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定向棱镜激光腔模式模拟研究
引用本文:石岩,金挺,李松,周辉,翁兴涛.定向棱镜激光腔模式模拟研究[J].红外与激光工程,2005,34(5):521-525,539.
作者姓名:石岩  金挺  李松  周辉  翁兴涛
作者单位:武汉大学,电子信息学院,湖北,武汉,430079;浙江省质量技术监督检测研究院,浙江,杭州,310013
摘    要:为了探究定向棱镜谐振腔激光模式分布情况,通过连续利用反射系统的光线矢量的反射定律,推导出具有二面角误差的角锥棱镜相位模型,首次创新性地建立了定向棱镜腔的光场数学模型,并运用FOX-LI的理论。研制了一套求解各种腔形的稳态模的场分布软件。用这套软件模拟出了定向棱镜谐振腔自再现模的分布。同时,针对免调试固体激光器(定向棱镜腔)进行实验,将模拟所得结果与实际激光器的输出近场、远场光斑,以及与光束质量分析仪检测分析结果进行了对比,取得了较好的效果。

关 键 词:激光模式  角锥棱镜  数值计算  角度误差  面形误差
文章编号:1007-2276(2005)05-0521-05
收稿时间:2004-11-10
修稿时间:2004-11-102005-01-09

Models simulation of oriented prism laser resonator
SHI Yan,JIN Ting,LI Song,ZHOU Hui,WENG Xing-tao.Models simulation of oriented prism laser resonator[J].Infrared and Laser Engineering,2005,34(5):521-525,539.
Authors:SHI Yan  JIN Ting  LI Song  ZHOU Hui  WENG Xing-tao
Affiliation:1.School of Electronics Information,Wuhan University,Wuhan 430079, China; 2.Zhejiang Measurement and Test Institute for Quality and Technique Supervision,Hangzhou 310013 ,China
Abstract:In order to develop a field distribution program that resolves the model of stable resonator any cavity,the phase model of the cube comer prism is established using continuously the law of reflection of ray vector. A mathematical model of the oriented prism laser field distribution is developed at first. A field distribution program that resolves the model of stable resonator in any cavity is developed. And the modes of stable resonator consisting of directional prism are investigated with FOX-LI iterative method. The amplitude and phase distributions of the output mirror are presented.In the experiment,the avoidance adjust solid state laser is used. Both the experimental results about the output near-field speckle of laser, far-field speckle of laser and the result from the laser beam quality analyzer are compared with 3-D numerical simulation.The simulation results are in agreement with experimental results.A good effect is obtained in practical application.
Keywords:Laser mode  Cube-comer prism  Numerical computation  Dihedral angle offset  Flatness error
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