[1] Manka K,McLean E A,Mostovych A N,et al.Laser-target interaction with induced spatial incoherence[J].Phys Rev Lett,1986,56:2807-2810.

[2] Skupsky S,Short R W,Kessler T,et al.Improved laser-beam uniformity using the angular dispersion of frequency-modulated light[J].Appl Phys,1989,66:3456-3462.

[3] Pennington D M,Henesian M A,Dixit S N,et al.Effect of bandwidth on beam smoothing and frequency conversion at the third harmonic of the Nova laser[C]//Proc of SPIE.1993,1870:175-185.

[4] Murray J R,Smith J R,Ehrlich R B,et al.Experimental observation and suppression of transverse stimulated Brillouin scattering in large optical components[J].J Opt Soc Am B,1989,6:2402-2410.

[5] Ross I N,Matousek P,Geoffrey H,et al,Analysis and optimization of optical parametric chirped pulse amplification[J].J Opt Soc Am B,2002,19(12):2945-2956.

[6] Auerbach J M,Milam D,Barker C E,et al.Frequency-conversion modeling[R].UCRL-LR-105821-96-4.

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

[8] Robert W S,Skupsky S.Frequency conversion of broad-bandwidth laser light[J].IEEE J of Quantum Electronics,1990,26(3):580-588.

[9] 李琨,张彬,袁晓东,等.晶体级联方式宽带三倍频光的参数优化[J].强激光与粒子束,2005,17(7):995-999.(Li K,Zhang B,Yuan X D,et al.Optimizing parameters of third harmonic generation of broadband laser using cascade crystals.High Power Laser and Particle Beams,2005,17(7):995-999)

[10] Craxton R S,Stephen D,Joseph E,et al.Basic properties of KDP related to the frequency conversion of 1 μm laser radiation[J].IEEE J of Quantum Electronics,1981,17 (9):1782-1785.

[11] Eimerl D.Electro-optic,linear,and nonlinear optical properties of KDP and its isomorphs[J].Ferroelectrics.1987,72:95-139.

[12] Eimerl D,Auerbach J M,Barker C E,et al.Multicrystal designs for efficient third-harmonic generation[J].Opt Lett,1997,22 (16):1208-1210.