Optical Characteristics of Metallic Photonic Crystals

ZHAO Ya-li; MA Fu-hua; JIA Kun; LI Xu-feng; WANG Quan; LEI Yi-san; ZHANG Jie

doi:10.3788/fgxb20194008.1001

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Optical Characteristics of Metallic Photonic Crystals

Synthesis and Properties of Materials | 更新时间：2020-08-12

- Optical Characteristics of Metallic Photonic Crystals
- Chinese Journal of Luminescence Vol. 40, Issue 8, Pages: 1001-1010(2019)
- 作者机构：
  
  1. 太原科技大学应用科学学院,山西太原,030024
  2. 晋中学院,山西太原,030619
  3. 电磁防护材料及技术山西省重点实验室,山西太原,030006
- 作者简介：
- 基金信息：
- DOI：10.3788/fgxb20194008.1001
  CLC： TQ156.2;TQ594;TQ171.7
- Received：18 December 2018，
  
  Revised：26 February 2019，
  
  Published Online：26 March 2019，
  
  Published：05 August 2019
- 稿件说明：
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赵亚丽, 马富花, 贾琨等. 金属光子晶体的可见光光谱特性[J]. 发光学报, 2019,40(8): 1001-1010

ZHAO Ya-li, MA Fu-hua, JIA Kun etc. Optical Characteristics of Metallic Photonic Crystals[J]. Chinese Journal of Luminescence, 2019,40(8): 1001-1010
赵亚丽, 马富花, 贾琨等. 金属光子晶体的可见光光谱特性[J]. 发光学报, 2019,40(8): 1001-1010 DOI： 10.3788/fgxb20194008.1001.

ZHAO Ya-li, MA Fu-hua, JIA Kun etc. Optical Characteristics of Metallic Photonic Crystals[J]. Chinese Journal of Luminescence, 2019,40(8): 1001-1010 DOI： 10.3788/fgxb20194008.1001.

摘要

设计了一种由金属Ag和ITO（In

:Sn锡掺氧化铟）薄膜呈周期排布的金属光子晶体（Metal photonic crystals，MPCs）。采用时域有限元差分法（Finite difference time domain，FDTD）计算仿真了周期和周期数对其可见光透光率和反射率的影响规律。研究表明，当金属Ag和ITO组分比一定时，随周期增加，可见光透光率曲线相应变宽，强度降低。当周期数大于4以后，可见光透光率曲线不再随周期数增加而相应变宽。随着入射角度的提高，可见光透光率曲线峰值发生蓝移，宽度相应变宽，强度相应降低。随着Ag膜层层数的增加，可见光透光率的共振峰（透射峰）相应增加。MPCs的可见光透光率峰值与反射率的峰谷具有较好的一一对应关系。

Abstract

Metal photonic crystals (MPCs) consisting of periodic Ag-ITO multilayers were demonstrated in the paper. The optical transmittance and reflectance of MPCs with different cycle size and number were simulated by finite difference time domain (FDTD) method. It is found that the optical transmittance of the MPCs broadens and the intensity accordingly decreases as the cycle size increasing. For one hand

As the numbers of cycle increasing

the numbers of transmitting resonant peaks correspondingly increase

and the bandwidth of transmittance obviously broadens until the number of cycle reaching to 4. For the other hand

the location of center wavelength evidently blue shifts as the incident angle increasing. At same time

the bandwith of transmittance broadens and the intensity of that distinctly decreases. Meanwhile

the numbers of transmittance peak obviously grow up as the layers of metal films increasing. It is also demonstrated that the location of transmittance peaks and reflectance valley is one to one relationship.

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references

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