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MgO∶LiNbO_3晶体中超短中红外非共线相位匹配光参量放大过程角度的优化选择
引用本文:邓颖,朱启华,曾小明,张颖,王凤蕊,谢旭东,王逍,黄征,郭仪,孙立.MgO∶LiNbO_3晶体中超短中红外非共线相位匹配光参量放大过程角度的优化选择[J].中国激光,2007,34(7):915-919.
作者姓名:邓颖  朱启华  曾小明  张颖  王凤蕊  谢旭东  王逍  黄征  郭仪  孙立
作者单位:中国工程物理研究院激光聚变中心,中国工程物理研究院激光聚变中心,中国工程物理研究院激光聚变中心,中国工程物理研究院激光聚变中心,中国工程物理研究院激光聚变中心,中国工程物理研究院激光聚变中心,中国工程物理研究院激光聚变中心,中国工程物理研究院激光聚变中心,中国工程物理研究院激光聚变中心,中国工程物理研究院激光聚变中心 四川绵阳621900,四川绵阳621900,四川绵阳621900,四川绵阳621900,清华大学工程物理系,北京100084,四川绵阳621900,四川绵阳621900,四川绵阳621900,四川绵阳621900,四川绵阳621900,四川绵阳621900
摘    要:计算了MgO∶LiNbO3中超短中红外光参量放大(OPA)过程中晶体的相位匹配角与非共线角的优化选择。结果表明,对于800nm波长的抽运光,信号光波长为1053nm时,非共线角α优化在1.74°~2°之间;当信号光波长在1046~1067nm内变化时,α在1.05°~2.18°之间,并且当信号光波长为1057nm,α=1.76°时,可实现三波间群速度的完全匹配。同时还得到了抽运光中心波长在780~810nm之间变化时,实现完全群速度匹配时的注入信号光波长与对应的中红外光以及相应的非共线角与相位匹配角。

关 键 词:非线性光学  超短中红外激光  群速度匹配  非共线相位匹配光参量放大  MgO∶LiNbO晶体
收稿时间:2006/11/21

Angle Optimization for Ultra-Short Mid-Infrared Non-Collinear Phase Matching Optical Parametric Amplification in MgO∶LiNbO3Crystal
DENG Ying,ZHU Qi-hua,ZENG Xiao-ming,ZHANG Ying,WANG Feng-rui,XIE Xu-dong,WANG Xiao,HUANG Zheng,GUO Yi,SUN LiResearch Center of Laser Fusion,China Academy of Engineering Physics,Mianyang,Sichuan ,China.Angle Optimization for Ultra-Short Mid-Infrared Non-Collinear Phase Matching Optical Parametric Amplification in MgO∶LiNbO3Crystal[J].Chinese Journal of Lasers,2007,34(7):915-919.
Authors:DENG Ying  ZHU Qi-hua  ZENG Xiao-ming  ZHANG Ying    WANG Feng-rui  XIE Xu-dong  WANG Xiao  HUANG Zheng  GUO Yi  SUN LiResearch Center of Laser Fusion  China Academy of Engineering Physics  Mianyang  Sichuan  China
Affiliation:DENG Ying1,ZHU Qi-hua1,ZENG Xiao-ming1,ZHANG Ying1,2,WANG Feng-rui1,XIE Xu-dong1,WANG Xiao1,HUANG Zheng1,GUO Yi1,SUN Li11Research Center of Laser Fusion,China Academy of Engineering Physics,Mianyang,Sichuan 621900,China2Department of Engineering Physics,Tsinghua University,Beijing 100084,China
Abstract:The phase matching angle and the non-collinear angle for ultrashort and mid-infrared optical parametric amplification (OPA) in MgO∶LiNbO3 are calculated. With pump light wavelength fixed at 800 nm, the non-collinear angle should be optimized between 1.74° and 2° when the seeded signal wavelength is 1053 nm, and the non -collinear angle should be optimized between 1.05° and 2.18° when the seed signal wavelength changes between 1046 and 1067 nm. Especially, when the seeded signal wavelength is 1057 nm and the non-collinear angle is 1.76°, the group velocities mismatching can be almost completely compensated with the pump light wavelength fixed at 800 nm. The series of signal light wavelength, mid-infrared light phase matching angle and non-collinear angle are also achieved when the group velocities are almost completely compensated with the pump light changing between 780 and 810 nm.
Keywords:nonlinear optics  ultra-short mid-infrared laser  group velocity matching  non-collinear phase matching optical parametric amplification  MgO∶LiNbO3 crystal
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