用户名: 密码: 验证码:
高功率激光靶面均匀辐照技术的研究
详细信息    本馆镜像全文|  推荐本文 |  |   获取CNKI官网全文
摘要
在惯性约束聚变(ICF)等精密物理实验研究中对高功率激光靶面辐照的均匀性提出了苛刻的要求。实现靶面均匀辐照是实验成败的关键因素,也是当前该领域中前沿性课题,具有重要的学术价值和实际意义。本论文主要研究在强激光技术中对靶面均匀辐照问题有重要意义的列阵式均匀辐照光学系统,取得了以下主要结果:
     1.首次提出了正交柱透镜列阵光学系统(OCLA),应用标量衍射积分理论和傍轴矩阵光学的方法,给出了系统的设计原理和OCLA系统远场和准远场光强分布的解析表达式,并对OCLA系统的匀滑特性进行了详细的数值模拟和优化设计。提出了应用离焦打靶和消衍射方法抑制OCLA系统的大尺度不均匀性。
     2.提出了两种焦斑可调的列阵式点聚焦系统,①焦斑可调的透镜列阵均匀辐照光学系统,②可变焦正交柱透镜列阵均匀辐照光学系统。应用矩阵光学和广义衍射积分理论分析了两变焦均匀辐照光学系统的工作原理和优化设计的参数。对两可变焦列阵式均匀辐照光学系统的数值模拟和Zemax光学软件的检验,证实了其匀滑的效果。
     3.通过理论和实验详细研究了正交光楔列阵(CSWA)聚焦系统的小尺度不均匀性的变化规律。根据波动物理光学,首次推导出了CSWA系统的多光束干涉条纹主极大和两相邻主极大间的次极大间距公式,应用柯林斯公式和ABCD传输矩阵理论由数值模拟计算证明了CSWA的小尺度不均匀性的变化规律。对两种抑制CSWA系统小尺度不均匀性(the SSRNU)的方法楔角偏差和离焦打靶建设进行了理论和实验研究,两者符合的非好。给出了楔角偏差和离焦量的最佳设计参数。
     4.应用偏振控制板(PCP)和正交柱透镜列阵结合的方法抑制靶面的小尺度辐照不均匀性。应用物理光学软件GLAD对该方案的匀滑效果进行了详细的三维数值模拟,并通过适当离焦,均匀度和能量利用率都可达到最佳值。
     5.基于部分相干光的传输规律和广义衍射积分理论,由高斯—谢尔模型(GSM)光束描述准单色部分空间相干光,建立了部分相干光PCL通过透镜列阵系统光强分布的理论模型以降低焦斑的小尺度(高阶模)不均匀性,通过详细的三维数值计算分析表明,与完全相干光通过该匀滑系统时相比更能显示该方案匀滑效果的优越性。如果考虑横向热平滑效果以及靶面适当离焦时,靶面上的高频空间光强调制可以得到进一步的抑制,可得到最好的辐照均匀性和能量利用率。
In the sophisticated physical experimental researches, such as inertial confinement fusion (ICF), there are the harsh demands for the irradiation uniformity on the target surface with high-power laser. Achieving uniform irradiation of laser intensity on the target is a critical factor in experiments and also the forefront of current issues in the field, which has important academic value and practical significance. In this thesis, array uniform irradiation optical systems are studied, and the following main results are listed:
     1.An orthogonal cylindrical lens array (OCLA) optical system is presented for uniform irradiation on target surface.Based on the paraxial matrix optics and scalar diffraction integral theory, we put forward the designing principle of the OCLA system and the analytical expression of the intensity distribution; simultaneously, the OCLA system both in far field and in semi-far field has also been considered. Through numerical simulation, the smoothing characteristics and optimized designing for this system are obtained in details.The elimination of large-scale non-uniformity with the defocused irradiation and diffraction-weakened methods are proposed.
     2.Two kinds of point-focusing array systems with controllable focal spot are proposed:(a) lens arrays optical system with vari-focal-spot, and (b) orthogonal cylindrical lens arrays (OCLA) system with controllable focus length. Based on the paraxial matrix optics and generalized diffraction theory, the principles of the two vari-focus array optical systems, and the optimization of these optical systems parameters are analyzed in details. The smoothing performances of the two vari-focal array systems are confirmed by the numerical simulation and the theoretical calculation with Zemax optics design software.
     3. The variation in small-scale non-uniformity (SSINU) of intensity in crossed segmented wedge array (CSWA) focus system is studied theoretically and experimentally. Based on the physical optics, the separation between the major interference maxima and secondary maximum of interference fringes for the CSWA focus system are derived firstly. The variation of the SSINU has been confirmed by the numerical calculations on the basis of the Collins formula and ABCD propagation matrix theory.From the theory and experiment, we have studied the two methods of reducing the SSRNU, named after the deviation of wedge angles (DWA) and the off-focal laser radiation on target (OFLRT), and results demonstrated that they have a quite good agreement. The DWA, the OFLRT, and their optimized parameters are presented.
     4. Suppression of small-scale non-uniformity is realized, using the combination of the orthogonal cylindrical lens array and polarization control plate.The smoothing performance of the scheme is also analyzed by the detailed three-dimensional simulations with GLAD physical optics software. Moving the target slightly away from the exact focal plane of the principal focusing lens, a well-irradiating laser spot with small non-uniformity and great energy efficiency can be obtained accordingly.
     5.Based on propagation law of partially coherent light (PCL) and generalized diffraction theory, a PCL model is established, in which a quasi-monochromatic spatially partial coherent light is described by Gaussian Schell-Model (GSM) beams through the lens array system. Detailed three-dimensional numerical calculations show that the partial coherent light is advantageous in smoothening effects and reducing the small-scale non-uniformity over the complete coherent light. Moving the target slightly from the exact focal plane of the principal focus, and taking advantage of the effect of lateral thermal conduction smoothing, the high spatial-frequency intensity fluctuation can be further eliminated, which indicates the best possible irradiation uniformity and energy efficiency on the target.
引文
[1]王淦昌,袁之尚.惯性约束核聚变[M].北京:原子能出版社,2005.
    [2]贺贤士.惯性约束核聚变研究进展和展望[J].核科学与工程,2000,20(3):248-251.
    [3]朱士尧.核聚变原理[M].合肥:中国科大出版社,2002.
    [4]Lawson. J D. Some Criteria for a Power Producing Thermonuclear Reactor[J]. Proc. Phys. Soc.1957, B70(1):6-10.
    [5]张家泰.激光等离子体相互作用物理与模拟[M].郑州:河南科学技术出版社,1999.
    [6]Wang G C. Suggestion of Neutron Generation with Powerful lasers[J]. Chinese J of Lasers,1987, 14(11):641-644.
    [7]巴索夫等著,华欣生主译.稠密等离子体诊断学[M].强激光与粒子束杂志社,1992.
    [8]Nuckolls J H, Wood L, Hiessen A T et al.. Laser compression of matter to super-high densities: thermonuclear (CTR) application[J]. Nature,1972,239(15):139-142.
    [9]范滇元,贺贤土.惯性约束聚变能源与激光驱动器[J].大自然探索,1999,18(67):31-35
    [10]林尊琪.激光核聚变的发展[J].中国激光,2010,37(9):2202-2207.
    [11]Bodner S E, McCrory R L, Afeyan B B. Direct-drive laser fusion:Status and prospects[J]. Phys.Plasmas,1998,5(5):1901-1918.
    [12]Lindl J. Development of the indirect-drive approach to inertial confinement fusion and the target physics basis for ignition and gain[J]. Phys. Plasmas,1995,2(11):3933-4024.
    [13]肖峻,吕百达,翟群.激光间接驱动聚变柱形腔靶内壁光斑参数计算[J].强激光与粒子束,1998,10(1):62-65.
    [14]Campbell E M.21世纪的惯性聚变科学技术[J].激光与光电子学进展,2003,40(6):1-5.
    [15]范滇元,张小民,激光核聚变与高功率激光:历史与进展[J].物理,2010,39(9):589-596
    [16]彭翰生,张小民,范滇元.高功率固体激光装置的发展与工程科学问题[J].中国工程科学,2001,3(3):1-8.
    [17]江少恩,丁永坤,缪文勇等,我国激光惯性约束聚变实验研究进展[J].中国科学G辑物理学力学天文学2009,39(11):1571-1583.
    [18]Yamanaka C, Inertial fusion research over the past 30 years[J]. Fusion Engineering and Design 1999, 44:1-12.
    [19]Skupsky S, Lee K. Uniformity of energy deposition for laser driven fusion[J]. J. Appl. Phys.,1983. 54(7):3662-3671.
    [20]Schmitt A J. Absolutely uniform illumination of laser fusion pellets[J]. Appl. Phys. Lett.,1984, 44(4):399-401.
    [21]Mccrory R and Verdon C. Inertial Confinement Fusion [M]. Compositor, Bologna.Italy:edited by Caruso A and Sindoni E,1989,183.
    [22]Rothenberg J E, Eimerl D, Key M H et al. Illumination uniformity requirements for direct drive inertial confinement fusion [R], UCRL-JC-121195,1995.
    [23]Howard J E. Uniform targets illumination of spherical laser fusion [J]. Appl. Opt.977.16: 2764-2770.
    [24]Scannapieco A J and Btysk H. Illumination and energy deposition in a multibeam laser fusion system[J]. J. Appl. Phys.1979,50(8):5142.
    [25]肖峻,吕百达,冯国英等.激光直接驱动聚变球靶初始辐照均匀性分析[J].光学学报,1998,18(12):1646-1651.
    [26]谢永杰,刘晶儒,赵学庆.ICF中光束平滑及靶面辐照均匀性技术评述[J].激光技术,2001,25(6):454-459.
    [27]Chandrasekhar S. The stability of superposed fluids:the Rayleigh-Taylor Instability, Hydrodynamic and Hydromagnetic Stability[M]. Press, Oxford University.1961, chapter 10.
    [28]Emery M H, Gardner JH and Boris J P. Rayleigh-Taylor and Kelvin Helmholtz Instabilities in Targets Accelerated by Laser Ablation [J]. Phys. Rev. Lett.1982,48(10):677-680.
    [29]Takabe H, Mima K, Montierth L et al. Morse. Self-consistent growth rate of the Rayleigh-Taylor instability in an ablatively accelerating plasma[J]. Phys. Fluids,1985,28(12):3676.
    [30]Murakami M. Analysis of radiation symmetrization in hohlraum targets[J].1992, Nucl. Fusion 32(10):1715-1724.
    [31]Rothenberg J E, Auerbach J M, Moran B D et al. Implementation of smoothing by spectral dispersion on beamlet and NIF[R]. UCRL-JC-129771,1998.
    [32]肖峻,吕百达,翟群.激光间接驱动聚变柱形腔靶内壁光斑参数计算[J].强激光与粒子束,1998,10(1):62-65.
    [33]常铁强.激光等离子体相互作用与激光聚变[M].长沙:湖南科学技术出版社,1991:54-55.
    [34]郑志坚,谢平,孙可熙等.黑腔物理定律规律[J].强激光与粒子束,1993,5(4):575-580.
    [35]陈家斌,郑志坚,道源等.靶激光能量注入率的新途径[J].强激光与粒子束,1998,2(5):239-242.
    [36]Villeueuve D M, Enright G D and Baldis H A. Novel laser line focus geometry applied to X-ray lasers[J].Opt. Commun.,1991,81(1,2):54-58.
    [37]陈万年,工树森,陈斌等.用于x射线激光实验研究的列阵柱而透镜线聚焦系统[J].光学学报.1991,11(9):829-833.
    [38]X. Deng, X. Liang, Z. Cheng et al.. Uniform illumination of large targets using a lens array [J]. Appl. Opt..1986,25(2):377-381.
    [39]江秀娟,林尊琪.高功率激光驱动器光束匀滑技术的研究进展[J].激光与光电子学进展,2010,47(9):22-29.
    [40]Born M, Wolf E. Principles of Optics [M]. Great Britain:Pergamon Press,1978.
    [41]Tsubakinoto K, Nakatsuka M, Nakano H et al. Suppression of interference speckles producced by a random phase plate, using a polarizaLion control plate[J]. Opt.Communl..1992,91(1,2):9-12
    [42]Miyanaga N, Nakano H, Tsubakimoto K et al. Partially coherent light for improving irradiation uniformity in directly driven laser fusion experiments[R]. Laser Interaction and Related Plasma Phenomena, Editctl by G.H.Miley and H.Hora, Plenum Press. New York,1992,10:251-280.
    [43]Lehmberg R H, Schmitt A J, Bodner S E, Theory of induced spatial incoherence [J]. J.Appl.Phys.1987, (62)7:2680-2701.
    [44]Zhou S L, Lin Z Q, Jiang X J. Two-dimensional performance of uniform irradiation with the use of an edge-softened lens array and spectral dispersion [J]. Appled Optics2007, (46)16:3164-3168.
    [45]Kato Y, Mima K, Miyannaga N et al. Random phasing of high-power lasers for uniform target acceleration and plasma-instability suppression[J].Phys. Rev. Lett.,1984,53 (11):1057-1060.
    [46]Skupdky S, Kessier T J. Speckle-free plate (diffuser) for far-field application[J]. J. Appl. Phys., 1993,74(7):4310-4316.
    [47]肖峻,吕百达.用零相关相位板匀滑散斑的理论研究[J].光学学报,2000,20(10):1341-1346.
    [48]Kao Y, Mina K, Miyanaga N, et al. Ramdom phasing of high-power laser for uniform target acceleration and plama-instability suppression [J]. Physical Review Letters,1984,53(11): 1057-1060.
    [49]Stevenson R M, Norman M J, Bett T H et al. Binary-phase zone plate arrays for the generation of uniform focal profiles[J]. Opt. Lett.,1994,19:363-365.
    [50]肖峻,吕百达.偏振控制板对干涉斑纹的匀滑特性[J].中国激光,2000,27(7):627-632.
    [51]郑建洲,蔡邦维,吕百达等.二维正交光楔阵列大焦斑均匀照明光学系统的实验研究[J].中国激光.1997,(A24)12:1008-1012.
    [52]Yoon G, Jitsuno T,.Nakatsuka M et al. Kato. Development of a large aperture deformable mirror for the wavefront control[J]. proc. SPIE,1997 (3047):777-782.
    [53]Dixit S N, Lawson J K, Manes K R et al. Kinoform phase plates for focal plane irradiance profile control [J]. Opt. Lett.1994,19(6):417-419.
    [54]Rothenberg J E. Electro-Optic Deflectors as a method of beam smoothing for inertial confinement fusion[J]. SPIE,1997,3047(12):707-712.
    [55]Nakano H, Kanabe T, Yagi K et al..Amplification and propagation of partially coherent amplified spontaneous emission from Nd:glass[J].Opt. Commun.,1990,78:123-127.
    [56]Nakano., Tsubaltimoto K, Miyanaga N, et al. Spectally dispersed amplified spontaneous emission for improving irradiation uniformity into high power Nd:glass laser system[J]. J. Appl. Phys.,1993, 73(5):2122-2131.
    [57]Nakano H, Miyanaga N, Yagi K et al.. Partially coherent light generated by using single and multimode optical fibers in a high-power Nd:glass laser system[J]. Appl. Phys. Lett.,1993,63(5): 580-582.
    [58]金国藩,严瑛白,邬敏贤.二元光学[M].北京:国防工业出版社,1998.
    [59]Lin Y, Kessler T J, Lawrence G N. Distributed phase plates for super-Gaussian focal-plane irradiance profiles[J]. Opt. Lett.1995,20(7):764-766.
    [60]Neauport J, Ribeyre X, Daurios J, et al.Design and optical characterization of a large continuous phase plate for laser integration line and laser Megajoule facilities[J]. Applied Optics,2003;42(13): 2377-2382.
    [61]陈波,工涵子,韦辉等.用于惯性约束聚变束匀滑的完全连续相位板设计方法[J].光学学报.2001,21(4):480-483.
    [62]江秀娟,周申蕾,林尊琪.利用二维光谱色散和透镜列阵改善靶面辐照均匀性[J]中国激光2007,34(11):1533-1537.
    [63]Morkry P. Computer-generated diffraction optical elements[J]. Proc.Soc.Photo.Opt. Instrum. Eng. 1989,1052:163-170.
    [64]杨国祯,顾本源.衍射光学元件的设计方法[J].物理,1995,23:200-205.
    [65]Moharam M G, Gaylord T K. Rigorous coupled-wave analysis of planar-grating diffraction[J]. J.Opt.Soc.Am,1981,71:811-818.
    [66]Moharam M G, Gaylord T K. Rigorous coupled-wave analysis of grating diffraction E-mode polarization and losses[J]. J. Opt. Soc. Am,1983,73:451-455.
    [67]Pomment D A, Moharam M G. Limits of scalar diffraction theory for diffractive phase elements[J]. J.Opt.Soc.Am.A,1994,11:1827-1834.
    [68]Born M and Wolf E. Principles of optics[M].6th edition, London:Pergamon Press,2007.
    [69]高福华.衍射光学在ICF激光驱动系统中的应用研究[D](博士学位论文),四川大学,2004:1530.
    [70]严瑛白.应用物理光学[M].北京:机械工业出版社,1990:239-241.
    [71]Dixit S N, Thomas I M, Woods B W et al. Random phase plates for beam smoothing on the Nova Laser[J]. Appl. Opt.,1993,32(14):2543-2554.
    [72]丘悦,黄宏一,范滇元等.可变焦列阵柱面透镜均匀线聚焦系统[J].光学学报,1994,14(11):1198-1203.
    [73]Skupsky S, Lee K. Uniformity of energy deposition for laserdriven fusion[J]. J. Appl. Phys.,1983, 54(7):3662-3671.
    [74]Siegman A E. Lasers, California. University Science Books, Mill Valley,1986.
    [75]韦伯H.激光谐振腔[M].武汉,华中工学院出版社,1983.
    [76]郑建洲,于清旭.正交柱透镜列阵光学系统及优化设计[J].光电工程,2006,33(7):28-33.
    [77]Miyanaga N, Matsuoka S, Ando A et al. Improvement of laser irradiation uniformity in Gekko Ⅻ glass laser system[J]. SPIE,1995,2633:183-190.
    [78]Pepler D A, Danson C N, Bann R, et al. Focal spot smoothing and tailoring for high-power laser applications [J]. SPIE,1993,1870:76-87.
    [79]Lu B, Zhang B, Cai B, Zheng J. Changes in small-scale intensity modulations of several array focus system[J]. Optik,1998,108(3):124-128.
    [80]刘忠永,吕百达,蔡邦维等.用偏振和有规位相分布抑制线聚焦系统的小尺度不均匀性[J].光学学报,1995,15(12):1626-1632.
    [81]Skupsky S, Short R W, Kessier T et al..Improved laser-beam uniformity using the angular dispersion of frequency-modulated light[J]. J. Appl. Phys.,1989,66(8):3456-3462.
    [82]傅思祖,孙玉琴,黄秀光等.“神光—Ⅱ”装置靶面均匀辐照系统的优化设计[J].中国激光,2003,30(2):129-133.
    [83]刘忠永,蔡邦维,吕百达.用正交光楔列阵获得连续可调的均匀方形光斑[J].1996,A23(8):702-706.
    [84]Lu B D, Cai B W, Lui Z Y et al. Improved segmented wedge arrays system with controllable line focus length. [J]. Opt. Commun.1996,125(4):48-52.
    [85]郑建洲,于清旭,卢永军.焦斑可调的透镜阵列均匀辐照光学系统[J].中国激光,2007,34(3):331-336.
    [86]Zheng J Z, Yu Q X, Bin D et al. Improved two-dimensional orthogonal cylindrical lens Arrays optical system with controllable focus profile for uniform irradiation[J].proc. SPIE.2008,7282: 72820Y1-72820Y10.
    [87]Lu B, Zheng J, Cai B. Tow-dimensional focusing of laser beams to provide uniform irradiation[J]. Opt Commun.1998,149(1):19-26.
    [88]丘悦,钱列加,黄宏一等.用消衍射方法改善透镜列阵的辐照均匀性[J].中国激光,1995,A22(1):27-31.
    [89]钱列加,龚伟,文国军等.波纹圆孔光阑的衍射及其设计[J].光学学报,1995,15(1):117-121.
    [90]Rothenberg J E, Weber S V. The impact of beam smoothing method on direct drive target performance for the NIF[J]. Proc of SPIE.1997,3047:736-745.
    [91]Pennington D M, Dixit S N, Weiland T L et al. Implementaltion and performance of beam smoothing on 10 beams of the Nova laser[J]. SPIE,3047:725-730.
    [92]Lowenthal F, Prog A, Balmer J, E. Reduction of small-scale intensity modulation in a line focus produced by a cylindrical lens array using polarization control and wedge angles [J]. Opt. Commun. 1997,135(1)7-13.
    [93]Nakano H, Miyanaga N, Yagi K et al. Partially coherent light generated by using single and multimode optical fibers in a high-power Nd:glass laser system [J]. Appl. Phys. Lett.1993,63(5):580-582.
    [94]Zhou S L, Lin Z Q, Jiang X J. Beam smoothing by lens array with spectral dispersion [J]. Opt. Commun.2007,272(1):186-191.
    [95]Tsubakimoto K, Jitsuno T, Miyanaga N et al. Suppression of speckle contrast by using polarization property on second harmonic generation, Opt. Communn.,1993,103(3,4):185-188.
    [96]Tsubakmoto K. Studv on improving irradiation unifmrnity of spherical target for laser fusion[D]. Ph. Dissertation D. Chap. V. Osaka University,1993,77-87.
    [97]丹尼蒂JC编,黄乐天、王天及等译.激光斑纹及有关现象[M],第二章,激光斑纹的统计特性,科学出版社,1981.
    [98]郑建洲,于清旭,关寿华.正交光楔列阵光学系统小尺度不均匀性的研究[J],光学精密工程,2009年,Vol.17,No.1:1195-1201.
    [99]Jianzhou Zheng, Wenyang Zheng,Yu Qingxu et al. Improved uniformity of target irradiation by combining an Orthogonal Cylindrical Lens Array and the polarization control, Proc. of SPIE, Vol. 7654:765400-1-7654008.
    [100]吕百达.激光光学[M].高等教育出版社,2003.
    [101]周申蕾,林尊琪.谱色散平滑与透镜列阵联用实现均匀照明[J],光学学报,2007年,vol.27.No2:275-279.
    [102]2000,7(5):2062-2068.
    [103]Shirai T, Asakura T. Spatial coherence of light generated from a partially coherent source and its control using a source filter. Optik,1993,94(1):1-15.
    [104]Lu B D, Zhang B, Liu Z Y et al. Modelling the cylindrical lens array line focus system illuminated by partially coherent light [J] Opt. Comm.1995,114(1):181-188.

© 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