• Chinese Optics Letters
  • Vol. 21, Issue 2, 023401 (2023)
Jinyu Cao1、2, Shuhui Li1、2, Yajun Tong3, Ming Tang1、2, Wenbin Li1、2、*, Qiushi Huang1、2, Huaidong Jiang3, and Zhanshan Wang1、2
Author Affiliations
  • 1MOE Key Laboratory of Advanced Micro-Structured Materials, Shanghai 200092, China
  • 2Institute of Precision Optical Engineering, School of Physics Science and Engineering, Tongji University, Shanghai 200092, China
  • 3Center for Transformative Science, ShanghaiTech University, Shanghai 201210, China
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    DOI: 10.3788/COL202321.023401 Cite this Article Set citation alerts
    Jinyu Cao, Shuhui Li, Yajun Tong, Ming Tang, Wenbin Li, Qiushi Huang, Huaidong Jiang, Zhanshan Wang. Damage resistance of B4C reflective mirror irradiated by X-ray free-electron laser[J]. Chinese Optics Letters, 2023, 21(2): 023401 Copy Citation Text show less
    Schematic of an XFEL beam incident on a B4C/Si-sub mirror under grazing incidence.
    Fig. 1. Schematic of an XFEL beam incident on a B4C/Si-sub mirror under grazing incidence.
    Absorbed energy fractions along the depth direction for B4C(50 nm)/Si-sub irradiated by XFEL at 1 keV and 12 keV with the grazing incidence angle of 2 mrad.
    Fig. 2. Absorbed energy fractions along the depth direction for B4C(50 nm)/Si-sub irradiated by XFEL at 1 keV and 12 keV with the grazing incidence angle of 2 mrad.
    Time-dependent depth distribution of enthalpy for B4C(50 nm)/Si-sub irradiated by XFEL at the fluence of (a) 1250 J/cm2 at 1 keV and (b) 2.4 × 105 J/cm2 at 12 keV. The grazing incidence angle is 2 mrad in both cases. The interface between B4C and Si-sub is marked by dashed gray lines, and the damage boundary is marked by solid white curves.
    Fig. 3. Time-dependent depth distribution of enthalpy for B4C(50 nm)/Si-sub irradiated by XFEL at the fluence of (a) 1250 J/cm2 at 1 keV and (b) 2.4 × 105 J/cm2 at 12 keV. The grazing incidence angle is 2 mrad in both cases. The interface between B4C and Si-sub is marked by dashed gray lines, and the damage boundary is marked by solid white curves.
    Absorbed energy fraction for B4C/Si-sub mirror with different B4C film thicknesses at the photon energy of 12 keV and the grazing incidence angle of 2 mrad.
    Fig. 4. Absorbed energy fraction for B4C/Si-sub mirror with different B4C film thicknesses at the photon energy of 12 keV and the grazing incidence angle of 2 mrad.
    Damage thresholds of B4C mirrors with different B4C film thicknesses (solid black squares) at 12 keV and the grazing angle of 2 mrad; reflectivity of B4C mirrors as a function of film thickness calculated with IMD software (blue line).
    Fig. 5. Damage thresholds of B4C mirrors with different B4C film thicknesses (solid black squares) at 12 keV and the grazing angle of 2 mrad; reflectivity of B4C mirrors as a function of film thickness calculated with IMD software (blue line).
    Damage threshold of the B4C(50 nm)/Si-sub mirror at different X-ray energies (solid blue squares). The theoretical reflectivity was calculated using IMD software (solid red line). The absorption K-edge of Si at 1.839 keV is indicated by a green dashed line.
    Fig. 6. Damage threshold of the B4C(50 nm)/Si-sub mirror at different X-ray energies (solid blue squares). The theoretical reflectivity was calculated using IMD software (solid red line). The absorption K-edge of Si at 1.839 keV is indicated by a green dashed line.
    Jinyu Cao, Shuhui Li, Yajun Tong, Ming Tang, Wenbin Li, Qiushi Huang, Huaidong Jiang, Zhanshan Wang. Damage resistance of B4C reflective mirror irradiated by X-ray free-electron laser[J]. Chinese Optics Letters, 2023, 21(2): 023401
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