NUCLEAR TECHNIQUES, Volume. 47, Issue 7, 070201(2024)

Numerical analysis of X-ray free-electron laser interaction with metal ruthenium using the two-temperature model

Xue HAI1...2,3, Feifei ZHANG1,2, Ali WEN1, Yaru YIN3,4, Cuilan REN1,*, and Ping HUAI1,3,45,** |Show fewer author(s)
Author Affiliations
  • 1Shanghai Institute of Applied Physics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2University of Chinese Academy of Sciences, Beijing 100049, China
  • 3Center for Transformative Science, ShanghaiTech University, Shanghai 201210, China
  • 4(Shanghai High Repetition Rate XFEL and Extreme Light Facility (SHINE), ShanghaiTech University, Shanghai 201210, China)
  • 5Shanghai Synchrotron Radiation Facility, Shanghai Advanced Research Institute, Chinese Academy of Sciences, Shanghai 201204, China
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    Figures & Tables(8)
    Diagram of gaussian pulse light source (a) and interaction between laser pulse and materials (b) (color online)
    Temporal evolution of electron and lattice temperature of the front surface, middle part and back surface of ruthenium thin film (a), and the contour plots of lattice temperature (b) (color online)
    Evolution of electron pressure (a) and blast force (b) with time and space (color online)
    Temporal evolution of electron and lattice temperature (a) at the front surfaces of ruthenium thin film, and the maximum electron temperature and the temperature for the equilibrium (b) under different energy density (color online)
    Temporal evolution of electron and lattice temperature (a) at the front surfaces of ruthenium thin film, and the maximum electron temperature and the temperature for the equilibrium (b) under different pulse durations (color online)
    Temporal evolution of electron and lattice temperature (a) at the front surfaces of ruthenium thin film, and the maximum electron temperature and the temperature for the equilibrium (b) under different pulse durations (color online)
    Temporal evolution of electron and lattice temperature (a) at the front surface of ruthenium thin film, and the relationship between the time of electron-lattice equilibrium and its electron-phonon coupling coefficient under different electro-phonon coupling coefficient (b) (shaded area represents trend range) (color online)
    • Table 1. Model parameters and the related physical parameters of the metal Ru

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      Table 1. Model parameters and the related physical parameters of the metal Ru

      参数Parameters

      数值

      Value

      参考文献

      Reference

      薄膜厚度Film thickness,Lx / nm50
      脉冲宽度Pulse duration,τL / ps0.2
      吸收能量密度Absorbed fluence,Fabs / Jm-2403.43
      熔点Melting point,Tmelt / K2 527[33]
      电子热容系数Electron-specific heat constant,γ / Jm-3∙K-2400[26]
      电声子耦合系数Electron-phonon coupling factor,gei / W∙m-3∙K-118.5×1017[34]
      电子热导率Equilibrium thermal conductivity,κe / W∙m-1∙K-1117[35]
      晶格热容Lattice heat capacity,Cl / Jmol-1∙K-124.861[36]
      电子平均自由程Electron mean free path,λ / nm6.59[37]
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    Xue HAI, Feifei ZHANG, Ali WEN, Yaru YIN, Cuilan REN, Ping HUAI. Numerical analysis of X-ray free-electron laser interaction with metal ruthenium using the two-temperature model[J]. NUCLEAR TECHNIQUES, 2024, 47(7): 070201

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    Paper Information

    Category: Research Articles

    Received: Mar. 11, 2024

    Accepted: --

    Published Online: Aug. 27, 2024

    The Author Email: REN Cuilan (任翠兰), HUAI Ping (怀平)

    DOI:10.11889/j.0253-3219.2024.hjs.47.070201

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