Calculation of optimum parameters in single frequency LDP intracavity frequency doubled Nd:YAG laser

J. Yao, J.B. Yang, W.D. Sheng, Y. Zheng
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Abstract

The experiment setup of the laser is shown in Fig. 1. The bireffequent effect of KTP crystal, together with the Brewster-plate(B-plate) function in the cavity as a loss modulator. Define δ-phase delay angle, γ-angle between the polarization orientation of the slow ray in KTP crystal and the P-plane polarization direction of the B-plate. P-polarization is the polarization direction along which the loss that a light wave passes through the B-plate is zero. Previous calculation results from many other literatures show that the optimum value of γ is 45°, with the mode selecting ability of the crystal reaching the peak value.
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激光器的实验装置如图1所示。利用KTP晶体的双频效应,结合腔内的布鲁斯特板(b板)功能作为损耗调制器。定义了KTP晶体中慢射线的偏振方向与b板的p面偏振方向之间的δ相位延迟角、γ相位延迟角。p偏振是光波穿过b片时损耗为零的偏振方向。先前许多文献的计算结果表明,γ的最佳值为45°,晶体的模式选择能力达到峰值。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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