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CLEO: QELS-Fundamental Science Tuesday, 11 June

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Executive Ballroom210AExecutive Ballroom210BExecutive Ballroom210CExecutive Ballroom210D<strong>CLEO</strong>: <strong>QELS</strong>-<strong>Fundamental</strong> <strong>Science</strong>JOINT<strong>CLEO</strong>: <strong>QELS</strong>-<strong>Fundamental</strong> <strong>Science</strong><strong>CLEO</strong>: <strong>Science</strong>& Innovations16:30–18:30QTu3A • HyperbolicMetamaterials IIPresider: Natalia Litchinitser;University at Buffalo, The StateUniversity of New York, UnitedStates16:30–18:30JTu3B • Symposium onAdvances in Extreme UV<strong>Science</strong> and Applications:Advances in Extreme UV<strong>Science</strong> and Applications IPresider: Patrick Naulleau;Lawrence Berkeley NationalLaboratory16:30–18:30QTu3C • Selected Topics inQuantum OpticsPresider: Barry Sanders,University of Calgary, Canada16:30–18:30CTu3D • Short-wave IR Lasersand Laser Beam PropagationPresider: Gregory Wagner;Lockheed Martin CoherentTechnologies, United States<strong>Tuesday</strong>, <strong>11</strong> <strong>June</strong>QTu3A.1 • 16:30 InvitedTopological Transitions in Metamaterials: QEDand Related Effects, Vinod M. Menon 1 , HarishKrishnamoorthy 1 , Zubin Jacob 2 , Tal Galfsky 1 ,Evgenii E. Narimanov 3 , Ilona Kretzschmar 4 ;1Physics, CUNY Queens College & GraduateCenter, USA; 2 Electrical and Computer Engineering,University of Alberta, Canada; 3 Electrical andComputer Engineering, Purdue University, USA;4Chemical Engineering, CUNY - City College, USA.We demonstrate a topological transition in theiso-frequency surface of a strongly anisotropicmetamaterial and show the potential of this opticaltopological transition for controlling light-matterinteraction.QTu3A.2 • 17:00Blue shift of spontaneous emission in hyperbolicmetamaterial, Lei Gu 1 , Thejaswi Tumkur 1 , GuohuaZhu 1 , Mikhail A. Noginov 1 ; 1 Center for MaterialsResearch, Norfolk State University, USA. Wehave observed sizable blue shifts in spontaneousemission of DCM and R6G dyes embedded intolamellar metamaterials with hyperbolic dispersion.The effect is explained by dispersion of the densityof photonic states.JTu3B.1 • 16:30 InvitedCoherent EUV High Harmonic Sources for Applicationsin Imaging, Materials Dynamics andNanometrology, Margaret M. Murnane 1 , HenryKapteyn 1 , Tenio Popmintchev 1 , daniel adams 1 ,Matthew Seaberg 1 , Damiano Nardi 1 , KathleenHoogeboom-Pot 1 ; 1 University of Colorado atBoulder, USA. Coherent high harmonic lightsources in the extreme ultraviolet and soft x-rayregion are ideally suited for range of nano-imaging,nano-metrologies, and dynamic measurements ofmaterials, thin film and magnetic samples.JTu3B.2 • 17:00 InvitedHigh Average Power, 100 Hz Repetition Rate,Table-top EUV/Soft X-ray Lasers, Brendan A.Reagan 1 , Keith Wernsing 1 , Cory Baumgarten 1 ,Leon Durivage 1 , Mark A. Berrill 1 , Federico Furch 1 ,Alden Curtis 1 , Chase Salsbury 1 , Brad Luther 1 ,Dinesh Patel 1 , Carmen S. Menoni 1 , Jorge Rocca 1 ;1Department of Electrical and Computer Engineering,Colorado State University, USA. Compactλ=13.9 nm and λ=18.9 nm lasers with >0.1 mWaverage power at 100 Hz repetition rate driven by adiode-pumped, 1 J, CPA laser were demonstrated.Wavelength scaling to λ=10.9 nm will be discussed.QTu3C.1 • 16:30Experimental Study of the Past of a Photon, ArielDanan 1 , Demitry Farfurnik 1 , Shimshon Barad 1 ,Lev Vaidman 1 ; 1 School of Physics and Astronomy,Tel Aviv University, Israel. Tiny perturbation, indifferent places, probe where was a photon passingthrough an interferometer. A surprising pictureemerges, which is not a continuous trajectory orset of continuous trajectories.QTu3C.2 • 16:45Direct Bell States Generation on a III-V SemiconductorChip at Room Temperature, AdelineOrieux 1 , Guillaume Boucher 1 , Andreas Eckstein 1 ,Aristide Lemaître 2 , Pascal Filloux 1 , Ivan Favero 1 ,Giuseppe Leo 1 , Thomas Coudreau 1 , Arne Keller 3 ,Pérola Milman 1 , Sara Ducci 1 ; 1 Laboratoire Matériauxet Phénomènes Quantiques Université ParisDiderot/CNRS, France; 2 Laboratoire de Photoniqueet Nanostructures CNRS, France; 3 Institut de <strong>Science</strong>sMoléculaires d’Orsay Université Paris Sud/CNRS, France. We demonstrate the generationof polarization entangled Bell states at roomtemperature and telecom wavelength on a 3-5semiconductor chip. A theoretical model providesways to understand and control the amount ofentanglement.QTu3C.3 • 17:00Photon-number-resolved detection of photonsubtractedthermal light, Yanhua Zhai 1 , FranciscoBecerra-Chavez 1 , Boris L. Glebov 1 , Jingyun Fan 1 ,Sae Woo Nam 2 , Alan Migdall 1 ; 1 JQI NIST andUniversity of Maryland, USA; 2 National Instituteof Standards and Technology, USA. We examinethe photon statistics of photon-subtracted thermallight with photon-number-resolving detection.We show the photon-number distribution transformingfrom a Bose-Einstein distribution to aPoisson distribution as the number of subtractedphoton increases.CTu3D.1 • 16:30Recent Advances in High Power, High EnergyTunable Cr:ZnS/Se Lasers, Sergey B. Mirov 1,2 ,Vladimir V. Fedorov 1,2 , Igor Moskalev 2 , SergeyVasyliev 2 , Dmitri Martyshkin 1,2 , Mikhail Mirov 2 ,Valentin P. Gapontsev 3 ; 1 University of Alabama atBirmingham, USA; 2 IPG Photonics Corporation,USA; 3 IPG Photonics Corporation, USA. We reporton recent progress in development of high power;high energy; tunable (1.9-3.3 μm), mid-IR Cr:ZnS/Se lasers operating in CW (>20 W), gain-switched(>20 mJ@7ns) and long pulse ( >1 J@7ms) regimes.CTu3D.2 • 16:45Multi-stage Cr:ZnSe power amplifier pumpedwith Q-switched Tm:YAG laser, Masaki Yumoto 1 ,Norihito Saito 1 , Utako Takagi 1 , Takayuki Tomida 1 ,Satoshi Wada 1 ; 1 RIKEN, Japan. We demonstratedthree-stage Cr:ZnSe power amplifier pumpedwith Tm:YAG laser. Maximum pulse energy of52.2 mJ was obtained at 2.41 µm in the three-stageamplifier. Energy conversion efficiency reachedmore than 44%.CTu3D.3 • 17:00Performance of High Power 2 µm Ho:YAG Laser,yingjie shen 1 , Bao-Quan Yao 1 , Xiao-Ming Duan 1 ,Tong-Yu Dai 1 , You-Lun Ju 1 , Yue-Zhu Wang 1 ;1Harbin institute of technology, China. We presenta CW and Q-switched Ho:YAG laser resonantlydual-end-pumped by four diode-pumped Tm:YLFlasers at 1.908 µm. The maximum CW outputpowers of <strong>11</strong>1 W at 2.122 µm have been obtained.<strong>11</strong>6<strong>CLEO</strong>: 2013 • 9–14 <strong>June</strong> 20132013<strong>CLEO</strong> <strong>Tuesday</strong>.indd 255/17/13 3:<strong>11</strong> PM

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