[1] [1] W.H.Williams,J.M.Auerbach,M.A.Henesian et al..Modeling characterization of the National Ignition Facility focal spot [C].SPIE,1998,3264:93～97

[2] [2] J.A.Fleck,J.R.Mirrors.Calculation of the small scale self-focusing ripple gain spectrum for the cyclops laser system:a status report [R].UCID-17356,1976

[3] [3] J.T.Hunt,K.R.Manes,P.A.Renard.Hot images from obscurations [J].Appl.Opt.,1993,32(30):5973～5982

[4] [4] M.D.Feit,J.A.Fleck,Jr..Beam nonparaxiality,filament formation,and beam breakup in the self-focusing of optical beams [J].J.Opt.Soc.Am.B,1988,5(3):633～640

[6] [6] M.Henesian,P.Renard,J.Auerbach et al..The use of beam propagation modeling of beamlet and Nova to ensure a "safe" National Ignition Facility laser system design [C].SPIE,1997,3047:84～95

[7] [7] J.A.Fleck,J.R.Mirris,E.S.Bliss et al..Small-scale self-focusing effects in a high power glass laser amplifier [J].IEEE J.Quantum Electron.,1978,QE-14(5):353～363

[9] [9] G.P.Agrawal,N.K.Dutta.Semiconductor Laser [M],chapter 6,second edition,New York:Van Nostrand,1992