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宏-微脉冲激光激发钠信标回波光子数的数值计算与探讨 被引量:2

Numerical calculation and discussion on the return photon number of sodium laser beacon excited by a macro-micro pulse laser
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摘要 当采用低功率的宏-微脉冲激光激发钠信标时,尽管激光传输和钠信标光斑大小受到大气湍流影响,但是钠信标具有回波光子数无起伏且激发品质因数高的优点.除此之外,宏-微脉冲激光激发钠信标还与激光的宏脉冲线型有关.对于高斯线型的宏脉冲,增大微脉冲的宽度有利于提高激发钠信标的品质因数和激发态概率.为了获得更多的钠信标回波光子和较小的钠信标半径,增大激光功率的同时要考虑良好的光束质量、适当的激光发射口径以及光谱宽度等影响因素.因此,优选宏-微脉冲激光的参数、发射口径、发射方式等对于激发优良特性的钠信标有着重要的现实意义. Sodium laser beacon (SLB) excited by a macro-micro pulse laser with low power has the following advantages: the return photons without fluctuations and the high merit quantity, although the laser beam propagation and the size of SLB suffer form the atmospheric turbulence. In addition, the macro-pulse profile may influence the interaction of laser and sodium atoms. For the macro-pulse with a Gaussian profile, it is useful to enhance the merit quantity and the excitation probability of the SLB to increase the width of micropulse. In order to obtain more of the return photons in the SLB, while increasing the laser power, the fine beam quality, the appropriate launch diameter, and the spectral width of the laser etc. must be considered. Therefore, it is of practical significance for the SLB with fine characteristics to optimize the laser parameters, the launch diameter and launch pattern.
出处 《物理学报》 SCIE EI CAS CSCD 北大核心 2015年第9期317-327,共11页 Acta Physica Sinica
基金 安徽省高校自然科学基金(批准号:KJ2013A260 KJ2013B331) 国家自然科学基金(批准号:61107066)资助的课题~~
关键词 宏-微脉冲激光 钠信标 品质因数 发射口径 macro-micro pulse laser, sodium laser beacon, merit quantity, launch diameter
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参考文献18

  • 1Bradley L C 1992 J.Opt.Soc.Am.B 9 1931.
  • 2Telle J M,Milonni P W,Hiliman P D 1998 Proc.SPIE 3264 37.
  • 3Kibllewhite E,Shi F 1998 Proc.SPIE 3353 300.
  • 4Milonni P W,Thode L E 1992 Applied Optics 31 785.
  • 5Stephen C R 2010 Nonlinear and Quantum Optics using the Density Matrix (British: Oxford University Press) p43.
  • 6Temkin R J 1993 J.Opt.Soc.B 10 830.
  • 7Jelonek M P,Fugate R Q,Lange W J,Slavin A C,Ruane R E,Cleis R A 1994 J.Opt.Soc.Am.A 11 806.
  • 8Telle J M,Milonni P W,Hiliman P D 1998 Proc.SPIE 3264 37.
  • 9Humphreys R A,Bradley L C,Herrmann J 1992 The Lincoln Laboratory Journal 6 45.
  • 10朱文越,黄印博,钱仙妹,饶瑞中,王英俭.激光大气传输模拟程序CLAP及其应用[J].大气与环境光学学报,2007,2(6):451-458. 被引量:16

二级参考文献9

  • 1[1]Strohbehn J W.Laser Beam Propagation in the Atmosphere[M].New York:Springer-Verlag,1978.
  • 2[2]Gebhardt F G.Twenty-five years of thermal blooming:an overview[C].Proc.SPIE,1990,1221:2-25.
  • 3[3]Beland R R.Propagation Through Atmospheric Optical Turbulence[M].The Infrared and ElectroOptical Systems Handbook.Bellingham:SPIE Optical Engineering Press,1993.
  • 4[4]Mehta,Naresh C.GRAND:a 4-D wave optics code for atmospheric laser propagation[C].Proc.SPIE,1991,1487:398-409.
  • 5[11]Knepp D L.Multiple phase-screen calculation of the temporal behavior of stochastic waves[J].Proc.of the IEEE,1983,71(6):722-737.
  • 6[12]Martin J M,Flatte S M.Intensity images and statistics from numerical simulation of wave propagation in 3-D random media[J].Appl.Opt.,1988,27(11):2111-2126.
  • 7[13]Coles W A,Filice J P,Frehlich R G,et al.Simulation of wave propagation in three-dimensional random media[J].Appl.Opt.,1995,34(12):2089-2101.
  • 8[14]Horwath J,Perlot N,Giggenbach D,et al.Numerical simulations of beam propagation through optical turbulence for high-altitude platform crosslinks[C].Proc.of SPIE,2004,5338:243-252.
  • 9[15]Martin J M,Flatte S M.Simulation of pointsource scintillation through three-dimensional random media[J].J.Opt.Soc.Am.A,1990,7(5):838-847.

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