacific Univ., USA, Univ., Pacific 1 Glen Ellen Glen ; 3 - pre is patients esophagus Barrett’s in Vincent M. Rossi M. Vincent Oregon Oregon Health & Science Univ., USA, , Neil Neil Terry 3 in vivo , Adam Wax 2 VCA VCA Raleigh Hills USA. Hospital, Animal A multi- Shaheen North North Carolina, USA. A clinical angle-resolved low identify to designed system interferometry coherence dysplasia 23 of study clinical a of results the discuss We sented. the device. using patients esophagus Barrett’s Univ., USA, Univ., fiber array is used for diffuse reflectance spectroscopic reflectance diffuse for used is array fiber measurements of visible and near-IR light in bone. resulting fitting by determined are properties Optical spectra versus source-collector fiber separation and absorbers. spectra native of FME5 • 2:45 p.m. and Cost Low for Imaging Light Scattered Multiply , Pathology Subretinal of Detection Flexible S. Muller, Ann E. Elsner, Dean A. VanNasdale, Benno Benno VanNasdale, A. Dean Elsner, E. Ann Muller, S. USA. A Univ., Indiana Optometry, of School Petrig; L. between switch rapidly and easily to technique novel a modes using imaging indirect-scattered and direct inexpensively to applied is aperture electronic rolling degradation. layer retinal of signs detect early FME6 • 3:00 p.m. Angle-Resolved Low Coherence Interferometry DysplasiaBarrett’s in Endoscopicof Detection for Esophagus, 4 FME • Tissue Imaging and Spectroscopy—Continued FME3 • 2:15 p.m. Withdrawn Paper FME4 • 2:30 p.m. - Us Bone of Optical the Properties Characterizing ing a Multi-Fiber Array and Diffuse Reflectance Spectroscopy Steven Steven L. Jacques Monday, October 12 48 entanglement. spatial of photons’degree the to relatedinversely is photonsdown-conversion parametric spontaneous of efficiency collection single-mode the that show experimentally and Wetheoretically USA. LLC, ics, S. Goodman Coupling Single-Mode Optimal and Entanglement Spatial JMA7 •3:15p.m. USA, and MeasurementI—Continued JMA •EntanglementGeneration ______2 Univ.Connecticut,USA, of JOINT FiO/LS , RyanBenninkS. 2 , Andrew T. Ryan Empire 1 , Warren, P. Grice 3 ; 1 Oak Ridge Natl. Lab, 3 Redwood Photon Redwood 1 , Doug , - memristors. resembling properties with nanostructures optical study we media, nonlinear optical second-order with metamaterials combining By fields. optical theoretically examine the notion of memristors with we metamaterials, epsilon-near-zero and negative of Pennsylvania, USA. Using the concepts of epsilon- materials? Meta- UsingMemristor Optical an WeHave Can FMA7 •3:15p.m. Continued FMA •MetamaterialsI— Nader Engheta, Michael E. Young;Univ.E. Michael Engheta, Nader Crystal 3:30 p.m.–4:00p.m. FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Coffee Break,Regency and Imperial Ballroom Foyer, Fairmont Hotel have superior efficiency. cells DWELL area small Consequently,carriers. of recombinationsuppressing diffusion edge bylateral to insensitivity relatively are cells solar (DWELL) dots-in-a-well quantum that found experimentally is it cells, control GaAs to Compared Mexico,USA. Ctr.HighTechnology forter; Materials,Univ. New of MohamedEl-Emawy,A. Andreas Stintz, LukeF. Les- , Cells Solar Dot Quantum Resistance to Edge Recombination in InAs/InGaAs FMB5 •3:15p.m. Energy—Continued FMB •OpticsforRenewable NOTES Gold igi u Ki Yang, Kai Gu, Tingyi • October 11–15,2009 FiO distribution and its single parameter scaling. whilst preserving the universalitypath of free the conductance mean transport of reduction a in results propagation wave in modes evanescent of account proper that demonstrateWeTechnology, USA. and Mahler,Yamilov;G. Alexey Missouri Univ. Scienceof bution in Disordered Waveguides, Effect of Evanescent Modes on Conductance Distri - FMC6 •3:15p.m. Continued I— FMC •AndersonLocalization Valley Ben Ben Payne, Tom single disc structure modulatingsingle disc when at FSR. the a to compared bandwidth and sensitivity the both RF-optical modulators have been analyzed resonant,to enhance diameter), of ratio (1:2 dual-disc optical H. Steier; Univ. of Southern California, USA. Electro- Resonators, ModulatorsResonant FSROptical Using Coupled of Product Sensitivity-Bandwidth the Increasing FMD7 •3:15p.m. FMD •RFPhotonics—Continued Yoo Seung Lee, Sang Shin Lee, WilliamLee, Shin Sang Lee, YooSeung California Monday, October 12 49 Hillsborough LSMD • Ultrafast X-Ray X-Ray LSMD • Ultrafast Science I—Continued LS Piedmont LSME: Laser I, Symposium on Undergraduate Research Science October 11–15, 2009 • Fairfield Room, Fairmont Hotel (See the Program in your registration bag.) registration your in Program (See the Hotel Fairmont Room, Fairfield NOTES 2:00 p.m.–4:00 p.m. Sacramento LSMB • Advances in Chiroptical in Chiroptical LSMB • Advances I—Continued Spectroscopy Regency and Imperial Ballroom Foyer, Fairmont Hotel Fairmont Foyer, Ballroom Imperial and Coffee Break, Regency P. Ben P. Dixon, David FiO/LS/AO/AIOM/COSI/LM/SRS 2009 3:30 p.m.–4:00 p.m. Atherton FMF • Spatial Nonlinearities: FMF • Spatial Beams—Continued Solitons and FMF8 • 3:15 p.m. Interferometric via Measurement Deflection Beam Weak Value , Amplification J. Starling, J. Andrew N. Starling, Jordan, John C. Howell; Univ. of USA. Rochester, We report on the use of an in- terferometric weak value technique to amplify very small transverse deflections of an optical beam. We measured the linear travel of a piezo actuator down 20 femtometers. to , FiO 2,3 , Jennifer Jennifer , 2 College of Optical Optical of College 2 Dept. Dept. of Electrical 3 , Raymond K. Kostuk K. Raymond , , Erich De Leon De Erich , 2,3 2 MIT, USA, MIT, 1 ; 1,4 Glen Ellen Glen , Paul J. Gelsinger J. Paul , 1 , Jennifer K. Barton K. Jennifer , 2 ______Singapore-MIT Singapore-MIT Alliance for Res. and Technology and and Computer Engineering, of Univ. Arizona, USA, A spatial-spectral multiplex multiplex spatial-spectral A Singapore. Ctr., (SMART) volume holographic pupil with phase contrast is information highused frequency enhance feature to of biological structures. We demonstrate imaging by with performance illuminated biological samples time. in real LED an Harwell 4 FME • Tissue Imaging and Spectroscopy—Continued FME7 • 3:15 p.m. Microscope, Phase Contrast Volume-Holographic Luo Yuan George Barbastathis George Sciences, Univ. Sciences, of Univ. Arizona, USA, Monday, October 12 50 resonant excitation are predicted. upon contrast transmission dB 15 and % 70 above collection Photoluminescence dipole. the to access fiber optical efficient, highly providing waveguide optical an in embedded emitter single a investigate Univ. of Maryland at Baltimore, USA. We theoretically quantum photonic circuits. silica-on-silicon integrated optical realizations of key high-fidelity demonstrateWe scalability. and tion architectures for improved performance, miniaturiza- based on photons will likely require integrated optics O’Brien;Univ. ofBristol, UK. Andre Stefanov, Siyuan Yu, Mark G. Thompson, Jeremy MariaZhou,MartinRodas, JohnJ.Cryan, Rarity, G. Matthews, Anthony Laing, Pruet Kalasuwan, Xiao-Qi Chip, a onPhotons with Information QuantumScience ence and Technology, NIST, USA, FMG1 •4:00p.m. USA, Presider Prem Kumar; Northwestern Univ., Waveguides I FMG •QuantumOpticsin 4:00 p.m.–6:00p.m. Davanco , Dipole Quantum Single a to Interface WaveguideFiber-Based Optical Efficient, An FMG2 •4:30p.m. Alberto Peruzzo, Alberto Politi,Peruzzo,AlbertoAlbertoJonathanF. C. 1,2 , , Kartik Srinivasan Empire Invited 1 Quantumtechnologies ; ; 1 Ctr. for Nanoscale Sci 2 Maryland NanoCtr., Marcelo I. Marcelo FiO - investigate coupling their properties. ties of three-dimensional metallic metamaterials and Germany. Matters, pling - Metamaterials:Cou Metallic Three-Dimensional ously reported. previ- that higher much measured, is 1340x to up single-molecule’sfactors bya emission fluorescence doped into a thin polymer layer, the enhancement of molecules fluorescent with nanoantenna bowtie Germany. A. Kinkhabwala A. Nanoantenna Bowtie , a by Produced ments - Enhance Fluorescence Single-Molecule Large FMH2 •4:30p.m. Univ.,USA, FMH1 •4:00p.m. Ossietzky Univ., Germany, Presider Christoph Lienau; Carl von FMH •MetamaterialsII 4:00 p.m.–5:45p.m. Avlasevich
By coating a lithographically-fabricated a coating By We are going to discuss the optical proper 2 , Klaus Mullen 2 Max-Planck-Inst. for Polymer Res., Res., Polymer for Max-Planck-Inst. Harald Giessen; Univ. of Stuttgart, Stuttgart, of Univ. Giessen; Harald 1 , Zongfu Yu Zongfu , Crystal 2 Invited , W. E. Moerner FiO/LS/AO/AIOM/COSI/LM/SRS 2009 1 Sahi Fan Shanhui , 1 ; 1 Stanford 1 Anika Anika , Yuri Yuri , - JMB1 •4:00p.m. ing and future instruments. how interferometric detectors work, and review exist- astrophysical and cosmological sources. I will explain and study gravitational waves emitted by a variety of MIT, USA. GravitationalWave Interferometry, Presider Rana Adhikari; Caltech, USA, I Interferometers JMB •GravitationalWave 4:00 p.m.–6:00p.m. scientist of Advanced the LIGO project. Massachusetts Institute of Technology. He is the chief Peter Fritschel is a Principal Research Scientist at the Thank youforattending know yourthoughtson post-conference survey FiO/LS/Fall Congress. JOINT FiO/LS via emailandletus Gravitational wave detectors aim to detect Look foryour the program. Gold Tutorial • PeterFritschel; October 11–15,2009 present presented. worldwide be also efforts will and kJ petawatt peak power laser systems. A survey of femtosecond both for technologies present reviews and amplification pulse laser duration ultrashort USA. Lab, tions, - Technologies:Direc New PowerPeakLaser High Presider to Announced Be Technology I FMI •HighPeak Power Laser 4:00 p.m.–5:45p.m. lasers andlasers X-ray applications. Society for his pioneering work on intense short-pulse Optical TheFellow of a elected physics.Hewas and engineering chemistry,medicine, science, materials optics, lasers, in topics spanning talks, invited 100 over presented and manuscripts approximately150 published has He Lasers. Intensity Ultrahigh on Committee International the of Co-Chair the is he Conference on Ultrahigh Intensity Lasers. Currently,International the and Optics Ultrafast on meeting career he has founded both the biennial international ing from North Carolina State University. During his honors in chemistry, physics and chemical engineer Stanfordfrom University with bachelordegreesand physics applied in degrees M.S. and Ph.D. includes more National Laboratory. His academic background Science and Applications Program at Lawrence Liver Dr. C. P. J. Barty is the Program Director of the Photon FMI1 •4:00p.m. Christopher Barty; Lawrence Livermore Natl.Livermore Lawrence Barty; Christopher This tutorial introduces the basics of basics the introduces tutorial This Valley Tutorial FiO - - rable FOG. compa - a of that than lower significantly is which rate, rotation detectable the on bound lower a sets expression for the exponential sensitivity. Shot-noise derive and gyroscopes, CROW degenerate-modes of performance the TelUniv.,AvivWestudyIsrael. formanceAnalysis, PerGyro: Exponential Base Structure Light Slow FMJ3 •4:30p.m. of Michigan, USA, of Electrical Engineering and Computer Science, Univ. An average sensitivity deflection of 0.32×10 aY-branchsplitter.and waveguide rib multimode double-step asymmetric an of consisting splitter transductionof microcantilevers differentialusinga Brigham Young Univ., USA. We report the all-photonic P.GregoryKim, SeunghyunNordin;RyanAnderson, Waveguide, Rib Double-Step a UsingSplitter Differential a by Arrays cantilever Micro- of Transduction All-Photonic In-Plane FMJ2 •4:15p.m. fringe measurements were demonstrated. white-light Laboratory applications. tracking fringe andon-chiphad electro-opticmodulation phase for band L at operated device The waveguides. niobate nomical beam combiner was fabricated using lithium astro- mid-infrared, optic, integrated An USA. gan, Presider Wan Kuang; BoiseState Univ., USA, FMJ •IntegratedOpticalSensors 4:00 p.m.–6:00p.m. demonstrated for multiple microcantilever arrays. kai Hsiaokai Combiner Beam for Stellar Interferometry, Astronomical Optic Integrated Mid-Infrared A FMJ1 •4:00p.m. 1 , Kim, WinickA. 2 California Dept. of Astronomy, Univ. of Michi of Univ. Astronomy, of Dept. Ben Z. Steinberg,Z. Ben Jacob Scheuer; 1 , John, D. Monnier Jong Wook Noh, Noh, Wook Jong -3 2 nm ; Hsien- 1 Dept. -1 is is - - Monday, October 12 51 Yves Yves We have Invited Invited . Sorgenfrei, W. F. Schlotter, Schlotter, F. F. Sorgenfrei, W. A spin-polarized current can be can current spin-polarized A Hillsborough 4:00 p.m.–5:45 p.m. 4:00 p.m.–5:45 Science II X-Ray LSMH • Ultrafast Accelerator Natl. SLAC Fritz; David Presider USA, Univ., Stanford Lab, LSMH2 • 4:30 p.m. LSMH1 • 4:00 p.m. Magnetization Magnetization Dynamics on the Nanoscale, Lab, Accelerator Natl. SLAC PULSE Inst., Acremann; USA. Univ., Stanford used to reverse the magnetization of a ferromagnet. We observed the switching mechanism involved in spin transfer devices using time resolved x-ray microscopy. Ultrafast Ultrafast X-Ray Physics with the X-Ray Split and Föhlisch; A. Delay Unit at FLASH, Wurth, W. Beeck, T. Beye, M. Nagasono, M. Ctr. and Hamburg Univ. Experimentalphysik, für Inst. for Free-Electron Laser Science, Germany. split X-ray femtosecond a implemented and designed and delay unit based on grazing incidence Mach- Zehnder optics at the Free-Electron-Laser at - Ham burg (FLASH), which generates through the SASE radiation. soft X-ray coherent intense, mechanism - Polytechnic 2 , Stephen Ar Stephen , 1 Binding Binding of Influenza A Invited Invited Frank Vollmer Frank LS Piedmont Daniel T. Chiu; Univ. of Washington, USA. of Washington, Univ. Chiu; T. Daniel Rowland Inst., Harvard Univ., USA, Univ., Harvard Inst., Rowland 1 ; 2 4:00 p.m.–6:15 p.m. 4:00 p.m.–6:15 II and Nanofluidics LSMG • Micro- Illinois, of C. Bailey; Univ. Ryan USA, Presider LSMG1 • 4:00 p.m. Inst., New York Univ., USA. Inst., New Univ., York virus particles is detected from the frequency shift of of shift frequency the from detected is particles virus posed limitations overcome To cavity. microsphere a sensing the to nanoparticles of transport diffusion, by forces. gradient optical by enhanced is region LSMG2 • 4:30 p.m. Optical Microcavities: Label-Free Detection downDetection OpticalMicrocavities:Label-Free Particles, Virus Single to Optical and Microfluidic for Techniques Cellular Analysis, The presentation will highlight some of the recent work in our lab that optical integrates - instrumenta biological studying for devices microfluidic with tion resolutions. single-cell with systems nold LSMI: Laser II, Science Symposium on Undergraduate Research , Bart 2 October 11–15, 2009 • Fairfield Room, Fairmont Hotel (See the Program in your registration bag.) registration your in Program (See the Hotel Fairmont Room, Fairfield , Erica Gunn Univ. of Washington, of Washington, Univ. 2 1,2 Invited Invited 4:30 p.m.–6:30 p.m. Sacramento John John Freudenthal Ellen Gualtieri, Victoria Hall, Sarah Harden, Harden, Sarah Hall, Victoria Gualtieri, Ellen New York Univ., USA, Univ., York New 1 ; Mueller matrix microscopy is matrix usedmicroscopy Mueller to evaluate 1,2 Kahr LSMF2 • 4:30 p.m. 4:00 p.m.–5:30 p.m. 4:00 p.m.–5:30 in Chiroptical LSMF • Advances II Spectroscopy of Univ. Barnes; Michael USA, Amherst, Massachusetts Presider LSMF1 • 4:00 p.m. USA. the heterogeneities and anisotropies in the circular birefringence and circular dichroism of crystalline materials. Chiroptical Imaging of Crystals by Mueller Matrix Matrix Mueller by Crystals of Imaging Chiroptical Microscopy, Chiral of Imaging Optical Nonlinear Second-Order Crystals, David Kissick, Ronald Debbie Wampler, Wanapun, Garth J. Simpson; Purdue USA. Univ., All chiral second-harmonic symmetry-allowedfor crystalsare - detec selective and sensitive a providing generation, tion approach for characterizing protein crystals and crystals of active pharmaceutical ingredients. described. are applications and Methods , - 1 , S. 1 , , N. Alic 2 , , M. L. Cooper 1 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Univ. of Univ. California at San Invited 1 ; ; 1 , , I. B. Divliansky 1 , , S. Zlatanovic Atherton 1 CREOL, CREOL, College of Optics - and Photon 2 , , S. Radic 1 Luca Dal Negro; Boston Univ., USA. Luca Dal In thisBoston Negro; Univ., J. J. S. Park , Diego, Diego, USA, FML2 • 4:30 p.m. Mixing Two-Pump Four-Wave in - Silicon Wave guides 4:00 p.m.–6:00 p.m. 4:00 p.m.–6:00 Photonics I FML • Silicon College CREOL, Fathpour; Sasan of Univ. Photonics, and Optics of USA, Presider Florida, Central ics, Univ. ics, of Univ. Central Florida, USA. We report dual- pump four-wave mixing in silicon waveguides and demonstrate generation of up to 10 sidebands with self-seeded higher order pumps. A conversion ef ficiency of -8.38dB was measured between the signal the between measured was -8.38dB of ficiency idler. phase-conjugated and FML1 • 4:00 p.m. J. J. M. Chavez-Boggio Mookherjea - Deterministic Aperiodic Nanoplas Structures for monics, - photolumines light scattering, combining by paper, cence, Raman and near-field optical measurements with accurate electrodynamics calculations I will specific and nanofabrication EBL design, the discuss - deterministic aperiodic nano of device applications (DANS). structures plasmonic , 3 FiO We , S. R. 2 Anasys Anasys Univ. of of Univ. 4 2 , A. Dazzi 2 , J. H. Rice , J. 2 Invited Hyunmin Hyunmin Kim, Eric Olaf , G. A. Hill , M. M. Reading 1 2 Stanford Univ., USA, Univ., Stanford 1 ; 4 Univ. Paris-Sud, Univ. France, 3 Glen Ellen Glen , C. Prater 4 , D. Q. M. Craig 2 East East Anglia, UK, FMK1 • 4:00 p.m. 4:00 p.m.–6:00 p.m. 4:00 p.m.–6:00 and OCT I FMK • Microscopy Biomedical of Dept. Wax; Adam USA, Univ., Duke Engineering, Presider Instruments Instruments Inc., USA. We performed nanoscale - chemi with imaging surface microscope force atomic cal identification and spatial resolution of 200 nm. The detection mechanism was based on recording resonant oscillations in the cantilever induced by a mid-IR excitation. tunable FMK2 • 4:30 p.m. Nano-Spectroscopy in the 2.5-10 - Micron Wave length Range Using Atomic Force Microscope, Konstantin Vodopyanov K. Kjoller Meech demonstrate demonstrate that four-wave-mixing microscopy is a convenient method for visualizing the nonlinear properties of individual nano-structures, and that it offers a route towards probing the ultrafast spatio- temporal dynamics of fundamental excitations in nanomaterials. Nonlinear Coherent Imaging of Nanostructures and Single Molecules, Potma; of Univ. California at Irvine, USA. Monday, October 12 52 Bromberg Lattices, Waveguide in Optics Quantum Regine Schmidt Regine Michael Morrissey coupled waveguides and simple input states. using periodic and a-periodic lattices of evanescently complex quantum correlations between photon pairs, Canada. present results for waveguides. leaky Welight. squeezed photons mode single two or also waveguides. The waveguides can be fed in by pairs of silica coupled in entanglement of evolution on reportWe Univ., USA. StateOklahoma Agarwal; S. Waveguides, Coupled in Entanglement Non-Gaussian and Gaussian FMG5 •5:30p.m. Laura Russell Laura ToolsAtomas Optics, in Fibers Optical Ultrathin FMG3 •4:45p.m. Waveguides I—Continued FMG •QuantumOpticsin Silberberg of rubidium vapor pressure is studied. rubidium atoms. The atom coldcloud ofprofile cloudas a a function of characteristics the probe to fiber optical tapered a using obtained resultsWe present Natl.Inst., Ireland, FMG4 •5:00p.m.
We study the generation and manipulation of 1 1 , Yoav Lahini ; 1 WeizmannInst. ofScience, Israel, 1,2 2 , Sile Nic Chormaic ; 1 Univ. College Cork, Ireland, 2,3 3 , Amy Watkins Cork Inst.Cork Technology,of Ireland. Empire 1 , Roberto Morandotti Amit Rai, Sumanta Das, G. G. Das, Sumanta Rai, Amit Invited 1,2 1,2 , Mary Frawley Mary , , Kieran Deasy 2 2 Tyndall Tyndall , Yaron 2 Yaron Yaron INRS, 2,3 1,2 FiO , , Theodore D. Moustakas D. Theodore Emmanouil Dimakis via plasmonicvia waveguides. links with compared as loss less much exhibit may distance given a at nanoantennas two between link wireless optical the that demonstrate theoretically we elements, nanocircuit using nanoantennas cal Texasof atAustin,properlyBy matching USA. opti - Silver Nanoparticles Silver Synthesized Chemically UsingWells Quantum InGaN from Emission Light Plasmon-Enhanced FMH4 •5:00p.m. merically calculated and calculated merically confirmed. experimentally Field intensity enhancement of LSP samples was nu- subwavelength patterns such as gratings and islands. improve total internal reflection microscopy based on localized surface plasmon (LSP) enhanced Kim; Yonsei Univ., Republic of Korea. We investigated Patterns, SubwavelengthVarious on Based Cells Live of Imaging Enhanced Plasmon Surface Localized FMH5 •5:15p.m. tained from InGaN quantum wells. ob- correspondingly are enhancements efficiency in flexible resin films. Substantial photoluminescence chemically synthesized silver nanoparticles embedded plasmonic nanostructures is demonstrated, based on to materials light-emitting solid-state couple to ta PlasmonicWaveguide Connections? with Compete Links Nanoantenna Optical Can FMH6 •5:30p.m. Univ., USA, hancement wideband TPE of spectrum. very the en- nonlinear for ideal are nano-cavities plasmonic of a plasmonic-nanoantenna. It is demonstrated that semiconductor two-photon emission to the near field We present two-surface plasmon emitter by coupling Technion-IsraelOrenstein; Technology,ofInst. Israel. Alex Hayat, Pavel Ginzburg, Nikolai Berkovitch, Meir Nanoantennasto Coupling byductor , - Semicon from Emission Plasmon Two-Surface FMH3 •4:45p.m. Continued FMH •MetamaterialsII— 1 , Andrea, Alù Kyujung Kim, Dong Jun Kim, Donghyun Donghyun Kim, Jun Dong Kim, Kyujung 2 Clemson Univ., USA. A simple technique 2 ; 1 Univ.Pennsylvania,of USA, 1 Crystal , Josh Abell Josh , , John Henson John 1 , Roberto Paiella Roberto , FiO/LS/AO/AIOM/COSI/LM/SRS 2009 1 , George Chumanov 1 , John HeckelJohn , NaderEnghe - AmirNevet, imaging to 1 ; 1 Boston Boston 2 Univ. 2 2 , , Daniel Shaddock Daniel WavesGravitationalSpace, fromDetecting LISA: spectral-density spectral-density of resolution is 6 x Bondu; Univ. de Rennes 1, France. WaveDetector,Gravitational Virgo The LISA measurement concept. space. This presentation will provide a tutorial of the in detector wave gravitational dedicated first the be will mission,NASA/ESAjoint a (LISA), antenna Natl. Univ., Australia. The laser interferometer space JMB4 •5:30p.m. optical-technologies. Virgo advanced discuss Wecontrol.interferometer coatings, laser frequency and amplitude stabilizations, Hz.. We show the performances of mirror surfaces and for inLISA. use materials various of stability the of measurements Wepresenttelescopes. will the and benches, optical the cavities, reference the as such structures stable ultra- several requires LISA USA. Florida, Univ.of Material Tests for LISA, JMB3 •5:15p.m. JMB2 •4:45p.m. Interferometers I—Continued Interferometers JMB •GravitationalWave JOINT FiO/LS 1,2 ; 1 JPL, Caltech, USA, Caltech, JPL, Gold Alix Preston, Guido Mueller; Invited Invited The interferometer 10 • -23 1/ 2 √HZ at 250 Australian October 11–15,2009 François anticipated programme. scientific its facility,including VulcanPW existing the on ity capabil- PW 10 a establish to plans our discuss and highlights from the UK’s high power laser programme ics, Swansea Univ., UK. Blanc Power Laser Programme, Laser Power High UK’s the of Activities the of Overview An Bottlenecks”, Laser Associated “The APOLLON/ILE: Prototype Its InfrastructureThe ExtremeProject Light ELI and Paillard École Polytechnique, UMS 3205, France, François Mathieu François 8501 Inst. d’Optique, Campus de Polytechnique, France, Georges FMI2 •4:45p.m. 4 3 (STFC), Rutherford Appleton Lab, UK, Laser Facility, Science and Technology Facilities Council ated described. technological be bottlenecks will Associ- presentlyconstruction.APOLLON isunder ILE/ called prototype laser beamline single French A infrastructure. users physicsintensity high based laser 200PW a in consistingProject ELI the present FMI3 •5:15p.m. Technology I—Continued FMI •HighPeak Power Laser LOA, ENSTA-École Polytechnique, UMR 7639, France, LULI, UMR7605, École Polytechnique, France. 4 , Patrick Audebert Patrick , 2 4 , Gilles Chériaux Gilles , Ptik Cavillac Patrick , 1 Grr Mourou Gérard , Valley en al Chambaret Paul Jean I will review recentreview I will scientific 4 Invited Invited 3 , Denis Douillet Denis , , Gilles Rey Gilles , 1 Dmnqe Fournet Dominique , John Collier John 1 ; 3 , Catherine Le Le Catherine , 2 1 2 Dept. of Phys- ILE, ENSTA-ILE, LCFIO, UMR 1,2 3 , Jean Luc Jean , ; 1 , Patrick Patrick , 1 Central Central We will FiO 1 , observed sensitivity was ~85 pm/ ~85 was sensitivity observed The radius. ring 4-μm a with resonator ring silicon a utilizing implemented and proposed was sensor temperature small ultra An Korea. of RepublicCtr., sensor measurements. The fast sweep time enables improveddemonstrated. time-resolved is μS 10 than less in resolution nm that can scan the 1525 nm to 1575 nm range with .001 technic State Univ., USA. A sensor interrogation source Shane O’Connor, Dennis J. Derickson; California Poly- Distributed Bragg Reflector , Lasers with 10 μS Sweep Period Utilizing Sampled Grating Interrogation Sensor Swept-Wavelength Optical FMJ5 •5:00p.m. Aaron R. Hawkins range around room the temperature. Sensor TemperatureResonator Silicon Small Based Ultra FMJ6 •5:15p.m. external (off-chip)external components. sensitivity to fluorescence signals without the need for filtering. These integrated filters can provide optical increased on-chip localized, for means the provides optofluidicanonsensor films thin dielectric oftion - deposi Selective USA. Cruz, Santa at California of 1 Lee Phillips , Sensors Optofluidic in Filters Notch Integratedfor Films Thin of Deposition Selective FMJ7 •5:30p.m. results are presented. fabrication and experimental Preliminary formed. per are analysis sensitivity and characterization, Optimization, analyzed. and presented is analytes of detection microfluidic for gratings diffraction on-insulator optical sensor design based on in-plane silicon- integrated compact, A Tech,USA. Georgia , Design Sensor Diffractive Silicon-on-Insulator Compact FMJ4 •4:45p.m. Sensors—Continued FMJ •IntegratedOptical Kwangwoon Univ., Republic of Korea, 1 , Boo-Taek Lim , 1 , Yue Zhao Gun-Duk Kim Gun-Duk Jonathan S. Maikisch, Thomas K. Gaylord; K. Thomas Maikisch, S. Jonathan 1 California ; 2 1 1 , Hee-Kyoung Bae , Philip Measor Brigham Young Univ., USA, 1 , Hak-Soon Lee Hak-Soon , 2 , Holger Schmidt o C over the 38 the over C 2 Brandon George, , Wan-Gyu Lee 2 Natl. NanoFab 1 , Sang-Shin , Brian S. S. Brian 2 Univ. o C 2 2 - , ; Monday, October 12 53 , Victor Victor , 1 Moscow 2 Mikhail N. Mikhail I will how fs show X-ray Invited , Vitaly Yakimenko Vitaly , Laser Pulses , 1 2 laser cavity. Proof-of-principle 2 Brookhaven Natl. Lab, USA, Lab, Natl. Brookhaven Hillsborough 1 ; 2 Hermann Hermann A. Dürr; Helmholtz Zentrum , Igor Pogorelsky Igor , 1 LSMH • Ultrafast X-Ray X-Ray LSMH • Ultrafast Science II—Continued experiments experiments combined with computer simulations allow evaluating the promise of this approach for applications. various LSMH3 • 5:00 p.m. T. Platonenko T. Polyanskiy High-repetition-rate High-repetition-rate Federation. Russian Univ., State gamma-source concept is based on Compton - back scattering from the relativistic electron beam inside a picosecond CO LSMH4 • 5:30 p.m. Scat- Compton on Based γ-Source High-Repetition tering of Picosecond CO Ultrafast Electron and Spin Dynamics in Complex in Dynamics Spin and Electron Ultrafast Materials, II, BESSY Berlin, Germany. pulses can probe the dynamical interplay between electronic, spin and lattice degrees of freedom materials complex of function the determines which such as ferromagnets, highly correlated transition metal oxides. , ; - 1 1 Alan J. Hunt; Univ. Univ. Hunt; J. Alan Sergey Mozharov , David Littlejohn 2 Durham Univ., Durham UK. Univ., Ra Invited 2 LS Piedmont Taking advantage of precise damage damage precise of advantage Taking , John Girkin 1 Univ. of Univ. UK, Strathclyde, LSMG • Micro- and LSMG • Micro- II—Continued Nanofluidics man man spectrometry is currently not well adapted for rapid process control in microreactors. We report an efficient low-cost Raman probe capable of rapid optimisation and monitoring of chemical reactions the microchip. of point any at 1 LSMG3 • 5:00 p.m. A Compact Raman Probe for Rapid Reaction Monitoring in , Microreactors Alison Nordon of Michigan, USA. Michigan, of for devices fluidic construct we lasers, femtosecond by demonstrate We diagnostics. and analyses biomedical lab-on-a-chip components for integrated chemical analysis, micro scale sensors, and nanopores for sensing. resistive-pulse and patch-clamp Ultrafast Ultrafast Laser of Nanomachining Analytical and Devices,Biomedical Diagnostic LSMG4 • 5:15 p.m. LSMI: Laser II, Science Symposium on Undergraduate Research October 11–15, 2009 • Fairfield Room, Fairmont Hotel (See the Program in your registration bag.) registration your in Program (See the Hotel Fairmont Room, Fairfield Mohan Mohan Srinivasarao; Invited Iridescent Iridescent metallic green beetle, 4:30 p.m.–6:30 p.m. Sacramento LSMF • Advances in Chiroptical LSMF • Advances II—Continued Spectroscopy LSMF3 • 5:00 p.m. Structural Origin of Circularly Polarized - Iri descence in Jeweled Beetles, USA. Georgia Tech, Chrysina gloriosa selectively reflects left circularly polarized light, possesses an exoskeleton decorated cells (~10μm). These structures hexagonal nearly by are analogous to defects on the free surface of a fluid. cholesteric
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, Luca Luca , 2 , Maria 1 Univ. College Univ. 1 , Rui Li Rui , 2 We present a ; 2 Dept. of Electrical Electrical of Dept. 2 Nicolae C. Nicolae Panoiu , Philippe M. Fauchet M. Philippe , FiO/LS/AO/AIOM/COSI/LM/SRS 2009 2 Jelena Jelena Vučković Invited , Selcuk Yerçi Selcuk , 1 Inst. of Optics, Univ. of Rochester, Rochester, of Univ. Optics, of Inst. 1 , Chee Wong Wei Atherton ; 2 1 Columbia Univ., Columbia USA. Univ., Dept. Dept. of Electrical Engineering and 2 1 , Jonathan Y. Lee 1 ; 2 , Yiyang Gong Yiyang , 1 Ali W. Elshaari, Preble; Rochester Stefan Ali F. W. , , respectively. Dept. Dept. of Electrical and Engineering, Computer -2 2 g v FML • Silicon FML • Silicon I—Continued Photonics USA, London, London, UK, Makarova Ginzton Lab, Stanford Univ., USA, Univ., Stanford Lab, Ginzton FML6 • 5:30 p.m. We present a present delay tunable USA. We of Technology, Inst. element that is inherently insensitive to free-carrier when even delays nanosecond to up achieves and loss tuned slowly. This will enable electrically tunable chip. a silicon on buffers FML3 • 4:45 p.m. Nanosecond Optical Tunable Delay Using Silicon Cavities and and Computer Engineering, Boston USA. Univ., demonstrated demonstrated enhancement of light emission from crystal silicon Er-doped photonic as cavities, well as cavity linewidth narrowing with increasing optical pump power at — low temperature an indication of in the system. gain differential Dal Negro rigorous theoretical rigorous and numerical analysis of pulse in propagation silicon photonic crystal waveguides, showing that in the slow-light regime linear as and group-velocity the on depend effects nonlinear We demonstrate that cross- demonstrate USA. We of Rochester, Univ. phase modulation induced nonlinear polarization- can rotation be used to realize sub-picosecond Kerr switching in a silicon waveguide using only a results experimental Our few power. peak pump of watts theory. with agree FML5 • 5:15 p.m. Propagation of Picosecond Pulses in Silicon - Pho tonic , Crystal Slab Waveguides FML4 • 5:00 p.m. , Switch Kerr Silicon Ultrafast an of Realization Yin anghong Govind Agrawal P. McMillan James F. and Erbium Doped Silicon Photonic Crystals for Light Crystalsfor Photonic Silicon Doped Erbium Sources and Amplifiers, - - FiO Jonathan M. Jonathan We present transfer Alexei V. Sokolov, Alexei Xi Sokolov, V. Wang; Glen Ellen Glen Shalin B. Mehta, Colin J. R. Sheppard; Sheppard; R. J. Colin Mehta, B. Shalin Sri Sri Rama Prasanna Pavani, Rafael Piestun; , FMK6 • 5:30 p.m. Function Transfer Analysis of Partially Coherent - Quanti for Evaluation and Methods Imaging Phase , Imaging tative Natl. of Bioengineering, Div. Lab, Bioimaging Optical of Univ. Singapore, Singapore. function based analysis of contrast generated by various partially coherent phase imaging methods with emphasis on nature quantitative of differential phase contrast (DPC) and differential interference (DIC). contrast FMK • Microscopy and FMK • Microscopy OCT I—Continued FMK3 • 4:45 p.m. Resonant a Using Spectroscopy CARS Single-Pulse Photonic Crystal Slab Filter (RPCS), Levitt, simple a Ori present Katz,We Israel. Eran Science, of Grinvald, Inst. Yaron Silberberg;Weizmann spec - vibrational single-beam performing for scheme troscopy with a single femtosecond pulse without a pulse-shaper. High-resolution microspectroscopy nar a using demonstrated is imaging vibrational and RPCS filter. an defined by probe rowband FMK5 • 5:15 p.m. 3-D Superlocalization with Double-Helix Micro scopes of Univ. Colorado at Boulder, USA. Double-helix microscopes localize the three-dimensional (3-D) position of multiple particles with nanometer-scale be can operated and image, single a using precisions bright-field, as such modalities microscope in directly dark-field, fluorescence, and PALM/STORM/F- nanoscopy. type superresolution PALM We use timed USA. femtosecond We A&M Univ., Texas laser pulses to demonstrate effective doubling of spatial resolution with which Raman coherence - micros CARS is for implications discuss and prepared, with copy, potential extensions to far-field imaging diffraction. by limited not FMK4 • 5:00 p.m. Far-Field Sub-Diffraction-LimitedToward CARS Microscopy via Molecular Coherence Driven by a Short-Pulse Sequence, Monday, October 12 54 two-photon transparency point. the to down injection current by reducedgressively transparency.pro- one-photonis luminescenceThe two-photon gain and lasing - namely the two-photon nonlinear based semiconductortowards step major Technology,Israel. We demonstrate a experimentally Technion-IsraelOrenstein; ofMeir Inst. Nevet,Amir Wells , Quantum Semiconductor in Injection Current by TransparencyTwo-Photon FMG6 •5:45p.m. Waveguides I—Continued FMG •QuantumOpticsin ______Empire Alex Hayat, Hayat, Alex 6:30 p.m.–8:30p.m. FiO OSA StudentMemberReception, O’Flaherty’s Irish Pub, 25N.Pedro Street, San Jose, California 95110,Phone: 408.947.8007 Crystal FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Interferometers I—Continued Interferometers JMB •GravitationalWave JOINT FiO/LS NOTES Gold • October 11–15,2009 Valley FiO of minimum the dip occurs. bifurcation or splitting a wavelength, critical the At non-lineardivergesworkinginfinity.andpointtois where the spectral sensitivity close to a certain critical Goldring;Tel Aviv Univ., reported is Israel. effect An ometer , Sensor Critical Sensitivity Effect in a Waveguided Interfer FMJ8 •5:45p.m. Sensors—Continued FMJ •IntegratedOptical Ronen Levy, Shlomo Ruschin, Damian California - Monday, October 12 55 Hillsborough
- Jacob C. Stephen Invited LS Piedmont LSMG • Micro- and LSMG • Micro- II—Continued Nanofluidics Nanofluidic Nanofluidic channels integrated into microfluidic - trans ion studying for platform unique a offer devices these fabricate to method a present We behavior. port - simultane permits which in-plane, devices integrated electrical and optical characterization. ous son, John M. Perry, Kaimeng Zhou; Indiana Univ., USA. Univ., Indiana Zhou; Kaimeng Perry, M. John son, Optical and Electrical Characterization of Fluid Channels, Nanoscale in Transport LSMG5 • 5:45 p.m. LSMG5 • 5:45 LSMI: Laser II, Symposium on Undergraduate Research Science October 11–15, 2009 • Fairfield Room, Fairmont Hotel (See the Program in your registration bag.) registration your in Program (See the Hotel Fairmont Room, Fairfield NOTES 4:30 p.m.–6:30 p.m. Sacramento FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Atherton O’Flaherty’s Irish Pub, 25 N. Pedro Street, San Jose, California 95110, Phone: 408.947.8007 Phone: 95110, California Jose, San Street, 25 N. Pedro Pub, Irish O’Flaherty’s Reception, OSA Student Member FML • Silicon FML • Silicon I—Continued Photonics FiO 6:30 p.m.–8:30 p.m. Glen Ellen Glen Raghu Ambekar Ramachandra Rao, Rao, Ramachandra Ambekar Raghu ______FMK • Microscopy and FMK • Microscopy OCT I—Continued FMK7 • 5:45 p.m. Quantitative Fourier Analysis of SHG Images of Cornea , Porcine Monal R. Mehta, Kimani C. of Jr.; Univ. Toussaint, analysis Fourier USA. Urbana-Champaign, at Illinois is applied to cornea images obtained using second- harmonic generation microscopy. The orientation in fibrils collagen of frequency spatial maximum and determined. are interest of selected regions Tuesday, October 13 56 Started 3-D Entertainment: A Revolution that has Already challenges and rewards. worldwide. I will discuss the current state-of-the-art, companies products optical to opportunities huge bring soon will industry entertainment the from change of wave This begun. has entertainment 3-D FTuA1 •8:00a.m. FTuA1 Univ. of Arizona, USA,Presider Hong Hua; Optical Sciences Ctr., Marketplace •3-DEntertainmentinthe FTuA 8:00 a.m.–9:30a.m. , Rod Archer; RealD Inc., USA. Inc.,RealDArcher; Rod Empire Keynote A new era of era new A FiO metamaterial structure. or in semiconductor materials incorporated into the substrate semiconductor the in excitation photo or depletion carrier via temperature room at quency fre- or phase, amplitude, transmission controllable actively enabling devices metamaterial terahertz AlamosNatl.Lab,USA. Los MetamaterialsTerahertz, Active FTuB1 •8:00a.m. FTuB1 Chris W.Gladden Chris purely nanowire dielectric lasers. operate below the photonic mode cut-off diameter of are not subjected to diffraction limitations, hence can confinement. These nanowire-based plasmonic lasers monic laser device exhibiting strong sub-wavelength LawrenceBerkeley Natl. Lab, WeUSA. plasa - report 2 Germany, Presider Harald Giessen; Univ. of Stuttgart, Resonators •PlasmonicEmittersand FTuB 8:00 a.m.–10:00a.m. Volker J. Sorger Plasmonic Nano-Laser below the Diffraction , Limit •8:30a.m. FTuB2 Dai Physics, Peking Univ., China, Engineering Ctr., Univ. of California at Berkeley, USA, State Key Lab for Mesoscopic Physics and School of School and PhysicsMesoscopic for Lab Key State 2 , Xiang Zhang Xiang , 1 , Rupert F. Oulton 1 , Guy Bartal Guy , 1,3 Crystal ; 1 NSF Nanoscale Science and Science Nanoscale NSF Invited Weplanardemonstrate 3 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Materials Sciences Div., 1 , Ren-Min Ma Ren-Min , 1 , Thomas Zentgraf
Hou-Tong Chen; Chen; Hou-Tong 2 , Lun , 1 , JTuA1 •8:00a.m. for analysis, beam was 88%. USA, Presider David H.Reitze; Univ. of Florida, II Interferometers JTuA •GravitationalWave 8:00 a.m.–10:15a.m. TEM output frequency powerpresented.is measuredThe ofgravitational wave detectors of210W with single- Germany. Hannovere.V.,ZentrumKracht, Weßels; Peter Laser Raphael Kluzik, Maik Frede, Veltkamp,Joerg Neumann, Christian Dietmar Puncken, Oliver Winkelmann, Power in TEM in Power 210 W Single-Frequency Laser with 88% of Output JTuA2 •8:30a.m. detectors and future prospects. wave gravitational interferometric of generation new the describe will I space-time. in fluctuations waves; gravitational for search to used being now are LIGO) as interferometers(such scale Kilometer Astronomy Wave Next Generation Interferometers for Gravitational 00 mode content, using a non-confocal ring cavity JOINT FiO/LS A solid-state laser for the next generationnext the for laser solid-state A 00 Mode for Advanced LIGO, Advanced for Mode ,
Rana Adhikari; Caltech, USA. Caltech,Adhikari; Rana Gold Invited • October 11–15,2009 Lutz Lutz
For Fall Congress presentations onTuesday, seepages116-124. Network technologies. wireless and optical of integration increasing and evolution graceful fromsingle-wavelength WDMto including networks generation third- and second- on focus will talk This well-defined. been nowhave Japan. Agile WDM Layer for FlexSelect for Layer WDM Agile Kazovsky AccessNetworksNext-Generation Optical , USA, Presider Gee-Kung Chang; Georgia Tech, •OpticalCommunication FTuC 8:00 a.m.–10:15a.m. FTuC2 •8:30a.m. FTuC2 agile interface.agile the multi-degree ROADM solutions and high-density on based layer WDM agile enhanced with network on next generation service-converging metro optical Yamashita Ciena’s FlexSelect USA. Corp., Ciena Blair; FTuC1 •8:00a.m. FTuC1
First-generation optical access networks access optical First-generation , 1
Shan Zhong, Jean-Luc Archambault, Loudon , Shing-WaWong, 2 ; 1 StanfordUniv., USA, TM architecture and share our vision Valley Invited Invited This talk will introduce will talk This 1 , She-Hwa YenShe-Hwa , 2 TM FujitsuLtd.,Labs Metro Optical Optical Metro 1 , Shinji Shinji , Leonid Leonid FiO optical frequency comb (with 300 GHz spacing) spacing) GHz 300 spans over 900nm. (with comb frequency optical measured The reported. is fiber optical flattened tion of cascaded four-wave mixing using a dispersion Bland-Hawthorn Sweden, very compact lasers. fiber very of performance the enhance to designs cavity laser novel and glasses, active highly-doped fiber, tured will discuss recent progress in combining microstruc- , Designs Novel Fiber Lasers with Advanced Glasses and Fiber at San Diego, USA, Diego, San at FTuD1 •8:00a.m. FTuD1 Slaven Moro Slaven Presider Jonathan Knight; Univ. of Bath, UK, •NovelFiberDevicesI FTuD 8:00 a.m.–10:00a.m. Highly Nonlinear Fiber, Nonlinear Highly Optimized Dispersion in Generation Mixing Four-Wave- Cascaded Octave-Spanning Nearly •8:30a.m. FTuD2 3 Univ. of Sydney, Australia. Efficient genera- Axel Schülzgen;AxelUniv. Arizona,ofUSA. 1 , Nikola Alic Nikola , 3 , StojanRadic, California 2 Chalmers Univ. of Technology,of Univ. Chalmers 1 Invited , Magnuss Karlsson Magnuss , Jose M. Chavez Boggio Chavez M. Jose 1 ; 1 Univ.Californiaof 2 , Joss Joss , We We 1 , Tuesday, October 13 57 Majed Majed Chergui; Lab of Invited Invited We will We present different Photo excitation of molecules of excitation Photo Hillsborough LSTuC1 • 8:00 a.m. LSTuC1 Structural Tracking of Chemical Reactions in Solution by Time-Resolved X-Ray , Scattering of Univ. Ctr., Nielsen; Martin Meedom Nano-Science Denmark. Copenhagen, - bimolecu initiate can and structures transient creates using tracked been have processes Such reactions. lar to scattering X-ray picosecond and optical pumping probe key elements of transient structures in liquid environments Sub-Picosecond Intersystem Crossings and Struc- Sub-Picosecond Intersystem tural Dynamics: Combined Ultrafast Optical and X-Ray Absorption , Studies Ultrafast École Spectroscopy, Fédérale Polytechnique de Lausanne, Switzerland. hard and optical of combination the where examples complete a obtain to us allowed spectroscopies X-ray picture of the dynamics of molecular processes in solutions. 8:00 a.m.–10:00 a.m. 8:00 a.m.–10:00 Science III Ultrafast X-Ray • LSTuC of Republic KAIST, Ihee; Harry Presider Korea, LSTuC2 • 8:30 a.m. LSTuC2 , T. , T. 2 , M. 1 ion is + Max-Planck- 2 Keith Schwab; Schwab; Keith K. Vahala
, G. Saathoff 2 A trapped Mg trapped A Invited Invited Caltech, USA, Caltech, 1 LS ; , V. , Batteiger V. 2 2 Piedmont , Th Udem Th , , S. Knünz 2 2 LSTuB1 • 8:00 a.m. • 8:00 LSTuB1 - Resona Mechanical a of Detection and Preparation Motion, of State Ground the Near tor Cornell Univ., Cornell USA. Univ., We have cooled the motion of a radio-frequency nanomechanical resonator by frequency microwave driven a to coupling parametric observedoccu- have and resonator superconducting expect We 1.3. +/- 3.8
2 CREOL, CREOL, College of Optics and Photonics, of Univ. Central Central Florida, USA. Here we designed, fabricated and tested a novel optical sensor for bio/chemical applications based on multimode interference (MMI) effects in a no-core multimode fiber that PDMS is and sections fiber single-mode with integrated channels. microfluidic FTuE1 • 8:00 a.m. Integrated Fiber Based Multimode Interference Bio/Chemical Sensor, A. Basurto-Pensado 8:00 a.m.–10:00 a.m. 8:00 a.m.–10:00 FTuE Fiber Optics Sensors • at California of Univ. Boyraz; Ozdal USA, Presider Irvine, Mexico, Morelos, 4 FTuE2 • 8:15 a.m. Low Energy Type II Fiber Bragg Mihailov; , J. Gratings Stephen Smelser, W. Christopher Grobnic, Res. Canada, Ctr. Canada. II Type Communications made with energy are low gratings infrared ultrafast help that grating I type a of inscription the after pulses exposure II type the during radiation the of coupling the threshold. lower and FTuE3 • 8:30 a.m. Mexico, Mexico, Patrick LiKamWa Patrick Aerospace Engineering, Univ. of Central Florida, USA, Florida, Central of Univ. Engineering, Aerospace Advances in Chemical and Biological Sensing Using Using Sensing Biological and Chemical in Advances Emerging Soft Glass Optical , Fibers - Ste Shahraam, V. Afshar Ebendorff-Heidepriem, Heike Adelaide, of Univ. Monro; Tanya Warren-Smith, phen Australia. tured fibers provide new ways of interacting light with light interacting of ways new provide fibers tured materials for sensing applications. Developments in the design, fabrication and application of these fibers for the sensitive-detection of chemicals and will bebiomolecules reviewed. Tutorial - Queen of Doherty; Univ. Andrew Glen Ellen Glen This This talk will introduce numerical JOINT FiO/LS JOINT Andrew Andrew Doherty is a Senior Lecturer in Physics at the University of Queensland. He completed his Ph.D. under the supervision of Professor Dan Walls at the University of Auckland in 1999. From 2000–2003 he was a postdoctoral research at the California and of Institute he Technology moved to the of University Queensland in 2003. His research interests are in quantum measurement control and information. quantum JTuB1 • 8:00 a.m. JTuB1 8:00 a.m.–10:00 a.m. 8:00 a.m.–10:00 Generation • Entanglement JTuB II and Measurement USA, Illinois, of Univ. Kwiat; Paul Presider Efficient Algorithms for Quantum State and - Pro , Tomography cess sland, Australia. and and analytical techniques of convex optimization. wideapplication found have these techniques While in quantum information, we will focus on - applica tions to data analysis in quantum state and process tomography. Tuesday, October 13 58 for minimizing them. I will discuss the causes of these effects and strategies visual performance and increased visual discomfort. decreased distortions,perceptual including displays stereoscopic of use the in arise issues perceptual of Banks; Univ. of California at Berkeley, USA. Displays? 3-D Constructing in Perception Depth Human about Know We Should What University of Wales, Cardiff. the of Professor Honorary an and Development, and Perception in Contribution for Award Koffka the of recipient first the lectureships, Howard and Scientific Contribution, recipient of the Gottsdanker Early AwardforMcCandless the ofrecipient ences, Center for the Advanced Study of the Behavioral - Sci of the American Psychological Society, Fellow of the AdvancementAssociationFellow forthe Science, of man eye. Professor Banks is a Fellow of the American other stereo displays that bypass the opticsand of the cues hu- focus correct nearly present that displays stereonoveldevelopment of the involvedin was He organs. sensory different from cues of integration the onresearch his for and depth, of perception the his research on human visual perception, particularly University of California at Berkeley. He is known for the at Neuroscience andPsychology, Science, sion ViOptometry,- of Professor a is Banks S. Martin •8:45a.m. FTuA2 Marketplace—Continued •3-DEntertainmentinthe FTuA Empire Tutorial A variety Martin Martin FiO Jelena Vučković 2 experimentally demonstrated.experimentally are 2.3 of factor a to up emission of Enhancements enhance emission from erbium doped silicon nitride. odically patterned metal-insulator-metal structures to - peri in modes plasmonic use to Wepropose USA. Nitride Silicon Amorphous in Erbium with Interaction for Structures Metal-Insulator-Metal Plasmonic •8:45a.m. FTuB3 semiconductor gain. is feasible loss in metal iswhich the compensated by model. We discuss the regime where nano-ring laser is simulated using multi-level, multi-electron FDTD design laser ring pumped electrically nano-scale A Huang tor Gain Model , Gain tor - Semiconduc Realistic on Based Laser Nano-Ring Plasmonic Semiconductor of Simulation FDTD •9:00a.m. FTuB4 polymer interface. polaritonsplasmonpropagatinggold- surface the at from originates emission stimulated the that gests sug- structure mode The wire. gold a on deposited polymer dye-doped by formed cavity microring in emission stimulated demonstrated haveWe USA. nov Resonators—Continued •PlasmonicEmittersand FTuB Gold Core Gold with Cavity Microring in Emission Stimulated •9:15a.m. FTuB5 Data Storage Inst., Singapore,Inst., Storage Data 1 ; 1 Norfolk StateNorfolkUniv., USA, 3 , Seng-Tiong HoSeng-Tiong , , Yiyang Gong , J.KiturK. 1 ; 1 Stanford Univ., USA, Xi Chen Xi Crystal 1 , Selçuk Yerci 1 , V., PodolskiyA. 1 ; 1 Northwestern Univ.,NorthwesternUSA, 1 , Bipin Bhola Bipin , FiO/LS/AO/AIOM/COSI/LM/SRS 2009 3 2 OptoNet. Inc, USA. Inc, OptoNet. Oregon StateUniv.,Oregon 2 , Luca Dal Negro Dal Luca , 2 2 Boston Univ., , M. A. NogiA. M. , - 2 , Yingyan Yingyan , 2 ,
JTuA3 •8:45a.m. wave detector. GEO 600 long-baseline interferometric gravitational discuss the design, status and plans for upgrades to the UK. Glasgow,Univ. of Rowan; Sheila WaveDetector , Gravitational Interferometric for GEO600 and Directions in Optics Related Research power systems. laser aberrations high correction ofastigmaticin thermal ments. One application of the proposed system is for ele- optical in effects photo-thermal induced heat demonstrationmental shapingadaptiveof beam via Physics, Univ. of Florida, USA. We present an - experi of Dept. Reitze; Tanner,H. B. Mueller,David David fects Ef Photothermal Using Shaping Beam Adaptive JTuA4 •9:15a.m. Interferometers II—Continued Interferometers JTuA •GravitationalWave , Muzammil A. Arain,GuidoMuzammilKorth,William A. Z. JOINT FiO/LS Gold Invited • This talk will will talk This October 11–15,2009 - For Fall Congress presentations onTuesday, seepages116-124. Adolfo F. HerbsterF.Adolfo Mirim, Brazil, C. Bordonalli C. nels (C-Band). control and enable add/drop of any number of chan- reduction SHB provide scheme controlattenuation VOA and pump simultaneous A demonstrated. is minimize gain error due to SHB based on HGC-EDFA Continued •OpticalCommunication— FTuC Systems earity in on-off Keyed 40 Gb/s WDM Transmission Electronic Compensation of Optical Fiber Nonlin- •9:00a.m. FTuC3 , Range Gain Dynamic Generalized with HGC-EDFAUsing Burning Hole Spectral to Due Error Gain ofMinimization •9:15a.m. FTuC4 increase overall the system margin by >1.0dB. analysis Our shows that proposed the technique can keyed 40Gb/s long-haul WDM transmission systems. technique to compensate fiber nonlinearitynovel in a on-off- analyze and proposeWe USA. Duluth, at , Nisar Ahmed, M. I. Hayee; Univ. of Minnesota 2 2 ; A method to Univ. to of Campinas, method Brazil. A 1 CPqD Foundation,Mogi-CampinasCPqD 1,2 , Juliano R. F. OliveiraF. R. Juliano , Valley Júlio C R. F. de Oliveira de F. R. C Júlio 1 , Aldário , FiO 1 , Russian Federation,Russian horov General Physics Inst., Russian Acad. of Sciences, Marciante Igor V. Mel’nikov Bang gitudinally gitudinally Varying Taper, - Lon a in Shift Self-Frequency Soliton Enhanced •9:00a.m. FTuD4 switched switched Nd hybridQ- a of made system present compactlaser a at 1-10-kHz repetition rate. pulses fornanosecond achieved dB 20-25 as high as an Yb-doped specialty-fiber amplifier with gain factor single-polarization fiber. SP1060 Corning are polarizers fiber the and fiber, silica terbium-doped 56-wt% uses rotator Faraday demonstrated.opticalisolationis dB of 18 fiber The Valueisolatorwith all-fiber PhotonicsAn Inc.,USA. 2 2 the solitonthe wavelength. at nonlinearity and dispersion the optimizes which PCF with a carefully designed waist diameter profile tapered a in shift self-frequency soliton the of ment enhance - the for method a proposeWe Denmark. of Sydney, Australia,Sydney, of C. Mägi C. Sun RotationFaraday, on Based Isolator All-Fiber •9:15a.m. FTuD5 Devices I—Continued •NovelFiber FTuD Rate Repetition Multi-kHz a at Fiber Specialty a from Output 1-ns ~1-mJ, A System:MOFA Compact •8:45a.m. FTuD3 Lab for Laser Energetics, Univ. of Rochester, USA, Ctr. de Investigaciones en Óptica, Mexico, 1,2 , 2 Alexander V. Kir’yanov , Benjamin, J. Eggleton , Shibin Jiang Shibin , 1 Rv Pant Ravi , 1,2 ; 3+ 1 :YAG/Cr Inst.ofOptics, Univ. ofRochester, USA, 1,4 ; California 1 Optolink Ltd., Russian Federation, 3 4 , Jonathan D. Zuegel D.Jonathan , 1 We We Canada.Inc., Labs, Q High , C. Martijn de Sterke de Martijn C. , 2 4+ Technical Univ. of Denmark, Denmark, of Univ.Technical :YAG microchip laser seeding 1 1,2 , Boris T. Boris , Kuhlmey Alexander C. Judge , Sergey M. Klimentov 3 A M Prok M A 2 , John R. R. John , 1 ; 1 1 Univ. 1 , Eric , , Ole 3 Ad Lei Lei 1,3 - - , Tuesday, October 13 59 This This talk Invited Hillsborough LSTuC • Ultrafast X-Ray Ultrafast X-Ray • LSTuC Science III—Continued Ultrafast Ultrafast Photochemical Dynamics in , Solution USA. of Khalil; Munira Washington, Univ. spectroscopy absorption X-ray of use the outline will changes geometric and electronic probing (XAS)for processes transfer charge ultrafast following dynamics in solution. metal complexes in transition LSTuC3 • 9:00 a.m. LSTuC3
- Sumei Mani Hos Caltech, USA. Caltech, 2 Ctr. for High Technology Technology High for Ctr. 1 ; 2 LS Piedmont , Kerry Vahala Kerry , 1 We show We how a type I optical parametric amplifier inside the cavity can aid the normal mode cavity splitting optical the with coupled mirror movable the of regime. sideband in the resolved Huang, Girish S. Agarwal; Oklahoma State Univ., USA. Univ., State Oklahoma Agarwal; S. Girish Huang, LSTuB4 • 9:15 a.m. LSTuB4 Mode Splitting of a Nanomechanical Oscillator under Parametric Interactions in a Cavity, LSTuB3 • 9:00 a.m. LSTuB3 Optomechanical RF Signal , Processing sein-Zadeh Materials, Univ. of New Mexico, USA, Mexico, New of Univ. Materials, LSTuB • Cavity Optomechanics I— Cavity Optomechanics • LSTuB Continued We have explored the applications of optomechanical optomechanical of applications the explored have We element. signal-processing RF an as (OMO) oscillator RF frequency-conversion and injection locking in the in demonstrated are domain optomechanical the OMO. a microtoroidal of context For Fall Congress presentations on Tuesday, see pages 116-124. Congress presentations on Tuesday, For Fall
Ctr. Ctr. 1 Oleg ; , 1 October 11–15, 2009 - Caval G. Eric , • 1 Qiong Y. He Y. Qiong , Peter D. Drummond D. , Peter 1 Physics Inst., Univ. of Bonn, 1 ; 2 Sacramento Physics Dept., Queens College, CUNY, USA. CUNY, College, Queens Dept., Physics 2 , Lev Deych Kaushik Kaushik Roy Choudhury, A. F. J. Levi; Univ. 1 , Margaret D. Reid D. , Margaret 2 Ctr. for Quantum Dynamics, Griffith Univ., Australia. Univ., Griffith Dynamics, Quantum for Ctr. LSTuA5 • 9:00 a.m. LSTuA5 Diagrammatic Semiclassical Laser Theory Zaitsev LSTuA6 • 9:15 a.m. LSTuA6 Behavior of Lasers in the Small Particle Number Limit, of Southern California, USA. Master equations and dominant the study to used are methods walk random role of quantum fluctuations in determining the steady-state and temporal-behavior of small lasers. Suppression of lasing threshold and de-pinning of observed.carriers is LSTuA4 • 8:45 a.m. • 8:45 LSTuA4 Multipartite Quantum Nonlocality Using - Func , Inequalities Bell tional We We show that arbitrary functions of hidden localcontinuous of tests generate to used be can variables and detectors non-ideal of effect The theories. variable functional optimized that revealing included, is noise robust. are inequalities 2 canti Germany, Germany, We derive We semi-classical laser equations valid in all representation diagrammatic A nonlinearity. of orders - popula of effect weak a account into take to us allows the treating while way, controlled a in pulsations tion exactly. nonlinearity for Quantum-Atom Optics, Swinburne Univ., Australia, Australia, Univ., Swinburne Optics, Quantum-Atom for LSTuA • General Laser • LSTuA Science— Continued , 1 Chao Roshni , , Jin Zhang 1 Univ. of Univ. California at 1 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 ; 2 FiO NASA NASA Ames Res. Ctr., USA. A 2 Atherton , Rebecca Newhouse , Bin Chen 1 2 , Claire Gu 1 FTuE Fiber Optics Sensors— • Continued FTuE5 • 9:15 a.m. Antiresonant-Guiding Photonic Crystal for Refractive Fibers Index Gradients Sensing - H. Kulhand Mehta, Gaurav Kandel, Mikhail Biswas, jian, Aleksandr Verevkin, Adly T. Fam, design Natalia propose, M. We USA. Buffalo, SUNY Litchinitser; and experimentally demonstrate a novel, simple, distributed refractometric sensor based on unique photonic anti-resonant-guiding of properties spectral crystals fibers for gradients. measuring temperature Design optimization and potential willapplications be discussed. molecular sensing system is theoretically analyzed and analyzed theoretically is system sensing molecular - pho core hollow a with demonstrated experimentally scattering Raman enhanced surface fiber crystal tonic portable a and sensitivity high achieve to probe (SERS) flexibility. achieve to spectrometer Raman Santa Santa Cruz, USA, Kazuki Kazuki Tanaka FTuE4 • 9:00 a.m. Portable Photonic Crystal Fiber Sensor Based on , (SERS) Scattering RamanEnhanced Surface Shi , , 1 1,2 Univ. Univ. 2 , Stephen 1 , Jonathan Leach Jonathan , 1 Univ. of Glasgow, UK, Glasgow, of Univ. 1 Barry Jack Warren Grice; Oak Ridge Natl. Natl. Ridge Oak Grice; Warren ; 1 Manuel Manuel de la Cruz Gutierrez Clarendon Lab, Oxford Univ., 1 , , Sonja Franke-Arnold We use spatial light modulators to to modulators light spatial use We 1 ; ; 1 Glen Ellen Glen , Miles Padgett Miles , JOINT FiO/LS JOINT 2 Univ. of Univ. Houston, USA. We implemented a 2 JTuB3 • 9:00 a.m. JTuB3 - Us Measurement Bell-State Optic Linear Improved , Photons Ancillary ing It is not possible to construct a linear optic optic linear a construct to possible not is It USA. Lab, Bell four all discriminates unambiguously that device efficiency measurement Bell-state the However, states. introducing by unity to close arbitrarily made be can photons. entangled additional UK, Barnett JTuB2 • 8:45 a.m. JTuB2 - Pro Design Experiment Optimal an of Evaluation Photonic for Optimization Convex Based on tocol State Tomography of Strathclyde, UK. Strathclyde, of observe single-photon, non-trivial superpositions of of superpositions non-trivial observesingle-photon, the Using states. (OAM) momentum angular orbital analogy between polarisation and two-dimensional subspaces, we OAM alsobe - measure entanglement modal superpositions. tween these complex Jacquiline Jacquiline Romero Ian Ian A. Walmsley model-based optimized method of data acquisition for two-qubit tomography both theoretically and experimentally. Limitations of the method’s results and their potential for larger qubit systems were also established. JTuB4 • 9:15 a.m. JTuB4 Entanglement Measure to Modulators Light Spatial , States Spatial between JTuB • Entanglement Generation Generation • Entanglement JTuB II—Continued and Measurement Tuesday, October 13 60 Empire 9:00 a.m.–12:00p.m. FiO and metamaterials. forandopticalformbasiscould sensorsnanoscale a merit of figures sensing high show structures These ing sub-radiant and Fano-type modes are described. implementationsofplasmonic nanocavities sustain - Feng Hao Feng ity advantage of plasmon surface polaritons. relatively high-Q hybrid mode with the large sensitiv- micro-disk resonator is proposed. The structure has a Peter Nordlander Sonnefraud Modes, Fano and Sub-Radiant with tors Design and Implementation of Plasmonic Resona- •9:30a.m. FTuB6 Resonators—Continued •PlasmonicEmittersand FTuB London, UK, London, Physics and Chemistry, Katholieke Univ. Leuven, Leuven, Univ. Belgium, Katholieke Chemistry, and Physics nators through the whispering-gallery mode of a SiN Tech, USA. Yegnanarayanan,Momeni,BabakAdibi;Ali Georgia Siva Soltani,Chamanzar,MaysamrezaMohammad tonic Microresonators Using Momentum Matching , Strong Mode Coupling in Hybrid Plasmonic-Pho- •9:45a.m. FTuB7 4 4 Rice Univ.,USA. Rice
, Victor Moshchalkov Victor , Efficient Efficient coupling to plasmonic ring reso- 1 Student Programming:Painless Publishing,SciencePolicy andOSATravelingLecturer, Regency Ballroom II,Fairmont Hotel , Niels VerellenNiels , 2 IMEC, Belgium, IMEC, 4 , Stefan A. Maier Crystal Design principles and principles Design FiO/LS/AO/AIOM/COSI/LM/SRS 2009 10:00 a.m.–4:00p.m. 2,3 10:00 a.m.–10:30a.m. , Heidar Sobhani Heidar , 3 3 Inst. for Nanoscale Nanoscale for Inst. , Pol Van Dorpe VanPol , 1 ; 1 Imperial College Yannick 4 2 x , ,
tory of Japan, Japan. DECIGO Working Group; Natl. Astronomical - Observa be described in the talk. inthe described be Japanese future space gravitational wave antenna, will DECIGO, the and mine, Kamioka the in built be to gravitationaldetectorwave cryogenic Japanese 3km JTuA5 •9:30a.m. for gravitational wave detection. bandwidth than what is achievable in advanced LIGO signal recycling, yielding much higher sensitivity and for mirror compound a as acting cavity light white a of design non-invasive a Univ.,We describe USA. Salit,Honam Yum, Shahriar;NorthwesternSelimM. WaveGravitational a in Detector , Recycling Signal Broadband Sensitivity, High for Mirror A White Light Cavity as a Non-Invasive, Compound JTuA6 •10:00a.m. DECIGO, Japanese Gravitational Wave Detectors: LCGT and Interferometers II—Continued Interferometers JTuA •GravitationalWave JOINT FiO/LS Exhibit HallOpen,Imperial Ballroom, Fairmont Hotel
Seiji Kawamura, LCGT Collaboration, Collaboration, LCGT Kawamura, Seiji Coffee Break,Imperial Ballroom, Fairmont Hotel The current status of LCGT, the Gold Invited • October 11–15,2009 Mary Mary For Fall Congress presentations onTuesday, seepages116-124. between crosstalk eventsbetween are studied. distributions governing crosstalk and the correlation states creating undesirable crosstalk. The underlying orbital angular momentum is transferred to adjacent plexed free-space optical link affected by turbulence, Anguita; Univ. of the Andes, Chile. In a vortex-multi - , Link Optical Multi-VortexFree-Space a in Distribution Momentum Angular Orbital •9:30a.m. FTuC5 Continued •OpticalCommunication— FTuC measurement results. the in improvement an to leads then which factor, correction the enhanced that system transmission optical compensated dispersion a along (CD) sion been proposed for the mapping of chromatic disper has formulation new Technology,A Japan.of Inst. TransmissionSystem, Optical Compensated Dispersion along Mapping Dispersion Chromatic on Losses Splice of Effect •10:00a.m. FTuC7 Hoda sphere TurbulentAtmo- the in and Space Free in Kinds Different of Beams of Spreading of Comparison •9:45a.m. FTuC6 and turbulent inthe atmosphere. beam preserves its beam like form both in free space a which to up propagation of distance the estimate to used is criterion a type, beam the on Depending of Engineering and Technology,Pakistan,and Engineering of 1 , Shinya Sato Shinya , , Anabil Chaudhuri; Univ. of Rochester,Univ.USA. Chaudhuri;Anabilof 2 , Masaaki ImaiMasaaki , Valley Mirza ImranBaigMirza 2 ; 1 Sir Syed Univ.Syed Sir 1 , Faisal ul Faisal , 2 Jaime A. A. Jaime Muroran Muroran FiO - liquid level around multimode the fiber. nm, which can be made continuous by increasing the 40 almost of range tuning a for allows scheme This interferencebandpass(MMI) demonstrated.isfilter trónica, Mexico. An optofluidically tunable multimode May-Arrioja;Inst. Natl. Astrofísica,de ElecÓptica- y A. Sanchez-Mondragon,Daniel J. Jose May-Arrioja, A. Hernandez-Romano,Antonio-Lopez,IvanDaniel Optofluidic Tuning of MMI Bandpass Filter , •9:30a.m. FTuD6 reduces threshold the ofIIdamage. type hydrogenof presence the that suggests morphology grating The fiber. core all-silica doped fluorine in demonstrated are gratings Bragg fiber stable Canada. Canada,Ctr. Res. tions Smelser, Dan Grobnic, Stephen Mihailov; Communica- Hydrogen All-Silica Loaded Core Fiber, Temperaturein GratingsHigh Bragg Fiber Stable •9:45a.m. FTuD7 Devices I—Continued •NovelFiber FTuD California High temperature High Christopher Christopher Jose E. Tuesday, October 13 61 , 2 , Tae-Kyu Kim Tae-Kyu , , Robert - Schoen 1,2 3 We report the first first the report We Advanced Light Source, Source, Light Advanced 4 Invited , Ha Na Cho Na Ha , 1 Pusan Natl. Univ., Republic of Korea, Korea, of Republic Univ., Natl. Pusan , James McCusker 2 3 Hillsborough Nils Huse Nils , Chemical Chemical Sciences Div., Lawrence Berkeley 1 ; 4,1 Michigan State Univ., USA, Univ., State Michigan LSTuC4 • 9:30 a.m. • 9:30 LSTuC4 LSTuC • Ultrafast X-Ray Ultrafast X-Ray • LSTuC Science III—Continued Ultrafast Ultrafast Soft X-Ray Spectroscopy of Spin- Transition-Metal Solvated Dynamicsin Crossover Complexes Natl. Lab, USA, Lab, Natl. 3 Lindsey Lindsey Jamula Lawrence Berkeley Natl. Lab, USA. Lab, Natl. Berkeley Lawrence measurements X-ray soft time-resolved femtosecond spec- L-edge complexes. transition-metal solvated of troscopy directly reveals dynamic changes in ligand spin the with associated 3-D-orbitals of splitting field changes. ligand-bond by mediated and transition, lein Invited LS We describe high-Q parametric We Michael Tobar; Univ. Michael of Tobar; Univ. Western
Piedmont LSTuB5 • 9:30 a.m. • 9:30 LSTuB5 Cooling Acoustic Oscillators with Electromag- netic Parametric Transducers and Prospects of Measuring below the Standard Quantum Limit of , Displacement transducers developed at the of University Western Australia for precise displacement measurements. with transducers, niobium and sapphire includes This the potential to reach the Standard Quantum Limit Demolition. Non Quantum and Australia. Australia, LSTuB • Cavity Optomechanics I— Cavity Optomechanics • LSTuB Continued For Fall Congress presentations on Tuesday, see pages 116-124. Congress presentations on Tuesday, For Fall Ctr. for Ctr. 1 , Nathan ; October 11–15, 2009 1 1 Ronald W. Ronald W. • , Luke F. Lester , Luke F. 2 , , Nader A. Naderi 1 The behavior of a zero-detuned Sacramento Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Coffee Break, Imperial , Vassilios Kovanis , Vassilios Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Exhibit Hall Open, Imperial 2 Michael Michael C. Pochet , US US AFRL, USA. injection-locked injection-locked Quantum-Dash Fabry-Perot laser under varied injected field ratios is investigated theoretically and experimentally. A low slave laser line-width enhancement factor is found to inhibit operation. chaotic/Period-2 B. B. Terry LSTuA8 • 9:45 a.m. LSTuA8 A Self-Injection Locked Unidirectional Diode Pumped Solid State Ring Laser Cavity, USA. We Univ., State Pennsylvania O’Hara; Ken Stites, laser. ring unidirectional single-mode novel a present beam one from power of amount small a injecting By path from the output coupler back into the other, many eliminating forced, is operation unidirectional elements. intracavity LSTuA7 • 9:30 a.m. • 9:30 LSTuA7 Operational Behavior of an Injection-Locked - Zero-Detun Laserat Fabry-Perot Quantum-Dash ing 2 High Technology Materials, Univ. of New Mexico, USA, USA, Mexico, New of Univ. Materials, Technology High LSTuA • General Laser • LSTuA Science— Continued , 2 , , M. R. Shenoy 2 10:00 a.m.–10:30 a.m. 10:00 a.m.–4:00 p.m. FiO/LS/AO/AIOM/COSI/LM/SRS 2009 - Instru Scientific Central 1 ; Indian Inst. of Technology, Technology, of Inst. Indian 1 2 FiO Carbon-dioxide-laser-induced Carbon-dioxide-laser-induced Atherton , , K. Thyagarajan 1 , Pawan Kakur Regency Ballroom II, Fairmont Hotel II, Fairmont Ballroom Regency Lecturer, and OSA Traveling Publishing, Science Policy Student Programming: Painless 1 Michael R. Hutsel, Thomas K. Gaylord;
Fabrication and experimental characterization characterization experimental and Fabrication FTuE6 a.m. • 9:30 - Tempera and Strain of Measurement Simultaneous , Fiber Doped Erbium in Written FBG an Using ture Umesh K. Tiwari FTuE Fiber Optics Sensors— • Continued Georgia Tech, Georgia USA. Tech, long-period fiber gratings are fabricated near fiber effects The sensors. as use for assessed and end-faces of changing the surrounding refractive index are characterized. A solvent vapor sensor is fabricated experimentally evaluated. and FTuE7 • 9:45 a.m. End-of-Fiber Long-Period Fiber Grating-Based Sensors, India. mea- FBG a of novel can simultaneously sensor that shown is It presented. is temperature and strain sure temperature and pm/με 0.8 is sensitivity strain the that 12 pm/0C. is sensitivity Nahar Singh Nahar ments Organization, India, India, Organization, ments 9:30 a.m.–12:00 p.m. Nathan Nathan Kurz, Gang Shu, Glen Ellen Glen Gang Shu, Nathan Kurz, Matthew R. Matthew Kurz, Gang Shu, Nathan JOINT FiO/LS JOINT - R.of Wash Matthew Dietrich, Boris B. Univ. Blinov; numerical high a incorporated have We USA. ington, aperture spherical mirror and aspherical corrector collection photon improve to trap ion barium a with efficiency by more than an order of magnitude for entanglement. ion-photon of generation JTuB5 • 9:30 a.m. JTuB5 High-Efficiency Single Photon Collection from Trapped Barium , Ions Dietrich, Dietrich, Boris B. Blinov; Dept. of - spheri Physics, N.A. high a of Univ. integrated We USA. Washington, by image its improved and trap Paul a into mirror cal based trap a designed We correctors. aspheric special on metallic spherical which mirror increases greatly efficiency. entanglement the ion-photon/ion-ion JTuB6 • 9:45 a.m. JTuB6 - Integrat by Collection Fluorescence Ion Improving ing High Numerical Aperture Spherical Mirror , into Ion Trap JTuB • Entanglement Generation Generation • Entanglement JTuB II—Continued and Measurement Tuesday, October 13 62 previous system. the of that than higher times four was images 3-D of 7680 x 4320 pixels. The resolution of the displayed extremely high-resolution video that had a resolution Res. Labs, Japan. Technicaland Science Arai,JunNHK FumioOkano; High-Resolution Video System, 3-D TV Based on Integral Method Using Extremely of image quality. analysis and materials the of optics the present will 3-D appearance and exhibit full motion parallax. We true have that products image inventedintegral has 3M Corp., USA. Douglas S. Dunn, Robert L. Smithson, Steven Images, J. Integral Rhyner; of Development Display by Integral Imaging, and Visualization, Sensing, Three-Dimensional 3 1 •10:30a.m. FTuF1 Berkeley, USA,Presider Martin Banks; Univ. of California at and Displays FTuF • 3-D Capturing, Visualization 10:30 a.m.–12:00p.m. FTuF2 •11:00a.m. FTuF2 challenges will be discussed. challenges be will technical and Variousapplicationspresented. be will results experimental and Theoretical imaging. in 3-D sensing, visualization, and display by integral Thisinvited paperpresents of advances an overview Martinez-Corral FTuF3 •11:30a.m. FTuF3 Ben Gurion Univ. of the Negev,Israel,Univ.the Gurion of Ben Univ. of Connecticut, USA, Development of Integral Images 3M We developed integral 3-D TV using 2 , Adrian Stern Adrian , Empire 2 Invited Invited Invited Univ. of Valencia, Spain, Bahram Javidi Bahram 3 Masahiro Kawakita, , Edward WatsonEdward , iga Wu, Pingfan 4 AFRL, USA. AFRL, 1 , , Manuel 4 ; Univ. of Miami, USA. turbulent atmosphere. of andLaserCom LIDAR systems operating through coherence and polarization to improve performance of such statistical properties of light sources as states of are possible. optical vortices lenses, and highly chromatic elements norAchromaticrefractive. fractive elementsas such dif neither are elements weight light thin, These introduced. is element optical designed computer USA. RIT, Science, Imaging for Ctr. ments, - Ele Optical Computer-GeneratedVectographic erating in Atmospheric Turbulence, ties of Beams for Communications and LIDARs - Op Modulation of Coherence and Polarization Proper Charlotte,USA, rable beams of uniform polarization. compa- than scintillation smaller appreciably have to demonstratedare investigated.They numerically are turbulence atmospheric in propagating beams tion properties of a class of non-uniformly polarized in Atmospheric TurbulenceAtmospheric, in Beams Polarized Nonuniformly of Scintillation •11:30a.m. FTuG3 •11:00a.m. FTuG2 Korotkova at Charlotte, USA,Presider Greg Gbur; Univ. of North Carolina Sensing I Information Transportand •WavefrontFTuG Designfor 10:30 a.m.–11:45a.m. FTuG1 •10:30a.m. FTuG1 Grover A. Swartzlander, Jr.; Chester F. Carlson 2 , Greg Gbur Greg , 2 Univ.Miami,of - scintilla The USA. Crystal We will demonstrate the ability 1 ; 1 Univ. of North Carolina atCarolina North Univ. of Invited Invited FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Yalong Gu Yalong
Olga Korotkova; A new class of class new A 1 , Olga , - - conserving optical bottom the accessconserving via wall. the need for multi-step lithographic procedures while channels. The simple fabrication technique alleviates micro-fluidic in measurements rate flow perform to used is grating diffraction elastomeric assembled self- A Univ.,USA. Harvard Crozier; B. Kenneth Velocimetry, idic - Microflu forGrating Diffraction Self-Assembled •11:15a.m. FTuH3 FTuH1 •10:30a.m. FTuH1 simple yet efficient. is method recording The display. 3-D rewritable for applied be can which time decay two-hour and time response subsecond with hologram polymeric photorefractive report We reviewed. is holograms USA. Louis, St. at souri Holograms, Dynamic quality imaging. high perform to system a such of ability the shows CCD’sindividual by taken images monochromatic the recombinedfromimage The gratings. lographic ho- volume multiplexed on based system imaging Univ.,USA.Northwestern Gratings Holographic on Based System Imaging 3CCD A •11:00a.m. FTuH2 and SPPs. mixed leaky-mode SPPsexcitedclassical ofthe structure field andlocal leaky-modes. We compare the spectral characteristics resonant and (SPPs) polaritons surface-plasmon both of excitation permits substrate metallic a on Univ. of Texas at Arlington, USA. A dielectric grating strates Modes with GratingsDielectric over Metallic Sub- Excitation of Surface Plasmon Polaritons and Leaky •11:30a.m. FTuH4 Presider to Announced Be Optics I •DiffractiveandHolographic FTuH 10:30 a.m.–12:00p.m. , Mehrdad Shokooh-Saremi, Robert Magnusson; , Selim M. Shahriar, Xue Liu, Shih Tseng; Shih Liu, Xue Shahriar, M. Selim Antony Orth, Ethan Schonbrun, Schonbrun, Ethan Orth, Antony FiO Gold Guoqiang Li; Univ. of Mis- Univ.of Li; Guoqiang Recent work on dynamic on work Recent Invited We present a 3CCD a presentWe • October 11–15,2009 For Fall Congress presentations onTuesday, seepages116-124. tailoring and power distribution flexibility. OPA, such as gain and bandwidth increase, spectrum simple tocompare benefits We demonstrateseveral discussed. are conversion wavelength and fication RAOPA. the experimentally Performances of ampli - and WeUniv.,theoretically investigateLehighUSA. perimental Results , cation (RAFOPA): Numerical Simulations and - Ex Raman-Assisted Fiber Optical Parametric Amplifi- •11:15a.m. FTuI3 are discussed. dispersionschromatic and loss bend coefficient, nonlinear including devices nonlinear to fibers the are presented. Important characteristics for applying processings nonlinear various of platform as fiber Recent progresses high-confinementon silica-based Japan. Ltd., Industries, Electric SumitomoHirano; Fibers, High-Confinement in Advances sampling for first time. the stemming from one’s ability to perform polychromatic implicationsphysics, basic andconstruction discuss es with respect to ultrafast waveform processing. We in parametric devices have led to fundamental chang- Univ. of California at San Diego, USA. Polychromatic High Speed Sampling, FTuI1 •10:30a.m. FTuI1 background photocurrent. is capable of resolving a quasi- 2 Tb/s signal with low sampling pulses below the half-bandgap. The system using photodiode, GaAs a in absorption photon two- non-degenerate on based sampling optical demonstrateWe USA. Park, College at Maryland Univ.of Murphy; E. Apiratikul,Thomas Paveen , Photodiode GaAs a in AbsorptionTwo-Photon NondegenerateUsing Sampling Optical Ultrafast •11:00a.m. FTuI2 Presider Inst., Univ. College Cork , Ireland, Roderick P. Webb; Tyndall Natl. Processing I •All-OpticalSignal FTuI 10:30 a.m.–12:00p.m. FTuI4 •11:30a.m. FTuI4 Cyril L. Guintrand, Jean Toulouse; Valley Invited Invited Recent advances Stojan Radic; Msaaki Msaaki
correlation using analysis. time-frequency and modes of evolution time the studyWe media. random of quasimodes fortransmission in patterns speckle field and linewidths frequencies, central the found haveWe USA. CUNY,College, Queens ization of Light of ization - Local the and Statistics Mesoscopic Universal •11:15a.m. FTuJ3 random are media proposed. of spectroscopy diffusing-wave performing of ways Novelestablished. is localization Anderson and tics random medium. A link photocountbetween statis - a in light of scattering multiple in effects quantum petrov; CNRS, Univ. Joseph Fourier, France. Media, Random of Optics Quantum , Echos Loschmidt via Systems Absorbing in Localization Probing CUNY,USA, Univ., USA, aul Gilman Samuel FTuJ4 •11:30a.m. FTuJ4 •10:30a.m. FTuJ1 one-dimensional waveguides. quasi- disordered with measurements experimental based on a random matrix approach, is supported by media even in the presence of randomabsorption. Our theory,localized or diffusive probe we dynamics at San Antonio, USA,Presider Andrey A.Chabanov; Univ. of Texas II •AndersonLocalization FTuJ 10:30 a.m.–12:00p.m. Waves Electromagnetic Modes and Dynamics of Localized •11:00a.m. FTuJ2 for Gaussian waves. conductance,”intensity oftistical distribution a and parameter,“stasingle the a of- function mesoscopic a of mixture a to dimensional one from changes ability distribution of intensity through layered media , Jing Wang, Azriel Genack; Dept. of Physics, of Dept. Genack; Wang,Azriel Jing 2 Max-Planck-Inst., Germany. 2 ChiralprobPhotonicsThe - Inc.,USA. 1 , Azriel Genack Azriel , , California Jongchul ParkJongchul
smio Kottos Tsampikos Invited Invited 1 ; 1 , Sheng Zhang Sheng , 1 Queens College, College, Queens 1,2 Sergey E. Ski- E. Sergey ; Using echo 1 Wesleyan We study 1,2 , Tuesday, October 13 63 I
Univ. Univ. of Illinois 1 ; 2 Univ. of Univ. Notre Dame, 2 Invited Invited , Paul Bohn 1 Hillsborough Yoshinobu Baba; Yoshinobu Nagoya Japan. Univ.,
Actively-switchable transport can Actively-switchable be achieved LSTuF2 • 11:00 a.m. LSTuF2 Sensor, Level Liquid Optic Fiber Quasi-Continuous USA. A Technology, of Inst. Florida H. Murshid; Syed quasi-continuous liquid level sensor that exploits changes in reflection upon contact with a target fluid has been successfully developed and tested for a host of liquids including liquid nitrogen, oils and water. boiling • 11:15 a.m. LSTuF3 An FPGA-Based Anti-Brownian Electrokinetic Trap for Studying Single Molecules in , Solution Quan Alexandre Wang, Fürstenberg, Samuel - Bock enhauer, E. W. Moerner; Stanford USA. Univ., We have designed and implemented an Anti-Brownian ELectrokinetic (ABEL) trap on an FPGA platform, online and feedback algorithms with programmable sub-10nm of Trapping parameters. trapping tunable achieved. is in buffer seconds for bio-molecules • 11:30 a.m. LSTuF4 Micro- Micro- and Nanofluidics for Single Biomolecule , Analysis Single Molecule Tracking as a Probe of Free Volume Volume Free of Probe a as Tracking Molecule Single Transitions in Stimulus-Responsive Polymers- --Do Single Molecules Behave Like Caribou? Lindsay C. C. Elliott 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 III Micro- and Nanofluidics • LSTuF Dame, Notre of Univ. Bohn; Paul USA, Presider USA. in stimulus-responsive polymer brushes. Single molecule trajectories are used to understand local diffusion and, in turn, to study the polymer free distribution. volume at Urbana-Champaign, at USA, Urbana-Champaign, LSTuF1 • 10:30 a.m. LSTuF1 will describe real-time of monitoring an interaction between a single and DNA an enzyme molecule, an atto litre chamber for single enzymatic molecular single and molecular - traf reaction characterization, cell. in a single ficking analysis - - Pierre Pierre Konrad We We illustrate the
Invited Invited Invited We measure the motion of a of motion the measure We LS Piedmont Matt Eichenfield, Jasper Chan, Ryan Ryan Chan, Jasper Eichenfield, Matt , We present the We theory and experimental - real LSTuE1 • 10:30 a.m. LSTuE1 • 11:00 a.m. LSTuE2 Sensing Nanomechanical Motion with a Shot-Noise Shot-Noise a with Motion Nanomechanical Sensing , Interferometer Cavity Microwave Limited Meystre; Univ. Meystre; of Univ. Arizona, USA. W. Jennifer Donner, Tobias Teufel, D. John Lehnert, W. Manuel Harlow, A. Castellanos-Betran; JILA, NIST, USA. Colorado, of Univ. the beyond precision with oscillator nano-mechanical inter microwave a using by limit, quantum standard Control Control and Sensing of Ultracold Atoms and Molecules by Nanomechanical Cantilevers, Optomechanics of Phononic-Photonic Crystal Caltech, DefectCavities Painter; J. Oskar Vahala, J. Kerry Camacho, M. USA. and optical coupled strongly localized and of ization acoustic modes in periodic nanostructures. Proper frequencies Gigahertz with localizedphonons of ties and sub-picogram masses are studied via all-optical measurements. limit. the shot-noise near operates that ferometer LSTuE3 • 11:30 a.m. LSTuE3 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 II Cavity Optomechanics • LSTuE USA, Caltech, Kerry Vahala; Presider potential of cavity optomechanics (COM) for control control for (COM) optomechanics cavity of potential and sensing in two examples: a bi-stable - configura tion that the controls many-body state of ultra-cold inertial COM-based of limit quantum the and atoms; sensors. mass For Fall Congress presentations on Tuesday, see pages 116-124. Congress presentations on Tuesday, For Fall ; - 1 Kai-Mei Kai-Mei October 11–15, 2009 , The The inter , Lachlan J. 1 • Australian Natl. Univ., Univ., Natl. Australian Invited Invited 2 , Raymond G. Beausoleil 2 , Paul E. Barclay 1 Sacramento Vahid Sandoghdar; Vahid ETH Zurich, - Swit
Polarization and photoluminescence Strong Strong coupling of laser light to an emitter Haw Yang; Princeton Univ., USA. Princeton Univ., Haw Yang; , Neil B. Manson 2 , Charles Santori 1 Hewlett-Packard Labs, USA, Labs, Hewlett-Packard LSTuD1 • 10:30 a.m. LSTuD1 Strong Strong Coupling of Propagating Laser Light to Single Emitters: From Absorption to Stimulated , Emission zerland. will from beranging discussed contexts, in different absorption spectroscopy of single quantum dots at single of emission stimulated and temperature room cryogenic temperatures. molecules at dye Single Quantum Dots Localfor Probing - Environ , ments emission of dots individual mittent makes quantum We changes. time-dependent probe to challenging it explain strategies to these overcome difficulties and discuss using them as ratiometric resonance energy sensors. temperature as and probes transfer-based Australia. excitation spectroscopy are used to measure the nitrogen-vacancy center optical transition polariza- Finite temperature. of function a as linewidth and tion relaxation and line-broadening is observed even at 25~K. below temperatures 1 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 Photophysics of Quantum • LSTuD I Dots and Nanostructures Natl. Gaffney; SLAC J. Kelly Univ., Stanford Lab, Accelerator USA, Presider LSTuD2 • 11:00 a.m. LSTuD2 LSTuD3 • 11:30 a.m. LSTuD3 Dependence of Temperature the and Polarization Linewidth of the Optical Transitions of Single Centers Nitrogen-Vacancy in Diamond C. Fu Rogers Chris , , Phillip B. Phillip The The use of Anirban Mitra, Mitra, Anirban Achieving Achieving cellular FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Invited Invited Atherton molecular microensdoscopy. This requires requires This microensdoscopy. molecular Imaging of Targeted Drug Delivery to in vivo FTuL3 • 11:15 a.m. In vivo Tumors Based on Fluorescence Resonance En- , Optical and Tomography Diffusion ergy Transfer A. Kularatne, Sumith Kevin Webb, Gaind, J. Vaibhav results Experimental USA. Univ., Purdue Low; S. Philip for imaging a model for targeted anti-cancer drug delivery to a tumor in a mouse using fluorescence diffuoptical energy(FRET) and - transfer resonance presented. are (ODT) tomography sion co-development co-development of optical technologies with - mo lecular probes. We have identified unique peptides that provide molecular contrast for miniaturized microscopes. confocal 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 FTuL Molecular Imaging and • Nanomedicine USA, Univ., Yale Levene; J. Michael Presider FTuL4 • 11:30 a.m. FTuL1 • 10:30 a.m. FTuL2 • 11:00 a.m. Detec - Background-Free and Phase-Free Real-Time tion of Nanoparticles and , Viruses Bradley Bradley Deutsch, Filipp Ignatovich, Lukas Novotny; - phase-sensi implement USA. We Rochester, of Univ. tive optical detection and characterization of nano- particles. The elimination of the phase contribution to the detected signal helps improve the measured particle size accuracy and resolution, compared to techniques. interferometric standard Biomimetic Strategies for Modification of Surfaces Surfaces of Modification for Strategies Biomimetic , Moieties and Targeting with Passivating Messersmith; Northwestern USA. Univ., nanoparticles in medicine requires great attention to surface properties due to the high surface areas of nanoparticles. In this talk I will describe - biologi bio-interfacial controlling for strategies inspired cally surfaces. at phenomena Molecular Probes for Microendoscopy Contag; Stanford USA. Univ., resolution and molecular specificity is the objective of FiO Daniel , Franz Edward 1
, Vladimir 1 Todd Todd Ditmire;
We will report on the We Max-Planck Max-Planck Inst. für , Laszlo Veisz 1 1 Invited Invited ; 1,3 HASYLAB/DESY, Germany, Germany, HASYLAB/DESY, 2 , Christopher Sears 1 Glen Ellen Glen , Raphael Tautz 1 , Ferenc Krausz , Karl Schmid 3 2 Ludwig-Maximilian-Univ. München, Germany. Ludwig-Maximilian-Univ. We FTuK3 • 11:30 a.m. Generation of Sub-Three-Cycle, 16-TW Light Pulses through , Noncollinear OPCPA Herrmann Tavella FTuK2 • 11:00 a.m. Quantenoptik, Germany, Germany, Quantenoptik, 3 FTuK1 • 10:30 a.m. 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 Laser Power FTuK High Peak • II Technology Florida, of Univ. H. Reitze; David USA, Presider Pervak present a 16-TW (7.9 fs, 130 mJ) non-collinear optical optical non-collinear mJ) 130 fs, (7.9 16-TW a present This system. amplification chirped-pulse parametric servecan source unique PW-class as seed for source lasers and by itself allows for new experiments in high-field physics. The Texas The Petawatt LaserTexas and Technology Devel- opment toward an Exawatt Laser, Status Status of the National Ignition , Facility I. Moses; Lawrence Natl. Livermore Lab, USA. I will capabilities NIF and NIF of status current the discuss in opportunities new fusion, demonstrating including astrophysics and other areas of high energy density science, and LIFE, the near-term goal of clean fu- energy. sion USA. at Austin, of Texas Univ. performance of the Texas Petawatt Laser and the We system. this on pursuing are we program science will also discuss how this technology might scale to laser. Exawatt-class an Tuesday, October 13 64 and Displays—Continued FTuF • 3-D Capturing, Visualization ______Empire 12:00 p.m.–1:30p.m. 12:00 p.m.–2:00p.m. OSA Fellow Silicon MemberLunch, Valley Capital Club, 50W. San Fernando, Suite 1700,San Jose, California 95113,Phone: 408.971.9300 Crystal FiO/LS/AO/AIOM/COSI/LM/SRS 2009 1 12:00 p.m.–1:30p.m. st InternationalOSAStudentChapterSolarMini-CarFinalRaces,Imperial Ballroom, Fairmont Hotel 12:00 p.m.–1:30p.m. Woods ning to linear scanning. - scan sinusoidal nonlinearconverting forcapability zooming with element corrective optical fabricated we test and characterize our previously designed and Optics I—Continued •DiffractiveandHolographic FTuH tion dal Scanning: Interference Approach Implementa- Binary Diffractive Element for Linearizing Sinusoi - •11:45a.m. FTuH5 USA, , 2 aae Haji-Saeed Bahareh SolidState Scientific Corp.,paperIn this USA. 1 , JohnKierstead, Exhibit Only Time, ImperialExhibit OnlyTime, Ballroom, Fairmont Hotel NOTES FiO Gold 2 ; 1 Lunch Break(on yourLunch own) AFRL, Sensors Directorate,Sensors AFRL, 1 , Jed Khoury Jed , • 1 , Charles L. L. Charles , October 11–15,2009 For Fall Congress presentations onTuesday, seepages116-124. Processing I—Continued •All-OpticalSignal FTuI Valley Continued II— •AndersonLocalization FTuJ California Tuesday, October 13 65 Hillsborough LSTuF • Micro- and • LSTuF III—Continued Nanofluidics LS Piedmont LSTuE • Cavity Optomechanics II— Cavity Optomechanics • LSTuE Continued For Fall Congress presentations on Tuesday, see pages 116-124. Congress presentations on Tuesday, For Fall , ; 1 1 October 11–15, 2009 • Arka Majumdar , Jelena Vučković 1 (on your own) Lunch your Break (on Coherent Coherent USA. Univ., Harvard 2 NOTES Sacramento , Andrei Faraon 2 Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Exhibit Only Time, Imperial Stanford Univ., USA, Univ., Stanford LSTuD • Photophysics • LSTuD Dots and of Quantum I—Continued Nanostructures LSTuD4 • 11:45 a.m. • 11:45 LSTuD4 Single Quantum Dot Spectroscopy via Non- Resonant Dot-Cavity , Coupling 1 quantum dot spectroscopy is performed in a quantum quantum a in performed is spectroscopy dot quantum dot coupled to a photonic crystal cavity by - exploit ing non-resonant dot-cavity coupling. This enables readout and levels dot quantum the of manipulation emission. cavity through Dirk Englund 12:00 p.m.–1:30 p.m. Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Final Races, Imperial International OSA Student Chapter Solar Mini-Car st 12:00 p.m.–1:30 p.m. 1 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Atherton Silicon Valley Capital Club, 50 W. San Fernando, Suite 1700, San Jose, California 95113, Phone: 408.971.9300 95113, Phone: California Jose, 1700, San Suite Fernando, San 50 W. Club, Capital Valley Member Lunch, Silicon OSA Fellow FTuL Molecular Imaging and • Nanomedicine—Continued 12:00 p.m.–2:00 p.m. FiO 12:00 p.m.–1:30 p.m. Glen Ellen Glen Xudong Xie, Xudong Qihua Zhu, Xiaoming , We We demonstrated high energy broadband ______FTuK4 a.m. • 11:45 Generation of 100-J Sub-Picosecond Laser Pulse - Ampli ChirpedPulse Nd:Glass Energy High from fication System Yanlei Zhou, Kainan Huang, Xiaojun Wang, Xiao Zeng, Zuo, Feng Jing, Haiwu Res. Yu; of Ctr. Laser Fusion, China. chirped pulse amplification at Nd:glass amplifiers system. Seed was amplified pulse by generated OPA by fs 710 to recompressed and 5.5nm with 168J to up compressor. tiled gratings FTuK • High Peak Power Laser Power FTuK High Peak • II—Continued Technology Tuesday, October 13 66 Focus Cues, PresentsthatDisplayNearlyCorrect Novel 3-D A may causeintroduced. fatigue be visual will convergenceaccommodativeand andtween stimuli be discrepancy with images stereoscopic viewing behaviors of accommodation and convergence when tempts to measure and analyze the static and dynamic KazuhikoWasedaUkai; Univ., Japan. Accommodation Responses to Stereoscopic Images, M. HoffmanM. research and various applications. with correct focus cues. It has great potential for vision display, to construct a temporally-multiplexed image the to synchronized (1000Hz), lens switchable fast, UK. 1 •1:30p.m. FTuM1 Connecticut, USA,Presider Bahram Javidi; Univ. of Frontiers I Technologies andResearch •Emerging3-DDisplay FTuM 1:30 p.m.–3:00p.m. FTuM2 •2:00p.m. FTuM2 Univ. of California at Berkeley, USA, We describe a stereoscopic system that uses a uses that system stereoscopic a describe We
1 Martin S. Banks , Philip, J.W. Hands Empire Invited Invited 1 , Gordon D. Love D. Gordon , 2 , AndrewKirby, K. 2 Durham Univ., Our recentat- Our 2 , David David , 2 - ; Optical Metamaterials, Optical plasmonic lasers. sub-wavelength and frequencies optical at cloaking negative refraction and negative-index metamaterials, These include sub-diffraction imaging and focusing, plasmonics. and metamaterials with associated ena experimental demonstrations of intriguing phenom- USA. Berkeley,at California FTuN1 •1:30p.m. FTuN1 Republic of Korea, Presider Dai-Sik Kim; Seoul Natl. Univ., and Cloaking •NegativeIndexFTuN Materials 1:30 p.m.–3:30p.m. low-loss invisibility. and broadband enables which materials dielectric isotropic of only consists cloak carpet The surface. reflecting curved a under object an conceals that cloak optical dielectric realizationa of experimental an report We USA. Berkeley, at California Univ.of Jensen Li, Thomas Zentgraf, Guy Bartal, Xiang Zhang; Optical Cloaking Using , Dielectrics •2:00p.m. FTuN2 Crystal Invited Xiang Zhang; Univ.of Zhang; Xiang FiO/LS/AO/AIOM/COSI/LM/SRS 2009
I will discuss recent discuss will I Thank youforattending know yourthoughtson post-conference survey FiO/LS/Fall Congress. Jason Valentine, via emailandletus Look foryour the program. sional Optics, sional Three-Dimen- of Engineering and Applications tion properties. polariza- and spatial, spectral, unique exhibit that elements optical highlights talk This applications. many enable to decade last the over evolved have LC, USA. Menelaos Menelaos Poutous FTuO1 •1:30p.m. FTuO1 Louis, USA,Presider Guoqiang Li; Univ. of Missouri at St. Optics II •DiffractiveandHolographic FTuO 1:30 p.m.–3:30p.m. 1 determining phases of the diffracted beams. determining phases of diffracted the X-ray diffraction experiments; namely the problem of from media crystalline of determination structure longstandingofproblem encounteredtheory the in a to solution presentWe Rochester,USA. Univ.of from MeasurementsX-Ray Diffraction , Media Crystalline of Determination Structure of Theory the in Problem Phase the of Solution •2:00p.m. FTuO2 Univ. of North Carolina at Charlotte, USA, Diffractive and Diffractive micro-optical components Eric Johnson Eric 1 , Zachary Roth Zachary , FiO Gold Invited 1 , Pradeep Srinivasan Pradeep , 1 , Raymond Rumpf Raymond , • 2 Emil Wolf; Prime Res. October 11–15,2009 1 2 ; , For Fall Congress presentations onTuesday, seepages116-124. WDM-PON addressed. be will reach long for factors limiting and achievements Recent TDM-PON. a with compared loss splitting attractivefor long distance PON, since it has small a most is WDM-PON A offices. central of solidation con- enable reach extended with (PONs) networks Korea. of RepublicKAIST, Lee; Hee Reach Extended Passive NetworksOptical , FTuP1 •1:30p.m. FTuP1 HDTV signals with 100GHz signals channelHDTV spacing. of channels 125 accommodate can It diodes. laser Fabry-Pérot injected mutually using transmission Republic of Korea. TechnologyTelecomLab,NetworkKorea Dept., Res. Rochester, USA,Presider Anabil Chaudhuri; Univ. of •OpticalAccess FTuP 1:30 p.m.–3:30p.m. Hee Lee Sil-Gu Mun Sil-Gu Noise Mutually Injected Fabry-Pérot Laser , Diodes Low Employing Transmission Signal Broadcast •2:00p.m. FTuP2 1 ; 1 KAIST, Republic of Korea, 1 , Sang-Min Oh Sang-Min , We demonstrated a broadcast signal Valley Invited 1 , Ki-Man ChoiKi-Man , 2 Next Generation Passive optical Passive 2 , Chang- , Chang- of interest. wavelengths all for retina and lens cornea, human for exist limits exposure international and US sure. - expo laser to respect with radiation—particularly established thresholds for injury from ocular optical cal Physicist, USA. Extensive biomedical research has Light and Eye Safety, FTuQ1 •1:30p.m. FTuQ1 American Society forAmerican Photobiology, Society 2008–2009. Corp., New York, 1980). He served as PublishingPresident (Plenumof Sources” the Optical Other and authored the 1000-page handbook, “Safety with Lasers LIA in 2005 and the Wilkening Award in 2004. He co- AwardSchawlow the the fromreceived and 1977 in Yugoslaviato Scholar Fulbright a was He ICNIRP). sources (ANSI, ISO, ACGIH, IEC, WHO, optical NCRP,high-intensity other and and lasers from ticular par in radiation non-ionizing against protection for standards safety of establishment the in active of numerous committees and institutions, which are surgery. He served as member, advisor and chairman hazards applicationslaser andlaser andmedicine in laser-tissueeye,upon the interactions,effects UV to 2007. His research interests focus on subjects related PreventiveMedicine for many years untilretiringin and PromotionHealth for Center U.S.Army the at Program Radiation Laser/Optical the of Manager the was Ophthalmology.He Instituteof London, of in biophysics and medical physics from the University University, Emory from health logical Ph.D.his and radio- andphysics in PolytechnicM.S. Institute,his Virginiafromphysics in B.S. his receivedDr. Sliney Waterloo, Canada, Presider Melanie C.Campbell; Univ. of •LightintheEye FTuQ 1:30 p.m.–3:30p.m. California David Sliney; Consulting Medi- Tutorial - Tuesday, October 13 67 We The The talk Invited Invited Hillsborough LSTuI1 • 1:30 p.m. LSTuI1 Fast Fast Electron Migration in Finite Systems during XFEL Pulsesand , Attosecond Exposure Intense to Ulf Saalmann, Ionut Georgescu, Christian Gnodtke, Alexey Rost; Mikaberidze, Jan-Michael Max-Planck- Germany. Systems, Complex of Physics the for Inst. in scale time 1-fs a on electrons of migration analyze following rare-gas-clusters irradiation of the cluster will as it - XFEL-pulse beor avail attosecond with an XFEL in Hamburg. and in Stanford LCLS at able Regime, X-Ray the in Physics Atomic Strong-Field Louis DiMauro; Ohio State USA. Univ., examines the scalingthe into physics of strong-field experiments first the on report status A regime. X-ray XFEL LCLS the using team AMOS the by performed will also be SLAC presented. at LSTuI2 • 2:00 p.m. LSTuI2 1:30 p.m.–3:30 p.m. 1:30 p.m.–3:30 Field Dynamics I • High LSTuI Natl. SLAC Guehr; Markus Univ., Stanford Lab, Accelerator USA, Presider
Jeremy Jeremy - ob the report We Harvard Univ., USA. Univ., Harvard 2 Thomas J. Watson Labs Labs Watson J. Thomas 1 Invited Invited ; 2 LS - Ham Klemens Groeblacher, Simon Piedmont , Federico Capasso Federico , 1 of Applied Physics, Caltech, USA, Caltech, Physics, Applied of servation of optomechanical normal mode splitting, modenormal splitting, servation optomechanical of which evidenceis unambiguous coupling for strong of cavity photons to a mechanical This resonator. paves the way towards full quantum optical control devices. micromechanical and nano- of Demonstration Demonstration of Micromechanics in the Strong Regime, Coupling Aspelmeyer; IQOQI,Markus Vanner, Michael merer, Austria. Sciences, of Acad. Austrian Casimir Repulsive and Attractive of Measurement Nanomechanics, to Applications and Forces Munday LSTuH1 • 1:30 p.m. LSTuH1 The Casimir force results from quantum fluctuations fluctuations quantum from results force Casimir The between objects. We discuss the measurement of attractive and repulsive forces, how they can lead to ultra-low static friction devices, and the idea of torque. a QED 1:30 p.m.–3:30 p.m. 1:30 p.m.–3:30 III Cavity Optomechanics • LSTuH Arizona, of Univ Meystre; Pierre USA, Presider LSTuH2 • 2:00 p.m. LSTuH2 For Fall Congress presentations on Tuesday, see pages 116-124. Congress presentations on Tuesday, For Fall , , , 1 1 Inst. Inst. 2 , Olga , Yurii , Yurii 1 1 Inst. Inst. of 3 October 11–15, 2009 , Andrew P. 3 , Kelly Zewe 1 , Alexei I. - Tol Zernike Inst. for for Inst. Zernike • 3 2 , David J. Hagan 3 , Honghua , Hu Honghua 1 Invited , Lazaro A. Padilha CREOL, CREOL, College of Optics 1 1 ; 1 , James H. Werner 2 Sacramento , Gizelle A. Sherwood , Davorin Peceli 1 , Alexei D. Kachkovski 1,2 3 Scott Scott Webster Fluorescence microscopy is used to probe probe to used is microscopy Fluorescence , Carnegie Mellon Univ., USA, Univ., Mellon Carnegie , Vladimir V. , Kurdyukov Vladimir V. 1 3 ; 3 Ctr. for Integrated Nanotechnologies, Los Alamos Natl. Natl. Alamos Los Nanotechnologies, Integrated for Ctr. LSTuG2 • 2:00 p.m. LSTuG2 Enhancement of Triplet Yields in Cyanine-Like Molecules Using Using Fluorescence Microscopy of Oligomer Aggregates to Understand the Properties of Con- jugated Polymers Used in Photovoltaic Devices Linda Peteanu machov LSTuG1 • 1:30 p.m. LSTuG1 V. Przhonska V. and and Photonics, of Univ. Central Florida, USA, Shreve 3 1:30 p.m.–3:45 p.m. 1:30 p.m.–3:45 Optoelectronic Materials • LSTuG Characterization of Univ. Early; T. Kevin USA, Amherst, Massachusetts Presider Labs, USA. Labs, lifetime emission and structure vibronic in variations - aggre with trends and aggregates individual between gate size and oligomer chain length. The results are polymers. to and models theoretical to compared Advanced Materials, Univ. of Groningen, Netherlands, Netherlands, Groningen, of Univ. Materials, Advanced Organic Chemistry, Natl. Acad. Natl. Organic of Chemistry, Sciences, Ukraine. A series of oxo- and thio-squaraine dyes were in- vestigated by femto/pico/nanosecond pump-probe techniques. Thio-squaraines show increased triplet quantum yields which are explained by quantum calculations. chemical of of Physics, Natl. Acad. of Sciences, Ukraine, Jurjen Jurjen Wildeman Eric W. Van Stryland L. Slominsky FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Tutorial - Col CREOL, Richardson; Martin Atherton EUV lithography promises to bepromises EUV the lithography next, and Martin Martin Richardson made his dissertation research and in the UK in the plasmas mid-60’s, in lasers and had made many contributions to these fields Herzberg since. the at programs research major lead has He CNRC Laboratories Institute, in Ottawa, at the uni- now is and Florida Central and Rochester of versities the Laserfounding director of the Institute, Townes a new laser center at UCF associated with CREOL and the College of Optics and His Photonics. group potential the recognize to first the of one was UCF at EUV for sources laser-plasma repetition-rate high for He lithography. has held visiting appointments at other institutions including the Max-Born-Institute and the Max-Planck-Institute for Quantum Optics in Germany, the Institute for Laser Engineering at Osaka and University, the Prokhorov General in Physics Institute the Soviet A Union. of recipient he the has Schardin Medal, 500 over an OSA fellow, and publications patents, numerous is a past Assoc. Editor of JQE, and has organized conferences many laser applications. lasers and on 1:30 p.m.–3:15 p.m. 1:30 p.m.–3:15 FTuS Short Wavelength • and Applications I: Generation EUV to X-Rays From of Univ. C. Kapteyn; Henry USA, Presider Boulder, at Colorado FTuS1 • 1:30 p.m. , Lithography EUV Florida, Central of Univ. Photonics, and Optics of lege USA. maybe the last, technology - develop the to review extend Law We Moore’s chips. computer of fabrication it as faces technology this challenges and status ment, implementation. nears , 2 FiO Tampere Tampere We have We 2 , G. Genty 1 Ctr. de Mathématiques de Mathématiques Ctr. 3 J. J. M. Dudley Invited Invited , We We discuss recent studies of
Glen Ellen Glen Univ. of Univ. France, Franche-Comté, 1 ; 3 FTuR2 • 2:00 p.m. large large amplitude extreme value rogue “optical wave” instabilities, focusing both on their intrinsic optical characteristics and their links with their oceanic counterparts. et et de Leurs École Applications, Normale Supérieure de Cachan, France. FTuR1 • 1:30 p.m. 1:30 p.m.–3:30 p.m. 1:30 p.m.–3:30 and Related Waves FTuR Rogue • Phenomena Labs, Bell McKinstrie; J. Colin Presider USA, Alcatel-Lucent, F. Dias F. Finland, of Technology, Univ. Rogue Waves Rogue in Waves Optics Freak Ocean Waves Freak in Ocean One Waves and , Dimensions Two Peter Janssen, Jean-Raymond Bidlot; European Ctr. UK. Forecasts, for Weather Medium-Range oceanfreak of generation the theorya for developed extreme sea for measure The resulting waves. states, namely maximum wave height, is compared with observations. buoy Tuesday, October 13 68 accurate to depth cues perception. vergence reduceconflicts, fatigue, and provide more accommodation/ overcome distances, viewing ent differ at objects position optically to levels, focus different with beams light superimposed multiple ington, USA. , Light Scanned Multi-Focal Using Display 3-D TrueVolumetric FTuM3 •2:30p.m. FTuM3 Frontiers I—Continued Technologies andResearch •Emerging3-DDisplay FTuM Thank youforattending know yourthoughtson post-conference survey FiO/LS/Fall Congress. via emailandletus Our Our novel 3-D volumetric displays scan Look foryour the program. Brian Schowengerdt;BrianUniv. Washof - Empire Invited - on Blair John light of 580nm. reported a negative refractive index of -0.25 at yellow tance, and corresponding numerical simulations, we - reflec transmittance, its studying By miniaturized. further was design fishnet based silver established Drachev, Vladimir Shalaev; Purdue Univ., well A USA. Xiao, Uday K. Chettiar, Alexander Kildishev, Vladimir Yellow Light Negative-Index Metamaterials, •2:15p.m. FTuN3 USA, mittivity Per Negative with Material Optical Metal-Free •2:45p.m. FTuN5 numericalthe simulations. microscopy. The dataexperimental agreed well with directly byvisualized the near-field scanning optical was performance cloak array.The nano-rod silicon usingimplemented was cloak plane ground quency Foreignof Studies,freRepublic- Korea.optical of An metamaterials with low loss and optical gain. to a new generation of nanoplasmonic materials and optical material (laser dye). This result paves the road metal-free in permittivity negative demonstrated Rhee Barnakov Colorado, USA, Colorado, and Cloaking—Continued •NegativeIndexFTuN Materials Silicon Nanorod Array, Nanorod Silicon on Based Cloak Plane Ground Near-Infrared •2:30p.m. FTuN4 3 , ChristopherJ., Summers 2 We have experimentally experimentally haveWe Univ., USA. Purdue , 1 G. Zgu G. , M. A. Noginov A. M. , 2 , Jin-HyoungLee , 2 Georgia Tech,USA, Georgia 1 , E. E. NarimanovE. E. , Crystal Venkata Ananth TammaAnanthVenkata 1 ; FiO/LS/AO/AIOM/COSI/LM/SRS 2009 2 1 1 , Won, Park ofl Sae Univ., State Norfolk , Qi Wu Qi , 2 , H. Li H. , 3 Hankuk Univ.Hankuk 1 , Seuk-Joo , 1 ; 1 1 , Yu.A. , Univ.of Shumin Shumin 1 - , fields in the ferroelectric domains. ferroelectric inthe fields internal the by induced modulation index the from obtained easily be could quantities statistical scopic of periodically poled lithium niobate crystals. Micro - an efficient diffraction method for quality evaluation Pusan Natl. Univ., Republic of Korea. WeCha;Myoungsik Kim, Joodemonstrate Byoung Lim, HongHwan fraction Poled Domains of Lithium Niobate Crystal by Dif- Non-Destructive Quality Evaluation of Periodically •2:15p.m. FTuO3 in phase-shifting holography. light sources for applicability as low cost light sources diodes (LEDs) have been investigated as low coherent tive and partially transparent samples. Light emitting allowsquantitative phase contrast imaging of - reflec Technology IPT, Germany. Phase-shifting holography Productionfor Inst.Fraunhofer Schmitt; Robert LEDs with Inspection Surface •2:30p.m. FTuO4 Lõhmus Saari , Pulses Ultrashort ing Spatio-Temporal- the Diffract Measuringof Field •2:45p.m. FTuO5 USA, wave pulses including superluminal their speeds. boundary observe we disk, opaque an and aperture temporal and µm-spatial resolutions. Using a circular temporal field of diffracting ultrashort pulses with fs- spatio- the measure directly we TADPOLE, SEA Optics II—Continued •DiffractiveandHolographic FTuO 2 2 , Rick Trebino Inst. of Physics, Univ.Physics,Tartu,Inst.of ofUsing Estonia. 2 , , Peeter Piksarv Krishnamoorthy Pandiyan, Yeon Sook Kang, 1 ; 1 School of Physics, Georgia Tech, FiO Gold 2 , Heli Valtna-Lukner aea . Bowlan R. Pamela , Stephan Stürwald, Stürwald, Stephan • October 11–15,2009 1 2 , Madis Madis , , Peeter For Fall Congress presentations onTuesday, seepages116-124. Plastic Optical Fiber (GI-POF) Links Beyond 100 Gb/s Transmission over Graded-Index •2:45p.m. FTuP4 jevic Fibers Multimode Graded-Index in Modes Principal 2 can be achieved.can be over100Gb/s ofperfluorinated-GI-POF-links500m at transmission that showWe scheme. proposed that channel-capacity can be closely approached with communication over GI-POF-links. We demonstrate for suitable scheme, LDPC-coded-OFDM adaptive FTuP3 •2:15p.m. FTuP3 as square-root the of length. scale DMDs coupling, high At length. with linearly scale (DMDs) delays mode differential dependent; At low coupling, the impulse response is polarization- coupling. polarization-mode and spatial- including Univ.,USA. FTuP •OpticalAccess—Continued FTuP WeUSA. power-variable-rate-Labs,present a NEC 1 , Lei Xu Lei , ,
Mahdieh Shemirani, Joseph Kahn; StanfordKahn; JosephShemirani, Mahdieh 2 We model multimode propagation, multimode model We , Ting WangTing , Valley Invited 2 ; 1 Univ. of Arizona, USA, Arizona,Univ. of , Ivan B. Djord- imaging modalities. ocular new developing when considered be must cells retinal to poses light to excessivethatexposure However,perception. visual risk in the step first the phototransduction, initiate to necessary is light to Francisco,Univ.SanUSA. Californiaat of Rochester, USA, Light Exposure and the Retina the and Exposure Light Standard ANSI the below Damage Retinal Unexpected William H. Merigan H. William permissible exposure. maximum ANSI the below levels at light visible to in the ophthalmoscope, we have discovered retinal changes fluorescence-equipped adaptive optics scanning laser FTuQ2 •2:15p.m. FTuQ2 FTuQ3 •2:45p.m. FTuQ3 Continued •LightintheEye— FTuQ in vivo in , Jennifer HunterJennifer macaque retina resulting from exposure 2 Univ. of Pennsylvania, USA. California 1 , David R. Williams R. David , Invited Invited 1 , Jessica I. W.Morgan I. Jessica , , Jacque Duncan; Duncan; Jacque 1 ; Exposure 1 Univ.of Using a 2 , Tuesday, October 13 69 , , , I 1 1 2 Wen Li Wen , Craig W. W. Craig , , Margaret Margaret , 1 4 , Arvinder Sandhu 1 JILA, Univ. of Colorado Colorado of Univ. JILA, 1 , Serguei Patchkovskii ; 1 1 Invited Kansas State Univ., USA. Univ., State Kansas 4 , C. Lewis Cocke Lewis C. , 4 , Vandana Sharma Vandana , 3 Natl. Res. Council Canada, Canada, Canada, Canada, Council Res. Natl. 2 Hillsborough , Etienne Gagnon , Phay Ho Phay , 2 3 , Robynne Lock 1 , Henry C. Kapteyn C. Henry , 1 , Predrag Ranitovic Predrag , 1 Argonne Natl. Lab, USA, Lab, Natl. Argonne LSTuI • High Field • High LSTuI Dynamics I—Continued Probing Coupled Probing Electronic and Nuclear Dynam- , X-Rays Electronsand Coherent Using ics at Boulder, USA, Boulder, at Hogle Murnane 3 will present will three studies in present which the elec- coupled probed are molecules in dynamics nuclear and tronic HHG-based (HHG), generation harmonic high using field ionization. strong laser and X-ray ultrashort Xibin Xibin Zhou Albert Stolow SantraRobin LSTuI3 • 2:30 p.m. LSTuI3 We Invited LS Nergis Nergis Mavalvala; MIT, USA. Piedmont , LSTuH • Cavity • LSTuH III—Continued Optomechanics LSTuH3 • 2:30 p.m. LSTuH3 Exploring Exploring the Quantum Limit in Gravitational Detection Wave describe experiments in which macroscopic radiation cool pressure and trap optically to used are forces technique this of applications discuss and oscillators, to gravitational-wave detection, and to observation - mechani macroscopic effects involving quantum of cal oscillators. For Fall Congress presentations on Tuesday, see pages 116-124. Congress presentations on Tuesday, For Fall Dept. Dept. 2 Physics Physics , Zohar 1 , Sharon Sharon , 2 1 ; October 11–15, 2009 4 • , Lev Chuntonov , Uri El-Hanany Uri , 1 3 - demon We Israel. St., Gordon 43C 4 Sacramento , Mordechai , Segev Mordechai Adarsh Kumaran Nair Valsala Devi 1 , Emil Zolotoyabko Emil , , 2 Dept. of Materials Engineering, Technion-Israel Inst. of of Inst. Technion-Israel Engineering, Materials of Dept. LSTuG • Optoelectronic Materials Optoelectronic Materials • LSTuG Characterization—Continued LSTuG3 • 2:15 p.m. • 2:15 LSTuG3 in Exciton Generation Phonon Acoustic Coherent , Strength Coupling on Dependence Self-Trapping: Jason Mance, F. X. Morrissey, Susan L. Dexheimer; USA. The dynamics Univ., State of self- Washington studied in are quasi-one- formation trapped exciton dimensional systems using femtosecond impulsive excitation techniques. Low temperature - measure ments reveal the generation of coherent acoustic the of localized associated with the waves formation deformation. lattice Shwartz strate a light-induced method to enhance, control, and and control, enhance, to method light-induced a strate crystals. CZT:V bulk in two-photon-absorption tune - enhance and real-time, in reversible is technique The ment scales linearly with control-beam intensity, the original values. 2.5 times of reaching Amitay 3 • 2:45 p.m. LSTuG5 a-SiGe in Transport Dispersive Disorder-Mediated Spectroscopy, Terahertz Time-Resolved by Studied C. R. Susan Hamner, L. Dexheimer; Washington USA. carrier Photo-excited dynamics in Univ., State a-SiGe:H are studied using optical-pump/terahertz- - domi are that dynamics find We spectroscopy. probe time-dependent a with transport dispersive by nated of degree the with systematically varies that mobility in the material. disorder Technology, Israel, Israel, Technology, Dept., Technion-Israel Inst. of Technology, Israel, Israel, Technology, of Inst. Technion-Israel Dept., LSTuG4 • 2:30 p.m. LSTuG4 Light-Induced Tuning and Enhancement of Two in Single Bulk Semiconductor Absorption Photon Crystal of Chemistry, Technion-Israel Inst. of Technology, Israel, Israel, Technology, of Inst. Technion-Israel Chemistry, of
, , , 1 2 1 , Fan Jian 2 Colorado State 1 ; 2 Lukasz Lukasz Urbanski , Carmen S. Menoni S. Carmen , 1 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 , Artak Isoyan Invited 1 James Dunn; Lawrence Livermore Livermore Lawrence Dunn; James Atherton , Franco Cerrina , Franco , Jorge J. Rocca J. Jorge , 1 2 Plasma-based X-ray lasers are ultra- lasers Plasma-basedare X-ray Univ. of Univ. USA. Wisconsin-Madison, 2 FTuS • Short Wavelength FTuS Short Wavelength • and Applications I: Generation EUV to X-Rays—Continued From FTuS3 • 2:30 p.m. We We discuss different nanopatterning approaches using table top extreme ultraviolet lasers based on self imaging and Talbot lithography, interferometric lithography. projection holographic Univ., USA, Univ., Przemyslaw W. Wachulak W. Przemyslaw Cheng Yang-Chun C. Mario Marconi FTuS2 p.m. • 2:15 Table SchemesTop for Nano-Patterning with Extreme Ultraviolet Lasers, High High Brightness Plasma-Based Soft X-Ray Lasers , Applications and USA. Lab, Natl. bright, compact sources with continued - improve ments in efficiency, output energy, repetition rate, coherence and related characteristics. Results are presented for recent developments in sources and applications. FiO SUNY SUNY 1 ; 2 Invited , Richard , O. Richard Moore 1 Glen Ellen Glen New New Jersey Inst. of USA. Technology, 2 Gino Biondini , FTuR3 • 2:30 p.m. FTuR • Rogue Waves and Related and Related Waves FTuR Rogue • Phenomena—Continued Buffalo, Buffalo, USA, Methods Methods for Simulating Rare Events in Optical Systems We describe the application of importance sampling sampling importance of describe the application We Carlo efficiencyMonte the of improve to techniques in- probabilities, event of rare various computations - communi soliton-based in deviations phase cluding generation. frequency comb and cations Tuesday, October 13 70 ______Empire scattering at fundamental the frequency. with uncloaked scenarios, while having relatively low monic induced dipoles can be enhanced as compared theoretically show that relative values of second-har around second-order nonlinear optical materials, we Univ.Pennsylvania,of Using USA. cloaks plasmonic Optical Optical Nonlinearity, Second-Order with Cloaking Plasmonic Mixing •3:15p.m. FTuN7 on invisible the sphere presented. be will proposed for their fabrication. A comprehensive study in assessing performance of imperfect metamaterials devices such as invisibility cloaks in action are useful Singapore, Singapore. Visually stunning depictions of , Cloaks Invisibility Polarization-Dependent and Devices, Index ent Photorealistic Rendering of Metamaterials, Gradi- •3:00p.m. FTuN6 and Cloaking—Continued •NegativeIndexFTuN Materials 4:30 p.m.–5:30p.m. 3:30 p.m.–5:30p.m. Crystal Aaron J. Danner; Natl. Univ.Natl.of Danner; J.Aaron Uday Chettiar, Nader Engheta; 3:30 p.m.–4:00p.m. FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Minorities andWomen inOSA(MWOSA)Tea, Sainte Claire Room, Sainte Claire Hotel Meet theEditorsofAPSJournals,Bamboo Lounge, Fairmont Hotel - demonstrated examples. on several and discussed are structures photonic advanced of frequency domain method for simulating the behavior numerical robust and efficient the as analysis wave coupled rigorous aperiodic the of extensions and Technical Univ., Czech Republic. Recent improvementsCzech Engineering, Physical and SciencesNuclear of Wave Analysis, Coupled Rigorous Aperiodic of Improvements •3:15p.m. FTuO7 multiplexers. cies were achieved for three, four and five 1-D beam - efficien diffraction high algorithm, phase-retrieval Usingarray. imaging terahertz passive receiving heterodyne in multiplexer beam oscillator local as France. UMR-8507; UPMC Univ. Paris 06; Univ Paris-Sud 11, CNRS/ Dégardin,SUPELEC/LGEP;Kreisler;AlainJ. Multiplexing THzBeam , Wayof Elegant An Gratings: Phase Reflection •3:00p.m. FTuO6 Optics II—Continued •DiffractiveandHolographic FTuO Coffee Break/Exhibits,Imperial Ballroom, Fairmont Hotel Reflection phase gratings offer great potential Pavel Kwiecien, Ivan Richter; Faculty NOTES FiO Gold VishalJagtap,S. Annick F. • October 11–15,2009 For Fall Congress presentations onTuesday, seepages116-124. is presented. propagatingchannelsmultiplexedhelically spatially for model Dispersion fiber. multimode index step of strand single wavelengtha oversame channelsof separated spatially of co-propagation allows ing multiplex- domainTechnology, Spatialof Inst.USA. Fibers Multimode Index Step Wavelengthin Same of ing Spatial Domain Multiplexing (SDM) Channels Dispersion Model of Two Simultaneously Propagat- •3:00p.m. FTuP5 FTuP •OpticalAccess—Continued FTuP , Syed H. Murshid, Abhijit Chakravarty; Florida Valley Campbell Degeneration, Macular Related TreatingAge- and Studying for Model Eye Rat A •3:15p.m. FTuQ4 Kostadinka Bizheva Kostadinka hardt Bird AMD-like damage in vivo. livery in potential therapies. We induced and tracked de- light localized and structures fundusof imaging resolution high both givedegeneration can macular Physics Inst., Canada. The rat eye model of age-related Continued •LightintheEye— FTuQ 1,2 1 , Marsha L. Kisilak L. Marsha , ; 1 Univ. of Waterloo, Canada, 1,2 , Aden SeamanAden , California 1,2 , LauraGowing , 1 1 , Christopher J. Cookson J. Christopher , , Dafna SussmanDafna , 2 Guelph WaterlooGuelph eai C W. C. Melanie 1 , Kaitlin, Bung - 1,2 , Mark, 1 , Tuesday, October 13 71 , G. , M. 2 2 , F. , A. F. 2 , A. Trita 1 , G. Giuliani , J. P. , Davis J. P. 2 1 Univ. Univ. of Glasgow, UK, 1 ; ; J. J. Javaloyes 3 We - have investi CSIC, We Spain. 3 , I. Cristiani , D. Duncan 2 1 , , S. Balle 3 Hillsborough Aerospace Mass Properties Analysis, USA, Analysis, Properties Mass Aerospace 1 ; 2 G. R. White , F. Bragheri 1 , , , A. Scire 1 Naval Naval Air Systems Command, USA. We describe a Univ. di Pavia, Italy, di Pavia, Italy, Univ. LSTuI • High Field • High LSTuI Dynamics I—Continued LSTuI4 • 3:00 p.m. • 3:00 LSTuI4 Ultrafast All-Optical Switching of Bistable Semi- conductor Ring Lasers, Narducci Mezosi technique technique by which optical switching between two non-collinear beams can be achieved using recoil resonances in cold atoms. experimentally We dem- fundamental the explore and technique this onstrate speed. the switching to limitations 2 2 gated the all-optical switching properties of bi-stable bi-stable of properties switching all-optical the gated semiconductor ring lasers acting as a logic memory element. Theoretical results are in agreement with experiments on fabricated devices. Switching times attained. ps are few of • 3:15 p.m. LSTuI5 Cold in Resonances Recoil Using Switch All-Optical Atoms Sorel Invited Hong Hong X. Univ., Yale Tang; LS Piedmont We We demonstrate the convergence of silicon LSTuH • Cavity • LSTuH III—Continued Optomechanics LSTuH4 • 3:00 p.m. • 3:00 LSTuH4 Silicon Silicon , Optomechanics USA. nanomechanics and nanophotonics by building silicon based optomechanical devices that operate optomechanical to routes Practical forces. optical on cooling via - and amplifications circuit coupled opto will be cavities discussed.mechanical For Fall Congress presentations on Tuesday, see pages 116-124. Congress presentations on Tuesday, For Fall , - 1 Michael Michael October 11–15, 2009 Victor Victor I. - Kli • Invited , T. Balasubramanian 1 Dept. Dept. of Physics, Natl. Inst. of 1 NOTES Dept. of Materials Engineering, ; 2 2 Sacramento , , M. Ashok 1 Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Coffee Break/Exhibits, Imperial LSTuG • Optoelectronic Materials Optoelectronic Materials • LSTuG Characterization—Continued New New Aspects of Nanocrystal Lasing, mov; Los Alamos Natl. Lab, USA. In this talk, I will review our recent spectroscopic studies of specially sig- a exhibit that nanocrystals core-shell engineered nificant suppression of Auger recombination. This property greatly simplifies real-life applications of technologies. in lasing nanoparticles colloidal Technology, India, Technology, LSTuG6 • 3:00 p.m. • 3:00 LSTuG6 Synthesis and Characterization of Nanospherical Hydroxyapatite Using SDS , as Template S. L. Shanthi Spherical nano crystalline nano Spherical Chile. Concepcion, of Univ. pre been has nm ~200 diameter with hydroxyapatite - pat XRD and FTIR method. co-precipitation by pared obtained results The HAp. of phase the confirmed tern also discussed. EDS analysis and SEM from • 3:15 p.m. LSTuG7 R. Mangalaraja V. , 1 Bamboo Lounge, Fairmont Hotel Fairmont Lounge, Meet the Editors of the APS Journals, Bamboo Sainte Claire Room, Sainte Claire Hotel Claire Sainte Room, Claire Sainte in OSA (MWOSA) Tea, Minorities and Women , Giuseppe 1 , Jose F. Trull 3 Univ. Politècnica Politècnica Univ. 1 ; 2 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 , Rama Raj 3:30 p.m.–4:00 p.m. 3 C. M. Bowden Res. Facility, USA, USA, Facility, Res. Bowden M. C. 2 , Crina M. Cojocaru Atherton 1,2 3:30 p.m.–5:30 p.m. , Michael Scalora Michael , 1 , Fabrice Raineri Fabrice , 2 4:30 p.m.–5:30 p.m. Vito Vito Roppo , France. We et de Nanostructures, de Photonique Lab FTuS • Short Wavelength FTuS Short Wavelength • and Applications I: Generation EUV to X-Rays—Continued From d’Aguanno FTuS4 p.m. • 3:00 The Role of the Phase Locking Phenomenon in LocalizaCavity - Harmonics Third and Second the tion theoretically and experimentally study how the phase- the how study experimentally and theoretically the of dispersion effective changes mechanism locking medium at the harmonic frequencies making them to designed cavity opaque an inside localized become field. the fundamental for be resonant 3 de Catalunya, Spain, Spain, Catalunya, de Ramon Ramon Vilaseca FiO Can Can Sun, Dylov, Dmitry V. Glen Ellen Glen ______FTuR5 • 3:15 p.m. Characterisation and Optimisation of the Soliton Self-Frequency Shift in Photonic Crystal , Fibres Ravi Pant, Alexander Judge, Eric C. Mägi, Boris T. Kuhlmey, Martijn develop de We Sterke, Australia. Benjamin Sydney, J. of Eggleton; Univ. IPOS, CUDOS, the self-frequency shift in analyze model to a simple shift frequency the predict to it use We fibers. optical by prediction the confirm and fibers, different two in full simulations. and numerical experiment FTuR4 p.m. • 3:00 Spectral Dependence of Spatially-Incoherent Modulation , Instability present We USA. Univ., Princeton Fleischer; W. Jason the first experimental study of spatially-incoherent modulation instability for different spectral distri - Characteristic depends behavior sensitively butions. on the underlying profiles. The setup and results introduce a new experimental degree-of-freedom optics. statistical nonlinear into FTuR • Rogue Waves and Related and Related Waves FTuR Rogue • Phenomena—Continued Tuesday, October 13 72 petroleum exploration. and imaging medical as such fields to value add butmay occurred, yetnotcommercialadoption has Widespreadangle. viewing wide a and parallax full with usually imagery, 3-D volume-filling create USA. Inc., SystemsActuality plays and Their Applications Their and plays Dis- Three-Dimensional Volumetric in Progress rewritten many times. and erased be can that displays 3-D updateable 6” holographic3-D display. We have demonstrated 6”x mers are shown to be suitable for large area dynamic barian;Univ. of Arizona, USA. Polymers, PhotorefractiveUsing UpdateableDisplaysHolographic3-D Area Large FTuT1 •4:00p.m. FTuT1 Washington, USA,Presider Brian Schowengerdt; Univ. of Frontiers II Technologies andResearch •Emerging3-DDisplay FTuT 4:00 p.m.–5:30p.m. FTuT2 •4:30p.m. FTuT2 Empire Invited Invited Photorefractivepoly - Volumetric displaysVolumetric , Gregg E. Favalora; E. Gregg Nasser Peygham- Nasser FTuU2 •4:30p.m. FTuU2 be surprisinglybe high. can resolution focusing The materials. such inside even and through light focus to possible is it show dentlight. By controlling incident the wavefront, we Disorderedphotonic materials scatter and blur inci - Materials, Optimal Transmission of Light through Disordered of various phase contrast techniques. of a microscope allowing, for instance, the emulation either in the imaging path or in the illumination path applications of spatial light modulators (SLMs) placed Marte;Innsbruck Medical Univ., Austria. copy with Spatial Light Modulators, WavefrontMicros- for ShapingMicroscopy: SLM FTuU1 •4:00p.m. FTuU1 USA, Presider Olga Korotkova; Univ. of Miami, Sensing II Information Transportand •WavefrontFTuU Designfor 4:00 p.m.–5:30p.m. Allard Mosk; Univ. of Twente, Netherlands. Crystal Invited Invited FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Monika Ritsch- Wepresent integrated circuits. nano-optical of design the in account into taken be should which obtained, is nano-slit a on beam incident by launched polariton plasmons surface transit the for Maxwell’sequations the of solution Canada. Univ.Laval, Sheng; Nano-Slit, Metal a of tion - Diffrac Polaritonthe Plasmon in Surface of Role Kenneth B. Crozier B. Kenneth Pipes Light Optical Ratio Aspect High of Fabrication •4:30p.m. FTuV2 •4:00p.m. FTuV1 Canada, Presider Yanina Shevchenko; Carleton Univ., Technologies •MetamaterialsinEmerging FTuV 4:00 p.m.–5:30p.m. were demonstrated.degrees 89.5 of angle sidewall a and 2.8:1 of ratio a 10μm thick SiO thick 10μm a in pipes light vertical ratio aspect high for niques tech- fabrication Wereport TechnologiesUSA. Inc., , Winnie N. YeWinnieN. 2 layer. Light pipes with an aspect aspect an with pipes layer.Light 1 1 ; , Peter Duane Peter , FiO Gold 1 Harvard Univ.,USA, Harvard Invited an rvl Yunlong Gravel, Yann Closed-form rigorous Closed-form 2 , Munib WoberMunib , • October 11–15,2009 2 Zena Zena 2 , For Fall Congress presentations onTuesday, seepages116-124. Cork, Ireland, Univ., UK, nois tor Amplifiers Optical , All-Optical Header Processing Using - Semiconduc R. J. Manning J. R. Electronics Engineering and Computer Science, Science, Computer and Univ.,China,Peking Engineering Electronics of School Networks, and CommunicationSystems FTuW1 •4:00p.m. FTuW1 Lucent, USA,Presider Inuk Kang; Bell Labs, Alcatel Processing II •All-OpticalSignal FTuW 4:00 p.m.–5:30p.m. atBerkeley, USA, Engineering and Computer Sciences, Univ. of California Amann future optical networks. packet-based protect to developed being firewall optoelectronic an in screening initial provide will It data. 42Gb/s locates programmable patterns of arbitrary length in comprisingsystemtion SOA-basedthree gates logic cal Injection-Locked VCSELs, Injection-Locked cal Physical Origin of Data Pattern Inversion in Opti - •4:30p.m. FTuW2 with experiments. Simulation reflection. masterresultslaser wellagree of effect interference the including model novel a with explained areVCSELs locked injection optical in inversionpattern data adjustable for criteria and origin physical The Germany.Munich, Univ.of cal Guo 3 1,2 , D. Cotter D. , , Devang Parekh , Devang 4 , Connie J. Chang-Hasnain 3 CIP Technologies, UK. 1 2 , G. D. Maxwell School of Electrical Engineering, Bangor 1 ; 2 1 StateKey Lab of Advanced Optical Tyndall Natl. Inst., Univ.College Inst., Natl. Tyndall Valley 1 3 , Werner Hofmann Walter Schottky Inst., TechniInst.,Walter Schottky- Roderick P. Webb Invited 3 , A. J. Poustie Weijian YangWeijian 1 A pattern recogni- ; 1 Dept. Dept. of Electrical 1 , Markus C. 1 3 , X. Yang , S. Larde- 1 , Peng , 2 , due to photorefractive inPPLN crystal. effect in an un-doped PPLN under magnetic field at ~ 0.45 T PPLN crystal was investigated. A π phase shift occurs netic field dependence of terahertz wave generation in gang Chen i Wang Qi Univ., China, Ofer Shapira; MIT, USA,Presider Structures •NovelOpticsofPeriodicFTuX 4:00 p.m.–5:30p.m. lattices is successfully observed. 3-D such in coupling and modulation waveguide the to due diffraction discrete Enhanced technique. photonic lattices by employing the optical induction three-dimensional reconfigurable of demonstration experimental first the on report WeUniv.,China. Discrete , Diffraction Enhanced and Lattices Photonic Dimensional Three- Optically-Induced of Demonstration •4:15p.m. FTuX2 inabove-thresholdlasers operation. of types different between compared are efficiency effects, the modal pump level and energy conversion saturation gain including By lasers. Bragg circular vertically-emitting the forderivedrelation is energy USA. Yariv;AmnonCaltech,XiankaiSun, Power,, Lasers Vertically-EmittingBragg Circular High- Large-Area, of Analysis Above-Threshold •4:00p.m. FTuX1 Guohong Guohong Ma Field, Magnetic External by Induced PPLN doped Un- an in ShiftTerahertz of π-Phase Observation •4:30p.m. FTuX3 1 , WeimingLiu, 1,2 ; 1 2 1 , Jielong Shi Jielong , Natl. Univ. of Singapore, Singapore. Mag San Francisco State Univ., USA, California Peng Zhang 2 1 , Sing Hai TangHai Sing , , Qibiao Zhu 1 , Robert Egger 1 , Chunfang Li 2 ; 1 Shanghai An exact exact An 2 Nankai Nankai 1 , Zhi- 1 - , Tuesday, October 13
73 Matt K. Kalinski; Dept. Invited Hillsborough John John D. Bozek; SLAC Natl. Accelerator Lab, , LSTuL1 • 4:00 p.m. LSTuL1 First First Science with the LCLS X-Ray Free Electron Laser available. not USA. Abstract Univ., Stanford LSTuL2 • 4:30 p.m. LSTuL2 Trojan-Like Wavepackets on in 8-ShapedLinearly Polarized Electromagnetic Field Orbits in Hydrogen Ion Molecule , of Chemistry and Biology, Utah State USA. Univ., We discover the existence of 8-shaped orbits in the hydrogen ions molecules capable to maintain shape oscillatory wavepackets in linearly polarized field when frequency its twice or is in the resonance the motion. frequency of 4:00 p.m.–5:45 p.m. 4:00 p.m.–5:45 II High Field Dynamics • LSTuL Natl. SLAC Guehr; Markus Univ., Stanford Lab, Accelerator USA, Presider
Swiss Federal Federal Swiss 1 ; 1,2 We observed- We optom Invited Invited LS Piedmont Tobias J. Kippenberg J. Tobias
A. Heidmann, P. Verlot, A. Tavernarakis,
, Max-Planck-Inst. of Max-Planck-Inst. Quantum Optics, Germany. LSTuK1 • 4:00 p.m. LSTuK1 Resolved-Sideband Laser Cooling and - Measure the to Close Oscillator Micromechanical a of ment Limit, Quantum Optomechanical Correlations between Light and Mirrors Cohadon; C. Lab A. Molinelli, Kuhn, Briant, T. P.-F. Pierre Univ. Supérieure, Normale École Brossel, Kastler et Curie, Marie CNRS, France. pressure radiation by induced correlations echanical between a light beam and the theresulting mirror to - dis down extended be can scheme This placements. quantum level, with applications in high-sensitivity optics. quantum and measurements LSTuK2 • 4:30 p.m. LSTuK2 4:00 p.m.–5:15 p.m. 4:00 p.m.–5:15 IV Cavity Optomechanics • LSTuK USA, Univ., Yale Tang; Hong Presider Inst. of Technology Lausanne (EFPL), Switzerland; 2 Abstract not available. not Abstract For Fall Congress presentations on Tuesday, see pages 116-124. Congress presentations on Tuesday, For Fall October 11–15, 2009 • Invited Rudolph Rudolph A. Marcus; Caltech, Sacramento Kevin T. Early, Michael Y. Odoi, Pallikkara Pallikkara Odoi, Y. Michael Early, T. Kevin There is There a bodynow substantial of data on the Quantum Dots, Experiments, Theory, Predictions, Predictions, Theory, Experiments, Dots, Quantum and Tests , Unknowns USA. intermittent fluorescence of quantum dots (QD), CdSe. as such 4:00 p.m.–5:30 p.m. 4:00 p.m.–5:30 of Quantum • Photophysics LSTuJ II Dots and Nanostructures of University Barnes; Michael USA, Amherst, at Massachusetts Presider LSTuJ2 • 4:30 p.m. LSTuJ2 Photoluminescence from Single Quantum Dot/ Organic Nanostructures: Ligand Effects on PL Dynamics, of Univ. Barnes; D. Michael Emrick, S. Todd Sudeep, K. photoluminescence The USA. Amherst, Massachusetts dynamics and saturation profiles of quantum dot/ organic composites have been studied at the single - multiexci for evidence strong find We level. particle from arising particles photoexcited in character tonic the surface. to coordinated ligands LSTuJ1 • 4:00 p.m. LSTuJ1
, , 4 1,2 , I. I. , 3 , C. 1 Ultrafast , W. Chao W. , 1 , F. Brizuela 1 , V. V. Kondratenko V. V. , , A. V. Vinogradov V. A. , 4 Colorado Colorado State Univ., 1,2 1 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 ; Technical Univ., Ukraine. Univ., Technical 4 , B. M. Luther M. B. , 1,4 1 Invited Invited C. S. Menoni , Atherton , F. Pedaci F. , 1 , D. T. Attwood T. D. , , J. J. Rocca 1 1,2 , A. G. Ponomareko G. A. , 3 Henry C. Kapteyn, Margaret M. Murnane; , Y. Wang , 1 P. N. P. Lebedev Physical Inst., Russian Acad. of Lawrence Berkeley Natl. Lab, Univ. of California, California, of Univ. Lab, Natl. Berkeley Lawrence 3 2 USA, A. Artioukov A. Brewer Sciences, Russian Federation, Federation, Russian Sciences, USA, 4:00 p.m.–5:30 p.m. 4:00 p.m.–5:30 FTuZ Short Wavelength • and Applications II: Generation and Microscopy Spectroscopy Central of Univ. Richardson; Martin USA, Presider Florida, FTuZ1 • 4:00 p.m. FTuZ2 • 4:30 p.m. E. H. Anderson H. E. M. C. Marconi We We describe the successful implementation of full- field microscopes based on λ=13.2 nm and λ= 46.9 nm table-top lasers that can image nanostructures in transmission and reflection modes with a spatial ~50 nm. of resolution Nanoscale Microscopy with Extreme Table-Top Ultraviolet Lasers Coherent Coherent X-Rays from Ultrafast Lasers, and Nonlinear Meets Science Applications—Attosecond Optics JILA, of Univ. Colorado at Boulder, USA. high-harmonic using sources light short-wavelength generation provides a tabletop coherent EUV light new source for science. show advances Recent rapid - wave X-ray hard even and soft at sources bright that feasible. now are lengths FiO Ethan , Yiwu 2 Resonant 2 I will describe , Debra Wawro 1 Invited Glen Ellen Glen RobertMagnusson Univ. of Univ. Texas at Arlington, USA, 1 ; 2 FTuY3 • 4:30 p.m. F. Schonbrun, Adam R. Abate, Paul Steinvurzel, David David Steinvurzel, Paul Abate, R. Adam Schonbrun, F. USA. By Univ., Harvard Crozier; B. Kenneth Weitz, A. we microfluidics, the and optics the both parallelizing a present system fluorescence capable measurement The of highsystem extremely produces throughput. - measure fluorescence discrete 52,000 approximately per second. ments FTuY2 • 4:15 p.m. Confocal Fluorescence Detection Using a Zone Array Plate in a Microfluidic, Drop Splitter Ding FTuY1 • 4:00 p.m. Guided-Mode Resonance Biochemical Sensor , Technology 4:00 p.m.–5:45 p.m. 4:00 p.m.–5:45 FTuY Optical Biosensing • at Texas of Univ. K. Dunn; Andrew USA, Presider Austin, Sensors Sensors Inc., USA. Optical leaky-mode resonance effects associated with periodic waveguides are - re viewedpotential in and biosensing their application is explained. Use of resonant sensors for - transmis label-free Novel described. is monitoring biochemical discussed. are designs sion-based sensor a label-free-biosensor that exploits the localthe surface- exploits that label-free-biosensor a plasmon-resonance of noble metal nanostructures; abolishes that glass on polymer-brush-interface a and lim- femtomolar a to leading adsorption non-specific blood. in whole analytes protein of it-of-detection Designing Designing Interfaces for Optical , Biosensors Ashutosh Chilkoti; Duke USA. Univ., Tuesday, October 13 74 surfaces. freeform with combined display power low bright, a in resolution HD bring will generation coming reality.The augmented see-through full supporting the last 5 years, a new generation of HWDs emerged, Kevin Thompson Kevin WornDisplays , Head of Generation Coming The USA, makci Frontiers II—Continued Technologies andResearch •Emerging3-DDisplay FTuT FTuT3 •5:00p.m. FTuT3 2 1 Inst. of Optics, Univ. of Rochester, USA. , JannickP.Rolland, 1 , James P.McGuireJames , Empire Invited 2 ; 1 Optical Res. Associates, Res. Optical 1 , Ozan Cak- Ozan , Within 7:00 p.m.–10:00p.m. FTuU3 •5:00p.m. FTuU3 Florida, USA.Abstract not available. Central Univ.of Photonics, and Optics of College , Announced Be to Title Sensing II—Continued Information Transportand •WavefrontFTuU Designfor Crystal 6:00 p.m.–7:00p.m. 6:00 p.m.–7:00p.m. Aristide Dogariu; CREOL, Dogariu; Aristide Invited Laser ScienceBanquet, Gordon Biersch,Laser 33 East San Fernando Street, San Jose, California, Phone: 408.294.6785 7:00 p.m.–8:30p.m. FiO/LS/AO/AIOM/COSI/LM/SRS 2009 DLS AnnualBusinessMeeting,California Room, Fairmont Hotel OSA AnnualBusinessMeeting,Piedmont Room, Fairmont Hotel Simple Lattice and a Superlattice , Nonlinear Surface States at the Interface between a •5:15p.m. FTuV5 directions. desired in focused-beams achieve can oneradiators antenna and layered-substrate the manipulating by that illustrateWe layered-substrate. engineered an nanoantennasby placing plasmonic core-shells over demonstrates a novel approach for designing photonic Univ.,USA. NortheasternMosallaei; Communication, Optical EnablingNanoantennas Array Plasmonic •5:00p.m. FTuV4 Zhigang Chen Zhigang tenna is demonstrated. the radiation performance. A directive QCL nanoan- manipulateto device (QCL) laser cascade quantum a with integrated (PC) crystal photonic patterned focus of this paper is to develop an array of dielectric Wu, Hossein Mosallaei; Northeastern Univ., USA. The , Device QCL Emission Directive Featuring NanoantennaPattern Dielectric Metamaterial A •4:45p.m. FTuV3 2 Zhang excitation location. or staggered phase) were observed depending on the lattices. Two types of interface solitons (with uniform riodic) and super (bi-periodic) semi-infinite photonic at the interface between optically-induced simple - (pe Univ., China. We demonstrate nonlinear surface states Technologies—Continued •MetamaterialsinEmerging FTuV Northwestern PolytechnicalUniv.,China,Northwestern OSA MemberReception, Ballroom, Sainte Claire Hotel 1 , Fajun Xiao 1,3 ; 1 San Francisco State Univ., USA, USA, Univ., State Francisco San 2 Shabnam Ghadarghadr, Hossein Ghadarghadr, Shabnam , Xiaosheng Wang FiO Gold Robert Egger • 1 , Jianlin Zhao This paper This October 11–15,2009 3 Nankai Nankai 1 , Peng Jing 2 , For Fall Congress presentations onTuesday, seepages116-124. performance as co-propagating the signals. same the almost yield counter-propagating signals the that showed and device SOA-DI an in signals propagating signals with those using co-propagating counter- using conversion wavelength of results Ctr. Canada, Canada. We Res. have compared Communications simulation Noad; Julian Cao, Shaochun SOA-DIWavelengthConverter , an in Signals ing WavelengthConversion Using Counter-Propagat - •5:00p.m. FTuW4 and self-phase modulation inoptical fibers. dispersion third-order and second- for observed is mixing in silicon waveguides. Excellent compensation poral imaging system based on broadband four-wave conjugationtemphase - demonstratea with spectral Turner-Foster, Michal Lipson; Cornell Univ., We C. AmyUSA. Gaeta, Foster,L. AlexanderA. Mark Salem, Imaging, TemporalUsing Conjugation Phase Spectral •4:45p.m. FTuW3 thermal stabilitythermal and low power operation. interferometer as switches due to their compact size, semiconductor optical amplifier and Mach-Zehnder optical material. The all-optical proposed circuits use fast arithmetic circuits are presented using nonlinear Al-Zayed;S. Kuwait Univ., Kuwait. ultra- All-optical linear Optical Materials, All-Optical Ultra-Fast Arithmetic Units Using Non - •5:15p.m. FTuW5 Processing II—Continued •All-OpticalSignal FTuW Onur Kuzucu, YoshitomoKuzucu, OnurReza Okawachi, Valley Abdallah K. Cherri, Ayman Lithography Structures Fabricated via Multi-Beam-Interference Crystal Photonic of Calculation Structure Band •5:00p.m. FTuX5 with complete band gaps are presented. structures 3-D and 2-D of Examples theoretically. calculated are lithographymulti-beam-interference via defined structures photonicand3-D 2-D crystal both of structures band The Tech,USA. Georgia Eudenilson L. Albuquerque L. Eudenilson the appliedthe field. of direction the on depends and nonreciprocal, is ferromagnet in an external magnetic field. This shift beam on reflection, at oblique incidence, off an anti- reflected the of shift Norte, lateral a Weinvestigatedo Brazil. Grande Rio do Federal Univ. Jundaí, de Grande do Norte, Brazil,Norte, Grandedo Dumelow Incidence Reflection off Antiferromagnets Oblique on Shift Goos-Hänchen Nonreciprocal •4:45p.m. FTuX4 eral do Rio GrandeRioNorte,Brazil,eral dodo de-multiplexing. division time/wavelength for and buffer optical an as application its for investigated also is Itvelocity. group slow for infiltration crystal liquid on based hole silicon-on-insulator photonic crystal waveguide ing, Univ. of Delhi, India. We propose an elliptical air Rawal,Ravindra Sinha;K. Delhi College ofEngineer Application andin Photonic Device , Crystal Propagation Light Slow Assisted Crystal Liquid •5:15p.m. FTuX6 Structures—Continued •NovelOpticsofPeriodicFTuX 1,2 , FrancineteLima , , Justin L. Stay, Thomas K. Gaylord; Gaylord; K. Thomas Stay, L. Justin California 2 Dept. de Física, Univ.Física, de FedDept. - 2 ; 1 2,3 Univ.Rio do Estado do , José A. P. da Costa P.da A. José , 3 Escola Agrícola Escola , Thomas Thomas Swati Swati 1 - , Tuesday, October 13 75 High High , Pierre Pierre , 1 , Oliver 2 Technische 2 , Franz Pfeiffer Invited 2 Invited , Cameron M. Kewish M. Cameron , 1 Stephen R. Leone; Lawrence Berkeley Berkeley Lawrence Leone; R. Stephen
Hillsborough , Martin Dierolf 1 Paul Paul Scherrer Inst., Switzerland, 1 Andreas Menzel Andreas ; 1 LSTuL • High Field Dynamics II— High Field Dynamics • LSTuL Continued Ptychographic Ptychographic Imaging in Materials and Life Sci- ences, - in the At High Field of Ionization X-Ray Probing Limit, tosecond USA. at Berkeley, of California Univ. Lab, Natl. order harmonics of a Ti:Sapphire laser are used to investigate high field ionization and dissociative ionization by the method of time-resolved X-ray core level spectroscopic transient absorption down time limits. attosecond and femtosecond to LSTuL3 • 4:45 p.m. • 4:45 LSTuL3 LSTuL4 • 5:15 p.m LSTuL4 Bunk - imag diffractive Coherent Germany. München, Univ. microscopy, X-ray in resolution ultimate promises ing and the use of ptychographic methods has proven in - ma Applications particularly and robust. reliable sciences will life terials be and discussed. Thibault
Sumei LS Piedmont LSTuK • Cavity • LSTuK IV—Continued Optomechanics We show squeezing of a nanomechanical mirror can can mirror nanomechanical a of squeezing show We and light vacuum squeezed injecting by generated be regime. sideband resolved the in cavity the into laser 70% squeezing. than more obtain can We Huang, Girish S. Agarwal; Oklahoma State Univ., USA. Univ., State Oklahoma Agarwal; S. Girish Huang, LSTuK3 • 5:00 p.m. LSTuK3 Squeezing of a Nanomechanical , Oscillator For Fall Congress presentations on Tuesday, see pages 116-124. Congress presentations on Tuesday, For Fall - - Xi , Megan 2 October 11–15, 2009 , Alexander 4 • Ballroom, Sainte Claire Hotel Claire Sainte Ballroom, OSA Member Reception, , Sara Maccagnano- Cornell Univ., USA, 2 3 , Keith Kahen 2 Piedmont Room, Fairmont Hotel Fairmont Room, OSA Annual Business Meeting, Piedmont California Room, Fairmont Hotel Fairmont Room, DLS Annual Business Meeting, California Invited Univ. Univ. of Rochester, USA, 1 ; 1,5 , George E. Cragg 3 Sacramento , Xiaofan Ren 1 Inst. of Optics, Univ. of Rochester, USA. of Rochester, of Inst. Optics, Univ. 5 , Manju Rajeswaran 1 , Todd Krauss 4 , John Silcox 3 Eastman Eastman Kodak Co., USA, NRL, USA, 7:00 p.m.–8:30 p.m. LSTuJ • Photophysics of Quantum Photophysics of Quantum • LSTuJ II— Dots and Nanostructures Continued L. Efros Non-Blinking Non-Blinking Semiconductor Nanocrystals, aoyong Wang The photoluminescence The from photoluminescence single semiconductor nano-crystals fluctuations, known exhibits intensity CdZnSe/ZnSe core-shell discuss will We “blinking.” as nano-crystals non-blinking that exhibit continuous, may nano-crystals these how and photoluminescence, applications. in photonics breakthroughs enable 2 4 LSTuJ3 • 4:45 p.m. LSTuJ3 Dot/ Quantum Hybrid from Antibunching Photon Conjugated Organic Composite Sudeep, , K. Nanostructures Pallikkara Early, T. Kevin Odoi, Y. Michael Todd S. Emrick, Michael D. Barnes; of Univ. Mas photo-physical the studied have We USA. sachusetts, properties of isolated CdSe-OPV hybrid - nanostruc tures with photon-pair correlation spectroscopy. observed We a strong wavelength dependent multi- out and in excitation the tuning by emission excitonic absorption. the ligand of LSTuJ4 • 5:00 p.m. LSTuJ4 A. A. Hahn Zacher Gordon Biersch, 33 East San Fernando Street, San Jose, California, Phone: 408.294.6785 Phone: California, Jose, San Street, Fernando San 33 East Laser Biersch, Science Banquet, Gordon 6:00 p.m.–7:00 p.m. 6:00 p.m.–7:00 p.m. FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Invited Matt Zepf; Queen’s Univ. Matt - Bel Zepf; Univ. Queen’s 7:00 p.m.–10:00 p.m. Atherton Relativistically oscillating surfaces have oscillating Relativistically surfaces have FTuZ3 • 5:00 p.m. FTuZ • Short Wavelength FTuZ Short Wavelength • and Applications II: Generation and Microscopy— Spectroscopy Continued Extreme Extreme High Harmonics from Relativistically Oscillating , Surfaces Ireland. fast, developed are poised to provide a step change in the performance of attosecond pulses, by providing a route to achieving both extreme brightness and keV. many to extending energies photon
FiO James Ctr. Ctr. for 1 Eben Ol- Eben ; , Svetlana , Svetlana 1 2 Sherman Fairchild Sherman Fairchild 2 , Gaoshan Jing 1 , Filbert Bartoli 3 Dept. Dept. of Chemical Engineering, 3 Yu Wang Glen Ellen Glen , Susan Perry 2 FTuY4 • 5:00 p.m. Label-Free Screening of Protein Binding to Small Molecule Compound Microarray with a High- throughput Optical Scanning Microscope, P. Landry, Yiyan Fei, Yung-Shin Sun, Juntao Kit Luo, S. Lam, Xiangdong Zhu; of Univ. California at Davis, USA. Using a label-free high-throughput optical scanning microscope we detected endpoints and binding kinetics of vascular endothelial growth factor (VEGF) protein with microarrays of small molecule from compounds the NCI Developmental Program. Therapeutics FTuY5 • 5:15 p.m. Spectral the Voltage-Sensitive of Characterization Dye di-4-ANEPPDHQ Applied to Probing Live GT1-7 , Neurons Tatic-Lucic FTuY Optical Biosensing— • Continued Optical Technologies, Dept. of Electrical and Computer Computer and Electrical of Dept. Technologies, Optical Engineering, Lehigh USA, Univ., Ctr., Ctr., Dept. of Electrical and Computer Engineering, Lehigh USA, Univ., Lehigh Univ., Lehigh USA. Univ., The voltage-sensitive dye di-4- various in characterized spectrally was ANEPPDHQ and solutions in GT1-7 spectraIts neurons. depend on the local chemical and electrical environment. The excitation and emission bands are 430-515nm GT1-7. 550-640nm for and FTuY6 • 5:30 p.m. Broad-Beam Fluctuation Spectroscopy for Non- Diagnostics, Clinical and Cytometry Flow son, Richard Torres, Michael J. Levene; Yale Univ., USA. Univ., Yale Levene; J. Michael Torres, Richard son, We present a novel scanning fluctuation spectroscopy spectroscopy fluctuation scanning novel a present We system, which we term Broad-beam Scanning - Fluc BSFS cytometry. performing for Spectroscopy, tuation is a viable alternative to flow cytometry for a wide cell-basedvariety of clinical diagnostics. Wednesday, October 14 76 FWA2 •8:30a.m. FWA1 •8:00a.m. Natl. Lab, USA,Presider Csaba Toth; Lawrence Berkeley Ultrafast Lasers FWA •BiomedicalApplicationsof 8:00 a.m.–10:00a.m. croscopy Mi Two-PhotonFluorescence in Improvements neurons innematodes. of function the identify help to and cells living in processes biological study to technique this apply ablate cell structures at the submicrometer Wescale. USA. Univ.,Harvard Mazur; Eric Nuzzo, Valeria Chung, Lasers Femtosecond with Nanosurgery experimental resultsexperimental are presented. performance of two-photon microscopy. Theory and differential aberration imaging (DAI) to improve the Univ.,USA. Boston Femtosecond laser pulses make it possible to possible it make pulses laser Femtosecond ,
Kengyeh K. Chu, Tom Bifano, Jerome Mertz; Empire We present a technique called called technique a presentWe Invited Invited ,
Samuel Samuel - their applicationstheir for biochemical sensing. explore and systems nano-plasmonic optofluidic of of optical fields, investigate fabrication and integration structures for localization and resonant transmission USA. Diego, San at California of Univ. Ptasinski; Joanna Sensing, Biochemical for Nano-Plasmonics Optofluidic Presider Kevin Kelly; Rice Univ., USA, Metamaterials the AgeofNanophotonicsand Processing andTransportin FWB •OpticalInformation 8:00 a.m.–10:00a.m. computingof devices. element basic a of model a as used were liquids aromatic by filled core a with fibers elastic optical reviewed for data processing applications. Magneto- rotation spectra for different transparent liquids were Egamov; Samarkand State Univ., Uzbekistan. Faraday , Rings Aromatic with Core Liquid ganic Or Containing Fiber Elastic Magneto-Optical on Based Computing Quantum of Modeling FWB3 •8:45a.m. FWB1 •8:00a.m. vector inputs. beam and scalar arbitrary for applicable is It proposed. is resolutionspatial measurements high sometric with for methods obtaining noiseimmune absolute ellip - inverse and parametersStokes utilizes thatprotocol A Urbana-Champaign,USA. at Illinois Univ.Jr.;of Resolution Spatial High with Measurements Ellipsometric Absolute Noise-Immune Obtaining for Protocol FWB2 •8:30a.m. We explore metal-dielectric nano-plasmonic metal-dielectric exploreWe Yeshaiahu Fainman, Lin Pang, Boris Slutsky, , Santosh Tripathi, Kimani C. Toussaint, C. Tripathi,Kimani Santosh Crystal Invited FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Shukhrat Shukhrat - and Control and Terahertz Nanogap Devices for Field Enhancement Shih behavior spectrally. transmissions. Their interactions lead optical to anti-crossingenhanced of sources the as identified are modes surface guided and resonance cavity Both numerically.and experimentally studied is film Taiwan. S. Kyoung S. S. S. Choi S. S. KimDai-Sik Lee Soonil Nanotube Film Nanotube Carbon Single-Walled in Apertures Rectangular Wavesthrough THz of TransmissionResonant FWC1 •8:00a.m. assisted by shape resonance. is which transmission terahertz enhanced obtain we arrays, holesubwavelength with films Using the good metallic properties and a Drude-like dispersion. rication of single-walled carbon nanotube films with Natl.Univ.,Korea.Wefab - demonstrateofRepublic Rochester, USA,Presider Zhimin Shi; Inst. of Optics, Univ. of and StructuredSurface Transmission FWC •Extraordinary 8:00 a.m.–10:00a.m. 2 2 L. HughesL. Wan Kuang Interactions of Cavity Resonance and Surface Mode, Crystals: Plasmonic in Transmission Enhanced FWC2 •8:15a.m. FWC3 •8:30a.m. these structures. these of applications discuss Wenanoantenna. and gap nano in observed are enhancement field resonant and non-resonant Both devices. nanogap λ/10,000 through transmit waves electromagnetic terahertz Sun Moon Univ., Republic of Korea. of Univ.,RepublicMoon Sun Natl. Tsing Hua Univ.,Taiwan,TsingHua Natl. 3 , William B. Knowlton Transmission of periodically modified Ag modified periodically Transmissionof 1 1 1 2 , Bernard YurkeBernard , , S. M. Koo M. S. , , Rotermund FabianRotermund , ; 1 , Alex English 2 1 , ; Seoul Natl. Univ., Republic of Korea, Korea, of Republic Univ., Natl. Seoul D. S. Kim S. D. 1 Ajou Univ., Republic of Korea,Univ.,Ajouof Republic , Doo-Jae Park Doo-Jae FiO Gold 1 , N. K. Park K. N. , 1 , M. A. Seo A. M. , 1 , Z.-C. Chang Invited 1 1 ; , Jeunghoon Lee 1 Boise State Univ.,State Boise USA, 1 1 , Yeong-Hwan, Ahn , Jin-YoungMoon, 3 Academia Sinica, Sinica, Academia 1 1 • , H. R. Park R. H. , , O. K. Suwal K. O. ,
We show that show We 2 , , Min-Hsiung 1 October 11–15,2009 , William 2 Seoul Seoul 1 , J. , 1 2 1 - , , , For Fall Congress presentations onWednesday, seepages125-131. FWD1 •8:00a.m. these correlations.these of signature a observe experimentally and emerge, correlations field universal nonlinearities strong forWe thatlattice. 1-D find periodic nonlinear a in propagating fields thermal of properties statistical Optics Thermodynamic Approach of Statistical Nonlinear Zealand, wave theory. kinetic confirms predictions of energy equipartition based on all-optical bump-on-tail instabilities. The observation soliton turbulence via the coupled interaction of two Inst. of Science, Israel,Science, Inst. of A. Kudlinski A. UK, Presider Medium-Range Weather Forecasts, Peter Janssen; European Ctr. for Nonlinear Phenomena FWD •Turbulence andOther 8:00 a.m.–10:00a.m. 1 5 berg System Universal Correlations in a Nonlinear Periodic 1-D FWD3 •8:45a.m. nonlinear optics. recent progress on this kinetic approach of statistical based on the wave turbulence theory. Wearguments thermodynamic shall review by detail in described propertiesof random nonlinear optical can fields be experimentally observe the experimentally algebraicobserve We Univ.,USA. Princeton W.Fleischer; Jason Sun, Bump-on-TailInstabilities, Coupled via Turbulence Soliton of Observation FWD2 •8:30a.m. Univ. de Nice Sophia Antipolis, France. Univ. de Bourgogne, France, 1 , EranSmall, , , B.Kibler Yaron Silberberg 3 Princeton Univ., USA, 4 , P.Aschieri , 1 1 , B.Barviau , , Roberto MorandottiRoberto , Valley 2 We Canada.the study INRS, 1 , Yoav Lahini Invited 5 , G. Millot G. , 2 1 Univ. of Auckland, New , S. Coen S. , Dmitry V. Dylov, Can V.Dylov, Dmitry 4 Univ. de Lille, France, k The coherence 1 1 -2 2 , Yaron Brom- , A. Picozzi A. , 2 , J., Fleischer ; spectrum of spectrum 1 Weizmann 1 3 ; , by of use holograms digital generated on aGPU. direct real-time preferential excitation of fiber modes alities of fiber systems.alities of fiber paving the way to unprecedented complex - function resulting in a momentous increase density,in device fiber meters-long over devices semiconductor of ment of optoelectronic fibers enabled the fabrication Shapira; MIT, USA. Systems , and Devices Fiber Multimaterial UK, Grace Excitation, Fiber for SLM Real-Time FWE3 •8:45a.m. can enhance image resolution. collimator which micro mirror.a reportWe further scanning micro two-dimensional a synthesizer,and displayincluding of opticRGB sources, color fiber a Korea. of Univ.,Republic Display, ning - Scan Micro for Synthesizer Color Optic Fiber FWE2 •8:30a.m. California San Diego, USA,Presider Jose M.Chavez Univ. Boggio; of FWE •NovelFiberDevicesII 8:00 a.m.–9:45a.m. FWE1 •8:00a.m. 2 GSI Group, UK. We present a novel technique for 1 , Steffan A. E. Lewis Hesam Arabi, S. An, K. Oh; YonseiOh; K. An, S. Arabi,Hesam California Recent advances in the develop- In this paper we report a report we paper this In 2 Invited ; 1 Imperial College London, dad J. Edward
Ofer Ofer Wednesday, October 14 77 Two- We report report We Gregory D. Scholes, Scholes, D. Gregory Invited Invited Hillsborough LSWC1 • 8:00 a.m. 8:00 a.m.–10:00 a.m. 8:00 a.m.–10:00 LSWC • Multidimensional I Spectroscopy Washington, of Univ. Khalil; Munira USA, Presider LSWC2 • 8:30 a.m. Coherence in Electronic Energy Transfer: The Regime, Coupling Intermediate Canada. Toronto, of Univ. Collini; Elisabetta a study of the role of coherence dynamics in the intermediate coupling regime of electronic energy transfer. Theoretical developments as well as the results of two-dimensional electronic spectroscopy will be described. Investigating the Major Light Harvesting Complex Harvesting Light Major the Investigating Spectroscopy, Electronic 2-D with II Photosystem of G. Ginsberg, S. N. R.Calhoun, T. Schlau-Cohen, S. G. USA. Berkeley, at California of Univ. Fleming; R. on experiments spectroscopy electronic dimensional II, photosystem of complex harvesting light major the ultrafast monitor light harvester, the most abundant the behind principles design the reveal and dynamics complex. protein this pigment of functionality
- SFG Invited Invited Ian M. Craig, Benjamin J.
LS Gabor A. Somorjai, George J.
Piedmont LSWB1 • 8:00 a.m. LSWB2 • 8:30 a.m. Holinga; Univ. Holinga; of Univ. California at Berkeley, USA. adsorbedthe molecules at investigate to was applied solid-gas (liquid) interfaces and - reaction intermedi metal at surfaces. catalytic reactions was of SFG ates used to characterize polymer films, electrochemical adsorption. biomolecule and interfaces, 8:00 a.m.–10:00 a.m. 8:00 a.m.–10:00 Nonlinear LSWB • Second-Order Optics I Univ., Purdue Simpson; J. Garth USA, Presider The The electronic structure polymer/ of the conjugated metal interfaces that are present in polymer-based this In understood. poorly are devices optoelectronic opti non-linear of results preliminary present we talk, conjugated characterizing at aimed measurements cal polymer/metal interfaces. Schwartz; Univ. Schwartz; of Univ. California at Los Angeles, USA. Nonlinear Optical Studies of Conjugated Polymer Polymer Conjugated Optical of Studies Nonlinear Films and , Interfaces Sum Sum Frequency Generation (SFG) Vibrational Spectroscopy and Its Application in Surface Sci- ence and , Catalysis For Fall Congress presentations on Wednesday, see pages 125-131. pages see Wednesday, on presentations Congress Fall For October 11–15, 2009 • Invited Invited W. E. W. Moerner; Univ., Stanford Samuel Samuel Hess; of Univ. Maine, USA. Sacramento Single-molecule Single-molecule emitters provide nanoscale - Superresolu Imaging, Biophysical Single-Molecule , tion, and Trapping USA. light sources yielding unprecedented new - informa tion about biological systems. Novel methods and molecules, including superresolution imaging in three dimensions and anti-Brownian electrokinetic trapping of single biomolecules in solution, will be reviewed. Fluorescence Nanoscopy: Breaks the FPALM Dif- fraction Limit, small many image methods microscopy Localization coordinates the determine molecules, single of subsets of each molecule by localization, and combine data image fluorescence a create to molecules many from significantly nm) (10-40 resolution with sample the of - Biologi resolution. diffraction-limited the than better presented. methods are such of cal applications LSWA2 • 8:30 a.m. LSWA2 8:00 a.m.–10:00 a.m. 8:00 a.m.–10:00 • Single-Molecule LSWA I Biophysics Tech, Georgia Payne; Christine USA, Presider LSWA1 • 8:00 a.m. LSWA1 In In this FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Invited Atherton Chia-Chu Chen, John F. Whitaker; Univ. Univ. Whitaker; F. John Chen, Chia-Chu Brett Brett R. Nadler, Eric J. Jason Tremblay, H. David David Erickson; Cornell USA. Univ.,
FWG2 • 8:30 a.m. Range Finding Using a Masked Folded Optic , Imager Diego, San at California of Univ. Ford; E. Joseph Karp, USA. images High-resolution of an unfocused laser beam were obtained by masking the aperture of yielded an processing Image imager. optic folded annular calibrated distance measurements correlated to the the beam spots. of separation 8:00 a.m.–10:00 a.m. 8:00 a.m.–10:00 Sensing Devices FWG • Photonic Univ., Carleton Albert; Jacques Presider Canada, FWG3 • 8:45 a.m. Sensing the Microwave Poynting Vector with a Electric/Magnetic Telluride Manganese Cadmium Sensor, Field Poynting microwave the of map A USA. Michigan, of vector along a 50-Ω microstrip was experimentally determined using a single cadmium manganese - tel luride crystal that exhibits both the Pockels and effects. Faraday FWG1 • 8:00 a.m. Optical Manipulation Using Silicon - Nanopho , tonics paper I review our work on the use of silicon - nano photonics for optical of manipulation nanoparticles and biomolecules, focusing on ways in which these space free over improvement an represent techniques manipulation.
FiO Univ. Univ. 1 ; 2 E. F. Chillcce, Chillcce, F. E. Optical fibers
Corning Corning Inc., USA. 2 , Karl W. , Koch Karl W. 1 Invited Arash Mafi Glen Ellen Glen , FWF1 • 8:00 a.m. 8:00 a.m.–9:45 a.m. 8:00 a.m.–9:45 Bandgap Devices FWF • Photonic State Francisco San Zhang; Peng USA, Presider Univ., FWF3 • 8:45 a.m. Birefringence of Photonic Crystal Fibers with a General Lattice FWF2 • 8:30 a.m. in Entrained Dots Quantum PbS of Luminescence , Samples Fiber Microstructured Silica L. C. Barbosa, R. L. Braga, R. E. Ramos-Gonzales, A. C. C. A. Ramos-Gonzales, E. R. Braga, L. R. Barbosa, C. L. A preliminary Brazil. Campinas, of Univ. Bordonalli; luminescence spectral analysis of micro-structured silica fibers whose core regions are surrounded fiber by core Dual presented. is quantum-dots PbS-core 785nm a and sizes dot quantum different with samples used. laser were pump of Wisconsin-Milwaukee, of USA, Wisconsin-Milwaukee, We We report on the influence of lattice and shape fibers crystal on photonic the of properties birefringence vanishing or large very as such properties novel show cores. and lattices in nonsymmetric birefringence with holes in them, either in their cladding or forming forming or cladding their in either them, in holes with can a becore, describeused theas fiber sensors. We physics and related technologies enabling new and configurations. sensor improved Why Why Use Photonic Crystal Fibers for Sensing? Jonathan Knight; of Univ. Bath, UK. Wednesday, October 14 78 to monitor neuronal activation. discriminate between different melanins to in tissue used and are effects These absorption. nonlinear or modulationcross-phaseand self- signaturesas such ser pulse shaping permit detection of novel molecular FWA3 •9:00a.m. Ultrafast Lasers—Continued FWA •BiomedicalApplicationsof full cortical thickness. cortical full the of imaging allowing and cortex of surface the to perpendicular to parallel from field-of-view the ing mouse enable of cortex Univ., the into Microprisms inserted USA. Mouse , Cortex Microprisms for FWA4 •9:30a.m. , Pulses Laser Femtosecond Shaped with Imaging Tissue Thank youforattending know yourthoughtson post-conference survey
FiO/LS/Fall Congress. Warren S. Warren; Duke Univ., USA. via emailandletus Look foryour the program. in vivo in Thomas Chia, Michael J. Levene; Yale in vivo in Empire multiphoton microscopy, rotat- Multiphoton Microscopy of Invited Rapid - la Quantum DotsQuantum, Slow and Fast Light Propagation in Semiconductor FWB4 •9:00a.m. Arka Majumdar Arka explained directly intime-domain paper. inthis be will phenomena The experimentally. observed tigated and both slow and fast light propagation were pulse in semiconductor quantum dots has been inves- laser a of velocity group PolytechnicThe Inst.,USA. Strongly Coupled Quantum Dot Quantum Coupled Strongly a with Modulator Optical Driven Electrically FWB5 •9:15a.m. achievable withdevice. this are~1fJ/bitanddemonstrated. 10GHzat Operation is laser probe coupled coherently a of (150MHz) modulation Electro-optic controlled. electrically dot strongly coupled to a photonic-crystal cavity was at Santa Barbara, USA. The frequency of a quantum- Tabibi Vučković Metamaterials—Continued the AgeofNanophotonicsand Processing andTransportin FWB •OpticalInformation theoretical models. earlier from prediction beyond observed, been has metal film by confocal microscope. A large phase thin shift on holes plasmonic individual from emerging light squeezed the of delay phase the Wemeasured Urbana-Champaign,USA. at Illinois Univ.of Fang; , Film Metal Thin on Hole Sub-WavelengthPlasmonic in Squeezed Light of Measurement Microscopy Confocal FWB6 •9:30a.m. 1 , William Yu William , 1 ; 1 StanfordUniv., USA, 1 , Hyochul Kim Hyochul , QiguangYang 2 ; Hyungjin Ma, Jun Xu, Nicholas Xu, Jun Ma, Hyungjin Crystal 1 Hampton Univ., USA, FiO/LS/AO/AIOM/COSI/LM/SRS 2009 2 , Pierre Petroff 1 , JaeTae, Seo 2 Univ.Californiaof , nri Faraon Andrei 2 Worcester 1 , Bagher , 2 , Jelena 1 ,
DomenicoCegliade Packard Res. Lab, USA, 3 mer Perot cavity composed of two gold films. Fabry- a into index refractive negative of structure “fishnet” of layer single a inserting by numerically demonstrated is size sub-wavelength deep of nator ogy and Zhejiang Univ., China. An optical cavity reso- greater than skindepth. the decay, often leading to EOT even for thicknesses much that these structures can significantly impede the field numerically.investigatedWe was find structures lic transmission through multi-layered systems of - metal Optical USA. Charlotte, at Carolina North Univ.of , Films Thin Metallic Corrugated of Systems Multi-Layered through (EOT)Transmission Optical Extraordinary FWC4 •9:00a.m. ovski SH mostly signal generated by χ between nonlinear response produced in metals and a semiconductor substrates to highlight the on differences carved slits single in responses nonlinear and linear between correlation the Weinvestigate USA. Res. Ctr. AMSRD-AMR-WS-ST, US Army RDECOM, and Applied Physics, Royal Inst. of Technology, Sweden, with with Fishnet, Resonators Cavity Optical Sized Sub-Wavelengh FWC5 •9:15a.m. Maria AntoniettaVincentiMaria , Range UV the in Semiconductors for Response Nonlinear and Transmission Extraordinary FWC6 •9:30a.m. Continued and StructuredSurface— Transmission FWC •Extraordinary Joint Res. Ctr. of Photonics of the Royal Inst. of Technol- 2 ; 1 , Shih-Yuan Wang 1 Politecnico di Bari, Italy,Bari, Politecnicodi Jingjing Li 2 , Michael, Scalora FiO Gold Choon How Gan, Greg Gbur; Greg Gan, How Choon 2 1 KTH Dept of Microelectronics , Stanley Williams 1 , Lars Thylen 1,2 , Antonella D’OrazioAntonella , 2 2 Charles M. Bowden M. Charles contribution. • 1,2,3 2 , Mark, J.Bloe - , Alex Bratk- 1 ; October 11–15,2009 1 Hewlett- 1 , For Fall Congress presentations onWednesday, seepages125-131. other and practical fundamental applications. have may and fibers optical in generation tinuum supercon- in role paramount plays phenomenon This light. blue-shifts and traps solitons optical by howdescribe an intriguing gravity-like force created continuum Super Fiber and Light on Effects Gravity-Like Weill Amplified Spontaneous Noise in Laser , Cavities by Induced Interaction Pulse Light Casimir-Like FWD5 •9:30a.m. experimental evidence for evidence experimental unique this effect. time-light domain Casimir-like mechanism. We show lasers induced by amplified spontaneous noise. It is a mechanism for light pulse interaction in mode-locked nology, Israel, FWD4 •9:00a.m. Bekker Nonlinear Phenomena—Continued FWD •Turbulence andOther 1 , Omri Gat 1 , Baruch Fischer , Dmitry Skryabin;Dmitry Univ. Bath,UK. of 2 Hebrew Univ., Israel. We present a new 2 , Vladimir Smulakovsky Valley 1 ; 1 Technion-Israel Inst. of Tech- Invited 1 , Alexander Rafi Rafi I’ll I’ll - Byoung-Su Byoung-Su Lee offers a new method to functionalise fiber tapers. offers fiber to functionalise method anew this particles, these of spectroscopy and detection lected microparticles on optical tapers.fiber Beyond a segmented linear Paul-trap to deposit single prese- HumboldtBenson; Univ. Germany.Berlin,of We use Detection and Spectroscopy forTapers Fiber Optical on Nanoparticles Single Preselected of Soft-Landing FWE4 •9:00a.m. number respectively. parity different with resonators the to applied is It medium. gain doping in microsphere outermost the of parameters the adjusting by investigated is subluminal and superluminal between transition The Technology,China.of Inst. Yuan;Harbin Ping System Fiber Optical Microspheres Multiple for luminal Sub- and Superluminal between Transition The FWE6 •9:30a.m. 2 additional infrared cutoff filter included. between two silver films, were demonstrated with no in sandwiched film thin oxide an of consists which etalon, Fabry-Perot simple a on based filters color Yeo-TaekYoon Etalon, Fabry-Perot a Incorporating Filter Color FWE5 •9:15a.m. Continued FWE •NovelFiberDevicesII— Three Korea. of Technologies,SiliconFileRepublic , Yundong Zhang, Jing Zhang, Xuenan Zhang, , Alexander Kuhlicke, Markus Gregor, Oliver 2 ; 1 1 , Hong-Shik Lee Hong-Shik , Kwangwoon Univ., Republic of Korea, California 1 , Sang-Shin Lee Sang-Shin , 1 , Wednesday, October 14 79 Andrew T.
S. T. Cundiff, A. Invited Invited Optical two-dimensional Fourier Hillsborough LSWC • Multidimensional LSWC • Multidimensional I—Continued Spectroscopy LSWC3 • 9:00 a.m. LSWC3 • 9:00 LSWC4 • 9:30 a.m. Exciton Exciton Relaxation and Energy DynamTransfer - ics in Size Selected , Polythiophenes Optical Two-Dimensional Fourier Transform Spectroscopy of , Semiconductors D. Bristow, D. Karaiskaj, X. Dai; JILA, NIST, Univ. of USA. Colorado, transform spectroscopy is used to study excitonic resonances in semiconductor nanostructures. The - contribu many-body of dominance the show spectra to observed due are coherences Two-quantum tions. states. many-body and both biexcitons Healy, Nathan P. Wells, Bryan W. Boudouris, Marc A. Marc Boudouris, W. Bryan Wells, P. Nathan Healy, David A. Hillmyer, of Blank; USA. Univ. Minnesota, - pho two-color and upconversion fluorescence Using initial the investigated have we spectroscopy echo ton dynamics energy transfer subsequent and relaxation in a series of size-selected polythiophenes with and termination. fullerene without ; 1,2 , Cruz 1 Univ. of Univ. 1 ; , Emilio J. 1 1,2 , Luis Roso Rocio Borrego Borrego Rocio 3 Lab de Óptica, Univ. Univ. Óptica, de Lab 3 Ctr. de Láseres Pulsados Pulsados Láseres de Ctr. Lawrence Berkeley Natl. Natl. Berkeley Lawrence 2 2 Invited , Benjamin Alonso , Benjamin 1 , Pablo Artal 3 LS Richard Richard J. Saykally Piedmont By By exploiting the strong charge-transfer- , Javier R. de Vázquez Aldana , Carolina Romero , Carolina 2 , Juan M. Bueno 1 3 Univ. de Salamanca, Spain, Spain, Salamanca, de Univ. LSWB • Second-Order Nonlinear Nonlinear LSWB • Second-Order Optics I—Continued Varillas LSWB4 • 9:15 a.m. Analysis of Aberrations Effect in Nonlinear - Pro PulsesLaser, Femtosecond for cesses LSWB5 • 9:30 a.m. Gualda California at Berkeley, USA, Berkeley, at California Méndez 1 de de Murcia, Spain. A method for the analysis and control of femtosecond pulse wavefronts generated processes mixing three-wave by crystals non-linear in efficiency the improve to possibility The presented. is discussed. is these processes of Ultracortos Ultraintensos, Spain, Spain, Ultraintensos, Ultracortos LSWB3 • 9:00 a.m. LSWB3 • 9:00 OpticalAllModula- Bandwidth High Atto-Joules, , Vapor Alkali in Embedded Nano-Fiber a with tion Kenneth Salit, Mary Salit, - Krishna Subramanian Prem Wang, Ye murthy, Selim Kumar, M. Shahriar; Northwestern USA. Univ., We report an all-optical tapered a using GHz, 2 at photons 75 with modulator nanofiber embedded in - The an switch alkali vapor. ing energy is 19 atto-Joules, a record low value for this speed. at modulation Lab, Lab, USA. to-solvent (CTTS) resonances characteristic of all anions in aqueous electrolytes, their interfacial spectroscopy measured in using properties SHG are the deep ultraviolet. Resonant Resonant UV SHG Studies of Ion Adsorption at Aqueous , Interfaces For Fall Congress presentations on Wednesday, see pages 125-131. pages see Wednesday, on presentations Congress Fall For October 11–15, 2009 • Invited Randall H. Goldsmith, Yan Jiang, Randall H. Jiang, Goldsmith, Yan Sacramento LSWA • Single-Molecule • Single-Molecule LSWA I—Continued Biophysics LSWA5 • 9:30 a.m. LSWA5 LSWA4 • 9:15 a.m. LSWA4 Single-Molecule Action: in Photophysics Watching Photosynthetic Trapped a of Studies Solution-Phase , Antenna Protein E. W. Moerner; Stanford USA. Univ., Simultaneous fluorescence intensity and lifetime fluctuations are observed in single molecules of Allophycocyanin in - photophys different of observation allowing solution, - hetero conformational which suggest ical processes Brownian cancels that trap electrokinetic An geneity. measurement. solution-phase enables motion Structured-Illumination Microscopy of Live CellsLive, of Microscopy Structured-Illumination Francisco, San at California of Univ. Gustafsson; Mats available. not USA. Abstract LSWA3 Withdrawn Paper FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Invited Atherton Surface Surface plasmon resonance based - Technol of Inst. Indian Gupta; D. Banshi FWG • Photonic Sensing FWG • Photonic Devices—Continued FWG5 • 9:30 a.m. Uniformity of Concentration Factor and BFL in , Applications Detectors Image for Array Microlens Fathi, Mohammad Randone, Enrico Martini, Giuseppe Silvano Donati; Pavia, Univ. We Italy. report a 35x gain for a 32x32, 50-micron diameter polymer cast microlens array used to recover fill-factor loss in a Concentration spread is array. < 6% SPAD and BFL <0.5µm. is spread FWG4 • 9:00 a.m. FWG4 • 9:00 Fiber Fiber Optic Sensors Based on Surface Plasmon , Resonance ogy Delhi, India. fiber optic sensors with different probe designs are presented. The modeling of each probe is carried probe each of performance The optics. ray using out sensitivity. of in terms evaluated is ; FiO 1,2 Carel - Lind , , Philip , Philip 3 1 Murtaza Murtaza Univ. Univ. of St. We We present 3 Univ. of Sydney, of Sydney, Univ. 1 ; , Willem L. Vos 1 3 FOM Inst. AMOLF, , Tom P. White P. Tom , 2 2 Allard P. Mosk P. Allard Glen Ellen Glen Max-Planck-Inst. für Quantenoptik, 3 , Ross , C. Ross McPhedran 2 , Kokou B. Dossou B. Kokou , , Pepijn H. W. Pinkse 1 CUDOS, School of Mathematical Sciences, Sciences, Mathematical of CUDOS,School 1,2 2 We present the present first experiments We on - reso Univ. Twente, Netherlands, Univ. Askari, Askari, Ali Adibi; Georgia Tech, USA. bends efficiency high of demonstration experimental for low group velocity modes in photonic crystal waveguides. We show that careful modification of bend region can help improve bend bandwidth by 1.55µm wavelength. 15nm for FWF6 • 9:30 a.m. Very High Efficiency Bends for Low - Group Ve locities in Photonic Crystal, Waveguides Netherlands, Netherlands, Univ. of Univ. Sydney, Australia, Technology, Efficient coupling between fast and slow slow and fast between coupling Efficient UK. Andrews, evanescent strong if possible is modes waveguide PC modes are needed to match the fields across the interface. This occurs when the propagating modes modal fields. different substantially have Germany. crystals. The photonic in Cesiumvapor, atoms, nant photonic by modified strongly are transitions atomic with band structures of opal. interpreted Results are model. transfer-matrix improved an 1 FWF4 • 9:00 a.m. of Cesium Resonant Interactions Atoms Photonic and OpalCrystals Photonic , FWF • Photonic Bandgap FWF • Photonic Devices—Continued say C. say Botten FWF5 • 9:15 a.m. Photonic Light Slow into Coupling Efficient Direct, , Modes Evanescent of Role Waveguide: Crystal Sterke de M. Australia, Australia, J. J. Harding Wednesday, October 14 80 other organs. millimeters in mouse intestine, heart, lung, brain and mouse organs. We achieved imaging depths of clearedseveral optically and fixed intact, entire of imaging harmonic second and microscopy fluorescence multiphoton present We YaleUniv.,USA. Levene; Organs, Mouse Intact Entire of Histology Multiphoton FWA5 •9:45a.m. Ultrafast Lasers—Continued FWA •BiomedicalApplicationsof ______oi Pra Jsp P Zne, ihe J. Michael Zinter, P. Joseph Parra, Sonia Empire 9:00 a.m.–12:00p.m. Vamsi K. Komarala VamsiK. dot-mirror distance. of function a as dots quantum single of properties correlation and statistical modified the studyWe can be modified and controlled by an optical mirror. quantum dots CdSe/ZnS single statisticsofblinking 1 Quantum Dots in a Half Cavity, Half a in Dots Quantum Colloidal Single of Statistics Blinking Controlled FWB7 •9:45a.m. Metamaterials—Continued the AgeofNanophotonicsand Processing andTransportin FWB •OpticalInformation Univ.USA, Arkansas,of Crystal 1 , YanpengZhang , Export Regulation Fundamentals fortheOpticsandPhotonicsIndustry, Sainte Claire Room, Sainte Claire Hotel 2 NankaiUniv.,The China. FiO/LS/AO/AIOM/COSI/LM/SRS 2009 10:00 a.m.–4:00p.m. 10:00 a.m.–10:30a.m. Ningning Xu Ningning 1 , Min Xiao Min , 1,2 1 ; , rigorous numerical approaches. studied and modeled, using several approximate and with/without supporting corrugations is theoretically apertures the including structures, sub-wavelength plasmonic of classes various with wavetromagnetic - elec an of interaction The Republic. Czech Prague, TechnicalUniv.in Czech Engineering, Physical and Sciences Nuclear of Faculty Richter; Ivan Fiala, Jan Sub-WavelengthStructures, Plasmonic through Theory and Simulations of Enhanced Transmission FWC7 •9:45a.m. Continued and StructuredSurface— Transmission FWC •Extraordinary Exhibit HallOpen,Imperial Ballroom, Fairmont Hotel Coffee Break,Imperial Ballroom, Fairmont Hotel NOTES FiO Gold • October 11–15,2009 For Fall Congress presentations onWednesday, seepages125-131. dicted bydicted anonlinear Gaussian-Schell model. pre- scaling dynamical the confirm widths beam of and self-defocusing nonlinear media. Measurements partially-coherent spatial beam in both self-focusing experimentally and theoretically, the propagation of a Jason W. Fleischer; Princeton Univ., USA. We consider, Beams Spatial Coherent Partially- of Defocusing and Focusing Nonlinear FWD6 •9:45a.m. Nonlinear Phenomena—Continued FWD •Turbulence andOther Valley , Can Sun, Dmitry V. Dylov, California Wednesday, October 14 81 Hillsborough LSWC • Multidimensional LSWC • Multidimensional I—Continued Spectroscopy LS Piedmont LSWB • Second-Order Nonlinear Nonlinear LSWB • Second-Order Optics I—Continued For Fall Congress presentations on Wednesday, see pages 125-131. pages see Wednesday, on presentations Congress Fall For October 11–15, 2009 • NOTES Sacramento Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Coffee Break, Imperial Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Exhibit Hall Open, Imperial LSWA • Single-Molecule • Single-Molecule LSWA I—Continued Biophysics , 2 , M. R. 1 , S.C. Jain S.C. , 2 10:00 a.m.–10:30 a.m. 10:00 a.m.–4:00 p.m. FiO/LS/AO/AIOM/COSI/LM/SRS 2009 , K. Thyagarajan , Nahar Singh Nahar , 2 1,2 Sainte Claire Room, Sainte Claire Hotel Claire Sainte Room, Claire Sainte and Photonics Industry, for the Optics Fundamentals Export Regulation Atherton Indian Inst. of Technology Delhi, 1 ; 2 , Vandana Mishra Vandana , Umesh Umesh K. Tiwari Central Central Scientific Instruments Organization, , 1,2 2 Experimental measurements on a novel dual Shenoy FWG • Photonic Sensing FWG • Photonic Devices—Continued FWG6 • 9:45 a.m. DualInsensitive Chirped LPG Temperature Bend Sensor India. very exhibits which presented is design LPG chirped sensitivity. bend high and sensitivity temperature low entirely are design proposed the of properties Sensing LPG. normal from different Pawan Kapur India, India, FiO 9:00 a.m.–12:00 p.m. Glen Ellen Glen ______Wednesday, October 14 82 to periodic trains ofto periodic fast pulses. applicable is and fields stationary for Wolf shift the generalizes result This predicted. are fields random cyclostationary, of spectra generalized the in shifts propagation-inducedCorrelation-dependent, USA. Scott Univ. Carney; of Illinois at Urbana-Champaign, Fields Cyclostationary for Shift Wolf Generalized The FWH3 •11:00a.m. 1 Fields, netic - Electromag Focused of Description the for Bases FWH1 •10:30a.m. Central Florida, USA,Presider of Optics and Photonics, Univ. of Y.Boris Zeldovich; CREOL, College Fundamental OpticsI FWH •Coherenceand 10:30 a.m.–12:15p.m. partially coherentpartially field. a and polarization azimuthal and linear, radial with cases are presented, including monochromatic fields test simple Several described. are fields aperture numerical high of modeling efficient the for bases from scattering experiments. media random stationary of potentials scattering of functions correlation the determine to generalized is experiments diffraction neutron and X-ray from media crystalline of structure the determining for method classic The Rochester,USA. Wolf;Univ.of fromScattering , Experiments Media Stochastic of Determination Structure FWH2 •10:45a.m. Beloit College, USA, , Robert W. Schoonover, Brynmor J. Davis, P. Davis, J. Brynmor Schoonover,W. Robert Nicole J. Moore J. Nicole 2 Empire Univ. of Rochester, USA. Discrete 1 , Miguel A. Alonso A. Miguel , MayukhLahiri, Emil 2 ; AFRL, USA, AFRL, as optical delay lines. operate can elements these that shown is Itstudied. are elements these of properties phase spectral The optimization. swarm particle with designed are filters bandpass resonance Leaky-mode USA. Wang, Robert Magnusson; Univ. of Texas at Arlington, Resonance Structures, Optical Delay Line Elements Based on Leaky-Mode FWI3 •11:00a.m. Stephen Carr Stephen Charles Woods Self-Assembled Self-Assembled Quantum Dot, a in Sidebands Phonon Resolved of Generation FWI2 •10:45a.m. 1 Medical Univ., Austria, Presider Monika Ritsch-Marte; Innsbruck Sciences FWI •OpticsinInformation 10:30 a.m.–12:00p.m. the fuzzy-logic maximum fuzzy-logic the operation on data. video systems. Our design was modeled in Simulink® using of a new design for smart optical receivers in LADAR propose using the smart antenna principle as the basis Enhancement View of Field for Receiver Optical Compound FWI1 •10:30a.m. to an QD. embedded nanomechanicalresonatorcouplinga of via cooling This constitutes an important step towards sideband wave inducing phonon sidebands acoustic of the surface fluorescence. a with modulated are (QD) dots NIST, USA, 2 1 Univ. of Maryland, USA. InAs quantum 2 , Solomon S. Glenn S. Solomon , We We USA. Corp., Scientific State Solid 1 , , John Kierstead aae Haji-Saeed Bahareh Crystal Mehrdad Shokooh-Saremi, Xin FiO/LS/AO/AIOM/COSI/LM/SRS 2009 2 ; Michael B. Metcalfe 1 Sensors Directorate, 1,2 , John R. Lawall R. John , 1 , Jed Khoury Jed , 1,2 1 1 ; , , FWJ3 •11:00a.m. Route to Better PhotonsBetterRouteto , A Fiber: Birefringent in Generation Pair Photon waveguides using continuous pumping. circular 2-D and planar 1-D in down-conversion parametric spontaneous via biphotonsgenerated of entanglement polarization and spectral, modal, of applications and properties the of study theoretical Physics, Boston Univ., USA. We offer a comprehensive Teich , guides WavePPLN - Engineered Photons Domain Type-II from Entangled Polarization of Generation FWJ2 •10:45a.m. Dan Ostrowsky Dan LuganiJasleen Boston Univ.,USA, Boston operation of waveguide quantum gates. logic loring these characteristics is crucial for high-fidelity with desiredand spectral spatial characteristics. Tai- photons produce to us allow fibers, optical as such UK. Oxford, Council Canada, Canada, Canada, Council Presider Autónoma de México, Mexico, Alfred B. Univ. U’Ren; Nacional Waveguides II FWJ •QuantumOpticsin 10:30 a.m.–12:15p.m. 1 3 ferent processes. SPDC simultaneously satisfying the conditions for two dif- by pairs photon entangled polarization degenerate non generating for Niobate Lithium in engineering tipolis, France. We propose scheme anew of domain Photonics, Univ. of Central Florida, USA, Florida, Central Univ.of Photonics, Technology Delhi, India,Technology Delhi, Mohammed F. Saleh Down-Conversion, ParametricGuided-Wave in Entanglement Polarization and Spectral, Modal, FWJ1 •10:30a.m. hen LPMC, CNRS UMR 6622, Univ.AnSophiaNice- 6622, of UMR CNRS LPMC, Inst. for Natl. Measurement Standards, Natl. Res. Res. Natl. Standards, Measurement Natl. for Inst. 2 , Pierre Mahou 1,3 ; 1 Dept. of Electrical and Computer Engineering, rsn Thyagarajan Krishna We show that birefringent waveguides,birefringent Wethat show 1 3 , Sankalpa Ghosh Sankalpa , , Sebastian TanzilliSebastian , 2 , Brian J. Smith J. Brian , 1 2 , Bahaa E. A. Saleh CREOL, College of Optics and Optics of College CREOL, FiO Gold 2 Univ. of Maryland, USA, USA, Maryland, of Univ. Jeff S. LundeenJeffS. Invited 2 Clarendon Lab, Univ.of Lab,Clarendon 1 , Kanupriya Sinha Kanupriya , 2 1 , Ian A. Walmsley , Olivier Alibart Olivier , 3 ; • 1 Indian Inst. of Inst.Indian 1,2 , Malvin C. 1 - Co Offir , October 11–15,2009 3 Dept. of Dept. 2 3 2 ; , , For Fall Congress presentations onWednesday, seepages125-131. will be discussed. be will monitoring performance speed high Applicationto based on highly nonlinear chalcogenide waveguides. circuits integrated photonic developing in progress Australia. Sydney, Barrier, Second per Terabitthe Breaking Chip: a on Optics Nonlinear tunable range. nm 95 - wide a over obtained are dB 30 exceeding SNR with pulses picosecond ps 2.2 GHz High-quality 40 tunable architecture.cavity-less a using source pulse optical wavelength a demonstrate We USA. Diego,Univ.Radic;SanStojan California at of Alic, Nikola Myslivets, Evgeny Bres, Camille-Sophie Pulse , Source Picosecond GHz 40 Widely-TunableCavity-Less FWK2 •11:00a.m. FWK1 •10:30a.m. USA, Presider Alexander Gaeta; Cornell Univ., Processing III FWK •All-OpticalSignal 10:30 a.m.–12:00p.m. Bill Ping Piu Kuo, Andreas O. J. Wiberg,
This paper reviews our recent our reviews paper This
Valley Benjamin J. Eggleton; Univ.of Eggleton; J. Benjamin Invited Parekh Delfyett ida, USA, ida, College of Optics and Photonics, Univ. of Central Flor atBerkeley, USA, Engineering and Computer Sciences, Univ. of California Sarper Sarper Ozharar , Laser Locked Mode- Stabilized Frequency Jitter Ultra-Low FWL1 •10:30a.m. experimental results.experimental the with agreement excellent shows model this on based Calculation lasers. surface-emitting cavity the cavity mode behavior of injection-locked vertical- analyze to equationsrate injection-locked on based Univ., China. A novel ellipse graphic tool is established Electronics Engineering and Computer Science, Peking of School Networks, and CommunicationSystems Akbulut Locked Locked VCSELs, Injection- Optically for Model Ellipse Novel A FWL3 •11:00a.m. 1 San Diego, USA,Presider Nikola Alic; Univ. of California at Devices FWL •OpticalCommunication 10:30 a.m.–12:00p.m. Univ. of Central Florida, USA, Florida, Central Univ.of source is suitable for time-stretched photonic ADC. frequency.fundamental cavitylaser The the to laser mode-locked 2.56GHz, SCOWA-based mode-locked demultiplexingharmonically time bya developed is sub-100MHz low-noise, Laser Mode-Locked Demultiplexed Temporally a on Train Noise,Pulse Sub-100MHzBased Ultra-Low FWL2 •10:45a.m. optical <1kHz. linewidth and fs 3 of 100MHz) - jitter(1Hz timing a with lon, intracavity finesse - 1000 eta with laser mode-locked stabilized, semiconductor based, 10.287 GHz actively USA, CREOL and FPCE, College of Optics and Photonics,and Optics of College FPCE, and CREOL , 3 NIST, frequency noise,We low USA. a report 1 Dimitrios Mandridis Dimitrios , Connie J. Chang-Hasnain 1 1 , Jason J. Plant , Nazanin Hoghooghi 2 MIT LincolnMIT semiconductorLab,A USA. 2 , Franklyn Quinlan Franklyn , Ibrahim T. Ozdur T. Ibrahim Peng Peng Guo 2 California StateKey Lab of Advanced Optical 2 , Paul W. Juodawlkis Paul , repetition rate laser source laser rate repetition 1,2 1 , Ibrahim Ozdur , Wei Jian Yang 1 , Dimitrios , Mandridis Dimitrios 2 Northwestern Univ.,Northwestern 1 ; 3 1 , Peter J. Delfyett Dept. Dept. of Electrical 1 , Mehmetcan , 2 ; 1 1 1 , Devang CREOL, , Peter J. 1 1 - ; , Wednesday, October 14 83 - - Heidi
Adap , Invited and viewing of Xin Wei, Larry N. David David Merino, Austin in vivo Cupertino JOINT FiO/AO JOINT arbitrary stimuli nearly free of optical blur. blur. optical of free nearly stimuli arbitrary Combining these abilities has created new neural and retinal the study to opportunities vision. on limits 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 in Adaptive JWB • Advances of the Living Optics Imaging I Retina Indiana Burns; A. Stephen USA, Presider Univ., Adaptive Adaptive Optics Psychophysics Hofer; of Univ. Houston, USA. tive optics allows imaging of individual photoreceptors JWB1 • 10:30 a.m. Off-Axis Estimation of Ocular Aber rations via Scanning Shack-Hartmann , Wavefront-Sensor Univ., Indiana Optometry, of School Thibos; developed a Scanning Hartmann USA. We Shack wavefront sensor by coupling the scan- a with aberrometer Hartmann Shack off- measures instrument This system. ning accurately eye human the of aberration axis efficient manner. in an precisely and JWB2 • 10:45 a.m. Optimal Correction of Subject - Prescrip for Scanning System an Adaptive on tion Retinal , Imaging Roorda; School of Optometry, of Univ. California at USA. Berkeley, The effect on an on prescription subject’s of quality image dif- considering Models assessed. is AOSLO in literature available configurations ferent when consider to Factors studied. been have real on these configurations implementing addressed. are systems JWB3 • 11:00 a.m.
, , - 1 1 The water The water Invited Invited Damien Damien Laage
, Fabio Sterpone , 1 École Normale Supérieure, Supérieure, Normale École 1 ; 1,2 Hillsborough Univ. of Colorado, USA. Colorado, of Univ. 2 LSWF2 • 11:00 a.m. Guillaume Stirnemann James T. Hynes 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 LSWF • Multidimensional II Spectroscopy of Univ. Khalil; Munira USA, Presider Washington, LSWF1 • 10:30 a.m. France, France, Watching Ultrafast Molecular Dynamics: Molecular Ultrafast Watching Spectroscopy , Exchange Chemical IR 2-D Michael D. Fayer; Stanford USA. Univ., Ultrafast 2-D IR vibrational echo chemi cal exchange spectroscopy is described. The measurements enable observation of thermal- equilib under moleculeprocesses molecular to Applications conditions. rium isomerization, hydrogen bond dynamics, and proteins structural substate switching presented. are Water and Hydrogen-Bond Dynamics in Aqueous Solutions - investigat is dynamics hydrogen-bond and numerical on Based solutions. aqueous in ed an offer we models, analytic and simulations for the interpretation recent time-resolved experiments. spectroscopy vibrational
, 3 David
Quantum 2 We We describe Invited Invited , Xiang Zhang , Xiang 1 John T. Fourkas; Fourkas; T. John For Fall Congress presentations on Wednesday, see pages 125-131. pages see Wednesday, on presentations Congress Fall For , Physics Physics Dept., of Univ. 1 LS ; 1 , Feng Wang , Feng October 11–15, 2009 2 Piedmont • , Wei Wu , Wei 1 Dept. Dept. of Mechanical Engineering, of Univ. Univ. of Univ. Maryland at College Park, USA. Vibrational sum-frequency generation probing for technique powerful a is (VSFG) interfaces. at molecules of organization the We will discuss how different processes, transfer, energy and reorientation including can lead to new interpretations of VSFG spectra. Science Res., Hewlett-Packard Labs, USA, Yuen-Ron Yuen-Ron Shen LSWE1 • 10:30 a.m. California California at Berkeley, USA. spectroscopic studies of ultrafast photo- modulation of the negative refraction of a fishnet metamaterial and resonant wave mixing processes in the metamaterials of structures. Cheveron and fishnet 3 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 LSWE • Second-Order II Nonlinear Optics of Univ. M. Kelley; Anne USA, Merced, at California Presider LSWE2 • 11:00 a.m. California California at Berkeley, USA, , Metamaterials in Optics Nonlinear Cho New Perspectives in Vibrational Sum- Frequency Spectroscopy , , 1 2 , W. , W. Haw 2 Kent
2 , Hsiao-lu D. Invited 1 - mac Biological , Marissa K. Lee 1 , Reichel Samuel 1 , Robert J. Twieg 2 Stanford Univ., Stanford USA, Univ., Samuel Samuel J. Lord 1 , Na Liu ; 2 1 Sacramento , Nicholas R. Conley 1 LSWD2 • 11:00 a.m. Fluorophores Push-Pull Photoactivatable for Single-Molecule Imaging in and out of Cells, Yang; Princeton Univ., USA. Univ., Princeton Yang; all in move can organelles and romolecules extremely it making cell, a inside directions processes biochemical follow to challenging new a discuss We resolution. molecular with technique that can potentially overcome this difficulty. State Univ., State USA. Univ., We have designed a se- ries of photoactivatable push-pull organic fluorophores, single molecules of which - Photoactivat cells. living in imaged be can superresolution needed for are probes able control active require that schemes imaging single-molecule emission. of Michael Michael A. Thompson Ryan Weber E. Moerner Lee 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 LSWD • Single-Molecule II Biophysics of Univ. Yildiz; Ahmet USA, Berkeley, at California Presider Real-Time Real-Time 3-D Single-Particle Tracking DynamicsCellular, for Spectroscopy LSWD1 • 10:30 a.m. , , - 2 1 Ya FiO/LS/AO/AIOM/COSI/LM/SRS 2009 , - com CMOS Invited , Yingyan Huang Yingyan , , Chongyang , Liu Chongyang 1 1 Northwestern Univ., Mahmoud Mahmoud S. Rasras; 3 , Data Storage Inst., Agency Agency Inst., Storage Data 1 ; 3 Atherton , Qian Wang 1 , Yongqiang Wei Yongqiang , 1 OptoNet OptoNet Inc., USA, dong dong Wang FWN2 • 11:00 a.m. Integration Electronic-Nanophotonic for Science, Technology and Res., Singapore, Singapore, Res., and Technology Science, for Ng Doris Ho Seng-Tiong USA. Nanophotonic integration of III-V on silicon based on top-down coupling is - am for up coupled be can Light presented. for down coupled or plification/absorption bonding wafer Interlayer processing. passive described. is this integration for 2 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 Photonics II FWN • Silicon Boston Negro; Dal Luca USA, Presider Univ., Photonic Photonic Signal Processing in CMOS- Compatible Silicon USA. Lucent, Alcatel Labs, Bell patible photonics creates new information through solutions transport and processing integration. electronic/photonic monolithic Optical filters provide significant insight will We technology. this of viability the into in this area. developments recent present FWN1 • 10:30 a.m. , FiO 1,2 Yan Jiang Yan - Fryd Judith , 4 Invited Dept. of Chemistry Chemistry of Dept. 3 Dept. of Chemistry, Dept. of Chemistry, 1 ; - Phys Applied of Dept. 1 2 , Nick Douglas Nick , 1,3 Glen Ellen Glen Kenneth Kenneth B. Crozier; Harvard Univ., Microfabricated optical Microfabricated tweezers are , W. E. Moerner , W. 4 Dept. of Biological Sciences, Stanford Univ., Univ., Stanford Sciences, Biological of Dept. FWM2 • 11:00 a.m. - Bind ATP Single-Molecule Determining ing Stoichiometry in a Multi-Subunit Enzyme with a Hardware-Based Anti- , Trap Electrokinetic Brownian Adam Cohen Adam USA. We developed a high-speed Anti- Brownian Electrokinetic trap capable of trapping sub-10nm fluorescent objects in solution. Single chaperonin enzymes loaded with Cy3-ATP are trapped, and display stepwise photobleaching intensity traces corresponding to the ATP binding stoichiometry. man 4 FWM1 • 10:30 a.m. 10:30 a.m.–11:45 a.m. 10:30 a.m.–11:45 Trapping and FWM • Optical I Micromanipulation NIST, López-Mariscal; Carlos USA, Presider ics, Stanford Univ., USA, Univ., Stanford ics, and Chemical Biology, Harvard Univ., USA, USA, Univ., Harvard Biology, Chemical and Stanford Univ., USA, Univ., Stanford Optical Trapping and Manipulation Using Using Manipulation and Trapping Optical Microfabricated Optical BasedTweezers on Diffractive Optics and Surface - Plas , mons USA. to shown are zone plates reviewed. Fresnel traditional to performance comparable offer efficiencydiffraction when tweezers, optical is the demonstrate taken into account. We surface using nanoparticles of manipulation polaritons. plasmon Wednesday, October 14 84 topological charge is identified. conservation rule with a discrete rotational symmetry of finite order.system a A of action the to due singularities phase of We present a study of the dynamics and decay pattern 2 3 Singularities Phase for Rule Selection Charge Topological A FWH4 •11:15a.m. Fundamental OpticsI—Continued FWH •Coherenceand Valencia, Spain, Univ.dePolitecnica Aplicada, y PuraMatematica Zacarés the locationthe of pinholes the is arbitrary. ture of polarization singularities is found even when are investigated. For netic fields diffracted by an D. Visser characterizes temporal the profile of pulses. fully and dimensions spatial two from information in Kerr materials. SRSI provides phase and amplitude investigate nonlinear propagation of ultrashort pulses Spatially Resolved Spectral Interferometery (SRSI) to Jeff A. Squier; Colorado School of Mines, USA. We use Propagation Nonlinear of Spatio-TemporalCharacterization FWH7 •12:00p.m. A 78,063831(2008). beams advanced in a previous paper Physical light Review of vector characteristic new a of existence the demonstrate to shown are (2008) 787 319, Science haiUniv., in reported data experimental China.The , Beams Light Physical Evidence for New Characteristic Vector of FWH5 •11:30a.m. Nuclear, Univ. de Valencia and IFIC (UV-CSIC), Spain, Pinhole Interferometer, an with Singularities Polarization Creating FWH6 •11:45a.m. Departament d’Optica, Univ. de Valencia (UV), Spain. Delft Univ.Delft Technology,of Netherlands. Electromag 1 , Javier VijandeJavier , 2 ; 1 Univ. of Illinois Urbana-Champaign, USA, , , Chun-Fang Li; Dept. of Physics, Shang- Daniel E. Adams, Charles G. Durfee, Durfee, G. Charles Adams, E. Daniel Miguel-Angel Garcia-MarchMiguel-Angel 2 Dept. de Física Atómica, Molecular y Empire N larger than two,- a rich struc 2 , Albert Ferrando Albert , Robert W. Schoonover N -pinhole interferometer 3 ; 1 1 , Mario Mario , Inst. de Inst. 1 , , Taco N - -
found generic to innature. be contact with an environment. This behavior is further in qubits entangled two of dynamics entanglement the in periods dark and bright to lead interactions State Univ., USA. We show that coherent qubit-qubit a single run. in factors the obtaining allows and factors trial the of pre-checking the avoids realizations, past the to respect which, algorithm, factorization sums Gauss new a of realization experimental the presentWe Garuccio Levon Mouradian Levon more County, USA, County,more thélémy Vincenzo Tamma Run, Single a in Numbers Different Factoring FWI4 •11:15a.m. Qubits Interactions in the Entanglement Dynamics of Two Competing Effects of Environment and Inter-Qubit FWI6 •11:45a.m. dispersive similariton. measurements, based on the generation of nonlinear- trotemporal imaging for femtosecond scale temporal spectral interferometry and parabolic lensing - - spec of methods similariton-referencing novel of study Recherche,deFrance. comparative We the on report Imaging, Spectrotemporal and Interferometry Spectral Optics: Ultrafast in Similariton of Applications FWI5 •11:30a.m. Sciences—Continued FWI •OpticsinInformation , 2 ; Sumanta Das, Girish Agarwal; Oklahoma Agarwal; Girish Das, Sumanta 2 1 , YanhuaShih , YerevanStateUniv., Armenia, rm Zeytunyan Aram 1,2 1 , Frederic LouradourFrederic , , Heyi Zhang Crystal 2 Univ. degli Studi di Bari, Italy.Bari, di Studi Univ.degli 1 ; 1 Univ. of Maryland, Balti- Maryland, Univ.of FiO/LS/AO/AIOM/COSI/LM/SRS 2009 1 Grgn Yesayan Garegin , 1 , Xehua He Xehua , 2 , Alain Bar Alain , 2 XLIM Inst.XLIM 1 , , Augusto 1 - ,
FWJ5 •11:45a.m. length linear optics quantum controlled-NOT gate. telecommunications-wavea - of characterization on information processing. We present the latest results quantum communications-based for infrastructure telecommunicationsexisting the leverage can range wavelength 1.5-micron the in gates and states tum JosephB.Altepeter; Northwestern Univ., USA. Kumar, Monika Patel, Milja Medic, Matthew A. Hall, tanglement in the Telecommunications Band, - En Fiber-Generated with Gates Logic Quantum within a certain window.within acertain falls timescale correlation noise the if significantly help can detuning laser the Increasing analyzed. is presencescattering the ofexcited-statein dephasing Raman by photonsproducedindistinguishability of quantum The USA. Hewlett-PackardLabs, soleil; Beau - G. Barclay,Raymond E. Paul Fu, C. Kai-Mei Scattering , Raman by Produced Photons of Indistinguishability FWJ4 •11:30a.m. Waveguides II—Continued FWJ •QuantumOpticsin Charles Santori, David Fattal, Fattal, David Santori, Charles FiO Gold Invited • October 11–15,2009 Quan
Prem Prem - For Fall Congress presentations onWednesday, seepages125-131. Zhai Amnon Yariv Amnon able by using Bragg ashort grating. fiber amplitude-assistedrealiz- filters phase-onlyspectral which is based on the simultaneous utilization of two proposed, is approach shaping and multiplication pulse simultaneousUniv., all-optical novel Japan.A ShizuokaEngineering,Electronic and Electrical of Filter, FBG Only Phase- Amplitude-Assisted the on Based Shaping and Multiplication Pulse Optical Simultaneous FWK5 •11:45a.m. Detection Differential and Compression Pulse via Signals Ultra-Wideband of Generation All-Fiber Flexible FWK3 •11:15a.m. are demonstrated. of 25 GHz, as well as FCC mask compliant waveforms, ear fiber and differential detection. Center frequencies proposed, using pulse compression in highly nonlin- generatingwaveformsforultra-widebandscheme is simple and flexible A USA. California, Southern of Pr a in transparency induced electromagnetically via Weintroducedangular multiplexing storagelight in NankaiCtr.,PhysicsScience, ofUniv.,College China. Nonlinear Photonics, Nankai Univ., China, between neighboringbetween channels. selectively reading out stored pulses without cross-talk addressable all-optical routing were demonstrated by , Solid ency Transpar Induced Electromagnetically an in ing Addressable Optical Buffer via Angular Multiplex- FWK4 •11:30a.m. Processing III—Continued FWK •All-OpticalSignal 3+ :Y 1,2 2 , Jingjun Xu Jingjun , SiO , 5 crystal. Multi-channel buffer memory and Avi Zadok Avi YanfeiTu 1 , Alan E. Willner 1,2 Xuxing Chen, Hongpu Li; Dept. Dept. Li; Hongpu Chen, Xuxing ; 1 Valley , Xiaoxia Wu 1,2 1 MOE Key Lab of Weak LightWeak of Lab Key MOE , GuoquanZhang, 2 ; 1 Caltech, USA, 2 , Jacob Sendowski 1,2 2 , Zhaohui, Photonics Photonics 2 Univ. 1 - , and lidar systems. 100 GHz, what is importantover for reach laser communicationcan tunability the that predicts Theory large tunability is proposed via dynamic Stark effect. Technology,China. of Inst.Harbin Liu;Yuna,Shuangqiang Ping Wu, , Effect Stark Dynamic via Filter Optical Tunable Large-Scale FWL6 •11:45a.m. applications. speed high for suitable and free bias intrinsically is which implementation,convenient with generation number random true for approach new a propose we diode, laser of emission photon random the on Based Univ.,China.Peking Science, Computer and Wei Wei, Hong Guo; School of Electronics Engineering A Bias Free, Quantum Random Number Generator, FWL4 •11:15a.m. photonic networks. on-chip leading any to compared latency and tion consump- power reduced much a with bandwidth Tb/sec 2.56 provides scheme proposed The chips. network-on- photonic a implement to technology We USA. Arizona,Univ. of Louri; Ahmed Zhang, Xiang Architectures, Many-Core Future for Technology Stacked 3-D and Interconnects Nanophotonic FWL5 •11:30a.m. Devices—Continued FWL •OpticalCommunication
explore silicon photonics and 3-D stacked 3-D and photonics silicon explore Yundong Zhang, Zhusong He, Hao He, ZhusongYundong Zhang, California An optical filter scheme with a with scheme filter optical An Wednesday, October 14 85 - - Alaster Pablo Pablo De Quantitative Quantitative Cupertino JOINT FiO/AO JOINT JWB4 • 11:30 a.m. Experimental Test of Simulated Retinal Images Using Adaptive , Optics Gracia, Carlos Dorronsoro, Lucie Sawides, Enrique Gambra, Susana Marcos; Inst. de Óptica, Spain. Ocular degradation is - fre quently assessed convolving images with estimated point-spread-function, ocular the from the wave-aberration. Comparisons of visual acuity measured using aberrated cor adaptive-optics through (viewed targets aber natural under and aberrations) rected discrepancies. consistent reveal rations JWB • Advances in Adaptive JWB • Advances of the Living Optics Imaging I—Continued Retina JWB5 • 11:45 a.m. High Resolution Sensing Wavefront and Mirror Control for Vision Science by Quantitative Phase Imaging, J. Meehan, Phillip Bedggood, Brendan - All man, Keith A. Nugent, Andrew B. Metha; Australia. Melbourne, of Univ. Phase Imaging displays attractive features for ocular wavefront aberrometry. An adaptive-optics mirror control algorithm for ophthalmoscopy is demonstrated that takes advantage of its superior lateral resolution and similar accuracy compared systems. Hartmann-Shack to , Kelly , J. Kelly 3 Invited Stockholm Univ., 3 , Michael , Odelius Michael 1,2 Hillsborough Korea Korea Univ., Republic of Korea, 1 In In aqueous perchlorate solutions, ;
2 Stanford Univ., Stanford USA, Univ., LSWF • Multidimensional LSWF • Multidimensional II—Continued Spectroscopy water-water and water-anion H-bond struc- H-bond water-anion and water-water H-bond well-separated. spectrally are tures exchange dynamics of water is studied by - molecular and 2DIR spectroscopy dynam ics simulations. Gaffney 2 Sweden. Ultrafast Ultrafast Dynamics of Hydrogen Bond Exchange in Aqueous Ionic , Solutions Sungnam Park LSWF3 • 11:30 a.m. Invited For Fall Congress presentations on Wednesday, see pages 125-131. pages see Wednesday, on presentations Congress Fall For LS Polarization-rotation and Polarization-rotation October 11–15, 2009 Piedmont Keng Keng C. Chou; of Univ. British
• LSWE • Second-Order LSWE • Second-Order II— Nonlinear Optics Continued Polarization-Rotation Polarization-Rotation and - Two-Di mensional IR-Visible Sum Frequency Generation Spectroscopy for Surface , Analysis LSWE3 • 11:30 a.m. Columbia, Columbia, USA. frequency sum IR-visible two-dimensional generation spectroscopy will be discussed for studying surface phase transitions of electronic surface and polymers amorphous polymers. conjugated of states I , Ke 3 Invited , Chandra - Ra Stanford Univ., 1 1 Aubrey V. Weigel, Weigel, V. Aubrey ; 1 Georgia Tech, Georgia USA. Tech, 4 , , Andrew Berglund 1,2 CNST Nanofabrication Res. 3 Sacramento , Charles Limouse Lab of Chemical Physics, NIDDK, 1 , Hideo Mabuchi 2 1,4 LSWD4 • 11:30 a.m. USA, Zhang NIH, NIH, USA, will describe our group’s ongoing willresearch ongoing describe our group’s utilizing feedback microscopy to obtain tens-of-seconds per-molecule observation times in solution FCS and FRET mechanics assays. DNA on studies recent of Results will be presented. LSWD • Single-Molecule LSWD • Single-Molecule II—Continued Biophysics Group, Group, NIST, USA, Tracking Fluorescence Correlation Spec- Correlation Fluorescence Tracking troscopy of Individual Biomolecules, Kevin McHale man LSWD3 • 11:15 a.m. LSWD3 • 11:15 Tracking Single Potassium Channels in Live Mammalian Cells, Colorado Krapf; Diego Tamkun, M. Michael USA. Single molecule tracking Univ., State in concert with mean displacement square and cumulative distribution function analysis is used to study Kv2.1 ion - chan nel dynamics. Results show the channels are confined to clusters and they undergo subdiffusion. anomalous
, 1 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Intel Corp., Corp., Intel 1 ; 1 Invited Haisheng Rong Haisheng We demonstrate Masato Masato Hata, Daiki Atherton , Mario Paniccia , Mario 2 Intel Intel Corp., Israel. 2 FWN • Silicon Photonics II— Photonics Silicon • FWN Continued Tanaka, Hiroyuki Tsuda; Graduate Tanaka, School Japan. Univ., Keio Technology, and Science of lens Fresnel integrated an proposed have We with multiple slits in a Si slab waveguide. The slit width and the slit spacing were optimized and the integrated lens had a 0.38 dB. reflective of loss FWN4 • 11:45 a.m. Integrated Fresnel Lens Structure in a , Si-Slab Waveguide Omri Raday USA, USA, a cascaded silicon Raman laser using a tunable ring resonator cavity whose - reso nance frequency and coupling coefficient can be tuned to their optimal values post fabrication to achieve desired lasing performance. FWN3 • 11:15 a.m. FWN3 • 11:15 Cascaded Silicon Raman Laser Using Ring Resonator, Tunable FiO , Brian K. 1 , William H. 2 Vanderbilt Vanderbilt Inst. for 2 , Lloyd M. Davis 1 Univ. of Tennessee Space Inst. of Tennessee Univ. 1 Glen Ellen Glen ; 1 , Philip C. Sampson 1 Integrative Biosystems Integrative Res. and Education, USA. Univ., Vanderbilt We discuss the construction and characterization of a microfluidic device for the electrokinetic manipulation of sub-micron particles. A electrodes four of tetrahedral arrangement - pro to used is separation 100-micron with dimensions. in three vide control FWM4 • 11:30 a.m. Microfluidic Device for the 3-D Electro- Molecules , Single of Manipulation kinetic Jason K. King Hofmeister FWM3 • 11:15 a.m. Time Averaged Optical Traps for the Investigation of Superfluidity in , BEC Erik Weegink, Kristian Schnelle, K. Sebastian R. Norman Davis, J. Matthew Ooijen, van D. Heckenberg, Halina Rubinsztein-Dunlop; - of Queen Univ. Sciences, of Physical School realization the present We Australia. sland, of a time averaged optical trap for the use with Bose-Einstein condensates. The trap is able to spatially scan a laser beam to create arbitrary two dimensional static or potentials. dynamic FWM • Optical Trapping and FWM • Optical I— Micromanipulation Continued at Tullahoma, at USA, Tullahoma, Canfield Wednesday, October 14 86 lina Rickenstorff-Parrao Giuseppe A. Cirino A. Giuseppe Photomask, Diffractive by TransferPattern JWC4 index up to 97. rendering color high a with K 2200 to K 2760 from objects. It has a variable correlated color temperature new LED light source suitable for illumination of gold a WeTechnicalreport Denmark.Denmark, Univ. of Fotonik,DTU Petersen;Michael Paul Dam-Hansen, A New LED Light Source for Display , Cases JWC3 applications. possible of examples by illustrated and discussed are techniques these of potentialities The proposed. are length coherence transverse and polarization of degree desired with source secondary a generating LuizNetoG. Arrizón Victor achieved resolution as 1μm. as good the improvementofan show results The hologram. Fresnelonfabricateda is computer-generatedbased photomask for operation in proximity printing mode Univ. of São Paulo, Brazil. A phase-shift lithographic 2 OstrovskyS. PropertiesStatistical, Desired with Source Secondary a Generating forTechniques Two JWC2 like solarrial, cell. in machining and inspection for rough surface mate- apparatus.opticaleffective especially is method The posed to improve detecting accuracy pro- and miniaturizeis mirror elliptic using by method measuring TechnologyRes. Inst., Taiwan. novelA auto-focusing IndustrialHorng;Yu-HsiuJi-Bin Chang,Lin, Cheng Tsai,Meng-CheYang-Pin-HaoHu,Chia-Hsu Chen, Using Elliptic Optical Apparatus, by Method Auto-FocusingAccurate an of Design JWC1 Posters Optical DesignandInstrumentation São Paulo Univ., Brazil, Physics Inst., Campinas State Univ.,Brazil, State Campinas Inst., Physics Verdonck of São Paulo, Brazil, INAOE, Mexico. Two complementary techniques for 3 , Lucila H. Cescato H. Lucila , 1,2 1 ; , Miguel A. Olvera-SantamaríaMiguelA. , 1 2 EESC, Dept.ofElectricalEESC, Engineering, ; 1 Univ.Autonoma Puebla,de Mexico, 1 3 , Ronaldo D. Mansano D. Ronaldo , IMEC, Belgium, 2 1 PSI, Polytechnic School, Univ. , Gabriel Martínez-Niconoff 4 , Euclydes Marega Jr MaregaEuclydes , Yung-Hsing Wang, 4 Gleb Wataghin 2 , Patrick Patrick , 1 Carsten Carsten Andrey Andrey , Caro- , 5 IFSC, IFSC, 5 2 , , at rates of 13Hz. adhered disc fiducial to realize real time measurement camera,DSPccd andsingle system a anTheutilizes ing of heartbeats using image processing is reported. sens - remote Optical USA. Univ.Dallas,Texas atof Processing, Real Time Optical Vibrocardiography Using Image JWC9 ferential equations. orderdif- first solution the of the arefromobtained proposed. Lens surface profiles for extended sources emitting into circle and LEDsquare illuminationfor areas lenses are of type refractive and Reflective Federation.Moscow,RussianTechnologyCtr., LG Aslanov; Emil Tananaev, Georgy Petrov, I. Nikolai Illuminationfor, FreeformLenses EmittingWide JWC8 is presented.method the of principle the and device The designed. been has holograms focused non synthetizing for device original an models, computer 3-D of holograms rainbowcolorcreatingRGB of needs the cordingto Czech Technical Univ. in Prague, Czech Republic.Ac Holograms Rainbow Color RGB Synthetizing for Device a of Design JWC7 with sparseness values of 0.25or less. We achieve reliable performance by using data pages depend on the similarities among the stored data sets. tion signals in a defocused holographic storage system Technology Delhi, India. The characteristics of correla - Bhargab Das, Joby Joseph, Kehar Singh; Indian Inst. of focused Volume Holographic Data Storage System, Reliability of Content-Addressable Search in a - De JWC6 distortion is proposed. image ofsimultaneously.compensation for Method can be viewed by the observers around the hologram resultedprocess, the traditionalmultiplex hologram hologram-recording in planes film the and object the Univ.,CentralNatl. both Lin; Taiwan. tilting By Multiplex Holography Disk-TypeTraditional Viewable 360-Degree JWC5 Chester Wildey, Duncan MacFarlane; MacFarlane; Duncan Wildey, Chester , , Jakub Svoboda, Pavel Fiala; Fiala; Pavel Svoboda, Jakub Yih-Shyang Cheng, Shie-Hen FiO/LS/AO/AIOM/COSI/LM/SRS 2009 -
Zaïr ence Optical Wafers by Using Fabry-Perot Type Interferof Indices Refractive of Measurement Accurate JWC11 nonlinear or non-trivial effects optic systems. complex beams characterization as those produced by interferometryon spectral is presented, available for based pulses laser of reconstruction phase and tude amplispatio-temporal- performing device compact Láseres Pulsados Ultracortos y Ultraintensos, Spain. A index-measurement methods. implement,conventionalsimpleto compared the to silica), insensitive to environmental perturbation, and College of Engineering and Technology,India,and Engineering of College Technique, tion Hardness in AISI 304 SS by Laser Surface - Modifica Oscar VarelaOscar ug i Ju Jin Jung Moon Seb Han Inst. of Technology,of Inst.India, Méndez India, form Spectral Interferometry, Spectral form tion of Complex Beams by Means of Fourier-Trans- Spatio-Temporal Amplitude and Phase - Reconstruc JWC10 Characteristic Characteristic Study of Si JWC12 SciencePosters Laser 2 Korea, tive indices. This method is accurate (~10 interference from optical wafers to measure the refrac- Republic of Korea. of Republic substrate processed was laser at 59J/mm the while prevailed (850HV) hardness enhanced conditions surface with free crackand Smooth tion. treatedwas laser for topological- charactermodifica India. Sastikumar JWC •JointFiO/LSPoster Session Korea Res. Inst. of Standards and Science, Republic of 1 , , Luis Roso AISI 304 SS with preplaced Si Hee Joo Choi Joo Hee 4 3 Raja RamannaRaja Ctr. Advancedfor Technology, Electronics and Telecommunications Res. Inst., 1,2 JOINT FiO/LS , Julio San Román JulioSan , 12:00 p.m.–1:30p.m. 3 Imperial Ballroom 2 ; , Rakesh Kaul Rakesh , 1 , Íñigo Sola 1 Pusan Natl. Univ., Republic of Korea, of RepublicUniv., Natl. Pusan 1,2 1 , Myoungsik Cha Myoungsik , ; eciuh Rajarajan Petchimuthu We investigatedFabry-Perot type 1 Univ. of Salamanca, Spain, 1 , Hwan Hong Lim HongHwan , 1 , Rocío Borrego Varillas 3 , Asish Kumar Nath Kumar Asish , 3 3 India Inst. of Technology,of Inst.India N 1 , Camilo PrietoCamilo , 4 in the Enrichment of Benjamín Alonso Benjamín 1 , Tae Bong Eom BongTae , 3 N • 4 -Zr-Ni coating 1 , In-Ho Bae In-Ho , 1 2 , Dillibabu , . -5 for fused fused for October 11–15,2009 1 , Amelle, 4 ; 2 1 Ctr. de 1 , Cruz 2 Angel Angel Natl. 1 2 1 - , , , For Fall Congress presentations onWednesday, seepages125-131. Wang Doped NaYF Doped Ion- Earth Rare in Upconversion Visible Strong JWC13 Roger K. Sunahara Sergey Sarkisov Sergey particles forparticles extended observation. (HDL) lipoprotein density high single of trapping allows This geometries. microfluidic in solution in particles single Brownianofmotion the cancel cally electrokineti- to feedback voltage uses trap (ABEL) Anti-Brownian TheELectrokinetic USA. School,cal USA, Univ., Stanford Physiology, Cellular and Molecular Vance 1 Samuel Bockenhauer Samuel ParticlesLipoprotein, (HDL)Density High Single Anti-Brownian ELectrokinetic (ABEL) Trapping of JWC16 and analyzed. recorded were pulse optical and pulse current The reach more than 20 w when under pulsed condition. power output the respectively, diameters µm 600 and µm 400 of VCSEL 980nm fabricated haveWe Yongqiang Li, China. Sciences,Ning, LijunWang;of Acad. Chinese Qin Zhang, Yan Jingjing, Shi Tian, PowerVCSELPeak High, Pulsed 980nm JWC15 ~ 140psduration. wereanddesigns shown realised toexhibit ofpulses passively Q-switched microchip lasers. The resultingof performance the predict to used was equations, Australia. MacquarieUniv.,Physics, of W.Dept. Coutts;David , Laser Microchip Generating from Ultra-Short a Pulses Q-Switched JWC14 to understand upconversion the mechanisms. tensities of the upconverted emissions were obtained sion signals were recorded. Laser power and signal in- laser excitation, 408nm, 539nm and 655nm upconver prepared by simple synthetic method. Under 980nm Technologies, LLC, USA. NaYF Dept. of Chemistry, Stanford Univ.,StanfordUSA, Chemistry, of Dept. 3 1 1 Dept. of Pharmacology, Univ. of Michigan Medi- , , Michael Bokoch , Newton King Newton , A numerical model, based on the laser rate 4 Crystals 2 ; 1 OakwoodUniv., USA, 3 , Brian K. Kobilka Alex C. Butler, David J. Spence, Spence, J. David Butler, C. Alex 1 1 , , Malcolm Jessup , Alexandre, Fürstenberg 2 , Xiao Jie Yao Jie Xiao , , Darayas N. Patel N. Darayas 4 :Er 3+ ,Yb 2 2 , W. E. Moerner 1 , Brian DeVree , Lekara Green 3+ crystals crystals were 2 SSS OpticalSSS Zhenhua 1 2 , Calvin Calvin , Dept. of Dept. 1 , Quan, 3 1 1 - ; , , Lucie Krajcarová Radomír Malina Kizek in the Visible the Pulses in Ultrashort Measuring for Device Simple JWC17 Michaela Galiová Michaela by Laser-Induced Breakdown Spectroscopy , (LIBS) Multielemental Mapping of Archeological Samples JWC18 includes almost entire the visible spectrum. short pulses. By angle-tuning a thick crystal, its ultra- range visible measuring for ideal (GRENOUILLE) device (FROG) frequency-resolved-optical-gating simple extremely an demonstrateWe USA. Optics, research and development of that system. discuss will presentation This way. deterministic controlled a in operation for cavities optical main its prepare to system locking auxiliary an requires The advanced LIGO gravitational wave interferometer Yeaton-Massey,David Adhikari;Rana Caltech,USA. Gravitational Wave Interferometer, System for Locking Advanced the LIGO Auxiliary JWC20 images from fluorescence microscopy. maps obtained by this technique were compared with of the heavy metals in a plant tissue slices. Elemental mapping the nutrition elements and the accumulationfor utilized was LIBS pulse Double Republic. Czech Univ., Czech Republic, Univ., Czech Republic, Republic, Spectroscopy in Plant Tissue Slices by Laser-Induced Breakdown Mappingof Nutrition andHeavy Elements Metals JWC19 LIBS techniques are compared. discussed. The outcomes of double- and single pulse archeological samples with high-spatial resolution is mappingmulti-elementaloffor Spectroscopy down Republic. Procházka 3 , VojtĕchAdam , The capability of Laser-Induced Break- Laser-Induced of capability The 3 2 Mendel Univ. of Agriculture and Forestry,andAgriculture Univ.of Mendel , , Miroslav Liška , , ae Novotný Karel 2 Dongjoo Lee, Rick Trebino; Swamp Trebino; Rick Lee, Dongjoo 1 , Aleš Hrdlička Aleš , , Jozef Kaiser 1 , Jozef Kaiser Jozef , 2 2 Brno Univ. of Technology, Czech Brno Univ. of Technology, Czech 3 , Miroslav Liška Miroslav , 2 , Viktor Kanický Viktor , 2 , Viktor Kanicky Viktor , 1 1 , Michaela Galiová Michaela , , Jan Novotný Jan , 2 Krl Novotný Karel , Aidan F. Brooks, 2 ; 1 ; 1 1 Masaryk Masaryk Masaryk Masaryk 2 , David David , 1 , René 1 1 , , Wednesday, October 14
87 , , , , - - - 1 1 1 1 Dept. Dept. Dept. 1 2 index , Brian ; -6 2 2 Nanobio 2 , Seok Song Application of Application 1 Daniel Daniel Lopez-Cortes Yang Joo , Ivan Hernandez-Romano Ivan , INAOE, Mexico, Mexico, INAOE, 2 1 , Robert Magnusson , Renato de Araujo ; , Jose J. Sanchez-Mondragon J. Jose , 2 1 1 2 Jesus A. Nuñez Quintero, Jesus Serguei A. Quintero, Nuñez , Kyu Lee 2 School of Physics. Univ. College of Dublin, College of Dublin, Univ. of School Physics. 1 Dept. Dept. of Electronics and Systems, Federal Diego Rativa ; 2 1 Vohnsen resolution resolution and sub-nm detection limit for sensing achievable. are biomolecules We propose a technique technique a propose We Brazil. Pernambuco, of Univ. a as sensor wavefront Hartmann-Shack the exploiting the Unlike characterization. optical nonlinear for tool technique presented the method, Z-scan conventional scattering, linear misalignment, to sensitive so not is imperfections. sample and JWC44 SensorsLong-Range Surface-Plasmon Waveguide with µ-Fluidic Channel, JWC41 Fiber Optic Bending Sensor Based on Multimode Interference (MMI) Effects, Ireland, of Physics, Univ. of Hanyang, Republic of Korea, Korea, of Republic Hanyang, of Univ. Physics, of at Arlington, of Texas Univ. of Engineering, Electrical USA. Long-range surface-plasmon waveguide sen - sors consisting of asymmetric double metalfilms, a sandwiched channel µ-fluidic and grating resonance between the metal layers are described. 10 photonics Group, DICIS, Univ. de Guanajuato, Mexico. Guanajuato, de Univ. DICIS, Group, photonics Here we report a fiber bending sensor based on multimode interference effects. Sensing is achieved through losses induced in the propagating modes, which directly affects the intensity of the imaged fiber. the multimode by formed JWC42 Adaptive Interferometer for Detection of Laser Ultrasonic Signals Using Saturable Yb-Doped Fiber at 1064 nm, Stepanov; Ctr. de Científica Investigación y de Edu de Mexico. Ensenada, Superior cación in gratings population dynamic via mixing waves two nm 1064 at absorption saturable with fibers Yb-doped for detecting laser induced ultrasonic signals in the linear configuration of an adaptive interferometric reported. is vibrometer JWC43 Hartmann-Shack Sensing Wavefront of Zernike Polynomials for Nonlinear Materials Character , ization Jose R. Guzman-Sepulveda R. Jose Torres-Cisneros Miguel Daryl Ussery Daniel Daniel A. May-Arrioja Indian 1 ; 2 , Emmanuel, 1 Lab Hubert Lab Curien, Hubert 2 LPGs by electric arc Dual layer waveguides are used are waveguides layer Dual , Jean-Pierre , Meunier Jean-Pierre 1 Saurabh M. Tripathi M. Saurabh doped multimode fibers are most 2 Yoichi Taira, Hidetoshi Numata; IBM Numata; Hidetoshi Res., Taira, Yoichi - grat population of recording sensitivity High Gagandeep Purohit, Bibhuti Bhushan Padhy, Bhushan Padhy, Gagandeep Bibhuti Purohit, , Arun Kumar , 2 Doped MMF, Doped 2 Marin to to realize The an channel arbitrary shuffler. channel mapping of two parallel waveguides is determined laser of consist which vias, optical of positions the by mirrors. 45 degree two processed JWC40 Employing Structures SMS in CriticalWavelength GeO method in panda fiber at different exposure angles are are angles exposure different at fiber panda in method inscribed. The peculiarity of the inscription process made the LPG to behave as thermo-optic switch for in communication. application its JWC38 Bandwidth Enhancement in Multimode , Fibers Arash of Mafi; Univ. at Wisconsin USA. Milwaukee, We report on a substantial improvement in the caused fibers multimode index graded of bandwidth Scattering coupling. mode intentional controlled a by from micron size core inclusions induce the mode loss. power minimum with coupling JWC39 Arbitrary Shuffler Using Cross-Point Waveguide , Mirrors Japan. Lab, Res. Tokyo Sandipan Sandipan Nalawade, Harneet Thakur; Defence Inst. India. of Technology, Advanced Photonics Posters JWC36 Population Dynamic of Recording Sensitivity High in Yb-DopedSaturable Gratings Fibers 976nm, at Daniel García-Casillas, Serguei Stepanov; CICESE, Mexico. wavelength pumping typical at fiber Yb-doped in ings and (amplitude mixed Effective reported. is λ≈976nm below times formation with gratings dynamic phase) level. CW power sub-mW at recorded were 1ms JWC37 Inscribed Grating Period Long by Switching Optical Communi - Fiber in Application for Fiber Panda in cation Inst. of Technology Delhi, India, India, Delhi, of Technology Inst. sensitive sensitive near a critical wavelength and show - op change to respect with it spectral around posite shift temperature. in ambient Univ. de Univ. demonstrate Lyon, France. We experimen- tally and explain theoretically that SMS structures employing GeO For Fall Congress presentations on Wednesday, see pages 125-131. pages see Wednesday, on presentations Congress Fall For , ; 2 Gates October 11–15, 2009 -1/2 , Min Xiao 1 gates with 0≤ α 0≤ with gates • -α Univ. of Arkansas, Univ. 2 Hong Lin, Erik G. Born, Born, G. Erik Lin, Hong Henry Henry Baker, Spencer , Xudong Yu 1 Towards the Superstrong Cou- the Superstrong Towards _ Jing Jing Zhang Imperial Ballroom Imperial is the only perfect entangler and capable of of capable and perfect entangler only the is JOINT FiO/LS JOINT -1/2 Inst. Inst. of China, Opto-Electronics, ≤1constitute one edge of Weyl chamber, the geometric the chamber, Weyl of edge one ≤1constitute this In family, gates. structure of nonlocal two-qubit SWAP Multi-normal-mode splitting peaks are experi- are peaks splitting Multi-normal-mode USA. mentally observed in a system - with doppler-broad ened two-level inside atoms a long relatively optical regime. coupling” in the “superstrong cavity JWC31 Construction of CNOT Using SWAP constructing controlled-NOT. constructing JWC32 of Self-Trapping and Diffraction Symmetry-Broken , Lattices Photonic Triangle in Beams Inst. Multi-Vortex Zhao; Jianlin Gan, Xuetao Zhang, Peng Liu, Sheng - North Technology, and Science Information Optical of linear the study We China. Univ., Polytechnical western multi-vortex of dynamics propagation nonlinear and beams The in symmetry-a lattice. triangle photonic of state diffractionself-trapping moving and broken observed. beam are multi-vortex the input JWC33 Polarization Dynamics of Individual Transverse Laser Surface-Emitting Vertical-Cavity a of Modes Feedback, Optical to Subject Nola J. Palombo, Madeline C. White; Bates College, USA. We have experimentally studied polarization dynamics of transverse modes in a vertical-cavity - Correla feedback. optical with laser surface-emitting components polarized orthogonally of property tion of the first-order mode is different from that in the mode. fundamental JWC34 Timing Jitter in Prelase-Initiated, Single-Mode Pulses from a Repetitively Q-Switched, Diode- Pumped, Laser , Nd:YAG Kimori, John R. Thompson, Thomas Shaffner, Troy USA. Single-mode Inst., Military Virginia Siemers; J. tim- substantial display laser Nd:YAG an from pulses which Q-switch, the of opening the to relative jitter ing is driven by proximate fluctuations prelase intensity the Q-switch. of the opening to JWC35 Multi-Normal-Mode Splitting of a Cavity in the Atoms of Presence pling pling Regime, 1 Subramanian Balakrishnan, - Ramasubramanian Technology-Tiruchi of Inst. Natl. Sankaranarayanan; SWAP that found We India. rappalli, - JWC • Joint FiO/LS Poster Session—Continued FiO/LS Poster JWC • Joint Natl. 1 ; ; Bhaskar Bhaskar 2 Timothy , Arnab Mitra, Mitra, Arnab Simon Huang, Huang, Simon FiO/LS/AO/AIOM/COSI/LM/SRS 2009 , , Shyama Rath 1 The Beam India. of Delhi, Univ. 2 Eui Eui Su Lee, Bin Young Ji, Sang Hoon Kim, , , Hem C. Kandpal 1 Coherence-Polarization Coherence-Polarization (BCP) matrix for a pair beam laser of expanded an of cross-section the in points is investigated theoretically and determined experi - in a modified rotators and polarizers using mentally interferometer. Young’s of version Physical Lab, India, India, Lab, Physical Quantum Electronics Posters JWC28 Atmospheric Propagation of Fiber and Solid State Lasers in Maritime Environments O. Matthew Murphy, A. Leigh, Andrew Baronavski, Adin Kawate; Envisioneering, Inc., USA. We report in lasers for measurements propagation atmospheric at the maritime environments Pacific Missile Range Facility. Visible and near-IR lasers were directed to and helicopter, a into boat, a into shorelines, along island. a neighboring JWC29 of Motion Circular and Interaction of Observation , Lattices Ring Bessel-Like in Solitons Chen; Zhigang San State Wang, Francisco Xiaosheng in- particle-like soliton demonstrate USA. We Univ., lattices. photonic Bessel-like in rotation and teraction planet-like as well as rotations repulsive and Attractive different observed with were solitons two of orbiting relations. initial phase JWC30 Nonclassical Nature of Counting Probabilities in , DPO the from Light of Detection the JWC26 Terahertz Propagation on Plasmonic Crystal , Surface Korea. of Republic Univ., Maritime Korea Jeon; Tae-In present experimental We and theoretical studies on terahertz surface plasmon propagation on slit and rectangular aperture arrays in an aluminum sheet. Terahertz waves are coupled onto the plasmonic waveguide. viastructures a parallel plate JWC27 Determination of the Beam Coherence-Polariza an Expandedfor tion Matrix Laser Beam, USA. of Arkansas, Univ. Singh; Surendra Vyas, Reeta show We that both photon number and - photoelec tron counting probabilities can be used the directly from light to of nature nonclassical the demonstrate oscillator. parametric degenerate Kanseri , J. J. 1 .[1]. MIT, MIT, 1 al ; 1,2 , Norihide Meenakshi Meenakshi 2 , , ± 20GHz are 2 Genesia Genesia Corp., 3 Takahiro Takahiro Iijima /Ag, were analyzed analyzed were /Ag, 2 Tokai Tokai Univ., Japan, , 1 ; 3 Film 2 Monte D. Anderson; Air Force Force Air Anderson; D. Monte , George Barbastathis 1 and Ag/GeS and 2 , Yoshihisa Murakami 1 , Yoshikazu , Kanai Yoshikazu /Ag/GeS 3 2 Aditya Aditya Bhakta Singapore-MIT Alliance - for Alliance Singapore-MIT Res. and Technol , The photodoping characteristics of multilayer multilayer of characteristics photodoping The 2 Tsukuba Univ. of Technology, Japan, Japan, of Technology, Univ. Tsukuba Takeyama Kohli, K. T. Kapale; Western Illinois Univ., USA. Illinois Univ., Kohli, K. Kapale; Western T. We have theoretically devised and are experimentally implementing schemes for simultaneous - measure momentum angular orbital and polarization of ment (OAM) of light with the aim of understanding light carrying OAM emitted by rapidly rotating - astro objects. physical - switch polarization generates device electronic That current. the threshold also reduces and ing JWC24 Light Beam around Travel a Line Heat Source in Water and compared with the conventional two layer films. layer two conventional the with compared and films three layered to optical to The apply feasibility discussed. were waveguide memory and JWC23 Electronic Model for VCSELs: Switching Mode, Control of Threshold Cameroon. Current and , Yaoundé, Saturation of Univ. Woafo; P. Mbe, Talla H. the on based VCSELs of model electronic an build We mathematical rate equations of Danckaert et 2 Inst. of Technology, USA. Inst. optical of Tunable delays Technology, are observed in alkali vapor near resonant absorption lines. Pulses delayed across cesium D JWC21 Slow Light Delay Predictions and Measurements , Vapor Cesium Hot in Optical Sciences Posters Optical Sciences measured and compared to model predictions. to compared and measured JWC22 Microscopic Observation Process of Photodoping in Multilayer Ag/GeS USA, Moriaki Wakaki Japan. GeS films, ogy, ogy, Singapore. A heat source placed in quiescent fluid gives rise to a laminar convective plume. We compute the evolution of a laser beam due to the the by induced index refraction of changes resultant profile. temperature JWC25 and Polarization of Measurement Simultaneous On Orbital Angular Momentum of Light Wednesday, October 14 88 Satoshi Ebisawa Satoshi Noise, Low-Frequency Applying by munication - Com Chaotic Optical for Control Error Bit JWC49 pattern-dependence. tion conversion of a 500Gb/s data-stream without any - polariza all-optical the perform to capable scheme SOA-basedinterferometric an of performances the analyzinginvestigated numerically been haveSOAs Italy. Crognale,Antonella Giansante; Di Technolabs S.p.A., at 500Gb/s by Using Nonlinearities in SOAs, All-Optical TE-TM Polarization Mode Conversion JWC48 and impact the of gain the saturation is revealed. amplitude and frequency distributions are estimated, within a nonlinear transmission, are investigated. The operating amplifier erbium-doped single-mode in originatingare which pulses, optical bright trashort - ul Steady Mexico.Electrónica, y Óptica Astrofísica, Univ.,Japan, low-frequency noise. applying by decreased be can rate error bit the that show and scheme, arraytransmitter-receiver diode laser chaotic the in channelnoiseof effect the study Alexandre S. Shcherbakov S. Alexandre Mode Fiber Amplifier, Fiber Mode Bright Optical Pulses in an Erbium-Doped Single- Statesof Steady Saturationon Gain the of Impact JWC47 in 50MHz steps up presented. to be 0.5GHz will demonstrated. Experimental results for phase shifting Campus Loma Bonita, Mexico,Bonita, Loma Campus with capability of continuous 0 switching and modulation optical on based shifter Hulman Inst. of Technology, USA. A photonic RF phase Engineering,OpticalRose-Siahmakoun;and Physics Shifter , Phase Fiber-OpticRF JWC46 isof responsible beam signal for oscillations. the modulation ratio has been studied. Such amplification and materials of coefficient absorption on coupling dependence of parametric RamAnjore Yadav; Banaras Hindu Univ., India. The Cavity Ring Photorefractive Unidirectional in rameters Pa- Crystal on Gain Parametric of Dependence JWC45 Extreme optical gain nonlinear features in features nonlinear gain optical Extreme , Mahendra K. Maurya, TarunMaurya,Mahendra KumarYadav,K. 2 WasedaUniv., WeJapan.numerically 1 Siih Komatsu Shinichi , Mauro Sánchez Sánchez Sánchez Mauro gain due to the two-beam 2 ; 1 o Univ. del Papaloapan delUniv. -360 AlexMulvihill, Azad 2 Inst. Nacional de NacionalInst. o phase-shifting is 2 ; 1 Gakushuin Gakushuin Claudio 1 , Design and Fabrication of Multilayer Si/SiO Multilayer of Fabrication and Design JWC53 reasonably of efficient eavesdropping. detecting for method new a proposeand diodes receiverlaser of parameter mismatch the transmitter between and chaotic communication system, we discuss the effect point-to-multipointof characteristics optical the on StorageInst.,Singapore, tion and etching of 6~8μmmultilayer Si/SiO proposed and designed. We report success in - deposi of nanowaveguide to ~10μm of single-mode-fiber, is sub-0.5μm from transformation mode-size optical asymmetric GRIN lens (length:10~20μm) for vertical Optical Fiber Coupling Fiber Optical Super-High N.A. GRIN Lens for Nanowaveguide to Keh-Ting Ng Compact multilayer Si/SiO multilayer Compact Univ.,USA. western Suyama Communication, Chaotic Optical tipoint Point-to-Mulfor- Eavesdropping of Detection JWC52 simulated output data are presented paper. inthis plotand three dimensional profiles beam with CAD intensityTwo dimensional software. CAD available optical system has been designed using commercially Technology, USA. A four channel spatially multiplexed of Inst. Florida Biswas; Chakravarty,AbhijitRaka Fibers , Optical Wavelengthin Same of Channels (SDM) Multiplexed Domain Spatial Co-Propagating Four of Analysis CAD JWC50 1 plural plasmon surface polariton modes. plasmonic sources having different phases for exciting The dual sub-wavelength slits are used to generate two sub-wavelengthgratings. surface slits withdielectric We numerically examine beaming properties of dual Korea. of Univ.,RepublicNatl. Seoul Lee; Byoungho Gratings Surface Dielectric with Sub-WavelengthSlits Dual of Properties Beaming Light Plasmonic JWC54 Waseda Univ., Japan, 1 , , Satoshi Ebisawa Satoshi , Seyoon Kim, Junghyun Park, Yongjun Lim, 1 , , Yingyan Huang 2 Gakushuin Univ., Japan. Based 2 , OptoNetInc.,USA, Ter-Hoe Loh 2 2 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 , Seng-Tiong Ho Siih Komatsu Shinichi , Syed H. Murshid, Murshid, H. Syed 1 , Qian Wang 2 3 3 . North ; Kengo 1 Data Data JWC •JointFiO/LSPoster Session—Continued 1 1 - 2 2 , ;
Martha Alicia Palomino Ovando Palomino Alicia Martha Robert Magnusson Robert Univ., Republic of Korea, Mendieta Song Song and Waveguide, Devices Fabrication of Surface Plasmon-Polariton Couplers JWC56 and we superluminal find phenomenon. gapthat tunnelingappearthe at tuned in the modes are packets the dielectric-metamaterial, of layers alternate of structure periodic a traversing packets Gaussian electromagnetic of time transit calculate Mexico, Waveguides, Plasmonic Surface in Resonances Guided-Mode JWC57 nanophotonic devices. design flexibility andfor high efficiency various SPP with coupling consistent provides This structures. metallic on excitation (SPP) plasmon-polariton surface efficient for platforms waveguide and plers cou grating of stepping-lithographyfabrication holographic is Described Korea. of Univ.,Republic optical spectrum measurements.optical spectrum and patternsradiation far-field and near- measured Simulation results are presented in comparison with lasers. emitting surface vertical-cavity crystal nic photo- defect single on performed are calculations domain time difference finite Three-dimensional Shay, Gregory Kilby; United States Military Acad., USA. Simulations, FDTD 3-D Using Lasers Surface-Emitting Vertical-Cavity Crystal Photonic Single-Defect in Studies Depth Hole JWC58 couplingmode are presented. SP through tuning resonance and (SPs) plasmons investigated theoretically. The excitation been of have the slits surface periodic with films metal thin layer USA. Guided-mode resonances in single- and double- through Metamaterials, through WavesPropagation Electromagnetic of Study JWC55 2 1 ; , Kyu Jin Lee JinKyu , 1 Univ. of Texas at Arlington, USA, Arlington, at Texas Univ. of JOINT FiO/LS 2 2 We We Mexico.Sonora, de Univ.Autónoma ; Imperial Ballroom 1 Benemérita Univ. Autónoma de Puebla, Univ.de AutónomaBenemérita Hahn Y. Song 3 ; 1 1 , Robert Magnusson Robert , KAIST, Republic of Korea, 3 Univ. of Texas at Arlington, Daryl Daryl Ussery 1 , Sangin Kim Héctor Kinto Ramírez Kinto Héctor Kirk Ingold, Lisa Ingold,Kirk 1 , Felipe Ramos Ramos Felipe , • 1 , Hahn Young 2 , Kyu J. Lee 1 , Seok Ho Seok , 2 October 11–15,2009 Hanyang 2 Ajou 1 3 - , ,
For Fall Congress presentations onWednesday, seepages125-131. by using multiframe superresolution. still providing simultaneous high resolution imaging registering the trapped particle subpixel motion, while camera for the characterization of optical tweezers by We propose a novel approach for using a high-speed Chile. Concepcion, Torres;Univ.of Sergio Saavedra, as, tion of Optical Tweezers Using High-Speed Camer SuperresolutionImagingForceand - Characteriza JWC63 inoptical beam tweezers. laser inhomogeneous spatially generated intra-cavity by microorganism nanoparticles (253 nm.) and also low refractive index Delhi, India. We demonstrate multiple trapping of Au Shakher, Dalip Singh Mehta; Indian Inst. of Technology , Sensors Plasmonic to Nanoparticles/ Au Multiple Trappingof Optical Endorsed Beam Spatial JWC62 couple of inour holes, work. is described orientation and length, equal joining centers of each made from a number of couples of points with various diagnostic phase singularities using stochastic screen, Natl.V. Vernadsky Univ., Ukraine.ofpossibility The TauridaV.Shostka;Nataliya Shostka, I. Vladimir which Passed Stochastic , Screen Monochromaticin tices Polychromaticand Light, Vor Optical of PatternsInterference of Analysis JWC61 opticalfocus trap with variable wavelength. particles are manipulated and studied using Singlea single- object. trapped the of resonance optical the study the effects of optical tweezing near and far from trical and Computer Engineering, Rice Univ., We USA. Carly Levin analyzed and compared solitons. with ideal soliton-like behavior. Their waveguide properties are media are propagated numerically obtaining a spatial tributions for a positive and negative nonlinear Kerr ta Univ. Autónoma de Puebla, Mexico. Novel field dis- Arroyo Carrasco, Marcelo D. Iturbe Castillo; Beneméri- Ramírez Martínez, Maribel M. Méndez Otero, M. Luis Media, Kerr Waveguidein PropertiesTheir New Distributions with Soliton-Type Behavior and JWC59 Brooke C. Hester Resonance, from Far and near Tweezing Optical JWC60 Optics inBiologyandMedicinePosters Juan P. Staforelli, Jose M. Brito, Esteban Vera, Carlos 2 , Naomi Halas E.coli bacteria, which is made possible 1 , Rani Kishore Rani ,
2 Ranjeet Kumar, ChandraKumar, Ranjeet ; 1 NIST, USA, 1 E. coli E. , Kristian Helmerson Vladlen G. Shvedov, and Gateway and 2 Dept. Dept. of Elec Daysi 1 - - - , Digital-Optical Experimental Set up for up Set Experimental Digital-Optical JWC67 proteins insolution. ofteractionfibroblast growth factorand its receptor in- the study to used was technique scattering light SurendraUniv. Singh;Dynamical Arkansas,USA. of Its Sharma, Dakshinamurthy and Rajalingam, Factor T. K. S. Kumar, Growth Scattering, Light Using Complex Receptor Fibroblast of Study A JWC66 optical resonator. an of cavity the in structure biological a of section a of dispersion and spectrum absorption the of ing tion. PetersburgPolytechnical StateUniv., RussianFedera - Method, Spectroscopy Laser ity Characteristic Mathematical Modeling by Intracav- Optical Structure Biological Multilayered The JWC65 that enables real-time 3-Dmanipulation. hologramtype generated by a fast parallel algorithm Fresnel- the on light of diffraction by generated are optical tweezers based on an LCoS SLM. Optical traps holographic compact a report WeRepublic. Czech Nyvlt, Marek Skeren; Czech Technical Univ. in Prague, Trapping Optical TimeManipulation and , Compact Optical Tweezers Based on SLM for Real- JWC64 nique TechCorrelation- Cross on Based Tracking Cell EduardoAguilera-Gómez Javier J. Sanchez-MondragónJ. Javier G. Aviña-CervantesG. latent tuberculosis. say. This work enables for a method diagnosisthe of accomplished using a fluorescence-based immunoas- Antigen 85b, an antigen released by of tuberculosis, level was molecule single the at detection and cation identifi- Krapf; successful The Diego Univ.,USA. State Colorado McNeil, R. Michael Spencer, S. John W.Jevsevar,V.AubreyHill,Jarvis Weigel, L. Kristen Sensitivity Latent Tuberculosis Antigens with Single Molecule of Detection the for Immunoassay Fluorescence JWC68 The consuming time was reduced about 70%. Fourier transforms were done by an optical correlator. Image operations were performance by a FPGA while ing system in based the NCC technique is proposed. Óptica y Electrónica, Mexico. An automatic cell track- and Physical Optics Lab, Inst. Nacional de Astrofísica, Group, DICIS, Univ. de Guanajuato, Mexico, A mathematic model is constructed for predict- , Irais V.Solís Irais , Barbara S. Smith, Michael S. Scherman, MichaelSmith,S. S. Barbara 1 1 , Miguel Torres-CisnerosMiguel , , Oscar G. Ibarra-Manzano G. Oscar , 1 , HectorPlascencia-Mora, 2 ; 1 Nanobiophotonics Kirill Kulikov; St. Kulikov; Kirill 2 Photonics Photonics in vitro in Martin Martin Pallavi Pallavi 1 , Juan Juan , 1 1 , ,
Wednesday, October 14 89 - Jacob Jacob E. Alberto Lencina,
3-D field correlation of Chien-Sheng Chien-Sheng Liu, Chia-Hsu Chen, Optics in Information Science Posters Optics in Information JWC82 High for ColoredPulse Lasers Photography Novel Speed , Imaging Chia-Chao Chung, Po-Heng Lin, Kung-Hsuan Lin; Res. Industrial Technology This Inst., Taiwan. study color obtain to photography laser colored a proposes images. Based on the RGB synthesis technique, a novel colored pulse lasers photography is designed high speed for imaging. JWC83 3-D Field Correlation of Speckles Generated by Pupils with Multiple , Apertures Myrian Tebaldi, Néstor Bolognini; Myrian CIOp Tebaldi, (CONICET La Plata - CIC), Argentina. objective speckles is evaluated for systems whose pupils have multiple apertures. Minimal - supposi As properties. pupil speckle and on made were tions square for correlations longitudinal case, particular a analyzed. are apertures JWC84 LightRadio the in of Momentum Angular Orbital Range of the Electromagnetic Spectrum, Illinois Western Physics, of Dept. Kapale; T. K. Brown, or of detection and generation study We USA. Univ., radio the in light of (OAM) momentum angular bital potential with spectrum electromagnetic the of range by emitted that light OAM understand to application objects. astrophysical radio-active - - Juan Tabernero, Juan Frank Tabernero, Schaeffel; Azadeh Faylienejad, Vasudevan Azadeh Faylienejad, Vasudevan , No No significant differences in Strehl
Damber Damber Thapa, Andre Fleck, William
, JWC79 of Validation Computational Model for Predict ing Visual Acuity from Aberration Wavefront , Measurements Canada. Pre of Waterloo, Univ. Lakshminarayanan; visual by dictions of a acuity evaluated by model are comparing to experimental results. Different levels of internal noise and thresholds were used. This template matching model gives good results in the aberrations. of presence JWC80 A New Fast Scanning Infrared Photoretinoscope Refraction of as a Function Peripheral Measure to Accommodation A new Germany. Res. Tubingen, Ophthalmic for Inst. (4 measurements fast provide to designed instrument horizontal (±45º refraction peripheral the of seconds) vertithe- in refraction Peripheral presented. is field) the of function a as measured was meridian pupil cal state. accommodative JWC81 Strehl Ratio and Visual Acuity in a Pre-School Population R. Bobier, Vasudevan Lakshminarayanan; Univ. R. of Univ. Lakshminarayanan; Bobier, Vasudevan from calculated were ratios Strehl Canada. Waterloo, These images. Hartmann-Shack from obtained MTFs were compared to three visual acuity groups of 6/6, 6/9 and 6/12. observed. were ratios For Fall Congress presentations on Wednesday, see pages 125-131. pages see Wednesday, on presentations Congress Fall For - Tom , Carol 1,3 October 11–15, 2009 • Dept. of Ophthalmology Ophthalmology of Dept. 3 (on your own) Lunch your Break (on , MichelleMcFarlane, 2 Hospital For Sick Children, Canada, 1 ; Kvar Kvar C. L. Black, Jose G. Rivera, Kelly
Imperial Ballroom Imperial 1,3 , Josefin Nilsson Josefin , JOINT FiO/LS JOINT 1,2 The first Stiles-Crawford effect describes a pupil- a describes effect Stiles-Crawford first The Sahlgrenska Acad., Sweden, Sweden, Acad., Sahlgrenska A. Westall Vision and Color Posters Vision JWC77 Spectral and Spatial Characteristics of the First Stiles-Crawford Effect: - Ire Experiment Dublin, and College Theory , Univ. Rativa; Diego Vohnsen, Brian land. new Here beam. light narrow a of visibility dependent experiments are compared with theoretical analysis spectrum to visible the across waveguiding retinal of pigments. cone the influence of elucidate JWC78 A Potential S-Cone Dominated ERG Response Shows Robust Delays in Type 1 , Diabetes Wright 2 JWC76 Formation and Functionalization of Metallic Nanoparticles with Biomimetic Multifunctional , Catechols M. Luckasevic, Zhongqiang Liu, Phillip B. Messer smith; Northwestern USA. Univ., Catechols are employed by many organisms for diverse functions such as photoprotection, adhesion, immunity, and neuromodulation. We report the use of catechol- containing molecules as a biomimetic strategy to form and functionalize optically-active metallic (NPs). nanoparticles Diabetic Canada. Toronto, of Univ. Sciences, Vision and retinopathy is a common, irreversible outcome of diabetes. Early detection is essential for response successful ERG dominated s-cone new A intervention. shows delays robust in adolescents with 1 Type dia- retinopathy. to betes prior ; 2 JWC • Joint FiO/LS Poster Session—Continued FiO/LS Poster JWC • Joint 12:00 p.m.–1:30 p.m. Univ. of Univ. 2 Yasuyuki , Norio Miyoshi 2 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Fan-Ching Fan-Ching Chien, Peilin Kyu Hyun Kim, Tyler K. Drake, Michael Michael K. Drake, Tyler Kim, Hyun Kyu , Yukihiro Fukunaga 1 Pascal Dufour, Gabrielle DePascal Thériault, Dufour, Yves The blinking effects of quantum dots have Kurume Natl. College of Technology, Japan, Japan, of Technology, College Natl. Kurume JWC72 Super-Resolution Localization Microscopy by Quantum Dot Blinking, Sinica, Academia Sciences, Applied for Ctr. Res. Chen; Taiwan. been utilized to localize - microsco individual quantum conventional dots, by resolved be couldn’t which could dots quantum that demonstrated been has It py. resolution. be localized nanometer sub-10 with JWC73 Study of the Transversal Misalignment of an , Axicon Canada. We Laval, Univ. McCarthy; Nathalie Koninck, Gaussian a of misalignment the of effect the calculated beam with respect to an axicon and - resolu found its that preserves for line focal the displacements, small axis. the optical parallel to remains and tion JWC74 Noninvasive Estimation of Cultured Cell Condi- tions by a Laser Speckle , Microscopy Hirakawa Microscopic laser speckle observations observations speckle laser Microscopic Japan. Fukui, of three types of human prostate cancers revealed that the laser speckle fluctuated differently depend- ing not only on the cell line but also on divide. to ability the cell’s JWC75 Co- Low Multiplexed Integrated an of Development and herence Fluorescence Interferometer Clinical Endoscope, G. DeSoto, Marcus H. a USA. of The performance Henderson, Univ., Duke Wax; Adam David F. Katz, multiplexed integrated with endoscope clinical novel LCI and fluorescence measurements is evaluated. and accuracyFeasibility measuring for microbicidal gel distribution and thickness in the vaginal tract will be assessed. 1 - - Dept. Dept. 1 , Fan- Taiwan Taiwan ; 2 3 1,2,3 Res. Ctr. for for Res. Ctr. 3 , Peilin Chen 3 Shobhit Charan Diwakar Turaga, Timothy Diwakar Timothy Turaga, , July July A. Galeano Zea, Patrick Sandoz; , Narendra , Singh Narendra 3 We have We Taiwan. Sinica, Sciences, Academia Applied developed a nanoparticle based Raman probe (Ag@ Nile Red), which was of the targeting capable lipids, therefore, revealing the location of lipid droplets in . (C. elegans) elegans Caenorhabditis live JWC70 Pseudo-Periodic Pattern for Absolute - Bidimen under Interest of Zone a of Retrieval Position sional Microscope, School of USA. Medicine, Univ. E. Holy; Washington the in (DM) mirror deformable a introduced have We emission path of an OCPI microscope to allow for adaptive optics using phase diversity imaging. Cur algorithms diversity phase implementing are we rently the DM. calibrate to Vision system is used is system Vision France. Franche-Comte, de Univ. view of zone a of measurement position absolute for under microscope using pseudo-periodic pattern. Superimposition of recorded images in a common position reference system with subpixel accuracy is phase-computation. by obtained JWC71 Deformable Towards Mirror Calibration Using Phase Diversity in Objective Coupled Planar Il- lumination , Microscopy Ching Ching Chien JWC69 for Probes Raman Targeted Lipid of Development Caenorhabditis elegans of of Chemistry, Natl. Taiwan, Univ., Taiwan Intl. Intl. Graduate Program, Nanoscience and Technol ogy Program, Academia Sinica, Taiwan, Taiwan, Sinica, Academia ogy Program, Wednesday, October 14 90 atom-atom interactions catalyzed by one photon. andphotons single forrouter efficient an including for diverse advances in quantum information science, cro-toroidal resonators, thereby providing capabilities atom and photon has been achieved with high-Q mi- Caltech, USA. ToroidalMicro-Resonators with Photons and Atoms Single of InteractionsStrong Liège, Belgium, JWD1 •1:30p.m. Computing, Canada, Presider Kevin J. Resch; Inst. for Quantum and MeasurementIII JWD •EntanglementGeneration 1:30 p.m.–3:30p.m. Gillet , Blockade Dipole in Atoms of Saturation and Antibunching Entanglement, Quantum JWD2 •2:00p.m. optical transitions. the saturating by lifted be can blockade dipole how show Wefurther atoms. of antibunching and ment entangle- quantum to leads blockade dipole how 1 , Girish Agarwal Girish , JOINT FiO/LS Strong radiative coupling between one 2 Oklahoma State Univ., show USA. We Empire 2 , Thierry Bastin Thierry , Invited ,
H. Jeff Kimble; Kimble; Jeff H. 1 ; 1 Univ. de de Univ. Jeremie Research and Applications, 2009) Nanophotonicsand Photonics (Integrated optics. on-chip for need the driving ultimately stringent, increasingly become requirements cost and density Power,computers. today’sPetaflop 1000X is which viewed, emphasizing Exaflop performance circa 2020, re- aresupercomputers future and present in nects cale, - Exas to Road Supercomputing:The in Photonics FWO2 •2:00p.m. material structure. (Nonlinear Optics, 2009) materials incorporated into the sub-wavelength - meta photoexcitation of carriers into active semiconducting via control, frequency or substrate semiconductor control, via carrier injection or depletion in the active amplitude/phase either exhibiting metamaterials USA. Lab,Natl. Alamos Los Taylor;J.Antoinette Azad, K. AbulO’Hara,F. John Metamaterials,Terahertz Active FWO1 •1:30p.m. Presider Michael Duncan; NRL,USA, Highlights I FWO •OSATopical Meeting 1:30 p.m.–3:30p.m.
Jeffrey Kash; IBM Res., USA. Res., IBM Kash;Jeffrey Crystal Invited Invited FiO/LS/AO/AIOM/COSI/LM/SRS 2009 We demonstrate THz THz demonstrate We Optical intercon - Optical Hou-Tong Chen, Chen, Hou-Tong polariton dynamics. plasmon polaritons and excitons drastically alters the demonstrate that the strong coupling between surface angle-resolved pump-probe-spectroscopy. Our results using nanostructures metal-J-aggregate hybrid, of nonlinearities optical ultrafast the time, first the Univ.,Germany.Ossietzky von Carl Nanostructures, J-Aggregate Metal- Hybrid in Nonlinearities Optical Ultrafast FWP1 •1:30p.m. Republic of Korea, Presider Yeonghwan Ahn; Ajou Univ., FWP •MetamaterialsIII 1:30 p.m.–3:30p.m. length as inconventional methods. waveguide the changing physically without tained ob- is loss The configuration.transverse a in power metal-insulator-metal waveguides from the reflected in modes plasmonic characterizing for presented is method prism-coupler-based A Tech,GeorgiaUSA. Coupling Approach, Prism-Metal-Insulator-MetalofWaveguidesa by Modes Plasmonic in Loss the of Characterization FWP2 •2:00p.m. Chien-I Lin, Thomas K. Gaylord; Gold Invited
Christoph Lienau; Lienau; Christoph • We study for studyWe October 11–15,2009 FiO For Fall Congress presentations onWednesday, seepages125-131. FWQ1 •1:30p.m. Netherlands. Electrical Engineering, Eindhoven Univ. of Technology, Phase Space Optics, Space Phase and Coherence, Partial Distribution, Wigner USA, Presider Markus Testorf; Dartmouth College, 21 forthe Optical SystemTheory FWQ •PhaseSpaceOptics— 1:30 p.m.–3:15p.m. ings of conferences. scientific international scientific journals, books and proceed- the author and co-author of more than 175 papers in is a Fellow of OSA and a senior member of IEEE. He is Wigner distribution) and related issues. Dr. Bastiaans (suchby as the means spectrum frequency of a local main current research interest is in describing signals all kinds of problems that arise in Fourier optics. His and includesapproach signal-theoretical a theory of ferent aspects in the general field of signal and system dif- covers research Group.His Systems Processing Signal the in Technology,currently of University the Department of Electrical Engineering, Eindhoven with professor associate an been has he 1985, since tively. In 1969, he became an assistant professor and, Technology,respec- 1983, and 1969 Netherlands,in Universityof Eindhoven from sciences technical in Ph.D.degree a honors) and (with engineering trical Martin J. Bastiaans received andegree in - elec M.Sc. optical perspective. phase-space and radiometric a fromsystemsoptical first-order through propagation their and signals coherent optical treatpartially tomeans perfect a as st Century I Century
The Wigner distribution is presented is distribution Wigner The Valley
Martin J. Bastiaans; Dept. of Dept. Bastiaans; J. Martin Tutorial applications. progress in the field and highlight important clinical ing of the human body. This presentation will review at San Diego, USA, confocal microendoscope systems for systems microendoscope confocal of application and design the in made been have USA. Arizona, Univ.of Rouse; cation Appli - and Design Microendoscope in Advances Nanostructures, Plasmonic and Biomolecular Sensing with Ultrafine Optical Fibers ing, Univ. of California at San Diego, USA, Diego, San at CaliforniaUniv. of ing, Sarah Baker Sarah functionalization, and multiplexed sensing. are integrated into microfluidic flow cells for chemical bio-detection systems discussed. These optical cavities field evanescentcompact in use their presentedand be will nanostructures semiconductor dimensional USA. Lab,Natl. LivermoreLawrence Directorate, Sciences Life and FWR1 •1:30p.m. Univ. of Arizona, USA,Presider LLC and College of Optical Sciences, JohnR. Koshel; Photon Engineering in EmergingTechnologies I FWR •NovelOpticalArchitectures 1:30 p.m.–3:30p.m. Esener FWR2 •2:00p.m. 1,2 , Arthur Gmitro,Makhlouf,AndrewHoussineArthur , 1 NanoEngineering Dept., Univ. of California 3 , Sanja Zlatanovic Unique optical properties of one- of properties optical Unique California 2 Electrical and Computer Engineer Invited Invited 2 , Jason Steiner Significant advances Significant Donald J. SirbulyJ.Donald in vivo in 3 Physical 1 , Sadik imag 1 - - , Wednesday, October 14 91
, 2 - Zhi , 1 Inst. Inst. for 2 A relaxation-assisted relaxation-assisted A , Grigory I. Rubtsov I. Grigory , 1 Invited Invited , Valeriy M. Kasyanenko M. Valeriy , Tulane Univ., USA, Tulane Univ., 1 1 ; 1 Hillsborough , Christopher S. Keating S. Christopher , 1 Igor V. Rubtsov V. Igor LSWI1 • 1:30 p.m. 1:30 p.m.–3:00 p.m. 1:30 p.m.–3:00 LSWI • Multidimensional III Spectroscopy Minnesota, of Univ. Blank; David USA, Presider LSWI2 • 2:00 p.m. James P. James Donahue P. Federation. Russian Res., Nuclear two-dimensional infrared spectroscopy method in molecu- a on transport energy on relies that discussed in amplifications cross-peak strong shows and level lar model peptides, including systems, molecular various metal complexes. transition and compounds, Femtosecond Vibrational Femtosecond OpticalVibrational Activity and IR EchoPhoton Studies of Small Organic Molecules, MinHaeng Cho; Korea Republic Univ., of Korea. Ultrafast characterization of vibrational circular dichroism and optical rotatory dispersion is shown to be experimentally feasibly by using heterodyned spectral interferometric detection of the phase and free-induction- activity optical infrared of amplitude field time. in decay Molecular a on Time Transport Energy Correlating Level with Distance Using Relaxation-Assisted , 2DIR wei Lin wei Invited Invited LS Piedmont The The theory and phenomenology of Anne Anne M. Kelley; of Univ. California at
, tensor elements of thin films, enabling (2) Nonlinear optical Stokes ellipsometry (NOSE) Stokes optical Nonlinear imaging imaging applications with detailed polarization characterization. 1:30 p.m.–3:15 p.m. 1:30 p.m.–3:15 Nonlinear LSWH • Second-Order Optics III at California of Univ. Ben Schwartz; USA, Presider Angeles, Los LSWH1 • 1:30 p.m. Imaging Imaging Nonlinear Optical Stokes Ellipsometry Characterization, Microparticle and Film Thin for Nathan J. Begue, Garth J. Simpson; USA. Purdue Univ., parts few a of precision provide routinely to shown is determination for times acquisition ms 12 in 1000 in of the χ Electronically Resonant Hyper-Raman Scattering in Solution Merced, USA. from scattering hyper-Raman resonant electronically organic molecules in solution is reviewed nonlinear and resonant its electronically other to relationship discussed. is spectroscopies vibrational LSWH2 • 2:00 p.m. For Fall Congress presentations on Wednesday, see pages 125-131. pages see Wednesday, on presentations Congress Fall For We October 11–15, 2009 • Invited Invited Hrvoje Petek; Univ. of Pittsburgh, Pittsburgh, of Univ. Petek; Hrvoje Tahei Tahara; RIKEN, Tahara; Tahei Japan.
Sacramento By By time-resolved two-photon photoemission 1:30 p.m.–3:30 p.m. 1:30 p.m.–3:30 I Spectroscopy LSWG • Ultrafast of Univ. Achermann; Marc USA, Amherst, Massachusetts Presider LSWG2 • 2:00 p.m. LSWG1 • 1:30 p.m. Ultrafast Ultrafast Photoemission Electron Microscopy: Imaging Nonlinear Plasmonic Phenomena on the Scale, Femto/Nano USA. electron microscopy, we generate movies with surface of <50 rate frame as 330 and resolution spatial nm formed lithographically by defined dynamics plasmon films. in silver elements nano-optical New Interface-Selective Electronic Spectroscopy and Extension Its to Femtosecond Time-Resolved , Measurements report multiplex electronic sum-frequency generation generation sum-frequency electronic multiplex report femtosecond to extension its and spectroscopy (ESFG) time-resolved measurements (TR-ESFG), which provide unprecedentedly high-quality electronic and static on information rich containing data spectral molecules. interfacial of properties dynamic - FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Invited Jacques Jacques Albert, Maria De
Mohamad G. Banaee, Kenneth B. B. Kenneth Banaee, G. Mohamad Atherton Standard Standard optical fibers coated with
was obtained. was 6 FWT2 • 2:00 p.m. Gold with Spectroscopy Raman Surface-Enhanced , Dimers Nanoring Crozier; School of Engineering and Applied Science, Harvard USA. Univ., Surface-enhanced Raman scattering of benzenethiol on gold nanoring dimers with 20 nm gaps was studied. The localized surface using determined was wavelength resonance plasmon factor enhancement SERS A spectroscopy. reflection 2.0x10 of 1:30 p.m.–3:15 p.m. 1:30 p.m.–3:15 Sensors FWT • Plasmonic of Inst. Indian Gupta; D. Banshi Presider India, Delhi, Technology FWT1 • 1:30 p.m. rosa, Anatoli Ianoul, Yanina rosa, Shevchenko, Anatoli Alexander Ianoul, Yanina Beliaev, David A. D. Blair, Nur Ahamad; Carleton Canada. Univ., Plasmonics Plasmonics on Optical Fibers: New Tools for Biochemical , Sensing metal layers support plasmonic resonances at near infrared wavelengths. We use a fiber Bragg grating to measure their response to surface biochemical proteins. and DNA involving reactions FiO NSF 1 ; 1,3 , Douglas Douglas , Lawrence 1 3 , James Chan , Tobias Moritz Tobias , 1 Dept. Dept. of Science, Applied 1,3,4 Dept. Dept. of Pediatrics, Univ. 4 2 Invited Rui Liu Rui Glen Ellen Glen We have developed a number of We optical Wesley Wong; Rowland Wesley Wong; Inst., Harvard
, , Dennis Matthews 1,2 FWS1 • 1:30 p.m. 1:30 p.m.–3:30 p.m. 1:30 p.m.–3:30 Trapping and FWS • Optical II Micromanipulation Be Announced to Presider Ctr. for Biophotonics Science and Technology, Univ. of of Univ. Technology, and Science Biophotonics for Ctr. California at Davis, USA, Univ. of Univ. California at Davis, USA. The translation of laser tweezers Raman spectroscopy is impeded by several instrumentation limitations. This paper 10s (< faster a developing in work latest our presents automated fully for system compact time), acquisition cellsingle analysis. Taylor of of California at Davis USA, Medical Ctr., Livermore Natl. Lab, USA, Lab, Natl. Livermore FWS2 • 2:00 p.m. High-Throughput and Compact a of Development Laser Trap Raman System for Fully Automated , Analysis Cell Single High-Resolution, High-Stability, High-Frequency High-Resolution, High-Stability, Optical Tweezers Methods with a Simple Video Camera USA. Univ., tweezers techniques for performing high-resolution (3-D, angstrom-level), high-stability (1-2 nm - long term), high-frequency (> 100 kHz) measurements using inexpensive video microscopy. Experimental demonstrations include quantification of protein kinetics. folding Wednesday, October 14 92 Photon-Holes Entanglement Photons Energy-Time between and JWD5 •2:45p.m. Bell’s inequality. of violation allowing hole, the with entangled time accompanied by emission of a photon that is energy- is creationphoton-hole the byproduct, a As beams. coherent photon-holesin creates that source a pose Technology,Technion-IsraelIsrael.of WeInst. pro and MeasurementIII—Continued JWD •EntanglementGeneration of Queensland, Australia,Queensland, of Jack chemistry, and materials science. which promises to be a powerful new tool in biology, chemistry,quantum efficient of demonstration experimental first the is This molecule. hydrogen the simulate to computer quantum photonic a use field 1 FirstSteps , andProspects Computer: Quantum a on Chemistry Quantum JWD3 •2:15p.m. Orbital Angular Momentum, and Angle for ParadoxVariable EPR Continuous JWD4 •2:30p.m. M. Barnett M. Kassal Barbieri entangled light field. the of naturequantum the demonstratingtherefore position and orbital angular momentum correlations angular strongWe show light. of statesmomentum Podolsky-Rosen paradox for angle and orbital angular Strathclyde,UK. of Univ. of Glasgow, UK, 1 2 , Jacq Romero Jacq , , G. G. GillettG. G. , 2 , J. D. Biamonte 1 JOINT FiO/LS , A. Aspuru-Guzik 3 , Sonja Franke-ArnoldSonja , , Serge Rosenblum, Meir Orenstein; Orenstein; Meir Rosenblum, Serge 1 , M. E. Goggin E. M. , 1 We demonstrate the Einstein- the demonstrateWe , Bob Boyd Bob , Empire 2 2 , M. Mohseni Univ. of Rochester, USA, 2 2 , Andrew G. White We We Univ.,USA. Harvard B.P. Lanyon Jonathan Leach 2 , Anand Jha Anand , 1 , M. P.M. , Almeida 1 2 , Miles Padgett Miles , , B. J. Powell 1 , J., D. Whit - 1 2 1 ; , Steve Steve , , Barry 3 1 Univ. Univ. 1 , M. 1 , I. , 1 - ; FWO3 •2:30p.m. Highlights I—Continued FWO •OSATopical Meeting Applications, 2009) Trapping excitation.(Optical fluorescence of means manipulation. The subsequent reaction is probed by optical via fused are nanodroplets the when mix nanodroplets the in sequestered reagents Chemical nanodroplets. aqueous within reactions volume at Charlotte, USA. Jofre,Faulk, Univ.Ben Jason Case; NorthCarolinaof Aqueous Ana Applications, Femtoliter Nanochemistry for of Droplets Manipulation Optical We control and observe femtoliter Crystal Invited FiO/LS/AO/AIOM/COSI/LM/SRS 2009 operate visible inthe range. systems Our properties. polarization specific with particular chiral structures) to design optical devices (in nanostructures metallic by plasmons surface of control the through offered possibility the on focus Univ.France.Ebbesen; StrasbourgCNRS, and de W.Thomas Genet, C. Drezet, A. Lombard, E. Laux, Nanostructures, Metallic through Light Visible of States PolarizationTailoring Radio Astronomy,Ukraine,Radio Politécnica de Valencia, Spain, Daniel E. Ceballos Physics. Natl. Univ. of Ireland, Ireland, stantin YuBliokh stantin Continued FWP •MetamaterialsIII— 3 cada (IUMPA),Univ.cada Valencia,Politécnicade Spain, Spain, these systems.these in solitons spatial via polaritonsplasmon surface of excitation of possibility the discuss We structures. metal/dielectric/Kerr in excitation quasi-particle of type new a of existence the on based phenomena optical novel presentWe Mexico. A.C., Óptica en Structures, Metal/Dielectric/Kerr at Excitations Soliplasmon FWP3 •2:15p.m. FWP4 •2:30p.m. Technion-Israel Inst. of Technology,Technion-IsraelIsrael,of Inst. 2 Inst. Universitario de Matemática Pura y Apli - Albert Ferrando Albert 4,5 7 ; , MarioZacarés, 1 Dept. d’Òptica, Univ. de València, Gold Invited 1,2 5 Dept. of Experimental of Dept. 7 , YuriP.Bliokh, Ctr. de Investigaciones 2 , Carles MiliánCarles ,
• J.-Y. Laluet, E. E. Laluet, J.-Y. 6 ITACA, Univ. October 11–15,2009 4 Inst. of Inst. 3 , Kon- , We We 2,6 FiO , For Fall Congress presentations onWednesday, seepages125-131. FWQ3 •2:45p.m. 21 forthe Optical SystemTheory FWQ •PhaseSpaceOptics— that extend depth the of field,inatunable fashion. foranalyzing novela ofphase-only family set masks We apply the ambiguity function for identifying and Jorge Ojeda-Castañeda; Univ. of Guanajuato, Mexico. forNovel Field of Extended Devices ViewOptical , and compared. the propagation of waves based on rays are described presented, and many standardis methods models for waveestimating and ray the between connection the understanding of ways several of survey A Rochester,USA. Univ.of Optics, of Inst. Alonso; A. Wavesand Rays , between Connection The FWQ2 •2:15p.m. st Century—Continued Valley Invited Invited Miguel Miguel
high numericalhigh aperture micromirror. (~17%) across a 15 mm object space by integrating a systemimaging f/2.55 traditionalover a 18 of factor a by collection light source point of enhancement Univ.,WeDuke Kim;demonstratedhavesangUSA. Justin Migacz, Caleb Knoernschild, Taehyun Kim, Jung- Optics, Using Multiscale Source cent FluoresPoint- a from Collection Light Enhanced FWR4 •2:45p.m. Technologies I—Continued Architectures inEmerging FWR •NovelOptical rates of 10Hz. at measurement motion 6-DOF time real realize to fiducial 3-dimensional a and DSP camera, ccd environment is reported. The system utilizes a single MRI for trackerthe head optical An atUSA. Dallas, Wildey,MacFarlane;ChesterTexasDuncanUniv. of , Camera Single a UsingEnvironment MRI the in Correction Motion Real-Time forTracking Head FWR3 •2:30p.m. California Rachel Noek,Rachel Wednesday, October 14 93 - Kuo- Dmitry Pestov, Vadim V. Lozovoy, Lozovoy, V. Vadim Dmitry Pestov, Hillsborough LSWI • Multidimensional LSWI • Multidimensional III—Continued Spectroscopy LSWI4 • 2:45 p.m. Control and Coherence, Spectroscopy, State Excited in , Solution of Polyenes in the Isomerization G. Kenneth Chun Spears, Tang, Roseanne J. Sension; - absorp transient UV-Visible USA. Michigan, of Univ. excited- the study to used been has spectroscopy tion and 7-dehydrocholesterol of dynamics reaction state cis-stilbene in has solution. been UV-pulse-shaping influence and pulse excitation the manipulate to used dynamics. reaction LSWI3 • 2:30 p.m. Character and Generation Sequence Pulse Optical Comb Independent Multiple Phase-Only via ization Shaping , (MICS) Marcos Dantus; USA. Michigan State Univ., de- We - opti of synthesis for technique shaping pulse a scribe pump-probe for suitable deemed sequences, pulse cal experiments and multidimensional spectroscopy. It manipulation, programming, straightforward enables and self-characterization of multi-pulse waveforms shaping. phase-only via one-dimensional Invited Steven Steven Baldelli; of Univ. LS Piedmont LSWH • Second-Order Nonlinear Nonlinear LSWH • Second-Order Optics III—Continued LSWH3 • 2:30 p.m. Title Title to Be Announced, Abstract not available. not USA. Abstract Houston, For Fall Congress presentations on Wednesday, see pages 125-131. pages see Wednesday, on presentations Congress Fall For , 1 October 11–15, 2009 • , Virginia Martín Virginia , 2 , Inmaculada García- 1 , Olga García Olga , 1 Inst. de Inst. Física Química Rocasolano, 1 Sacramento ; Angel Costela 2 - Políme de Tecnología y Ciencia de Inst. 2 , Luis Cerdán Luis , 1 LSWG • Ultrafast LSWG • Ultrafast I—Continued Spectroscopy CSIC, Spain, Spain, CSIC, ros, ros, CSIC, Spain. report We on efficient and highly photostable solid-state lasers based on dye-doped polymer crosslinked with polyhedral oligomeric silsesquioxane (POSS) nanoparticles. Mechanisms for the improved laser action induced by the POSS will bepresence discussed. LSWG4 • 2:45 p.m. Solid- Advanced as POSS-Copolymers Nanohybrid State Lasers, Roberto Roberto Sastre LSWG3 • 2:30 p.m. ZnO Thin Films for , Optoelectronic Applications T. Prasada Rao, M. C. Santhosh Kumar; Dept. of Physics, Natl. Inst. of India. Effects Technology, of substrate temperature on crystallization behavior, optical, and electrical properties of the observedfilms was was emission asymmetrical Visible studied. in photoluminescence spectra. Electrical resistivity - increas and decreasing are concentration carrier and respectively. ing, Moreno - , Antonio Antonio , 1 Yizhuo Chu, Chu, Yizhuo sensors with with sensors 2 Gustavo O. Caval FiO/LS/AO/AIOM/COSI/LM/SRS 2009 , Eduardo Fontana Eduardo , 2 . 8 Atherton Univ. Federal de Pernambuco, Brazil, 1 ; ; 1 , Sergio C. Oliveira C. Sergio , 1 Univ. de Univ. Brazil. Pernambuco, We investigate both FWT • Plasmonic Sensors— FWT • Plasmonic Continued FWT3 • 2:15 p.m. and Wavelength Pd Thickness Optimization for SPR-Based Hydrogen Sensors, Azevedo 2 Mohamad Mohamad G. Banaee, Kenneth B. Crozier; Harvard USA. Univ., We report surface-enhanced Raman monolayer benzenethiol a of measurements scattering The structure. plasmon surface resonance double a on light scattered Raman and excitation enhances device The simultaneously. largest enhancement factor is be to 1.1×10 measured FWT4 • 2:30 p.m. Interfering SPR Sensor with Radial , Polarization Chiao Tung Natl. Tien; Lan, Chung-Hao Tzu-Hsiang - refrac the sensor, SPR collinear a For Taiwan. Univ., objective by constrained was range tive-index-sensing demonstrated we SPPs, interfering the Utilizing lens. 1.3 from range measured the extend to scheme new a microscopy. in a 1.45-NA 1.5 to FWT5 • 2:45 p.m. Surface-Enhanced Raman Scattering from a , Structure Plasmon Double-Resonance theoretically and experimentally the performance of of performance the experimentally and theoretically surface the on based detection hydrogen for films Pd plasmon resonance effect. Results yield important H SPR-based of design the for findings maximum sensitivity. maximum canti FiO Invited We will discuss We our recent Changhuei Yang, Meng Changhuei Cui, Yang, Emily Glen Ellen Glen Marek Škereň, Marek Martin Nývlt, David Optical manipulation is presented with various various with presented is manipulation Optical FWS3 • 2:15 p.m. FWS3 • 2:15 Optical Manipulation with Particles Using the Microflu- Special on Tweezers Optical Holographic idic , Substrates as working substrates relief special on micro-particles prepared are substrates The devices. microfluidic the - real is manipulation The lithography. laser the using tweezers. optical the holographic ized using FWS • Optical Trapping and FWS • Optical II—Continued Micromanipulation - Re Czech Univ., Technical Czech Fiala; Pavel Najdek, public. FWS4 • 2:30 p.m. Optical Phase Conjugation for - Tissue Turbid ity , Suppression USA. Caltech, McDowell; findings on the use of optical-phase-conjugation to undo optical tissue scatterings. Amongst other results, we discovered that light scattered hundreds of times still retains sufficient memory to enable retracing. path Wednesday, October 14 94 and MeasurementIII—Continued JWD •EntanglementGeneration Information Processing with Remote Ions Remote with Processing Information Measurement-BasedEntanglement Quantumand JWD6 •3:00p.m. the ionsthe violates inequality. aBell of state entangled The 89%. of fidelity gate average an measure and ions ytterbium trapped remote two between gate entangling probabilistic a ment NIST,USA. andMarylandUniv. Inst., of N. Matsukevich, Christopher Monroe; Joint Quantum Dzmitry Hayes, David Olmschenk, Steven Maunz, ______JOINT FiO/LS Empire Invited Weimple- ,
Peter Peter Highlights I—Continued FWO •OSATopical Meeting Solid-State Photonics, 2009) (Advanced discussed. are spectroscopy and sensing coherent imaging, biomedical for applications and mechanism FDML The waveforms. output swept wavelength rapidly narrowband, generating lasers, of regime operating stationary new a is (FDML) München, Germany. Sensing, and Ranging Profilometry, Imaging, Biomedical for Applications and Regime Operating Laser New A (FDML): Locking Mode Domain Fourier FWO4 •3:00p.m. Robert Huber; Ludwig-Maximilians-Univ. Huber; Robert Crystal Fourier Domain Mode Locking Invited 3:30 p.m.–4:00p.m. FiO/LS/AO/AIOM/COSI/LM/SRS 2009 efficient nanoantennaefficient array. an as act andcoherence in radiatenanocavities that films through surface propagating plasmons. metal Wein nanocavitiesshow in created be can excitations perimentally demonstrate that hybridized plasmonic Univ.,USA. Boston Altug; Hatice Erramilli, mons, Plas- Propagating Surface through Nanocavities in Excitations Plasmonic Hybridized of Creation FWP6 •3:15p.m. Zhang sensitivity is studied. the and derived, resonant-incident-angleis the and displacement the relating expression analytical An angle. incident resonant the using displacement the measures that plasmons, surface using sensor, Singapore. ElectronicEngineering, Nanyang Technological Univ., turing Technology, Singapore, Continued FWP •MetamaterialsIII— Using Surface Plasmons Surface Using by Sensor Displacement Optical Sensitive High FWP5 •3:00p.m. Coffee Break/Exhibits,Imperial Ballroom, Fairmont Hotel 1 , Yeng, ChaiSoh Ahmet A. Yanik,Adato,ShyamsunderRonenA. Ahmet We present a new optical-displacement new a presentWe NOTES Gold 2 ; 1 SingaporeInst. Manufacof - , Zhaogang Dong Zhaogang 2 School of Electrical and • October 11–15,2009 We ex We 1,2 , Ying , FiO - For Fall Congress presentations onWednesday, seepages125-131. 21 forthe Optical SystemTheory FWQ •PhaseSpaceOptics— st Century—Continued Valley Technologies I—Continued Architectures inEmerging FWR •NovelOptical cavity is now possible. integratingan scatteringin ofaerosolsspectroscopy ring-down that high so is region spectral micron 1 to nm 250 the in reflectivity whose developed been has reflector diffuse new A Univ.,USA. State and packaging constraints are included. Performancelimitationsbymanufacturing imposed coupling. maximum theoretical the achieves that parameterization, and optimization layout,to create initial a uses design that described is couplers LED Optical Res. Associates, USA. A design procedure for Design of an Optimal LED , Coupler FWR6 •3:15p.m. 2 Fry Integrating Cavity Integrating an in Spectroscopy Absorption Ring-Down FWR5 •3:00p.m. Dept. of Physics and Astronomy, Stephen F. AustinF.Astronomy, Stephen and Physics of Dept. 1 , Joseph A. Musser A. Joseph , California , Michael T. Cone T. Michael 2 ; 1 Texas A&M Univ., USA, USA, Univ., A&M Texas Anurag Gupta; 1 , Edward S. S. Edward , Wednesday, October 14 95 Hillsborough - LS in type-II monolithic matching , Waveguides Reflection Bragg As Piedmont -2 1-x cm Ga -1 x %W We report the observation of second-har 4 LSWH • Second-Order Nonlinear Nonlinear LSWH • Second-Order Optics III—Continued Payam Abolghasem, Junbo Han, Bhavin J. of Toronto, Bijlani,S. Univ. Amr Helmy; Arjmand, Arghavan Canada. monic generation with a conversion efficiency of 1.14x10 LSWH4 • 3:00 p.m. LSWH4 • 3:00 inEfficiency Conversion Second-Harmonic Record Al Improved layer-enhanced layer-enhanced Bragg reflection waveguides for a 2 power. 3.3 mW average with pump picosecond For Fall Congress presentations on Wednesday, see pages 125-131. pages see Wednesday, on presentations Congress Fall For Gary October 11–15, 2009 Efforts Efforts in our • Invited NOTES Sacramento Imperial Ballroom, Fairmont Hotel Fairmont Ballroom, Coffee Break/Exhibits, Imperial LSWG • Ultrafast LSWG • Ultrafast I—Continued Spectroscopy LSWG5 • 3:00 p.m. LSWG5 • 3:00 Ultrafast Ultrafast Hybrid Plasmonics: New Routes to , EnergyPropagation and Imaging Nanoscale USA. Lab, Natl. Argonne Wiederrecht; group for the imaging and ultrafast spectroscopy of hybrid plasmonic nanostructures are discussed, specifically applied to plasmonic continuum spec - troscopy, metal nanoparticle photoluminescence, coupled from arise that states optical unique the and nanostructures. FiO/LS/AO/AIOM/COSI/LM/SRS 2009 3:30 p.m.–4:00 p.m. Atherton Jingjing Jingjing Li, David Fattal, Zhiyong Li; FWT • Plasmonic Sensors— FWT • Plasmonic Continued FWT6 • 3:00 p.m. SERS for Structures Plasmonic/Dielectric Periodic , Applications rational a discuss We USA. Lab, Res. Hewlett-Packard localthe electromagnetic amplifying designtowards antennas optical plasmonic integrating by filed (EM) with periodic dielectric structures. The radiation process of an excited molecule on such devices is also studied.
, 1 FiO Univ. Univ. 1 ; 1 Carlos López- Carlos Allard Mosk P. , Johanna , M. Johanna van den 1 , Vinod Subramaniam Vinod , FOM Inst. AMOLF, Netherlands. AMOLF, Inst. FOM 1,2 2 Glen Ellen Glen , Yanina Cesa , Yanina 1 , Willem L. Vos L. Willem , 1 ______FWS6 • 3:15 p.m. Manipulating by Proteins Fluorescent Controlling , States Photonic of LocalDensity the FWS5 • 3:00 p.m. FWS5 • 3:00 , Hydrosomes of Manipulation Optical present We USA. NIST, Helmerson; Kristian Mariscal, a novel implementation of optical tweezers and production controlled the for allow that microfluidics in droplets water monodisperse of manipulation and - hydrosomes. phase immiscible an FWS • Optical Trapping and FWS • Optical II—Continued Micromanipulation Twente, Netherlands, Netherlands, Twente, Christian Blum Broek We demonstrate nanophotonic control demonstrate of nanophotonic We the - emis sion rate of fluorescent proteins by variation of the variations strong observed The states. of density local of theallow us rate emission to determine the - emis moment. dipole sion Wednesday, October 14 96 Taco D. Visser Vortex Beam Vortex Coherent Partially a in Singularities of Evolution FWU2 •4:15p.m. Rochester,USA, analogy between coherence between analogy and polarization. close a reveals vibrations light between similarity statistical of notion the that shown be will It USA. Polarization, Light of tions and Its Role in the Theories of Coherence and The Concept of Statistical Similarity of Light Vibra- FWU3 •4:30p.m. are found to develop. propagation. At the same time coherence singularities with a phase singularity that gradually disappears on of singularities in a vortex beam. The beam starts off evolution the Technology,studyWe Netherlands.of Agrawal Coupling of Stochastic Electromagnetic Beams Beams Fibers, Optical into Electromagnetic Stochastic of Coupling FWU1 •4:00p.m. USA, Presider Jason Fleischer;Princeton Univ., Fundamental OpticsII FWU •Coherenceand 4:00 p.m.–5:30p.m. confirm this result. this confirm coherent. We cite completelyexperiments spatially with laser modes be which not may beams light matic monochro- belief, common to contrary that, show Mayukh Lahiri, Emil Wolf; Univ. of Rochester, We USA. matic Electromagnetic Beams and of Laser Modes, Monochro- of Properties Coherence Spatial FWU4 •4:45p.m. illustrate result the with anumerical example. tromagnetic beam is coupled into an optical fiber. We is derived for the case when a partially coherent - elec USA. A general expression for the coupling efficiency 1,2 ; 1 Dept. of Physics and Astronomy,Physicsand of Dept. Univ. of , 1,2 Thomasvan Dijk ; 1 2 Free Univ., Netherlands, Inst. of Optics, Univ. of Rochester, of Univ. Optics, of Inst. Empire MohamedF.Salem EmilWolf; Univ. Rochester,of 1 , Hugo, F. Schouten 1 2 , Govind P.Govind , Delft Univ. FiO 1 , write processes. (Slow and Fast Light, 2009) exploit dynamic tuning of slow-light media for read/ realizing ultimate slow-light waveguides. Second, we for nanocavities coupled of applicability study we in photonic crystals for manipulating slow light. First, Labs, Japan. Tanabe, E. Kuramochi, H. Taniyama; Basic Res. NTT Arrays, Coupled Their and ties Manipulating Slow Light by Q Ultrahigh- Häusler Meter, to Nanometer from Metrology 3-D- Interferometry: Challenges Deflectometry S. Peterhänsel S. Presider Michael Duncan; NRL,USA, Highlights II FWV •OSATopical Meeting 4:00 p.m.–5:30p.m. FWV2 •4:30p.m. Three-Dimensional Imaging, 2009) and Holography (Digital applications. unexpected and sensors new enable scalability- andsimplicity, -incoherence, source encoding, high dynamical range, point of view. The intrinsic features of deflectometry theoretical information the from physicist’sand Germany. Erlangen-Nuremberg,Germany, FWV1 •4:00p.m. 1,2 , M. C. Knauer C. M. , We will discuss deflectometry from the from deflectometry discuss will We We investigate Q ultrahigh- nanocavities 1 , C. KranitzkyC. , Crystal Invited Invited 1 , C. Faber C. , FiO/LS/AO/AIOM/COSI/LM/SRS 2009 1 , K. Veit K. , MasayaNotomi, T. 2 3D-Shape GmbH, GmbH, 3D-Shape 1 , C. Richter C. , 2 Nanocavi ; 1 Univ. of of Univ. Gerd Gerd 1 - , possible applications. tangled polarization/spatial-mode states-and discuss en- ofexample-remotepreparation oneWe present metrology.and communicationquantum in bilities capa- new (“hyperentangled”),enabling freedom of may be simultaneously entangled in multiple degrees bridge Res. Lab, UK, Metrology Hyperentangled Photons for Communication and Austria. Andrew J. Shields J. Andrew TadanagaOsamu linoisat Urbana-Champaign, USA, Japan, USA, Presider Warren Grice; Oak Ridge Natl. Lab, and MeasurementIV JWE •EntanglementGeneration 4:00 p.m.–6:00p.m. Ichi Harada Ichi over 200kilometers of optical fiber. long distance and efficient entanglement distribution photodiodes have successfully been applied to ultra- andlow-costself-differencing InGaAscal avalanche eavesdropper’s error probability must 0.28. exceed Takesue , Photodiodes Avalanche InGaAs UsingSelf-Differencing Fiber Kilometers 200 over Distribution Entanglement Efficient JWE2 •4:30p.m. probability10 than less error with fiber low-loss of km 50 overMbit/s 50 at illumination permits Alice and Bob to communicate Illumination, Quantum with Eavesdropping Passive Defeating JWE3 •4:45p.m. JWE1 •4:00p.m. 3 NTT NTT Photonics Labs, NTT Corp., Japan. - Practi 2
Photons from spontaneous downconversion , Zhiliang YuanZhiliang , , 2 Paul Kwiat Paul , Toshimori, Honjo Jeffrey H. Shapiro; MIT, USA. Quantum 1 3 ; , Yoshiki, Nishida JOINT 1 2 Toshiba Res. Europe Ltd., Cam- Ltd., EuropeToshiba Res. NTT NTT Basic Res. Labs, NTT Corp., Gold 1 -6 , Julio, Barreiro 1 while the optimum the passive while , Andrew W.Sharpe Andrew , Invited James F. Dynes F. James 2 , HidehikoKamada, 3 2 , Masaki AsobeMasaki , Univ.Innsbruck, • 1,2 ; 1 Univ.of Il - October 11–15,2009 1 , Hiroki Hiroki , 1 , Ken- , 3 2 , , For Fall Congress presentations onWednesday, seepages125-131. FWW1 •4:00p.m. design tasks is pointeddesign out. tion are obtained and their application in analysis and output relationships for this phase-space representa- input/ The systems. optical 1st-order of description Radon-Wigner transform is presented as a tool for the València,Spain. Univ.de Furlan; Walter D. Systems, Optical First-Order to The Radon-Wigner Transform and Its Application odic , Signals Peri- Other and Sampled Cross-TermsWignerin T. Sheridan Univ. of Rochester, USA,Presider Miguel A.Alonso; Inst. of Optics, 21 forthe Optical SystemTheory FWW •PhaseSpaceOptics— 4:00 p.m.–5:30p.m. analytic results for Gaussian signals. present and signal a such of function distribution Wigner-Ville the in replicas periodic the between in frequency. We examine the cross-terms that occur lege Dublin, Ireland. FWW2 •4:30p.m. st Century II Century 2 ; 1 William T. Rhodes Florida Atlantic Univ., USA, A sampled wave field is periodic Valley Invited Invited 1 , John J. Healy Genaro Saavedra, Genaro 2 Univ. Col- 2 , John The The FiO Haubrich , Ophthalmoscope Miniaturization of Adaptive Optics Scanning Laser scanning laser ophthalmoscope.scanning laser present the design and results from a MEM-based AO and demonstrate robust and compact systems. We will design to isophthalmoscopy for systems optics tive An important step to facilitate dissemination of adap- Kaccie Y. LiY.Kaccie of Physics,TexasUniv.,of A&M USA, other components under study. fabrication of photonic crystal structures and discuss the GHz/THz range. We will report on our successful fabrication suitable for producing volumetric optics in nowis typingcapable technology ofhigh-resolution Michael E. Gehm; Univ. proto of Arizona, USA. Rapid Rapid Prototyping via Optics VolumetricGHz/THz of Fabrication FWX2 •4:30p.m. Berkeley, USA, USA, Presider Arthur Gmitro; Univ. of Arizona, in EmergingTechnologies II FWX •NovelOpticalArchitectures 4:00 p.m.–5:30p.m. the requisitethe resolution. functions. It is suitable for phase arbitrary for waters natural of coefficient ing instrumentation to directly measure the backscatter We present the ocean optics community with the first Univ.,Astronomy,StateF.USA. AustinandStephen FWX1 •4:00p.m. Coefficient b Coefficient Backscattering the Measure to Instrument An FWX3 •4:45p.m. 1 , Edward S. Fry EdwardS. , 1 , YuhuaZhang , b for Arbitrary Phase Functions, 2 Univ. of Alabama, Birmingham, USA. California
, Austin Roorda Austin Wei-Ren Ng, Ziran Wu, Hao Xin, 1 Invited in situ in , Joseph A. MusserJosephA. , 2 ; 1 Univ. of California at California Univ.of applications and has 1 , David Merino David , 2 Dept. of Physicsof Dept. 2 ; 1 David David Dept. 1 - - , Wednesday, October 14 97 , , - 1 1 Don , Anna , Anna 1 . Here we we . Here Stephen A.
Univ. Laval, 1 , Cong Deng 1 ; in vivo 1 Guelph Waterloo Waterloo Guelph 3 , Simon Thibault 2,3 Indiana Univ., USA, Univ., Indiana Ultrahigh resolution resolution Ultrahigh 1 ; 1 Adaptive optics imaging imaging optics Adaptive , Ermanno F. Borra F. , Ermanno Invited Invited 1 , Weiyao , Zou Weiyao 1 Fairfield Inc., USA. Inc., , Xiaofeng Qi , Xiaofeng 2 , Azadeh Naderian 1 , Melanie , C. Melanie Campbell 1 Univ. of Waterloo, Canada, Canada, Waterloo, of Univ. Sciences Denis Brousseau 2 JOINT FiO/AO JOINT , , Zhangyi Zhong 1 Physical of the retina presents unusual design challenges. AO AO challenges. design unusual presents retina the of the across beam the of steering allowing instruments retina, large amounts of defocus, and variable pupil sizes will be discussed. Burns Physics Physics Inst., present Canada. a We novel ferrofluid mirror design which will result in an inexpensive adaptive optics element with large stroke for use in imaging. ophthalmic JWF3 • 4:45 p.m. Canada, M. Ritcey 4:00 p.m.–5:30 p.m. 4:00 p.m.–5:30 in Adaptive Optics JWF • Advances II the Living Retina Imaging of of College Medical Rha; Jungtae USA, Presider Wisconsin, 2 Julie Julie Drapeau JWF2 • 4:30 p.m. - Appli Science Vision for Mirror Ferrofluid New A cations JWF1 • 4:00 p.m. Daniel Ferguson , Retina the of Imaging Optics-OCT Adaptive USA. Univ., Indiana Miller; T. ald OCT with adaptive optics provides unprecedented theretina of cellular 3-D resolution the utility of thisinvestigate imaging for instrument individual retinal nerve fiber bundles, retinal - capil photoreceptors. laries, and Adaptive Adaptive Optics , Instrumentation - Yan-yan Yan-yan Quantita Invited Invited Taka-aki Ishibashi; Hiroshima Ishibashi; Hiroshima Taka-aki
Piedmont Vibrationally-electronically Vibrationally-electronically doubly- LSWK1 • 4:00 p.m. 4:00 p.m.–5:45 p.m. 4:00 p.m.–5:45 Nonlinear LSWK • Second-Order Optics IV British of Univ. Chou; Chang Keng USA, Presider Columbia, LSWK2 • 4:30 p.m. Xu, Xu, Feng Wei, Guo, Yuan Hongfei Inst. Wang; of China. Sciences, of Acad. Chinese Chemistry, of degree and states enantiomer on measurement tive achieved be can surfaces chiral of (DCE) excess chiral in surface second order nonlinear spectroscopy. sum- and harmonic second with given are Examples frequency surface studies. Measurement of Surface ChiralityMeasurement with Nonlinear Spectroscopy: A Quantitative , Approach Vibrationally-Electronically Doubly-Resonant Sum-Frequency Generation Spectroscopy of - Mo lecular Thin Films, Japan. Univ., resonant sum-frequency generation (DR-SFG) is a powerful technique for studying structures of enhances resonance Electronic films. thin molecular the sensitivity and selectivity. Our instrumentation spectroscopy will of DR-SFG and some applications be presented. For Fall Congress presentations on Wednesday, see pages 125-131. pages see Wednesday, on presentations Congress Fall For LS ; - 1,2 Ul October 11–15, 2009 Peter Peter Baum
• Invited Invited Sacramento Recent developments in ultrafast laser- Recent developments
Bert Koopmans; Eindhoven Univ. of Technology, Bert of Koopmans; Eindhoven Univ. Technology, Max-Planck-Inst. of Quantum Optics, Germany, Germany. München, Ludwig-Maximilians-Univ. LSWJ2 • 4:30 p.m. trashort electron pulses allow visualizing atomic-scale atomic-scale visualizing allow pulses electron trashort We time. and space of dimensions four all in motions phase- ultrafast during pathways structural on report transformations and present concepts for reaching motion. electron attosecond of the domain into 1 2 4:00 p.m.–6:15 p.m. 4:00 p.m.–6:15 Spectroscopy II LSWJ • Ultrafast Pittsburgh, of Univ. Petek; Hrvoje USA, Presider LSWJ1 • 4:00 p.m. Visualization Visualization of Nuclear and Electron Motion by Ultrafast Electron Diffraction, Ultrafast Laser-Induced Magnetization Dynam- ics, Netherlands. induced magnetization dynamics will be presented. Particular emphasis will be on efforts aiming processes, at microscopic a of understanding fundamental in espe- transfer momentum spin laser-induced and multilayers. magnetic cially engineered Sasan Fathpour; FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Invited Payam Alipour, Ehsan Shah Alipour, Payam Harvesting Harvesting the optical energy Atherton FWZ2 • 4:30 p.m. Athermal Operation in Polymer-Clad Silicon Microdisk , Resonators Hosseini, Ali Asghar Babak Eftekhar, Momeni, Ali Adibi; Georgia USA. Tech, A method for thermal- stabilization of silicon microdisk resonators, based Two proposed. is coatings, polymer thermo-optic on stability thermal in improvement magnitude of orders - chal fabrication major and Q on Effectsobserved. is discussed. are lenges FWZ3 • 4:45 p.m. Maximization of Phase and Group Birefringence of Single-Mode , - param Silicon-on-Insulator The Waveguides Kuwait. Univ., Kuwait Ramadan; A. Tarek optimized are waveguides silicon-on-insulator of eters for maximum phase and group birefringence under are designs strip-loaded Two condition. single-mode 1.03 of birefringence group and phase with reported 1.64, respectively. and 4:00 p.m.–5:30 p.m. 4:00 p.m.–5:30 Photonics III FWZ • Silicon USA, Corp., Intel Paniccia; Mario Presider FWZ1 • 4:00 p.m. CREOL, CREOL, College of Optics and Photonics, of Univ. Florida, USA. Central photonic integrated in absorption two-photon to lost devices offers two advantages: reduced optical loss and simultaneous electrical power generation. This nonlinear photovoltaic effect may pave the path photonics. integrated green towards Green Green Integrated Photonics, FiO Arthur Mechanical Mechanical Roberta Zambrini; IFISC Zambrini; Roberta
Invited Glen Ellen Glen FWY2 • 4:30 p.m. Brownian Vortex Induced by Optical , Tweezers Bo Sun, David Grosberg, Alexander Grier; New York non-conservative overlooked Previously USA. Univ., force exerted by optical tweezers drives a trapped continuously When vortex. a Brownian particle into vortex Brownian the temperature, or power changing flux. its reverse FWY3 • 4:45 p.m. Modes Gallery Whispering to Coupling Integrated , Platform Microfluidic a in Microspheres of Nitkowski, Nitkowski, Michal Lipson; Cornell USA. Univ., We of whispering excitation gallerydemonstrate modes with trapping optical using microspheres dielectric in measured are Resonances waveguides. nitride silicon from waveguide transmission thus providing an integrated platform for using microspheres in lab- applications. biosensing on-a-chip FWY1 • 4:00 p.m. 4:00 p.m.–5:30 p.m. 4:00 p.m.–5:30 Trapping and FWY • Optical III Micromanipulation Univ., Harvard Crozier; B. Kenneth USA, Presider (UIB-CSIC), Univ. (UIB-CSIC), Illes Univ. Balears, Spain. properties of beams resulting from superposition and of modesinterference different are studied. Lo- multimode such of momenta angular and energycal propose some beams experiments can be tuned. We scheme. measurement interferometric an and , Action in Light Multimode Wednesday, October 14 98 Lossy Lossy Spheroidal Particle , a by Beam Laser Shifted Focused a of Scattering FWU6 •5:15p.m. intensities are illustrated. sorption and beam shift effects on angular scattering Ab- methods. spectrum waves plane and T-matrix with an arbitrary laser beam are calculated using the illuminated particles spheroidal elongated of sities Univ., Egypt, Hany L. Ibrahim in the farin the zone and realizability the condition. mations.results includeOur polarization properties light sources beyond the scalar and paraxial approxi- secondary partially-coherent for model a sources, quasihomogeneousof ties isotropic electromagnetic James; Univ. of Toronto, Canada. We study the proper Sources, tromagnetic - Elec Isotropic Quasihomogeneous of Properties FWU5 •5:00p.m. Fundamental OpticsII—Continued FWU •Coherenceand 2 Telecom Egypt, Egypt. Scattering inten- 2 ; 1 Electrical Engineering Dept., Assiut Dept., Engineering Electrical Empire Asma Al-Qasimi,AsmaDanielF. V. Elsayed Esam M. Khaled 6:30 p.m.–8:00p.m. FiO 1 - , Highlights II—Continued FWV •OSATopical Meeting General Hospital, USA) Massachusetts and SchoolMedical Harvard Bouma; by presented originally 2009; Microscopy, in epithelial and endothelial surfaces. (Novel Techniques organ entire of imaging diagnostic high-resolution of possibility the open and speeds imaging faster dramatically enabled have tomography coherence illuminationandstrategiesfor detectionopticaland Hospital, General USA. Massachusetts Bouma; E. Brett Implications, Clinical and Advances Recent OCT: Invasive Minimally Field, Wide FWV3 •5:00p.m. Recentadvances minimally-invasivein probes FiO Postdeadline Paper Sessions,Seethe Postdeadline Papers Book in your registration bag for times exact and locations Crystal Invited FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Ben Vakoc, Ben Brett Brett indistinguishable single photons. generate and dots quantum excite coherently to photon absorption and emission are efficient methods two- cavity-assisted that showWe cavities. crystal photonicto coupled quantumdots in enhancement rate transition two-photon presentWe Univ., USA. , Science tion Applicationsand tumDots QuantumtoInforma - Two-PhotonCavity-Enhanced Processes in - Quan JWE5 •5:30p.m. and MeasurementIV—Continued JWE •EntanglementGeneration promising for quantum feedback. effect and we reconstruct the field’s state. This tool is in a cavity. We evidence quantum jumps of light, Zeno Non Demolition measurement of the photon number France.Supérieure,Normale Haroche;École S. Brune, M. Gleyzes, S. Dotsenko, I. Cavity Quantum Field State Control and Measurement in a common bath and squeezed decoherence. the a in qubits two of entanglement the of revival and Chile. We study the relation between the sudden death dez, Miguel Orszag; Pontificia Univ. Católica de Chile, in a Common , Squeezed Reservoir Decoherence and Disentanglement for Two Qubits JWE6 •5:45p.m. JWE4 •5:00p.m. ,
J. M. Raimond, S. Deléglise, C. Sayrin, X. Zhou, Ziliang Lin, Jelena Vučković; StanfordVučković;Jelena Lin, Ziliang JOINT Gold Invited We realize a Quantum a Werealize Maritza Hernan - • October 11–15,2009 For Fall Congress presentations onWednesday, seepages125-131. Abramochkin Design of Rotatingof Beams, Design FWW3 •5:00p.m. 2 Federation. is proposed. systems optical isotropic propagationthrough their beams anisotropically rotating in phase space during formalism, a simple method for generation of paraxial 21 forthe Optical SystemTheory FWW •PhaseSpaceOptics— PN Lebedev Physical Inst., Samara Branch, RussianBranch,Samara Inst., Physical Lebedev PN st Century II—Continued Century
Based on the ray transformation matrixtransformation ray the on Based 2 ; 1 Univ. Complutense de Madrid, Spain, Valley Invited TatianaAlieva 1 , Eugeny, FiO Continued in EmergingTechnologies II— FWX •NovelOpticalArchitectures of numerical modeling of CBG. results the confirming found, is reflection of phase and amplitude for expression Analytic (CBG). ings Grat- Bragg Chirped by coupledpropagatingwaves counter- for equations the of solutions study and Sarper Ozharar Sarper Mandridis Dimitrios Mokhov VolumeGratingBragg , Analytic Theory of Light Reflection from a Chirped FWX5 •5:15p.m. is demonstrated. rangedynamic 30dB with 4.65km of range a at tion resolu- sub-millimeter with measurementsresolved range for scheme heterodyne modulation phase a employing system lidar pulsed chirped frequency Central Florida, USA, Florida, Central 1 of Optics and Photonics, Univ. of Central Florida, Florida, USA, Central of Univ. Photonics, and Optics of , Pulses Chirped Frequency Stretched,Temporally Using Sub-Millimeter Resolution Resolved, Range Lidar FWX4 •5:00p.m. CREOL, College of Optics and Photonics, Univ.of Photonics, and Optics of College CREOL, 2 Radiance, Inc., USA. Inc.,Radiance,
1 Mohammad Umar Piracha Umar Mohammad , Vadim I. Smirnov I. Vadim , 1 , Peter J. Delfyett J. Peter , California 1 , , Ibrahim Ozdur 2 Wepresent USA. OptiGrate, LeonidGlebovB. A temporally stretched, temporally A 2 , Boris Ya. ZeldovichYa. Boris , 1 ; 1 CREOL, College CREOL, 1 1 , Dat Nguyen Dat , , Tolga Yilmaz 1 , Sergiy V.Sergiy , 1 1 2 ; , , Wednesday, October 14 99 , ; 2 1 , , David R. Williams 2 Ctr. Ctr. de en Investigaciones , Armando Gómez-Vieyra Armando , 2 1 Expressions Expressions for minimal - astig Fairfield AlfredoDubra
JOINT FiO/AO JOINT Univ. of Univ. USA, Rochester, JWF • Advances in Adaptive Optics in Adaptive Optics JWF • Advances II— the Living Retina Imaging of Continued 1 JWF4 • 5:15 p.m. First-Order Design of Off-Axis Reflective Oph- thalmic Adaptive Optics Systems Using Afocal , Telescopes Daniel Malacara-Hernández Optica Optica AC, Mexico. matism in image and planes pupil in off-axis reflec- tive afocal telescopes formed by pairs of spherical angles small for evaluated and presented are mirrors incidence. of , , - 1 1 MIT, MIT, 2 Sergey Sergey , Gevorg 2 Spectralus Spectralus 2 , Greg Nemet 1 , Colin J. R. - Shep Andrei Andrei Shchegrov 2 , Hakob Danielyan 2 , Stepan Essaian Piedmont , Peter T. C. So 1 1 Spectralus Spectralus Corp., USA, 1 ; 2 has been has experimentally achieved. 2 Natl. Univ. Natl. of Univ. Singapore, Singapore, 1 ; 1 LSWK • Second-Order Nonlinear Nonlinear LSWK • Second-Order Optics IV—Continued Mironov, Mironov, Vladimir Lozhkarev, Vladislav Ginzburg, Efim Khazanov; Inst. of Applied energy Physics, 60% Russian The Federation. Russian Sciences, of Acad. generation harmonic second of efficiency conversion process in 1mm KDP crystal peak at input intensity 0.6TW/cm LSWK3 • 5:00 p.m. LSWK3 • 5:00 Highly Efficient Second Harmonic Generation of Super Strong Femtosecond Laser Pulses, We present a CJSC, microchip We green Armenia. laser architecture This crystal. PPMgOLN on based source power output for 12% of efficiency wall-plug achieves levels of 50-150mW and fits into a small package pico-projectors. for suitable We USA. address We the problem of nonlinear scatter ing ing by scatterers of irregular shapes. Our approach assumes the scatterer to be made up of coupled dipoles which interact among themselves and with field. the incident John John Khaydarov Gabrielyan Suren Suren Soghomonyan pard LSWK4 • 5:15 p.m. Microchip Green Laser Source Based on Second- Harmonic Generation in Periodically Poled, MgO-Doped Lithium , Niobate LSWK5 • 5:30 p.m. Coupled Dipole Model for Nonlinear , Scattering Naveen K. Balla For Fall Congress presentations on Wednesday, see pages 125-131. pages see Wednesday, on presentations Congress Fall For LS We October 11–15, 2009 - Alessan , 1 , David A. A. David , 1 • Lawrence Berkeley Berkeley Lawrence 1 ; 1 Invited Invited , Ferenc Borondics Ferenc , , Michael C. Martin C. Michael , 1 1,2 Univ. of California at Berkeley, USA. Berkeley, at California of Univ. 2 Sacramento We study the coupling between - theexci coupling study We , Robert A. Kaindl A. Robert , Tobias Hertel, Tobias Zipeng Zhu, Dominik 1,2 Hyunyong Choi Hyunyong , Shuyun Zhou Shuyun , Marc Marc Achermann; of Univ. Massachusetts at
1,2 LSWJ • Ultrafast Spectroscopy II— Spectroscopy Ultrafast • LSWJ Continued We report the broadband optical conductivity and ul- and conductivity optical broadband the report We graphene, epitaxial few-layer of dynamics THz trafast revealing electrodynamics consistent with a dense response THz a Dirac and plasma transient electron carriers. hole excess of recombination by dominated LSWJ3 • 5:00 p.m. LSWJ3 • 5:00 Gra- Epitaxial Few-Layer of Studies THz Ultrafast , phene Siegel LSWJ4 • 5:15 p.m. draLanzara LSWJ5 • 5:45 p.m. Natl. Lab, USA, Lab, Natl. Dynamic Signatures of Exciton-Plasmon - Interac tions - in Nanostruc Hybrid Semiconductor-Metal , tures USA. Amherst, semi- of assemblies in (SPs) plasmons surface and tons conductor nanocrystals and metal nanostructures. will We discuss emission dynamics, SP-coupled SP- systems, donor-acceptor in transfer energy mediated enhancements. rate radiative SP-induced and One-Dimensional Exciton Dynamics in Carbon Nanotubes, Germany. Wurzburg, of Univ. Crochet; Jared Stich, discuss femtosecond time-resolved in- pump-probe sorted structurally in dynamics exciton of vestigations aggregates. nanotube carbon and nanotubes carbon Yinying Yinying , Raymond G. - Beau 1 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Univ. of Southern California, California, Southern of Univ. 1 ; 1 , Yang Yue , Yang See the Postdeadline Papers Book in your registration bag for exact times and locations and exact times for bag registration your in Book Papers Postdeadline Sessions, See the Paper FiO Postdeadline 1 Atherton Jeffrey M. Shainline, Gustavo Fernandes, Fernandes, Gustavo M. Jeffrey Shainline, , Lin Zhang 1 We propose a slot waveguide in waveguide slot a propose We USA. Labs, HP 2 , Alan E. Willner E. Alan , 2 FWZ • Silicon Photonics III— FWZ • Silicon Continued soleil FWZ4 • 5:00 p.m. Qual- High with Microdisks Silicon Subwavelength , ity Factors a present We USA. Univ., Brown Xu; Jimmy Liu, Zhijun micro-cavities silicon subwavelength first the of study and to our knowledge the smallest to micro-cavities directly or spectroscopy fiber tapered with probed be a waveguide. to coupled USA, which a sub-core is incorporated into the slot itself. various under waveguide the simulate numerically We exhibit can guided-wave the that show and conditions confinement. two-dimensional highly enhanced FWZ5 • 5:15 p.m. , Sub-Core a Incorporating Waveguide Slot Xiao-Li , 2 FiO David P. P. David 6:30 p.m.–8:00 p.m. , Maurice Whelan Maurice , 2 Stokes Res. Inst., Univ. of Limerick, of Limerick, Univ. Res. Inst., Stokes Glen Ellen Glen 1 ; 1 , Jean-Michel Gineste Jean-Michel , 1 Inst. Inst. for Health and Consumer Protection, 2 FWY4 • 5:00 p.m. , Binding Optical in Polarization of Effects FWY • Optical Trapping and FWY • Optical III—Continued Micromanipulation - Col CREOL, Dogariu; Aristide Sukhov, Sergey Haefner, Florida, Central of Univ. Photonics, and Optics of lege USA. We investigate the influence of incident field particles. bound optically of dynamics on polarization in interaction optical to due torques of existence The - applica and demonstrated is system multi-particle the discussed. are machines nano-rotator to tions Ireland, European European Commission DG Joint Res. Ctr., A Italy. Heterodyne Mac-Zehnder to interferometer extract phase images of cells and demodulation method to retrieve instantaneous frequency of a phase object, undergoing sinusoidal modulation (amplitude-200 nm and frequency-30 Hz and mimicking cell - vibra presented. is tion) David Newport FWY5 • 5:15 p.m. Development of Dynamic Phase Demodulation Technique to Investigate Live-Cell Dynamics, , Heterodyne Using Mach-Zehnder Interferometer Joseph Shiju Thursday, October 15 100 properties of LCLS. source unique the utilizing instrument Imaging X-Ray the Coherentof program scientific the and capabilities the describe will I world. the in laser free-electron X-ray hard first the be will LCLS Univ.,USA. StanfordAcceleratorLab, Natl. SLAC Boutet; LCLS, at Instrument Imaging X-Ray Coherent The putational tasks and some recent progress insolving them. challenge in data processing. We describe for non-experts the com- molecules with X-ray free-electron lasers present an unprecedented Loh; Cornell Univ., USA. Experiments and How Do We Process It? Imaging Single-Molecule in WeExpect Do Data of Kind What LSThA1 •8:00a.m. Stanford Univ., USA,Presider Aymeric Robert; SLAC Natl. Accelerator Lab, LSThA •X-Ray ImagingI 8:00 a.m.–10:00a.m. LSThA2 •8:30a.m. The proposed experiments to image single Empire Invited Invited LS Veit Elser, Duane Ne-Te
Sébastien The The FThA1 •8:00a.m. FThA1 , Light with Nanostructures Sculpting •8:45a.m. FThA2 for extreme the ultraviolet. diffractive optics and zone plates for soft X-rays, and reflective optics optics to form images at or near the diffraction limit. These include Natl.Lab,USA. BerkeleyLawrence Introduction to Diffraction Limited X-Ray Optics, edu/AST/sxreuv and www.coe.berkeley.edu/AST/srms. www.coe.berkeley.at and youtube.com at archived, electronically 2000). His lectures are regularly broadcast live over the Internet and Radiation: Principles and Applications (Cambridge University Press, Optical Society. He is author of The and Society Physical American the ofFellowMember a is He (1985–1988) first Scientific Directorwas of and the Advanced(CXRO), Light Optics Source X-Ray (ALS). for Center the of Director contiguous Lawrence Berkeley National Laboratory, he is founding ment and use of coherent sources at these short wavelengths. At the of novel Fourier optics, image contrast techniques, and the develop - and EUV lithography. He and his students are also active in the use microscopy X-ray soft specific element includeinterest particular range.1-30nm Applicationsultravioletextreme the radiation in of of use short wavelength electromagnetic radiation, X-rays soft and the on center interests research His Committee. Executive its on Technologyserves and andPh.D.programApplied Science the of University of California at sinceBerkeley 1989. He was co-founder at Residence in Professor a been has He 1972. YorkUniversityin New from Physics Applied in Ph.D. his received Attwood David Presider Ian McNulty; Argonne Natl. Lab, USA, •NanofocusingOpticsI FThA 8:00 a.m.–10:00a.m. molecule spatialmolecule resolution with light in3dimensions. the far-field diffraction barrier. We also present approaches to single- nanostructures with long-wavelength photons, effectively breaking USA, 2 We show that it is possible to pattern to possible LumArray,is itWe that USA. Inc.,show FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Tutorial Crystal Soft X-Rays and Extreme Ultraviolet We discuss the ability of X-ray of ability the We discuss Rajesh Menon Rajesh
David Attwood; 1,2 ; 1 MIT, Lei Tian Lei Holography , Digital UsingDistributions Size Wide with Flows Air-WaterMixture High-Density in Measurement Size Bubble •8:00a.m. FThB1 FThB3 •8:30a.m. FThB3 amplitude of light at multiple incident angles of illumination. tissues. The technique and features cells simultaneous live detection in of phase index and refractive of mapping 3-D resolution high Wonshik Choi; MIT, USA. Live Cell Imaging with Field-Based 3-D Microscopy, density air-water mixture flowswithsize distribution. awide of using in-line digital holography to measure bubble sizes in high- Technology (SMART) Ctr., Singapore. We present experimental results Barbastathis Yunlong Sheng; Univ. Laval, Canada, Presider •DiffractiveandHolographicOpticsIII FThB 8:00 a.m.–10:00a.m. micron, respectively. measure the transverse and axial resolution to be below 1.6 and 2.2 microfabricateda zoneplate. Using fluorescentsingle sphere,a we We demonstrate a compact confocal fluorescence microscope using Plate Confocal Fluorescence Microscopy Using a Microfabricated Zone •8:15a.m. FThB2 , Ethan F. Schonbrun, Kenneth B. Crozier; Harvard Univ., USA. • 1 , Nick Loomis Nick , 1,2 ; October 11–15,2009 1 MIT, USA, MIT, 1 , Jose A. Dominguez-Caballero A. Jose , We report field-based 3-D microscopy for Invited For Fall Congress presentations onThursday, seepages132-136. 2 FiO Singapore-MIT Alliance for Res. and Res. for AllianceSingapore-MIT Gold
Michael Feld, 1 , George , crospheres around the aroundcrospheres Mi- in Modes Gallery Whispering ofTuning Thermo-Optical •8:30a.m. FThC2 FThC1 •8:00a.m. FThC1 retical model areretical model agreement ingood withdata. experimental coupled disc microresonators the results of rigorous universal - theo to their potential applications and unique optical characteristics. For Germany. Practical applicationsPractical of resonators these are discussed. developmentfuture the field. trendsthe in on the of speculateand resonators, mode gallery whispering crystalline ultra-high-Q in USA. Inc.,OEwaves, Seidel; David Ilchenko, S. Savchenkov,Vladimir A. vances and Future Trends, Ad- Recent Resonators: Mode Gallery Whispering Crystalline USA, Carsten Schmidt Carsten Spectral Characteristics of Coupled Silica Disc Micro Resonators , •8:45a.m. FThC3 is of interest for cavity-QED experiments. 1 1 Presider to Announced Be •Micro-CavityDevicesI FThC 8:00 a.m.–10:00a.m. ing transition of gallery modes in microspheres and demonstrate tuning to the - cool ofTechnology, Ireland. We present for method tuninga whispering Ernst-Bernhard Kley Ernst-Bernhard Chormaic Nic Sile Univ.College Cork, Ireland, Friedrich-Schiller-Univ.Germany,Jena, 3 Wephenomena opticalof recently variety observed a review Fraunhofer Inst. for Applied Optics and Precision Engineering, Coupled optical microresonators are of great interest due 1 , , Arkadi Chipouline 85 Rb. The tuning method can be used in UHV and 1,2 , Jonathan M. WardM. Jonathan , 1 , Andreas TünnermannAndreas , 85 Rb Cooling Transition Cooling , Rb Invited
Lute Maleki, Andrey B. Matsko, Anatoliy Valley 2 TyndallNatl. Inst., Ireland, 1 , Thomas Käsebier 2,3 2 , Michael J. Morrissey J.Michael , Queens College, CUNY, College, Queens 1,3 , Thomas Pertsch Thomas , Laura Russell Laura 1 , Lev Deych Lev , 3 CorkInst. ,2,3 1,2 1 2 ; , ; , Thursday, October 15 101 - Univ. of 3 , Russell A. 2 Latest developments developments Latest , David M. Shemo JDS Uniphase, USA, 1 2 FiO Invited Invited Sacramento Scott Scott McEldowney We We present photo-aligned liquid crystal polymer Microsoft Microsoft Corp., USA, 1 Qiwen Zhan; Univ. of Dayton, USA. Dayton, of Univ. Zhan; Qiwen
; 3 8:00 a.m.–10:00 a.m. 8:00 a.m.–10:00 FThF Birefringence in and • Polarization I Optical Design USA, Arizona, of Univ. Chipman; Russell Presider Chipman FThF2 • 8:30 a.m. of spatial polarization engineering that can benefit optical imaging imaging optical benefit can that engineering polarization spatial of - opti variant spatially of Applications presented. are instrumentation cal polarization in nonlinear optical imaging, plasmonic focusing will be discussed. control focal fieldand 3-D polarization - Po Engineered Spatially with Instrumentation Imaging Optical , larization Photoaligned Liquid Crystal Polar Polymers for Space Variant ization , Control Arizona, Arizona, USA. devices for creating space variant polarization control. We dem- polarization random and systematic creating components onstrate orientation profiles. Theoretical and experimental properties of presented. are speckle control and retarders vortex FThF1 • 8:00 a.m. ; 1,2,4,5 , Michael , J. Michael 1,2 , Manuel F. Juette F. Manuel , 2,3,4,5 Keith Berland, David G. Lynn, Lynn, G. David Berland, Keith Inst. for Molecular Biophysics, Biophysics, Molecular for Inst. Joerg Joerg Bewersdorf
2 Nucleation and growth mechanisms mechanisms growth and Nucleation LS Invited Invited For Fall Congress presentations on Thursday, see pages 132-135. Congress presentations on Thursday, For Fall Atherton Dept. Dept. of Physics and of Univ. Astronomy, Particle localization at the nanometer scale nanometer the at localization Particle 3 , Stefanie E. K. Kirschbaum K. E. Stefanie , Dept. Dept. of Biophysical Chemistry, of Univ. Heidelberg, October 11–15, 2009 4 1,2 Dept. of New Materials and Biosystems, Max-Planck-Inst. Max-Planck-Inst. Biosystems, and Materials New of Dept. 5 • Yale Univ. School of Medicine, USA, Medicine, of School Univ. Yale Germany. Res., Metals for super- localization-based and tracking particle in role central a plays performance experimental the compare We microscopy. resolution Additionally, methods. localization (3-D) three-dimensional two of proteins. fluorescent photoactivatable different characterize we Germany, Germany, 1 8:00 a.m.–10:00 a.m. 8:00 a.m.–10:00 III Biophysics LSThB • Single-Molecule at Carolina North of Univ. Fecko; Chris Presider USA, Hill, Chapel Mlodzianoski LSThB1 • 8:00 a.m. The The Jackson Lab, USA, Maine, Maine, USA, Investigating Investigating Amyloid Nucleation and Growth Using Single , Microscopy Fluorescence Molecule USA. Univ., Emory Liang; Yan fluorescence molecule single using resolved are materials amyloid in molten intermolecular an identify Results spectroscopy. and imaging pathway. the nucleation of intermediate a key as state globule 3-D Localization in Fluorescence Photoactivation Localization Microscopy and , Particle Tracking LSThB2 • 8:30 a.m. , , , , 1 2 2 2 , Tobin Tobin , 2 Dept. of of Dept. , Boyang Boyang , 1 1 HP Labs, ; 2 4 Lin Zhang , Jun Liu 2 Technical Univ. of Univ. Technical 1 , Fang Ou 1 ; 1 , Hiroshi Takahashi 1 , Raluca Dinu Raluca , Fei Yi Fei 4 , Raymond G. Beausoleil 1 , Lars Hagedorn Frandsen 1 , Yiliang Wang Yiliang , 1 Graduate School of Science School and Graduate 1 ; , Dan Jin Dan , 1 Koichi Kato 3 NTT Photonics Labs, NTT Corp., 2 , Jian Wang 1 , Jørn Märcher Hvam Märcher Jørn , 1 Minhao Minhao Pu Glen Ellen Glen
, , Alex Jen Alex , 3 We demonstrate a mi- a demonstrate We Denmark. A/S, Koheras , Seng-Tiong Ho Seng-Tiong , 2 1 Univ. of Univ. Southern California, USA, 1 ; ; , Hiroyuki Tsuda , Hiroyuki 1 2 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 , Kresten Yvind Kresten , 1 , Yinying , Xiao-Li Yinying 1 , Jingdong Luo Jingdong , 2 Dept. Dept. of Chemistry, Material Res. Ctr., Northwestern Univ., We report a new promising voltage-size voltage-size promising new a report We USA. Corp., Lumera We have We proposed an all-order waveguide-type dispersion Dept. of Material Science and Engineering, Univ. of Washington, Washington, of Univ. Engineering, and Science Material of Dept. 2 4 3 , Yingyan Huang Yingyan , 1 Seiji Fukushima Haiyan Ou Haiyan Yue Yang Alan E. Willner croring resonator working at TM mode integrated with nano-taper nano-taper with integrated mode TM at working resonator croring loss insertion measured The loss. insertion total 3.6dB with couplers mode. TM 1.3dB for only was coupler the nano-taper of USA, J. Marks J. Liu performance record (0.6V-cm) of the organic EO modulator using using modulator EO theorganic of (0.6V-cm) record performance conducting transparent oxides as the bridge electrodes. The - com theoretical prehensive analysis predicts large electrical bandwidth achievable. is (>40GHz) 8:00 a.m.–10:00 a.m. 8:00 a.m.–10:00 FThE Optics • Integrated USA, Colorado, of Univ. C. Sullivan; Amy Presider Denmark, Denmark, Technology, Keio Japan, Technology, Univ., FThE4 • 8:45 a.m. All-Order Dispersion Waveguide-Type Compensator Using Arrayed , Waveguide Gratings Japan. method compensation using arrayed waveguide gratings (AWGs). We have estimated the dispersion compensation performances for a given diffraction order and number of arrayed waveguides in each AWG. USA. We show dispersion-flattened silicon slot waveguides with high nonlinearity for on-chip signal-processing applications, which exhibits a flat near-zero dispersion within ±0.12ps/nm/m to up γ coefficient nonlinear with range wavelength 302-nm a over 1550nm. 4300/m/W at FThE2 • 8:15 a.m. Achieving Uniform Chromatic Dispersion over a - Wide Wave length Range in , Highly Nonlinear Slot Waveguides Electrical Electrical Engineering and Computer Science, Northwestern Univ., USA, USA, FThE3 • 8:30 a.m. Low Ultra with Modulator (EO) Electro-Optic Organic Compact Con- Transparent Using Bandwidth Large and Voltage Switching Electrodes, Bridge (TCO) Oxides ducting FThE1 • 8:00 a.m. Low Insertion Loss SOI Microring Resonator Integrated with Couplers Nano-Taper - FiO Stu 1640W CW high CW 1640W Invited Invited We We have demonstrated the first world’s California Qihong Lou, Jun Zhou, Bin He, Songtao Du; Songtao He, Bin Zhou, Lou, Jun Qihong FThD2 • 8:30 a.m. FThD1 • 8:00 a.m. 8:00 a.m.–10:00 a.m. 8:00 a.m.–10:00 FThD Lasers Fiber • High-Power I Be Announced to Presider , Array Laser MOPA Jankevics, Nd:YAG Combined Andrew Coherently 100-kW Injeyan, Hagop Asman, P. Charles McNaught, J. art Machan, Jason Komine, Hiroshi Jones, C. Gina Johnson, F. M. Adam Jay Marmo, Michael McClellan, Randy Simpson, Jeff Sollee, Marcy M. S. Mark Weber, Valley, Benjamin Weiss; Northrop Grumman Aerospace Systems, USA. 100-kW solid-state laser system with good beam quality. Seven laser are amplifier) chains oscillator-power (master 15-kW MOPA beam. output a single achieve to combined coherently High Power CW and Pulsed and CW Lasers Fiber Claddingwith Double Power High Fiber Made in China, - ob are pulsedoutput rate high150W repetition and output power structure laser The fibers. core multimode China-made with tained in detail. given technology are amplifier pulse and China. Mechanics, Fine and Optics of Inst. Shanghai Thursday, October 15 102 LSThA •X-Ray ImagingI—Continued , Announced Be to Title Anton Barty Phenomena, Nanoscale Ultra-Fast of Snapshots X-Ray Lasers: Electron Free with Imaging Diffraction Dynamic Femtosecond and materials science. of applications in fundamental atomic-physics, ultrafast-chemistry in extraordinary new capabilities in X-ray science, with a wide range pulses offered by a new generation of free-electron lasers is ushering TechnischeUniv.Germany.Berlin, tet Stanford Linear Accelerator Ctr., USA, DESY, Germany, 1 LSThA3 •9:00a.m. Shapiro ence, Univ. Hamburg, Germany, LSThA4 •9:30a.m. Carl Caleman Carl Möller Thomas TschentscherThomas Plönjes Elke Bruce W. Woods of California at Davis, USA, Davis, at California of R. R. N. C. Maia Natl. Lab, USA.Abstract not available. Lawrence Livermore Natl. Lab, USA, 1,3,4 , MatthiasFrank, 5 , KeithHodgsonO., 1 6 , Henry N. Chapman Mro Kuhlmann Marion , 4 4 , Abraham Szöke , Gösta Huldt Gösta , 8 1 , Christoph Bostedt Christoph , 7 , Saša Bajt Spiller X-Ray Optics, USA, 1 6 , StefanP., Hau-Riege , Jochen R. Schneider R. Jochen ,
Stefan Hau-Riege; Lawerence LivermoreLawerenceHau-Riege; Stefan 1 4 3 , W. Henry Benner Empire , Bianca , IwanBianca , David van der Spoelder van David , Invited Invited 1,4 LS 6 3 Deutsches Elektronen-Synchrotron, Elektronen-Synchrotron, Deutsches Stanford Synchrotron Radiation Lab, , Nicusor Timneanu 2 6 , Michael J. Bogan , Rolf TreuschRolf , The ultrafast, ultrabright X-ray ultrabright ultrafast, The 8 2 , Matthias HoenerMatthias , Ctr. for Free Electron Laser - Sci 4 Uppsala Univ., Sweden, 4 , M. Marvin Seibert 8 Inst. für Atomare Physik, 1 , StefanoMarchesini, 1 6 , Richard A. London , Eberhard Spiller Eberhard , 6 , Stefan Düsterer Stefan , 4 , MagnusBergh , 1 4 , Sébastien Bou - , Janos Hajdu 8 , David A. A. David , 4 , Filipe Filipe , 5 Univ. 1,5 3,4 7 4 6 1 ; , , , , , (lens-free) hard X-ray phase-contrast imaging. μm <10 and microscopy zone-plate X-ray soft nm <25 including sources, liquid-jet high-brightness compact on based systems ing Sweden. Skoglund, P. P.Takman,Reinspach, J. Otendal,T. M. Tuohimaa,Nilsson, D. Lundström, U. Lindblom,U. Vogt; Royal Inst. of Technology, Bertilson, E. Chubarova, O. Hemberg, O. v Hofsten, A. Holmberg, M. Laboratory X-Ray Micro- and Nano-Imaging , Singular and Other Novel X-Ray Diffractive Optics, FThA •NanofocusingOpticsI—Continued FThA FThA4 •9:30a.m. FThA4 other imaging capabilities. resolution by enabling phase contrast, extended depth of field, and developed for X-ray microscopy. These optics enhance contrast and USA. nawat;Lawrence Berkeley Natl. Lab, Univ. ofCalifornia at Berkeley, FThA3 •9:00a.m. FThA3 10:00 a.m.–10:30a.m. Singular and other novel X-ray diffractive optics have been been have optics diffractive X-ray novel other and Singular
We summarize recent progress in laboratory X-ray imag- X-ray laboratoryWe progressin recentsummarize FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Invited Invited Crystal Coffee Break,Regency and Imperial Ballroom Foyer, Fairmont Hotel Hans M. Hertz, M. Anne Sakdi - Vasilyeu Generating Superpositions of Higher Order Bessel , Beams •9:30a.m. FThB6 Optics III—Continued •DiffractiveandHolographic FThB Cells Labeled with Gold Nanoparticles, Gold with Labeled Cells Live of Imaging 3-D for Microscopy Holographic Heterodyne •9:00a.m. FThB4 France, Moisan KwaZulu-Natal,Africa,South ment theoretically. calculated with those is presented. The experimentally produced fields are in good agree- Bessel beams by means of a spatial light modulator and ring aperture An experimental setup to generate a superposition of higher-order results are shown. vortex interferometer. Analytical calculation as well as experimental optical on based system optical introduceauthors The presented. transparentforcharacterization ismethod sidewalls of media new Technology, The WroclawPoland.Univ.of Masajada; Jan Leniec, Media, Transparent in Sidewalls of Determination •9:15a.m. FThB5 been investigatedbeen theoretically both and experimentally. pulses. The second harmonic generation of these vortex beams has light modulator (SLM) to produce optical vortices (OVs) with 50 spatial fs crystal liquid a used WehaveUniv., StateUSA. Diego San Shaper, Pulse Programmable a Second Harmonic Generation of Femtosecond Vortex Beams with •9:45a.m. FThB7 Inst.Physics,ofNatl. Belarus, Belarus,Acad.of Sciences of Fadwa Joud of simultaneously. particles sensitivity. Fast acquisition times enable selective localization of tens shot-noiselimitedwith particles, gold 40nm with labeled cells live of imaging 3-D for used is reflection internal total in microscopy holographic HeterodyneFrance. Monod, Jacques Inst. Cellulaire, 3 2 , Gilles TessierGilles , 1 • Lab Kastler Brossel de l’ENS, France, , , Angela Dudley 2 , Philippe Bun Philippe , October 11–15,2009 1 ; 2,3 1 Inst. Langevin, CNRS UMR 7587, ESPCI, 7587, UMR CNRS Langevin,Inst. 3 , N. Khilo , Sarah Suck Sarah , For Fall Congress presentations onThursday, seepages132-136. FiO Gold 3 CSIR Natl. Laser Ctr.,Africa.Natl.South Laser CSIR NicolasCusnir, Matt Anderson;E. 1 , Andrew Forbes Andrew , 1 , Michel Gross Michel , NilanthiWarnasooriya 3 Départment Départment de Biologie 2,3 2 , Maité Coppey- ; 1 B.I. Stepanov 2 Monika Monika Univ.of Ruslan Ruslan 1 , Continued •Micro-CavityDevicesI— FThC Singapore, Singapore, Jena, Germany,Jena, nermann yan Huang yan Absorption-Controlled Resonator for All-Optical Memory, •9:30a.m. FThC5 microring/microdisk photonic based communication devices. tems. We highlight recent advances and future challenges in Q high- Q high- resonance in optical and RF-photonic communication - sys NewMexico,of USA. tion Applications of High-Q Silica/Silicon Disc Micro Resonators, Micro Disc Silica/Silicon Hybrid and Silica in Nonlinearities Electron Free and Thermal •9:45a.m. FThC6 power-efficient memory. all-optical ~100 Gbps is demonstrated, makingapt the device for ofhigh-speed, speed maximum a with along requirement power sub-mW A analysis. semi-analytical a with explored is resonator controlled absorption- an in induced Bistability Univ.,USA. Northwestern Engineering, Germany, Germany, Engineering, less sensitive to optical higher powers. nonlinearresponses promisemicroresonators disc way a design to investigated experimentally and numerically.are resonatorsThe opposite signs of microdisc silca-silicon hybrid and silica in effects Chipouline USA, FThC4 •9:00a.m. FThC4 , Mani Hossein-Zadeh; Ctr. for High Technology Materials, Univ. 2 Data Storage Inst., Agency for Science, TechnologyRes., Science,and for AgencyInst.,Storage Data 1,2 1 , Lev Deych Lev , 1 3 , Thomas Käsebier , Vivek, Krishnamurthy Dept. of Electrical Engineering and Computer Science, Computer and Engineering Electrical of Dept. 2 Fraunhofer Inst. for Applied Optics and Precision and Optics Applied for Inst.Fraunhofer This talk summarizes various applicationsvarioussummarizes talk ofThis 3 , Thomas Pertsch Thomas , Optical Microresonators in - Communica 3 Bistability Bistability USA. CUNY,College, Queens Invited Valley 1 , Ernst-Bernhard Kley 2 , Seng-Tiong, Ho 1 ase Schmidt Carsten ; 1 Friedrich-Schiller-Univ. 3 ; 1 , Andreas Tün- 1 OptoNetInc., 1 , Arkadi , Ying - Thursday, October 15 103 ; - 2 Faculty of Faculty , Ryosuke Katarzyna Katarzyna 3 1 , Roberto - Mo 3 , , Eustace L. Dereniak 2 Kazuhiko Kazuhiko Oka Jing Ma, Michelle Povinelli; Univ. of Univ. Povinelli; Ma, Jing Michelle , Boris A. Malomed 1 FiO Univ. of Univ. Arizona, USA. The imaging , , Darren Miller 2 1 Sacramento , Yoav , Linzon Yoav 1,2 INRS-Énergie INRS-Énergie et Matériaux, du Univ. Québec, Canada, 1 ; 1 , Masayuki Ohnuki 1 Hokkaido Univ., Hokkaido Japan, Univ., Faculty of Physics, Warsaw Univ. of Technology, Poland, Poland, of Technology, Univ. Warsaw of Physics, Faculty randotti FThF4 • 9:15 a.m. Snapshot Imaging Polarimeter for Polychromatic Light Using Savart Plates and Diffractive Lenses , polarimeter polarimeter using the Savart plates is modified for use with polychromatic light the by incorporating an imaging system utilizing visible the for simulated numerical is feasibility Its lenses. diffractive 50nm-bandwidth. with light 2 1 Suda We present Israel. We the Univ., Aviv Engineering, Tel theoretical and experimental of demonstration light collapse in control nonlinear magneto-optical Kerr media. The required management of the the Cotton-Mouton of via achieved is a combination birefringence effects. Faraday and FThF Birefringence in and • Polarization I—Continued Optical Design FThF39:00 a.m. • Enhancement of Polarization Rotation in Azobenzene Films, Chandra S. Devulapalli Rao; V. Yelleswarapu, of Univ. - Massachu setts Boston, USA. We observed enhancement of photoinduced polarization rotation, as much as 24°, when the input laser beam propagates through azobenzene doped polymer thin films that placed in tandem. were FThF5 • 9:30 a.m. Strip Silicon of in Birefringence Waveguides LargeTwo Tuning via Optomechanical , Motion Southern California, USA. Adjusting the separation between two strip waveguides by an optical force, we obtain widely tunable birefringence dependent on the separation. The maximum differ ence of phase birefringence before and after tuning is calculated beto 0.026. FThF6 • 9:45 a.m. Collapse, Light Nonlinear of Control Magneto-Optical A. Rutkowska LS Invited Invited For Fall Congress presentations on Thursday, see pages 132-135. Congress presentations on Thursday, For Fall Atherton We report a single molecular imaging method imaging molecular single a report We October 11–15, 2009 • Quantum dots (QDs) are fluorescent inorganic probes that that probes inorganic fluorescent are (QDs) dots Quantum
LSThB3 • 9:00 a.m. LSThB3 • 9:00 LSThB • Single-Molecule Biophysics III— Biophysics LSThB • Single-Molecule Continued LSThB4 • 9:30 a.m. Single Single Molecule Imaging of in Axonal Transport Live, Neurons Harsha V. Mudrakola, Chengbiao Wu, Kai Zhang, Bianxiao Cui; USA. Univ., Stanford super-resolution a and neurons, live in transport axonal tracks that - microtu individual resolves that tracking object dynamic method, the diffraction below barrier. neurons in live bules Probing Cellular Events with Single Quantum Dot , Imaging Maxime Dahan; Lab Kastler Brossel, École France. Normale Supérieure, state-of- The cells. live in molecules single of visualization the enable important as some as well the willart tracking in QD be presented challenges. remaining ; 2 , Steve 1 Edward Edward Galen B. B. Galen Channel 3 Ting Ting Han , , Robbie , Charters Robbie 1 Regency and Imperial Ballroom Foyer, Fairmont Hotel Fairmont Foyer, Ballroom Imperial and Coffee Break, Regency RPO Inc., Australia. UV- 2 waveguide have been related related been have waveguide 3 , Barry Luther-Davies 1 Glen Ellen Glen FiO/LS/AO/AIOM/COSI/LM/SRS 2009 chalcogenide chalcogenide glass films on thermally oxidized silicon 0.8 , Mathew Zhang , Mathew 1 Se 0.2 10:00 a.m.–10:30 a.m. Australian Australian Natl. Australia, Univ., to to the of structural BPM. and SIMS The by comparison properties method BPM the and experiment the between diameters mode the been performed. have substrates using electron beams. Numerical modeling of the funda- the of modeling Numerical beams. electron using substrates 2.0. of effective index TE mode an yields mental Madden Waveguide Waveguide in Comparison with Beam Propagation , Method Jieda Li, Jay Kirk, Marc Christensen; P. Southern Methodist Univ., LiNbO Ti: of properties Optical USA. 1 Nanoimprint lithography is demonstrated to be a low cost and high and cost low a be to demonstrated is lithography Nanoimprint optical devices. We complicated to technique replicate throughput waveguides optical Polysiloxane nanoimprinted quality high present system. WDM devices for grating waveguide and FThE Optics—Continued • Integrated FThE6 • 9:15 a.m. Characterization of Guided Modes of Ti: LiNbO Hoffman, Wei Zhou, R. Sooryakumar, Ronald M. Reano; Ohio State State Ohio Reano; M. Ronald R. Sooryakumar, Zhou, Wei Hoffman, waveguides rib write direct of fabrication the report We USA. Univ., in Ge FThE7 • 9:30 a.m. Fabrication of Rib in Waveguides Germanium-Selenium Chal - , cogenide Glass Electron through Beam Direct Writing FThE59:00 a.m. • Nanoimprinted Polysiloxane Optical Devices FThE8 • 9:45 a.m. Modeled with Writing GAFFE, Asymmetric Waveguide J. Grace; Imperial College London, UK. For the first time to knowledge our we numerically demonstrate the effect pattern of “bite-mark” simple characteristic the self- of generation the on focusing writing. waveguide in transverse
, 1 FiO Ctr. de de Ctr. 3 , , Olivier Mercedeh 1,2 , , Miguel A. Bello-Jiménez A. Miguel , 2 Univ. of Dayton, USA, Dayton, of Univ. 2 Baldemar Baldemar Ibarra-Escamilla John John R. Marciante; Univ. of Rochester,
Invited California , Joseph Haus W. 1 INAOE, Mexico, Mexico, INAOE, 1 ; 1 , Evgeny A. Kuzin A. Evgeny , 3 Simulations and experiments will be used to reveal the spatial spatial the reveal to used be will experiments and Simulations Khajavikhan, Khajavikhan, James Robert Leger; of Univ. Minnesota, USA. - spatial supermodes cavi of in Michelson-type exploitation Proper ties reduces the sensitivity to path-length The variations. radiance is improvement experimentally demonstrated in a common-path generalized cavity Michelson formed by polarization multiplexing arms. gain the two FThD5 • 9:30 a.m. Ariel Flores-Rosas Ariel Pottiez FThD4 • 9:15 a.m. Figure-Eight Erbium-Doped Wavelength-Tunable Fiber Laser with a Sagnac Fiber , Filter FThD • High-Power Fiber Lasers I—Continued FThD39:00 a.m. • Experimental Demonstration of Reduced Path-Length Sensi- tivity in Coherent Beam Combining Architectures A passively mode-locked Erbium- mode-locked passively A Mexico. Optica, en Investigaciones doped figure-eight with fiber laser is interferometer, fibercontinuously wavelength-tunable a using nm 1555 to 1525 from range a over spectrum pulse 3.1 ps and 1.5 nm. trace of of autocorrelation an USA. filtering properties of large-mode-area gain-tailored fibers, where preferential provides modes various the with gain the of overlap the levels. high saturation even at modal discrimination Spatial Spatial Filtering Properties of Large-Mode-Area Fibers with Confined Gain , Dopants Thursday, October 15 104 not available. , Announced Title toBe LCLS. status The design, and capabilities of XCS presented. be will the matterusing nanometric densed lengthscales systemstodown con- in phenomena dynamical probe will (XCS)Instrument copy Lab,Stanford Univ., USA. Aymeric Robert; Linac Coherent Light Source, SLAC Natl. Accelerator The X-Ray Photon Correlation Spectroscopy Instrument at LCLS, LSThC1 •10:30a.m. Stanford Univ., USA,Presider Sébastien Boutet; SLAC Natl. Accelerator Lab, Spectroscopy LSThC •X-Ray PhotonCorrelation 10:30 a.m.–12:00p.m. LSThC2 •11:00a.m. SimonMochrie; Yale Univ., USA. The X-rayThe Photon Correlation Spectros- Empire Invited Invited LS Abstract FThG2 •11:00a.m. FThG2 FThG1 •10:30a.m. FThG1 micron and nanometer resolution. emphasis put be will on which methods aim those to produce sub- main The instrumentation. beamlines synchrotron in elements standard become which optics refractive X-ray of statuslatest the EuropeanSynchrotron Radiation Facility, France. Nanofocusing, for Optics Refractive X-Ray HZB, Nano-Tomographyat X-Ray talk, we present applications. andtalk, selected TXM new the tor beamline, which provides an energy resolution up to 104. In the BESSY undulator U41 at a focusing the spherical gratingat monochromaoperates- system The spectroscopy. and cryo-tomography new full-field transmission X-ray microscope (TXM) for automated Natl.sion,Inst.,Cancer Natl. Inst.Health, Weof USA. a developed Presider Lahsen Assoufid; Argonne Natl. Lab, USA, •NanofocusingOpticsII FThG 10:30 a.m.–12:00p.m. mann erring BESSY II, Germany, Zentrum Berlin für Materialien und Energie GmbH, Elektronenspeich- 1 , StefanHeim, FiO/LS/AO/AIOM/COSI/LM/SRS 2009 1 , Waltraud, Müller 2 Lab of Receptor Biology and Gene Expres - Crystal Invited Invited Gerd Schneider Gerd 2 , JimMcNally,
Anatoly Snigirev; Snigirev; Anatoly The paper coverspaper The 2 1 ; , Peter Gutt- Peter , 1 Helmholtz- Element Optical Systems Optical Element Extending Stavroudis’s Solution of the Eikonal Equation to Multi- •11:00a.m. FThH2 FThH1 •10:30a.m. FThH1 are demonstrated for shortcomings. these related-complicationsfabrication, design, arein and testing.Solutions There sight. first at unintelligible are and digits unnecessary many hold coefficients its problematic: is asphere’sshape an of USA. TechnologiesInc., QED Me? for Asphere this YouMake/Measure Can Presider Marty Valente; Univ. of Arizona, USA, Alignment I Design,Characterizationand Surfaces: •AsphericandFreeform Optical FThH 10:30 a.m.–11:45a.m. 1 1 optical systems. multi-element to applied be to it allowing surface, refracting or reflecting arbitratry an across continued be can k-function the of We show how Stavroudis’s solution to the eikonal equation in terms tions polynomials spaceand of field inboth pupil Zernike space. systems with tilted and decentered elements, derived from combina- thogonal field-dependent aberrations, foruseful describing optical Systems Orthogonal Field-Dependent Aberrations for Misaligned Optical •11:15a.m. FThH3 Univ.Arizona,USA, of USA, Hoffnagle, A. John • , Anastacia M. Manuel M. Anastacia October 11–15,2009 2 DxO Labs,France.DxO Weor of set presenta 2 Univ. of Alabama at Birmingham,USA. Univ.Alabamaat of , For Fall Congress presentations onThursday, seepages132-136. Invited John A. Hoffnagle A. John FiO Gold The conventional characterizationconventional The 1 , James H. Burge H. James , 1 , David L. Shealy L. David , 1 , Régis TessieresRégis , Greg Forbes; Forbes; Greg 2 2 - ; ; eration in Disordered Nonlinear Media, Nonlinear Disordered in eration - Gen Harmonic Second on Distribution Domain of Effect The •10:30a.m. FThI1 Labs, Inc., Canada, Diffraction and Hybrid Nonlinearity, Hybrid and Diffraction Saddle-Shaped between Balance to Due Light Self-Trappingof •11:00a.m. FThI3 Saltiel envelopes, temporal and phase are shifts explicitly. calculated of the modified Korteweg-de Vries - sine Gordon equation. The pulse two-component nonlinear medium is studied within the framework Romania. Engineering, controllable quantities using anumerical for model first time. the experimentally Weto beams. period nonlinearelegantlyrelate the periodic integrated nanostructures using nonparaxial Bessel-Gauss We investigate the exploitation of self-focusing for the composition of Andrew W. Norfolk, Edward J. Grace; Imperial College London, UK. Harnessing Self-Focusing: Direct Writing of Periodic Structures, •10:45a.m. FThI2 second harmonic. of pattern emission affect greatly structure domain disordered of features specific the that showWe domains. ferroelectric of tion distribu- random with crystal nonlinear in generation harmonic Bulgaria. Medium , Two-Componenta Solitonsin Interaction Optical Few-Cycleof •11:15a.m. FThI4 Catalunya, Spain,Catalunya, Vilaseca Zhang 1 USA, Presider Nathaniel Phillips; College of William & Mary, •NovelNonlinearOpticalPhenomena FThI 10:30 a.m.–12:00p.m. China, Univ., USA, M. Cojocaru M. observed gap solitons.observed with phase and spectrum characteristics different from all previously gapsolitons,spatialdiscreteof type self-trapping new to a ofleads hybrid nonlinearity in a two-dimensional ionic-type photonic lattice Univ. of Angers, France, 2,3 1,2,3 2 Northwestern Polytechnical Univ., China, , WenjieWang, 1 , KestutisStaliunas, , J. ZhaoJ. , We study theoretically and experimentally the second the experimentally and theoretically studyWe Herve Herve Leblond 4 1 Univ. of Vermont, USA. Saddle-shaped anddiffraction , Dragomir N. NeshevDragomirN. , 2 , J. XuJ. , 2 4 Australian Natl. Univ.,Australia,Natl.Australian Horia Hulubei Natl. Inst. for Physics and Nuclear The interaction of few-cycle optical pulses in a 2 , Ksawery KalinowskiKsawery , 1 2 1 , , Igor V. Mel’nikov Optolink Ltd., Russian Federation, , J. YangJ. , 1 Valley , YuriKivshar, S. 4 , ZhigangChen , 2 , WieslawKrolikowski, i Hu Yi 2,3 Vito Roppo Vito , , Dumitru Michalache 2 2 ; , Jose F.TrullJose , 1 Univ.Politécnica de 3 1 San Francisco State , Cibo Lou Cibo , 1,3 ; 1 NankaiUniv., 3 1,2 Sofia Univ., Sofia , Solomon , 2 , Ramon , 1 3 , Crina , High Q 1 , Peng , 4 ; Thursday, October 15 105 Amber Amber Russell A generalization of the Jones cal - Jones the of generalization A FiO Invited Dean P. Brown, Thomas G. Brown; Inst. Inst. G. Brown; Thomas Brown, P. Dean Sacramento FThL3 • 11:15 a.m. Illumination Described Vortex Using Nonparaxial Polarization , Matrix a 2x2 Correlation dimensions three in fields Vector USA. Rochester, of Univ. Optics, of (second-order) describe to matrix correlation 3x3 a require generally can that fields nonparaxial of class a describe We field. the of statistics matrix. correlation be described a two-dimensional using FThL2 • 11:00 a.m. Polarimetry Using Stress-Engineered Optical Elements, FThL1 • 10:30 a.m. describe We USA. Rochester, of Univ. Brown; G. Thomas Beckley, M. a method of polarimetry optical elements. using stress-engineered By using the due of retardance deterministic, nature space-variant from deduced be can parameters Stokes the birefringence, stress to frame. camera a single 10:30 a.m.–11:45 a.m. 10:30 a.m.–11:45 FThL Birefringence in and • Polarization II Optical Design USA, Presider Microsoft, McEldowney; Scott Polarization Aberration Functions in Three Dimensions, Dimensions, Three in Functions Aberration Polarization USA. Arizona, of Univ. Chipman; polarization to calculus Jones the applying in difficulties avoids culus ray tracing, a eliminating minus sign, notorious and clarifying the systems. optical non-polarizing of description
Drosophila Christopher J. Fecko; Univ. of North Univ. J. Fecko; Christopher LS Multiphoton microscopy can resolve resolve can microscopy Multiphoton Invited Invited For Fall Congress presentations on Thursday, see pages 132-135. Congress presentations on Thursday, For Fall Atherton October 11–15, 2009 • Nancy Thompson; Univ. of North Carolina at Chapel Hill, USA. Hill, Chapel at Carolina North of Univ. Thompson; Nancy
, Recent advances in combining total internal reflection illumination illumination reflection internal total combining in advances Recent with fluorescence correlation spectroscopy will be described. If with illumination reflection internal total combining permits, time will also be presented. photobleaching continuous - multipho of utility the exploring are We tissues. gland salivary larval of movement three-dimensional the observe to photoactivation ton in transcription. involved proteins 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 IV Biophysics LSThD • Single-Molecule USA, Presider Lab, Bewersdorf; Jackson Joerg LSThD2 • 11:00 a.m. LSThD1 • 10:30 a.m. , Imaging Gene Transcription USA. Hill, Chapel at Carolina Spectros- Correlation Fluorescence with Reflection Internal Total copy actively actively transcribed genes within live polytene cells of , 1 Ctr. for for Ctr. 1 OptoNet OptoNet , Yicheng Yicheng , ; 2 1 1 IBM Systems Systems IBM Data Storage Storage Data Data Data Storage 2 1 1 ; ; Chang-Yi Chang-Yi Lin 2 3 Chee Wei Lee Wei Chee , Luke F. Lester F. Luke , 1 Perfect matched layer with layer matched Perfect , Seng-Tiong Ho Seng-Tiong , 1 , Seng-Tiong , Ho Seng-Tiong 2 Glen Ellen Glen QianWang , , Furqan L. Chiragh L. Furqan , 1 , Boyang Liu 2 Northwestern Univ., USA. Univ., Northwestern 2 FiO/LS/AO/AIOM/COSI/LM/SRS 2009 , Yan Li Yan , 2 Dept. Dept. of Electrical Engineering and Computer Science, 3 , Yingyan , Huang Yingyan 1 un-split un-split field for gain medium in FDTD incorporating simulation validation Numerical presented. is model multi-electron multi-level under effectively wave the absorb can derived boundary the indicates currents). (injection carrier densities different Inc., Inc., USA, Yongchun Xin Yongchun Inst., Agency for Science, Technology and Agency Inst., for Res., Science, Singapore, Technology Inst., Singapore, Singapore, Inst., We present technique of achieving high- achieving of technique present We USA. Univ., Northwestern InP/InGaAsP-based in intermixing well quantum spatial-resolution deeply-etched submicron-width utilizes It structures. well quantum indicate Results intermixing. the during diffusion-stopper as trench blueshift. >100 nm bandgap with control <0.4 µm spatial and Technology Group, Semiconductor Solutions, USA. Atheory Solutions, for Semiconductor Group, Technology and the cavity design dash mode-lockedof passively quantum lasers is reported is perspective. baseda It - photonics valu on a microwave passively dash quantum InAs/InP monolithic realizing for tool able mode-locked lasers. Lai High Technology Materials, Univ. of New Mexico, USA, Mexico, New of Univ. Materials, Technology High FThK4 • 11:15 a.m. UPML Gain for Medium in with Simulation FDTD Multi-Level Multi-ElectronModel 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 FThK • Optoelectronics Presider USA, Univ., Northwestern Yi; Fei FThK2 • 10:45 a.m. Analysis of the Relative Intensity Noise Characteristics of the Strained AlGaInN LDs under Hongik Dept., High Engineering Frequency Electronic , Modulation Yi; Chang Jong Cho, Uk Hyung Republic Univ., of Korea. The RIN characteristics in AlGaInN LDs were investigated using the rate equations with the quantum Langevin noise model. The device parameters were extracted by using the self-consistent multiband Hamiltonian for the strained crystal.wurtzite FThK3 • 11:00 a.m. Technique Intermixing Well Quantum High-Spatial-Resolution , Fabrications Nano-Device All-Optical for FThK1 • 10:30 a.m. Cavity Design of Monolithic InAs/InP Long-Wavelength Quantum Dash Passively Mode-Locked Lasers, - FiO Photonics 2 , Harendra 1 Optoelectron 1 ; 1 We experimentally Jayanta Jayanta Mukherjee , , John G. , McInerney John 2 Invited Valentin Gapontsev; IPG Photonics Corp., Corp., Gapontsev; IPG Photonics Valentin California , Brian , Corbett Brian 1 Weihua Guan, John R. Lab Weihua for Marciante; Laser - En FThJ3 • 11:15 a.m. Far-Field Splitting in Broad Area Quantum Dot Lasers via Thermo-Optic Cavity Detuning ics Group, ics Dept. Group, of College Physics, Univ. Cork, Ireland, Sources Sources Group, Tyndall Natl. Inst., Ireland. demonstrate the collapse of a single lobed far-field into multiple lobes via thermo-optic detuning of the cavity in broad area - quan tum dot laser under CW in operation, with accordance our recent analysis. Maxwell-Bloch FThJ2 • 11:00 a.m. Scaling Power of Single-Frequency Brillouin/Ytterbium Hybrid Fiber Lasers , ergetics and USA. Inst. of of Optics, The Rochester, Univ. proposed dual-clad fiber 80 W lasersingle-frequency of output can generate with a side-mode suppression ratio (SMSR) affects greater scattering Brillouin than stimulated 50 multi-order dB. limit, this Beyond the laser efficiency SMSR. and N. J. N. Fernando J. FThJ1 • 10:30 a.m. 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 FThJ Lasers Fiber • High-Power II Grumman Northrop McNaught; J. Stuart Presider USA, Technology, Space Abstract not available. not USA. Abstract Title Title to Be Announced, Thursday, October 15 106 Spectroscopy—Continued LSThC •X-Ray PhotonCorrelation quench gives test anew of dynamical scaling. temperaturea after functions correlation two-time lar,measuring is used to study non-equilibrium fluctuations in Cu3Au. In - particu Mark Sutton; McGill Univ., Canada. Using X-Ray Correlation Spectroscopy to Test , Dynamical Scaling LSThC3 •11:30a.m. ______Empire Invited LS X-ray correlation spectroscopy FThG3 •11:30a.m. FThG3 correction system. wavefront on-site an with mirror coated multilayer and figured elliptically an using by achieved was 0.06nm of wavelength the of Yamauchi; Osaka Univ.,Mirrors, Japan.KB by X-Rays Hard of Focusing 10nm-Level FThG •NanofocusingOpticsII—Continued FThG FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Crystal Invited 10nm-level line focusing of hard X-ray 12:00 p.m.–1:30p.m.
Kazuto NOTES Lunch Break(on yourLunch own) , Theory Aberration Nodal Using Aberrations Misalignment Induced Alignment from Error Figure Mirror Astigmatic Separating •11:30a.m. FThH4 Alignment I—Continued Design,Characterizationand Surfaces: •AsphericandFreeform Optical FThH Central Florida, USA, P. Thompson P. 3 astronomical telescopes. for demonstrated and derived be will differences These error. figure mirror astigmatic by caused positions nodal signature than dependence field signature different a displays astigmatism ment - misalign that revealed (NAT)has theory aberration Nodal USA. Inst. of Optics, Univ. of Rochester,USA, Univ.of Optics, of Inst. • Tobias Schmid 4 ; October 11–15,2009 1 CREOL, College of Optics and Photonics, Univ.of Photonics, and Optics of College CREOL, 2 1 Large Binocular Telescope Observatory, USA, , Andrew Rakich Andrew , For Fall Congress presentations onThursday, seepages132-136. FiO Gold 2 , Jannick P. Rolland Jannick , 4 Optical Res. Associates, Res. Optical 1,3 , Kevin Phenomena—Continued •NovelNonlinearOptical FThI fluctuations improving states. squeezed intracavity photonic crystals modify their stability as well as quantum correlations in the transverse profile of emitted light. We show how metric oscillators (OPOs) are known to induce non-classical spatial IFISC (UIB-CSIC), Campus Univ. Illes Balears, Spain. Optical para OPOs Photonic ActingCrystals on Instabilities Statesand Squeezed in •11:45a.m. FThI6 in such processes discussed. is also equation are investigated. The impact of intrapulse Raman scattering complexGinzburg-Landau the by described systems sipativefiber dis- in states multisolitonbound formationof the and interaction V.C. Sofia Latas,Mário F. Ferreira; Univ. Aveiro,of Portugal. Pulse Soliton Interaction and Bound States in Dissipative Fiber Systems , •11:30a.m. FThI5 , M. Moreno, M. A. García March, D. Gomila, R. Zambrini; R. Gomila, March,D. García A. Moreno,M. M. Valley - Thursday, October 15 107 FiO Sacramento FThL Birefringence in and • Polarization II—Continued Optical Design FThL411:30 a.m. • Stroboscopic Illumination Mueller Matrix Photonics, of Dept. Image Chao; , Polarimetry Yu-Faye Tsai, Tsung-Han Tsai, Hsiu-Ming illumination stroboscopic Utilizing Taiwan. Univ., Tung Chiao Natl. technique, we present a Mueller matrix imaging polarimetry with will methodology this of merit of figure The modulator. Photoelastic others. with will be compared results be its discussed, and , 2 Crystal structures of , Vanessa C. DeRocco C. Vanessa , 2 North Carolina State Univ., USA, USA, Univ., State Carolina North 1 ; 2 LS Invited , Lauryn E. Sass E. Lauryn , 1 For Fall Congress presentations on Thursday, see pages 132-135. Congress presentations on Thursday, For Fall Atherton , Dorothy A. Erie A. Dorothy , 1 October 11–15, 2009 Keith R. Weninger R. Keith • Univ. of North Carolina at Chapel Hill, USA. at of Hill, Chapel North Carolina Univ. Trevor Anderson Trevor LSThD • Single-Molecule Biophysics IV— Biophysics LSThD • Single-Molecule Continued mismatch repair proteins bound to mismatched DNA reveal kinked reveal DNA mismatched to bound proteins repair mismatch switching observed dynamic we FRET molecule single With DNA. bending of dynamics the suggests which states, bent different among repair. mismatch influence may 2 DNA DNA Repair Protein Dynamics through Single-Molecule Fluo - rescence , LSThD3 • 11:30 a.m. LSThD3 • 11:30 (on your own) Lunch your Break (on , 2 NOTES Tyndall 2 , Herendra N. J. , Yingyan Huang Yingyan , 1 1,2 Northwestern Univ., USA. Univ., Northwestern 3 , Yicheng Lai Yicheng , Optoelectronics Group, Physics 1 1 Ehsan Sooudi ; 12:00 p.m.–1:30 p.m. 1,2 Glen Ellen Glen Optonet Inc., USA, Inc., Optonet 2 Koustuban Ravi Koustuban , Data Storage Inst., Agency for Science, Technology for Science, Agency Technology Inst., Data Storage 1 ; FiO/LS/AO/AIOM/COSI/LM/SRS 2009 3 , John G. McInerney 1,2 Natl. Natl. Inst., College Univ. Cork, Ireland. We report CW injection locking of a Fabry-Perot InAs/InP quantum dash laser. Injection power (~0.1 mW) at 1.5 Ith is sufficient to obtain 30 dB SMSR of modesingle output. locked Seng-Tiong Ho Seng-Tiong FThK511:30 a.m. • A Computationally Efficient Finite Difference Time Domain Gain - in Opto Well Quantum Incorporating Model (FDTD) for Devices electronic Dept., Dept., Natl. of Univ. College Ireland, Univ. Cork, Ireland, A new computationally efficient FDTD model for quantum wells is is wells quantum for model FDTD efficient computationally new A simulation Gain system. multi-electron multi-level, a using proposed results concur with standard This theory. scheme is useful for the geometries. devices complex with of simulation Fernando and Res., Singapore, Res., Singapore, and FThK6 • 11:45 a.m. Observation of Injection Locking in a Long-Cavity InAs/InP 1.56 µm Quantum Dash Laser, FThK • Optoelectronics—Continued , - FiO 1,2 Andreas Tünnermann Andreas
Friedrich-Schiller Univ. Friedrich-Schiller Jena, Univ. 1 ; 1,2 Invited California , Jens Limpert 1,2 We report on the current status of our developments developments our of status current the on report We Fraunhofer Inst. for Applied Optics and Precision Engineer Precision and Optics Applied for Inst. Fraunhofer 2 ______Germany. ing, in high power fiber laser and amplifiers for continuous wave and for basis the is which components, their as well as operation pulsed further scaling. performance Thomas Thomas Schreiber Germany, Germany, FThJ4 a.m. • 11:30 FThJ Lasers Fiber • High-Power II— Continued , Amplifiers and Lasers Fiber High-Power Thursday, October 15 108 them using the new method of usingthem method new X-ray the ptychography. problem of domain structures. This talk hardersummarises progress the solving comes patterns, diffraction three-dimensional their using Diffraction X-ray Coherent by objects small imaging initio Univ.Robinson;UK. IanLondon, College , Diffraction X-Ray Coherent by Structures Domain of Imaging data.experimental ankylographywiththeoreticalanalysis, numerical simulations and Wemonochromatic a beam. incidentusing exposure demonstrate raphy, enabling complete 3-D structure determination from a single USA. I will present a novel 3-D imaging modality, denoted ankylog- from a Single View, Determination Structure Three-Dimensional Ankylography: LSThE2 •2:00p.m. LSThE1 •1:30p.m. Veit Cornell Elser; Univ., USA,Presider LSThE •X-Ray ImagingII 1:30 p.m.–2:45p.m. Jianwei Miao; Univ. of California at Los Angeles, Empire Invited Invited LS Following successful ab- successful Following FThM2 •2:00p.m. FThM2 •1:30p.m. FThM1 composition. elemental and structure crystal local of studies practical foroptics nanofocusing X-ray hard stable develop to efforts describe We nanodiffraction. and nanospectroscopy for advantages important USA. Lab,Natl. Argonne Source, Nanoscale X-Ray Focusing with Reflective Optics, Reflective with Focusing X-Ray Nanoscale Abstract not available. Microscopy, Localization tion Intracellular Nanoscale Imaging with Fluorescence Photoactiva- Gene Ice; Oak Ridge Natl. Lab, USA,Presider Instruments I •NanoscaleMethodsand FThM 1:30 p.m.–3:30p.m. USA, Lahsen Assoufid Lahsen Jonathan Z. Tischler 2 Pohang Accelerator Lab, Republic of Korea, FiO/LS/AO/AIOM/COSI/LM/SRS 2009 3 , Deming Shu Deming , 1 , Jae-Young Choi Invited Invited Crystal 3 , Chian Liu Chian , SamuelHess; Univ. Maine,of USA. Achromatic mirror optics offer optics mirror Achromatic 2 , Wenjun Liu 3 ; 1 Oak Ridge Natl. Lab,Natl.Ridge Oak 3 Advanced Photon 3 , Ali Khounsary Gene E. Ice E. Gene 1 3 , , FThN1 •1:30p.m. FThN1 Single Single Element See-through Head-Worn Display Application of Radial Basis Functions to the Design of a Freeform Fabrication and Testing of Large Free-Form Surfaces, aspherical to surfaces optical precision. optical metrology, now allow fabrication of large diameter free-form and mechanical in advances withequipment, combinedpolishing Univ.ofArizona, USA. University of Arizona. The fromPh.D. and M.S. his UniversityStateandhis Ohio from receivedB.S. He SPIE. of fellow a and ASME, OSA, of member a is Burge Dr. Lab. Mirror Observatory Steward the atproject scientist as worked he Sciences, Optical of College the at faculty the joining to Prior Arizona. of University Sciences, Optical of optomechanicsteaches College at the also engineering opticaland Burge Dr. telescopes. astronomical for mirrors large making for methods manufacturing controlled computer of implementation and systems metrology of development the led has Burge Dr. USA, Presider Peter Blake; NASA Goddard Space Flight Ctr., Alignment II Design,Characterizationand Surfaces: •AsphericandFreeform Optical FThN 1:30 p.m.–3:30p.m. see-through head-wornsee-through display is presented.element free-form single a of example design A surfaces. optical from polynomials to radial basis functions for describing free-form of Rochester, USA. Jannick Jannick Rolland FThN2 •2:15p.m. FThN2 • October 11–15,2009 2 ; 1 This paper presents the impact of a change of basis Optical Res. Associates, USA, Moderncomputer-controlled andgrinding Tutorial Invited For Fall Congress presentations onThursday, seepages132-136. FiO Gold 2 Inst. of Optics, Univ. ,
Ozan Cakmakci
James Burge; 1 , and is precisely laser the tuned using temperature control. mode microspheregallery as whispering an etalon. a Single-mode lasing using is laser demonstrated loop fiber Erbium an stabilizing for the Science of Light, Germany. We present acompact of method jamin Sprenger, Harald G. L. Schwefel, L. J. Wang; Max-Planck-Inst. , Laser Loop Fiber a ofStabilization Microcavity Spherical •1:45p.m. FThO2 and Q-factor of about 1000. light laser mode at visible wavelengths, with aoflinewidth afew Å light-emitting polymer nanofibers. The single nanofiber emit single del Salento, Italy. Salento, del Elisa Mele, Luana Persano, Roberto Cingolani, Dario Pisignano; Univ.fibers Microscale Lasers Based on Patterned Electrospun Polymer Nano- •1:30p.m. FThO1 FThO3 •2:00p.m. FThO3 Patrice FéronPatrice UsingLasers WhisperingMode ResonatorGallery Er:ZBLALiP , Wavelength-Tunableof Singlemode Oscillation Simultaneous Tomoyuki Yoshie; Duke Univ., USA,Presider •Micro-cavityDevicesII FThO 1:30 p.m.–3:30p.m. 1, France, beat note signal. resulting the and characteristics emission the studyWe neously. simulta- obtained be to emissions laser mode single independent two allows Er:ZBLALiP resonatorin micro-spherical same the on Solide-LCAES, CNRS-UMR, France. YannBoucher G. , Andrea Camposeo, Stefano Pagliara, Francesca Di Benedetto, 2 Xiamen Univ., China, 1 , Lei Xiao Lei , In this work we demonstrate cavity effects in single 1 , ZhiPing CaiZhiPing , 1,2 , Stéphane Trébaol Stéphane , Invited Valley 2 , MichelMortier , 3 Lab de Chimie Appliqúee de l’Etat
The coupling by two half tapers 1 , YannickDumeige , 3 ; 1 Univ.Rennes de - Ben 1 , Thursday, October 15 109 Nicholas Nicholas We We present a Joseph Rosen,
- achieve the illustrate We FiO Invited Invited Sacramento 1:30 p.m.–3:30 p.m. 1:30 p.m.–3:30 FThR and Imaging • Computational I Photography Presider USA, Levin; MIT, Anat Barak Barak Katz; Ben Gurion of Univ. the Negev, Israel. new holographic system operating in a synthetic aperture mode. Spatial resolution exceeding the Rayleigh limit is obtained by digital tiling severalhologram a into of elements complete Fresnel the observed object. , Systems Imaging Computational Emerging Integrated USA. Rochester, of Univ. Chi; Wanli George, ments of ICIS in extended depth of field as well as in an emerging system. camera new correlation-based Multi-Channel Incoherent Digital , Holography FThR2 • 2:00 p.m. FThR1 • 1:30 p.m. , 1 , Bridget S. 1 Univ. of New New of Univ. 2 Nathan P. Wells P. Nathan , Live Live cell imaging with , Peter M. Goodwin 1 LS For Fall Congress presentations on Thursday, see pages 132-135. Congress presentations on Thursday, For Fall Invited Invited Atherton Los Alamos Natl. Lab, USA, Lab, Natl. Los Alamos 1 ; 1 , M. Lisa Phipps 2 October 11–15, 2009 We have designed a fluorescence microscope that uses that microscope fluorescence a designed have We • , James Werner , James 2 Christine Christine Payne; Georgia USA. Tech, , Wilson Diane Diane S. Lidke LSThF2 • 2:00 p.m. 1:30 p.m.–3:00 p.m. 1:30 p.m.–3:00 V Biophysics LSThF • Single-Molecule USA, Presider Univ., Emory Berland; Keith Mexico, USA. Mexico, a unique spatial filter geometry and active biologically feedback at to dots follow the quantum individual of motion dimensional three (microns/second). rates transport relevant Non-Scanning Non-Scanning Two-Photon Microscopy for Imaging in Live Cells two-photon microscopy is limited by the scanning necessary to construct an image. We describe the application doesof that configuration two-photon reflection internal total a in used excitation scanning. require not Following Dimensions: Three in Dots Quantum Single Tracking Cell Receptor Traffic and Membrane Topology LSThF1 • 1:30 p.m. Ann Ann E. Elsner, A scanning laser scanning A - Lon College Univ. Fitzke; Frederick Tutorial Glen Ellen Glen FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Optical imaging of the eye has considerable advantages for for advantages considerable has eye the of imaging Optical Fred Fred Fitzke is Professor of Visual Optics and Psychophysics in the Department of Visual Neuroscience of University in College B.A. a holds He IoO). (UCL Ophthalmology of Institute London SciencesNatural from The and Johns Hopkins University a Ph.D. the of is Director He London. of the University from in Biophysics Foundation Fighting Blindness Research Center for the Study of Eye Moorfields and theDiseases UCL IoO at Retinal Degenerative Hospital and founding Investigator for the National Institute for Health Research Biomedical Research Centre for Ophthalmology. been has and 1970s the in beginning OSA of member a been has He - Physiologi of Laboratory the heads he where 1982 since IoO UCL at cal Optics. His research covers two broad areas: the development visual of investigations and eye the imaging for techniques novel of methods. psychophysical function using 1:30 p.m.–3:30 p.m. 1:30 p.m.–3:30 FThQ Eye Imaging in the • Molecular Berkeley, at California of Univ. Roorda; Austin USA, Presider , Eye the in Imaging Molecular UK. don, molecular of techniques non-optical to compared imaging molecular - An and Protein Fluorescence Green autofluorescence, for imaging eye. in the living imaging confocal V apoptosis nexin FThQ2 • 2:15 p.m. Near with Comparison and nm 594 at Autofluorescence Fundus Infrared Reflectance and Fluorescence , Imaging Stephen A. Burns, Benno Haggerty, Dean Bryan A. P. VanNasdale, USA. Univ., Indiana Muller; S. Matthew Peetrig, L. loca- retinal at features reveals nm 594 at technique autofluorescent seentions with near infrared reflectance imaging and polarization techniques. The autofluorescence from melanin is too weak to 594 nm autofluorescence. for account FThQ1 • 1:30 p.m. , - 3 FiO , Florian 1 , Michael Schmidt 3 Azhar Zam , Erlangen Erlangen Graduate School 1 Dept. of Medical Informatics, Informatics, Medical of Dept. 4 ; ; ex vivo 1 Dept. Dept. of Oral and Maxillofacial 2 Invited California , Katja Tangermann-Gerk Katja , 2 - interven an is (PDT) therapy Photodynamic , Alexandre Douplik 4 Tayyaba Hasan; Massachusetts General Hospital, Harvard Harvard Hospital, General Massachusetts Hasan; Tayyaba
Katherine A. Baker, Wade Rich, Neil Finer, Joseph E. Ford; Ford; E. Joseph Finer, Neil Rich, Wade Baker, A. Katherine Bavarian Laser Ctr., Germany, Germany, Ctr., Laser Bavarian , Emeka Nkenke Emeka , 3 2 Werner Werner Adler Surgery, Friedrich-Alexander Univ. Surgery, of Friedrich-Alexander Univ. Ger Erlangen-Nuremberg, many, Stelzle FThP3 • 2:15 p.m. Design and Prototype Fabrication of a Neonatal Video Laryn- goscope, min - prototype a describe We USA. Diego, San at California of Univ. infants, weight birth low extremely for laryngoscope video iaturized guide light depressor, tongue curveda a acrylicas acts where blade a 1.8mm CCD imager. holds and LED illuminator, an for FThP2 • 2:00 p.m. Tissue-Specific Laser Surgery: Hard Tissue Differentiation by Diffuse Reflectance Spectroscopy Biometry and Epidemiology, Friedrich-Alexander Univ. of Erlangen- of Univ. Friedrich-Alexander Epidemiology, and Biometry Diffuse Germany. reflectance Nuremberg, spectroscopy provides a optical - for tissue differentia and approach simple straightforward hard differentiating for a potential show obtained tion. The results tissue-specific laser surgery. for guidance as tissues FThP1 • 1:30 p.m. 1:30 p.m.–3:30 p.m. 1:30 p.m.–3:30 FThP in Interventional • Optics Medicine Be Announced to Presider Photodynamic Photodynamic Therapy: A Bridge between Technology and Medicine, in in Advanced Optical Friedrich-Alexander of Univ. Technologies, Germany, Erlangen-Nuremberg, Medical School, USA. School, Medical tional treatment modality for the destruction of on impact cancerous its and and PDT of overview An pathologies. non-neoplastic will diagnostics be and presented. therapy Thursday, October 15 110 LSThE •X-Ray ImagingII—Continued Optics, Univ.Optics, Rochester,of USA, direct, non-iterative reconstruction. a allows and structure referenceholographic off-axis an as serves wires crossed of pair a of region overlap The imaging. diffractive coherent x-ray for technique reconstruction image closed-form ford Synchrotron Radiation Lightsource, USA. We introduce a novel of Crossed Wires, Crossed of Pair a ofReference Using a Reconstruction Image Holographic LSThE3 •2:30p.m. R. Fienup R. 1 , Benny WuBenny , aul Guizar-Sicairos Manuel 2,3 , Andreas Scherz Andreas , Empire LS 2 StanfordUniv., USA, 3 , Joachim StöhrJoachim , 1 , Diling Zhu Diling , 3 SSRL, StanSSRL, - 3 2,3 ; 1 , James , Inst. of Inst. FThM3 •2:30p.m. FThM3 transmission imaging. full-field and coherent Braggand diffraction, diffraction rescence, materials and devices with high spatial-resolution using X-ray - fluo providescharacterizing ofcomposition andofstructurenanoscale USA. Lab, Natl. Argonne Fuesz; Peter Stephenson, Brian Gregory Rose, Laboratory National Argonne at Beamline Nanoprobe X-Ray Hard The Germany.GmbH, Optics Laser Zeiss Carl Lasser; H. Thiess, Fabrication of Freeform Mirrors: Metrology and Figuring, Instruments I—Continued •NanoscaleMethodsand FThM FThM4 •3:00p.m. FThM4 geometries and of sets specifications are discussed. Specifications and achieved results of examples. finalized recentmirrors by with illustrated different be shall Optics Laser Zeiss Carl at metrology appropriateits and manufacturing mirror of plication The hard X-ray nanoprobe at the Advanced Photon Source PhotonAdvanced the at nanoprobe X-ray hard The 3:30 p.m.–4:00p.m. , JörgMaser, Martin V. Holt, P.Robert Winarski, Volker FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Invited Invited Crystal Coffee Break,Regency and Imperial Ballroom Foyer, Fairmont Hotel Helge Ap - Scott M. JoblingM. Scott , Metrology Surface forVirtual-InterferometerTechnique A •3:00p.m. FThN4 Alignment II—Continued Design,Characterizationand Surfaces: •AsphericandFreeform Optical FThN source extent and emission pattern. the for account to order in algorithm iterative an into embedded is that algorithm generation shape a uses method This reflectors. Associates, USA. We propose a design method for tailored freeform Engineering, Univ. of Illinois at Urbana-Champaign,USA, at Illinois Univ.of Engineering, Florida,USA, and shallow profiles. deep in deployed compensation path tool and exploration space parametric processing SPDT combines method This discussed. is (SPDT) Turning Diamond Point Single during waviness surface India. Organisation,Instruments Scientific Central Kapur; Pawan Singh, Mishra, Dole Ram, Amandeep Singh, Amrinder Kumar, Ganga Sharan ing Parameters vs. Surface , Quality Deterministic Approach for Aspheric Fabrication: SPDT Process- •2:45p.m. FThN3 sarly reconstructed several surfaces with surfaces reconstructed 40-nmRMSerror. several have we optic, an of displacements via gradients surface measure wavefront-feedbackwithin systems. Byusingwavefront sensingto demonstratednovela technique for performingmetrology surface Urbana-Champaign,USA. at Illinois Univ.of Physics, of Sources Non-Lambertian Extended for Reflectors FreeformTailored •3:15p.m. FThN5 3 ; A systematic compensation procedure to minimize aspheric 1 CREOL, College of Optics and Photonics, Univ. of Central Univ.of Photonics, and Optics of College CREOL, • , Florian R. Fournier FlorianR. 2 October 11–15,2009 Inst.ofOptics,Univ. ofRochester, USA, 1 , Paul G. KwiatPaulG. , For Fall Congress presentations onThursday, seepages132-136. 1 FiO , Jannick, P. Rolland Gold 2 ; 1 Dept. of ElectricalandComputerofDept. Rama Gopal V. Sarepaka, Vinod 1,2 , William, J.- Cas 3 OpticalRes. We haveWe 2 Dept. Dept. FThO •Micro-cavityDevicesII—Continued FThO directional Output , directional Uni- with Lasers Micro-Resonator Radial-Waveguide-Coupled •2:30p.m. FThO4 of High Performance Computing, Singapore, Gap Small a of Effects Lasers: Coupled Face-to-Face of Dynamics •3:00p.m. FThO6 Huang 1 2 Tomes we demonstrate four-wave mixing and Raman lines. mental studies and commercial applications. As a proof-of-concept - funda for source energy its micro-resonatorand a of integration evaluation of Ga GaAsP/InP quantum wells microdisk lasers were fabricated for the In Frateschi;Brazil. Univ.C. Campinas(UNICAMP), de Estadual Beam Ion Focused by Fabricated Laser Microdisk QW InGaAsP/InP •3:15p.m. FThO7 composite-mode coupling. in modifications gap-induced the with explained arewavelength. results the The of order the on size with gap a by separated are they when drastically change lasers coupled face-to-face two of the sidewalls were sidewalls the investigated. optical proprieties were investigated and the effects of the milling in , Laser Diode-Microresonator Hybrid •2:45p.m. FThO5 threshold with >0.2mWoutput. lasing 11.5mA has laser pumped electrically 20μm-diameter The mechanism. coupling output enhanced-radiation-loss new a on from micro-resonator laser using a radially placed waveguide based gapore. We demonstrate single-directional output coupling of light Seng-Tiong Ho Coherix Corp., USA. We present a new technology allowing on-chip Univ.UK, Exeter,of , HartmutErzgräber , 1 2 , Carl C. Aleksoff C. Carl , Luis A. M. Barea, Felipe Vallini, David S. L. Figueira, Newton , Eng-Huat Khoo 1 ; + 1 Northwestern Univ., USA, focused ion beam milling of mirrors. Electrical and Fang Ou Fang 2 Locking characteristics Locking UK. Univ.Bristol, of 3 , Er-Ping Li 2 1 , Tal CarmonTal , , Sebastian, Wieczorek Valley 1 , Xiangyu Li Xiangyu , 3 , Iftikhar Ahmed 1 ; 1 Univ. of Michigan, USA, USA, Michigan, Univ.of ine Yang Tianhe 2 OptoNet Inc., USA, 1 4 , Boyang LiuBoyang , Data Storage Inst., Sin- 1 , Bernd Krauskopf Bernd , 3 , Qian Wang 1 , Matthew , 1 , Yingyan, 3 Inst. 2 4 - ; , Thursday, October 15
111 - , Emir 1 , George , Peter L. 1 2 , Colin J. R. - Shep 2 Div. of Bioengineering, Bioengineering, of Div. 2 Laura Laura Waller Christian Christian Pedersen
Dept. of Biological Sciences, , Preben Buchhave 3 1 We present We the in-phase focal , Nanguang Chen , Nanguang 2 Singapore-MIT Singapore-MIT Alliance for Res. and FiO 2 DTU Fotonik, Technical Univ. of Denmark, Denmark, of Univ. Technical Fotonik, DTU 1 ; Sacramento 2 , Wei Gong , Wei 1 , Jeppe D. Seidelin 1 Kaiqin Kaiqin Chu, Nicholas George, Chi; Wanli Inst. of MIT, MIT, USA, 1 ; Ke Si 1,2 DTU Physics, Technical Univ. DTU of Physics, Univ. Technical Denmark, Denmark. 2 NUS Graduate School for Integrative Sciences and Engineer and Sciences Integrative for School Graduate NUS 1 ; 1,2,3 Based on continous-wave enhanced up-conversion we demonstrate demonstrate we up-conversion enhanced continous-wave on Based a novel and highly efficient method for converting a full from one part of the image electromagnetic spectrum a into new desired region. wavelength pard Natl. Univ. Natl. of Univ. Singapore, Singapore, ing (NGS), Natl. Univ. of Singapore, Singapore, Singapore, Singapore, of Univ. Natl. (NGS), ing Denmark, Denmark, Natl. Univ. of Natl. Singapore. Univ. Singapore, conventional the with Compared (IPFMM). microscopy modulation background reject effectively more can IPFMM microscopy, confocal depth. penetration imaging greater achieve can signal, thus FThR and Imaging • Computational I—Continued Photography Technology (SMART) Technology Ctr., Singapore. introduce We a method for recovering-phase information inspired by transport of intensity (TIE). Instead of images at multiple planes, we use defocused im- ages at a single plane with multiple wavelengths, obtained using filters. Bayer standard FThR4 • 2:45 p.m. Enhanced Background Rejection in In-Phase Focal Modulation , Microscopy FThR5 • 3:00 p.m. Incoherently Combining Logarithmic Aspheres for Extended Depth of Field, logarithmic concentric from Images USA. Rochester, of Univ. Optics, much as field of depth the extend to incoherently combined are lenses as 14 times the Rayleigh limit for a lens. conventional Diffraction digital processing. after also is obtained resolution limited FThR6 • 3:15 p.m. 2-D Nonlinear Image Up-Conversion and Filtering Using En- hanced Sum Frequency , Generation Barbastathis Karamehmedović Tidemand-Lichtenberg FThR32:30 p.m. • Phase from Defocused Color , Images - LS For Fall Congress presentations on Thursday, see pages 132-135. Congress presentations on Thursday, For Fall Invited Atherton Ahmet Ahmet Yildiz; of Univ. California at Berkeley, October 11–15, 2009 • Single Single molecule assays on kinesin bipedal-motor showed LSThF • Single-Molecule LSThF • Single-Molecule V—Continued Biophysics that that it moves by alternating of movement its two motor-domains. Such coordination is mediated by intramolecular tension gener Dissecting the Molecular Mechanism of Kinesin with Single Molecule , Imaging USA. ated by the neck-linkers, mechanical elements that span between the motor-domains. LSThF3 • 2:30 p.m. LSThF3 • 2:30 Jason Porter; Univ. Univ. Porter; Jason Regency and Imperial Ballroom Foyer, Fairmont Hotel Fairmont Foyer, Ballroom Imperial and Coffee Break, Regency imaging techniques in rodent rodent in techniques imaging Joseph Joseph Izatt; Dept. of Biomedical
in vivo Invited Invited Glen Ellen Glen Developing Developing FiO/LS/AO/AIOM/COSI/LM/SRS 2009 3:30 p.m.–4:00 p.m. , Retina Rodent the of Imaging Cellular FThQ4 • 3:00 p.m. models models will enhance our understanding of disease mechanisms and treatments. We review a fluorescence adaptive optics scan- ning laser ophthalmoscope that can resolve sub-cellular features retinae. rat in living Molecular Imaging with OCT, of Houston, USA. Houston, of In vivo available. not USA. Abstract Univ., Duke Engineering, FThQ Eye— Imaging in the • Molecular Continued FThQ32:30 p.m. • FiO This talk This Richard Torres, Michael Michael Torres, Richard Invited California Oscar Oscar D. Amit Ayala, S. Tianyi Paranjape, Vasan Venugopalan; Univ. of California at Irvine, USA. Irvine, at California of Univ. Venugopalan; Vasan FThP6 • 3:15 p.m. ExpanLaserThermo-Elastic - Induced1210nm of Measurement Source Swept Using Nanoparticles with Phantoms Tissue in sion Phase-Sensitive OCT, experimentalWang, Li demonstrate L. We USA. Ma, Austin, Keith at P. Johnston, Texas of Roman Kuranov, Univ. Thomas Milner; E. excited laser of expansion thermo-elastic of measurement for results nanoparticles absorbing near-infrared containing tissue phantoms we call nanorose. Our technique uses excitation at 1210nm and 1328nm. PhS-OCT at FThP5 • 3:00 p.m. - Distribu Multimer Factor Willebrand Von of Measurement FCS , Subtyping Disorder Coagulation for tions - of von Wille measurement present USA. We Univ., Levene; J. Yale brand Factor (vWF) multimer distributions using FCS as an early diagnostics. clinical laboratory to applicability its of example FThP42:30 p.m. • FThP in Interventional • Optics Medicine— Continued - Biophoton for Tools Computational Open-Source User-Friendly, ics, will introduce the Virtual Photonics Technology Initiative which tools computational open-source to aims disseminate and develop processes in for the cells of biophotonic simulation and tissues via user interface. graphical a user-friendly, Thursday, October 15 112 nm, Resonant Nonlinear Optical Transmission in Pure Water at 1445 •4:30p.m. FThS3 light storage. on mixing four-waveresonant of effects the study andvapor, Rb hot in transparency induced electromagnetically of conditions the under pulses signal optical weak of propagation the analyze College,USA, USA, Maxwell-Garnett and Bruggeman theory. by XRD and TEM. Optical absorption werespectra analyzed using wereanalyzed films The methods. sol-gel wereprepared the using transmission for 5mmpath was observed lengths. relative in increase 500% to Upwater. of resonance nm 1445 the on pulses femtosecond intense of transmission the investigating iveira Third-Order Nonlinearity of Nickel Nanocolloids, •4:00p.m. FThS1 Florida, USA,Presider Muzammil A.Arain; Dept. of Physics, Univ. of Materials •OpticalNonlinearPropertiesof FThS 4:00 p.m.–5:45p.m. Araújo ZrO Yokoyama,HironobuWakaki;MoriakiSakata, Tokai Univ., Japan. ticles in ZrO in ticles Par Nano Silver of Properties Optical on Analysis Dielectric •4:45p.m. FThS4 correlating values their with nanoparticles’ the sizes. absorption coefficient was explained with basis on a quantum model, nonlinearandindex nonlinear refractivebehavior their of the and synthesized were nanoparticles nickel containing Colloids Brazil. Irina Novikova Irina Four-Wave Mixing in a Stored Light , Regime •4:15p.m. FThS2 2 thin films containing silver nanoparticles in wide molar ratio David Lukofsky David 1 , Gemima Barros 2 1 We experimentally and theoretically and experimentally WeUniv., USA. Harvard ; 1 Univ. Federal de Pernambuco, Brazil, 2 2 Thin Film Prepared by Sol-Gel Method, Sol-Gel by Prepared Film Thin WeUSA. NRL, experimentresults anpresentof the 1 , Alexey V.Alexey Gorshkov, 1 , Ulf Österberg Ulf , 1 , André Galembeck Empire 2 ; 1 , Marc Currie Marc , 1 College of William & Mary,William& of College 1 , Luis A. Gómez 2 Univ. de Pernambuco, Nathaniel B. Phillips 2 Tâmara R. Ol- ; 1 Dartmouth Dartmouth 2 , Cid B. de de B. Cid , Eisuke Eisuke FiO 1 - , FThT3 •4:45p.m. FThT3 X-ray optics with sub-microradian precision. super-high-quality of profile surface the characterize to suitable both at-wavelength and conventional optical-metrology techniques program at the Advanced Light Source, LBNL, directed to establish Padmore; Lawrence Berkeley Natl. A. Lab,Howard Mochi, USA. IacopoWe Rekawa, B. describe a Senajith new R&D Morrison, Gregory V.Yashchuk, Richard Celestre, Tony Warwick, Wayne McKinney, R. for Nanofocusing at the ALS, At-Wavelength and Optical Metrology of Bendable X-Ray Optics •4:30p.m. FThT2 Multi-Modal Scanning X-Ray Microscopy, XRADIA Inc., USA.Abstract not available. Future Developments for Hard X-Ray Zone Plates, FThT1 •4:00p.m. FThT1 Thibault Oliver Bunk USA, Presider David Attwood; Lawrence Berkeley Natl. Lab, Instruments II •NanoscaleMethodsand FThT 4:00 p.m.–5:15p.m. the sizeofthe X-ray the probe. diffractive imaging allows image resolution to be increased beyond coherentcombination with The modes. contrast of variety wide a Fédérale de Lausanne, Switzerland. 1 , Martin Dierolf Martin , 1 ; 1 Paul Scherrer Inst., Switzerland, FiO/LS/AO/AIOM/COSI/LM/SRS 2009 Crystal 2 Invited Invited , Cameron M. Kewish M. Cameron , Sheng Yuan, Kenneth Goldberg, Valeriy Scanning Scanning X-ray microscopy offers
Andreas Menzel 2 École Polytechnique 1 , Franz Pfeiffer Franz , Wenbing Yun; 1 , Pierre 2, 2, ______• October 11–15,2009 For Fall Congress presentations onThursday, seepages132-136. NOTES Gold designs enable 3-Doptical integration insemiconductor wafer. waveguide and resonator developed The wafers. GaAs in crystals and two etching processes, is utilized to construct woodpile photonic USA. Simple fabrication method, which consists of two lithography 3-D Integrated Optics, WoodpileOn-Chip and forPhotonic Localization Light Crystal •4:15p.m. FThU2 FThU3 •4:30p.m. FThU3 information to quantum gravity, presented. be will talk new directions of Rydberg interactions, ranging from quantum this in measurements,fundamental of history long a has QED ity J. Dunningham, B. T. H. Varcoe; Univ. of Leeds, UK. Quantum Computing with Rydberg Atoms in Cavities, USA, Presider Mani Hossein-Zadeh; Univ. of New Mexico, •Micro-CavityDevicesIII FThU 4:00 p.m.–6:00p.m. strated with experimentally Q>20000. demon- are substratediamond crystal single a in centers vacancy whispering gallery mode microcavities optically coupled to nitrogen USA. Hewlett-PackardLabs, Barclay,E. Kai-Mei Fu,CharlesC. Santori, RaymondBeausoleil; G. Centers , NV Diamond to Coupled Microcavities On-Chip •4:00p.m. FThU1 Lingling Tang, Tomoyuki Yoshie; Duke Univ., Invited Valley FiO High-Q gallium phosphide (GaP) (GaP) phosphide gallium Microwave cav- M. Everitt, Paul Paul Thursday, October 15 113 We Whereas previous reported reported previous Whereas Invited Invited Sacramento of Science, Israel. Inst. Levin; Weizmann Anat Andrew Harvey, Mads Demenikov, Gonzalo D. Muyo, Muyo, Gonzalo D. Demenikov, Mads Harvey, Andrew 4:00 p.m.–6:00 p.m. 4:00 p.m.–6:00 FThX and Imaging • Computational II Photography Israel, Univ., Ben Gurion Rosen; Joseph Presider wavefront wavefront coding research has emphasised constancy of the PSF, in systems for occurs normally quality image optimal that show we which the PSF varies significantly; placing increased demands on algorithms. restoration image Optimization and of Optimization Hybrid Optical-DigitalApplication - Imag , ing Systems UK. Univ., Heriot-Watt Vettenburg; Tom 4-D Frequency Analysis of Computational Cameras for Depth of of Depth for Cameras Computational of Analysis Frequency 4-D Field , Extension and space lightfield 4-D the in systems field of depth extended study preserve. can they content frequency maximal the on bounds derive designs. all the DOF known of extending a new lens propose We FThX2 • 4:30 p.m. FThX1 • 4:00 p.m. Min-Suk Kwon; Kwon; Min-Suk Michelle Y.-C. Xu, J. , FiO For Fall Congress presentations on Thursday, see pages 132-135. Congress presentations on Thursday, For Fall Atherton October 11–15, 2009 Domenico Domenico de Ceglia, Maria Antonietta Vincenti, Vito • FThW2 • 4:15 p.m. Sub-Wavelength in Generation Harmonic Phase-LockedSecond Channels, Roppo, Neset Akozbek, Mark J. Bloemer, Michael Scalora; Charles M. Bowden Res. RDECOM, Ctr. AMSRD-AMR-WS-ST, USA. The - been has inves process generation harmonic second phase-locked tigated The thin,for extremely channels. - possibil sub-wavelength ity to circumvent resolution exploiting the trapping and dragging mechanisms between the fundamental and the phase-locked SH discussed. is pulse 4:00 p.m.–5:45 p.m. 4:00 p.m.–5:45 FThW and Devices Waveguides • Plasmonic Wisconsin-Milwaukee, of Univ. Mafi; Arash USA, Presider FThW3 • 4:30 p.m. Dispersion and Polarization Dependence on the Geometry of Non-Ideal effective theStripe simulate Plasmonic Waveguides We Canada. Toronto, of Univ. Aitchison; Stewart modes plasmon surface guided the of polarizations the and indices nm 1550 both at shapes, waveguide stripe silver the of function a as 633 nm wavelengths. and FThW4 • 4:45 p.m. Metal-Insulator-Silicon a on Based Interferometer Mach-Zehnder , Polariton Plasmon Surface a and Mode Waveguide Dept. of Optical Engineering, Sejong Republic Univ., of Korea. An which is Mach-Zehnder integrated-optical shorter interferometer, than 5 μm and has extinction larger than 60 dB, is proposed and investigated theoretically. It is based on a metal-insulator-silicon polariton. a surface plasmon mode and waveguide FThW1 • 4:00 p.m. Canada. We Experimental IPP Results Waveguides: and Integrated Toronto, Devices, of Univ. Aitchison; Stewart J. Xu, Y.-C. Michelle demonstrate a waveguide structure to confine waveguides, the of interface dispersion plasmon loss, the characterized We polaritons. splitters. power functional y-junction demonstrated as well as , 1 Baylor 2 Kirill LarinKirill Univ. of Houston, USA, Houston, of Univ. 1 ; 2 For measuring neuronal activity, planar planar activity, neuronal measuring For - Washing Turaga; Diwakar Holy, Timothy
Invited Glen Ellen Glen , Mary E. Dickinson E. Mary , FiO/LS/AO/AIOM/COSI/LM/SRS 2009 2 FThV2 • 4:30 p.m. Early Mammalian Embryonic Imaging at Different Develop- , Tomography Coherence Optical with Stages mental Irina Larina V. College of Medicine, USA. College of Live Medicine, imaging of mammalian embryos is important for many biomedical applications including early - as sessment of cardiovascular abnormalities. Here we demonstrate capability of OCT for high-resolution structural imaging of live stages. developmental different at embryos mouse 4:00 p.m.–6:00 p.m. 4:00 p.m.–6:00 FThV and OCT II • Microscopy at California of Univ. Venugopalan; Vasan USA, Presider Irvine, FThV1 • 4:00 p.m. FThV3 • 4:45 p.m. Biologi- of Imaging Muellermetric Two-Dimensional Complete cal , Tissue Heterodyned Using Optical Coherence USA. ATomography Univ., Northwestern Tseng; Shih Liu, Xue Shahriar, M. Selim tomography coherence optical heterodyned polarization-sensitive, system is used to of images measure partially-polarizedMueller-metric 4×4 reflections complete The from sample. a tendon porcine a system. such using produced is the sample within a layer Advances in Advances High-Speed Imaging by Objective-Coupled Planar , Microscopy Illumination USA. Louis, St. in Univ. ton illumination microscopy possesses advantages resolution of improve speed to and strategies optical low describe will I phototoxicity. function. neuronal measuring applications as well as NOTES California ______Thursday, October 15 114 Na[AlSiO Sukhovatkin of Silicates by Action of CO The Creation of Metallic and Silicon Nanoclusters at the Surface •5:15p.m. FThS6 formalism.function andobserved the results is is discussed based on a quantum-dotsfour-band envelop smaller for 2PA the of increasing slight a dots, absorption (2PA) is measured for different sizes of lead-salt quantum andComputer Engineering, Univ. Toronto,of Canada.Two-photon Post-annealing of HfOcility,Post-annealingof USA. Annealing, Modifications in the Optical Properties of Thin Film Oxides with •5:30p.m. FThS7 creationthe ofand metallic silicon nanoclusters at surface. the Quantum Dots, Quantum Salt Lead in AbsorptionTwo-Photon of Dependence Size •5:00p.m. FThS5 Materials—Continued •OpticalNonlinearPropertiesof FThS The continuous and pulsed CO pulsed and continuous The Federation.Univ.,Russian galieva, Anatolii M. Bondar’, Igor M. Swedov; Moscow States Mining irradiation (10 irradiation sic defects andsic defects photo-induced respectively. defects These effects are explained by modifications in the density breakdown. of laser subpicosecondintrin- the and μm, 1 at loss absorption Opticsand Photonics, Univ. ofCentral Florida, USA, USA, Carmen Menoni D. Nguyen David J. Hagan Univ. of Central Florida, USA, 3 StanfordUniv., USA, 4 2 ], rodonite - CaMn , L. Emmert Peter Peter Langston 3 , Edward H. Sargent H. Edward , 5 1,2 -10 1 , Eric W. Van Stryland ; Gero NootzGero 1 Colorado State Univ., USA, 7 W/cm 5:30 p.m.–8:00p.m. 2 , , W. Rudolph 1 , Dinesh Pate Dinesh , 2 Empire ) of silicates (quartz-SiO silicates of ) 4 2 ThomasJefferson Natl. Accelerator Fa - 1,2 3 Laser Radiation, 4 Edward S. Rogers Sr. Dept. of Electrical , Lazaro A. PadilhaA. Lazaro , [Si 5 3 O ; 2 2 and SiO and 15 1 , R. Route R. , CREOL and FPCE, College of College FPCE, and CREOL ], zircon - ZrSiO 1 1,2 , A. Markosyan , Larissa Levina 2 thin films affects the the affects films thin 3 2 , M. Fejer Univ. of New Mexico, Anel F. Mukhamed - 1 , Scott WebsterScott , 2 2 PhysicsDept., , nepheline - nepheline , 2 4 , Erik Krous Erik , etc.) lead to 3 Science Educators'Day, McCaw Hall, Frances C.Arrillaga Alumni Center, Stanford Univ., 326Galvez Street, Stanford, California 94305,Phone: 650.723.2021 , M. Shinn 3 , Vladimir 2 laser laser FiO 1 4 1 , , , Instruments II—Continued •NanoscaleMethodsand FThT Thank youforattending know yourthoughtson post-conference survey FiO/LS/AO/AIOM/COSI/LM/SRS 2009 FiO/LS/Fall Congress. via emailandletus Crystal Look foryour the program. ______• October 11–15,2009 For Fall Congress presentations onThursday, seepages132-136. NOTES Gold of optical pulses with an of extinction 24dB. uses a time-division sampling method to ensure complete isolation isolator The microcavities. conversionin wavelength adiabatic on based isolator optical integrated an presentWeTechnology, USA. , in Microcavities Active Isolator Optical Using Adiabatic Wavelength Conversion •5:00p.m. FThU4 relies on neither gain medium nor mirrors. reflective highly This unique resonance does not require distributed reflections, and it the resonance phenomenon in subwavelength high contrast gratings. Berkeley,simpleA USA. analyticformalism presentedis toexplain at CaliforniaVadimKaragodsky,Chang-Hasnain;Univ. of Connie Gratings, Contrast High Subwavelength in Resonance High-Q •5:15p.m. FThU5 to ~10 the new photothermal tuning spectroscopy technique. Q-factors up liquid microdroplets standing on a superhydrophobic surface using Turkey. Univ., Koç Kiraz;Yorulmaz, Alper C. Saime Mestre,Michael Gündogan, , TuningSpectroscopy Photothermal by Microdroplets Direct Measurement of High Q-Factors in Individual Salt-Water •5:30p.m. FThU6 Continued •Micro-CavityDevicesIII— FThU with an infrared laser. crodroplets standing on a superhydrophobic mi- NaCl-water surface single by of local heating modes gallery whispering the of tuning Turkey. Yorulmaz, Michael Mestre, Metin Muradoglu, Alper Kiraz; Koç Univ., lets on a Superhydrophobic Surface, Reversible Photothermal Tuning of Single Salt-Water Microdrop- •5:45p.m. FThU7 5 are observed from aremodes. degenerate observed gallery whispering We demonstrate large (up to 15 nm) and reversible spectral We present measurements of high quality (Q) factors in Ali W. Elshaari, Stefan F. Preble; Rochester Inst. of Valley FiO Yasin Karadag, Saime Cigdem Mustafa Mustafa Thursday, October 15 115 - Christo Ori Katz, Yaron Bromberg, Bromberg, Yaron Katz, Ori Sacramento James R. Fienup; Inst. of Optics, Univ. of Rochester, Rochester, of Univ. Optics, of Inst. Fienup; R. James Jixiong Jixiong Pu, Baosuan Chen, Ziyang Chen; Huaqiao , In the tightly focusing system, the modulation of FThX5 • 5:30 p.m. - Compu for Wavefronts Aspheric Highly of Propagation Efficient , Imaging tational needed wavefronts of propagation the of computation Efficient USA. by accomplished is systems imaging computational some analyze to approach. a divide-and-conquer FThX6 • 5:45 p.m. Modulation of and Polarization Phase of Beams in a Tight - Fo cusing System China. Univ., desired generate to used been have beams of phase and polarization beams, bottle sub-wavelength as such spots, focused sub-wavelength etc. beams top-hat and FThX and Imaging • Computational II—Continued Photography FThX35:00 p.m. • , Sensing Compressed via Imaging Ghost describe an We of Science, Inst. Israel. Weizmann Silberberg; Yaron ghost pseudothermal for algorithm reconstruction image advanced imaging, based on compressed sensing. Utilizing this algorithm, required the in reduction 10-fold a demonstrate experimentally we reconstruction. image faithful times for acquisition holographic The USA. Univ., Princeton Fleischer; W. Jason Barsi, pher - veri experimentally is media nonlinear in objects of reconstruction axiallyfor thick, optically a approach simple demonstrate fied. We results compare crystal and photorefractive a in potentials induced experiment. a scattering with FThX4 • 5:15 p.m. , Optically Potentials of InducedReconstruction Digital Michelle Y.-C. Xu, J. Changjun Min, Georgios Georgios Min, Changjun Triranjita Srivastava, Arun Triranjita FiO For Fall Congress presentations on Thursday, see pages 132-135. Congress presentations on Thursday, For Fall Atherton October 11–15, 2009 • FThW7 • 5:30 p.m. Design of Novel Plasmonic , Waveguide Stewart Canada. of Aitchison; Univ. present We Toronto, effective novel a of demonstrations experimental and analysis method index structure. waveguide polariton plasmon interface FThW and Waveguides • Plasmonic Devices—Continued FThW5 5:00 p.m. • All-Optical Absorption Switches in Subwavelength Metal- , Waveguides Plasmonic Dielectric-Metal compact extremely introduce We USA. Univ., State Louisiana Veronis; metal-dielectric- subwavelength for switches absorption all-optical either cavity a of consist switches The waveguides. plasmonic metal directly-coupled or side-coupled to the and waveguide, filled with coefficient. absorption tunable with material active an FThW6 • 5:15 p.m. Long Utilizing Couplers Directional of Characteristics Coupling Range Surface Plasmon , Polaritons Kumar; Indian Inst. of Delhi, Technology, India. We examine the characteristics coupling of lateral and vertical directional couplers utilizing long range surface plasmon polaritons. In both the minimum cases exhibit to found is stripes metal the of thickness optimum lengths. coupling
Chandra Chandra S. Alexey Yelleswarapu, Max Max Diem; Northeastern USA. Univ., Invited
Glen Ellen Glen Qiaofeng Qiaofeng Wu, Brian E. Alvin Applegate, T. Yeh; FiO/LS/AO/AIOM/COSI/LM/SRS 2009 We present a microscope that uses single source Abstract not available. not Abstract FThV and OCT II—Continued • Microscopy FThV45:00 p.m. • Cornea Microstructural and Mechanical Response Measured with Microscopy Optical Nonlinear and Coherence Optical Using Sub-10-fs Pulses, Co-registered nonlinear optical microscopy microscopy optical nonlinear Co-registered USA. Univ., A&M Texas (OCM) microscopy coherence optical domain Fourier and (NLOM) are integrated using sub-10-fs laser pulses. mechanical and This microstructure cornea NLOM-OCM characterize to used is setup depth. a function of as response Title Title to Be Announced, FThV5 • 5:15 p.m. Trimodal Optical , Microscopy and single detector, and capable of imaging multiple features like brightfield+fluorescence, phase+fluorescence, and edge need the without specimen biological the of enhanced+fluorescence fusion. and registration image of FThV6 • 5:30 p.m. Veraksa, Devulapalli Veraksa, G. V. L. N. Rao; of Univ. Massachusetts - Bos ton, USA. McCaw Hall, Frances C. Arrillaga Alumni Center, Stanford Univ., 326 Galvez Street, Stanford, California 94305, Phone: 650.723.2021 94305, Phone: California Stanford, Street, Galvez 326 Univ., Stanford Center, Alumni C. Arrillaga Frances Hall, McCaw Science Educators' Day, NOTES California 5:30 p.m.–8:00 p.m. ______