用户名: 密码: 验证码:
基于频域全息法的激光尾场测量技术研究
详细信息    本馆镜像全文|  推荐本文 |  |   获取CNKI官网全文
摘要
超短超强脉冲激光在稀薄等离子体中激发的等离子体振荡波(也称为尾场)用来加速电子,是目前激光驱动等离子体加速器的重要工作机制之一,因其具有超高加速梯度和较小的加速结构而具有广阔的应用前景,特别是激光尾场加速器(LWFA)在实验上已经被证明具有产生超高电场梯度(超过100GeV/m)的能力,因此成为当前国际学术界十分关注的前沿课题。
     激光尾场加速器产生相对论电子束的光束质量取决于等离子体振荡波的时空结构,能够直接观测这种结构对了解和控制激光尾场加速器的电子束输出是至关重要的。本论文的研究内容是:利用频域全息探测方法(Frequency-domain holography,FDH),对以接近光速传播的等离子体波实现单束瞬态时空测量开展理论性研究。
     主要工作包括以下几个方面:
     1.简述激光—尾场电子加速器的需求背景、意义以及发展现状。重点介绍了基于频域干涉探测法(Frequency-domain interferometry,FDI)和频域全息探测法的激光尾场测量技术国内外进展,特别是针对近些年国际上有代表性的尾场测量技术方案及其技术指标进行了较为详细的调研分析。
     2.概括性地介绍了激光尾场的激励原理、加速电子的工作机制和四种技术方案。针对尾场的时空测量,特别介绍了超短超强脉冲激光与等离子体相互作用共振激发等离子体波的条件,尾场的时空特征及其对探测脉冲的相位调制,为测量实验参数的选择给出理论依据。
     3.由于频域全息探测方法的理论基础是两束啁啾脉冲之间的频谱干涉(SpectralInterferometry,SI),因此对傅里叶变换频谱干涉技术(Fourier Transformation SpectralInterferometry,FTSI)的工作原理以及确定两束相干宽带脉冲之间相对延迟时间的方法进行了理论、模拟和实验上的研究。重点探讨了线性啁啾脉冲的频谱干涉技术的原理和特性。
     4.阐述频域全息探测技术的基本原理,对实现频域全息探测技术的两种方法:基于直接映射模式的频—时相移转换和基于傅里叶变换模式的频—时相移转换法分别进行了系统的理论分析,并对两种相移转换方法进行了比较。指出基于傅里叶变换模式的频—时相移转换法更适合激光尾场的瞬态时空测量。
     5.提出基于皮秒啁啾脉冲的频域全息测量法对激光尾场的瞬态时空演变进行实时测量的方案。基于小信号下啁啾高斯脉冲的宽带二次谐波的频谱特性,在理论上和实验验证两个方面展开共轴光路下参考脉冲.探测脉冲产生机制的研究。
     6.基于中国工程物理研究院激光聚变研究中心的SILEX-Ⅰ超短激光装置平台,以800nm,30fs,30TW脉冲作为泵浦光,400nm,1ps啁啾脉冲作为参考-探测光脉冲对,展开尾场测量的实验设计。并根据频域全息方法激光尾场探量技术的理论分析,对各光路中所需的光学实验参数进行理论计算。为具体实验实施打下理论基础。
     在低密度等离子体中激发尾场来加速电子,是一个非常复杂的过程,将受多种不稳定性的制约。本文通过对基于频域全息方法探测尾场瞬态时空变化的理论研究,对实现尾场的实时测量和控制,以获得高质量的高能电子具有非常重要的意义。
Using ultra-short ultra-intense laser pulse to excite the electron plasma wave(wakefield、Langmuir waves or electron density "bubbles") is one of main mechanism for laser-driven plasma accelerators to accelerate electrons in the low-density plasma.This accelerator with ultrahigh accelerating gradients and compact size is promising for the next-generation particle accelerators,and is one of the most attractive frontiers.In particular,it has been experimentally demonstrated that laser wake-field acceleration(LWFA) has great potential to produce ultrahigh field gradients excited by intense ultrashort laser pulses(>100GeV/m). However,the beam quality of relativity electron beams produced by LWFA depends on the space-time structures of the wake-field,and it is important for controlling electron beams from LWFA that these structures are directly observed.Based on frequency domain holography(FDH),the single-shot real-time measurement for temporal and spatial evolution of the wake-field propagating near light speed,is investigated theoretically in this dissertation, including the following research topics:
     1.The development,application and general status of laser wake-field accelerator are summarized.Domestic and oversea development for measuring techniques of laser-wakefield, using Frequency domain interferometry and Frequency domain holography,are emphatically introduced,respectively.Especially,representative technical schemes and qualifications are given a presentation in detail.
     2.Excitation principle of laser-wakefield,mechanism of electron acceleration and four schemes for laser driven plasma accelerators are briefly depicted.The resonance conditions between the ultra-short ultra-intense pulse laser and plasma,temporal and spatial characteristics of wakefields and phase perturbation of the probe pulse imposed by wakefields are specially discussed for the appropriately choice of experiment parameters.
     3.Because supporting technology of the frequency-domain holography is spectral interference(SI) between two chirped pulses,FDH is an extension of Frequency domain interferometry(FDI).Fourier-transform spectral interferometry(FTSI) and the measurement of delay time between two pulses are analyzed theoretically,numerically and experimentally, respectively.Thereinto,the characteristics of spectral interferometry between two linear chirped pulses are mostly studied.
     4.Two methods for frequency-domain holography,direct mapping mode and full Fourier transform mode,are theoretically investigated,respectively.With the direct mapping mode, the spectral phase shifts are transformed to time-domain by time-frequency relation,while the spectral phase shifts are transformed to time-domain by Fourier transform with the full Fourier transform mode.Comparison of the two modes is given,and results show that more accuracy can be obtained through the full Fourier transform mode for the measurement of the wake-field.
     5.The measurement scheme for transient time-space evolution of the wakefield induced by the ultra-short ultra-intense laser pulse is presented,based on FDH using picosecond chirped pulses.The coaxial generation of the reference and probe pulses is investigated theoretically and experimentally,based on spectral characteristics of the generated pulse in the process of broadband second-harmonic generation.
     6.According to the theoretical analysis of FDH,the optical layout and experimental parameters of FDH are designed based on the SILEX-I,a Ti:sapphire laser system at CAEP, where the wake-field is excited in a He gas jet pumped by a pulse of~30TW/800nm/30fs,and probed by two chirped pulses of~1ps/400nm.
引文
[1]TAJIMA.T,and DAWSON.J.M.Laser electron accelerator[J].PHYSICAL REVIEW LETTERS.1979,43:267-270.
    [2]T.Katsouleas et al.,Accelerator physics:Electrons hang ten on laser wake[J],Nature(London)431,515-516(2004)
    [3]彭翰生,惯性约束聚变和高功率激光技术[A].见:惯性约束聚变暑期班讲义(一)[C],乐山,2003
    [4]彭翰生,超强固体激光及其在前沿学科中的应用[J].中国激光,2006,33(6-7)
    [5]M.D.Perry,Crossing the patawatt threshold[J],Sci.& Technol.Rev.,1996,(Dec.):4-11
    [6]S.Backus,C.G.Durfee III,M.M.Murnane et al.High power ultrafast lasers[J].Rev.Sci.Instrum.,1988,69(3):1207-1223
    [7]魏晓峰,吕志伟,曾小明等.光参量啁啾脉冲饱和放大的增益稳定性[J].强激光与粒子束.2004,16(12),1540-1544.
    [8]P.Maine,D.Strickland,P.Bado et al.Generation of ultrahigh peak power pulsers by chirped pulse amplification[J].IEEE J.Quantum Electron.,1988,24(2):398-403
    [9]G.A.Mourou,C.P.J.Batty,M.D.Perry,Ultrahigh-intensity lasers:Physics of the extreme on a tabletop[J],Phys.Today,1998,22(1):22-28
    [10]M.D.Perry,D.Pennington,B.C.Staurt et al,Pettawatt laser pulses[J],Opt.Lett.,1999,24(3):161-162.
    [11]H.S.Peng,X.J.Huang,Q.H.Zhu et al,286-TW Ti:sapphire laser at CAEP[C],SPIE,2004,5627:1-5
    [12]H.S.Peng,W.Y.Zhang,X.M.Zhang et al,Progress in ICF programs at CAEP[J],Laser and Particle Beams,2005,23:205-209
    [13]Huang Xiaojun,Peng Hansheng,Wei Xiaofeng et al,Ultra-short ultra-intense Ti:sapphire laser facility with peak power of hundered-terawatt-level[J],High Power Laser and Particle Beams.2005,17(11):1685-1688
    [14]H.S.Peng,X.J.Huang,Q.H.Zhu et al.SILEX-I:300-TW Ti:sapphire laser[J],Laser Physics,2006,16(2):244-247
    [15]华剑飞,安维明,黄文会等,SILEX-I装置上等离子体尾场加速电子初步实验[J],高能物理与核物理,2006,30,Supp.1,108-110
    [16]W.P.Leemans,B.Nagler,A.J.Gonsalves et al.GeV electron beams from a centimeter-scale accelerator[J],Nature Phys.2006,2,696-699
    [17]Takashi Kameshima,Wei Hong,Kiyohiro Sugiyama,Xianlun Wen et al.,0.56GeV Laser Electron Acceleration in Ablative-Capillary-Discharge Plasma Channel[J]. App.Phys.Exp, 1(2008) 066001
    [18] N. H. MATLIS et al., Snapshots of laser wakefields[J], Nature Phys. 2, 749-753(2006)
    [19] E.Tokunaga, A .Terasaki and T. Kobayashi, Frequency-domain interferometer for femtosecond time-resolved phase spectroscopy[J], Opt. Lett. 17(1992), 1131.
    [20] GEINDRE.J.P, AUDEBERT.P, ROUSSE.A, et al, Frequency-domain interferometer for measuring the phase and amplitude of a femtosecond pulse probing a laser-produced plasma [J]. OPTICS LETTERS, 1994, 19(23):1997-1999.
    [21] H. Hamster et al. , Subpicosecond, electromagnetic pulses from intense laser-plasma interaction[J], Phys. Rev. Lett. 71,2725-2728(1993)
    [22] J. R. Marques, J. P. Geinder, F. Amiranoff, P. Audebert, J. C. Gauthier, A. Antonetti, and G. Grillon, Temporal and Spatial Measurements of the Electron Density Perturbation Produced in the Wake of an Ultrashort Laser Pulse[J], Phys. Rev. Lett. 76,3566-3569(1996) [23] J. R. Marques, F. Dorchies, P. Audebert, J. P. Geinder, F. Amiranoff, J. C. Gauthier, G. Hammoniaux, A. Antonetti, P. Chessa, P. Mori, and T. M. Antonsen, Jr., ibid. 78,3463(1997)
    [24] J. R. Marques, F. Dorchies, F. Amiranoff, P. Audebert, J. C. Gauthier, J. P. Geinder, A. Antonetti, T. M. Antonsen, Jr., P. Chessa, and P. Mori, Laser wakefield: experimental studies of nonlinear radial oscillations[J], Phys. Plasmas 5,1162-1177(1998)
    [25] C. W. Siders, S. P. Le Blanc, D. Fisher, T. Tajima, and M. C. Downer, Laser wakefield excitation and measurement by femtosecond longitudinal interferometry[J], Phys. Rev. Lett. 76,3570-3572(1996)
    [26] C. W. Siders, S. P. LeBlanc, A. Babine, A. Stepanov, A. Sergeev, T. Tajima, and M. C. Downer, Plasma-based accelerator diagnostics based upon longitudinalinterferometry with ultrashort optical pulses[J], IEEE Trans. Plasma Sci. 24,301-315(1996)
    [27] C. Froehly, A. Lacourt, and J.-C. Vienot, "Time impulse response and time frequency response of optical pupils. Experimental confirmations and applications[J]", Nouv. Rev. Optique 4,183-196(1973)
    [28] REYNAUD.F, SALIN.F and BARTHELEMY.A, Measurement of phase shifts introduced by nonlinear optical phenomena on subpicosecond pulses[J], OPTICS LETTERS, 1989,14(5): 275-277.
    [29] Eiji Takahashi, Hiroshi Honda, Eisuke Miura, Noboru Ygami, Yasushi Nishida and Kiminori Kondo, Laser Wakefield in Low Density Plasma[J], Journal of the Physical Society of Japan 69, 3266-3275(2000)
    [30] Takahashi E, et al, Observation of spatial asymmetry of THz oscillating electron plasma wave in a laser wakefield [J], Phys. Rev. E, 2000, 62, 7247-7250.
    [31] E. Takahashi, K. Katsura, E. Miura, N. Yugami, Y. Nishida, H. Honda and K. Kondo: in High-Power Lasers in Energy Engineering[A], ed. K. Mima, G. L. Kulicinski and W. Hogan: Proceedings of SPIE, 3886, pp. 136-144
    [32]HIDEYUKI KOTAKI,MASAKI KANDO,TAKATSUGU OKETA,et al.Direct measurement of coherent ultrahigh wakefields excited by intense ultrashort laser pulses in a gas-jet plasma[J].PHYSICS OF PLASMAS,2002,9(4):1392-1400.
    [33]S.P.LeBlanc,E.W.Gaul,N.H.Matlis,A.Rundquist,and M.C.Downer,Single-shot measurement of temporal phase shifts by frequency-domain holography[J],Opt.Lett.25,764-766(2000)
    [34]K.Y.Kim,I.Alexeev,and H.M.Milchberg,Single-shot supercontinuum spectral interferometry[J].Appl.Phys.Lett.81,4124-4126(2002)
    [35]Y.Kitagawa,H.Fujita,R.Kodama.Prepulse-free petawatt laser for fast ignitor[R].ILE Osaka Univ.Ann.Progr.Rep.,2002.12-21
    [36]J.D.Bonlie,F.Patterson,D.Price et al.Production of>10~(21)W/cm~2 from a large-aperture Ti:sapphire laser system[J],Appl.Phys.B,2002,70(Suppl.):155-160
    [37]K.Yamakawa,M.Aoyama,Y.Akahane et al.Generation of a 0.55-PW,33-fs laser pulse from a Ti:sapphire laser system[J].Laser Letter,2002,30(12):747-748
    [38]M.Aoyama,K.Yamakawa,Y.Akahane et al.0.85-PW,33-fs Ti:sapphire laser[J].Opt.Lett.,2003,28(17):1594-1596
    [39]K.Yamakawa,M.Aoyama,S.Matsuoka et al.100-TW sub-20-fs Ti:sapphire laser system operating at a 10-Hz repetition rate[J].Opt.Lett.,1998,23(18):1468-1470
    [40]A.Antonetti,F.Blasco,J.P.Chambaret,et al,A laser system producing 5×1019 W/cm2 at 10 Hz[J],Appl.Phys.B,65,197,1997
    [41]C.P.J.Barty,C.L.Gordon,B.E.Lemoff,et al,Methods for generation of 10-Hz 100-TW optical pulses SPIE,2377,311,1995
    [42]B.C.Stusrt,M.D.Perry,J.Miller,et al,125-TW Ti:sapphire/Nd:glass laser system[J],Opt.Lett,22,242-244,1997
    [43]Esarey E et al Overview of plasma-based accelerator concepts[J],1996 IEEE Trans.Plasma Sci.24252
    [44]Sprangle P et al Stable Laser-Pulse Propagation in Plasma Channels for GeV Electron Acceleration[J],2000 Phys.Rev.Lett.85 5110-5113
    [45]Wagner R et al 1997 Phys.Rev.Lett.21 3125
    [46]Tabak M et al Ignition and high gain with ultrapowerful lasers[J],1994 Phys.Plasmas 1 1626-1634
    [47]Zhang J T,STUDY ON THE MECHANISM OF THE FAST IGNITION IN LASER FUSION[J],et al 2001 Acta Phys.Sin.5 921(in Chinese)[张家泰 2001 物理学报 5 921]
    [48]Xu H et al Frequency shift of laser pulse propagating in wakefield[J],2004 Acta Phys.Sin.53 171(in Chinese)[徐涵等 2004 物理学报 53 171]
    [49]Sheng Z M et al,KINETIC EQUATION AND TRANSPORTS OF PLASMA IN A CIRCULARL Y-POLARIZED INTENSE LASER FIELD[J],1994 Acta Phys.Sin.43 37(in Chinese)[盛政明等1994 物理学报 43 37]
    [50]Sheng Z M et al 1993 J.Opt.Soc.Am.B 10 122
    [51]Gordon D F et al Asymmetric Self-Phase Modulation and Compression of Short Laser Pulses in Plasma Channels[J],2003 Phys.Rev.Lett.90 215001
    [52]Glant V E,Zhilinsky A P,Sakharov I E.Fundamentals of Plasma Physics[M],New York,Wiley,1980p.65
    [53]Dendy R.Plasma Physics:An Introductory Course[A],Combridge University Press,1993
    [54]王竹溪,朱洪元主编.中国大百科全书:物理卷[M].北京:中国大百科全书出版社,1987
    [55]朱少平,激光等离子体相互作用.见:惯性约束聚变暑期班讲义(二)[C],乐山,2003
    [56]徐涵,激光尾流场加速电子机理的粒子模拟研究[D].博士学位论文,长沙:国防科技大学,2002
    [57]W.B.Mori,On beat wave excitation of relativistic plasma wave[J],IEEE Trans.Plasma.Sci.PS-15:88,1987
    [58]D.Umstadter,et al,Nonlinear plasma wave resonantly driven by optimized laser pulse train[J],Phys.Rev.Lett.,72:1224,1994
    [59]N.E.Andreev,et al,Resonant excitation of wakefield by a laser pulse in a plasma[J],JETP.Lett.,bf 55:571,1992.
    [60]S.Dalla,et al,Large amplitude plasma wave excitation by means of sequences of short laser pulse[J],Phys.Rev.E.,49:1819,1994
    [61]D.Umstadter,et al.,Resonant laser-driven plasma waves for electrons accelerator[J],Phys.Rev.E.,51:3484,1995
    [62]C.E.Clayton,C.Joshi,C.Darrow et al.Relativistic plasma-wave excitation by collinear optical mixing[J].Phys.Rev.Lett.,1985,53(21):2343-2346
    [63]Y.Kitagawa,T.Matsumoto,T.Minamihata et al.Beat wave excitation of plasma wave and observation of accelerated electrons[J],Phys.Rev.Lett.,1992,68(1):48-51
    [64]C.E.Clayton,K.A.Marsh,A.Dyson et al.Ultrahigher gradient acceleration of injected electrons by laser-excited relativistic electron plasma wave[J].Phys.Rev.Lett.,1993,70(1):37-40
    [65][1]Y.Kitagawa et al.,Beat-wave excitation of plasma wave and observation of accelerated electrons[J],Phys.Rev.Lett.68,48-51(1992)
    [66]C.E.Clayton et al.,Ultrahigh-gradient acceleration of injected electrons by laser-excited relativistic electron plasma waves[J],Phys.Rev.Lett.70,37-40(1993)
    [67]N.A.Ebrahim,Laser beat-wave acceleration of electrons[J],J.Appl.Phys.76,7645(1994)
    [68]L.M.Gorbunov and V.I.Kirsanov,Sov.Phys.JETP 66,290(1987)
    [69]P.Sprangle,E.Esarey,J.Krall et al.Propagation and guiding of intense laser pulses in plasma[J].Phys. Rev.Lett.,1992,69(15):2200-2203
    [70]T.M.Antonsen,Jr,P.Mora.Self-focusing and Raman scattering of laser pulses in tenuous plasmas[J],Phys.Rev.Lett.,1992,69(15):2204-2207
    [71]E.Esarey et al.,Frequency shifts induced in laser pulses by plasma waves[J],Phys.Rev.A 42,3526-3531(1990)
    [72]Gordon D.et al.,Observation of electron energies beyond the linear dephasing limit from a laser-excited relativistic plasmawave[J],Phys.Rev.Lett,1998,80:2133-2136
    [73]Sprangle P,Esarey E,and Ting A.Nonlinear theory of intense laser-plasma interactions[J],Phys.Rev.Lett,1990,41:4463-4469
    [74]高宏,刘盛纲.激光-等离子体加速器研究综述[J].,强激光与粒子束,1999,11,499-503
    [75]Sheng.Z.M et al.,Generation of low frequency electromagnetic solitons in plasmas near the critical density with ultrashort intense laser pulses[J],2003 Acta Phys.Sin.52 125(in Chinese)[盛政明等2003 物理学报 52 125]
    [76]Li B et al.,Study on the spatial localized structure in short and intense laser pulse with underdense plasma[J],2003 High Power Laser and Particle Beams 15 450(in Chinese)
    [77]Liu M W et al.,Variational method in the study of intense laser beams propagation in plasma channels[J],2004 Acta Phys.Sin.53 1419-1424(in Chinese)
    [78]Xu H et al.,Frequency shift of laser pulse propagating in wakefield[J],2004 Acta Phys.Sin.53171-175(in Chinese)
    [79]Yu W et al Frequency conversion of radiation pulses in the presence of plasma waves[J],Phys.Rev.A 46 8021-8023(1992)
    [80]T.Katsouleas,IEEE Trans.Plasma Sci.PS-15(1987),86
    [81]A.L.Akhiezer and R.V.Polovin,Theory of wave motion of an electron plasma[J],Sov.Phys.JETP,3:696,1956.
    [82]ZHAO SHANG-HONG,SHI LEI,LI YU-JIANG,et al,Filamentation of femtosecond laser pulse in atmosphere and its application(in Chinese)[J],LASER TECHNOLOGY.2003,27(3):256-258.
    [83]CHEN LIMING,NAKAJIMA KAZUHISA,HONG WEI,et al,Chinese Optics Letters,2007,5(s1):133-135.
    [84]WAYNE H.KNOX,NATHANIEL M.PEARSON,KATHRYN D.LI,et al.Interferometric measurements of femtosecond group delay in optical components[J].OPTICS LETTERS,1988,13:574-576.
    [85]CHIEN.C.Y,LA FONTAINE.B,DESPAROIS.A,et al.Single-shot chirped-pulse spectral interferometry used to measure the femtosecond ionization dynamics of air[J].OPTICS LETTERS,2000,25(8):578-580.
    [86]RICHARDSON.C.J.K,SPICER.J.B,HUBER.R.D,et al.Direct detection of ultrafast thermal transients by use of a chirped,supercontinuum white-light pulse[J],OPTICS LETTERS,2001,26(14):1105-1107.
    [87]KIM.K,ALEXEEV.I,and MILCHBERG.H,Single-shot measurement of laser-induced double step ionization of helium[J],OPTICS EXPRESS,2002,10(26):1563-1572.
    [88]L.Lepetit,G Cheriaux,and M.Joffre,"Linear techniques of phase measurement by femtosecond spectral inteferometry for applications in spectroscopy[J]",J.Opt.Soc.Am.B 12,2467-2474(1995)
    [89]D.N.Fittinghoff,J.L.Bowie,J.N.Sweetser,R.T.Jennings,M.A.Krumbugel,K.W.DeLong,R.Trebino,and I.A.Walmsley,"Measurement of the Intensity and Phase of Ultraweak,Ultrashort Laser Pulse[J]",Opt.Lett.21,884-886(1996)
    [90]G.Liu,and P.D.Scott,"Phase retrieval and twin-image elimination for in-line Fresnel holograms[J]",J.Opt.Soc.Am.A 4,159-165(1986)
    [91]GOODMAN.JOSEPH W.Introduction to Fourier Optics(in Chinese)[M].Third Edition,Beijing:Publishing House of Electronics Industry,2006,357-360.
    [92]P.Audebert,P.Daguzan,A.Dos Santos,et al,Space-Time Observation of an Electron Gas in SiO2[J].Phys.Rev.Lett.1994,73,1990-1993.
    [93]Marques,J.R.et al.Laser wakefield:experimental studies of nonlinear radial oscillations[J].Phys.Plasmas,1998,10,1124-1134.
    [94]J.-P.Geindre,P.Audebert,S.Rebibo,and J.-C.Gauthier,"Single-shot spectral interferometry with chirped pulses[J]," Opt.Lett,2001,26.1612-1614.
    [95]Y.-H.Chen,S.Varma,I.Alexeev,and H.M.Milchberg,"Measurement of transient nonlinear refractive index in gases using xenon supercontinuum single-shot spectral interferometry[J]".Opt.Express,2007,15,7458-7467
    [96]Piasecki J,Colombeau B,Vampouille M,Froehly C,and Arnaud J A,Nouvelle methode de mesure de la reponse impulsionnelle des fibres optiques[J],1980 Appl.Opt.19.3749-3755.
    [97]Chai L,He T Y,Gao F,Wang Q Y,Xing Q R,and Zhang Z G,Numerical simulation for characterizing femtosecond optical pulses with the SPIDER algorithm[J],2004 Chinese Physics.13,1487-1492.
    [98]K.Osvay,I.N.Ross.Efficient tuneable bandwidth frequency mixing using chirped pulses[J].Opt.Comm.,1999,166:133-119.
    [99]K.Osvay,I.N.Ross.Broadband sum-frequency generation by chirp-assisted group-velocity matching[J].J.Opt.Soc.Am.B,1996,13:1431-1438
    [100]韩伟,折返点匹配宽带二倍频研究[D].硕士学位论文,绵阳:中国工程物理研究院,2006
    [101]Pablo Gabolde and Rick Trebino.Single-shot measurement of the full spatio-temporal field of ultrashort pulses with multi-spectral digital holography[J].OPTICS EXPRESS.2006.14. 11460-11467
    [102]黄小军,彭翰生,魏晓峰等,100TW级超短超强钛宝石激光装置[J],强激光与粒子束,2005,17,1685-1688.

© 2004-2018 中国地质图书馆版权所有 京ICP备05064691号 京公网安备11010802017129号

地址:北京市海淀区学院路29号 邮编:100083

电话:办公室:(+86 10)66554848;文献借阅、咨询服务、科技查新:66554700