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Target Density Effects on Charge Transfer of Laser-Accelerated Carbon Ions in Dense Plasma.
Ren, Jieru; Ma, Bubo; Liu, Lirong; Wei, Wenqing; Chen, Benzheng; Zhang, Shizheng; Xu, Hao; Hu, Zhongmin; Li, Fangfang; Wang, Xing; Yin, Shuai; Feng, Jianhua; Zhou, Xianming; Gao, Yifang; Li, Yuan; Shi, Xiaohua; Li, Jianxing; Ren, Xueguang; Xu, Zhongfeng; Deng, Zhigang; Qi, Wei; Wang, Shaoyi; Fan, Quanping; Cui, Bo; Wang, Weiwu; Yuan, Zongqiang; Teng, Jian; Wu, Yuchi; Cao, Zhurong; Zhao, Zongqing; Gu, Yuqiu; Cao, Leifeng; Zhu, Shaoping; Cheng, Rui; Lei, Yu; Wang, Zhao; Zhou, Zexian; Xiao, Guoqing; Zhao, Hongwei; Hoffmann, Dieter H H; Zhou, Weimin; Zhao, Yongtao.
Afiliación
  • Ren J; MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xi'an 710049, China.
  • Ma B; MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xi'an 710049, China.
  • Liu L; MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xi'an 710049, China.
  • Wei W; MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xi'an 710049, China.
  • Chen B; MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xi'an 710049, China.
  • Zhang S; MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xi'an 710049, China.
  • Xu H; MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xi'an 710049, China.
  • Hu Z; MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xi'an 710049, China.
  • Li F; MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xi'an 710049, China.
  • Wang X; MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xi'an 710049, China.
  • Yin S; MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xi'an 710049, China.
  • Feng J; MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xi'an 710049, China.
  • Zhou X; MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xi'an 710049, China.
  • Gao Y; MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xi'an 710049, China.
  • Li Y; MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xi'an 710049, China.
  • Shi X; MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xi'an 710049, China.
  • Li J; MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xi'an 710049, China.
  • Ren X; MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xi'an 710049, China.
  • Xu Z; MOE Key Laboratory for Nonequilibrium Synthesis and Modulation of Condensed Matter, School of Physics, Xi'an Jiaotong University, Xi'an 710049, China.
  • Deng Z; Science and Technology on Plasma Physics Laboratory, Laser Fusion Research Center, China Academy of Engineering Physics, Mianyang 621900, China.
  • Qi W; Science and Technology on Plasma Physics Laboratory, Laser Fusion Research Center, China Academy of Engineering Physics, Mianyang 621900, China.
  • Wang S; Science and Technology on Plasma Physics Laboratory, Laser Fusion Research Center, China Academy of Engineering Physics, Mianyang 621900, China.
  • Fan Q; Science and Technology on Plasma Physics Laboratory, Laser Fusion Research Center, China Academy of Engineering Physics, Mianyang 621900, China.
  • Cui B; Science and Technology on Plasma Physics Laboratory, Laser Fusion Research Center, China Academy of Engineering Physics, Mianyang 621900, China.
  • Wang W; Science and Technology on Plasma Physics Laboratory, Laser Fusion Research Center, China Academy of Engineering Physics, Mianyang 621900, China.
  • Yuan Z; Science and Technology on Plasma Physics Laboratory, Laser Fusion Research Center, China Academy of Engineering Physics, Mianyang 621900, China.
  • Teng J; Science and Technology on Plasma Physics Laboratory, Laser Fusion Research Center, China Academy of Engineering Physics, Mianyang 621900, China.
  • Wu Y; Science and Technology on Plasma Physics Laboratory, Laser Fusion Research Center, China Academy of Engineering Physics, Mianyang 621900, China.
  • Cao Z; Science and Technology on Plasma Physics Laboratory, Laser Fusion Research Center, China Academy of Engineering Physics, Mianyang 621900, China.
  • Zhao Z; Science and Technology on Plasma Physics Laboratory, Laser Fusion Research Center, China Academy of Engineering Physics, Mianyang 621900, China.
  • Gu Y; Science and Technology on Plasma Physics Laboratory, Laser Fusion Research Center, China Academy of Engineering Physics, Mianyang 621900, China.
  • Cao L; Advanced Materials Testing Technology Research Center, Shenzhen University of Technology, Shenzhen, 518118, China.
  • Zhu S; Science and Technology on Plasma Physics Laboratory, Laser Fusion Research Center, China Academy of Engineering Physics, Mianyang 621900, China.
  • Cheng R; Institute of Applied Physics and Computational Mathematics, Beijing 100094, China.
  • Lei Y; Graduate School, China Academy of Engineering Physics, Beijing 100088, China.
  • Wang Z; Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Zhou Z; Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Xiao G; Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Zhao H; Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Hoffmann DHH; Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
  • Zhou W; School of Nuclear Science and Technology, University of Chinese Academy Sciences, Beijing 101408, China.
  • Zhao Y; Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China.
Phys Rev Lett ; 130(9): 095101, 2023 Mar 03.
Article en En | MEDLINE | ID: mdl-36930918
We report on charge state measurements of laser-accelerated carbon ions in the energy range of several MeV penetrating a dense partially ionized plasma. The plasma was generated by irradiation of a foam target with laser-induced hohlraum radiation in the soft x-ray regime. We use the tricellulose acetate (C_{9}H_{16}O_{8}) foam of 2 mg/cm^{3} density and 1 mm interaction length as target material. This kind of plasma is advantageous for high-precision measurements, due to good uniformity and long lifetime compared to the ion pulse length and the interaction duration. We diagnose the plasma parameters to be T_{e}=17 eV and n_{e}=4×10^{20} cm^{-3}. We observe the average charge states passing through the plasma to be higher than those predicted by the commonly used semiempirical formula. Through solving the rate equations, we attribute the enhancement to the target density effects, which will increase the ionization rates on one hand and reduce the electron capture rates on the other hand. The underlying physics is actually the balancing of the lifetime of excited states versus the collisional frequency. In previous measurement with partially ionized plasma from gas discharge and z pinch to laser direct irradiation, no target density effects were ever demonstrated. For the first time, we are able to experimentally prove that target density effects start to play a significant role in plasma near the critical density of Nd-glass laser radiation. The finding is important for heavy ion beam driven high-energy-density physics and fast ignitions. The method provides a new approach to precisely address the beam-plasma interaction issues with high-intensity short-pulse lasers in dense plasma regimes.

Texto completo: 1 Colección: 01-internacional Banco de datos: MEDLINE Tipo de estudio: Prognostic_studies Idioma: En Revista: Phys Rev Lett Año: 2023 Tipo del documento: Article País de afiliación: China

Texto completo: 1 Colección: 01-internacional Banco de datos: MEDLINE Tipo de estudio: Prognostic_studies Idioma: En Revista: Phys Rev Lett Año: 2023 Tipo del documento: Article País de afiliación: China