Finite element analysis of the zero-crossing temperature of a long Fabry–Perot cavity

被引:0
|
作者
Junjuan Shang
Junya Ma
Xianwei Zhu
Hongfang Song
Peilin Zhou
Jiandong Hu
Zhihua Yuan
Huinan Huang
Mengjiao Zhang
机构
[1] Henan Agricultural University,College of mechanical and Electrical Engineering
[2] Henan International Joint Laboratory of Laser Technology in Agriculture Sciences,Zhengzhou Key Laboratory of Agricultural Equipment Intelligent Design and Green Manufacturing, College of Mechanical and Electrical Engineering
[3] Henan Agricultural University,Zhengzhou Key Laboratory of Agricultural Biomimetic Materials and Low Carbon Technology, College of Mechanical and Electrical Engineering
[4] Henan Agricultural University,Zhengzhou Key Laboratory of Agricultural Equipment Intelligent Design and Green Manufacturing, College of Mechanical and Electrical Engineering
[5] Henan Agricultural University,undefined
[6] School of Science,undefined
[7] Huzhou University,undefined
[8] College of Science,undefined
[9] Henan Agricultural University,undefined
来源
Indian Journal of Physics | 2023年 / 97卷
关键词
Fabry–Perot; Zero-crossing temperature; Finite element analysis;
D O I
暂无
中图分类号
学科分类号
摘要
An ultra-stable Fabry–Perot (F–P) cavity is designed, whose spacer is made of an ultra-low-expansion (ULE) glass and mirrors made of fused silicon (FS). The spacer aperture is composed of three holes, among which a long and small hole is in the middle, and a short and large hole is on each side. The fused silicon (FS) mirrors are placed in the large holes of the spacer aperture, and the FS rings are mounted on the end face of the spacer. FS mirrors, aperture and FS rings are coaxial. The thermal noise limit of the cavity is 9.1×10-17\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$9.1\times 10^{-17}$$\end{document}. By finite element analysis, the specific FS rings are choose to successfully tune the zero-crossing temperature from −10 to 27 K, which enables the cavity zero-crossing temperature easily be tuned above room temperature. In the meantime, this design makes the machining error has little effect on the zero-crossing temperature of the cavity, and it is convenient to manufacture a long F–P cavity.
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页码:2523 / 2529
页数:6
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