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考虑晶体应力情况下的单块非平面环形腔分析 被引量:2

Analysis of Monolithic Nonplanar Ring Oscillators by Considering the Stress-Induced Birefringence
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摘要 简要分析了单块非平面环形腔单频激光器的基本原理 ,并采用琼斯矩阵计算了单块单向行波非平面环形腔内的本征偏振态。深入分析了磁场强度、输出面偏振反射系数、入射角、非平面角及腔内其它参量对各本征偏振态的损耗及两本征偏振态间损耗差的影响 ,并且指出如何选择各参量以降低本征偏振态的损耗且增大两本征偏振态间的损耗差。最后还通过计算晶体应力在两个本征偏振态方向引起的相位差 ,讨论了应力作用方向以及应力双折射系数对腔内本征偏振态的损耗和两本征偏振态间损耗差的影响。 The principle of monolithic nonplanar ring single-frequency laser was introduced, and eigenpolarization states of monolithic unidirectional traveling wave nonplanar ring oscillator (NPRO) were calculated by Jones matrix. The influences of magnetic field strength, reflection coefficients of the output coupler, incident angle, nonplanar angle and other parameters inside cavity on the loss and loss difference of eigenpolarizations were analyzed. How to choose the parameters of cavity to decrease the loss of eigenpolarization states and increase the loss difference between two eigenpolarization states was pointed out. The influences of the stress direction and the stress-induced birefringence coefficient on the loss and loss difference of the eigenpolarization states in the cavity were discussed by calculating the phase difference between two eigenpolarization states induced by stress birefringence.
出处 《光学学报》 EI CAS CSCD 北大核心 2004年第2期279-283,共5页 Acta Optica Sinica
基金 国家"十五"预研项目资助课题
关键词 单频激光器 非平面环形腔 本征值 应力双折射 损耗差 琼斯矩阵 磁场强度 偏振反射系数 laser techniques single-frequency laser nonplanar ring oscillators eigenvalue stress-induced birefringence loss difference
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  • 1赵达尊,波动光学,1988年

共引文献9

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  • 1王欣,杨苏辉,孙文峰,赵长明.激光二极管抽运单块高斜度效率环形腔单频固体激光器[J].中国激光,2005,32(2):149-152. 被引量:21
  • 2郑耀辉,卢华东,李凤琴,张宽收,彭堃墀.全固态高输出功率单频Nd:YVO_4/KTP激光器[J].中国激光,2007,34(6):739-742. 被引量:16
  • 3J. J. Zayhowski. Single frequency microchip Nd lasers[J]. Opt. Lett., 1989, 14: 24-26.
  • 4J. J. Zayhowski. Frequency-modulated Nd: YAG microchip lasers[J]. Opt. Lett., 1989, 14:618-620.
  • 5R. Knappe G. Bitz, K. J. Boller et al.. Compact singlefrequency diode pumped Cr : LiSAF lasers [J]. Opt. Commun, 1997, 143:42-46.
  • 6V. Evtuhov, A. E. Siegman. A "twisted-mode" technique for obtaining axially uniform energy density in a laser[J]. Appl. Opt. , 1965, 4(1): 142-143.
  • 7K. Nakagewa, Y. Shimizu, M. Ohtsu. High power diode-laser pumped twisted mode Nd : YAG laser[J]. IEEE Pohton. Technol. Lett., 1994, 6(4): 499-501.
  • 8T. J. Kane, R. L. Byer. Monolithic, unidirectional single-mode Nd:YAGringlaser[J]. Opt. Lett., 1985, 10(2): 65-67.
  • 9I. Freitag, A. Tiinnermann, H. Welling. Power scaling of diode-pumped monolithic Nd: YAG lasers to output powers of severalwatts[J]. Opt. Commun. , 1995, 115:511-515.
  • 10I. S. Kubo, T. J. Kane. Diode-pumped lasers at five eye-safe wavelengths [ J ]. IEEE J. Quantum Electron. , 1992, 28:1033-1040.

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