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讨论两种散射,导出相应的分布函数,运用蒙特卡罗法模拟光子在无序介质中的随机行走过程,得到非相干背散射空间分布及反射率.计算结果表明:散射不同,非相干背散射空间分布和反射率不同,非相干背散射反射率随光入射角增大而增大;非相干背散射反射率随无序介质吸收系数增大而减小,通过测量非相干背散射反射率可得吸收系数,进一步可得每次散射光子被微粒吸收的概率;非相干背散射反射率随光子平均自由程增大而减小,通过测量非相干背散射反射率可得平均自由程,这比检测相干背散射来得到平均自由程要容易.最后,讨论了背散射对无序激光器的影响.

参考文献

[1] Letokhov V S.Generation of light by scattering medium with negative resonance absorption[J].Soy.Phys.JEPT,1968,26:835.
[2] Lawandy N M,Selschandran R M,Lgomes A S,et al.Laser action in strongly scattering media[J].Nature,1994,368(3):436-438.
[3] Wiersma D S,Lagendijk A.Light diffusion with gain and random lasers[J].Phys.Rev.E,1996,54:4256.
[4] Cao H,Zhao Y G,Ho S T,et al.Random laser action in semiconductor powder[J].Phys.Rev.Lett.,1999,82(11):2278-2282.
[5] Cao H,et al.Ultraviolet lasing in resonators formed by scattering in semiconductor polycrystalline films[J].Appl.Phys.Lett.,1998,73:3656-3658.
[6] Strangi G,Ferjani S,Barna V,et al.Random lasing and weak localization of light in dye-doped nomadic liquid crystals[J].Opt.Expr.,2006,14(17):7737-7744.
[7] Anderson P W.Absence of diffusion in certain random lattices[J].Phys.Rev.,1958,109:1492-1505.
[8] Cao H.Lasing in random media[J].Waves Random Media,2003,13:R1-R39.
[9] Fu Fangzheng,Li Ming.Calculating the threshold of random laser by using Monte Carlo method[J].Acta Physica Sinica(物理学报),2009,58(9):6258-6263(in Chinese).
[10] Fu Fangzheng,Li Ming.Spatial distribution of output laser in random laser[J].Chinese Journal of Quantum Electronics(量子电子学报),2009,26(5):543-547(in Chinese).
[11] Niginov M A,Bahoura M,Noginova N E,et al.Stimulated emission in scattering and composite dielectric media(random lasers):effect of particle size[C].SPIE,2003,5218:124-129.
[12] Wolf P E,Maret G.Weak localization and coherent backscattering of photons in disordered media[H].Phys.Rev.Lett.,1985,55:2696-2699.
[13] van der Mark M B,Lagendijk A,et al.Light scattering in strongly scattering and weak localization[J].Phys.Rev.B,1988,37:3575-3592.
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