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Acta Optica Sinica, Volume. 38, Issue 5, 0514004(2018)

Three-Dimensional Inversion Method for High Power Laser Multi-Pass Amplifier

Xianghe Guan1,2, Yanli Zhang1, Junyong Zhang1, and Jianqiang Zhu1、*
Author Affiliations
  • 1 Key Laboratory of High Power Laser and Physics, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2 University of Chinese Academy of Sciences, Beijing 100049, China
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    AbstractGet PDF(in Chinese)
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    Spatial and temporal distributions of normalized intensity of input pulse (method one). (a) Time waveforms at different coordinate points; (b) one-dimensional spatial distribution at different time

    Fig. 1. Spatial and temporal distributions of normalized intensity of input pulse (method one). (a) Time waveforms at different coordinate points; (b) one-dimensional spatial distribution at different time

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    Three-dimensional intensity distribution of input pulse (method one)

    Fig. 2. Three-dimensional intensity distribution of input pulse (method one)

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    Spatial and temporal distributions of normalized intensity of output pulse (method one). (a) Time waveforms at different coordinate points; (b) one-dimensional spatial distribution at different time

    Fig. 3. Spatial and temporal distributions of normalized intensity of output pulse (method one). (a) Time waveforms at different coordinate points; (b) one-dimensional spatial distribution at different time

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    Distributions of (a) normalized power waveforms and (b) normalized one-dimensional flux density of output pulse (method one)

    Fig. 4. Distributions of (a) normalized power waveforms and (b) normalized one-dimensional flux density of output pulse (method one)

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    Relative deviation of output pulse (method one)

    Fig. 5. Relative deviation of output pulse (method one)

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    Spatial and temporal distributions of normalized intensity of input pulse (method two). (a) Time waveforms at different coordinate points; (b) one-dimensional spatial distribution at different time

    Fig. 6. Spatial and temporal distributions of normalized intensity of input pulse (method two). (a) Time waveforms at different coordinate points; (b) one-dimensional spatial distribution at different time

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    Three-dimensional intensity distribution of input pulse (method two)

    Fig. 7. Three-dimensional intensity distribution of input pulse (method two)

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    Spatial and temporal distributions of normalized intensity of output pulse (method two). (a) Time waveforms at different coordinate points; (b) one-dimensional spatial distribution at different time

    Fig. 8. Spatial and temporal distributions of normalized intensity of output pulse (method two). (a) Time waveforms at different coordinate points; (b) one-dimensional spatial distribution at different time

    Download full size
    Distributions of (a) normalized power waveforms and (b) normalized one-dimensional flux density of output pulse (method two)

    Fig. 9. Distributions of (a) normalized power waveforms and (b) normalized one-dimensional flux density of output pulse (method two)

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    Relative deviation of output pulse (method two)

    Fig. 10. Relative deviation of output pulse (method two)

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    Xianghe Guan, Yanli Zhang, Junyong Zhang, Jianqiang Zhu. Three-Dimensional Inversion Method for High Power Laser Multi-Pass Amplifier[J]. Acta Optica Sinica, 2018, 38(5): 0514004

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    Paper Information

    Category: Lasers and Laser Optics

    Received: Nov. 14, 2017

    Accepted: --

    Published Online: Jul. 10, 2018

    The Author Email: Zhu Jianqiang (jqzhu@siom.shc)

    DOI:10.3788/AOS201838.0514004

    Topics

    laser devices and laser physics
    Lasers and Laser Optics
    Laser physics
    laser manufacturing
    Instrumentation, Measurement and Metrology