[1] [1] PEREZ-MARTIN P, PRENCIPE I, SOBIELLA M, et al. A novel multi-shot target platform for laser-driven laboratory astrophysics experiments[J]. High Power Laser Science and Engineering, 2023, 11（17）: 1-9.

[2] [2] BETTI R, HURRICANE O A. Inertial-confinement fusion with lasers[J]. Nature Physics, 2016, 12（5）: 435-448.

[3] [3] HOCQUET S, PENNINCKX D, BORDENAVE E, et al. FM-to-AM conversion in high-power lasers[J]. Applied Optics, 2008, 47（18）: 3338-3349.

[4] [4] ZHENG W G, WEI X F, ZHU Q H, et al. Laser performance upgrade forprecise ICF experiment in SG-Ⅲ laser facility[J]. Matter and Radiation at Extremes, 2017, 2（5）: 243-255.

[5] [5] HUANG X D, ZHANG X M, WANG J J, et al. The effect of dispersionon FM-AM coversion in high power laser front end [J]. Acta Physica Sinica,2010, 59（3）: 1857-1862.

[6] [6] FAN M Q, TIAN X C, ZHOU D D, et al. Two-dimensional tunable and temperature-insensitive Lyot filter for FM-to-AM compensation[J]. Photonic Sensors, 2020, 11（3）: 325-333.

[7] [7] QIAO Z, WANG X C, FAN W, et al. Suppression of FM-to-AM modulation by polarizing fiber front end for high-power lasers [J]. Applied Optics,2016, 55（29）: 8352-8358.

[8] [8] LI R, FAN W, JIANG Y, et al. Tunable compensation of GVD-inducedFM-AM conversion in the front end of high-power lasers [J]. Applied Optics,2017, 56（4）: 993-998.

[9] [9] LI P, WANG W, SU J Q, et al. Analysis on FM-to-AM conversion ofSSDbeam induced by etalon effect in a high-powerlasersystem[J]. High Power Laser Science and Engineering, 2019, 7（21）: 1-6.

[10] [10] YIN J H, LU L H, CUI Y W, et al. Functional gradient films on aluminum alloy with high absorption efficiencies and damage thresholds forinertial confinement fusion applications [J]. Ceramics International, 2022,48（13）: 19180-19190.

[11] [11] XU D P, ZHANG R, TIAN X C, et al. Progress on FM-to-AM effectand its suppression in high power laser driver [J]. Laser & OptoelectronicsProgress, 2017, 54（2）: 57-68.

[12] [12] LI L, BO Z, XIA Y W, et al. Correlation of temporal profile and spectrum for small broadband frequency modulation pulse in high power laserfacility [J]. Laser & Optoelectronics Progress, 2017, 54: 1-6.

[13] [13] JIANG S B, WANG L J, TANG C, et al. Compensation system forFM-to-AM effects in high-power laser system [Z]. AOPC 2015: Advances inLaser Technology and Applications. 2015: 1-6

[14] [14] XU D P, HUANG Z H, WANG J J, et al. A fiber-based polarization–rotation filter utilized to suppress the FM-to-AM effect in a large-scale laserfacility [J]. Journal of Optics, 2013, 15（8）: 1-4.

[15] [15] XU D P, WANG J J, LI M Z, et al. Weak etalon effect in wave platescan introduce significant FM-to-AM modulations in complex laser systems[J]. Optics Express, 2010, 18（7）: 6621-6627.

[16] [16] STEVE H, GEOFFREY L, DENIS P. Compensation of frequencymodulation to amplitude modulation conversion in frequency conversionsystems [J]. Applied Optics, 2009, 48（13）: 2515-2521.

[17] [17] ZHANG Y J, FAN W, WANG J F, et al. Theoretical analysis of frequency modulation-to-amplitude modulation on the final optics and targetof the SG II-Up laser facility [J]. High Power Laser Science and Engineering,2023, 12（9）: 1-15.

[18] [18] CHANG Z, WANG Y S, SUN Y H, et al. 1.5 kW polarization-maintainedYb-dopedamplifierwith13GHzlinewidth bysuppressingthe self-pulsing and stimulated Brillouin scattering[J]. Applied Optics, 2019, 58（23）: 1-6.

[19] [19] WANG Y S, SUN Y H, PENG W J, et al. 3.25 kW all-fiberized andpolarization-maintained Yb-doped amplifier with a 20 GHz linewidth andnear-diffraction-limited beam quality [J]. Applied Optics, 2021, 60（21）: 1-8.

[20] [20] CHU Q H, SHU Q, LI F Y, et al. Power scaling of high-power linearlypolarized fiber lasers with <10GHz linewidth [J]. Frontiers in Physics, 2023,21（4）: 1-8.