• Chinese Optics Letters
  • Vol. 22, Issue 5, 051401 (2024)
Yi Yu1,2,3, Jiayu Yi3, Liu Xu3, Jianli Shang3..., Jing Wu3, Lixin Tong3,*, Qingsong Gao3, Chun Tang3, Wei Zhang3 and Lei Chen1|Show fewer author(s)
Author Affiliations
  • 1Department of Optical Engineering, Nanjing University of Science and Technology, Nanjing 210094, China
  • 2Graduate School of China Academy of Engineering Physics, Beijing 100193, China
  • 3Institute of Applied Electronics, China Academy of Engineering Physics, Mianyang 621900, China
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    DOI: 10.3788/COL202422.051401 Cite this Article Set citation alerts
    Yi Yu, Jiayu Yi, Liu Xu, Jianli Shang, Jing Wu, Lixin Tong, Qingsong Gao, Chun Tang, Wei Zhang, Lei Chen, "Large aperture disk standing-wave unstable resonator with intra-cavity adaptive correction," Chin. Opt. Lett. 22, 051401 (2024) Copy Citation Text show less
    Experimental setup of the disk standing-wave unstable resonator.
    Fig. 1. Experimental setup of the disk standing-wave unstable resonator.
    Schematic of the disk gain module.
    Fig. 2. Schematic of the disk gain module.
    Photo of the composite ceramic disk.
    Fig. 3. Photo of the composite ceramic disk.
    Small signal gain coefficient versus pulse peak pumping power.
    Fig. 4. Small signal gain coefficient versus pulse peak pumping power.
    Logical diagram of synergic controlling process.
    Fig. 5. Logical diagram of synergic controlling process.
    Average output power versus time.
    Fig. 6. Average output power versus time.
    (a) The RTWF after tilt and defocus correction (the corresponding profiles of the near field and far field are shown in the insets). (b) The RTWF after tilt, defocus, and high order aberrations correction (the corresponding profiles of the near field and far field are shown in the insets).
    Fig. 7. (a) The RTWF after tilt and defocus correction (the corresponding profiles of the near field and far field are shown in the insets). (b) The RTWF after tilt, defocus, and high order aberrations correction (the corresponding profiles of the near field and far field are shown in the insets).
    The RMS value of the RTWF versus iterations.
    Fig. 8. The RMS value of the RTWF versus iterations.
    (a) The output power versus total input power. The inset (b) shows the oscilloscope trace of a single pulse.
    Fig. 9. (a) The output power versus total input power. The inset (b) shows the oscilloscope trace of a single pulse.
    Devices Correction RangeControl Bandwith
    M4Tilt±10 mrad10 Hz
    DM1Defocus20 µm10 Hz
    DM2PV8 µm50 Hz
    RMS1 µm
    Table 1. Compensating Capabilities of Correcting
    Yi Yu, Jiayu Yi, Liu Xu, Jianli Shang, Jing Wu, Lixin Tong, Qingsong Gao, Chun Tang, Wei Zhang, Lei Chen, "Large aperture disk standing-wave unstable resonator with intra-cavity adaptive correction," Chin. Opt. Lett. 22, 051401 (2024)
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