期刊文献+

神光-Ⅲ原型装置全光路系统波前测量方法 被引量:2

Entire Beam Wavefront Measurement in Prototype of SG-Ⅲ Facility
原文传递
导出
摘要 为进一步提高神光-Ⅲ原型装置8束三倍频激光焦斑的能量集中度,需要对神光-Ⅲ原型装置的全光路系统波前进行校正。其中的关键技术之一就是要准确获得全光路系统的波前畸变。神光-Ⅲ原型装置的8束激光主放诊断包内均配置了一套哈特曼波前传感器,可以较为方便地获得主放大系统输出波前,但却无法直接获得靶场系统波前。解决方法主要有逆向标定和靶点直接测量两种,通过比较两种方法的技术复杂性、测量准确性等指标,结合对校正前后远场焦斑的测量,最终确定采用靶点直接测量的方法能简单、有效地获得全光路系统波前畸变。 In order to improve focal spot concentration of 3ω laser,entire beam wavefront should be corrected.One of key technologies is to get entire beam wavefront aberration exactly.With Hartman wavefront sensor located at parameters diagnosis unit of main amplifier,wavefront of output main amplifier can be obtained.However,wavefront of target system can′t be measured directly.There are two methods to solve this problem including reverse calibration and direct measurement at target point.By comparing complexity and accuracy of the two methods,and combining far field measurement with and without correction,direct measurement at target point is a simple and correct method to get entire beam wavefront.
出处 《中国激光》 EI CAS CSCD 北大核心 2011年第2期45-47,共3页 Chinese Journal of Lasers
基金 中国工程物理研究院科学技术发展基金(2009A0401023)资助课题
关键词 激光光学 高功率固体激光 标定 哈特曼波前传感器 波前 焦斑 laser optics high power solid-state laser calibration Hartman wavefront sensor wavefront focal spot
  • 相关文献

参考文献7

  • 1M. L. Spaeth, K. R. Manes, C. C. Widmayer et al.. National ignition facility wavefront requirements and optical architecture [J]. Opt. Eng., 2004, 43(12): 2854-2865.
  • 2Y. D. Zhang, Z. P. Yang, H. F. Duan et al.. Characteristics of wavefront aberration in the single beam principle prototype of the next generation ICF system [C]. SPIE, 2002, 4825: 249-256.
  • 3J. T. Salmon, E. S. Bliss, J. L. Byrd et al.. An adaptive optics system for solid-state laser systems used in inertial confinement fusion [C]. SPIE, 1997, 2633: 105-113.
  • 4R. A. Zacharias, E. S. Bliss, S. Winters et al.. Wavefront control of high-power laser beam in the national ignition facility [C]. SPIE, 2000, 3889: 332-343.
  • 5代万俊,胡东霞,周维等.TIL装置原型自适应光学系统应用技术研究.光学学报,2008,.
  • 6代万俊,胡东霞,周维等.激光驱动器波前补偿系统的方案设计.中国激光,2009,.
  • 7代万俊,胡东霞,周维,刘红婕,赵军普,张崑,蒋学君,景峰.高功率固体激光装置哈特曼传感器参考波前标定方法[J].强激光与粒子束,2008,20(9):1413-1416. 被引量:5

二级参考文献8

  • 1Zhang Y D, Yang Z P, Duan H F, et al. Characteristics of wavefront aberration in the single beam principle prototype of the next generation ICF system[C]//Proc of SPIE. 2002, 4825:249-265.
  • 2Spaeth M L, Manes K R, Widmayer C C, et al. National Ignition Facility wavefront requirements and optical architecture[J]. Opt Eng, 2004, 43(12) 22854-2865.
  • 3Hartley R, Kartz M, Behrendt W, et al. Wavefront correction for static and dynamic aberrations to within 1 second of the system shot in the NIF beamlet demonstration facility[C]//The 2^nd Annual International Conference on Solid-State Lasers for Application to ICF. 1996.
  • 4Zacharias R, Bliss E, Winters S, et al. Wavefront control of high-power laser beams in the National Ignition Facility[C]//Proc of SPIE. 2000, 3889:332-343.
  • 5Jiang W H, Rao X J, Ling N, et al. Laser wavefront measurement of ICF amplifiers using Hartmann-Shaek wavefront sensor[C]//Proc of SPIE. 2000, 4124 : 148-157.
  • 6Salmon J T, Bliss E S, Karts M W, et al. Absolute wavefront measurements of high-energy laser beams in the Beamlet Demonstration Project for the National Ignition Facility[R]. UCRL-JC-119004, 1995.
  • 7Chernyshov A, Ster U, Fritz R, et al. Calibration of a Shack-Hartmann sensor for absolute measurements of wavefronts[J]. Optical Society of America, 2005, 44(30) :6419-6425.
  • 8Zacharias R A, Beer N R, Bliss E S, et al. National Ignition Facility alignment and wavefront eontrol[C]//SPIE International Society for Optical Engineering Photonics West 2004. 2004, 5341 : 168-179.

共引文献4

同被引文献24

  • 1P J Wegner, M A Henesian, D R Speck, et al: Harmonic con- version of large-aperture 1.05-μm laser beams for inertial-confine- ment fusion research[J]. Appl Opt, 1992, 31(30), 6414-6426.
  • 2C A Haynam, P J Wegner, J M Auerbach, et al: National Igni- tion Facility laser performance status [J]. Appl Opt, 2007, 46(16): 3276-3303.
  • 3H M George, I M Edward, R W Craig. The National Ignition Fa- cility[J]. Opt Eng, 2004, 43(12): 2841-2843.
  • 4E I Moses, R E Bonanno, C A Haynam, et al: The National Ig- nition Facility: path to ignition in the laboratory[J]. Eur Phys J D, 2007, 44(2): 215-218.
  • 5M L Spaeth, K R Manes, C C Widmayer, et al: National Ignition Facility wavefront requirements and optical architecture[J]. Opt Eng, 2004, 43(12): 2854-2857.
  • 6J M Auerbach, C E Barker, S A Couture, et al: Modeling of fre- quency doubling and tripling with converter refractive index spa- tial non-uniformities due to gravitational sag[C]. SPIE, 1999, 3492: 472-474.
  • 7L Olivier, G Claude. Modeling of the effects of KDP crystals grav- ity sag on third harmonic generation[C]. SPIE, 1999, 3492: 802-808.
  • 8S Moaveni. Finite Element Analysis: Theory and Application with ANSYSEM]. London: Prentice Hall PTR Upper Saddle River, 1999. 168-231.
  • 9P W Milonni, J M Auerbach, D Eimerl. Frequency conversion modeling with spatially and temporally varying beams[C]. SPIE, 1997, 2633: 230-241.
  • 10Y Altintas, D Montgomery, E Budak. Dynamic peripheral millingof flexible structures[J]. J Engineering for Industry, 1992, 114(2) : 137-145.

引证文献2

二级引证文献3

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部