Volume 47 Issue 1
Jan.  2018
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Shen Hui, Quan Zhao, Yang Yifeng, Zhao Xiang, Bai Gang, He Bing, Zhou Jun. Polarization control of combined laser beams based on optical homodyne polarization detection and phase locking[J]. Infrared and Laser Engineering, 2018, 47(1): 103007-0103007(6). doi: 10.3788/IRLA201746.0103007
Citation: Shen Hui, Quan Zhao, Yang Yifeng, Zhao Xiang, Bai Gang, He Bing, Zhou Jun. Polarization control of combined laser beams based on optical homodyne polarization detection and phase locking[J]. Infrared and Laser Engineering, 2018, 47(1): 103007-0103007(6). doi: 10.3788/IRLA201746.0103007

Polarization control of combined laser beams based on optical homodyne polarization detection and phase locking

doi: 10.3788/IRLA201746.0103007
  • Received Date: 2017-06-10
  • Rev Recd Date: 2017-08-20
  • Publish Date: 2018-01-25
  • As a critical technique for increasing the brightness of narrow-linewidth fiber lasers, coherent polarization beam combining can achieve common aperture joining of multiple lasers, while maintaining higher beam quality and linear polarization state. A polarization control system of combined lasers was investigated based on the linear phase locking technique. A physical model for optical homodyne polarization detection and a mathematical equation for linear phase-locking loop were established and analyzed in detail. The polarization phase of combined lasers was checked by employing high-precision optical homodyne method and then fed back to phase lock lasers in real time. A linear polarization laser was output with the power of 279 mW. After phase locking, the polarization extinction ratio of combined lasers attained 19.3 dB and the control bandwidth was 39.6 kHz. The residual phase noise is 710-4 rad/Hz(1 Hz) and 310-4 rad/Hz. When the power was increased to 1 W, the polarization extinction ratio was -15 dB, which was restricted by power-induced phase noise and spatial mismatch of beam spots.
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    [2] An Haixia, Deng Kun, Bi Zhiyue. Miniaturization and lightweight technology of high-power laser equipment[J]. Chinese Optics, 2017, 10(3):321-330. (in Chinese)安海霞, 邓坤, 闭治跃. 高功率激光装备小型化轻量化技术[J]. 中国光学, 2017, 10(3):321-330.
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    [4] Wang Huisheng, Liu Yang. Phase-locking of two fiber lasers based on a beam splitter[J]. Optics and Precision Engineering, 2009, 17(8):1845-1850. (in Chinese)王会升, 刘洋. 基于分束镜的两路光纤激光器相干合成研究[J]. 光学精密工程, 2009, 17(8):1845-1850.
    [5] Lou Qihong, He Bing, Zhou Jun. Fiber lasers and its coherent beam combination[J]. Infrared and Laser Engineering, 2007, 36(2):155-159. (in Chinese)楼祺洪, 何兵, 周军. 光纤激光器及其相干组束[J]. 红外与激光工程, 2007, 36(2):155-159.
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Polarization control of combined laser beams based on optical homodyne polarization detection and phase locking

doi: 10.3788/IRLA201746.0103007
  • 1. Shanghai Key Laboratory of All Solid-State Laser and Applied Techniques,Shanghai Institute of Optics and Fine Mechanics,Chinese Academy of Sciences,Shanghai 201800,China;
  • 2. University of Chinese Academy of Sciences,Beijing 100049,China

Abstract: As a critical technique for increasing the brightness of narrow-linewidth fiber lasers, coherent polarization beam combining can achieve common aperture joining of multiple lasers, while maintaining higher beam quality and linear polarization state. A polarization control system of combined lasers was investigated based on the linear phase locking technique. A physical model for optical homodyne polarization detection and a mathematical equation for linear phase-locking loop were established and analyzed in detail. The polarization phase of combined lasers was checked by employing high-precision optical homodyne method and then fed back to phase lock lasers in real time. A linear polarization laser was output with the power of 279 mW. After phase locking, the polarization extinction ratio of combined lasers attained 19.3 dB and the control bandwidth was 39.6 kHz. The residual phase noise is 710-4 rad/Hz(1 Hz) and 310-4 rad/Hz. When the power was increased to 1 W, the polarization extinction ratio was -15 dB, which was restricted by power-induced phase noise and spatial mismatch of beam spots.

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