Chinese Journal of Lasers, Volume. 51, Issue 11, 1101028(2024)
Intertwined Development of Near-Infrared High-Power Lasers and Reflective Holographic Surface-Relief Diffraction Gratings
Fig. 1. Overview of power climb in intense laser technology. (a) Power milestone for ultra-intense ultra-short lasers and high-energy continuous wave lasers; (b) mechanism of chirped-pulse amplification (CPA); (c) mechanism of spectral beam combining (SBC)
Fig. 2. Performance indicators of reflection pulse compression gratings for different high-power laser systems
Fig. 3. Classification of diffraction gratings commonly used in high-power laser system
Fig. 5. Numerical simulation of groove profile of gold grating. (a) Common functions such as sine, gauss, moth-eye; (b) image to curve; (c) characteristic profile function
Fig. 8. Relationship between diffraction efficiency of gold grating and polarization of TM and TE, and relationship between diffraction efficiency of gold grating and groove depth at different linear densities. (a)‒(b) Relationship between diffraction efficiency of gold grating and polarization of TM and TE; (c)‒(d) relationship between diffraction efficiency of gold grating and groove depth at different linear densities[48]
Fig. 9. 400 nm ultra-broadband gold grating[58]. (a) Measured -1 order diffraction efficiency of 1443 g/mm at 50° (red line) and 1527 g/mm (blue line) at 62°, both with TM polarization, and an ultra-broadband gold grating is shown in the inset pictures; (b) grating profiles are measured by atomic force microscope (AFM) and focused ion beam-scanning electron microscope (FIB-SEM); (c) scanning photometric diffraction efficiency map at 950 nm
Fig. 10. Threshold rule of gold film and gold grating under 1053 nm pulsed laser radiation[48]
Fig. 12. Typical damage morphologies of gold gratings fabricated by e-beam evaporation and magnetron sputtering.[55] (a) E-beam evaporation; (b) magnetron sputtering
Fig. 13. Pulse-width dependence of LIDT of a 1480 g/mm gold grating with a gold thickness of 200 nm, test wavelength is 1053 nm, and test angle is 52°[60]
Fig. 14. Typical damage morphologies of gold gratings with (a) pulse width of 60 fs and (b) pulse width of 450 ps
Fig. 15. Damage-test table in the front end for the station of extreme light (SEL)[58]. (a) Damage test platform layout; (b) measured and FTL pulse duration of the compressed laser pulse in S1; (c) measured spectrum in S1 and S2; (d) measured beam spot in S2
Fig. 16. Changes in height, LIDT, and morphology of gold gratings with the number of pulses. (a) Change in the height of the blister with number of pulses; (b) evolution of LIDT versus number of pulses; (c)‒(i) SEM images of blisters with different numbers of pulses near the LIDT; (j) a FIB cross-section picture of figure (d)
Fig. 17. Damage probability curve (red line and solid diamond) and temperature rise (circle) at 100 kHz repetition frequency[65]. Color of circles represents different irradiation time, and values in color circles are measured temperature rise
Fig. 18. Mixed metal grating photographs and 1-on-1 damage threshold. (a) Photographs of mixed metal grating; (b) 1-on-1 damage threshold
Fig. 19. Domestic and foreign representative of high-quality SBC grating products
Fig. 21. Thermal response detection of SBC grating, including temperature rise test, diffracted light far-field beam quality, and grating surface thermal distortion. The pump light is a high-energy beam laser, and the probe laser is used to form interference fringes based on Michelson interferometry for real-time detection of grating surface aberrations
Fig. 22. Evolution mechanism from temperature rise and thermal distortion to catastrophic damage of a SBC grating. (a) Temperature rise; (b) thermal stress damage; (c) blister; (d) wavefront distortion; (e) beam quality degradation; (f) catastrophic damage
Fig. 23. Influence of different cleaning processes on elemental content, diffraction efficiency, surface roughness, and temperature rise performance of spectral beam combining gratings. (a) Elemental content; (b) surface roughness; (c) diffraction efficiency; (d) temperature rise performance
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Yunxia Jin, Yuxing Han, Hongchao Cao, Fanyu Kong, Jianda Shao. Intertwined Development of Near-Infrared High-Power Lasers and Reflective Holographic Surface-Relief Diffraction Gratings[J]. Chinese Journal of Lasers, 2024, 51(11): 1101028
Category: laser devices and laser physics
Received: Feb. 15, 2024
Accepted: Apr. 22, 2024
Published Online: Jun. 10, 2024
The Author Email: Jin Yunxia (yxjin@siom.ac.cn)
CSTR:32183.14.CJL240593