[1] [1] Basov N G, Krohkin O H. The conditions of plasma heating by optical generation of radiation[C]Proceedings of the 3rd International Congress on Quantum Electronics, 1963.

[3] Nuckolls J, Wood L, Thiessen A. Laser compression of matter to super-high densities: thermonuclear (CTR) applications[J]. Nature, 239, 139-142(1972).

[4] Moses E, Wuest C R. The National Ignition Facility: status and plans for laser fusion and high-energy-density experimental studies[J]. Fusion Science and Technology, 43, 420(2003).

[5] André M L. The French Megajoule Laser Project (LMJ)[J]. Fusion Engineering and Design, 44, 43-49(1999).

[8] Lindl J D, Amendt P, Berger R L. The physics basis for ignition using indirect-drive targets on the National Ignition Facility[J]. Physics of Plasmas, 11, 339-491(2004).

[9] Lindl J, Landen O, Edwards J. Review of the National Ignition Campaign 2009-2012[J]. Physics of Plasmas, 21, 020501(2014).

[10] [10] Wilcox R B, Behrendt W, Browning D F, et al. Fusion laser oscillat pulsefming system using integrated optics[C]Proc of SPIE. 1993, 1870: 5363.

[11] Skupsky S, Short R W, Kessler T. Improved laser-beam uniformity using the angular dispersion of frequency modulated light[J]. Journal of Applied Physics, 66, 3456-3462(1989).

[12] [12] Heebner J, Bden M, Miller P, et al. A programmable beam shaping system f tailing the profile of high fluence laser beams[C]Proc of SPIE. 2010, 7842: 40.

[13] Lin Y, Kessler T J, Lawrence G N. Design of continuous surface-relief phase plates by surface-based simulated annealing to achieve control of focal-plane irradiance[J]. Optics Letters, 21, 1703-1705(1996).

[14] Regan S P, Marozas J A, Craxton R S. Performance of 1-THz-bandwidth, two-dimensional smoothing by spectral dispersion and polarization smoothing of high-power, solid-state laser beams[J]. Journal of the Optical Society of America B Optical Physic, 22, 998-1002(2005).

[15] Rothenberg J E. Polarization beam smoothing for inertial confinement fusion[J]. Journal of Applied Physics, 87, 3654-3662(2000).

[16] Moody J D, Macgowan B J, Rothenberg J E. Backscatter reduction using combined spatial, temporal, and polarization beam smoothing in a long-scale-length laser plasma[J]. Physical Review Letters, 86, 2810-2813(2001).

[17] Spaeth M L, Manes K R, Kalantar D H. Description of the NIF laser[J]. Fusion Science and Technology, 69, 25-145(2016).

[18] Zhang R, Jia H, Tian X. Research of beam conditioning technologies using continuous phase plate, multi-FM smoothing by spectral dispersion and polarization smoothing[J]. Optics and Lasers in engineering, 85, 38-47(2016).

[22] [22] Zhang Rui, Su Jingqin, Yuan Haoyu, et al. Research of beam conditioning technologies on SGIII laser facility[C]Proc of SPIE, 2014, 9293: 92930E.

[23] Zhang R, Su J, Wang J. Experimental research on the influences of smoothing by spectral dispersion on the Technical Integration Line[J]. Applied Optics, 50, 687-695(2011).

[24] Zheng W, Wei X, Zhu Q. Laser performance upgrade for precise ICF experiment in SG-Ⅲ laser facility[J]. Matter Radiat Extrem, 2, 243-255(2017).

[25] Hao L, Zhao Y, Yang D. Analysis of stimulated Raman backscatter and stimulated Brillouin backscatter in experiments performed on SGIII prototype facility with a spectral analysis code[J]. Phys Plasmas, 21, 072705(2014).

[26] Lan K, Li Z, Xie X. Experimental demonstration of low laser-plasma instabilities in gas-filled spherical hohlraums at laser injection angle designed for ignition target[J]. Phys Rev E, 95, 031202(2017).

[27] Dewald E L, Glenzer S H, Landen O L. First laser–plasma interaction and hohlraum experiments on the National Ignition Facility[J]. Plasma Physics and Controlled Fusion, 47, B405-B417(2005).

[29] [29] Jones O S, Speck D R, Williams W H, et al. The NIF’s power energy ratings f ICFshaped pulses[C]Proc of SPIE. 1998, 3492: 4954

[30] Hu Dongxia, Dong Jun, Xu Dangpeng. Generation and measurement of complex laser pulse shapes in the SG-III laser facility[J]. Chinese Optics Letters, 13, 041406(2015).

[31] Li Ping, Wang Wei, Jin Sai. The shaped pulses control and operation on the SG-III prototype facility[J]. Laser physics, 28, 045004(2018).

[32] Hocquet S, Penninckx D, Gleyze J F. Nonsinusoidal phase modulations for high-power laser performance control: stimulated Brillouin scattering and FM-to-AM conversion[J]. Applied Optics, 49, 1104-1115(2010).

[33] [33] Browning D F, Rothenberg J E, Wilcox R B. The issue of FM to AM conversion on the National Ignition Facility[C]Proceedings of SPIE. 1999, 3492.

[34] Hocquet S, Penninckx D, Bordenave E. FM-to-AM conversion in high-power lasers[J]. Applied Optics, 47, 3338-3349(2008).

[35] Xu D, Wang J, Li M. Weak etalon effect in wave plates can introduce significant FM-to-AM modulations in complex laser systems[J]. Optics Express, 18, 6621-6627(2010).

[36] Li Rao, Fan Wei, Jiang Youen. Tunable compensation of GVD-induced FM–AM conversion in the front end of high-power lasers[J]. Appl Opt, 56, 993-998(2017).

[37] Li Ping, Wang Wei, Su Jingqin. Analysis on FM-to-AM conversion of SSD beam induced by etalon effect in a high-power laser system[J]. High Power Laser Science and Engineering, 7(2019).

[38] Bagnoud V, Zuegel J D. Independent phase and amplitude control of a laser beam by use of a single-phase-only spatial light modulator[J]. Optics Letters, 29, 295-297(2004).

[39] Bespalov V I, Talanov VI. Filamentary structure of light beams in nonlinear liquids[J]. JETP Lett, 3, 307-310(1966).

[40] Campillo A J, Shapiro S L, Suydam B R. Periodic breakup of optical beams due to self-focusing[J]. Applied Physics Letters, 23, 628-630(1974).

[41] Jokipii J R, Marburger J. Homogeneity requirements for minimizing self-focusing damage by strong electromagnetic waves[J]. Applied Physics Letters, 23, 696-698(1974).

[42] Jia Huaiting, Xu Bing, Wang Fang. Small-scale self-focusing in a tapered optical beam[J]. Applied Optics, 51, 6089-6094(2012).

[43] Wen Shuangchun, Fan Dianyuan. Small-scale self-focusing of intense laser beams in the presence of vector effect[J]. Chin Phys Lett, 17, 731-733(2000).

[44] [44] Parham T G, Azevedo S, Chang J, et al. Large aperture optics perfmance. 2009, LLNLTR410955.

[45] Manes K R, Spaeth M L, Adams J J. Damage mechanisms avoided or managed for NIF large optics[J]. Fusion Science and Technology, 69, 146-249(2016).

[47] Hunt J T, Manes K R, Renard P A. Hot images from obscurations[J]. Appl Opt, 32, 5973-5982(1993).

[48] Wang Y W, Wen S C, Zhang L F. Obscuration size dependence of hot image in laser beam through a Kerr medium slab with gain and loss[J]. Appl Opt, 47, 1152-1163(2008).

[49] [49] Millerd J E, Brock N J, Hayes J B, et al. Modern approaches in phase measuring metrology [C]Proc of SPIE. 2005, 5856: 1322.

[50] [50] Ravizza F L, Nostr M C, Kegelmeyer L M, et al. Process f rapid detection of fratricidal defects on optics using Linescan Phase Differential Imaging [R]. LLNLPROC420837, 2009.

[53] Li Ping, Jin Sai, Zhao Runchang. The special shaped laser spot for driving indirect-drive hohlraum with multi-beam incidence[J]. High Power Laser Science and Engineering, 5, 49-54(2017).