• High Power Laser Science and Engineering
  • Vol. 6, Issue 3, 03000e41 (2018)
Xiaocong Peng1、2, Yuanan Zhao1、3, Yueliang Wang1、2、4, Zhen Cao1、2, Guohang Hu1, and Jianda Shao1
Author Affiliations
  • 1Laboratory of Thin Film Optics, Key Laboratory of Materials for High Power Laser, Shanghai Institute of Optics and Fine Mechanics, Chinese Academy of Sciences, Shanghai 201800, China
  • 2University of Chinese Academy of Sciences, Beijing 100049, China
  • 3State Key Laboratory of Applied Optics, Changchun Institute of Optics, Fine Mechanics and Physics, Chinese Academy of Sciences, Changchun 130033, China
  • 4National Engineering Laboratory for Modern Materials Surface Engineering Technology, Guangdong Institute of New Materials, Guangzhou 510650, China
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    DOI: 10.1017/hpl.2018.35 Cite this Article Set citation alerts
    Xiaocong Peng, Yuanan Zhao, Yueliang Wang, Zhen Cao, Guohang Hu, Jianda Shao. Variation of the band structure in DKDP crystal excited by intense sub-picosecond laser pulses[J]. High Power Laser Science and Engineering, 2018, 6(3): 03000e41 Copy Citation Text show less
    Representative OA Z-scan trace for the DKDP crystal at an excitation intensity of . The circular symbols represent the experimental data, while the solid line is the theoretical fitting result by the use of the 4PA theory. The inset is the 4PA coefficient of the DKDP crystal at different excitation laser intensities, while the error bars are the standard deviation from five Z-scan experiments.
    Fig. 1. Representative OA Z-scan trace for the DKDP crystal at an excitation intensity of . The circular symbols represent the experimental data, while the solid line is the theoretical fitting result by the use of the 4PA theory. The inset is the 4PA coefficient of the DKDP crystal at different excitation laser intensities, while the error bars are the standard deviation from five Z-scan experiments.
    Representative OA Z-scan trace for the DKDP crystal at the excitation intensity of . The circular symbols are the experimental data, while the solid (dotted) line is the theoretical fitting result by the use of the () PA theory (() PA theory).
    Fig. 2. Representative OA Z-scan trace for the DKDP crystal at the excitation intensity of . The circular symbols are the experimental data, while the solid (dotted) line is the theoretical fitting result by the use of the () PA theory (() PA theory).
    (a) The OA Z-scan traces for the DKDP crystal at the excitation intensity of . Squares, circles and triangles are the experimental data before excitation with , after excitation with and about 10 min after excitation with , respectively. The solid (dotted) line is the theoretical fitting result using the () PA theory (() PA theory). (b) The OA Z-scan traces for the DKDP crystal at . Squares and circles are the experimental data before excitation with and after excitation with , respectively. The solid line is the theoretical fitting result obtained using the () PA theory.
    Fig. 3. (a) The OA Z-scan traces for the DKDP crystal at the excitation intensity of . Squares, circles and triangles are the experimental data before excitation with , after excitation with and about 10 min after excitation with , respectively. The solid (dotted) line is the theoretical fitting result using the () PA theory (() PA theory). (b) The OA Z-scan traces for the DKDP crystal at . Squares and circles are the experimental data before excitation with and after excitation with , respectively. The solid line is the theoretical fitting result obtained using the () PA theory.
    Schematic illustration of the band structure. The solid arrows indicate the absorption of photons, whereas the dash-dotted arrows indicate the relaxation process. S1 and S2 are the states located in the band gap.
    Fig. 4. Schematic illustration of the band structure. The solid arrows indicate the absorption of photons, whereas the dash-dotted arrows indicate the relaxation process. S1 and S2 are the states located in the band gap.
    SymbolValueComment
    1PA cross section
    1PA cross section
    2PA cross section
    3PA cross section
    Table 1. Value of the parameters used in the fitting.
    Xiaocong Peng, Yuanan Zhao, Yueliang Wang, Zhen Cao, Guohang Hu, Jianda Shao. Variation of the band structure in DKDP crystal excited by intense sub-picosecond laser pulses[J]. High Power Laser Science and Engineering, 2018, 6(3): 03000e41
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