Chinese Optics Letters, Volume. 22, Issue 2, 021402(2024)

High-power mode-programmable orbital angular momentum beam emitter with an internally sensed optical phased array

Jinhu Long1, Yu Deng1, Zhiqiang Gao1, Hongxiang Chang1, Qi Chang1, Yanxing Ma1, Jian Wu1, Rongtao Su1,2,3、*, Pengfei Ma1,2,3, and Pu Zhou1、**
Author Affiliations
  • 1College of Advanced Interdisciplinary Studies, National University of Defense Technology, Changsha 410073, China
  • 2Nanhu Laser Laboratory, National University of Defense Technology, Changsha 410073, China
  • 3Hunan Provincial Key Laboratory of High Energy Laser Technology, National University of Defense Technology, Changsha 410073, China
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    Figures & Tables(8)
    Geometric construction of the OPA for the OAM beam generation.
    Schematic drawing of the experiment setup. SL, seed laser; PA, pre-amplifier; FS, fiber splitter; PM, phase modulator; VDL, variable delay line; CFA, polarization-maintained cascaded fiber amplifier; CO, collimator; SP, small beam splitter; BE, beam expander; LC, liquid crystal; L, lens; PD, photodetector.
    Normalized PIB detected by the PD (a) open loop, (b) closed loop, and (c) their power spectral densities.
    Schematic drawing of observing the OAM beam emitting. HRM, high reflectivity mirror; L, lens; CCD, camera.
    Results of emitting the OAM beam when l = 0. (a) Phase structures of the OPA in the source plane, and the intensity distribution of the combined beam in the far field when the phase-sensing system was (b) turned off and (c) turned on.
    Results of emitting the OAM beam when l = −1, +1. (a1), (b1) Phase structures of the OPA in the source plane; (a2), (b2) accordingly experimental intensity distribution of OAM beams in the far field; (a3), (b3) accordingly theoretical intensity distribution; and (a4), (b4) phase distribution.
    Results of emitting the OAM beam when l = −2, −3. (a1), (b1) Phase structures of the OPA in the source plane; (a2), (b2) accordingly experimental intensity distribution of OAM beams in the far field; (a3), (b3) accordingly theoretical intensity distribution; and (a4), (b4) phase distribution.
    Results of presenting the OAM beam copier with l = −1. (a) Phase structures of the OPA in the source plane; (b) accordingly experimental intensity distribution of the OAM beam in the far field; (c) accordingly theoretical intensity distribution; and (d) phase distribution.
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    Jinhu Long, Yu Deng, Zhiqiang Gao, Hongxiang Chang, Qi Chang, Yanxing Ma, Jian Wu, Rongtao Su, Pengfei Ma, Pu Zhou, "High-power mode-programmable orbital angular momentum beam emitter with an internally sensed optical phased array," Chin. Opt. Lett. 22, 021402 (2024)

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    Paper Information

    Category: Lasers, Optical Amplifiers, and Laser Optics

    Received: Aug. 29, 2023

    Accepted: Oct. 12, 2023

    Posted: Oct. 12, 2023

    Published Online: Feb. 23, 2024

    The Author Email: Rongtao Su (surongtao@126.com), Pu Zhou (zhoupu203@163.com)

    DOI:10.3788/COL202422.021402

    CSTR:32184.14.COL202422.021402

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