Marriott San JoseSalon IIIMarriott San JoseSalon IVMarriott San JoseSalon V & VIMarriottWillow Glen I-III<strong>CLEO</strong>: Applications& Technology<strong>CLEO</strong>: <strong>Science</strong>& Innovations<strong>CLEO</strong>: <strong>QELS</strong>-<strong>Fundamental</strong> <strong>Science</strong>ATu3M • Symposium on ThePath to Sustainable Energy:Laser Driven Inertial FusionEnergy: Technology of ICF: DriveLasers, Optical and NuclearDiagnostics—ContinuedCTu3N • Imaging &Microscopy II—ContinuedCTu3O • Micro and Nano-scaleImaging Microscopy—ContinuedQTu3P • Symposium onNanophotonics at the DOE/SCNanoscale <strong>Science</strong> ResearchCenters: Nanoplasmonics—ContinuedCTu3N.7 • 18:15Temporal focusing generated via a height-staggeredmicrolens array can be used for wide-fieldoptical-sectioning microscopy, Jiun-Yann Yu 1 ,Daniel B. Holland 1 , Geoffrey A. Blake 1 , Chin-LinGuo 1 ; 1 California Institute of Technology, USA. Wetheoretically investigate the temporal-focusing effectgenerated by a microlens array with patternedheight differences among the microlenses, andshow how such an effect can be utilized for widefieldoptical-sectioning microscopy.18:30–20:30 Conference Reception and JTu4A • POSTER SESSION I: Nanophotonics, Lightwave Communications and Biophotonics,Exhibit HallNOTES__________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________________<strong>Tuesday</strong>, <strong>11</strong> <strong>June</strong>Concurrent sessions are grouped across four pages. Please review all four pages for complete session information.1272013<strong>CLEO</strong> <strong>Tuesday</strong>.indd 365/17/13 3:<strong>11</strong> PM
Exhibit Hall 3JOINT18:30–20:30JTu4A • POSTER SESSION I: Nanophotonics, Lightwave Communications and Biophotonics Poster Session<strong>Tuesday</strong>, <strong>11</strong> <strong>June</strong>JTu4A.01Single-notch Filter Based on a Compact AsymmetricMicrofiber Coupler, Xinliang Zhang 1 , LeiShi 1 , Ping Zhao 1 ; 1 Huazhong Univ of <strong>Science</strong> andTechnology, China. A novel single-notch filter isexperimentally demonstrated based on a compactasymmetric microfiber coupler. With an extinctionratio over 30 dB, a single narrow transmission dipin a wavelength range over 300 nm was obtained.JTu4A.02Watt-order direct green laser oscillation at522nm in Pr3+-doped waterproof fluoroaluminate-glassfiber, Jun Nakanishi 1 , TsuyoshiYamada 1 , Motoichiro Murakami 2 , Yasushi Fujimoto2 , Osamu Ishii 3 , Masaaki Yamazaki 3 ; 1 Nidek.co.,Ltd., Japan; 2 ILE Osaka Univ, Japan; 3 SumitaOptical Glass, Inc, Japan. We have demonstrateda high power green watt-order fiber-laser with aPr3+-doped waterproof fluoro-aluminate glassfiber. The maximum output power of the 522nmlaser beam was measured to be 1.53W.JTu4A.03Characterization of the DFB fiber laser resonatorstrength and α-parameter by response toexternal feedback, Geoffrey A. Cranch 1 , Gary A.Miller 1 , Joanne Harrison 2 , Scott Foster 2 ; 1 US NavalResearch Laboratory, USA; 2 Defence <strong>Science</strong> andTechnology Organisation, Australia. A method tocharacterize the linewidth enhancement factoror alpha-parameter of erbium doped fiber frommeasurements of the sensitivity to backreflectionof DFB fiber lasers with a range of known resonatorstrengths is presented.JTu4A.04400-Wavelength Raman Comb Lasing in aRing Cavity Based on Nonlinear PolarizationRotation, Weiqing Gao 1 , Meisong Liao 1 , DinghuanDeng 1 , Tonglei Cheng 1 , Takenobu Suzuki 1 ,Yasutake Ohishi 1 ; 1 Research Center for AdvancedPhoton Technology, Toyota Technological Institute,Japan. We demonstrate Raman comb lasing in aring cavity. The intensities of lines are equalizedby the nonlinear polarization rotation mechanism.More than 400-wavelength lasing with the signalnoiseratio higher than 10 dB is obtained.JTu4A.05Self-starting S-band mode-locked fiber ringlaser by polarization additive pulse modelocking,Ling-Gang Yang 1 , Siao-Shan Jyu 1 ,Chien-Hung Yeh 2 , Chi-Wai Chow 1 , Yinchieh Lai 1 ;1Photonics, Electro-Optical Engineering, NationalChiao Tung University, Taiwan; 2 Information andCommunications Research Laboratories, IndustrialTechnology Research Institute (ITRI), Taiwan. Wehave experimentally demonstrated a self-startingmode-locked fiber laser source operating at 1503nm with 9 nm output bandwidth. The modelockedlaser works stably with a pumping thresholdof 225 mW at 980 nm.JTu4A.06Comparison of timing noise properties ofcarbon nanotubes, graphene and grapheneoxide as saturable absorbers for a mode-lockedEr-doped fiber laser, Qijie Wang 1 , Xiaohui Li 1,3 ,Kan Wu 2 , Perry Ping Shum 2 , Yonggang Wang 3 ,Yishan Wang 3 ; 1 School of Electrical and ElectronicEngineering, Nanyang Technological University, Singapore;2 Centre for Disruptive Photonic Technologies,Nanyang Technological University, Singapore;3State Key Laboratory of Transient Optics andPhotonic, Xi’an Institute of Optics and PrecisionMechanics, Chinese Academy of <strong>Science</strong>s, China.We compare the timing noise properties of threemost typical carbon materials, i.e., single walledcarbon nanotubes, graphene and graphene oxideas saturable absorbers in a passively mode-lockedEr-doped fiber laser as a test platform.JTu4A.07Random lasing from capillary fiber, Ja-Hon Lin 1 ,Guo-Lun Hong 1 , Ying-Li Hsiao 1 , Cheng-Ling Lee 2 ;1National Taipei University of Technology, Taiwan;2National United University, Taiwan. Multiemissionpeaks with sub-nanometer spectrumbandwidth has been generated from dye dopedliquid crystal infilling capillary tube with axialpumping by the frequency doubling Q-switchedNd:YAG laser to demonstrate the random lasingbehavior.JTu4A.08Switchable Dual Wavelength Erbium-dopedFiber Laser in C- and L-band, Seungbin Ahn 1 ,Hyun-Joo Kim 1 , Young-Geun Han 1 ; 1 HanyangUniversity, Republic of Korea. We propose anovel scheme for a switchable dual wavelengtherbium-doped fiber laser based on a polarizationdependentsurface long-period grating. The lasingwavelength was switched in C- and L-band with aresponse time of 270 μs.JTu4A.09Experimental study on thermal profile ofgraphite filament and its effect on optical fiberfusion splicing, Donghui Zhao 1 , Samir Ghalmi 1 ,Giorgio Giaretta 1 , Jean-Michel Pelaprat 1 ; 1 VytranLLC, USA. By utilizing a novel high-temperaturemeasuring method, we investigated thermal profileof graphite filament for fiber fusion splicing. Theexperimental results indicate its excellent uniformitywith less than 6.42% temperature fluctuationover 1.5mm diameter area.JTu4A.10Generation and Amplification of Stable NanosecondPulses in a Thulium-doped FiberLaser, Jiang Liu 1 , Pu Wang 1 ; 1 Beijing University ofTechnology, China. We demonstrated that SESAMmode-locked thulium-doped fiber laser producedstable nanosecond pulses from 2.5ns to 12.5ns atrepetition rates between 1.72MHz and 258kHz.Average power of 5.6W at 1942nm was obtainedby two-stage all-fiber amplifiers.JTu4A.<strong>11</strong>Mid-infrared Fluorotellurite Glasses and Fibers,Huan Zhan 1 , Aidong Zhang 1 , Jianli He 1 , ZhiguangZhou 1 , Lu Li 1 , Aoxiang Lin 1 ; 1 Xi’an Inst of Opticsand Precision Mech, China. We report on thefabrication and characterization of rare earthions-doped water-free fluorotellurite glasses andfibers. For 2.8 mm glass fiber rods, its backgroundloss was ~12 dB/m in the range of 2.5~4.2 µm.JTu4A.12Generation of Polarizing Sections in HighlyBirefringent Photonic Crystal Fibers via Post-Processing, Priscila Romagnoli 1 , Claudecir R.Biazoli 2 , Marcos A. R. Franco 3 , Cristiano M. B.Cordeiro 2 , Christiano J. S. de Matos 1 ; 1 MackGrafe,Mackenzie Presbyterian University, Brazil; 2 Institutode Fisica “Gleb Wataghin”, Universidade Estadualde Campinas - UNICAMP, Brazil; 3 Laboratoriode Eletromagnetismo Computacional, Instituto deEstudos Avançados (IEAv), Brazil. The structureof a commercial highly birefringent PCF waslocally tapered to create a polarizing section. Apolarization-depended loss of at least 32.2 dB overa 1-cm length was induced in the 1550-nm region.JTu4A.13Coupling Light into Fiber Using Second OrderFiber Bragg Gratings, Nai-Hsiang Sun 1 , Chia-Ming Hu 1 , Jung-Sheng Chiang 1 , Wen-Fung Liu 2 ,Gary A. Evans 3 , Jerome K. Butler 3 ; 1 Department ofElectrical Engineering, I-Shou University, Taiwan;2Department of Electrical Engineering, Feng ChiaUniversity, Taiwan; 3 Department of ElectricalEngineering, Southern Methodist University, USA.Light is successfully coupled into the fiber by usingsecond-order FBGs. The measured power from thetwo ends of the FBGs are 10.715 nW and 10.233nW, respectively, with an input power of ~12 mW.JTu4A.14Arbitrary Triggerable and Wavelength TunablePs-source in the Visible Range with High OffbandRejection, Kristian Lauritsen 1 , ThomasSchoenau 1 , Thomas Eckhardt 1 , Romano Härtel 1 ,Philipp Kubina 1 , Torsten Siebert 1 , Rainer Erdmann1 ; 1 PicoQuant GmbH, Germany. A tunablecoherent ps-source is presented that covers thevisible range from 480 nm to 700 nm and featuresa 57 db out-of-band rejection and user-triggerablepulses in the 1 - 40 MHz repetition rate range.JTu4A.15Fabrication and Photoluminescence Propertyof the PbS-doped Silica Optical Fiber, JianxiangWen 1 ; 1 Shanghai University, China. A new techniqueof atomic layer deposition (ALD) has beenthe first introduced to fabricate PbS-doped silicafiber, whose optical properties are measured. Thefiber exhibits photoluminescence property in thewavelength range <strong>11</strong>00-<strong>11</strong>85 nm.JTu4A.16Soliton rains in normal dispersion Yb fiberlaser with dual-filter, Chengying Bao 1 , XiaoshengXiao 1 , Changxi Yang 1 ; 1 Tsinghua University,China. We report an observation of soliton rainsin normal dispersion Yb fiber laser. The cavity consistedof a narrow filter and a broad birefringentplate filter. Soliton rain was obtained in the weakmode-locking regime.JTu4A.17Broadband multipoint sensing with single-armfrequency-shifted interferometry, Yiwei Zhang 1 ,Fei Ye 1 , Bing Qi 1,2 , Hoi-Kwong Lo 1,2 , Li Qian 1 ;1Department of Electrical & Computer Engineering,University of Toronto, Canada; 2 Center for QuantumInformation and Quantum Control, Universityof Toronto, Canada. Using a broadband source,a slow detector, and a modulator, we proposeand demonstrate a single-arm frequency-shiftedinterferometer capable of sensing multiple weakreflections simultaneously in parallel and in seriesat 0.1-m spatial resolution.JTu4A.18Impact by fiber dispersion, nonlinearity, and saturableabsorption in short-cavity mode-lockedfiber lasers, Yuta Hasegawa 1 , Shinji Yamashita 1 ;1Dept. of Electrical Engineering and InformationSystems, The University of Tokyo, Japan. We numericallyinvestigate the temporal and spectral changeof optical pulses in short cavity mode-locked fiberlasers. We found that the shorter cavity length hasless impact by fiber dispersion and nonlinearity.JTu4A.19Dissipative Soliton Resonance in an Anomalous-Dispersion Figure-Eight Fiber Laser, Zhi-ChaoLuo 1 , Qiu-Yi Ning 1 , Hai-Lan Mo 1 , Shi-Ke Wang 1 ,Hu Cui 1 , Jin Liu 2 , Ai-Ping Luo 1 , Wen-Cheng Xu 1 ;1Laboratory of Nanophotonic Functional Materialsand Devices, South China Normal University,China; 2 South China Academy of Advanced Optoelectronics,South China Normal University, China.We report on the mode-locked rectangular pulseoperating in dissipative soliton resonance (DSR)region in an anomalous-dispersion figure-eightfiber laser. The results demonstrate that theformation of DSR pulse is independent of modelockingtechniques.JTu4A.20Generation of higher-order bound solitons in acarbon nanotube mode-locked fiber laser, XinZhao 1 , Qi Wang 1 , Zheng Gong 1 , Zheng Zheng 1 ;1School of Electronic and Information Engineering,Beihang University, China. Various bound statesconsisting of up to five solitons have been stablygenerated from a passively mode-locked fiberlaser for the first time, using a carbon nanotubemodelocker through intracavity gain/loss tuning.JTu4A.21Femtosecond CPA System operating at 1560nm Seeded by a Graphene Mode-Locked FiberLaser, Grzegorz J. Sobon 1 , Jaroslaw Sotor 1 ,Karol Krzempek 1 , Grzegorz Dudzik 1 , KrzysztofM. Abramski 1 ; 1 Laser & Fiber Electronics Group,Wroclaw University of Technology, Poland. Wedemonstrate a chirped pulse amplification setupseeded by a fiber laser mode-locked by graphenesaturable absorber. The system provides 1 W ofoutput power with 800 fs pulse duration at 1560nm wavelength.JTu4A.22Electrochemically exfoliated graphite nanosheetmode-locker for sub-picosecond L-bandfiber lasers, Chun-Yu Yang 1 , Yung-Hsiang Lin 1 ,Chung-Lun Wu 1 , Gong-Ru Lin 1 ; 1 National TaiwanUniversity, Taiwan. The electrochemically exfoliatedgraphite nano-sheets with diameter of 500nm and area density of 8300 #/mm 2 is employedto passively mode-lock the L-band fiber laser withpulsewidth of 850 fs and linewidth of 2.8 nm.JTu4A.23All-solid tellurite microstructured opticalfiber with one layer of high-index rods, TongleiCheng 1 , Zhongchao Duan 1 , Weiqing Gao 1 ,Meisong Liao 1 , Dinghuan Deng 1 , Takenobu Suzuki1 , Yasutake Ohishi 1 ; 1 ofmlab, Japan. A simpleall-solid tellurite microstructured optical fiberwhich has only one layer of high-index rods isproposed and fabricated. The core and claddingare made from the TZNL glass, and the high-indexrods are made from the TLWMN glass.128<strong>CLEO</strong>: 2013 • 9–14 <strong>June</strong> 20132013<strong>CLEO</strong> <strong>Tuesday</strong>.indd 375/17/13 3:<strong>11</strong> PM
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