[1] Lindl J D, Mead W C. Two dimensional simulation of fluid instability in laser fusion pellets[J]. Phys Rev Lett, 1975, 34(20): 1273-1276.
[2] Nakat Suka M, Miyanaga N, Kanabe T, et al. Partially coherent light source for ICF experiment[C]//SPIE, 1993, 1870: 151-162.
[3] Mat Suoka S, Miyanaga N, Ando A, et al. Flexible pulse shaping of partially coherent light on GEKKO Ⅻ[C]//SPIE, 1995, 2633: 627-633.
[4] Boyd R D, Bliss E S, Boege S J, et al. Alignment and diagnostics on the National Ignition Facility laser system[C]//SPIE, 1999, 3782: 496-501.
[5] Xia Yanwen, Sun Zhihong, Zhao Runchang, et al. Improvement of infrared temporal profile measurement system for SG-Ⅲ prototype laser facility[J]. Infrared and Laser Engineering, 2012, 41(6): 1453-1457. (in Chinese)
[6] Lu Zonggui, Xia Yanwen, Tang Jun, et al. Pulse-shape measurement technology for multi-beams infrared laser[J]. Infrared and Laser Engineering, 2011, 40(6): 1129-1132. (in Chinese)
[7] Thomas S, Boyd B, Davis D T, et al. Temporal multiplexing for economical measurement of power versus time on NIF[C]//SPIE, 1997, 3047: 700-706.
[8] Milan D. Measurements at 351nm of temporal dispersion in fibers; UCRL-ID-132866, 1998(12): 1-24.
[9] Haynam C A, Wegner P J, Auerbach J M, et al. National Ignition Facility laser performance status[J]. Applied Optics, 2007, 46(16): 3276-3303.
[10] Pan Xue, Li Xuechun, Li Guoyang, et al. Enhanced-dynamic-range single-shot measurement of nanosecond optical pulse based on fiber pulse replication loop. [J]. Chinese Journal of Lasers, 2012, 39(4): 0408005. (in Chinese)