Y型腔正交偏振氦氖激光器及其基本特征

肖光宗; 龙兴武; 张斌

doi:10.3788/OPE.20111911.2558

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Y型腔正交偏振氦氖激光器及其基本特征

现代应用光学 | 更新时间：2020-08-12

- Y型腔正交偏振氦氖激光器及其基本特征
- Orthogonal polarized He-Ne laser with Y-shaped cavity and its characteristics
- 光学精密工程 2011年19卷第11期页码：2558-2564
- 作者机构：
  
  国防科学技术大学光电科学与工程学院光电工程系,湖南长沙,410073
- 作者简介：
- 基金信息：
  
  国防科技大学优秀研究生创新基金资助项目(No.B090703)()
- DOI：10.3788/OPE.20111911.2558
  中图分类号： TN248.2
- 收稿日期：2011-03-17，
  
  修回日期：2011-04-15，
  
  网络出版日期：2011-11-25，
  
  纸质出版日期：2011-11-25
- 稿件说明：
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肖光宗, 龙兴武, 张斌. Y型腔正交偏振氦氖激光器及其基本特征[J]. 光学精密工程, 2011,19(11): 2558-2564

XIAO Guang-zong, LONG Xing-wu, ZHANG Bin. Orthogonal polarized He-Ne laser with Y-shaped cavity and its characteristics[J]. Editorial Office of Optics and Precision Engineering, 2011,19(11): 2558-2564
肖光宗, 龙兴武, 张斌. Y型腔正交偏振氦氖激光器及其基本特征[J]. 光学精密工程, 2011,19(11): 2558-2564 DOI： 10.3788/OPE.20111911.2558.

XIAO Guang-zong, LONG Xing-wu, ZHANG Bin. Orthogonal polarized He-Ne laser with Y-shaped cavity and its characteristics[J]. Editorial Office of Optics and Precision Engineering, 2011,19(11): 2558-2564 DOI： 10.3788/OPE.20111911.2558.

摘要

研制了基于Y型腔结构的正交偏振氦氖激光器

介绍了该激光器的基本结构和基本原理。实验研究了该激光器的输出光模式、输出光功率、输出光频差调谐特性和频差闭锁特性。通过改变共用段反射镜上压电陶瓷的电压

观察了激光器闭锁状态时两偏振光光强随着总腔长调谐变化的规律

并分析了闭锁状态下不同偏振态纵模之间的相互作用机理。与以往产生双频激光的方案进行对比

分析了Y型腔正交偏振氦氖激光器的特点

给出了其在频差稳定性方面的优势和制约因素。实验结果表明

利用Y型腔结构可以实现氦氖激光器的频率分裂

激光器最大输出功率约为235.2 W;通过调节共用段反射镜上压电陶瓷的电压可以线性调节激光器的输出频差;实验中激光器的频差为22~1 018 MHz

闭锁阈值频差约为22 MHz。

Abstract

Based on the Y-shaped cavity frequency splitting method

an orthogonal polarized He-Ne laser was designed and implemented. The structure and basic principle of the laser were introduced in detail

and the transverse and longitudinal models

output powers

the ellipticity of output light and frequency difference lock-in phenomenon and frequency difference tuning characteristics were experimentally investigated. By changing the voltage of piezoelectric transducer applied to the common cavity mirror

the power tuning characteristics of S polarized and P polarized lights were observed and summarized. Furthermore

the interaction mechanism of S polarized and P polarized lights as above-mentioned was also analyzed. Compared with the traditional dual frequency lasers

the characters of the laser

as well as its merits and demerits on the frequency difference stability were presented. Experiments show that the maximum output power of the laser is about 235.2 W. By adjusting the voltage of the piezoelectric transducer in the P cavity

the frequency difference between the S polarized and P polarized lights is linearly varied from 22 MHz to 1 018 MHz and lock-in frequency difference of the laser is about 22 MHz.

关键词

Keywords

references

姜亚南. 环形激光陀螺[M]. 北京:清华大学出版社,1985 JIANG Y N. Ring Laser Gyro[M]. Beijing: Tsinghua University Press, 1985. (in Chinese)[2] Keijser R A J.Polarization properties of internal mirror He-Ne lasers in a strong transverse magnetic field[J].Optics Communications,1977,23(2):194-198.[3] 张书练. 正交偏振激光原理[M]. 北京:清华大学出版社,2005: 224-228. ZHANG SH L. The Theory of Orthogonal Polarized Laser[M]. Beijing: Tsinghua University Press, 2005: 224-228. (in Chinese)[4] YANG S, ZHANG S L. The frequency plit phenomenon in a He-Ne laser with rotation quartz crystal plate in its cavity[J]. Optics Communication,1988,68:55-57.[5] ZHANG S L, LU M, WU M X,et al.Laser frequency spilt by an electron-optical element in its cavity[J]. Optics Communication, 1993,96(4):245-248.[6] ZHANG S L, HE W K. Laser spilt by rotating an intracavity, tilt cut crystal quartz plate around its surface normal axis[J]. Optics Communications,1993,97(3):210-214.[7] ZHANG S L, WU M X, JIN G F. Birefringence tuning double frequency He-Ne laser[J]. Applied Optics, 1990,29:1265-1267.[8] JIN Y Y, Z ZHANG S L, LI Y, et al.. Zeeman birefringence dual frequency laser[J]. Chinese Physic Letters,2001,18(4):533-536.[9] ROPARS G, FLOCH A L. Polarization control mechanisms in vectorial bistable lasers for one-frequency systems[J]. Physical Review A, 1992,(1):623-640.[10] HOLZAPFEL W, NEUSCHAEFER-RUBE S, KOBUSCH M. High-resolution, very broadband force measurements by solid-state laser transducers[J].Measurement,2000,28:277-291.[11] 倪志波,宋连科,刘建苹等. 单轴晶体双折射率随温度变化的双光路测量[J]. 激光技术,2007,31(4):358-363. NI ZH B, SONG L K, LIU J P, et al.. Measurement of birefringence of a single axis crystal varying with tempreture based on double light paths[J].Laser Technology, 2007,31(4):358-363. (in Chinese)[12] 赵媛媛. LD泵浦内腔倍频双频固体激光技术的研究 . 西安:西安理工大学,2006:41-48. ZHAO Y Y. Study of LD-pumped Intracavity frequency-doubled dual-frequency solid-state Laser technique .Xian: Xian University of Technology,2006:41-48. (in Chinese)[13] 焦明星,刑俊红,刘芸等. 双腔大频差双频全固态激光器设计与实验研究[J]. 中国激光,2010,37(11):2784-2789 JIAO M X, XING J H, LIU Y, et al.. Design and experimental study of two-cavity dual-frequency all-solid state laser with large frequency difference[J].Chinese Journal of lasers, 2010,37(11):2784-2789.(in Chinese)[14] 龙兴武,肖光宗,张斌. 一种新型的高精度激光加速度计[J].光学学报, 2010,30(11):3227-3232. LONG X W, XIAO G Z, ZHANG B. A novel high-precision laser accelerometer[J].Acta Optica Sinica, 2010,30(11):3227-3232.(in Chinese)[15] 蓝信钜.激光技术[M]. 北京:科学出版社, 2009:214-215. LAN X J.Laser Technology [M]. Beijing:Science Press,2009:214-215. (in Chinese)[16] 周炳琨,高以智,陈调嵘等. 激光原理[M]. 北京:国防工业出版社,2002:24-64. ZHOU B K,GAO Y ZH,CHEN T R, et al.. Theory of Lasers[M].Beijing: National Defense Industry Press,2000:24-64. (in Chinese)[17] 吕可诚,巴恩旭,张春平. 内腔双纵模He-Ne激光器偏振方向的竞争效应[J]. 光学学报,1984,4(1):44-49. LU K CH, BA EN X, ZHANG CH P. Competition effect of polarization in two-mode internal mirror He-Ne lasers[J]. Acta Optica Sinica, 1984,4(1):44-49. (in Chinese)

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