[1]Chang Zenghu,Rundquist,A.,Wang Haiwen et al.,Generation of coherent soft X-rays a 2.7 nm using high harmonics,Phys.Rev.Lett.,1997,79(16): 2967-2970.[2]Schnurer,M.,Spielmann,Ch.,Wobrauschek,P.et al.,Coherent 0.5 keV X-ray emission from Helium driven by a sub-10-fs laser,Phys.Rev.Lett.,1998,80(15): 3236-3239.[3]Corkum,P.B.,Plasma perspective on strong-field multiphoton ionization,Phys.Rev.Lett.,1993,71(13): 1994-1997.[4]Lewenstein,M.,Balcou,Ph.,Yu.M.et al.,Theory of high-harmonic generation by low frequency laser fields,Phys.Rev.A,1994,49(3): 2117-2132.[5]Li,X.F.,L'Huillier,A.L.,Ferray,M.et al.,Multiple-harmonic generation in rare gases at high laser intensity,Phys.Rev.A,1989,39(11): 5751-5761.[6]L'Huillier,A.,Schafer,K.J.,Kulander,K.C.,Theoretical aspects of intense field harmonic generation,J.Phys.B,1991,24(),3315-3341.[7]L'Huillier,A.,Balcou,Ph.,Candel,S.et al.,Calculation of high-order harmonic-generation processin Xeon at 1064 nm,Phys.Rev.A,1992,46(5): 2778-2790.[8]Balcou,Ph.,L'Huillier,A.,Phase-matching effects in strong-field harmonics generation,Phys.Rev.A,1993,47(2): 1447-1459.[9]Race,S.C.,Burnett,K.,Detailed simulation of plasma-induced spectral blueshifting,Phys.Rev.A,1992,46(2): 1084-1090.[10]Wood,W.M.,Siders,C.W.,Downer,M.C.,Measurement of femtosecond ionization dynamics of atmosphere density gases by spectral blueshifting ,Phys.Rev.Lett.,1991,67(25): 3523-3526.[11]Le Blanc S.P.,Sauerbrey,R.,Rae,S.C.et al.,Spectral blue shifting of a femtosecond laser pulse propagating through a high-pressure gas,J.Opt.Soc.Am.B,1993,10(10): 1801-1809.[12]Le Blanc,S.P.,Sauerbrey,R.,Spectral,temporal,and spatial characteristics of plasma-induced spectral blue shifting and its application to femtosecond pulse measurement,J.Opt.Soc.Am.B,1996,[13](1): 72-88.13.Burnett,N.H.,Corkum,P.B.,Cold-plasma production for recombination extreme-ultraviolet lasers by optical-field-induced ionization,J.Opt.Soc.Am.B,1989,6(6): 1195-1199.[14]Lehemeier,H.J.,Leupacher,W.,Penzkofer,A.,Nonresonant third-order hyperpolarizability of rare gases and N2 determined by third harmonic generation,Opt.Comm.,1985,56(1): 67-72.[15]The index of rare gases for high harmonics can get from http//:cindy.lbl.gov.[16]Becker,W.,Long,S.,McIver,J.K.,High-harmonic production in a model atom with short-range potential,Phys.Rev.A,1990,41(7): 4112-4115.[17]Krause,J.L.,Schafer,K.J.,Kulander,K.C.,High-order harmonic generation from atoms and ions in the high intensity regimes,Phys.Rev.Lett.,1992,68(24): 3535-3538.[18]Krause,J.L.,Schafer,K.J.,Kulander,K.C.,Calculation of photoemission from atoms subject to intense laser fields,Phys.Rev.A,1992,45(7): 4998-5010.[19]Reed,V.C.,Burnett,K.,Ionization of atoms in intense laser pulses using the Krammers-Henneberger transformation,Phys.Rev.A,1990,45(5): 3152.[20]Constant,E.,Garzella,D.,Breger,P.et al.,Optimizing high harmonic generation in absorbing gases: Model and experiment,Phys.Rev.Lett.,1999,82(8):1668-1671.[21]Ranka,J.K.,Schirmen,R.W,Gaeta,A.L.,Observation of pulse splitting in nonlinear dispersive media,Phys.Rev.Lett.,77(1996): 3783.[22]Alfnao,R.R.ed.,The Supercontinuum Laser Source,New York: Springer-Verlag,1989.[23]Xu,Z.,Li,R.,Li,Z.et al.,Frontiers of Laser Physics and Quantum Optics,Berlin: Springer-Verlag,1999,57-76.[24]Xu Zhizhan,Wang Yingsong,Zhai Kan et al.,The experimental study of the high-order harmonic generation in Ar and Ne with 45 fs Ti:sapphire intense laser field,Science in China (in Chinese),Series A,1999,29(3): 270-275.
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