Transcription
2013 ConferenceonLasers andElectro-Optics(CLEO 2013)San Jose, California, USA9-14 June 2013Pages 533-1254J .UT'r W? 3pP CEC2/5IEEEISBN:Catalog Number:CFP13CLE-POD978-1-4799-0960-5
QM2E.4Free-space Trajectory Management of Self-Accelerating Beams Through533Fourier-space Phase Chremmos,Z.Generation andY.Liang,P.M.Nemirovsky,D.Liu,Deng,Beams in CurvedI. Kaminer, M.Zhang,J.Xu,OpticalandcrystalZhi,K.Efremidis,D. rohaber,VorticesSokolov;A.Measurement of hov,aRaman-United StatesAngularMoya Cessa,Momentum Spectra of Ultra-Interferograms543Morita; JapanNegative Optical ForcesW.Ding,C.Qiu,of vectorial Bessel beamsChristodoulides; United3DR.Yang, K. Yamane, Y. Toda,Evolution539Z. Chen; China541Experimental DemonstrationV.QM3E.5Y. Gao, N.propagation of partially spatiallyD. Song, C. Lou, X.Quasi-real-timeZ.QM3E.4535along arbitrary trajectoriesbroadband Optical Vortices from Fork-likeQM3E.3CanadaGeneration of femtosecond optical vortices by molecular modulation inactiveQM3E.2Morandotti;United StatesAcceleratingQM3E: Non-conventional BeamsQM3E.1J.Zhang,Chen;Linear and NonlinearR. Bekenstein, J.QM2E.7R.Chen,Bessel-like beamsChristodoulides,QM2E.6Z.Bongiovanni,M. Miri, A.WavesDogariu;549United States547Perez-Leija,StatesAccelerating ElectromagneticA.at Dielectric InterfacesI.Kaminer,M.Segev,D. N.545
M. -coregas-filledphotonic crystal fibers551Biancalana; Germanyin adynamicsSheinfux,intrappingF.Saleh,Kaminer, M. A. Alonso,I.Soliton-radiationM. F.QM3E.7Bandres,polarizability553diffracting trapping -trapping of light ticlesS. Fardad, A. Bezryadina, P. Zhang, Z. Chen, D. N. Christodoulides; United StatesQM4E: Nonlinear Imaging and Spatial and Temporal EffectsQM4E.1Dispersion ofthe Electronic Third-OrderH. Hu, T. R.Stryland,QM4E.2M.A.Regensburger, C. nska,E. W. VanPhotonic LatticeTemporalOnishchukov,M. Miri, G.LightinSemiconductor OpticalaD. N.United StatesTemporalCloakD. E. Leaird, A. M.Insensitive Phase559Amplifier for563Weiner;United StatesRestoration of Blurred Images Due to Phase Distortion BasedX.557561Prucnal;A Telecom-BasedJ. M.QM4E.5P. R.Chang,O.MoleculesPeschel; GermanyMicrowave PhotonicsM.SymmetricReichert,Observation of Discrete Solitons in aWimmer,ofHagan; United StatesChristodoulides,QM4E.3M. Seidel, M. Ferdinandus, M.Ensley,D. n-in Second-Order Nonlinear Medium: Novel SchemeZou, X. Lin, P. Zhao, P. Hong, Y. J. Ding, X. Mu, H. Lee, S. K. Meissner, H. Meissner;United StatesQM4E.6Imaging cross-correlationfieldsF.QM4E.7Eilenberger,Second harmonicS.FROG: retrieval ofultrashort, complex, ion forE. A.Khazanov,A.T.Kaiser,T.Pertsch; GermanyPW class lasersShaykin,569V. Lozhkarev, V.Tcheremiskine, O. Uteza,M.Sentis, V. Ginzburg; Russian FederationQM4E.8Observation of Collapse Arrest in Pure Kerr Media Sustained ThlE: Quantum PhotonicsQThlE.lCorrelated Photon-Pair Generation in the Low-Raman Window ofGell.5As24Se64.5C.Xiong,J.He,nanowireA. S.Clark,aChalcogenide573M. J.Collins,X.Gai,D.Choi,S. J.Madden,B. Luther-565
Davies, B. J. Eggleton; AustraliaQThlE.2Photon pairC. ini,D. N.Solntsev,resonators andS.in nonlinear . S.P.Strain,M.L. G.Sorel,575structuresAustraliaKivshar;generation of correlated photon pairs577Galli,waveguidingSukhorukov,photonic moleculesHelt,in siliconJ. E.Sipe,ringD.Gerace,M.Bajoni; ItalyA down-conversion source oftelecomA. A.positively spectrallycorrelated and decorrelated579photon pairsT. Lutz, P. L. Kolenderski, T. Jennewein; CanadaQThlE.5Enhanced transmission for ultra-low-power nonlinear opticsin Rubidium vaportapered optical fibersT. B.QThlE.6M.Pittman,Bell's Measureas aElectromagneticK.QThlE.7L.Cohen,J. D.Franson; United StatesQuantitativeFieldsG. DiKagalwala,ExperimentalLai,experiments using581Tool in ClassicalOpticalCoherence of583Giuseppe,super resolvedA. F.phaseAbouraddy,B. Saleh; United Statesmeasurements at the shot noise limit585H. Eisenberg, D. Istrati, L. Dovrat; IsraelQTh3E: Plasmonic perimentNanoparticles:588Giessen; GermanyThe Influence of590Kingsborough,K.Hamad,A.Swiston,G. Geurtsen, M.LoopsKovalenko,Schmidt;inNanosphere Extinction Spectra: Theory592Singh,L.Vuong; United StatesGeneration of ultrashort acoustic0.Fano structuresH. W.United StatesM. Moocarme, N. D.O.Lippitz,M.of PlasmonicThe Role of Plasmonic Currentandcomplex plasmonicSchumacher,and SolventSworin,V. Liberman, M.QTh3E.5T.Optical PropertiesMaterial, Size, ShapeQTh3E.4587Ropers; GermanyThird harmonicB.QTh3E.3Effects in Metallic NanostructuresV.Shalagatskyi,T.pulsesin cobaltbyPezeril,V.V. V.Gusev,ballistic electrons inTemnov,D.Makarov,goldL.FranceQTh4E: Integrated Nonlinear PhotonicsQTh4E.lMicroresonator-Based Parametric Frequency Comb Generation WithoutExternalPumpLaserA. R. Johnson, Y.an596Okawachi,M. Lamont, J. S.Levy,M.Lipson,A. L.Gaeta; United594Han,
StatesQTh4E.2Phase Noise Spectrum and CarrierOptomechanical Oscillators 598A.Grine,Wu,QTh4E.3SolitonT.E. Grutter, T. Rocheleau, N. Quack, T.K.C. T.V.QTh4E.4K.Wang,Sun,QTh4E.7microresonatorsC. Y.Jost,Wang,X.superfluidZhang, C. Schuck,M.Kondratiev,Gorodetsky, T.J.AmplificationinAmorphousSiliconsilicon disk cavities604H. X.Tang; UnitedStatesin a-Si:H NanowireOptical Nonlinearities606WaveguidesPagan, J.J. Wathen, K. Wang, A. C. Foster, T. E. Murphy; United StatesFormation and control ofV. Ardizzone, P.Baudin,J.Turing patternsA.Diziain,interacting polaritons in coupledY.Tse,P. nol, R. Binder,J.Abbarchi,Tignon,E.S.FranceFreestanding cher;S.N. M.600ultrahigh-Q wavelength-sizedheliumsemiconductor microcavitiesQTh4E.8I. Jutla, M. C.602Non-InstantaneousV. R.Zheng,SwitzerlandNonlinear optical effects ofX.Z.A. C. Foster; United Statesimmersed inQTh4E.6opticalBroad-bandwidth Near-IR ParametricWaveguidesQTh4E.5inJ. D.Brasch,Kippenberg;Beyazoglu,PerformanceUnited StatesNguyen;mode-lockingHerr,Modeling of HighPowerniobatephotonic crystalcavities for y,A.Tunnermann,T.Pertsch;GermanyQTulE: Laser Cooling and Novel PheonomenaQTulE.lCryogenic IntracavityLaserCooling Using HighSurface Emitting Lasers (VECSELs)M.Ghasemkhani,Sheik-Bahae;QTulE.2A. R.Albrecht, S. Melgaard,D. V.Seletskiy,J. G.Cederberg,Phonon-assisted Bandtail Anti-Stokes Photoluminescence of GaN: NovelG. Sun, R.Chen,Y. J.Ding;614United StatesOptical refrigeration achievesS.QTulE.4Cavity612United StatesMechanism for Laser CoolingQTulE.3Power Vertical ExternalMelgaard,D. V.An event horizon inM.PTElazar,symmetryV.Seletskiy,anFleurov,AT 180KM.Sheik-Bahae; United Statesoptical analogS.Barad;616ofaLaval nozzleIsraelin coherent atomic media620618M.
;optical nonlinearitiesM.MicroscopyN.inUnited Statesquantum-confined systems622United J.Yeh,Hone,625Osgood; UnitedR. M.StatesLaser Filamentationin airNitrogen lasingA.QW1E.2R.Shafei,OpticalChristodoulides,M. Miri, D. N.control ofTopologicalS.QTulE.7Sheng,R. B.Dogariu,627Miles; United StatesPropagation Dynamicsof Dressed629Optical FilamentsM. Mills; United StatesQW1E.3Absolute Measurements of theDirect,in GasesJ. le gasZ.Nan,J.Wave EmissionbyKartashov,D.United StatesdynamicsH.Jhajj,N.JetX.Zhao,femtosecond filamentationonLight through DisruptedConical Emission635ChinaZhu;Mid-IR Filaments in SolidsA.633Milchberg; United StatesPugzlys,D. Faccio, A.637Zheltikov,A. Voronin, A.Austriameter scale ACMysyrowicz;discharges byBrelet,A. Houard, G. Point, Y.QW1E.8Milchberg;H.Wahlstrand,Alisauskas,Guiding ofY.Super-luminescentYu,Baltuska;QW1E.7longJ. K.Generation ofZ.QW1E.6Wahlstrand,The effect ofY.Nonlinear Refractive L.639Arantchouk,A.FranceInfluence of the anomalous dispersionfemtosecond laser filamentationD. M. Maeva, K.Mysyrowicz,laser filamentation in airA.Lim,on theV. Jukna, E. McKee, M.Couairon;supercontinuum generation by641Baudelet,A.Houard,M.Richardson,A.FranceQW3E: Supercontinuum Generation and Temporal 3Amiranashvili,Linking frequency combstoC.Bree,F.QW3E.3PropagationY.R. Xu, S.Erkintalo,Xiao,ofMurdoch,J. M.Maywar,Steinmeyer; GermanyG. P.from cascaded645Dudley,few-cycle pulses in nonlinearD. N.G.supercontinuum generation:four-wave mixing to Cherenkov radiationM.Mitschke,G. Genty; FinlandKerr media: HarmonicAgrawal; United Statesgeneration647
QW3E.4Raman-assisted octave-spanning continuum generation in single-crystal diamondsub-cycle pulse ,J.Kartashov,.PCFsinstabilityinducedresonance inby parametric653Armaroli,S.Kasparian,J.Kudlinski,A. Mussot, A.Alisauskas,Wolf,P.A. Voronin, A.Baltuska;A.Experimental ObservationFibersFS 06:A.United StatesJoshi;M.Droques; GermanySupercontinuum Generation by Mid-IR femtosecond Filaments in MolecularD.QW3E.8C.Scalar and vector modulationalF.3 psusing651pulsesPigeon,from 2-20 urn in GaAssupercontinuum generationperiodically taperedQW3E.7649Li, M. Zhi, A. Sokolov, S. Yang, A. Kung; TaiwanRaman enhancedC02QW3E.6Lu,F.Pugzlys,A.Zheltikov,GasesM. Petrarca, P. Bejot,Austriaof Three-Soliton Molecules ,F.Mitschke; Germanyand PlasmonicsQF1A: Quantum Nanooptics & DetectorsQF1A.1Quantum PlasmonsandScholl,J. Dionne, eslami,H.Alaeian,A.A.Atre,Koh;United StatesQF1A.2Single-emitter quantum electrodynamicscontinuum farP.Kolchin,beyond the diffractionIN.Pholchai,M.inlimitMikkelsen, J.Oh,aone-dimensional tesQF1A.3Enhancement oftoaPlasmonicB.QF1A.4Demory,Spontaneous EmissionCavityP.Ku;QuantumDotCoupledUnited StatesUltrafast Electrical Modulation of the Exciton Energy for the Dynamic Control ofCavity Quantum ElectrodynamicsF.QF1A.5Rate in an InGaN661Pagliano,MicrocavityF. V.Otten,EnhancedY. CHEN, Y.663Linfield,T. Xia, L. Li, E.A. Fiore; NetherlandsQuantum Well Infrared PhotodetectorTodorov,B.Askenazi,A. Vasanelli, G.Biasol,R.665Colombelli,L.Sorba,C.Sirtori; FranceQF1A.6Membrane-integrated superconductingF.D.QF1A.7Najafi,J.Mower,Englund, K.Near-fieldK.X.Hu,F.Berggren;Probing ry,L.detectorsCheong,K.667Sunter,United StatesPlasmonic Nanostructures withaSingle QuantumDot669655
C.Z.Ropp,S.Cummins,H.yi,EfficientR.Yalla,F. LeGoffard,ofGerard,D.United States671Fofang,I. Brener, Y. S. Kivshar; AustraliaK.Morinaga,P. Miska, A.onArraysS. Liu, E. Gonzales, J. Dominguez, M.Photons intoSingleModeOpticalFiber675Hakuta; JapanBaudrion,M.677nanocrystalsVergnat,quantum statisticsTheuerholz,A.Carmele,M.Richter,Radiation Pattern of PlasmonicT.Waks;United semiconductor hybridin679Realizedby Liquid-ImmersionS.Sugita,Maeda,Plasmonic AntennasF. BernalQF2A.8D. N.Impact of Forster couplingT.QF2A.7Shapiro,Electric Resonances for All-Dielectric A.6T. S.Cubukcu;E.Plasmon-enhanced luminescence from siliconJ.QF2A.5Reed,.A. E.Staude,Decker,QF2A.4Zhu,Merging Magnetic andI.QF2A.3B.Thermal Plasmomechanical Infrared DetectorF.QF2A.2Fourkas,& AbsorbersQF2A: Nano-antennas, CouplingQF2A.1J. T.Nah,Arango,Radiation andH. F.Knorr; n,Antennas inKadoya; JapanHybridized with Dielectric WaveguidesA.683Koenderink; NetherlandsGain ofReceivingTobisu,Nano-optical Yagi-UdaAntenna Embedded in685Slab Dielectric WaveguideK. Yanazawa, Y.A.S.Maeda,H. F.Y.Hofmann,Kadoya; JapanQM1B: Near-field Imaging & SpectroscopyQM1B.1StrongInteraction between aMicroresonatorM.QM1B.2Zhang,Desiatov,G. S.I.Goykhman,plasmonsWiederhecker,MappingNonlinear ultrasonics insurfaceM.QM1B.4M.Sub-diffractionQM1B.5Shafiei,P. L. McEuen, M.Lipson;United States689Levy; IsraelU.gold-cobalt bilayerstructuresprobedwith F.Opticalof Photonic and Plasmonic DevicesTzur,V. V. Temnov, C. Klieber, K. A.Makarov,an687Barnard,Nanoscale TemperatureB.QM1B.3A.Carbon Nanotube andSingleC. Wu, X.Nelson,Bratschitsch;of nited StatesBroadband Near-Field Detection withMulti-FrequencyProbeMicroscopy695673
D. C.QM1B.6Kohlgraf-Owens,Near fieldofimagingL.complexazobenzene ayer,V.J.Haglund;Plasmonic Silver NanorodC.Jakab,Fan,Kerr EffectNeutzner,D.Dregely,effect in SPP-MOKER.Saenz,Wehlus,I. A.Akimov,705configurationFranceCarminati;707United StatesCaldwell;709United States711ItalySensitivity: calSensor For Ultra-thinLayerLi, Y. Huang; ChinaNanocavities onConductingSubstrates forStrong718Altug;United StatesGrapheneGraphene Nano-optoelectronics720Koppens; SpainGraphene Micro-andP.T.703716Active Plasmonics &F.QThlB.2Zheludev; SingaporeN.Soennichsen; GermanyAsymmetric Ring/DiskA. E.Nene,and701713Fa no-InterferenceQThlB.lS.Integrated SPP-Dielectric Hybrid Coupler BasedB.ofGiessen; GermanyG. Mistura, M. Merano;Jayaswal,DetectionQThlB:Shen,Weak measurement of the Goos-Hanchen shift.A.QM4C.8magnetic recordingMagneto-OpticalBelotelov,H. W.Marinchio,R. F.Appavoo,TreatmentQM4C.7Z.Plasmon Drag Effect in Metal NanostructuresG.use& Novel EffectsN. Noginova, V. Rono, B. Bates, J. D.QM4C.5theIsraelSegev;needle for heat assistedKreilkamp,M.Stritzker,Vincent,M.Enhanced TransverseL.Chin,B.R.Polarization-Dependent Phase-Changing NanoswitchK.onControlling Symmetry, Broadening, Width,Extraordinary onically3. Y.metal nanostructures basedDogariu; United States699QM4C: Hybrid PlasmonicsQM4C.1A.FrancePlain;Super-oscillatory achelot,Y. DeGreusard, S. Sukhov,J.Nano-PlasmonicsStrait, W.Rana; UnitedStatesChan,C.Manolatou,722J. W.Kevek,S.Tiwari, P.L.McEuen,F.
QThlB.3Broad electricalYao,Y.QThlB.4M.tuningofgraphene-loaded opticalP. Genevet, N. Yu, Y.Kats,Modulation of Mid-infraredLargeSong,J.antennasF.Kong,724Capasso; United StatesLight Using Graphene-MetalPlasmonic Antennas726N. yu; United StatesQThlB.5Electrical Control ofJ.Kim,Optical PlasmonH. Son, D. Cho, B. Geng, W.Resonance with GrapheneS. Shi, K. Kim, A.Regan,728Zettl,Y.Shen,F.Wang;United StatesQThlB.6Plasmonic Absorber EnabledElectrically TunableF.730Tong; ChinaC. Meng, L.QThlB.7NanofibersGraphene-doped Polymer Opticalyi, E. Shim, A. Zhu, H. Zhu,.Reed,E.byCubukcu;Indium Tin Oxide732United StatesQTh3B: Thermal & Optomechanical MetamaterialsQTh3B.lPhonon Polariton Spectroscopy in the Thermal Near-FieldB. O'Callahan, M. B.QTh3B.2High TemperatureY. Guo,QTh3B.3Temporal ndhu,theoryC. R.Otey,for thermal emission fromM. B.Sinclair,Optical Response usingChiralMetamaterialF.Raschke; United StatesPlasmonicsZ.Jacob;734T. S.Luk,Phase-shifts inS.asingleaFan;emitter738United StatesPlanar Plasmonic740Eftekhari,T. J. Davis; AustraliaEpsilon-Near-Zero Subwavelength Optoelectronics: ElectricallyTunable ENZ742Strong CouplingY. Jun, J. L. Reno, M. B. Sinclair, I. Brener; United StatesQTh3B.6Near-field cavityA. C.QTh3B.7Hryciw,ExperimentalQTh3B.8B. Khanaliloo, M. Wu, C. 3.Descharmes,U.Dharanipathy,Z.of nanomechanicsHealey,demonstration of resonantphotonic crystal cavityin a hollowN.optomechanical probingP.Barclay; Canadaoptical trapping and back-actioneffects746Diao,M. Tonin, R.Houdre;SwitzerlandNanostructured Transparent Conductive Oxide Films for Plasmonic ApplicationsJ. Kim, Y.Zhao,G. V.Naik,N. K. Emani, U.Guler,United StatesQTh4B: Nanoemitters & Lasers and SpasersQTh4B.l744Fiber-coupled dual-railH.Lim,C.Lee,B.nanobeam lasersAhn,Y. Lee;750Korea, RepublicofA.Kildishev,A. Alu, A. Boltasseva;748
QTh4B.2emission enhancement viaSpontaneousLEDsnanorod-arrayP. Anderson, C.QTh4B.3QTh4B.4Lin,Xing,Guler,Quest forMeng,X.Zhang; Unitedfrom ZnSe NanowiresSingaporeLengthJ. K.versusShalaev,Khurgin,M. A.Kitur,SPEDG.A.Kildishev;Noginov;758United Statesplasmons polaritons760United States762United StatesSun;of surfaceInvestigationonV. M.756Stateslow-threshold stimulated emission of surfaceTumkur,SPASERJ.QTh4B.8United StatesPovinelli;Unidirectional lasing with symmetry broken core-shell nanoparticleT.QTh4B.7modes in GaNCoherence-Enhanced Surface Plasmon Polariton PropagationU.QTh4B.6M.J. Luo, H. Li, B. Wu, X. Liu, C. Huan, H. Fan, T. Sum;P. K. Jha, X. Yin, X.QTh4B.5resonanceCharge Carrier Dynamics and Upconversion LasingUltrafastG.guided752Nd:YV04 crystalin finite-widthplasmon amplificationgold striplinebased764T. Vo, A. Maleki, J. E. Downes, D. W. Coutts, J. M.Dawes;AustraliaQTulB: Mid-IR Plasmonics & ion nanospectroscopyJin,MultispectralM. A.QTulB.3Raschke,X.Xu;Quantitative MappingD.Dregely,Hinrichs,M. B.768Raschke;of Plasmonic Near-fieldsUnited uller,Using Infrared Far-fieldH. W.Giessen; GermanyAbsorption Spectroscopy ofMolecular774United StatesAntenna-Mediated Near FieldFrequency770772Multi-Band Surface Enhanced InfraredMonolayers}QTulB.6nano-imagingUnited StatesVibrational SpectroscopyQTulB.5K.Ultrafast infrared near-field vibrational nano-spectroscopyM. B.QTulB.4Andreev,766United StatesBelkin;infrared vibrationalB. Pollard, G. 0.via molecular force detectionH. A.Spectroscopic Imaging: Extensionto the Time and776Bechtel, B. Pollard,R. L. Olman, M. J. Martin, M. B.Raschke; UnitedStatesQTulB.7Tunable, Epitaxial, SemimetallicE.Krivoy,A.Vasudev,Brongersma, S. Bank;H. P.Nair,Films and for PlasmonicsV. D.United StatesDasika,R.Synowicki,778R.Salas,S. J.Maddox,M.754
QTu2B:QTu2B.lUltrafast and Nonlinear PlasmonicsUltrafast Laser-excited Relativistic Plasmonic RadiationY.QTu2B.2Huang,K.Y.Chen,Wang,780M. Wu; TaiwanPhotonic Crystal Formation On Tapered Optical Nanofibers Using FemtosecondLaser AblationK. P.QTu2B.3C.Huang,782TechniqueNayak,Hakuta; JapanK.Mode Matched Harmonic Generation in Plasmonic NanostructuresK. P.O'Brien, H. Suchowski,J.A.Rho,Salandrino, B. Kante,X. Yin, X.784Zhang;UnitedStatesQTu2B.4Second harmonicgenerations pumped bynonelectrically .Biancalana,Sih,J.Lee,The ChemicalC. B.M. B.M.Marini,A.inTasaka; Japansingle semiconductorX.Wang,T. d Statesdynamics ofsurfaceplasmon polaritonsingoldConforti,G.ofDelia Valle; GermanyQuantumDotsCoupledto a PhotonicSaucer,A. J.Martin,J. M.Millunchick;United Statesof PlasmonicBuilding BlocksN/AUnited StatesNanoparticles796SwitzerlandPlasmonic NanostructuresL. T.Varghese,NanolithographyY.788Tong; China& Plasmonic Chiral Plasmonic Films andD.QW1N.4Liu,S.Kawata,794QW1N: Novel NanoopticalQW1N.3Ono,786Y.792Time-resolved NonlinearV.QW1N.2W.Atkin,J. M.Crystal CavityQW1N.1Gu,Ultrafast interband nonlinearnanowiresQTu2B.8Suto,A.Slow Light Femtosecond Pulses by Adiabatic Plasmonic cy generationH. Yu, W.QTu2B.6T.Surface Plasmon enhanced fields inLiu,through Resistless Nanoimprinting inMetalY. Xuan, M. Qi; United Statesbased onTwo-Surface-Plasmon-Polariton-Absorption799L. Xiao, Y. Huang; ChinaQW3N: Waveguide & PlasmonicsQW3N.1PlasmonicOptically DefinedFrequenciesH.Wong,Waveguides in CrystallineSemiconductors at801A. S.Helmy;CanadaEngineering Metallic NanocavityRadiation for EfficientUni-/Bi-directionalOptical797
QW3N.2M. Kim, Z. Li, M. C. Wu,QW3N.3C.Diziain,S.Li,Plasmonic nano-coaxialHoleymetallic lens forHybrid ckstuhl,waveguidesofT.Pertsch; GermanyEmission fromfor807Aligned Hybrid Gold NanorodsA.M.80990-degree bends and T-splittersM.Veronis,light focusingS. Fan; United StatesBrongersma,811Kildishev; JapanTaperedDecker,G.Catrysse,Gold Double-Helices for FrequenciesFreymann,vonA few tens ofExponentially GrowingBekenstein, G. Bartal,R.Kaminer,Y. S.M.Segev;Beams815IsraelPhysicsQF1C: XUV & X-ray Sources BasedonHigh-harmonic Generationfull-coherent EUV-FEL seededmicrojouleby high-order harmonic817Takahashi,T.Yamanouchi,T.E. J.K.805hybrid plasmonic-dielectric waveguidesSelf-Accelerating PlasmonsSchley,beamStatesAustraliaFS 07: High-FieldQF1C.1C.Helgert,Shalaev,S. Ishii, V. M.QW3N.7Going,L. Gan, Z. Li; ChinaLiu,W. Shin, W. Cai, P. B.QW3N.6Choo; UnitedH.Macroscopic Engineering of PolarizedJ.QW3N.5R.Plasmonic nanoparticle interaction inT. Kaiser, S.QW3N.4803Integrated H.S.Aoyama, K. Yamakawa, T. Sato, A. Iwasaki, S. .Ishikawa;JapanQF1C.2Efficient table-topH.QF1C.3N.by Few-CycleIshii,Xu,K.P.Ranitovic,IR PulsesKaneshima,K.Generation of e Phase-Dependent HighWindowQF1C.4S.WANG,of ultrashort XUVsourcelaserMashiko,Generation ofY.Wu,E.K.Oguri,T.T.doublerate819Harmonic Generation in the WaterS.Watanabe,J. Itatani;JapanK-edge (284 eV) with onlyoptical gating247 uJ823Sogawa; JapanHigh-Flux AttosecondCunningham,repetitionR. A. Kaindl; United StatesKanai,in carbonusing generalizedat 50-kHz821Kitano,pulsepulsesJ.Li,H.XUV Continuum with a 10 TWDrivingLaser825Zang, M. Chini, X. Wang, Y. Wang, K. Zhao, Z. Chang;United StatesQF1C.6Isolated optical attosecond pulses827T. Luu, M. T. Hassan, A. Moulet, O. Razskazovskaya, N. Kaprowicz, V. Pervak, F. Krausz,
E.QF1C.7Goulielmakis; GermanySparsity-based super-resolutionimages echtman,Measurement ofY. C.anEldar,M.O.Segev,IsraelCohen;Injection-Seeded Table-TopSoftX-RayE.Wang,Oliva,L.B.Yin,Luther,G.D. Ros, P. Zeitoun, J.Maynard,Spectroscopy of Atoms and MoleculesAbsorption SpectroscopySansone,Poletto,ProbingY.Li,United er,A.ofimaging829831Rocca;QF2C:extreme UV radiation.Single-Shot WavefrontLasercoherent diffractiveF.Reduzzi,M.in moleculesA. Dubrouil, C.Feng,M.833F.Nisoli,Calegari, C. Lin,W.Chu,L.Frassetto; ItalyElectronWave-packet tabilized Interferometric Attosecond Timing MeasurementsC. Miranda, M. Kotur,E.Witting-Larsen, P. Johnsson, J. Mauritsson, S. Ristinmaa-Sorensen, M. Gisselbrecht,A.L'Huillier; SwedenQF2C.4Measurement of Attosecond Photo-ionization Delay in XenonA.A.Verhoef,M.Mitrofanov,Krikunova,N. Observation of ultrafast electronattosecondF.A. Trabattoni, S. Anumula, M.Calegari,Hochlaf,QF2C.6pulsesdynamicsin N2 molecules inducedG. Sansone, issociative Ionization Dynamics of Nitrogen Molecule with InterferometricT.Okino,Furukawa,Y.Yamanouchi,K.A. AmaniEilanlou,Y.Nabekawa,843E. J.Takahashi,probed byphotoelectron spectroscopy with high harmonic pulses845Makida,H.K.Midorikawa; JapanUltrafast recovery of valence electrons in Sekikawa; JapanQThlD: Strong-field InteractionsQThlD.lM.Nisoli; ItalyM.Autocorrelation of a-few-pulse Attosecond Pulse TrainQF2C.7by841Probing Sub-Cycle DynamicsAbsorptionM.Chini,Statesof Virtual States with Attosecond Chu,Z.Chang; United
QThlD.2fieldsControlling dielectric properties with lightE. M. Bothschafter, A. Sommer, er, V. Apalkov, M. Stockman, F. Krausz, V. S. Yakovlev; GermanyQThlD.3TunnelingElectron Shell Ionization of Atoms withEkanayakeN.Boge,A. Ludwig, S.C. Cirelli, L.Heuser,Keller; SwitzerlandU.Gallmann,R.Weger,J. Maurer, A. S. Landsman, M.QThlD.4851Time in Ultrafast Science is Real and Probabilistic,L. Howard, S.Tramontozzi,W.Grugan,S. Luo, P.Wells,Classical,Crosby,RelativisticCamilo,A.C. Mancuso, B. C.A.Walker;United StatesQThlD.5F.QThlD.6enhancement of psCavityaHou,Generation of coherentfieldsK.N2 Krushelnick,United StatesThomas;A.emissions in a857plasma stringwith two-color laser859J. Yao, G. Li, J. Ni, H.Chin,QThlD.8855of Femtosecond Laser Pulses in Ionization-Induced PlasmasFree Flow Gas Jet at Relativistic IntensitiesZ. He, J. A. Nees, B.QThlD.7with 30 000 Zhang,B.W.Zeng,C.Chu,Jing,H.Y.Xie,Cheng, S.Z. Xu; Chinatenuous laserSpatio-temporal phase-contrast imaging ofChang,Z. Li, Y.M. C.Downer;structuresplasma861United StatesQTh3A: Particle Acceleration by LasersQTh3A.lLaser Plasma Acceleration of Electrons and PlasmaFieldsDiagnosticsatHighLaser863M. C. Downer; United StatesQTh3A.2Utilization ofInteraction0.QTh3A.3Study Relativistic Laser-Plasma865Jackel,A. Savert, M.Schwab,Nicolai,M.M.Reuter,J. Polz, M. Kaluza; germanyLaser-Wakefield Accelerator at 0.5a867Z. He, A.Faure;Thomas,B.Beaurepaire,Hou,J. A. Nees, on ofX.K.Krushelnick,J.United StatesLaser Driven Neutron Generation at the Texas Petawatt1.QTh3A.5Beam toDiffraction of Electron Pulses Generated inkHzQTh3A.4Few-Cycle ProbeaE.M.Gaul,D.Henderson,Gautier,Hegelich;2 GeV ElectronsZ.Li,R.869byD.Jung,A.Meadows,United StatesLaser WakefieldKorzekwa,Y.Chang,C. Pai, H.
Tsai, A. Yi, V. Khudik, tmire,M. C.Borger,Do;United StatesQM3B: Quantum Optics with Quantum DotsQM3B.1Third-orderphoton correlationsquantum dot coupled ndquist,A.Majumdar,T.Sarmiento,K. G.Lagoudakis,J.Vuckovic;United kovic;QM3B.3FanoQM3B.4K.inDotsCoupledto ,J. Lu, T.Sarmiento, J.United StatesQuantumH.Gotoh,Burgers,DotsSanada,Direct Detection ofA.Deterministically Charged QuantumQuantum InterferenceSystemH.ofNanoresonatorsJ.Effects in Exciton-BiexcitonCoherently Coupled877H.Yamaguchi,Optical RabiSchaibley, G.T.Sogawa; JapanOscillations fromMcCracken,D.D.Steel,aSingle QuantumGammon,A.DotBracker,879L.Sham;United StatesQM3B.5On-Chip Quantum Optics using Electrically Driven l,M.Kamp, S. Reitzenstein; GermanyQM3B.6K.QM3B.7Stark effect in aDynamicquantum dot strongly coupledRoy Choudhury, R. Bose, E. Waks; United StatesUltrafast downconversion1550-nmPelc,K. -photonL. Yu, J.quantum interface forC.ato a883cavitysingle quantumdotspin and885McMahon,Schneider,C. Natarajan, N. Kim, E.M.Kamp,S.Hoefling,Abe,R. H.V.Hadfield,A.Forchel,United StatesPhotons from Site ControlledV. Dimastrodonato, T.Chung,A.Gocalinska,Pyramidal QuantumE.DotsPelucchi; IrelandQThlL: Optical Memories and Atomic EnsemblesQThlL.lSolid-state Quantum Memory for Quantum CommunicationM. T.QThlL.2Afzelius;A ReversibleL.Veissier,Optical MemoryA.889SwitzerlandNicolas,for Twisted PhotonsL. GINER, D.Maxein,A.891Sheremet,E.Giacobino,J. Laurat;FranceQThlL.3Simultaneous observation ofsuper-Heisenberg scalingandspin squeezing ina887
nonlinear measurement of atomicR.Sewell,893spinsMitchell;F. Martin Ciurana, M. W.Colangelo,N. Behbood, G.Napolitano,M.SpainQThlL.4Spin coolingvia incoherent feedback inanColangelo,Generation of planar quantum squeezing inanN.Behbood,895ensemble of cold Rb atomsM.F. Martin Ciurana, G.Napolitano,R.M. W.Sewell,Mitchell;SpainQThlL.5Colangelo,G.N. Behbood, F. MartinCiurana,atomic ensemble897Sewell,M. W.G. Puentes, R.Mitchell;SpainQThlL.6Narrowband source of correlatedatomic ensemble.B.Srivathsan, G.via four-wavephoton atsukevich,D.A.Cere,C.Kurtsiefer; SingaporeQThlL.7Sensitive cavityWu,903United Statesfrequency of cesium 6S-8S hyperfineAbsoluteinterferedQTh4C3shifts in coldD. S. Weiss; United StatesTang,A Cold-atom Laser with 1C.lightAtoms and MoleculesQTh4C: Quantum Optics withJ.vector901K. Zhu, N.QTh4C.lusingmeasurementpolarizationtransitionby two-photon904spectrumT. Liu, R. Lee, W.Cheng;TaiwanDiscriminating between the Autler-Townes Splitting and the ElectromagneticallyInduced Transparency ModelsL. GINER, L. Veissier, B. M.Scherman, S.Burks,I.:aTool forSparkes,Shomroni,A.ProbingSheremet,D. V.the MediumA.Kupriyanov,Nicolas,P.Lam,906PropertiesO. S.Mishina,M.E. Giacobino, J. Laurat;FranceQTh4C.4Rydberg ow,P.J.Hung,Kimble;J. D.Petrovic,Fiber908Russell; GermanyGerhardt;VaporgermanyCrystalsR. Norte, A.910912Goban, S. Yu, J. Hood,United StatesA multi-state interferometerI.Cohen,Crystalwith SodiumAtoms in One-Dimensional PhotonicPainter,J.Euser,R.Single MoleculeG. Stein, J.S. Meenehan, C.QTh4C7T. G.Kleinbach,K
QM3E.6 Soliton-radiation trappingin gas-filled hollow-core photoniccrystal fibers 551 M. F. Saleh, F. Biancalana; Germany QM3E.7 Soliton dynamics in a diffracting trapping potential 553 A. Sheinfux, M. Rechtsman, B. Osting, J. Marzuola, M. Segev; Israel QM3E.8 Tunable polarizability and self-trapping of light in colloidal suspensionsofgold .
