[1] Baisden P A, Atherton L J, Hawley R A, et al. Large optics for the National Ignition Facility[J]. Fusion Science and Technology, 69, 295-351(2016).

[2] [2] Wegner P J, Auerbach J M, Biesiada T A Jr, et al. NIF final optics system: frequency conversion beam conditioning[C]Proceedings of SPIE 5341. 2004: 180189.

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

[4] Spaeth M L, Manes K R, Bowers M, et al. National Ignition Facility laser system performance[J]. Fusion Science and Technology, 69, 366-394(2016).

[5] Feigenbaum E, Di Nicola J M G, Bude J D. Revisiting beam filamentation formation conditions in high power lasers[J]. Optics Express, 27, 10611-10630(2019).

[6] [6] Lanier T E, Cohen S J, Nicola J, et al. Timegated measurements of fusionclass laser beam profiles[C]Proceedings of SPIE 11259. 2020: 39

[14] [14] Shen Y R. The principles of nonlinear optics[M]. New Yk: John Wiley Sons, Inc, 1984.

[16] [16] Milam D, Hunt J T, Manes K R, et al. Modeling of filamentation damage induced in silica by 351nm laser pulses[C]Proceedings of SPIE 2966. 1996: 425428.

[18] [18] Erickson M A, Cohen S J, Di Nicola J M, et al. Spatially resolved Bintegral measurements on the NIF laser[C]Proceedings of SPIE 11259. 2020: 17.