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本文采用非同时读出条件下两波耦合实验装置,以532 nm的单频固体激光器为光源,在不同写入光夹角θ、抽运光的偏振方向与e偏振光的方向呈10°、信号光为e偏振光及不同信号光与抽运光光强比条件下,通过改变写入光在Ce: KNSBN晶体内的不同位置研究其对两波耦合有效增益的影响.研究结果表明,在相同角度下写入光强比为1: 10,写入光在晶体内位置d=0.1 cm时最佳,有效增益达到最大.在最佳写入光位置,写入光强比为1: 10时,在写入光夹角为24°时两波耦合有效增益为最大.并对实验结果进行了理论拟合与分析.

参考文献

[1] He Q B;Yeh P .Fanning Noise Reduction in Photorefractive Amplifiers Using Incoherent Erasures[J].Applied Optics,1994,33(02):283-287.
[2] Liang B L;Wang Z Q;Cartwright C M et al.Enhancement of Two-wave Coupling in Ce:KNSBN Crystal with Optimum Palrizations of Writing Beams[J].Applied Optics,2001,40(20):3359-3362.
[3] Arizmendi L;Lopez-Barbera JF;Carrascosa M .Twelve-fold increase of diffraction efficiency of thermally fixed holograms in Bi12SiO20[J].Journal of Applied Physics,2005(7):3505-1-3505-4-0.
[4] Hu Juguang;Mu Xiaodong;Chen Huanchu;Shao Zongshu;Xu Xinguang .Temperature dependence of photorefractive properties of a Cu-doped barium strontium potassium sodium niobate crystal[J].Optics Communications: A Journal Devoted to the Rapid Publication of Short Contributions in the Field of Optics and Interaction of Light with Matter,1999(4):219-222.
[5] Wang HY.;Lin JL.;Huang SH.;Yu JQ.;Chen HC.;Jiang QZ.;Tian MZ. .STUDY OF TWO-WAVE COUPLING IN CU, KNSBN USING RED LIGHT[J].Optics Communications: A Journal Devoted to the Rapid Publication of Short Contributions in the Field of Optics and Interaction of Light with Matter,1995(5/6):563-567.
[6] 朱瑞德;王韧;谭健华 等.掺杂的钾钠铌酸锶钡晶体的二波耦合增益系数的研究[J].物理学报,1992,41(09):1440-1447.
[7] 李盼来,郭庆林,邓泽超,王志军,张金平,梁宝来.Ce:KNSBN晶体中调制光耦合研究[J].人工晶体学报,2008(01):65-69.
[8] 赵建林,李振伟,杨德兴,马仰华,杨东升.外电场对SBN:Cr晶体二波耦合特性的影响及应用[J].物理学报,2004(11):3756-3760.
[9] 郭庆林,李彦,张云英,赵云,李盼来,哈艳.抽运光偏振态对晶体两波耦合增益的影响[J].人工晶体学报,2009(03):648-651,661.
[10] 刘思敏;郭儒;凌振芳.光折变非线性光学[M].北京:中国标准出版社,2004:48-51.
[11] Zhang G Y;Li Q X;Ho P P et al.Dependence of Soecklon Size on the Laser Beam via Photo-induced Light Scattering in LiNbO3:Fe[J].Applied Optics,1986,25(17):2955-2959.
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