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LIU Xiao-juan, FU Sheng-gui, HAN Ke-zhen, GE Xiao-lu. Recent progress in fiber yellow lasers[J]. LASER TECHNOLOGY, 2011, 35(2): 210-213. DOI: 10.3969/j.issn.1001-3806.2011.02.019
Citation: LIU Xiao-juan, FU Sheng-gui, HAN Ke-zhen, GE Xiao-lu. Recent progress in fiber yellow lasers[J]. LASER TECHNOLOGY, 2011, 35(2): 210-213. DOI: 10.3969/j.issn.1001-3806.2011.02.019

Recent progress in fiber yellow lasers

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  • Received Date: June 20, 2010
  • Revised Date: July 21, 2010
  • Published Date: March 24, 2011
  • Fiber yellow lasers are more compact and insensitive to alignment than their bulk laser counterparts.Because of the heat-dissipation characteristics of fibers and the excellent spatial mode characteristics,fiber yellow lasers are preferred candidates for various applications such as modern medicine,material processing,high-resolution spectroscopy,military applications and laser guided stars.Resent progress in fiber yellow lasers were reviewed.Key techniques and methods to realize fiber yellow lasers were analyzed and discussed.
  • [1]
    LI Ch Y,WANG Y G,HUANG L.Extra cavity 660nm SHG study of type-Ⅰ noncritical phase matched LBO crystal[J].Laser Technology,2003,27(5):428-430(in Chinese).
    [2]
    CAO H Zh,TAN H M,PENG H Y,et al.Laser diode end pumped Yb:YAG/LBO 537.8nm green laser[J].Laser Technology,2008,32(6):593-595(in Chinese).
    [3]
    WATANABE H,OMATSU T,TATEDA M.Efficient serf-pumped phase conjugation with a loop geometry in a Rhodamine-6G solid dye laser amplifier[J].Optics Express,2003,11 (2):176-180.
    [4]
    THOMAS V,ELIZEBETH A,THOMAS H.Studies on the growth and optical characterization of dysprosium praseodymium oxalate single crystals[J].Journal of Optoelectronics and Advanced Materials,2005,7 (5):2687-2692.
    [5]
    LIU B,ZHANG X Y,WANG Q P,et al.Diede-pomped intracavity frequency-doubled Nd:YVO4 self-Raman yellow laser[J].Acta Photoniea Sinica,2007,36(10):1777-1780(in Chinese).
    [6]
    HE Ch,CHYBA T H.Solid-state barium nitrate Raman laser in the visible region[J].Optics Commuications,1997,135 (4/6):273-278.
    [7]
    KAMINSKⅡ A A,McRAY C L,LEE H R,et al.High efficiency nanosecond Raman lasers based on tetragooul PbWO4 crystals[J].Optics Communications,2000,183 (1/4):277-287.
    [8]
    VESSELIN K,MALTE D,BARRY L D.Generation of tunable 589nm radiation as a Na guide star source using an optical parametric amplifier[J].optics Express,2009,17 (2):437-446.
    [9]
    LU Y F,XIE Sh Y,BO Y,et al.A high power quasi-continuouswave yellow laser based on intracavity sum-frequency generation[J].Aeta Physica Sinica,2009,58 (2):970-974 (in Chinese).
    [10]
    LU Y F,TAN H M,REN X Sh,et al.Laser diode pumped Nd:YVO4/LBO continuous wave orange-yellow laser with intracavity sum frequency mixing[J].Laser Technology,2005,29 (5):488-490(in Chinese).
    [11]
    GENG A C,BO Y,BO Y,et al.A 3W continuous-wave 589nm yellow laser based on the intracavity sum frequency generation in a V-shaped cavity[J].Acta Physiea Sinica,2006,55 (10):5227-5231(in Chinese).
    [12]
    ZHANG J Ch,WANG J X,SU P L,et al.Theoretical and experimental study of LD pumped Nd:YVO4 yellow laser with sum-frequency generation[J].Acta Optica Sinica,2008,28 (12):2365-2369 (in Chinese).
    [13]
    LIU T H,TAN H M,GAO L L,et al.lntracavity sum-frequency mixing with BIBO in 593nm laser[J].Acta Photonica Sinica,2007,36(7):1195-1197 (in Chinese).
    [14]
    SINHA S,LANGROCK C,DIGONNET M J F,et al.Efficient yellow-light generation by frequency doubling a narrow-linewidth 1150nm ytterbium fiber oscillator[J].Optics Letters,2006,31 (3):347-349.
    [15]
    DVOYRIN V V,MASHINSKY V M,MEDVEDKOV O I,et al.Yellow frequency-doubled serf-heated Yb fiber laser[C]//Conference on Lasers and Electro-Optics.California:Optical Society of America,2008:CWB5.
    [16]
    MARUYAMA H,SHIRAKAWA A,UEDA K I.1178nm all Yb-fiher laser source power-sealed by solid-core photonic bandgup fiber for 589nm generation[C]//Couference on Lasers and Electro-Optics.Munich,Germany:Optical Society of America,2009:CJ4_2.
    [17]
    DIANOV E M,SHUBIN A V,MELKUMOV M A,et al.,Highpower cw bismuth-fiber lasers[J].Journal of the Optical Society of America,2007,B24 (8):1749-1755.
    [18]
    PENNINGTON D M,DAWSON J W,DROBSHOFFA,et al.Compact fiber laser approach to 589nm laser guide stars[C]//Conference on Lasers and Electro-Opties.San Francisco,American:Optical Society of America,2004:CFD1.
    [19]
    GEORGIEV D,GAPONTSEV V P,DRONOV A G,et al.Wattslevel frequency doubling of a narrow line linearly polarized Raman fiber laser to 589nm[J].Optics Express,2005,13 (18):6772-6776.
    [20]
    RULKOV A B,POPOV S V,TAYLOR J R,et al.3W CW generation at 589nm with narrow line linearly polarized Raman fibre laser[C]//Advaneed Solid-State Photonics.Nevada,American:Optical Society of America,2006:MC4.
    [21]
    RULKOV A B,FERIN A A,POPOV S V,et al,Narrow-line,1178nm CW bismuth-doped fiber laser with 6.4W output for direct frequency doubling[J].Optics Express,2007,15 (9):5473-5476.
    [22]
    TAYLOR L,FRIEDENAUER A,PROTOPOPOV V,et al.20W at 589nm via frequency doubling of coherently beam combined 2MHz 1178nm CW signals amplified in Raman PM fiber amplifiers[C]//Conference on lasers and Electro-Optics.Munich,Germany:Opti-cal Society of America,2009:PDA_7.
    [23]
    TAYLOR L,FENGY,CALIA D B.High power narrowband 589nm frequency doubled fibre laser source[J].Optics Express,2009,17(17):14687-14693.
    [24]
    FENG Y,TAYLOR L R,CALIA D B.25W Raman-fiber-amplifier-based 589nm laser for laser guide star[J].Optics Express,2009,17(21):19021-19026.
    [25]
    TAYLOR L R,FENG Y,CALLA D B.50W CW visible laser source at 589nm obtained via frequency doubling of three coherently combined narrow-band Raman fiber amplifiers[J].Optics Express,2010,18 (8):8540-8555.
    [26]
    FENG Y,HACKENBERG W,CALLA D.Potential of fiber Raman laser in visible wavelength region[C]//Advanced Solid-State Photonics.Vancouver,Canada:Optical Society of America,2007:WB18.

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