• Chinese Optics Letters
  • Vol. 22, Issue 2, 021402 (2024)
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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    DOI: 10.3788/COL202422.021402 Cite this Article Set citation alerts
    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[J]. Chinese Optics Letters, 2024, 22(2): 021402 Copy Citation Text show less
    Geometric construction of the OPA for the OAM beam generation.
    Fig. 1. 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.
    Fig. 2. 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.
    Fig. 3. 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.
    Fig. 4. 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.
    Fig. 5. 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.
    Fig. 6. 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.
    Fig. 7. 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.
    Fig. 8. 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.
    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[J]. Chinese Optics Letters, 2024, 22(2): 021402
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