双脉冲诱导下光丝中的紫外谐波产生及其光谱调制
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摘要
飞秒激光问世以来,得益于其高峰值功率和高时间/频率分辨能力,已成为物理、化学、生物等学科和领域的重要研究手段和实验工具。不断深入的研究工作则要求超短激光技术继续朝着更短的脉冲持续时间和新的激光波段发展,这一般可通过飞秒激光同物质的非线性相互作用得到。其中,当强飞秒激光脉冲在许多气体介质中传输时,在非线性克尔自聚焦效应和等离子体散焦等效应的共同作用下,能形成长等离子体通道(光丝)。在这种通道中,激光与介质-等离子体之间存在着很强的非线性作用,使入射激光的时空特性受到强烈调制,可产生超连续白光、三次谐波、脉冲自压缩、THz辐射等现象。
     本论文的工作基于等离子体通道对飞秒强激光的调制作用,在三次谐波产生和光谱展宽两个方面开展研究。利用非共线等频双光束在气体中聚焦诱导形成等离子体通道,当两束等频激光在等离子体通道中满足时空交汇时,利用其交叉相位调制和分子取向等效应,在N_2气、空气中Ar气和均获得了三次谐波的增强,还在单光束条件下实现了近红外/紫外激光在Ar气中的光谱展宽,这种等离子体通道中三次谐波和频谱展宽的方法为紫外波段超短脉冲产生提供了一种有效途径:在UV和NIR双色激光场的条件下又使紫外脉冲光谱的得到进一步展宽,为该波段大能量紫外超短脉冲的获得提供有力支持。
     本论文的主要工作包括:
     1.等离子体通道中的三次谐波增强效应研究
     当泵浦光功率较高时,气体中单光束成丝产生的三次谐波信号将演化为轴向光斑和环状结构,其饱和效率约为10~(-4)。在单光束成丝三次谐波产生的基础上,引入第二束飞秒强激光,将两束等频激光非共线聚焦到气体样品中分别成丝,通过改变双光束的时间延迟和背景气压对双光束三次谐波产生进行操控,发现当两束激光在等离子体通道中满足时空交汇条件时,实验中出现了显著的三次谐波增强,其中,Ar气中可实现离轴无背景三次谐波辐射。而N_2气和空气中的谐波增强则出现在轴向,同时N_2中光谱宽度得到很大加宽(从66THz增宽至100THz)。显示了其在紫外超短脉冲获得方面的潜在价值。
     2.等离子体通道中的光谱展宽研究
     分析了飞秒强激光在气体介质中成丝展宽的一般机制,研究了激光能量和聚焦条件对成丝展宽的影响,获得的展宽趋势对实验工作有一定指导意义,并开展了Ar气中红外和紫外波段激光成丝展宽的实验研究。在红外波段获得了底宽从200nm~1100nm的超连续白光;在紫外波段则使激光谱宽由6.3THz增长至13.8 THz。
     为使大能量的紫外脉冲获得更显著的展宽,本论文中使用基频光和三倍频紫外光源在Ar气中共线成丝,利用交叉相位调制的影响,通过调节双光束时间延迟和背景气压,使紫外脉冲的光谱获得进一步展宽(从6.3 THz加宽至26.7THz)。
Due to its high peak power and high time/frequency resolution, femtosecond laser has become an important tool in physics, chemistry, and biology. The ultrafast laser technology is expanding to new waveband as well as to a less during time. When high intensity laser pulses propagate in many gases, due to the interplay between the Kerr self-focusing and plasma defocusing effect, long plasma filament would be formed. The temporal-space property of the laser pulses would be strongly modulated in the filament, thus leads to the generation of super continuum, third harmonic, THz radiation and pulse self-compression.
     This thesis is based on the modulation effect between the plasma filament and the laser pulse, and is composed by two aspects, the enhancement of TH and spectra broadening. The enhancement of TH in air, argon and nitrogen was achieved when focusing dual femtosecond laser beams of the same frequency into the gas ceil, and the two pulses are overlapped both in time and space. The enhancement in molecule gases was also effected by the cross-phase-modulation of the two pulses and the delayed Raman effect in the gas. This method provides an effective way to achieve ultrashort UV laser pulse. Spectra width of the UV laser was slightly broadened in argon gas through filamentaion, and then a two-color filamentaion method was applied to broaden its spetrca further, providing a strong support the generation of high power ultrashort UV pulses.
     The main work in the thesis includes:
     1. The research on the enhancement of third harmonic in filament
     When the power of the pump beam is very high in gases, the induced TH signal evolves into two parts, an on-axis component and a dispersive ring structure, and its total efficiency is merely 10"4. The author introduced another laser beam, and generated dual filaments by non-collinearlly focusing the two beams in the gas cell. Great enhancement was achieved when the two beams overlapped both in time and space. Background-free TH was observed in argon gas, while enhancement of TH on the axis was found in air and nitrogen. Spectra width of TH in nitrogen wassignificantly broadened from 66 THz to 100 THz, which showed a latency value inthe generation of ultrafast UV laser pulse.
     2. Spectra broadening in filament
     The generalized broadening mechanisms in filament were analyzed, then single-beam induced spetra broaden by filamentation was performed both in IR and UV waveband. Supercontinuum with bottom width from 200nm to 1100nm was achieved in ir waveband; while a broadening from 6.3 THz to 13.8 THz was achieved in UV region. A two-color co-filamentation setup in argon gas was used to further broaden the UV pulses. By adjusting the time delay, the background pressure and the overlapping of two filaments, the spetca of the UV laser was further broadened (from 6.3 THz to 26.7 THz)
引文
1 J.Jiang,Z.G.Zhang and T.Hasama,“Evaluation of chirped pulse amplification systems with Offner triplet telescope stretchers,” JOSA B 19,678(2002).
    2 J.P.Chambaret,C.Le Blanc,G.Cheriaux et al.,“Generation of 25-TW,32-fs pulses at 10 Hz,” Opt.Lett.21,1921(1996).
    3 J.T(u|¨)mmler,R.Jung,H.Stiel et al.,“High-repetition-rate chirped pulse amplification thin-disk laser system with joule-level pulse energy,” Opt.Lett.34,1378(2009).
    4 F.R(o|¨)ser,T.Eidam,J.Rothhardt et al.,“Millijoule pulse energy high repetition rate femtosecond fiber chirped-pulse amplification system,” Opt.Lett.32,3495(2007).
    5 D.E.Spence,P.N.Kean and W.Sibbert,“60-fsec pulse generation from a self-mode-locked Ti:sapphire laser,” Opt.Lett.16,42(1991).
    6 Y.Nabekawa,Y.Kuramoto,T.Togashi et al.,“Generation of 0.66-TW pulses at 1 kHz by a Ti:sapphire laser,” Opt.Lett.23,1384(1998).
    7 M.D.Perry,D.Pennington,B.C.Stuart et al.,“Petawatt laser pulses,” Opt.Lett.24,160(1999).
    8 M.Aoyama,K.Yamakawa,Y Akahane et al.,“0.85-PW,33-fs Ti:sapphire laser,” Opt.Lett.28,1594(2003).
    9 K.Yamane et al.,“Optical pulse compression to 3.4 fs in the monocycle region by feedback phase compensation,” Opt.Lett.28,2258(2003).
    10 黄小军,彭翰生,魏晓峰等,“100 TW级超短超强钛宝石激光装置,”强激光与粒子束17,1685(2005).
    11 D.Strickland,G.Mourou,“Compression of amplified chirped optical pulses,” Opt.Comm.56,219(1985).
    12 K.Yamakawa,A.Magana and P.H.Chiu,“Tunable Ti:Sapphire regenerative amplifier for femtosecond Chirped-Pulse Amplification,” Applied Physics B 58,323(1994).
    13 友清,“啁啾脉冲放大产生几太瓦30fs脉冲,”激光与光电子学进展32,21(1995).
    14 陈志宏,吕洪方,熊贵光,“啁啾脉冲放大技术,”半导体光电20,397(1999).
    15 A.Braun,G.Korn,X.Liu et al.,“Self-channeling of high-peak-power femtosecond laser pulses in air,”Opt.Lett.20,73 (1995).
    16 M.Rodriguez,R.Bourayou,G.Mejean et al.,“Kilometer-range nonlinear propagation of femtosecond laser pulses,”Phys.Rev.E 69,036607 (2004).
    17 B.L.Fontaine,F.Vidal,Z.Jiang et al.,“Filamentation of ultrashort pulse laser beams resulting from their propagation over long distances in air,”Phys.Plasmas 6,1615(1999).
    18 S.A.Hosseini,Q.Luo,B.Ferland et al.,“Effective length of filaments measurement using backscattered fluorescence from nitrogen molecules,”Appl.Phys.B 77,697 (2003).
    19 G.Mechain,C.D'Amico,Y.-B.Andre et al.,“Range of plasma filaments created in air by a multi-terawatt femtosecond laser,”Opt.Comm.247,171 (2005).
    20 E.T.J.Nibbering,P.F.Curley,G.Grillon et al.,“Conical emission from self-guided femtosecond pulses in air,”Opt.Lett.21,62 (1996).
    21 J.Kasparian,R.Sauerbrey,and S.L.Chin,“The critical laser intensity of seif-guided light filaments in air,”Appl.Phys.B 71,877 (2000).
    22 A.Becker,N.Akozbek,K.Vijayalakshmi et al.,“Intensity clamping and re-focusing of intense femtosecond laser pulses in nitrogen molecular gas,”Appl.Phys.B 73,287(2001).
    23 W.Liu,S.Petit,A.Becker et al.,“Intensity clamping of a femtosecond laser pulse in condensed matter,”Opt.Comm.202,189 (2002).
    24 W.Liu,S.L Chin,O.Kosareva et al.,“Multiple refocusing of a femtosecond pulse in a dispersive liquid(methanol),”Opt.Comm.225,193 (2003).
    25 Silberberg and Yaron,“Collapse of optical pulses,”Opt.Lett.15,1282 (1990).
    26 G.Bbnsch and E.Potulski,“Measurement of the refractive index of air and comparison with modified Edlen's formulae,”Metrologia 35,133 (1998).
    27 B.Edlen,“The refractive index of air,”Metrologia 2,71 (1966).
    28 K.P.Birch and M.J.Downs,“Correction to the updated Edlen equation for the refractive index of air,”Metrologia 31,315 (1994).
    29 J.H.Marburger,“Self-focusing:Theory,”Prog.Quant.Electr.4,35 (1975).
    30 A.Couairon and A.Mysyrowicz,“Femtosecond filamentation in transparent media,”441,47 (2007).
    31 L.Berge,S.Skupin,G.Mejean et al.,“Supercontinuum emission and enhanced self-guiding of infrared femtosecond filaments sustained by third-harmonic generation in air,”Phy.Rev.E 71,016602 (2005).
    32 A.Couairon and L.Berge,“Modeling the filamentation of ultra-short pulses in ionizing media,”Phys.Plasmas 7,193 (2000).
    33 E.L.Dawes and J.H.Marburger,“Computer studies in self-focusing,”Phys.Rev.179,862(1969).
    34 A.Braun,G.Korn,X.Liu et al.,“Self-channeling of high-peak-power femtosecond laser pulses in air,”Opt.Lett.20,73 (1995).
    35 H.Nishioka and K.-l.Ueda,“Super-broadband continuum generation with transient self-focusing of a terawatt laser pulse in rare gases,”Appl.Phys.B77,171 (2003).
    36 M.Mlejnek,E.M.Wright,and J.V.Moloney,“Dynamic spatial replenishment of femtosecond pulses propagating in air,”Opt.Lett.23,382 (1998).
    37 H.S.Chakraborty,M.B.Gaarde and A.Couairon,“Single attosecond pulses from high harmonics driven by self-compressed filaments,”Opt.Lett.31,3662 (2006).
    1 Zhong Fangchuan,Hu Xueyuan,Deng jian et al.,“Third Harmonic Generation in Air Through Interaction with Ultrashort Intense Laser Pulses,”Acta Optica Sinica 22,10(2002).钟方川,胡雪原,邓健等,“超短强激光作用下空气的三次谐波辐射,”光学学报22,10(2002).
    2 Zhu Chang-Jun,Qin Yuan-Dong,Yang Hong et al.,“Third-Order Harmonic Generation in Atmospheric Air with Focused Intense Femtosecond Laser Pulses,” Chin.Phys.Lett.18,57(2001).
    3 Eiji J.Takahashi,Tsuneto Kanai,Kenichi L.Ishikawa et al.,“Coherent Water Window X Ray by Phase-Matched High-Order Harmonic Generation in Neutral Media,” Phys.Rev.Lett.101,253901(2008).
    4 Ch.Spielmann,N.H.Burnett,S.Sartania et al.,“Generation of Coherent X-rays in the Water Window Using 5-Femtosecond Laser Pulses,” Science 278,661(1997).
    5 Zenghu Chang,Andy Rundquist,Haiwen Wang et al.,“Generation of Coherent Soft X Rays at 2.7 nm Using High Harmonics,” Phys.Rev.Lett.79,2967(1997).
    6 A.B.Fedotov,A.N.Naumov,V.P.Silin et al.,“Third-harmonic generation in a laser-pre-excited gas:the role of excited-state neutrals,” Phys.Lett.A 271,407(2000).
    7 R.A.Bartels,N.L.Wagner,M.D.Baertschy et al.,“Phase-matching conditions for nonlinear frequency conversion by use of aligned molecular gases,” Opt.Lett.28,346(2003).
    8 K.Hartinger,S.Nirmalgandhi,J.Wilson et al.,“Efficient nonlinear frequency conversion with a dynamically structured nonlinearity,” Opt.Express 13,6919(2005).
    9 C.-C.Kuo,C.-H.Pai,M.-W.Lin et al.,“Enhancement of relativistic harmonic generation by an optically preformed periodic plasma waveguide,” Phys.Rev.Lett.98,033901(2007).
    10 Yen-Mu Chen,Ming-Yu Hsu,Yi-Hsian Hsieh et al.,“Enhancement of high-harmonic generation by laser-induced cluster vibration,” Opt.Lett.32, 2714(2007).
    11 N.Kortsalioudakis,M.tatarakis,N.Vakakis et al.,“Enhanced harmonic conversion efficiency in the self-guided propagation of femtosecond ultraviolet laser pulses in argon,” Appl.Phys.B 80,211(2005).
    12 H.R.Lange,A.Chiron,J.-F.Ripoche et al.,“High-Order Harmonic Generation and Quasiphase Matching in Xenon Using Self-Guided Femtosecond Pulses,” Phys.Rev.Lett.81,1611(1998).
    13 H.Yang,J.Zhang,W.Yu et al.,“Long plasma channels generated by femtosecond laser pulses,” Phys.Rev.E 65,016406(2001).
    14 S.L.Chin,F.Th(?)berge and W.Liu.,“Filamentation nonlinear optics,” Appl.Phys.B 86,477(2007).
    15 P.Sprangle,J.R.Pe(?)ano and B.Hafizi,“Propagation of intense short laser pulses in the atmosphere,” Phys.Rev.E 66,046418(2002).
    16 Todd A.Pitts,Ting S.Luk,James K.Gruetzner et al.,“Propagation of self-focusing laser pulses in atmosphere:experiment versus numerical simulation,” J.Opt.Soc.Am.B 21,2008(2004).
    17 J.Kasparian,R.Sauerbrey and S.L.Chin,“The critical laser intensity of self-guided light filaments in air,” Appl Phys B 71,877(2000).
    18 A.Becker,N.Ak(o|¨)zbek,K.Vijayalakshmi et al.,“Intensity clamping and re-focusing of intense femtosecond laser pulses in nitrogen molecular gas,”Appl.Phys.B 73,287(2001).
    19 F.Th(?)berge,N.Ak(o|¨)zbek,W.Liu et al.,“Third harmonic beam profile generated in atmospheric air using femtosecond laser pulses,” Opt.Comm.245,399(2005).
    20 N.Akbzbek,A.Iwasaki,A.Becker et al.,“Third-Harmonic Generation and Self-Channeling in Air Using High-Power Femtosecond Laser Pulses,” Phys.Rev.Lett.89,143901(2002).
    21 M.Kolesik,E.M.Wright,A.Becker et al.,“Simulation of third-harmonic and supercontinuum generation for femtosecond pulses in air,” Appl.Phys.B 85,531(2006).
    22 李海宁,张丽平,吴洪,李贤,丁良恩,“空气中激光等离子体通道的三次谐波光谱特性研究,”光谱学与光谱分析28,1201(2008).
    23 Klaus Hartinger and Randy A.Bartels,“Enhancement of third harmonic generation by a laser-induced plasma,” Appl.Phys.Lett.93,151102(2008)
    24 H.J.Eichler and A.Hermerschmidt,Light-Induced Dynamic Gratings and Photorefraction,In:P.G(u|¨)nter,J.-P.Huignard,Photorefractive Materials and Their Applications 1,Heidelberg,Springer Berlin(2006).
    25 L.Min,L.Wenxue,H.Wanyue,W.Eryu and D.Liang en,“Studies on 5TW/40 fs table-top Ti:sapphire laser system,” Acta Optica Sinica 26,81(2006).
    梁敏,李文雪,胡婉约,王二玉,丁良恩,“5TW/40fs级台式钛宝石激光系统研究,”光学学报26,81(2006).
    26 H.Wanyue,W.Eryu,L.Wenxue and D.Liang'en,“Aberration-free stretcher based on concentric diffraction for sub-10 fs pulses,” Acta Optica Sinica 27,181(2007).
    胡婉约,王二玉,李文雪,丁良恩,“适用于亚10fs的共心衍射无像差展宽器,”光学学报27,181(2007).
    27 A.V.Birulin,V.T.Platonenko and V.V.Strelkov,“Highharmonic generation in interfering waves,” JETP 83,32(1996).
    28 E.R.Peck and D.J.Fischer,“Dispersion of argon,” J.Opt.Soc.Am.,54,1362(1964).
    29 F.Th(?)berge,N.Ak(o|¨)zbek,W.Liu et al.,“Conical emission and induced frequency shift of third-harmonic generation during ultrashort laser filamentation in air,” Opt.Comm.276,298(2007).
    30 S.A.Trushin,S.Panja,K.Kosma et al.,“Supercontinuum extending from >1000 to 250 nm,generated by focusing ten-fs laser pulses at 805 nm into Ar,” Appl.Phys.B 80,399(2005).
    31 F.Calegari,C.Vozzi,S.Gasilov et al.,“Rotational Raman Effects in theWake of Optical Filamentation,” Phys.Rev.Lett.100,123006(2008).
    32 N.Ak(o|¨)zbek,M.Scalora,C.M.Bowden et al.,“White-light continuum generation and filamentation duaring the propagation of ultra-short laser pulses in air,” Opt.Comm.191,353(2001).
    33 T.-T.Xi,X.Lu and J.Zhang,“Interaction of Light Filaments Generated by Femtosecond Laser Pulses in Air,” Phys.Rev.Lett.96,025003(2006).
    34 Y.-Y.Ma,X.Lu,T.-T.Xi et al.,“Filamentation of interacting femtosecond laser pulses in air,” Applied Phys.B 93,463(2008).
    35 Ma Yuan-Yuan,Lu Xin,Xi Ting-Ting et al.,“Potential fields of merging and splitting filaments in air,”Chinese Physics 16,2731 (2007).
    36 Amiel A.Ishaaya,Taylor D.Grow,Saikat Ghosh et al.,“Self-focusing dynamics of coupled optical beams,”Phys.Rev.A 75,023813 (2007).
    37 L.Berge,S.Skupin and G.Mejean,“Supercontinuum emission and enhanced self-guiding of infrared femtosecond filaments sustained by third-harmonic generation in air,”Phy.Rev.E 71,016602 (2005).
    1 M.D.Perry,D.Pennington,B.C.Stuart et al.,“Petawatt laser pulses,” Opt.Lett.24,160(1999).
    2 C.N.Danson et al.,“Focued intensities of 10~(20) W/cm~2 with the upgrated Vulcan CPA interaction facility,” Proceeding of SPIE 82,3492(1998).
    3 A.Bayramian,J.Armstrong,G.Beer et al.,“High-average-power femto-petawatt laser pumped by the Mercury laser facility,” JOSA B 25,B57(2008).
    4 R.R.Alfano and S.L.Shapiro,“Observation of self-phase modulation and small-scale filaments in crystals and glasses,” Phys.Rev.Lett.24,5929(1970).
    5 胡明列,王清月等,“非均匀微结构光纤中超连续光的产生和传输,”中国激光 31,567(2004).
    6 R.G.Smith,“Optical power handling capacity of low loss optical fibers as determined bt stimulated raman and brillouin scattering,” Appl.Opt.11,2498(1972).
    7 R.L.Fork et al.,“Compression of optical pulses to six femtoseconds by using cubic phase compensation,” Opt.Lett.12,483(1987).
    9 P.B.Corkum and C.Rolland,“Supercontinuum Generation in Gases,” Phys.Rev.Lett 57,2268(1986).
    10 M.Rodriguez,R.Bourayou,G.Mejean et al.,“Kilometer-range nonlinear propagation of femtosecond laser pulses,” Phys.Rev.E 69 036607(2004).
    11 H.Wille,M.Rodriguez,J.Kasparian et al.,“teramobile:A mobile femtosecond-terawatt laser and detection system,” Eur.Phys.J.:Appl.Phys.20,183(2002).
    12 P.Rairoux,H.Schillinger,S.Niedermeier et al.,“Remote sensing of the atmosphere using ultrashort laser pulses,” Appl.Phys.B 71,573(2000).
    13 G.M(?)jean,J.Kasparian,E.Salmon et al.,“Towards a supercontinuum-based infrared lidar,” Appl.Phys.B 77,357(2003).
    14 T.R.Gosnell,A.J.Taylor,D.P.Greene,“Supercontinuum generation at 248nm using high-pressure gases,” Opt.Lett.15,130(1990).
    15 J.Kasparian,R.Sauerbrey and D.Mondelain,“Infrared extension of the supercontinuum generated by femtosecond terawatt laser pulses propagating in the atmosphere,” Opt.Lett.25,1397(2000).
    16 H.Yang,J.Zhang,Q.Zhang et al.,“Polarization-dependent supercontinuum generation from light filaments in air,” Opt.Lett.30,534(2005).
    17 S.L.Chin,S.A.Hosseini,W.Liu et al.,“The propagation of powerfulfemtosecond laser pulses in optical media:physics,applications,and new challenges,”Can.J.Phys.83,863 (2005).
    18 DP.Shelton,“Nonlinear susceptibilities of gases measured at 1064 and 1319 nm,”Phys.Rev.A 42,2578 (1990).
    19 J.-F.Ripoche,G.Grillon,B.Prade et al.,“Determination of the time dependence of n2 in air,”Opt.Comm.135,310 (1997).
    20 A.Couairon,H.S.Chakraborty and M.B.Gaarde,“From single-cycle self-compressed filaments to isolated attosecond pulses in noble gases,”Phys.Rev.A 77,053814 (2008).
    21 N.Akozbek,M.Scalora,CM.Bowden et al.,“White-light continuum generation and filamentation during the propagation of ultra-short pulses in air,”Opt.Comm.191,353 (2001).
    22 A.L.Gaeta,“Catastrophic Collapse of Ultrashort Pulses,”Phys.Rev.Lett.84,3582 (2000).
    23 H.Nishioka and K.-l.Ueda,“Super-broadband continuum generation with transient self-focusing of a terawatt laser pulse in rare gases,”Appl.Phys B77,177(2003).
    24 E.R.Peck and D.J.Fischer,“Dispersion of argon,”J.Opt.Soc.Am.54,1362 (1964).
    25 A.Dubietis,G.Tamosauskas,G.Fibich et al.,“Multiple filamentation induced by input-beam ellipticity,”Opt.Lett.29,1126 (2004)
    26 G.Fibich,S.Eisenmann,B.Han et al.,“Control of multiple filamentation in air,”Opt.Lett.29,1772 (2004).
    27 H.Schroeder and S.L.Chin,“Visualization of the evolution of multiple filaments in methanol,”Opt.Comm.234,399 (2004).
    28 N.Akozbek,A.Iwasaki and A.Becker,“Third-Harmonic Generation and Self-Channeling in Air Using High-Power Femtosecond Laser Pulses,”Phys.Rev.Lett.89,143901 (2002).
    29 I.Alexeev,A.C.Ting,D.F.Gordon et al.,“Characterization of the third-harmonic radiation generated by intense laser self-formed filaments propagating in air,” Opt.Lett.31),1503(2005).
    30 H.Yang,J.Zhang,J.Zhang et al.,“Third-order harmonic generation by self-guided femtosecond pulses in air,” Phys.Rev.E 67,015401(2003).
    31 F.Th(?)berge,W.Liu,Q.Luo et al.,“Ultrabroadband continuum generated in air(down to 230 nm) using ultrashort and intense laser pulses,” Appl.Phys.B 20,221(2004).
    32 M.Mlejnek,E.M.Wright and J.V.Moloney,“Femtosecond pulse propagation in argon:A pressure dependence study,” Phys.Rev.E 58,4903(1998).
    33 H.Nishioka,W.Odajima,K.-i.Ueda et al.,“Ultrabroadband flat continuum generation in multichannel propagation of terrawatt ti:sapphire laser pulses,”Opt.Lett.20,2505(1995).
    34 A.Couairon and A.Mysyrowicz,“Femtosecond filamentation in transparent media,” Phys.Rep.441,47(2007).
    35 梁敏,李文雪,胡婉约,王二玉,丁良恩,“5TW/40fs级台式钛宝石激光系统研究,”光学学报26,81(2006).
    36 胡婉约,王二玉,李文雪,丁良恩,“适用于亚10fs的共心衍射无像差展宽器,”光学学报27,181(2007).
    37 李文雪,梁敏,胡婉约,丁良恩等,“基于高功率的5TW/40fs系统放大技术的研究,”,Strong Field Laser Physics,Workshop Series:2005
    38 A.Talebpour,S.Petit and S.L.Chin,“Re-focusing during the propagation of a focused femtosecond Ti:Sapphire laser pulse in air,” Opt.Comm.171,285(1999).
    39 G.Fibich,S.Eisenmann,B.Ilan et al.,“Self-focusing distance of very high power laserpulses”,Opt.Express,13,5897(2005)
    40 H.Schroeder,S.L.Chin,“Visualization of the evolution of multiple filaments in methanol”,Opt.Comm.,234,399(2004)
    41 张丽甲,李海宁,吴洪,李贤,丁良恩,Ar气中超连续谱产生的研究,物理学报,57,904(2008)
    42 J.Schwarz,P.Rambo,J.-C.Diels et al.,“Ultraviolet filamentation in air”,Opt.Comm.,180,383(2000)
    43 N.Kortsalioudakis,M.tatarakis,N.Vakakis et al.,“Enhanced harmonic conversion efficiency in the self-guided propagation of femtosecond ultraviolet laser pulses in argon”,Appl.Phys.B,80,211(2005)
    44 J.Schwarz and J.-C.Diels,“Long distance propagation of UV filaments”,Journal of Modern Optics,49,2583(2002)
    45 Wang Yan-ling(王燕玲),Zhou Xu-gui(周绪桂),Wu Hong(吴洪),Ding Liang-en (丁良恩),“Efficient collinear frequency tripling of femtosecond laser with compensation of group velocity delay”,Chin.Phys.B,to be published
    46 王燕玲,周绪桂,吴洪,裁小民,丁良恩,“氩气中飞秒超强紫外激光成丝的实验研究”,光学学报,待发表
    1 J.R.Ackerhalt and P.Milonni,“Solitons and four wave mixing,” Phys.Rev.A 33,3185(1986).
    2 A.P.Hickman and W.K.Bischel,“Theory of Stokes and anti-Stokes generation by Raman frequency conversion,” Phys.Rev.A 37,2516(1988).
    3 J.R.Pe(?)ano,P.Sprangle,P.Serafim et al.,“Stimulated Raman scattering of intense laser pulses in air,” Phys.Rev.E 68,056502(2003).
    4 顾援,王琛,王伟等,“X射线激光在稠密等离子体诊断中的应用,”物理34,455(2005).
    5 刘明伟,“强激光在电离气体及等离子体介质中的传输研究,”华南师范大学硕士研究生学位论文(2004).
    6 A.Couairon and L.Berg(?),“Modeling the filamentation of ultra-short pulses in ionizing media,” Phys.Plasmas 7,193(2000).
    7 J.Kasparian,R.Sauerbrey and S.L.Chin,“The critical laser intensity of self-guided light filaments in air,” Appl.Phys.B 71,877(2000).
    8 A.Becker,N.Ak(o|¨)zbek,K.Vijayalakshmi et al.,“Intensity clamping and re-focusing of intense femtosecond laser pulses in nitrogen molecular gas,”Appl.Phys.B 73,287(2001).
    9 W.Liu,S.Petit,A.Becker,N.Ak(o|¨)zbek et al.,“Intensity clamping of a femtosecond laser pulse in condensed matter,” Opt.Comm.202,189(2002).
    10 P.Bejot,J.Kasparian,J.-P.Wolf et al.,“Dual-color co-filamentation in Argon,” Opt.Express 16,14115(2008).
    11 Wang Yan-ling(王燕玲),Zhou Xu-gui(周绪桂),Wu Hong(吴洪),Ding Liang-en(丁良恩),“Efficient collinear frequency tripling of femtosecond laser with compensation of group velocity delay,” Chin.Phys.B,to be published.
    12 A.Couairon and A.Mysyrowicz,“Femtosecond filamentation in transparent media,” Physics Reports 441,47(2007).
    13 M.Mlejnek,E.M.Wright and J.V.Moloney,“Femtosecond pulse propagation in argon:a pressure dependence study,” Phys.Rev.E 58,4903(1998).
    14 L.Berg(?),S.Skupin,G.M(?)jean et al.,“Supercontinuum emission and enhanced self-guiding of infrared femtosecond filaments sustained by third-harmonic generation in air,” Phy.Rev.E 71,016602(2005).
    15 王燕玲,周绪桂,吴洪,戴小民,丁良恩,“氩气中飞秒超强紫外激光成丝的实验研究,”光学学报,待发表.
    16 张丽萍,李海宁,吴洪,李贤,丁良恩,“Ar气中超连续谱产生的研究,”物理学报57,904(2008).