高透光率感性网栅膜的电磁屏蔽

刘小涵; 赵晶丽; 冯晓国; 申振峰; 高劲松; 张红胜

doi:10.3788/OPE.20122001.0080

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高透光率感性网栅膜的电磁屏蔽

现代应用光学 | 更新时间：2020-08-12

- 高透光率感性网栅膜的电磁屏蔽
- Electromagnetic shielding of highly transparent inductive mesh
- 光学精密工程 2012年20卷第1期页码：80-87
- 作者机构：
  
  1. 中国科学院长春光学精密机械与物理研究所中国科学院光学系统先进制造技术重点实验室,吉林长春,130033
  2. 中国科学院研究生院北京,100039
- 作者简介：
- 基金信息：
  
  国防科技预研基金资助项目(No.10.4.2.ZK1001)()
- DOI：10.3788/OPE.20122001.0080
  中图分类号： TN972;O484.4+3
- 收稿日期：2011-11-08，
  
  修回日期：2011-12-15，
  
  网络出版日期：2012-01-25，
  
  纸质出版日期：2012-01-25
- 稿件说明：
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刘小涵, 赵晶丽, 冯晓国, 申振峰, 高劲松, 张红胜. 高透光率感性网栅膜的电磁屏蔽[J]. 光学精密工程, 2012,20(1): 80-87

LIU Xiao-han, ZHAO Jing-li, FENG Xiao-guo, SHEN Zhen-feng, GAO Jin-song, ZHANG Hong-sheng. Electromagnetic shielding of highly transparent inductive mesh[J]. Editorial Office of Optics and Precision Engineering, 2012,20(1): 80-87
刘小涵, 赵晶丽, 冯晓国, 申振峰, 高劲松, 张红胜. 高透光率感性网栅膜的电磁屏蔽[J]. 光学精密工程, 2012,20(1): 80-87 DOI： 10.3788/OPE.20122001.0080.

LIU Xiao-han, ZHAO Jing-li, FENG Xiao-guo, SHEN Zhen-feng, GAO Jin-song, ZHANG Hong-sheng. Electromagnetic shielding of highly transparent inductive mesh[J]. Editorial Office of Optics and Precision Engineering, 2012,20(1): 80-87 DOI： 10.3788/OPE.20122001.0080.

摘要

在确保制作感性网栅膜后光学窗红外透射率下降小于5%的前提下

研究了影响感性网栅膜电磁屏蔽特性的主要因素。归纳了感性网栅膜红外透射率公式

运用含阻抗边界条件的谱域Galerkin法推导了周期结构金属网栅的电磁场积分方程

用周期矩量法计算出网栅的反射系数及透射系数

进而求出其电磁屏蔽效能;计算并分析了采用不同线宽、周期、衬底材料、衬底厚度时透明导电光窗(金属网栅膜)的电磁屏蔽效能。最后

采用激光直写、真空镀膜等工艺在ZnS基底上制作了周期为360 m360 m、线宽为12 m

方块电阻分别为13 、25 的样片

采用自由空间法测试了2~18 GHz频段的电磁屏蔽效能。测试与分析结果表明:当感性网栅膜在8~10 m波段引起的平均透射率下降小于2%的情况下

电磁屏蔽效能平均达到了20 dB以上。结果显示网栅的光电特性是矛盾的

线宽与周期越小电磁屏蔽效果越好

同时应尽量降低网栅的表面电阻。

Abstract

This paper studies the influencing factors on the electromagnetic shielding of an inductive metallic mesh when the infrared transmission reduction of optical window caused by the mesh is less than 5%. The infrared transmission formulas of the inductive mesh are summarized

then

the electromagnetic field integral equation for the periodic structure of metallic mesh is built based on Galerkin's method in the spectral domain. The transmission and reflection coefficients are derived by the Moment of Method(MOM). After that

the electromagnetic shield effectiveness of the mesh is calculated and the effects of different line widths

periods

substrate materials

substrate thicknesses on the electromagnetic shielding of the transparent conductive optical window (with metallic mesh) are calculated and analyzed. Finally

metallic mesh samples with a line width of 12 m

a period of 360 m360 m and the surface resistance of 13

25 are fabricated on a ZnS substrate by the laser direct writing figure

vacuum coating

et al

.. The electromagnetic shield effectiveness from 2 GHz to 18 GHz is tested by a free space method. Results indicate that the average electromagnetic shield effectiveness is more than 20 dB when the infrared transmission reduction caused by the metallic mesh is less than 2% in 8-10 m. Experiments indicate that the optical and electrical performance of metallic mesh film is inconsistent .The main solution method is to select a thinner line width and smaller period and to reduce the surface resistance value of the mesh as low as possible at the same time.

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Keywords

references

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