[1] Nuckolls J., Wood L. et al.. Laser compression of matter to super-high densities: thermonuclear (CTR) application [J]. Nature, 1972, 239(15):139-142

[2] Milonni P. W., Auerbach J. M., D. Eimerl D.. Frequency conversion modeling with spatially and temporally varying beams[C]. SPIE, 1997, 2622:230-241

[3] Okishev A., Skeldon M. D., Letzring S. A. et al.. The pulse-shaping system for the 60-beam,30-kJ OMEGA laser[C]. SPIE, 1996, 2770:10-18

[4] Dingxiang Cao, Xiongjun Zhang, Wanguo Zheng et al.. Thermal distortion and birefringence in repetition-rate plasma electrode Pockels cell for high average power[J]. Chin. Opt. Lett., 2007, 5(5):292-294

[5] Benjrajka V., Chang C. C., Emanuel A. W. R. et al.. Pulse shaping of incoherent light by use of a liquid-crystal modulator array[J].Opt. Lett., 1996, 21(21):1756-1758

[6] Ji Fan, Sui Zhan, Li Feng et al.. Analysis of pulse smoothing by multi-pulse interference in time domain[J]. High Power Laser and Particle Beams, 2006, 18(3):401-404

[7] Zeng Shuguang, Zhang Bin. Inverse problem of pulse shaping by pulse stacking[J]. Acta Optica Sinica, 2008, 28(12): 2272-2276

[8] Wegner P. J., Henesianm A., Speck D. R. et al.. Harmonic conversion of large-aperture 1. 05 μm laser beams for inertial-confinement fusion research [J]. Appl. Opt., 1992, 31(30):6414-6426

[9] Craxton R. S., Stephen D., Joseph E. et al.. Basic properties of KDP related to the frequency conversion of1μm laser radiation [J]. IEEE J. Quan. Eleatron., 1981, QE17(9):1782-1785

[10] Eimerl D., Auerbach J. M., Milonni P. W.. Paraxial wave theory of second and third harmonic generation in uniaxial crystals: I Narrowband pump fields [J]. J. Modern Opt., 1995, 42(5):1037-1067

[11] Li Kun, Zhang Bin. Inverse problem of monochromatic third-harmonic generation[J].Laser Technology, 2006， 30(2)：186～188