High Power Laser and Particle Beams, Volume. 34, Issue 8, 081002(2022)
Research progress on laser-induced damage mechanism and threshold improvement of pulse compression gratings
Fig. 3. Grating damage morphology and electric field distribution caused by nodular defects at different positions of s-polarized Ti:Sapphire laser with an incident angle of 65° and a pulse duration of 32 fs[41]
Fig. 4. Damage evolution of grating film under irradiation of 120 fs, 796 nm, 10 Hz laser[40]. (a)(d) nano bumps; (b)(e) surface roughness; (c) nano cracks; (f) film falling off
Fig. 6. Grating damage morphologies of Ti: Sapphire laser with different laser injection energy and film deposition methods at a frequency of 1 kHz and a pulse duration of 60 fs[50]
Fig. 7. Damage morphology of ACG prepared by electron beam evaporation with Ti: Sapphire laser at frequency 1 kHz and pulse duration 60 fs[51]
Fig. 8. Changes of LIDT of SiO2 sol-gel film with pollution time[63]
Fig. 9. Damage morphologies of MMDG with 1.48 J/cm2 of particulate pollutants at pulse duration of 8.6 ps[64]
Fig. 11. Laser-induced damage thresholds of HfO2 films at annealing temperatures of 353 K, 423 K, 503 K and 573 K[65]
Fig. 13. Damage state of Ti: Sapphire laser in the state of single-pulse and double-pulse radiation at a frequency of 10 Hz and a pulse duration of 35 fs[70]
Fig. 15. Damage probability of introduced gas under vacuum and different pressures[80]
Fig. 16. Scientific and technical issues in the research on laser-induced damage of pulse-compressed gratings
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Qingshun Bai, Hao Sun, Yuhai Li, Peng Zhang, Yunlong Du. Research progress on laser-induced damage mechanism and threshold improvement of pulse compression gratings[J]. High Power Laser and Particle Beams, 2022, 34(8): 081002
Category: High Power Laser Physics and Technology?Overview
Received: Jul. 6, 2021
Accepted: May. 24, 2022
Published Online: Aug. 8, 2022
The Author Email: Qingshun Bai (Qshbai@hit.edu.cn)