High Power Laser Science and Engineering, Volume. 6, Issue 3, 03000e41(2018)
Variation of the band structure in DKDP crystal excited by intense sub-picosecond laser pulses
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.
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).
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.
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.
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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
Category: Research Articles
Received: Feb. 4, 2018
Accepted: May. 14, 2018
Published Online: Aug. 28, 2018
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