Frontiers in Optics 2010/Laser Science XXVI

FiO/LS 2010 wrapped up in Rochester after a week of cutting- edge optics and photonics research presentations, powerful networking opportunities, quality educational programming and an exhibit hall featuring leading companies in the field. Headlining the popular Plenary Session and Awards Ceremony were Alain Aspect, speaking on quantum optics; Steven Block, who discussed single molecule biophysics; and award winners Joseph Eberly, Henry Kapteyn and Margaret Murnane.

Led by general co-chairs Karl Koch of Corning Inc. and Lukas Novotny of the University of Rochester, FiO/LS 2010 showcased the highest quality optics and photonics research—in many cases merging multiple disciplines, including chemistry, biology, quantum mechanics and materials science, to name a few. This year, highlighted research included using LEDs to treat skin cancer, examining energy trends of communications equipment, quantum encryption over longer distances, and improvements to biological and chemical sensors. Select recorded sessions are now available to all OSA members. Members should log in and go to “Recorded Programs” to view available presentations.

FiO 2010 also drew together leading laser scientists for one final celebration of LaserFest – the 50th anniversary of the first laser. In honor of the anniversary, the conference’s Industrial Physics Forum brought together speakers to discuss Applications in Laser Technology in areas like biomedicine, environmental technology and metrology. Other special events included the Arthur Ashkin Symposium, commemorating Ashkin's contributions to the understanding and use of light pressure forces on the 40th anniversary of his seminal paper “Acceleration and trapping of particles by radiation pressure,” and the Symposium on Optical Communications, where speakers reviewed the history and physics of optical fiber communication systems, in honor of 2009 Nobel Prize Winner and “Father of Fiber Optics” Charles Kao.

The annual meeting serves as the venue for the Optical Society to announce its board election results. Donna T. Strickland of the University of Waterloo was elected as the 2011 vice president. Strickland will become president-elect the following year and serve as president of OSA in 2013. Naomi J. Halas, Eric Mazur and Jannick P. Rolland were all elected to serve three-year terms as directors at large. Maser pioneer James Gordon was also named honorary member of OSA for his numerous high-impact, seminal contributions to quantum electronics and photonics, including the first demonstration of the maser.

With higher attendance in 2010—more than 1,700 attendees and 85 exhibiting companies—and more than 850 technical presentations, FiO 2010 was the place to be for researchers, businesspersons, educators and anyone with an interest in the optics and photonics field. Join us next year as we head back to San Jose, California, USA for FiO 2011, October 16 – 20. About FiO/LS

FiO/LS Pre-Conference Schedule The Optical Society (OSA) The APS Division of Laser Science (DLS) Archives Frontiers in Optics 2007 Archive (PDF) Frontiers in Optics 2008 Archive (PDF) Frontiers in Optics 2009 Archive (PDF) Future Dates

Join your colleagues at the Rochester Riverside Convention Center in Rochester, NY USA, for a variety of themes, topics, and invited speakers at the Frontiers in Optics (FiO) 2010/Laser Science (LS) XXVI conference.:

• FiO 1: Optical Design, Fabrication and Instrumentation • FiO 2: Optical Sciences • FiO 3: Optics in Biology and Medicine • FiO 4: Optics in Information Science • FiO 5: Photonics • FiO 6: Quantum Electronics • FiO 7: Vision and Color

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 Call for Papers Submission Site Opens for Week of March 29, 2010 FiO/LS 2010

May 25, 2010, 12:00 p.m. noon EDT FiO/LS Papers Submission Deadline (16.00 GMT) Registration and Housing Open June 2010 Authors of submitted papers are notified July 2010 of acceptance/rejection

FiO/LS 2010 Conference Program August 2010 Available Online

September 28, 2010 Housing Deadline September 28, 2010 Pre-registration deadline

October 1, 2010 Post deadline Paper Submission Deadline

Authors of post deadline papers are October 12, 2010 notified of acceptance/rejection

FiO/LS held at the Rochester Riverside October 24–28, 2010 Convention Center

The Optical Society (OSA)

FiO 2010—the 94th OSA Annual Meeting—and LS XXVI 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 2010 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 XXVI 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 2010/LS XXVI Plenary Session and Awards Ceremony is on Monday, October 25.

Plenary Session

Frederic Ives Medal/Jarus W. Quinn Endowment Winner Presentation

Arthur L. Schawlow Prize in Laser Science Winner Presentation

Awards Recipients Ceremony

Hanbury Brown and Twiss and other atom- The Biophysics of Gene Regulation, Studied atom correlations: from photon to atom One Molecule at a Time quantum optics Steven M. Block Alain Aspect Stanford Univ., USA Laboratoire Charles Fabry de l’Inst. d’Optique, France Abstract: Advances have led to a new field, single molecule biophysics. Prominent among Abstract: Fifty years ago, R. Hanbury Brown the enabling technologies is the laser-based and R. Q. Twiss, invented a new method to optical trap, or optical tweezers. This lecture measure the angular diameter of stars, based on will focus on our current work on single the observation of correlations in light. The biological macromolecules. analysis of their experiment led to the development of modern quantum optics, based Biography: Steven M. Block is the S.W. on photon-photon correlation experiments. Ascherman Chair of Sciences in the departments of Applied Physics and Biology at Similar quantum correlations can be observed Stanford University. He holds degrees from with bosonic and fermionic atoms. I will Oxford University (B.A. 1974; M.A. 1978) and present such experiments, after recalling the the California Institute of Technology (Ph.D. significance of the HBT landmark experiment. 1983).

Biography: Born in 1947, Alain Aspect studied After postdoctoral work at Stanford (1983-87), at the Ecole Normale Supérieure de Cachan and he served as staff scientist at the Rowland Université d’Orsay. After a three years teaching Institute for Science, Lecturer at Harvard assignment in Cameroon, he started in 1974, a University (1987-1993), and then Professor of series of experiments on the foundations of Molecular Biology at Princeton University quantum mechanics. His "Experimental Tests (1994-1999) prior to joining the Stanford of Bell's Inequalities with Correlated Photons", faculty in 1999. were the subject of his doctorate thesis presented in 1983. In 1983-86, with his student Block is a fellow of the National Academy of Philippe Grangier, he developed the first source Sciences, the American Academy of Arts & of single photons and made fundamental Sciences, the American Association for the experiments on wave-particle duality of light. Advancement of Science, and the Biophysical Society. From 1985 to 1992 he worked with Claude Cohen-Tannoudji at the Laboratoire Kastler He is a recipient of the Delbrück Prize in Brossel de l’ENS and Collège de France, on Biological Physics from the American Physical cooling atoms with lasers, in particular “cooling Society (2008), the Young Investigator (1994) below the one photon recoil”. and Outstanding Investigator in Single Since 1991, he is head of the group of Atom Molecule Biophysics Awards from the BPS Optics that he has established at the Institut (2008), and served as the Biophysical Society’s d’Optique, now in Palaiseau. Recent scientific National Program Chair (1999) and President production concerns mainly Bose Einstein (2005-2006). Condensates, Atom Lasers, Quantum Atom Optics with metastable Helium, Anderson Block’s research lies at the interface of physics localization of ultracold atoms. and biology, particularly in the study of molecular motors, such as kinesin and RNA A CNRS senior scientist (”Directeur de polymerase, and the folding of nucleic acid- recherché CNRS”) at Laboratoire Charles based structures. His laboratory has pioneered Fabry de l’Institut d’Optique, Alain Aspect is the use of laser-based optical traps, also known also professor at Institut d’Optique and Ecole as ‘optical tweezers,’ to study the nanoscale Polytechnique, Palaiseau. motions of individual biomolecules.

He is member of the French Académie des Sciences, and of the Académie des Technologies, as well as of foreign academies (USA, Austria). He is a fellow of the Optical Society of America, of the European Optical Society, of the American Physical Society, and has received several honorary doctorates (Ecole Polytechnique and University of Montreal, National Australian University at Canberra, Herriott Watt University at Glasgow). He is frequently invited as a distinguished lecturer, and has received major awards, among them: the OSA Max Born award (1999), the CNRS Gold Medal (2005), the Quantum Optics senior prize of the European Physical Society (2009), the Wolf prize in Physics (2010). APS Arthur L. Schawlow Prize in Laser Science

The Arthur L. Schawlow Prize recognizes outstanding contributions to basic research which uses lasers to advance our knowledge of the fundamental physical properties of materials and their interaction with light.

2010 Recipients: Henry C. Kapteyn of JILA, University of Colorado, USA and Margaret M. Murnane of JILA, University of Colorado, USA

Citation: For critical advances in the science and technology of high-harmonics generation, with particular relevance to sub-femtosecond pulse generation and related attosecond-scale physics.

Schawlow Prize Lecture Title: "Attosecond Light and Science at the Time-scale of the Electron - Coherent X-Rays from Tabletop Ultrafast Lasers"

Abstract: Using the extreme nonlinear process of high harmonic generation, light from an ultrafast laser can be coherently upshifted, generating bright ultrafast coherent beams extending into the soft and soon hard x-ray regions of the spectrum. Applications in molecular and materials dynamics, as well as nano- and attosecond science, will be discussed.

Biographies: Henry Kapteyn and Margaret Murnane have made important contributions to the development of coherent x-ray sources and have helped establish the foundations of attosecond science. In the 1990s, they led the development of new ultrafast laser technologies using Ti:sapphire to generate unprecedented high peak power pulses only a few optical cycles in duration. They then did pioneering work in developing an understanding of extreme nonlinear optics to efficiently upshift femtosecond laser light into the soft X-ray region of the spectrum.

Henry Kapteyn is Professor of Physics and Fellow of JILA, University of Colorado, Boulder. He holds a B.S. from Harvey Mudd College, M.S. from Princeton University and a Ph.D. from the University of California, Berkeley. He previously held faculty positions at Washington State University and the University of Michigan. He is a Fellow of OSA, APS, and AAAS, and recipient of the OSA Adolph Lomb Medal, the ACS Ahmed Zewail Award, and the R.W. Wood Prize.

Margaret Murnane is Professor of Physics and Fellow of JILA, University of Colorado Boulder. She received her B.S. and M.S. degrees from University College Cork, Ireland, and her Ph.D. from the University of California, Berkeley. She previously held faculty positions at Washington State University and the University of Michigan. She is member of the NAS, a Fellow of OSA, APS and AAAS, and recipient of a MacArthur Foundation Fellowship, the ACS Ahmed Zewail Award and the R.W. Wood Prize. OSA Frederic Ives Medal/Jarus W. Quinn Endowment

The Frederic Ives Medal/Jarus W. Quinn Endowment is OSA’s highest award and recognizes overall distinction in optics.

2010 Recipient: Joseph H. Eberly, University of Rochester, U.S.A.

Citation: For many important research contributions to quantum optics and optical physics, his leadership as a teacher and educator, and his tireless and visionary service to the optics community

Ives Medal Address Title: “When Malus tangles with Euclid, who wins?"

Biography: Joseph Eberly has a B.S. degree from Pennsylvania State University and a Ph. D from Stanford University. Eberly has been teaching graduate and undergraduate classes in the department of physics and astronomy at the University of Rochester since the 1970s. He is currently the Andrew Carnegie Professor of Physics and also a Professor of Optics.

His long-time research interests in quantum optics and radiation physics have led to a number of discoveries and innovations; including the initial description of the spontaneous collapse and revival effect, the first observation of Bessel beams, predictions of the recently observed non- spreading localized states of electrons in atoms, and the sudden-death effect in quantum entanglement.

Eberly received the Charles Hard Townes Award from OSA, the Goergen Award for Creative Undergraduate Teaching from the University of Rochester and has been designated a Distinguished Alumnus of the Penn State College of Science. He was awarded the Smoluchowski Medal by the Polish Physical Society. Eberly has mentored more than 35 Ph.D. graduates and published more than 350 research papers, as well as three graduate texts: Optical Resonance and Two-Level Atoms with L. Allen; Lasers and Laser Physics, both with P.W. Milonni.

He is the founding editor of the journal Optics Express, and he has served as president of OSA and chair of the APS Division of Laser Physics, on the APS Council and the AIP Board of Governors, and as a member of the Advisory Boards of the Kavli Institute for Theoretical Physics and ITAMP-Harvard. He is a Fellow of OSA and APS and he is an elected Foreign Member of the Polish Academy of Science.

Honors to be presented during the Award Ceremony

APS/Division of Laser Science Awards AND HONORS

APS/Division of Laser Science Fellowships

Arthur L. Schawlow Prize Recipients: Henry C. Kapteyn, JILA, University of Colorado and Margaret M. Murnane, JILA, University of Colorado

OSA AWARDS AND HONORS OSA Fellowships

OSA Honorary Member Recipient: Arthur Ashkin, Alcatel-Lucent Bell Labs, USA

Frederic Ives Medal/Jarus W. Quinn Endowment Recipient: Joseph H. Eberly, University of Rochester, USA

Esther Hoffman Beller Medal Recipient: Eustace Dereniak, University of Arizona, USA

Distinguished Service Award Recipient: Gary C. Bjorklund, Bjorklund Consulting, USA

Paul F. Forman Engineering Excellence Award Recipient: Alan E. Willner, Univ. of Southern California, USA

Joseph Fraunhofer Award/Robert M. Burley Prize Recipient: Shin-Tson Wu, University of Central Florida, USA Edwin H. Land Medal Recipient: Eli Peli, Schepens Eye Research Institute, USA

OSA Leadership Award Recipient: Rod C. Alferness, Bell Laboratories, Alcatel-Lucent,USA

Emmett N. Leith Medal Recipient: Juris Upatnieks, University of Michigan/Environmental Research Institute of Michigan (retired), USA

Adolph Lomb Medal Recipient: Jeremy O’ Brien, University of Bristol, U.K.

William F. Meggers Award Recipient: Frédéric Merkt, ETH Zürich, Switzerland

FiO Invited Speakers

Check back often as speakers are still being confirmed and updated!

FiO 1: Optical Design, Fabrication and Instrumentation FiO 2: Optical Sciences FiO 3: Optics in Biology and Medicine FiO 4: Optics in Information Science FiO 5: Photonics FiO 6: Quantum Electronics FiO 7: Vision and Color

View Symposia Speakers

FiO 1: Optical Design, Fabrication and Instrumentation

1.1 Image-Based Wavefront Sensing

Wednesday, October 27, 2010

Invited Speakers:

10:30 AM, Measurement-Diverse Wavefront Sensing, Rick Paxman, General Dynamics Corp., USA

11:00 AM, Rays and Waves in Wavefront Sensing, Jim Fienup, Univ. of Rochester, USA 4:00 PM, Sequential Diversity Imaging: Phase Diversity with AO Changes as the Diversities, Bob Gonsalves, Tufts Univ., USA

4:30 PM, JWST Integrated System Modeling, Scott Knight, Ball Aerospace and Technologies Corp., USA

1.2 Diffractive and Holographic Optics

Thursday, October 28, 2010

Tutorial Speaker:

1:30 PM, What Is and Is Not a Hologram and Why it Matters, H. John Caulfield, Alabama A&M Univ., USA

Invited Speakers:

2:15 PM, 3-D Optics: From Diffractive to Subwavelength, George Barbastathis; MIT, USA

4:00 PM, Theoretical and Practical Implementation of Novel Nanostructured Diffractive and Micro-Optics, Mohammad R. Taghizadeh, Andrew J. Waddie; Heriot-Watt Univ., UK

4:30 PM, Plasmonic Diffractive Optics - Its Analogy to Classical Diffractive Optics and Use for Subwavelength Metallic Devices, Byoungho Lee¹, Junghyun Park¹, Seung-Yeol Lee¹, Hwi Kim², Seong-Woo Cho¹, Seyoon Kim¹; ¹Seoul Natl. Univ., Republic of Korea, ²Korea Univ., Republic of Korea

1.3 Three-Dimensional Structure Design, Fabrication and Nanopatterning

Wednesday, October 27, 2010

Invited Speakers:

1:30 PM, Active and Passive Nanophotonics for Information Systems Applications, Shaya Fainman, Univ. of California at San Diego, USA

2:00 PM, Nanopatterning Technology and the Future of Semiconductor Devices beyond 32nm, Bruce W. Smith, Rochester Inst. of Technology, USA

Thursday, October 28, 2010

Invited Speakers:

4:00 PM, Understanding Three-Dimensional Meta-Materials, from Refractive Index Concept to Rigorous Photonic Band Theory, Shanhui Fan, Stanford Univ., USA 4:30 PM, 3-D Integration of RF and Photonic Devices for High Frequency Operation, Dennis Prather, Univ. of Delaware, USA

1.4 Optical Design for Biomedical Systems (Joint with FiO 3: Optics in Biology and Medicine)

Tuesday, October 26, 2010

Invited Speakers:

10:30 AM, Degrees of Freedom in Computational Volume Optics, Rafael Piestun, Univ. of Colorado, USA 11:00 AM, Optical Ring Resonator Based Biological and Chemical Sensors, Xudong (Sherman) Fan, Jonathan D. Suter, Yuze Sun, Jing Liu, Hao Li, Karthik R. C. Balareddy; Univ. of Michigan, USA

Wednesday, October 27, 2010

Invited Speakers:

4:00 PM, High Resolution Optical Volumetric Imaging of Blood Perfusion with Microcirculation Tissue Beds, Ruikang Wang, Oregon Health and Science Univ., USA 4:30 PM, Breaking the Optical Diffusion Limit: Photoacoustic Tomography, Lihong Wang, Washington Univ. in St. Louis, USA

1.5 Optical Design with Unconventional Polarization

Wednesday, October 27, 2010

Tutorial Speaker:

8:00 AM, Some Applications of the Unified Theory of Coherence and Polarization of Light, Emil Wolf, Univ. of Rochester, USA

Invited Speakers:

8:45 AM, Unconventional Polarization States Applied to Projection Imaging, Thomas Brown, Univ. of Rochester, USA

1:30 PM, Polarization and the Focusing of Light, Colin Sheppard, Natl. Univ. of Singapore, Singapore

2:00 PM, Polarization and Modal Degrees of Freedom for Tight Confinement of Light, Uriel Levy, The Hebrew Univ. of Jerusalem, Israel 1.6 Astrophotonics (joint with FiO 5: Photonics) NEW!

Tuesday, October 26, 2010

Invited Speakers:

4:00 PM, Fibers Are Looking Up: Optical Fiber Transition Structures in Astrophotonics, Tim Birks¹, Antonio Diez², Jose L. Cruz², Sergio G. Leon-Saval³, Dominic F. Murphy4; ¹Univ. of Bath, UK, ²Univ. of Valencia, Spain, ³Univ. of Sydney, Australia, 4Univ. of Adelaide, Australia

4:30 PM, Processing in Next Generation Telescope Arrays: Coherent Signal Combining, Pierre Kern, Univ. of Grenoble, France

Wednesday, October 27, 2010

Tutorial Speaker:

8:00 AM, Astrophophotonics: A New Generation of Astronomical Instruments, Joss Bland- Hawthorn, Univ. of Sydney, Australia

Invited Speaker:

9:00 AM, Coronagraphy for Exo-Planetary Detection, Richard Lyon, NASA Goddard Space Flight Ctr., USA

1.7 Adaptive Optics for the Eye (joint with FiO 7: Vision and Color)

Tuesday, October 26, 2010

Invited Speakers:

8:00 AM, Multifunctional Imaging Device for Adaptive Optics Compensation in Humans and Small Animals, Daniel X. Hammer1, R. Daniel Ferguson1, Mircea Mujat1, Ankit H. Patel1, Nicusor Iftimia1, T. Y. P. Chui2, J. D. Akula2, A. B. Fulton2; 1Physical Sciences Inc., USA, 2Children’s Hospital and Harvard Medical School, USA.

8:30 AM, Designing AO Retinal Imaging Systems for Real World Uses: Issues and Limitations, Steve Burns, Indiana Univ., USA

9:00 AM, Optical Design of Clinical Adaptive Optics Instruments for Retinal Imaging, Alf Dubra, Univ. of Rochester, USA

8:00 AM, Multifunctional Imaging Device for Adaptive Optics Compensation in Humans and Small Animals, Dan Hammer, Physical Sciences Inc., USA

View speakers for 5.6 Photonics and Optics for Energy Efficiency and Sustainability

FiO 2: Optical Sciences

2.1 Attosecond Optics and Technology

Tuesday, October 26, 2010

Tutorial Speaker:

4:00 PM, Carrier to Envelope Offset and Carrier to Envelope Phase—How Their Control Impacts Femtosecond and Attosecond Phenomena, Jean-Claude Diels, Univ. of New Mexico, USA

Invited Speakers:

5:00 PM, High-Order Harmonic Generation on Plasma Mirrors: Toward Attosecond Sources of Second Generation, Fabien Quere, Inst. du CEA Saclay, France

Wednesday, October 27, 2010

Invited Speakers:

8:00 AM, XUV Time-Domain Spectroscopy Using Isolated Attosecond Pulses from Double Optical Gating, Zenghu Chang; Kansas State Univ., USA

9:00 AM, Molecular Orbital Imaging Using Laser Driven Attosecond Emission, Bertrand Carre, SPAM, Inst. du CEA Saclay, France

2.2 Advances in High-Energy Ultrafast Laser Systems

Monday, October 25, 2010

Invited Speakers:

5:00 PM, Advances in Energetic Short-Pulse Fiber Lasers, Michael J. Messerly1, Jay W. Dawson1, John K. Crane1, David J. Gibson1, Constantin Haefner1, Miroslav Y. Shverdin1, Henry H. Phan1, Richard P. Hackel1, Craig W. Siders1, Christopher P. J. Barty1, Matthew A. Prantil2; 1Photon Science and Applications Program, Lawrence Livermore Natl. Lab, USA, 2Lawrence Berkeley Natl. Lab, USA.

5:30 PM, Grating Development for High-Peak-Power CPA Laser Systems, Terrance J. Kessler; Lab for Laser Energetics, Univ. of Rochester, USA.

Tuesday, October 26, 2010 Invited Speakers:

10:30 AM, New Source of Ultra-Broadband Mid-IR Frequency Combs for Spectroscopic Applications, Konstantin Vodopyanov1, Nick C. Leindecker1, Alireza Marandi1, Robert L. Byer1, Vladimir Pervak2; 1Stanford Univ., USA, 2Ludwig-Maximilians-Univ. München, Germany

Tutorial Speaker: 1:30 PM, Optical Dispersion Management in Laser Amplifier Systems, Catherine LeBlanc, LULI - École Polytechnique, France

Invited Speakers: 3:00 PM, Development and Operation of Large-Aperture Tiled-Grating Compressors for High-Energy, Petawatt-Class Laser Systems, Jie Qiao, A. Kalb, T. Nguyen, D. Canning, J. Price; Lab for Laser Energetics, Univ. of Rochester, USA

2.3 Laser-Plasma Based Particle Acceleration

Wednesday, October 27, 2010

Tutorial Speaker:

10:30 AM, Laser Plasma Accelerators: Concepts, Progress and Dreams, Wim Leemans, Lawrence Berkeley Natl. Lab, USA

Invited Speakers:

11:15 AM, Acceleration of Electrons by A Laser Wakefield Accelerator (LWFA) Operating in the Self-Guided Regime, Chan Joshi, C. Clayton¹, D. Froula², K. Marsh¹, A. Pak¹, J. Ralph¹,²; ¹Univ. of California at Los Angeles, USA, ²Lawrence Livermore Natl. Lab, USA

1:30 PM, Recent Advances in Proton Acceleration and Beam Shaping, Marcus Roth¹, V. Bagnoud², T. Burris³, S. Busold¹, T. Cowan³, O. Deppert¹, M. Geissel4, D. P. Grote5,6, K. Harres¹, G. Hoffmeister¹, G. Logan5, F. Nürnberg¹, G. Schaumann¹, M. Schollmeier4, D. Schumacher¹; ¹Technische Univ. Darmstadt, Germany, ²Helmholtzzentrum für Schwerionenforschung, Germany, ³Forschungszentrum Dresden-Rossendorf, Germany, 4Sandia Natl. Labs, USA, 5Lawrence Berkeley Natl. Lab, USA, 6Lawrence Livermore Natl. Lab, USA

2:00 PM, Ion Acceleration with Ultra-Intense Lasers, Anatoly Maksimchuk, Univ. of Michigan, USA

2:30 PM, Particle Acceleration by the Light Pressure of High-Power Laser Pulses, Joerg Schreiber, MPQ, Garching, Germany

2.4 High-Peak-Power THz Field Generation and Applications

Thursday, October 28, 2010 Tutorial Speaker:

1:30 PM, High-Peak-Power THz Field Generation and Applications, Keith Nelson, MIT, USA

Invited Speakers: 4:00 PM, High Energy THz Pulse Generation by Tilted Pulse Front Excitation and Its Applications, János Hebling, József A. Fülöp, László Pálfalvi, Gábor Almási; Dept. of Experimental Physics, Univ. of Pécs, Hungary

4:30 PM, Ultrafast THz Studies of Electronic Dynamics and Correlations in Carbon Nanomaterials, Robert Kaindl, Lawrence Berkeley National Lab., USA

2.5 Laser Systems for Fusion and Fast Ignition

Thursday, October 28, 2010

Invited Speakers:

8:00 AM, Progress in Experiments for the National Ignition Campaign, Brian MacGowan, Lawrence Livermore Nat'l Lab., USA

8:30 AM, Inertial Confinement Fusion Research at the Laboratory for Laser Energetics, David Meyerhofer, Lab. for Laser Energetics, Univ. of Rochester, USA

9:00 AM, Fast Ignition Integrated Experiments Using Gekko-XII and LFEX Lasers, Hiroyuki Shiraga, Inst. of Laser Engineering, Osaka Univ., Japan

9:30 AM, Status of the HiPER Project, Chris Edwards, Central Laser Facility, Rutherford Appleton Lab, UK

FiO 3: Optics in Biology and Medicine

3.1 Optical Trapping and Manipulation

Tuesday, October 26, 2010

Invited Speakers:

10:30 AM, Suppression of Brownian Motion Explores Cooperativity for Single Multi- Subunit Enzymes in Solution, Yan Jiang¹,², Nick Douglas³, Nick Conley&sup4;, Eric Miller³, Judith Frydman³, W.E. Moerner¹; ¹Chemistry Dept., Stanford Univ., USA, ²Applied Physics Dept., Stanford Univ., USA, ³Biology Dept., Stanford Univ., USA, &sup4;Radiology Dept., Stanford Univ., USA 11:30 AM, Optical Sculpting: Changing the Shape of Micromanipulation, Kishan Dholakia, Janelle Shane, Michael Mazilu, Tomas Cizmar; Univ. of St. Andrews, UK

Wednesday, October 27, 2010

10:30 AM, High-Speed Holographic Tweezers and Imaging, Miles Padgett¹, Richard Bowman¹, Daryl Preece¹, Arran Curran¹, Graham Gibson¹, David Carberry², Mervyn Miles²; ¹Univ. of Glasgow, UK, ²Univ. of Bristol, UK

11:30 AM, Applications of Spatial Light Modulators for Optical Trapping and Imaging, Monika Ritsch-Marte, Medizinische Univ. of Innsbruck, Germany

3.2 Microscopy and OCT

Monday, October 25, 2010

4:00 PM, Improving 2-Photon Microscopy by Beam Multiplexing and Extended Excitation Bandwidth, Thomas Pingel, LaVision Biotec, Germany

Tuesday, October 26, 2010

Invited Speakers:

8:00 AM, Nonlinear Optical Tools for Studying Small-Stroke at Microscopic Scales, Nozomi Nishimura, Cornell Univ., USA

Tutorial Speaker:

4:45 PM, Coherence Imaging, Adam Wax, Duke Univ., USA

3.3 Optics for Diagnostics and Therapy

Monday, October 25, 2010

1:30 PM, Monitoring Breast Cancer Tumor Response at Different Timepoints during Pre- Surgical Chemotherapy with Diffuse Optical Spectroscopic Imaging, Albert Cerussi¹, Vaya W. Tanamai¹, Darren Roblyer¹, Shigeto Ueda¹, Amanda F. Durkin¹, Rita S. Mehta², David Hsiang², John Butler², Bruce J. Tromberg¹; ¹Beckman Laser Inst., Univ. of California at Irvine, USA, ²Chao Comprehensive Cancer Ctr., Univ. of California at Irvine, USA

Tuesday, October 26, 2010

1:30 PM, Laser Speckle Imaging of Blood-Flow Dynamics During Laser Surgery of Vascular Birthmarks, Bernard Choi; Univ. of California at Irvine, USA

View speakers for 1.4 Optical Design for Biomedical Systems View speakers for 6.3 Non-Linear Imaging

View speakers for7.2 Emerging in vivo Imaging Techniques for Ocular Imaging

FiO 4: Optics in Information Science

4.1 Encoding Optical Information—Nano-Photonics, Diffractive Optics and Refractive Optics for Shaping Optical Signals

Thursday, October 28, 2010

Invited Speakers:

1:30 PM, Fundamental Limits to Optical Components, David Miller, Stanford Univ., USA

2:00 PM, Progress towards Windows Performing Forbidden Light-Ray Direction Changes, Johannes Courtial, Univ. of Glasgow, UK

2:30 PM, On Breaking The Abbé Diffraction Limit In Optical Nanopatterning, Nicole Brimhall1, Trisha Andrew2, Rajakumar Manthena1, Mohit Diwekar1, Rajesh Menon1; 1Univ. of Utah, USA, 2MIT, USA.

4.2 Sensing in Higher Dimensions—Theory and Hardware for Computational Imaging

Wednesday, October 27, 2010

Invited Speakers:

10:30 AM, Computational Photography in 4-D, 6-D and 8-D, Ramesh Raskar, MIT, USA

Thursday, October 28, 2010

Invited Speakers:

10:30 AM, Spatio-Temporal Processing Methods for Mitigating Bandwidth Issues Associated with Advanced Infrared Sensors, Dean Scribner, Northrop Grumman, USA

4.3 Plasmonics and Metamaterials for Information Processing

Wednesday, October 27, 2010

Invited Speakers: 1:30 PM, Infrared Plasmonic Metamaterials for Slow-Light Applications, Gennady Shvets, Univ. of Texas Austin, USA

Thursday, October 28, 2010

Invited Speakers:

1:30 PM, Super-Resolution Imaging Based on Interfering Plasmon Waves, Peter So, MIT, USA

4:00 PM, Simple Demonstration of Visible Evanescent Wave Enhancement with Far-Field Detection, Rene Lopez, Univ. of North Carolina at Chapel Hill, USA

4.4 Structured Wavefields for Communications and Sensing

Monday, October 25, 2010

Invited Speakers:

1:30 PM, Effects of Type of Incidence on the Second and Fourth Order Moment Parameters Evaluated in Turbulent Atmosphere, Yahya Baykal, Cankaya Univ., Turkey

4:00 PM, Optical Coherence Microscopy Using Bessel Beam, Kye-Sung Lee, Univ. of Rochester, USA

5:30 PM, Advanced Studies of ‘Non-Diffracting’ Light Fields, Kishan Dholakia, Jörg Baumgartl, Tomas Cizmar, Xanthi Tsampoula, Frank Gunn-Moore, Michael Mazilu; Univ. of St. Andrews, United Kingdom.

4.5 Generalized Imaging and Non-Imaging Techniques for Diagnostics and Sensing

Tuesday, October 26, 2010

Invited Speakers:

10:30 AM, Quantum Inspired Imaging with Compressive Sensing, Ori Katz, Yaron Bromberg, Yaron Silberberg; Weizmann Inst. of Science, Israel.

Wednesday, October 27, 2010

Invited Speakers:

4:15 PM, Infrared Spectroscopic Imaging for Label-Free and Automated Histopathology, Rohit Bhargava, Rohith K. Reddy, Jason Ip, Frances N. Pounder, Matthew V. Schulmerich, David Mayerich, Xavier Llora, Rong Kong, Michael J. Walsh; Univ. of Illinois at Urbana- Champaign, USA Thursday, October 28, 2010

Invited Speakers:

10:30 AM, Spatial Light Interference Microscopy (SLIM), Zhuo Wang, Huafeng Ding, Gabriel Popescu; Univ. of Illinois at Urbana-Champaign, USA

FiO 5: Photonics

5.1 Novel Fiber Optical Devices

Tuesday, October 26, 2010

Invited Speakers:

10:30 AM, Self Assembled Periodicity in a Liquid Filled Hollow Optical Fiber, Kyunghwan Oh¹, Hojoong Jung¹, Sohee An¹, Yongmin Jung²; ¹Yonsei Univ., Republic of Korea, ²Optoelectronics Res. Ctr., Univ. of Southampton, UK

10:30 AM, Short-Pulse Fiber Lasers Based on Dissipative Solitons, Frank Wise; Cornell Univ., USA

4:00 PM, Semiconductor Core Optical Fibers, John Ballato; Clemson Univ., USA

Wednesday, October 27, 2010

Invited Speakers:

10:30 AM, Fibers for Dispersion Management in fs Fiber Lasers, Lars Grüner-Nielsen, Kim G. Jespersen, Martin E. V. Pedersen, Bera Pálsdóttir; OFS Denmark, Denmark

4:00 PM, Manipulation of Pulse Duration and Wavelength Conversion in Optical Fibres, William Wadsworth; Univ. of Bath, UK

5.2 Optical Communication

Tuesday, October 26, 2010

Invited Speakers:

4:00 PM, Rate-Adaptive Transmission Techniques for Optical Fiber Systems, Joseph Kahn; Stanford Univ., USA 4:30 PM, Digital Compensation of Fiber Nonlinearities, Guifang Li; CREOL, Univ. of Central Florida, USA

Wednesday, October 27, 2010

Invited Speakers:

10:30 AM, Promising Technologies for Capacity Growth in Future Optical Networks, R. J. Essiambre; Bell Labs, Alcatel-Lucent, USA

11:15 AM, Next Generation 400 Gb/s Transmission, I. B. Djordjevic; Univ. of Arizona, USA5.3 Integrated Optics

Monday, October 25, 2010

Invited Speakers:

4:00 PM, Monolithic Ge-on-Si Lasers, Lionel Kimerling, Jifeng Liu; MIT, USA

Tuesday, October 26, 2010

Invited Speakers:

8:00 AM, Noise, Broadband Gain, Inverse Stimulated Scattering, and Extreme Value Fluctuations; Recent Developments in Silicon Raman Amplifiers, Bahram Jalali; Univ. of California at Los Angeles, USA

9:00 AM, Nonlinear Mixing in Silicon Waveguides for Short Wave Infrared and Mid- Infrared Applications, Sanja Zlatanovic; Univ. of California at San Diego, USA

Wednesday, October 27, 2010

Invited Speakers:

2:00 PM, Theoretical Investigation of Attractive Optical Force in Periodically-Patterned Silicon Waveguides, Jing Ma, Michelle Povinelli; Univ. of Southern California, USA

5.4 Photonic Sensing Devices

Monday, October 25, 2010

Invited Speakers:

1:30 PM, Long-Term Monitoring of Local Temperature and Strain Changes in a Buried Fiber-Optic Cable Using Brillouin OTDR, Jon Nagel; AT&T Labs, USA 2:30 PM, Raman-Based Distributed Temperature Sensors, Arthur Hartog; Schlumberger, UK

4:30 PM, New Imaging and Sensing Techniques Base on Surface Plasmon Resonance, N. J. Tao, Arizona State Univ., USA

Wednesday, October 27, 2010

Invited Speakers:

8:00 AM, Sensor Challenges for Deep Tissue Imaging, Martin Leahy, Univ. of Limerick, Ireland

5.5 Novel Hybrid Integration NEW!

Tuesday, October 26, 2010

Invited Speakers:

1:30 PM, Hybrid Integration of III-V and Si for Photonic Integrated Circuits, John Bowers; Univ. of California at Santa Barbara, USA

2:30 PM, Active-Passive Photonic Integration with an Eye Toward Large Scale Integration, James Jaques; LGS Innovations, LLC, USA

3:00 PM, Hybrid Chalcogenide/Lithium Niobate, Christi Madsen; Texas A&M Univ., USA

Wednesday, October 27, 2010

Invited Speakers:

8:00 AM, Rare-Earth-Ion Doped Waveguide Amplifiers and Lasers in Alumina and Polymers, Markus Pollnau, Univ. of Twente, Netherlands

9:00 AM, Optimized Nonlinear Optical Molecules for Silicon-Organic-Hybrid Systems, Ivan Biaggio, Lehigh Univ., USA

5.6 Photonics and Optics for Energy Efficiency and Sustainability (joint with FiO 1: Optical Design, Fabrication and Instrumentation) NEW!

Monday, October 25, 2010

Invited Speakers: 1:30 PM, Luminescent Solar Concentrators: From Optical Heat Pumps to Solar Pumped Lasers, C. Rotschild¹, M. Tomes², H. Mendoza¹, T. Carmon², M. Baldo¹; ¹MIT, USA, ²Univ. of Michigan, USA

2:00 PM, Depleted Heterojunction Colloidal Quantum Dot Solar Cells, Illan Kramer, Univ. of Toronto, Canada

2:30 PM, Nanoscale Photon Management for Efficient Photovoltaic Energy Harvesting, Mark Brongersma, Stanford Univ., USA

Tuesday, October 26, 2010

Invited Speakers:

8:00 AM, Organic Semiconductors for Photovoltaic and Light-Emitting Devices: Status and Promise, Bernard Kippelen, School of Electrical and Computer Engineering., Georgia Tech, USA

8:30 AM, Optical Transmission Energy Consumption in the Internet, Dan Kilper, Bell Labs, Alcatel-Lucent, USA

9:00 AM, Photonics and Optics for Energy Efficiency and Sustainability – Is this Green Photonics?, Michael Lebby, Optoelectronics Industry Development Association, USA

View speakers for 1.6 Astrophotonics

View speakers for 6.6 Nonlinear Optics in Micro/Nano-Optical Structures

FiO 6: Quantum Electronics

6.1 Opto-Mechanics and Quantum Measurement

Tuesday, October 26, 2010

Invited Speakers:

10:30 AM, Quantum Back Action in Tabletop Interferometers, Jack Harris, Yale Univ., USA

11:30 AM, Silicon Monolithic Acousto-Optic Modulators, Sunil Bhave, Cornell Univ. USA

4:00 PM, The Engima of Optical Momentum, Stephen M. Barnett; Univ. Strathclyde, UK

4:45 PM, Testing Macroscopic Quantum Superpositions, Dirk Bouwmeester, Univ. of California at Santa Barbara, USA 6.2 Quantum Information and Communciations

Monday, October 25, 2010

Invited Speakers:

2:45 PM, Quantum Optics in Wavelength Scale Structures, John Rarity, Univ. of Bristol

4:00 PM, Interference of Photons from Remote Solid-State Sources, A. J. Bennett¹, R. B. Patel¹,², I. Farrer², C. A. Nicoll², D. A. Ritchie², Andrew Shields¹; ¹Toshiba Res. Europe Ltd., United Kingdom, ²Cavendish Lab, Cambridge Univ., UK

Tuesday, October 26, 2010

Invited Speakers:

2:00 PM, Quantum Limits to Lossy Optical Interferometry, Luiz Davidovich; Univ. Federal do Rio de Janeiro, Brazil.

6.3 Non-Linear Imaging (joint with FiO 3: Optics in Biology and Medicine)

Monday, October 25, 2010

Invited Speakers:

1:30 PM, Non-Linear Imaging with Ultrashort Shaped Pulses, Marcos Dantus, Michigan State Univ., USA

2:15 PM, Nonlinear Imaging of Coherent Fields Demetri Psaltis, École Polytechnique Fédérale de Lausanne, Switzerland

3:00 PM, Stimulated Raman Scattering Microscopy for Biology and Medicine, Sunney Xie, Harvard University, USA

6.4 Nonlinearities and Gain in Plasmonics and Metamaterials

Wednesday, October 27, 2010

Invited Speakers:

8:00 AM, Metamaterials and Symmetry, Xiang Zhang, Univ. of California at Berkeley, USA

9:30 AM, Switchable and Nonlinear Metamaterials: Controlling Light on the Nanoscale, Nikolay I. Zheludev, Univ. of Southampton, UK Thursday, October 28, 2010

Invited Speakers:

10:30 AM, Active Plasmonic Metamaterials, Mikhail A. Noginov, Norfolk State Univ., USA

11:30 AM, Nonlinear Plasmonics, Lukas Novotny, Univ. of Rochester, USA

6.5 Transformation Optics and Cloaking with Metamaterials

Thursday, October 28, 2010

Invited Speakers:

8:00 AM, Transforming Integrated Optics, Jensen Li, City Univ. of Hong Kong, China

8:30 AM, Taming the Fields and Waves with Extreme Metamaterials, Nadar Engheta, Univ. of Pennsylvania, USA

9:00 AM, Active and Tunable Metamaterials, Vladimir M. Shalaev; Purdue Univ., USA

9:30 AM, Molding the Flow of Light with Artificial Optical Materials, Dentcho Genov, Louisana Tech, USA

6.6 Nonlinear Optics in Micro/Nano-Optical Structures (joint with FiO 5: Photonics)

Thursday, October 28, 2010

Invited Speakers:

8:45 AM, Nonlinear Optical Processes in Subwavelength Optical Waveguides—Revised Fundamentals and Implications, Shahraam Afshar, Univ. of Adelaide, Australia

10:30 AM, Nonlinear Silicon Photonics, Michal Lipson, Cornell Univ., USA

11:30 AM, Light Scattering in a Random but Non Diffusive Nonlinear Medium, Jordi Martorell, Inst. de Ciències Fotòniques, Spain

1:30 PM, CMOS Compatible All-Optical Chips, David Moss¹, A. Pasquazi², M. Peccianti², L. Razzari², D. Duchesne², M. Ferrera², S. Chu³, B. E. Little³, R. Morandotti²; ¹Univ. of Sydney, Australia, ²INRS-EMT, Canada, ³Infinera Corp., USA Tutorial Speaker:

2:30 PM, Phonon Lasers in Cavity Optomechanics, Kerry Vahala, Caltech, USA 6.7 Disorder in Integrated Optical Devices and Circuits

Tuesday, October 26, 2010

Invited Speakers:

1:30 PM, Strong Localization by Disorder in Photonic Crystal Waveguides, Frank Vollmer, Harvard Univ., USA

3:00 PM, Disorder-Induced Multiple Scattering and Light Localization in Photonic Crystal Waveguides, Stephen Hughes, Queen's Univ., Canada

Wednesday, October 27, 2010

Invited Speakers:

1:30 PM, Evolution of Photonic Band-Gap and Lasing from Polycrystalline to Amorphous Photonic Structures, Hui Cao, Yale Univ., USA

3:00 PM, Ultrasensitive Raman Sensor Based on Highly Scattering Porous Structures, Vladislav Yakovlev, Univ. of Wisconsin at Milwaukee, USA

FiO 7: Vision and Color

7.1 Individualized Optical Correction of the Eye

Monday, October 25, 2010

Invited Speakers:

1:30 PM, The Use of Adaptive Optics to Study Optical and Neural Impact on Visual Performance, Geunyoung Yoon, Univ. of Rochester, USA

2:15 PM, Performance of Aspheric IOLs, Susana Marcos, Inst. de Óptica, Spanish Council for Scientific Res., Spain

Tutorial Speaker:

2:45 PM, The Role of the Eye's Aberrations in Vision, Pablo Artal, Univ. de Murcia, Spain

7.2 Emerging in vivo Imaging Techniques for Ocular Imaging (joint with FiO 3: Optics in Biology and Medicine) Monday, October 25, 2010

Invited Speaker:

4:00 PM, Imaging the Development of Neural Circuits in the Mammalian Retina, Daniel Kerschensteiner; Washington Univ. in St. Louis, USA.

4:30 PM, Multimodal Retinal Imaging, Hao Zhang¹,², Qing Wei¹, Tan Liu¹, Jing Wang¹, Dennis P. Han³, Janice M. Burke³, Shuliang Jiao&sup4;; ¹Univ. of Wisconsin at Milwaukee, USA, ²Northwestern Univ., USA, ³Medical College of Wisconsin, USA, &sup4;Univ. of Southern California, USA

View speakers for 1.7 Adaptive Optics for the Eye

LS Invited Speakers

Check back often as speakers are still being confirmed and updated!

1. Frontiers in Cold Molecules 2. Hybrid Quantum Systems 3. Metrology and Precision 4. Novel Imaging, Spectroscopy and Manipulation in Microstructures 5. Attosecond and Strong Field Physics 6. Chemical Dynamics—Multi-Dimensional Ultrafast Spectroscopy 7. Photophysics of Nanostructured Materials 8. Photophysics of Energy Conversion 9. Single Molecule Approaches to Biology-Inspired Problems 10. Optofluidics in the Near-Field 11. Quantum Enhanced Information Processing 12. Nonlinear Optics 13. Nanophotonics, Photonic Crystals and Structural Slow Light

View Symposia Speakers View FiO Speakers

1. Frontiers in Cold Molecules

Tuesday, October 26, 2010

Invited Speakers:

4:00 PM, Tunable Excitons in Ordered Arrays of Ultracold Molecules of Optical Lattices, Roman Krems, Univ. of British Columbia, Canada 4:30 PM, Dipolar Effects in an Ultracold Gas of LiCs Molecules, Matthias Weidemeuller, Heidelberg Univ., Germany Thursday, October 28, 2010

Invited Speakers:

8:00 AM, Manipulation of Ultracold Chemistry, John Bohn, JILA, NIST, Univ. of Colorado, USA

8:30 AM, Implementation of a New Method to Produce Ultracold Polar Molecular Ions, Wade Rellergert, Scott Sullivan, Kuang Chen, Steven Schowalter, Eric R. Huson; Univ. of California at Los Angeles, USA

9:30 AM, Sympathetic Heating Spectroscopy: Probing Molecular Ions with Laser-Cooled Atomic Ions, Ken Brown, Georgia Tech, USA

1:30 PM, Laser Cooling of a Diatomic Molecule, David DeMille, E. S. Shuman, J. F. Barry; Yale Univ., USA

2:00 PM, Testing the Time-Invariance of Fundamental Constants Using Cold, and Not So Cold, Molecules, Rick Bethlem, Vrije Univ., Amsterdam

2. Hybrid Quantum Systems

Wednesday, October 27, 2010

Invited Speakers:

8:00 AM, Hybrid Nanophotonic and Nanomechanical Interfaces for Spin Qubits, Mikhail Lukin, Harvard Univ., USA

8:30 AM, Optical Manipulation and Detection of the Collective Motion and Spin of an Ultracold Atomic Gas, Dan Stamper-Kurn, Univ. of California at Berkeley, USA

9:30 AM, Measurement of Nanomechanical Motion with Precision Sufficient to Detect Zero-Point Motion, K. W. Lehnert, JILA, NIST, Univ. of Colorado, USA

10:30 AM, Quantum Measurement of Phonon Shot Noise Using Optomechanical Systems, Aashish Clerk, McGill Univ., Canada

11:00 AM, Nonlinear Optomechanical Couplings: Tools for Dealing with Solid Mechanical Objects in the Quantum Regime, Jack Sankey, Yale Univ., USA

11:30 AM, Measuring the Quantum Harmonic Oscillator, Andrew Cleland, Univ. of California at Santa Barbara, USA 12:15 PM, Title to Be Announced, Tobias J. Kippenberg, Max-Planck-Inst. fur Quantenoptik, Germany

3. Metrology and Precision Measurements

Invited Speakers:

Wednesday, October 27, 2010

8:00 AM, Precise Determination of h/M(Rb) Using Bloch Oscillations and Atomic Interferometry: A Mean to Deduce the Fine Structure Constant, Francois Biraben, Laboratoire Kastler Brossel, École Normale Supérieure, CNRS, France

8:30 AM, Optical Clock with Lattice-Confined Sr Atoms, Jun Ye, JILA, Univ. of Colorado

9:15 AM, Al+ Optical Clocks for Fundamental Physics, Geodesy, and Quantum Metrology, Till Rosenband, NIST, USA

1:30 PM, New Limit on Lorentz and CPT Violation for Neutrons, Michael Romalis, Princeton Univ., USA

Thursday, October 28, 2010

Invited Speakers:

2:00 PM, Results of Table-Top Fundamental Physics Experiments at Berkeley, Dmitry Budker, Univ. of California at Berkeley, USA

2:45 PM, An Improved Limit on the Permanent Electric Dipole Moment (EDM) of 199Hg, Tom Loftus, Univ. of Washington, USA

4. Novel Imaging, Spectroscopy and Manipulation in Microstructures

Monday, October 25, 2010

Invited Speakers:

4:00 PM, Linear and Nonlinear Optical Nano-Crystallography, Markus Raschke, Univ. of Washington, USA

4:30 PM, 10 kHz Accuracy Spectroscopy in Acetylene-filled Hollow-Core Kagome Fiber and Improved Linewidths, Kristan Corwin Kansas State Univ., USA

Tuesday, October 26, 2010

Invited Speakers: 10:30 AM, Coherent Rydberg Excitation in Microscopic Thermal Vapor Cells, Tilman Pfau, Univ. of Stuttgart, Germany

11:15 AM, Single-Particle Spectroscopy and Manipulation in Optofluidic Devices, Holger Schmidt, Univ. of Southern California

5. Attosecond and Strong Field Physics

Tuesday, October 26, 2010

Invited Speakers:

1:30 PM, Attosecond Physics: Real-Time Tracking of Valence Electron Motion in Atoms, Eleftherios Goulielmakis, Max-Planck-Inst. für Quantenoptik, Germany

2:00 PM, Probing Electron Dynamics by High Harmonic Generation, Markus Guehr, Stanford Univ., USA

Wednesday, October 27, 2010

Invited Speakers:

2:45 PM, High Order Harmonics Driven by 1.5μm Parametric Source: A Tool for Attosecond Science, Caterina Vozzi, Politecnico di Milano, Italy

4:00 PM, Time-Resolved High-Harmonic Spectroscopy of Photochemical Dynamics, Hans Jakob Worner, National Res. Council, Canada

4:45 PM, Ultrafast Dynamics in Helium Nanodroplets Studied by Femtosecond EUV Photoelectron and Ion Imaging, Oliver Gessner, Lawrence Berkeley Natl. Lab, USA

6. Chemical Dynamics—Multi-Dimensional Ultrafast Spectroscopy

Wednesday, October 27, 2010

Invited Speakers:

1:30 PM, Advances in Ultrafast 2-D Spectroscopy, Chris T. Middleton, Martin T. Zanni; Univ. of Wisconsin at Madison, USA

2:00 PM, Multiply Resonant Coherent Multidimensional Spectroscopy, John Wright, Univ. of Wisconsin at Madison, USA

2:45 PM, Watching Chemical Reactions and Dynamics with Ultrafast Multidimensional Infrared Spectroscopy, Carlos R. Baiz, Jessica M. Anna, Robert McCanne, John T. King, Kevin J. Kubarych; Univ. of Michigan, USA Thursday, October 28, 2010

Invited Speakers:

8:00 AM, Two Dimensional Ultraviolet Spectroscopy of Proteins and Amyloid Fibrils, Jun Jiang, Shaul Mukamel; Univ. of California at Irvine, USA

8:30 AM, Two-Dimensional Electronic Spectroscopy of the Photosystem II Reaction Center, J. A. Myers, K. L. M. Lewis, F. Fuller, P. F. Tekavec, J. P. Ogilvie; Univ. of Michigan, USA

7. Photophysics of Nanostructured Materials

Monday, October 25, 2010

Invited Speakers:

1:30 PM, Photophysical Consequences of Interactions Between Conjugated Chromophores, Lewis Rothberg, Univ. of Rochester, USA

2:00 PM, Effects of Aggregation on the Emission Spectra and Dynamics of Electrolumine Scent Materials, Linda Peteanu, Carnegie Mellon Univ., USA

2:30 PM, Transient Microwave Conductivity Studies of Poly (3-alkyl thiophene)s and Blends with PCBM, Garry Rumbles, Natl. Renewable Energy Lab., USA

Tuesday, October 26, 2010

Invited Speakers:

8:00 AM, Excitonic Dynamics of Quantum Dots Monitored by Near-Infrared Transient Absorption, Emily Weiss, Northwestern Univ., USA

8:30 AM, Quantum Dot Electron Transfer Probed by Transient Photoluminescence, Marcus Jones; Univ. of North Carolina at Charlotte, USA.

11:00 AM, Two-Dimensional Photon Echo Measurements on CdTe/CdSe Heterostructured Quantum Dots, Shun Shang Lo1, Roman Vaxenburg2, Cathy Y. Wong1, Efrat Lifshitz2, Gregory D. Scholes1; 1Univ. of Toronto, USA, 2Russell Berrie Nanotechnology Inst. and Solid State Inst., Israel.

10:30 AM, Mixed Quantum Classical Simulations of Vibrational Excitations in Peptide Helices, Anne Goj, Eric Bittner; Univ. of Houston, USA.

8. Photophysics of Energy Conversion Wednesday, October 27, 2010

Invited Speakers:

8:00 AM, Multi-Exciton Dissociation Dynamics in CdSe Quantum Dots, Tianquan Lian, Emory Univ., USA

8:30 AM, Inter- and Intra-chain Electronic Coherence in Conjugated Polymers, Greg Scholes, Univ. of Toronto, Canada

9:00 AM, Transient Absorption Studies of Charge Photogeneration in Organic and Dye Sensitized Solar Cells, James Durrant, Imperial College London, UK

9:45 AM, Exciton Diffusion and Interfacial Charge Separation in Photovoltaic Materials Studied by Microwave Conductivity, Tom J. Savenije, Laurens D. A. Siebbeles; Delft Univ. of Technology, Netherlands.

1:30 PM, Spin Signatures of Light Induced Charge Separated States in Polymer-Fullerene Bulk-Heterojunctions: High-Frequency Pulsed EPR Spectroscopy, Oleg Poluektov¹, Salvatore Filippone², Nazario Martín², Andreas Sperlich³, Carsten Deibel³, Vladimir Dyakonov³; ¹Argonne Natl. Lab, USA, ²Univ. Complutense de Madrid, Spain, ³Julius-Maximilians Univ. of Würzburg and Bavarian Ctr. for Applied Energy Res. e. V., Germany

2:00 PM, Optically and Electrically Detected Magnetic Resonance Studies of Organic Light-Emitting Materials and Devices, Joe Shinar, Iowa State Univ., USA.

2:30 PM, Carrier Dynamics of Films of Zinc Phthalocyanine and C60 Measured by Terahertz Time Domain Spectroscopy, Paul Lane, NRL, USA

3:00 PM, Time-Resolved Microwave Conductivity, Nikos Kopidakis, Natl. Renewable Energy Lab., USA

9. Single Molecule Approaches to Biology-Inspired Problems

Wednesday, October 27, 2010

Invited Speakers:

10:30 AM, Optical Chirality and Superchiral Fields, Adam Cohen, Harvard Univ., USA

11:00 AM, Local Dynamics Probing by Real-Time Single-Particle Tracking Spectroscopy, Li Sun, Princeton Univ., USA

11:30 AM, Exploring Chromatin Biochemistry with Single-Molecule Fluorescence Diffusometry, Hideo Mabuchi, Stanford Univ., USA 4:00 PM, Bacteriophager Lambda Life Cycle: The View from the Single Virus, Ido Golding, Baylor College of Medicine, USA

4:30 PM, Imaging Dynamic Events Inside Living Cells: Intracellular Degradation of LDL, Christine Payne, Georgia Tech, USA

5:00 PM, Time-Resolved 3D Tracking of Individual Quantum Dot Labeled Proteins in Live Cells via Confocal Feedback, Jim Werner, Los Alamos Natl. Lab, USA

Thursday, October 28, 2010

Invited Speakers:

10:30 AM, Single Molecule Photon Trajectories and Transition Paths in Protein Folding, Bill Eaton, NIH and Natl. Inst. of Diabetes and Digestive and Kidney Diseases, USA

11:00 AM, Title to Be Announced, Norbert Scherer, Univ. of Chicago, USA

11:30 AM, Superresolution Optical Fluctuations Imaging (SOFI) , Shimon Weiss, Univ. of California at Los Angeles, USA

10. Optofluidics in the Near-Field

Tuesday, October 26, 2010

Invited Speakers:

1:30 PM, The Reactive Sensing Principle (RSP) in Optically Resonant Biosensing and Nanoparticle Trapping within a WGM Carousel, Stephen Arnold, Siyka I. Shopova, Stephen Holler; Polytechnic Inst. of New York Univ., USA.

2:00 AM, Title to Be Announced, Sudeep Mandal, Cornell Univ., USA

2:30 PM, Surface Optofluidics, Andreas E. Vasdekis1, Wuzhou Song1, Julien R. Cuennet1, Luciano De Sio2, Jae-Woo Choi1, Demitri Psaltis1; 1École Polytechnique Fédérale de Lausanne, Switzerland, 2Univ. of Calabria,, Italy.

3:00 PM, Optofluidic Ring Resonator Lasers, Xudong (Sherman) Fan, Yuze Sun, Jonathan D. Suter, Chung-Shieh Wu, Wonsuk Lee, Balareddy Chinna Reddy Karthik; Univ. of Michigan, USA.

4:00 PM, Optofluidic Nano-Plasmonics for Biochemical Sensing, Shaya Y. Fainman, L. Pang, B. Slutsky, J. Ptasinski, L. Feng, M. Chen; Univ. of California at San Diego, USA.

4:30 PM, Plasmonics for Optical Manipulation and Enhanced Spectroscopy, Kenneth Crozier, Harvard Univ., USA 11. Quantum Enhanced Information Processing

Wednesday, October 27, 2010

Invited Speakers:

10:30 AM, Entanglement and Quantum Algorithms with Superconducting Circuits, Robert Schoelkopf, Yale Univ., USA

11:00 AM, Benchmarking Quantum Information Processing Devices, Raymond Laflamme, Univ. of Waterloo, Canada

11:30 AM, Coherent Splitting, Rocking and Blinding of Single Atoms in an Optical Lattice, Dieter Meschede, Inst. für Angewandte Physik der Univ. Bonn Wegelerstr, Germany

4:00 PM, Progress towards Scalable Quantum Information Processing with Trapped Ions, David Hanneke, NIST, USA

5:00 PM, Quantum Illumination for Improved Detection, Imaging, and Communication, Jeffrey Shapiro, MIT, USA

Thursday, October 28, 2010

Invited Speakers:

10:30 AM, Quantum Teleportation And Quantum Information Processing, Akira Furusawa, Univ. of Tokyo, Japan

11:00 AM, Integrated Quantum Photonics, Jeremy L. O'Brien; Univ. of Bristol, UK

12. Quantum Nonlinear Optics

Tuesday, October 26, 2010

Invited Speakers:

8:00 AM, Toward Single-Photon Nonlinear Optics via Self-Assembled Ultracold Atoms, Daniel J. Gauthier, Duke Univ., USA

8:30 AM, Prospects for Strong Cavity Free Single Atom Nonlinearity at the Few Photon Level, Gerd Leuchs; Max-Planck-Inst. for the Science of Light and Inst. of Optics, Univ. Erlangen-Nuremberg, Germany.

1:30 PM, Spatial Light Modulators, a Tool for Measuring the Quantum Entanglement of Transverse Modes, Miles Padgett, Univ. of Glasgow, UK 2:00 PM, Gas-Phase Integrated-Photonics Quantum Technologies, Andrew White, Univ. of Queensland, Australia

13. Nanophotonics, Photonic Crystals and Structural Slow Light

Thursday, October 28, 2010

Invited Speakers:

10:30 AM, Cavity Quantum Electrodynamics with Quantum Dots, Antonio Badolato, Univ. of Rochester, USA

8:00 AM, Spontaneous and Stimulated Emission of Light into Surface Plasmon Modes, Pierre Berini, Univ. of Ottawa, Canada

8:30 AM, Enhancing Light-Matter Interactions in Nanophotonic Structures by Slow Light, Jesper Moerk, Technical Univ. of Denmark, Denmark

11:00 AM, Novel Light-Guiding Properties in Photonic Crystals, R. Hamam, I. Celanovic, Z. Wang, Y. Chong, J.d. Joannopoulos, Marin Soljacic; MIT, USA. Special Symposia at Frontiers in Optics 2010/Laser Science XXVI

Check back often as speakers are still being confirmed and updated!

Arthur Ashkin Honorary Symposium Industrial Physics Forum Laser Science Symposium on Undergraduate Research Symposium on Optical Communications

Arthur Ashkin Honorary Symposium

Symposium organizers: Mihaela Dinu¹, Mara Prentiss², Steve Rolston³; ¹Bell Labs, Alcatel- Lucent, USA; ²Harvard Univ., USA, ³Univ. of Maryland at College Park, USA

This symposium commemorates Arthur Ashkin's contributions to the understanding and use of light pressure forces on the 40th anniversary of his seminal paper '”Acceleration and trapping of particles by radiation pressure.” Light pressure forces have served as the foundation for many cutting-edge research fields, such as work with optical tweezers, trapping of neutral particles and Bose-Einstein condensation. It is not an overstatement to say that the discovery and understanding of light pressure forces has led to a renaissance in atomic and molecular physics as well as optical science. Several historical overviews as well as new research that rest upon Arthur Ashkin's foundational work will be presented. We invite all conference attendees to help us honor Art and gain a deeper understanding of the far-reaching impact of his work in light- matter interactions.

Read the OPN article by McGloin and Reid (March 2010) about the 40th anniversary of Ashkin’s seminal paper “Acceleration and trapping of particles by radiation pressure.”

Invited Speakers include:

Tuesday, October 26, 2010

1:30 PM, Optical Trapping and Manipulation of Small Neutral Particles Using Lasers, Arthur Ashkin; Alcatel-Lucent Bell Labs, USA

1:55 PM, The Biophysics of Gene Regulation, Studied One Molecule at a Time, Steven M. Block; Stanford Univ., USA

2:20 PM, Title to Be Announced, James Gordon P.; Consultant, Bell Labs, USA

2:45 PM, Non-conservative Forces in Optical Tweezers, David G. Grier; New York Univ., USA

3:05 PM, Torsional Studies Of Single Biological Molecules, Michelle Wang; Cornell Univ., USA

4:00 PM, The Man and His Science, John Bjorkholm; Consultant, USA

4:25 PM, A Subjective History of Laser Cooling, Hal Metcalf; Stony Brook Univ., USA

4:50 PM, Multi-Photon Laser Cooling, James (Trey) Porto, Saijun Wu, Roger Brown, W. P. Phillips; NIST Res. Library, USA.

5:15 PM, Laser Cooling and Trapping the Most Magnetic Atom, Dysprosium, Benjamin Lev, Mingwu Lu, Seo Ho Youn; Univ. of Illinois at Urbana-Champaign, USA

Industrial Physics Forum

Symposium organizers: OSA and AIP Corporate Associates The Industrial Physics Forum (IPF) brings together invited speakers to address relevant and timely topics in the industrial sector. In celebration of LaserFest 2010, this 52nd IPF is themed "Applications of Laser Technology". Three themed sessions range in topic from biomedical applications to environmental applications to metrology. A special Frontiers in Physics session addresses the most exciting physics research going on today, regardless of field.

Invited Speakers Include:

Monday, October 25, 2010

Biomedical Applications of Lasers

1:30 PM, Laser Refractive Cataract Surgery with the LenSx Laser, Michael Karavitis, Lens X, USA

2:00 PM, Applications of Table Top Lasers Developed from the FEL, David Piston, Vanderbilt Univ., USA

2:30 PM, From Photonics to Genomics: Lasers and Imaging Technology Enables Next- Generation DNA Sequencing, Suzanne Wakelin; Ilumina, USA.

3:00 PM, Biomedical Imaging with Optical Coherence Tomography, James Fujimoto, MIT, USA Environment Applications of Lasers

4:00 PM, NASA’s Space Lidar Measurements of Earth and Planetary Surfaces, Jim Abshire, NASA Goddard Space Flight Ctr., USA

4:30 PM, The Physics and Technology of Quantum Cascade Lasers, Federico Capasso, Harvard Univ., USA

5:00 PM, Tunable Infrared Laser Measurements of Industrial Process and Product Emissions, Charles Kolb, Aerodyne Res., USA

5:30 PM, Laser Remote Sensing of the Earth: Calipso and beyond, Carl Weimer, Ball Aerospace, USA

Tuesday, October 26, 2010

Laser Applications in Metrology

8:00 AM, Use of Lasers in Time and Frequency Applications (or Metrology), Scott Diddams, NIST, USA

8:30 AM, Laser Fuse Processing for Advanced Memory Designs, Joohan Lee, GSI Laser Systems, USA

9:00 AM, Dynamic Interferometry for on-Machine Metrology, Michael North Morris, 4D Technology, USA

9:30 AM, The Electronic Kilogram and Lasers, Richard Steiner, NIST, USA

Frontiers in Physics

10:30 AM, Viewing the High-Energy Universe with the Fermi Gamma-ray Space Telescope, Peter Michelson, SLAC, USA

11:30 AM, Epitaxial Graphene: Designing a New Electronic Material, Walter de Heer, Georgia Tech, USA

12:00 PM, The Status of the CERN Large Hadron Collider (LHC), Dan Green, Fermilab, USA

11:00 AM, Quantum Entanglement and Information, Chris Monroe, Univ. of Maryland at College Park, USA

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 10th 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 more than 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.

Click here to view the complete Laser Science Symposium on Undergraduate Research.

Symposium on Optical Communications

Symposium organizers: Karl Koch¹, Colin McKinstrie²; ¹Corning Inc., USA, ²Bell Labs, Alcatel- Lucent, USA In 2009, Charles Kuen Kao was awarded a Nobel Prize in Physics “for groundbreaking achievements concerning the transmission of light in fibers for optical communications.” (See http://nobelprize.org/nobel_prizes/physics/laureates/2009/press.html.)

In recognition of this honor, there will be a special symposium on optical communications. An illustrious collection of invited speakers will review the history and physics of optical fiber communication systems, from the first demonstration, in which a video signal was transmitted over 20 meters, to contemporary systems, which transmit information at rates of 10 gigabits per second and higher over distances of thousands of kilometers.

Invited Speakers include:

Wednesday, October 27, 2010

1:30 PM, Historical Overview of Optical Communications, Tingye Li; AT&T Labs, USA

2:00 PM, Development of Low-Loss Fibers, P. Schultz; Corning, USA

2:30 PM, Title to Be Announced, David Payne; Univ. of Southampton, USA

4:00 PM, Development of Semiconductor DFB Lasers and Modulators, T. Koch; Lehigh Univ., USA

4:30 PM, Solitons, Nonlinearities and Noise in Long-Haul Optical Transmission Systems, L. Mollenauer; Bell Labs, USA

5:00 PM, Integrated Optics in Optical Communication Systems, Hiroshi Takahashi; NTT Photonics Labs, Japan

5:30 PM, Capabilities of the Undersea Telecommunications Industry, Neal S. Bergano; Tyco Telecommunications, USA Short Courses

Register Now! 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 28, 2010. 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.

2010 Courses

Sunday, October 24, 2010, 9:00 a.m.-12:30 p.m.

NEW SC189. Photonic Quantum-Enhanced Technologies, Ian Walmsley; Univ. of Oxford, UK

SC306. Exploring Optical Aberations, Virendra N. Mahajan 1,2; 1Aerospace Corp., USA, 2 College of Optical Sciences, Univ. of Arizona, USA

SC321. Principles of Far-Field Fluorescence Nanoscopy, Andreas Schoenle, Stefan Hell; Max Planck Inst. for Biophysical Chemistry, Germany

Sunday, October 24, 2010, 1:30 p.m.–5:00 p.m.

SC323. Latest Trends in Optical Manufacturing, Paul Dumas; QED Technologies Inc., USA

SC324. Plasmonics, Stefan Maier; Experimental Solid State Group, Dept. of Physics, Imperial College London, UK

NEW SC354. Compressive Sensing, Kevin Kelly; Rice Univ., USA - CANCELLED

NEW SC355. Attosecond Science, Paul Corkum; Natl. Res. Council of Canada, Canada - CANCELLED 2010 Exhibitor & Sponsor List

4D Technology Corporation

ALPAO

American Elements American Institute of Physics

American Physical Society (APS)

ASE Optics, Inc.

Biophotonic Solutions, Inc.

Bond, Schoeneck & King, PLLC

Boston Micromachines Corporation

Cambridge University Press

Chroma Technology Corp.

Corning Tropel Corporation

CVI Melles Griot

Electronic Product Services LLC

Energetiq Technology, Inc.

Femtolasers, Inc.

Fianium Ltd.

Glass Fab, Inc.

G-S PLASTIC OPTICS

Hamamatsu Corporation

Idesta QE

IMRA America

Laser Focus World

LaserFest

Lumetrics, Inc.

Menlo Systems

Mildex, Inc.

Nature Publishing Group

Newport Corporation New Scale Technologies, Inc.

NKT Photonic Inc.

Nufern

Ohara Corporation

Omega Optical, Inc.

OPN, A Publication of OSA

Optikos Corporation

Optimax Systems, Inc.

Opto Alignment Technology, Inc.

OSA

OSA Foundation

PHASICS

Photonics Media/Laurin Publishing

Physics Today

Princeton Instruments, Inc.

Society of Vacuum Coaters

Solid State Cooling Systems

Swamp Optics, LLC

Sydor Optics, Inc.

Syntec Optics Taylor & Francis

TeachSpin, Inc.

Thorlabs

Toptica Photonics, Inc. University of Arizona, College of

Optical Sciences

University of Central Florida, CREOL University of Rochester, The Institute of Optics

VisiMax Technologies, Inc.

Volpi USA

Wiley-Blackwell

Wordingham Technologies

Zygo Corporation Special Events

OSA Divisional and Technical Groups Meetings

What’s Hot in Optics Today?

FiO/LS Welcome Reception

Plenary Session and Awards Presentation

Industrial Physics Forum

VIP Industry Leaders Networking Event: Connecting OSA Corporate Members and Young Professionals

Joint FiO/LS Poster Sessions

OSA Fellow Members Lunch

Meet the Editors of the APS Journals

Industrial Physics Forum Corporate Reception

OSA Member, Family and Friends Special Events

Minorities and Women in OSA (MWOSA) Tea

Division of Laser Science Annual Business Meeting

OSA’s Annual Business Meeting OSA Member LaserFest Reception

Industrial Physics Forum

Laser Science Banquet

Science Educators Day

FiO Postdeadline Session

Young Professionals and Student Activities

Omega Laser Facility tour at the Laboratory for Laser Energetics of the University of Rochester

Young Professional and Student Activities

OSA Member, Family, & Friends Program Events

OSA Divisional and Technical Groups 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.

Saturday, October 23, 12:30 p.m. - 1:00 p.m. Class of '62 Auditorium, Univ. of Rochester Vision and Color Division Business Meeting

Monday, October 25, 12:00 p.m. -1:30 p.m. Grand Ballroom F/G, Hyatt Regency Rochester Biomedical Optics Division Meeting

The chief topic of conversation will be requesting input on the design and implementation of an online community that links the new Biomedical Optics Express journal with the Biomedical Optics technical division. Please RSVP to Mindy Halpert at [email protected] if you are interested in attending.

Tuesday, October 26, 7:00 p.m. – 8:00 p.m. Grand Ballroom D, Hyatt Regency Rochester Joint meeting of the OSA Fabrication, Design and Instrumentation Division and the Rochester OSA Local Section

Better Specification of Aspheric Shapes, Greg Forbes, QED Technologies, Inc., Australia Modifying a widely used convention is a real challenge. This is especially so when it impacts on multiple groups, in our case, on optical designers, fabricators, and metrologists. Aspheric optics are an evolving technology that is currently burdened by the increasingly inadequate convention of expressing a rotationally symmetric asphere’s sag as the sum of a conic component and an additive polynomial. When more than just a few terms appear in the polynomial, this becomes problematic and ultimately unworkable. The associated coefficients are unintuitive and inefficient. This leads to error-prone communications and a lack of easy options to appreciate the difficulty of manufacturing any particular asphere. Thankfully, the design and manufacture of increasingly complex aspheres is facilitated by a modified representation that is also ideal for exploiting cost-effective shapes. In particular, an orthogonalised representation gives a description that functions with fewer coefficients and fewer digits —typically using only one third the number of digits for current designs— and allows easy interpretations and sanity checks as well as more direct assessments of manufacturability. Examples are presented to motivate us to make this change sooner rather than later.

Greg Forbes was on the faculty of The Institute of Optics at the University of Rochester for about ten years until the mid 90's. He returned to Australia as a Research Professor in Physics at Macquarie University in Sydney. For the last ten years he has been Senior Scientist at QED Technologies. He lives in Sydney but regularly comes to visit and work with his colleagues and friends in Rochester

What’s Hot in Optics Today?

Sunday, October 24, 4:00 p.m.–6:00 p.m. Lilac Ballroom North and South, Rochester Riverside Convention Center

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.

• What’s Hot in Bio-Medical Optics, Adam Wax; Duke Univ., USA • The Role of Optics in "Optical Communications", Juerg Leuthold; Univ. of Karlsruhe, Germany • Fabrication, Design and Instrumentation: Bio-Optical Design, R. John Koshel; Photon Engineering LLC and College of Optical Sciences/Univ. of Arizona, USA • What’s Hot in Information Acquisition, Processing and Display, David Brady; Duke Univ., USA • Extreme Light Sources: From Artificial Sun to New Planets, Irina Sorokina; Norwegian Univ. of Science & Technology, Norway • Vision and Color: Mapping the Visual Cortex, Alex Wade; Smith-Kettlewell Eye Res. Inst., USA

Welcome Reception

Sunday, October 24, 6:00 p.m.–7:30 p.m. Riverside Court and Galleria Lobby, Rochester Riverside Convention Center

Free to all Technical Conference Attendees: Get the FiO 2010/LS XXVI meeting off to a great start by attending the welcome reception! Meet with colleagues from around the world and enjoy light hors d’oeuvres.

Plenary Session and Awards Presentation

Monday, October 25, 8:00 a.m.–12:00 p.m. Lilac Ballroom North and South, Rochester Riverside Convention Center

The 2010 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.

Industrial Physics Forum

Monday, October 25, 1:30 p.m. - 6:00 p.m. Tuesday, October 26, 8:00 a.m. - 12:00 p.m. Highland J, Rochester Riverside Convention Center

Symposium organizers: OSA and AIP Corporate Associates

The Industrial Physics Forum (IPF) brings together invited speakers to address relevant and timely topics in the industrial sector. In celebration of LaserFest 2010, this 52nd IPF is themed "Applications of Laser Technology". Three themed sessions range in topic from biomedical applications to environmental applications to metrology. A special Frontiers in Physics session addresses the most exciting physics research going on today, regardless of field.

VIP Industry Leaders Networking Event: Connecting OSA Corporate Members and Young Professionals

Tuesday, October 26, 8:00 a.m.–9:30 a.m. - Free of Charge and includes a Hot Buffet Breakfast Grand Ballroom E & F, Hyatt Regency Rochester

Join OSA Corporate Members for an event that puts Young Professionals in contact with highly successful OSA members. After an informal networking session, each participant will have the opportunity for a brief visit with each corporate member to discuss careers, industry trends or any other topic. Corporate member participants include companies such as CVI Melles Griot and Toptica.

Space is limited. Members of OSA’s Young Professionals program will be given registration priority, but any recent graduate is welcome to RSVP.

To RSVP or to join the Young Professionals program, email April Zack at [email protected].

Joint FiO/LS Poster Sessions

Tuesday, October 26, 12:00 p.m.–1:30 p.m. Wednesday, October 27, 12:00 p.m.–1:30 p.m. Empire Hall, Rochester Riverside Convention Center

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 exhibit hall to enjoy the poster sessions.

OSA Fellow Members Lunch

Tuesday, October 26, 12:00 p.m. – 1:30 p.m. Grand Ballroom A & B, Hyatt Regency Rochester

(Sponsored by the OSA Foundation) All Fellow members are welcome, please RSVP via email at [email protected] by October 8, 2010. A RSVP is needed to reserve your space.

Meet the Editors of the APS Journals

Tuesday, October 26, 3:30 p.m.–5:00 p.m. Riverside Court, Rochester Riverside Convention Center

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.

Industrial Physics Forum Corporate Reception

Hosted by OSA and AIP Corporate Associates Tuesday, October 26, 4:00 pm – 5:00 pm Empire Hall, Rochester Riverside Convention Center

Join your colleagues for a special invitation only reception for conference and exhibit attendees in the corporate community. Exhibitors, OSA and AIP Corporate Members, Industrial Physics Forum attendees and others will have time to connect with company associates and meet new business partners during this hors d'oeuvre hour. RSVP required by October 8 to [email protected].

Minorities and Women in OSA (MWOSA) Tea

Tuesday, October 26, 4:30 p.m. – 5:30 p.m.(Free of Charge) Grand Ballroom E & F, Hyatt Regency Rochester

Every year OSA features a speaker who discusses current issues and trends in the field. Everyone is welcome to attend; refreshments will be served! Check back soon for details. Questions? Email [email protected].

Division of Laser Science Annual Business Meeting

Tuesday, October 26, 6:00 p.m.–7:00 p.m. Highland H, Rochester Riverside Convention Center

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 26, 6:00 p.m.–7:00 p.m. Highland A, Rochester Riverside Convention Center

Learn more about OSA and join the OSA Board of Directors for the Society’s annual business meeting. The 2009 activity reports will be presented and the results of the Board of Directors election will be announced. View the slate of candidates and vote.

OSA Member LaserFest Reception

Tuesday, October 26, 7:00 p.m. - 8:30 p.m.- Free Event for all OSA Members Lilac Ballroom North and South, Rochester Riverside Convention Center

OSA Members are invited to a special reception recognizing LaserFest, the celebration of the 50th anniversary of the laser. This free event 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 membership card. If you join OSA on-site, please bring your receipt.

Laser Science Banquet

Tuesday, October 26, 7:00 p.m.–10:00 p.m. Grand Ballroom A & B, Hyatt Regency Rochester

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 25.

FiO Postdeadline Papers

Wednesday, October 27, 7:00 p.m. – 8:30 p.m. TBD, Rochester Riverside Convention Center

The FiO 2010 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.

LaserFest: Celebrating 50 years of Laser Innovation

Tour the Omega Laser Facility at the Univ. of Rochester’s Laboratory for Laser Energetics (LLE)

Friday, October 29, 9:00 a.m. – 10:30 a.m. Free of Charge

Buses depart from Rochester Riverside Convention Center. Transportation 9:00 a.m. provided: Space is limited!

The tour will take 1 ½ hours including travel time to and from Laboratory. Buses Duration of Tour: will return you to the Rochester Riverside Convention Center.

Registration Limited seats are available – Register on-site until October 26, 2010 Deadline:

All Frontiers in Optics (FiO) and Laser Science (LS) Conference attendees are invited to tour the internationally renowned Omega Laser Facility at the University of Rochester’s Laboratory for Laser Energetics (LLE).

About the facility: In a steady march toward thermonuclear ignition and achievement of energy gain, the Laboratory for Laser Energetics has conducted inertial confinement fusion experiments since the early 1970's. Inertial confinement fusion involves heating and compressing fusion fuel that is exposed to intense laser or particle beams. A small spherical target containing fusion fuel is subjected to intense irradiation by high-power-energy sources that implode the target, compressing the fuel while heating the central core to thermonuclear temperatures. During the fall of 2009 and into the spring of 2010, LLE successfully developed and tested a technique to fill room-temperature, glass targets with deuterium–tritium (DT) fuel to 10 atm as is required for diagnostic purposes at the National Ignition Facility (NIF).

See the two lasers: OMEGA and OMEGA EP

• OMEGA stands 10 meters tall and is approximately 100 meters in length. This system delivers pulses of laser energy to targets in order to measure the resulting nuclear and fluid dynamic events. OMEGA’s 60 laser beams focus up to 40,000 joules of energy in approximately one billionth of a second onto a target that measures less than 1 millimeter in diameter. • OMEGA EP (extended performance) is an addition to OMEGA and extends the performance and capabilities of the OMEGA Laser System. It provides pulses having multikilojoule energies, picosecond pulse widths, petawatt powers, and ultrahigh intensities exceeding 1020 W/cm2. These beams are delivered to targets within the OMEGA target chamber, as well as an independent chamber within the OMEGA EP target area. The new laser supports a wide variety of target-irradiation conditions when coupled to OMEGA or operated in stand-alone mode. • Please visit LLE's website for more detailed information.

Agenda of Sessions — Sunday, October 24

7:00 a.m.–4:00 p.m. OSA Student Chapter Leadership Meeting, Bausch, Carlson and Douglass, Radisson Hotel Rochester Riverside

7:00 a.m.–6:00 p.m. Registration, Galleria, Rochester Riverside Convention Center

9:00 a.m.–12:30 p.m. SC189. Photonic Quantum-Enhanced Technologies, Ian Walmsley; SC306. Exploring Optical Aberations, Virendra N. Mahajan; SC321. Principles of Far-Field Fluorescence Nanoscopy, Andreas Schoenle, Locations will be provided at registration

12:30 p.m.–1:30 p.m. Lunch Break (on your own)

1:30 p.m.–5:00 p.m. SC323. Latest Trends in Optical Manufacturing, Paul Dumas; SC324. Plasmonics, Stefan Maier; SC354. Compressive Sensing, Kevin Kelly; SC355. Attosecond Science, Locations will be provided at registration

4:00 p.m.–6:00 p.m. What's Hot In Optics? Lilac Ballroom North and South, Rochester Riverside Convention Center

6:00 p.m.–7:30 p.m. FiO/LS Welcome Reception, Galleria Lobby/Riverside Court, Rochester Riverside Convention Center

7:30 p.m.–8:30 p.m. OSA Divison and Technical Group Meetings, Exact times and locations are listed on the Update Sheet Agenda of Sessions

Key to Shading Frontiers in Optics Laser Science Joint

FiO/LS 2010 • October 24–28, 2010 27 Agenda of Sessions — Monday, October 25

Highland A Highland B Highland C Highland D Highland E Highland F Highland G Highland H Highland J Highland K

7:00 a.m.–6:00 p.m. Registration, Galleria, Rochester Riverside Convention Center Registration, Galleria, Rochester Riverside Convention Center

8:00 a.m.–12:00 p.m. 2010 Joint FiO/LS Awards Ceremony and Plenary Session, Lilac Ballroom North and South, Rochester Riverside Convention Center 2010 Joint FiO/LS Awards Ceremony and Plenary Session, Lilac Ballroom North and South, Rochester Riverside Convention Center

10:00 a.m.–10:30 a.m. Coffee Break, Lilac Ballroom Foyer, Rochester Riverside Convention Center Coffee Break, Lilac Ballroom Foyer, Rochester Riverside Convention Center

12:00 p.m.–2:00 p.m. LSMA• Laser Science Symposium on Undergraduate Research Posters, Riverside Court, Rochester Riverside Convention Center LSMA• Laser Science Symposium on Undergraduate Research Posters, Riverside Court, Rochester Riverside Convention Center

12:00 p.m.–1:30 p.m. Lunch (on your own) Lunch (on your own) 1:30 p.m.–3:30 p.m. FMA • Photonics LSMB • Laser Science FMB • Structured Wavefields FMC • Photonic Sensor I FMD • Individualized Optical FME • Spectroscopy, FMF • Quantum Information FMG • Non-Linear Imaging SMB • IPF-Biomedical LMA • Photophysics of and Energy I Symposium on for Communications and Correction of the Eye Imaging and Detection and Communications I Applications of Lasers Nanostructured Materials I Undergraduate Research I Sensing I (ends at 3:15 p.m.)

3:30 p.m.–4:00 p.m. Coffee Break, Highland Ballroom Foyer, Rochester Riverside Convention Center Coffee Break, Highland Ballroom Foyer, Rochester Riverside Convention Center 4:00 p.m.–6:00 p.m. FMH • Silicon Photonics LSMC • Laser Science FMI • Structured Wavefields FMJ • Photonic Sensor II FMK • Emerging in vivo FML • Microscopy I FMM • Quantum Information FMN • Advances in High Energy SMD • IPF- Environment LMB • Novel Imaging, Symposium on for Communications Imaging Techniques for (ends at 5:30 p.m.) and Communications II Ultrafast Laser Systems Applications of Lasers Spectroscopy and Manipulation in Undergraduate Research II and Sensing II Retinal Imaging Microstructures I (ends at 6:30 p.m.) (ends at 5:30 p.m.) (ends at 5:30 p.m.)

6:30 p.m.–8:30 p.m. OSA/SPS Student Member Welcome Reception, Temple Bar & Grille, 109 East Avenue, Rochester, NY, Phone: 585.232.6000 OSA/SPS Student Member Welcome Reception, Temple Bar & Grille, 109 East Avenue, Rochester, NY, Phone: 585.232.6000

Key to Shading Frontiers in Optics Laser Science Joint Agenda of Sessions

28 FiO/LS 2010 • October 24–28, 2010 Highland A Highland B Highland C Highland D Highland E Highland F Highland G Highland H Highland J Highland K

7:00 a.m.–6:00 p.m. Registration, Galleria, Rochester Riverside Convention Center Registration, Galleria, Rochester Riverside Convention Center

8:00 a.m.–12:00 p.m. 2010 Joint FiO/LS Awards Ceremony and Plenary Session, Lilac Ballroom North and South, Rochester Riverside Convention Center 2010 Joint FiO/LS Awards Ceremony and Plenary Session, Lilac Ballroom North and South, Rochester Riverside Convention Center

10:00 a.m.–10:30 a.m. Coffee Break, Lilac Ballroom Foyer, Rochester Riverside Convention Center Coffee Break, Lilac Ballroom Foyer, Rochester Riverside Convention Center

12:00 p.m.–2:00 p.m. LSMA• Laser Science Symposium on Undergraduate Research Posters, Riverside Court, Rochester Riverside Convention Center LSMA• Laser Science Symposium on Undergraduate Research Posters, Riverside Court, Rochester Riverside Convention Center

12:00 p.m.–1:30 p.m. Lunch (on your own) Lunch (on your own) 1:30 p.m.–3:30 p.m. FMA • Photonics LSMB • Laser Science FMB • Structured Wavefields FMC • Photonic Sensor I FMD • Individualized Optical FME • Spectroscopy, FMF • Quantum Information FMG • Non-Linear Imaging SMB • IPF-Biomedical LMA • Photophysics of and Energy I Symposium on for Communications and Correction of the Eye Imaging and Detection and Communications I Applications of Lasers Nanostructured Materials I Undergraduate Research I Sensing I (ends at 3:15 p.m.)

3:30 p.m.–4:00 p.m. Coffee Break, Highland Ballroom Foyer, Rochester Riverside Convention Center Coffee Break, Highland Ballroom Foyer, Rochester Riverside Convention Center 4:00 p.m.–6:00 p.m. FMH • Silicon Photonics LSMC • Laser Science FMI • Structured Wavefields FMJ • Photonic Sensor II FMK • Emerging in vivo FML • Microscopy I FMM • Quantum Information FMN • Advances in High Energy SMD • IPF- Environment LMB • Novel Imaging, Symposium on for Communications Imaging Techniques for (ends at 5:30 p.m.) and Communications II Ultrafast Laser Systems Applications of Lasers Spectroscopy and Manipulation in Undergraduate Research II and Sensing II Retinal Imaging Microstructures I (ends at 6:30 p.m.) (ends at 5:30 p.m.) (ends at 5:30 p.m.) Agenda of Sessions 6:30 p.m.–8:30 p.m. OSA/SPS Student Member Welcome Reception, Temple Bar & Grille, 109 East Avenue, Rochester, NY, Phone: 585.232.6000 OSA/SPS Student Member Welcome Reception, Temple Bar & Grille, 109 East Avenue, Rochester, NY, Phone: 585.232.6000

FiO/LS 2010 • October 24–28, 2010 29 Agenda of Sessions — Tuesday, October 26 Highland A Highland B Highland C Highland D Highland E Highland F Highland G Highland H Highland J Highland K 7:00 a.m.–5:30 p.m. Registration, Galleria, Rochester Riverside Convention Center Registration, Galleria, Rochester Riverside Convention Center 8:00 a.m.–9:30 a.m. VIP Industry Leaders Networking Event: Connecting OSA Corporate Members and Young Professionals, Grand Ballroom E and F, Hyatt Regency Rochester VIP Industry Leaders Networking Event: Connecting OSA Corporate Members and Young Professionals, Grand Ballroom E and F, Hyatt Regency Rochester 8:00 a.m.–10:00 a.m. FTuA • Photonics FTuB • Adaptive FTuC • Nonlinear FTuD • General Optics in FTuE • General Optics FTuF • Microscopy II FTuG • Quantum Information LTuA • Photophysics of STuA • IPF-Laser LTuB • Nonlinear Optics I and Energy II Optics for the Eye Integrated Optics Information Science and Communications III Nanostructured Materials II Applications in Metrology (ends at 9:45 a.m.) 10:00 a.m.–12:00 p.m. Students and Young Professionals Forum on Public Policy, Carlson and Douglass, Radisson Hotel Rochester Riverside Students and Young Professionals Forum on Public Policy, Carlson and Douglass, Radisson Hotel Rochester Riverside 10:00 a.m.–10:30 a.m. Coffee Break, Empire Hall, Rochester Riverside Convention Center Coffee Break, Empire Hall, Rochester Riverside Convention Center 10:00 a.m.–4:00 p.m. Exhibit Open, Empire Hall, Rochester Riverside Convention Center Exhibit Open, Empire Hall, Rochester Riverside Convention Center 10:30 a.m.–12:00 p.m. FTuH • Novel Fiber Device FTuI • Optical Design for FTuJ • Ultrafast FTuK • Generalized FTuL • Frequency Combs FTuM • Trapping I FTuN • Opto-Mechanics and LTuC • Photophysics of STuB • IPF - Frontiers in Physics LTuD • Novel Imaging, Biomedical Systems I Fiber Laser Imaging and Non- for Spectroscopy Quantum Measurement I Nanostructured Materials III Spectroscopy and Manipulation Imaging Techniques for in Microstructures II Diagnostics and Sensing I 12:00 p.m.–1:30 p.m. Exhibit Only Time, Empire Hall, Rochester Riverside Convention Center Exhibit Only Time, Empire Hall, Rochester Riverside Convention Center 12:00 p.m.–1:30 p.m. Lunch (on your own) Lunch (on your own) 12:00 p.m.–1:30 p.m. OSA Fellow Member Lunch, Grand Ballroom A and B, Hyatt Regency Rochester OSA Fellow Member Lunch, Grand Ballroom A and B, Hyatt Regency Rochester 12:00 p.m.–1:30 p.m. JTuA • Joint FiO/LS Poster Session, Empire Hall, Rochester Riverside Convention Center JTuA • Joint FiO/LS Poster Session, Empire Hall, Rochester Riverside Convention Center 1:30 p.m.–5:40 p.m. STuC • Ashkin Symposium I, Grand Ballroom D, Hyatt Regency Rochester STuC • Ashkin Symposium I, Grand Ballroom D, Hyatt Regency Rochester 1:30 p.m.–3:30 p.m. FTuO • General Wavefront FTuP • Novel Hybrid FTuQ • Disorder In FTuR • Dispersion in Ultrafast FTuS • Therapy FTuT • Quantum Information LTuE • Attosecond and LTuF • Optofluidics in LTuG • Nonlinear Optics II Issues Integration I Integrated Optical Laser Amplifiers and Communications IV Strong Field Physics I the Near-Field I (ends at 3:15 p.m.) (ends at 3:15 p.m.) Devices and Circuits I 3:30 p.m.–5:00 p.m. Meet the Editors of APS Journals, Riverside Court, Rochester Riverside Convention Center Meet the Editors of APS Journals, Riverside Court, Rochester Riverside Convention Center 3:30 p.m.–4:00 p.m. Coffee Break, Empire Hall, Rochester Riverside Convention Center Coffee Break, Empire Hall, Rochester Riverside Convention Center 4:00 p.m.–5:00 p.m. Industrial Physics Forum Corporate Reception, Empire Hall, Rochester Riverside Convention Center Industrial Physics Forum Corporate Reception, Empire Hall, Rochester Riverside Convention Center 4:00 p.m.–5:30 p.m. FTuU • Astrophotonics I FTuV • Optical FTuW • Novel Fibers FTuX • Attosecond Optics FTuY • Coherence Tomography FTuZ • Opto-Mechanics and LTuH • Frontiers in Ultracold LTuI • Optofluidics in the Near- LTuJ • Laser Cooling and Trapping Communication I and Technnology I Quantum Measurement II Molecules I Field II

Agenda of Sessions (ends 4:45 p.m.) (ends 5:15 p.m.) (ends at 5:15 p.m.) (ends at 5:15 p.m.) 4:30 p.m.–5:30 p.m. Minorities and Women in OSA (MWOSA) Tea, Grand Ballroom E and F, Hyatt Regency Rochester Minorities and Women in OSA (MWOSA) Tea, Grand Ballroom E and F, Hyatt Regency Rochester 6:00 p.m.–7:00 p.m. OSA Business Meeting, Highland A, Rochester Riverside Convention Center OSA Business Meeting, Highland A, Rochester Riverside Convention Center 6:00 p.m.–7:00 p.m. LS Business Meeting, Highland H, Rochester Riverside Convention Center LS Business Meeting, Highland H, Rochester Riverside Convention Center 6:00 p.m.–7:00 p.m. OSA Graduation Party, Riverview Lounge, Radisson Hotel Rochester Riverside OSA Graduation Party, Riverview Lounge, Radisson Hotel Rochester Riverside 7:00 p.m.–8:30 p.m. OSA LaserFest Member Reception, Lilac Ballroom North and South, Rochester Riverside Convention Center OSA LaserFest Member Reception, Lilac Ballroom North and South, Rochester Riverside Convention Center 7:00 p.m.–10:00 p.m. LS Banquet, Grand Ballroom A and B, Hyatt Regency Rochester LS Banquet, Grand Ballroom A and B, Hyatt Regency Rochester 9:00 p.m.–11:00 p.m. OSA Student Member Party, Tavern 58 at Gibbs, 58 University Avenue, Rochester, NY, Phone: 585.546.5800 OSA Student Member Party, Tavern 58 at Gibbs, 58 University Avenue, Rochester, NY, Phone: 585.546.5800 Key to Shading Frontiers in Optics Laser Science Joint

30 FiO/LS 2010 • October 24–28, 2010 Highland A Highland B Highland C Highland D Highland E Highland F Highland G Highland H Highland J Highland K 7:00 a.m.–5:30 p.m. Registration, Galleria, Rochester Riverside Convention Center Registration, Galleria, Rochester Riverside Convention Center 8:00 a.m.–9:30 a.m. VIP Industry Leaders Networking Event: Connecting OSA Corporate Members and Young Professionals, Grand Ballroom E and F, Hyatt Regency Rochester VIP Industry Leaders Networking Event: Connecting OSA Corporate Members and Young Professionals, Grand Ballroom E and F, Hyatt Regency Rochester 8:00 a.m.–10:00 a.m. FTuA • Photonics FTuB • Adaptive FTuC • Nonlinear FTuD • General Optics in FTuE • General Optics FTuF • Microscopy II FTuG • Quantum Information LTuA • Photophysics of STuA • IPF-Laser LTuB • Nonlinear Optics I and Energy II Optics for the Eye Integrated Optics Information Science and Communications III Nanostructured Materials II Applications in Metrology (ends at 9:45 a.m.) 10:00 a.m.–12:00 p.m. Students and Young Professionals Forum on Public Policy, Carlson and Douglass, Radisson Hotel Rochester Riverside Students and Young Professionals Forum on Public Policy, Carlson and Douglass, Radisson Hotel Rochester Riverside 10:00 a.m.–10:30 a.m. Coffee Break, Empire Hall, Rochester Riverside Convention Center Coffee Break, Empire Hall, Rochester Riverside Convention Center 10:00 a.m.–4:00 p.m. Exhibit Open, Empire Hall, Rochester Riverside Convention Center Exhibit Open, Empire Hall, Rochester Riverside Convention Center 10:30 a.m.–12:00 p.m. FTuH • Novel Fiber Device FTuI • Optical Design for FTuJ • Ultrafast FTuK • Generalized FTuL • Frequency Combs FTuM • Trapping I FTuN • Opto-Mechanics and LTuC • Photophysics of STuB • IPF - Frontiers in Physics LTuD • Novel Imaging, Biomedical Systems I Fiber Laser Imaging and Non- for Spectroscopy Quantum Measurement I Nanostructured Materials III Spectroscopy and Manipulation Imaging Techniques for in Microstructures II Diagnostics and Sensing I 12:00 p.m.–1:30 p.m. Exhibit Only Time, Empire Hall, Rochester Riverside Convention Center Exhibit Only Time, Empire Hall, Rochester Riverside Convention Center 12:00 p.m.–1:30 p.m. Lunch (on your own) Lunch (on your own) 12:00 p.m.–1:30 p.m. OSA Fellow Member Lunch, Grand Ballroom A and B, Hyatt Regency Rochester OSA Fellow Member Lunch, Grand Ballroom A and B, Hyatt Regency Rochester 12:00 p.m.–1:30 p.m. JTuA • Joint FiO/LS Poster Session, Empire Hall, Rochester Riverside Convention Center JTuA • Joint FiO/LS Poster Session, Empire Hall, Rochester Riverside Convention Center STuC • Ashkin Symposium I, Grand Ballroom D, Hyatt Regency Rochester STuC • Ashkin Symposium I, Grand Ballroom D, Hyatt Regency Rochester

1:30 p.m.–5:40 p.m. Agenda of Sessions 1:30 p.m.–3:30 p.m. FTuO • General Wavefront FTuP • Novel Hybrid FTuQ • Disorder In FTuR • Dispersion in Ultrafast FTuS • Therapy FTuT • Quantum Information LTuE • Attosecond and LTuF • Optofluidics in LTuG • Nonlinear Optics II Issues Integration I Integrated Optical Laser Amplifiers and Communications IV Strong Field Physics I the Near-Field I (ends at 3:15 p.m.) (ends at 3:15 p.m.) Devices and Circuits I 3:30 p.m.–5:00 p.m. Meet the Editors of APS Journals, Riverside Court, Rochester Riverside Convention Center Meet the Editors of APS Journals, Riverside Court, Rochester Riverside Convention Center 3:30 p.m.–4:00 p.m. Coffee Break, Empire Hall, Rochester Riverside Convention Center Coffee Break, Empire Hall, Rochester Riverside Convention Center 4:00 p.m.–5:00 p.m. Industrial Physics Forum Corporate Reception, Empire Hall, Rochester Riverside Convention Center Industrial Physics Forum Corporate Reception, Empire Hall, Rochester Riverside Convention Center 4:00 p.m.–5:30 p.m. FTuU • Astrophotonics I FTuV • Optical FTuW • Novel Fibers FTuX • Attosecond Optics FTuY • Coherence Tomography FTuZ • Opto-Mechanics and LTuH • Frontiers in Ultracold LTuI • Optofluidics in the Near- LTuJ • Laser Cooling and Trapping Communication I and Technnology I Quantum Measurement II Molecules I Field II (ends 4:45 p.m.) (ends 5:15 p.m.) (ends at 5:15 p.m.) (ends at 5:15 p.m.) 4:30 p.m.–5:30 p.m. Minorities and Women in OSA (MWOSA) Tea, Grand Ballroom E and F, Hyatt Regency Rochester Minorities and Women in OSA (MWOSA) Tea, Grand Ballroom E and F, Hyatt Regency Rochester 6:00 p.m.–7:00 p.m. OSA Business Meeting, Highland A, Rochester Riverside Convention Center OSA Business Meeting, Highland A, Rochester Riverside Convention Center 6:00 p.m.–7:00 p.m. LS Business Meeting, Highland H, Rochester Riverside Convention Center LS Business Meeting, Highland H, Rochester Riverside Convention Center 6:00 p.m.–7:00 p.m. OSA Graduation Party, Riverview Lounge, Radisson Hotel Rochester Riverside OSA Graduation Party, Riverview Lounge, Radisson Hotel Rochester Riverside 7:00 p.m.–8:30 p.m. OSA LaserFest Member Reception, Lilac Ballroom North and South, Rochester Riverside Convention Center OSA LaserFest Member Reception, Lilac Ballroom North and South, Rochester Riverside Convention Center 7:00 p.m.–10:00 p.m. LS Banquet, Grand Ballroom A and B, Hyatt Regency Rochester LS Banquet, Grand Ballroom A and B, Hyatt Regency Rochester 9:00 p.m.–11:00 p.m. OSA Student Member Party, Tavern 58 at Gibbs, 58 University Avenue, Rochester, NY, Phone: 585.546.5800 OSA Student Member Party, Tavern 58 at Gibbs, 58 University Avenue, Rochester, NY, Phone: 585.546.5800

FiO/LS 2010 • October 24–28, 2010 31 Agenda of Sessions — Wednesday, October 27

Highland A Highland B Highland C Highland D Highland E Highland F Highland G Highland H Highland J Highland K

7:30 a.m.–5:00 p.m. Registration, Galleria, Rochester Riverside Convention Center Registration, Galleria, Rochester Riverside Convention Center 8:00 a.m.–10:00 a.m. FWA • Astrophotonics II FWB • Biochemical Sensing FWC • Optical Design with FWD • Novel Hybrid FWE • Attosecond Optics FWF • Biosensing FWG • Nonlinearities and Gain in LWA • Hybrid Quantum Systems I LWB • Metrology and LWC • Photophysics of Energy (ends at 9:45 a.m.) Unconventional Polarization I Integration II and Technnology II Plasmonics and Metamaterials I Precision Measurements I Conversion I (ends at 10:15 a.m.)

10:00 a.m.–10:30 a.m. Coffee Break, Empire Hall, Rochester Riverside Convention Center Coffee Break, Empire Hall, Rochester Riverside Convention Center

10:00 a.m.–2:00 p.m. Exhibit Open, Empire Hall, Rochester Riverside Convention Center Exhibit Open, Empire Hall, Rochester Riverside Convention Center 10:30 a.m.–12:00 p.m. FWH • Sensing in Higher FWI • Optical FWJ • Image-Based FWK • Fiber Laser FWL • Laser Based FWM • Trapping II FWN • Nonlinearities and Gain in LWD • Hybrid Quantum Systems II LWE • Quantum Enhanced LWF • Single Molecule Dimensions — Theory and Communication II Wavefront Sensing I Particle Acceleration I Plasmonics and Metamaterials II (ends at 12:45 p.m.) Information Processing I Approaches to Biology I Hardware for Computational (ends at 12:30 p.m.) Imaging I (ends at 11:45 a.m.)

12:00 p.m.–1:30 p.m. Exhibit Only Time, Empire Hall, Rochester Riverside Convention Center Exhibit Only Time, Empire Hall, Rochester Riverside Convention Center

12:00 p.m.–1:30 p.m. Lunch (on your own) Lunch (on your own)

12:00 p.m.–1:30 p.m. JWA • FiO Poster Session, Empire Hall, Rochester Riverside Convention Center JWA • FiO Poster Session, Empire Hall, Rochester Riverside Convention Center 1:30 p.m.–3:30 p.m. SWA • Optical FWO • Plasmonics FWP • Optical Design FWQ • Photonic Bandgap FWR • Laser Based FWS • Nanopatterning FWT • Disorder In Integrated LWG • General Laser Science LWH • Chemical LWI • Photophysics of Communications and Metamaterials for with Unconventional and Slow Light Particle Acceleration II and Meta-materials Optical Devices and Circuits II Dynamics I: Multi-Dimensional Energy Conversion II Symposium I Information Processing I Polarization II Ultrafast Spectroscopy

3:30 p.m.–4:00 p.m. Coffee Break, Highland Ballroom Foyer Rochester Riverside Convention Center Coffee Break, Highland Ballroom Foyer Rochester Riverside Convention Center 4:00 p.m.–5:30 p.m. SWB • Optical FWU • Plasmonics FWV • Image-Based FWW • Nonlinear FWX • Generalized FWY • Optical Design for FWZ • General Non-linear Optics LWJ • Quantum Enhanced LWK • Attosecond and LWL • Single Molecule Communications and Metamaterials for Wavefront Sensing II Fiber Optics Imaging and Non-Imaging Biomedical Systems II Information Processing II Strong Field Physics II Approaches to Biology II Symposium II Information Processing IV Techniques for Diagnostics

Agenda of Sessions and Sensing II

4:30 p.m.–8:00 p.m. Science Educators’ Day, Lilac Ballroom North and South, Rochester Riverside Convention Center Science Educators’ Day, Lilac Ballroom North and South, Rochester Riverside Convention Center

7:00 p.m.–8:30 p.m. FiO Postdeadline Paper Sessions, See the Postdeadline Papers Book in your registration bag for exact times and locations FiO Postdeadline Paper Sessions, See the Postdeadline Papers Book in your registration bag for exact times and locations

Key to Shading Frontiers in Optics Laser Science Joint

32 FiO/LS 2010 • October 24–28, 2010 Highland A Highland B Highland C Highland D Highland E Highland F Highland G Highland H Highland J Highland K

7:30 a.m.–5:00 p.m. Registration, Galleria, Rochester Riverside Convention Center Registration, Galleria, Rochester Riverside Convention Center 8:00 a.m.–10:00 a.m. FWA • Astrophotonics II FWB • Biochemical Sensing FWC • Optical Design with FWD • Novel Hybrid FWE • Attosecond Optics FWF • Biosensing FWG • Nonlinearities and Gain in LWA • Hybrid Quantum Systems I LWB • Metrology and LWC • Photophysics of Energy (ends at 9:45 a.m.) Unconventional Polarization I Integration II and Technnology II Plasmonics and Metamaterials I Precision Measurements I Conversion I (ends at 10:15 a.m.)

10:00 a.m.–10:30 a.m. Coffee Break, Empire Hall, Rochester Riverside Convention Center Coffee Break, Empire Hall, Rochester Riverside Convention Center

10:00 a.m.–2:00 p.m. Exhibit Open, Empire Hall, Rochester Riverside Convention Center Exhibit Open, Empire Hall, Rochester Riverside Convention Center 10:30 a.m.–12:00 p.m. FWH • Sensing in Higher FWI • Optical FWJ • Image-Based FWK • Fiber Laser FWL • Laser Based FWM • Trapping II FWN • Nonlinearities and Gain in LWD • Hybrid Quantum Systems II LWE • Quantum Enhanced LWF • Single Molecule Dimensions — Theory and Communication II Wavefront Sensing I Particle Acceleration I Plasmonics and Metamaterials II (ends at 12:45 p.m.) Information Processing I Approaches to Biology I Hardware for Computational (ends at 12:30 p.m.) Imaging I (ends at 11:45 a.m.)

12:00 p.m.–1:30 p.m. Exhibit Only Time, Empire Hall, Rochester Riverside Convention Center Exhibit Only Time, Empire Hall, Rochester Riverside Convention Center

12:00 p.m.–1:30 p.m. Lunch (on your own) Lunch (on your own)

12:00 p.m.–1:30 p.m. JWA • FiO Poster Session, Empire Hall, Rochester Riverside Convention Center JWA • FiO Poster Session, Empire Hall, Rochester Riverside Convention Center Agenda of Sessions 1:30 p.m.–3:30 p.m. SWA • Optical FWO • Plasmonics FWP • Optical Design FWQ • Photonic Bandgap FWR • Laser Based FWS • Nanopatterning FWT • Disorder In Integrated LWG • General Laser Science LWH • Chemical LWI • Photophysics of Communications and Metamaterials for with Unconventional and Slow Light Particle Acceleration II and Meta-materials Optical Devices and Circuits II Dynamics I: Multi-Dimensional Energy Conversion II Symposium I Information Processing I Polarization II Ultrafast Spectroscopy

3:30 p.m.–4:00 p.m. Coffee Break, Highland Ballroom Foyer Rochester Riverside Convention Center Coffee Break, Highland Ballroom Foyer Rochester Riverside Convention Center 4:00 p.m.–5:30 p.m. SWB • Optical FWU • Plasmonics FWV • Image-Based FWW • Nonlinear FWX • Generalized FWY • Optical Design for FWZ • General Non-linear Optics LWJ • Quantum Enhanced LWK • Attosecond and LWL • Single Molecule Communications and Metamaterials for Wavefront Sensing II Fiber Optics Imaging and Non-Imaging Biomedical Systems II Information Processing II Strong Field Physics II Approaches to Biology II Symposium II Information Processing IV Techniques for Diagnostics and Sensing II

4:30 p.m.–8:00 p.m. Science Educators’ Day, Lilac Ballroom North and South, Rochester Riverside Convention Center Science Educators’ Day, Lilac Ballroom North and South, Rochester Riverside Convention Center

7:00 p.m.–8:30 p.m. FiO Postdeadline Paper Sessions, See the Postdeadline Papers Book in your registration bag for exact times and locations FiO Postdeadline Paper Sessions, See the Postdeadline Papers Book in your registration bag for exact times and locations

FiO/LS 2010 • October 24–28, 2010 33 Agenda of Sessions — Thursday, October 28

Highland A Highland B Highland C Highland D Highland E Highland F Highland G Highland H Highland J Highland K

7:30 a.m.–5:30 p.m. Registration, Galleria, Rochester Riverside Convention Center Registration, Galleria, Rochester Riverside Convention Center 8:00 a.m.–10:00 a.m. FThA • Nonlinear FThB • Plasmonics FThC • Integrated Optics FThD • Novel Measurement FThE • Lasers for Fusion FThF • Transformation Optics and FThG • General Quantum LThA • Chemical Dynamics II: LThB • Frontiers in LThC • Nanophotonics, Photonic Optics in Micro/Nano- Techniques and Fast Ignition Cloaking with Metamaterials Electronics I Multi-Dimensional Ultrafast Ultracold Molecules II Crystals and Structural Slow Optical Structures I Spectroscopy Light I (ends at 9:45 a.m.) (ends at 9:45 a.m.)

10:00 a.m.–10:30 a.m. Coffee Break, Highland Ballroom Foyer Rochester Riverside Convention Center Coffee Break, Highland Ballroom Foyer Rochester Riverside Convention Center 10:30 a.m. –12:00 p.m. FThH • Nonlinear FThI • Optical Signal FThJ • Photonic Crystal FThK • Generalized FThL • Nonlinearities and FThM • Sensing in FThN • General Quantum LThD • Single Molecule LThE • Quantum Enhanced LThF • Nanophotonics, Photonic Optics in Micro/Nano- Processing Device Imaging and Non-Imaging Gain in Plasmonics and Higher Dimensions — Electronics II Approaches to Biology III Information Processing III Crystals and Structural Slow Optical Structures II Techniques for Diagnostics Metamaterials III Theory and Hardware for Light II and Sensing III (ends at 12:15 p.m.) Computational Imaging II (ends at 11:45 a.m.)

12:00 p.m.–1:30 p.m. Lunch Break (on your own) Lunch Break (on your own) 1:30 p.m.–3:30 p.m. FThO • Nonlinear FThP • General Optical FThQ • Micro Resonators FThR • Plasmonics FThS • Strong THz Fields FThT • Encoding Optical FThU • Lens Design LThG • Metrology and Precision LThH • Frontiers in Ultracold FThV • Diffractive and Optics in Micro/Nano- Instrumentation and Metamaterials for and Applications Information — Nano-photonics, Measurements II Molecules III Holographic Optics I Optical Structures III Information Processing II Diffractive Optics and Refractive (ends at 3:45 p.m.) (ends at 2:45 p.m.) Optics for Shaping Optical Signals

3:30 p.m.–4:00 p.m. Coffee Break, Highland Ballroom Foyer Rochester Riverside Convention Center Coffee Break, Highland Ballroom Foyer Rochester Riverside Convention Center 4:00 p.m.–6:00 p.m. FThW • Three-Dimensional FThX • Fabrication FThY • Plasmonics FThZ • THz Fields and FThAA • Optics in FThBB • Difractive and Meta-materials and Testing and Metamaterials for Nonlinear Optics Micro/nano Devices Holographic Optics II Information Processing III

Key to Shading Agenda of Sessions Frontiers in Optics Laser Science Joint

34 FiO/LS 2010 • October 24–28, 2010 Highland A Highland B Highland C Highland D Highland E Highland F Highland G Highland H Highland J Highland K

7:30 a.m.–5:30 p.m. Registration, Galleria, Rochester Riverside Convention Center Registration, Galleria, Rochester Riverside Convention Center 8:00 a.m.–10:00 a.m. FThA • Nonlinear FThB • Plasmonics FThC • Integrated Optics FThD • Novel Measurement FThE • Lasers for Fusion FThF • Transformation Optics and FThG • General Quantum LThA • Chemical Dynamics II: LThB • Frontiers in LThC • Nanophotonics, Photonic Optics in Micro/Nano- Techniques and Fast Ignition Cloaking with Metamaterials Electronics I Multi-Dimensional Ultrafast Ultracold Molecules II Crystals and Structural Slow Optical Structures I Spectroscopy Light I (ends at 9:45 a.m.) (ends at 9:45 a.m.)

10:00 a.m.–10:30 a.m. Coffee Break, Highland Ballroom Foyer Rochester Riverside Convention Center Coffee Break, Highland Ballroom Foyer Rochester Riverside Convention Center 10:30 a.m. –12:00 p.m. FThH • Nonlinear FThI • Optical Signal FThJ • Photonic Crystal FThK • Generalized FThL • Nonlinearities and FThM • Sensing in FThN • General Quantum LThD • Single Molecule LThE • Quantum Enhanced LThF • Nanophotonics, Photonic Optics in Micro/Nano- Processing Device Imaging and Non-Imaging Gain in Plasmonics and Higher Dimensions — Electronics II Approaches to Biology III Information Processing III Crystals and Structural Slow Optical Structures II Techniques for Diagnostics Metamaterials III Theory and Hardware for Light II and Sensing III (ends at 12:15 p.m.) Computational Imaging II (ends at 11:45 a.m.)

12:00 p.m.–1:30 p.m. Lunch Break (on your own) Lunch Break (on your own) 1:30 p.m.–3:30 p.m. FThO • Nonlinear FThP • General Optical FThQ • Micro Resonators FThR • Plasmonics FThS • Strong THz Fields FThT • Encoding Optical FThU • Lens Design LThG • Metrology and Precision LThH • Frontiers in Ultracold FThV • Diffractive and Optics in Micro/Nano- Instrumentation and Metamaterials for and Applications Information — Nano-photonics, Measurements II Molecules III Holographic Optics I Optical Structures III Information Processing II Diffractive Optics and Refractive (ends at 3:45 p.m.) (ends at 2:45 p.m.) Optics for Shaping Optical Signals

3:30 p.m.–4:00 p.m. Coffee Break, Highland Ballroom Foyer Rochester Riverside Convention Center Coffee Break, Highland Ballroom Foyer Rochester Riverside Convention Center Agenda of Sessions 4:00 p.m.–6:00 p.m. FThW • Three-Dimensional FThX • Fabrication FThY • Plasmonics FThZ • THz Fields and FThAA • Optics in FThBB • Difractive and Meta-materials and Testing and Metamaterials for Nonlinear Optics Micro/nano Devices Holographic Optics II Information Processing III

FiO/LS 2010 • October 24–28, 2010 35 Monday, October 25 36 Heat Pumps to Solar Pumped Lasers, Optical From Concentrators: Solar Luminescent M. Tomes dramatic increases in the efficiency ofdramatic LSCs. increases efficiency inthe of promise the with lasers, factor high-quality a of demonstrate experimentally non-resonant pumping concentrators (LSCs) do not need to track the sun. We USA, FMA1 •1:30p.m. Delaware, USA,Presider Sylvain G.Cloutier; Univ. of FMA •PhotonicsandEnergyI 1:30 p.m.–3:30p.m. 2 Univ. of Michigan, USA. Michigan,Univ. of 2 , H. Mendoza Highland A FiO 1 , T. Carmon T. , Invited Luminescent solar Luminescent 2 12:00 p.m.–2:00 p.m. LSMA: Laser ScienceSymposiumonUndergraduateResearch Posters, Riverside Laser 12:00 p.m.–2:00p.m.LSMA: Court, Rochester Riverside Convention Center , M. Baldo C. Rotschild 8:00 a.m.–12:00p.m. 1 ; 1 MIT, 1 , on UndergraduateResearch I ScienceSymposium LSMB •Laser 2:00 p.m.–4:00p.m. 10:00 a.m.–10:30a.m. Highland B 2010 Joint FiO/LS Awards Ceremony and Plenary Session, 2010 JointFiO/LSAwardsCeremonyandPlenary LS 7:00 a.m.–6:00p.m. FiO/LS 2010 12:00 p.m.–1:30p.m. Coffee Break,Lilac Ballroom Foyer, Rochester Riverside Convention Center correlations are compared for different types. beam correlations are evaluated and the behaviour of these atmospheric turbulence. Received field and intensity second and fourth order moments are formulated in Turkey. Univ., Turbulent Atmosphere, Yahya K.Baykal ; Çankaya in Evaluated Parameters Moment Order Fourth and Second the on Incidence of Type of Effects Associates, USA,Presider Kevin Thompson; Optical Res. Communications andSensingI FMB •StructuredWavefields for 1:30 p.m.–3:15p.m. FMB1 •1:30p.m. Registration,

Using a general type incidence, the incidence, type general a Using • Highland C October 24–28,2010 Invited Galleria, Rochester Riverside Convention Center Lunch (on yourLunch own) Lilac Ballroom North and South, Rochester Riverside Convention Center Labs-Res., USA.Abstract not available. OTDR, Using Brillouin Cable Fiber-Optic Buried a in Changes Strain Long-TermTemperatureMonitoring ofLocal and FMC1 •1:30p.m. Presider N. J. Tao; Arizona State Univ., USA, FMC •PhotonicSensorI 1:30 p.m.–3:30p.m. Highland D FiO ; AT&TNagelJonathan; A. Invited aberrated eyes. highly in performance visual on blur optical of impact detrimental the of some for compensated aberrations order higher native their to adaptation was found with adaptive Itoptics performance. that visual long-term on neural impact its and eye the of adaptive optics enhanced our understanding of optics Yoon Neural Impact on Visual Performance, and Optical Study to Optics Adaptive of Use The FMD1 •1:30p.m. Presider Jason Porter, Univ. of Houston, Correction oftheEye FMD •IndividualizedOptical 1:30 p.m.–3:30p.m. ; Univ. of Rochester,USA. Univ.of ; Highland E Invited Recent advances in advances Recent Geun-Young Monday, October 25 37 , 1 , M. M. , 2 , O. Kas O. , 1 Lewis Rothberg Lewis Univ. Univ. of Rochester, 1 We study - We phenylen ; 2 Invited , D. McCamant D. , 1 LS , K. Kiick 2 Highland K Highland , J. Rhinehart 1 , M. Galvin 2 Univ. of USA. Univ. Delaware, 2 evinylene evinylene chromophore pairs whose spacing and peptide to them coupling by varied be can orientation are excitations interchromophore Copious backbones. observedyields in fluorescence reduced explain and solutions. to films polymer relative conjugated 1:30 p.m.–3:30 p.m. LMA • Photophysics of Nanostructured Materials I Mellon Carnegie Peteanu; Linda USA, Presider Univ., S. Paquette S. USA, Photophysical Photophysical Consequences of Interactions Be- Chromophores, Conjugated tween Charati LMA1 • 1:30 p.m. At Invited ; LenSx Lasers, Inc., USA. Inc., Lasers, LenSx ; Highland J Highland JOINT FiO/LS JOINT Michael Karavitis Michael 1:30 p.m.–3:30 p.m. Applications IPF-Biomedical • SMA of Lasers Chroma Stanley; Michael USA, Presider Corp., Technology SMA1 • 1:30 p.m. Laser Refractive Cataract Surgery with the LenSx Laser, LenSx Lasers, we have developed a femtosecond laser femtosecond a developed have we Lasers, LenSx ultrashort of precision high The surgery. cataract for safer a in results tissue in photodisruption pulse laser tradi- over outcomes visual enhanced with procedure surgery. cataract tion Lilac Ballroom North and South, Rochester Riverside Convention Center Convention Riverside Rochester South, and North Ballroom Lilac Dispersion Dispersion (on your own) Lunch your (on Galleria, Rochester Riverside Convention Center Convention Riverside Rochester Galleria, Invited October 24–28, 2010 Yair Andegeko, Vadim V. Lovozoy, Lovozoy, V. Vadim Andegeko, Yair • Highland H Highland Registration, Registration, Dmitry Pestov, Pestov, Dmitry FMG1 • 1:30 p.m. 1:30 p.m.–3:30 p.m. FMG • Non-Linear Imaging Univ., Fleischer; Princeton Jason USA, Presider Non-Linear Imaging with Ultrashort Shaped Puls- Shaped Ultrashort with Imaging Non-Linear es, USA. Univ., State Michigan Dantus; Marcos of ultrashort compensation pulses at the focal plane presentation Our signal. greater significantly to leads - photoen and photobleaching observed on focus will long for signal fluorescent two-photon of hancement pulses. (sub-15fs) ultrashort (200fs) and Lilac Ballroom Foyer, Rochester Riverside Convention Center Convention Riverside Rochester Foyer, Ballroom Coffee Break, Lilac ; 12:00 p.m.–1:30 p.m. 1 FiO/LS 2010 , Lijun , , Colin 1 1 Single Single photon 7:00 a.m.–6:00 p.m. 7:00 a.m.–6:00 , Kartik , Srinivasan Kartik 2 Univ. of Oregon, USA, Univ. 1 ; 3 Matthew T. Rakher T. Matthew , Michael , G. Michael Raymer 1 2010 Joint FiO/LS Awards Ceremony and Plenary FiO/LS Awards Ceremony 2010 Joint Session, FiO , Xiao , Tang Xiao 2 Univ. Univ. of California at San Diego, 3 Highland G Highland 10:00 a.m.–10:30 a.m. , Stojan Radic 2 waveguide using a 1550 nm pump. The (0)=0.165. 3 (2) Frequency Frequency translation of single-photon states g , Oliver , Slattery Oliver 2 Ctr. for Nanoscale Science and Technology, USA, Information Technology Lab, Information Technology USA. Bell Bell Labs, USA, FMF2 • 1:45 p.m. Quantum Transduction of Telecommunications- band Single Photons from a Quantum Dot by Upconversion, Frequency USA. in optical fiber through use of the Bragg scattering mixing four-wave process is achieve studied. 28 We nature nonclassical the verify and translation percent light. the involved of FMF1 • 1:30 p.m. of Frequency Single-Photon States by Translation Mixing Four-Wave in a Photonic Crystal Fiber, Hayden J. McGuinness emission emission from an dot quantum InAs emitting at 1.3 periodically-poleda in nm 710 to upconverted is µm LiNbO 1 2 1:30 p.m.–3:15 p.m. FMF • Quantum Information and Communications I do Federal Univ. Davidovich; Luiz Presider Brazil, Janeiro, de Rio 2 J. J. McKinstrie upconverted upconverted light exhibits photon anti-bunching with Ma - , Rita S. , Darren Darren , 1 1 8:00 a.m.–12:00 p.m. 8:00 a.m.–12:00 , Bruce - J. Trom 2 Riverside Court, Rochester Riverside Convention Center Convention Riverside Rochester Court, LSMA:12:00 p.m.–2:00 p.m. Laser Riverside Posters, on Undergraduate Research Science Symposium Chao Comprehen 2 Invited , Vaya Tanamai W. 1 , Amanda F. , Durkin Amanda F. , John Butler 1 Diffuse OpticalSpectroscopic 2 Highland F Highland Albert Cerussi Albert , Shigeto Ueda 1 , David Hsiang Beckman Laser Inst., USA, Laser Inst., Beckman 2 1 ; 1 Roblyer 1:30 p.m.–3:30 p.m. Imaging and FME • Spectroscopy, Detection sive Cancer Ctr., USA. Ctr., Cancer sive Imaging (DOSI) provides non-invasive functional biomarkers that correlate with final pathological chemotherapy (neoadjuvant) pre-surgical to response various at measured are that patients cancer breast in the therapy throughout timepoints Gregory R. Kilby; United States States United R. Kilby; Gregory USA, Presider Acad., Military FME1 • 1:30 p.m. Mehta Monitoring Monitoring Breast Cancer Tumor Response at Different Timepoints During Pre-Surgical Che- motherapy with Diffuse Optical Spectroscopic Imaging, berg Monday, October 25 38 FMA3 •2:30p.m. carriers are effectively apart. pulled light in regionsthose of a cell where photogenerated efficiency of solar cells by directing and concentrating interestfor conversion its energy ability the toboost Stanford Univ., USA. Harvesting, Energy tovoltaic PhotonNanoscale Management for Pho - Efficient Contacts, Metal Low-Cost Employing Cells Solar Dot Quantum Colloidal Heterojunction Depleted Cells Solar QuantumDot Heterojunction Depleted Colloidal Toronto, Canada, over 5%power conversion efficiency. The resulting 3-dimensional heterojunction exhibits shortcomings. their addressing while dotsquantum accentuates the benefits of lead chalcogenide colloidal simultaneouslythatarchitecture cell solar a present Zheng-Hong Lu Wang Xihua Andras G. Pattantyus-Abraham uddin 4 FMA2 •2:00p.m. Energy I—Continued FMA •Photonicsand Fischer Swiss Federal Inst. of Technology,Switzerland.of Inst. Federal Swiss 4 , Michael Grätzel 1 , Gerasimos Konstantatos 1 , Larissa Levina Larissa , 1,3 , Ines Raabe Ines , Highland A 2 ICFO, Spain, Illan Kramer Illan Plasmonics is gaining significant FiO 4 , Edward H. Sargent Invited Invited 4 , Mohammad K. Nazeer 1 1 3 Jag Tang Jiang , , Aaron R. Barkhouse R. Aaron , Yunnan Univ., China, Mark Brongersma ; Mark 1,2 1 Rtn Debnath Ratan , , Mark T. Greiner 1 ; 1 , Armin Armin , 1 Univ. of of Univ. We We 1 1 1 - , , , Research I—Continued Symposium onUndergraduate Science LSMB •Laser Highland B LS FiO/LS 2010 Self-Similar Structured Fields in Coherent Dif Coherent in Fields Structured Self-Similar FMB4 •2:30p.m. fusing Media, fusing turbulence regime. strong the in atmosphericeven turbulencestrength, Martin P. J. Lavery i Davidson Nir Yankelev Dimitry in the limitin the of dominating diffusion. vapor thermal in dynamics polariton of description quasi-eigenmodes a obtainWe diffraction. optical ofcoherentGaussian analogous tomodes diffusion, under fields evolving self-similarly measure and Sensing I—Continued for Communicationsand FMB •StructuredWavefields 3 C parameter strength turbulence atmospheric of tion - func a as dislocation ring of radius of expression USA. Charlotte, at Carolina North Beam, Vortexby Measurement of Atmospheric Turbulence Strength FMB3 •2:15p.m. This allows of sorting optical OAM components. momentum (OAM) becomes transverse momentum. same the distort time such them that orbital angular tics is used to image two planes into each other and at Orbital Angular Momentum, Optical Measure toTransformation UsingOptics FMB2 •2:00p.m. Israel, Tyc MasarykUniv., CzechRepublic. n 2 has been derived. It can be used to measure to used be can It derived. been has 3 ; 1 Univ. of Glasgow, UK, 2 Weizmann Inst. of Science, Israel. Science, of WeizmannInst. 2 ; 1 Technion-Israel Inst. of Technology,of Technion-IsraelInst. Ofer Firstenberg Ofer • Highland C 1 1 , Rami Pugatch Rami , , Gregorius C. G. Berkhout aog Gu Yalong October 24–28,2010 2 Leiden Univ., Netherlands, Johannes K. Courtial , Greg Gbur; Univ.of Gbur; Greg , Transformationop - 2 , Moshe Shuker Moshe , 1 An approximate An , Paz London Paz , We deriveWe 2 , Tomáš 1 1 1 - , , , FMC4 •2:30p.m. in harsh environments are discussed. also reliabilityandperformancedevelopments system in distributed temperature sensing and discusses recent practical challenges and main applications of Raman UK. Ctr., ogy Hartog Arthur TemperatureSensors, Distributed Raman-Based the datathe is discussed. of stability temporal The model. empirical simple a the statistics of these fluctuations can be captured by Surprisingly,apparatus. OTDR photon-counting a stochastic fluctuations in Rayleigh backscattering with Misha Brodsky Fibers? Individual Identify to Used Be it Could - Fibers Optical from Backscattering Rayleigh FMC3 •2:15p.m. 1 at low frequencies. systems interferometric fiber of limit precision the on perspective new a providesresult The Theorem. Fluctuation-Dissipationthe on based model 1-D a using analyzed is damping structural by caused USA. Huntsville,Alabama, of InterferometricFiber Systems, in Noise Thermal Damping-Induced Structural FMC2 •2:00p.m. Continued FMC •PhotonicSensorI— AT&T Labs, USA, AT&TLabs, 1 The paper reviews the technology, the reviews paper The ; Schlumberger Fiber-Optic TechnolFiber-OpticSchlumberger - ; , Jungmi Oh Highland D 2 TelAvivUniv., Israel. FiO Invited 1 , Moshe Tur Moshe , Fiber thermal noise thermal Fiber ; Univ.DuanLingze; 2 , Paul Henry Weprobe 1 ; Performance of Aspheric IOLs, Aspheric of Performance nez-Alfaro Lourdes Llorente Lourdes and aspheric new designs. models, eye customized using performance, optical on misalignment of effect the eyes, pseudophakic in aberrations Weoptical presentlenses. crystalline young emulate to order in aberration spherical Jiménez-Díaz,Spain. Sergio BarberoSergio FMD3 •2:15p.m. of diffractive profile.of diffractive distance in relation with refractive error and location reading describes presbyopiapaper This correction. cal intraocular lenses are currently a viable option for AMO Groningen BV, Netherlands. Marrie van der Mooren, Henk Weeber, Patricia Piers; Reading Distance of Multifocal Intraocular Lenses, FMD2 •2:00p.m. Correction oftheEye—Continued FMD •IndividualizedOptical Thank youforattending know yourthoughtson post-conference survey via emailandletus 2 ; 1 Inst. de Optica, CSIC, Spain, Look foryour the program. 1 , Patricia Rosales 1 Highland E , Carlos DorronsoroCarlos , FiO/LS.  AsphericnegativeIOLsinduce Invited 1 , Alberto de Castro Diffractive Diffractive Multifo- Susana Marcos Susana 1 , Ignacio JiméIgnacio- , 2 Fundación 1 1 , , Monday, October 25 39 , 1 Using Using Ctr. Ctr. for 3 Zernicke , Andrew Andrew , 2 3 Natl. - Renew Natl. 1 ; , Jurjen - Wilde 1 1 , Andrew , Ferguson Andrew 1 Invited Invited , Peter M. Goodwin M. Peter , Plextronics, Inc., USA. Inc., Plextronics, LS 3 2 , Garry Rumbles 2 Highland K Highland , Gizelle Sherwood 1 , Nikos , Kopidakis Nikos 1 Carnegie Carnegie Mellon USA, Univ., 1 ; ; 3 , E. Sheina 2 Chain Chain aggregation in electroluminescent - ma , James H. Werner H. James , 2 LMA • Photophysics of LMA • Photophysics Materials I— Nanostructured Continued Integrated Nanotechnologies Los Nanotechnologies Integrated Alamos Natl. Labs, USA. terials affects profoundly their emission and charge fluorescence time-resolved aggregate Single transport. oligomer MEH-PPV shorter-chain of studies imaging - rational that details morphological reveal aggregates properties. emission ize their unusual able Energy USA, able Lab, flash photolysis, transient microwave conductivity we we conductivity microwave transient photolysis, flash polythiophene two on results preliminary some report - with the theubiqui results compare and derivatives tous poly(3-hexylthiophene). The data provide an into dissociation exciton of efficiency the into insight free carriers; charge a that result is of importance to solar cells are that photovoltaic bulk heterojunction, a construct of a blend of polymers of this type with the soluble fullerene, [6,6]-phenyl-C61-butyric acid (PCBM). ester, methyl Inst. Inst. of Advanced Materials, Netherlands, P. S hre v e LMA3 • 2:30 p.m. man D. Laird Transient Transient Microwave Conductivity Studies of (3-alkyl Poly thiophene)s and Blends with PCBM, David Coffey Effects of Aggregation on the Emission Spectra and Dynamics of Electrolumine Scent Materials, Linda Peteanu LMA2 • 2:00 p.m. LMA2 • 2:00 p.m.

- ; Illumina, USA. Invited Invited Highland J Highland Suzanne Wakelin David ; Piston W. USA. Univ., Vanderbilt JOINT FiO/LS JOINT SMA • IPF-Biomedical Applications Applications IPF-Biomedical • SMA of Lasers—Continued SMA3 • 2:30 p.m. SMA2 • 2:00 p.m. SMA2 • 2:00 From From Photonics to Genomics: Lasers and - Imag ing Technology Enables Next-Generation DNA Sequencing, Massive optical parallelism used in current Genome parallelism usedoptical Genome in current Massive Sequencing “Next-Generation” that means Analyzers the explores presentation This reality. present-day a is of types these enabling in optics and lasers of role key technologies. sequencing DNA Applications of Table Top Lasers DevelopedTop of Applications from Table the FEL, Discoveries made with Free-Electron Lasers in the IR the in Lasers Free-Electron with made Discoveries dedicated for opportunities a open spectra x-ray and applica and developments Current systems. table-top and x-rays monochromatic for systems such of tions IR will be described.

Alexandre Alexandre Christopher Invited The The field generated through October 24–28, 2010 • Highland H Highland , , Jason Fleischer; W. Princeton USA. Univ., ; École Polytechnique Fédérale de de Fédérale Polytechnique École ; Psaltis Demetri FMG • Non-Linear Imaging— FMG • Non-Linear Continued FMG2 • 2:00 p.m. FMG2 • 2:00 Theory, Abbe of Extensions Nonlinear Barsi FMG3 • 2:15 p.m. Nonlinear Nonlinear Imaging of Coherent Fields, Goy, Lausanne, Switzerland. is nonlinear propagation holographically measured. reconstruct to used is propagation reverse Nonlinear medium. the nonlinear the field throughout Abbe theoryAbbe describes in imaging captured terms of diffracted orders, with higher orders providing better resolution. We show, experimentally and numerically, that nonlinearity breaks down linear limits, as high-frequency spatial modes mix with ones. low-frequency

FiO/LS 2010 Alex Xiaoying Xiaoying , Scott M. , Myungshik , Myungshik 2 , Matthäus M. 1 Inst. for Mathematical Mathematical for Inst. 2 Junlin Junlin Liang , Mark S. Tame 1 FiO We perform a parametric down- parametric a perform We , Jérémie Fulconis 1 Highland G Highland By By pumping a birefringent photonic Univ. of Bristol, UK, of Bristol, Univ. 1 , John G. Rarity ; 1 , Bryn Bell 2 1 , , Liang Cui, Ningbo Zhao; China. Univ., Tianjin FMF • Quantum Information and Information and FMF • Quantum I—Continued Communications - Bal Maryland of Univ. Pittman; B. Todd Hendrickson, USA. County, timore using experiment interference two-photon conversion a and interferometers Mach-Zehnder unbalanced two The pump. continuous-wave short-coherence-length coherence pump the of role the explores experiment interferometry. in two-photon FMF3 • 2:00 p.m. The Role of Pump Coherence in a Two-photon Interference Experiment, Signal and idler photon pairs at about 0.8 and 1.4 μm, respectively, are generated from 1-meter-long photonic crystal fiber. By using pump pulses correlated with positively frequency wavelengths, different obtained. are pairs photon de-correlated and Li FMF4 • 2:15 p.m. Photon Pairs with Tailored Spectral Generated Properties from Photonic Crystal Fiber, FMF5 • 2:30 p.m. Sources, Fibre Using Generation State Cluster Clark Halder S. Kim Sciences, Sciences, UK. time- generate we directions opposite in crystalfibre - Perform pairs. photon entangled limited bandwidth ing a fusion gate on from photons two independent sources we create and characterize a four-qubit cluster state. , 2 Aalto 3 SNOM , Sergey 1 - Got Paul , 1 Aeon Imaging, Aeon Imaging, 1 ; 2 The use of dynamic The use dynamic of , Rachel Schneerson Rachel , 2 Srinivasan Iyer Royal Inst. of Technology, Technology, of Inst. Royal 1 , 1 ; 1,3,4 AlexandraAlimova City City College of New USA, York, , , Ann E. Elsner 1 1 1 ; 1 , John Robbins John , Highland F Highland Univ. of Univ. Joensuu, Finland. 2 4 Sergei Sergei Popov Indiana Univ., USA. Univ., Indiana 2 , Ari T. Friberg T. Ari , Waterford Inst. of Technology, Ireland, Ireland, Technology, of Inst. Waterford AlvinKatz 2 2 Spectroscopy Spectroscopy of avian influenza - hemaggluti , Jerry Keith Jerry , 1 Natl. Inst. of Child Health and Human Development, Development, Human and Health Child of Inst. Natl. FME3 • 2:15 p.m. Fluorescence of Influenza Surface Hemagglutinin Protein, LLC, USA, LLC, tlieb fixation targets in the Laser Scanning Digital Camera Camera Digital Scanning Laser the in targets fixation creates sufficient inter-frame image differences to rapidly remove central reflection artifacts in post- Analysis. Component Principal using processing Univ., Finland, Univ., USA. nin reveals changes in peak position and emission of intensity tryptophan fluorescence upon exposure to an acidic environment. These are attributed induced to hemagglutinin the in changes conformational pH. lower by 2 FME2 • 2:00 p.m. - Ophthalmo Laser Scanning from Removal Artifact Analysis, Component Principal Using Images scope Matthew S. Muller FME • Spectroscopy, Imaging and FME • Spectroscopy, Detection—Continued technique used in THz range demonstrates enhanced enhanced demonstrates range THz in used technique scattering in far-field region and increased - resolu tion of the scanned image. We develop a rigorous numerical model which can properly describe both these phenomena. Sergeyev Swapan Swapan K. Gayen Sweden, Sweden, FME4 • 2:30 p.m. Pulsed THz Radiation in near-Field Domain: Enhanced Scattering and Exceeding Diffraction Limitations, Monday, October 25 40 fraction offraction indirectly excited Erions (>50%) films show low threshold efficient excitation of large Er, followed by low temperature annealing, codoped nanostructured films formed by Si nanoparticles and Nanostructured SiNPs-Er Codoped Al Codoped SiNPs-Er Nanostructured FMA5 •3:15p.m. Spain. CSIC, Optics, Inst.of Nuñez-Sanchez, Serna; Rosalia Conditions, Flux Photon Low Under Amplification forPotential High Showing photovoltaic cells. enhanced plasmon of performance the improving behavior in Ag nanoparticles that is beneficial towards scattering resonant plasmon fundamental identify we measurements, spectrometer and modeling (FDTD) time-domain finite-difference theory, Mie Fauchet; Univ. of Rochester, USA. Cells, tovoltaic Pho - Enhanced Plasmon Improving for Arrays Nanoparticle Silver in Scattering Understanding FMA4 •3:00p.m. Energy I—Continued FMA •Photonicsand

Report an one-step preparation process of process preparation one-step an Report Highland A , Philippe M. M. Philippe P.Clarkson, Jeffrey FiO , Sara Sara Roque , Pablo Through the use of 2 O 3 Films Films Research I—Continued Symposium onUndergraduate Science LSMB •Laser Highland B 3:30 p.m.–4:00p.m. LS FiO/LS 2010 Coffee Break,Lilac Ballroom Foyer, Rochester Riverside Convention Center of unique the beam-shaping phenomena. evanescent wave model provided a good explanation diffractive composite and analyses time-domain Finite-difference grooves. metallic periodic 1-D in beam formation from a sub-wavelength slit embedded Republic of. Republic Kang Sehun Grooves, Metallic in Embedded WavelengthSlit Sub- through Transmission Directive Highly Using Generation Beam Bessel-Like Quasi-1-D FMB6 •3:00p.m. communication. prove to be very useful in increased-bandwidth optical could system this design, straightforwardits to Due components. optical custom two on based states momentum angular optical sort to way efficient an Marco W.Beijersbergen Marco Univ.,Netherlands, Sensing I—Continued for Communicationsand FMB •StructuredWavefields BV,Netherlands, Berkhout Transformation, Geometric a on MomentumAngular StatesOptical Sorting Based FMB5 •2:45p.m. 1,2 , MartinP., J.Lavery

We report unique quasi-1-D Bessel-like Bessel-like quasi-1-DWe unique report , Kyunghwan Oh; Yonsei Univ., Korea, Univ.,Yonsei Oh; Kyunghwan , • Highland C 3 Univ. of Glasgow,Univ.UK. of 2 cosine Science & Computing Computing & Science cosine October 24–28,2010 1,2 , Miles J. Padgett J. Miles , 3 , Johannes, Courtial Gregorius C. G. C. Gregorius Wepresent 3 ; 1 Leiden 3 , wata UsedDiodes Laser in Robot, Recycling Plastic Identification Sensor with Five Wavelength FMC6 •3:15p.m. plastics, are demonstrated at stores. sort can which robots, recycling plastic new The are identified by a sensor with five wavelengths lasers. technology for recycling. Six different types of plastics California at Santa Cruz, USA, Shaowei Chen Shaowei Raman Raman Scattering (SERS), Portable Fiber Sensors Based on Surface-enhanced FMC5 •3:00p.m. 2 1 the high sensitivity. high the fiber and a liquid core photonic crystal fiber to multimode achieve tip-coated a both using demonstrated surface-enhanced Raman scattering is experimentally USA. Continued FMC •PhotonicSensorI— Photonics Advanced Res. Ctr., Osaka Univ., Japan,Univ., Osaka Ctr., Res. Advanced Photonics IDEC Corp., Japan. Corp., IDEC 1 , A portablesensingA molecularon system based Koji Koji Inada 1 , Jin Z. Zhang Z. Jin , Highland D 2 , , Tadaetsu Hirao Plastic identification is a key a is identification Plastic FiO Xuan Xuan Yang 1 , 2 Claire Gu Claire NASA Ames Res. Ctr., 2 , , Toshihiro Fujita 1,2 , Bin Chen 1,2 Satoshi Ka Satoshi ; 1 Univ.of 1,2 2 - ; , will be revised. be will vision for relevance its and eye human the of ties proper optical main The performance. visual final the produce to interact factors neural and retinal However,optical, eye’soptics. the of quality the by Artal Eye’sthe of Role The AberrationsVision, in Journal of Vision. the and A America of Society Optical Journal the of studentsHe andcurrentlyispost-docs. editor of the graduate many of mentor and Ophthalmology and numbera oftechnologies applied Visionin research in research institutions around the world. Inventor of seminars 150 around and meetings international in 4000 citations, presented more than than 150 invited more talks received that papers reviewed 130 than morepublished hasUniversity Murciaand ofthe at the founder and director of the Laboratorio de Optica is awards.internationalHeresearchand national of gural) of ARVO in 2009. Prof. Artal received a number (OSA) America in 1999 and a fellow member (inau- of Society Optical the of fellowmember elected was Adaptive Optics, Biomedical Optics & Photonics. He Instrumentation, Optical Optics, Visual in interest of Murcia, Spain. An optical and Vision scientist with professora Pablois UniversityatArtal ofOptics the FMD4 •2:45p.m. Correction oftheEye—Continued FMD •IndividualizedOptical ; Univ. de Murcia, Spain. Highland E Tutorial Spatial vision is limited Pablo Pablo - Monday, October 25 41 , Fan Univ. Univ. 1 2 , Joel M. Joel , 1 , Stephen 1 Xin Ma We We report on , Thomas E. O. O. E. Thomas , 1 Dept. of Electrical and 1 , Jon Matichak Joseph W. Perry Joseph W. 2 ; Georgia Tech, USA, Tech, Georgia 1 1,2 ; 1 LS , Matteo Cozzuol Matteo , 1 Highland K Highland Third-order nonlinearities and optical optical and nonlinearities Third-order , Seth R. Marder , Harry L. Anderson 1 2 , San-Hui Chi San-Hui , 1 Sylvain Sylvain G. Cloutier , 1 Delaware Delaware Biotechnology Inst., USA. LMA • Photophysics of LMA • Photophysics Materials I— Nanostructured Continued Computer Engineering, Univ. of Delaware, USA, Xu 2 Hales Screen the polymer chain morphology in polymer solvents of LED kinds different using fabricated structures and baking, of effect the non-aromatic), and (aromatic and property transport charge on consequences their device performance. of Oxford, UK. Oxford, of switching and limiting figures of merit are reported for several conjugated organic materials. - Polyme hyperpolarizability imaginary to real large with thines nonlinear strong with polymers conjugated and ratios will beabsorption discussed. LMA4 • 3:00 p.m. Organic Materials for All-Optical Signal - Process Optical and Limiting, ing LMA5 • 3:15 p.m. Solvent and Baking Effect on Polymer - Morphol ogy and PLED Device Performance, Barlow OCT generates generates OCT Invited ; MIT, USA. MIT, ; Highland J Highland Jim Fujimoto Jim JOINT FiO/LS JOINT SMA • IPF-Biomedical Applications Applications IPF-Biomedical • SMA of Lasers—Continued SMA4 • 3:00 p.m. high resolution, cross-sectional and 3-D diagnostic images standard of a become has It pathology. tissue in ophthalmology and is making rapid advances in cardiovascular imaging. This presentation reviews development. its the technology and Biomedical Imaging with Optical Coherence - To mography, , , 3 2 Yan- , Weijun Tong Weijun , 3 Yangtze Optical Optical Yangtze 3 Univ. of California Univ. 1 ; 1 ; Harvard Univ., USA. Univ., Harvard ; We report multimodal report We , Mikhail Slipchenko 1 , Su Chen Su , 3 Invited October 24–28, 2010 Sunney Xie Sunney • Purdue Univ., USA, Univ., Purdue Highland H Highland 2 Jay Jay E. Sharping , Huifeng Wei Huifeng , 2 , 2 , Christiane Pailo 1 FMG • Non-Linear Imaging— FMG • Non-Linear Continued Abstract not available. not Abstract FMG5 • 3:00 p.m. FMG4 • 2:45 p.m. FMG4 • 2:45 Fiber OPO for Multimodal CARS Imaging, Hua Zhai China. Co.Ltd., Cable and Fibre a with imaging scattering Raman anti-Stokes coherent a on based is which oscillator parametric optical fiber crystal fiber fiber. a photonic lasercompact and Ji-Xin Cheng Ji-Xin DelongZhang - Biol for Microscopy Scattering Raman Stimulated Medicine, and ogy at Merced, USA, Merced, at , , Lilac Ballroom Foyer, Rochester Riverside Convention Center Convention Riverside Rochester Foyer, Ballroom Coffee Break, Lilac 2 1 FiO/LS 2010 Univ. of Bristol, Univ. 1 , Chengyong Hu ; 1 2 , Lucas Worschech Lucas , 1 We discuss - interac We Invited FiO , Ruth OultonRuth , , Sven Hofling 1 2 3:30 p.m.–4:00 p.m. Highland G Highland , Andrew , B. Andrew Young 1 Germany. Würzburg, Univ. 2 FMF6 • 2:45 p.m. FMF6 • 2:45 p.m. FMF • Quantum Information and Information and FMF • Quantum I—Continued Communications UK, Christian Christian Schneider Arthur C. T. Thijssen T. C. Arthur tion tion between light and matter in optical structures scale the at are thisthat wavelength illustrating with recent results from pillar microcavities containing dots. quantum single Quantum Quantum Optics in Scale Wavelength Structures, G. John Rarity , - 2 Us

Jason W. W. Jason Deepu K. Inst. of Optics, Univ. Univ. Optics, of Inst. 1 ; We develop a method a develop We 1 , Masahiko Takahata Masahiko , 1 Ctr. for Musculoskeletal Res., Univ. Univ. Res., Musculoskeletal for Ctr. A Raman spectroscopy system has has system spectroscopy Raman A 2 Highland F Highland Jason R. Maher , Andrew J. Berger J. Andrew , 2 Dmitry V. Dylov, Laura Waller, Waller, Laura Dylov, V. Dmitry USA. Univ., Princeton ; Fleischer using by images noise-hidden and diffused recover to - recov Optimal instability. seed to nonlinearity spatial ery depends on signal content, scattering statistics, strength. coupling nonlinear and FME7 • 3:15 p.m. DetectedRaman by Osteoporosis Induced Steroid Spectroscopy, of Rochester, USA, Rochester, of George , Andrea Markelz; SUNY Buffalo, USA. FME6 • 3:00 p.m. The Peptide Dynamical Transition, ing ing terahertz spectroscopy we show that “protein requirement. size critical a has transition” dynamical have transition and down Poly-Alanine Poly-Lysine dynamics the suggesting below, not but peptides, 5 to network. scale hydration a larger requires FME5 • 2:45 p.m. Seeded by Diffused Images Recovery of Nonlinear Instability, FME • Spectroscopy, Imaging and FME • Spectroscopy, Detection—Continued of Rochester, USA. Rochester, of been constructed to study the chemical perturbations perturbations chemical the study to constructed been to cortical bone associated with steroid bone induced of measurements Transcutaneous osteoporosis. also discussed. are Hani A. Awad A. Hani Monday, October 25 42 Sun Cloutier Monolithic Ge-on-Si lasers, lasers, Ge-on-Si Monolithic nm at room temperature. room at nm exhibit that doing, n-type and strain tensile byband-engineered lasers, USA. College, sic Kimerling FMH1 •4:00p.m. Jifeng Liu; MIT, USA,Presider FMH •SiliconPhotonics 4:00 p.m.–6:00p.m. Molecular Beam Epitaxy, Beam Molecular by Grown Silicon on Islands Germanium-Rich of Characterization Optical and Structural FMH2 •4:30p.m. of strain and doping. optical-communication frequencies due to the effects at light-emission their in improvement the and islands grown on Silicon by Molecular Beam Epitaxy Germanium-rich of properties photo-emissive and Biotechnology Inst., USA. feasibility pumping. of electrical the verifies devices heterojunction from nescence 1 , M. Coppinger M. , 1 , Rodolfo Camacho-AguilRodolfo , 1,2 1 , Jurgen MichelJurgen , ; 1 Univ. of Delaware, USA, Delaware, Univ.of WedemonstrateGe-on-Simonolithic Highland A 1 direct , F. GerleinF. , FiO gap emission around 1600 aroundemission gap We report on the structural 1 Invited ; 1 Direct MIT, USA, MIT, . Nataraj L. Jifeng Liu Jifeng 1 , J. Kolodzey J. , 1 Yn Cai Yan , gap electrolumi- gap 1 1,2 , N. Suster N. , 2 Dartmouth Dartmouth 2 , Xiaochen , Delaware Delaware 1 , Lionel Lionel , 1 , S. G. S. - on UndergraduateResearch II ScienceSymposium LSMC •Laser 4:30 p.m.–6:30p.m. Highland B LS FiO/LS 2010 in aconfocal imaging system using afiber. pressed by more than 20 dB over 5 mm depth of focus generatedareaxiconsup byanfunction - Bessel a of Rochester,USA. Kye-SungSophie, Lee Vo, Jannick P. Rolland; Univ. of Optical Coherence Microscopy Using Bessel Beam, USA, Presider Jannick P. Rolland; Inst. of Optics, Communications andSensingII FMI •StructuredWavefields for 4:00 p.m.–6:00p.m. elastic wave. longitudinalstanding a by acousto-opticdiffraction lithium niobate crystal under the collinear anisotropic results perimental of light a in modulation observed TechnicalFederation.Univ.,Russian YulaevAlexander Type,Nonresonance and Resonance of Filters Acousto-Optic Collinear in Modulation Light FMI2 •4:30p.m. FMI1 •4:00p.m. We demonstrate that the side lobes lobes side the Wethatdemonstrate • Highland C , Yuri Zyuryukin; Saratov StateSaratov Zyuryukin;Yuri , October 24–28,2010 Invited We report ex- report We cells and tissues. imagingfor tools proteinnew andmicroarrays,and ties may be used as new detection platforms for DNA density.capabilicurrentchargeandimaging - These of surface plasmon resonance (SPR) on surface local dependence sensitive the on based are techniques imaging new the of principles The developed. are optically current electrochemical and impedance measuring refractive index changes of 10 of changes index refractive measuring attenuationandinteraction oflength capableandof form are presented. This configuration is independent results for the compact silicon diffractive sensor plat- Tech, USA. GeorgiaGaylord; K. Thomas Maikisch, JonathanS. Performance, Sensor Diffractive Silicon Compact FMJ2 •4:15p.m. State Univ.,USA. State Resonance, Plasmon Surface on Base Techniques Sensing and Imaging New configuration. MZI unbalanced an in used been have PCWs tion, detec- of ease For regime. light slow their in PCWs operating by achieved is sensitivity high A sensor. index refractive based PCW compact a present Tech,USA. Yegnanarayanan,Georgia Adibi; Ali Sensor, Index Refractive Based Waveguide Crystal Photonic FMJ1 •4:00p.m. spectral measurement.spectral Presider to Announced Be FMJ •PhotonicSensorII 4:00 p.m.–6:00p.m. FMJ3 •4:30p.m. Simulation, fabrication, and experimental Murtaza Askari Murtaza Highland D

Methods to image local surface local image to Methods FiO Invited ; ArizonaTao J.; N. , Sivasubramaniam Sivasubramaniam , -8 without without We We FMK2 •4:30p.m. been developed. been ophthalmoscopy,has autofluorescenceimaging and scanning laser tomography,confocal coherence cal ophthalmoscopy,opti photoacoustic of merits the A multimodal retinal imaging system that combines Multimodal Retinal Imaging, Retinal Multimodal retinal circuits during development. of assembly the study to imaging multiphoton and confocal with structures neuronal subcellular of ers ongoing studies that combine novel fluorescent mark- Washington Univ. in St. Louis, USA. Retina, Mammalian the in Circuits Neural of Development the Imaging Wei FMK1 •4:00p.m. of Wisconsin, USA, Wisconsin, USA,Presider Jungtae Rha; Medical College of Techniques forRetinal Imaging FMK •EmerginginvivoImaging 4:00 p.m.–5:30p.m. Burke kee, USA, 1 , Tan Liu 3 , Shuliang Jiao 2 Northwestern Univ., USA, 1 , Jing Wang Highland E 4 Univ. of Southern California, USA. 4 ; 1 Univ. of Wisconsin at Milwau- 1 Invited Invited , Dennis P. Han Daniel KerschensteinerDaniel Hao Zhang Hao I will describe two 3 Medical College 3 , Janice M. 1,2 , Qing , - ;

Monday, October 25 43 , ; - 2 2 A CW transition , Chenchen Chenchen , 1 3 +ν 1 ν , Fetah Benabid Fetah , 1 , Natalie Wheeler 1 , Kevin Knabe 1 Univ. of UK. Bath, Univ. 2 Invited Invited LS , Jinkang Lim 1 Highland K Highland , Brian R. Washburn R. Brian , 2 inside large-core kagome fiber using FM Kristan L. Corwin L. Kristan 2 Markus Markus B. ;Raschke Univ. of Washington, H , Shun Wu 2 1 The The symmetry of second-harmonic sensitivity C 12 Kansas State Univ., USA, Univ., State Kansas LMB2 • 4:30 p.m. spectroscopy spectroscopy techniques and characterized with a explored. are widths line Improved comb. frequency fiber laser is stabilized to the P(13) 1 4:00 p.m.–5:30 p.m. 4:00 p.m.–5:30 Imaging, LMB • Novel in and Manipulation Spectroscopy I Microstructures USA, Univ., Cornell Wise; Frank Presider Wang LMB1 • 4:00 p.m. François Couny François of 10 kHz 10 AccuracykHz Spectroscopy in Acetylene-filled Hollow-Core Kagome Fiber and Improved Lin ewidths, Linear and Nonlinear Optical Nano-Crystallog- raphy, USA. generation and k-vector selectivity of phonon Ra- man scattering in combination with tip-enhanced resolved nanometer for allows microscopy near-field for demonstrated as order domain ferroic of imaging selected multiferroics. ferroelectrics and In the the In

; NASA Goddard NASA ; Invited Invited This presentation will give an an willgive presentation This James B. Abshire B. James Highland J Highland JOINT FiO/LS JOINT ; Harvard Univ., USA. Univ., Harvard Capasso; Federico short space of fifteen-years since their first invention invention first their since fifteen-years of space short useful most the become have lasers cascade quantum mid-infrared sources of tunable laser The radiation. applications ranging wide the and science underlying will be discussed. SMB1 • 4:00 p.m. 4:00 p.m.–6:00 p.m. 4:00 p.m.–6:00 Environmental SMB • IPF- of LasersApplications Lucent Kogelnik; Herwig USA, Presider Technologies, SMB2 • 4:30 p.m. The Physics and Technology of Quantum Cascade Quantum of Technology and Physics The Lasers, NASA’s Space Lidar NASA’s Measurements of Earth and Surfaces, Planetary Space Flight Ctr., USA. Ctr., Flight Space using for plans and work, ongoing history, of overview planetary surfaces. of measurements for space lidar , , , - - 4 1 1,4 We Natl. Natl. Univ. Univ. 3 1 ; , Xiaowei Xiaowei , , Frédéric , Frédéric 1 1,2,3,4 2,4 Alexander Alexander , Julia Mikhailo Julia , JST, Japan, Japan, JST, 1,3 2 Thales Optronique Optronique Thales 3 Inst. Inst. de la Lumière Max-Planck-Inst. für Max-Planck-Inst. , Daniel Herrmann Daniel , 2 1 1 ; 1 Osaka Univ., Osaka Japan. Univ., Aurelie Jullien Aurelie 4 A 80µJ, 5fs, CEP-stable Lab d’Optique Appliquée, Lab d’Optique Appliquée, We present the successful present We 1 Ludwig-Maximilians-Univ. Ludwig-Maximilians-Univ. , Jean-Philippe Rousseau 2 ; , Alain Pellegrina , Alain , Lourdes Patricia Ramirez 4 1 1,3 October 24–28, 2010 2,4 LS für - und Photonik Optoelek 3 , Raphael Tautz Raphael , 1 , Takayoshi Kobayashi , Takayoshi 1,2 • Highland H Highland , Laszlo Veisz Lab Lab Charles Fabry de d’Optique, l’Inst. 1,2 4 , Chris M. S. Sears S. M. Chris , 1 Jun Liu Jun , Patrick Georges , Aurélien Ricci , Karl Schmid 4 1,2 1,2 LS für BioMolekulare Optik, Ludwig-Maximilians- Optik, BioMolekulare für LS 4 , Xun Gu Xun , 1 FMN1 • 4:00 p.m. High-Fidelity Injector for High-Intensity High- Lasers, Few-Cycle Contrast S.A., France, S.A., France, 4:00 p.m.–6:00 p.m. 4:00 p.m.–6:00 in High Energy FMN • Advances Ultrafast Laser Systems USA, State, Penn Jovanovic; Igor Presider École LeBlanc; Catherine Presider France, Polytechnique, FMN3 • 4:30 p.m. Femtosecond of Contrast Improvement Temporal Bulk Kerr a in Self-DiffractionProcess a Pulsesby Medium, Druon München, Germany, Germany, München, Univ. Paris-Sud, Univ. France. (0.3rad RMS) injector with high spectro-temporal - The basedsystem, is quality compres on presented. sion in a hollow-core fiber followed by XPW filter ing, is an ideal seed for high-power high-contrast systems. OPCPA Germany. München, Univ. implementation of cross-polarized wave generation Wave Light system, laser Terawatt few-cycle our into Synthesizer - 20 leading to a contrast improvement magnitude. of orders four than more by of Electro-Communications, Japan, Japan, Electro-Communications, of Chiao Tung Univ., Taiwan, Taiwan, Chiao Univ., Tung Rodrigo Rodrigo Lopez-Martens Dimitris Papadopoulos Krausz Ferenc Quantenoptik, Germany, Germany, Quantenoptik, improved improved the temporal contrast of a femtosecond pulse to the value higher than the cubic of that its incident pulse in of a 0.5-mm-thick glass The plate. efficiency 12%. energy transform about is tronik, Ludwig-Maximilians-Univ. München, Germa - München, Ludwig-Maximilians-Univ. tronik, ny, Chen France, Paris-Sud, Univ. Extrême, École Polytechnique, École France, Polytechnique, va FMN2 • 4:15 p.m. Pulse Cleaning of Few-Cycle PulsesOPCPA by Cross-Polarized Generation, Wave Buck - FiO/LS 2010 , Hye Hye , 2 , C. A. C. , 2 N00N state Toshiba Res. Toshiba 1 ; 1 , I. Farrer I. , 1,2 Univ. of Rochester, of Rochester, Univ. 1 ; 1 Invited , R. B. Patel R., B. , Kam Wai Clifford Chan Clifford Wai Kam , 1 FiO 1 , Andrew Shields , Andrew 2 Cavendish Cavendish Lab, Cambridge Univ., 2 Highland G Highland , Robert Boyd W. 1,3 A. J. Bennett J. A. We We demonstrate experimentally quantum Heedeuk Shin Heedeuk Rochester Optical Manufacturing Co., USA,

, D. A. Ritchie 2 2 We report a device in which the emission energy emission the which in device a report We Korean Intellectual Korean Property Intellectual Office, Republic of UK. of single quantum dots can be Starkshifted 25meV. tune We transitions in remote quantum dots to the same energy and observe twophoton interference their emission. with Europe Europe Ltd., UK, Jeong Jeong Chang FMM2 • 4:30 p.m. Spatial Quantum of ExperimentalDemonstration Superresolution by Optical Centroid Measure ments, ments, 3 4:00 p.m.–6:00 p.m. 4:00 p.m.–6:00 Information and FMM • Quantum II Communications Be Announced to Presider Nicoll FMM1 • 4:00 p.m. by measuring the centroid positions of the entangled entangled the of positions centroid the measuring by photons. The optical centroid measurement shows higher detection efficiency than the conventional absorption. based multiphoton scheme on Korea. with two-photon spatial superresolution USA, Interference Interference of Photons from Remote Solid-State Sources,

- Liang , Noah Tomasz 1 , 2 - techni report We Vanderbilt Univ., USA. Univ., Vanderbilt 2 , Robert T. Kester Invited 2 , David Piston W. 1 Highland F Highland Rice Univ., USA, Univ., Rice 1 ; 1 , Nathan Hagen 1 , Amicia D. Elliott 1 Bedard - hy is a non-scanning Spectrometer Mapping Image complete a providing perspectraltechnique imaging spectral-spatial information IMS simultaneously. acquires, analyzes and displays data at 5-10 frame/ sec rates. Imaging results for cells expressing GFP/ presented. YFP/CFP are FML1 • 4:00 p.m. 4:00 p.m.–5:30 p.m. 4:00 p.m.–5:30 I FML • Microscopy Univ., Cornell Nishimura; Nozomi USA, Presider tiplexing tiplexing and Extended Excitation Bandwidth, Spiecker; Heinrich Andresen, Thomas , Pingel Volker Germany. GmbH, BioTec LaVision excitation rate, frame increase that improvements cal bandwidth and penetration depth of 2-photon mi- a flat croscopes novel significantly by implementing - Para Optical an integrating and splitter beam optics microscope. the 2-photon into metric Oscillator Improving Improving 2-Photon Microscopy by Beam Mul S. Tkaczyk S. FML2 • 4:30 p.m. Time Real for (IMS) Spectrometer Mapping Image Hyperspectral Fluorescence Microscopy, Gao Monday, October 25 44 of 25dB. ratio extinction and microseconds, 141 of time rise microwatts, 540 of power switching a in result nm demonstrated.Measurementsis 1550 waveguidesat switchusing free-standing silicon-on-insulator strip thermo-opticinterferometer Mach-Zehnder A PengSun, Switches, Thermo-Optic Submilliwatt for guides WaveStrip - Silicon-on-Insulator Free-Standing FMH3 •4:45p.m. Continued FMH •SiliconPhotonics— pump signal a of configuration coupling side using absorption carriers free linear on based waveguide silicon optical broadband modulation of light in submicron Israel.Jerusalem, of Goykhman Waveguide, Silicon Submicron In lation Modu- Broadband Amplitude-based All-optical FMH5 •5:15p.m. introducedcally fabrication inthe process. small area, avoiding write-field stitching errors, typi - long Bragg gratings to fabricatedbe on an extremely Bragggratings on an SOI chip. approach Our allows at San Diego, USA. ziar P. Nezhad, Yeshaiahu Fainman; Univ. of California Zamek Curved Waveguide Bragg Gratings on a Chip, FMH4 •5:00p.m. ______, Dawn T. H. Tan, Mercedeh Khajavikhan, Ma- Ronald M. ReanoOhioStateRonaldM. ; Univ., USA. , Boris Desiatov, Uriel Hebrew Levy; Univ. Highland A We demonstrate curved waveguide Weall- on-chipdemonstrate an FiO Steve Steve Ilya Continued on UndergraduateResearch II— ScienceSymposium LSMC •Laser Highland B LS FiO/LS 2010 distribution as function its conditions. initial Wigner the use to method Hamiltonianray-tracing through ray-tracing. We accomplish this by adapting simply medium inhomogeneous an in phenomena optics wave simulating for method novel a present for Res. and Technology (SMART) Ctr., Singapore. Continued Communications andSensingII— FMI •StructuredWavefields for Barbastathis fit experimental datafit experimental well. theoretically and experimentally in detail. Simulations The phase matching condition was characterized both electromagnetically induced via transparency effect. generated in a solid based on stored atomic coherence Univ.,China.Nankai Zhai ohui Solids, in WaveAtomic Coherence on Based Conjugation Phase of Generation Phase-Matched FMI3 •4:45p.m. geneous Media, geneous Inhomo - in WavePropagation for Function tion Distribu- Wigner with Ray-TracingHamiltonian FMI5 •5:15p.m. interference.destructive by suppressed is component carrier The doubling. ated from a modulated light at 1550 nm by frequency gener is nm 775 ofwavelength a at photonicsignal and Technology, Japan. Noda, Takashi Tokuda, Jun Ohta; Nara Inst. of Science Frequency Doubling, on Based Generation Signal Photonic W-Band FMI4 •5:00p.m. , GuoquanJingjunYilingZhang,Xu;Dou,, 1,2 ; 1 MIT,USA, • Highland C Hanhong Gao Hanhong NOTES Kiyotaka Sasagawa Kiyotaka A two-tone W-band (96 GHz) Phase conjugation wave was wave conjugation Phase October 24–28,2010 2 Singapore-MITAlliance 1 , Lei Tian Lei , , Toshihiko 1 , George , Zha We We - - m*Hz minimum detectable electric-field strength of 17μV/ a with structure electro-optic GaAs enhanced tor transparentconduc- a andantennaT-shaped micro a by enabled detector electric-field ultra-sensitive Ho; Northwestern Univ.,Seng-Tiong USA. Huang, Yingyan Liu, Boyang Ou, Fang Structure, (EO) Electro-optic Enhanced (TC)Transparent Conductorand Antenna Micro by Enabled Detector Electric-field Ultra-sensitive FMJ5 •5:15p.m. ticle detection. interactionsandimprove sensitivityofnanopar the light-matterenhance can gainWe optical thatshow threshold.lasing the aboveand below pumped cally demonstrated in active microcavities which are opti- USA. Louis, St demir,JiangangYang; Lan Zhu, Washington Univ. in Microcavities, Optical Active in Coupling Modal Mediated Scatterer FMJ4 •5:00p.m. Continued FMJ •PhotonicSensorII— -1/2 and response frequency above 1GHz. Scattering induced mode splitting is splitting mode induced Scattering Highland D FiO Lina He Lina We propose a compact , Şahin Kaya Öz- Kaya Şahin , e Yi Fei - , of eliminating stray reflections. interferometry (LCI) set-up is demonstrated capable coherence low A gating. coherence using by sensor depth range of a physical Shack - Hartmann wavefront UK. sor, sor, Coherence-gated Shack-Hartmann Wavefront - Sen FMK4 •5:15p.m. dry eyeor cataract. dry the ocular fundus. The increase is not associated with increase with aging in scattered light returning from rimetry technique using near infrared light reveals an IndianaUniv., USA. P. Haggerty; VanNasdale,Bryan A. Papay,Dean A. teriorSegment, An- the with Associated not Aging with Changes and Infrared Near the in Light Scattered Fundus FMK3 •5:00p.m. Continued Techniques forRetinal Imaging— FMK •EmerginginvivoImaging Simon Tuohy, Simon We investigate the possibility of narrowing the the narrowing of possibility We the investigate AnnTomothy, Elsner E. Hobbs, Joel Highland E AdrianPodoleanu;Univ. Kent,of - pola laser scanning confocal A Monday, October 25 45 , , 2 2 Univ. Univ. 2 , Jonathan Ward 1,2 We present thepresent first We Luiz Gustavo Cançado Gustavo Luiz In In our work we aim to , 1 Univ. Univ. College Cork, Ireland, LS 1 , Mark Daly ; 1,2 1,2 Univ. of Univ. USA, Rochester, 1 Highland K Highland ; 1 RyanBeams Mary Frawley Tyndall Tyndall Natl. Inst., Ireland. LMB • Novel Imaging, LMB • Novel in and Manipulation Spectroscopy I—Continued Microstructures Federal de Gerais, Brazil. Minas Federal optical measurement of the phase-breaking length in graphene extracted from the Raman scattering originating at an edge in the lattice. The results are electrical to measurements. compared investigate the trapping and moving of microspheres microspheres of moving and trapping the investigate the investigate will We nanofiber. optical an along on generation of standing waves within the fiber and mode interference. higher order exploit 2 LMB3 • 5:00 p.m. Optical and Trapping Manipulation of Micron- Sized Particles Using a Bright Tapered Optical Fiber, Lukas Lukas Novotny Sile Sile Nic Chormaic LMB4 • 5:15 p.m. Length Phase-Breaking the of Measurement Optical Graphene, in Advances Advances in Charles Charles E. , Kolb Invited Highland J Highland JOINT FiO/LS JOINT SMB • IPF- Environmental Environmental SMB • IPF- of Lasers—ContinuedApplications SMB3 • 5:00 p.m. Tunable Infrared Laser Measurements of Industrial Industrial of Measurements Laser Infrared Tunable Process and Herndon, Product C. Emissions, Scott McManus, Barry J. Nelson, D. David S. Mark Zahniser; Res., Aerodyne USA. - process signal and detectors lasers, infrared tunable - emit pollutants of quantification real-time allow ing ted during the distribution and manufacture, use of of deployment and Development products. industrial will be sensors described. pollutant advanced robust , 1 - Christo , 1 , Miroslav Y. 1 Photon Science Science Photon 1 , John K. Crane K. John , ; 1 2 , Craig W. Siders W. Craig , Invited 1 October 24–28, 2010 NOTES , Jay W. Dawson W. Jay , 1 Lawrence Lawrence Berkeley Natl. Lab, USA. , Constantin Haefner • Highland H Highland 2 1 , Matthew A. Prantil A. Matthew , 1 , Henry H. Phan H. Henry , 1 FMN • Advances in High Energy in High Energy FMN • Advances Ultrafast Laser Systems— Continued and Applications and Program, Applications Lawrence Livermore Natl. Lab, USA, FMN5 • 5:00 p.m. Energetic short-pulse fiber lasers feed or drive many many drive or feed fiberlasers short-pulse Energetic at applications LLNL, including petawatt lasers and present sources. We gamma-ray Compton-scattered the to fiberscalinglasers in advances and challenges range. millijoule pher P. J. Barty J. P. pher FMN4 • 4:45 p.m. FMN4 • 4:45 Withdrawn David David J. Gibson Shverdin Advances Advances in Energetic Short-Pulse Fiber Lasers, Messerly J. Michael ; 1 We FiO/LS 2010 Univ. Univ. order order 3 nd , Claudio G. 1 - compari SNR , Giovanni Di

1 , Malvin C. Teich 1,3 We show We We We present designs of Boeing Res. & Technology, Technology, & Res. Boeing 1 ; 2 Justin Justin ,Dressel Andrew N. FiO Univ. of Camerino, Italy, of Italy, Camerino, Univ. 2 Barbara Barbara A. Capron Highland G Highland Mohammed Mohammed F. Saleh , Bahaa E. A. Saleh , Jeff C. Adams C. Jeff , order ghost images from PDC and 2 and PDC from images ghost order 1 2,3 th SpectraNet, Inc., USA. Inc., SpectraNet, 2 Boston Univ., USA, Boston Univ., FMM • Quantum Information and Information and FMM • Quantum II—Continued Communications FMM4 • 5:00 p.m. Experimental Comparison of the Signal to Noise Ratio (SNR) of Ghost Images for Entangled and Thermal Light, thermal images from single beams. Ghost imaging yields low background and shows improvement of SNR. thermal light over light the entangled FMM5 • 5:15 p.m. Leggett-garg Non-local a of Violation Experimental Inequality Using Non-local Weak Measurements, Curtis J. Broadbent, USA. of C. John Rochester, Jordan, Univ. Howell; experimentally demonstrate the violation of a non- local Leggett-Garg inequality using non-local weak biphotons. entangled polarization on measurements Due to measurement degeneracy, multiple strange weak values are required to infer violation of the inequality. Leggett-Garg 1 Giuseppe Parazzoli sons of 4 of of Central Florida, USA. and separation, the generation, for circuits photonic manipulation of modal, polarization, and spectral photonic qubits generated in two-mode diffused- channel Ti:LiNbO3 waveguides via spontaneous downconversion. parametric USA, FMM3 • 4:45 p.m. FMM3 • 4:45 Photonic Circuits - for Pro Quantum Information Diffused-Channel Integrated Two-Mode in cessing Waveguides, , - This This By By switching Roman SchmidtRoman We We demonstrate , , Ilaria Chris Testa, Highland F Highland Andreas Andreas Schönle Jason Jason M. , Kellicker Gregory J. Kowalski, ______tian Eggeling, Stefan for Biophysical W. Chemistry, Germany. Hell; Max-Planck-Inst. FML4 • 5:00 p.m. Single Emitter Switching Based Multicolor Nanoscopy, we can states dark long-lived into dyes conventional record their fluorescence time-sequentially even if they are closely packed. This allows for - with simultane species dye four to up of imaging nanoscale ous minimal cross-talk. FML3 • 4:45 p.m. Nanoscopy, Optical 3-D - isoSTED FML • Microscopy I—Continued FML • Microscopy research, research, through a rigorous optical, thermal and mechanical computational analysis, demonstrates from light tag to Microscopy Photothermal of use the of depth and contrast improve thereby and focus, the scatter. out-of-plane by limited imaging FML5 • 5:15 p.m. Microscopy Photothermal of Model Computational in Tissue, USA. Univ., A. Charles Northeastern DiMarzio; Alexander Egner, Stefan W. Hell; Max-Planck-Inst. for for Max-Planck-Inst. Hell; W. Stefan Egner, Alexander Biophysical Chemistry, Germany. the unique, non-invasive isoSTED imaging of sub-wavelength sized biological and manufactured nanostructures and report on recent advances in the field. Monday, October 25 46 of ~400ps. in submicron waveguides lifetime with carrier afree pulses. Enhanced nonlinear coefficients are reported ultra-short of transmission the through waveguides hydrogenated-amorphoussilicon in nonlinearities nology, USA. Narayanan Waveguides,Silicon Amorphous genated Hydro- in Nonlinearities Based Carrier and Kerr FMH7 •5:45p.m. confinement of optical the mode. submicron shows measurements field Near profile. its controlling for guidelines provide and silicon of silicon waveguidescale fabricated oxidation by local tion and experimental characterization of submicron- Jerusalem, Israel. Desiatov Process, Locos Optimized ViaWaveguide Realization Of Submicron-scale Square-like Silicon FMH6 •5:30p.m. Continued FMH •SiliconPhotonics— ______, Ilya Goykhman, Uriel Levy; Hebrew Univ. of , StefanF., Preble;TechRochesterInst. of - We experimentally measure the optical We demonstrate the design, fabrica- Highland A FiO Karthik Karthik Boris Boris 6:30 p.m.–8:30p.m. Continued on UndergraduateResearch II— ScienceSymposium LSMC •Laser Highland B LS OSA StudentMemberReception, Temple Bar &Grille, 109East Avenue, Rochester, NY, Phone: 585.232.6000 FiO/LS 2010 light that fields exhibit parabolic trajectories. Airy and modes light Bessel using studies includes This fields. light ‘non-diffracting’ of biophotonics propagation and applications in optical trapping and UK. Andrews, St. Univ.of Mazilu; MichaelGunn-Moore,Tsampoula,XanthiFrank Dholakia Kishan Advanced Studies of ‘Non-Diffracting’ Light Fields, FMI6 •5:30p.m. Continued Communications andSensingII— FMI •StructuredWavefields for • Highland C , Jörg Baumgartl, Tomas Cizmar, Tomas Baumgartl, Jörg , NOTES October 24–28,2010 Invited We explore the exploreWe refractive index at vicinity the of resonator. the droplets on-chip, enabling the control of micro- the effective driving allows system Our Microfluidics. micro-resonatornitride conceptusing the of Digital Israel. Goykhman, Boris Desiatov, Uriel Hebrew Levy; Univ., Platform, Microfluidics Digital on Based ResonatorTunable Micro-ring On-chip FMJ7 •5:45p.m. an optofluidic chip. in molecules DNA 8-9 to down detection of limit a enablesamplification lock-in numerical or physical ferent sizes, integrated-waveguide laser excitation and dif- 17 of DNA molecules dye-labeled of separation Netherlands.Twente, Univ.of W.M.Hoekstra,J. Hugo Dongre, DNA Molecules in An Optofluidic Chip, Electrophoretic Separation and Detection of a Few FMJ6 •5:30p.m. Continued FMJ •PhotonicSensorII—

We demonstrate the tunability of a silicon a of tunability the demonstrateWe Highland D FiO After electrophoretic After Markus Pollnau; Markus YoavZuta Chaitanya Chaitanya , Ilya Ilya , Highland E Monday, October 25 47 LS Highland K Highland

; ; Ball Aerospace, USA. Invited Highland J Highland Carl Weimer JOINT FiO/LS JOINT SMB • IPF- Environmental Environmental SMB • IPF- of Lasers—ContinuedApplications SMB4 • 5:30 p.m. SMB4 • 5:30 Laser Remote Sensing of and theBeyond, Earth: CALIPSO The CALIPSO satellite has been characterizing aerosols using and atmosphere clouds in the Earth’s include will missions Future lidar. wavelength dual a lidars for measuring the forests’ role Earth’s in the cycle. carbon ; Lab for Laser Diffraction- grat Invited October 24–28, 2010 NOTES • Highland H Highland Terrance Terrance J. Kessler FMN • Advances in High Energy in High Energy FMN • Advances Ultrafast Laser Systems— Continued FMN6 • 5:30 p.m. FMN6 • 5:30 Grating Grating Development for High-Peak-Power CPA Laser Systems, Energetics, Univ. of Rochester, USA. of Rochester, Univ. Energetics, ings have competing performance requirements when used in high-peak-power CPA laser systems. Diffraction efficiency, wavefront quality, and laser damage threshold are interdependent criteria for MLD gratings. Critical fabrication related artifacts will be discussed.

, - 1 We FiO/LS 2010 , Michael Michael , 2 Martin P. Martin van P. Exter, , Tijmen Euser Tijmen , Temple Bar & Grille, 109 East Avenue, Rochester, NY, Phone: 585.232.6000 Phone: NY, Rochester, Avenue, 109 East & Grille, Bar Temple OSA Student Member Reception, 1 Univ. Leiden, Netherlands, Netherlands, Leiden, Univ. 1 J. P. J. (Han) P. Woerdman ; 2 FiO , Eric Eliel Eric , 1 Highland G Highland , Philip St Russell 2 Germany. Light, of Science the for Inst. Planck Max Scharrer FMM7 • 5:45 p.m. Measuring and Modifying the Spiral Spectrum of Entangled Photon Pairs, Netherlands. Univ., Leiden Pires; Lorenzo Di Henrique - distribu probability complete the measured have We are that modes momentum angular orbital the of tion generated in parametric spontaneous down conver show how sion. on-purpose We phase mismatching modal the flattens and bandwidth spiral the increases distribution. FMM • Quantum Information and Information and FMM • Quantum II—Continued Communications FMM6 • 5:30 p.m. Transport of OAM-based QuNits through Few- Mode Optical Fibers, 2 Wolfgang Loeffler Wolfgang report how entangled photons carryingsuperposi a - photons entangled how report eigenstates (OAM) momentum angular orbital of tion few- a through transported when de-coherence suffer Kagome hollow-core that find We fiber. optical mode the de-coherence. least far by fibers show 6:30 p.m.–8:30 p.m. Highland F Highland ______Tuesday, October 26 48 jecting through next the decade. jecting proand- todaynetworks of models using examined is networks communication data of consumption energy the to systems transmission optical of tion Bell Labs, Alcatel-Lucent, USA. Internet, Optical Transmission ConsumptionEnergy in the and sustainability.efficiency technological areas that are expected to impact energy two lighting, solid-state for devices light-emitting photovoltaic devices for power generationorganic and in organic advances recent of overview an provide Kippelen Bernard Promise, and Status Devices: Light-Emitting and Photovoltaic for Semiconductors Organic FTuA1 •8:00a.m. FTuA1 Netherlands, Presider Markus Pollnau; Univ. of Twente, FTuA •PhotonicsandEnergyII FTuA 8:00 a.m.–10:00a.m. FTuA2 •8:30a.m. FTuA2 DanKilper W.G. , Atkinson, Korotky;K. S. Highland A ; Georgia Tech, USA. Invited Invited The relative contribu- This talk will Thiswill talk P. Chui Animals, Small and Humans in Compensation Optics Adaptivefor Device Imaging Multifunctional Burns Limitations, and Issues Uses:World Real for Systems Imaging Retinal AO Designing Mircea Mujat Mircea FTuB2 •8:30a.m. FTuB2 •8:00a.m. FTuB1 limited number of subjects. performancea characterizedin was animals.Device small and humans both from images tomography scanning laser ophthalmoscopy and optical coherence ously acquire high resolution adaptive opticscorrected USA. School, Health, USA,Presider Rongguang (Ron) Liang; Carestream •AdaptiveOpticsfortheEye FTuB 8:00 a.m.–10:00a.m. Inc., USA, Inc., developed. have we systems scanning AO three contrast and compare and patients, clinical with use research systems considering when arise that issues the of for different purposes. In this talk I will present some turity that allows development of systems specialized ma- of level a reach to starting are systems imaging ; IndianaUniv.,; USA. 2 , J. D. Akula Daniel X. Hammer X. Daniel 2 Children’sHospitalHarvardMedicaland 1 A system was developed to simultaneto- developed was system A , Ankit H. Patel Highland B 2 , A. B. Fulton 7:00 a.m.–5:30p.m. Invited Invited Adaptive Optics retinal Optics Adaptive 1 1 , Nicusor Iftimia 10:00 a.m.–4:00p.m. , R. DanielFerguson R. , 2 ; 1 Physical Sciences Stephen A. Stephen 1 , T. Y. FiO/LS 2010 1 , Moss enza” Univ., Italy, Bahram Jalali Bahram Amplifiers, Raman Silicon in Developments Recent Fluctuations;Value Extreme and tering, - Scat Stimulated Inverse Gain, Broadband Noise, YongwooPark Fathpour 2 4 2 USA, Presider Yoshitomo Okawachi; Cornell Univ., Optics •NonlinearIntegrated FTuC 8:00 a.m.–10:00a.m. and extreme value fluctuations. phenomenon, scattering Raman inverse gain, band the achievable noise figure and gain, creating broad- laboratory Raman amplification in silicon, including USA. compatible nonlinear high-Q ring resonator. on four-wave based anmixingintegratedin CMOS- ultrahigh repetition rate, passively mode-locked laser subpicosecond, a presentWe Australia.Physics, of FTuC1 •8:00a.m. FTuC1 ing Resonatoring , Based on A C-MOS Compatible Integrated Micror Laser Soliton Speed High Ultra Subpicosecond •8:30a.m. FTuC2 Inst. for Chemical and Physical Processes, CNR, “Sapi- CREOL, College of Optics, Univ. of Central Florida, CentralUniv. ofOptics, of College CREOL, TannerUSA, Inc.,Res. Registration, Galleria, Rochester Riverside Convention Center 4 , This talk will review recent progress in our in progress recent review will talk This Roberto Morandotti Roberto 4 Exhibit Open,Rochester Riverside Convention Center ; 1 Univ. of California at Los Angeles, USA, Angeles, Los at CaliforniaUniv. of 1 1 , Brent E. Little E. Brent , , D., Solli Marco Peccianti Marco • Highland C 3 Infinera Ltd, USA, FiO October 24–28,2010 2 3 , P., Koonath Booz-Allen-Hamilton,USA, Invited 1 ; 3 1 , Sai T.Chu Sai , INRS-EMT, Canada, INRS-EMT, 1,2 , Alessia, Pasquazi 4 2 CUDOS, CUDOS, School , D., Borlaug 3 , Dave J. Dave , 3 , S. , 1 - , Glasgow, UK,Presider Johannes K.Courtial; Univ. of Information Science •GeneralOpticsin FTuD 8:00 a.m.–9:45a.m. Xu, Hyperspectral THz Image , Reconstruction •8:15a.m. FTuD2 ily of diffusers. particulate agreement with experiments is obtained using a fam emphasis on the wavelength decorrelation. Excellent a thick diffuser, a hastheory been developed with an Inst. of Optics, Univ. of Rochester, USA. For speckle in Particles Small with Diffuser Thick a Propagationthrough •8:00a.m. FTuD1 Specific Spectroscopy Specific Experimental Demonstration of Adaptive Feature- •8:30a.m. FTuD3 reconstruction improved. can be the of quality the bands, spectral these across tion informa hyperspectral the using by that showWe independently. band spectral each at data the treat Many existing methods for terahertz image processing low SNR scenarios. in architecturestraditional than times classification time-to- dramatically-shorter achieves system The presented. is (AFSS) Spectroscopy Feature-Specific Adaptiveof validation Experimental USA. Arizona, Univ.of Gehm; E.V. Dinakarababu,Michaelbabu Edmund Edmund Y. Lam , Nienan Chang Nienan Highland D ; Univ. of Hong Kong, Hong Kong. Hong Kong, Hong of Univ. ; , , Nicholas George, Wanli Chi; , Dinesh , Rodriguez Ivan Zhimin Zhimin - - -

USA, Presider Richard D. Averitt; Boston Univ., Berkeley Natl. Lab, USA,Presider Robert A.Kaindl; Lawrence •GeneralOptics FTuE 8:00 a.m.–10:00a.m. in clarifying this relationship. this in clarifying roleimportant an ago,playsyears many introduced purity, cross-spectral of concept the that showWe discussed. is domains space-frequency and time space- in coherence optical of theories the between EmilWolf; Univ. Rochester,of relationshipThe USA. Domains, Space-Frequency the in Theory of Optical Coherence in the Space-Time and •8:00a.m. FTuE1 samples insingle-pulse CARSexperiments. limitNyquist the of <30% using spectra vibrational sparse resolve experimentally Wemeasurements. time-domain N than less muchusing spectrum rier an obtaining for approach sensing compressive- a describe WeIsrael. Science, of Inst. Katz Compressive Fourier Transform , Spectroscopy •8:30a.m. FTuE3 noise.data hiddeninthe that is otherwise that pulses are inherently sparse enables us to retrieve photodiode inherent resolution limit. The knowledge the exceeds significantlyresolution atthat struction recon - pulse-shape We experimentally demonstrate Technology,Israel.of Inst. Israel Technion - Cohen; Oren Segev,MordechaiEldar, Yonina C. Szameit, Sidorenko Implementing Sparseness-Based Algorithms, Photo-Detectors in Pulse-Shape Measurements by of Limit Resolution Inherent the Exceeding •8:15a.m. FTuE2 , Jonathan M. Levitt, Yaron Silberberg; Weizmann , Snir Gazit, YoavSchechtman,AlexanderGazit, Snir , Highland E MayukhLahiri , N -point Fou- -point Pavel Pavel Ori Ori

Tuesday, October 26 49 ,; ,; The

Daniel Gerd Leuchs Gerd Invited Invited LS Highland K Highland , Joel A. USA. Duke Greenberg; Univ., LTuB2 • 8:30 a.m. LTuB2 8:00 a.m.–10:00 a.m. • Nonlinear Optics I LTuB of Univ. G. White; Andrew Presider Australia, Queensland, LTuB1 • 8:00 a.m. LTuB1 Gauthier We observe spontaneous parametric oscilla- tion in a laser-driven cloud of cold The atoms. - dramati lowered is instability this for threshold that gratings atomic self-assembled to due cally wave atom-field of matching self-phase for allow processes. mixing Prospects for Strong Cavity Free Single Atom Level, Photon Few the at Nonlinearity for the Science Max-Planck-Inst. of and Light of Inst. Optics, Germany. Erlangen-Nuremberg, Univ. progress and prospect of non-linear photon-atom reviewed. is level photon a few at coupling Toward Single-Photon Toward Nonlinear Optics via Self-Assembled Ultracold Atoms, Abstract Abstract ; NIST, USA. NIST, ; Invited Invited Highland J Highland Scott Diddams Scott Control Control of laser parameters such as Joohan Joohan Lee , James Cordingley; GSI Laser JOINT FiO/LS JOINT Systems, Systems, USA. pulses multiple polarization, shape, pulse wavelength, and ultra-short pulses improves the laser cutting for used are that fuses pitch fine various of reliability redundancies. modern circuit Laser Fuse Processing for Advanced Memory Designs, Use of Lasers in Time and Frequency Applications Applications Frequency and Time Lasersin of Use Metrology), (or STuA1 • 8:00 a.m. STuA1 8:00 a.m.–10:00 a.m. • IPF-Laser Applications in STuA Metrology Griot, CVI Melles Nadorff; Georg USA, Presider STuA2 • 8:30 a.m. STuA2 not available. not - Emily This This talk ; Univ. ; of Univ. Opto-electronic Opto-electronic Marcus Marcus Jones Invited Invited October 24–28, 2010 LS ) excitonic state. ) excitonic 3/2 • Highland H Highland 1S e Rochester Riverside Convention Center Convention Riverside Rochester Exhibit Open, - Kath Morris-Cohen, J. Adam McArthur, A. Eric , Galleria, Rochester Riverside Convention Center Convention Riverside Rochester Galleria, Registration, LTuA2 • 8:30 a.m. LTuA2 LTuA1 • 8:00 a.m. LTuA1 8:00 a.m.–10:00 a.m. • Photophysics of LTuA II Nanostructured Materials Rochester, of Univ. Lewis Rothberg; USA, Presider Excitonic Excitonic Dynamics of Quantum Dots Monitored by Near-Infrared Transient Absorption, Weiss ryn E. USA. Knowles; Northwestern Univ., near-infrared of analysis regression global a describes (TA) absorptions transient nm) 1300 - nm 900 (NIR, photoexcited (QDs) dots CdSe colloidal of quantum their (1S first to Quantum Dot Electron Probed - by Transfer Tran sient Photoluminescence, North Carolina at Charlotte, USA. applications of nanocrystals rely on generation and exploitation of mobile charge carriers. Under standing nanocrystal electron transfer processes is therefore important. photoluminescence Transient this unravel to helping is that technique versatile a is field. complex , 1 FiO/LS 2010 , Raphael , 1 Oak Ridge Ridge Oak 1 ; 1,2 Warren Warren Grice 10:00 a.m.–4:00 p.m. 10:00 a.m.–4:00 , Travis Humble 1 7:00 a.m.–5:30 p.m. 7:00 a.m.–5:30 , Daniel F. V. James; Dept. , BrianWilliams, 1,2 Seyed Mohammad Hashemi Univ. of Univ. USA. Tennessee, Photon 2 Highland G Highland , Philip Evans Philip , 1 ,; Univ. ,; of Univ. USA. Rochester, By studying Asma Al-Qasimi , Jason Schaake Jason , 1 , of of Physics, of Canada. Univ. We Toronto, study the properties of a general quantum correlation known studied been recently has which discord, quantum as as a resource for quantum - computation. We inves tigate the relations between discord, entanglement entropy. and FTuG3 • 8:30 a.m. Strong Spectral Entanglement Parametric in, Down-Conversion Spontaneous pairs pairs with a high degree of spectral entanglement have a very large capacity for carrying information. We describe methods for generating this type of discuss applications. and entanglement 8:00 a.m.–10:00 a.m. FTuG • Quantum Information and Communications III USA, Tech, Georgia Voss; Paul Presider Pooser FTuG2 • 8:15 a.m. Quantum Discord, Quantum Entanglement, and Linear and Entropy, the Relationship Between Them Natl. Natl. Lab, USA, Rafsanjani the algebra of creation and annihilation operators, we obtain theoretical evidence that emphasizes the ``bosonic” how determining in entanglement of role (distinguishable fermions two of system composite a is. identical) or FTuG1 • 8:00 a.m. What Determines How Bosonic a Cooper Pair Is? , Entanglement Ryan BenninkRyan FiO ; Cornell , Warren Warren , Baolei Li . We use multiphoton use multiphoton . We Invited Nozomi Nishimura in vivo Highland F Highland Nonlinear Nonlinear optical interactions enable S. Warren, S. Martin C. Warren, Fischer; USA. Duke Univ., We demonstrate a homodyne coherent anti-Stokes Raman scattering technique based on femtosecond laser pulse shaping (phase-cycling). This technique utilizes a self-generated non-resonant background as a local oscillator to retrieve phase of information signal.the Raman FTuF2 • 8:30 a.m. Scattering Raman Anti-Stokes Coherent Enhancing Struc- Cycled Phase with Suppression Background PulsesLaser, Femtosecond tured 8:00 a.m.–10:00 a.m. FTuF • Microscopy II FTuF1 • 8:00 a.m. Adam Wax; Dept. of Biomedical Biomedical of Dept. Wax; Adam USA, Univ., Duke Engineering, Presider Nonlinear Optical Tools for Studying Small-Stroke Small-Stroke Studying for Tools Optical Nonlinear at Microscopic Scales, USA. Univ., observation and manipulation of biological tissues with resolution cellular microscopy and femtosecond laser ablation to study to study laser ablation femtosecond and microscopy health and function of brain cells after disruption microvessels. of Tuesday, October 26 50 Sustainability - Is This Green Photonics? Green This Is - Sustainability and Efficiency Energy for Optics and Photonics Lebby FTuA3 •9:00a.m. FTuA3 Continued •PhotonicsandEnergyII— FTuA ; OIDA, USA.Abstract not available. Highland A Invited Michael with footprints than asquare smaller foot. devices such of design the presenting by illustrated be will rules These instruments. optics adaptive reduceophthalmicastigmatism reflective off-axis in Rochester,USA. Díaz-Santana;Univ.Gómez-Vieyra,Y.LuisSulai, of Imaging, Retinal for struments In- Optics Adaptive Clinical of Design Optical FTuB3 •9:00a.m. FTuB3 Eye—Continued •AdaptiveOpticsforthe FTuB Simple design rules can be used to used be can rules design Simple Highland B Invited Alfredo Dubra Alfredo , A. , FiO/LS 2010 FTuC4 •9:00a.m. FTuC4 and Mid-IR Applications, Mid-IR and Nonlinear Mixing in Silicon Waveguides for SWIR Park Michal Lipson Michal Mark A. Foster of California at San Diego,USA, SanCalifornia atof K. W.K. Lau Nanowaveguides , Silicon in metric-mixing Para- Continuous-wave Broadband Mid-infrared •8:45a.m. FTuC3 potential for Mid-IR applications. great offering modulation complex and linewidth narrow combine can source silicon parametric widely-tunableThis sources.ultra-compacttelecom from derived signals using 2μm beyondwaveguides We present results on four-photon mixing in silicon- Photonics,andUniv.Optics USA. CentralFlorida,of 2 Divliansky Cornell Univ.,USA, Cornell conversion bandwidth of over 350nm. mixing in silicon nanowaveguides. We measure a 3-dB conversion to the mid-infrared region four-wavevia demonstrate broadband continuous-wave frequency Cornell for Nanoscale Science, Cornell Univ., We USA. plied and Engineering Physics, Cornell Univ., USA, USA, Univ., Cornell Physics, Engineering and plied Optics—Continued •NonlinearIntegrated FTuC School of Electrical and Computer Engineering, Engineering, Computer and Electrical of School 1 , S. Moro 1 2 , Michaël, Ménard , N. Alic 1 2,4 , J. M. Chavez-Boggio 1 , Amy C. Turner-Foster , Alexander L. Gaeta AlexanderL. , • Highland C 1 , S. Mookherjea 3 FiO PicoLuz, USA, PicoLuz, October 24–28,2010 Invited Sanja Zlatanovic Sanja 2 , Yoshitomo, Okawachi 2 CREOL, College of College CREOL, 1 1 , F. Gholami F. , , S. Radic 1 ; 2 4 1 , Reza Salem Kavli Inst. at Inst.Kavli School of Apof- School 1 ; 1 1 1 Ryan Ryan , J. S. J. , Univ. , I. B. 3 1 , , of fingerprint. the the shifted position and correcting the rotation angle appropriatelyimage encrypted an without detecting decrypting of purpose the for image plain the from ogy, Japan. We propose a method to eliminate the tags Takashi Obi, Nagaaki Ohyama; Tokyo Inst. of Technolfumi - Takeda, Hiroyuki Suzuki, Masahiro Yamaguchi, Keys , Fingerprint Using Encoding Phase Random Double Invariant Rotation and Shift •9:15a.m. FTuD6 munity to noise using when proposed the method. showimprovementconditionim- matrixand the of Results method. trajectories”“blurred the of results experimental preliminary presentWeUniv., Israel. Armenia, sion sum-frequency generation inthe process. technique of frequency tuning and spectral compres- ize it by means of its chirp measurement through the dispersive similariton in a passive fiber, and character France. aei Yesayan Garegin , Experiment Condition- Matrix Improving for Design Optical •9:00a.m. FTuD5 Louradour Similariton, Broadband of Characterization and Generation •8:45a.m. FTuD4 Information Science—Continued •GeneralOpticsin FTuD We generate a 100 nm-bandwidth nonlinear- 2 XLIM Inst. de Recherche, Univ. de Limoges, 2 , AlainBarthélémy, Iftach Iftach Klapp Aram Zeytunyan Aram Highland D 1 , Levon Mouradian Levon , , David Mendlovic; Tel Aviv 2 ; 1 1 , Anush MuradyanAnush , YerevanStateUniv., 1 , Frédéric , Masa 1 - - , in SBS-Active Media, SBS-Active in Pulses Laser of Self-Focusing Three-Dimensional •9:15a.m. FTuE6 remain locked. amongaperturesrelativephases the while apertures various among delay group relative the control to system. Two slow-light mechanisms are demonstrated radar (SLIDAR) and demonstrate a proof-of-concept laser slow-light multi-aperture a proposeWe USA. Rochester,Univ.Vornehm,W.of Boyd; Jr.,Robert E. (SLIDAR), Radar Laser Slow-Light a of Demonstration •9:00a.m. FTuE5 the experimental results. experimental the with along ratio noise to signal the of investigation an through quantified is utility The deflections. beam transverse amplify to technique weak-value Howell; Univ. C. of John Rochester, Jordan, USA. We N. report Andrew an interferometric Vudyasetu, K. Dixon Deflection Measurements with Weak Values, •8:45a.m. FTuE4 Stefan Skupin Stefan modulations can achieve. weaken backscattering, which appropriate amplitude regime, phase-modulated broadband pumps may not for nanosecond laser pulses in silica. In self-focusing Brillouin scattering (SBS) is numerically investigated stimulated and filamentation Kerr between pling couFriedrich-Schiller-Univ.,- Optics,The Germany. Planck-Inst. for the Physics of Complex Systems, Systems, Complex of Germany, Physics the for Planck-Inst. FTuE •GeneralOptics—Continued FTuE , David J. Starling, Nathan S. Williams, Praveen 3 Inst. of Condensed Matter Theory and Theory Matter Condensed of Inst. Zhimin Shi Zhimin 2,3 ; Highland E 1 CEA-DAM, DIF, France,DIF, CEA-DAM, , AaronSchweinsberg,Joseph, Sarah Mauger Sarah 1 , Luc Bergé Luc , 2 P. B e n n e B P. Max- 1 , Tuesday, October 26 51 - , Jing Zhang, Jinfang LS Asaf Eilam, Ido Azuri, Anton V. V. Azuri, Ido Asaf Eilam, Anton Highland K Highland Yundong Yundong Zhang , ; Bar-Ilan Univ., Univ., Bar-Ilan ; Wilson-Gordon D. Arlene We show that a system characterized by long- a characterized by system that show We LTuB • Nonlinear Optics I— • Nonlinear Optics LTuB Continued Wang, Xuenan Zhang, Wang, Dan Wu, Ping Harbin Yuan; disper the investigate We China. Technology, of Inst. sion characteristics of coupled resonator induced transparency and absorption in the microspheres between switch The system. taper fiber a with coupled superluminal and subluminal could be realized by the gain. doping LTuB3 • 9:00 a.m. LTuB3 The Transition between Superluminal and - Sub luminal for Multiple Gain-assisted Microspheric Resonators LTuB4 • 9:15 a.m. LTuB4 - Popu Coherent on Based Memory Optical Spatial lation Oscillations, Sharypov, Israel. as such (CPO), oscillations population coherent lived can state, shelving a via decays that system two-level a memory. be optical used a spatial construct to ; 4D Technology Corp., Invited Highland J Highland on polishing equipment is presented. presented. is equipment polishing on in situ JOINT FiO/LS JOINT A compact, vibration insensitive interferometer interferometer insensitive vibration compact, A

Michael Michael North Morris STuA3 • 9:00 a.m. STuA3 STuA • IPF-Laser Applications in STuA Metrology—Continued Dynamic Interferometry for on-Machine - Metrol ogy, USA. The The system employs a single-frame-phase sensor that permits acquisition in tens of microseconds to mitigate the effects of vibration or relative-motion with the test-part. The theory of operation is - pre sented along with experimental test results, which characterize and repeatability under precision static conditions. high-vibration and design that is well suited for measuring optics while mounted , - 1 Latha , Andrew H. 2 Swapan Swapan K. Gayen Physics Dept.,CUNY, 1 ; 2 October 24–28, 2010 , Flory K. Wong LS 1 ; Univ. of - Dela G. Sylvain Cloutier; Univ. • Highland H Highland Chemistry Chemistry Dept., CUNY,USA. Optical spec 2 , Valeria Balogh-Nair 2 LTuA4 • 9:15 a.m. LTuA4 A Near-infrared Emitting Self-assembled Pbs- dendrimer , Nanocomposite LTuA • Photophysics of • Photophysics LTuA Materials II— Nanostructured Continued LTuA3 • 9:00 a.m. LTuA3 Direct-Bandgap Emission from Hydrostatically Germanium NanocrystalsTensile-Strained , Xu, Fan Nataraj, - lumi room-temperature high report We USA. ware, synthesized nanocrystals Germanium from nescence by mechanical grinding. Optical spectroscopy mea- and electron with HRTEM consistent are surements diffraction, suggesting high tensile strains favoring transitions. band-to-band direct USA, Mohammad Mohammad Alrubaiee troscopy troscopy of a nanocomposite of PbS quantum dots and poly(amido amine) dendrimer exhibits a 750- nm band-edge absorption peak, partially-polarized and nm, 940 peak at with fluorescence nm 820-1150 785 ns. of lifetime a fluorescence Byro

, , 3 1 FiO/LS 2010 Mary - Bris of Univ. 2 , Barry Jack 1 , Steve Barnett Steve , 1 ; Univ. ; of Univ. Maryland, USA. , Jonathan Leach 1 , Xu Wang; Univ. of Rochester, USA. Rochester, of Univ. Wang; Xu , Univ. of Glasgow, UK, Glasgow, of Univ. Highland G Highland 1 , Sonja Franke-Arnold Sonja , ; 2 1 James Franson We holographically holographically We UK. Strathclyde, of Univ. 3 The The quantization of the electromagnetic field in the Lorentz gauge produces longitudinal and scalar photons. transverse theusual to addition in photons produce can photons additional these that shown is It atoms. between distant entanglement FTuG5 • 9:00 a.m. Entangled Tangles of Phase , Singularities Jacquiline Romero FTuG and Quantum Information • III—Continued Communications the dynamics and Following of entanglement atoms a of dynamics entanglement the how study we fields, - dimensional own its affected by is system bi-partite a model of reservoir with the dimensionality and ity interacts. which it FTuG4 a.m. • 8:45 Qutrit Influence on Entanglement Dynamics, AgarwalShantanu tol, UK, tol, measure entangled tangles measure of phase singularity lines down- parametric spontaneous via generated light in This type conversion. is of interesting entanglement extend that features topological between is it because volumes. isolated macroscopic, finite, over FTuG6 • 9:15 a.m. Entanglement from Longitudinal and Scalar , Photons Mark R. Dennis R. Mark Padgett J. Miles - FiO Duke , Ivan , Ivan 1 1 Xiaox , Lukas Lukas , ; 2 1 ,Zachary Lapin 1,2 ; Univ. of Rochester, USA. In Rochester, of Univ. ; , Warren , S. Warren Warren Thomas E. Matthews 2 Highland F Highland Duke Univ. Duke Hospital, Univ. USA. Two-color 2 Inst. of Physics, Univ. of Münster, Germany, Germany, Münster, of Univ. Physics, of Inst. 1 Edward Brown ; 2 , Maria A. Selim Christiane Höppener Christiane 1 , -Pumps -Pumps in the Plasma of Membrane Erythro- 2+ Inst. of Optics, Univ. of Rochester, USA. High-Resoof - of Inst. Rochester, Optics, Univ. FTuF4 • 9:00 a.m. Epi-Detected Ratio of forward-Propagating to Signal, Harmonic Second Back-Propagating ing Han, Han, ing this paper, we present a method to determine, for the for determine, to method a present we paper, this first time, the SHG F/B ratio in vivo on the surface of intact or biopsy tissue any tissue without samples epi-detection. only sectioning, using two-photon spectroscopy allows us for the first time first the for us allows spectroscopy two-photon - pheomela and eumelanin of distribution the image to nin in tissue slices, giving histology-like detail in and changes morphological and chemical highlighting benign to lesions. compared melanoma FTuF5 • 9:15 a.m. Antenna-Assisted Colocalization of Individual Ca lution lution Imaging with Single Sensitivity Protein holds promise for studies of the chemical organization of important are investigations Such structures. cellular distri- spatial regular the from abnormalities reveal to proteins. specific of membrane bution 2 FTuF3 a.m. • 8:45 Eumelanin of Imaging High-Resolution Nonlinear and Pheomelanin Distributions in Normal Skin , Tissue and Melanoma FTuF Microscopy II—Continued • Novotny cytes Piletic Univ., USA, Univ., Tuesday, October 26 52 oag Liu Boyang density of 2.5kA/cm2. mode CW lasing is achieved with a threshold current spatial Single demonstrated. experimentally is ends laser with micro-loop mirror as high reflectors at both heterogeneouslyintegratedSi/AlGaInAsevanescent electrically-pumped An Singapore..Inst., Storage 1 Reflector (MLM) Mirror Micro-loop with Lasers nescent Eva- Silicon/III-V Integrated Heterogeneously •9:45a.m. FTuA5 Fu , in SemiconductorChaotic Dynamics Laser Injected Optically an Power-over-FiberUsing •9:30a.m. FTuA4 Continued •PhotonicsandEnergyII— FTuA Wang 5-km single-mode fiber is demonstrated. fiber single-mode 5-km a through 838mW of transmission that such chaos scattering is effectively suppressed by the broadband Brillouin Stimulated delivery.power-over-fiber for applied is laser semiconductor injected optically an ing,Univ. Hongfrom ofKong, signal China. Chaotic China, Kong, Hong Univ.of City Engineering, Electronic of Northwestern Univ., USA, 1 , , ______Sze-Chun Sze-Chun Chan 3 , YongqiangWei, 2 Dept. of Electrical and Electronic Engineer Electronic and Electrical of Dept. , Yunan Zheng Yunan 2 Ynmn Tu Yongming , Highland A 1 , , Kenneth Kin-Yip Wong 3 , Doris Ng Doris , 1 , 2 Yingyan Huang Yingyan Optonet Inc., USA, 1 , Seng-Tiong HoSeng-Tiong , 3 , Chee Wei Lee Wei Chee , 10:00 a.m.–12:00p.m. 2 , Yadong, 2 ; ; Xuelei 1 3 Dept. Data Data 1,3 3 - ; , the adverse boundary effect. adversethe boundary demonstratedimprovementreducingby imaging in have we Ophthalmoscope, Laser Scanning Optics surement. With our dual deformable-mirror Adaptive handling condition the boundary of wavefront - mea carefully requires controlwavefront Accurate USA. Stephen A. Burns; School of Optometry, Indiana Univ., for Adaptive Optics Retinal Imaging, Condition WavefrontBoundary the Improving •9:45a.m. FTuB5 2 M. Oliveira using currently available phones. diopters ~0.5 of error average an revels evaluation User eyes. human of properties refractive assessing for software interactive an and display phone cell a Sul, Brazil. We describe an optical design that retrofits Phones, Dual of Shack-Hartmann Optometry Using Mobile •9:30a.m. FTuB4 Eye—Continued •AdaptiveOpticsforthe FTuB Inst.Informática,de Univ. Federal RiodoGrande do VitorF. Pamplona 1,2 , Ramesh Ramesh Raskar Highland B 10:00 a.m.–10:30a.m. Students andYoung ProfessionalsForum onPublicPolicy, Carlson and Douglass, Radisson Hotel Rochester Riverside 1,2 , Ankit, Mohan 1 ; 1 MIT Media Lab, USA, Weiyao Zou Weiyao 1 , Manuel, FiO/LS 2010 , Recovery Gain Fast with Amplifiers Optical conductor - Semi in Four-WaveMixing Interband Efficient •9:45a.m. FTuC6 designed composition.designed specially a with wafer AlGaAs an in written guides wavemixing tunable range14-nm withina wavein - Govind P. Agrawal Govind and wavelength conversion regeneration signal all-optical include applications and signal detunings exceeding 6.5 nm. The potential semiconductor optical amplifiers at low pump powers ficient interband four-wave mixing (with net gain) in ef- observe WeTechnology, USA. of Inst. Rochester phase shift of 5 demonstrate self-phase modulation with a nonlinear Computer Engineering, Univ. of Toronto, We Canada. Ng, Li Qian, Stewart Aitchison; Dept. of Electrical and AlGaAs Waveguides, 1-cm-long in MixingFour-wave and Modulation, Cross-phase Modulation, Self-phase Broadband •9:30a.m. FTuC5 USA, Optics—Continued •NonlinearIntegrated FTuC Coffee Break,Empire Hall, Rochester Riverside Convention Center 2 Telecommunications Engineering Technology,TelecommunicationsEngineering , Prashant P.Baveja Prashant π , cross-phase modulation, and four- • Highland C 1 ; 1 Inst. of Optics, Univ. of Rochester, NOTES FiO Ksenia Ksenia , Dolgaleva Wing Chau October 24–28,2010 1 , Drew N. Maywar N. Drew , 2 , the numberthe of keys. correct the decryption decryption key and the encryption key and counting means of calculating a Euclidean distance between the tribution of the key-space in the phase-only DRPE by Tokyo Inst. of Technology, Japan. We analyzed the dis- Masahiro Yamaguchi, Takashi Obi, Nagaaki Ohyama; , Encoding Phase Key-Space Analysis of Phase-Only Double Random •9:30a.m. FTuD7 Information Science—Continued •GeneralOpticsin FTuD Highland D KazuyaNakano Hiroyuki, Suzuki, tonics, Univ. of Central Florida, USA, Florida, Central Univ.of tonics, , Beams Astigmatic in Anomaly Phase Gouy Measuring and Modeling •9:30a.m. FTuE7 Rochester,USA, Thompson Schmid Associates, USA, Associates, Interferometer. results with experimental data using a modified Mertz with lens design software and compare computational beams using a beam propagation algorithm integrated Gouy phase anomaly near astigmatic foci of Gaussian predicted the Wesimulate Rochester,USA. Univ.of or produced fields by lasers. mode-locked spectroscopy comb of trains pulse the e.g. statistics, results These apply tostochastic periodic with fields experimentally.demonstrated are fields tationary - cyclos of spectra generalized the in shifts predicted Previously Urbana-Champaign,USA. at Illinois of Univ. P.Carney; Oelze,Scott Lavarello, J.MichaelL. Fields, tationary Cyclos- of WolfShifts for Evidence Experimental •9:45a.m. FTuE8 FTuE •GeneralOptics—Continued FTuE 2 , John TamkinJr.John , 3 , Emil WolfEmil , 2 Highland E CREOL, College of Optics and Pho- andOptics of College CREOL, 4 Dept. of Physics and Astronomy, and Physics of Dept. , Roberto Roberto W.Schoonover, Robert Jannick P.Rolland Jannick 1,4 ; 1 , Kye-SungLee , 1 Inst. of Optics, Univ.of Optics, of Inst. 3 Optical Res. Res. Optical 1 , Kevin P. Kevin , 1,2 , Tobias, Tuesday, October 26 53 ; - - 1,4 - Ku Prem , 1 , Vadim Lo - , Vadim 1 Northwestern 2 Biophotonic Solu Biophotonic 4 , Marcos Dantus Muthiah Annam gas jet in ambient 3 2 Spectra Spectra Energies LLC, 2 , Dmitry Pestov 1 , Michael Vasilyev Michael , LS 1 , James R. Gord 2 Highland K Highland Paul Wrzesinski Paul Univ. of Texas at Arlington, USA, Arlington, at Texas of Univ. Propulsion Directorate, USA, USA, Directorate, Propulsion , Sukesh Roy Sukesh, , 1 3 1 ; , Nikolai Stelmakh Nikolai , Fermi dyads. Fermi 2 1 2 Michigan Michigan State USA, Univ., LTuB • Nonlinear Optics I— • Nonlinear Optics LTuB Continued LTuB5 • 9:30 a.m. • 9:30 LTuB5 Amplifier Image Phase-Sensitive of Modes Spatial with Elliptical Gaussian , Pump alai LTuB6 • 9:45 a.m. LTuB6 Single-beam Towards CARS Imaging of Reacting Flows tions Inc., USA. tions of Inc., Imaging a CO Univ., USA. Univ., We develop the formalism to for find shapes the their and eigenmodes supported of number a spatially broadband frequency-degenerate optical parametric amplifier with elliptical Gaussian pump, squeezed. independently is each eigenmode where air via single-beam CARS technique is demonstrated. demonstrated. is technique CARS single-beam via air chemical the provide to used is shaping phase Binary contrast through selective excitation of one of the CO USA, 1 mar zovoy Richard Richard Invited The The best measurements of the Highland J Highland JOINT FiO/LS JOINT ; NIST, ; USA. NIST, STuA • IPF-Laser Applications in STuA Metrology—Continued The The Electronic Kilogram and Lasers, Planck constant are from the electronic kilogram project at the National Institute of Standards and are measurements position laser Precise Technology. this system. of components the many of one Steiner STuA4 • 9:30 a.m. • 9:30 a.m. STuA4 , 1 Jiong Jiong Shan, Shen Xu, China. ; WeUniv., Fudan Elsayed Esam M. Khaled October 24–28, 2010 LS NOTES Lei Xu photo-isomerization yield yield tophoto-isomerization cis ElectricalEngineeringDept., Assiut 1 Analytical Analytical Egypt. Co., Egypt Telecom • Highland H Highland ; 2 2 trans r Cente Convention Riverside Rochester Hall, Coffee Break, Empire LTuA • Photophysics of • Photophysics LTuA Materials II— Nanostructured Continued LTuA5 • 9:30 a.m. • 9:30 LTuA5 Photoluminescence Enhancement from an Axi- symmetric Zinc Sulfide Particle Illuminated with a Focused Laser Beam, analysis of photoluminescence enhancements from a from enhancements photoluminescence of analysis cylindrical or sulfide - particleillumi zinc spheroidal illustrated. is beam laser shifted focused a with nated This enhancement can also be obtained by doping cores. particles copper with such report that the that report of azobenzene molecule can be tuned in a range of 8% to 40% when the molecules are placed close to nanostructures. gold different LTuA6 • 9:45 a.m. LTuA6 Efficiency Quantum Photoisomerization of Control by Metallic , Nanostructures Liu, Shi, Liying Wei Hany L. Ibrahim L. Hany University Egypt, University , FiO/LS 2010 ,; Univ. of Toronto, Carlson and Douglass, Radisson Hotel Rochester Riverside Rochester Hotel Radisson Douglass, and Carlson on Public Policy, Forum Professionals Students and Young 10:00 a.m.–10:30 a.m. Highland G Highland Omar Gamel , Paul L. France. Georgia Tech, Voss; , We find the effective Hamiltonian for the FTuG and Quantum Information • III—Continued Communications FTuG7 a.m. • 9:30 A Provably Secure Streamcipher Based on a High Speed Quantum Random Number Generator Zheshen Zhang We propose a novel low-complexity streamcipher device based on random numbers from quantum sources with security from NP-complete problems. 20 Gbit/s. of rate a generation demonstrate We FTuG8 • 9:45 a.m. Time Averaged Density Matrix and the Effective Hamiltonian Canada. evolution of the time-averaged density matrix of decoherence a nonunitary with along system, quantum Stark AC to Theory applied form. Lindblad in terms Transitions. Raman 3-level Shift, and . FiO , Robert mutans 1 10:00 a.m.–12:00 p.m. and Inst. Inst. of Optics, Univ. 1 ; 1 Brooke Brooke D. Beier ; Univ. ; of Univ. Illinois at Urbana- Ctr. Ctr. for Oral Biology, of Univ. 2 Highland F Highland Streptococcus Streptococcus sanguis Raghu Ambekar Ramachandra Rao, , Andrew J. Berger 2 ______G. Quivey FTuF7 • 9:45 a.m. - Streptococ of Microspectroscopy Raman Confocal cus Sanguis and , Mutans Champaign, Champaign, USA. We discuss the application of harmonic analysis in second-harmonic generation microscopy in developing useful quantitative - met rics for assessing tissue A morphology. comparison between the information content in forward and also is presented. images SHG backward FTuF6 a.m. • 9:30 Development of Metrics Quantitative for Second- Collagen-Based of Imaging Generation Harmonic , Structures Kimani Toussaint, Jr. FTuF Microscopy II—Continued • Rochester, USA. Rochester, Confocal Raman microscopy has been used to distinguish between biofilms of oral bacteria species This capability has been applied to the study of mixed of study the to applied been has capability This plaque. dental a model for as biofilms of Rochester, of USA, Rochester, Tuesday, October 26 54 low Optical Fiber, Optical low Hol - Filled Liquid Periodicitya Assembled in Self Sohee An Sohee FTuH1 •10:30a.m. FTuH1 Denmark, Denmark, Presider Lars Grüner-Nielsen; OFS •NovelFiberDevice FTuH 10:30 a.m.–12:00p.m. Korea, , and optofluidic applications are explored. and irradiating UV light, respectively. Their photonic inside hollow-fiber by traversing a micro-heat-source, fabricatedwere structures polymer-airperiodic and liquid-air reproducible Highly fiber. hollow-optical sefl-assembled manner was observed in a liquid-filled ton, UK. band rejection filter. transmissionforwere the analyzed in shifts spectral Consistentwaist. taper the overapplyingtorsion by 1700nm to 1000nm from achieved experimentally was coupler fiber fussed a in coupling light tunable Ultra-wide of. RepublicUniv.,YonseiKorea, Oh; the Waist, Applying Coupler by Locally Torsional Stress over Ultra-Wide Tunable Coupling in Fused Taper Fiber •11:00a.m. FTuH2 shape and core shape asymmetries. birefringenceunderlying the bytocaused latticethe index profile of a PCF single lattice unit in comparison refractive the ofanisotropy the by caused fringence bire- the on Wisconsin-Milwaukee,Wereport USA. Mafi, Arash Anisotropy, Unit-CellVersus Shape Lattice ding - Clad Fibers: Crystal Photonic in Birefringence •11:15a.m. FTuH3 2 A novel route to form a periodic structure in a Optoelectronics Res. Ctr., Univ. of Southamp- 1 , Yongmin, Jung Honggu Honggu Choi Parisa Gandomkar Yarandi Gandomkar Parisa Highland A KyunghwanOh , Yunseop Jeong, Kyunghwan 2 ; 1 YonseiUniv., Republicof Invited 1 , HojoongJung, ; Univ.of ; 1 , ment discussed. directions be will develop and research future Finally,environment. gas and aqueous in sensing chemical and biological introduced, be followedfirst applicationsby their in will structures resonator ring various presentation USA. Michigan, Univ. of Balareddy; C. Suter,D.than Yuze JingSun,Karthik Liu,HaoLi, R. Chemical Sensors, Sensors, Chemical and Biological Based Resonator Ring Optical USA. Abstract not available. Optics, VolumeComputational in Freedom of Degrees Louis, USA,Presider Guoqiang Li; Univ. of Missouri at St. Biomedical SystemsI •OpticalDesignfor FTuI 10:30 a.m.–12:00p.m. FTuI1 •10:30a.m. FTuI1 FTuI2 •11:00a.m. FTuI2 Rafael Piestun; Univ. of Colorado at Boulder, Highland B Jona Fan , (Sherman) Xudong Invited Invited In this In FiO/LS 2010 - - a normal-dispersion for laser first time. the fiber other has a double-humped structure, was observed in ponents, one of which is a single-hump pulse and the polarizationcomorthogonal- tons, twoconsiting of Univ.,- soli dissipativeSingapore.vector High-order TechnologicalNanyangEngineering,Electronic and Zhao, Han Zhang, Randall J. Knize; School of Electrical , in a Fiber Laser Evidence of High-Order Vector Dissipative Soliton •11:00a.m. FTuJ2 be reviewed. be will developments Recent lasers. fiber prior over advantages practical and performance major offer formationdissipative-soliton on based lasers fiber Solitons, Dissipative on Based Lasers Fiber Short-Pulse FTuJ1 •10:30a.m. FTuJ1 USA, Presider Guifang Li; Univ. of Central Florida, •Ultrafastfiberlaser FTuJ 10:30 a.m.–12:00p.m. locked Er:fiber laser at laser a repetition ratelocked Er:fiber of 225 MHz. mode a from directly generation pulse level fs 30 Zong, Zhigang Zhang; Peking Univ., China. We report , Er:fiber Laser an from Directly Generation Pulse Level fs 30 •11:15a.m. FTuJ3 Frank Wise Frank Ding Ma Ding • Highland C Xuan Wu Xuan ; Cornell Univ., USA. FiO October 24–28,2010 , Chun Zhou, Yue Cai, Weijian , Dingyuan Tang, Luming Invited Short-pulse , Pulses sical Temporalof- Properties Clas with Imaging Ghost •11:00a.m. FTuK2 ing a10-fold reduction inimage acquisition time. algorithm based on compressive-sensing, demonstrat- beam. We further develop an advanced reconstruction single single-pixel detector and a spatially modulated depth-resolved computational ghost imaging using a Israel. Science, of WeizmannInst. Sensing, Compressive with Imaging Inspired Quantum Friberg FTuK1 •10:30a.m. FTuK1 of Eastern Finland, Finland, resultant image quality are discussed. condition the imagingand the on incidentpulses of conventional ghost imaging with thermal light. Effects sical pulses is asdescribed a temporal counterpart of clas- with imaging TemporalSweden.ghost (KTH), Associates, USA,Presider Kevin Thompson; Optical Res. Diagnostics andSensingI Non-Imaging Techniques for •GeneralizedImagingand FTuK 10:30 a.m.–12:00p.m. filter to and model predict light propagation. manyin planes, using an extended complex Kalman plex-field retrieval from noisy intensity measurements bastathis; MIT, USA. We propose a method for com- Waller Filter, Kalman A UsingMeasurements sity AmplitudeNoisyfromAndImagingInten Phase - •11:15a.m. FTuK3 , Mankei Tsang, Sameera Ponda, George Bar Tsang,MankeiGeorgePonda, Sameera , 2,3,4 Ori Ori Katz, Yaron Bromberg, Yaron Silberberg; ; 1 AIST, Japan, Tomohiro Shirai Tomohiro Highland D 2 Aalto Univ., Finland, 4 Invited Royal Inst. of Technology 1 , TeroSetälä , We demonstrateWe 2 , Ari T. Ari , Laura Laura 3 Univ. - Vodopyanov Combs for Spectroscopic Applications, New Source of Ultra-Broadband Mid-IR Frequency C. CosselC. Francois Couny Francois Mondloch Erin FTuL1 •10:30a.m. FTuL1 Piotr Maslowski Piotr Byer L. Robert gases in<1minutegases of acquisition time. lution, detecting ppb-level concentrations of various ing in the ~2200-3700-cm comb-based Fourier transform spectrometer operat- Mikolaja Kopernika, Poland. We present a frequency- Optics and Dept. of Physics,Univ. of Oregon, USA, USA, Oregon, of Physics,Univ. of Dept. and Optics 2 Lawrence, USA,Presider Science and Applications Program, Michael J. Messerly; Photon Saclay, France, Presider Bertrand Carre; Inst. du CEA Spectroscopy •FrequencyFTuL Combsfor 10:30 a.m.–12:00p.m. centered at 3.1μm. comb frequency 1400-nm-wide > produced source The pulses. laser Er-fiber femtosecond 1560-nm by optical parametric oscillator synchronously pumped mid-infrared frequency combs by using subharmonic We implement a new approach for creating broadband acquisition of broadband spectra with 0.01 cm cal Frequency Comb Generation Comb Frequency cal Opti- Raman in Correlations Phase Spontaneous •11:00a.m. FTuL2 medium as a125THz phase modulator. Raman optical comb spectrum. The model treats the generated spontaneously a in lines multiple among and experimentally observe strong phase correlations Materials, Univ. of Bath, UK. We theoretically predict USA, Univ.Colorado,of USA, Fourier Transform SpectrometerTransform, Fourier Comb Frequency Mid-Infrared High-Resolution •11:15a.m. FTuL3 Dept. of Physics, Ctr. for Photonics and Photonic and Photonics for Ctr.Physics, of Dept. 2 Ludwig-Maximilians-Univ. München, Germany. 1 , Travis, BrilesC. 1 , Nick C. Leindecker 1 1 , Vladimir Pervak Vladimir , , Michael Raymer Michael , 2 1,2 , Fetah Benabid Fetah , Highland E , Aleksandra FoltynowiczAleksandra , 2 InstytutFizyki,Uniwersytet 1 -1 , Jun, Ye range which allows rapid Invited 1 2 1 , Alireza Marandi 1 2 ; , Yingying WangYingying , ; ; 1 , 1 1 Oregon Ctr. forCtr. Oregon Florian Adler Florian JILA, NIST andNIST JILA, Stanford Univ.,Stanford Chunbai WuChunbai Konstantin Konstantin 1 , Kevin Kevin , -1 reso 1 1 2 1 - , , , ,

Tuesday, October 26 55 , 1 , R. 1,2 Holger , , 2 , Brian S. 1 , , H. Kübler 1 , J. P. Shaffer , J. P. 1 Ricardo Ricardo Jimenez- Univ. of Oklahoma, Oklahoma, of Univ. 2 We review We the state of Invited Invited Philip Measor , A. Kölle Tilman Tilman Pfau 1 LS , , Aaron R. Hawkins 2 Highland K Highland , B. Huber 1 Univ. Univ. of California at Santa Cruz, USA, W. Clark W. Griffith, Svenja Knappe, John 1 ; 1 , , Evan J. Lunt 2 Univ. Stuttgart, Germany, Germany, Stuttgart, Univ. 1 We show that coherence times of We ~ 100 ns are ; 1 Brigham Young Univ., USA. Univ., Brigham Young LTuD2 • 11:00 a.m. LTuD2 High Bandwidth Optical Magnetometry with a Micromachined CellVapor , Martinez, describe USA.We Div., Frequency and Time Kitching; an optical magnetometer that retains its sensitivity within a bandwidth of 10 kHz. The device relies on laser spectroscopy of alkali atoms contained in a 2 cell. vapor mmX 1mmX 1mm micromachined LTuD1 • 10:30 a.m. LTuD1 Philips the art of planar optofluidic devices using liquid-core liquid-core using devices optofluidic planar of art the waveguides for ultrasensitive particle detection and manipulation. 2 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 • Novel Imaging, LTuD in and Manipulation Spectroscopy I Microstructures California of Univ. E. Sharping; Jay USA, Presider Merced, at Löw USA. spectroscopy atom Rydberg coherent with achievable in micrometre-sized thermal vapour cells making them robust and promising candidates for scalable sources. devices single-photon like quantum Schmidt T. Baluktsian T. LTuD3 • 11:15 a.m. LTuD3 Single-Particle Single-Particle Spectroscopy and Manipulation in Optofluidic Devices, Coherent Coherent Rydberg Excitation in Microscopic Thermal Cells,Vapor - Chris Quantum Quantum Peter Peter ; F. Michelson Invited Invited The The Fermi Gamma-ray Space Highland J Highland ; Univ. ; of Univ. Maryland, USA. JOINT FiO/LS JOINT STuB2 • 11:00 a.m. STuB2 Viewing the High-Energy Universe with the Fermi Fermi the with Universe High-Energy the Viewing Gamma-ray Space Telescope, USA. Stanford Univ., Quantum Entanglement and Information, systems can store entangled superpositions of information, offering the possibility of enhanced performance in many applications. This talk will scale entangled large usedmake to hardware outline light. and atoms using states, Telescope has completed 2 years of observations of the of observations of years 2 completed has Telescope - provid GeV, 300 than more to keV 10 from sky entire a new the view high-energying of Universe. topher Monroe 10:30 a.m.–12:30 p.m. 10:30 a.m.–12:30 in Physics - Frontiers • IPF STuB of Inst. American Ben Snavely; Presider USA, Physics, STuB1 • 10:30 a.m. STuB1

, 1 Anne Goj, The The theory of Univ. of Toronto, of Toronto, Univ. , Cathy Y. Wong 1 2 ; 1 Invited Invited October 24–28, 2010 LS Here Here we report results obtained

. • Highland H Highland Roman Vaxenburg Roman , 1 , Gregory , D. Gregory Scholes 2 Russell Russell Berrie Inst. Nanotechnology and Solid 2 using using two-dimensional photon echo spectroscopy (2DPE) to study ultrafast dynamics in CdTe/CdSe dots. quantum heterostructured State State Inst., Israel LTuC1 • 10:30 a.m. LTuC1 USA, 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 of • Photophysics LTuC Materials III Nanostructured Univ., Northwestern Weiss; Emily USA, Presider Efrat Lifshitz LTuC2 • 11:00 a.m. LTuC2 Mixed Quantum Classical Simulations of - Vibra tional Excitations in Peptide Helices, Eric Bittner; of Univ. Houston, USA. using studied been been has largely solitons Davydov semi-classical techniques that invoke an adiabatic approximation. We test for the soliton formation under conditions that include important features of solvent, a temperature, system-300K biological true a reforming. and breaking bond hydrogen Two-Dimensional Photon Echo Measurements on CdTe/CdSe Heterostructured Quantum Dots, Shun Shang Lo , - - 1,2 FiO/LS 2010 , Cheng Cheng , 1 , Steven M. Girvin 1 Invited Yale Univ., Dept. of Applied Dept. of Applied Univ., Yale 2 , Benjamin M. Zwickl M. Benjamin , 1 , Simon Kheifets, David Medellin, Medellin, David Kheifets, Simon , Joel Joel , Rubin Lev Deych; Dept. of Highland G Highland We We present a scheme for measur , , Kjetil Børkje 1,2 Tongcang Li Tongcang Yale Univ., USA, Univ., Yale 1 ; 1 FTuN2 • 11:00 a.m. Optical and Trapping Cooling of Glass - Micro , spheres FTuN3 • 11:15 a.m. Optomechanics Interacting ofwith Whispering Gallery Unbound Modes of NanoparticlesMicrospheres USA. Physics,CUNY, Dynamics of a free - subwave whispering optical an with interacting particle length We theoretically. studied galleryare mode resonator show that the optical forces can capture the par ticle ticle in quasi-stationary orbital motion around the resonator. FTuN1 • 10:30 a.m. Yang Physics, Physics, USA. ing the shot noise of radiation pressure in a room temperature, table top and interferometer, discuss this goal. towards experimental progress 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 FTuN Opto-Mechanics and • I Quantum Measurement Michigan, of Univ. Carmon; Tal USA, Presider Nathan Flowers-Jacobs Nathan Quantum Back Action in Tabletop Interferometers, Interferometers, Tabletop in Action Back Quantum Jack Harris Mark Mark G. Raizen; of Univ. at Texas Austin, USA. We report optical trapping of glass microspheres in air motion Brownian of measurement and vacuum, and are We pressures. different at single of microspheres working on cooling the motion center-of-mass of a microsphere. trapped FiO The The , Eric 4,1 , Simon Simon , A high-A 1 Chemistry Chemistry 1 ; 1 San Francisco State State Francisco San 1 , Nick Conley , Nick ; , Peng Zhang Peng , 3 1 1,2 Applied Applied Physics Dept., 2 Invited , W.E. Moerner , W.E. 3 Biology Biology Dept., Stanford Univ., 3 , Nick Douglas , Nick Highland F Highland , Zhigang Chen Zhigang , 1,2 1,2 TEDA TEDA Applied Physics School, Nankai 2 DanielHernandez , Kimani C. Toussaint, Toussaint, C. Kimani , Roxworthy J. Brian , Yi Hu , Judith Frydman , Judith 1 Radiology Dept., Stanford Univ., USA. Univ., Stanford Dept., Radiology 3 4 Yan Jiang Yan FTuM3 • 11:15 a.m. Controlled Rotation of Micro-Particles with Moiré by Generated Tweezers Rotating Multi-Trap , Technique USA, Stanford Univ., USA, Stanford Univ., Miller FTuM2 • 11:00 a.m. π - Phase Cylindrical Vector Beams in Optical Tweezers, USA. Urbana-Champaign, at of Illinois Univ. Jr.; use of π - phase cylindrical vector - rela beams the in tuning optical that find We investigated. is trapping tive phase between the eigenmodes comprising the forces. the axial trapping optimize can beams FTuM1 • 10:30 a.m. 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 FTuM Trapping I • Innsbruck Ritsch-Marte; Monika Presider Austria, Univ., Medical Univ., China. Univ., We demonstrate controlled rotation of micro-particles with tweezers multi-trap rotating established with optical propelling beams. Such propelling beams contain rotating intensity blades mechanical no with but technique Moiré by generated interference. phase-sensitive or movement speed Anti-Brownian ELectrokinetic trap enables objects fluorescent sub-10nm of observation extended enzymes chaperonin single example, For solution. in - photobleach stepwise display Cy3-ATP with loaded ing traces intensity to - corresponding bind the ATP cooperativity. and stoichiometry ing/hydrolysis Dept., Dept., Stanford USA, Univ., Suppression of Suppression Brownian Motion Explores Coop- Solu - in Enzymes Multi-Subunit Single for erativity tion, Huang Univ., USA, Univ., Tuesday, October 26 56 investigated. was domain spectral the in evolution degeneracy The eigen-modes. of degeneracy 3-fold unique a providing hole air central a with core triangular a has which fabricated, and proposed is fiber optical tonicTechnology, Germany. micro-structured new A Physics, Yonsei Univ., Korea, Republic of, Unger Lee Fiber, Optical Triangular-CoreHollow a of Breaking the Two-fold Degeneracy in Eigen Modes •11:30a.m. FTuH4 Continued •NovelFiberDevice— FTuH evaluated for firstby time the direct measurement. are fabrication of mechanisms Physical performed. in CO in 2D the refractive index and stress axial distributions of measurements Independent Tech,USA. Georgia Irradiation, Laser Carbon-Dioxide to Due Index Refractive and Stress Fiber Optical in Changes of Profiling •11:45a.m. FTuH5 1 , Woosung Ha Woosung , 2 2 , -laser-induced long-period fiber gratings are gratings fiber long-period -laser-induced

Kyunghwan Oh MichaelHutsel R. Thomas, Gaylord;K. Highland A 1 , Jens Kobelke Jens , 1 ; 1 Inst. of Physics and Applied 2 , Kay Schuster Kay , 2 Inst. of Pho- Sejin Sejin 2 , S. , of Michigan, USA, of Optical Ring Resonator Biosensors, Resonator Ring Optical of Capability Sensing Ultimate of Characterization •11:30a.m. FTuI3 Xudong Fan biosensors. resonator ring for benchmark the set results The limit. detection its near investigated experimentally is detection molecule small label-free and detection index refractive bulk in resonator ring optofluidic the of capability sensing The Univ.,China. Fudan neering, School of Information Science and Engineering, domain detections. coherence for wells quantumphotorefractive in ing demonstrate potential applications of two-wave mix- forlowa superluminescent lightemitting We diode. fraction or photoelectromotive force has testedbeen Photorefractive two-wave mixing based on either dif- Jeffrey LaCroix, Jeffrey , Detections Domain Coherence Adaptive for Two-WavePhotorefractiveMixing •11:45a.m. FTuI4 Biomedical SystemsI—Continued •OpticalDesignfor FTuI 1 ; 1 Dept. of Biomedical Engineering, Univ. Highland B Ping YuPing 2 12:00 p.m.–1:30p.m. Dept. of Optical Science and Engi- 12:00 p.m.–1:30p.m. ; Univ. of Missouri, USA. Missouri, Univ.of ; Adam Drewery, Drewery, Adam a Li Hao FiO/LS 2010 1,2 12:00 p.m.–1:30p.m. ,

Exhibit Only Time, EmpireExhibit OnlyTime, Hall, Rochester Riverside Convention Center USA, USA, Shahraam Afshar V.AfsharShahraam optimal strategies. design dynamics within these systems, and give insight into pulse interesting reveal simulations The oscillators. parametric optical fiber ultrafast for model gation propa- pulse nonlinear straightforward a introduce Gerlein , Laser Ring Fiber Femtosecond Dual-Mode a from Pulses Gain-Guided and Noise-Like •11:30a.m. FTuJ4 theory will be presented. be will theory soliton pulse generation regime. Detailed results and the noise-like pulse generation mode or gain-guided eitheroperationfor stabletunedin be canthat laser fiber erbium-doped femtosecond mode-locked a Oscillators, Parametric Optical Fiber Ultrafast of Modeling •11:45a.m. FTuJ5 Continued •Ultrafastfiberlaser— FTuJ OSA Fellow Grand MemberLunch, Ballroom Aand B, Hyatt 2 2 DelawareBiotechnology Inst., WeUSA. report In this paper we paper this Univ.Adelaide,Australia.In of 1 , Sylvain G. Cloutier G. Sylvain Jay E. Sharping E. Jay • Highland C 2 ; FiO 1 Univ.CaliforniaMerced,atof October 24–28,2010 1,2 Lunch (on yourLunch own) ; 1 1 , Wen Qi Zhang Qi Wen , Univ. of Delaware, Univ.of Felipe Felipe 2 , for Nonparaxial Fields, Nonparaxial for Ambiguity Function and Phase Space Tomography •11:45a.m. FTuK5 nonparaxial fields. and applied to the problem of coherence retrieval for the properties of its paraxial counterpart is presented generalization of the ambiguity function that retains Rochester,USA. Univ.of Alonso; A. for accurate and unique recovery. signal relationshipsestablish to used is signal complex the of periodicity The coherentself-imaging. contextof the in investigatedare methods retrieval phase istic USA. Phase-space tomography and related determin- Talbot Effect Deterministic Phase Retrieval And The Fractional •11:30a.m. FTuK4 Continued Diagnostics andSensingI— Non-Imaging Techniques for •GeneralizedImagingand FTuK , Markus E. Testorf; Dartmouth College, Highland D Seongkeun Cho Seongkeun A nonparaxial A , Miguel Miguel , 10 broadening. linewidth sizeable to leads fluctuation air by caused 1 propagation distance. Fractional instability ~10 instability Fractional distance. propagation transferred in the atmosphere over a 60-m round-trip are references frequency Optical USA. Huntsville, P.Gollapalli , Comb Frequency a UsingAtmosphere Delivery of Optical Frequency References through •11:45a.m. FTuL5 sensitivity and resolution. and absorption signal, improving both measurement background empty-cavity retrieve simultaneously saturated-absorptiondecoupleandto allows regime cavity ring-down spectroscopy with the sample gas in for Non-linear Spectroscopy, Italy. Giusfredi copy Saturated-Absorption Cavity Ring-Down - Spectros •11:30a.m. FTuL4 Spectroscopy—Continued •FrequencyFTuL Combsfor Inst. Nazionale di Ottica-CNR, Italy,Inst.Ottica-CNR,Nazionale di -13

, at 1s is observed and large phase modulation phase large and observed is 1s at Pablo Cancio Pastor 1,2 , Davide Mazzotti Davide , , Lingze Duan; Univ. of Alabama atAlabama Univ. of Duan; Lingze , Highland E 1,2 , Iacopo Galli Iacopo , 1,2 , Paolo De Natale De Paolo , A novel approach to to approach novel A 2 EuropeanLab 1,2 , Giovanni , Giovanni Ravi Ravi -14 1,2 - ; Tuesday, October 26 57 Jan C. , , LS Highland K Highland , Jan Hald; Danish Metrologi, Fundamental LTuD • Novel Imaging, • Novel Imaging, LTuD in and Manipulation Spectroscopy I—Continued Microstructures Petersen ammonia of spectroscopy High-resolution Denmark. in a hollow-core photonic bandgap fiber around 1.55 μm is discussed. The complex spectra in this wavelength region have been studied by saturated absorption, microwave-optical double resonance, spectroscopy. two-photon and LTuD4 • 11:45 a.m. LTuD4 High-Resolution Spectroscopy of Ammonia in Hollow-Core Photonic Bandgap Fibers - Ab The The LHC is the Invited Invited ; Fermilab, USA. ; Fermilab, Highland J Highland Walter de Walter ; Heer Georgia USA. Tech, JOINT FiO/LS JOINT Dan Green highest energy particle accelerator in the world. The The in the world. energyhighest particle accelerator associated-experiments are the largest and most complex-scientific instruments ever built. Each detector is like camera a which 100-megapixel takes per second. pictures 40-million STuB • IPF - Frontiers in Physics— - Frontiers • IPF STuB Continued The Status of the CERN Large Hadron Collider (LHC), Epitaxial Epitaxial Graphene: Designing a New Electronic Material, STuB4 • 12:00 p.m. STuB4 STuB3 • 11:30 a.m. STuB3 stract not available. stract not

- , Medhat , Medhat 1 p-type - conduc , M. C. Santhosh , M. C. Santhosh 1 P-type ZnO thin (on your own) Lunch your (on Telecom Egypt Co., Egypt. Co., Egypt Telecom 2 October 24–28, 2010 Dept. of Physics, Natl. Inst. of Dept. Inst. of Natl. Physics, LS 2 • Elsayed Esam M. Khaled Highland H Highland Talakonda Prasad Rao Talakonda Dept. Dept. of Physics, Natl. Inst. of Tecnnology 1 Assiut Univ., Egypt, Univ., Assiut ; 1 2 ; 2 Grand Ballroom A and B, Hyatt B, A and Ballroom Member Lunch, Grand OSA Fellow LTuC • Photophysics of • Photophysics LTuC Materials Nanostructured III—Continued LTuC4 • 11:45 a.m. LTuC4 Scattering of a Focused Gaussian Beam by a Di electric Spheroidal Particle with a Nonconcentric Spherical Core, Angular scattering intensities of a spheroidal particle spheroidal a of intensities scattering Angular focused a with illuminated core nonconcentric a with Gaussian beam are calculated using the T-matrix method. Effects of the offset core’s are illustrated. applicable. are Other particles shapes E. Aly E. Kumar Tiruchirappalli, India, India, Tiruchirappalli, LTuC3 • 11:30 a.m. LTuC3 a Using Films Thin Zno p-type Stable of Realization - Ap Optoelectronic for Doping Acceptor Dual Li-N , plications Technology Tiruchirappalli, India. Tiruchirappalli, Technology and lithium with dual-doping realized by films were nitrogen using spray pyrolysis. The tivity of (Li,N):ZnO stable is and with reproducible, were properties optical The quality. crystal acceptable photoluminescence. using studied Empire Hall, Rochester Riverside Convention Center Convention Riverside Rochester Hall, Exhibit Only Time, Empire 12:00 p.m.–1:30 p.m. FiO/LS 2010 Abstract Abstract not Invited 12:00 p.m.–1:30 p.m. 12:00 p.m.–1:30 p.m. Highland G Highland FTuN Opto-Mechanics and • I— Quantum Measurement Continued FTuN4 a.m. • 11:30 Silicon Silicon Monolithic Acousto-Optic Modulators, Sunil A. ; Bhave Cornell USA. Univ., available. FiO  We FiO/LS. the program. the program. Look for your via email and let us post-conference survey post-conference know your thoughts on Thank you for attending , Janelle Shane, Michael Michael Shane, Janelle , Invited Highland F Highland Kishan Dholakia Kishan FTuM4 • 11:30 a.m. FTuM Trapping I—Continued • - Microma of Shape the Changing Sculpting: Optical nipulation, UK. Andrews, St. of Univ. Cizmar; Tomas Mazilu, explore how sculpting the phase media and turbid amplitude through of trapping optical for allows light using novel wavefront correction. Addtionally we trapping. on pulsed laser light of the role explore Tuesday, October 26 58 Tsong Chang Tsong tat Yin Stuart band Optical band Filters Optical WideforNanostructures- Plasmonic Multiplexed JTuA02 proposed.tion is also design configura- mirror Better understanding. theoretical the deformation of the mirror is performed for better on analysis element finite Numerical investigated. is mirror rotational high-speed a of deformation the of TaiwanmeasurementUniv., Taiwan. Optical Engineering and Dept. of Electrical Engineering, Natl. 1 Speed Rotational Mirror , Optical Measurement of the Deformation of a High- JTuA01 Labs, Taiwan,Labs, these spheres.these of surface the along evolution from shown is phase LG modes as their eigenstates, i.e poles. A geometric described. The two spheres share circularly polarized are beams vector cylindrical for spheres Poincare Two USA. CUNY, Dept., Physics Alfano; R. Robert cal Vector , Beams Geometric Phase and Poincare Sphere for - Cylindri JTuA04 and properties the medium. of dielectric the The tunability is achieved by changing the fill fraction for applications to beam steering and demultiplexing. consistingofsilver nanorods medium anddielectric USA. We propose tunable anisotropic metamaterials Kwang W. Oh, Natalia M. Litchinister; Venugopal, SUNY Buffalo, Gayatri Panchapakesan Rajagopal, Metamaterials Anisotropic in Steering Beam JTuA03 structures. metallic periodic simple from different quite are which properties spectral optical novel have films metamaterial nanostructure periodic Multiplexed metamaterial. structure periodic of cell unit each in coupling effects of multiplexed plasmonic resonators USA, Instrument Technology Res. Ctr., Natl. Applied Res. AppliedNatl. Ctr., Technology InstrumentRes. 2 Pennsylvania State Univ., USA. We investigated 2 ; 1 1 Univerisity of Alabama in Huntsville, Huntsville, in Alabama of Univerisity , Jingshown Wu Jingshown , 2 Graduate Inst. of Communication of Inst. Graduate Giovanni Milione Giovanni , Boyang Zhang Po-Hsuan Huang 2 , Ting-Ming Huang Ting-Ming 1 , Henry I. Sztul, , Junpeng Guo 1 , Shenq- 1 1 , ; , deep-subwavelength confinement. mode for size relative mode the shrink further to material top-coat high-index using of possibility the show and devices, plasmonic spoof in waves THz of tion Technology, USA. We numerically study the propaga- Yang Applications THz forWaveguides monic Plas - Spoof Subwavelength Deep Silicon-Coated JTuA08 fluorescent beads. using confirmed were images The nanoislands. increment is based on excitation by hotspots between resolution microscopy.The reflection internal total in resolution spatial improve to imaging plasmon Korea,Republic of. Univ.,Yonsei Engineering, Electronic and Electrical M. Torres-CisnerosM. 1 2 Kim Nanoislands, Metallic by Localized cence Fluoresof- Excitation Random on Based Imaging JTuA07 with hastelloy sensors. notably reduced are analyzer the of measurements Porosity,temperaturecorrosion high and the affects paper. this in discussed is Analyzer Oxygen TDLS a The implementation of a Hastelloy material sensor in ogy, Yonsei Univ., Korea, Republic of, RepublicUniv.,YonseiKorea, ogy, Eduardo Pérez-Careta Eduardo an Optical Oxygen Analyzer in a Refinery Heather, in Sensor Element ImplementationDiffusion a of JTuA06 nanofibers.silica through sources external by excited were which microstructures active optical fabricated have we tion induced polymerization. By using doped samples polymeric structures by using the two-photon absorp- microscopic fabricate to pulses femtosecond used We Brazil.Paulo, São Univ.of Carlos, São de Física rêa,Marcos Cardoso, R. Cleber Mendonça; R. Inst. de Cor S. DanielPacheco, H. RafaelTribuzi Vinicius, Nanofibers Silica with Connected structures Micro Polymeric Active Optical of Fabrication JTuA05 Photonics and Optical Physics Lab,INAOE,PhysicsMexico.OpticalPhotonics and Program for Nanomedical Science and Technoland - ScienceNanomedical for Program 1 , Wangshi Zhao, Zhaolin Lu; Rochester Inst. of Inst. Rochester Lu; ZhaolinWangshi Zhao, , , Youngjin Oh Youngjin , We surface investigated localized 1 2 ; , WonjuLee , 1 Univ. of Guanajuato, Mexico, Guanajuato, of Univ. 1 , J. J. Sánchez-MondragónJ. J. , 2 , Donghyun Kim Donghyun , Empire Hall,Rochester RiversideConventionCenter 2 School of of School Kyujung , Ruoxi FiO/LS 2010 1,2 2 - - ; , , JTuA •JointFiO/LSPoster SessionI Rodriguez Fabry-Perot InterferometerFabry-Perot Single a Considering Design Sensor Gas Dual JTuA09 Sidney S. Yang MonicaTrejo-Duran Vapor Organic Detect to Gratings Fiber Period Long JTuA13 whitish through system. the by a black ring and white background appeared to be surroundeddot red small A pupileye. mm 4 the on aberration spherical produce to system (AO) optics adaptive Ireland,Galway, Ireland.Weused Univ.of Delestrange, Alexander Goncharov, ChrisDot, Dainty; Red Small Natl. of pearance Ap - Color the on Aberration Spherical of Effect JTuA12 image quality by noise. decreasing speckle the the improve to methods the and generated, be can which the complex 2-D subdiffraction-limited images in studies consecutive three of results experimental Technology, the TaipeiTaiwan.Univ.presentofWe Optical Elements Optical diffraction- Limited Features by Use of Diffractive Implementation of Phase-Shift Patterns with Sub- JTuA11 andidentify quantify such variations. signal this work the Fourier discrete transform was used to change.In signal the quantifycannot However they gratings. acting the identify usually gratings Bragg de Puebla, Mexico. Multipoint laser sensors based on Pérez, Univ.BeneméritaAutónomaMixcóatl; CastilloJuan Beltrán Georgina Aguirre, Muñoz Severino FFT, Using Sensor Laser Based Gratings Bragg a of Method Interrogation JTuA10 provided. be will Interferometer. Simulations and experimental results Fabry-Perotsingle a using spectroscopy correlation on based sensor gas dual a of design the analyze we Ayala 2 tivity was related to sample the molecularweight. the transmission spectrum change. The sensor sensi- deposited on an LPFG. The response was measured as organic vapor sensor was fabricated by a PDMS film An Mexico.Puebla, Univ.de AutónomaBenemérita Pérez, Severino Muñoz Aguirre, Juan Castillo Mixcoatl; Autonomus Univ. of work Tamaulipas, this Mexico. In 1 , Jose Andrade-LucioJose , , JOINT FiO/LS , Georgina Beltrán Beltrán Georgina , Reyes Epitacio Viterbo 12:30 p.m.–1:30p.m. 1 , Daniel May-ArriojaDaniel , 1 ; 1 Natl. Tsing Hua Univ., Taiwan, • , Yu-WenChen 1 ; 1 October 24–28,2010 Univ.Guanajuato,of Mexico, 1 , Roberto Rojas-LagunaRoberto , , Zepeda Méndez Oscar Huanqing Guo Huanqing , Everardo Vargas-Everardo 2 1 , Julian Estudillo- Julian , , Wei-FengHsu 2 , Elie Elie , Natl. 2 1 , , sional de-excitation of state this was observed. gaporeInst.Manufacturingof Technology, Singapore, (I=10 eration. Plasma created by the femtosecond laser pulse Volkov,Savel’ev;A. Moscow State Univ., Russian Fed - Target External , EmissionPlasma in X-Ray and Laser Corpuscular Femtosecond by Induced Processes Secondary JTuA18 optimal lengths. with single-mode-fiber by pulses femtosecond to dechirped be can pulses picosecond chirped highly original The solitons. dissipative of compression system is proposed to investigate the generation and laser all-fiber compact A China. Sciences, of Acad. Xi’an Inst. of Optics and Precision Mechanics, Chinese Xueming Liu, Yongkang Gong, Dong Mao, Xiaohui Li; in a Compact All-Fiber Laser System, Compression and Generation Soliton Dissipative JTuA17 agreement with experiment the results. chip Nd:YAG lasers. The theoretical analysis is in good of optical feedback in orthogonally polarized micro- model to explain the dynamic response phenomenon China.We present anopticalrate feedback equation Univ.,Tsinghua Zhang; Shulian Tan, Yidong Wan, Optical Feedback Rate Equation, onally Polarized Microchip Nd:YAG Laser Based on Dynamic Response of Optical Feedback in - Orthog JTuA16 in “non bump” stars. bandsthreeare these always absentwhile 1011.53A, and 1007.29A, 1004.56A, atbands absorption sharp intense display invariably stars“bump” 2175A of USA. I explain why the (999A - 1013A) FUSE spectra Photoexcited Coherently are“Bump” 2175A the Displaying Stars OB of Atmospheres Gaseous the in PresentMolecules H2 that Evidence Spectroscopic New JTuA15 correctlycan reconstructed. be resultsshow asphericformwavefrontthatof the the simulation and theoretically proved and onstrated dem- wavefront.is Itaspheric measure to proposed is methodology sensing wavefront reference-free x-rays to excite 14.4 keV nuclear state of 2 Wenjiang Guo Wenjiang Reference Free Aspheric Wavefront Measurement , JTuA14 A novel TechnologicalNanyang A Univ.,Singapore. 17 W/cm , 2 ) was used as a source of electrons and Peter P. Sorokin Peter 1,2 , Liping Zhao Liping , , D. Uryupina, R. R. Uryupina,D. , Golovin Gregory 1 ; IBM Res. (Emeritus), , I-Ming Chen I-Ming , Zhou , Ren Xinjun Leiran WangLeiran 57 Fe. Conver 2 ; 1 Sin - - , of ProteinBiomarkersof , Metallic Nanoparticles: Applications for Detection of Detection Lens Photothermal Sensitivity High JTuA20 fittedbe by adipole model. can profiles polarization the and motion rotational its by affected is solvent a in ICG of spectroscopy polarization fluorescence time-resolved The USA. CUNY, Alfano; R. Robert Wang, Wubao Yang Pu, trast Agent, ICG, Influenced by Rotational Motion, Time-Resolved Fluorescence Spectroscopy of - Con JTuA19 Xiao Xiao Qun Auto-Biosensing System for Early , Detection JTuA21 protein biomarkers. of detection for nanoparticles metallic of use the ppb.We0.5 discuss of limits demonstratedetection Wesamples. serum and water in nanoparticles lic - metal of detection lens photothermal a on report Noureddine Melikechi; Delaware State Univ., We USA. Marcano,YuriMarkushin, Chandran Sabanayagam, bacterial cells has been shown. cells has been bacterial properties, growth and accumulation abilities of this been investigated. Correlation between light-diffusion acetoxidanshasof influence metals heavy the under sizes cells of sulfurreducing bacteria Desulfuromonas different of content RelativeLviv, Ukraine.Univ. of Low . Bilyy O. Ukraine, 1 ence of Heavy Metals, Bacteria Desulfuromonas Acetoxidans under Influ- Sulfurreducing of Properties Light-Diffusion JTuA22 concentration is low to 0.01mg/ml. security information system. The measurable protein and system, analyzingsampling, auto an of consists system The urine. in protein total the detecting for nescence based auto-biosensing system was invented Materials Res. and Engineering, Singapore. Photolumi- Biological Faculty, Ivan Franco Natl. Univ. of Lviv, of Univ.Natl. Franco IvanFaculty, Biological 2 ; 1 Inst. for Infocomm Res., Singapore, Res.,Infocomm for Inst. 2 , Vasyl B. Getman B. Vasyl , 2 1 Faculty of Electronics, Ivan Franco Natl. Franco Ivan Electronics, of Faculty , Han Ming Yong Oresta M. Vasyliv Franz W.Franz Delima 2 , Ng Soon Huat 2 , Svitlana O. Hnatush O. Svitlana , 1 , Olexandr 1 , Aristides, , Michelle 2 Inst. of Inst. Zhou 1 ; Tuesday, October 26 59 , ; , - 2 1 1 Okla 2 , Hsiao- , Roman , Glenn S. Glenn , 1,2 1,2 1 We study , Jie Zhang 1 Corning Inc, USA. Inc, Corning Kishor T. Kapale T. Kishor 3 , Arnab Arnab Mitra , John Lawall John , 1 Univ. of USA, Arkansas, Univ. 1 ; 1 , Adalberto Alejo-Molina 3 , Koichiro Sakaguchi, Yasunori Western Illinois Univ., USA, Univ., Illinois Western 1 Omar S. Magaña-Loaiza S. Omar ; 2 Reeta Reeta Vyas Paulina S. Kuo S. Paulina , Natl. Natl. Inst. of and Standards Technology, 1 , 1 , Jose J. Sanchez-Mondragon 2 ; Univ. of Rochester, USA, of Rochester, Univ. 1,2 2 We experimentally USA. We Inst., Quantum Joint 2 Natl. Natl. Inst. for Astrophysics Optics and Electronics, California California State USA. Polytechnic Univ., JTuA41 Tailoring the Beam Profile of an 808-nm Pump Laser Diode Using Lloyd’s Mirror , Interference FukushimaTakehiro Tokuda; a Dept.demonstrate We Japan. ofUniv., Prefectural Okayama Communication commercial a of profile Engineering,beam the tailoring for method output circular almost An diode. laser pump 808-nm 7.2° approximately of divergence vertical a with beam interference. mirror Lloyd’s using obtained was JTuA42 Sudden Death of BetweenEntanglement Coupled Quantum Dots in a Cavity, Sobolewski We show the experimental generation and detection, detection, and generation experimental the show We as well as theoretical studies, of unusual coherent acoustic phonons on a high quality silicon-on-glass suggest sample. a We photonic crystal based on the sample. studied JTuA44 Sub-nanoscale Resolution for Microscopy via Coherent Population Trapping harng harng Shiau investigate investigate quasi-phasematched, second-harmonic generation (SHG) in GaAs microdisks. We predict 0.1% conversion efficiency using 1 mW pump SHG. resonant doubly through Solomon 1 2 Lon- Detect and Generate to Used Optics Ultrafast Silicon Quality High in Phonons Acoustic gitudinal Sample, Glass on Carlo Carlo Kosik-Williams Agarwal S. Girish - popula coherent a present We USA. Univ., State homa tion trapping based scheme to attain sub-nanoscale resolution for microscopy using three-level atoms modulated fields---amplitude optical two to coupled field. coupling dependent a spatially field and probe JTuA45 GaAs Microdisks Cavities for Second-Harmonic Generation USA, Mexico, Mexico, generation generation and time evolution of entanglement between two coupled quantum dots inside a driven entanglement the dissipation of presence the In cavity. show or asymptotically, decay stationary, remain may death. sudden JTuA43 - Ctr. Ctr. 2 , Ali 2 , Jose J. , Daniel Daniel , 1 2 - Nacio Inst. 1 ; 4 , M R Shenoy, K. Vassar College, Box 745, 745, Box College, Vassar 1 ; 1 using diffraction using elegans C. Ruchi Garg , Alvaro Zamudio-Lara Alvaro , 1 IBM, Japan. Numata; , Hidetoshi , Kathleen M. Raley-Susman M. Kathleen , 1 Adalberto Adalberto Alejo-Molina , Miguel Torres-Cisneros Miguel , 3 , Rebecca Eells Rebecca , 1 Univ. Univ. Autonoma de Tamaulipas, Mexico, 3 Yoichi Taira Yoichi Here we present present we Here USA. 731, Box College, Vassar 2 JennyMagnes , We found We Mexico. de Autonoma Guanajuato, Univ. JTuA36 Analysis of Graded-Index Segmented Channel Laser Femtosecond to Application with Waveguides , Waveguides Written India. Delhi, of Technology Inst. Indian Thyagarajan; We present an analysis of graded-index segmented channel waveguides with z-dependent refractive index variation in the high-index segments, and explain the stability behavior of recently fabricated ‘pearl chain waveguides’ using femtosecond laser inscription. JTuA37 Optical Packaging Design for Silicon Photonic Chips, We evaluated packaging design options of silicon fan-out achieving for processors with chips photonics of the optical signal lines, maintaining mechanical robustness, and signal connection to the external packaging. the conventional like signal paths JTuA38 Metallo- Ternary a in Gaps Band Omnidirectional Dielectric , Stack nal nal de Astrofisica Optica y Mexico, Electronica, - bio and physical observe to technique alternative an live of parameters logical of laser beams. We differentiate the of differentiate locomotion of laser a beams. We . C. elegans a crawling and swimming JTuA40 , in Nonlinear Absorption Multimode Waveguides Armand Rosenberg, Steven R. Flom, S. Richard Pong, James S. G. Shirk; NRL, USA. withThe waveguides energy- multimode of absorption dependent experimen- studied been has cores nonlinear strongly tally The and presence of numerically. a discrete set of waveguide modes is found to substantially lower threshold. the nonlinear ciaSampson the dispersion relation of a metallo-dielectric quarter- metallo-dielectric a of relation dispersion the wave like stack for oblique incidence (transversal electric and magnetic modes). This structure has omnidirectional band gaps not only in the bottom high frequencies. also at but JTuA39 Diffrac - through Elegans C. of Analysis Locomotive tion Sanchez-Mondragon 4 USA, A. May-Arrioja A. for Res. in Engineering and Applied Sciences. UAEM, Sciences. UAEM, and for Applied Res. in Engineering Mexico,

; 3 Arsen Ivan Ivan B. , 1 , , Banshi Beijing Jiaotong 3 , Shuisheng Jian 2 Jianyong Zhang , Oleg Semyonov, Rajneesh Verma October 24–28, 2010 Lucia Lucia A. M. , Saito Eunezio A. • Univ. of Univ. Arizona,Dept. of Electrical 2 Serge Serge Luryi , Hussam G. Batshon 2 JOINT FiO/LS JOINT Beijing Beijing Jiaotong Institute of Univ., - Lightwave Tech D. D. Gupta; Indian Inst. of Delhi, Technology India. SPR based ITO coated tapered optical fiber sensor for detection in infrared region of the spectrum is 5 times about of enhancement Sensitivity presented. gold coated fiber to optic as conventional compared reported. is sensor and and Computer Engineering, USA, JTuA32 Diagram Constellation Signal Achieving Capacity of Fiber-Optic Channel , nology, nology, China, Univ., Key Univ., Lab of Alloptical Network & Advanced Network of Telecommunication EMC, China. We signal describetheoptimum determine methoda to channel. fiber-optic arbitrary of diagram constellation The numerical results indicate that the optimized non- and amplitude discrete has signal constellation phase. circular JTuA33 through Luminescence of Propagation Anomalous Bulk , n-InP of Zhichao Chen; NY Univ. State at Subashiev, Stony a as semiconductor a of USA.Implementation Brook, photo-diode surface lattice-matched a with scintillator luminescence efficient requires detection radiation for collection. Low and heavily doped bulk n-InP has transmission luminescence optimize to studied been recycling. via photon JTuA34 50 km Ultralong Erbium Fiber Laser with Soliton Pulse , Compression Brazil. Mackenzie, We Presbiteriana De Souza; Univ. ac- laser fiber Erbium ultralong km 50 a demonstrated 1 from varying rate repetition with locked mode tively determined were widths pulse output The GHz. 10 to 2.5 GHz 1 and at regime soliton by JTuA35 Surface Plasmon Resonance (SPR) Based Indium Tin Oxide (ITO) Coated Tapered Optical Fiber Sensor for IR Region, 1 Djordjevic , - 1 FiO/LS 2010 JTuA • Joint FiO/LS Poster Session I—Continued FiO/LS Poster • Joint JTuA Empire Hall, Rochester Riverside Convention Center Convention Riverside Hall, Rochester Empire Vitor V. Vitor Nasci V. , Evandro - Con 1 , Arash Mafi; Univ. Univ. Mafi; Arash , , Vitor B. Ribeiro 1 Univer. of Campinas Univer. 1 ; 2 CPqD Foundation, Brazil, 1 ; 2 Univ. of Campinas - UNICAMP, UNICAMP, - Campinas of Univ. 2 Eduardo Eduardo C. Magalhães , Krishna Mohan Gundu Mohan Krishna Julio Julio C. R. F. Oliveira , , Aldårio Aldårio C. Bordonalli 1,2 , 2 A dynamic gain spectrum gain A dynamic equal - Brazil. UNICAMP, We show that the the that show of We USA. Wisconsin-Milwaukee, convergence problems in Fourier modal methods also arise from the square truncation of boundary matching conditions and that by seeking minimum least squared solution of rectangular truncation, be can achieved. convergence JTuA29 Dynamic Gain Spectrum Equalizer for in EDFAs Reconfigurable Optical , Networks JTuA28 On Convergence of Fourier Modal Methods Used for Computing Scattering from Metallic Binary Gratings mento An An Brazil. empirical characterization of wavelength conversion of phase modulated channels based on a around a 3-nm range For is presented. SOA-FWM negative in product FWM first the carrier, modulated performance. the best conversion showed detuning izer izer based on a cascade of sinusoidal superior optoceramic A demonstrated. is EDFAs to applied filters performance on power imbalance compensation and OSNR maintenance is obtained after different scenarios experimental evaluation. JTuA30 Fast and Wide Fiber Wavelength-Swept Optical , Dispersion-Tuning on Based Oscillator Parametric P. Yang, Sigang Qin Li, Cheung, K. , Y. Zhou Kim Yue C. Chui, Kenneth K. Y. Wong; of Univ. Hong Kong, a demonstrate fast We Kong. Hong and wide tuning dispersion-tuned a on based source wavelength-swept fiber optical parametric achieved oscillator. We the sweep rate of 40 kHz and the wavelength tuning 109 nm. of range JTuA31 Conversion Wavelength Characterization of 2-14 Gb/s BPSK Channels Based on SOA-FWM Properties 2 - UNICAMP, Brazil, Brazil, UNICAMP, - Aldario Aldario C. Bordonalli forti , ; - 2 2 AFRL, AFRL, 2 Dean P. Dean P. , Alphan Samuel I 1 , Bilal Khan 1 Harran Univ., Univ., Harran 1 ; 2,3 Univ. of Texas at Ar at of Texas Univ. 2 UES, Inc., USA, Inc., UES, 1 ; 2 Switzerland. Zurich, ETH , Georgios Alexandrakis 3 2 Devrim Tarhan , Daniel Rohrbach, Nestor Rigual, Rigual, Nestor Rohrbach, Daniel , , Duncan L. MacFarlane L. Duncan , 1 , Hanli Liu 2 , Özgür Müstecaplıoğlu 2 Ulas Sunar Ulas Koç Univ., Turkey, Turkey, Univ., Koç 2 , Augustine M. Urbas M. Augustine , A high density Taiwan. Univ., Formosa ; Natl. 1 Univ. of Texas at Dallas, at USA, of Texas Univ. Erin Tracy, Erin Ken Tracy, Keymel, Michele T. Cooper, Heinz Cancer Park Roswell Henderson; H. Barbara Baumann, during obtained results initial present We USA. Inst., photo-dynamic therapy (PDT) in a head sig- and induced PDT neck showed results Our patient. cancer noninvasive by assessed photobleaching drug nificant diffuse methods. optical JTuA25 Measuring Dispersion in , Metamaterials Brown We utilize a multiphoton intrapulse interference interference intrapulse multiphoton a utilize We USA. the group measure phase scanto (MIIPS) technique find and metamaterials of (GVD) dispersion velocity it to be four orders of magnitude larger than that of glasses. optical dispersive JTuA26 Lensing Properties of Ultraslow Light in Bose- Einstein , Condensate Functional Near Infrared Spectroscopy Spectroscopy Infrared Near Functional USA. lington, (fNIRS) may be a impaired using by achieved is absorption sensitivity from Improved the hair. subject’s thread to designed tips fiber with optrode redesigned scalp contact. better for the hair through JTuA24 Monitoring Photodynamic Therapy of Head and Neck Cancer with Optical Spectroscopy: Initial , Results 1 JTuA23 Improved fNIRS Using a Novel Brush Optrode, Wildey Chester En Lin microholographic using concept storage disk optical - Simultane method was demonstrated. multiplexing ous readout of multiple bits in a single storage pit is accomplished with a D/ROE head using a white source. light We have investigated lensing properties of ultraslow properties of ultraslow lensing investigated have We light in an atomic Bose-Einstein condensate by using an off-resonant electromagnetically induced scheme. transparency JTuA27 Inkjet Color on Development and Implementation High Density Data , Storage Technology Sennaroglu Turkey, Turkey, Fenghua Fenghua Tian Tuesday, October 26 60 background and foregrounds. No significant difference was found by reversing the point of subjective spherical refraction was evaluated. foreground colors of the Duochrome test on the end India. cal Refraction, cal Background on the End Point of Subjective Spheri- Effects of Changing Duochrome’s Foreground and JTuA50 of eye. the lines and edges as of such the optical images and retinal in componentsinterest of features the locate to used was minimization energy active for algorithm programming dynamic discrete time-delayed The Lakshminarayanan;Waterloo,Canada.Univ.of Components, Image Ocular of Detection for Model Contour Active JTuA49 and hyperopes inour study. original myopes of vision the in difference a caused targets various subjects. Results indicate that multivergence LogMAR chart at infinity was used to test the vision of of New South Wales, Australia. A unique holographic Avudainayagam, Kodikullam V. Avudainayagam; Univ. VisionTest, to Infinity True at Chart LogMAR Holographic JTuA48 including of steepening. self effect the cubic nonlinearity. Further, we numerically solved it with metamaterials nonlinear type Kerr in pulses few-cycle and sub- for field electric real in equation India. ilesh Kumar Mishra; Indian Inst. of Technology Delhi, materials with Cubic Nonlinearity , Modeling of Ultrashort Pulse Propagation in Meta- JTuA47 mask.tion and of pulse energy the spectral-phase by measuring the plasmon absorption band as - func 1 HAuCl of reduction two-photon-induced via nanoparticle productiongoldof study the work weBrazil. this In donça; Inst. de Física de São Carlos - LeonardoUniv. de Boni, Linode Misoguti,São CleberPaulo, Renato Men - Marcelo Gonçalves Vivas, Jonathas de Paula Siqueira, Nanoparticles, Gold of ReductionTwo-photon-induced the of Study JTuA46 vasa Varadharajan vasa Univ. of Waterloo, Canada, The effect of interchanging the background and We present 4 . The nanoparticle formation was monitored , Chitralekha S. S. Chitralekha Nguyen , H. Nicholas Mahalakshmi Ramamurthy Mahalakshmi a generalized nonlinear evolutionnonlinear generalized a 2 , Yamuna, Devi Paulo Henrique D. Ferreira, D. Henrique Paulo , Vasudevan Thapa , Damber 2 Elite School of Optometry, 2 , Sarasa MohanSarasa , Ajit Kumar 1 , Srini- , , Akh , 2 - ;

China, tion Multiple-image Optical Compression and - Encryp for Structure Time-frequency RMS the Using JTuA51 experiment has proved validity the of method. this achieve absolute angle measurement. The theory andalso can method This presented. is interference small-angle measurement based on laser self-mixing high-precision for method effective but simple A JinanUniv.,Chen; Zhen Chen, ChunChina. Qi, Pan InterferenceSelf-Mixing , Laser on Based Measurement Small-Angle High-Precision JTuA55 presented. be also will resonance power-broadening-free to approach induced transparency. Theoretical model for a general demonstrate it using a system of electromagnetically experimentally and resonance, broadening-free power-achieve to Wetechnique USA. FM a suggest Xu Power-Broadening-Free, Spectroscopy forTechnique Modulation Frequency Laser JTuA54 paraffin-coated cell. comparablecells gasbuffer coherence the in to time a demonstrate and calculation density-matrix a ent coated cell and buffer gas cells of same size. We pres- Poland. Lab,Photonics andKraków-Berkeley AtomicPhysics JointWojciechGawlik;Budker, Dmitry Acosta, M. ParkKyu in Paraffin-coated Cells snd Buffer Gas , Cells Rotation Magneto-Optical Amplitude-modulated JTuA53 pulse trains with different relative delays. generated the interference signal between two pairs of modes of a short pulsed. The modified optical pulses frequency repetition of parts high-frequency select Tokyo,Japan. Takamasu,KiyoshiMatsumoto;Univ.Hirokazuof Fiber Laser Mode-locked a of Modes Repetition frequency High- Using Measurement Distance Absolute JTuA52 cupy same areas. - oc spectra their where case the in even encryption and compression optical multiple-image for used criterion spectral a of performance good the show France, 1 , Pengxiong Li Pengxiong , , Ayman Alfalou We compare AMOR signals in a paraffin- a in signals AMOR compareWe 2 2 Nanjing Univ.,NanjingChina, UBO, France. UBO, , Afrooz Family, Szymon Pustelny,VictorFamily, Szymon Afrooz , , Narin Chanthawong We develop a Fabry-Perot etalon to etalon Fabry-Perot a develop We 1 , , , 1 , Chritian Brosseau , Chritian YanhongXiao In this communication we communication this In 3 Univ. of Arkansas, Arkansas, of Univ. , Satoru Takahashi, 1 JingangZhong, ; 1 2 Fudan Univ.,Fudan ; Empire Hall,Rochester RiversideConventionCenter 1 ISEN Brest, , Xiwei , Byung Byung JTuA •JointFiO/LSPoster SessionI—Continued FiO/LS 2010 ablation assembly. and InP colloidal quantum dots using the same laser ent a simple synthesis route for obtaining both GaAs L. Carlos pres- will Thomaz, UNICAMP,we work Cesar; this InBrazil. de A. André Pelegati, B. Vitor Dots Synthesis UsingQuantum AblationLaser , Colloidal InP and GaAs Simple JTuA60 over plasmon localized spatiotemporally. localized plasmon at metal nanostructures to control femtosecond of characterizationspatiotemporal the of a spectral interferometry combined with NSOM in Kannari; Keio Univ., Japan. We apply a novel method Matsuishi NSOM with for bined Adaptive Control , Interferometry Plasmon by Spectral - Com calized Spatiotemporal Measurement of Femtosecond - Lo JTuA59 gest may 2Dmodel the not sufficient. be and linear polarization anisotropies in emission sug- considered. Observed defocused interference patterns the optical properties of CdSe-ZnS quantum dots are USA. Wang, M. D. Barnes; Univ. of Massachusetts Amherst, terns, Dots and Correlation with Defocused Emission Pat- PolarizationQuantumAnisotropies Individual in JTuA58 data. experimental observed the of majority the interprets model proposed The observed. is irradiation laser of doze from LII of behaviourNon-monotonical studied. is matrixes incandescence (LII) of carbon microparticles in epoxy Shevchenko Natl. Univ. of Kyiv, Ukraine. Laser-induced Stadnytskyi Valentyn Excitation, Microparticles Laser Pulsed under Carbon Resin Epoxy in of Emission Thermal JTuA57 respectively. helium and nitrogen by shifts, +1.2 and -2.5 and broadening 5.8 and 5.2 measure we torr, per MHz In line. D1 silver of shifts and broadening pressure of measurement the on YaleWeUniv.,report USA. Karaulanov 1 by Nitrogen and Helium, and Nitrogen by Line D1 Silver of Shifts and Broadening Pressure JTuA56 Univ.California,of Berkeley, USA, 2D and 2D+1D dipole models for predicting for models dipole 2D+1D and 2D Austin Cyphersmith, JOINT FiO/LS , Takuya Harada, Jun Oi, Yu Oishi, Fumihiko 1 , Alex O. Sushkov O. Alex , • , Victor Garashchenko; TarasGarashchenko;Victor , October 24–28,2010 Byung Kyu ParkKyuByung A. Maksov, J. Graham, Y. 2 , Dmitry Budker Dmitry , Diogo Diogo B. Almeida, 2 Dept. of Physics,ofDept. Keiichiro Keiichiro 1 , Todor, 1 ; with electron acceptor PC acceptor electron with blended PFPDT and PFDCN, PFDCNIO,polymers side-chainconjugated donor-π-bridge-acceptor in gapHOMO-LUMO decreasing of function a as USA. ington, stable locking and line width of laser ~300kHz. duced dichroism in atomic vapor. The setup achieves in- magnetically and absorptionsaturated on based opticalsystem for lockingoflaser frequency diode a David C. Hall; Goucher College, USA. We present an Dichroism, Induced Magnetically Doppler-Free on Based Locking Frequency Laser Diode Simple JTuA65 ionized to produce avelocity-tunable ion source. photo- is atoms of beam slow The (LVIS). Source trap (MOT) modified to create a Low Velocity Intense strontium ion source consisting of a magneto-optical Durfee; Brigham Young Univ., USA. We present a cold JamesArchibald,L. Christopher J.Erickson,Dallin S. Source, Ion Strontium Cooled Laser JTuA64 and two-step excitation process. absorption two-photon by recorded were Gratings pulses. laser femtosecond shaped of amplification applicationfortwo-wavemixing ofpulses laser ond Hayden Felipe A. VallejoFelipeA. , Cells Solar for Polymers Side-Chain Acceptor Donor-π-Bridge- in Transfer Dynamics Charge JTuA61 formation in Fe:LiNbO Univ.,Japan.KeioKannari; fication, Maryland Baltimore County, USA, County,BaltimoreMaryland Pulses in Fe:LiNbO in Pulses Grating Formation with Shaped Femtosecond Laser JTuA63 positive-P and Q-representation. in those with compared are and function Wigner using studied are oscillators parametric optical the of fluctuations phase and quadrature Field USA. SurendraPuli, Singh, and Q-representations, Field Fluctuations of the OPO in Wigner, Positive-P, JTuA62 optical-pump THz-probe spectroscopy. 1 , Hin-Lap YipHin-Lap , , Yu Oishi, FumihikoOishi, Yu Kabir , Masudul Md. We report charge transfer dynamics transfer charge report We 1 , PaulCunninghamD., 3 forTwo-wave AmpliMixing- Reeta VyasReeta Univ.; Arkansas,of 3 crystals by 800 nm femtosec - 2 William Rawlinson, Harish G. , Alex K.-Y. JenK.-Y.Alex , We investigate grating investigateWe 70 BM measured using measured BM 2 Univ. of WashUniv.of- 1 ay Lyon Mary , L. MichaelL. , 2 ; 1 Univ. of of Univ. , to sweep direction and relative optical phase. beyond our previous work and show strong sensitivity rapid passage on two-level atoms have been extended adiabaticby forcesproduced optical large of studies NumericalUniv.,HaroldBrook Metcalf;StonyUSA. Passage, RapidAdiabatic by Produced Forces Optical in Effects Dynamic JTuA66 Daniel Stack Daniel , JohnElgin,, Tuesday, October 26 61 October 24–28, 2010 NOTES • FiO/LS 2010 ______Tuesday, October 26 62 STuC1 •1:30p.m. Presider to Announced Be STuC •AshkinSymposiumI 1:30 p.m.–3:30p.m. STuC2 •1:55p.m. . Univ., USA.Abstract not available. Announced, Be to Title mentioned. be will lasers. Recent work on highly efficient solar using collectors particles neutral small of manipulation and brief survey of work on the subject of optical trapping USA. Labs, Alcatel-LucentBell Lasers, Using Particles Neutral Small of Manipulation Trappingand Optical Hyatt Regency Rochester JOINT FiO/LS Grand BallroomD ; StanfordBlock ; M. Steven Invited Invited This talk will give a give will talk This Arthur Ashkin Arthur ; segmented or continuous-surface types. either of mirrors deformable by defined are that through successive suppression of aberration modes approachmulti-resolution a in wavefronts optical of correction andmeasurement the forpresented is technique A USA. LLC, Alethus Spivey; Christopher conventional Michelson interferometer. a with compared measurements phase-change and displacementimproving information phase and spatial provides pattern intensity varying spatially ence of radially and azimuthally polarized beams. The demonstrate a new interferometer based on interfer man PolarizationInterferometer Radial , •2:00p.m. FTuO3 of vortex detection are shown. results Experimental detection. of method potential vortex adapted an and sensor wavefrontHartmann in atmospheric turbulence conditions, using a Shack- experiments are carried out to detect optical vortices, Laboratory Ireland.Galway,Ireland, Univ. of Natl. phy Mirror-Based Aberration Modes, Aberration Mirror-Based of Suppression through Wavefront Correction •1:30p.m. FTuO1 USA, Presider Jannick P. Rolland; Inst. of Optics, •GeneralWavefrontFTuO Issues 1:30 p.m.–3:15p.m. a Shack-Hartmanna Wavefront , Sensor Vortices ofOptical Detection Experimental Using •1:45p.m. FTuO2 , Daniel Burke, Nicholas Devaney, Chris Dainty; Chris Devaney,NicholasBurke, Daniel , , Uriel Levy; Hebrew Univ. of Jerusalem, Israel.We Highland B Feiling Wang Feiling Gilad M. Ler M. Gilad Kevin Mur Kevin FiO/LS 2010 - - - , FTuP1 •1:30p.m. FTuP1 the III-V/SOIthe material platform is discussed. wellintermixed andonDFB microlasers lasers ring tion. The realization of silicon AWG lasers, quantum integra- III-V/SOI the realize to used is technology bonding enhanced plasma oxygentemperature low for inter-chip and intra-chip optical interconnects. A suitable lasers, ofdemonstration the forintegration heterogeneous (SOI) silicon-on-insulator on III-V Univ. of California at Santa Barbara, USA. Di Liang, Hui Wen Chen, Martijn Heck, IntegratedCircuits, Photonic for Si and III-V of Integration Hybrid Yingyan Huang Yingyan Integrated Circuits, Electronic-photonic in Applications WDM for Grating Super-compact with Laser Silicon/III-V •2:00p.m. FTuP2 Lucent, USA,Presider Inuk Kang; Bell Labs, Alcatel- •NovelHybridIntegrationI FTuP 1:30 p.m.–3:30p.m. 3 1 Lee power of 2.35mW. lasing threshold is 150mA giving a maximum output grating suitable for WDM applications in EPICs The diffraction curved super-compact ultra-large-angle heterogeneously integrated Si/III-V laser based on an NorthwesternUniv.,a Wedemonstrated have USA. Data Storage Inst., Singapore,Inst., Storage Data 1 , YunanZheng , 2 , Yongming, Tu • Highland C 3 , Boyang Liu Boyang , Yadong Wang Geza Kurczveil, Geza Siddharth Jain, October 24–28,2010 Invited 3 , Doris Ng Doris , 2 2 OptoNet Inc, USA, USA, Inc, OptoNet , Seng-Tiong HoSeng-Tiong , 1 , Yongqiang Wei John ; Bowers 1 We review , CheeWei, 1,3 FiO 1 ; , Abstract not available. tal Waveguides, Strong Localization by Disorder in Photonic - Crys Felix Dreisow FTuQ1 •1:30p.m. FTuQ1 Nolte at San Antonio, USA,Presider Andrey A.Chabanov; Univ. of Texas Optical DevicesandCircuitsI •DisorderinIntegrated FTuQ 1:30 p.m.–3:30p.m. 2 Lattices, WaveguideAmorphous in Gaps Band Photonic •2:00p.m. FTuQ2 are always more localized. Anderson states, but defect states residing in the gap of comprise bands Here, diffraction. Bragg lacking exhibitingband-gap andnegative mass,yet effective lattices photonic amorphous experimentally, and Germany.AppliedPhysics, Courant Inst. of Mathematical Sciences, USA, 3 , Mordechai Segev Mordechai , Alexander Szameit Alexander 3 , , Matthias Heinrich Frank Vollmer Highland D 1 ; Invited We present, theoreticallyWe present, 1 Solid State Inst., Israel, Israel, Inst., State Solid 1 , Mikael C. Rechtsman ; Harvard Univ., USA. 3 , , Robert Keil 3 3 , , Stefan Inst. of 2 , intensity facilities that laser are using them. these techniques and show several examples of high- advantagesillustrate the of will differentwesystems techniques and also non-linear techniques. Through amplifiers. We will lineardescribe passive and active differentcompensationfordispersiontechniques in France. Systems, Optical Dispersion Management in Laser Amplifier FTuR1 •1:30p.m. FTuR1 a consultant Systems. for Laser Thales the project and the associated diagnostics. She is also compressorstretcherresponsibleandof the for part is and project ILE the on works she Currently sors. on new gratings techniques for high energy compres- PW class laser in Nd:Glass amplifiers and she worked with a CNRS position and was the project leader of a LULI the joined BLANC LE Catherine 1999 fiers.In ampliSapphire- Ti in shaping pulse on Barty Chris at San Diego in the Kent Wilson group, working with University the California ofin time some spent also tems, OPAs, and 10-Hz, 100-TW Ti:S amplifiers. She several ultrashort laser sources such as kHz, TW sys- she joined LOA as a Research scientist and worked on ratoired’Optique Ph.D.Appliquéeher (LOA). After first Terawatt Ti:Sapphire systems,laser at- the Labo technique in 1993, in laser Physics, building one of the PolyEcole - Ph.D.from her Orsay. receivedSud She Paris Universitéde the from graduated She France. Versailles, in 1966 in born was Blanc Le Catherine Natl. Lab, USA,Presider Csaba Toth; Lawrence Berkeley Amplifiers Laser •DispersioninUltrafast FTuR 1:30 p.m.–3:30p.m. In this tutorial we will give an overview of overview an give will we tutorial this In Catherine LeBlanc Catherine Highland E Tutorial ; École Polytechnique, Polytechnique, École ; Tuesday, October 26 63 ; 2 We Miles Miles , Jacquiline 1 , Stephen Barnett 1 , , Barry Jack 1 Invited Invited Controllably Controllably entangling Univ. of UK. Univ. Strathclyde, 2 Andrew Andrew G. ; White of Univ. Highland K Highland , Jonathan Leach , Sonja Franke-Arnold 1 1 Univ. of UK, Univ. Glagow, 1 1:30 p.m.–3:15 p.m. 1:30 p.m.–3:15 II • Nonlinear Optics LTuG USA, Univ., Duke Gauthier; Daniel Presider LTuG2 • 2:00 p.m. LTuG2 Romero show show spatial light (SLM) modulators can be used to measure optical modes with a selectivity sufficient to reveal their quantum correlations. SLMs can be updated at video rates allowing rapid switching states. between measurement Padgett Quantum Information and Nonlinear Optics: at Together Last? Queensland, Australia. single photons is the key requirement for photonic quantum information. We review solutions to this through nonlinearity no from range problem_which to full cavity-QED_and recent progress which - sug be enough. may modest nonlinearities gests Spatial Light Modulators: A Tool for Measuring the Measuring for Tool A Modulators: Light Spatial Quantum Entanglement of Spatial Modes, LTuG1 • 1:30 p.m. LTuG1 - ; Poly ; Cornell Stephen Arnold Sudeep Sudeep Mandal Invited Invited LS Highland J Highland Reactive Reactive Sensing Principle (RSP) in Optically LTuF2 • 2:00 p.m. LTuF2 1:30 p.m.–3:30 p.m. 1:30 p.m.–3:30 the Near- • Optofluidics in LTuF Field I USA, Univ., Cornell Erickson; David Presider LTuF1 • 1:30 p.m. LTuF1 Abstract not available. not USA. Abstract Univ., Title Title to Be Announced, The Resonant Biosensing and Nanoparticle Trapping within a WGM Carousel, We will discuss USA. We Univ., York New of Inst. technic our current understanding of the interaction of the near-field of a WGM resonator with nanoparticles and show how size, particle-resonator proximity, interaction-potentials, and plasmon enhancements the RSP. using experiments extracted from are , - - 1,2 , S. , V. V. , 1 7 , M. 1 Lawrence 4 , Philip H. 1,2 , M. F. Kling , M. F. , I. Grguras 1 3,4 , N. Rohringer N. , , Joe Farrell P. 5,6 1,2 Eleftherios Gouliel High High harmonic spec- Argonne Argonne Natl. Lab, USA, 5 Lawrence Lawrence Livermore Natl. Invited Invited 7 , T. Pfeifer , T. Max-Planck-Inst. für - Quan Max-Planck-Inst. 1 1 October 24–28, 2010 Dept.s Dept.s of Physics and Applied ; , R.Santra , , Limor S. Spetor 2 1,2 3,4 1,2 Ludwig-Maximilians-Univ., Ger Ludwig-Maximilians-Univ., 2 , M. Th. Hassan 1 • Highland H Highland PULSE Inst., SLAC Nat. Acc. Lab and and Lab Acc. Nat. SLAC PULSE Inst., Markus Guehr 1 ; 1,2 We demonstrate triggering demonstrate and real-time We , F. Krausz , F. , Z- H. Loh H. Z- , , Z. Zherebtsov 2 3,4 1,2 Univ. of California at Berkeley, USA, Berkeley, at California of Univ. , A. Wirth 3 1 Univ. of Univ. Chicago, USA, R. Leone Stanford Univ., USA, Stanford Univ., Bucksbaum Yakovlev LTuE1 • 1:30 p.m. LTuE1 Berkeley Berkeley Natl. Lab, USA, 6 1:30 p.m.–3:30 p.m. 1:30 p.m.–3:30 and Strong • Attosecond LTuE I Field Physics Berkeley Lawrence Gessner; Oliver USA, Presider Lab, Natl. Physics, Physics, Stanford USA. Univ., and atomic about information rich contains troscopy molecular electronic structure. The combination of HHG studies with grating transient multiple-orbital structure electronic monitoring for allow techniques processes. relevant chemically during change Schultze LTuE2 • 2:00 p.m. LTuE2 Brian K. McFarland tenoptik, Germany, Germany, tenoptik, Lab, USA. Lab, atoms in motion electron valence-shell of observation and we discuss the basic attosecond technologies that enable complete control of electron dynamics the nanoscale. at many, Attosecond Physics: Real-Time Tracking of Valence Valence of Tracking Real-Time Physics: Attosecond Electron Motion in Atoms, Probing Electron Dynamics by High Harmonic Generation, makis FiO/LS 2010 Charles Santori, Paul E. Paul Santori, Charles Invited , Roland Probst, Probst, Roland , Ropp Chad ; Univ. Federal do Rio de Janeiro, Highland G Highland Kai-Mei C. Kai-Mei Fu, , We We find an analytical lower bound for the The optical properties of nitrogen-vacancy cen- nitrogen-vacancy of properties optical The FTuT3 • 2:00 p.m. 1:30 p.m.–3:30 p.m. 1:30 p.m.–3:30 FTuT and Quantum Information • IV Communications UK, Bristol, of Univ. G. Rarity; John Presider FTuT2 • 1:45 p.m. Photon Single of Nano-manipulation Deterministic , Integration for Sources Li, Linjie John T. Zachary Rakesh Kumar, Cummins, Benjamin Waks, Edo Raghavan, R. Srinivasa Fourkas, of USA. Maryland, Univ. Preselected Shapiro; single photon sources are positioned and immobilized to nanometer precision using flow control and local important find could technique This polymerization. in applications integration of single photon sources devices. quantum for structures nanophotonic with FTuT1 • 1:30 p.m. Engineering Nitrogen-vacancy Centers near the Surface of Diamond for Coupling to Optical Mi- crocavities Barclay, Raymond Beausoleil; Hewlett-Packard Labs, Raymond Beausoleil; Hewlett-Packard Barclay, USA. diamond of surface the from nanometers created ters of the Deterministic charge control investigated. are state is demonstrated and recent progress toward presented. is cavities to centers single coupling Quantum Quantum Limits to Lossy Optical Interferometry, Luiz Davidovich Brazil. phase shift estimation uncertainty in lossy optical interferometry, which implies that it scales - asymp totically with the number of photons at best as the limit. noise shot , , - 1 1 FiO Rolf Rolf B. Saager , , Kristen M. Kelly 2 Optical methods are Modulated Imaging, Inc., Imaging, Modulated 2 Invited Beckman Beckman Laser Inst., of Univ. 1 ; 1 Highland F Highland , Steven Saggese , Benjamin R. Giesselman, Soumya 2 California at California Irvine, USA, FTuS1 • 1:30 p.m. 1:30 p.m.–3:30 p.m. 1:30 p.m.–3:30 FTuS Therapy • at California of Univ. Choi; Bernard USA, Presider Irvine, USA. A LED based spatial frequency domain - imag ing (SFDI) system has been developed to provide personalized photodynamic therapy for BCC. We present the instrument design, validation of per formance and initial characterization of wide-field BCC. of properties FTuS2 • 2:00 p.m. A LED Based Spatial Frequency Domain Imaging Therapy Photodynamic of Optimization for System of Basal Cell Carcinoma (BCC) Anthony Anthony J. Durkin David David J. Cuccia used widely in PDT. Spectroscopy of photosensitizer photosensitizer of Spectroscopy PDT. in widely used fluorescence and tissue optical properties has been - imag Molecular trials. clinical human into integrated host and expression gene of visualization enables ing . vivo in cell responses Mitra; Univ. of Rochester, USA. of Rochester, Univ. Mitra; Optical Imaging and Spectroscopy in - Photody Applications, Clinical and Research Therapy namic Thomas Foster Tuesday, October 26 64 STuC4 •2:45p.m. STuC3 •2:20p.m. namics of optically trapped objects. and also has a surprising influence on the - thermody machines, all-optical drive to harnessed be can that component solenoidal a includes trap optical an by vid G. ; Grier New York Univ., USA. Bell Labs, USA.Abstract not available. Non-conservative Forces in Tweezers,Optical Title to Be Announced, Continued STuC •AshkinSymposiumI— Hyatt Regency Rochester JOINT FiO/LS Grand BallroomD James P. Gordon James Invited Invited The force exerted ; Consultant, Da - UK, Miguel Alonso Miguel Alasdair C. Hamilton field behind METATOYs. behind field be wave-optically forbidden. Here we study the wave to appear that fields light-ray create can that sheets propagation with 3-Dcaustic. their and study their intensity shift and invariance through relation to rays and geometrical wavefront aberrations the non-diffracting Airy beams: we unveil their exact of description optics geometric a presentWe USA. Issues—Continued •GeneralWavefrontFTuO Univ. of Rochester,USA, Univ.of Wave Optics of METATOYs, •2:30p.m. FTuO5 ohe Vo Sophie , Beams Airy of Description Optics Geometric A •2:45p.m. FTuO6 through an arbitrary angle around an arbitrary axis. rays light of direction METATOY the rotatesa that ofstructure the rays. lightHere describe we of) tion direc - the (change “refract” that sheets transparent Univ.Glasgow,UK. of; Courtial K. Hamilton,C. Sundar,Bhuvanesh Alasdair Axes, Arbitrary Rotationaround Light-Ray Local •2:15p.m. FTuO4 2 Masaryk Univ., Czech Republic. METATOYs are 1 , Kyle FuerschbachKyle , 1 Jnik Rolland Jannick , Highland B 1 , Tomáš Tyc 2 Optical Res. Associates, Associates, Res. Optical Johannes K. Courtial 1 , Kevin Thompson Kevin , 2 ; 1 ; 1 Univ. of Glasgow, METATOYsare 1 Inst. of Optics, Optics, of Inst. Johannes Johannes FiO/LS 2010 2 1 , , Innovations, LLC, USA.Abstract not available. toward Large Scale Integration,toward Scale Large Eye an with Integration Photonic Active-Passive Yingyan Huang Yingyan current density of 2.8kA/cm layer. A continuous-wave laser with silicona lasing the threshold in defined reflector right-angled-wedge cally pumped Silicon/AlGaInAs evanescent- electri laser with an of results experimental and design the iang Weiiang FTuP4 •2:30p.m. FTuP4 Singapore, Ho Hybrid IntegrationI—Continued •Novel FTuP Retro-Reflector Right-Angled-wedge High-reflectivity with Laser Integrated Heterogeneouly AlGaInAs Silicon/ •2:15p.m. FTuP3 1 ; 1 Northwestern Univ.,USA, Northwestern 2 , Cheewei Lee Cheewei , 3 Wereport Incorporation,USA. OptoNet 3 , Yadong WangYadong , • Highland C , Yongming Tu Yongming October 24–28,2010 2 , Boyang Liu Boyang , Invited 2 is achieved. 2 , Doris Ng Doris , 2 Data Storage Inst.,Storage Data James Jaques 1 , YunanZheng , 3 , Seng-Tiong Seng-Tiong , 2 , Yongq, - ; LGS FiO 1 , Autonoma de Baja California, Mexico, cion Superior de Ensenada, Mexico,Ensenada, de Superior cion Aplicada,Ctr. Investigacionde Cientıfica Educade y - fiber lasers applications. lasers fiber random for suitable is and configurations disorder technique provides an easy way to fabricate different The presented. is disorder controlled with fiber cal theoreticalstudy of light transmission through opti - and Experimental Technology,USA. and Science of Alexey G. YamilovG. Alexey Diffusion in Disordered WaveguidesDisordered in , Diffusion Position-dependent as Localization Anderson •2:15p.m. FTuQ3 the wave-frontthe shaping technique. with optimized be can medium random a through transmission the which over bandwidth frequency the study we simulations numerical Using USA. Yamilov Waveguides, Disordered of Eigenmodes between Correlation Frequency •2:30p.m. FTuQ4 waveguides, eveninpresence of absorption. abinitiosimulations ofwave disorderedtransportin of results the with agreement quantitative in be to shown is coefficient diffusion position-dependent with localizationAndersonof self-consistent theory Milieux Condenses, CNRS, France. Recently developed Modelisationdes et Physique de Fourier,Lab Joseph Puente Fibers , Optical the of Core the in Disorder Controlled of Characterization and Fabrication •2:45p.m. FTuQ5 Univ. of Science and Technology,USA, and Science Univ.of G. YamilovG. Continued Optical DevicesandCircuitsI— •DisorderinIntegrated FTuQ 1 , Elena Chaikina Elena , ; Missouri Univ. of Science and Technology,and Science Univ.of Missouri ; 3 ; 1 Facultad Ingenieria-Ensenada, Univ. Ingenieria-Ensenada, Facultad Highland D 1 , Sergey E. Skipetrov E. Sergey , 2 , Sumudu Herath Sumudu , Ben Payne, Ben 3 Missouri Univ.Missouri 2 Div. de Fısica Ben Payne Ben 2 2 ; Alexey G. Alexey Universite 1 3 Missouri Missouri , Alexey Alexey N. P. N. 1 , the theoreticalthe calculation. results Experimental method. are agreementin with the by measured are laser short-pulse aperture large- typical a in distortion pulse-front of types oninterferometrybased spectral is presented. Three method new A China.EngineeringPhysics, of Acad. lens and crystal. the the relative between changingdistance the by tuned be can SH the of wavelength central the presented; femtosecond pulses focused with diffractive lenses is of generation harmonic second of study A Spain. I, Spain, Omel Mendoza-Yero Méndez of Radio Electronics, Ukraine,Electronics, Radio of Front Distortion Front Pulse- the of Measurement the for Method New •2:45p.m. FTuR4 , (DOE´s) Optics Elements Diffractive and Lasers Ultraintense with Generation Harmonic Second of Description •2:30p.m. FTuR3 Lucio formation is found. shape parabolic nearlyforrequired length fiber and misfit parameter. Optimal conditions for soliton order using calculated was parabolic ideal the from pulses Mexico. The deviation of the shape of quasi-parabolic sion of Nonlinear Fiber, Disper ofFar Field the in Pulses Quasi-Parabolic •2:15p.m. FTuR2 Borrego-Varillas V. ShulikaV. Laser Amplifiers—Continued Laser •DispersioninUltrafast FTuR 2 , Arturo Garcia-PerezArturo , 2 Ctr. de Láseres Pulsados, Spain,Pulsados,Ctr. Láseres de 2 , Benjamín Alonso Benjamín , 1 , Igor A. Sukhoivanov A. Igor , 1 , Javier R. Vázquez de Aldana Highland E , YanleiZuo 3 , Luis Roso Luis , Carolina Romero Carolina Sergii O. Sergii Yakushev 1 , Gladys Mínguez-VegaGladys , 2 ; , Mingzhong, ChinaLi; 2 2 1 Univ. of Guanajuato,Univ.of ; ; Kharkov Natl. Univ. Natl. Kharkov 1 2 Univ. of Salamanca, , Jose A. Andrade- A. Jose , 3 Univ.Jaume 1 1 , Oleksiy , Rocio , 1 , Cruz 3 - , Tuesday, October 26 65 ; Univ. ; of Univ. , David J. Hagan, Eric W. Van Van Eric W. , David Hagan, J. Takayoshi Kobayashi Highland K Highland Scott Webster Jun Jun Liu, LTuG • Nonlinear Optics II— • Nonlinear Optics LTuG Continued LTuG3 • 2:30 p.m. LTuG3 Three-Photon Absorption in Semiconductors, Claudiu M. Cirloganu, Peter D. Olszak, Lazaro Padilha, A. Three-photon USA. Florida, Central of Univ. Stryland; absorption of several semiconductors (ZnS, mea- ZnSe,were InAs) GaAs, CdTe, CdSe, ZnTe CdS ZnO, - analyti existing to Comparisons Z-scans. using sured fits good while inconsistencies produced formulas cal model. 4-band a Kane using obtained are LTuG4 • 2:45 p.m. LTuG4 Tunable Sub-13fs Pulse from Tandem Cascaded Four-wave Mixing in Simple Transparent Glass Media, Japan. Electro-Communications, Multicolored - fem tosecond pulses were generated in glass transparent media using cascaded mixing. four-wave Moreover, the sidebands can be simultaneously amplified and using media bulk transparent another in compressed amplification. parametric optical four-wave , Wuzhou Wuzhou , , Jae-Woo , Jae-Woo 1 2 Univ. of Univ. Calabria,, Italy. 2 , Luciano De Sio Invited 1 École Polytechnique Fédérale Fédérale Polytechnique École 1 LS Andreas E. Vasdekis E. Andreas ; 1 Highland J Highland DemitriPsaltis , Julien R. Cuennet , 1 1 LTuF • Optofluidics in the Near- • Optofluidics in LTuF Field I—Continued LTuF3 • 2:30 p.m. LTuF3 Surfaces Surfaces -defined as interfaces between fluids and solids- can determine the function of optofluidic devices. Examples include monolayers for - birefrin gence control and imaging in microfluidics, near field gain, diffractive or plasmonic structures and membranes. deformable Choi Song de de Lausanne, Switzerland, Surface Optofluidics, Surface

, 1 , S. , 1 Caterina , M. Nisoli M. , 2 Univ. di Padova, Padova, di Univ. 2 , S. De Silvestri De S. , 2 , F. Frassetto F. , 1 Invited ,; Univ. ,; of Univ. USA. Rochester, October 24–28, 2010 , P. Villoresi P. , 1 • Highland H Highland , F. Calegari F. , 1 Xu Wang . We generated broadband continua above above continua broadband generated We . 2 , G. Sansone G. , Politecnico di Milano, Italy, Italy, Milano, di Politecnico 2 1 ; 1 , M. Negro M. , We We exploited a few-cycle, carrier-envelope- 1

LTuE • Attosecond and Strong and Strong • Attosecond LTuE I—Continued Field Physics LTuE3 • 2:30 p.m. LTuE3 Ellipticity Dependence of Nonsequential Double , Ionization Using a classical ensemble method, we predict that (NSDI) probability double ionization nonsequential the expectfrom would one than higher much be can circular and elliptical highly for [1] model recollision polarization. Stagira LTuE4 • 2:45 p.m. LTuE4 150 eV in a two-color scheme. 150 eV in a two-color L. Poletto L. Italy. phase-stabilized IR parametric source for spectral extension of high-harmonics emission. We studied impulsively form HHG in structures HOMO-related CO aligned - Paramet 1.5μm by Driven Harmonics Order High Science, Attosecond for Tool A Source: ric Vozzi ; 2 FiO/LS 2010 Robert - Yoshi , 2 , Kiyomi 1 , Andreas 1 Univ. of Univ. Electro- 1 ; ; 1 , Alexander Szameit 1 Natl. Natl. Inst. for Material 2 , Hideki T. Miyazaki T. Hideki , 1 , Matthias Heinrich 1 Kali Kali Prasanna Nayak Highland G Highland , , Kohzo Hakuta 2 , Stefan Nolte 1 Physics Dept. and Solid State Inst., Technion, Technion, Inst., State Solid and Dept. Physics , Fam Le Kien Le Fam , 2 2 We theoretically analyse the propagation of , Felix Dreisow 1 Inst. of Applied Physics, Friedrich-Schiller-Univ. Jena, Jena, Friedrich-Schiller-Univ. Physics, Applied of Inst. FTuT and Quantum Information • IV—Continued Communications Nakajima Israel. photon pairs in two-dimensional photonic lattices by calculating their number photon and correlation perform classical intensity correlation experiments number photon the for simulator quantum a as acting correlation. Tünnermann FTuT5 • 2:45 p.m. Optical Nanofiber Cavity: a Novel Workbench for , Cavity-QED Keil FTuT4 • 2:30 p.m. - Wave Two-Dimensional in Correlations Quantum , Simulation Classical Their and Arrays guide Communications, Japan, Communications, Germany, Germany, We introduce the realization of optical optical of realization the introduce We Japan. Science, nanofiber cavity by drilling periodic nano-grooves on a sub-wavelength-diameter silica-fiber using focused-ion-beam milling. The strong confinement cavity nanofiber such makes guided-mode in field of cavity-QED. for workbench a promising 1 masa Sugimoto , - 1 FiO Univ. Univ. 2 , Jannick Rol P. 3,1 , Thomas H. Foster; Vitor M. Vitor Schneider, Cristina Canavesi Univ. of Rochester Medical Univ. 3 , Thomas H. Foster H. Thomas , Highland F Highland 2,1 Timothy Timothy M. Baran , , Inst. of Optics, Univ. of Rochester, USA, Rochester, of Univ. Optics, of Inst. 1 ; 1,2 FTuS5 • 2:45 p.m. Design of a Lightpipe Device for Photodynamic Therapy of the Oral Cavity, FTuS4 • 2:30 p.m. Compact Low Energy Fiber Laser Femtosecond Deactivation of Viral Species , O’Malley; M. Shawn Soni, P. Meenal Verrier, Florence Corning, Inc., USA. A compact 1550 nm low used pulse is laser fiber femtosecond doped erbium energy to inactivate viruses via Impulse Stimulated Raman was method this using Inactivation (ISRS). Scattering cells. not selective the virus to and The non-imaging methodology developed methodology non-imaging The USA. Ctr., to design an efficient and compact lightpipe-based device for superficial photodynamic therapy of the oral cavity is reported, together with a study of the the device. of feasibility fabrication FTuS Therapy—Continued • FTuS3 p.m. • 2:15 A New Monte Carlo Model of Cylindrical Diffus- ing Fibers Univ. of Univ. USA. Rochester, We present a new Monte Carlo model of cylindrical diffusing fiber sources in tissue. Differences are shown between our model the of ability predictive the and schemes, simpler and demonstrated. model is of of Central Florida, USA, Florian Fournier Florian land Tuesday, October 26 66 STuC5 •3:05p.m. Inst., USA.Abstract not available. Michelle Wang; Cornell Univ., Howard Molecules, HughesBiological Single Medical of TorsionalStudies Continued STuC •AshkinSymposiumI— ______Hyatt Regency Rochester JOINT FiO/LS Grand BallroomD Invited 2 Issues—Continued •GeneralWavefrontFTuO microscopes, provided information the is sparse. non-optical to applied be can methods The images. features from the measured optical far-field of sparse sub-wavelength of reconstruction the demonstrate Technology,to of sensing compressedIsrael.We use Eldar Szameit Far-FieldImages , Sparse Optical of the from Sub-WavelengthFeatures Reconstructing •3:00p.m. FTuO7 Dept. of Electrical Engineering, Technion - Israel Inst. 3:30 p.m.–5:30p.m. 2 , Mordechai Segev Mordechai , 1 , Yoav ShechtmanYoav , Highland B 3:30 p.m.–4:00p.m. 1 ; 1 1 , Snir Gazit Snir , Solid State Inst., Israel, Israel, Inst., State Solid Meet theEditorsofAPSJournals,Riverside Court, Rochester Riverside Convention Center 1 , Yonina C. C. Yonina , Alexander FiO/LS 2010 Coffee Break,Empire Hall, Rochester Riverside Convention Center ring resonators. electro-optic control and tight bend radii needed for chalcogenide waveguides. This combination provides waveguides vertically coupled to high-index-contrast lithium-niobate of consisting platform optic grated Univ., USA. guides, WaveNiobate - Chalcogenide/Lithium Hybrid FTuP5 •3:00p.m. FTuP5 Hybrid IntegrationI—Continued •Novel FTuP Christi Christi Madsen, Wee Chong Tan; Texas A&M We review recent work on a hybrid inte- • Highland C NOTES October 24–28,2010 Invited FiO Patterson Waveguides, Crystal Photonic in Localization Light and Scattering Multiple Disorder-Induced Stephen Hughes Stephen FTuQ6 •3:00p.m. FTuQ6 coherent scattering and light localization. multipleof regimes highlighting propagationmaps, periments of light transmission and frequency-delay in photonic crystal waveguides.We directly model ex- andanalysisof disorder-induced multiple scattering Res.and Technology, France. Continued Optical DevicesandCircuitsI— •DisorderinIntegrated FTuQ 1 , S. Combrié S. , Highland D 1 ; 1 Queen’sUniv.,Canada, 2 , G. Demand G. , Invited We ourtheory describe 1 , A. De Rossi De A. , 2 Thales Thales M. 2 , ics, Univ. of Rochester, USA, Petawatt-Class Laser Systems, High-Energy,for Compressors Tiled-Grating Large-Aperture of Operation and Development high-energy shots will be presented. shots be high-energy will class system.laser The tiling methods and results on developed and deployed for the OMEGA EP petawatt- (TGA’s), been assemblies have tiled-grating four of USA. Nguyen FTuR5 •3:00p.m. FTuR5 Laser Amplifiers—Continued Laser •DispersioninUltrafast FTuR Two 1.5-m grating compressors, each consisting 1 , D. Canning D. , Highland E 1 , J. Price J. , Invited 2 Helicos BioSciences Corp., 1,2 ; 1 Jie Qiao Lab for Laser Energet- 1 , A. Kalb 1 , T. Tuesday, October 26 67 - We , Sreelatha 1 D.B.Pampa Col D.B.Pampa 1 ; 2 Parameswar Lakshmi , Joseph K. Babu K. Joseph , 2 Highland K Highland India. Vidyapeetham, Vishwa Amrita 2 LTuG • Nonlinear Optics II— • Nonlinear Optics LTuG Continued K. SavithriammaK. lege, India, India, lege, study study the possibility of using solitons for two beam coupling. This process can be modeled using the coupled nonlinear Schrodinger Equations. We also found the soliton solution for this equation under certain conditions. LTuG5 • 3:00 p.m. • 3:00 LTuG5 Two Beam Coupling Using Solitons in Photo Refractive , Media - - Xudong (Sher Xudong Various optofluidic Various ring Invited LS Highland J Highland , Yuze Sun, Jonathan D. Suter, Chung-Shieh Chung-Shieh Suter, D. Jonathan Sun, Yuze , LTuF • Optofluidics in the Near- • Optofluidics in LTuF Field I—Continued LTuF4 • 3:00 p.m. • 3:00 LTuF4 Optofluidic Ring Resonator Lasers, Resonator Ring Optofluidic man)Fan Karthik; Reddy Chinna Balareddy , Lee, Wonsuk Wu, of Univ. Michigan, USA. resonator lasers will be overviewed and their per formance will be compared with other optofluidic lasers. Direct and indirect excitation schemes will be discussed, followed by possible applications and directions. research future October 24–28, 2010 , Chunlei Guo; Inst. of Optics, NOTES • Highland H Highland Linsen Linsen Pei , LTuE • Attosecond and Strong and Strong • Attosecond LTuE I—Continued Field Physics USA. Double ionization and dissociation of CO2 is electronic the that show Studies work. this in studied structure plays a key role for nonsequential double the as similar CO2, molecule, triatomic of ionization molecules. diatomic LTuE5 • 3:15 p.m. LTuE5 Double Ionization And Dissociation Of CO2 Molecule Empire Hall, Rochester Riverside Convention Center Convention Riverside Rochester Hall, Coffee Break, Empire FiO/LS 2010 , P. Fallahi, Riverside Court, Rochester Riverside Convention Center Convention Riverside Rochester Court, Meet the Editors of the APS Journals, Riverside 3:30 p.m.–4:00 p.m. Selman Tunc Yilmaz Highland G Highland , 3:30 p.m.–5:30 p.m. FTuT and Quantum Information • IV—Continued Communications FTuT6 p.m. • 3:00 Optimal Quantum Memory with Hot - Wil Rb of , Atoms College Novikova; Irina , Phillips B. Nathaniel liam & USA. Mary, present an We analysis of pulse electromagnetically of conditions under propagation Rb hot in mixing four-wave and transparency induced investigate theoretically and experimentally We vapor. storage. dual-mode light of the prospect FTuT7 • 3:15 p.m. Electron-Spin Single-Photon Interface in a Quantum Dot A. Imamoglu; Inst. of Quantum Electronics, ETH Zurich, Switzerland. Using resonance fluorescence from a single-electron charged quantum dot with 0.1% collection efficiency, we realize a single spin- photon interface where the detection of a scattered photon projects the electron spin to a definite spin eigenstate. - FiO Temel Inst. of of Inst. /pulse. /pulse. Joshua , Murat 1 Tensile Tensile 3 , Hamit , Hamit 2 Teknofil

1 ; 3 3 ). 2 μm 4 Dept. of Preventive Lab Lab for Laser Ener 3 2 , Peter Rechmann Peter , , Ozgur Tabakoglu 1 , Alphan Sennaroglu Alphan , 3 1,2 Highland F Highland , Wolf Seka Wolf , , Adnan Kurt 1,2 2 Biomedical Engineering Inst., Boğaziçi Univ., Univ., Boğaziçi Inst., Engineering Biomedical Dept. of Physics, Koç Univ., Turkey, Turkey, Univ., Koç Physics, of Dept. 1 2 ; 1 , Nermin Topaloglu , Nermin 1 ______FTuS7 • 3:15 p.m. Tensile Strength Analysis of Laser Skin Welding Performed with Thulium Laser , System Bilici Gulsoy FTuS6 p.m. • 3:00 Selective Near-UV Laser Ablation of Subgingival CalculusAngle, Dental a 20° Irradiation at FTuS Therapy—Continued • E. Schoenly E. and Restorative and Dental Restorative Sciences, of Univ. California USA. The rates removal of average at San Francisco, subgingival dental calculus ablated at 400 nm and 20° are 11±6 μm/pulse and 2.4±0.8×10 Kalaycioglu Turkey, Turkey, Large Large error bars on removal rates reflect biological the calculus. of variability mechanical and LaserLtd. Şti., skin Turkey. welding was performed with a thulium laser system (35 W/cm getics, Univ. getics, of Univ. USA, Rochester, Optics, Univ. of Rochester, USA, of Rochester, Optics, Univ. strength analysis shows that the thulium laser system system laser thulium the that shows analysis strength closure the than welds stronger provided nm 1980 at technique. suture by Tuesday, October 26 68 STuD1 •4:00p.m. Presider to Announced Be STuD •AshkinSymposiumII 4:00 p.m.–6:00p.m. STuD2 •4:25p.m. view beginning in the 1980’s. inthe beginning view personal a present will I introduction, brief a After lasers. tunable of advent the with began cooling of of optical forces comes from Maxwell, the modern era Metcalf Cooling, Laser of History Subjective A man and his many accomplishments. for many years. In this talk I will reminisce about the am fortunate to have worked closely with Art Ashkin Science, His and Man The Hyatt Regency Rochester ; Stony Brook Univ., USA. JOINT FiO/LS Grand BallroomD Invited Invited John BjorkholmJohn Although the notion ; USA. ; Harold Harold I . Murphy F. of functions. powerful suitablemultiplexing, it bringsconvenient a toolbox to addition In telescopes. of network a by delivered beams the combine to instruments think to way France.Grenoble, de Etienne; Lab d’Astrophysique de Grenoble, Observatoire Coherent Signal Combining, Arrays:Telescope Generation Next in Processing Astrophotonics,in Structures Transition Fiber Optical Up: Looking are Fibers ground-based IRastronomy. suppress the atmospheric OH emission that hampers multi-mode and multiple single-mode cores can help single between transitions example, For discussed. transitionsare taper fibreapplications optical nic of Australia. San Diego, USA,Presider Nikola Alic; Univ. of California at •AstrophotonicsI FTuU 4:00 p.m.–5:30p.m. Diez Spain, FTuU2 •4:30p.m. FTuU2 •4:00p.m. FTuU1 2 , Jose L. Cruz JoseL. , 3 Univ.Sydney,of Australia,

4 Recent developments in the astrophoto- the in developments Recent ; 1 Univ. of Bath, UK, Bath, Univ.of Highland B 2 , Sergio G. Leon-SavalG. Sergio , Astrophotonics brings a new a brings Astrophotonics Invited Invited Pierre Pierre , Kern Le Coarer Tim BirksTim 2 4 Univ. of Valencia, of Univ. Univ.Adelaide,of 3,1 1 , Dominic, , Antonio, FiO/LS 2010 presentation. this in emphasized be will transmission WDM and polarization effects for polarization-multiplexed Efficient algorithms toward real-time implementation presented. be will processing signal digital and tion compensationnonlinearitycoherent in usingdetec- fang Li fang Digital Compensation of Fiber Nonlinearities, Gbit/s over distances of 650/2000/3000 km. variable-rate FEC codes yields bit rates of 200/100/50 and (PM-16/8/4-QAM) constellation variable rate, symbol fixed Transmissionusing unavailable. is rate adaptation, extending reach where regeneration Univ.,USA. Stanford Systems,Fiber cal Rate-Adaptive Transmission Techniques for Opti- FTuV2 •4:30p.m. FTuV2 FTuV1 •4:00p.m. FTuV1 Lucent, USA,Presider Inuk Kang; Bell Labs, Alcatel- •OpticalCommunicationI FTuV 4:00 p.m.–5:30p.m. ; Univ. of Central Florida, USA. • Highland C Joseph Kahn Joseph Future networks may employ may networks Future October 24–28,2010 Invited Invited , Gwang-Hyun, Gho; Recent progress Gui FiO - wide Bandgap wide Ultra- with Fiber Crystal Photonic Core Solid •4:30p.m. FTuW2 power delivery. vance the fields of nonlinear fiber optics and infrared This classnew of optical may fibers significantly ad- ofsemiconductor glass-clad field core opticalfibers. USA. Semiconductor Core Optical Fibers, Thomas Hawkins experimentally usingexperimentally apolymer optical fiber. this confirm We octave. an as large as bandwidth uninterrupted an have can inclusions ring-shaped, core microstructured optical with high-index, fibers Australia. Boris T. Kuhlmey, Alexander Argyros; Univ. of Sydney, •4:00p.m. FTuW1 1 Australia, Presider Shahraam Afshar; Univ. of Adelaide, •NovelFibers FTuW 4:00 p.m.–5:30p.m. Burka Clemson Univ.,USA, Clemson This paper will review progress in the nascent the progressin review will paper This 1 , , Stephanie Morris Using a simple model we argue that solid solid that argue we model simpleUsing a , Martijn de Sterke de Martijn Highland D 1 , Paul Foy 2 Northrop Grumman Corp., Corp., Grumman Northrop 1 , Roger Stolen Invited 1 , Colin McMillen , Thomas Grujic, Thomas , 1 John Ballato , Robert Rice 1 , Laura 1 2 ; , attosecond science. pulse) impact of fields the ultrasensitive sensors and (single EnvelopePhase to Carrier andtrains) (pulse Offset Envelope to Carrier of concepts confused combine high temporal and spectral resolution. Often Univ. of New Mexico, USA. Phenomena, Attosecond and Femtosecond Impacts Control Their Phase_How Carrier to Envelope Offset and Carrier to Envelope FTuX1 •4:00p.m. FTuX1 USA, Presider Zenghu Chang; Kansas State Univ., Presider Olivier Albert; LOA, France, Technnology I •AttosecondFTuX Opticsand 4:00 p.m.–5:30p.m. Society of America. Society Optical the of Fellow is He America. of Society cal Opti- the Awardof Engineering in Excellence 2006 the of recipient the and Mexico, New ofUniversity the of Award Lecture Research Annual 51st the of mentored 50 PhD students. Dr. Diels is the recipient and Phenomena) Pulse (Ultrashort textbook one chapters, book 5 patents, 14 papers, refereed 260 publications, invited 90 has HeTexas. Denton, in Professor of Physics at the University of North Texas was Diels Dr. UNM, joining BeforeGermany. gen, InstitutePlanckGottinMaxNetherlands,at- and in staff at Phillips Research Laboratories in Eindhoven, scientific Angeles, Los USC, at Professor Associate at(Professor Berkeley UC E..L.Hahn), and Research Technology Materials.High Hefor served as Center research the scientist at member staff and (UNM) Mexico New of University the at Physics of ment Jean-Claude Diels, Ph.D., is Professor in - the Depart Highland E Tutorial Femtosecond pulse trains ; Diels Jean-Claude Tuesday, October 26 69 , B. B. , 1 , Jon Jon , 1 , Dwight Dwight , 2 Azure Azure , Hansen , Jon P. Davis P. Jon , 1 Inst. for Quantum for Quantum Inst. 3 Naval Naval Air Systems 1 ; 3 Naval Air - Systems Com Naval 1 ; 2 , Sara A. DeSavage A. Sara , Francesco A. Narducci A. Francesco 2 AMPAC, USA, AMPAC, 2 Highland K Highland Widener Univ., USA. Widener Univ., In this work, we 2 Francesco A. Narducci Francesco , George R. Welch 2 , , Kyle H. Gordon H. Kyle , 1 , Tony AbiSalloum , Tony 2 mand, mand, USA, reveal the physical origin of three resonances that are are that resonances three of origin physical the reveal N- four-level of characteristics observed of root the at pathways excitation Explicit systems. atomic Scheme interest. of the resonances with associated are Science Science and Engineering and Dept. of Physics and USA. In this work we discuss our recent Astronomy, experiments to measure recoil-induced resonances that revealed, in addition to the expected narrow resonance, a much broader resonance that does not models. seem current fit to L. Duncan 4:00 p.m.–4:45 p.m. 4:00 p.m.–4:45 • Laser and Trapping Cooling LTuJ Young Brigham Durfee; S. Dallin USA, Presider Univ., Command, USA, Command, P. D av i s Henry LTuJ3 • 4:30 p.m. LTuJ3 - Atom N-Scheme Four-level in Pathways Excitation icSystems LTuJ1 • 4:00 p.m. LTuJ1 and Transfer Storage of Optical Information in a Spinor Bose-Einstein , Condensate P. Nicholas Bhattacharya, Mishkatul Leslie, Suzanne L. the demonstrate We USA. Rochester, of Univ. Bigelow; and retrieval storage of optical information transfer, in a spinor condensate using a two-photon Raman technique. The stored information is read out by beams. Raman the two of one reapplying LTuJ2 • 4:15 p.m. LTuJ2 Three Laser Recoil-induced Resonance in a , Trap Magneto-Optical , L. Pang, B. Slutsky, J. Invited Invited LS ; Harvard ; Harvard B. Crozier Kenneth We explore We metal-dielectric nano- Highland J Highland Field enhancement from surface plasmon plasmon surface from enhancement Field Shaya Y. Fainman 4:00 p.m.–5:15 p.m. 4:00 p.m.–5:15 the Near- • Optofluidics in LTuI Field II Univ., Cornell Mandal; Sudeep USA, Presider LTuI1 • 4:00 p.m. LTuI1 LTuI2 • 4:30 p.m. LTuI2 Plasmonics Plasmonics for Optical Manipulation and En- hanced Spectroscopy, USA. Univ., structures presents new opportunities for optical spectros- Raman enhanced surface and manipulation nanoparticle on work recent review We (SERS). copy propulsion using surface plasmons, and on high substrates. SERS performance Optofluidic Nano-Plasmonics for Biochemical Sensing, Ptasinski, L. Feng, M. Chen; of Univ. California at San Diego, USA. plasmonic structures for localization and resonant fabrication fields,optical of investigate transmission and integration of optofluidic nano-plasmonic sys- tems and explore their for applications biochemical sensing. ; Univ. Univ. ; Krems Roman We consider collective We Invited Invited October 24–28, 2010 • Highland H Highland - sphotoas the on results recent present We

Matthias ;Matthias Weidemüller Heidelberg Univ., 4:00 p.m.–5:15 p.m. 4:00 p.m.–5:15 in Ultracold • Frontiers LTuH I Molecules UCLA, USA, Presider Hudson; Eric LTuH2 • 4:30 p.m. LTuH2 LTuH1 • 4:00 p.m. LTuH1 Tunable Excitons Tunable in Ordered Arrays of Ultracold Lattices, Optical of Molecules Canada. Columbia, of British excitations of internal energy in ordered lattice. arrays optical of an in trapped molecules polar ultracold can fieldelectric dc external an that demonstrate We excitons rotational of dynamics the modify to used be in an ensemble of closed-shell molecules and - mag molecules open-shell of ensemble an in excitons netic in optical lattices. The systems of proposed simulation here quantum may time-domain for used be thus transfer excitation spin and phenomena localization media. in disordered Dipolar Effects in an Ultracold Gas of LiCs - Mol ecules, Germany. sociation sociation and optical of trapping an ultracold gas of LiCs molecules in low states. rovibrational Inelastic - redis state and analyzed, are collisions atom-molecule observed. is relaxation vibrational by tribution - - FiO/LS 2010 , Mat Stephen Stephen M. There There are eminently Xingyu Zhang , Invited Highland G Highland ; Univ. Strathclyde, UK. Strathclyde, ; Univ. FTuZ1 • 4:00 p.m. 4:00 p.m.–5:15 p.m. 4:00 p.m.–5:15 FTuZ Opto-Mechanics and • II Quantum Measurement USA, Univ., Yale Harris; Jack Presider FTuZ2 • 4:30 p.m. Gyroscopic Optomechanics thew Tomes, Tal Carmon; Univ. of Michigan, USA. We Michigan, of Univ. Carmon; Tal Tomes, thew - originat forces, optical gyroscopic of use the suggest polar circularly of momentum angular the from ing nano-waveguide, bent a inside propagating light ized to facilitate mechanical deformation. Right-handed opposite induce polarizations circular left-handed and displacements. The Engima of Optical Momentum, Barnett photon a of momentum the that arguments reasonable in a medium as than greater or less than its value in Both, course! correct? which is of but free space, - FiO Rui - Jan , Ruhr- 1 1 ; , Nils C. 1 1 , Franco N. , Franco 1 Dept. Dept. of Electrical 1 Inst. of Optics, Univ. Univ. Optics, of Inst. 2 ; 1 We We use a windowed Georg Georg Agricola of Univ. 2 Panomsak Meemon Panomsak , Martin Hofmann 2 , Christoph Kasseck , Edmund Y. Lam Y. , Edmund 1 1,2 Highland F Highland - Photon and Optics of College CREOL, 1 ; 1,2 , Hubert Welp , Kenneth K. Y. Wong 1 2 We have Res. have Lab of Electronics, MIT, USA. We 2 Volker Volker Jaedicke , Kyle H. Y. Cheng H. Y. , Kyle 1 and Electronic Engineering, Univ. of Hong Kong, Hong Hong Kong, Hong of Univ. Engineering, Electronic and Kong, FTuY3 • 4:30 p.m. Optical Doppler Range Dynamic Velocity Variable , Tomography Coherence Univ. Bochum, Univ. Germany, Gerhardt C. Wong ics, Univ. of Central Florida, USA, Florida, Central of Univ. ics, developed a wavelength-swept source based on fiber on based source wavelength-swept a developed mode domain Fourier and parametric amplification locking with increased power and speed to take full disper and enhancement resolution 2x of advantage sion cancellation of phase-conjugate OCT. phase-conjugate of cancellation sion FTuY1 • 4:00 p.m. Enhanced Power and Fast Source Swept for Phase Conjugate Optical , Coherence Tomography Zhu 4:00 p.m.–5:30 p.m. 4:00 p.m.–5:30 FTuY Coherence Tomography • Biomedical of Dept. Wax; Adam USA Univ., Duke Engineering, FTuY2 • 4:15 p.m. Substance Identification in Spectroscopic Optical Coherence Tomograhpy Using Pattern Recogni- tion, Applied Applied Sciences, Germany. Fourier transform in the spatial regime to calculate depth resolved spectra from multilayer absorbing samples. Depth resolved substance identification is algorithm recognition pattern a on based performed spectralusing features. nick Rolland nick We present a present modified USA. algorithm We of Rochester, DOCT phase-resolved will thefor that extend lower maintaining while range dynamic velocity the of limit increase hence and velocity, detectable maximum the range. dynamic velocity detectable the overall Tuesday, October 26 70 dipole moment. magnetic unsurpassed Dy’s to due atom complex electronically this confines MOT The (MOT). trap magneto-optical repumper-free a using atoms Dy STuD4 •5:15p.m. STuD3 •4:50p.m. Atom, Dysprosium, Magnetic Most Trappingthe and Cooling Laser 3-Dcoolingefficient and trapping. demonstrate we states, excited two coupling beams In a MOT with the laser beams along z replaced with scattering between electronically excited atomic states. light using cooling laser exploreLibrary,USA.We Res. NIST P.Phillips; W. Brown, Roger Wu, Saijun Cooling, Laser Multi-Photon We report the first laser cooling and trapping of 5x10 Ho Youn; Univ. of Illinois at Urbana-Champaign, USA. Continued STuD •AshkinSymposiumII— Hyatt Regency Rochester JOINT FiO/LS Grand BallroomD Benjamin Lev Benjamin Invited Invited James (Trey) Porto,(Trey) James , Mingwu Lu, Seo 8

sion of astronomical light by SFG. instrument taking advantage of the frequency conver We propose a new version of high angular resolution France. 6172, CNRS UMRPhotonique, Dept. XLIM Nemanja JovanovicNemanja Ellis Simon Robertson Betters Astronomical Spectrograph Astronomical Array-WaveguideGrating an of Development •5:15p.m. FTuU4 Continued •AstrophotonicsI— FTuU tory, Australia, Australia, tory, of Sydney, Australia,Sydney, of astronomical spectroscopy. multiplexed for devices grating arrayed-waveguide using demonstrator technology on-telescope an for designs and characterisation laboratory a from astronomy.forresults benefits the describe Herewe Germany. Del Rio, A. Tonello, L. Delage, Tonello,L. A. Rio, Del L. Brustlein, S. Ceus, D. Imaging, Resolution High forUsed be Can Generation Frequency SumHow •5:00p.m. FTuU3 3 , Joss Bland-HawthornJoss , Photonic devices offer many potential many offer devices Photonic 3 ; 3 , Roger Haynes Roger , 1 Australian Astronomical Observa Astronomical Australian 2 Macquarie Univ.,Australia,Macquarie Highland B 1,2 , Sergio Leon-Saval Sergio , 4 Astrophysics Inst. Potsdam, Potsdam, Inst. Astrophysics , Jon Lawrence 4 , Anthony Horton Anthony , 3 François Reynaud; François , Nick Cvetojovic Nick , 3 , Gordon Gordon , 1,2 , Chris 3 Univ. FiO/LS 2010 1 2 - - , ,

ing element is varied entanglement when the alignment of the compensat- ofcompensationdeath transition sudden to the and mode dispersion (PMD). We observe non-local PMD polarization- with fibers optical through photons Israel. Brodsky Death, Sudden Entanglement to pensation Dispersion in Optical Fibers: from Nonlocal - Com ModePolarization to Due Disentanglement •5:00p.m. FTuV3 Labs, USA, Labs, Continued •OpticalCommunicationI— FTuV general (and more realistic) hinge behavior. simulatemore generationalso mechanisms,butcan model of PMD. The model reproduces previous PMD model to characterize anisotropic effects in the hinge SUNY at Buffalo, USA. We propose a hybrid waveplate Marzec,Biondini,GinoZachary SystemsTransmission Installed of Dispersion Mode Polarization for Model Hinge Hybrid A •5:15p.m. FTuV4

Wepolarization-entangledofpropagate pairs 1 , Cristian Antonelli Cristian , 2 Univ.dell’Aquila, Italy, • Highland C October 24–28,2010 2 Mr Shtaif Mark , Jonathan Schuster Jonathan 3 Tel Aviv Univ.,AvivTel 3 ; 1 Misha AT&T FiO ; , verse sizeof an continuous axially feature. Rayleigh-Plateau instability sets the minimum the trans- that find Wefiber. optical multi-material a in featuresof reduction size on limits the theoretically and We experimentally Photonics,UCF,studyUSA. F.man Abouraddy Tapering, during Fiber Multi-material a Optical of Core the InstabilityRayleigh-plateau the in of Observation •5:00p.m. FTuW4 mission as 97%was as demonstrated. high , Losses and Spinel Surfaces to Ceramic Reflection Reduce Fiber Glass Chalcogenide of Microstructuring •4:45p.m. FTuW3 sources inprototype microfluidic devices. fibers produced by electrospinning as polarized light- demonstrate the integration of light-emitting polymer we work CNR-Inst.Italy.Nanoscienze, this nano; In , poseo Stefano Pagliara, Alessandro Polini, Dario Pisig- 2 Kung Busse surfaces. surfaces. In the case of multimode As due to the antireflective properties of microstructured of spinel ceramics and chalcogenide glasses and fibers transmission Weenhanced demonstrateUSA. LLC, Sanghera Sources for Microfluidic Systems, Microfluidic for Sources Light Novel Nanofibers: Polymer Conjugated •5:15p.m. FTuW5 FTuW •NovelFibers—Continued FTuW NRL, USA, NRL, 3 2 , Jim NoleJim , , Guillermo Villalobos Guillermo , Catalin Florea Catalin 2 , Ishwar, Aggarwal SoroushShabahang, Joshua Kaufman, 3 Univ. Res. Fundation, USA, Fundation,Univ. Res. 4 , Douglas HobbsDouglas , Highland D ; CREOL,; The College of Optics & 1 , Fritz Miklos Fritz , 2 , Brandon, Shaw 2 , Woohong Kim Woohong , 4 ; 1 GTEC Inc, USA, Inc, GTEC 2 S Andrea Cam Andrea 3 fibers, trans- 1 , Jasbinder , 4 TelAztec 2 , Lynda, 2 , Fred Fred , Ay - - Generation, Generation, Second of Sources Attosecond toward Mirrors: Plasma on Generation Harmonic High-Order Kieffer provide on laser-plasma the interaction dynamics. attosecond light sources and the information resulting they can the of properties the discuss and mirrors, plasma from generation harmonic high-order in France. France, C, Thaury Jean-Pierre Wolf Bruno E. Schmidt tawa, Canada, tawa, Compression with Bulk Material, Pulse IR Cycle Two Sub Stable TowardsCEP •4:45p.m. FTuX2 4 du CEA Saclay,France, CEA du FTuX3 •5:00p.m. FTuX3 atcycles 1.8micron wavelength. 1.9 to down compression pulse enables dispersion anomalous the in glass through propagation linear by followed hollow-fiber a in propagation during and experimentally numerically that self-steepening et Télécommunications,et Canada, INRS, Technnology I—Continued •AttosecondFTuX Opticsand Univ.Switzerland.Genève, de 1

, Paul B. Corkum B. Paul , I will present the two mechanisms involvedmechanisms two the present will I 3 Commissariat à l’Energie Atomique/DAM, l’Energie à Commissariat 1 , Ph. Martin Fabien Quere 3 4 CNRS, Univ. de Bourgogne, France, Bourgogne, Univ.de CNRS, , David M. Villeneuve Highland E 1,2 , Andrew D. Shiner 1 , A. Malvache 2 CNRS-Ecole Polytechnique,CNRS-Ecole 2 Invited ; 1 , H. Vincenti 1 Ctr. Énergie Matériaux Énergie Ctr. Wedemonstrate both François Légaré 2 , R. Nuter 2 2 , Pierre Béjot , Jean-Claude 1 2 , H. George Univ.Ot- of 3 ; 1 Inst. 3 1 1 , , , Tuesday, October 26 71 Highland K Highland ; CNR - Isituto Isituto - CNR ; PietroFerraro LS Highland J Highland Sara Sara Coppola, Melania Vespini, Veronica LTuI • Optofluidics in the Near- • Optofluidics in LTuI Field II—Continued LTuI3 • 5:00 p.m. LTuI3 2-D in Nano-drops of Manipulation and Dispensing and 3-D by Pyro-EHD (electro-hydro-dynamic) Effect, Grilli, Simonetta Paturzo, - ap opto-nanofluidic new A Italy. Ottica, di Nazionale streaming for presented is Pyro-EHD named proach effect pyroelectric through nano-pico-droplets liquid of 3-D and 2-D in Manipulation laser. IR by activated drops atto-Liter with printing liquid and nano-drops demonstrated is - , PatWakim E. Amy Grand Ballroom A and B, Hyatt Regency Rochester Regency Hyatt B, and A Ballroom LS Banquet, Grand October 24–28, 2010 • Highland H Highland Highland H, Rochester Riverside Convention Center Convention Riverside H, Rochester DLS Annual Business Meeting, Highland Highland A, Rochester Riverside Convention Center Convention Riverside A, Rochester OSA Annual Business Meeting, Highland Grand Ballroom E and F, Hyatt Regency Rochester Regency Hyatt F, E and Ballroom Grand in OSA (MWOSA) Tea, Minorities and Women LTuH • Frontiers in Ultracold • Frontiers LTuH I—Continued Molecules rick Zabawa, Amanda Neukirch, Nicholas P. Bigelow; Bigelow; P. Nicholas Neukirch, Amanda rick Zabawa, optical an on will report We USA. Rochester, of Univ. pumping method designed to transfer ultracold of initial distribution an molecules from NaCs polar the enhance to X1Σ+ the in molecules bound deeply ν=0 population. LTuH3 • 5:00 p.m. LTuH3 , NaCs Of Luminorefrigeration Lilac Ballroom North and South, Rochester Riverside Convention Center Convention Riverside Rochester South, and North Ballroom OSA LaserFest Lilac Member Reception, 7:00 p.m.–10:00 p.m. FiO/LS 2010 6:00 p.m.–7:00 p.m. 6:00 p.m.–7:00 p.m. 4:30 p.m.–5:30 p.m. Invited 6:30 p.m.–8:00 p.m. Highland G Highland FTuZ Opto-Mechanics and • II— Quantum Measurement Continued FTuZ3 p.m. • 4:45 Testing Macroscopic Testing Quantum Superpositions, Dirk ; Bouwmeester of Univ. California at Santa available. not Abstract USA. Barbara, - FiO ; Dept. of Biomedical Biomedical of Dept. ; This This tutorial reviews Tutorial Adam Wax Adam Highland F Highland Adam Wax received dual B.S. degrees in 1993, one in one 1993, in degrees B.S. dual received Wax Adam electrical engineering from Rensselaer Polytechnic State the from physics in one and NY Troy, Institute, de- the Ph.D. and Albany, at York New of University in NC Durham, University, Duke from physics in gree Spectroscopy Harrison R. George the joined He 1999. - Technol of Institute Massachusetts the at Laboratory Institutes National the of fellow postdoctoral a as ogy, of Health immediately after his doctorate. Dr. Wax joined the faculty of the Department of Biomedical and 2002 of fall the in University Duke at Engineering currently is as appointed His an associate professor. and scattering light of use the in are interests research of properties biophysical the probe to interferometry cells for both diagnosis of disease and fundamental cell biology studies. FTuY Coherence Tomography— • Continued FTuY4 p.m. • 4:45 Coherence Imaging, Imaging, Coherence USA. Duke Engineering, Univ., coherence imaging approaches for biomedical ap plications. plications. Subjects will include digital holography and optical coherence tomography modalities with functional formation, image of basis on emphasis an applications. biological and extensions Wednesday, October 27 72 copy inalmost acentury. - spectros in development radical most the arguably is photonicmultimode which spectrograph PIMMS the include developments Recent decade. coming the in instrumentation astornomical revolutionize astronomy—will and photonics of interface the at Australia.Sydney, of nomical Instruments, nomical Astro- of Generation New A Astrophophotonics: Joss is a recipient of the 2008 Muhlmann AwardMuhlmann 2008 the of recipient a is Joss Express. Optics of Issue Focus the in featured was field this 2009, Feb in - photonics and astronomy of interface the at sits that astrophotonics of field new the proposed he 2002, In communications. laser interplanetary and gratings filters, tunable on work pioneering out carried has JossHoneycomb. Starbugs, Dazle, Shuffle, & Nod like names with conceptsastronomical pioneered that group cessful suc- highly a of Head was he where Observatory and Texas. In 1993, Hawaii he in moved appointmentsto the faculty Anglo-Australian up taking to prior astrophysics from the Royal Greenwich Observatory instrumentation.in in obtainedPhDhe hisIn 1986, renownedfor breakthroughshis astrophysicsin and world is and papers, research 200 over has Joss ics. University of Sydney where he is a Professor the of Physat- Fellow Federation a is Bland-Hawthorn Joss FWA1 •8:00a.m. Presider Tim Birks; Univ. of Bath, UK, FWA •AstrophotonicsII 8:00 a.m.–9:45a.m. Highland A Astrophotonics—which lies Astrophotonics—which Joss Bland-Hawthorn Joss Tutorial ; Univ.; not available. MartinJ. Leahy Univ.; ofLimerick, Ireland. Imaging, Tissue Deep for Challenges Sensor spectroscopy and autocorrelation analysis. dark-field inexpensive using range spectral visible is demonstrated by protein monolayer sensing in the arrays aperiodic deterministic of shifts spectral and technique based on distinctive colorimetric signatures Univ., USA, Fiorenzo G. Omenetto G. Fiorenzo Res., USA,Presider Jonathan A.Nagel; AT&T Labs- FWB •BiochemicalSensing 8:00 a.m.–10:00a.m. FWB1 •8:00a.m. vanus Y. Lee ministic Aperiodic Metal Nanoparticle Arrays, Biosensing with Colorimetric Signatures of Deter FWB2 •8:30a.m. 2 1 Tufts Univ., USA. , Jason J. Amsden Highland B 2 , Luca Dal Negro Dal Luca , Invited 7:00 a.m.–5:30p.m. 2 A novel optical sensing , Svetlana V. Boriskina Svetlana , 10:00 a.m.–4:00p.m. 1 ; Abstract 1 Boston Boston Syl FiO/LS 2010 1 - - , will be presented. be will them ofapplications.some of many useful review A finding is 2003, in formulated light, of polarization Rochester, USA. PolarizationandLight, ofence Some Applications of the Unified Theory of Coher FWC1 •8:00a.m. around world. the recipient of seven honorarythe degrees is from universitiesHe Australia. and India, 1978), in President ofof the Optical Societies America (of which he was member honorary an contributionsis and scientific Wolfsor recipient the numerousofis awards forhis review articles on optics and related subjects. Profes- of Progress in Optics, an ongoing series of volumes of Coherence and Polarization of Light. He is the editor He is also the author of Introduction to the Theory of Mandel, of Optical Coherence and Quantum Optics. Optics, now in its seventh edition, and with Leonard of Principles book well-known a of Born, Max with published more than 400 papers. He is the co-author, Heoptics. physical in areester.researches main His and also Professor of Optics at the University of - Roch Emil Wolf is the Wilson Professor of Optical Physics Univ. of Arizona, USA,Presider LLC and College of Optical Sciences, JohnR. Koshel; Photon Engineering Unconventional Polarization I FWC •OpticalDesignwith 8:00 a.m.–10:00a.m. Registration, Galleria, Rochester Riverside Convention Center Exhibit Open,Rochester Riverside Convention Center The unified theory of coherence and • Highland C FiO October 24–28,2010 Tutorial Emil WolfEmil Univ.; of - distributed-feedback lasers in Al in lasers distributed-feedback narrow-linewidth and C-band, telecom the across Gbit/s data transmission, microring operatinglasers Ridder, K. deWörhoff; M. Univ. R. Bernhardi,of Twente, H. Netherlands.Yang,E. J.Bradley, B. D. J. in AluminaLasers and Polymers, Waveguide and Doped Amplifiers Rare-earth-ion munication wavelengths. telecom- at electroluminescenceroom-temperature efficient achieved we dots, quantum PbS with host heterostructure type-II polyfluorene-basedhybrid a light-emitting diodes integrated on silicon chip. Using polymer-based hybrid of properties optoelectronic Univ.Delaware,; Cloutier USA. of Heterojunctions, II on Silicon Using Hybrid Polyfluorene-based Type- LEDs Polymer-based nm High-Performance1550 FWD2 •8:30a.m. LLC, USA,Presider James Jaques; LGS Innovations, FWD •NovelHybridIntegrationII 8:00 a.m.–10:00a.m. FWD1 •8:00a.m. are presented. silicon on waveguides polymer Nd-doped in lasers on silicon, as well as amplifiers and continuous-wave Highland D Xin Ma, Fan Xu, Fan Ma, Xin Invited 2 O We report on the the Weon report Markus Pollnau, 3 :Er waveguides :Er Sylvain G. G. Sylvain 170 Zenghu Chang Zenghu Gating, Optical Double from Pulses Attosecond Isolated Using Spectroscopy Time-Domain XUV Fleischer Cohen 2 Mexico, USA,Presider Jean-Claude Diels; Univ. of New Technnology II FWE •Attosecond Opticsand 8:00 a.m.–10:00a.m. Driving Laser, Driving Continuous-Wavea of Harmonics High-Order FWE2 •8:30a.m. gallery micro-resonator.gallery whispering a to coupled are that antennas nano of consists device The laser. driving continuous-wave a of harmonics high-order bandwidth ultra-narrow ence of Light, Germany. electron dynamics innoble gas atoms. correlated revealed that continuumconductedwere super the using experiments Transientabsorption generatedwasattosecond byaneV switch. light600 to 20 coveringTemporally spectrum coherentXUV USA. Florida, CentralUniv. of CREOL, and Physics FWE1 •8:00a.m. Univ. of Michigan, USA, 1 ; 1 1 , Tal Carmon Technion-Israel Inst. of Technology, Israel, Technology, of Inst. Technion-Israel 1,2 Maxim Kozlov Maxim ; Highland E 1 Kansas State Univ., USA, 2 We propose a device that emits , Harald G. L. Schwefel 3 Max-Planck-Inst. for the - Sci Invited 1 , Ofer Kfir Ofer , 2 1 Dept. of , Avner , 3 , Oren - Wednesday, October 27 73 Recent Recent

; Emory Univ., USA. Univ., Emory ; Gregory Gregory Scholes, Inchan Invited Invited Tianquan Lian Highland K Highland LWC1 • 8:00 a.m. • 8:00 a.m. LWC1 • 8:30 a.m. LWC2 Inter- Inter- and Intra-chain Electronic Coherence in Conjugated Polymers, Hwang, John Casey; of USA. Univ. Toronto, experimental studies of electronic coherence in chemical and biological systems are summarized. play can transfer energy quantum-coherent role The in long-range light-harvesting in organic solar cells described.is Multi-Exciton Multi-Exciton Dissociation Dynamics in CdSe Dots, Quantum We report studies of ultrafast exciton dissociation dynamics in quantum dots by electron transfer to adsorbed molecular acceptors. Up to three excitons - pho multiple by (generated dots CdSeper quantum be can dissociated. absorption) ton 8:00 a.m.–10:15 a.m. of Energy • Photophysics LWC Conversion I Renewable Natl. Garry Rumbles; USA, Presider Lab, Energy Jun Rym François François We will discuss will We We report a measurement measurement a report We Invited Invited LS Highland J Highland ; École Normale Supérieure, Pierre Univ. et ; JILA, NIST, Univ. of Colorado, USA. Colorado, of Univ. NIST, JILA, ; LWB1 • 8:00 a.m. • 8:00 a.m. LWB1 of of the atomic recoil using atom interferometry and Bloch oscillations. Such a measurement yields to a determination of the fine structure constant with a 4.6 ppb. of uncertainty relative Atoms, Sr Lattice-Confined with Clock Optical of an optical accurate atomic the development latest clock using ultracold Sr atoms confined in a magic wavelength optical lattice, focusing on the progress frequency shift. collisional of in the control Bouchendira, Bouchendira, Malo Cadoret, Estefania de Mirandes, Pierre Cladé, Saïda Nez, Guellati, François Biraben France. CNRS, Curie, Marie Ye Precise Determination of h/M(Rb) Using Bloch Oscillations and Atomic Interferometry: A Mean to Deduce the Fine Structure Constant, 8:00 a.m.–10:00 a.m. and Precision • Metrology LWB Measurements I California of Univ. Budker; Dmitri USA, Presider Berkeley, at LWB2 • 8:30 a.m. LWB2 - - The ; Harvard Univ. Univ. of California at 1 ; Mikhail Mikhail Lukin 1,2 Invited Invited October 24–28, 2010 • Highland H Highland Lawrence Berkeley Natl. Lab, USA. Lab, Natl. Berkeley Lawrence 2 We will We describe our recent theoretical Rochester Riverside Convention Center Convention Riverside Rochester Exhibit Open, Dan Dan Stamper-Kurn Galleria, Rochester Riverside Convention Center Convention Riverside Rochester Galleria, Registration, Hybrid Hybrid Nanophotonic and Nanomechanical In terfaces for Spin Qubits, USA. Univ., and experimental work towards developing novel quantum nanomechanical and nanophotonic hybrid interfaces and quantum transducers for spin qubits techniques these of applications Possible diamond. in will be discussed. Optical Manipulation and Detection of the Col lective Motion and Spin of an Ultracold Atomic Gas, 8:00 a.m.–10:00 a.m. Systems I • Hybrid Quantum LWA Univ., McGill Clerk; Aashish Presider Canada, LWA1 • 8:00 a.m. LWA1 LWA2 • 8:30 a.m. LWA2 Berkeley, USA, Berkeley, interaction of an optical cavity field with the collective the with field cavity optical an of interaction motion or spin of cold atoms allows investigations of cavity and optomechanics novel magneto-optical - theoreti and experimental present will I phenomena. this idea. of cal investigations FiO/LS 2010 ; Univ. ; Xiang Zhang Univ. 10:00 a.m.–4:00 p.m. 10:00 a.m.–4:00 I will discuss recent ex- recent discuss will I 7:00 a.m.–5:30 p.m. 7:00 a.m.–5:30 Invited , Da Huang, David R. Smith; R.Smith; David DaHuang, , We derive theWe expressions for the Highland G Highland EkaterinaPoutrina FWG2 • 8:30 a.m. - Metamateri Electromagnetic Nonlinear of Analysis als, FWG1 • 8:00 a.m. 8:00 a.m.–10:00 a.m. and Gain in FWG • Nonlinearities I Plasmonics and Metamaterials Karlsruhe, Univ. Linden; Stefan Presider Germany, Metamaterials Metamaterials and Symmetry, USA. Berkeley, at California of perimental demonstrations of intriguing phenomena phenomena intriguing of demonstrations perimental These plasmonics. and Metamaterials with associated include new symmetries in metamaterials, negative refraction and Negative-index, cloaking at optical lasers. plasmonic sub-wavelength and frequencies Duke Univ., USA. Duke Univ., effective nonlinear susceptibilities of a metacrystal strongly couple that elements resonant from formed the illustrate experimentally We field. magnetic the to framework. theoretical our accuracy of validity and - FiO The The Kyu , Elisa We We have investigated Sudeshna Sudeshna Pal We demonstrate biological demonstrate We , Seunghyun Kim, Kim, Seunghyun , Nordin P. Gregory Highland F Highland 8:00 a.m.–10:00 a.m. FWF • Biosensing Ryan R. Anderson, Stanley J. Ness, Weisheng Hu, Jong Jong Hu, Weisheng Ness, J. Stanley Anderson, R. Ryan W. Noh, William C. Dahlquist, Danny C. USA. Richards; Univ., Young Brigham designed gold nanoparticle dimer is employed to dark hyperspectral using By DNA. label-free quantify characteristic of measurement the spectroscopy, field spectra shows versatile quantification of label-free concentration. molar atto to up DNA FWF3 • 8:30 a.m. Microcantilever-Based Biologi- of Demonstration - Transduc Photonic in-Plane with Array Sensor cal Mechanism, tion molecule detection with photonic microcantilever array and in-plane photonic detection using the biotin-streptavidin material system and integrated microfluidics. (PDMS)-based polydimethylsiloxane , Joseph Irudayaraj; Purdue Univ., USA. Univ., Purdue wan Irudayaraj; Lee , Joseph FWF2 • 8:15 a.m. Optical Quantification of Label-Free DNA, FWF1 • 8:00 a.m. Nanocavities in Photonic for Label-Free Crystal Biosensing, Waveguides Guillermain, Benjamin L. Miller, Philippe M. - Fau chet; of Univ. USA. Rochester, resonant nanocavities coupled to photonic crystal fabricated are devices The biosensing. for waveguides using electron beam lithography and reactive-ion- etching. Preliminary results demonstrate successful detection of human IgG molecules and refractive sensing. index Urs Utzinger, Univ. of Arizona, Arizona, of Univ. Utzinger, Urs Presider USA, Chair, Wednesday, October 27 74 FWA3 •9:00a.m. Merton Fellow. College the and Oxford to ProfessorVisiting Leverhulme the is he 2010, In Society. Astronomical Royal the fromAward Achievement Group 2008 inaugural the of recipient a astronomy,and experimental for Continued FWA •AstrophotonicsII— applications. Astrophotonicfor detectors these using for pects pros- future and field the of state the summarize will I talk, this In photon. incoming each from information available all extract detectors limited RochesterFiger; Inst. Technology,of USA. Future Detectors for Astrophotonics, for Detectors Future FWA2 •8:45a.m. Abstract not available. Lyon ard CoronagraphyDetection, for Exo-Planetary ; NASA Goddard Space Flight Ctr., USA. USA. Ctr., Flight Space Goddard NASA ; Highland A Invited Quantum- Donald F. F. Donald Rich - effects areeffects investigated. fluidic and optical Both analytes. targeted to forces gradient optical additional providing by system ing the mass transport in a surface microfliudic biosens- plasmonic nano-slits array structures that can change SPR excitation is measured and insensing. used experiments. transmission by supported are results for sensing using transmission mode SPR. Simulation platformstandingmembranes free siliconprovide a USA. David Z. Fang, Philippe M. Fauchet; Univ. of Rochester, Zhu 4 China, China, China, Biosensors, Microfluidic in Limitation Transport Mass the Alleviate to Array Nano-slits Plasmonic On-chip FWB5 •9:15a.m. Biological Biological and Chemical Sensing, forMembranes Porous Ultrathin Metallized FWB3 •8:45a.m. different solution particle concentrations. evolution of mode splitting spectra corresponding to microresonatorwater.a in in We different observed splitting mode using water in nm 50 of radius with nanoparticles polystrene of detection demonstrated USA. Louis, St. Yang;atWashington university Lan He, Lina Zhu,Jiangang Ozdemir,Kaya Sahin Microresonator, Optical An in ting Split Mode Waterby in Detection Nanoparticle FWB4 •9:00a.m. China, Continued FWB •BiochemicalSensing— PennsylvaniaState Univ., USA. 2 , Tao ZhouTao , Metallized ultrathin porous silicon and oxidized 2 Natl.Ctr.NanoscienceTechnologyandfor of Xin Zhao 3 New Jersey Inst. of Technology,of Inst.USA, Jersey New 3 Highland B , Jiangtao Cheng Jiangtao , 1 , Zheng Zheng Wepropose on-chip 4 Krishanu Krishanu Shome ; 1 , Wei Li 1 Beihang Univ., Beihang WoosungKim , 1 , Jinsong We We FiO/LS 2010 - , Full Full Poincaré Beams, FWC3 •9:15a.m. FWC2 •8:45a.m. Univ. of Rochester, USA.Abstract not available. jection Imaging, jection Unconventional Polarization States Applied to Pro- Brown the use of use the astressed window discussed. is also The experimental production of these beams through whose polarizations span the entire Poincare sphere. Finland. Rochester, USA, Continued Unconventional Polarization I— FWC •OpticalDesignwith 1 ,

MiguelAlonso A. We theoretically a familydescribe of beams 2 Dept. of Applied Physics, Aalto Univ., • Highland C Thomas G. Brown G. Thomas FiO Amber M. Beckley October 24–28,2010 Invited 1,2 ; 1 Inst.Optics,ofUniv. of ; Inst.Optics,; of 1 , Thomas G. waveguides of KY(WO of waveguides channel microstructured in achieved was operation Markus Pollnau ; Univ. of Twente, Netherlands. Wörhoff,Kerstin Grivas, Christos Aravazhi,mugam absorption to silicon the photonics platform. and deliver all-optical switching without two-photon ganic coating when vapor-deposited on any substrate, compared to their size create a high optical quality or organic molecules with large third-order nonlinearity Silicon-Organic-Hybrid Systems, for Molecules Optical Nonlinear Optimized output power. mW 76 and power, pump launched versus 62% of efficiency slope mW,a 5 only of threshold a in ing KY(WO In Lasers Waveguide Channel Microstructured FWD3 •8:45a.m. Breiten USA, FWD4 •9:00a.m. Integration II—Continued FWD •NovelHybrid 2 Lab für Organische Chemie, Switzerland. 2 , F.Diederich , 4 ) 2 :Gd 3+ , Lu , Highland D 3+ 2 , , Yb , Ivan Biaggio Ivan 4 ) Invited 2 :Gd 3+ , Dimitri Geskus, Shan- Geskus, Dimitri 3+ Lu , M. L. Scimeca 3+ 1 ; , Yb , 1 Lehigh Univ.,Lehigh 3+ , result- , Small Laser Laser 1 , B. - Attosecond Emission, Attosecond Driven Laser Using Imaging Orbital Molecular Ruchon attosecond-temporal resolution. wavepacket is performed with Ångström-spatial and tomographic reconstruction of the bound electronic- FWE4 •9:00a.m. and focusing attosecond pulses. attosecond square pulses, spatio-spectral Airy beams including characteristics, intrigue exhibits emission wave-mixing with a mid-IR field. The generated X-ray through keV to attosecondpulses ofphoton-energy Technology,Israel.of Inst.Israel Technion - Cohen; Oren Fleischer,Avner Beams, Airy X-Rays Spatio-Spectral Producing Pulses: Attosecond Ultraviolet Extreme Up-Conversionof Frequency FWE3 •8:45a.m. Rayonnement, UPMC Univ., France, trand Carre trand Saclay,France, from small aligned molecules (CO molecules fromaligned small Advanced characterization of the attosecond emission Caillat to their structural and dynamical properties. In N In properties. dynamical and structural their to Technnology II—Continued FWE •Attosecond Opticsand 2,3 1 , T.Auguste, , W.Boutu , 1 , R. Taïeb R. , 2 Lab de Chimie Physique-Matièreet Chimie de Lab Highland E 1 1 , C. Giovanetti-TeixeiraC. , , P.Breger, 2,3 We propose to amplify the amplify to proposeWe , Maxim Kozlov, Kozlov, Maxim , Kfir Ofer , P.Salières , S. Haessler S. Invited 1 , A. Maquet A. , 2 , N , 1 1 ; 3 , Z. Diveki Z. , CNRS, France. 1 2 Inst. du CEA du Inst. ) gives) access 2,3 , 2,3 Ber 1 , T. T. , , J. J. , 2 - , Wednesday, October 27 75 Invited ; Imperial College London, Highland K Highland James R. Durrant My talkMy will address the use optical of transient LWC • Photophysics of Energy Photophysics of Energy • LWC I—Continued Conversion LWC3 • 9:00 a.m. LWC3 Transient Transient Absorption Studies of Charge - Photo generation in Organic and Dye Sensitized Solar Cells, UK. techniques, primarily on the nano- to millisecond timescales, to interrogate photoinduced charge separation in dye sensitized and organic thin films devices. photovoltaic and - We and -18 , C. C. , Rosenband Till , James L. Archibald, Archibald, L. James , optical clocks. Despite + Invited . LS -1/2 (τ/s) Highland J Highland -15 ChristopherErickson We present a strontium ion interferometer for a ion present interferometer strontium We , within the accuracy limit of the older clock. Optical Clocks for Fundamental Physics, Ge- + -17 LWB • Metrology and Precision Metrology and Precision • LWB I—Continued Measurements many many differences, their rates agree to 1.8 +/- 0.7 x 10 odesy, and Quantum Metrology, Metrology, Quantum and odesy, USA. NIST, Wineland; J. D. Hume, B. D. Chou, W. compare the compare rates of two Al LWB3 • 9:00 a.m. LWB3 Precision Metrology with a Strontium Ion Inter ferometer, Mary Lyon, Dallin S. Durfee; Brigham Univ., Young USA. use as an electromagnetic field sensor with - unprec edented sensitivity. Applications include - measure ments of fringing fields, studies of tests image ultra-precise charge and superconductors, in scattering electromagnetism. of Al LWB4 • 9:15 a.m. LWB4 stability near 10 near stability The The newer clock has an accuracy of 8.6 x 10 , , 1 2 , Yifu 2 Jiepeng We report We Georgia Tech, 1 ; 1 , Stewart Jenkins 1 , Alexander G. Radnaev G. Alexander , Long-distance Long-distance quantum 1

, Gessler Hernandez 2 October 24–28, 2010 , Ran Zhao 1 • Highland H Highland , Brian Kennedy 1 Jacob Z. Blumoff Z. Jacob , Xiaogang Wei Physics Div., Los Alamos Natl. Lab, USA, Southampton, Southampton, UK. 1,2 1 2 ; 2 Dept. of Physics, Florida Intl. Univ., USA. Univ., Florida Intl. Dept. of Physics, LWA • Hybrid Quantum LWA Systems I—Continued LWA3 • 9:00 a.m. LWA3 Tunable Broadband White-Light Cavity Using Anomalous Dispersion in Cold Atoms, Zhang Zhu the demonstration of a broadband white-light cavity cavity white-light broadband a of demonstration the of consists that system QED cavity a on based scheme and cavity optical an in confined atoms cold multiple a free-space laser field. by driven coherently 2 Yaroslav Yaroslav O. Dudin Alex Kuzmich information information networks require information storage, retrieval and transmission at telecommunications wavelengths. We demonstrate conversion between 795 and 1367 nm light with efficiency 52% and between measure non-classical correlations telecom memory. and light USA, USA, LWA4 • 9:15 a.m. LWA4 and Light Telecom Between Correlations Quantum Memory, , - - - 2 FiO/LS 2010 Hamidr We We discuss , Ramy El-Ganainy Ramy , 1 Wesleyan Univ., USA, Univ., Wesleyan 1 ; We show that nonlinear nonlinear that show We 2 , Gayatri Venugopal Natalia Highland G Highland We present a hyperbolic metamaterial metamaterial hyperbolic a present We , Tsampikos Kottos Tsampikos , 1 , Zubin Jacob, Guru V. Naik, Evgenii Evgenii Naik, V. Guru Jacob, Zubin , Kim Ji-young Univ. of Central Florida, USA. Florida, Central of Univ. substrate for radiative decay engineering. The sponta The engineering. decay radiative for substrate moleculeslifetime of emission is due neous reduced This metamaterial. the with interaction near-field to fluorescence metamaterial-based for route the opens detection. and sensing FWG • Nonlinearities and Gain in and Gain in FWG • Nonlinearities and Metamaterials I— Plasmonics Continued 2 FWG3 • 8:45 a.m. - Metamate Hyperbolic Near Emission Spontaneous rials, E. Narimanov, Alexander Boltasseva, Engineering/Purdue Vladimir Computer M.and Electrical Shalaev; USA. university, Demetrios N. Christodoulides N. Demetrios FWG4 • 9:00 a.m. Optical Diode, PT-Symmetric Nonlinear ezaRamezani parity-time parity-time symmetric optical structures, can act as unidirectional optical valves. This is possible, by exploiting the interplay between the nonreciprocal induced self-trapping with , propagation parity-time nonlinearities. Kerr by FWG5 • 9:15 a.m. Asymmetric Positive-Negative Index Nonlinear Waveguide Couplers, M. Litchinitser; at Univ. Buffalo, USA. consisting couplers asymmetric in propagation wave of positive and negative index channels with differ ent nonlinear coefficients. We find the dispersion relations, constants of motion and various regimes structures. in such interactions wave of , - 3 FiO NCSR NCSR 3 , Veronica , Veronica Giancarlo , Gualtiero 3 , , Francesco 1 Microoptical Microoptical 1,2 , Georgios Tsek 1 Ctr. Studi Ctr. e Ricerche 2 Sara Coppola , Stavros Chatzandroulis Stavros , , Silvia Soria 3 1 , Maurizio Ferrari We We report the fabrication of IFN IFN CNR, Italy. 1 3 , Christos Pandis Christos , 1 Simone Simone Berneschi Natl. Technical Univ. of Athens, 1 Highland F Highland ; 1 IFAC CNR, IFAC Italy, , Stefano Pelli 1 1 ; 1 Biomedical Res. Biomedical Greece, Foundation, , Franco Cosi 2 1 A new and simple method is presented here for for here presented is method simple and new A

, Panagiotis Dimitrakis Panagiotis , Maria Kandyla Maria 2 FWF5 • 9:00 a.m. Optical Microspherical Resonators for - Biomedi cal Applications, Enrico Enrico Fermi, Italy, FWF4 • 8:45 a.m. - Microprint Laser Direct by Fabrication Biosensor ing, FWF • Biosensing—Continued Baldini Nunzi Nunzi Conti C. Righini microbiosensors by Laser Induced Forward Transfer. Transfer. Forward Induced Laser by microbiosensors Two kinds of biosensors are discussed: capacitive biosensors. amperometric polyaniline and biosensors Laser fabrication allows for low-cost, maskless - pat miniaturization. of the potential with terning Demokritos, Demokritos, Greece. Ioanna Ioanna Zergioti enis Greece, Greece, devices Gallery based Whispering on exhibit Modes peculiar properties, the most notable being a very high quality factor. Here results are presented on the development of an immunosensor based on a glass resonator. microspherical FWF6 • 9:15 a.m. A Pyro-Electrohydrodynamic Nanodispenser for Biochemical Applications, Vespini, Melania Paturzo, Vespini, Simonetta Grilli, Napoli, Pietro of Unit Ottica, di Nazionale Inst. CNR Ferraro; Italy. a through pico-droplets and nano- liquid dispensing non-invasive electrode-less configuration using the into effect pyroelectric the by generated field electric a dielectric crystal. Wednesday, October 27 76 single-mode system.single-mode limited” “near-diffraction a and fibre multimode a between low-loss achieving for behaviour modal its studyWe fibre. multimode a within place take to function photonic single-mode a for allows Australia.Sydney, Univ.of Leon-Saval, Alexander Argyros, Joss Bland-Hawthorn; Lanterns, Photonic in Evolution Mode FWA4 •9:30a.m. Continued FWA •AstrophotonicsII— ______Highland A The “photonic lantern”“photonic The Sergio G. Sergio Hai-Sheng Leong Hai-Sheng on asingle device. plasmoningand surface analysis resonance spectral sens- of combinesfunctions device arraynano-hole super-periodic The sensing. biochemical integrated nano-hole arrayformetallic plasmon surface device Univ.,USA. Resonance Biochemical Sensor, Biochemical Resonance Plasmon Surface Array Nano-hole Integrated FWB7 •9:45a.m. length, Wave970nm - at Applications Biophotonic for Resonator Microring Nitride Silicon Ultra-thin FWB6 •9:30a.m. Continued FWB •BiochemicalSensing— light-mater interaction are presented Optimization parameters for improved sensitivity and favorable for large variety of biophotonic applications. is that 970nm of wavelength at operatingresonator microring nitride silicon ultra-thin an demonstrate Hebrew Univ. of Jerusalem, Israel. Brady 2 ; 1 Ilya Goykhman Ilya Univ.Alabamaof Huntsville, in USA, Wehave demonstrated super-periodica Highland B 1 , Robert G. Lindquist G. Robert , 10:00 a.m.–10:30a.m. , Boris Desiatov, Uriel Levy; Desiatov,Levy; Uriel Boris , We experimentally Junpeng Guo Junpeng 1,2 , David J. David , 2 Duke Duke FiO/LS 2010 1 , vector beams is discussed. hybrid unique Stokespolarimetry.ofbyGeneration measured experimentally and calculus Jones with analyzed is elements optical conventional through the spin and orbital parts of cylindrical vector beams Alfano; Physics Dept., CUNY, USA. elliptically-polarized nanoscaleoptical spots. and circularly into radiation diffraction-limited linearly-polarized convert can nanoaperture gular rectan- A polarization. same the with spots optical polarized diffraction-limited radiation into nanoscale demonstrated that a square nanoaperture can mediate Öğüt SubwavelengthApertures, Nanoscale from Radiation Near-Field of Aspects Polarization FWC5 •9:45a.m. Hybrid Vector Beams, Transformationsand Beam Vector Cylindrical FWC4 •9:30a.m. Continued Unconventional Polarization I— FWC •OpticalDesignwith Coffee Break,Empire Hall, Rochester Riverside Convention Center , Kürşat Şendur; Sabanci Univ.,Turkey.Sabanci Şendur; Kürşat , • Highland C FiO NOTES October 24–28,2010 Giovanni Milione Giovanni Transformations of , Robert R. Erdem Erdem

It is is It μW is achieved. ~200 of power output laser high scheme, coupling fiber butt-endUsing dissipation.a thermal efficient of substrate a onto wafer-bonded laser band-edge photonicsurface-emittingcrystal operationofwave Univ., Korea, Republic of. Sunghwan Kim Laser, Band-edge Crystal Photonic uous-wave Contin- from Power Output Fiber-coupled High FWD5 •9:30a.m. Germany, rial Sciences Ctr. and Faculty of Physics, Philipps-Univ., Bernardette Kunert Bernardette Liebich Sven 1 Nadir Hossain Nadir Integrated Ga(NAsP)/(BGa)P/Si Lasers, QWcally Monolithi- of Temperature Dependence the On FWD6 •9:45a.m. threshold current. to dominate the temperature dependence of the laser found is process leakage carrier A substrate. silicon Ga(NAsP)/(BGa)Pgrown lasers monolithically on a tion up to 120K is reported in novel direct band-gap Integration II—Continued FWD •NovelHybrid Advanced Technology Inst., Univ. of Surrey, UK, 3 NAsP III/V GmbH, Germany. 2 , Peter Ludewig Peter , 1 , Jeongkug Lee, Heonsu Jeon; Seoul Natl. , ShirongJin, R. Highland D 3 , Kerstin VolzKerstin , We demonstrate continuous- 1 2 , StephenJ., Sweeney Mri Zimprich Martin , 2 , WolfgangStolz , Lasing Lasing opera- 2 Mate 2 2 1 - ; , , based on harmonic cascade based generation collinearly. around 500 attosecond is proposed and demonstrated tical frequency pulse trains generation with duration p-polarized reflectance. p-polarized vs. s- of ratio measured the from characterized are copper,metals constantsuranium,forother andcal EUV. the optiin - materialsThe constants of optical high-orderLaser harmonics are used to measure the Astronomy,andYoung PhysicsBrighamUniv., USA. NickMichaelHerrick, Ware, JustinPeatross; of Dept. Harmonics, Extreme Ultraviolet Polarimetry Using Laser High FWE5 •9:30a.m. Natl. Tsing Hua Univ.,Taiwan,TsingHuaNatl. and waveform controlled 10 alternative approach of carrier-envelope-phase(CEP) Yat-SenUniv.,Taiwan.Sun Natl. Chen Pulse Train by Multi-Colored Laser Fields, Light Waveform Control of Synthesized Attosecond FWE6 •9:45a.m. Technnology II—Continued FWE •Attosecond Opticsand 1 , Chao-Kuei Lee Nathan Heilmann Nathan Highland E 2 , Ci-Ling Pan 14 W/cm 2 Dept. of Photonics, of Dept. , Nicole Brimhall, Brimhall, Nicole , 1 In this work, an work, this In ; 2 1 peak power op power peak Dept. of Physics, Wei-Jan - Wednesday, October 27 77 - It is It Sur Marina Stavytska-Barba, Stavytska-Barba, Marina Invited Tom J. , Savenije Tom Laurens D. A. Highland K Highland LWC • Photophysics of Energy Photophysics of Energy • LWC I—Continued Conversion LWC5 • 9:45 a.m. • 9:45 a.m. LWC5 LWC4 • 9:30 a.m. LWC4 Interaction the of Study EnhancedRaman Surface - Plasmoni with Components Cell Solar Organic of Nanoparticles, Active cally USA. Merced, California, of Univ. ; Kelley M. Anne Exciton Exciton Diffusion and Interfacial Charge Separa - tion in Photovoltaic Materials Studied by - Micro wave Conductivity, Netherlands. of Technology, Univ. Delft Siebbeles; Time-Resolved laser-induced the how demonstrated de- to used be can Technique Conductivity Microwave length diffusion exciton triplet or singlet the termine in organic dye layers, as well of Knowledge as the semiconductor. a efficiency into injection for electron - optimiza for importance prime of is processes these photovoltaics. hybrid (nanostructured) of tion - charac to used is spectroscopy Raman enhanced face terize the interaction of a common poly(thiophene) based component of organic polymer photovoltaic cells, PEDOT:PSS, with plasmonically active metal nanoparticles that are reported to enhance solar efficiency. conversion - Selim M. Selim We show, theo show, We LS Highland J Highland ; Northwestern Univ., USA. Univ., ; Northwestern Honam Yum, Joshua Yablon, Ye Wang, Wang, Ye Yablon, Joshua Yum, Honam LWB • Metrology and Precision Metrology and Precision • LWB I—Continued Measurements retically and experimentally, how a how ring laser can be retically experimentally, and far light of velocity group the where regime a to tuned superluminal a realizing veocity, vacuum the exceeds perturbations. to high with sensitivity laser, Shahriar LWB5 • 9:45 a.m. LWB5 Ring Superluminal withA Sensing Ultra-sensitive Laser, - , J. Har W. 1 JILA, NIST, Univ. of Univ. JILA, NIST, 1 ; 2 , T. , Donner T. We detect the motion of of motion the detect We 2 Invited October 24–28, 2010 NOTES • Highland H Highland NIST, USA. NIST, 2 , J. D. Teufel 1 , R. W. , Simmonds R. W. 2 , D. Li 1 Empire Hall, Rochester Riverside Convention Center Convention Riverside Rochester Hall, Coffee Break, Empire LWA • Hybrid Quantum LWA Systems I—Continued Measurement Measurement of Nanomechanical Motion with Precision Sufficient to DetectMotion, Zero-Point K. Lehnert W. a suspended micro- and nano- mechanical elements, elements, mechanical nano- and micro- suspended a cooled been has motion of mode fundamental whose using ground-state the of quanta of 10s few a within to cryostat. temperature ultra-low an LWA5 • 9:30 a.m. LWA5 Colorado, USA, Colorado, low - FiO/LS 2010 ; Univ. Univ. Zheludev; Nikolay Invited We overview our recent results results recent overview our We 10:00 a.m.–10:30 a.m. Highland G Highland FWG • Nonlinearities and Gain in and Gain in FWG • Nonlinearities and Metamaterials I— Plasmonics Continued FWG6 • 9:30 a.m. FWG6 • 9:30 - Control Metamaterials: Nonlinear and Switchable Nanoscale, the on Light ling UK. Southampton, of in nanostructured photonic metamaterials - contain ing nonlinear and active media such as switchable chalcogenide glass, carbon nanotubes, graphene, semiconductor quantum dots and report on super metamaterials. plasmonic conducting ; FiO 1,2 Dustin Yasuaki Yasuaki We We analyzed , Satoshi Kawata 2 RIKEN, Japan. 2 Highland F Highland , Atsushi Taguchi 1,2 , Andrew J. Berger; Univ. of Rochester, USA. of Rochester, Berger;J. Univ. , Andrew ______Osaka Univ., Osaka Japan, Univ., W. Shipp Integrated Raman- and Angular-scattering - Micros data morphological and chemical uses (IRAM) copy immune resting and activated between differentiate to time over changes these monitor now can IRAM cells. process. cell activation the immune study to FWF7 • 9:30 a.m. Time-Lapsed Integrated Raman- and Angular- Scattering Microscopy of Immune Cells, 1 FWF8 • 9:45 a.m. Analysis of Raman Spectral Evolution of HeLa Cells under Deep-Ultraviolet Exposure, Kumamoto FWF • Biosensing—Continued deep-ultraviolet deep-ultraviolet Raman spectral evolution of HeLa cells at varied exposure duration and excitation that found We light. deep-ultraviolet of wavelengths and 244 and 257 nm DNA can be probing better for respectively. protein, Wednesday, October 27 78 MIT Media Lab. probes being developed at the Camera Culture group, 8-D and displays 6-D cameras, 4-D novel describes Talktools. modern using synthesized and analyzed light-transport can be up to 8-D. They can be sensed, Ramesh Raskar Computational Photography in 4-D, 6-D and 8-D, FWH1 •10:30a.m. USA, Presider Markus Testorf; Dartmouth College, for ComputationalImagingI andHardware Dimensions–Theory FWH •SensinginHigher 10:30 a.m.–11:45a.m. generality incomputational imaging. plenoptic cameras as an example and demonstrate its projection relationship of the light field capture with as a linear integration process, we derive an accurate Kong, Hong of Kong.Hong Univ. Engineering, Electronic and ture, Cap- Field Light of Analysis Projection Spatial A FWH2 •11:00a.m. Zhimin Xu Zhimin By modeling the light field acquisition field light the modeling By ; MIT, USA. , Edmund Y. Lam; Dept. of Electrical Highland A Geometric-dimensions of Invited that to approach used can be such limits. cal fibers can carry. We discuss advanced technologies nonlinearity on the quantity of information that opti- Kerr fiber by imposed limitations possible showing Bell Labs, Alcatel-Lucent, USA. Networks, Optical Future in Growth Capacity for TechnologiesPromising FWI1 •10:30a.m. Presider Xiang Liu; Alcatel-Lucent, USA, FWI •OpticalCommunicationII 10:30 a.m.–12:00p.m. such asystem. for results and setup experimental presents This bandwidth. the quadruple to fiber silica multimode index step a over de-multiplexed and multiplexed spatially been have wavelength same of channels Technology,USA. of AbhijitMurshidInst., Chakravarty;FloridaH. Syed Wavelength, Same UsingFibers Silica Multimode of Bandwidth Quadruples Fiber Optical Tapered FWI2 •11:00a.m. Highland B Four co-propagating optical co-propagating Four Invited René-Jean Essiambre; René-Jean We present an analysis FiO/LS 2010 Fienup WavefrontSensing, Wavesin and Rays diversity inpolarimetry. anddiversity, perspective diversity,wavelength ing includ- sensing, wavefront for mechanisms diverse measurement-wavefrontsensor.otherWe examine image-based effective an be to shown been has sity Paxman; General Dynamics Corp., USA. Measurement-Diverse Wavefront Sensing, FWJ1 •10:30a.m. Flight Ctr., USA,Presider Bruce Dean; NASA Goddard Space Sensing I FWJ •Image-basedWavefront 10:30 a.m.–12:00p.m. retrieval combinesretrieval robustness, speed, and accuracy. phase with technique ray-based new a of Marriage compared. are optics wave and ray using sensing CoherentTechnologies, USA. of Optics, Univ.Optics, of Rochester,of USA, FWJ2 •11:00a.m. 1 , Alden S. Jurling • Highland C FiO October 24–28,2010 1 , Samuel T. Thurman Invited Invited Image-basedwavefront 2 Lockheed Martin Lockheed Phase diver James R. R. James Richard 1,2 ; 1 Inst. - ratio up to 57dBis achieved. suppression side-mode with oscillation SLM Stable Er-doped fiber ring laser with high-birefringence PCF. high-performance, tunable, fiers arefiers treated. also amplipulse - chirped in compressor use forgratings Stretcherdescribed. with fibers dispersion matching are mode order higher a in propagation on based Denmark. Martin E. V. Pedersen, Bera Pálsdóttir; OFS Denmark, Lasers, Fiber fs in Management Dispersion for Fibers FWK1 •10:30a.m. Presider John Ballato; Clemson Univ., USA, FWK •FiberLaser 10:30 a.m.–12:00p.m. Chung; Gwangju Inst. of Science and Technology, Technology, and Republic ofKorea. Science of Inst. Gwangju Chung; YoungjooLyong, Choi Kim,BongKyun Im , Jooeun Er-doped Fiber Laser with High-Birefringence PCF, A Wavelength Tunable Single-Longitudinal-Mode FWK2 •11:00a.m. , Kim G. Jespersen, Jespersen, G. Kim Grüner-Nielsen, Lars All All fiber devices with anomalous dispersion Highland D We

experimentally demonstrate experimentally a single-longitudinal-mode Invited Dreams, Laser Plasma Accelerators: Concepts, Progress and sources and colliders. radiation hyperspectral compact of development generated from structures that are been cm-scale enablinghave beams electron GeV discussed. be will accelerators plasma laser developing in challenges Lab,USA. FWL1 •10:30a.m. received outstanding dissertation awards. have that three including students, graduate PhD Fellow.IEEE Heresearch hasbeen advisor for many and the 2009 E.O. Lawrence Award. He is an APS and Achievement in Accelerator Physics and Technology,for Prize School Accelerator Particle States United HalbachAward for X-ray Instrumentation, 2005 the thesis research work in plasma physics, the 1996 Klaus Society Simon Ramo award for outstanding doctoral Physicalawards,American ‘92 includingseveral the received He sources. radiation hyperspectral and interests are in laser plasma based accelerator science 1991 and joined LBNL in 1991. His current research in UCLA from EE in Ph.D. a and 1985, in Belgium Brussel”,Universiteit“Vrije the from degree (EE) Nevada, Reno. He obtained an electrical engineering Berkeley and an adjunct professor at the University of LOASISresearchphysicistProgramLBNL,at UC at the of Head the scientist, senior a is Leemans Dr. Natl. Lab, USA,Presider Csaba Toth; Lawrence Berkeley Acceleration I BasedParticle FWL •Laser 10:30 a.m.–12:00p.m. Wim Leemans Wim The basic principles, progress and future and progressprinciples, basic The Highland E ; Lawrence Berkeley Natl. Natl. Berkeley Lawrence ; Tutorial Wednesday, October 27 79 We Adam ; Princeton Li Sun Invited Invited Highland K Highland LWF2 • 11:00 a.m. LWF2 LWF1 • 10:30 a.m. • 10:30 a.m. LWF1 E. Cohen, Yiqiao Harvard Tang; USA. Univ., - electromag the of chirality the of measure a introduce to Maxwell’s netic solutions field. exist simple There Equations with much greater chirality than that of polarized light. circularly Local Dynamics Probing by Real-Time Single- Particle Tracking Spectroscopy, available. not USA. Abstract Univ., Optical Chirality and Superchiral Fields, 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 Single Molecule • LWF to Biology I Approaches at California of Univ. Yang; Haw Presider USA, Berkeley, ; Univ. of Waterloo, Robert J. ; Schoelkopf Invited Invited LS Highland J Highland I will describe experiments in which in experiments describe will I Raymond Laflamme I will describe benchmarking of quantum

Canada. error quantum of light the in processors information which theorem threshold accuracy the and correction says that if noise sufficently low it is still possible to efficiently. compute quantum LWE1 • 10:30 a.m. • 10:30 a.m. LWE1 • 11:00 a.m. LWE2 Benchmarking Quantum Processing Information Devices, Yale Univ., USA. Univ., Yale - includ entangled, are bits quantum superconducting and (CHSH) two for bounds classical of violation ing three (Mermin) qubit inequalities, and the - demon stration of quantum algorithms with an electronic, system. solid-state Entanglement Entanglement and Quantum Algorithms with Superconducting Circuits, 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 Quantum Enhanced • LWE Processing I Information Wisconsin of Univ. Saffman; Mark USA, Presider Madison, at Aashish Aashish Clerk; , Cheng Benjamin Yang, Invited Invited October 24–28, 2010 I will discuss theoretical work work theoretical discusswill I • Highland H Highland Jack Sankey We demonstrate several demonstrate different forms We LWD2 • 11:00 a.m. LWD2 LWD1 • 10:30 a.m. • 10:30 a.m. LWD1 Quantum Quantum Measurement of Phonon Shot Noise Using Optomechanical Systems, Canada. Univ., McGill used be can systems optomechanical how describing energya of driven fluctuations quantum to measure of moments higher the how and resonator, mechanical properties. possess unusual fluctuations such Nonlinear Optomechanical Couplings: Tools for Quan- the in Objects Mechanical Solid with Dealing tum Regime, G. Jack M. E. Jayich, Harris; Yale Andrew M. Zwickl, USA. Univ., and quadratic, (linear, coupling optomechanical the of spectrum the in crossings avoided at realized quartic) of an optical cavity containing a flexible dielectric . situ in tunable is Each coupling membrane. 10:30 a.m.–12:15 p.m. 10:30 a.m.–12:15 II Hybrid Quantum Systems • LWD USA, Univ., Yale Harris; Jack Presider , , 1 4 FiO/LS 2010 , Yu. Yu. , Inst. Inst. 1 2 Surface Surface ENSTA- , Grégory , Grégory 1 1 , Arnaud 1 ; 1 Myhalong, , 4 , J. E. Livenere E. J. , 1 , M. Bahoura M. , 1 Norfolk State Univ., Norfolk State Univ., 1 , Jean-Paul Geindre , Jean-Paul 3 ; 2 , Lei Gu Lei , 1 , Denis Douillet 1,2 Antonin Antonin Borot , R. Mundle 1 We We demonstrate experimentally Highland G Highland , Nikolai Berkovitch, Alex Hayat, Pavel Pavel Hayat, Alex Berkovitch, Nikolai , , Rodrigo Lopez-Martens 2 M. A. Noginov A. M. , V. , A. V. Podolskiy , Patrick , Audebert Patrick 1 1,2 , Xiaowei , Chen Xiaowei We report high-harmonic generation from from generation high-harmonic report We 1 Lab pour l’Utilisation des Lasers Intenses, 3 , A. K. Pradhan K. A. , Univ. of Univ. Massachusetts Lowell, USA. 1 2 Amir Nevet FWN2 • 10:45 a.m. Khz-driven High Harmonic Generation From Overdense Plasmas, FWN3 • 11:00 a.m. Telecom for Materials Plasmonic Gold: Than Better Wavelengths, plasmon plasmon polaritons (SPPs) at telecom wavelengths wide-gap degenerate in confinement better much have than semiconductors in silver or gold. For the same lower is semiconductors in loss SPP the confinement, in gold. that than FWN1 • 10:30 a.m. Emission Two-Photon of Enhancement Broadband from Semiconductors - by Plasmonic Nano-Anten nas, Ofir Ginzach, Sorias,Orenstein; Shai Meir Ginzburg, Israel. Technion, and theoretically a broadband enhancement of the emission spontaneous two-photon from AlGaAs by with structures Plasmonic nano-antennas. plasmonic effective small very but quality-factors low inherently be to optimal. shown are volumes Iaquaniello USA, de de la Lumière Extrême, CNRS, Ecole Polytechnique, ENSTA ParisTech, Inst. d’Optique, Univ. Paris-Sud, France, 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 and Gain in FWN • Nonlinearities and Metamaterials II Plasmonics State Norfolk Noginov; Mikhail USA, Presider Univ., Ecole Polytechnique-CNRS, Ecole France, Polytechnique-CNRS, Portugal. by rate 1kHz repetition driven at plasmas overdense milliJoule laser pulses at intensities <1018 W/cm2. We observe characteristic coherent wake emission spectra with reproducible CEP-dependent features in the few-cycle regime. A. Barnakov Malvache Gérard Mouro Zhu G. ParisTech-Ecole Polytechnique-CNRS,, France, Polytechnique-CNRS,, ParisTech-Ecole

, , 1 FiO 2,3 Sergio , Univ. of 1 2 We We report , , Alexander 2 , Daryl Preece 1 , David Carberry 1 Invited Tiffany C. Y. Tang Y. C. Tiffany Univ. of New Univ. South Wales, 1 ; 1 Univ. of Univ. Glasgow, UK, 1 Highland F Highland ; , , Maryanne C. J. Large , Richard Bowman 2 1 , Graham Gibson 2,3 1 Dept. Dept. of Physics, of Univ. Bristol, UK. 3 Univ. of Univ. Sydney, Australia. 2 , Peter J. Reece 2 the first demonstration of 3-D optical trapping of microstructured hollow-core a inside microparticles beam. tweezers external an with fiber optical polymer We map the trapping properties to determine the the microstructure. influence of Holographic Holographic optical tweezers, using the latest spa- tial light modulators and graphics-cards calculate 200Hz, at holograms fast the enough to compensate imaging high-speed with Coupled motion. Brownian particles, of multiple various new system - configura possible are tions G. Leon-Saval FWM1 • 10:30 a.m. 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 II FWM • Trapping Rochester, of Univ. Moore; Nicole USA, Presider Argyros Bristol, Bristol, UK, FWM2 • 11:00 a.m. - Micro Hollow-Core a Inside Trapping Optical 3-D Fiber, Opticalstructured Arran Curran Mervyn Miles High-Speed Holographic Tweezers and Imaging, Miles Padgett Australia, Australia, Wednesday, October 27 80 methods formethods analyzing image the refocus process. systems. Specifically we demonstrate the use of these to analyze problems involving 4-D light field imaging methods modeling general as methods space phase Ben-Gurion Univ. of the Negev, Israel.Negev,the Univ.of Ben-Gurion Adrian Stern Is Super-Resolution from a Single Image Possible? FWH3 •11:15a.m. Continued for ComputationalImagingI— andHardware Dimensions–Theory FWH •SensinginHigher about details. fine the imaging process that indirectly captures information 2) resolutiondetails, high infersthat reconstruction image 1) approaches: two between distinguishWe image. single from resolution super of meaning the Kong, Hong Kong. Hong Kong, Univ.HongY.W.EdmundLam; of ChanC. , Aaron Image Refocus in Geometrical Optical Phase Space, FWH4 •11:30a.m. , Yair, Rivenson, Gil Paz, OlegAvremko; Highland A

We introduce matrix optics and optics matrix introduceWe

We discuss discuss We coded-OFDM. tions based optical transmission, and (iii) multi-band constella- signal optimum (ii) coded-modulation, multidimensional single-carrier (i) paper: invited Gb/s opticalserial transport will be in described this USA. Djordjevic Transmission, Gb/s 400 Generation Next FWI3 •11:15a.m. the design of design the multiple-transmitter efficient links. between received signals and establish key elements in ous system settings we quantify the cross-correlation communication link using spatial diversity. For vari- laser a of performance the analyze experimentally Chile. Andes, the Univ.of Cisternas; E. Jaime Transmitter Terrestrial FSO Link, Multiple- A In Measurements Diversity Spatial FWI4 •11:45a.m. Continued FWI •OpticalCommunicationII— Different strategies for enabling beyond 400 beyond enabling for strategies Different , Hussam G. Batshon; Univ. of Arizona, Arizona, of Univ. Batshon; G. Hussam , Highland B 12:00 p.m.–1:30p.m. Invited Jaime A. Anguita Ivan Ivan

We We FiO/LS 2010 12:00 p.m.–1:30p.m. , Exhibit Only Time, EmpireExhibit OnlyTime, Hall, Rochester Riverside Convention Center Zielinski Algorithm, Retrieval Phase Diverse DeterminationSamplingofthe Factor Phase- a in FWJ3 •11:30a.m. Aronstein Rochester,USA. are that are rotationally symmetric. rotationallybut, symmetric, contain optical surfaces polynomial expansion for optical Zernike systems that FRINGE are the not in terms of dependence field 1 Flight Ctr., USA, Ctr.,Flight determining Qfrom image data. for method a presentWe results. retrieval accurate Knowledgequantityof this foressential is obtaining plane. image and pupil the between relationship USA. Symmetry, of Zernike Coefficients in Optical Systems without Dependence Field the forExpression Analytic An FWJ4 •11:45a.m. Sensing I—Continued FWJ •Image-basedWavefront Optical Res. Associates, USA, The sampling factor (Q) determines the scale scale the determines (Q) factor sampling The 1 1 , Bruce H. Dean , James R. Fienup JamesR. , Kevin P. Thompson Kevin We present an analytic form for the Wethe forform analytic presentan • Highland C 2 Inst. of Optics, Univ. of Rochester,Univ.of Optics, of Inst. FiO October 24–28,2010 1 , Jeffrey S. Smith 2 ; 2 1 Lunch (on yourLunch own) Inst. of Optics, Univ. of NASA Goddard Space Goddard NASA 1 , Jannick P. Rolland Thomas P. Thomas 1 , David L. 2 ; Fiber Lasers, Fiber Lasers, Mode High-Order in Efficiency Power Extraction FWK4 •11:30a.m. ester, USA, 1 kin USA, Electro-Optic Sampling System,Electro-Optic LiminJi Novel a Applicationin Its and Laser Fiber Doped Erbium- Mode-Locked Active the ofStability The FWK5 •11:45a.m. USA, USA. Donaldson actively mode-locked fiber lasers. actively fiber mode-locked novel electro-optic sampling system is proposed with A laser. fiber erbium-doped mode-locked active an stabilizing of process the during observed is width pulse the and modulation high-harmonic of ship Smith Fiber, Helical-core a Using formation - De Mode Bend-Induced of Measurement Direct FWK3 •11:15a.m. limit at kWpower levels. lasers. The efficiency approaches the quantum defect power extraction in efficiency Yb and Er HOM onfiber nulls intensity mode of effect the study to used between model and model between measurement is 3.4%. directly verified for the first time. The rms is difference fibers bent in deformation mode predict to used FWK •FiberLaser—Continued Lab for Laser Energetics, Inst. of Optics, Univ. of Roch- 2 , Theodore F. Morse

2 The Marcuse equivalent index model that is that model index equivalent Marcuse The 2 1 Boston Univ., USA. Lab for Laser Energetics, USA. Energetics, Laser for Lab , John R. Marciante R. John , 2,1 2 Electro-Optics Program, Univ. of Dayton, , Thomas Hsiang Thomas , Richard S. Quimby S. Richard Highland D 2 ; 1 Worcester Polytechnic Inst., Numerical simulations are 1 , Andrew M. Sarangan M. Andrew , 1 ; 1 Univ. of Rochester, of Univ. 1 , Roman Shuboch- The relation- The Richard C. Richard 1 , William 2 ; Tautz Regime, Accelerator (LWFA) Operating inthe Self-Guided Wakefield Laser A by Electrons of Acceleration Christian M. S. Sears S. M. Christian electron are beam demonstrated. stantial quality improvements on the monoenergetic plasma wave using a μm-scale density transition. Sub tion from the background plasma into a laser driven presentcontrolledofnovel a injecelectronmethod - tum Optics, Germany,Optics, tum Angeles, USA, Angeles, creating abubble-like wakefield-structure. by length Rayleigh of tens wake-over the by guided shown that short but intense laser-pulses can be self- is Itexplored. experimentally been has acceleration The so-called “self-guided” regime of laser wakefield Krausz Marsh München, Germany,München, Density Transitions, Sharp Wavesat Plasma into Injection Electron FWL3 •11:45a.m. FWL2 •11:15a.m. Acceleration I—Continued BasedParticle FWL •Laser 1,2 1 1,2 , A. Pak , Daniel , Herrmann Daniel , Laszlo VeiszLaszlo , Chan Joshi Chan 1 2 , J. Ralph Lawrence Livermore Natl. Lab, USA. Lab,Natl.Livermore Lawrence Highland E 3 Karl Karl Schmid 1 Queen’sUK. Univ.Belfast, 1 1 , C. Clayton C. , ; , Julia Mikhailova Julia , 2 1,2 1 Ludwig-Maximilians-Univ. Ludwig-Maximilians-Univ. Max-Planck-Inst. of Quan- Max-Planck-Inst.of 1,2 ; 1 Invited , Michael Geissler Univ. of California at Los 1 , Alexander Buck 1 , D. Froula D. , 1 , Raphael , 3 , Ferenc 2 , K. K. , We We 1 - , Wednesday, October 27 81 Hideo Hideo Charles B. We utilize We real-time Invited Highland K Highland ; Stanford Univ., USA. ; Univ., Stanford LWF • Single Molecule Approaches Molecule Single • LWF I—Continued to Biology LWF3 • 11:30 a.m. • 11:30 a.m. LWF3 Exploring Exploring Chromatin Biochemistry with Single- Molecule Fluorescence Diffusometry, Straight, F. Aaron M. Colin J. Limouse, Fuller, Mabuchi feedback feedback to track individual dye-labeled chromatin - buf aqueous in motion Brownian undergoing fibers fluorescence of recording simultaneous enabling fer, and data, hydrodynamic new providing insight into conformational dynamics and self-association of arrays. nucleosome - ; Univ. Univ. ; D. Bonneau, P. Dieter Meschede Dieter Invited Invited LS We We show that a single trapped Highland J Highland LWE • Quantum Enhanced • LWE Processing I— Information Continued Caesium Caesium atom trapped can coherently be split and recombined, An efficient sideband cooling method - refrac the control to method a and describedbe will atom. a single of index tive of of Bonn, Germany. Coherent Splitting, Rocking and Blinding of Single of Blinding and Rocking Splitting, Coherent Lattice, Optical an in Atoms Kalasuwan, A. Laing, T. Lawson, Jcf Matthews, JP Shadbolt, JP Hadden, A. Har K. Peruzzo, P. Poulios, B. Ld Ho, Y- rison,L. Marseglia, A. C. Stanley-Clark, Lobino, M. Halder, M. Jiang, P. Rarity, G. J. Patton, R. Thompson, Mg Zhou, X-q Verde, Rodas M. Politi, L. A. Kingdom. United Bristol, of ; Univ. L. O’Brien Jeremy We describe recent developments in integrated quantum photonics, including waveguide circuits to implement quantum logic operations, quantum walks. quantum metrology and Integrated Integrated Quantum Photonics, LWE4 • 11:00 a.m. LWE4 LWE3 • 11:30 a.m. • 11:30 a.m. LWE3 - , Jai- 2 , Moonjoo Moonjoo , 1 , Christopher 2 , Michael Feld , Michael 2 (on your own) Lunch your (on , Wontaek Seo Seoul Natl. Univ., Korea, Korea, Univ., Natl. Seoul 1 1 Invited ; 1 October 24–28, 2010 , Wonshik , Choi Wonshik 1 ; Univ. ; of Univ. California at Santa Bar • Highland H Highland G. R. Harrison Spectroscopy Lab, MIT, 2 Hyun-Gue Hong Hyun-Gue By coupling a superconducting quantum quantum superconducting a coupling By , Kyungwon An Kyungwon , 1 , Ramachandra Dasari , Ramachandra 2 We report the measurement of the cavity-QED cavity-QED the of measurement the report We , Younghoon Song 1 LWD • Hybrid Quantum • LWD Systems II—Continued Lee LWD4 • 12:00 p.m. LWD4 Spectrum Measurement Of The Cavity-QED Mi- crolaser: Deviation From The Schawlow-Townes Linewidth, USA. microlaser linewidth near threshold by using the photon-counting-based second-order correlation linewidth the of rise-and-fall abrupt The spectroscopy. observed. is thereshold near Measuring Measuring the Quantum Harmonic Oscillator, Andrew Cleland LWD3 • 11:30 a.m. • 11:30 a.m. LWD3 Fang-Yen Hyung Lee Hyung Republic Republic of, bara, USA. bara, bit to microwave electromagnetic and mechanical - resona the achieve demonstrably can we resonators, ground states, quantum and and photon create tors’ Fock phonon states, and arbitrary superpositions of states. Fock photon Empire Hall, Rochester Riverside Convention Center Convention Riverside Rochester Hall, Exhibit Only Time, Empire , , , ; 12:00 p.m.–1:30 p.m. - 3 1 1 FiO/LS 2010 Negative Negative We We show Yan Guo Yan , Gilad M. 1 Local power , Yifang Chen Yifang , Optoelectronics Optoelectronics Shangai Inst. of of Inst. Shangai 2 1 2 - Bucking Roger , 1 ; , Meir , Orenstein Meir 1 School School of Physics Pavel Pavel Ginzburg 2 4 , Uriel , Levy Uriel 2 , Shaowei Wang Shaowei , 1 , Alexander Normatov 12:00 p.m.–1:30 p.m. 1 Israel. Univ., Hebrew 2 Highland G Highland Nikolay Zheludev Nikolay Anagnostis Tsiatmas Anagnostis , 4 , Avner Yanai , Avner 2 , Vassili Fedotov Vassili , 1 Rutherford Rutherford Appleton Lab, UK, Technion, Israel, Israel, Technion, FWN • Nonlinearities and Gain FWN • Nonlinearities and in Plasmonics II—Continued Metamaterials FWN4 • 11:15 a.m. FWN4 • 11:15 Superconducting Plasmonics and Extraordinary Transmission, concentration of efficiently coupled radially-polarized coupled efficiently of concentration Radial presented. is needle plasmonic conical in light with needle DBR as defect was fabricated plasmonic for NSOM and nonlinear conversion experiments. calculated. are resonances dependent length Needle Lerman 1 3 Res. Ctr., Univ. of Southampton, UK, Southampton, of Univ. Ctr., Res. Technical Physics, Technical Chinese Acad. of Sciences, China, Miriam Miriam Deutsch; of Univ. Oregon, USA. gener is wave electromagnetic harmonic third a that a nonlinear at propagating surface plasmons by ated intensity and angular- The interface. metal-dielectric dependence of the generated wave are calculated analyzed. and FWN6 • 11:45 a.m. Field Enhancement By Efficient Nano-coupling To Plasmonic Conical Needle, FWN5 • 11:30 a.m. Third Harmonic Generation Using Surface - Plas mon at Nonlinear Polaritons Interfaces, and Astronomy, Univ. of Southampton, UK. of Southampton, Univ. Astronomy, and dielectric constant and dominant kinetic resistance intriguing make plasmonic media.superconductors we Here report on the effect of extraordinary - trans mission through an array of sub-wavelength holes in a perforated film of high-temperature YBCO superconductor. P.A.J. de Groot P.A.J. Nikolai Berkovitch ham , 2 FiO The

, Jun Ki Kim 1 - applica present We Monika Monika ; Ritsch-Marte Invited , Jongki Kim 1 Yonsei Yonsei Univ., Korea, Republic of, 1 Highland F Highland ; 1 Sung Sung Rae Lee Wellman Ctr. Wellman for Photomedicine, Harvard Medical FWM4 • 11:30 a.m. - all-fibercom structure Besselfrom beam generated posed of single mode fiber, coreless silica fiber, and formed on the micro-lens fiber facet a showed good non- its confirming trapping optical for performance diffracting nature. self-reconstructing and School, School, Massachusetts General Hospital, USA. 2 FWM3 • 11:15 a.m. all-Fiber Basedon BeamBessel of Generation The Device and Its Optical of Trapping Dielectric Particles, FWM • Trapping II—Continued FWM • Trapping Kyunghwan Oh Kyunghwan tions of spatial light modulators for optical trapping optical for tions trapping of spatial light modulators with low (¡0.2) NA and large field of view, creation en- fields, of freely designable contrast force and for microscopy. methods in optical hancement - Opti for Modulators Light Spatial of Applications cal and Trapping Imaging, Austria. Univ., Medical Innsbruck Empire Hall, Rochester Riverside Convention Center JOINT FiO/LS

12:00 p.m.–1:30 p.m. JWA • FiO Poster Session II

JWA01 JWA06 JWA11 JWA16 JWA21 Singular Optics and Structurally Stable Beam, Computer-Generated Volume Holograms in the Stable Optical Lift, Timothy J. Peterson, Alexandra A Simple Calibration Method for Liquid Crystal Ultra-sensitive Acclerometry Using Anomalous Rahul Mandal, Ajay Ghosh; Univ. of Calcutta, India. A THz, Wei-Ren Ng, Andrew Pyzdek, Ziran Wu, Hao Artusio-Glimpse, Grover A. Swartzlander; Rochester Pulse Shaper, Jonathas de Paula Siqueira, Paulo Dispersion in a Sagnac Laser, Joshua Yablon, Honam structurally stable beam has been generated contain- Xin, Michael E. Gehm; Univ. of Arizona, USA. Recent Inst. of Technology, USA. When placed in a uniform Henrique Dias Ferreira, Sérgio Carlos Zílio, Cleber Yum, Selim M. Shahriar; Northwestern Univ., USA. ing numerous singularities in various positions. The advances in rapid prototyping provide the promise of stream of light, an airfoil shaped refractive object may Renato Mendonça, Lino Misoguti; Univ. de São Paulo, We show that a zero-area Sagnac ring laser, configured singularities have been produced in a predetermined direct, rapid fabrication of volumetric optical compo- experience a transverse lift force having a large lift Brazil. We present a simple method to calibrate spatial in an L-shape, can perform as an ultrasensitive accel- manner by modifying the azimuthal coordinate term nents in the terahertz. We are investigating use of this angle with respect to the forward scattering force. light modulator (SLM) employed for pulse shaper. erometer when operated in the so-called superluminal of the circular cylindrical coordinate. new technology for fabrication of a Bragg-selective Such method is based on light scattering induced by regime by inducing anomalous dispersion with a dipin computer-generated volume hologram. JWA12 abrupt index refraction change instead of traditional the gain profile JWA02 Measurement of the Optical Properties of Nano- interferometric methods. Volume Phase Plates for Optical Beam Control, JWA07 rose, Tianyi Wang1, Li L. Ma1, Jinze Qiu1, Xiankai JWA22 Marc SeGall, Vasile Rotar, Julien Lumeau, Leonid Gle- Simple Technique for Experimental Synthesis Li2, Keith P. Johnston1, Marc D. Feldman2, Thomas E. JWA17 Simulation Algorithm of Near-Middle Distance bov; CREOL, College of Optics and Photonics, Univ. of and Characterization of Partially Coherent and Milner1; 1Univ. of Texas at Austin, USA, 2Univ. of Texas Backscattering Technology of Cerebral Oxygen- in Target and Jamming Infrared Simulator, Chong Central Florida, USA. Permanent binary phase plates Partially Polarized Source, Miguel A. Olvera- Health Science Ctr. at San Antonio, USA. Nanorose ation Measurements, Yuri A. Chivel; Inst. of Applied Huang, Haiqing Chen, Binbing Liu, Shuang Zhao; with high tolerance to laser radiation are recorded in Santamaría, Esteban Juárez-Velez, Andrey S. Os- is used to target macrophages in atherosclerotic Physical Problems, Belarus. A technology of cerebral Wuhan Natl. Lab for Optoelectronics, College of Op- the volume of photo-thermo-refractive glass using trovsky; Autonomous Univ. of Puebla, Mexico. Two plaques. Experimental measurement and simula- oxygenation measurements based on time resolved toelectronic Science and Engineering, Huazhong Univ.

binary amplitude masks. Conversion of a Gaussian coupled Mach-Zehnder interferometers are used for tion of nanorose absorption (σa) and scattering (σs) registration of backscattered radiation of probing of Science and Technology, China. Infrared simulation -14 beam to higher order modes is shown. the experimental synthesis and characterization of a cross-sections give, respectively, σa = (3.1±0.5)×10 picosecond laser pulse are developed. algorithm of near-middle distance and motion state 2 partially coherent and partially polarized source. We m and σa/σs = 10.5. of target and jamming relative to the field diaphragm JWA03 show that the results of the experiments are in good JWA18 aperture is demonstrated. Meanwhile, the simulation Optical Manipulation with Counter Propagat- agreement with theoretical predictions. JWA13 Far-Field Analysis of Spectral Shifts in Stochastic algorithm of jamming dropping controlled by a scan- ing Helical Beams, Lisa Dixon, David Grier; New Optical Sensing of Bacteria by Means of Light Beams Propagating through Media with Arbitrary ning mirror is presented. York Univ., USA. We present a novel method for JWA08 Diffraction, Igor Buzalewicz, Halina Podbielska; Refractive Properties, Zhisong Tong, Olga Korotkova; using multiple beams to exert optical forces using Laser-Induced Magnetization Precession in Thin Inst. of Biomedical Engineering and Instrumentation, Univ. of Miami, USA. We will demonstrate the far-field JWA23 holographically generated phase masks. Here we use Films of Fe/MgO and Py/Si, Douglas L. P. Lacerda, Wroclaw Univ. of Technology, Poland. The novel sen- spectral shift in the paraxial region does not depend Classification Of Motion Blurred Images By Means counter propagating helical modes with opposite Carlos A. C. Bosco, A. Azevedo, Lúcio H. Acioli; Univ. sor based on Fourier transform optical system with either on the degree of coherence of the source or on A Discriminative Feature Selection Method Based charge to manipulate mesoscopic particles. Federal de Pernambuco, Brazil. We study the role of the converging spherical wave illumination is proposed its spatial extent, or on the refractive index. On Circular Moments, Carina Toxqui-Quitl, Al- anisotropy field in the laser-induced magnetization for bacteria species characterization. Examination of fonso Padilla-Vivanco; Univ. Politecnica de Tulancingo, JWA04 dynamics on thin films of Fe/MgO and Py/Si. We the individual bacteria colony diffraction pattern can JWA19 Mexico. Circular moments along with a discriminative Rapid Projector Display Based Characterization also characterize the local anisotropy and the Gilbert be used to distinguish bacteria species. Characterization of Phonons in Molecular Crystals, feature selection method are considered for the invari- of Large Reflectors, Deepthi Chakilam1, Duncan damping constant. Rohit Singh, Deepu George, A. G. Markelz; Dept. ant classification of motion blurred images. With a MacFarlane1, Cristian Penciu2, Victor Penciu2; 1Univ. JWA14 of Physics, SUNY Buffalo, USA. We demonstrate a minimum resolution in the image, only one descriptor of Texas at Dallas, USA, 2Pulsar Energy, USA. A JWA09 Manipulating IR Surface Plasmon Polaritons on new technique for characterizing the phonons in is available to discriminate between shapes. projector display is used to provide rapid feedback Widely Tunable, Narrow Linewidth, Ytterbium Graphene, Ashkan Vakil, Nader Engheta; Univ. of molecular crystals, Modulated Orientation Sensitive on the focusing performance and the curvature of Fiber Laser, Keith G. Petrillo, Jin U. Kang; Johns Pennsylvania, USA. Exploiting the dependence of Terahertz Spectroscopy (MOSTS). The technique JWA24 large mirrors for use as solar collectors. Hopkins Univ., USA. An ytterbium fiber ring laser was graphene conductivity on the electric bias field, we suppresses crystal defects and solvent contributions, Gray Scale E-Beam Lithography to Fabricate 3-D demonstrated by utilizing a Fabry-Perot filter and a theoretically investigate the manipulation, routing, and enhances contributions due to molecular struc- Micro-Sized Waveguide and Grating Coupler in JWA05 1 1 1 Wednesday, October 27 Wednesday, sagnac loop in the fiber ring with a linewidth of less waveguiding and scattering of surface-plasmon po- ture and anisotropy. SU-8, Lin Dong , Srinivasan Iyer , Sergei Popov , Ari Nonscanning Method for Measuring Gaussian Laser than 2MHz and a tuning range spanning 50nm. laritons along graphene at IR wavelengths, proposing T. Friberg1,2,3; 1Royal Inst. of Technology, Sweden, 2Aalto Beam Diameters Using Photodiode Array, Abdallah a “flatland” paradigm for optical metamaterials. JWA20 Univ., Finland, 3Univ. of Joensuu, Finland. Gray scale Cherri; Kuwait Univ., Kuwait. A novel method that JWA10 Design and Fabrication for Diffractive Optics in electron beam lithography is applied to prototype eliminates mechanical translation of knife edges and/ Polarization-Dependent Two-Photon Absorption JWA15 Multi Force Optical Tweezers, Samuel I En Lin, 3-D waveguides and grating output couplers in SU-8 or precise alignment of gratings is proposed to mea- of π-Conjugated Molecules, Marcelo G. Vivas, A Near-IR Frequency Comb for Astronomical Hung Wen Hsu, S. L. Chang; Natl. Formosa Univ., with simple and accurate method. The lag effect in sure Gaussian laser beam diameters. The proposed Leonardo De Boni, Cleber R. Mendonca; Inst. de Calibration, Giulia Schettino1,2, Pablo Cancio Taiwan. The laser beam passes through a diffrac- reactive ion etching of Silicon-on-insulator gratings technique facilitates integrating photodiode arrays Física de São Carlos, Univ. de São Paulo, Brazil. In Pastor3,4, Carlo Baffa2, Elisabetta Giani2, Massimo tive device to form a multi Gaussian laser spots is avoided here. with laser beam tracking in instruments. this report, we present a broadband analysis of the Inguscio1,4, Ernesto Oliva2, Andrea Tozzi2; 1Dept. di with 100μm of separation. Demonstration on the circular linear dichroism (CLD) effect on two-photon Fisica e Astronomia, Univ. di Firenze, Italy, 2INAF- cell trap and optical element design are included JWA25 absorption (2PA) cross-section of organic molecules Osservatorio Astrofisico di Arcetri, Italy, 3Inst. Nazi- in this work. Tight Focusing of Polarized Ulrashort Light Pulses, employing an extension white-light continuum Z- onale di Ottica-CNR, Italy, 4LENS, Italy. We present Jixiong Pu, Limin Hua, Baosuan Chen, Ziyang Chen; scan technique (WLC). here the planned setup for the wavelenght calibrator Huaqiao Univ., China. We investigate the tight focus- of the IR astronomical spectrograph GIANO. We ing of polarized ultrashort light pulses. It is found that describe the required performances of the optimal near the focus the slow light and fast light phenomena calibrator source and how we will realize them using occur, depending on the numerical aperture of the a laser-comb. focusing objective system.

82 FiO/LS 2010 • October 24–28, 2010 Empire Hall, Rochester Riverside Convention Center JOINT FiO/LS

JWA • FiO Poster Session II—Continued

JWA26 JWA31 JWA36 JWA40 JWA44 Detection of Subsurface Objects and Coherence SPR Based Fiber Optic Sensor for Gas Sensing in Intrinsic Fiber Optic Pressure Sensor Based on Mul- On Absorption Properties of GaAs/AlGaAs Nano- Speckle Statistics of Localized Waves in Random Analysis, Markus Testorf; Dartmouth College, USA. Visible Range Using Nanocomposites Thin Film, timode Interference Device as Sensitive Element, wire Arrays, Zongquan Gu1, Bahram Nabet1, Paola Media, Abe Pena1, Andrey Chabanov1, Azriel Genack2; The cross-Wigner distribution function is introduced Sarika Singh, Banshi D. Gupta; Indian Inst. of Tech- Victor I. Ruiz-Perez1, Miguel A. Basurto-Pensado2, Prete2, Fabio Marzo3, Ilio Miccoli4, Nico Lovergine4; 1Univ. of Texas at San Antonio, USA, 2Queens Col- as a measure for the mutual coherence of electromag- nology Delhi, India. Surface plasmon resonance based Daniel May-Arrioja3, Jose J. Sánchez-Mondragón1, 1Drexel Univ., USA, 2IMM-CNR, Italy, 3Dept. of innova- lege of CUNY, USA. We discuss remarkably simple netic signals. The averaged cross-Wigner distribution nanocomposite coated fiber optic sensor for gas sens- Patrick LiKamWa4; 1Inst. Nacional de Astrofísica,, tion Engineering, Italy, 4Univ. of Salento, Italy. Arrays statistics of speckle patterns of localized waves. The function is applied to the detection of subsurface ing is analyzed. Performance of the sensor is evaluated Mexico, 2Univ. Autónoma del Estado de Morelos, of well-aligned GaAs/AlGaAs core-shell nanowires speckles brightness and structure are associated, objects with radar. for different nanocomposite films. The sensor oper- Mexico, 3Univ. Autónoma de Tamaulipas, Mexico, have strong potential for photovoltaic applications. respectively, with coupling into and out of the sample, ates in the visible region of the spectrum. 4CREOL, The College of Optics and Photonics, Univ. of We analyze simulated reflection, transmission and while the speckle statistics reveals the conductance JWA27 Central Florida, USA. Experimental results of applica- absorption spectra of periodic arrays of these nano- distribution. Optodigital Protocol To Avoid An External Refer- JWA32 tions in a novel intrinsic Fiber-Optic Pressure-Sensor structures, showing high absorption that compares ence Beam In A Jtc Encrypting Processor, Carlos A. Spatial Combination of Optical Channels in a based on a Multimode Interference are presented. The favorably with experimental data. JWA45 Rios1, Edgar Rueda1, John F. Barrera1, Rodrigo Henao1, Multimode Waveguide, Syed H. Murshid, Jamil sensitive element consists in a single-mode - multi- Creation of Entanglement of Two Atoms Coupled Roberto Torroba2,3; 1Grupo de Óptica y Fotónica, Inst. Iqbal; Florida Inst. of Technology, USA. Spatial domain mode - single-mode fiber structure embedded in a JWA41 to Two Distant Cavities with Losses, Victor A. Mon- de Física, Univ. de Antioquia, Colombia, 2Ctr. de Inves- multiplexing allows co-propagation of multiple chan- membrane pressure. Colorimetric and SERS Detection of Explosives tenegro, Miguel A. Orszag; Pontificia Univ. Catolica de tigaciones Ópticas (CONICET-CIC), Argentina, 3UID nels of same wavelength over a single strand of optical using Plasmonic-Photonic Coupled Arrays, Alyssa Chile, Chile. We consider two microwave cavities con- OPTIMO, Facultad de Ingeniería, Univ. Nacional de la fiber. Spatial multiplexer in multimode waveguides is JWA37 J. Pasquale, Linglu Yang, Bo Yan, Bjoern Reinhard, nected with an optical fiber, we find that for different Plata, Argentina. We use a JTC optodigital approach, presented and contrasted with spatial multiplexers in Fiber Bragg Grating Strain Sensor Array Based Luca Dal Negro; Boston Univ., USA. Detection of coupling constants and atom-cavity detuning a wide but avoiding an external reference beam to record the the branching waveguides. on Multi-Wavelength Tunable Fiber Laser, Satoshi 2,4-Dinitrotoluene in part-per-billion sensitivity is plateau in time is generated in the concurrence. encoded information. We only encode a master key Tanaka, Atsushi Wada, Nobuaki Takahashi; Natl. demonstrated utilizing plasmonic-photonic scat- in a Mach-Zehnder arrangement, leading to a cor- JWA33 Defense Acad., Japan. A fiber-optic strain sensor array tering in gold nano-particle arrays with different JWA46 responding simpler encrypting procedure. Coherence-Converting Plasmonic Hole Arrays, using a multi-wavelength laser is proposed, in which lattice constants. We show that plasmonic-photonic Au Nanoparticle-Assisted Random Lasing from Greg Gbur1, Yalong Gu1, Choon How Gan2, Taco D. FBGs are used as wavelength selection components. resonances of nanoparticle arrays can be utilized in GaN Powder, Toshihiro Nakamura, Tomohiro JWA28 Visser3; 1Univ. of North Carolina at Charlotte, USA, In the experiment, simultaneous multi-point strain SERS sensing of DNT. Hosaka, Sadao Adachi; Gunma Univ., Japan. We 2

Microscope Multifocus Image Fusion based on Lab Charles Fabry de l’Inst. d’Optique, Univ. Paris- measurements are demonstrated with higher resolu- demonstrate random lasing from powdered GaN as- Wednesday, October 27 a Zernike Moment Algorithm, Alfonso Padilla- Sud, France, 3Delft Univ. of Technology and Free Univ. tion and S/N ratio. JWA42 sisted by Au nanoparticles. GaN band edge emission Vivanco, Carina Toxqui-Quitl; Univ. Politecnica de Amsterdam, Netherlands. Simulations are presented Development of a System to Detect Ethanol Vapor is enhanced by depositing Au. The enhancement is Tulancingo, Mexico. A novel technique of microscope that demonstrate that the global state of coherence of JWA38 Using a CCD Camera in an Interferometer, Carlos caused by surface plasmon. We find lasing lines ap- multifocus image fusion using Zernike moments a wavefield can be altered on transmission through Index Contrast Measurement Using Scanning Martinez-Hipatl, Severino Muñoz-Aguirre, Juan pear in this sample. is presented. The test images are obtained by both a hole array in a metal plate that supports surface Optical Frequency Domain Reflectometry, Eric D. Castillo-Mixcoatl, Georgina Beltran-Perez; Benemerita the bright field and DIC techniques. Numerical and plasmons. Moore, Robert R. McLeod; Univ. of Colorado, USA. We Univ. Autonoma de Puebla, Mexico. The response JWA47 experimental results are presented. demonstrate direct measurements of local refractive of a polydimethylsiloxane sensor was measured Fano Resonances and Electromagnetically Induced JWA34 index contrast using a scanning optical frequency using an interferometer and a CCD camera. The Absorption and Transparency-like Effects in Single JWA29 Transmission Characteristics of Silver Nano- domain reflectometer. Measurement results for step advantage is to have a great amount of sensors. From Silica Microspheres, Sile Nic Chormaic1,2, Yuqiang Discrete Solitons in Novel Two Dimensional Wave- Apertures, Lei Zhu, Sarath Samudrala, Mutiah index fiber, gradient index fiber, and a volume holo- ethanol responses was found that the system works Wu 2,1, Jonathan Ward2, Amy Watkins2,1; 1Univ. College guide Arrays, Angel Vergara Betancourt, Erwin A. Annamalai, Nikolai M. Stelmakh, Michael Vasilyev; graphic grating are presented. appropriately. Cork, Ireland, 2Tyndall Natl. Inst., Ireland. Fano reso- Martí Panameño, Gregorio Mendoza González, Luz del UTA, USA. The polarization-dependent transmission nances and electromagnetically induced absorption Carmen Gomez Pavón; Benemerita Univ. Autonoma spectra of silver nanoapertures are investigated. A JWA39 JWA43 and transparency-like effects have been observed in de Puebla, Mexico.Based on the numerical experi- strong transmission loss in the region of plasmonic Transmission OoThree Co-propagating Channels Generation of a Narrowband Biphoton in a Two- a microsphere coupled with a tapered fiber. Applica- ment techniques we demonstrate the existence of resonance and a suppression of cut-off attenuation in of Same Wavelength in Step Index Multimode Fi- Level System with an Intermediate Metastable tions lie in enhancing the sensitivity of biosensors and bi-dimensional discrete solitons in novel waveguide the donut aperture are observed. bers for Lan Applications, Syed H. Murshid, Abhijit State, Anton V. Sharypov, Arlene D. Wilson-Gordon; controlling the group velocity of light. arrays, for which the required generation energies Chakravarty; Florida Inst. of Technology, USA. Spatial Bar-Ilan university, Israel. We show that, due to lower than in the honeycomb array. JWA35 domain multiplexing (SDM) allows co-propagation four-wave mixing, narrowband biphotons with a JWA48 FDTD Simulation of Photonic Crystal Vertical- of multiple spatially separated channels over a single controllable waveform can be produced in a pumped Bases for Focused Waves in Two Dimensions, JWA30 Cavity Surface-Emitting Lasers, Gregory R. Kilby, strand of step index multimode fiber. Three such SDM two-level system that decays via an intermediate Krista Lombardo1, Miguel A. Alonso2,3; 1Dept. of Active and Passive Photonics Devices Produced by Lisa Shay; United States Military Acad., USA. Pho- channels for LAN applications are reported. metastable state. Physics and Astronomy, Univ. of Rochester, USA, 2Inst. Direct Writing with Femtosecond Laser Pulses in tonic crystal vertical-cavity surface-emitting lasers of Optics, Univ. of Rochester, USA, 3Dept. of Applied Novel Transparent Materials, Thiago B. N. Lemos1, have potential applications in optical interconnects, Physics, Aalto Univ., Finland. We present a new fam- Davinson M. Silva2, Luciana R. P. Kassab3, Anderson S. extended area coherent sources, and steerable beams. ily of closed-form solutions to the two-dimensional L. Gomes1; 1UFPE, Brazil, 2Dept. of Electronic Systems Full three-dimensional FDTD simulations are used Helmholtz equation, which form a complete basis Engineering, Brazil, 3Faculty of Technology of São Paulo to understand the effects of fabrication variances and are nonparaxial analogs of the Hermite-Gauss (FATEC-SP), Brazil. Active and passive waveguides in these devices. beams. Their scattering off circular obstacles is also fabricated in tellurite and GeO2-PbO-Ga2O3 (GPG) discussed. glasses using direct femtosecond laser (at 800 nm, 1 kHz, 130 fs) writing is demonstrated. Internal gain of 2.7dB/cm is obtained at 1535 nm.

FiO/LS 2010 • October 24–28, 2010 83 Empire Hall, Rochester Riverside Convention Center JOINT FiO/LS

JWA • FiO Poster Session II—Continued

JWA49 JWA53 JWA56 JWA59 JWA62 Image-Plane Reflection-Type Alcove Multiplex Role of Nonlinearity and Transverse Localiza- Modal Gain Analysis of GaNAsP Heterostructures Spectroscopic Ellipsometry Study of a Swiss Cross Interferometric Measurement of Thickness and Re- Hologram, Yih-Shyang Cheng, Zen-Yuan Lei, Chih- tion of Light in a Disordered Coupled Optical on Silicon, Nektarios Koukourakis1, Dominic A. Metamaterial, M.L. Miranda- Medina1,2, B. Dast- fraction Index on Transparent Thin Films Hung Chen; Dept. of Optics and Photonics, Natl. Cen- Waveguide Lattice, Somnath Ghosh1, Bishnu P. Funke1, Nils C. Gerhardt1, Martin R. Hofmann1, malchi2, H. Schmidt3, E.-B. Kley3, I. Bergmair4, K. Carlos A. Vargas1,2, Edwin Tangarife1; 1Inst. de Física, tral Univ., Taiwan. A three-step holographic process, Pal1, R. K. Vrshney1, Govind P. Agrawal2; 1Indian Inst. Bernardette Kunert2, Sven Liebich3, S. Zinnkann3, M. Hingerl2, J.J. Sanchez-Mondragon1; 1INAOE, Mexico, Univ. de Antioquia, Colombia, 2Facultad de Ingenieria, which enables the incorporation of the image-plane of Technology Delhi, India, 2Inst. of Optics, USA. We Zimprich3, A. Beyer3, S. Chatterjee3, C. Bückers3, S. W. 2Johannes Kepler Univ., Austria, 3Inst. of Applied Phys- Univ. Católica de Oriente, Colombia. A Mach-Zenhder technique in the fabrication of the reflection alcove report a numerical investigation on the transverse Koch3, K. Volz3, W. Stolz3; 1Ruhr-Univ. Bochum, Ger- ics, Friedrich-Schiller-Univ., Germany, 4PROFAC- interferometer is proposed with a thin film on one of multiplex hologram, is described. Experimental localization of light in a lattice of disordered coupled many, 2NAsP III/V, Germany, 3Philipps-Univ. Marburg, TOR GmbH, Austria. We present spectroscopic its arms, the sample can be rotated, measuring the pat- result demonstrating the feasibility of this method waveguides. The interplay of disorder with medium’s Germany. We present modal gain measurements of ellipsometry measurements of a metamaterial, taken tern fringes for each incidence angle, sample thickness is presented. nonlinearity in localization from application point of GaNAsP multiple quantum well structures grown under different incidence-angles and compared with and refraction index are calculated. view is studied. lattice-matched on silicon using the stripe-length calculations based on the RCWA method. We find that JWA50 method. High modal gain values of up to 80 cm-1 resonances for (Psi, Delta) do not disappear changing JWA63 Characterization of a Low Voltage Micro-Electron- JWA54 are observed at room temperature. the incidence angle. Phase Diversity Selection Using Spatial Light Column for Scan Field Size and Visibility of Current Temperature Dependence Of Closed Mode Q- Modulator, Norihide Miyamura; Univ. of Tokyo, Image, Won K. Jang1, Jun Ho Park1, Ho Seob Kim2; Factor In Terahertz Metamaterial Superlattice, JWA57 JWA60 Japan. We used a spatial light modulator to generate 1Hanseo Univ., Korea, Republic of, 2Sunmoon Univ., J. H. Woo1, E. S. Kim1, Boyoung Kang1, E. Y. Choi1, Capabilities of Trapping in Single Gratings and Directional Etching Methods for Realizing Wood- phase diversities (PD). The laboratory experimental Korea, Republic of. The optical technology for focus- Hyun-Hee Lee1, J. Kim1, Y. U. Lee1, Tae Y. Hong2, Jae Switching in Double-Sided Gratings for Normal pile Photonic Crystal with Different Crystal Ori- results show that the estimation accuracy of the ing and manipulating electron beam was applied for H. Kim2, J. W. Wu1; 1Ewha Womans Univ., Korea, Incident Light, Hideo Iizuka1, Nader Engheta2, entations, Lingling Tang, Shu-Yu Su, Ozlem Senlik, wavefront aberration is improved using the optimal the optimal operation for many applications such Republic of, 2Yonsei Univ., Korea, Republic of. Tera- Hisayoshi Fujikawa3, Kazuo Sato3, Yasuhiko Takeda3; Tomoyuki Yoshie; Duke Univ., USA. High-precision PD instead of conventional defocus PD. as large area scanning LCD panel and aberration hertz metamaterial superlattice is fabricated with 1Toyota Res. Inst., USA, 2Univ. of Pennsylvania, USA, three-dimensional woodpile photonic crystal and Please add: compensated beam shaping for fine scanning com- double-split ring resonators oriented alternately. By 3Toyota Central R&D Labs, Japan. We present a high-quality-factor nanocavities in various crystal JWA64 munication devices. cooling down to cryogenic temperature 4K, changes technique for light trapping into the SiO2 substrate orientations are fabricated with two types of direc- in Q-factor of closed mode resonance originating using a TiO2 grating, and the switching capability of tional etching methods in a simple two-patterning Physics of Light and Optics: A Free Online Text- JWA51 from coherent coupling in metamaterial superlattice the double-sided gratings with the horizontal quarter- process. book, Justin Peatross, Michael Ware; Dept. of Physics Observation of Soliton-based Image Transmis- is investigated. period shift between the top and bottom gratings. and Astronomy, Brigham Young Univ., USA. We high- sion Through Self-Defocusing Photonic Lattices, JWA61 light an electronic textbook available free of charge in Yi Hu1,2, Peng Zhang1, Masami Yoshihara1, Jianke JWA55 JWA58 Wavefront Sensing, Melquiades Soto Garcia, Fermin PDF format at optics.byu.edu. The target audience is Yang 3, Zhigang Chen1,2; 1San Francisco State Univ., Versatile 780-nm Pump Source for High-Repetition Mimicking an Amplitude Damping Channel for A. Granados, Alejandro R. Cornejo; INAOE, Mexico. upper-division physics undergraduates. USA, 2Nankai Univ., China, 3Univ. of Vermont, USA. Rate Entanglement Generation, Jemellie Galang, Laguerre Gaussian Modes, Angela Dudley1,2, M. Wavefront. The irradiance transport equations ex- We demonstrate that self-defocusing photonic lattices Joshua C. Bienfang, Charles W. Clark; NIST, USA. Nock1, T. Konrad1, F. S. Roux2, A. Forbes1,2; 1School of press the relation between wavefront and its intensity. JWA65 support various shapes of soliton clusters (such as We demonstrate a tunable pump source based on Physics, Univ. of KwaZulu-Natal, South Africa, 2CSIR We propose to solve the ITE using the approximation Radiation Scattering by Localized Electron Wave Y-shape and H-shape) which remain robust dur- frequency-doubled EDFA-amplified pulses carved Natl. Laser Ctr., South Africa. An amplitude damp- of derivatives by finite differences instead to get the Packets, John P. Corson, Michael Ware, Scott Glas- ing propagation. We propose soliton-based image from a narrow-line CW laser at rates up to 1.25 GHz. ing channel for Laguerre-Gaussian (LG) modes is wavefront for optical testing. gow, Justin Peatross; Brigham Young Univ., USA. We transmission through photonic structures induced We find self-phase modulation in the EDFA limits the presented. Experimentally the action of the channel examine the role of wave-packet localization in the in bulk materials. peak output-pulse power. on LG modes is in good agreement with that predicted dynamics of radiation scattering by free electrons. theoretically. The applicability of classical field assumptions is JWA52 discussed. Ultrafast Optics Used to Study Carrier Dynamics of High Quality Silicon on Glass Sample, Omar S. 1 2 Wednesday, October 27 Wednesday, Magaña-Loaiza , Roman Sobolewski , Jose J. Sanchez- Mondragon1, Carlo Kosik-Williams3, Jie Zhang2; 1Natl. Inst. for Astrophysics Optics and Electronics, Mexico, 2Univ. of Rochester, USA, 3Corning Inc, USA. We study, experimentally and theoretically, the carrier dynamics in high quality silicon on glass sample by a model that relates the reflectance time dependence with the carrier dynamics.

84 FiO/LS 2010 • October 24–28, 2010 NOTES ______

______Wednesday, October 27 ______

FiO/LS 2010 • October 24–28, 2010 85 Wednesday, October 27 86 SWA1 •1:30p.m. Technologies, USA,Presider Herwig Kogelnik; Lucent Symposium I SWA •OpticalCommunications 1:30 p.m.–3:30p.m. SWA2 •2:00p.m. ing, USA.Abstract not available. Development of Fibers, Low-Loss Tingye Li; AT&T Labs, USA.Abstract not available. Communications, Optical of Overview Historical Highland A Invited Invited P. Schultz; - Corn plasmonic antennas are presented. on based structures slow-light broad spectrally of of double-Fano resonance. Specific implementations phenomenon the Weutilize proposed. is structures Austin, at Texas of USA. Univ. Khanikaev; Alexander Fondamentale, Univ. Paris Sud, France, ty Applications, Slow-Light Metamaterialsfor Plasmonic Infrared Daniele Costantini Daniele We probe SSP the mid-infrared via imaging. etched facet of a mid-infrared quantum-cascade laser. is directly excited on a metal/air interface using a dry device for surface plasmon(SP)generation. A SP mode Nanostructures,France. Presider to Announced Be Processing I Metamaterials forInformation FWO •Plasmonicsand 1:30 p.m.–3:30p.m. ESPCI ParisTech,France, ESPCI goire Beaudoin Polaritons, Mid-Infrared Direct Coupling of Surface-Plasmon FWO2 •2:00p.m. FWO1 •1:30p.m. 2 , Ioana Moldovan-Doyen A new approach to slowing light in plasmonicapproachin slowing lightnew to A Adel Bousseksou 3 , Isabelle Sagnes Gennady Shvets Gennady Highland B 1 , , Raffaele Colombelli We demonstrate a compact a Wedemonstrate Invited 3 2 Lab de Photonique et de et Photonique de Lab , Yannick De Wilde 1 , Jean-Philippe Tetienne 3 ; 1 Inst. d’Electronique , Chih-Hui Wu, Wu, Chih-Hui , 2 1 Inst. Langevin, , Arthur Babu Arthur , 2 , Gré- FiO/LS 2010 1 - , electric dipole term. electric the maximizing by maximized be can focus the at field electric The components. multipole magnetic and electric of sum a as expressed be can sphere Singapore. pard FWP1 •1:30p.m. focusing properties of optical the field. nanoscale the on effect crucial a have to shown are structures. Polarization and modal degrees of freedom plasmonicusing light ofconfinement tight onwork Israel. Jerusalem, Univ.of Hebrew Desiatov; Boris Goykhman, Yanai,Ilya Avner man, Tight Confinement of Light, for Freedom of Degrees Modal and Polarization Polarization and the Focusing of Light, Univ. of Rochester, USA,Presider Thomas G.Brown; Inst. of Optics, Unconventional Polarization II FWP •OpticalDesignwith 1:30 p.m.–3:30p.m. FWP2 •2:00p.m. ; Div. of Bioengineering, Natl. Univ. of Singapore,

The field on the Gaussian reference Gaussian the on field The • Highland C FiO October 24–28,2010 Invited Invited Uriel Levy

We describe our describe We Colin Colin Shep , Gilad Ler - - Quantum Dots, Quantum InAs Single of Spectroscopy Broadband Efficient forWaveguides GaAs Suspended Fiber-coupled FWQ1 •1:30p.m. mode delocalizationmode and slow light effects. and a substrate. We show that the force is enhanced waveguide by silicon periodically-patterned a between fornia, USA. Jing Ma, Force in Periodically-Patterned Silicon Waveguides, Optical Attractive of Investigation Theoretical Jelena Vuckovic FWQ3 •2:00p.m. T. RakherT. Makarova Los Angeles, USA,Presider Bahram Jalali; Univ. of California at Slow Light FWQ •PhotonicBandgapand 1:30 p.m.–3:30p.m. 3 1 Crystal Nanobeam Cavities, Cavities, Nanobeam Crystal Photonic to Coupled Nitride Silicon doped Erbium- in Narrowing Linewidth of Observation FWQ2 •1:45p.m. at different optical pump powers. cavities is studied at cryogenic and room temperatures the from Photoluminescencelayer. nitride silicon amorphous Er-doped an in fabricated are cavities USA. tion by one order of magnitude. - collec exceedingfree-space into collection fiber the tion of individual dots is performed, with fluorescence of InAs quantum dots. Above-band and p-shell excita- waveguides are for realized broadband spectroscopy Dept. of Astronomy and Physics, USA. CNST - NIST, USA, NIST, - CNST One-dimensional nanobeam photonic crystal crystal photonic nanobeam One-dimensional Michelle L. Povinelli 1 1 , Selcuk YerciSelcuk , , Antonio Badolato Antonio , We investigate the attractive optical force 1 ; Highland D 1 Stanford Univ., USA, Marcelo I. Davanco I. Marcelo 2 Maryland Nanocenter, USA, USA, Nanocenter, Maryland 2 , Rui Li Rui , Invited ; Univ. of Southern Cali - 3 Yiyang GongYiyang , Kartik Srinivasan Kartik , 2 , Luca Dal Negro Dal Luca , Fiber-coupled 2 Boston Univ., 1,2 , Matthew , 1 , Maria , 1 2 , ; ley Natl. Lab, USA, Lab,Natl. ley Michigan presented. be will of University the at facilities laser T-cubed the and efforts in laser-driven ion acceleration at the Hercules the performed theoretical work and the experimental Maksimchuk Ion Acceleration with Ultra-Intense Lasers, Shaping, Recent Advances in Proton Acceleration and Beam S. Busold S. F. NürnbergF. FWR2 •2:00p.m. Los Angeles, USA,Presider Chan Joshi; Univ. of California at Acceleration II BasedParticle FWR •Laser 1:30 p.m.–3:30p.m. of warm-dense-matter. etries for ion-driven fast-ignition and the generation geom- using results and targets new and structures beam-transport with ion-beams laser-accelerated combine and control to experiments on focus with USA. many, . Grote P. FWR1 •1:30p.m. Germany, Schumacher Germany, A report on recent-developments be will given 2 Helmholtzzentrum für Schwerionenforschung, 5,6 1 , K. Harres K. , , T. CowanT. , 4 Markus Roth Markus 3 Sandia Natl. Labs, USA, Forschungszentrum Dresden-Rossendorf, Dresden-Rossendorf, Forschungszentrum 1 1 ; Univ. of Michigan, USA. , G. Schaumann G. , ; 1 Technische Univ. Darmstadt, Ger TechnischeUniv.Darmstadt, Highland E 6 Lawrence Livermore Natl. Lab,Natl. Livermore Lawrence 3 1 , O. Deppert O. , , G. Hoffmeister G. , 1 , V.Bagnoud , Invited Invited 1 , M. Schollmeier M. , 1 5 , M. Geissel M. , Lawrence Berke Lawrence An overview of 1 2 , G. Logan G. , , T. Burris T. , Anatoly Anatoly 4 4 , D. , , D. , 3 5 - - , , Wednesday, October 27 87 ; - 3 , An Oleg 2 ; Iowa State Univ., Univ., State Iowa ; , Nazario Martín Nazario , , Vladimir Dyakonov Vladimir , 2 3 - Ma de Complutense Univ. 2 Invited Invited JosephShinar Highland K Highland , Carsten Deibel Carsten , 3 Julius-Maximilians Univ. of Würzburg and and Würzburg of Univ. Julius-Maximilians 3 , Salvatore Filippone Salvatore , 1 Optically Optically and electrically detected magnetic Argonne Natl. Lab, USA, Lab, Natl. Argonne USA. resonance studies of luminescent thin π-conjugated films and organic light-emitting devices (OLEDs) have provided striking insight into their various excitations. LWI1 • 1:30 p.m. • 1:30 p.m. LWI1 • 2:00 p.m. LWI2 Germany. V., e. Res. Energy Applied for Ctr. Bavarian in thin polymer-fullerene films of polarons Charged electron light-induced by investigated are composites paramagnetic resonance. Comparative analysis of photogenerated charge separation states in organic photovoltaic cells and natural photosynthetic - pro given. are teins drid, Spain, Spain, drid, Optically and Electrically Detected Magnetic - Ma Light-Emitting Organic of Studies Resonance Devices, and terials Spin Signatures of Light Induced Charge Separated Charge Induced Light of Signatures Spin Bulk-Heterojunctions: Polymer-Fullerene in States High-Frequency Pulsed EPR Spectroscopy, Poluektov 1:30 p.m.–3:30 p.m. 1:30 p.m.–3:30 Photophysics of Energy • LWI II Conversion USA, Univ., Emory Lian; Tianquan Presider 1 dreas Sperlich dreas Chris T. ; Univ. ; of Univ. Wisconsin at Invited Invited - Madi at Wisconsin of Univ. ; LS Highland J Highland Multiply Multiply resonant methods create John Wright MartinZanni This talk will cover recent developments in developments recent cover will talk This LWH2 • 2:00 p.m. LWH2 Multiply Multiply Resonant Coherent Multidimensional Spectroscopy, Middleton, Middleton, USA. son, for technology shaping pulse femtosecond of use the - appli their and spectra Vis 2-D and IR 2-D collecting topics. energy related and biophysical to cations Madison, USA. multidimensional of measurement domain frequency involving coherences quantum multiple using spectra states quantum vibrational and electronic individual and coherent their of measurement domain time and examples. discuss many We dynamics. incoherent Advances Advances in Ultrafast 2-D Spectroscopy, 1:30 p.m.–3:45 p.m. 1:30 p.m.–3:45 I: Chemical Dynamics • LWH Ultrafast Multi-Dimensional Spectroscopy of Univ. Ogilvie; P. Jennifer USA, Presider Michigan, • 1:30 p.m. LWH1 , Boris Sergiy 1 , Vadim Vadim , 2 We investigate phase investigate We , Amiel A. A. Amiel Ronen, Eitan , George Venus OptiGrate OptiGrate Corp., USA. 1 CREOL, CREOL, The College of 2 1 ; 1 October 24–28, 2010 , Christine Spiegelberg Christine , 1 • Highland H Highland We demonstrate phase locking of a linear linear a of locking phase demonstrate We , Amiel A. Ishaaya; Ben Gurion Gurion Ben Ishaaya; A. Amiel Ronen, Eitan , Leonid Glebov 1 , Apurva Jain Apurva , , Oleksiy Andrusyak 1 2 Zeldovich Multiplexed Bragg grating recorded in photo-thermo- in recorded grating Bragg Multiplexed coherent for combiner efficient be can glass refractive locking of high-power lasers. Spectral properties of are two-channel combiner studied theoretically and experimentally. Multi-channel scaling of this - ap discussed. is proach 1:30 p.m.–3:00 p.m. 1:30 p.m.–3:00 General Laser • LWG Science Air Naval Narducci; A. Francesco USA, Presider Command, Systems LWG3 • 2:00 p.m. LWG3 Novel a and Arrays Laser in LockedClusters Phase Them, Detecting For Method Israel. Univ., Gurion Ben Ishaaya; in locked a clusters diffractively linear coupled fiber phase observedistinct experimentally We array. aser method novel a demonstrate and clusters laser locked the array. of coherence the spatial measuring for Optics Optics and Photonics, USA, LWG2 • 1:45 p.m. LWG2 Multiplexed Reflective Volume Bragg Grating for Passive Coherent Beam Combining, Mokhov Smirnov LWG1 • 1:30 p.m. LWG1 PhaseLocking Diffractive Laser Fiber a Via Array Coupling, Israel. Univ., array of seven fiber lasers via diffractive coupling. of 82% was contrast the Fringe measured at far field very with locking high efficiencies. anti-phase for , 2 FiO/LS 2010 We

Dept. Dept. 4 , Robert Robert , , Victor 3 3 We experimentally We Solid Solid State Inst., Israel, , Yaroslav V. Kartashov V. Yaroslav , 1 1 ; 2 Invited , Matthias Heinrich Matthias , 3 , Andreas Tünnermann 3 Highland G Highland Inst. of Applied Physics, Germany, Germany, Physics, Applied of Inst. 3 , Lluis Torner 4 , Felix Dreisow Felix , 3 AlexanderSzameit , Jin-Kyu Yang, , Heeso Yang, Jin-Kyu Noh, Seng-Fett Liew, , Stefan Nolte 3 ICFO, Spain, Spain, ICFO, FWT1 • 1:30 p.m. Keil 2 1:30 p.m.–3:30 p.m. 1:30 p.m.–3:30 In Integrated FWT • Disorder and Circuits II Optical Devices Be Announcedr to Presider A. Vysloukh demonstrate demonstrate disorder-induced localization near a boundary of truncated one-dimensional disordered photonic lattices and uncover that localization near the boundary requires a higher disorder level than lattices. in bulk Mexico. de Fisica y Matematicas, FWT2 • 2:00 p.m. Anderson Surface in Waves Disordered Photonic Lattices, Peter Zeil Peter Evolution of Photonic Band-Gap and Lasing and from Band-Gap Photonic of Evolution Structures, Photonic Amorphous to Polycrystalline Hui Cao Carl Schreck, Corey O’Hern; USA. Univ., Yale of density photonic of gap the in transition a out map structures. polycrystalline amorphous to from states Lasing has been realized in both polycrystalline and amorphous photonic structures with distinct characteristic. ; FiO , A. Simic, Simic, A. , We We present Bruce Smith Invited Invited Shaya Y. ShayaFainman Y. Highland F Highland O. Bondarenko, B. Slutsky, A. Mizrahi, M. P. Nezhad; Nezhad; M. P. A. Mizrahi, B. Slutsky, Bondarenko, O. of Univ. California at San Diego, USA. of combination a using paradigms nanophotonic new - nano composite semiconductor and metal, dielectric, structures and devices for optical communications, sensing. and signal processing, and information FWS1 • 1:30 p.m. 1:30 p.m.–3:30 p.m. 1:30 p.m.–3:30 and meta- FWS • Nanopatterning materials Delaware, of Univ. Lu; Zhaolin USA, Presider FWS2 • 2:00 p.m. Nanopatterning Nanopatterning Technology and the Future of 32nm, beyond Devices Semiconductor Dept. of Microelectronic Engineering, Rochester Inst. of of Inst. Rochester Engineering, Microelectronic of Dept. available. not USA. Abstract Technology, Active and Passive Nanophotonics for Information Information for Nanophotonics Passive and Active Applications, Systems Wednesday, October 27 88 Southampton, UK.Abstract not available. SWA3 •2:30p.m. Title to Be Announced, Be to Title Symposium I—Continued SWA •OpticalCommunications Thank youforattending know yourthoughtson post-conference survey via emailandletus Look foryour the program. Highland A FiO/LS.  Invited David Payne David ; Univ.of ; Engheta recently reported [B. D. F. Casse Casse F.D. [B. reported recently three-dimensional metamaterials nanolens has been Univ.,USA. ern NortheastSridhar;- Srinivas Menon,Latika Gultepe, Wentao, Casse Frederic T. Lu, Yongjian Huang, Evin Nanolens, Metamaterials wires Nano- 3-D a Using Limit Diffraction the Beating FWO3 •2:15p.m. Platform, ticles in an Integrated Hybrid Photonic-Plasmonic Excitation of Individual Gold Plasmonic Nanopar FWO4 •2:30p.m. tion of incident field. connected in series or parallel depending on - polariza elementscircuitlumped two-dimensionaloptical as with deep subwavelength cross sections may operate Processing I—Continued Metamaterials forInformation FWO •Plasmonicsand perimentally verify that arrays of Si of arrays that verify perimentally USA. Austin, at extensive control experiments. the superresolution imaging by the nanolens through Lett.96,023114(2010)]. Here, we present validation of Yong Sun Yong Wavelengths,IR at Elements Circuit Lumped cal VerificationExperimental of the Concept of Opti - FWO5 •2:45p.m. enhancementsfield are achieved on-chip. are used to extract nanoparticle coupling ratios. Large strated. Transmission amplitude and phase responses structures is theoretically and experimentally demon- dividual plasmonic nanorods using integrated Si3N4 Tech,USA. GeorgiaYegnanarayanan, Adibi;Siva Hosseini,Ali 1 ; 1 1 Bin Edwards Brian , Univ. of Pennsylvania, USA, Maysamreza Chamanzar Maysamreza Efficient and controlledin- excitationandof Efficient Highland B Using FTIR spectrometry, we ex- we spectrometry, FTIR Using Super-resolution imaging using a using imaging Super-resolution 1 , Andrea Alù Andrea , et al. et Bernard Didier Didier Bernard 2 3 , Ehsan Shah Ehsan , Univ. of Texas N 4 Appl.Phys. nanorods 1,2 , Nader Nader FiO/LS 2010 - Univ. of Ireland Galway, Ireland, land, Natl.Physics,Univ.of School Ireland, of Galway, Ire - This can be observed via fine splitting fine via ofThis observed can caustics. be interaction. spin-orbit the describing contribution polarization-dependent a has momentum angular orbital The field. electromagnetic monochromatic spinandorbitalangular momentanon-paraxial a of Applied Physics, Aalto Univ., Finland. Dainty Bliokh Space, Free in Light Nonparaxial of Interaction Spin-Orbit and Momenta Angular FWP4 •2:45p.m. CollegeLondon, UK, Herrera spin-Hall of light. effect observe sensitive angular momentum conversion and to the polarization distribution of the output light. We translatesoflight which subwavelength information nanoparticle is accompanied by spin-orbit interaction Univ.,Australia.Natl. lian Continued Unconventional Polarization II— FWP •OpticalDesignwith of Light, Interaction Spin-Orbit via Nanoprobing Optical FWP3 •2:30p.m. 2 Inst. of Optics, Univ. of Rochester, USA, 1 1 ; , Miguel A. Alonso A. Miguel , 1 1 , David Lara David , Applied Optics Group, School of Physics, Natl. Konstantin Y. Bliokh • Highland C 3 2 NonlinearPhysics Ctr., Austra - FiO , Elena A. OstrovskayaA. Elena , October 24–28,2010 2,3 Optical microscopy of a of microscopy Optical ; 1 Applied Optics Group,OpticsApplied 1 2 , Oscar G. Rodriguez- Blackett Lab, Imperial We calculate the Konstantin Y. Konstantin 3 Dept. Dept. of 3 , Chris , YuzheXiao Dynamic Frequency Shifts in Photonic Structures, FWQ5 •2:45p.m. 1 structures. photonicintegrated of range broad a study to plied ap- be can method This structures. photonic linear in occurring shift frequency dynamic the study to USA. DFB configuration. multi-segment by smoothed and enhanced be can incorporated slab-waveguide. Transmission spectrum effect at 1.55 micron wavelength in sub-micron DFB- modulatorEO slowbyutilizinglight forMZI-based nic Inst., USA. Shengling , Deng Z.Rena Huang; Rensselaer Polytech- Dimension Reduction of Electro-optic Modulators, Slow Light Effect in Distributed Feedback (DFB) for FWQ4 •2:30p.m. Slow Light—Continued FWQ •PhotonicBandgapand Univ. of Rochester, USA, Wesimpleapproachdevelopa systems-theory 1 , Drew N. MaywarN. Drew , A length reduction of 3-fold is shown Highland D 2 Rochester Inst. of Technology, 2 , GovindP., Agrawal 1 ; this novelthis erafor acceleration. particle efficient GeV GeV energies predicted at intensities beyond 10 is poised to revolutionize laser ion acceleration - with Germany.tenoptik, Power Laser Pulses, cm FWR3 •2:30p.m. Acceleration II—Continued BasedParticle FWR •Laser Particle Acceleration by the Light Pressure of High- 2 . First experimental results reveal the beginning of Highland E Radiation Pressure AccelerationPressure Radiation Joerg Schreiber; MPI für Quan- Invited 21 W/ Wednesday, October 27 89 , Okan Okan , Optical 2 1,2 We studied studied We NRL, USA, 1 ; 2 , Joseph S. Melinger S. Joseph , 1 Invited Highland K Highland Paul Lane Paul , Edwin J. Heilweil 2 Carrier Dynamics of Films of Zinc Phthalocyanine Zinc of Films of Dynamics Carrier LWI • Photophysics of Energy Photophysics of Energy • LWI II—Continued Conversion Esenturk and C60 Measured by Terahertz Time Domain Spectroscopy, Technology Div., Physics Lab, NIST, USA. NIST, Lab, Physics Div., Technology photocarrier dynamics in organic photovoltaics by THz terahertz time Transient domain spectroscopy. absorption decays in C60 and zinc phthalocyanine span a wide range of timescales and reveal how to yields. photocarrier optimize LWI3 • 2:30 p.m. • 2:30 p.m. LWI3 - Invited LS Two-dimensional Two-dimensional femtosecond , Kristina , C. Kristina McCamant David W. Highland J Highland ; Univ. Kevin of ; J. Michigan, Kubarych Univ. Using Using equilibrium and non-equilibrium - mul LWH • Chemical Dynamics I: Chemical Dynamics • LWH Ultrafast Multi-Dimensional Spectroscopy—Continued LWH4 • 2:45 p.m. LWH4 Watching Chemical Reactions and Dynamicswith and Chemical Reactions Watching Spectroscopy, Infrared Multidimensional Ultrafast Carlos R. Baiz, Jessica M. Anna, Robert McCanne, King, T. John USA. tidimensional infrared spectroscopy, we can track chemical reactions with exquisite detail. Examples exchange, chemical ultrafast will we discuss include: bimolecular recombination, charge transfer and dynamics. solvation Wilson, Randy D. Mehlenbacher, Brendon Lyons; Univ. tional Coupling, Univ. Lyons; Brendon Mehlenbacher, D. Randy Wilson, of USA. Rochester, LWH3 • 2:30 p.m. LWH3 Raman Stimulated Femtosecond Dimensional Two Spectroscopy: A New Technique to Probe Vibra stimulated Raman spectroscopy (2D-FSRS) can potentially quantify vibrational coupling. However, far thus measured signals all that indicate results our are attributable to a 3rd-order cascade and not the mechanism. 5th-order intended - We investigated the investigated We October 24–28, 2010 • Highland H Highland A novel radiation emission from travel from emission radiation novel A ; Natl. Inst. for Materials Materials for Inst. Natl. ; Ochiai Tetsuyuki Camila Camila C. Dias, Eunézio A. de Souza; Univ. LWG • General Laser • LWG Science— Continued LWG5 • 2:30 p.m. LWG5 Comparison of Spontaneous Behavior in a - Syn chronously and Asynchronously Mode-Locked EDFL, Brazil. Mackenzie, Presbiteriana Erbium-doped-fiber-laser an of behavior spontaneous synchronously and asynchronously mode-locked operating at 10GHz. We observed that the central wavelength shifts to a lower one. This knowledge is necessary the mode-locking achieve stabilization. to LWG6 • 2:45 p.m. LWG6 Imitating the Cherenkov Radiation in Backward Directions, Japan. Science, theo- demonstrated is vacuum in particles charged ing Cherenkov the in as conical is radiation This retically. directions backward in emitted be can but radiation, particle trajectories. of LWG4 • 2:15 p.m. LWG4 Genera - of Studying Theoretical and Experimental tion and Amplification in Disc Yb:YAG Crystals, Palashov, Oleg Mukhin, Perevezentsev, Ivan Evgeniy Efim Khazanov; Inst. of Applied Physics of the - Federation. Rus Russian RAS), (IAP Sciences of Acad. sian Self-consistent calculation carried out to obtain the Yb:YAG in temperature and energy storied of amount disks taking into account amplified spontaneous emission. Studied the generation and amplification pulse-periodic and continuous for elements active in mode.

FiO/LS 2010 , Jing Jing , , D. Y. Y. D. , 2 Dynamics Hong Hong Kong 3 zhou shi zhou , Azriel Genack Azriel , 2 Sunghwan Kim, Jeongkug Jeongkug Kim, Sunghwan - the transmis measured We Univ. of Texas at San Antonio, Antonio, San at Texas of Univ. 1 ; 3 , Jing Wang Jing , 1 Highland G Highland Queens Queens College of CUNY, USA, 2 ; Seoul Natl. Univ., Korea, Republic of. Republic Korea, Univ., Natl. Seoul ; Jeon Heonsu , Zhaoqing Zhang Zhaoqing , 3 FWT • Disorder In Integrated FWT • Disorder and Circuits II— Optical Devices Continued USA, USA, Lu Wang, Azriel Wang, Z. Genack; Queens College of the City USA. York, New of Univ. FWT4 • 2:30 p.m. Measuring Transmission Eigenchannels of Wave Media, Random through Propagation sion matrix for localized and diffusive waves positioned in randomly a with filled waveguide quasi-1D scatterers and compare the results to predictions of theory. matrix random FWT5 • 2:45 p.m. Dynamics of Fluctuations of Localized Waves, Chabanov Andrey FWT3 • 2:15 p.m. in Localized Modes and Extended of Actions Lasing Crystals,Mixed Photonic Lee, Kong. Hong Technology, and Science of Univ. localizedreflect of waves fluctuations mesoscopic of the evolving contributions of short- and long-lived electromagnetic modes of the random medium. Complex transport phenomena for localized waves a modal analysis. be applying can clarified by By employing band-edge laser platforms, we produced produced we platforms, laser band-edge employing By crystals mixed photonic in binary randomly format, Lasing semiconductors. mixed to analogy photonic a actions of both extended and localized modes were crystals. photonic the mixed using achieved FiO Eric Highland F Highland Multi-beam-interference Multi-beam-interference lithography - param FWS4 • 2:45 p.m. Permanent Holographic Waveguide Arrays, USA. Colorado, of Univ. McLeod; R. Robert , Moore D. arrays waveguide optical two-dimensional Permanent are demonstrated by exposing diffusion-mediated photopolymer with a multiple-beam interference a ensures system control phase fiber-based A pattern. exposure. during pattern interference stable FWS3 • 2:30 p.m. Ge - Point of Optimization Parametric Constrained Lithography, Multi-Beam-Interference in ometries Guy M. , Burrow Thomas K. Gaylord; Georgia Tech, USA. High optimized. and analyzed systematically are eters absolute contrast and a variety of point geometries ranging from elliptical to rectilinear or rhombic demonstrated. are profiles intensity FWS • Nanopatterning and meta- FWS • Nanopatterning materials—Continued Wednesday, October 27 90 ______Highland A the design of design the various components. facilitate will model This sign. oppositehave ments function singularity when the permittivity tensor ele- is presented. Resonance cones result from the Green’s function analysis foranisotropic cylindrically media Liu kan Green’sMetamaterials:A Analysis, Function Anisotropic Cylindrically in Cones Resonance FWO7 •3:15p.m. for circularly or linearly light. polarized patterns of different symmetries we observe this effect forward and backward propagation. For metamaterial for different be can metamaterials planar thorough intensity of light transmitted at non-normal incidence Univ.; NikolayZheludev Southampton, of UK. cularly Polarized Light, Metamaterial Optical Diodes for Linearly and Cir FWO6 •3:00p.m. Processing I—Continued Metamaterials forInformation FWO •Plasmonicsand , Kevin J. Webb; Purdue Univ., USA. 3:30 p.m.–4:00p.m. Highland B Eric Plum, Vassili A. Fedotov, A Green’s Total Total Hui Coffee Break,Highland Ballroom Foyer Rochester Riverside Convention Center FiO/LS 2010 - - according to spin the state of atoms. the beam vector the of modulation spatial a produces cally pumped warm rubidium vapor. Optical pumping have vector used cylindrical beams to probe an opti- Light, Light, Radially-Polarized Using States Atomic Imaging microscopy, trapping particles FWP6 •3:15p.m. and sensing. illumination structured in used be can that pattern structured dependent wavelength a generates ence ly-like” polarized field. The surface plasmons interfer elliptical plasmonic lens illuminated by a TM “radial- Hebrew Univ. of Jerusalem, Israel. M. ,Lerman Avner Yanai, Nissim Ben-Yosef, Urielluminated with PolarizedRadially-Like Levy;Field, - Il DemonstrationPlasmonic Lens of anElliptical FWP5 •3:00p.m. Continued Unconventional Polarization II— FWP •OpticalDesignwith , G. Beadie; NRL, USA. FatemiBeadie;NRL, K. FredrikG. , • Highland C FiO NOTES October 24–28,2010 We demonstrate an Gilad Gilad We We - PCW simulations. a unique method to efficiently absorb these modes for slow group velocity modes in PCWs. We also present absorbingin wellwork not do PMLs reportedously these two nonlinearthese are effects enhanced. regime, light slow in that observed is It waveguide. process in silicon-on-insulator (SOI) photonic crystal on two photon absorption and self phase modulation College of Engineering), India. TechnologicalDelhiDelhiUniv. (FormerlySinha; K. Application, Device with Waveguide Crystal PhotonicSilicon-on-Insulator in Effects Nonlinear on Light Slow of Impact FWQ7 •3:15p.m. Georgia Tech, USA. Askari Waveguides, Crystal Photonic of tion Slow Group Velocity Modes in Numerical Simula- Absorbing for Layer Matched Perfectly Adiabatic FWQ6 •3:00p.m. Slow Light—Continued FWQ •PhotonicBandgapand , Babak Momeni, Charles M. Reinke, Ali Adibi; Highland D We previ the of some why show , Ravindra Ravindra Rawal , Swati The effect of slow light Murtaza Murtaza - of an optical wavelength. wave packets that are spread over an electron area individualon the from scale radiation the measure to USA. YoungWare;MichaelPeatross,Univ.,BighamJustin Cunningham Eric Focus, Laser Relativistic a of Side the outEmitted Packets Wave Electron Large by Photoemission FWR4 •3:00p.m. XUV and nuclear radiation. of generation cooperative to applications possible and effects WeCEP pulses. discuss laser ultra-short strong with interacting systems nuclear and atomic tion transfer and excitation of quantum coherence in Physics, Univ. of North Texas, USA. Radiation, Nuclear and X-Ray of Generation and Effects CEP Pulses: Atomic and Nuclear Coherence Excited by Optical FWR5 •3:15p.m. Acceleration II—Continued BasedParticle FWR •Laser We provide an update on an experimental effort Highland E , JacobJohansen,GraysonTarbox,, YuriDeaprtmentof; Rostovtsev We study popula- Wednesday, October 27 91 - The Nikos Invited Highland K Highland ; Natl. Renewable Energy Lab, USA. LWI • Photophysics of Energy Photophysics of Energy • LWI II—Continued Conversion pump-probe pump-probe Time-Resolved Microwave Conduc tivity technique under pulsed laser excitation is increasingly being used to study the photophysics of nanostructured photovoltaics. Its principles of systems material various to applications and operation will be discussed. Time-Resolved Time-Resolved Microwave Conductivity, Kopidakis LWI4 • 3:00 p.m. LWI4 , Steven Steven , Optical Optical , Galan , Denis 2 1 1 ; Inst. for NRL, USA. 2 , Xingcan Dai 1 Kenji Ohmori , DanielGammon, Alan D. Bristow 2

LS Highland J Highland - Technol and Standards of Inst. Natl. JILA, 1 ; , Allan S. Bracker S. Allan , 1 1 , Mark E. Siemens 1 LWH • Chemical Dynamics I: Chemical Dynamics • LWH Ultrafast Multi-Dimensional Spectroscopy—Continued LWH5 • 3:15 p.m. LWH5 Coherent Linewidths of Interfacial GaAs Quan- tum Dot Excitons and Incoherent Coupling from Quantum Well Excitons, Karaiskaj Moody Molecular Molecular Science, Japan. We have experimentally temporal the on based gate logic new a demonstrated optically An function. wave molecular a of evolution tailored vibrational wave-packet 4- implements and with arbitrary 8-element discrete Fourier-transform imaginary and inputs. real two-dimensional Fourier-transform spectroscopy two-dimensional is Fourier-transform (QDs). dots quantum GaAs interfacial used study to extractWe the temperature dependence of the QD from energy linewidth and relaxation homogeneous energy QDs. the lower to excitons well quantum • 3:30 p.m. LWH6 with a Femtosecond- Ultrafast Transform Fourier Laser-Driven Molecule, T. Cundiff T. ogy and Univ. of Colorado, USA, Colorado, of ogyUniv. and October 24–28, 2010 NOTES • Highland H Highland ; FiO/LS 2010 Highland Ballroom Foyer Rochester Riverside Convention Center Convention Riverside Rochester Foyer Ballroom Coffee Break, Highland A substantially substantially A Vladislav V. Yakovlev V. Vladislav Invited Highland G Highland 3:30 p.m.–4:00 p.m. FWT • Disorder In Integrated FWT • Disorder and Circuits II— Optical Devices Continued FWT6 • 3:00 p.m. FWT6 • 3:00 p.m. Univ. of Wisconsin at Milwaukee, USA. Milwaukee, at Wisconsin of Univ. performance of a improved Raman sensor based on enhanced light scattering in porous structures is demonstrated. Ultrasensitive Ultrasensitive Raman Sensor Based on Highly Structures, Porous Scattering , FiO Sara Coppola Space variant optics optics variant Space Highland F Highland ______Veronica Vespini, Melania Paturzo, Simonetta Grilli, Paturzo, Melania Vespini, Veronica Pietro Ferraro; CNR Inst. Nazionale di Ottica, Italy. Nano- and pico-droplets have been extracted and film liquid reservoirs or sessile drop dispensed from an or tip hot a by activated effect pyroelectric through dielectric polar on substrates. IR laser source FWS6 • 3:15 p.m. Dispensing Nanolitre Droplets for Liquid - Nano printing and Nanopatterning, FWS5 • 3:00 p.m. FWS5 • 3:00 Mirrors, ReflectivityGraded Varying Azimuthally Zachary A. ,Roth Menelaos K. Poutous, Srinivasan, Aaron PradeepPung, Eric G. Johnson; Ctr. for of Univ. Communication, Optical and Optoelectronics USA. Charlotte, at Carolina North properties. spectral and spatial useful and novel have In we this a present paper, optical novel component structures to the properties exploits of that resonant varying spectral azimuthally an filter. make FWS • Nanopatterning and meta- FWS • Nanopatterning materials—Continued Wednesday, October 27 92 each other and insomewith noise. cases, in the NLS (Non-Linear Schrödinger) equation with from interaction of the dispersive and nonlinear results terms important!) (but surprising some describe LucentTechnologies Labs, USA. , TransmissionOptical Systems, Long-Haul in Noise and Nonlinearities Solitons, Modulators, and Lasers DFB Semiconductor of Development SWB2 •4:30p.m. SWB1 •4:00p.m. Alcatel-Lucent, USA,Presider Colin J. McKinstrie; Bell Labs, Symposium II SWB •OpticalCommunications 4:00 p.m.–5:30p.m. not available. ; Lehigh Univ.,USA. Lehigh KochT.; Highland A Invited Invited L. Mollenauer; In this talk, I shall shall I talk, this In Abstract Bell Bell length confinement. subwavewith light- guide effectively cannanoshells The excitation of propagating plasmon modes in the cores. dielectric cylindrical nano-shelled metallic in waveguides plasmonic of kind new a on Wereport Technology,Australia, through structure. the propagation energy on effect no has waveguide the and load the mismatch impedancebetween the that showing cavities, and loads terminal with guides wave- one-way in wavespropagating of interaction USA. Pennsylvania,of Loads, of Matching Impedance One-WayandWaveguides FWU3 •4:30p.m. Technology, Netherlands, Presider Taco D. Visser; Delft Univ. of Processing IV Metamaterials forInformation FWU •Plasmonicsand 4:00 p.m.–5:15p.m. conventional methods. in as length waveguide the changing physically without measured is loss The configuration.(ATR) reflection attenuatedtotal the on based waveguides metal-insulator-metal in modes plasmonic of tion Tech,USA. Reflection, TotalAttenuated by WaveguidesInsulator-Metal Metal- in Modes Plasmonic in Measurement Loss FWU2 •4:15p.m. Turner Mode Confinement, Mode Subwavelength with WaveguidePlasmonic A FWU1 •4:00p.m. 1,2 , Baohua JiaBaohua , Ndr nht; Univ. Engheta; Nader Luukkonen , Olli Chien-I Chien-I Lin We report experimental characteriza- experimental report We Highland B 1 , MinGu , 2 CRC for Polymers, Australia.Polymers, for CRC , Thomas K. Gaylord; Georgia Md M. Hossain M. Md We theoretically investigate theoretically We 1 ; 1 SwinburneUniv. of 1 , Mark D. D. Mark , FiO/LS 2010 alignment process. on-orbit the of analysis the in role its and model the describes paper This Observatory. the of model images-out to photon-in fidelity high a is Model Technologies Corp., USA. AerospaceandBall Lightsey; A. PaulActon, Scott D. JWST Integrated System Modeling, ages and AO the changes are phase the diversities. optical medium. Sequential images are the diverse im- frame-rate is about 10 the times faster than if the changing imager phase-diversity a be can (AO) Optic TuftsUniv., USA. AO Changes as the Diversities, Sequential Diversity Imaging: Phase Diversity with FWV1 •4:00p.m. FWV2 •4:30p.m. Dynamics Corp., USA,Presider Richard Paxman; General Sensing II FWV •Image-basedWavefront 4:00 p.m.–5:30p.m. • Highland C A digital camera with an Adaptivean with camera digital A FiO October 24–28,2010 The JWST Integrated System Invited Invited Robert Robert A. ; Gonsalves J. Scott Knight, J. McKinstrieJ. louin scattering threshold enhancement. noise source was used for the pumps’ stimulated - Bril ferential phase-shift-keyed signal. A radio-frequency dif- non-return-to-zero 10.7-Gb/s a for measured performance errorless an with amplifier parametric fiber-optictwo-pump 66dB-gain Wea demonstrate hollow-core fibre are discussed. solid core fibre, to pulsehigh energy compression in in generation parametric or supercontinuum from pulses, laser transforming for platform a as fibres crystal photonic of limits, some and possibilities, UK. Bath, Univ.of Knight; C. JonathanStone, sworth Fibres, Optical in Conversion Wavelengthand Duration Pulse of Manipulation Slaven Moro 66dB Gain and Errorless Performance, Two-Pump Fiber-Optic Parametric Amplifier with FWW2 •4:30p.m. FWW1 •4:00p.m. USA, Presider Marcelo I.Davanco; CNST -NIST, FWW •NonlinearFiberOptics 4:00 p.m.–5:15p.m. - San Diego, USA, Diego, San - , Laure Lavoute, Peter J. Mosley, James M. M. James Mosley, J. Peter Lavoute, Laure , 1 , Nikola Alic Nikola , 2 , Stojan Radic Stojan , Highland D 2 Bell Labs, Alcatel-Lucent,USA. Labs, Bell 1 , Arthur J. Anderson Invited 1 ; 1 Univ. of California California of Univ. William J. WadJ.- William Ana Peric Ana 1 , Colin

The The 1 ,

analysis and optical theory. by combining infrared imaging, chemometrics, image petitive performance in cancer detection is achieved Human-com humansupervision. orwithoutstains - diseases and types cell into tissue classify to used is USA. Champaign, Urbana- at IllinoisWalsh; Univ. of Rong J.Michael Kong, Llora, Xavier Mayerich, David Schulmerich, Pounder,V.MatthewN. FrancesIp, Reddy, Jason K. Automated Histopathology, Infrared Spectroscopic Imaging for Label-Free and FWX2 •4:15p.m. molecular interactions. ofunderestimation possible indicate models logical Deviations of experimental results from phenomeno- are modulated by physical and molecular properties. TL in trends where presented are binary-mixtures spectroscopy, (TL) thermal-lens ogy,Kanpur, India. mar Liquids Binary Mixtures, in Spectroscopy Thermal-Lens FWX1 •4:00p.m. Group Inc., USA,Presider Andrey V. Kanaev; Global Strategies Diagnostics andSensingII Non-Imaging Techniques for FWX •GeneralizedImagingand 4:00 p.m.–5:30p.m. , Debabrata Goswami; Indian Inst. of Technolof - Inst.Indian Goswami; Debabrata , Indrajit Bhattacharyya, Bhattacharyya, Indrajit Highland E Infrared spectroscopic imaging spectroscopic Infrared Usingfemtosecondpump-probe Invited , Rohith Rohit Rohith Bhargava, experiments in experiments Pardeep Ku- Pardeep Wednesday, October 27 93 ; Christine Payne ; Baylor College of Invited Invited The The intracellular degradation Ido Ido Golding Highland K Highland We study We the life-cycle of bacterio- LWL1 • 4:00 p.m. • 4:00 p.m. LWL1 Imaging Imaging Dynamic Events Inside Living Cells: - In tracellular Degradation of LDL, Bacteriophager Lambda Life Cycle: The View from from View The Cycle: Life Lambda Bacteriophager the Single Virus, LWL2 • 4:30 p.m. LWL2 4:00 p.m.–5:30 p.m. 4:00 p.m.–5:30 Approaches Molecule Single • LWL II to Biology of Inst. Natl. A. Eaton; William Diabetes of Inst. Natl. and Health Diseases, Kidney and Digestive and USA, Presider Georgia Tech, Georgia USA. Tech, of LDL was probed with single particle tracking labeled were particles LDL microscopy. fluorescence increase an to leads degradation enzymatic that such in fluorescence allowing us to relate endosomal degradation. to dynamics Medicine, Medicine, USA. of individual viruses lambda the at phage resolution and cells. I will present some of our recent findings with to open regards long-standing in questions the system. lambda , , , 1 1 Univ. Univ. 2 We use

, Qi Zhang Qi , 1 , Sabih Khan 1 Hans Hans Jakob Wörner Kun Zhao Kun Invited A magnetic-bottle electron LS Kansas Kansas State USA, Univ., , Michael Chini 1 1 Highland J Highland ; 1,2 LWK2 • 4:30 p.m. LWK2 Magnetic-Bottle Electron Spectrometer for - Mea Pulses, as 25 Isolated suring LWK1 • 4:00 p.m. • 4:00 p.m. LWK1 Time-Resolved Time-Resolved High-Harmonic Spectroscopy of Photochemical Dynamics, Julien Julien B. Bertrand, Paul B. Corkum, David M. - Vil leneuve; Joint Lab for Attosecond Science, Natl. Canada. Res. Ottawa, of Univ. and Canada Council high-harmonic spectroscopy to observe the evolution evolution the observe to spectroscopy high-harmonic of the electronic structure of molecules undergoing transient the Using reactions. photochemical ultrafast grating technique allows us to determine amplitude emission. state the excited of phase and 4:00 p.m.–5:30 p.m. 4:00 p.m.–5:30 and Strong Attosecond • LWK II Field Physics Council Res. Natl. Villeneuve; David Presider Canada, Canada, of Central of Florida, Central USA. energy spectrometer was designed and constructed simulations Numerical pulse. XUV as 25 a measure to is spectrometer the showed results experimental and capable to meet the energy resolution required by measurements. such Steve Steve Gilbertson Zenghu Chang Mark Mark We demonstrate demonstrate We Xianli Xianli L. Zhang, ; Jeffrey H. Shapiro Invited October 24–28, 2010 • Highland H Highland Quantum Quantum illumination transmits part of ; Univ. of USA. ; Wisconsin, Univ. LWJ2 • 4:30 p.m. LWJ2 Deterministic Entanglement of Two Neutral Atoms Using Rydberg Blockade, Thad Gill, G. Walker, T. Alex Larry Isenhower, Saffman medi- state Rydberg using gate CNOT atom neutral a deterministically to used is gate The interactions. ated Bellentangled with create a states fidelity of F=0.71, atoms. of loss for correcting without Quantum Quantum Illumination for Improved Detection, and Communication, Imaging, USA. MIT, an entangled state, retaining the rest for subsequent - commu or imaging, detection, in measurement joint the of systems classical-state outperforms It nication. entanglement- over energy transmitted average same channels. breaking 4:00 p.m.–5:30 p.m. 4:00 p.m.–5:30 Quantum Enhanced • LWJ Processing II Information Univ., Yale Schoelkopf; J. Robert USA, Presider LWJ1 • 4:00 p.m. • 4:00 p.m. LWJ1 ; 1 FiO/LS 2010 Ecole 3 1Dept. 1Dept. of , Antonio , Antonio Princeton 2 1 1 , Yifu Zhu Yifu , ; 1 1,3 College College of - phys 3 We We demonstrate the , Xiaogang Wei Xiaogang , , Christopher Barsi , Christopher We We report an experimental 1 1,2 , Jason W. Fleischer , Jason W. 3 Highland G Highland , Shu Jia , Shu 1 We We demonstrate novel four-wave mix- Inst. Carnot de Bourgogne, France, France, Bourgogne, de Carnot Inst. 2 Jiepeng Zhang Jiepeng , Sergio Rica Joel Joel A. , Greenberg Daniel J. Gauthier; Duke 2 Can Sun Physics Div., Los Physics Div., USA, Lab, Alamos Natl. ics, ics, Jilin China. Univ., demonstration of all-optical switching in a cavity atoms three-level multiple of consisting system QED mode. in a cavity confined 1 4:00 p.m.–5:30 p.m. 4:00 p.m.–5:30 Non-linear Optics FWZ • General of Univ. Broderick; Neil Presider UK, Southampton, Physics, Physics, Florida Intl. USA, Univ., FWZ3 • 4:30 p.m. All-Optical Switching in a Coupled Cavity-Atom System, FWZ1 • 4:00 p.m. CondensaObservation- of Classical Optical Wave tion, Univ., USA, Univ., Picozzi Normale Normale Superieure, France. nonlinear nonlinear condensation of classical optical waves. as is a observed function The condensation directly, of nonlinearity and wave kinetic energy, in a self- crystal. photorefractive defocusing FWZ2 • 4:15 p.m. Self-Phase Matched Mixing Four-Wave in Cold Vapor, USA. Univ., atomic to due arise that vapor cold a in processes ing spatial self-organization. This leads to a reduced parametric oscillation threshold and a more rapid power. pump with gain of increase FiO Photoacoustic Photoacoustic functional and in vivo Invited Invited , Gene K. Beare; Lihong Wang Highland F Highland - optical microangiogra for The basic principle FWY1 • 4:00 p.m. 4:00 p.m.–5:30 p.m. 4:00 p.m.–5:30 Design for FWY • Optical Systems II Biomedical Be Announced to Presider Breaking Breaking the Optical Diffusion Limit: - Photoa coustic Tomography, tomography combines optical (endogenous or exogenous, fluorescent or contrast non-fluorescent) and ultrasonic resolution for optical the beyond Super-depths imaging. molecular diffusion limit have been reached with high spatial resolution. Washington Univ. in Univ. Washington St. Louis, USA. High High Resolution Optical Volumetric Imaging of Beds, Tissue Microcirculation with Perfusion Blood Science Univ., and Health ; Oregon K. Wang Ruikang USA. phy is presented, and its potential applications in a number of animal models will discussed, including injury. brain traumatic and hemorrhage, stroke, FWY2 • 4:30 p.m. Wednesday, October 27 94 speculate on what’s to come infuture builds. state-of-the-art systems, discuss key technologies, and these of overview an give will presentationI this In capacity.terra-bit multiple with installed routinely are cables telecommunications transoceanic dersea Industry, Capabilitiesof Underseathe Telecommunications coherent transmission. for devices integratedstate-of-the-art and switches, such as wavelength multi/demultiplexers and optical devices commercialized reviews talk This systems. long-haulcommunicationandopticalmetro access, Japan. Systems, Communication Optical in Optics Integrated SWB3 •5:00p.m. SWB4 •5:30p.m. Symposium II—Continued SWB •OpticalCommunications

Optical waveguide devices are widely used in areused widelywaveguide devices Optical Hiroshi TakahashiHiroshi ; TE SubCom, USA. SubCom, TE Bergano; S. Neal Highland A Invited Invited ; NTT Photonics Labs, Photonics NTT ; Un - to 0.04λ-by-0.03λ. plasmonic waveguide with mode cross section down ing electromagnetic (EM) waves in a designer surface We experimentally demonstrate squeezing and guid- Yang, Zhaolin Lu; Rochester Inst. of Technology, USA. Plasmons, Surface Designer on WaveguidingBased length Subwave- Deep of Demonstration Experimental FWU4 •4:45p.m. Processing IV—Continued Metamaterials forInformation FWU •Plasmonicsand Turkey, size and location. waveguide can be enhanced by changing the the antenna inside intensity field the antennas, using that demonstrateWe antennas. dipole using waveguide Ag/SiO2/Ag 100-nm-core a into coupled was nm) Nanotechnology, Turkey. Onbasli Metal-Insulator-Metal Waveguides, Subwavelengthfor Couplers Antenna Dipole FWU5 •5:00p.m. 4:00 p.m.–9:00p.m. 3 1 UNAM,Natl. Inst. for Materials Scienceand , Ali K. Okyay K. Ali , Omar M. Eldaiki, M. Omar Highland B 2,3 Near-infrared light (λ=1550 ; 1 MIT,USA, See the Postdeadline Papers Book in your registration bag for times exact and locations. WangshiZhao Science Educators’Day, Lilac Ballroom North and South, Rochester Riverside Convention Center Mehmet Cengiz 2 BilkentUniv., 7:00 p.m.–8:30p.m. , Ruoxi , FiO/LS 2010 diverse phase retrieval. focus- multi-aperturewithor systems segmented in solves the capture range problem for segment tip-tilt It introduced. is sensing wavefront image-based Rochester,USA. Univ.of Fienup; Systems, Segmented for Retrieval Phase Focus-Diverse in Problem Range Capture the Solving for Method Improved FWV4 •5:15p.m. Aronstein Space-Optics Control, Space-Optics JWST for Recovery Amplitude Pupil and Phase FWV3 •5:00p.m. Zielinski Flight Ctr., USA, Ctr.,Flight USA. Sensing II—Continued FWV •Image-basedWavefront of NIRCam. the error bars and to provide an optical characterization Two algorithm approaches are considered to establish data.JWSTtest OMA usingfor the NIRCam sented

Phase and pupil amplitude recovery are pre- are recovery amplitude pupil and Phase 1 , Jeff S. Smith 1 , James R. Fienup JamesR. , • Highland C 2 FiO Postdeadline Paper Sessions Inst. of Optics, Univ. of Rochester,Univ.of Optics, of Inst. 1 FiO , Matthew R. Bolcar October 24–28,2010 Alden S. Jurling S. Alden Bruce H. Dean H. Bruce 2 ; 1 NASA Goddard Space Goddard NASA A new method of method new A 1 , Thomas P.Thomas , , James R. R. James , 1 , David L. numerically. and experimentally demonstrated is evolution train and temporal feedback the phase on spectrum pulse supercontinuumfor of manipulation.influence The possibilities new creates system generating tinuum Germany.Physics, Applied of Inst.Fallnich; Carsten Groß, Petra Kues, Phase, Feedback Optical the Via AdjustmentSupercontinuum FWW4 •5:00p.m. Continued FWW •NonlinearFiberOptics— 130nm, with a peak power exceeding130nm, with apeak 10mW. morethan ofrange spectral tunablea overis source ing 2.4µm, based on cascaded four-wave-mixing. The wavelength silica fiber optic source, capable of reach- California- San Diego, USA. Univ.Radic;Stojan Zlatanovic,Alic,ofNikola Sanja µm, 2.4 at Source Parametric SWIR Tunable All-Fiber FWW3 •4:45p.m. Faezeh Gholami Faezeh Highland D Nicoletta Brauckmann Nicoletta Optical feedback in a supercon- a in feedback Optical , Jose M. Chavez Boggio, Boggio, Chavez M. Jose , We report a record long- , Michael , state-of-the-art cameras exist. transfers the image information to the NIR range were unit converter The unit.up-converter wavelength a and camera CCD standard a using realized is range Denmark. Lichtenberg; Technical Univ.Tidemand-Peter Pedersen, Christianof Sørensen, Denmark, DTU Fotonik, Camera, ImageAcquisition Mid-IR Using Standard a CCD FWX5 •5:15p.m. Physical Problems, Belarus, western Univ., USA, spraying processes. A new approach has been made in diagnostics of the vanced technological processes have been developed. France. Mueller-metric imaging. full of capable state, polarization input variable a of the Stokse parameters in signal, the withreflected componentsfour all detect can that radar laser safe eye imaging Stokesmetric automated an report We A. Chivel A. Processes, Industrial of Monitoring Optical FWX4 •5:00p.m. Shih TsengShih An Automated Stokesmetric Imaging Laser Radar, FWX3 •4:45p.m. Continued Diagnostics andSensingII— Non-Imaging Techniques for FWX •GeneralizedImagingand

Optical systems for monitoring of some ad- some monitoringof for systems Optical 1 , I. SmurovI. , , Knud Palmelund Knud Dam , Seidelin Jeppe 1,2 Direct image acquisition in the 3-5 µm 3-5 the in acquisition image Direct , Xue LiuXue , Highland E 2 Digital Optics Technologies, USA. 2 1 , D. ZatiaginD. , , Selim M. Shahriar M. Selim 2 Ecole Natl.e d’Ingenieurs, 1 ; 1 Inst. of AppliedInst.of 1 ; 1 North Yuri Yuri -

Wednesday, October 27 95 Univ. Univ. of , Bridget 2 2 , Peter M. 1 , Diane S. Lidke 2 Invited , M. Lisa Phipps 1 We have developed a microscope have We Highland K Highland Los Los Alamos Natl. Lab, USA, 1 Jim Jim Werner ; 2 , Patrick J. Cutler J. , Patrick 1 LWL • Single Molecule Approaches Molecule Single • LWL II—Continued to Biology Goodwin Time-Resolved Time-Resolved 3D Tracking of Individual Quan- Confocal via Cells Live in Proteins Labeled Dot tum Feedback, LWL3 • 5:00 p.m. • 5:00 p.m. LWL3 New Mexico, USA. Mexico, New individual follow to feed-back active uses that system - dimen three in moving proteins labeled dot quantum 100 with velocities transport um/s at cells live in sions resolution. temporal picoseconds S. Wilson , 1 Oliver Univ. of 2 , , 1,2 , Oleg Kornilov 1 ;Kalinski UtahK. Matt ) reveal rich electronic 6 Invited Femtosecond time resolved resolved time Femtosecond LS , , Daniel M. Neumark 1,2 Highland J Highland We discover an enormous sensitivity sensitivity enormous an discover We Oliver Oliver Bünermann Lawrence Berkeley Natl. Lab, USA, Lab, Natl. Berkeley Lawrence 1 ; 1 LWK • Attosecond and Strong Attosecond • LWK II—Continued Field Physics Gessner LWK3 • 4:45 p.m. LWK3 Ultrafast Dynamics Studied in by Femtosecond EUV Photoelectron Helium and Nanodroplets Ion Imaging, California Berkeley, USA. Berkeley, California pure of studies imaging ion and EUV photoelectron (~2x10 helium nanodroplets Stephen R. Leone and and nuclear dynamics. Inter-band relaxation in the superfluid clusters and emission of Rydberg atoms in real-time. monitored are LWK4 • 5:15 p.m. LWK4 in Configurations Two-Electron Langmuir-Trojan Displaced with Dots Quantum Spherical Harmonic Fields, Magnetic in Impurity USA. Univ., State of 3-dimensional harmonic spherical dots quantum in the static electric and magnetic fields or with the displaced impurity being loaded with two electrons configuration. Langmuir in theper static dot ; , Qiongyi He, David Hanneke Invited October 24–28, 2010 FiO Postdeadline Paper Sessions Paper FiO Postdeadline • Highland H Highland Peter D. Drummond Recent advances in trapped-ion quantum quantum trapped-ion in advances Recent We develop strategies for generating spatial spatial generating for strategies develop We

LWJ • Quantum Enhanced • LWJ Processing II— Information Continued LWJ3 • 4:45 p.m. LWJ3 EPR Entanglement Using BEC and Beam Splitter Interactions, Margaret D. Reid; Swinburne Univ. of Technology, Australia. EPR entanglement in a trapped double-well atomic BEC with - spin By multiple ap eigenstates. applying spatial how show we criteria, entanglement propriate detected. and be can generated entanglement Progress Towards Scalable Quantum Information Progress Towards Processing with Trapped Ions, USA. NIST, information processing include the combination of a complete set of scalable techniques as well as development of scalable trap technologies, high- quantum and networks, quantum operations, fidelity simulation. LWJ4 • 5:00 p.m. • 5:00 p.m. LWJ4

- - An FiO/LS 2010 Luis 7:00 p.m.–8:30 p.m. Utsab , Khadka Utsab Lilac Ballroom North and South, Rochester Riverside Convention Center Convention Riverside Rochester South, and North Ballroom Lilac Science Educators’ Day, excited states in states excited 3/2 P 5 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 See the and 5/2 D 5 ; Johns Hopkins USA. Univ., Highland G Highland ; Univ. ; Estadual Univ. de Campinas, Brazil. 4:00 p.m.–9:00 p.m. FWZ • General Non-linear Optics— FWZ • General Continued FWZ4 • 4:45 p.m. Electromagnetically-Induced Phase Grating, de Araujo atomic phase grating, based on the giant Kerr - non transpar induced electromagnetically under linearity and efficient highly is grating described.The is ency, diffracts close to 30% of a probe beam into the first diffraction order. FWZ5 • 5:00 p.m. Between Four-Wave-Mixing the Upper-Excited in a States Cascade Configuration, Huaibin Zheng, Min Xiao; of Univ. Arkansas, USA. Two-color resonant four-wave-mixing radiation is the between generated FWZ6 • 5:15 p.m. All-Band Bragg Solitons and CW Eigenmodes, Alexander E. Kaplan atomic atomic rubidium vapor using atomic coherence via mecha absorption two-photon and EIT Doppler-free in the frequency domain. studied and nisms, We found We an amazingly simple intensity “all-band” arbirary for solitons Bragg or bandgap any of profile parameters of the system; we also found nonlinear eigen-modes of the system propagating without between waves. energy exchange FiO Using Using only ~5 mw Liping Liping , Cui Knox; Inst. Wayne of Highland F Highland A novel parallel 3-D confocal optical im- optical confocal 3-D parallel novel A FWY3 • 5:00 p.m. Enhancement of Penetration Depth for Back- scattering-Mode Nonlinear-Absorption Imaging in Media, Turbid Optics, of Univ. USA. Rochester, laser power, we imaged in backscattering mode a nonlinear absorbing object at 2.5 mm depth, which is five times the mean-free-path-length in a turbid the detection. optimizing by medium, FWY • Optical Design for FWY • Optical Systems II—Continued Biomedical FWY4 • 5:15 p.m. Lens, Varifocal with Imaging Confocal 3-D Parallel St. at Missouri of Univ. Fang; Hongbing , Li Guoqiang USA. Louis, varifocal electro-optic an with equipped system aging micromirror digital and scanning depth rapid for lens device for parallel transverse confocal scanning and presented. is acquisition image fast hence Thursday, October 28 96 Airy beams were and performed Airy analyzed. ments of second harmonic generation of - Experi 1-D and 2-D crystal. nonlinear poled periodically dratic mixing processes of accelerating beams in qua- Airy AdyArie;Tel Aviv Univ., Israel. Volatier brooke, Canada, brooke, Marc Marc Sorel Constantino De Angelis pumped at 1.55um. matchedquasi-phased second-harmonicgeneration relatively low propagation losses and highly efficient achieved and process, growth MBE temperature low the introducing by waveguides ridge AlGaAs periodically-inverted high-quality fabricated have Tokyo,Japan.Univ.of TakashiKondo; Ohta, at 1.55 µm, Waveguides High-QuarityAlgaas in tion Pumped - Genera Second-Harmonic Quasi-Phase-Matched •8:15a.m. FThA2 David Duchesne David UsingSource PhotonicAlGaAs Wire Waveguides, Harmonic WaveSecond Continuous Integrated, •8:30a.m. FThA3 7 2 Quadratic Nonlinear Photonic Crystals, in Beams Airy of Generation Harmonic Second •8:00a.m. FThA1 Catalunya, Spain, Presider Jordi Martorell; Univ. Politecnica de Univ. of Central Florida, USA, conversion. wavelength integrated for ideal it making process AlGaAs waveguide device offers a robust fabrication sub-micron The wavelengths. telecommunication atdemonstrated experimentally is source harmonic second tunable wavelength wave,continuous a ing, Aimez hamed Chaker hamed Nano-Optical StructuresI •NonlinearOpticsinMicro/ FThA 8:00 a.m.–10:00a.m. Univ.Arkansas,of USA. WarsawUniv. Technology,of Poland, 3 , 3 Roberto Morandotti Roberto , Francois LegareFrancois , 6 , Gregory J. Salamo Tomonori Matsushita 1 , Daniele, Modotto Highland A 1 , Katarzyna RutkowskaKatarzyna , 4 Univ. di Brescia, Italy,Brescia, Univ.di 4 , Demetrios Christodoulides Using modal phase matchUsingphase - modal 1 , Sebastien Delprat Sebastien , 1 7 ; , Richard Ares Richard , 6 1 Univ. of Glasgow, UK, Wewavestudythree INRS-EMT,Canada, 4 , Andrea, Locatelli , Junya Ota, Ikuma 3 Univ.Sher of Ido Dolev 1,2 5 3 , , Vincent CREOL, CREOL, , Maite Maite , 1 Mo , We We 5 4 - - , , , Nanostructures, Metal U-shaped Periodic in Effect Near-field to due Resonance Transmission Extraordinary •8:00a.m. FThB1 enhances depolarization. strongly regime coupling quasistatic the that found We fields. scatted the of depolarization the through clusters plasmonicparticle packed close couplingin mentally investigate the role of long-range diffractive Ari T.AriFriberg is revisited. nanostructure metal U-shaped subwavelength odic - peri a from arising resonances transmission of numerically.studied interpretationis The incidence metallic nanostructures on a glass substrate at normal far-fieldofcrescent-likeThe transmission spectrum 2 Univ., USA,Presider Mark L.Brongersma; Stanford •Plasmonics FThB 8:00 a.m.–10:00a.m. insensitive broadband photo-detectors. polarization- plasmonic-enhanced, for devices plasmonic novel of engineering the in result could characterized for the first time. These new structures various geometries have been designed, fabricated and BostonUniv., USA. rals, ization of Deterministic Aperiodic Plasmonic Spi - Character Scattering Dark-Field andFabrication •8:15a.m. FThB2 Walsh Nano-Arrays, Plasmonic Coupled fractively Dif- by Radiation Scattered of Depolarization •8:30a.m. FThB3 Aalto Univ.,Finland,Aalto JacobTrevino , Luca Dal Negro; Boston Univ., USA. 1,2,3 ; Highland B 1 Royal Inst. of Technology,Inst.of Royal Sweden, Srinivasan Iyer Srinivasan , Nate, Lawrence, Luca DalNegro; Plasmonic aperiodic spiralswithPlasmonic aperiodic 3 Univ. of Joensuu, Finland.Joensuu, Univ.of 7:30 a.m.–5:30p.m. 1 , Sergei Popov Sergei , We - experi Gary Gary FiO/LS 2010 1 - ,

independent hybrid waveguide coupler. We described. is present ofpolarization a design the mediumlowadjacenta withspacer index metal toa index high a of consisting waveguide hybrid a of of Toronto,Canada. of Alam Waveguides,Insulator on Silicon for Coupler Hybrid Independent polarization A •8:30a.m. FThC3 Presider California at San Diego, USA, Sanja Zlatanovic; Univ. of •IntegratedOptics FThC 8:00 a.m.–10:00a.m. three-cornered hat method. the andtechniqueself-heterodyne the using kHz 13 resonator.resultingThe measured is linewidth tobe for ring lasers using a CaF2 whispering mode gallery many. Wang;MaxPlanckLight, Inst. of Science theGer for Svitlov,J. Sergiy L. Lu, H. Z. Schwefel, L. G. Harald Laser, Stabilized Mode Gallery Three-Cornered-Hat Measurement of a Whispering •8:00a.m. FThC1 dicts the beam waist beam the dicts position and accurately. mode FDTDsimulation preshows that- methodology this are estimated Near-Field via and Far-Field methods. are studied. waist Beam positions of beams reflected Univ.,USA. NorthwesternHo;Seng-Tiong Huang,Yingyan Li, Strongly Guiding Waveguide, for Reflector Elliptical Efficiency High of Design •8:15a.m. FThC2 Registration, Galleria, Rochester Riverside Convention Center , J. S. Aitchision, Mohammad Mojahedi; Univ.Mojahedi;MohammadAitchision, S. J. ,

Westabilizationcompactpresent techniquea Elliptical reflectors used as on-chiplensas used reflectors Elliptical • Highland C

The polarization dependence polarization The FiO October 24–28,2010 , Xiangyu Zhenyu Xiangyu Hou, BenjaminSprenger, Muhammad Z. Z. Muhammad - rates, fluctuations. laser with high repetition low at characterization experimental for useful particularly is mentdevice The ofpulses. two measure- simultaneous for optimized presented, is USA. sity and Phase of Picosecond Pulses, Highly Simplified Device for Measuring the Inten- •8:30a.m. FThD3 Dongjoo Lee Dongjoo Techniques •NovelMeasurement FThD 8:00 a.m.–10:00a.m. 1 Univ. of Rochester, USA,Presider Jie Qiao; Lab for Energetics, Laser Presider Olivier Albert; LOA, France, Jovanovic products over 100. time-bandwidth with long 15ps to up pulses of measurementsintensity-and-phasecomplete report Wepulses. long relatively measuring for device (GRENOUILLE) frequency-resolved-optical-gating onstrate an extremely simple high-spectral-resolution the time delay time the bands. isolated between spectral toused both generate an internal reference and scan is shapingPhase-and-amplitude distortions. phase pulse laser of compensation and measurement free shaper-based sonogram technique for spectrometer- Univ.,USA. StateMichigan Pestov Dmitry Dispersion Measurement and Pulse Compression, Single-Beam Multiphoton Sonogram Technique for •8:00a.m. FThD1 acterization, Two-Beam Spider for Dual-Pulse Single-Shot Char •8:15a.m. FThD2 Georgia Tech,Georgia USA, A novel ultrashort pulse characterization device 1 ; 1 Purdue Univ.,PurdueUSA, 2 DougFrench Vkat Chauhan Vikrant , , Vadim V. Lozovoy, Marcos Dantus; MarcosLozovoy,V.Vadim , Highland D 2 Swamp Optics, USA. SwampOptics, 1 , Christophe, Dorrer We demonstrate all- demonstrateWe 2 Univ.Rochester,of 1 , Rick TrebinoRick , Jacob Cohen Wedem- 2 , Igor 1 1 - ; , density ever measured, ~0.3 g/cm ~0.3 measured, ever density has demonstrated the highest deuterium-tritium areal confinement fusion research using the OMEGA Laser Energetics,for Laser Univ. ofRochester, USA. ratory for Laser Energetics, Inertial Confinement Fusion Research at the - Labo Facility laser. DT, compressed by the high power Nationalcryogenic Ignitioncontaining capsules in gain fusion and ignition to lead will that experiments of progress USA. Lab,Natl. Campaign, forProgress Experiments Nationalin the Ignition obtained on Joint the European Torus. parameter, performance Natl. Lab, USA,Presider Wim Leemans; Lawrence Berkeley Presider Igor Jovanovic; Purdue Univ., USA, Ignition forFusion andFast •Lasers FThE 8:00 a.m.–10:00a.m. FThE2 •8:30a.m. FThE2 FThE1 •8:00a.m. FThE1 Brian MacGowan Brian Highland E An update will be provided on provided be will update An Invited Invited P τ , comparable to that to comparable , τ David David Meyerhofer; Lab ; Lawrence LivermoreLawrence ; 2 , and a Lawson’sa and , Inertial Inertial Thursday, October 28 97 - We , Torben Torben , Moerk Jesper Invited Invited Highland K Highland Spontaneous and stimulated emission emission stimulated and Spontaneous , Israel De Leon; Univ. of Ot- of Univ. Leon; De Israel BeriniPierre, 8:00 a.m.–9:45 a.m. 8:00 a.m.–9:45 Photonic • Nanophotonics, LThC Crystals Structural Slow and Light I of Univ. Badolato; Antonio USA, Presider Rochester, LThC2 • 8:30 a.m. LThC2 LThC1 • 8:00 a.m. LThC1 - Nanopho in Interactions Light-Matter Enhancing Light, Slow by Structures tonic Denmark. Denmark, of Univ. Technical Nielsen; R. crystal photonic which under conditions the discuss inter light-matter enhance to used be can dispersion actions, e.g. by increasing the absorption sensitivity or the degree of light-speed control obtained via transparency. induced electromagnetically Spontaneous and Stimulated Emission into Surface into Emission Stimulated and Spontaneous Plasmons, Canada. tawa, into long-range surface plasmons is discussed. Of interest is the interaction of a dipolar gain medium with on thinplasmons metal stripes, - where amplifi cation and suppressed spontaneous emission were observed. simultaneously

; Bohn L. John I will discuss the discuss will I Wade Wade Rellergert, Invited Invited LS Highland J Highland David DeMille; Yale Univ., USA, Univ., Yale DeMille; David Presider 8:00 a.m.–10:00 a.m. 8:00 a.m.–10:00 in Ultracold • Frontiers LThB Molecules II LThB1 • 8:00 a.m. LThB1 • 8:30 a.m. LThB2 We We present recent data from our experimental effort to produce ultracold, internal ground-state polar molecular ions via sympathetic cooling with a Ca MOT. Implementation Implementation of a New Method to Produce Ultracold Polar Molecular Ions, Scott Sullivan, Kuang Chen, Steven Eric Schowalter, R. Huson; of Univ. California at Los Angeles, USA. Manipulation of Ultracold Chemistry, Chemistry, Ultracold of Manipulation JILA, NIST, Univ. of Colorado, USA. Colorado, of Univ. NIST, JILA, molecular physics underlying recent experimental reactions chemical over, control and of, observations at JILA. For these polar species, possible handles for control include the quantum statistics of the molecules, the temperature, applied electric fields, geometry. reduced-dimensional in confinement and These aspects of control are described remarkably ideas. theoretical simple by well , Shaul Mukamel; Mukamel; Shaul , J. J. A. Myers, K. L. Two dimensional Two J. P. Ogilvie ; J. P. Univ. JunJiang Invited Invited October 24–28, 2010 We present two-dimensional elec- two-dimensional present We • Highland H Highland Galleria, Rochester Riverside Convention Center Convention Riverside Rochester Galleria, Registration, LThA1 • 8:00 a.m. LThA1 David McCamant; Univ. of of Univ. McCamant; David USA, Presider Rochester, 8:00 a.m.–9:45 a.m. 8:00 a.m.–9:45 II: • Chemical Dynamics LThA Multi-Dimensional Ultrafast Spectroscopy - Pro of Spectroscopy Ultraviolet Dimensional Two Fibrils, Amyloid and teins of at Irvine, California USA. Univ. and backbone spectra(2DUV) protein ultraviolet of side chains are simulated. The signals provide new insights theinto structure and dynamics of proteins Fibrils. Amyloid and Two-Dimensional Electronic Spectroscopy of the Photosystem II Reaction Center, Tekavec, F. M. Lewis,P. Fuller, F. USA. Michigan, of D1-D2 of dynamics the on studies spectroscopy tronic - photo plant from complexes center reaction cyt.b559 two-dimensional our compare We K. 77 at II system models. exciton spectra current with LThA2 • 8:30 a.m. LThA2

, We FiO/LS 2010 , Alaa , Alaa Masaki Tsunekane , Zachary Perret, Warren Warren Perret, Zachary , 7:30 a.m.–5:30 p.m. 7:30 a.m.–5:30 Mojtaba Hajialamdari Highland G Highland We have demonstrated the generation of 200 of generation the demonstrated have We

Prathyush Samineni Prathyush FThG2 • 8:15 a.m. Femtosecond Laser Pulse Shaping Improves Self- Phase Modulation Measurements in Scattering Media, S. Martin C. Warren, Fischer; USA. Duke Univ., demonstrate that our recently developed spectral re-shaping technique improves the accuracy and precision of self-phase modulation measurements in scattering media over the conventional Z-scan method. 8:00 a.m.–10:00 a.m. 8:00 a.m.–10:00 FThG Quantum • General Electronics I Be Announced to Presider FThG1 • 8:00 a.m. Mid- for Amplifier PulseChirped Fiber Two-Color Infrared Generation, M. Al-Kadry, Donna Strickland; Univ. of Waterloo, Canada. µW of power at ~18 µm by mixing the from output a two-color Yb:fiber system. The modelled optimal amplifier fiber lengths are in reasonable agreement experimental with results. FThG3 • 8:30 a.m. Nd:YAG/ Ceramic Composite Edge-Pumped, Diode Microchip Sm:YAG Lasers, Takunori Taira; Inst. Taira; Takunori for Molecular Science, Japan. Diode edge-pumped, composite microchip lasers core consisting and of a a ceramic ceramic Nd:YAG pump Sm:YAG waveguide were demonstrated. A passively Q-switched, energy output of 1.76mJ with obtained. was 1.5ns of width a pulse FiO Univ. Univ. 2 , Xiang 2 , Thomas Thomas , 1 Jensen Li Jensen By extending - the trans extending By ; Univ. of Pennsylvania, , Nicholas Tapia 2 Invited Invited Highland F Highland Nader Engheta , Jason Valentine City Universtiy of Hong Kong, China, China, Kong, of Hong Universtiy City 2 1 ; 2 Metamaterials Metamaterials with extreme parameter values 8:00 a.m.–10:00 a.m. 8:00 a.m.–10:00 FThFand Optics • Transformation Cloaking with Metamaterials Zhang FThF1 • 8:00 a.m. Xiang Zhang; Univ. of California at at California of Univ. Zhang; Xiang USA, Presider Berkeley, Zentgraf FThF2 • 8:30 a.m. of California, Berkeley, USA. Berkeley, California, of developed materials the and scheme optics formation for optical cloaking, we demonstrate integration of multiple functions into a single transformation becompact useful designing can in device.It optical systems. optical integrated USA. can manipulate electromagnetic fields and waves at various length scales, providing a platform for metatronic circuits, optical wires, plasmonic cloak- ing, enhanced emission at extended regions, and channels in narrow supercoupling Taming the Fields and Waves with the Extreme - Fields Meta and Waves Taming materials, Transforming Integrated Optics, Optics, Integrated Transforming Thursday, October 28 98 plications are discussed. ap - possible and results Experimental presented. is polarization nonlinear and Raman, Kerr,including waveguides, these in processes nonlinear of theory fundamental The waveguidesfield. nonlinear the in era new a opened haveSubwavelength-waveguides Australia.Adelaide, Univ.of Monro; Tanya M. Implications, and Fundamentals Waveguides—Revised Optical Subwavelength in Processes Optical Nonlinear 1 •8:45a.m. FThA4 Continued Nano-Optical StructuresI— •NonlinearOpticsinMicro/ FThA the detection limitthe of 1.5GHz. MHz~30 to beyond frequenciesbetween that occur nonlinear optical fiber a numerous acoustic highly- resonance standard a in (FSBS) scattering Brillouin Jiaotong Univ., China. EMC,BeijingTelecommunication vancedof Network Ad- & Network Optical All of LabTechnology, Key hui Zhu hui tering in a Standard Highly-Nonlinear Fiber, Observation of Forward Stimulated Brillouin - Scat •9:15a.m. FThA5 Physics Dept., Duke Univ.,USA, Duke Dept., Physics 1 , Jing Wang Shahraam Afshar Shahraam Highland A 1,2 We observe forward stimulated , Rui Zhang Invited 1 , Daniel Gauthier 2 , Wen Qi Zhang, Zhang, Qi Wen , Inst. of Lightwaveof Inst. Yun 1 - ;

fast switching time. enables IR emitters with low power consumption and and low thermal mass of thin free standing substratesconductivity heat low The membranes. polyimide fabricated plasmonic infrared (IR) emitters on flexible tial refractive index sensortial is discussed. The performance of such perforated films as a poten - method. element finite three-dimensional vectorial using modeled is nanoholes double subwavelength with film Au thin a through light of transmission N. Chigrin N. Univ. of Arizona, USA, Arizona, Univ.of Nasser PeyghambarianNasser Index Sensors, Sensors, Index Refractive as Film Metal a in Nanoholes Double •8:45a.m. FThB4 2 T. FribergT. properties are established. Relations between the dimer’s geometry and its chiral shown to act as “atoms” in planar chiral metamaterials. analytically and numerically. Asymmetric dimers aredetermined is dimers nanorod metallic planar of Germany.Wuppertal, of Sergei V.Zhukovsky Sergei Meta-Atoms, Chiral Planar as Dimers Plasmonic •9:00a.m. FThB5 Kropachev Substrates, Polyimide Flexible on Emitters IR Plasmonic •9:15a.m. FThB6 FThB •Plasmonics—Continued FThB Aalto Univ., Finland, 1,2,3 2 2 ; , Terje SkotheimTerje , IsmailAraciE. 1 Univ.Toronto,of Canada, ; 1 Royal Inst. of Technology, Sweden, Sweden, Technology, of Inst. Royal Srinivasan Iyer Srinivasan Highland B 1,2 3 Univ. of Joensuu, Finland. 1 , Christian Kremers Christian , ; 2 1 Intex Corp, USA. Corp, Intex College of Optical Sciences,Optical of College Electromagnetic response Electromagnetic 1 , Veysi, Demir 2 , Robert A. Norwood A. Robert , 1 , Sergei Popov Sergei , 2 IHCT,Univ. 1 , Alexandr,

2 We have have We , Dmitry Dmitry , 1 , Ari , The FiO/LS 2010 1 , tures, Superstruc- Grating in Resonances Mode Guided •9:15a.m. FThC6 the nano-waveguidesthe is characterized as well. of nonlinearity Optical properties. optical excellent show cavity micro-ring and waveguide fabricated prepared.The are wafer silicon on nm 200 to down Univ., China. Zhang, Xiang Wu, ming Li, Devices, Nano-waveguide Chalcogenide On-chip of Characterization and Fabrication •8:45a.m. FThC4 G. Brown G. tor Lasers, Lasers, tor Coupler for High-Power Single-Mode - Semiconduc Non-Adiabatically Tapered Multimode Interference •9:00a.m. FThC5 first-order order of diffracted structure. defect the between the zeroth-order specular reflection and the energy of transfer resonant a mediates excitation mode guided The defects. periodic with fabricated Weguided-mode-resonancefilter a test andanalyze output with 98%one-way efficiency. system. The taper allows for a broad area, single-mode for use in a self-organizing semiconductor laser-array interference coupler has been designed and simulated Univ.Rochester,of USA. Continued •IntegratedOptics— FThC MichaelJ.Theisen 1 ; 1 Inst. of Optics, USA, Optics, of Inst. Jordan P.Leidner Jordan

Buried Buried As • Highland C FiO 2 October 24–28,2010 S A 1 x 8 tapered multimode tapered 8 x 1 A 3 1 nano-waveguides with size , Jason, D. Neiser Liying Liu, Lei Xu; Fudan , John R. Marciante; R. John , 2 Ctr. College, USA. Ctr.College, 2 , Thomas, Qiming Qiming Univ. of Rochester,USA, Univ.of modern techniques,modern evenon adark fringe. rivals method this using measurement phase a of amplification. We show that the signal-to-noise ratio cal experiment that makes use of weak value inspired Howell; Univ. of Rochester, USA. Dixon, Nathan S. Williams, Andrew N. Jordan,Fringe, Dark Johna C.on ments Measure- Phase Optical Limited Quantum Near •8:45a.m. FThD4 F. V.F.James Toronto, Canada, Toronto,Canada, Fisher College, USA, of polarization. degree same the and coherence of degree same the have beams the if different,even be may beams two by generated detectors two at fluctuations intensity USA. and X-ray soft applications. ultraviolet extreme forintensity field large and tion diffraction formula, and it can give high spatial resolu- modified zone plates are studied by Fresnel-Kirchhoff Univ.,Taiwan. Yao-Jen Tsai, by a Set of Two Modified Zone Plates, IntensityField Large andResolution Spatial High •9:15a.m. FThD6 Qasimi Effect, Brown-Twiss Hanbury the on The ofInfluence of Cross-Polarizationthe Degree •9:00a.m. FThD5 Techniques—Continued •NovelMeasurement FThD We show by example that correlations between 1 , Mayukh Lahiri Mayukh , 1 , Emil WolfEmil , Jia-Han Li, Kuen-Yu Tsai; Natl. Taiwan The focal properties of a set of two of set a of properties focal The Highland D 2 Dept. of Physics and Astronomy,and Physics of Dept. 4 Inst. of Optics, Univ. of Rochester, 2,4 ; 2 3 1 , David Kuebel David , Dept. of Physics, St. John St. Physics, of Dept. , P.Starling Ben , J. David Dept. of Physics, Univ.of Physics, of Dept. We describe an opti- Zhan-Yu Liu, Asma Al- Asma 2,3 , Daniel Daniel , havs achieved. been heating fast to due generation neutron the of ment University. Osaka Enhance- at lasers LFEX and XII Gekko- with performed been haveproject FIREX-1 fortargets Ignition(FI) Fastof experiments heating Laser Engineering, Osaka Univ., Japan. Lasers, LFEX and XII Fast Ignition Integrated Experiments Using Gekko- FThE3 •9:00a.m. FThE3 Ignition—Continued forFusion andFast •Lasers FThE Highland E Hiroyuki Shiraga Hiroyuki Invited

Implosion and ; Inst. of Inst. ; Thursday, October 28 99 , 1 We

, Thomas 3 , Andrey , A. - Andrey Sukho Thomas P. Thomas White P. 2 - Jin , Zhang Yundong Australian Australian Natl. Univ., 1 ; 1 Univ. of Univ. Sydney, Australia, 3 We report the measurement measurement the report We , Martijn de Sterke 2 Highland K Highland , Marko , Spasenovic Marko 1 FOM Inst. for Atomic and Molecular Physics Physics Molecular and Atomic for Inst. FOM , Yuri S. Kivshar 2 4 , Kobus Kuipers 1 Univ. of St Andrews, UK. Andrews, St of Univ. LThC • Nanophotonics, Photonic • Nanophotonics, LThC Crystals Slow and Structural Light I—Continued LThC4 • 9:15 a.m. LThC4 Superluminal and Slow Light Propagation in a Resonator, Ring Fiber Nested Zhang, Xuenan Cai, Yuanxue Zhang, Jing Wang, fang Ping Harbin Yuan; Inst. of China. Technology, observe both superluminal and slow light - propaga in tion a simultaneously nested fiber ring resonator. The two outputs of the resonator exhibit different absorption characteristics that produce opposite performance. dispersion LThC3 • 9:00 a.m. LThC3 Observation of Evanescent Modes in Slow Light Photonic Crystal Waveguides, rukov Australia, Australia, 4 of slowly propagating and weakly evanescent modes weakly evanescent and propagating slowly of crys - photonic of points inflection dispersion to close tal modes Evanescent waveguides. play a key role in crystals photonic modes of slow to light coupling Sangwoo Ha (AMOLF), (AMOLF), Netherlands, F. F. Krauss ; , - 1 Univ. Univ. 1 ; 1 , B. Butscher 1 James Shaffer , R. Löw 1,2 Cold Rydberg gases are are gases Rydberg Cold LS , J. p. , Shaffer J. p. , V. Bendkowsky , V. 1 Homer L. Dodge Dpt. Homer of Physics 1 2 Highland J Highland , J. Balewski 1 Tilman Pfau Tilman LThB • Frontiers in Ultracold • Frontiers LThB II—Continued Molecules LThB4 • 9:15 a.m. LThB4 Ultracold Cs Rydberg Molecules, University of Oklahoma, USA. Oklahoma, of University at interact can atoms Rydberg the because interesting atom Rydberg describe We microns. 3-10 of distances the where formation molecule to lead that interactions 3-7 microns. are separations internuclear and Astronomy, The Univ. of Oklahoma, USA.Molecu Oklahoma, of Univ. The Astronomy, and lar spectra of ultralong-range Rydberg molecules are are molecules Rydberg ultralong-range of spectra lar superposi- Coherent models. theoretical to compared studied are states bound and free between states tion by an echo and Ramsey methods. Coherence times found. are regime in the microsecond LThB3 • 9:00 a.m. LThB3 Coherent Control Of Long Range Rydberg - Mol ecules, Stuttgart, Germany, Germany, Stuttgart, J. J. Nipper ; - 2 Harvard 2 , James K. Utter 1 , Alan Aspuru-Guzik Alan , 2 Mark Mark E. Siemens, Galan October 24–28, 2010 , Geoffrey A. Lott • Highland H Highland 1 We derive analytical forms for resonance resonance for forms analytical derive We , Alejandro Perdomo-Ortiz Alejandro , 1 Oregon Ctr. for Optics, Univ. of Oregon, USA, Oregon, of Univ. Optics, for Ctr. Oregon LThA • Chemical Dynamics II: • Chemical Dynamics LThA Ultrafast Multi-Dimensional Spectroscopy—Continued LThA3 • 9:00 a.m. LThA3 Fourier Two-dimensional In Lineshapes Resonance Spectroscopy, Transform Cundiff; Steven T. D. Bristow, Li, Alan Hebin Moody, USA. JILA, lineshapes in two-dimensional Fourier transform theorem projection-slice the Applying spectroscopy. of 2D Fourier transforms provides diagonal and cross-diagonal lineshapes in the 2D frequency data inhomogeneity. arbitrary for LThA4 • 9:15 a.m. LThA4 Structure and Energy Transport in Membrane- Bound Porphyrin Aggregates by Fluorescence Detected 2-D Electronic Coherence Spectroscopy, Andrew Marcus 1 Univ., USA. studied the We Univ., electronic coupling and - tetraphe meso magnesium of dynamics state excited nylporphyrin dimers, which self-assemble in room temperature lipid bilayer vesicles. This was - accom two-dimensional detected fluorescence using plished spectroscopy. coherence electronic back FiO/LS 2010 Scott time- Univ. of Univ. , Alexey 1 , Judy G. , Judy 4 3 Jeremy A. Jeremy ; 1 Spin Hall ef- Hall Spin Chun-Fang ; Li Chun-Fang Rice Univ., USA, USA, Univ., Rice 4 Hendrix College, USA, College, Hendrix 2 , Junichiro , Kono Junichiro , David Hilton 4 3 We use We ultrafast terahertz , Takahisa Tokumoto , Takahisa 2 A dielectric’s ultra-wide band band ultra-wide dielectric’s A dictates optimal control of “in-and- of control optimal dictates Highland G Highland , Stephan McGill , Xiangfeng Wang 5 3 , Jon D. , Moore D. Jon 1 Texas A&M USA. Texas Univ., Natl. High Magnetic Field Lab, USA, Lab, Field Magnetic High Natl. FThG Quantum • General I—Continued Electronics FThG5 • 9:00 a.m. The THz Frequency Hall Conductivity of a High- Gas, Electron Two-Dimensional Mobility Curtis Belyanin spectroscopy to study the magnetoconductivity tensor tensor magnetoconductivity the study to spectroscopy of a 2DEG as a function of temperature (0.4 K-100 K). The magnetoconductivity line width decreases temperature. with monotonically FThG6 • 9:15 a.m. Hall of EffectSpin of Light,Nature China. Univ., Shanghai Physics, of Dept. fect of light is shown to result from the polarization momentum angular orbital transverse of dependence for light beams that have global polarization, where the previously observed characteristic vector plays role. essential an 3 5 Cherian FThG48:45 a.m. • New Time Reversal Parities and Optimal Control Dielectricsof EnergyFree for Manipulation, Corson; Brigham John A. , Glasgow Chris Verhaaren, USA. Univ., Young spectrum reversal media. energy real-time in dispersive flows out” Alabama-Birmingham, USA, Alabama-Birmingham, - FiO Tunable Tunable Vladimir M. Invited  FiO/LS. Highland F Highland the program. the program. Look for your via email and let us , Shumin Xiao, Vladimir Drachev, P. X. Ni, post-conference survey post-conference know your thoughts on Thank you for attending FThF3 • 9:00 a.m. FThFand Optics • Transformation Metamaterials— Cloaking with Continued Active Active and Tunable Metamaterials, Shalaev USA. Kildishev; Univ., Purdue Alexander V. and active metamaterials can enable a new power ful paradigm of engineering space for light with transformation optics, leading to a family of new applications ranging from a planar hyperlens to hole. black optical Thursday, October 28 100 narrow-band non-classical light source. low-threshold, a towards step first the is This disk. polished LiNbO phase matched frequency conversion at 1064nm in a Mary,liam& USA. Eugeniy E. Mikhailov, Irina Novikova; College of Wil- for Quantum Optics Applications, Mode ResonatorsDeveloping Whispering Gallery •9:45a.m. FThA7 in conventional optical fibers. higher threshold power in contrast to muchbullet-like atvoids observed were voids tadpole-like where hollowa in for effect optical time,first fiber the fuse YonseiOh; Univ., Korea, Republic of. Fiber, cal High Threshold Fiber Fuse Effect in a Hollow Opti- •9:30a.m. FThA6 Continued Nano-Optical StructuresI— •NonlinearOpticsinMicro/ FThA ______WoosungHa Yoonseob, Jeong, Kyunghwan 3 whispering mode gallery resonator Highland A Wenon-critically haveachieved Matt T. Simons, We fiber report Tal EllenbogenTal Michael Volodarsky Michael lariton inaMetal-Nonlinear Boundary, Dielectric Plasmon-Po- Surface of Conversion Frequency •9:45a.m. FThB8 nonlinear of coefficient crystal. the the modulating periodically or thickness metal the varying by either achieved be can matching Phase the metal-nonlinear dielectric boundary is analyzed. Frequency doubling of a surface plasmon-polariton in 2 enhancement at apex the is of observed tip. the nanotip coupled to the silicon waveguide. metallicStrong field in (SPPs) polaritons plasmon surface of focusing nanoscale on-chip the experimentally and Univ. of Jerusalem, Israel. Desiatov Boris Nanotip, Metallic by Light of Focusing On-Chip •9:30a.m. FThB7 FThB •Plasmonics—Continued FThB ImperialCollegeLondon,UK, 10:00 a.m.–10:30a.m. , Ilya Goykhman, Uriel Levy; Hebrew Goykhman,Levy; UrielIlya , 3 Ay Arie Ady , Highland B 1 , Ido Dolev Ido , We investigate numerically 1 ; 1 Tel Aviv Univ., Israel, Israel, Univ., Aviv Tel 3 HarvardUniv., USA. 1 Yntn Sivan Yonatan , FiO/LS 2010 Coffee Break,Highland Ballroom Foyer Rochester Riverside Convention Center 2 , with other plasmonic structures. integratedreadily be pumpandthresholdslow with lasing deep-subwavelength enable could structure plasmon waveguide is proposed. The easy-to-fabricate hybrid edge-coupled an on based laser plasmonic Jinsong Zhu 3 Ctr. for Nanoscience and Technology of China, China, Waveguide, Plasmon Hybrid Edge-Coupled an an Based Laser Plasmonic Coplanar Deep-Subwavelength •9:45a.m. FThC8 orders of magnitude, enhancement of LDOS. find unique confined plasmon modes and large, three MIM structures using analytical scattering theory. circular Weconcentric in LDOS and scattering ment, We systematically investigate the near-field enhance- Lawrence Nate Density of States in Co-Axial Plasmonic Nanowires, Local and Localization Field Scattering, Light •9:30a.m. FThC7 Continued •IntegratedOptics— FThC New Jersey Inst. of Technology, USA. 2 , Tao Zhou YushengBian , Luca Dal Negro;LucaDal Boston, Univ., USA. • Highland C FiO 3 NOTES October 24–28,2010 ; 1 Beihang Univ., China, 1 , Zheng Zheng Zheng A novel coplanar 1 , YaLiu , 2 Natl. 1 , gating “double-blind” up. set FROG reliably retrieved in a novel single-shot polarization- be can pulses unknown arbitrary two that mentally Tech, USA. Consoli FROG, Double-Blind Using Robustly and Simultaneously Pulses Two Retrieving •9:45a.m. FThD8 Peter VaughanPeter Trebino bandwidth products >250,000. waveforms with ~40 fs temporal resolution measure and time- it, using and, waveforms optical arbitrary for measuring the full temporal field of very complex ric pulse-measurement technique, MUD TADPOLE, Georgia Tech, USA. hen Interferometry, Spectral Crossed-Beam Multiple-DelayUsing 65,000 Exceeding Products Measuring Ultrashort Pulses with Time-Bandwidth •9:30a.m. FThD7 Techniques—Continued •NovelMeasurement FThD , Pamela Bowlan, Vikrant Chauhan, Rick Trebino; 2 1 ; , Vikrant, Chauhan 1 Univ. Politécnica de Madrid, Spain, We demonstrate theoretically and - experi 2 , FranciscoLopéz-HernándezJ., Highland D We introduce a new interferomet- 2 , Jacob, Cohen 2 , Lina, Xu Jacob Co Jacob Antonio Antonio 2 Georgia Georgia 1 , Rick , 2 - , Appleton Lab, UK.Abstract not available. Status of the HiPER Project, FThE4 •9:30a.m. FThE4 Ignition—Continued forFusion andFast •Lasers FThE Highland E Invited Mike Dunne ; Rutherford ; Rutherford Thursday, October 28 101 - , Guo Yiling Qi Yiling A peculiar discrete Highland K Highland LThC • Nanophotonics, Photonic • Nanophotonics, LThC Crystals Slow and Structural Light I—Continued LThC5 • 9:30 a.m. • 9:30 LThC5 Peculiar Discrete Diffraction Characteristic of Lattice, Backbone Two-Dimensional quan Zhang; MOE Key Lab of Weak Light Nonlinear Nonlinear Light MOE Zhang; quan Key Lab of Weak China. Photonics, Nankai Univ., diffraction pattern in two-dimensional backbone lattice is illustrated through numerical simulations when the light is injected into a low-index site of the backbone lattice. The corresponding formation also is discussed. mechanism Ken Sympathetic Sympathetic heating Invited LS Highland J Highland ; Georgia Tech, USA. LThB • Frontiers in Ultracold • Frontiers LThB II—Continued Molecules LThB5 • 9:30 a.m. • 9:30 LThB5 Sympathetic Sympathetic Heating Spectroscopy: Probing - Mo lecular Ions with Laser-Cooled Atomic Ions, Brown spectroscopy spectroscopy measures atomic and molecular ion spectra by observing the heating of a laser-cooled control ion. Limits of the method are tested using two isotopes of for calcium. molecular Applications discussed. are ions October 24–28, 2010 NOTES • Highland H Highland - Highland Ballroom Foyer Rochester Riverside Convention Center Convention Riverside Rochester Foyer Ballroom Coffee Break, Highland FiO/LS 2010 , Peter 1 Joseph W. , 2 We numerically numerically We The transmitted transmitted The Inst. Nacional de - As Nacional Inst. 2 , Qiwen Zhan Azriel Z. ,Genack Jing 1,2 Highland G Highland Renjie Renjie Zhou 10:00 a.m.–10:30 a.m. , Baldemar Ibarra-Escamilla 1 pattern pattern of localized microwave radiation is Univ. of Dayton, USA, Univ. 1

; 1 FThG Quantum • General I—Continued Electronics E. Powers Mexico. Electronica, y Optica trofisica, demonstrate that periodically placed fibers element. can fiber area be mode large a using together phased images that mirror Talbot a is element fiber LMA The input. the fibers’ the reflected at beams Haus FThG79:30 a.m. • Modes in Random Media, speckle cor Strong modes. underlying the into decomposed modes. between neighboring found is relation Wang; CUNY Queens College, USA. College, Queens CUNY Wang; FThG8 • 9:45 a.m. Phase Locking Mirror Fibers Multiple by a Talbot Fiber Device, FiO , Xiang 2 NSF, NSEC, Univ. Univ. NSEC, NSF, 2 We propose to link the link to propose We , Shuang Zhang Shuang , 1 Invited Highland F Highland Dentcho A. Genov A. Dentcho Louisiana Tech Univ., USA, USA, Univ., Tech Louisiana 1 ; 2 ______Zhang FThF49:30 a.m. • FThFand Optics • Transformation Metamaterials— Cloaking with Continued Molding Molding the Flow of Light with Artificial Optical Materials, of California at Berkeley, USA. Berkeley, at California of - mechan celestial and metamaterials optical of fields ics, opening the light way to phenomena investigate and attractors strange motion, orbital of reminiscent environment. laboratory in a controlled chaos, Thursday, October 28 102 Univ., USA.Abstract not available. Nonlinear Silicon Photonics, Process, Optical Nonlinear by Beams Airy of Location Peak and Direction Acceleration the Controlling •11:00a.m. FThH2 to change location the of intensity. its peak sign and magnitude of the acceleration direction and the control all-optically to enables crystal photonic nonlinear poled asymmetrically an in beam Airy Univ., Israel. FThH1 •10:30a.m. FThH1 Presider to Announced Be Nano-Optical StructuresII •NonlinearOpticsinMicro/ FThH 10:30 a.m.–12:00p.m. Ido Dolev Nonlinear generation of an accelerating Highland A , Tal Ellenbogen, Ady Arie; Tel Aviv Invited Michal Lipson Michal ; Cornell Cornell ; product approaching remarkable the value of 100. The offersdevice an unprecedented time bandwidth resonator.micro-ring compatible CMOS fully and integrated an using by waveforms complex optical arbitrary of temporal-integration speed ultra-high Elettronica,Univ.Italy,Pavia, di E. LittleE. Moss cello Ferreracello Integration, All-Optical On-Chip Ultra-Fast •10:30a.m. FThI1 Presider to Announced Be Device •OpticalSignalProcessing FThI 10:30 a.m.–12:00p.m. 4 optical bandwidth. on demand the reduces and product bandwidth time- the improves technique This demonstrated. proposedandis experimentally converter (TSADC) analog-to-digital time-stretch photonic in tiplexing Spectral efficiency improvement via polarization mul- BahramJalali; Univ. California,of Angeles, Los USA. larization Multiplexing, Po- by Converter Analog-to-Digital Time-Stretch Photonic of Efficiency Spectral the Doubling •11:00a.m. FThI3 chirping and pi-phase-shift. waveformslike RF variousgenerate to cascaded are demonstrated. Sixteen resonators with tunable heaters and fabricated designed, (RFAWG)generationis waveform arbitrary frequency radio on-chip for USA. Hao Shen, Leo T. Varghese, Minghao Qi; PurdueWaveform Generation, Univ., Arbitrary quency Fre Radio Programmable On-Chip 16-Channel •10:45a.m. FThI2 CUDOS, CUDOS, School of Physics, Australia. 4 , Jose Azana Jose , A 16-channel microring based spectral shaper spectral 16-channel microringA based 3 , Sai T.SaiChu , 1 , YongwooPark , Highland B 1 ; 3 1 , INRS-EMT, Canada,INRS-EMT, Roberto Morandotti Roberto Ali Fard Ali 1 , Luca Razzari Luca , 3 Infinera Ltd, USA, InfineraLtd, , Brandon Buckley, We report about 1 2 1,2 , Dave J.Dave , Dept. di Dept. i Fan Li , Brent , Mar FiO/LS 2010 - - , Physics, Univ. of Sydney,Univ.Australia,Physics,of ten Photonic Topological Crystals, Transport, Curvature, Potential and Geometric in •10:30a.m. FThJ1 Australia, Kokou B. Dossou Dossou B. Kokou Felix Dreisow State Inst., Israel,Inst.,State Nolte C. McPhedran C. Sterke Southern California, USA,Presider Michelle L.Povinelli; Univ. of •PhotonicCrystal FThJ 10:30 a.m.–12:00p.m. 3 odd andodd evenmodes. longerno arehere modes the thatand BZ the along sign and magnitude change coefficients coupling their Wethat lattices.hexagonal find in waveguides tralia. Technology,Univ.Ausof- MathematicalSciences, of demonstrated. are tunneling Zener and oscillations Bloch like mechanismsTransport waveguide. slab undulated solelycrystals, formed by a geometric potential of an topological of realization experimental first the on Lattices, Coupled Photonic Crystal Waveguide in Hexagonal •11:00a.m. FThJ3 cavity resonances. methods and enables rapid design of heterostructure numerical existing than faster magnitude of orders crystal heterostructure cavities. The method is several new method for designing mode fields of 3D photonic TechnologyUniv.Sydney,ofAustralia. Double-Heterostructures, Crystal Photonic in Modes Cavity Engineering •10:45a.m. FThJ2 Dept. di Fisica, Politecnico di Milano, Italy. 2 , C. Martijn de Sterke 2 , Andreas Tünnermann

1 ; We investigate dispersion curves of coupled of curves dispersion investigateWe 1 CUDOS, School of Physics, Univ. of Sydney,Univ.Physics,of of School CUDOS, J. Scott Brownless Scott J. 2 CUDOS, Dept. of Mathematicalof Sciences, Dept. CUDOS, 2 , , Matthias Heinrich 1 , Lindsay C. Botten C. Lindsay , 2 • Highland C , Felix J. Lawrence 2 2 Inst. of AppliedGermany,Physics,ofInst. , Christopher G. Poulton G. Christopher FiO October 24–28,2010 1 ; 1 1 , Sahand MahmoodianSahand , CUDOS, CUDOS, IPOS, School of 2 Sahand Mahmoodian Sahand , Stefano Longhi Alexander Szameit Alexander 2 , , Robert Keil 1 2 2 , Lindsay C. Bot - CUDOS, School CUDOS, , C. Martijn de Martijn C. , We present a Wepresent We report 2 3 , , Stefan 2 ; , Ross Ross , 1 Solid Solid 1 1 1 , , , Zhuo Wang, Huafeng Ding,Wang, HuafengZhuo (SLIM), Microscopy Interference Light Spatial Univ. of Rochester, USA,Presider Jie Qiao; Lab for Energetics, Laser Diagnostics andSensingIII and Non-ImagingTechniques for •GeneralizedImaging FThK 10:30 a.m.–12:00p.m. registration, and piston phase-error correction. improved focus correction, frame-to-frame sub-pixel Weframes. mosaickingarrayansingleof developed holographybylaboratorysynthesisfor digital the in Rochester,Univ.USA. of phy, Improved Aperture Synthesis for Digital Hologra- •11:00a.m. FThK2 FThK1 •10:30a.m. FThK1 Gabor’s holography. microscopyand contrast Zernike’sphase imaging: temporally. SLIM combines two classic ideas in light 0.03nm and spatially nm 0.3 of changes pathlength optical measuring method optical new a SLIM, Urbana-Champaign,USA. at Illinois of Abbie E. Tippie, Sapna A. Shroff, James R. Fienup; Highland D We demonstrated apertureWe demonstrated Invited Gabriel Popescu Gabriel We presentWe ; Univ.; and stimulated emission innanoplasmonic systems. will review recent efforts aimed at the reduction of loss plasmonic systems and plasmonic metamaterials. We nano- of challenges majoramong arecontrol active Norfolk State Univ., USA. Metamaterials, Plasmonic Active Yingyan Yingyan Huang ogy, and Res. (A*STAR), Singapore,(A*STAR), Res. and ogy, USA, Southampton, UK,Presider Nikolay Zheludev; Univ. of Plasmonics andMetamaterialsIII •NonlinearitiesandGainin FThL 10:30 a.m.–12:00p.m. operation explored. is also temperature Low 1550nm. at lasing stable achieved ring”.Both coupled “waveguide a and resonator” “square a including model, FDTD multi-electron multi-level by simulated are designs resonator laser USA. Waveguide Rings, Coupled and Resonators Square Model: Gain conductor - Semi Realistic on Based 1550nm at Nano-Lasers Plasmonic Semiconductor of Simulation FDTD •11:00a.m. FThL2 FThL1 •10:30a.m. FThL1 Two new nano-scale plasmonic-semiconductor 2 Data Storage Inst., Agency for Science, Technol- 3 , Seng-Tiong Ho Highland E Optical lossOptical and a forneed Invited Xi Chen Xi 1 ; 1 Northwestern Univ., M. A. Noginov A. M. 1 , Bipin, Bhola 3 OptoNet Inc, Inc, OptoNet 2 ; , Thursday, October 28 103

We present present We ; MIT, USA. MIT, ; Invited Invited ; Univ. ; of Univ. USA. Rochester, Highland K Highland Marin Soljacic Marin Antonio Antonio Badolato R. Hamam, I. Celanovic, Z. Wang, Y. Chong, J.d. J.d. Chong, Y. Wang, Z. Celanovic, I. R.Hamam, LThF2 • 11:00 a.m. LThF2 10:30 a.m.–11:45 a.m. 10:30 a.m.–11:45 Photonic • Nanophotonics, LThF Crystals Slow and Structural Light II Rochester, of Univ. Boyd; W. Robert USA, Presider Cavity Quantum Electrodynamics with Quantum Dots, - semicon in effects electrodynamics quantum Cavity ductor quantum dots coupled to photonic crystals nanocavities are presented. In this framework, the single photon nonlinear regime is explored for implementation of strongly correlated quantum- systems. optical Crys - Photonic in Properties Light-Guiding Novel tals, Joannopoulos, two two photonic crystal enabled platforms, exhibiting novel light-guiding properties: a system exhibiting angular photonic bandgap, and a system exhibiting propagation. light uni-directional LThF1 • 10:30 a.m. LThF1 - Japan. of Tokyo, ; Univ. Invited LS Tripartite Tripartite entangled states are Highland J Highland Akira Furusawa Emily Emily A. Alden, Aaron E. Leanhardt; Univ. 10:30 a.m.–11:30 a.m. 10:30 a.m.–11:30 • Quantum Enhanced LThE Processing III Information of Univ. Laflamme; Raymond Presider Canada, Waterloo, LThE1 • 10:30 a.m. LThE1 • 11:00 a.m. LThE3 Calculation Entangledof Tripartite States Gener ated by Spontaneous CascadeTwo-Photon Emis- sion, of Michigan, USA. generated from spontaneous two-photon cascade ground spin-1/2 with systems three-level in emission W produced and GHZ are states Prototypical states. for certain initial conditions and photon emission directions. Quantum Teleportation and Quantum Information Information Quantum and Teleportation Quantum Processing, Teleportation-based quantum Teleportation-based information - process reviewed. is ing

Photon Norbert Hoi Hoi Sung Chung, This This talk concerns Invited Invited October 24–28, 2010 • Highland H Highland ; Univ. ; of Univ. Chicago, USA. LThD1 • 10:30 a.m. LThD1 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 • Single Molecule LThD to Biology III Approaches Rochester of University Lee, Andrea LThD2 • 11:00 a.m. LThD2 Single Single Molecule Photon Trajectories and - Transi tion Paths in Protein Folding, USA. Health, of Inst.s Natl. ; Eaton A. William molecules single immobilized of protein trajectories labeled with donor and acceptor fluorophores have been measured to locate transitions between folded - transi measuring of goal the with states, unfolded and times. path tion Driving and Controlling Biological Function by Chemical Perturbation Spectroscopy, Scherer pulsed periodic of studies simulation and experiment chemical the to perturbations synchronize cell cycle calcium nonlinear novel drive to and crecentus C. of beta in islets. cells insulin coupled of dynamics An FiO/LS 2010 A A full Nicole Nicole , Thomas 1 Delft Univ. Delft Univ. 1 ; We study the study We 4 Beloit Beloit College, USA, 1 ; Free Univ., Netherlands, Netherlands, Univ., Free 2,3 2 , Emil Wolf Aalto Univ., Aalto Finland. Univ., 3 3 Taco Taco D. Visser Highland G Highland , Miguel A. Alonso, Alonso, A. Miguel Beckley , M. Amber Univ. of Rochester, USA. of Rochester, Univ. 4 , Miguel A. Alonso , Dave G. Fischer 1 2 Univ. of Univ. USA, Rochester, NASA, USA, NASA, of Technology, Netherlands, Netherlands, of Technology, van van Dijk FThN2 • 10:45 a.m. Diffraction Free Stokes Distributions in a Full Beam, Poincare Thomas G. Brown; of Univ. USA. Rochester, states possible all comprises that one is beam Poincare demonstrate We sphere. Poincare the of surface the on a beam whose Stokes parameters remain stationary propagation. under 2 10:30 a.m.–12:00 p.m. 10:30 a.m.–12:00 FThN Quantum • General II Electronics Hong of Universtiy City Li; Jensen Presider China, Kong, 3 FThN1 • 10:30 a.m. The Effects of Spatial Coherence on the Angular Distribution of Radiant Intensity Generated by Scattering on a Sphere, effects of spatial coherence of the incident beam on the of modifications Strong sphere. a by scattering the predicted. are intensity radiant efficient model of Mie scattering for arbitrary incident incident arbitrary for scattering Mie of model efficient fields with high numerical aperture is - mono presented. including shown, are cases test simple Several chromatic fields with linear, radial and azimuthal polarization. FThN3 • 11:00 a.m. ArbitraryFocused of Fields, Scattering Mie J. Moore - FiO Compres , Adrian Stern, Joseph Invited Dean Dean Scribner; Northrop - Grum Highland F Highland Yair Rivenson Yair Presider to Be Announced to Presider FThM1 • 10:30 a.m. 10:30 a.m.–11:45 a.m. 10:30 a.m.–11:45 FThM in Higher • Sensing Dimensions—Theory and Computational Hardware for Imaging II FThM2 • 11:00 a.m. Compressive Sensing Approach for Reducing the Projection View Multiple in Exposures of Number Holography, Israel. Negev, the of Univ. Ben-Gurion Rosen; - Mitigat for Methods Processing Spatio-Temporal ing Bandwidth Issues Associated with Advanced Infrared Sensors, available. not USA. Abstract Corp., man sive sive imaging enables the reconstruction by of predicted images measurements of number fewer far from how demonstrate we Here theorem. sampling classical of number the reduce dramatically can approach this holography. projection in multi-view exposures Thursday, October 28 104 Nonlinear Medium, Nonlinear Diffusive Non but Random a in Scattering Light Xavier Vidal USA, rate of 20MHz/μs. optical fiber pumped by a swept source with a sweep an in scattering Brillouin stimulated via bandwidth wide a over ns 1.5 of delay pulse Wea demonstrate EMC, Beijing Jiaotong Univ., China. Network & Advanced Telecommunication Network of Source, Source, Swept-Frequency a with Light Slow Broadband •11:15a.m. FThH3 Continued Nano-Optical StructuresII— •NonlinearOpticsinMicro/ FThH Gauthier Bravo-Abad FThH4 •11:30a.m. FThH4 the lightthe generated from such domains. of interference field far the and domains nonlinear scattered randomly of patterns emission the from bate crystals is experimentally studied and explained generationtransparentfrom strontium-barium nio- Politècnica de Catalunya, Spain. 3 Univ. Autónoma de Madrid, Spain, Madrid, de Univ.Autónoma Rui Rui Zhang 1 ; 1 Duke Univ.,Duke USA, 2,3 1 , , Jorge L. Dominguez-Juarez Jordi Martorell Jordi Highland A 1 , Yunhui Zhu Francisco Rodríguez Francisco Invited 2 1,4 Key Lab of AllOpticalofKeyLab The second-harmonic ; 1 , , Jing Wang 1 ICFO, Spain, 1 , Can Yao 1,2 1 , Daniel , Daniel , Jorge Jorge , 4 2 Univ. MIT, 1 , numerically. frequencies spanning the S-L bands are demonstrated generated 13 structure, the Tailoringproposed. is resonator,ring crystal photonic a within embedded cavity heterostructure a reconfiguring dynamically via induced transitions intermodal by generation, Andrew G. Kirk; McGill Univ., Canada. USA, Hemmer Brillouin Gain, Gain, Brillouin Pumped Bi-Frequency Using Buffer Data Speed High- for Cavity Light White a ofDemonstration •11:15a.m. FThI4 ing it suitable foroptical networks. high-speed small footprint with a bandwidth of over 100nm - mak and 40Gb/s signals from a 5Gb/s input signal. It has a strate a novel broadband OTDM that generate 20Gb/s Preble; Rochester Inst. of Technology, F.USA. Stefan W.Elshaari, Ali Aboketaf , A. Abdelsalam Optical Time Division Multiplexer on Silicon Chip, •11:45a.m. FThI6 negligible distortion anddelay-bandwidth product high a with buffering data trap-door for suitable is WLC a Such peaks. gain Brillouin two for frequencies two by pumped resonator, fiber a using (WLC) white-light-cavity Crystal Ring Resonator, Ring Crystal Photonic a within Embedded Cavity erostructure Het - a via Generation Comb Frequency Optical •11:30a.m. FThI5 Device—Continued •OpticalSignalProcessing FThI 2 Texas A&M Univ.,USA. A&M Texas 2 , Selim M. Shahriar M. Selim Highland B oa Yum Honam Amin Khorshidahmad Amin 1 ; 1 1 My Kim May ,

NorthwesternUniv., We demonstrate a demonstrateWe Optical Optical comb

We demon- 1 , Philip Philip , FiO/LS 2010 12:00 p.m.–1:30p.m. , of, of, tals Surfaces, tals - Crys Photonic at Effect Goos-Hänchen Giant •11:30a.m. FThJ5 Byeong-HyeonAhn dielectric surface. dielectric from reflection internal total with comparison in magnitude of order one achieves and visualization microscopy optical far-field using surfaces crystals electromagneticwaves at one-dimensional photonic surface in observed directly is Goos-Häncheneffect and Electrochemistry RAS, Russian Federation. Park lasers bylasers changing position the of tapering end. parabolic-beam photonic fundamental crystal mode one-dimensional of properties emission the control Federation, Univ.,RussianState Moscow Lomonosov Physics, the propertiesthe of standing free membranes. cally flat and we compare the optical properties with substrate.indexrefractive arestructures These opti - low a to membranes crystal photonic standing free Univ.,Netherlands. Substrate, Index Refractive Low a to Transferred Crystals PhotonicTwo-Dimensional of Modes Leaky •11:45a.m. FThJ6 Beam Photonic Crystal Laser, Crystal Photonic Beam ControlEmissionof One-DimensionalParabolic- •11:15a.m. FThJ4 Moskalenko Continued •PhotonicCrystal— FThJ 2 KAIST, Korea, Republic of. RepublicKorea,KAIST, 1 , Yong-HeeLee , MichielJ. Ljubisa, Dood de Babic; Leiden 2 A.N. Frumkin Inst. of Physical Chemistry 1 , Andrey A. Fedyanin A. Andrey , Irina V.Soboleva Irina • Highland C We present a method to transferWe to method presenta 2 2 ; , Myung-Ki KimMyung-Ki , FiO 1 October 24–28,2010 Korea Univ., Korea, RepublicUniv.,Korea, Korea Lunch (on yourLunch own) We experimentallyWe Ju-Hyung Kang Ju-Hyung 1,2 Vlnia V. Valentina , 1 ; 2 , Hong-Gyu , 1 Faculty ofFaculty Giant Giant 1 , deviation from formula. classical the Rayleigh tance using infrared illumination. Results show major dis- optimalpinholefocal empiricalstudyan the on Manufacturing Technology, Singapore. Liping Zhao Liping TechnologicalUniv.,Singapore, Hartmann WavefrontSensing, Hartmann Thermal in Illumination Infrared Broadband for Empirical Study on Optimal Pinhole Focal Distance •11:30a.m. FThK4 relative to scanning direction. orientation and shape aperture to sensitivity shows results experimental with theory of Comparison apertures. example for demonstrated is position scattering media based on correlations over the object Webb; Purdue Univ., USA. Position, Object over Correlations with Imaging Speckle •11:15a.m. FThK3 by a specific instrument.by aspecific on an implementation of these errors from data taken rimetersusingsimulation calibrationa andperform - pola imaging microgrid ofcomponents ideal from USA. Arizona, of Univ.Tyo; Scott J. , LaCasse F. Charles Reconstruction in Microgrid Polarimetric Imagery, Polarimetric on Error Calibration of Effect The •11:45a.m. FThK5 Continued Diagnostics andSensingIII— and Non-ImagingTechniques for •GeneralizedImaging FThK We explore the effect of expected deviations expected of effect the exploreWe , ZhenyuNewmanJason, Wang,A. Kevin J. 2 , Xiang LiXiang , Highland D 2 , Ricky L. K. Ang K. L. Ricky , Speckle Speckle imaging in heavily 2 Kelvin J. A. Ooi A. J. Kelvin Singapore Inst. of Inst.Singapore We conducted 1 ; 1 Nanyang 1 , temperature lasing of Cr:ZnSe/As of lasing temperature room-Mid-IR fiber-lasers. formid-IR areproposed Goldstein χ as high as coefficients with optical-nonlinearities, Rochester,USA. of Plasmonics, Nonlinear Composite Materials, FThL4 •11:30a.m. FThL4 Igor Moskalev Igor and applications. results recent review and discuss Wewave-mixing. and harmonic-generation, luminescence, excited two-photon modulation, index efficient for ployed structures is demonstrated at 2.6and 2.4µm. waveguide planar Cr:ZnSe and material composite 1 USA, USA, Directorate, Manufacturing and Materials lab, Res. metal doped ZnSe/As doped metal Waveguide Structures And In Cr:ZnSe/As Planar Cr:ZnSe In Oscillation Laser Mid-IR •11:15a.m. FThL3 III—Continued Plasmonics andMetamaterials •NonlinearitiesandGainin FThL Univ. of Alabama at Birmingham, USA, Birmingham, at Alabama Univ.of (3) = 1 3 Photonics Innovations, Inc, USA. nm 2 , Dmitri Martyshkin 2 / V 2 3 . Metal-nanostructures can be em- be can Metal-nanostructures . , Renato Camata Renato , Highland E Noble metals exhibit strong exhibit metals Noble 2 S Jonathan Williams 3 :As ; Univ. Univ. Novotny ; Lukas Invited 2 Se 1,3 3 composite materials , Vladimir Fedorov 1 , 2 Sergey Mirov Sergey S 3 :As New transition 2 Se 1 , Jonathan 2 2 Air Force Force Air S 3 3 micro- :As 2 Se 1,3 1,3 3 ; ,

Thursday, October 28 105 We , Hyochul , Hyochul 1 Stanford Univ., Univ., Stanford 1 ; 1 , Arka Majumdar 1 , Jelena Vuckovic Jelena , 2 Highland K Highland Erik Erik D. Kim Univ. of Univ. California, Santa Barbara, USA. 2 , Pierre Petroff Pierre , 2 LThF • Nanophotonics, Photonic • Nanophotonics, LThF Crystals Slow and Structural Light II—Continued USA, Kim LThF3 • 11:30 a.m. LThF3 Differential Reflection Spectroscopy of Photonic Crystal Cavities Containing Coupled InAs Quan - tum Dots, obtain obtain differential optical reflectivity spectra from a photonic crystal nanocavity containing coupled quantum dots (QDs). Our technique employs Cou- lomb shifts in QD optical transition energies and is polarized cavities. linearly to restricted not , - 1 , Jon Davis P. 1 Insitute Insitute for Quan Naval Naval Air Systems 3 1 ; 3 LS AMPAC, USA, AMPAC, 2 Highland J Highland Francesco A. Narducci A. Francesco , George R. Welch 2 In In this work, we study the underlying physics LThE • Quantum Enhanced • Quantum Enhanced LThE Processing III— Information Continued Command, USA, Command, LThE4 • 11:15 a.m. LThE4 Phase Jumps in Electro-Magnetically Induced Transparency, Jon Jon H. Noble tum Science and Engineering and Dept. of Physics, USA. in the dynamics of an electro-magnetically induced with field one of phase the when system transparency changed. abruptly is the other respect to , , - 4 1 , R. Vogel 1 , J. Enderlein 3 Julius-Maximilians- 3 Georg August Univ., 4 , R. Colyer Invited (on your own) Lunch your (on 1 , M. Sauer 1 October 24–28, 2010 Univ. of Univ. California at Los Angeles, • Highland H Highland 1 , G. Iyer ; 2 1 T. T. Dertinger We demonstrate a We novel, simple, and fast Bielefeld Univ., Germany, Germany, Univ., Bielefeld 2 LThD • Single Molecule • Single Molecule LThD to Biology III— Approaches Continued LThD3 • 11:30 a.m. LThD3 USA, Univ. Würzburg, Germany, Würzburg, Univ. M. Heilemann Shimon Weiss Germany. Germany. superresolution imaging method that is based on blinking of fluorescence emitters and high order analysis. statistical Superresolution Optical Fluctuations Imag ing (SOFI), ; ; - 2 1 12:00 p.m.–1:30 p.m. FiO/LS 2010 , Paz Paz , 1 , Paul S. S. Paul , Praveen Praveen 1,2 Weizmann Weizmann 2 Spectral Ener Spectral 3 , Nir Davidson , John Howell 1 2 Wright-Patterson Wright-Patterson 1 ; 1 , Dimitry Yankelev 1 Anil K. Patnaik K. Anil Caltech, Caltech, USA.We present 2 Slow-light Slow-light polaritons in a , Amiram Ron 1 , James R. Gord 3 Highland G Highland Simultaneous Simultaneous two-channel control

, Ryan M. Camacho 1 Wright State Univ., USA, Univ., State Wright Ofer Firstenberg Ofer 2 , Moshe Shuker Moshe , 1 , Sukesh Roy Sukesh, 1,2 Univ. of Univ. USA, Rochester, Technion-Israel Inst. of Technology, Israel, Israel, Technology, of Inst. Technion-Israel of light speed in a single delay element of a Rb cell is is cell Rb a of element delay single speed a in light of demonstrated using a homogeneous magnetic field in conjunction with a single elliptically polarized signals. two laser containing resonant FThN411:15 a.m. • Electromagnetically for Induced Vector-Potential Light, Slow FThN Quantum • General II—Continued Electronics FThN5 • 11:30 a.m. Fast Reconfigurable Slow Light System based on Scheme, Absorption Raman Off-resonant K. Vudyasetu an off-resonant slow light system with fast switching switching fast with system light slow off-resonant an based This scheme dynamics Raman absorption. on combines the low dispersion broadening of double absorption system and all optical control of Raman absorption. FThN6 • 11:45 a.m. SpeedLight of Control Two-Channel Simultaneous Element, Delay Single a in Inst. Inst. of Science, Israel. when diffraction abnormal experience vapor thermal detuned from a pump laser. Diffraction - manipula tion is demonstrated for a uniform pump, and a Schrödinger-like dynamics with induced vector- pumps. structured for demonstrated is potential gies, gies, LLC, USA. AFB, AFB, USA, 1 1 London Hsu - FiO Univ. Univ. 1 ; 1 Zhiliang Zhiliang We present present We We present an an present We Beihang Univ., 2 Univ. of Univ. Science 1 - Mari V. , Adrian 2 ; 1,3 , Michael E. Gehm 2 , Bin Xiangli 2 MITRE Corp., USA. Corp., MITRE 2 Highland F Highland , Daniel J. Townsend J. , Daniel 1 China. Sciences, of Acad. Chinese 3 , Yan Yuan 1 , Michael D. Stenner 2 a snapshot imaging spectrometer using a light field camera combined with an array of narrow-band spectral filters. Simulation results demonstrate its post-processing performance, including spectrum acquisition, digital refocusing and correction of aberrations. chromatic ano imaging system for target tracking with compressive compressive with tracking target for system imaging for measurements large area persistent surveillance. system optical mask-based a with sensing Multiplexed - measure underdetermined from retrieval signal and explored. are l-1 minimization using ments and Technology and of Technology China, China, Zhou FThM3 • 11:15 a.m. Light Field Imaging Spectrometer: Concep tual Design and Simulated Performance, FThM in Higher • Sensing — TheoryDimensions and Computational Hardware for Imaging II—Continued FThM4 • 11:30 a.m. Compressive Measurements for Target Tracking, OsmanTariq of Arizona, USA, Arizona, of China, China, Thursday, October 28 106 CMOS Compatible All-Optical Chips, USA, Photonics - CREOL & FPCE - Univ. of Central Florida, Eric W.EricVan Stryland LazaroPadilhaA. Ferrera M. A. Pasquazi the degeneratethe 2PA over PbS for enhancement resonance state mediate inter >5x observe We CdSe. of studies earlier our of PbS quantum dots are measured and compared to nondegenerate two-photon absorption (2PA) spectra 3 1 •1:30p.m. FThO1 Presider to Announced Be Nano-Optical StructuresIII •NonlinearOpticsinMicro/ FThO 1:30 p.m.–3:30p.m. for computing. interconnects optical WDM on-chip and nications telecommu- for promise has platform This devices. integrated,compatible,CMOSin novelfunctionsof vatkin Absorption in PbS Quantum Dots, Quantum PbS in Absorption Two-Photonthe of Enhancement Resonance •2:00p.m. FThO2 Infinera Corp., USA. InfineraCorp., Univ. of Sydney, Australia,Sydney,Univ. of 2 2 Univ.of Toronto, Canada. , Edward H. Sargent H. Edward , 2 2 , S. Chu S. , , M. Peccianti Highland A 1 , Scott, Webster 3 , B. E. Little E. B. , 1 , Larissa Levina Larissa , We demonstrate a wide range wide Wea demonstrate 2 , L. Razzari Invited 2 ; 2 1 INRS-EMT, Canada, Canada, INRS-EMT, College of Optics and Optics of College Thedegenerate and 1 , 3 , R. Morandotti R. , David J. David Hagan 2 , D. Duchesne D. , 2 , Vlad Sukho - Vlad , David Moss David Gero Nootz Gero 2 1 1 2 1 - , , ; , , Data is discussed usingData of model the is discussed Nix-Gao. tip. corner cube using observed is loads increasing with hardness in Decrease presented. is films thin Presider to Announced Be Instrumentation •GeneralOptical FThP 1:30 p.m.–3:30p.m. the opticalthe design. refine and images the of parameters geometric the obtain to toolbox OcamCalib the adopting regions, imageiscomposed of front and lateral of fields view the which imager omnidirectional an presentWe Technology Res. Ctr., Natl. Applied Res. Labs, Taiwan. Chen, Ting-Ming Huang, Chia-Yen Chan; Instrument Huang Po-Hsuan ages for Panoramic Total Internal Reflection Lens, Im Omnidirectional of Calibration Geometric •2:00p.m. FThP3 indentation size effect (ISE) on HfO Rochester,USA. Univ.of Thin Films, Indentation Size Effects in Multilayer Hafnia-Silica •1:30p.m. FThP1 Spectral Spectral Holes, to Due Dispersion Using Detection Ultrasound •1:45p.m. FThP2 hole parameters. modest using sensitivity high showWe methods. have which large étendue compared toconventional materials hole-burning in effects dispersive using detection demonstrateWe conversion. amplitude to phase efficiency high requires ultrasound of tion Jevon J. Longdell; Univ. of Otago, New Zealand. Karan Mehrotra Jian Wei Tay Wei Jian Highland B , Ming-Fu Chen, Yung-Hsinag Yung-Hsinag Chen, Ming-Fu , An experimental study of study experimental An , Patrick M. Ledingham, , John C. Lambropoulos; 2 -SiO 2 multilayer Detec FiO/LS 2010 - - fluorescence microscope. confocal a in beam cw-laser nm, 532 a byirradiated edge of a chiral glassy photonic bandgap liquid crystal resonance was observed in the fluorescence at a band- USA. Optics, of Inst.Jr.; Stroud, R. Carlos Bissell, J. Luke Military Acad., USA,Presider Gregory Kilby; R. United States •MicroResonators FThQ 1:30 p.m.–3:30p.m. under CW-Irradiation, under Crystals Liquid Chiral Glassy in Resonances ity Photonic Band-Edge Circular Polarized - Microcav •1:30p.m. FThQ1 as mirrors for tunable lasers. single mode modes. The proposed structure may find applications coupling between two degenerate microring resonator inline single wavelength reflector based on engineered paign,USA. Lynford L. Goddard; Univ. of Illinois at Urbana-Cham- Wavelength Reflector, Single Inline Microring a of Design and Analysis •2:00p.m. FThQ3 energies of 1fJ/bit or less. photonic microcavities, crystal enabling modulation to achieve Q values above 100,000 in SiO2-clad silicon USA. P. Anderson, Philippe M. Fauchet; Univ. of Rochester, Microcavities, PhotonicSilicon Crystal Clad Ultra-low Energy Modulation Using High-Q SiO2- •1:45p.m. FThQ2 A circularly-polarized, 3 nm width microcavity We show that k-space engineering can used be Wepresent simulation ofan and design • Highland C FiO Amir Arbabi Amir October 24–28,2010 Svetlana G. Lukishova G. Svetlana , Young Mo Kang, Sean Sean , FThR1 •1:30p.m. FThR1 not available. Waves,Plasmon Interfering on Based Imaging Super-Resolution at Charlotte, USA,Presider Greg Gbur; Univ. of North Carolina Processing II Metamaterials forInformation •Plasmonicsand FThR 1:30 p.m.–3:30p.m. sion addressed. ver microwaveconventional the to difference and similarity the with studied is property transmitting The ground. the of out cable coaxial plasmonic a of metal inner the extending by designed is antenna USA. Hewlett-PackardLabs, Range, Plasmonic Monopole Antenna at Optical Frequency •2:00p.m. FThR2 Jingjing Li, Lars Thylén, StanleyR. Williams; Highland D ; MIT, USA. MIT, ; So T.Peter Invited Optical monopole Optical Abstract - Applications, and Generation Field THz High-Peak-Power FThS1 •1:30p.m. FThS1 and excitons. phonon-polaritons, and phonons optic phonons, entcontrol includingover modes acousticcollective and optical pulse shaping methods that enable coher terahertz of development the includes work Recent the collective degrees of freedom that mediate them. and rearrangements chemical and structural phase research includes ultrafast spectroscopy of condensed ulty of the MIT Department of Chemistry in 1982. His postdoctoral scholar at UCLA before joining the fac- a respectively,was and1981 and 1976 Universityin Keith A. Nelson received his B.S. and Ph.D. at Stanford Berkeley Natl. Lab, USA,Presider Robert A.Kaindl; Lawrence Hungary, Presider Janos Hebling; Univ. of Pecs, Applications •StrongTHzFieldsand FThS 1:30 p.m.–3:00p.m. control outlined. be objectives will coherent THz THz and discussed Nonlinear be will spectroscopy reviewed. be will fields terahertz high and pulses terahertz intense of generation for et Nelson Keith Highland E Tutorial ; MIT, USA. MIT, ; Methods Methods - Thursday, October 28 107 Tutorial FiO Highland K Highland ; Alabama A&M Univ., USA. A&M H. Univ., Caulfield; John Alabama Dr. H. John Caulfield works in various capacities for for capacities various in works Caulfield John H. Dr. two universities (Fisk and Alabama with A&M) etc.) President, and CTO, in (Director, capacities many is about ten John of editor companies. two journals, - edito the on past the in or now and one, of editor past honored widely is He journals. dozen a of boards rial (e.g. a five record from major awards SPIE), written in about newsstand and published airline magazine, books,(many book dozens and of patents, chapters, over 250 refereed journal articles. His most widely read article is the 1984 National Geographic cover story in Professor holography. Caulfield received a BA in Physics from Rice in 1958 and a Physics PHD from in Iowa State University in 1962. He did research in big companies (Texas Instruments, companies R&D Sperry-Rand),small and Raytheon, (Block Engineering and Aerodyne Research) and universities (UAH and Alabama A&M) before his “retirement.” current 1:30 p.m.–3:30 p.m. 1:30 p.m.–3:30 FThV and Holographic • Diffractive Optics I Heriot-Watt Waddie; J. Andrew UK, Presider Univ., FThV1 • 1:30 p.m. What What Is and Is Not a Hologram and Why it - Mat ters, the word But usually is foolish. definitions Debating “holography” is more abused than most and has come to stand for nonsense. Brilliant cosmologists, TV devotees alleditors, and “New Age” believe that magic. are holograms - We I willI David David De Invited Invited Netherlands. Univ., Vrije ; Highland J Highland LThH1 • 1:30 p.m. LThH1 1:30 p.m.–2:45 p.m. 1:30 p.m.–2:45 in Ultracold • Frontiers LThH III Molecules of JILA, Univ. L. Bohn; John Presider USA, Colorado, LThH2 • 2:00 p.m. LThH2 Testing the Testing Time-Invariance of Fundamental Molecules, Cold, So Not and Cold, Using Constants HendrickL. Bethlem discuss discuss the status of two experiments proton-to- the ultimately of time-invariance the testing at aimed molecules CO of beam thermal a using mass electron molecules in a fountain. ammonia cold using and Laser Cooling of a Diatomic Molecule, , E. S. Shuman, J. F. Barry; Yale Univ., USA. Univ., Barry; Yale F. J. , E. S. Mille Shuman, report report experiments the demonstrating laser cooling beam molecular cryogenic A molecule. diatomic a of one- to subjected is (SrF) monofluoride strontium of both observe We cooling. laser transverse dimensional mechanisms. cooling Sisyphus-type and Doppler LS ; Univ. ; of Univ. Ongoing Ongoing experiments ; Princeton USA. Univ., Invited Invited Dmitry Dmitry Budker October 24–28, 2010 GeV, improving previous limit limit previous improving GeV, -33 • Highland H Highland He co-magnetometer to constrain - neu to constrain co-magnetometer He 3 Michael Michael Romalis |<3.7×10 n LThG2 • 2:00 p.m. LThG2 LThG1 • 1:30 p.m. LThG1 1:30 p.m.–3:45 p.m. 1:30 p.m.–3:45 • Metrology and Precision LThG II Measurements of Univ. E. Leanhardt; Aaron Presider USA, Michigan, by a factor of 30. of a factor by tron tron spin coupling to a Lorentz quantum and of CPT models violating many in arising field background |b gravity, California California at Berkeley, USA. will be discussed: measurement of parity violation of variation for search dysprosium, and ytterbium in tests and dysprosium, in “constant” fine-structure the two-photon in photons for statistics Bose-Einstein of in barium. transitions New New Limit on Lorentz and CPT Violation for Neutrons, use a K- We Results of Fundamental Physics Table-Top Ex- periments at Berkeley, - A G. FiO/LS 2010 , Doug 1 Liquid CrystalLiquid 1 ; Liwei Li 1 , Multilayered gra Multilayered 1 eVision eVision Inc., USA. 2 Lei Shi - Mis of Univ. Li; Guoqiang , , Philip J. Bos 2 - applica wide has lens Adaptive for a typical lens. a typical for -4 Highland G Highland HongbingFang , DwightDuston , , James S. Shirk; NRL, USA. NRL, Shirk; S. James , 1 FThU3 • 2:00 p.m. Effects of Diffraction and Partial Reflection in Multilayered Gradient Index Polymer Lenses, Beadie many with fabricated are lenses polymer index dient It indices. refractive different with polymers of layers is shown that, in diffractiveprinciple, and reflective <4 x 10 losses are FThU2 • 1:45 p.m. Lens Refractive Tunable a of Design and Modeling Based on Liquid Crystals, Bryant Inst., Inst., Kent State USA, Univ., 1:30 p.m.–3:30 p.m. 1:30 p.m.–3:30 FThU • Lens Design Carestream Liang; Rongguang USA, Presider Health, FThU1 • 1:30 p.m. Electromagnetic by Actuated Lens Liquid Adaptive Solenoid, USA. Louis, St. at souri low-cost compact, A medicine. and industry in tions adaptive liquid lens actuated by electromagnetic solenoids is The lens presented. large tunable shows high performance. and power tunable tunable refractive lens is modeled, designed, and liquid and structure electrode proper with fabricated phase ideal calculates modeling The material. crystal electrode, each on applied voltage correct and profile focal the desired length. for FiO David , Tomáš Tomáš , 2 Masaryk 3 Johannes K. , Eric Logean Eric , 1 - with “commu Analysis Invited Invited Univ. of Univ. Glasgow, United 1 ; 2 Highland F Highland EPFL EPFL IMT OPT, Switzerland, 2 , Alasdair C. Hamilton C. Alasdair , 1 , Toralf , K. Toralf Scharf 3 We summarize recent work on on work recent summarize We Republic. Czech Univ., unusual perform that sheets transparent METATOYs, light-ray-direction changes. We concentrate on the classification of laws describing light-ray-direction changes as (un)natural, and on our experimental arrays. lenslet confocal of realization FThT1 • 1:30 p.m. P. Scott Carney; Univ. of Illinois at at Illinois of Carney; Univ. Scott P. USA, Presider Urbana-Champaign, 1:30 p.m.–4:00 p.m. 1:30 p.m.–4:00 FThT Optical • Encoding — Nano-photonics, Information Optics and Refractive Diffractive Optical Signals Optics for Shaping Kingdom, Kingdom, Tyc Courtial Progress Towards Progress Windows Towards Performing - Forbid den Light-Ray Direction Changes, Fundamental Limits to Optical Components, Components, Optical to Limits Fundamental USA. Univ., ; Stanford Miller nications modes” between volumes allows rigorous general limits on imaging and communications channels. Together with a new multiple scattering theorem, this approach also leads to fundamental components. optical to limits FThT2 • 2:00 p.m. Thursday, October 28 108 Vahala Optomechanics, Cavity in Lasers Phonon are reviewed. tions, and prospects for and science new technology implementa- example amplification, and cooling mechanical to application Its motion. mechanical andcouplelight to way new providinga is fields cal Biography not available. theory. with agreementexcellent in gain yielded effects parasitic reduce and interaction two-photon nonlinear the enhance to optimized Structures devices. ductor room-temperature electrically-pumped semicon- in specifically solids, in gain two-photon of servation Technion,Israel.Orenstein; AlGaAs, Pumped Electrically in Two-Photonof MeasurementGain •2:15p.m. FThO3 Continued Nano-Optical StructuresIII— •NonlinearOpticsinMicro/ FThO FThO4 •2:30p.m. FThO4 ; Caltech,USA. ; Highland A mr Nevet Amir Cavity enhancement of opti- ofenhancement Cavity Tutorial

We report the first ob first the report We , Alex Hayat, MeirHayat, Alex , Kerry Kerry - Alain J. Kreisler J. Alain using algorithm. phase-retrieval are reported and compared with results of simulation results experimental first The frequencies. terahertz at tested and fabricated were profiles continuous with gratings phase reflection multiplexers, beam Univ.France.Paris, nick F. Dégardin near diffraction-limited mode-locked output.near mode-locked diffraction-limited subsystem which produces 90 W of linearly polarized, 1319 nm master oscillator/power amplifier (MOPA) Technologies,Coherent USA. WilliamIanLee, Sawruk, J.Alford; LockheedMartin W.NicholasP.Jalali,Munib W.Prezkuta , Zachary System, Laser Guidestar a MOPAfor nm 1319 •2:45p.m. FThP6 with uniform sub-pulse polarization states. controlled to generate arbitrarily shaped packet pulse be could stacker fiber geometry, the reflection a ing novel fiber stacker for pulse packet generation. Featur Acad.Engineeringof Physics, China. anjun, Wang Mingzhe; Res. Ctr. of Laser Fusion, China Fiber Stacker, Packet Generation UsingbyPulse Optical Novela •2:30p.m. FThP5 deployment and utilization. practical ablebeen to integrate the two departments for faster has Optimax entities. independent been have floor shop manufacturing optical the and department Inc., USA. Mandina, Jessica De Groote Nelson; Optimax Systems Andrew A. Haefner Floor, Shop Manufacturing Optics the and R&D •2:15p.m. FThP4 Instrumentation—Continued •GeneralOptical FThP on Reflection Phase Gratings, First Experiment on THz Beam Multiplexers Based •3:00p.m. FThP7 Historically, the research and development Li Mingzhong, Lin Honghuan, Wang Ji- 1 Highland B 1 ; , Geoffroy Klisnick 1 Univ Paris-Sud, France,Paris-Sud, Univ , Robert R. Wiederhold, Michael P. To generate high efficiency 1-D efficiency To high generate This paper describes a describes paper This Vishal S. Jagtap 2 , Michel Redon We

developed a developed 2 UPMC 1 , An FiO/LS 2010 2 - - , tionship Qdegradation between thickness. and film rela - the explain to simulationsdeveloped FEM was on based model theoretical A shown. are coatings polystyrene and polymethymethacrylate both using polymer-silica microcavities with Q factors over 1E7 USA. California, Southern Univ.ofArmani; tors, Polymer Coated Silica Ultra-High-Q Microresona - •3:00p.m. FThQ7 are presented. results experimental and discussed, are ternatives - al conventional the over dioxide titanium using of advantages The microresonators. silicon-based of sensitivity temperature the reduce to material ding USA. Atabaki, Ali Asghar Eftekhar, Ali Adibi; Georgia Tech, sonators On SOI, On sonators Microre- Titania-clad In Performance Athermal •2:45p.m. FThQ6 with of ring losses 0.9dB/cm. intrinsic quality factor of 480,000 in 50 µm radii rings oxidation without any silicon etching. We achieve an high-Q silicon ring resonators fabricated by selective Univ.,MichalCornellLipson; USA. Wiederhecker,WeeGustavoS. Luo, JaimeCardenas, Resonators, Ring Silicon Etchless High-Q •2:30p.m. FThQ5 Isolation, Optical 18db with Isolator On-Chip Microring-Based Compatible CMOS A •2:15p.m. FThQ4 micrometer radius. 5 of microring high-Q silicon-on-insulator a with achieved was isolation 18dB to Up coefficients. coupling output and input asymmetric with filters strong optical nonreciprocity in microring add-drop ang, Minghao Qi; Purdue Univ., USA. Wang, Hao Shen, Leo T. Varghese, Ben Niu, Jing Ouy- Continued •MicroResonators— FThQ , Xiaomin Zhang, Andrea M. M. Andrea Zhang, Xiaomin Choi , Seok Hong We propose the use of titanium dioxide as clad- • Highland C Payam Alipour Payam FiO October 24–28,2010 Wedemonstrate We demonstrate , Amir HosseinAmir , Li Fan Li Hybrid Lian- , Jian , applying arelative plates. the between shift tunable filtering applications. The isdevice tuned by for structure metallic plates corrugated two novel a interactions of plasmonic and photonic modes within Levy Reflection, and Transmission Tunabilityof and Modes Photonic and Plasmonic of Interactions the of Control •3:00p.m. FThR6 Purcell effect atPurcell effect second the harmonics. the and frequency fundamentalenhancement the at field combining by enhanced be can media linear non- in generation second-harmonic the that show theoretically we nanoantennas, of pairs designing der Engheta; Univ. of Pennsylvania, USA. Second-Harmonic Generation, Enhancing for Nanoantennas Optical of Pairs •2:45p.m. FThR5 devices can be improved can be devices by cooling. cryogenic optical metal-based of performance that onstrates dem- directly This wavelengths. longer at drop a temperatures. The imaginary part of epsilon exhibits cryogenic constantsataremeasuredgold ofOptical AleksandarYeshaiahuSimic, Fainman;USA. UCSD, Temperatures, Cryogenic at Gold of Properties Optical the of Measurement •2:30p.m. FThR4 up to 18times. by rate emission spontaneous the enhances ment confine - while plasmons,of reflection internal total from arises feedback Strong wavelength. 1/20th to with strong cavity feedback and optical confinement Zhang;Berkeley,UC USA. F.Rupert Oulton,Volker Sorger,J.Xiang Bartal,Guy TemperatureLaser, PlasmonRoom •2:15p.m. FThR3 Processing II—Continued Metamaterials forInformation •Plasmonicsand FThR ; Hebrew Univ. of Jerusalem, Israel. Highland D Avner Yanai, Meir Grajower,Yanai,AvnerMeir Weplasmon reportlasers Maziar P.Nezhad , Maziar Uday Chettiar, Na - Ren-Min Ma, Ren-Min We study the By properly Uriel Uriel symmetric energy—momentumsymmetric tensor. diagonally traceless, a construct to used is dielectric gating electromagnetic field and negligibly reflecting Gordonunique.Theis momentum total propaofa - system closed thermodynamically a of momentum USA. RDECOM, Army US Bahder; B. Field in a Dielectric, Energy-Momentum Tensor for the Electromagnetic •2:45p.m. FThS4 of this structure is also discussed in this work. inthis of discussed structure this is also covered by nanostructures. The formation mechanism densely structure surface large-scale-wave unique a USA. TaekUniv.YongRochester,Guo; ChunleiofHwang , Metals, on WaveFormation Scale Large Covered Nanostructure- Laser-Induced Femtosecond •2:30p.m. FThS3 timescale. picosecond on pulse reflected disturbs strongly Surface plasmon-polaritons with Fano-type lineshape technique. cross-correlation time-resolved using from one-dimensional plasmonic crystal is observed Significant reshaping of femtosecond pulse reflected Univ.,StateMoscowLomonosovFederation. Russian Shcherbakov, Tatyana V. Dolgova, AndreyPolinaP. A. Vabishchevich, Fedyanin;FedorYu. Sychev, MaximR. Crystals, Plasmonic Planar in Plasmons Surface Enhanced Resonantly of Spectroscopy Cross-Correlation Femtosecond •2:15p.m. FThS2 Applications—Continued •StrongTHzFieldsand FThS Usingfemtosecond irradiation, welaser create Highland E Michael E. Crenshaw Vladimir O. Bessonov O. Vladimir The total The , Thomas , Thursday, October 28 109 , 1 , George Integrated Integrated Emil Emil Wolf Delft Univ. of Delft Univ. 2 We We present a Invited An explanation of the Gouy Gouy the of explanation An FiO Barbara Kilosanidze Highland K Highland Univ. of Rochester, USA, of Rochester, Univ. 1 ; 2 FThV and Holographic • Diffractive Optics I—Continued FThV2 • 2:15 p.m. Kakauridze; Inst. of Kakauridze; Georgia. Cybernetics, polarization-holographic element based on the dif- fraction gratings of the different type for complete in of light state and working of analysis polarization wide suggested. spectral 500 - 4200 nm is range Netherlands. Technology, shown is it and presented is focus near anomaly phase the of each near effect this of generalization a is there rays. pencil of astigmatic an focal of lines FThV4 • 3:00 p.m. Integral Polarization-Holographic Element for Real-Time Complete Analysis of the - Polariza tion State of Light, Taco Visser Taco 3-D 3-D Optics: From Diffractive to Subwavelength, George ; Barbastathis MIT, USA. - modu index refractive 3-D where devices of sequence lation at different scales – from several wavelengths to fraction of a wavelength — results in unique and with slicing confocal-like e.g. behavior, optical useful and simultaneously, planes several at focus multiplex arbitrary gradient index definition for aberration methods manufacturing and Fabrication correction. will also challenges be and discussed. FThV3 • 2:45 p.m. Gen- Its and Anomaly Phase Gouy the of Origin The eralization to Astigmatic Wavefields, We velocity velocity selection, STIRAP ; Univ. of ; Malaysia. Malaya, Univ. Highland J Highland Raymond Ooi LThH • Frontiers in Ultracold • Frontiers LThH III—Continued Molecules LThH3 • 2:30 p.m. LThH3 Selec- Velocity Zero by Molecules of CoolingLaser tion, present laser cooling scheme for molecules using repeated Raman zero deceleration and accumulation by single - spontane ous emission which circumvents the multilevels in molecules. Smulations with OH show practicality the scheme. of

LS - - -9 [Phys. Rev. Rev. [Phys. et al Hg EDM search search EDM Hg 199 Tom Loftus; Univ.Tom of e cm (95% C.L.). Hg, Hg, -29 199 Invited , John Lawall, Yicheng Wang; Wang; Yicheng Lawall, John , October 24–28, 2010 We describe the describe We • Highland H Highland Hg)| < 3.1 x 10 Hg)| A high resolution Fabry-Perot interfer 199 Mathieu Durand Mathieu 102, 101601 (2009)] which gives a new upper LThG • Metrology and Precision • Metrology and LThG II—Continued Measurements Washington, USA. Washington, recently completed by W. C. Griffith C. W. by completed recently Lett. |d( bound: ferometry: A Bridge Between the Meter and the Farad, USA. NIST, displacement. measure to designed is system ometer δL/L~1.25x10 of uncertainty fractional a achieve We LThG3 • 2:30 p.m. LThG3 Inter Displacement High Fabry-Perot Resolution without any optical any without frequency and standard, resolve 7 nm. over in a piezoelectric actuator hysteresis LThG4 • 2:45 p.m. LThG4 An An Improved Limit on the Permanent Electric of (EDM) Moment Dipole - FiO/LS 2010 Stan Szapiel, We We use interference

G. ,Beadie A. Rosenberg, ; Raytheon ELCAN Optical G. ,Beadie E. Fleet, James S. A state-of-the-art lens design - ap analytic an developed have We Highland G Highland Cheng-Fang Cheng-Fang ,Ho Wei-Cheng Lin, FThU • Lens Design—Continued FThU7 • 3:00 p.m. Optical Performance of Airborne Multi-Spectral Camera Lens, Chang, Shenq-Tsong Huang; Ting-Ming Instrument Taiwan. Labs, Res. Applied Natl. Ctr., Res. Technology - opto-mechan about method a provides research This ical design and assembly of ITRC airborne camera camera of parameters performance optical The lens. filed and function translation Modulation as such lens presented. and measured are curvature FThU4 • 2:15 p.m. Refractive Index Dispersion Curves Measured for Several Polymer Films, James S. Shirk; NRL, USA. fringes measured in spectratransmission combined with high-accuracy index measurements at point wavelengths to construct dense, high-accuracy refractive index curves across the visible for several films.polymer FThU5 • 2:30 p.m. Gradient Index Polymer Optics: Achromatic Singlet Lens Design, USA. NRL, Shirk; useful singlet designing for achromatic proximation lenses index gradient on based are designs The lenses. Ray materials. polymer nanolayered from fabricated traced results confirm the achromatic performance the designs. of FThU6 • 2:45 p.m. Implementing Lens Design Software in a Dis- tributed Computing Environment, Catherine Greenhalgh Canada. Technologies, software (CodeV®) is deployed and enabled in the distributed computing environment. Impact on other and optimization, global tolerancing, statistical design discussed. practices is lens ; , - 2 2 FiO Rajesh , 1 We report We , Trisha , Andrew Trisha 1 , Stefan Sinzinger 1 MIT, USA. MIT, 2 Technical Univ. Illmenau, Illmenau, Univ. Technical 2 Invited , Mohit Diwekar 1 Nicole Nicole Brimhall Highland F Highland Markus Testorf Optical free form surfaces implement

Univ. of Utah, USA, of Utah, Univ. 1 ; 1 Dartmouth College, USA, College, Dartmouth Germany. surfaces. optical ing elements with potentially large surface gradients and and gradients surface large potentially with elements diffraction approximate An depths. modulation large design and analyzing for tool a as developed is model FThT4 • 3:00 p.m. DiffractionApproximate Model for Optical Free Form Surfaces, 1 FThT3 • 2:30 p.m. FThT Optical • Encoding — Nano-photonics, Information Optics and Refractive Diffractive Optical Optics for Shaping Signals—Continued on a novel method of optical nanopatterning, where where nanopatterning, methodoptical of a novel on transformations photochemical wavelength-selective spatial sub-wavelength deep achieve to exploited are photons. visible and near-UV with resolution Rajakumar Manthena On Breaking the Abbé Diffraction Limit in Optical in Limit Diffraction Abbé the Breaking On Nanopatterning., Menon Thursday, October 28 110 two-photon absorption on the 5S Physics, USA. Engineering and Applied of School Gaeta; man Fibers, PhotonicBandgap in Rb Two-PhotonPowers with Milliwatt at Absorption •3:15p.m. FThO5 Continued Nano-Optical StructuresIII— •NonlinearOpticsinMicro/ FThO in the fiber.in the power of mW We~1 with absorption ~1% estimate fiber. bandgap photonic a to confined vapor Rb in , Kasturi Saha, Pablo Londero, Alexander L. L. Alexander Londero, Pablo Saha, Kasturi , We observe large enhancement of Doppler-free Highland A 1/2 Vivek Venkatara Vivek to 5D 5/2 transition - and calculation. prediction theoretical the well agrees dependence This concentration.dopant substrate silicon the on microtoroid depends silica the of factor (Q) quality USA. Choi, Andrea M. Armani; Univ. of Southern California,Toroidal Microcavities, of Factor Q the on Impurities Substrate of Effect •3:15p.m. FThP8 Instrumentation—Continued •GeneralOptical FThP We have experimentally demonstrated that the 3:30 p.m.–4:00p.m. Highland B Xiaomin Zhang , Hong Seok Coffee Break,Highland Ballroom Foyer, Rochester Riverside Convention Center FiO/LS 2010 direction waveguide coupling scheme. tangentialconventional the to compared output onstrates higher coupling efficiency into a single-port dem- simulationnumerically.investigated FDTD is disk lasers using radial direction coupling waveguide of Electrical Engineering and Computer Science, USA, ag Ou Fang 2 dial Direction Coupling Waveguide,Coupling Direction dial - Ra by Lasers Microdisk from Light of Extraction •3:15p.m. FThQ8 Continued •MicroResonators— FThQ OptoNetInc.,USA. 1 , Yingyan Huang Yingyan , • Highland C Extraction of light from micro- from light of Extraction FiO October 24–28,2010 2 , Seng-Tiong HoSeng-Tiong , Xiangyu Li Xiangyu 1 ; 1 Dept. Dept. 1 , the antennathe respectively. particles, difference,and relativea plasmonic enhancement of iour of a cross-dipole nanoantenna is due to a length behav- dichroic andbirefringent thatdemonstrated Weinvestigated. are nano-antennas plasmonic of Univ.,Turkey.banci Nano-Antennas, Birefringent and Dichroic Behaviour of Plasmonic •3:15p.m. FThR7 Processing II—Continued Metamaterials forInformation •Plasmonicsand FThR Highland D - Sa Sendur; Kursat , Ogut Erdem Birefringence and dichroism and Birefringence Highland E Thursday, October 28 111 , 1 AFRL, USA, 1 ; 2 , Kenneth , L. Kenneth Schepler 1 An electro-optic beamswitch beamswitch An electro-optic FiO Highland K Highland , Andrew Sarangan 2 Jonathan W. Evans Jonathan W. Univ. of Dayton, USA. Dayton, of Univ. FThV5 • 3:15 p.m. A Novel Electro-Optic Beam Switch in 5mol% Magnesium-Oxide Doped Congruent Lithium Niobate, FThV and Holographic • Diffractive Optics I—Continued was was designed to betweenswitch two discrete optical beam maximum for optimized was switch The paths. Simulation techniques. analysis ray using translation using a finite-difference beam propagation method analysis. verified the ray 2 Peter Peter E. Powers Highland J Highland LS , ; - 1,2 1,2 For the For first European labo European Jeongwon Jeongwon Lee, 2 , Paolo De Natale 1,2 Pablo Pablo Cancio Pastor October 24–28, 2010 , Simone Borri • Highland H Highland 1,2 A continuous tungsten carbide (WC) molecular (WC) carbide tungsten continuous A Inst. Nazionale di Ottica-CNR, Italy, Italy, Ottica-CNR, di Nazionale Inst. LThG5 • 3:15 p.m. LThG5 Continuous Supersonic Beams for an Electron Electric Dipole Moment Search, Jinhai Chen, Aaron Leanhardt; Univ. of Michigan, USA. of existence the for probe to developed being is beam (EDM) moment dipole electric permanent possible a beamthe of divergence fluxand The electron. the of characterized. are LThG • Metrology and Precision • Metrology and LThG II—Continued Measurements LThG6 • 3:30 p.m. LThG6 Metrological Towards Grade Mid-IR Quantum Cascade Laser Sources, 1 SaverioBartalini Italy. Spectroscopy, for Non-linear ratory time, the intrinsic QCL linewidth is measured and compared with the theory. The narrow linewidth, well beyond limit, the Schawlow-Townes “classical” opens new scenarios thefor molecular-based clocks mid-IR metrology. and FiO/LS 2010 Highland Ballroom Foyer, Rochester Riverside Convention Center Convention Riverside Rochester Foyer, Ballroom Coffee Break, Highland , Yuan-Chieh , Yuan-Chieh 2 Graduate Inst. of of Inst. Graduate 2 Instrument Technology Res. Technology Instrument 1 ; 2 , Yen-Liang , Liu Yen-Liang 1 Highland G Highland 3:30 p.m.–4:00 p.m. , Guo-Dung Su Wei-Yao Hsu Wei-Yao 1 This paper focuses on the design and fabrication fabrication and design the on focuses paper This

technologies of the PAL. The PAL surface is described is surface PAL The PAL. the of technologies by B-spline parameters. After the optimization of B-spline parameters, the surface is fabricated using technology. turning CXZ diamond FThU8 • 3:15 p.m. Addition Progressive the of Fabrication and Design Lens, FThU • Lens Design—Continued Ctr., Natl. Applied Res. Labs, Taiwan, Taiwan, Labs, Res. Applied Natl. Ctr., - Tai Univ., Taiwan Natl. Optoelectronics, and Photonics wan. Cheng , FiO 2,3,5 , W. 1 BER- -9 Dept. of of Dept. Jingjing 5 , Vikrant , William 1 We present the present We We present format format present We , Gary M. Carter Lab Lab for Physical Sci- 4 2 Jeffrey B. Driscoll Microelectronics Microelectronics Sciences 1 ; , Jerry I. Dadap 1 1 Manjunath Manjunath Somayaji Highland F Highland Ctr. Ctr. for Advanced Studies in Photonics , Yurii A. Vlasov 3 The The spatial frequency response of cubic 4 IBM T. J. Watson Res. Ctr., USA, Ctr., Res. Watson J. T. IBM 4 , Xiaoping Liu 2,3 , David Fattal, Marco Fiorentino, Raymond G. Labs, Labs, Columbia USA, Univ., FThT6 • 3:30 p.m. Conversion Format of 10 Transparent Gb/s NRZ- OOK Data to RZ-OOK in a Si Photonic-Wire Waveguide Using XPM, Astar FThT Optical • Encoding — Nano-photonics, Information Optics and Refractive Diffractive Optical Optics for Shaping Signals—Continued R. Bhakta, Marc P. R. Christensen; Bhakta, Marc Southern P. Methodist USA. Univ., extreme under imagers coding wavefront mask phase The experimentallymeasured. is defocusconditions results are compared against analytically derived expressions for optical transfer functions of these systems. imaging computational receiver-sensitivity receiver-sensitivity enhancement for the converted signal. Scalability of the technique beyond 160 Gb/s theoretically. shown is FThT7 • 3:45 p.m. Transfer Optical Exact of Validation Experimental Coding Function of Cubic Phase Mask Wavefront Imaging Systems, Computer Science and Electrical Engineering, Univ. of of Univ. Engineering, Electrical and Science Computer USA. County, Baltimore Maryland, conversion of 10-Gb/s NRZ-OOK to RZ-OOK via XPM in with a a Si 2.5-dB Photonic-Wire 10 method of designing optical cavities of high quality factors and small mode volumes with most of the by supported space, freethe in field standing optical non-periodic dielectric gratings. Li USA. Labs, Hewlett-Packard Beausoleil; FThT5 • 3:15 p.m. Optical Cavity Mode Standing in the Free Space from Non-Periodic Dielectric Gratings, Res., USA, USA, Res., Richard Richard M. Osgood, Jr. ences, ences, USA, M. M. J. Green Thursday, October 28 112 High Frequency Operation, Frequency High for Devices Photonic and RF of Integration 3-D rectifiers. thermal sub-wavelengthsuper-scatterer, and photon-baseda a meta-materials, plasmonic for theory band tonic pho- a include Examples structures. nanophotonic USA. Photonic Band Theory, Rigorous to Concept Index Refractive from rials, Meta-Mate- Three-Dimensional Understanding FThW2 •4:30p.m. FThW2 FThW1 •4:00p.m. FThW1 USA, Presider Zhaolin Lu; Univ. of Delaware, materials •Three-dimensionalMeta- FThW 4:00 p.m.–6:00p.m. properties of bulk semiconductor the material. with layers semiconductor crystalline conformable and deformable, flexible, of placement the enabling their substrates and redeposited on foreign substrates, semiconductor materials that have been released from USA. Delaware, of We review our recent works in the theory of theory the in works recent our review We Highland A Nanomembranes are crystalline crystalline are Nanomembranes Shanhui Shanhui Fan Invited Invited Dennis Prather Dennis ; Stanford Univ., ; Univ.; Wei-YaoHsu Applied Res. Labs, Taiwan, basis required for alevel of accuracy. of number minimize to surfaces freeform for RBFs of use extends Method given. is surfaces freeform optical describe toRBF-QR, method, function basis Rochester,USA. of Optics Surfaces, Optics Freeform for Method Function Basis Radial A •4:00p.m. FThX1 Wavefront Error, Slope, and PVr. outlined be here will include Mid-Spatial Frequency that Specifications elements. optical precision of intended to more thoroughly define figure and form tolerances and specifications to introduction an is Martucci Valley,to Peak than More Specifying •4:30p.m. FThX3 concentrate problem. two surfaces aspheric-cylindrical to solve the energy ment.We novela free-formdesign shapedwithlens - instru leveler laser green for lens shaped free-form This paper focuses on the design and fabrication of the TaiwanUniv.,Taiwan.Natl.Engineering, Electrical 1 USA, Presider Marty Valente; Univ. of Arizona, •Fabrication &TestingFThX 4:00 p.m.–6:00p.m. Engineering,Natl. Tsing Hua Univ., Taiwan, Jen WangJen for Laser Leveler Instrument, Design and Fabrication of Free-Form Shaped Lens •4:15p.m. FThX2 Univ.CentralUSA, ofFlorida, ; Optimax Systems Inc., USA. Inc., Systems Optimax ; 2 ; 1 Instrument Technology Res. Ctr., Natl. Ctr., Res. Technology Instrument 1 , Yi-Hsien Chen Yi-Hsien , Highland B Ilhan Kaya Ilhan Explicit formulation of a radial radial a of formulation Explicit 2 Dept. Dept. of Power Mechanical 1 , JannickP.Rolland, 3 Yuan-Chieh Cheng , Guo-Dung Su Guo-Dung , 2 Inst. of Optics, Univ.Optics,Inst. of Michael G. G. Michael This paper This 3 Dept.of 3 , Pei , FiO/LS 2010 1,2 1,2 , ;

Ray Detection, Far-Field with Enhancement Simple Demonstration of Visible Evanescent Wave FThY1 •4:00p.m. FThY1 Presider to Announced Be Processing III Metamaterials forInformation •Plasmonicsand FThY 4:00 p.m.–5:30p.m. North Carolina at Chapel Hill, USA, Hill,ChapelCarolina at North simple total internal configuration. reflection a in probed being and visible the in operating while ones propagating into waves evanescent converts and amplifies both that device grating diffraction demonstrate the fabrication of a simple metamaterial- Carolinaat Chapel Hill, Dept.ofChemistry, USA.We the periodicity twice of twice interparticle the spacing. periodicity the from originatingorders diffraction near resonances the spectrum is characterized by additional geometric alternatively,nanoparticles spherical gold and silver China. Arrays, terferences in Heterogeneous Ag/Au Nanoparticle Geometric Resonances Imposed by Destructive In- •4:30p.m. FThY2 1 , Meredith J. HamptonJ.Meredith , In a newly proposed binary array composed of Ying Gu, Jia Li, Qihuang Gong; Peking Univ., • Highland C FiO October 24–28,2010 Invited 2 , Rene Lopez Rene 2 Univ.North of 1 ; Emily A. A. Emily 1 Univ. of of Univ. resonances carbon nanotubes. insingle-walled intraexcitonic quasi-1-D and graphene in fermions yielding insight into the dynamics of quasi-2-D Dirac nanomaterials,carbon of studies for pulses infrared mid- and THz tunable of applications review will Kaindl Nanomaterials, Carbon in Correlations Ultrafast THz Studies of and Electronic Dynamics reviewed. be will applicationsfuture possible and present and TPFE, front-excitation (TPFE). THz pulse generation using be generated by velocity-matching using tilted-pulse- can systems table-top from pulses THz single-cycle Fontμ]]J) Symbol - [[UnsupportedCharacter Hungary.Pécs, Univ.of Physics, Experimental of Dept. Almási; Hebling Applications,Frontits andExcitation Pulse Tilted by Generation Pulse THz Energy High Keith Nelson; MIT, USA,Presider USA, Presider Richard D. Averitt; Boston Univ., Optics •THzFieldsandNonlinear FThZ 4:00 p.m.–5:45p.m. FThZ1 •4:00p.m. FThZ1 FThZ2 •4:30p.m. FThZ2 ; Lawrence; BerkeleyNatl. Lab, USA. , József A. Fülöp, László Pálfalvi, GáborPálfalvi, László Fülöp, A. József , Nowadays, highest energy (up to 30 to (up energy highest Nowadays, Highland D Invited Invited Robert A. Robert This talk talk This János János heating of agreen laser. absorptionheating of andan infraredresonantlaser the on based mechanism self-stabilization a using microdroplets located on a superhydrophobic surface salt-water individual from lasing Raman longed Universty,Turkey.Koç Kiraz; Alper Sennaroglu, Alphan Cankaya, Hüseyin Yüce,Yavuz Surface, Superhydrophobic a on WaterMicrodroplets Salt- Size-Stabilized in Lasing Raman Prolonged •4:15p.m. FThAA2 ven T.Cundiffven Lijun Yang Lijun Technology,USA, and Standards of Inst. Natl. and Colorado Univ.of fabrication scheme. facile this using electroluminescence temperature films as the active layer. We achieved efficient room- nanocrystal lead-sulfide dip-coated using diodes light-emitting infrared near low-cost of properties USA. XinXu,Ma, Nanocrystals, PbS On Based Devices cence Electrolumines Near-infrared Efficient Highly •4:30p.m. FThAA3 Karaiskaj Denis Quantumwells, Semiconductor in Resonances Dimensional Fourier-Transform Spectra of Exciton Two- in Coherences Many-Body Two-Quantum •4:00p.m. FThAA1 nia, USA, nia, Australia, Presider David Moss; Univ. of Sydney, Devices •OpticsinMicro/nano FThAA 4:00 p.m.–6:00p.m. separated from bound biexciton coherences. be can coherences many-body result, a As isolated. be to semiconductors in coherences two-quantum allows spectroscopy 2DFT interactions.many-body to attributed are spectra (2DFT)Fourier-transform USA. Two-quantum coherences intwo-dimensional We report on the structural and optoelectronic YasinKaradag 2 4 , ShaulMukamel, Natl. Inst. of Standards and Technology,and Standards of Inst. Natl. ; Univ.; Cloutier SylvainG. Delaware, of 2 ; 1 Univ. of South Florida, USA, Univ.Florida, South of Highland E 1 , Alan D. Bristow D. Alan , 3 Chemistry Dept., Univ.Dept.,Califor Chemistryof , Mustafa, Gündoğan,Mehdi 3 , Richard, P. Mirin 2 , Xingcan Dai Xingcan , We show pro show We 2 4 JILA, JILA, , Ste - , Fan Fan 2 - - - , Thursday, October 28 113 NOTES October 24–28, 2010 • FiO/LS 2010 ______, ; - 1 Korea 2 , Seyoon 1 , Junghyun Park 1 Andrew Andrew J. Waddie Invited Invited , Seong-Woo Cho , Seong-Woo 2 We present a nanostructured nanostructured a present We FiO Byoungho Byoungho Lee Highland F Highland , Hwi , Kim Hwi 1 Seoul Seoul Natl. Korea, Univ., Republic of, 1 ; 1 We show various analogies analogies various show We of. Republic Korea, Univ., diffractive classical to optics diffractive plasmonic of plasmonic of characteristics distinguished and optics diffractive metallic subwavelength optics. Novel de- also presented. vices based are those properties on Kim FThBB1 • 4:00 p.m. 4:00 p.m.–6:00 p.m. 4:00 p.m.–6:00 FThBBDifractive and • Optics II Holographic USA, MIT, Barbastathis; George Presider Seung-Yeol Lee Seung-Yeol Plasmonic Diffractive Optics - Its Analogy to Clas- to Analogy Its - Optics Diffractive Plasmonic Subwavelength for Use and Optics Diffractive sical Metallic Devices, Theoretical and Practical Implementation of Novel Novel of Implementation Practical and Theoretical Nanostructured Diffractive and Micro-Optics, Mohammad R. Taghizadeh, FThBB2 • 4:30 p.m. micro-optical micro-optical design technology, compatible with the stack-and-draw photonic crystal fibre fabrica Heriot-Watt Univ., UK. Univ., Heriot-Watt tion technique, which allows the of fabrication high NA microlenses and sub-wavelength diffraction gratings. Thursday, October 28 114 laos laos Efremidis conventional optical lens -Fourier transform. resolving power, but also have the basic functions of a super have only not superlenses Such superlensing. for metamaterials to mechanisms compensation USA. Diego, San at California Univ.of Liu; Zhaowei Ma, Changbao Superlenses, Metamaterial Compensated Phase •5:00p.m. FThW3 materials—Continued •Three-dimensionalMeta- FThW agreement with our theoretical predictions. induced three-dimensional photonic lattices, in good sion via coherent-destructive-tunneling in optically- transmisimage- and negativerefraction diffraction, anomalous of demonstration experimental first the kai Univ., China, Miller tive Tunneling in 3-D Photonic Lattices, - Destruc Coherent on Transmission ImageBased and NegativeRefraction, Diffraction, Anomalous •5:15p.m. FThW4 1 , Peng Zhang 3 ; 1 San Francisco State Univ., USA, 3 Highland A Univ. of Crete, Greece. We introduce two types of phase of types two introduceWe 1 , Yi Hu 1,2 , Zhigang Chen We report on Alexandra Alexandra 1,2 , Niko- 2 Nan - Elements, Elements, Micro-Retro-Reflecting Singulated ofFabrication •5:00p.m. FThX5 ton of NorthCarolinaof Charlotte,at USA, Univ.Communications,Optical and Optoelectronics drive cost out of design. the help will restrictions these Understanding shapes. restrictions that hinder producing particular aspheric geometrical are There design. lens aspheric during consider to topics with designers present will paper USA. Inc.,MichaelSystemsMandina;Optimax Designer, the for Considerations Manufacturing Asphere •4:45p.m. FThX4 estimating rms the of difference. this ability estimates are derived by tailoring methods for Manufactur surface. its over curvatures principal is typically related to the difference between the local gies Inc., USA. pheres, Simple Manufacturability Estimates for Optical As- •5:15p.m. FThX6 near infrared. the in retro-reflectivity for optimized are and film, thin metallic a with coated skeletons dielectric of photolithographypresented.is elementsThe consist conventionalusingelements optical retro-reflecting USA. Continued •Fabrication &Testing—FThX 2 , Stephen Leibholz Stephen , The fabrication and testing of singulated micro- Greg W. Forbes, P. E. Murphy; QED Technolo- Menelaos K. Poutous K. Menelaos Mark Schickler Mark The difficulty of fabricating an asphere Highland B 2 , Eric G. Johnson G. Eric , , Robert Wiederhold, Wiederhold, Robert , 1 , Michael J. Mas J. Michael , 2 VizorNet,Inc., 1 ; 1 Ctr. for Ctr. This FiO/LS 2010 - - Sciences Labs, Columbia Univ.,USA, Columbia Labs, Sciences Jonathan E. Spanier without compromising response. time 10 than greater factor a by increased is absorption Finite-difference Time-domain simulations. Substrate via investigated are GaAs on photodetector Metal Metal-Semiconductor- planar enhanced Plasmon USA. Arsenide, Arsenide, al-Semiconductor-Metal Photodetector on Gallium Optimization of a Surface Plasmon Enhanced Met- •4:45p.m. FThY3 transmission . enhanced an observe to taper fiber photoniccrystal perimentally investigated metalized nano-structured ex also Wearrangements. various for investigated numerically was film silver thin the in holes length sub-wave- of arrays through light Transmissionof of. RepublicYonseiUniv.,Korea, Kyunghwan Oh; Im, Seongil Park, Hoon Ji Park,Pournoury, Minkyu Taper,Fiber Crystal nic Photo Nano-Structured Metalized a through Transmission Optical Enhanced Plasmoically •5:15p.m. FThY5 composite system. the of distribution current the enhance can one gaps dipoles CNT inside particles plasmonic using that shown investigated.is Itis materials plasmonic with integrated antenna nanotubes carbon of array laei BabakMemarzadeh, Hao,Zhengwei monic Particles Offering Enhanced Characteristics, Plas- Nanotubes Integratedwith Carbon of Array •5:00p.m. FThY4 Processing III—Continued Metamaterials forInformation •Plasmonicsand FThY ; Northeastern Univ.,USA. Northeastern ; The effects of grating geometry on a Surface a on geometry grating of effects The Richard Richard R. Grote • Highland C 2 , Bahram Nabet Bahram , FiO October 24–28,2010 1 ea Arabi Hesam , Richard M. Osgood, Jr. The performance of performance The 2 ; 1 Hossein Mosal Microelectronics 2 Drexel Univ.,Drexel , Marzieh , 1 - - - ,

ment with previous measurements is reported. the absorption of a focused pump beam. Good agree- changes of a collimated probe light beam generated by nontransparent samples by measuring the reflectivity Univ.,USA. StateDelawareNoureddineMelikechi; Gwanmesia, Raghunath Dasari Raghunath Steve R. Flom R. Steve spectral region. spectral blue the in absorber nonlinear effective as potential their demonstrate kinetics intensity-independent with cross-sections excited-state-absorption Large ~1. yield with crossing intersystem rapid undergo based phthalocyanines are reported. These materials Tech,USA. Samples, Nontransparent of Diffusivity Thermal of tion Determina for Method Mirror Photo-Thermal •5:00p.m. FThZ3 San-Hui Chi San-Hui Phthalocyanine, Ruthenium-Based New a of ics Photophys- Blue: the in Absorption Nonlinear •5:15p.m. FThZ4 Optics—Continued •THzFieldsandNonlinear FThZ AristidesMarcano The photophysics of novel ruthenium- novel of photophysics The Weof diffusivity thermal the determine 1 1 , JamesShirk, S. , Sang Ho Lee Ho Sang , Highland D 2 , Seth R. Marder R. Seth , , Franz, Delima, Gabriel 1 ; 1 , Mason A. WalokA. Mason , 1 NRL, USA, NRL, 2 , Guy Beadie Guy , 2 Georgia Georgia 1 1 - , , high permittivity.high of material a with dotquantum the surrounding by ps 600 of value the to reduced be can dot quantum CdSe/ZnS a of lifetime spontaneous the that show USA. UTA,Vasilyev;Michael Stelmakh, M. Nikolai Samudrala, Sarath Zhu , Lei Core-Shell Quantum Dots at Air-Material Interface, CdSe/ZnSe of Lifetimes Emission Spontaneous •4:45p.m. FThAA4 tion in a Vapor Cell, Ireland, Ireland, Sile Nic Chormaic Nic Sile tion of rubidium vapor density is investigated. frequency shift in the absorption spectrum as a - func atom-surface interactions of a hot rubidium vapor. A the obtainedtoobserve usingtapered a optical fiber Vapor Cell, a in Nanofiber Optical an using Spectrum tion Absorp- Rb in Frequency-Shift a of Observation •5:15p.m. FThAA6 2 Ward presented for bio-sensing applications. of this device as a sensitive atom-optic sensing tool is to the cooling transition of for tuning whispering gallery modes in microspheres Modes in Microspheres to the Gallery Whispering ofTuning Thermo-Optic •5:00p.m. FThAA5 Devices—Continued •OpticsinMicro/nano FThAA Tyndall Natl. Inst., Ireland. 2 , 2 Sile Nic Chormaic Nic Sile Tyndall Natl. Inst., Ireland. Amy Watkins Highland E 1,2 Amy Watkins ; 1 Univ. College Cork, Ireland, Cork, College Univ. 1,2 85 We demonstrate a method , Kieran Deasy Rb in vacuum. The ability 1,2 ; 85 1 Univ. College Cork, Cork, College Univ. We experimentallyWe Rb Cooling Transi- 1,2 We present results , Jonathan Ward Jonathan , 2 , Jonathan 2 , Thursday, October 28 115 NOTES October 24–28, 2010 • FiO/LS 2010 ______Optical Optical , Jun Ke, Xin Zhang, Edmund FiO Matt Matt E. ; Anderson San Diego Femtosecond Femtosecond optical vortices are

Highland F Highland Xianglin Xianglin Li FThBB4 • 5:15 p.m. Reconstruction in OpticalBayesian - Scanning Ho lography, created with a reflective programmable pulse shaper. shaper. pulse programmable reflective a with created Patterns include the spiral phase mask, blazed will fork authors The phase. spiral modulated and grating, work. their latest present and discuss these results Y. Lam; of Univ. Hong Kong, Hong Kong. scans that technique a is (OSH) Holography Scanning 3-D objects onto a 2-D hologram. Here, we analyze - Bayes a from process reconstruction object OSH the solution. appropriate an provide perspective and ian State Univ., State USA. Univ., FThBB3 • 5:00 p.m. Generation of Modulated withVortices a - Femto second Laser and a Programmable Pulse Shaper, Antonio Talamantes, FThBBDifractive and • Optics II—Continued Holographic Thursday, October 28 116 intensity distribution of eachelement. light the controlling by realized is which shape, of terms in especially homogeneous be must elements tosecond laser pulse and the hologram, all fabricated Japan. Forum, Glass New Tanaka; Shuhei Suzuki, Jun’ichi quasicrystallographic photonicquasicrystallographic chiral structures. perimentally investigate for the ex- first we time the engineering, complex phase optical By shifts. phase engineered with structures complexphotonicchiral versatile single step fabrication approach for scalable IndianInst.Technologyof Delhi,India. Structures, Chiral tonic Pho - Complex Scalable FabricationofStep Single •5:45p.m. FThW6 Hologram, the by Microfabrication 3-D Homogeneous The •5:30p.m. FThW5 materials—Continued •Three-dimensionalMeta- FThW

For the 3-D microfabrication using the fem- the microfabricationusing 3-D the For Masahiro Yamaji Masahiro Highland A Jolly Xavier Jolly , Hayato Kawashima,Hayato , , Joby Joseph; Joby , Wepresenta on lens drawings. tolerances centration specify to how and software manufacturing errors can in modeled lensbe design how doublets, cemented and singlets in errors ing manufactur centration lens of sources at look will Light rors for Singlets and Cemented Doublets, Er Centration as-Built Modeling and Specifying •5:30p.m. FThX7 coated surface. a of measurement PSI a from data form surface interpreting accurately in difficulty discusses paper This examined. is measurementsinterferometric of coatings interference thin-film to due reflection on USA. Inc., Systems, faces, Sur Optical Coated Film Thin of Measurements InterferometricDistortionon Phase of Effect The •5:45p.m. FThX8 Continued •Fabrication &Testing—FThX ; Optimax Systems, USA. Systems, Optimax ; Jonathan T.Jonathan Watson Highland B The effect of phase distortion phase of effect The , DanielOptimaxSavage; , This presentation This Brandon Brandon FiO/LS 2010 - - - • Highland C FiO October 24–28,2010 and gas pressure was measured. chirp initial on dependence its and focused-beams, free-space to compared powers lower significantly at observed was SPM studied. was fibers bandgap photonic gas-filled in pulses femtosecond of (SPM) rion Univ. of the Negev, Israel. Fibers, Pulses in Gas Filled Hollow Core Photonic Bandgap Ultrashort Chirped of Modulation Phase Self •5:30p.m. FThZ5 Optics—Continued •THzFieldsandNonlinear FThZ Amir Amir Gilad Highland D , Amiel Ishaaya, Ilana Bar; Ben-Gu- Self-phase-modulation technique of electromagnetic patch antenna model. the fundamental physics of this problem using a novel properties are modified significantly. Here, we studied radiation itscavity, sub-wavelength a inside placed ParisTech,France. TELECOM optical admittance are presented. using quantumwells of propertieswave guided and free-space for models Compact constant. structure fine the by set is wells quantum semiconductor in admittance of interband and intersubband transitions Thomas Szkopek; McGill Univ., Canada. Devices, Optoelectronic forWells Quantum Semiconductor of Model Admittance Optical •5:30p.m. FThAA7 Jagtap Modes Cavity Antenna,Patch and to Feeds Dipole Using Coupling Radiation of Study •5:45p.m. FThAA8 Nanostructures, CNRS-LPN, France, Devices—Continued •OpticsinMicro/nano FThAA 1 , Christophe Minot Christophe , Highland E 2,1 ; 1 Lab of Photonics and Photonics of Lab When the dipole is dipole the When 2 Inst. TELECOM, The optical Vishal S. Vishal Thursday, October 28 117 NOTES October 24–28, 2010 • FiO/LS 2010 ______, 1 A phase , Zhangjie Nektarios 1 Res. Res. Dept., Integrity 2 , Martin R. Hofmann 1 We use photorefractive photorefractive use We Univ. of Univ. at Texas Austin, Jinyang Liang 1 ; 1 FiO Highland F Highland Photonics Photonics and Terahertz Technology, 1 , Nils C. Gerhardt C. Nils , ; 1 2 Southwest Southwest Jiaotong China. Univ., 2 , Michael F. , Becker Michael F. 1,2 compression technique is that compression demonstrated creates a peak to destructively interfere with the undesired diffractedzero-order beam in a produced hologram and precision Image SLM. phase-only pixelated, a by diffraction efficiency simulated. are of Small-Scale Systems/High-Temperature Materials, of Small-Scale Systems/High-Temperature Germany. Bochum, Ruhr-Univ. two-wave mixing gain in for amplification coherent of reconstruction the enables This holography. digital amplitude and phase images that are not detectable range. dynamic otherwise, enhanced an to leading FThBB6 • 5:45 p.m. Phase Compression Technique to Suppress the Zero-Order Diffraction from a Pixelated Spatial Light Modulator (SLM), Koukourakis FThBBDifractive and • Optics II—Continued Holographic FThBB5 5:30 p.m. • Mixing Photorefractive Two-Wave for Image Amplification in Digital Holography, Ruhr-Univ. Bochum, Germany, Ruhr-Univ. Cao Yiu Yiu Wai Lai USA, Key to Authors 131 , FTuV3 FMC3 FWA4 Bittner, Eric–LTuC1 Bittner, STuD1 John– Bjorkholm, , FWA1 Joss–FTuU4, Bland-Hawthorn, ,FWP4 FWP3 Y.– Konstantin Bliokh, M.– STuC2 Steven Block, LWA4Z.– Jacob Blumoff, LThH , LThB1 L.– Bohn,John R.–FWV3 Matthew Bolcar, Boltasseva, Alexander–FWG3 O.–FWS1 Bondarenko, D–LWE4 Bonneau, JTuA31 Aldårio C.– JTuA29, Bordonalli, V.–FWB2 Boriskina, Svetlana Kjetil–FTuN1 Børkje, D.–FTuC1 Borlaug, FWN2 Antonin– Borot, Rocio– FTuR3 Borrego-Varillas, Borri, Simone–LThG6 Bos, J.–FThU2 Philip A. C.–JWA08 Carlos Bosco, C.–FThJ2, FThJ3 Lindsay Botten, Rym–LWB1 Bouchendira, FWO2 Adel– Bousseksou, W.–FWE4 Boutu, FTuZ3 Dirk– Bouwmeester, FTuP1 John– Bowers, Bowlan, Pamela–FThD7 Richard–FWM1 Bowman, LThF FTuE5, RobertBoyd, W.–FMM2, Allan S.–LWH5 Bracker, B..–FWD1 D. J. Bradley, J.–FWB7 David Brady, FWW4 Nicoletta– Brauckmann, Jorge–FThH4 Bravo-Abad, P.–FWE4 Breger, B.–FWD4 Breiten, C.–FTuL3 Briles, Travis FWE5 Brimhall, Nicole–FThT3, LWH5 LThA3, D.–FThAA1, Alan Bristow, J.–FMM5 Curtis Broadbent, FWZ Neil– Broderick, Misha– Brodsky, Yaron–FTuK1 Bromberg, L.–FMA3, FThB Mark Brongersma, Chritian–JTuA51 Brosseau, JWA42 Beausoleil, Raymond G.– FThT5, FTuT1 FThT5, G.– Beausoleil, Raymond F.–FThBB6 Michael Becker, FWC3 , FThN2 M.– Amber Beckley, Noah–FML2 Bedard, FTuF7 D.– Brooke Beier, FMB5 W.– Marco Beijersbergen, Béjot, Pierre–FTuX2 Bell, Bryn–FMF5 JTuA13, JTuA10, Georgina– Pérez, Beltrán Belyanin, Alexey–FThG5 Nissim–FWP5 Ben-Yosef, LMB2 Fetah–FTuL2, Benabid, V.–LThB3 Bendkowsky, FMM1 Bennett, J.– A. Bennink, Ryan–FTuG3 S.–SWB4 Neal Bergano, Luc–FTuE6 Bergé, FWF7 FTuF7, J.–FME7, Andrew Berger, I.–JWA59 Bergmair, Berini,LThC1 Pierre– C. G.– FMB2, FMB5 Gregorius Berkhout, FWN6 Nikolai–FWN1, Berkovitch, Berneschi, Simone–FWF5 Bernhardi, E. H.–FWD1 B.–LWK1 Bertrand, Julien FThS2 O.– Vladimir Bessonov, Bethlem, L.–LThH2 Hendrick Chris–FTuU4 Betters, A.–JWA56 Beyer, R.–FThT7 Vikrant Bhakta, FWX2 Rohit– Bhargava, LTuJ1 Mishkatul– Bhattacharya, FWX1 Indrajit– Bhattacharyya, A.–FTuN4 Sunil Bhave, Bipin–FThL2 Bhola, FWD4 Ivan– Biaggio, Yusheng–FThC8 Bian, C.–JWA55 Joshua Bienfang, LTuJ1 P.–LTuH3, Nicholas Bigelow, FTuS7 Temel– Bilici, O.–JTuA22 Olexandr Bilyy, Gino–FTuV4 Biondini, LWB1 François– Biraben, , FWAFTuU1 Tim– Birks, J.–FThQ1 Luke Bissell, October 24–28, 2010 • FThV2, FTuK3 LTuG1 FThZ4, FWP6 Babic, Ljubisa–FThJ6 Babic, K.–LTuG5 Joseph Babu, Arthur–FWO2 Babuty, , LThF1 LThC Antonio–FWQ1, Badolato, Baffa, Carlo–JWA15 V.–FWR1 Bagnoud, B.–FThS4 Thomas Bahder, M.–FWN3 Bahoura, R.–LWH4 Baiz, Carlos R. Karthik FTuI2 C.– Balareddy, Baldini, Francesco–FWF5 M.–FMA1 Baldo, Balewski, J.–LThB3 , FWK FTuW1 John– Ballato, Valeria–LTuA4 Balogh-Nair, T.–LTuD1 Baluktsian, Ilana–FThZ5 Bar, M.–FTuS3 Timothy Baran, , FThBB George–FMI5, Barbastathis, Sergio–FMD3 Barbero, E.–FTuT1 Paul Barclay, R.–FMA2 Aaron Barkhouse, Stephen–LMA4 Barlow, A.–FWN3 Yu. Barnakov, Barnes, M. D.–JTuA58 FTuZ1, M.–FTuG5, Stephen Barnett, F.–JWA27 John Barrera, F.–LThH1 J. Barry, , FWZ1 FMG2 Christopher– Barsi, Bartal, Guy–FThR3 Bartalini, Saverio–LThG6 Alain–FTuD4 Barthélémy, FMN5 J.– P. Christopher Barty, A.– JWA36 Miguel Basurto-Pensado, JTuA32 G.–FWI3, Hussam Batshon, Heinz–JTuA24 Baumann, Jörg–FMI6 Baumgartl, FTuC6 P.– Prashant Baveja, K.–FMB1 Yahya Baykal, FThU3, FThU4, FThU5, Beadie, Guy– LMB4 Beams, Ryan– GeneBeare, K.–FWY2 Grégoire–FWO2 Beaudoin, FiO/LS 2010 An, Sohee–FTuH1 An, Yair–FMG1 Andegeko, J.–FWW2 Arthur Anderson, Harry L.–LMA4 Anderson, E.–FThBB3 Matt Anderson, R.–FWF3 Ryan Anderson, FThQ2 Sean P.– Anderson, JTuA09 A.– FTuR2, Jose Andrade-Lucio, Volker–FML1 Andresen, Trisha–FThT3 Andrew, Andrusyak, Oleksiy–LWG2 L. K.–FThK4 Ricky Ang, A.–FWI4 Jaime Anguita, M.–LWH4 Jessica Anna, LTuB5 Muthiah–JWA34, Annamalai, Aldo–LWB6 Antognini, Cristian–FTuV3 Antonelli, FThY5 Hesam– Arabi, E.–FThB6 Ismail Araci, FWD3 Shanmugam– Aravazhi, FThQ3 Amir– Arbabi, LWB3 L.–JTuA64, James Archibald, Richard–FThA3 Ares, FWM2 FWA4, Argyros, Alexander–FTuW2, FThB8, FThH2 Ady–FThA1, Arie, M.–FThP8, FThQ7 Andrea Armani, LTuF1 Stephen– Arnold, L.–FWJ3, FWV3 David Aronstein, FMD4 Artal, Pablo– JWA11 Alexandra– Artusio-Glimpse, STuC1 Arthur– Ashkin, FMJ1, FWQ6 Murtaza– Askari, Alan–LTHA4 Aspuru-Guzik, W–FThT6 Astar, FThQ6 Hossein– Amir Atabaki, G. W.–FTuA2 Atkinson, Patrick–FWN2 Audebert, T.–FWE4 Auguste, FThZ, FTuE D.– Richard Averitt, Oleg–FWH3 Avremko, Chitralekha S.–JTuA48 Avudainayagam, JTuA48 V.– Kodikullam Avudainayagam, A.–FME7 Hani Awad, Jose–FThI1 Azana, A.–JWA08 Azevedo, Azuri, Ido–LTuB4

, FWP4, JWA48 FWC3 FTuO6, FTuW Agarwal, Girish S.–JTuA44 Agarwal, Girish FTuG4 Agarwal, Shantanu– Aggarwal, Ishwar–FTuW3 K.–FThP Amit Agrawal, JWA53 P.–FTuC6, Govind Agrawal, Ahn, Byeong-Hyeon–FThJ4 Vincent–FThA3 Aimez, FTuC5 Stewart–FThC3, J. Aitchision, D.–FTuB1 J. Akula, Alaa M.–FThG1 Al-Kadry, FThD5, FTuG2 Al-Qasimi, Asma– Z.–FThC3 Muhammad Alam, FThD, FTuX Albert, Olivier– Alden, A.–LThE2 Emily , JTuA43 JTuA38 Adalberto– Alejo-Molina, JTuA23 Georgios– Alexandrakis, JTuA51 Ayman– Alfalou, JTuA19 JTuA04, Robert R.–FWC4, Alfano, J.–FThP6 William Alford, , FWW2, FWW3 FTuU Alic, Nikola–FTuC4, Alexandra–FME3 Alimova, FThQ6 Payam– Alipour, Gábor–FThZ1 Almási, JTuA60 B.– Almeida, Diogo Benjamín–FTuR3 Alonso, A.–FThN2, FThN3, FTuK5, Miguel Alonso, LTuA4 Alrubaiee, Mohammad– Andrea–FWO5 Alù, E.–LTuC4 Medhat Aly, Raghu–FTuF6 Rao, Ramachandra Ambekar J.–FWB2 Jason Amsden, Kyungwon–LWD4 An, AbiSalloum, Tony–LTuJ3 AbiSalloum, A.– FThI6 Abdelsalam Aboketaf, FTuW4 F.– Ayman Abouraddy, SMB1 B.– James Abshire, H.–JWA08 Lúcio Acioli, M.–JTuA53 Victor Acosta, S.–FWV2 D. Acton, Sadao–JWA46 Adachi, C.–FMM4 Jeff Adams, FWQ6 Ali–FMJ1, FThQ6, FWO4, Adibi, FTuL3 Florian– Adler, FThA4, FThO, FTuJ5, Shahraam– Afshar, Key to Authors and Presiders and Authors to Key Authors) Presider or Presenting (Bold denotes Key to Authors 132 Capron, Barbara A.–FMM4 Capasso, Federico–SMB2 Cao, Zhangjie–FThBB6 Cao, Hui–FWT1 Canning, D.–FTuR5 Cankaya, Hüseyin–FThAA2 Cancio Pastor, Pablo–FTuL4, JWA15, Cançado, Luiz Gustavo– LMB4 Canavesi, Cristina–FTuS5 Camposeo, Andrea–FTuW5 Camata, Renato–FThL3 Camacho-Aguil, Rodolfo– FMH1 Camacho, Ryan M.–FThN5 F.–LTuE4Calegari, Caillat, J.–FWE4 Cai, Yuanxue–LThC4 Cai, Yue–FTuJ3 Cai, Yan–FMH1 Cadoret, Malo–LWB1 C. Eldar, Yonina–FTuE2 Byro, Andrew H.–LTuA4 Byer, L.–FTuL1 Robert Igor–Buzalewicz, JWA13 Butscher, B.–LThB3 Butler, John–FME1 Busse, Lynda–FTuW3 Busold, S.–FWR1 Burrow, Guy M.–FWS3 T.–FWR1Burris, Burns, Stephen A.–FTuB2, FTuB5 Burke, Janice M.–FMK2 Burke, Daniel–FTuO2 Burka, Laura–FTuW1 Bünermann, Oliver–LWK3 Budker, Dmitry–JTuA53, JTuA56, LThG2, Bucksbaum, Philip H.–LTuE2 Buckley, Brandon–FThI3 Buckingham, Roger–FWN4 Bückers, C.–JWA56 Buck, Alexander–FMN2, FWL3 Bryant, Doug–FThU2 Brustlein, S.–FTuU3 Brownless, JS.–FThJ3 Brown, Thomas G.–FThC6,FThN2,FWC2, Brown, Roger–STuD3 Brown, Ken–LThB5 Brown, Edward–FTuF4 Brown, P.– Dean JTuA25 LThG6 LWB FWC3, FWP Chen, Wei-Jan–Chen, FWE6 Su–FMG4Chen, Shaowei–FMC5Chen, M.–LTuI1Chen, Ming-Fu–FThP3Chen, Kuang–LThB2Chen, Jinhai–LThG5Chen, I-Ming–JTuA14Chen, HuiChen, W.–FTuP1 Haiqing–JWA22Chen, Chih-Hung–JWA49Chen, Chun–JTuA55Chen, Baosuan–JWA25Chen, Bin–FMC5Chen, Chavez Jose Boggio, M.–FTuC4, FWW3 Chauhan, Vikrant–FThD3, FThD7,FThD8 Chatzandroulis, Stavros– FWF4 Chatterjee, S.–JWA56 Charati, M.–LMA1 Chanthawong, Narin– JTuA52 Chang, Zenghu–FTuX, FWE1LWK2 Chang, S.L.–JWA20 Chang, Shenq-Tsong–FThU7, JTuA01 Chang, Nienan–FTuD1 Chang, Hye Jeong–FMM2 Chan, Sze-Chun–FTuA4 Chan, Kam Wai Clifford– FMM2 Chan, Chia-Yen–FThP3 Chan, Aaron C.W.– FWH4 Chamanzar, Maysamreza– FWO4 Chakravarty, Abhijit–FWI2, JWA39 Deepthi–JWA04Chakilam, Chaker, Mohamed–FThA3 Chaikina, Elena–FTuQ5 Chabanov, Andrey A.–FTuQ,, FWT5 D.–FTuU3Ceus, Cesar, Carlos L.–JTuA60 FME1 Albert– Cerussi, Celanovic, I–LThF2 Caulfield, H.John–FThV1 Mixcóatl,Castillo Juan– JTuA10, JTuA13, D. Bernard Casse, Frederic.– FWO3 Casey, John–LWC2 Carter, M.–FThT6 Gary FWE4 Carre, Bertrand– Carney, P. Scott–FThT,FTuE8 Carmon, Tal–FMA1, FTuN, FTuZ2, FWE2 Cardoso, Marcos R.–JTuA05 Cardenas, Jaime–FThQ5 Carberry, David–FWM1 JWA44 JWA42 FiO/LS 2010 Clayton, C.–FWL2 Clarkson, Jeffrey P.–FMA4 Clark, Charles W.–JWA55 Clark,FMF5 Alex– Pierre–LWB1Cladé, Cizmar, Tomas–FMI6, FTuM4 Cisternas, Jaime E.–FWI4 Cirloganu, Claudiu M.–LTuG3 Chung, Youngjoo–FWK2 Chung, Hoi Sung–LThD1 Chui, T. Y. P..–FTuB1 Chui, P. C.–JTuA30 Chu, Sai T.–FThI1, FThO1,FTuC2 N.–FThA3, Christodoulides, Demetrios Christensen, Marc P.–FThT7 Chou, C.W.–LWB4 Chong, Y.–LThF2 Choi, Wonshik–LWD4 Choi, Jae-Woo–LTuF3 Choi, Honggu–FTuH2 Choi, Hong FThQ7 Seok–FThP8, Choi, E.Y.–JWA54 Choi,FTuS Bernard– Cho, Seongkeun–FTuK5 Cho, Seong-Woo–FThBB2 Chivel, Yuri A.–FWX4,JWA17 Chini, Michael–LWK2 N.–FThB5 Dmitry Chigrin, Chi, Wanli–FTuD1 Chi, San-Hui–FThZ4, LMA4 Cheung, Kim K.Y.–JTuA30 Chettiar, Uday–FThR5 Abdallah–JWA05Cherri, JudyCherian, G.–FThG5 Cheng, Yih-Shyang–JWA49 Cheng, Yuan-Chieh–FThU8, FThX2 Cheng, Kyle H.Y.–FTuY1 Cheng, Jiangtao–FWB5 Cheng, Ji-Xin–FMG4 Zhigang–JWA51Chen, Ziyang–JWA25Chen, Zhen–JTuA55Chen, Zhichao–JTuA33Chen, Zhigang–FThW4,Chen, FTuM3 Yu-Wen–JTuA11Chen, Yifang–FWN4Chen, Yi-Hsien–FThX2Chen, Yung-Hsinag–FThP3Chen, Xiaowei–FWN2Chen, FThL2 Xi– Chen, Xiaowei–FMN1Chen, FWG4 • October 24–28,2010 Dahlquist, William C.–FWF3 Dadap, I.–FThT6 Jerry Cyphersmith, Austin– JTuA58 Cvetojovic, Nick–FTuU4 Cutler, Patrick J.–LWL3 Curtis, Jeremy A.–FThG5 Curran, Arran–FWM1 Cunningham, Paul D.– JTuA61 Cunningham,FWR4 Eric– Cundiff, Steven T.–FThAA1, LThA3, LWH5 Cummins, Zachary–FTuT2 Cui, Liping–FWY3 Cui, Liang–FMF4 Cuennet, Julien R.–LTuF3 Cuccia, David J.–FTuS2 JoseCruz, L.–FTuU1 Crozier, Kenneth B.–LTuI2 Crenshaw, Michael E.–FThS4 Crane, John K.–FMN5 Cozzuol, Matteo–LMA4 Cowan, T.–FWR1 JohannesCourtial, K.–FMB2,FMB5, Couny, Francois–FTuL2, LMB2 Costantini, Daniele–FWO2 KevinCossel, C.–FTuL3 Franco–FWF5Cosi, Kristan L.–LMB2 Corwin, Corson, John P.–FThG4, JWA65 DanielCorrêa, S.–JTuA05 Cornejo, Alejandro R.–JWA61 Corkum, Paul B.–FTuX2, LWK1 Cordingley, James–STuA2 Coppola, Sara–FWF6, FWS6, LTuI3 Coppinger, M.–FMH2 Cooper, Michele T.–JTuA24 Consoli, Antonio–FThD8 Conley, Nick–FTuM1 Conforti, Evandro–JTuA31 Combrié, S.–FTuQ6 Colyer, R.–LThD3 Colombelli, Raffaele–FWO2 Oren–FTuE2,Cohen, FWE2,FWE3 Jacob–Cohen, FThD3, FThD7FThD8 AdamCohen, E.–LWF1 Coffey, David–LMA3 Cloutier, Sylvain G.–FMA,FMH2, Aashish–Clerk, LWA Cleland, Andrew–LWD3 FThT2, FTuD, FTuO4, FTuO5 LTuA3 FThAA3, FTuJ4, FWD2,LMA5, , LWD1 DeSavage, Sara A.–LTuJ2 Dertinger, T.–LThD3 O.–FWR1Deppert, MarkDennis, R.–FTuG5 Shengling–Deng, FWQ4 Demir, Veysi–FThB6 David–DeMille, LThB, LThH1 Demand, G.–FTuQ6 Delprat, Sebastien–FThA3 Delima, Franz W.–FThZ3, JTuA20 Delestrange, Elie–JTuA12 Delage, L.–FTuU3 Rio,Del L.–FTuU3 Carsten–LWI1Deibel, Dégardin, Annick F.–FThP7 Debnath, Ratan–FMA2 Deasy, Kieran–FThAA6 H.–FWJFWJ3,FWV3 Bruce Dean, Wilde,De Yannick–FWO2 de Thomaz, André A.–JTuA60 de Sterke, Martijn–FTuW2, LThC3 de Sterke, C.M.–FThJ2,FThJ3 Eunezio Souza, De A.–JTuA34, LWG5 Sio,De Luciano–LTuF3 Silvestri,De S.–LTuE4 Rossi,De A.–FTuQ6 de Ridder, M.–FWD1 R. Natale,De Paolo–FTuL4, LThG6 de Mirandes, Estefania– LWB1 Israel–LThC1 Leon, De de Heer, Walter–STuB3 GrooteDe Nelson, Jessica– FThP4 de Groot, P.A.J.–FWN4 Michiel J.–de Dood, FThJ6 de Castro, Alberto–FMD3 Leonardo–JTuA46,de Boni, JWA10 de Araujo, Luis–FWZ4 Angelis,De Constantino– FThA3 Dawson, Jay W.–FMN5 Davis, Jon P.–LThE3, LTuJ2, LTuJ3 Davidson, Nir–FMB4, FThN4 Davidovich, Luiz–FMF, FTuT3 Davanco, Marcelo I.–FWQ1 , FWW Dastmalchi, B.–JWA59 Dasari, Ramachandra–LWD4 Dasari, Raghunath–FThZ4 Dantus, Marcos–FMG1, FThD1,LTuB6 Dam, Jeppe S.–FWX5 Negro,Dal Luca–FThB2, FThB3,FThC7, Dainty, Chris–FTuO2, FWP3,JTuA12 Dai, Xingcan–FThAA1, LWH5 FWB2, FWQ2, JWA41 Key to Authors 133 , LWK3 FThB7, FWB6, FWP2 Georges, Patrick–FMN1 Georges, JWA56 FTuY2, C.–FThBB5, Nils Gerhardt, FTuJ4 Gerlein, Felipe–FMH2, Dimitri–FWD3 Geskus, LTuE Oliver– Gessner, B.–JTuA22 Getman, Vasyl Gwang-Hyun–FTuV1 Gho, FWW3 Faezeh–FTuC4, Gholami, Ajay–JWA01 Ghosh, Somnath–JWA53 Ghosh, Elisabetta–JWA15 Giani, J.–FMN5 David Gibson, Graham–FWM1 Gibson, R.– Benjamin FTuS1 Giesselman, FThZ5 Amir– Gilad, Gilbertson,Steve–LWK2 Alex T.–LWJ2 Gill, Shai–FWN1 Ginzach, FWN6 Pavel–FWN1, Ginzburg, C.–FWE4 Giovanetti-Teixeira, Girvin, M.–FTuN1 Steven Giovanni–FTuL4 Giusfredi, FThG4 A.–JWA65, Scott Glasgow, LWG2 Leonid–JWA02, Glebov, L.–FThQ3 Lynford Goddard, LTuC1 Anne– Goj, LWL1 Ido– Golding, Jonathan–FThL3 Goldstein, FTuL5 RaviGollapalli, P.– JTuA18 Gregory– Golovin, S. L.– JWA30 Anderson Gomes, Carmen–JWA29 del Luz Pavón, Gomez A.–FTuB3 Gómez-Vieyra, JTuA12 Alexander– Goncharov, Qihuang–FThY2 Gong, FWQ2 Yiyang– Gong, Yongkang–JTuA17 Gong, RobertGonsalves, A.–FWV1 M.–LMA2, LWL3 Goodwin, Peter R.–FThN6, LTuB6 James Gord, STuC3 P.– James Gordon, H.–LTuJ2 Kyle Gordon, Debabrata–FWX1 Goswami, Paul–FME3 Gottlieb, Goulielmakis, Eleftherios– LTuE1 Alexandre–FMG3 Goy, FMH5, FMH6, FMJ7, Ilya– Goykhman, J.–JTuA58 Graham, Meir–FThR6 Grajower, A.–JWA61 Fermin Granados, Michael–FMA2 Grätzel, FTuK2, JWA24 FTuK2, , LTuG LTuB1 FWU2 JWA44 French, Doug–FThD2 French, FThB1, FThB4, Ari T.–FME4, Friberg, D.–FWL2 Froula, Judith–FTuM1 Frydman, FTuT1 C.– Kai-Mei Fu, Xuelei–FTuA4 Fu, Kyle–FTuO6 Fuerschbach, Hisayoshi–JWA57 Fujikawa, SMA4 Jim– Fujimoto, Toshihiro–FMC6 Fujita, JTuA41 Takehiro– Fukushima, Jérémie–FMF5 Fulconis, Colin J.–LWF3 Fuller, F.–LThA2 Fuller, A.–FThZ1 József Fülöp, A. B.–FTuB1 Fulton, A.–JWA56 Dominic Funke, Akira–LThE1 Furusawa, L.–FThO5, FTuC3 Gaeta, Alexander JWA55 Jemellie– Galang, Galli, Iacopo–FTuL4 Galvin, M.–LMA1 FTuG8 Omar– Gamel, Daniel–LWH5 Gammon, How–JWA33 Choon Gan, FTuH3 Parisa– Yarandi, Gandomkar FMI5 Hanhong– Gao, Liang–FML2 Gao, JTuA57 Victor– Garashchenko, S.– JWA61 Melquiades Garcia, Arturo–FTuR2 Garcia-Perez, JTuA36 Ruchi– Garg, FWZ2, FThH3, J.–FThA5, Daniel Gauthier, Wojciech–JTuA53 Gawlik, K.–FME3, LTuA4 Swapan Gayen, FWS3, FTuH5, K.–FMJ2, Thomas Gaylord, FTuO7 Snir–FTuE2, Gazit, FThR, JWA33 Greg–FMB3, Gbur, JWA06 FTuD3, E.–FThM4, Gehm, Michael Jean-Paul–FWN2 Geindre, M.–FWR1 Geissel, Michael–FWL3 Geissler, AzrielGenack, Z.–FThG7, FWT4, FWT5, A.–FThF4 Dentcho Genov, Deepu K.–FME6, JWA19 George, H.–FTuX3 George, Nicholas–FTuD1 George, , FMG2, , FMG2, October 24–28, 2010 • FWB3, FWF1 FWB3, JTuA46 FWV3, FWV4 FWZ1 Fang, David Z.–FWB3 David Fang, , FWY4 FThU1 Hongbing– Fang, LWD4 Christopher– Fang-Yen, Ali–FThI3 Fard, P.–LTuE2 Joe Farrell, I.–FMM1 Farrer, FWP6 K.– Fredrik Fatemi, S.–FTuC1 Fathpour, David–FThT5 Fattal, FThQ2, M.–FMA4, Philippe Fauchet, Vladimir–FThL3 Fedorov, FWO6 A.–FWN4, Vassili Fedotov, A.–FThJ5, FThS2 Andrey Fedyanin, Michael–LWD4 Feld, D.–JWA12 Marc Feldman, L.–LTuI1 Feng, Andrew–LMA3 Ferguson, R. D.–FTuB1 Ferguson, Maurizio–FWF5 Ferrari, LTuI3 FWS6, Pietro–FWF6, Ferraro, JWA16, D.– Henrique Paulo Ferreira, FThO1 Marcello–FThI1, Ferrera, R.–FThK2, FWJ2, FWJ3, James Fienup, FWA2 F.– Donald Figer, Salvatore–LWI1 Filippone, Marco–FThT5 Fiorentino, FMB4, FThN4 Ofer– Firstenberg, Armin–FMA2 Fischer, G.–FThN1 Dave Fischer, C.–FThG2, FTuF2 Martin Fischer, Fleet, E.–FThU5 FWE3 Avner–FWE2, Fleischer, FME5, FMG W.– Jason Fleischer, R.–FThZ4, JTuA40 Steven Flom, Catalin–FTuW3 Florea, FTuN1 Nathan– Flowers-Jacobs, FTuL3 Aleksandra– Foltynowicz, A.–JWA58 Forbes, FThX6 W.– Greg Forbes, A.–FTuC3 Mark Foster, FTuS5 , FTuS3, H.–FTuS1 Thomas Foster, T.–FTuT2 John Fourkas, Florian–FTuS5 Fournier, Paul–FTuW1 Foy, LTuG1 FTuG5, Sonja– Franke-Arnold, FTuG6 James– Franson, F.–LTuE4 Frassetto, Mary–LMB3 Frawley, FiO/LS 2010 , LWB3 , FWU3, JWA14, JWA57 , FWU3, JWA14, FWO5 JWA58 Angela– Dudley, Dwight Duncan, L.–LTuJ2 FThE4 Mike– Dunne, LThG3 Mathieu– Durand, LTuJDurfee, Dallin S.–JTuA64, F.–FME1 Durkin,Amanda J.–FTuS2 Durkin,Anthony R.–LWC3 James Durrant, Dwight–FThU2 Duston, Vladimir–LWI1 Dyakonov, Dmitry V.–FME5 Dylov, , LWL A.–LThD1 William Eaton, Brian–FWO5 Edwards, Eells, Rebecca–JTuA39 Nikolaos–FThW4 Efremidis, Ali Asghar–FThQ6 Eftekhar, Christian–FML4 Eggeling, Alexander–FML3 Egner, Asaf–LTuB4 Eilam, Ramy–FWG4 El-Ganainy, M.–FWU4 Eldaiki, Omar C.–FTuO7 Yonina Eldar, Elgin, John–JTuA66 Eric–FMM6Eliel, FThH2 Ellenbogen, Tal–FThB8, Amicia D.–FML2 Elliott, Ellis, Simon–FTuU4 Ali W.–FThI6 Elshaari, E.–FME2, FMK3 Ann Elsner, J.–LThD3 Enderlein, FThF2, FThG, FThR5, Engheta, Nader– JTuA13 Reyes, Viterbo– Epitacio LWB3 JTuA64, Christopher– Erickson, LTuF David– Erickson, Okan–LWI3 Esenturk, FWI1 René-Jean– Essiambre, JTuA09 Julian– Estudillo-Ayala, Le Coarer–FTuU2 Etienne, Tijmen–FMM6 Euser, FThV5 W.– Jonathan Evans, Philip–FTuG3 Evans, , LTuI1 FWS1 Y.– Shaya Fainman, FThR4 Yeshaiahu–FMH4, Fainman, P.–FTuT7 Fallahi, Carsten–FWW4 Fallnich, Afrooz–JTuA53 Family, Li–FThI2, FThQ4 Fan, FThW1 Shanhui– Fan, LTuF4 , FTuI3, FTuI2 Xudong– Fan, FWT2 , FWB6, FWP2 , FWB6, FThB7 Deutsch, Miriam–FWN5 Deutsch, Nicholas–FTuO2 Devaney, Devi, Yamuna–JTuA50 Deych, Lev–FTuN3 FMI6, FTuM4 Dholakia, Kishan– FMM3 Giovanni– Di Giuseppe, FMM7 Henrique– Pires, Di Lorenzo Dias, Camila C.–LWG5 Luis–FTuB3 Díaz-Santana, STuA1 Scott– Diddams, Diederich, F.–FWD4 , FWE FTuX1 Jean-Claude– Diels, Diez, Antonio–FTuU1 A.–FML5 Charles DiMarzio, Panagiotis–FWF4 Dimitrakis, V.–FTuD3 Dineshbabu Dinakarababu, Huafeng–FThK1 Ding, Z.–FWE4 Diveki, I. B.–FTuC4 Divliansky, Mohit–FThT3 Diwekar, Lisa–JWA03 Dixon, Ben–FThD4, FTuE4 P. Dixon, FWI3, JTuA32 B.– Ivan Djordjevic, FThA1, FThB8, FThH2 Ido– Dolev, Dolgaleva, Ksenia–FTuC5 V.–FThS2 Tatyana Dolgova, L.– FThH4 Jorge Dominguez-Juarez, William–FWK5 Donaldson, Lin–JWA24 Dong, Chaitanya–FMJ6 Dongre, T.–LWA5 Donner, Christophe–FThD2 Dorrer, Carlos–FMD3 Dorronsoro, FThJ3 B.–FThJ2, Kokou Dossou, Yiling–FMI3 Dou, Douglas, Nick–FTuM1 Douillet, Denis–FWN2 P.–FThF3 Vladimir Drachev, FTuT4, FTuQ2, Felix–FThJ1, Dreisow, FMM5 Justin– Dressel, Adam–FTuI4 Drewery, FThT6 B.– Driscoll, Jeffrey LWJ3 D.– Peter Drummond, Frédéric–FMN1 Druon, , FTuL5 FMC2 Lingze– Duan, Alfredo–FTuB3 Dubra, David–FThA3 Duchesne, D.–FThO1 Duchesne, O.–LWA4 Dudin, Yaroslav Desiatov, Boris–FMH5, , FMJ7, FMH6 Desiatov, Key to Authors 134 Hald, Jan–LTuD4 Hakuta, Kohzo–FTuT5 Hajialamdari, Mojtaba–FThG1 Haggerty, P.–FMK3 Bryan Hagen, Nathan–FML2 Hagan, David J.–FThO2 , LTuG3 Haessler, S.–FWE4 Haefner, Constantin–FMN5 Haefner, Andrew A.–FThP4 Hadden, Jp–LWE4 Ha, Woosung–FThA6,FTuH4 Ha, Sangwoo–LThC3 Gwanmesia, Gabriel–FThZ3 Gupta, Banshi D.–JTuA35, JWA31 Guo, Yan–FWN5 Guo, Wenjiang–JTuA14 Guo, Junpeng–FWB7, JTuA02 Guo, Huanqing–JTuA12 Guo, Chunlei–FThS3, LTuE5 Gunn-Moore, Frank–FMI6 Gundu, Krishna Mohan– JTuA28 Gündoğan, Mustafa–FThAA2 Gultepe, Evin–FWO3 Gulsoy, Murat–FTuS7 Guillermain, Elisa–FWF1 Guellati, Saïda–LWB1 Guehr, Markus–LTuE2 Gu, Zongquan–JWA40 Gu, Yalong–JWA33 Gu, Ying–FThY2 Gu, Yalong–FMB3 Gu, Xun–FMN2 Gu, Min–FWU1 Gu, Lei–FWN3 Gu, Claire–FMC5 Grüner-Nielsen, Lars–FTuH, FWK1 Grujic, Thomas–FTuW2 Grote, RichardFThY3 R.– Grote, D. P.–FWR1 Groß, Petra–FWW4 Grivas, Christos–FWD3 Simonetta–FWF6,Grilli, FWS6, LTuI3 W.Griffith, Clark–LTuD2 Grier, David G.–JWA03, STuC4 Grice, Warren–FTuG3 Grguras, I.–LTuE1 Greiner, Mark T.–FMA2 Greenhalgh, Catherine– FThU6 Greenberg, Joel A.–FWZ2,LTuB1 Green, William M.J.–FThT6 Green, Dan–STuB4 Herrmann, Daniel–FMN2, FWL3 Herrick, Nick–FWE5 Herndon, Scott C.–SMB3 Hernandez, Gessler–LWA3 Hernandez, Daniel–FTuM3 Herath, Sumudu–FTuQ5 Henry, Paul–FMC3 Henry, B.–LTuJ3 Hendrickson, Scott M.–FMF3 Henderson, Barbara H.–JTuA24 Henao, Rodrigo–JWA27 Hemmer, Philip–FThI4 Hell, Stefan W.–FML3, FML4 Heinrich, Matthias–FThJ1, FTuQ2, FTuT4, Heilweil, J.–LWI3 Edwin Heilmann, Nathan–FWE5 Heilemann, M.–LThD3 Heck, Martijn–FTuP1 Hebling, János– FThS, FThZ1 He, Qiongyi–LWJ3 He,FMJ4, FWB4 Lina– Haynes, Roger–FTuU4 Hayden, L.Michael–JTuA61 Hayat, FWN1 Alex–FThO3, Hawkins, Thomas–FTuW1 Hawkins, Aaron R.–LTuD3 Haus, Joseph W.–FThG8 Hassan, M.T.–LTuE1 Hashemi Rafsanjani, Mohammad– Seyed Hartog, Arthur–FMC4 Harrison, Jp–LWE4 Harris, Jack G.E.–FTuN1, FTuZ, LWD, Harres, K.–FWR1 Harlow, J. W.–LWA5 Harada, Takuya–JTuA59 Hao, Zhengwei–FThY4 Hansen, Azure–LTuJ1 Hanneke, David–LWJ4 Han, Xiaoxing–FTuF4 Han, P.–FMK2 Dennis Hampton, Meredith J.–FThY1 Hammer, Daniel X.–FTuB1 Hamilton, C.–FThT2, Alasdair FTuO4, Hamam, R.–LThF2 Hall, David C.–JTuA65 Hales, Joel M.–LMA4 Halder, Matthäus M.–FMF5 Halder, M–LWE4 WT2 FTuG1 LWD2 FTuO5 FiO/LS 2010 Huson, R.–LThB2 Eric Hume, D. B.–LWB4 Humble, Travis–FTuG3 Hughes, Stephen–FTuQ6 Hudson,LTuH Eric– Huber, B.–LTuD1 Huang, Z.Rena–FWQ4 Huang, Yongjian–FWO3 Huang, Yingyan–FMJ5, FThC2,FThL2, Huang, Ting-Ming–FThP3, FThU7, Huang, Simon–FTuM3 Huang, Po-Hsuan– FThP3, JTuA01 Huang, Da–FWG2 Huang, Chong– JWA22 Hua, Limin–JWA25 Hu, Yi–FThW4, FTuM3, JWA51 Hu, Weisheng–FWF3 Hu, Chengyong–FMF6 Hsu, Wei-Feng–JTuA11 Hsu, Wei-Yao–FThU8, FThX2 Hsu, Paul S.–FThN6 Hsu, Hung Wen–JWA20 Hsiang, Thomas–FWK5 Hsiang, David–FME1 Howell, John C.–FThN5,FMM5,FThD4, Hou, Zhenyu–FThC2 Hossain, Nadir–FWD6 Hossain, Md M.–FWU1 Hosaka, Tomohiro–JWA46 Horton, Anthony–FTuU4 Höppener, Christiane–FTuF5 Honghuan, Lin–FThP5 Hong, Tae Y.–JWA54 Hong, Hyun-Gue–LWD4 Holler, Stephen–LTuF1 Hofmann, Martin FTuY2, R.–FThBB5, Hofling, Sven–FMF6 Hoffmeister, G.–FWR1 Hoekstra, Hugo J. W.M..–FMJ6 Hobbs, Tomothy–FMK3 Hobbs, Douglas–FTuW3 Ho, Y- L.–LWE4 Ho, Seng-Tiong–FMJ5, ThC2,FThL2, Ho, Cheng-Fang–FThU7 Hnatush, Svitlana O.–JTuA22 Hirao, Tadaetsu–FMC6 Hingerl, K.–JWA59 Hilton, David–FThG5 FThQ8, FTuA5, FTuP2, FTuP3 FTuE4 JWA56 FThQ8, FTuA5, FTuP2, FTuP3 • October 24–28,2010 JTuA01 Jimenez-Martinez, Ricardo–LTuD2 Jiménez-Alfaro, Ignacio–FMD3 Jiao, Shuliang–FMK2 Jianjun, Wang–FThP5 Jiang, Yan–FTuM1 Jiang, P–LWE4 Jiang, Jun–LThA1 Jian, Shuisheng–JTuA32 Jia, Shu–FWZ1 Jia, Baohua–FWU1 JI, LIMIN–FWK5 Jespersen, Kim G.–FWK1 Jeong, Yunseop–FTuH2 Jeong, Yoonseob–FThA6 Jeon, Heonsu–FWD5, FWT3 Jenkins, Stewart–LWA4 Jen, K.–JTuA61 Alex Jayich, Andrew M.–LWD2 Jaques, James– FTuP4, FWD Jang, Won K.–JWA50 James, Daniel F. V..–FThD5, FTuG2 Jalali, Munib P.–FThP6 Jalali, FTuC1 Bahram–FThI3, , FWQ Jain, Siddharth–FTuP1 Jain, Apurva–LWG2 Jagtap, Vishal S.–FThAA8,FThP7 Jaedicke, Volker– FTuY2 Jacob, Zubin–FWG3 Jack, Barry–FTuG5, LTuG1 Iyer, Srinivasan–FME4, FThB1FThB4 Iyer, G.–LThD3 Ishaaya, Amiel A.–FThZ5,LWG1, LWG3 Isenhower, Larry–LWJ2 Irudayaraj, Joseph–FWF2 Iqbal, Jamil–JWA32 Ip, Jason–FWX2 Inguscio, Massimo–JWA15 Inada, Koji–FMC6 Imamoglu, A.–FTuT7 Im, Seongil–FThY5 Im, Jooeun–FWK2 Iizuka, Hideo– JWA57 Iftimia, Nicusor–FTuB1 Ibrahim, Hany L.–LTuA5 Baldemar–FThG8Ibarra-Escamilla, Iaquaniello, Grégory–FWN2 Hwang, Taek Yong–FThS3 Hwang, Inchan–LWC2 Hutsel, MichaelFTuH5 R.– JWA24 Ke, Jun–FThBB4 Kaya, Ilhan–FThX1 Kawata, Satoshi–FMC6, FWF8 Kawashima, Hayato–FThW5 Kaufman, Joshua–FTuW4 Katz,FTuE3 Ori– , FTuK1 Katz, Alvin– FME3 Kasseck, Christoph–FTuY2 Kassab, Luciana P.–JWA30 R. Kas, O.–LMA1 Karthik, Balareddy C.Reddy.–LTuF4 Kartashov, Yaroslav V.–FWT2 Karavitis, Michael–SMA1 Karaulanov, Todor–JTuA56 Karaiskaj,FThAA1, LWH5 Denis– Karadag, Yasin–FThAA2 Kaplan, Alexander E.–FWZ6 Kapale, Kishor T.–JTuA44 Kannari, Fumihiko–JTuA59, JTuA63 Kang, Young Mo–FThQ3 Kang, Sehun–FMB6 Kang, Jin U.–JWA09 Kang, Ju-Hyung–FThJ4 Kang, Inuk–FTuP, FTuV Kang, Boyoung–JWA54 Kandyla, Maria–FWF4 Kanaev, Andrey V.–FWX Kalinski, Matt K.–LWK4 Kalb, A.–FTuR5 Kalaycioglu, Hamit–FTuS7 Kalasuwan, P–LWE4 Kakauridze, George–FThV4 Kaindl, A.–FThS,FThZ2FTuE Robert Kahn, Joseph–FTuV1 Kabir, Md. Masudul– JTuA63 Jurling, S.–FWJ2,FWV4 Alden Jung, Yongmin–FTuH1 Jung, Hojoong–FTuH1 Jullien, Aurelie–FMN1 Juárez-Velez, Esteban–JWA07 Jovanovic, Nemanja–FTuU4 Jovanovic, Igor–FMN, FThD2FTuR Joshi, Chan–FWL2, FWR Joseph, Joby–FThW6 Jordan, Andrew N.–FMM5,FThD4,FTuE4 Jones, Marcus–LTuA2 Johnston, Keith P.–JWA12 Johnson, G.–FThX5,FWS5 Eric Johansen, Jacob–FWR4 Joannopoulos, J.d.–LThF2 Jin, Shirong R.–FWD6 Key to Authors 135 FTuN2 Li, Jia–FThY2 FThU2 Li, Liwei– Li, Linjie–FTuT2 Li, Ming–FThC4 Li, Mingzhong–FTuR4 Li, Pengxiong–JTuA54 Li, Qin–JTuA30 Li, Rui–FWQ2 Li, Tongcang– SWA1 Li, Tingye– Li, Wei–FWB5 FMF4 Li, Xiaoying– Li, Xianglin–FThBB4 Li, Xiangyu–FThC2 Li, Xiang–FThK4 Xiangyu–Li, FThQ8 Xiaohui–JTuA17 Li, Xiankai–JWA12 Li, LWI LWC1, Tianquan– Lian, Di–FTuP1 Liang, FMF3 Junlin– Liang, FThBB6 Jinyang– Liang, , FTuB FThU (Ron)– Rongguang Liang, S.–LWL3 Diane Lidke, JWA56 Sven–FWD6, Liebich, Seng-Fett–FWT1 Liew, Efrat–LTuC2 Lifshitz, FThX7 Brandon– Light, A.–FWV2 Paul Lightsey, Patrick–JWA36 LiKamWa, Lim, Jinkang–LMB2 M..– LWF3 B. Charles Limouse, Lin, Chien-I–FWU2 , JWA20 I En–JTuA27 Lin, Samuel Lin, Wei-Cheng–FThU7 FWGLinden, Stefan– RobertLindquist, G.–FWB7 FThH1, FThQ5, FTuC3 Michal– Lipson, M.– JTuA03 Natalia Litchinister, FWG5 M.– Natalia Litchinitser, E.–FThI1 Brent Little, E.–FThO1, FTuC2 Brent Little, FTuP3 FTuP2, FTuA5, Boyang–FMJ5, Liu, Binbing–JWA22 Liu, FWO7 Huikan– Liu, Hanli–JTuA23 Liu, FMH, FMH1 Jifeng– Liu, FMN3 Jun– Liu, Jing–FTuI2 Liu, Jun–LTuG4 Liu, FThC4, LTuA6 Liying– Liu, Tan–FMK2 Liu, , FWM2 FWP5 FWB6, FWN6, FWO FThR6, FTuO3, FWP2, FWP5 Lee, Hyun-Hee–JWA54 Lee, Ian–FThP6 FWT3 Lee, Jeongkug–FWD5, LThG5 Lee, Jeongwon– Lee, Jai-Hyung–LWD4 STuA2 Lee, Joohan– , FTuE7 FMI1 Lee, Kye-Sung– FWF2 Lee, Kyuwan– Lee, Moonjoo–LWD4 Lee, Seung-Yeol–FThBB2 Ho–FThZ4 Lee, Sang Lee, Sejin–FTuH4 Rae– Lee,FWM3 Sung FWB2 Y.– Lee, Sylvanus Lee, Wonju–JTuA07 Lee, Wonsuk–LTuF4 Lee, Yong-Hee–FThJ4 U.–JWA54 Lee, Y. FThE, FWL1 Wim– Leemans, FTuX2 François–FThA3, Légaré, LWA5Lehnert, K. W.– Lei, Zen-Yuan–JWA49 Stephen–FThX5 Leibholz, FThC5 P.– Jordan Leidner, C.–FTuL1 Nick Leindecker, N..–JWA30 B. Lemos, Thiago Sergio–FTuU4 Leon-Saval, , FWA4 Sergio G.– FTuU1, Leon-Saval, LWK3 R.–LTuE1, Stephen Leone, Hai-Sheng–FWB7 Leong, , FWN6, FWP2, Lerman, Gilad M.–FTuO3 L. S.–LTuJ1 Leslie, LTuB2 Gerd– Leuchs, STuD4 Benjamin– Lev, Levina, Larissa–FMA2, FThO2 M.–FTuE3 Jonathan Levitt, FMH6, FMJ7, FThB7, Uriel–FMH5, Levy, Lewis, L. M..–LThA2 K. Li, Baolei–FTuF2 FThG6 Li, Chun-Fang– Li, D.–LWA5 FTuV2 , FTuJ Li, Guifang– FWY4 FTuI, Li, Guoqiang–FThU1, FTuI3 Li, Hao–FTuI2, Li, Hebin–LThA3 FThD6 Li, Jia-Han– FThF1, FThN Li, Jensen– FThR2, FThT5 Li, Jingjing– October 24–28, 2010 • FWH2, FWH4 Kues, Michael–FWW4 Kues, Boris T.–FTuW2 Kuhlmey, Kobus–LThC3 Kuipers, FWF8 Yasuaki– Kumamoto, JTuA47 Ajit– Kumar, FWX1 Pardeep– Kumar, Prem–LTuB5 Kumar, Rakesh–FTuT2 Kumar, JWA56 Bernardette–FWD6, Kunert, Fred–FTuW3 Kung, JTuA45 S.– Paulina Kuo, Geza–FTuP1 Kurczveil, Adnan–FTuS7 Kurt, Alex–LWA4 Kuzmich, FThK5 LaCasse, F.– Charles JWA08 Lacerda, Douglas P.– L. Jeffrey–FTuI4 LaCroix, , LWE2 LThE Laflamme, Raymond– FTuE1 Lahiri, Mayukh–FThD5, W.–FThBB5 Lai, Yiu Laing, A.–LWE4 D.–LMA3 Laird, LTuG5 Lakshmi, Parameswar– Vasudevan–JTuA49 Lakshminarayanan, FTuY1, , FThBB4, FTuD2 Y.– Lam, Edmund C.– FThP1 John Lambropoulos, LWI3 Paul– Lane, Zachary–FTuF5 Lapin, Lara, David–FWP3 C. J.–FWM2 Maryanne Large, FTuC3 K. W.– Ryan Lau, Roberto J.–FTuE8 Lavarello, FMB5 J.–FMB2, P. Martin Lavery, Laure–FWW1 Lavoute, LThG3 Lawall, John–JTuA45, J.–FThJ3 Felix Lawrence, FTuU4 Jon– Lawrence, FThC7 Nate–FThB2, Lawrence, T–LWE4 Lawson, LTuG1 Leach, Jonathan–FTuG5, FWB1 J.– Martin Leahy, LThG5 LThG, E.–LThE2, Aaron Leanhardt, FTuA3 Michael– Lebby, , FTuR1 FMN Catherine– LeBlanc, M.– FThP2 Ledingham, Patrick LThD Lee, Andrea– FThBB2 Lee, Byoungho– FTuP3 FTuP2, Lee, CheeWei–FTuA5, Lee, Chao-Kuei–FWE6 Lee, Dongjoo–FThD3 FiO/LS 2010 , SWA SMB3 E.– Charles Kolb, A.–LTuD1 Kölle, J.–FMH2 Kolodzey, Takashi–FThA2 Kondo, Rong–FWX2 Kong, Junichiro–FThG5 Kono, T.–JWA58 Konrad, Gerasimos– FMA2 Konstantatos, P.–FTuC1 Koonath, LWI4 Nikos–LMA3, Kopidakis, Oleg–LWK3 Kornilov, Olga–JWA18 Korotkova, S. K.–FTuA2 Korotky, FWC R. John– Koshel, JWA52 JTuA43, Carlo– Kosik-Williams, Tsampikos–FWG4 Kottos, , JWA56 FThBB5 Nektarios– Koukourakis, J.–FML5 Gregory Kowalski, FWE2, FWE3 Maxim– Kozlov, FMA2 Illan– Kramer, F.–LThC3 Thomas Krauss, FWL3 Ferenc–FMN2, Krausz, F.–LTuE1 Krausz, J.–FThP7 Alain Kreisler, Christian–FThB5 Kremers, LTuH1 Roman– Krems, Alexandr–FThB6 Kropachev, LWH4 J.– Kevin Kubarych, H.–LTuD1 Kübler, David–FThD5 Kuebel, Kippelen, Bernard–FTuA1 Kippelen, LWD5 J.– Tobias Kippenberg, Alper–FThAA2 Kiraz, G.–FThI5 Andrew Kirk, John–LTuD2 Kitching, S.–LThC3 Yuri Kivshar, FTuD5 Iftach– Klapp, E.-B.–JWA59 Kley, Kling, M. F.–LTuE1 Geoffroy–FThP7 Klisnick, Kevin–LMB2 Knabe, Svenja–LTuD2 Knappe, C.–FWW1 Jonathan Knight, FWV2 S.– J. Knight, RandallKnize, J.–FTuJ2 Kathryn E.–LTuA1 Knowles, Wayne–FWY3 Knox, FMN3, LTuG4 Takayoshi– Kobayashi, Jens–FTuH4 Kobelke, S. W.–JWA56 Koch, SWB1 T.– Koch, Herwig– SMB Kogelnik, , FWT2 FTuT4 Robert–FThJ1,FTuQ2, Keil, Jerry–FME3 Keith, LWC4 M.– Anne Kelley, M.–FML5 Jason Kellicker, M.–FTuS2 Kristen Kelly, Brian–LWA4 Kennedy, FTuU2 Pierre– Kern, Daniel–FMK1 Kerschensteiner, FMN6 J.– Terrance Kessler, Robert T.–FML2 Kester, Ken–JTuA24 Keymel, FWE3 Ofer–FWE2, Kfir, FWZ5 Khadka, Utsab– Mercedeh–FMH4 Khajavikhan, , LTuC4 Esam M.– LTuA5 Khaled, Elsayed Bilal–JTuA23 Khan, Sabih–LWK2 Khan, FWO1 Alexander– Khanikaev, Efim–LWG4 Khazanov, Simon–FTuN2 Kheifets, FThI5 Amin– Khorshidahmad, Jean-Claude–FTuX2 Kieffer, Le–FTuT5 Fam Kien, K.–LMA1 Kiick, R.– Gregory , JWA35 FME, FThQ Kilby, FThF3 V.– Alexander Kildishev, FThV4 Barbara– Kilosanidze, FTuA2 Dan– Kilper, BongKyun–FWK2 Kim, Donghyun–JTuA07 Kim, E. S.–JWA54 Kim, LThF3 ErikKim, D.– Hwi–FThBB2 Kim, Seob–JWA50 Ho Kim, Hyochul–LThF3 Kim, FWG3 Ji-young– Kim, Jongki–FWM3 Kim, Ki–FWM3 Jun Kim, J.–JWA54 Kim, H.–JWA54 Jae Kim, JTuA07 Kyujung– Kim, May–FThI4 Kim, Myung-Ki–FThJ4 Kim, S.–FMF5 Myungshik Kim, Seyoon–FThBB2Kim, FWD5 Sunghwan– Kim, Seunghyun–FWF3 Kim, Sunghwan–FWT3 Kim, Woohong–FTuW3 Kim, FWB4 Woosung– Kim, Lionel–FMH1 Kimerling, T.–LWH4 John King, Key to Authors 136 Lyon, Richard–FWA3 Lyon,JTuA64 Mary– , LWB3 Luukkonen,FWU3 Olli– Serge–JTuA33Luryi, Luo, Yuan–FMJ Luo, Lian-Wee–FThQ5 Lunt, Evan J.–LTuD3 Lumeau, Julien–JWA02 Lukishova, Svetlana G.–FThQ1 Lukin, Mikhail–LWA1 Ludewig, Peter–FWD6 Lu, Z.H.–FThC1 Lu, Zhaolin–FThW, FWS Lu, Zheng-Hong–FMA2 Lu, Wentao T.–FWO3 Lu, Mingwu–STuD4 Lu, D. Y.–FWT5 Lozovoy, Vadim V.–FThD1, LTuB6 Löw, R.–LThB3, LTuD1 Low, Michelle–JTuA21 Lovozoy, Vadim V.–FMG1 Lovergine, Nico–JWA40 Louradour, Frédéric–FTuD4 A.–LTHA4Lott, Geoffrey Lopez-Martens, FMN1,FWN2 Rodrigo– Lopéz-Hernández, Francisco J.– FThD8 Rene–FThY1 Lopez, Longhi, Stefano–FThJ1 Longdell, Jevon J.–FThP2 London, Paz–FMB4, FThN4 Londero, Pablo–FThO5 Lombardo, Krista–JWA48 Z-H.–LTuE1Loh, Logean, Eric–FThT2 Logan, G.–FWR1 Loftus, Tom–LThG4 Loeffler, Wolfgang–FMM6 Locatelli, Andrea–FThA3 Lobino, M–LWE4 Lo, Shun Shang–LTuC2 Llorente, Lourdes–FMD3 Llora, Xavier–FWX2 Livenere, J. E.–FWN3 Liu, Zhaowei–FThW3 Liu, Zhan-Yu–FThD6 Liu, Yen-Liang–FThU8 Liu, Ya–FThC8 Liu, Xueming–JTuA17 Liu, Xue–FWX3 Liu, Xiang–FWI Liu, Xiaoping–FThT6 , FWU4,JTuA08 Martyshkin, Dmitri–FThL3 Martucci, Michael G.–FThX3 Martorell, Jordi–FThA, FThH4 Martinez-Hipatl, Carlos– JWA42 Martin, Ph.–FTuX3 Martín, Nazario–LWI1 Martí Panameño, A.–JWA29 Erwin Marsh, K.–FWL2 Marseglia, L–LWE4 Marom, Dan–FThY Markushin, Yuri–JTuA20 Markelz, Andrea–FME6, JWA19 Mariano, Adrian V.–FThM4 Marder, LMA4 R.–FThZ4, Seth Marcus, Andrew–LTHA4 Marcos, Susana–FMD3 Marciante, John FWK3 R.–FThC5, Marcano, Aristides–FThZ3,JTuA20 Marandi, Alireza–FTuL1 Maquet, A.–FWE4 Mao, Dong–JTuA17 Manthena, Rajakumar–FThT3 Mandina, Michael P.–FThP4, FThX4 Mandal, Sudeep–LTuF2, LTuI Mandal,JWA01 Rahul– Malvache, Arnaud–FWN2 Malvache, A.–FTuX3 Maksov, A.–JTuA58 Maksimchuk, Anatoly–FWR2 Makarova, Maria–FWQ2 Majumdar, Arka–LThF3 Maikisch, Jonathan S.–FMJ2 Mahmoodian, Sahand–FThJ2, FThJ3 Maher, JasonFME7 R.– Magnes, Jenny–JTuA39 Magaña-Loaiza, Omar S.–JTuA43, JWA52 Magalhães, Eduardo C.–JTuA31 Mafi, Arash–FTuH3, JTuA28 Madsen,FThI, FTuP5 Christi– MacGowan, Brian–FThE1 MacFarlane, Duncan L.–JTuA23, JWA04 Mabuchi, Hideo–LWF3 Ma, FWD2,LMA5 Xin–FThAA3, Ma, Ren-Min–FThR3 Ma, L.–JWA12 Li Ma, Lijun–FMF2 Ma, Jing–FWQ3 Ma, Ding– FTuJ3 Ma, Changbao–FThW3 Lyons, Brendon–LWH3 Lyong, Choi–FWK2 FiO/LS 2010 Metcalf, Harold–JTuA66, STuD2 Messerly, Michael J.–FMN5, FTuL Meschede, Dieter–LWE3 Menon, Rajesh–FThT3 Menon, Latika–FWO3 Mendoza-Yero, Omel–FTuR3 Mendoza Gregorio– González, JWA29 Mendoza, H.–FMA1 Mendonça, JTuA05, R.– Cleber JTuA46, Mendlovic, David–FTuD5 Oscar–Méndez JTuA10 Zepeda, Méndez, Cruz–FTuR3 Ménard, Michaël–FTuC3 Memarzadeh, Babak–FThY4 Melinger, Joseph S.–LWI3 Melikechi, Noureddine– FThZ3,JTuA20 Mehta, Rita S.–FME1 Mehrotra, Karan–FThP1 Mehlenbacher, Randy D.– LWH3 Meemon, Panomsak– FTuY3 Medellin, David–FTuN2 Measor, Philip–LTuD3 McPhedran, Ross C.–FThJ2 McMillen, Colin–FTuW1 McManus, J. B.–SMB3 R.–FWS4,McLeod, Robert JWA38 McKinstrie, J.–FMF1, Colin FWW2,SWB McGuinness, Hayden J.– FMF1 McGill, Stephan–FThG5 McFarland, Brian K.–LTuE2 McCanne, Robert–LWH4 McCamant, David–LThA, LWH3 McCamant, D.–LMA1 McArthur, A.–LTuA1 Eric Mazzotti, Davide–FTuL4 Mazilu, Michael–FMI6, FTuM4 Maywar, Drew N.–FTuC6 Mayerich, David–FWX2 May-Arrioja, Daniel–JTuA09, JWA36, Mauger, Sarah–FTuE6 Matthews, Thomas E.–FTuF3 Matthews, Jcf–LWE4 Matsushita, Tomonori– FThA2 Matsumoto, Hirokazu– JTuA52 Matsuishi, Keiichiro–JTuA59 Matichak, Jon–LMA4 Maston, Michael J.–FThX5 Maslowski, Piotr–FTuL3 Marzo, Fabio–JWA40 Marzec, Zachary–FTuV4 JWA10, JWA16 JTuA38 • October 24–28,2010 Moro, Slaven–FTuC4, FWW2 Morandotti,FThA3, FThI1, Roberto– Moore, Nicole J.–FThN3, FWM Moore, Jon D.–FThG5 Moore, D.– Eric FWS4, JWA38 Shayan–FTuC4,Mookherjea, FWT Moody, Galan–LThA3, LWH5 Montenegro, Victor A.–JWA45 Monroe, Christopher–STuB2 Monro, Tanya M.–FThA4 Mondloch, Erin–FTuL2 Momeni, Babak–FWQ6 Mollenauer, L.–SWB2 Moldovan-Doyen, Ioana– FWO2 Mokhov,LWG2 Sergiy– Mojahedi, Mohammad– FThC3 Mohan, Sarasa–JTuA50 Mohan, Ankit–FTuB4 Moerner, W.E.–FTuM1 Moerk, Jesper–LThC2 Modotto, Daniele–FThA3 Mizrahi, A.–FWS1 Miyazaki, Hideki T.–FTuT5 Miyamura, Norihide–JWA63 Mitra, Soumya–FTuS1 Mitra, Arnab–JTuA42 Misoguti, Lino–JTuA46, JWA16 Mishra, K.–JTuA47 Akhilesh Mirov,FThL3 Sergey– Mirin, Richard P.–FThAA1 Miranda- Medina, M.L.–JWA59 Minot, Christophe–FThAA8 Mingzhong,FThP5 Li– Mingzhe, Wang–FThP5 Mínguez-Vega, Gladys– FTuR3 Ming Yong, Han–JTuA21 Milner, Thomas E.–JWA12 Miller, Eric–FTuM1 Miller, David–FThT1 Miller, Benjamin L.–FWF1 Miller, Alexandra–FThW4 Milione, Giovanni–FWC4, JTuA04 Miles, Mervyn–FWM1 Fritz–FTuW3Miklos, Mikhailova, Julia–FMN2, FWL3 Mikhailov, Eugeniy E.–FThA7 Middleton, T.–LWH1 Chris Michelson, Peter F.–STuB1 Michel, Jurgen–FMH1 Miccoli, Ilio–JWA40 Meyerhofer, David–FThE2 FThO1, FTuC2 Newman, Jason A.–FThK3 Nevet, Amir–FThO3, FWN1 Neumark, Daniel M.–LWK3 Neukirch, Amanda–LTuH3 Ness, Stanley J.–FWF3 Nelson, Keith–FThS1, FThZ Nelson, David D.–SMB3 Neiser, Jason D.–FThC6 Negro, M.–LTuE4 Nazeeruddin, Mohammad K.–FMA2 Nayak, Kali P.–FTuT5 Nataraj, Latha–LTuA3 Nataraj, L.–FMH2 Nascimento, Vitor V.–JTuA29 Narimanov, Evgenii E.–FWG3 Narducci, Francesco A.–LThE3, LTuJ2, Narayanan, Karthik–FMH7 Nakano, Kazuya–FTuD7 Nakamura, Toshihiro– JWA46 Nakajima, Kiyomi–FTuT5 Naik, Guru V.–FWG3 Nagel, Jonathan A.–FMC1, FWB Nadorff, Georg–STuA Nabet, JWA40 Bahram–FThY3, N. Maywar, Drew–FWQ5 Myers, J. A.–LThA2 Müstecaplıoğlu, Özgür– JTuA26 Murshid, Syed H.–FWI2,JWA32, JWA39 Murphy, P. E.–FThX6 Murphy, Kevin–FTuO2 Murphy, Dominic F.–FTuU1 Muradyan, Anush–FTuD4 Muñoz Aguirre, JTuA10, Severino– JTuA13, Mundle, R.–FWN3 Muller, Matthew S.–FME2 Mukhin, Ivan–LWG4 Mukamel, Shaul–FThAA1, LThA1 Mujat, Mircea–FTuB1 Mouro, Gérard–FWN2 Mouradian, Levon–FTuD4 Moss, Dave J.–FThI1, FTuC2 Moss, David–FThAA, FThO1 Mosley, Peter J.–FWW1 Moskalev, Igor–FThL3 Moskalenko, Valentina V.– FThJ5 Mosallaei, Hossein–FThY4 Morse, Theodore F.–FWK4 Morris-Cohen, Adam J.– LTuA1 Morris, Stephanie–FTuW1 LTuJ3, LWG JWA42 Key to Authors 137 LWE4 JWA25 Jixiong– Pu, JTuA19 Yang– Pu, N. P.–FTuQ5 Puente, Rami–FMB4 Pugatch, G.–JTuA62 Harish Puli, Aaron–FWS5 Pung, Szymon–JTuA53 Pustelny, Pyzdek, Andrew–JWA06 FThQ4 Minghao–FThI2, Qi, Pan–JTuA55 Qi, LThC5 Yiling– Qi, Li–FTuC5 Qian, , FTuR5 , FThK FThD Jie– Qiao, Jinze–JWA12 Qiu, FTuX3 Fabien– Quere, FWK4 S.– Richard Quimby, Robert G.–FTuF7 Quivey, JTuA21 X.– Qun, Zhou Raabe, Ines–FMA2 FTuC4 Radic, Stojan–FMF1, FWW3 Radic, Stojan–FWW2, G.– LWA4 Alexander Radnaev, R.– Srinivasa FTuT2 Raghavan, G.–FTuN2 Raizen, Mark FMF2, FWQ1 T.– Matthew Rakher, M.– JTuA39 Raley-Susman, Kathleen Ralph, J.–FWL2 JTuA50 Mahalakshmi– Ramamurthy, FWG4 Hamidreza– Ramezani, FMN1 Patricia– Ramirez, Lourdes G.–FMF5, FMF6, FMM, FTuT, John Rarity, LMB1 B.– Raschke, Markus , FWH1 Ramesh–FTuB4 Raskar, FWQ7 Swati– Rawal, William–JTuA62 Rawlinson, A.–FThY1 Emily Ray, Michael–FTuL2 Raymer, G.–FMF1 Michael Raymer, FThI1 Razzari, Luca–FThO1, M.–FMH3 Ronald Reano, Peter–FTuS6 Rechmann, C.– FTuQ2 Mikael Rechtsman, K.–FWX2 Rohith Reddy, Michel–FThP7 Redon, J.–FWM2 Reece, Peter D.–LWJ3 Margaret Reid, Bjoern–JWA41 Reinhard, M.–FWQ6 Charles Reinke, LThB2 Wade– Rellergert, FWD3 JWA24 Pfeifer, T.–LTuE1 Pfeifer, Henry H.–FMN5 Phan, S.–LTuD3 Brian Philips, FTuT6 B.– Nathaniel Phillips, P.–STuD3 W. Phillips, M. Lisa–LWL3 Phipps, Antonio–FWZ1 Picozzi, Patricia–FMD2 Piers, , FWY Rafael–FTuI1 Piestun, Piletic, Ivan–FTuF3 FML1 Thomas– Pingel, Dario–FTuW5 Pisignano, SMA2 W.–FML2, David Piston, B.–FMF3 Todd Pittman, Eric–FWO6 Plum, Halina–JWA13 Podbielska, Adrian–FMK4 Podoleanu, A.–FWN3 V. Podolskiy, L.–LTuE4 Poletto, Alessandro–FTuW5 Polini, L.–LWE4 A Politi, , FWD1, , FTuA FMJ6 Markus– Pollnau, LWI1 Oleg– Poluektov, Sameera–FTuK3 Ponda, G. S.–JTuA40 Richard Pong, Raphael–FTuG3 Pooser, FThK1 Gabriel– Popescu, FThB4, FThB1, Sergei–FME4, Popov, FMD Jason– Porter, STuD3 (Trey)– James Porto, K–LWE4 Poulios, FThJ2 G.– Christopher Poulton, N.–FWX2 Frances Pounder, Marzieh–FThY5 Pournoury, K.– FThX5, FWS5 Menelaos Poutous, FWG2 Ekaterina– Poutrina, L.–FThJ, FWQ3 Michelle Povinelli, E.–FThG8, FThV5 Peter Powers, A. K.–FWN3 Pradhan, A.–FMN5 Matthew Prantil, LTuC3 Talakonda– Rao, Prasad Dennis–FThW2 Prather, FThI6 F.–FMH7, Stefan Preble, Daryl–FWM1Preece, Paola–JWA40 Prete, FThP6 Zachary W.– Prezkuta, J.–FTuR5 Price, Roland–FTuT2 Probst, Demetri– LTuF3 FMG3, Psaltis, J.–LTuI1 Ptasinski, October 24–28, 2010 • JWA65 Parazzoli, Claudio G.–FMM4 Claudio Parazzoli, , JTuA56 JTuA53 Kyu– Byung Park, Hong-Gyu–FThJ4 Park, Junghyun–FThBB2 Park, Hoon–FThY5 Ji Park, Ho–JWA50 Jun Park, S.–FTuC4 J. Park, Minkyu–FThY5 Park, FTuC2 Yongwoo–FThI1, Park, JWA41 J.– Alyssa Pasquale, A.–FThO1 Pasquazi, Alessia–FTuC2 Pasquazi, H.–FTuB1 Ankit Patel, R. B.–FMM1 Patel, Anil K.–FThN6 Patnaik, G.–FMA2 Andras Pattantyus-Abraham, M.–FTuQ6 Patterson, B R.–LWE4 Patton, LTuI3 FWS6, Melania–FWF6, Paturzo, FWJ1, FWV Richard– Paxman, , FTuQ4 Ben–FTuQ3 Payne, Christine–LWL2 Payne, SWA3 David– Payne, Gil–FWH3 Paz, , JWA64 FWR4, Justin–FWE5, Peatross, FTuC2 Marco–FThO1, Peccianti, Christian–FWX5 Pedersen, FWK1 E. V.– Martin Pedersen, Linsen–LTuE5 Pei, B.–JTuA60 Vitor Pelegati, Alain–FMN1 Pellegrina, Stefano–FWF5 Pelli, JWA44 Abe– Pena, Cristian–JWA04 Penciu, Victor–JWA04 Penciu, LTHA4 Alejandro– Perdomo-Ortiz, LWG4 Evgeniy– Perevezentsev, JTuA06 Eduardo– Pérez-Careta, FWW2 Ana– Peric, Zachary–FThG2 Perret, LMA4 W.– Joseph Perry, A–LWE4 Peruzzo, Pervak, Vladimir–FTuL1 Dmitry–FMG1, FThD1, LTuB6 Pestov, Linda–LMA, LMA2 Peteanu, C.–LTuD4 Jan Petersen, J.–JWA11 Timothy Peterson, G.–JWA09 Keith Petrillo, Pierre–LThF3 Petroff, FThB6 Nasser– Peyghambarian, , LTuD1 LThB3 Tilman– Pfau, FiO/LS 2010 LTuG1 LWH6 Kenji– Ohmori, Ikuma–FThA2 Ohta, Jun–FMI4 Ohta, FTuD7 Nagaaki–FTuD6, Ohyama, Jun–JTuA59 Oi, JTuA63 Yu–JTuA59, Oishi, , FTuC3 FTuC Yoshitomo– Okawachi, Ali K.–FWU5 Okyay, Ernesto–JWA15 Oliva, JTuA29 C. R. F..– Julio Oliveira, M.–FTuB4 Manuel Oliveira, D.–LTuG3 Peter Olszak, A.– JWA07 Miguel Olvera-Santamaría, G.– FWB2 Fiorenzo Omenetto, Cengiz– FWU5 Mehmet Onbasli, A.–FThK4 J. Kelvin Ooi, LThH3 Raymond– Ooi, FWN1, FWN6 Meir–FThO3, Orenstein, A.–JWA45 Miguel Orszag, FThY3 M.– FThT6, Richard Jr., Osgood, FThM4 Tariq– Osman, Elena A.–FWP3 Ostrovskaya, S.–JWA07 Andrey Ostrovsky, Ota, Junya–FThA2 FThQ8 Fang–FMJ5, Ou, Ruth–FMF6 Oulton, F.–FThR3 Rupert Oulton, Jing–FThQ4 Ouyang, FWB4 Sahin Kaya–FMJ4, Ozdemir, Govind–FWQ5 Agrawal, P. Rafael H.–JTuA05 Pacheco, FWM1, FTuG5, Miles–FMB5, Padgett, A.–FThO2, LTuG3 Lazaro Padilha, JWA28 JWA23, Alfonso– Padilla-Vivanco, Stefano–FTuW5 Pagliara, Christiane–FMG4 Pailo, A.–FWL2 Pak, JWA53 P.– Bishnu Pal, FWF1 Sudeshna– Pal, Oleg–LWG4 Palashov, László–FThZ1 Pálfalvi, Bera–FWK1 Pálsdóttir, F.–FTuB4 Vitor Pamplona, Ci-Ling–FWE6 Pan, JTuA03 Rajagopal– Panchapakesan, Christos–FWF4 Pandis, L.–LTuI1 Pang, FMN1 Dimitris– Papadopoulos, A.–FMK3 Joel Papay, S.–LMA1 Paquette, , FTuH2, FTuH4, FWM3 FTuH4, , FTuH2, FTuH1 , LMB3 JWA47 Oh, Kwang W.–JTuA03 Kwang Oh, Youngjin–JTuA07 Oh, FWC5 Erdem– Öğüt, L.–LWE4 Jeremy O’Brien, M.–FTuS4 Shawn O’Malley, Corey–FWT1 O’Hern, FTuD7 Takashi–FTuD6, Obi, LWG6 Tetsuyuki– Ochiai, L.–FTuE8 Michael Oelze, LWH LThA2, P.– Ogilvie, Jennifer FThR7 Erdem– Ogut, Jungmi–FMC3 Oh, FThA6, FThY5, Kyunghwan–FMB6, Oh, Nicoll, C. A.–FMM1 Nicoll, R.–LThC2 Torben Nielsen, J.–LThB3 Nipper, , FTuF1 FML Nozomi– Nishimura, M.–LTuE4 Nisoli, Ben–FThQ4 Niu, H.–LThE3 Jon Noble, M.–JWA58 Nock, Toshihiko–FMI4 Noda, Mikhail–FThL1, FWN, FWN3 Noginov, Heeso–FWT1 Noh, W.–FWF3 Jong Noh, Jim–FTuW3 Nole, FWT2 FTuT4, FTuQ2, Stefan–FThJ1, Nolte, Gero–FThO2 Nootz, FWF3 P.– Gregory Nordin, Alexander–FWN6 Normatov, STuA3 Michael– Morris, North RobertNorwood, A.–FThB6 FTuT6 Irina–FThA7, Novikova, LMB4 FThL4, FTuF5, Lukas– Novotny, Hidetoshi–JTuA37 Numata, Sara–FMA5 Nuñez-Sanchez, FWF5 Gualtiero– Conti, Nunzi F.–FWR1 Nürnberg, R.–FTuX3 Nuter, Nez, François–LWB1 Nez, FThR4 P.–FMH4, Maziar Nezhad, M. P.–FWS1 Nezhad, FTuP3 FTuP2, Doris–FTuA5, Ng, Chau–FTuC5 Wing Ng, JWA06 Wei-Ren– Ng, H.– JTuA48 Nicholas Nguyen, T.–FTuR5 Nguyen, X.–FThF3 Ni, , FThAA5, FThAA6 Sile– Chormaic, Nic Key to Authors 138 Rubin, Joel–FTuN3 Roy, Sukesh–FThN6, LTuB6 Roxworthy, Brian J.–FTuM2 Roux, F. S.–JWA58 Rousseau, Jean-Philippe– FMN1 Rotschild, C.–FMA1 LMA1, LTuA Rothberg, Lewis– A.–FWS5Roth, Zachary Roth, Markus– FWR1 Rotar, Vasile–JWA02 Rostovtsev, Yuri–FWR5 Roso, Luis–FTuR3 Armand–FThU4,Rosenberg, JTuA40 Rosenband, Till–LWB4 Joseph–FThM2Rosen, Patricia–FMD3Rosales, Roque, Pablo–FMA5 Ropp,FTuT2 Chad– Ronen, Eitan–LWG1 Ron, Amiram–FThN4 Romero, Jacquiline– Mary FTuG5 Romero, Jacquiline–LTuG1 Romero, Carolina–FTuR3 Romalis, Michael–LThG1 Rolland, Jannick P.–FMI, FMI1,FThX1, JTuA09Rojas-Laguna, Roberto– Rohringer, N.–LTuE1 Rohrbach, Daniel–JTuA24 Rodriguez-Herrera, Oscar G.–FWP3 Ivan–Rodriguez, FTuD3 Francisco–FThH4Rodríguez, Verde,Rodas M–LWE4 Roblyer, Darren–FME1 Gordon–FTuU4Robertson, Robbins, John–FME3 Rivenson, Yair–FThM2, FWH3 Ritsch-Marte, Monika– FTuM, FWM4 Ritchie, D. A.–FMM1 CarlosRios, A.–JWA27 Nestor–JTuA24Rigual, GiancarloRighini, C.–FWF5 Richards, Danny C.–FWF3 Rice, Robert–FTuW1 Ricci, Aurélien–FMN1 Sergio–FWZ1 Rica, Ribeiro, Vitor B.–JTuA29 J.–LMA1Rhinehart, Jungtae–Rha, FMK Reynaud, François– FTuU3 Zhou–Ren, JTuA16 FWJ4 FTuE7, FTuO, FTuO6, FTuS5, FTuY3, , LWG3 Schickler, Mark–FThX4 Schettino, Giulia–JWA15 Scherer, Norbert–LThD2 Schepler, Kenneth L.–FThV5 Schechtman, Yoav–FTuE2 Schaumann, G.–FWR1 Scharrer, Michael–FMM6 Scharf, Toralf K.–FThT2 Schaake, Jason–FTuG3 Sawruk, Nicholas W.–FThP6 Savithriamma, Sreelatha K.–LTuG5 Savenije, Tom J.–LWC5 Savel’ev, A.–JTuA18 Savage, Daniel–FThX8 Sauer, M.–LThD3 Sato, Kazuo–JWA57 Sasagawa, Kiyotaka–FMI4 Sargent, Edward H.–FThO2 Sargent, Edward H.–FMA2 Sarangan, Andrew M.–FThV5, FWK3 Santra, R.–LTuE1 Santori, Charles–FTuT1 Santhosh Kumar, M.C.–LTuC3 Sansone, G.–LTuE4 Sankey, Jack–LWD2 Sanghera, Jasbinder–FTuW3 Sanchez-Mondragon, Jose J.– JTuA06, Samudrala, Sarath–FThAA4, JWA34 Sampson, Alicia–JTuA39 Samineni, Prathyush–FThG2 Salières, P.–FWE4 Reza–FTuC3Salem, MohammedSaleh, F.–FMM3 E.A.–FMM3 Bahaa Saleh, Salamo, Gregory J.–FThA3 Sakaguchi, Koichiro–JTuA41 Saito, Lucia A.M.–JTuA34 Kasturi–FThO5Saha, Sagnes, Isabelle–FWO2 Saggese, Steven–FTuS2 Saffman, Mark–LWE Sabanayagam, Chandran– JTuA20 Saager, Rolf B.–FTuS2 Rutkowska, Katarzyna– FThA3 Russell, Philip S.–FMM6 Rumbles,LMA3, LWC Garry– Ruiz-Perez, Victor I.–JWA36 Rueda, Edgar–JWA27 Ruchon, T.–FWE4 JWA59 JTuA38, JTuA43, JWA36, JWA52, , LWJ2 FiO/LS 2010 Shahriar, M.– FThI4, FWX3JWA21 Selim , Shah Hosseini, Ehsan–FWO4 Shaffer, James–LThB3, LThB4,LTuD1 Shadbolt, P–LWE4 Shabahang, Soroush–FTuW4 Tero–FTuK2Setälä, Rosalia–FMA5 Serna, Sergeyev, Sergey–FME4 Seo, Wontaek–LWD4 Sennaroglu, Alphan– FThAA2,FTuS7, Ozlem–JWA60Senlik, Sendur, Kursat–FThR7, FWC5 Semyonov, Oleg–JTuA33 MariaSelim, A.–FTuF3 Wolf–FTuS6Seka, Segev, Mordechai–FTuE2, FTuO7, FTuQ2 Marc–SeGall, JWA02 M.S..–FWL3 Christian Sears, M.S..–FMN2 Chris Sears, Scribner,FThM1 Dean– ThomasScreen, E.O..–LMA4 M.L.–FWD4 Scimeca, Schweinsberg, Aaron–FTuE5 Schwefel, Harald G.L..–FWE2 Schwefel, Harald G.L.–FThC1 Schuster, Kay–FTuH4 Schuster, Jonathan–FTuV4 Schumacher, D.–FWR1 Schultze, M.–LTuE1 Schultz, P.–SWA2 Schulmerich, Matthew V.– FWX2 Schreiber, Joerg–FWR3 Schreck, Carl–FWT1 Schowalter, Steven–LThB2 Schoonover, W.– Robert FTuE8 Schönle, Andreas–FML4 Schollmeier, M.–FWR1 Scholes, Gregory D.–LTuC2 Scholes, Gregory–LWC2 Schoenly, Joshua E.–FTuS6 Schoelkopf, J.– Robert LWE1, LWJ Schneider, Vitor M.–FTuS4 Schneider, Christian–FMF6 Schneerson, Rachel–FME3 Schmidt, Roman–FML3 Schmidt, Holger–LTuD3 Schmidt, H.–JWA59 Schmidt, Bruno E.–FTuX2 Tobias–FTuE7Schmid, Karl–FMN2,Schmid, FWL3 LWB5 JTuA26 • October 24–28,2010 Singh, Surendra–JTuA62 Singh, Rohit– JWA19 Simons, Matt T.–FThA7 Simmonds, W.–LWA5 R. Simic, Aleksandar–FThR4, FWS1 Silva, Davinson M.–JWA30 Yaron–FTuE3,Silberberg, FTuK1 Siemens, Mark E.–LThA3, LWH5 Siebbeles, Laurens D. A..–LWC5 Sidorenko, Pavel–FTuE2 Siders, Craig W.–FMN5 Shvets, Gennady–FWO1 Shverdin, Miroslav Y.–FMN5 Shuman, E.S.–LThH1 Shulika, Oleksiy V.–FTuR2 Shuker, Moshe–FMB4, FThN4 Shubochkin, Roman–FWK4 Shtaif, Mark–FTuV3 Shroff, Sapna A.–FThK2 Shreve, Andrew P.–LMA2 Shopova, Siyka I.–LTuF1 Shome,Krishanu– Shirk, James S.–FThU3,FThU4,FThU5, Shirai, Tomohiro–FTuK2 Shiraga, Hiroyuki–FThE3 Shipp, W.– Dustin FWF7 Shiner, Andrew D.–FTuX2 Shinar, Joseph–LWI2 Shin, Heedeuk–FMM2 Shields, Andrew–FMM1 Shiau, Hsiao-harng–JTuA42 Shi, Zhou–FWT4 Shi, Zhimin–FTuE5 Shi, Wei–LTuA6 Shi, Lei–FThU2 Gizelle–LMA2 Sherwood, Sheppard,FWP1 Colin– Shenoy, MR–JTuA36 Shen, Hao–FThI2, FThQ4 Sheina, E.–LMA3 Shechtman, Yoav–FTuO7 Shcherbakov, Maxim FThS2 R.– Shay, Lisa–JWA35 Shaw, Brandon–FTuW3 Sharypov, Anton V.–JWA43, LTuB4 Sharping, Jay E.–FMG4 , FTuJ5, LTuD Shapiro, Jeffrey H.–LWJ1 Shapiro, Benjamin–FTuT2 Shane, Janelle–FTuM4 Shan, Jiong–LTuA6 Shalaev, Vladimir M.–FThF3,FWG3 FThZ4, JTuA40 FWB3 Stagira, S.–LTuE4 Stadnytskyi, Valentyn– JTuA57 Stack, Daniel–JTuA66 Srivastava, Sachin K.–JTuA35 Srinivasan, Pradeep–FWS5 Srinivasan, Kartik–FMF2, FWQ1 Sridhar, Srinivas–FWO3 Sprenger, Benjamin–FThC1 Spivey, Christopher–FTuO1 Spiegelberg, Christine–LWG2 Spiecker, Heinrich–FML1 Spetor, Limor S.–LTuE2 Sperlich, Andreas–LWI1 Spasenovic, Marko–LThC3 Spanier, Jonathan E.–FThY3 Sorokin, Peter P.–JTuA15 Ofir–FWN1Sorias, Silvia–FWF5 Soria, Sorger, Volker J.–FThR3 Sørensen, Knud P.–FWX5 Sorel, Marc–FThA3 Huat,Soon Ng–JTuA21 Soni, Meenal P.–FTuS4 Song, Younghoon–LWD4 Song, Wuzhou–LTuF3 Somayaji, Manjunath–FThT7 Solomon, Glenn S.–JTuA45 D.–FTuC1Solli, Soljacic, Marin– LThF2 Roman–JTuA43,Sobolewski, JWA52 Irina V.–Soboleva, FThJ5 So, Peter T.–FThR1 Snider, W.–FTuP5 Snavely,STuB Ben– Smurov, I.–FWX4 Smith, Richard C.–FWK3 Smith, Jeffrey S.–FWJ3,FWV3 Smith, David R.–FWG2 Smith,FWS2 Bruce– Smirnov, Vadim–LWG2 Slutsky, B.–LTuI1 Slutsky, B.–FWS1 Slipchenko, Mikhail–FMG4 Slattery, Oliver–FMF2 Skupin, Stefan–FTuE6 Skotheim, Terje–FThB6 Skipetrov, E.–FTuQ3 Sergey Sivan, Yonatan–FThB8 Siqueira, Jonathas d.–JTuA46, JWA16 Sinzinger, Stefan–FThT4 Sinha, Ravindra K.–FWQ7 Singh,JWA31 Sarika– Key to Authors 139 JWA65 , JTuA62 Reeta–JTuA42 Vyas, A.–FWT2 Victor Vysloukh, Atsushi–JWA37 Wada, , FThV FThBB1 J.– Andrew Waddie, FWW1 J.– William Wadsworth, SMA3 Suzanne– Wakelin, E.–LTuH3 Amy Wakim, Edo–FTuT2 Waks, G.–LWJ2 Thad Walker, FTuK3 Laura–FME5, Waller, A.–FThZ4 Mason Walok, Gary–FThB3 Walsh, J.–FWX2 Michael Walsh, Xinjun–JTuA16 Wan, Chenchen–LMB2 Wang, FTuO1 Feiling– Wang, FThH3 FThG7, FThA5, Jing–FMK2, Wang, Jian–FThQ4 Wang, FWT5 Jing–FWT4, Wang, LTuB3 Jinfang–LThC4, Wang, FWY2 Lihong– Wang, JTuA17 Leiran– Wang, L. J.–FThC1 Wang, STuC5 Michelle– Wang, Jen–FThX2 Pei Wang, K.–FWY1 Ruikang Wang, Shaowei–FWN4 Wang, JWA12 Tianyi– Wang, Wubao–JTuA19 Wang, Xihua–FMA2 Wang, Xiangfeng–FThG5 Wang, LTuE3 Xu–FTuG4, Wang, Yadong–FTuA5 Wang, Yingying–FTuL2 Wang, , FTuP3 FTuP2 Yadong– Wang, Y.–JTuA58 Wang, Yicheng–LThG3 Wang, Ye–LWB5 Wang, Zhuo–FThK1 Wang, Zhenyu–FThK3 Wang, Z.–LThF2 Wang, FThAA6, JWA47 Jonathan–FThAA5, Ward, M.–LMB3 Jonathan Ward, FWR4, JWA64, Michael–FWE5, Ware, FTuF3 S.–FThG2, FTuF2, Warren Warren, R.–LMB2 Brian Washburn, FThAA6, JWA47 Amy–FThAA5, Watkins, FThX8 T.– Jonathan Watson, , FTuY4 , FTuY FTuF Adam– Wax, FWO7 J.–FThK3, Kevin Webb, JWA33 JWA14 Ashkan– Vakil, FThX Marty– Valente, Jason–FThF1 Valentine, A.–JTuA61 Felipe Vallejo, FMD2 Marrie– der Mooren, van Thomas–FThN1 Dijk, van FMM7 P.– Martin Exter, van LTuG3 FThO2, Stryland, Eric W.– Van Dean A.–FMK3 VanNasdale, JTuA50 Srinivasa– Varadharajan, JWA62 A.– Carlos Vargas, JTuA09 Everardo– Vargas-Rodriguez, FThQ4 Leo T.–FThI2, Varghese, E.–LTuF3 Andreas Vasdekis, LTuB5 JWA34, Michael–FThAA4, Vasilyev, M.–JTuA22 Oresta Vasyliv, Peter–FThD8 Vaughan, Roman–LTuC2 Vaxenburg, R.– FTuR3 Javier de Aldana, Vázquez Laszlo–FMN2, FWL3 Veisz, FThO5 Vivek– Venkataraman, , JTuA03 FWG5 Gayatri– Venugopal, George–LWG2 Venus, JWA29 Betancourt, Angel– Vergara Chris–FThG4 Verhaaren, JTuA35 Rajneesh– Verma, Florence–FTuS4 Verrier, LTuI3 FWS6, Veronica–FWF6, Vespini, Xavier–FThH4 Vidal, FTuW3 Guillermo– Villalobos, LWK1 LWK, M.–FTuX2, David Villeneuve, P.–LTuE4 Villoresi, H.–FTuX3 Vincenti, FThN1, FThV3, FWU, D.– Taco Visser, JWA10 G.–JTuA46, Marcelo Vivas, A.–FThT6 Yurii Vlasov, FTuO6 Sophie–FMI1, Vo, FTuL1 Konstantin– Vodopyanov, R.–LThD3 Vogel, Maite–FThA3 Volatier, R.–JTuA18 Volkov, FTuQ1 Frank– Vollmer, FThB8 Michael– Volodarsky, JWA56 Kerstin–FWD6, Volz, E.– FTuE5 Joseph Jr., Vornehm, FTuG7 L.–FTuG, Paul Voss, LTuE4 Caterina– Vozzi, R K.–JWA53 Vrshney, LThF3 Jelena–FWQ2, Vuckovic, K.– FThN5, FTuE4 Praveen Vudyasetu, October 24–28, 2010 • FWT2 Tippie, Abbie E.–FThK2 Abbie Tippie, FML2 S.– Tkaczyk, Tomasz Takashi–FMI4 Tokuda, Yasunori–JTuA41 Tokuda, Takahisa–FThG5 Tokumoto, M.–FMA1 Tomes, Matthew–FTuZ2 Tomes, A.–FTuU3 Tonello, Weijun–FMG4 Tong, JWA18 Zhisong– Tong, Nermin–FTuS7 Topaloglu, Lluis–FWT2 Torner, JTuA38 JTuA06, Miguel– Torres-Cisneros, Roberto–JWA27 Torroba, , FWL Csaba–FTuR Toth, FTuM2 C.– FTuF6, Kimani Jr., Toussaint, J.–FThM4 Daniel Townsend, , JWA28 Carina–JWA23 Toxqui-Quitl, Andrea–JWA15 Tozzi, Erin–JTuA24 Tracy, FThD8 FThD7, Rick–FThD3, Trebino, Monica–JTuA09 Trejo-Duran, FThB2 Jacob– Trevino, JTuA05 Vinicius– Tribuzi, Bruce J.–FME1 Tromberg, Kuen-Yu–FThD6 Tsai, Yao-Jen–FThD6 Tsai, Xanthi–FMI6 Tsampoula, Mankei–FTuK3 Tsang, Georgios–FWF4 Tsekenis, Shih–FWX3 Tseng, Anagnostis–FWN4 Tsiatmas, FThG3 Masaki– Tsunekane, FTuP3 FTuP2, Yongming–FTuA5, Tu, FThJ1, FTuT4, Andreas– Tünnermann, FMK4 Simon– Tuohy, Moshe–FMC3 Tur, D.–FWU1 Mark Turner, C.– FTuC3 Amy Turner-Foster, FTuO5 FThT2, Tomáš–FMB2, Tyc, S.–FThK5 J. Tyo, Shigeto–FME1 Ueda, S.–FTuH4 Unger, M.–JTuA25 Augustine Urbas, D.–JTuA18 Uryupina, K.–LTHA4 James Utterback, FWF Urs– Utzinger, FThS2 P.– Polina Vabishchevich, Kerry–FThH, FThO4 Vahala, FiO/LS 2010 , FMJ3 JWA26 FWJ4 FTuO6, Taïeb, R.–FWE4 Taïeb, Takunori–FThG3 Taira, JTuA37 Yoichi– Taira, SWB3 Hiroshi– Takahashi, Nobuaki–JWA37 Takahashi, Satoru–JTuA52 Takahashi, Masahiko–FME7 Takahata, Kiyoshi–JTuA52 Takamasu, FTuD6 Masafumi– Takeda, Yasuhiko–JWA57 Takeda, FThBB3 Antonio– Talamantes, S.–FMF5 Mark Tame, John–FTuE7 Jr., Tamkin H.–FMH4 T. Dawn Tan, Chong–FTuP5 Wee Tan, Yidong–JTuA16 Tan, Shuhei–FThW5 Tanaka, JWA37 Satoshi– Tanaka, W.–FME1 Vaya Tanamai, Dingyuan–FTuJ2 Tang, Jiang–FMA2 Tang, JWA60 Lingling– Tang, C. Y.–FWM2 Tiffany Tang, Xiao–FMF2 Tang, Yiqiao–LWF1 Tang, Edwin–JWA62 Tangarife, FMC J.– N Tao, Nicholas–FThF1 Tapia, Grayson–FWR4 Tarbox, Devrim–JTuA26 Tarhan, FWL3 Raphael–FMN2, Tautz, FThP2 Wei– Jian Tay, C.–FMM3 Malvin Teich, F.–LThA2 P. Tekavec, Ilaria–FML4 Testa, FWH, , FTuK4, FThT4 Markus– Testorf, FWO2 Jean-Philippe– Tetienne, D.–LWA5 J. Teufel, JTuA49 Damber– Thapa, C,–FTuX3 Thaury, FThC6 J.– Theisen, Michael C. T.–FMF6 Arthur Thijssen, FTuK, FTuE7, FMB, P.– Kevin Thompson, Mg–LWE4 Thompson, T.–FWJ2 Samuel Thurman, K–JTuA36 Thyagarajan, Lars–FThR2 Thylén, Fenghua–JTuA23 Tian, Lei–FMI5 Tian, FWX5 Peter– Tidemand-Lichtenberg, , FTuT4, FWT2 , FTuT4, FTuQ2 LTuB5 Tabakoglu, Ozgur–FTuS7 Tabakoglu, R.– FThBB1 Mohammad Taghizadeh, Atsushi–FWF8 Taguchi, Stenner, Michael D.–FThM4 Michael Stenner, FWH3 Adrian–FThM2, Stern, Roger–FTuW1 Stolen, JWA56 W.–FWD6, Stolz, M.–FWW1 James Stone, F.–LWF3 Aaron Straight, Donna–FThG1 Strickland, R.–FThQ1 Carlos Jr., Stroud, FThX2 Guo-Dung–FThU8, Su, Shu-Yu–JWA60 Su, Arsen–JTuA33 Subashiev, Yoshimasa–FTuT5 Sugimoto, A.–FTuR2 Igor Sukhoivanov, A.– LThC3 Andrey Sukhorukov, Vlad–FThO2 Sukhovatkin, Y.–FTuB3 Sulai, Scott–LThB2 Sullivan, Can–FWZ1 Sun, Li–LWF2 Sun, Peng–FMH3 Sun, Xiaochen–FMH1 Sun, Yuze–FTuI2 Sun, Yong–FWO5 Sun, Yuze–LTuF4 Sun, JTuA24 Ulas– Sunar, Bhuvanesh–FTuO4 Sundar, Alex O.–JTuA56 Sushkov, N.–FMH2 Sustersic, LTuF4 D.–FTuI2, Jonathan Suter, FTuD7 Hiroyuki–FTuD6, Suzuki, Jun’ichi–FThW5 Suzuki, Sergiy–FThC1 Svitlov, A.– JWA11 Grover Swartzlander, J.–FWD6 Stephen Sweeney, Y.–FThS2 Fedor Sychev, , FTuO7 FThJ1, FTuE2, Alexander– Szameit, Stan–FThU6 Szapiel, FThAA7 Thomas– Szkopek, Henry I.–JTuA04 Sztul, LWA2 Dan– Stamper-Kurn, SMA Michael– Stanley, A C.–LWE4 Stanley-Clark, FThD4, FTuE4 J.– David Starling, LWC4 Marina– Stavytska-Barba, STuA4 Richard– Steiner, M.– FThAA4, JWA34, Nikolai Stelmakh, Key to Authors 140 Woodward, S.L.–FMC1 Woo, J. H.–JWA54 Wong, Kenneth K.Y.–FTuY1 Wong, Kenneth K.Y.–JTuA30 Wong, Kenneth Kin-Yip– FTuA4 Wong, Franco N.C.–FTuY1 Wong, K.–LTuA4 Flory Wong, Cathy Y.–LTuC2 Wolf, Jean-Pierre–FTuX2 Wolf, FThN1,FThV3, Emil–FThD5, Woerdman, J. P. (Han)– FMM6 Wise, Frank–FTuJ1, LMB Wirth, A.–LTuE1 Wineland, D. J.–LWB4 Wilson-Gordon, Arlene D.– JWA43, LTuB4 Wilson, Kristina C.–LWH3 Wilson, Bridget S.–LWL3 Williams, Stanley–FThR2 R. Williams, Nathan S.–FThD4,FTuE4 Williams, Jonathan–FThL3 Williams, Brian–FTuG3 Wildey, Chester–JTuA23 Wildeman, Jurjen–LMA2 Wiederhold, FThP4 R.– Robert Wiederhold, Robert–FThX4 Wiederhecker, Gustavo S.–FThQ5 White, Thomas P.–LThC3 White, Andrew G.–LTuB Wheeler, Natalie–LMB2 Werner, James H.–LMA2 Werner, Jim–LWL3 Welp, Hubert–FTuY2 Welch, George R.–LThE3, LTuJ2 Weiss, Shimon– LThD3 Weiss, Emily–LTuA1, LTuC Weimer, Carl–SMB4 Weidemüller, Matthias– LTuH2 Wei, Yongqiang–FTuA5, FTuP2, FTuP3 Wei, Xiaogang–FWZ3, LWA3 Wei, Qing–FMK2 Wei, Huifeng–FMG4 Weeber, Henk–FMD2 Webster, Scott–FThO2, LTuG3 FTuE1, FTuE7, FWC1 , LTuG2 Yanai, Avner–FThR6, FWN6,FWP2,FWP5 Yan, Bo–JWA41 Yamilov, G.–FTuQ3, Alexey FTuQ4, FTuQ5 Yamaji, Masahiro–FThW5 Yamaguchi, Masahiro– FTuD6, FTuD7 Yakushev, O.– Sergii FTuR2 Yakovlev, Vladislav V.– FWT6 Yakovlev, V.–LTuE1 Yablon, Joshua–JWA21, LWB5 Xu, Zhimin–FTuD2, FWH2 Xu, Xiwei–JTuA54 Xu, Shen–LTuA6 Xu, Lina–FThD8 Xu, LTuA6 Lei–FThC4, Xu, Jingjun–FMI3 Xu, Fan–FThAA3, FWD2,LMA5,LTuA3 Hao–JWA06Xin, Sunney–Xie, FMG5 Xiao, Yanhong–JTuA54 Xiao, Yuzhe–FWQ5 Xiao, Shumin–FThF3 Xiao, Min–FWZ5 Xiangli, Bin–FThM3 X.–FTuP5Xia, Xavier, Jolly–FThW6 Wu, Ziran–JWA06 Wu, Yuqiang–JWA47 Wu, Xuan–FTuJ2 Wu, Xiang–FThC4 Wu, Saijun–STuD3 Wu, Shun–LMB2 Wu, J. W.–JWA54 Wu, Jingshown–JTuA01 Wu, Dan–LTuB3 Wu, Chung-Shieh–LTuF4 Wu, Chih-Hui–FWO1 Wu, Chunbai–FTuL2 Wrzesinski, Paul–LTuB6 Wright, John–LWH2 Worschech, Lucas–FMF6 Wörner, Hans Jakob–LWK1 Wörhoff, Kerstin–FWD1, FWD3 FiO/LS 2010 Zentgraf, Thomas–FThF1 Zeldovich, Boris–LWG2 Peter–FWT2Zeil, D.–FWX4Zatiagin, Martin–Zanni, LWH1 Zamudio-Lara, Alvaro– JTuA38 Steve–Zamek, FMH4 Zahniser, Mark S.–SMB3 Zabawa, Patrick–LTuH3 Yum, Honam–FThI4, JWA21, LWB5 Yulaev, Alexander–FMI2 Yüce, Mehdi Y.–FThAA2 Yuan, Yan–FThM3 Yuan, Ping–LThC4, LTuB3 Yu, Ping–FTuI4 Young, Andrew B.–FMF6 Youn, Ho–STuD4 Seo Yoshihara, Masami–JWA51 Yoshie, Tomoyuki–JWA60 Yoon, Geun-Young–FMD1 Yip, Hin-Lap–JTuA61 Yin, Stuart–JTuA02 Yilmaz, Selman Tunc–FTuT7 Yi, Fei–FMJ5 Yesayan, Garegin–FTuD4 Yerci, Selcuk–FWQ2 Yegnanarayanan, Siva–FMJ1, FWO4 Ye, Jun–FTuL3, LWB2 Yao, Can–FThH4 Yankelev, FThN4 Dimitry–FMB4, Yang, Xuan–FMC5 Yang, Sidney S.–JTuA11 Yang, Sigang–JTuA30 Yang, Ruoxi–FWU4, JTuA08 Yang, Linglu–JWA41 Yang, Lan–FWB4 Yang, Lijun–FThAA1 Yang, Lan–FMJ4 Yang, Jianke–JWA51 Yang, Jin-Kyu–FWT1 Yang, J.–FWD1 Yang, Haw–LWF Yang, Cheng–FTuN1, LWD2 • October 24–28,2010 Zhao,FWB5 Xin– Zhao, Wangshi–FWU4, JTuA08 Zhao, Shuang–JWA22 Zhao, Ran–LWA4 Zhao, Ningbo–FMF4 Zhao, Liping–JTuA14 Zhao, Luming–FTuJ2 Zhao, Liping–FThK4 Zhao, Kun–LWK2 Zhang, Zhaoqing–FWT5 Zhang, Zhigang–FTuJ3 Zhang, Zheshen–FTuG7 Zhang, Yundong–LThC4, LTuB3 Zhang, L.–LWJ2 Xianli Zhang, Xuenan–LThC4, LTuB3 FTuZ2Zhang, Xingyu– Zhang, Xiang–FWG1, FThR3 Zhang,FThP8, FThQ7 Xiaomin– Zhang, Xiang–FThF, FThF1,FThF4 Zhang, Xin–FThBB4 Zhang, Wen Q.–FThA4 Zhang, Wen Qi–FTuJ5 Zhang, Shulian–JTuA16 Zhang, Shuang–FThF4 Zhang, Rui–FThA5, FThH3 Zhang, Qi–LWK2 Zhang, Qiming–FThC4 Zhang, Peng–FThW4, FTuM3, JWA51 Zhang, Jiepeng–LWA3 Zhang, Jing–LThC4, LTuB3 Zhang, Jie–JTuA43, JWA52 Zhang, Jianyong–JTuA32 Zhang, Jiepeng–FWZ3 Zhang, Jin Z.–FMC5 Zhang, Han–FTuJ2 Zhang, Hao–FMK2 Zhang, Guoquan–FMI3, LThC5 Zhang, Delong–FMG4 Zhang, Boyang–JTuA02 Zhan, Qiwen–FThG8 Zhai, Zhaohui–FMI3 Zhai, Yan-Hua–FMG4 Zeytunyan, Aram–FTuD4 Zergioti, Ioanna–FWF4 Zyuryukin, Yuri–FMI2Zyuryukin, Zwickl, Benjamin M.–FTuN1, LWD2 Zuta, Yoav–FMJ7 Zuo, Yanlei– FTuR4 Zou, Weiyao–FTuB5 Zou, L.–FMC1 Zong, Weijian–FTuJ3 Zlatanovic, Sanja–FThC, FTuC4, FWW3 S.–JWA56Zinnkann, Zimprich, Martin–FWD6, JWA56 C.–JWA16Zílio, Sérgio Zielinski, Thomas P.–FWJ3, FWV3 Zhukovsky, Sergei V.–FThB5 Zhu, Yifu–FWZ3, LWA3 Zhu, Yunhui–FThA5, FThH3 Zhu, Rui–FTuY1 Zhu,FThAA4, JWA34 Lei– Zhu, Jinsong–FWB5 Zhu, Jiangang–FWB4 Zhu, Jinsong–FThC8 Zhu, Jiangang–FMJ4 Zhu, G.–FWN3 Zhou, Zhiliang–FThM3 Zhou, Yue–JTuA30 Zhou, X-q–LWE4 Zhou, Tao–FThC8, FWB5 Zhou, Renjie–FThG8 Zhou, I.–FTuP5 Zhou, Chun–FTuJ3 Zhong, Jingang–JTuA55 Zherebtsov, Z.–LTuE1 Zheng, Zheng–FThC8, FWB5 Zheng, Yunan–FTuA5, FTuP2, FTuP3 Zheng, Huaibin–FWZ5 Zheludev, Nikolay– FThL, FWG6, FWN4 FWO6