[1] Wu M T, Guo B, Zhao Q L. Laser machining micro-structures on diamond surface with a sub-nanosecond pulsed laser[J]. Applied Physics A, 124, 170(2018).

[2] Pavel N, Dascalu T, Salamu G et al. Ignition of an automobile engine by high-peak power Nd∶YAG/Cr4+∶YAG laser-spark devices[J]. Optics Express, 23, 33028-33037(2015).

[3] Zhao X. Experimental investigation of all-solid-state high repetition frequency sub-nanosecond pulsed laser and its application in all-optical photoacoustic imaging[D], 55-72(2020).

[4] Ma Z H, Ding N, Li Z et al. Spectral interference contrast based non-contact photoacoustic microscopy realized by SDOCT[J]. Optics Letters, 47, 2895-2898(2022).

[5] Li G Y, Zhou Q, Xu G Q et al. Lidar-radar for underwater target detection using a modulated sub-nanosecond Q-switched laser[J]. Optics & Laser Technology, 142, 107234(2021).

[6] Li Z P, Ye J T, Huang X et al. Single-photon imaging over 200 km[J]. Optica, 8, 344-349(2021).

[7] Qiao H Z, Zhong K, Li F J et al. Efficient MW-peak-power kHz-repetition-rate sub-nanosecond optical parametric generator tunable from near- to mid-infrared[J]. Optics & Laser Technology, 151, 108010(2022).

[8] Zhong K, Qiao H Z, Li F J et al. Tunable narrow-linewidth high-peak-power sub-nanosecond optical parametric generator by injection seeding[J]. Optics Express, 30, 16479-16488(2022).

[9] Liu Y X, Zhong K, Chen K et al. Research progress of microcavity optical parametric oscillator based on cavity phase matching[J]. Laser & Optoelectronics Progress, 62, 0900003(2025).

[10] Ling Z C, Liu C Q, Bai H C et al. Recent advances on the LIBS studies of Martian surface materials[J]. Bulletin of Mineralogy, Petrology and Geochemistry, 41, 92-112, 7(2022).

[11] Bi G J, Yang W S, Zhu X B et al. High repetition frequency and big energy mode-locking laser technology[J]. Chinese Journal of Lasers, 36, 1822-1825(2009).

[12] Hübner P, Kieleck C, Jackson S D et al. High-power actively mode-locked sub-nanosecond Tm3+-doped silica fiber laser[J]. Optics Letters, 36, 2483-2485(2011).

[13] Ren D M, Bai Y, Zhao W J et al. Experiment on Q-switched and active mode-locking Nd∶YAG picoseconds’ laser[J]. Infrared and Laser Engineering, 41, 885-888(2012).

[14] Zhou W J, Na Q X, Wang Y et al. Passively mode-locked Tm∶GdVO4 laser with sub-nanosecond pulse width[J]. Chinese Journal of Lasers, 50, 2201004(2023).

[15] Cai Z Q, Wang P, Wen W Q et al. LD end-pumped all-solid-state picosecond passively mode-locking lasers[J]. Chinese Journal of Lasers, 34, 901-907(2007).

[16] Lian Y D, Wang Y H, Zhang Y Q et al. Research progress of stimulated Brillouin scattering pulse compression technique[J]. High Power Laser and Particle Beams, 33, 051001(2021).

[17] Liu Z H, Wang Y L, Wang Y R et al. Pulse-shape dependence of stimulated Brillouin scattering pulse compression to sub-phonon lifetime[J]. Optics Express, 26, 5701-5710(2018).

[18] Feng C Y, Xu X Z, Diels J C. High-energy sub-phonon lifetime pulse compression by stimulated Brillouin scattering in liquids[J]. Optics Express, 25, 12421-12434(2017).

[19] Sun Z, Li Q, Jiang M H et al. Subnanosecond pulse generation from diode-pumped electro-optically Q-switched Nd∶YVO4 laser[J]. Journal of Optoelectronics·Laser, 23, 2074-2078(2012).

[20] Zhao X, Song Z, Li Y J et al. High efficiency sub-nanosecond electro‒optical Q-switched laser operating at kilohertz repetition frequency[J]. Chinese Physics B, 29, 084205(2020).

[21] Zayhowski J J, Dill C. Diode-pumped passively Q-switched picosecond microchip lasers[J]. Optics Letters, 19, 1427-1429(1994).

[22] Zayhowski J J. Passively Q-switched Nd∶YAG microchip lasers and applications[J]. Journal of Alloys and Compounds, 303, 393-400(2000).

[23] Lee H C, Chang D W, Lee E J et al. High-energy, sub-nanosecond linearly polarized passively Q-switched MOPA laser system[J]. Optics & Laser Technology, 95, 81-85(2017).

[24] Kawasaki T, Yahia V, Taira T. 100 Hz operation in 10 PW/sr·cm2 class Nd∶YAG micro-MOPA[J]. Optics Express, 27, 19555-19561(2019).

[25] Agnesi A, Dallocchio P, Pirzio F et al. Sub-nanosecond single-frequency 10-kHz diode-pumped MOPA laser[J]. Applied Physics B, 98, 737-741(2010).

[26] Liu L, Li N, Liu Y et al. 1 kHz, 430 mJ, sub-nanosecond MOPA laser system[J]. Optics Express, 29, 22008-22017(2021).

[27] Wang C H, Liu C, Shen L F et al. 1.6 MW peak power, 90 ps all-solid-state laser from an aberration self-compensated double-passing end-pumped Nd∶YVO4 rod amplifier[J]. Applied Optics, 55, 2399-2403(2016).

[28] Jiang Y W, Nie M M, Guo R et al. Pushing the limit of pulse duration in Q-switched solid-state lasers with high gain[J]. Optics & Laser Technology, 129, 106276(2020).

[29] Zhou Y P, Li X D, Wei C J et al. 5 kHz, 4.2 mJ, 900 ps end-pumped Nd∶YVO4 MOPA laser system[J]. Optics Express, 30, 29833-29840(2022).

[30] Kuznetsov I, Chizhov S, Palashov O. Yb∶YAG diverging beam amplifier with 20 mJ pulse energy and 1.5 kHz repetition rate[J]. Optics Letters, 48, 1292-1295(2023).

[31] Qiao H Z, Zhong K, Li F J et al. Near-diffraction-limit 1-kHz sub-nanosecond diode-end-pumped Nd∶YAG laser amplifier via self-compensating spherical aberration[J]. Optics & Laser Technology, 164, 109486(2023).

[32] Carlslaw H S, Jaeger J C[M]. Conduction of heat in solids, 189-229(1989).

[33] Pfistner C, Weber R, Weber H P et al. Thermal beam distortions in end-pumped Nd∶YAG, Nd∶GSGG, and Nd∶YLF rods[J]. IEEE Journal of Quantum Electronics, 30, 1605-1615(1994).

[34] Song X L, Guo Z, Li B B et al. Thermal relaxation time of crystal in pulsed laser diode end-pumped solid-state laser[J]. Chinese Journal of Lasers, 35, 1132-1138(2008).

[35] Li L, Nie J P, Shi P et al. Temperature field characteristic of YAG-Nd∶YAG composite crystal rod end-pumped by laser diode[J]. Chinese Journal of Lasers, 37, 917-922(2010).

[36] Zhang X Z, Zhong K, Qiao H Z et al. Theory and experiments of a power-ratio tunable dual-wavelength Nd∶YVO4/Nd∶GdVO4 laser by varying the pump wavelength[J]. Optical Engineering, 60, 086103(2021).

[37] Eichler H J, Haase A, Menzel R et al. Thermal lensing and depolarization in a highly pumped Nd∶YAG laser amplifier[J]. Journal of Physics D: Applied Physics, 26, 1884-1891(1993).

[38] Wang S, Eichler H J, Wang X et al. Diode end pumped Nd∶YAG laser at 946 nm with high pulse energy limited by thermal lensing[J]. Applied Physics B, 95, 721-730(2009).

[39] Liu B. Research on good beam quality high peak-power solid-state laser amplifier technology[D], 29-30(2018).

[40] Song X L, Li B B, Guo Z et al. Influences of pump beam distribution on thermal lensing spherical aberration in an LD end-pumped Nd∶YAG laser[J]. Optics Communications, 282, 4779-4783(2009).

[41] Liu B, Liu C, Shen L F et al. Beam quality management by periodic reproduction of wavefront aberrations in end-pumped Nd∶YVO4 laser amplifiers[J]. Optics Express, 24, 8988-8996(2016).

[42] Qi Y X, Zhao Z G, Liu C et al. Beam quality management in multi-stage side-pumped Nd∶YAG MOPA laser systems[J]. IEEE Journal of Selected Topics in Quantum Electronics, 21, 1600506(2015).

[43] Yang C, Peng H P, Chen M et al. Depolarization mechanism and compensation scheme of radially polarized beams[J]. Infrared and Laser Engineering, 50, 20200038(2021).

[44] Li X D, Zhou Y P, Xu H B et al. High-stability, high-pulse-energy MOPA laser system based on composite Nd∶YAG crystal with multiple doping concentrations[J]. Optics & Laser Technology, 152, 108080(2022).