• Chinese Optics Letters
  • Vol. 14, Issue 9, 091402 (2016)
Boheng Lai1,2,3, Lizhi Dong1,2, Shanqiu Chen1,2, Guomao Tang1,2..., Wenjin Liu1,2, Shuai Wang1,2, Xing He1,2, Kangjian Yang1,2,3, Ping Yang1,2,*, Bing Xu1,2,**, Chao Wang4, Xianda Liu4, Qingsheng Pang4 and Yang Liu4|Show fewer author(s)
Author Affiliations
  • 1Key Laboratory on Adaptive Optics, Chinese Academy of Sciences, Chengdu 610209, China
  • 2Institute of Optics and Electronics, Chinese Academy of Sciences, Chengdu 610209, China
  • 3University of Chinese Academy of Sciences, Beijing 100049, China
  • 4Institute of North Optics and Electronic, Beijing 100015, China
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    DOI: 10.3788/COL201614.091402 Cite this Article Set citation alerts
    Boheng Lai, Lizhi Dong, Shanqiu Chen, Guomao Tang, Wenjin Liu, Shuai Wang, Xing He, Kangjian Yang, Ping Yang, Bing Xu, Chao Wang, Xianda Liu, Qingsheng Pang, Yang Liu, "Hybrid adaptive optics system for a solid-state zigzag master oscillator power amplifier laser system," Chin. Opt. Lett. 14, 091402 (2016) Copy Citation Text show less
    Schematic of the hybrid AO system for the MOPA laser system.
    Fig. 1. Schematic of the hybrid AO system for the MOPA laser system.
    (a) 59-actuator DM and (b) the multipurpose HS.
    Fig. 2. (a) 59-actuator DM and (b) the multipurpose HS.
    HS aperture and the actuator positions in the AO system.
    Fig. 3. HS aperture and the actuator positions in the AO system.
    Software interface of the wavefront processor.
    Fig. 4. Software interface of the wavefront processor.
    (a) Typical spots of the wavefront senor of the laser beam and (b) the wavefront of laser beam.
    Fig. 5. (a) Typical spots of the wavefront senor of the laser beam and (b) the wavefront of laser beam.
    (a) Typical spots of the wavefront senor of the laser beam when AO is on and (b) the wavefront of the laser beam.
    Fig. 6. (a) Typical spots of the wavefront senor of the laser beam when AO is on and (b) the wavefront of the laser beam.
    Near-field of the laser beam at full power.
    Fig. 7. Near-field of the laser beam at full power.
    (a) Far-field intensity distribution of the beam after the low-order compensator, β=7.3. (b) The far-field intensity distribution of the beam after being corrected by the DM; β=1.9. (c) The 3D figure of the far field of (a) and (b).
    Fig. 8. (a) Far-field intensity distribution of the beam after the low-order compensator, β=7.3. (b) The far-field intensity distribution of the beam after being corrected by the DM; β=1.9. (c) The 3D figure of the far field of (a) and (b).
    PIB of the beam before and after the DM is on.
    Fig. 9. PIB of the beam before and after the DM is on.
    β overall process of the laser’s operation after the hybrid AO system.
    Fig. 10. β overall process of the laser’s operation after the hybrid AO system.
    Boheng Lai, Lizhi Dong, Shanqiu Chen, Guomao Tang, Wenjin Liu, Shuai Wang, Xing He, Kangjian Yang, Ping Yang, Bing Xu, Chao Wang, Xianda Liu, Qingsheng Pang, Yang Liu, "Hybrid adaptive optics system for a solid-state zigzag master oscillator power amplifier laser system," Chin. Opt. Lett. 14, 091402 (2016)
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