• Matter and Radiation at Extremes
  • Vol. 9, Issue 2, 027601 (2024)
Chaoxin Chen1, Tao Gong1, Zhichao Li1, Liang Hao2..., Yonggang Liu1, Xiangming Liu1, Hang Zhao1, Yaoyuan Liu1, Kaiqiang Pan1, Qi Li1, Sanwei Li1, Zhijun Li1, Sai Jin1, Feng Wang1 and Dong Yang1|Show fewer author(s)
Author Affiliations
  • 1Laser Fusion Research Center, China Academy of Engineering Physics, Mianyang, Sichuan 621900, People’s Republic of China
  • 2Institute of Applied Physics and Computational Mathematics, Beijing 100094, People’s Republic of China
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    DOI: 10.1063/5.0173023 Cite this Article
    Chaoxin Chen, Tao Gong, Zhichao Li, Liang Hao, Yonggang Liu, Xiangming Liu, Hang Zhao, Yaoyuan Liu, Kaiqiang Pan, Qi Li, Sanwei Li, Zhijun Li, Sai Jin, Feng Wang, Dong Yang. Study of the spatial growth of stimulated Brillouin scattering in a gas-filled hohlraum via detecting the driven ion acoustic wave[J]. Matter and Radiation at Extremes, 2024, 9(2): 027601 Copy Citation Text show less

    Abstract

    In an experiment performed on the Shenguang-III prototype laser facility, collective Thomson scattering (TS) is used to study the spatial growth of stimulated Brillouin scattering (SBS) in a gas-filled hohlraum by detecting the SBS-driven ion acoustic wave. High-quality time-resolved SBS and TS spectra are obtained simultaneously in the experiment, and these are analyzed by a steady-state code based on the ray-tracing model. The analysis indicates that ion–ion collisions may play an important role in suppressing SBS growth in the Au plasma; as a result, the SBS excited in the filled gas region is dominant. In the early phase of the laser pulse, SBS originates primarily from the high-density plasma at the edges of the interaction beam channel, which is piled up by the heating of the interaction beam. Throughout the duration of the laser pulse, the presence of the TS probe beam might mitigate SBS by perturbing the density distribution around the region overlapping with the interaction beam.
    dlI0(l)=κ0I0I0dωsω0ωs(τ1+Γis),

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    lis(l,ωs)=κsis+Σ+I0(τ1+Γis).

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    Γ=kI2e2me2c22πksk0ω0Imχe(1+χi)ε,

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    χic=ZTeTiα21xi253xi4+i109kIλiixi3,kIλii0.1,ZTeTiα21xi21151xi4+i16251kIλiixi5+iπ2xiexi2/2,0.1<kIλii<10,ZTeTiα21xi23xi4+i851kIλiixi5+iπ2xiexi2/2,kIλii10,

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    δne(kI,ωI)=12kI2e2neme2c2ωpe2χe(1+χic)εa0as*.

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    ITS(kTS,ωTS)=Iprre2ΔΩVdVδne(kI,ωI)2×[Vδn̄e(kI,ωI)]2.

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    ωpe2ω02νeivg0fLfscI0r=κQ1rTerr,

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    Chaoxin Chen, Tao Gong, Zhichao Li, Liang Hao, Yonggang Liu, Xiangming Liu, Hang Zhao, Yaoyuan Liu, Kaiqiang Pan, Qi Li, Sanwei Li, Zhijun Li, Sai Jin, Feng Wang, Dong Yang. Study of the spatial growth of stimulated Brillouin scattering in a gas-filled hohlraum via detecting the driven ion acoustic wave[J]. Matter and Radiation at Extremes, 2024, 9(2): 027601
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