• High Power Laser and Particle Beams
  • Vol. 35, Issue 6, 061003 (2023)
Tingting Sui1, Liening Wei2, Mingxia Xu2、*, Xinguang Xu2, Xun Sun2, and Xin Ju1、*
Author Affiliations
  • 1Department of Physics, University of Science and Technology Beijing, Beijing 100083, China
  • 2School of Crystal Materials, State Key Laboratory of Crystal Materials, Shandong University, Ji’nan 250100, China
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    DOI: 10.11884/HPLPB202335.220397 Cite this Article
    Tingting Sui, Liening Wei, Mingxia Xu, Xinguang Xu, Xun Sun, Xin Ju. Effects of Fe and its cluster defects on laser damage of KDP and ADP crystals using first-principles[J]. High Power Laser and Particle Beams, 2023, 35(6): 061003 Copy Citation Text show less
    Crystal structures of the pristine KDP (a) and ADP (b) as well as the crystals with FeP (c, d) defects
    Fig. 1. Crystal structures of the pristine KDP (a) and ADP (b) as well as the crystals with FeP (c, d) defects
    Schematic diagram of the structure for Fe replacing P atom
    Fig. 2. Schematic diagram of the structure for Fe replacing P atom
    Defect formation energies of the charged FeP defects in KDP and ADP as a function of Fermi energy with different magnetic states
    Fig. 3. Defect formation energies of the charged FeP defects in KDP and ADP as a function of Fermi energy with different magnetic states
    Micro-structural stress induced by various chemical bonds of FeP defect with different magnetic states in KDP and ADP crystals
    Fig. 4. Micro-structural stress induced by various chemical bonds of FeP defect with different magnetic states in KDP and ADP crystals
    Partial density of states of KDP and ADP crystals with charged FeP defects in different magnetic states, and the insets are electronic charge differences of charged FeP defects with different magnetic states
    Fig. 5. Partial density of states of KDP and ADP crystals with charged FeP defects in different magnetic states, and the insets are electronic charge differences of charged FeP defects with different magnetic states
    Imaginary part of the dielectric function ε2 (ω) of charged FeP defects with different magnetic states in KDP and ADP crystals
    Fig. 6. Imaginary part of the dielectric function ε2 (ω) of charged FeP defects with different magnetic states in KDP and ADP crystals
    locationdefect formation energy/eV
    FeH8.7
    FeP2.74
    FeK12.59
    Fei16.10
    Table 1. Defect formation energies of the KDP crystal with Fe in different locations
    defectdefect formation energy/eV
    KDPADP
    VOH8.560.15
    FeP+VOH24.3816.41
    Table 2. Defect formation energies of the KDP crystal with Fe atom in different locations
    defectsbond length of Fe−O/nm
    KDPADP
    pristine P-O0.1550.155
    NM FeP+0.1620.160
    NM FeP00.1630.162
    NM FeP0.1660.165
    NM FeP2−0.1700.169
    FM FeP+0.1620.160
    FM FeP00.1630.162
    FM FeP0.1660.165
    FM FeP2−0.1910.169
    AFM FeP+0.1620.161
    AFM FeP00.1630.162
    AFM FeP0.1660.165
    AFM FeP2−0.1700.169
    Table 3. Fe−O bond lengths in KDP and ADP with different magnetic states
    Tingting Sui, Liening Wei, Mingxia Xu, Xinguang Xu, Xun Sun, Xin Ju. Effects of Fe and its cluster defects on laser damage of KDP and ADP crystals using first-principles[J]. High Power Laser and Particle Beams, 2023, 35(6): 061003
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