张振国, 李英一, 鞠有伦, 吕志伟. 双楔镜腔长微调节结构研究[J]. 红外与激光工程, 2023, 52(8): 20230422. DOI: 10.3788/IRLA20230422
引用本文: 张振国, 李英一, 鞠有伦, 吕志伟. 双楔镜腔长微调节结构研究[J]. 红外与激光工程, 2023, 52(8): 20230422. DOI: 10.3788/IRLA20230422
Zhang Zhenguo, Li Yingyi, Ju Youlun, Lv Zhiwei. Study on cavity length adjustment configuration of double optical wedge[J]. Infrared and Laser Engineering, 2023, 52(8): 20230422. DOI: 10.3788/IRLA20230422
Citation: Zhang Zhenguo, Li Yingyi, Ju Youlun, Lv Zhiwei. Study on cavity length adjustment configuration of double optical wedge[J]. Infrared and Laser Engineering, 2023, 52(8): 20230422. DOI: 10.3788/IRLA20230422

双楔镜腔长微调节结构研究

Study on cavity length adjustment configuration of double optical wedge

  • 摘要: 腔长微调节结构在光学谐振器里有重要应用。一种由双楔镜组成的腔长微调节结构被提出,该结构可实现不依赖于腔镜的腔长调节。双楔镜结构由斜面平行对立放置的两个直角楔镜构成,通过在垂直方向上驱动楔镜移动实现双楔镜内部光程改变,进而改变所处谐振腔内光路的光程。双楔镜结构对光程改变量的理论计算公式被建立,根据公式,光程改变量与楔镜楔角大小成正相关关系,与楔镜折射率成正相关关系,与楔镜振幅成线性关系。楔镜的楔角和折射率共同决定双楔镜结构的光程调节效率。经理论设计,楔角29°、折射率1.81的YAG双楔镜结构具有较高的调节效率和较小的光损耗,调节系数为0.53。实验上,以双角锥环形腔为基础,实现了双楔镜结构对腔长的调节,验证确定了双楔镜结构对腔长调节的可行性和有效性。讨论分析了双楔镜结构的变形结构:直角面对立双楔镜结构、基于正楔镜的双楔镜结构、多级双楔镜结构的光程调节性能。对比了双楔镜结构和其变形结构在光程调节效率、光损耗、光路调节难易程度的性能,确定了各种双楔镜结构在实际应用中的优缺点,为双楔镜结构的设计和选择提供了参考依据。

     

    Abstract:
      Objective   The cavity length adjustment configuration has important applications in optical resonators. A cavity length adjustment configuration of double optical wedge (DOW) is proposed, which can adjust the cavity length independently of the cavity mirror. DOW configuration is composed of two right-angle wedges with beveled planes placed in parallel opposites. The optical path inside DOW is changed by driving the wedges to move in the vertical direction, and then the optical path in the resonator is changed. The theoretical formula for calculating the change of optical path of DOW configuration is established. According to the formula, the change of optical path is positively correlated with the wedge angle, the refractive index of wedge and the wedge displacement in the vertical direction. The wedge angle and refractive index determine the optical path adjustment efficiency of DOW configuration. According to the theoretical design, the YAG DOW configuration with wedge angle of 29° and refractive index of 1.81 has higher adjustment efficiency and less optical loss, and the adjustment coefficient is 0.53. In the experiment, the double corner cube retroreflector (DCCR) ring cavity is used to verify the cavity length adjustment, and the feasibility and effectiveness of DOW configuration to adjust the cavity length are verified. The deformable structure of DOW configuration is discussed and analyzed. The optical path adjustment properties of DOW configuration with beveled planes placed in parallel opposites, regular optical wedges and cascaded DOW configuration are discussed. The performances of DOW configuration and its deformed configuration in optical path adjustment efficiency, optical loss and the complexity of the optical path construction are compared, and the advantages of these DOW configurations in practical application are determined, which provides a reference for the design and selection of DOW configuration.
      Methods  In theory, by geometric calculation, the calculation formula of the optical path adjustment of the DOW configuration is derived, and the results are shown in Eq.(3). According to Eq.(3), there are three factors affecting the adjustment ΔL, namely wedge angle α, wedge refractive index n, and wedge displacement Δh1h2 in the vertical direction. The larger the wedge angle value of α is, the higher the adjustment efficiency is, and the data results are shown (Fig.4); The greater the refractive index n is, the higher the adjustment efficiency is, and the data results are shown (Fig.5). The larger the displacement Δh1h2 is, the higher the adjustment efficiency is. According to these factors, a DOW configuration with wedge angle α = 29° and material YAG is designed, and its adjustment coefficient is 0.53.
      Results and Discussions   The adjustment effect of DOW configuration to the cavity length is verified experimentally by using the DCCR ring cavity. The reflector of DCCR ring cavity is corner cube retroreflector, which can not be drived by PZT directly, thus the cavity length adjustment of DCCR ring cavity can be realized with DOW configuration. The experimental setup is shown (Fig.10). DOW configuration is inserted into the DCCR ring cavity, and 1.6 μm laser is injected into the cavity. When DOW configuration is operating, 1.6 μm laser will form a resonance signal and output from M3, through which the cavity length adjustment value ΔL caused by DOW configuration can be determined. The experimental results are shown (Fig.11). The appearance of resonance signal proves that the cavity length changes, and the change value ΔL is consistent with the theoretical expectation. The above experimental results prove that DOW configuration is effective in adjusting the cavity length.
      Conclusions  In this paper, a DOW configuration is proposed, which can be used in the special scenario where the cavity length cannot be adjusted by driving the cavity mirrors. The formula for calculating the adjustment value and adjustment coefficient of DOW configuration is given theoretically. The influence of wedge angle and refractive index on the adjustment efficiency is analyzed. DOW configuration with wedge angle of 29° and matrix of YAG is designed. DOW configuration has a large adjustment efficiency (adjustment coefficient is 0.53) and a small light loss, and is the better choice in various DOW configurations. The cavity length adjustment of the length of DOW configuration is realized experimentally in a double-corner cone ring cavity, which verifies the feasibility and effectiveness of the DOW configuration. Finally, different deformation structures of DOW configurations are given, and the property parameters of each deformation structure are compared. Compared with the traditional cavity length adjustment configuration, cavity length adjustment configurations of DOW has low adjustment efficiency and certain insertion loss, but it provides an adjustment mode independent of the cavity mirror, and provides a new choice for the cavity length adjustment in special application scenarios.

     

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