Volume 42 Issue 8
Feb.  2014
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Tao Mengmeng, Huang Qijie, Yu Ting, Yang Pengling, Chen Weibiao, Ye Xisheng. LD clad-pumped high efficient Tm-doped fiber lasers with different laser cavities[J]. Infrared and Laser Engineering, 2013, 42(8): 2008-2011.
Citation: Tao Mengmeng, Huang Qijie, Yu Ting, Yang Pengling, Chen Weibiao, Ye Xisheng. LD clad-pumped high efficient Tm-doped fiber lasers with different laser cavities[J]. Infrared and Laser Engineering, 2013, 42(8): 2008-2011.

LD clad-pumped high efficient Tm-doped fiber lasers with different laser cavities

  • Received Date: 2012-12-15
  • Rev Recd Date: 2013-01-03
  • Publish Date: 2013-08-25
  • LD clad-pumped high efficient Tm-doped fiber lasers with quantum efficiencies beyond the Stokes Limit were reported. Different laser cavities, including dichroic mirror with fiber end reflection, high reflective fiber Bragg grating(FBG) with fiber end reflection and dichroic mirror with low reflective FBG, were studied. A maximum slope efficiency of 56.9% was obtained with the dichroic mirror and the fiber end flection forming the laser cavity, corresponding to a quantum efficiency of 142%. Spectral linewidth of the laser output was closely related to the reflective mirrors used in different cavities. Selected by the broadband dichroic mirror, the laser resonated randomly with the high reflective band of the dichroic mirror. With an FBG as the high reflective mirror of the laser cavity, narrow linewidth of 38 pm was attained at an output of 1 W. In another laser configuration, one low reflective FBG was exploited as the output coupler, and narrow linewidth of 69 pm was achieved at an output of 0.9 W. And the laser linewidth was limited by the reflection bandwidth of the FBG used.
  • [1] Lou Qihong. Recent progress of laser technology and its application in solar cell research[J]. Infrared and Laser Engineering, 2012, 41(12):3187-3192. (in Chinese)楼祺洪. 激光技术新进展及其在光伏产业中的应用[J]. 红外与激光工程, 2012, 41(12): 3187-3192.
    [2] Li Jianfeng, Ou Zhonghua, Dai Zhiyong, et al. Theoretical analysis and design of mid-infrared ZBLAN fiber Raman laser[J]. Infrared and Laser Engineering, 2011, 40(8): 1432-1437. (in Chinese)李剑锋, 欧中华, 代志勇, 等. 中红外ZBLAN光纤拉曼激光器的理论分析与设计[J]. 红外与激光工程, 2011, 40(8): 1432-1437.
    [3] Szlauer R, Gostchl R, Razmaria A, et al. Endoscopic vaporesection of the prostate using the continuous-wave 2μm thulium laser: outcome and demonstration of the surgical technique[J]. Eur Urol, 2009, 55: 368-375.
    [4] Lippert E, Nicolas S, Arisholm G, et al. Midinfrared laser source with high power and beam quality[J]. App Optics, 2006, 45: 3839-3845.
    [5] Jackson S D. Cross relaxation and energy transfer upconversion process relevant to the functioning of 2μm Tm-doped silica fiber lasers[J]. Opt Commun, 2004, 230: 197-203.
    [6] McComb T S, Richardson M C, Bass M. High-power Fiber Lasers and Amplifiers[M]. New York: McGraw-Hill, 2010, 25.
    [7] Wang Yuezhu, Zhang Yunjun, Yao Baoquan, et al. Cladding-pumped Tm-doped large-mode-area fiber laser highly efficient output at approximately 2 μm[J]. Chin Phys Lett, 2006, 23(9): 2450-2451.
    [8] Tang Yulong, Xu Jianqiu, Chen Wei, et al. 150-W Tm-doped fiber lasers with different cooling techniques and output couplings[J]. Chin Phys Lett, 2010, 27(10): 104207.
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    [10] Zhang Yunjun, Yao Baoquan, Ju Youlun. et al. LD-cladding-pumped 50pm linewidth Tm-doped silica fiber laser[J]. Opt Express, 2008, 16(11): 7715-7719.
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    [12] Geng Jihong, Wang Qing, Luo Tao, et al. Single-frequency narrow-linewidth Tm-doped fiber laser using silicate glass fiber[J]. Opt Express, 2009, 34(22): 3493-3495.
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LD clad-pumped high efficient Tm-doped fiber lasers with different laser cavities

  • 1. State Key Laboratory of Laser Interaction with Matter,Northwest Institute of Nuclear Technology,Xi'an 710024,China;
  • 2. Research Center of Space Laser Information Technology,Shanghai Institute of Optics and Fine Mechanics,Chinese Academy of Sciences,Shanghai 201800,China

Abstract: LD clad-pumped high efficient Tm-doped fiber lasers with quantum efficiencies beyond the Stokes Limit were reported. Different laser cavities, including dichroic mirror with fiber end reflection, high reflective fiber Bragg grating(FBG) with fiber end reflection and dichroic mirror with low reflective FBG, were studied. A maximum slope efficiency of 56.9% was obtained with the dichroic mirror and the fiber end flection forming the laser cavity, corresponding to a quantum efficiency of 142%. Spectral linewidth of the laser output was closely related to the reflective mirrors used in different cavities. Selected by the broadband dichroic mirror, the laser resonated randomly with the high reflective band of the dichroic mirror. With an FBG as the high reflective mirror of the laser cavity, narrow linewidth of 38 pm was attained at an output of 1 W. In another laser configuration, one low reflective FBG was exploited as the output coupler, and narrow linewidth of 69 pm was achieved at an output of 0.9 W. And the laser linewidth was limited by the reflection bandwidth of the FBG used.

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