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基于介质-h-BN-介质结构的中红外波段声子极化激元波的滤波特性

Filtering Characteristics of Phonon Polaritons Waves Based on Dielectric-h-BN-Dielectric Structure in Mid-Infrared Band.

作者信息

Cai Ming, Wang Shulong, Liu Zhihong, Wang Yindi, Han Tao, Liu Hongxia

机构信息

Key Laboratory for Wide Band Gap Semiconductor Materials and Devices of Education, School of Microelectronics, Xidian University, Xi'an 710071, China.

出版信息

Nanomaterials (Basel). 2020 May 1;10(5):878. doi: 10.3390/nano10050878.

DOI:10.3390/nano10050878
PMID:32370104
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC7279279/
Abstract

Hyperbolic materials can be used to excite hyperbolic phonon polaritons in specific frequency bands, which causes abrupt interfaces with fluctuations of permittivity and different transmission characteristics at different incident wavelengths. Using the quasi-static approximation, the filtering characteristics of hexagonal Boron nitride (h-BN) and the transmission characteristics of phonon polaritons waves on a dielectric-h-BN-dielectric structure were studied in the paper. The results show that a smaller relative permittivity of the materials above and below h-BN and a thicker h-BN (ε = 1 (air), ε = 3.9 (SiO), d = 100 nm) will lead to better filtering characteristics for different wavenumbers' incident waves (propagation length from 0.0028 μm to 1.9756 μm). Simulation results in COMSOL validated the previous theoretical calculations. Moreover, the transmissivity and 3dB bandwidth of the type-II band were calculated with different structure widths. The maximum transmissivity of ~99% appears at a width of 100 nm, and the minimum 3dB bandwidth reaches 86.35 cm at a structure width of 1300 nm. When the structure width meets or exceeds 1700 nm, the 3dB bandwidth is equal to 0, and its structure length is the limit for the filter application. These characteristics reveal the excellent filtering characteristics of the dielectric-h-BN-dielectric structure, and reveal the great potential of using the dielectric-h-BN-dielectric structure to design optical filter devices with excellent performance in mid-infrared bands.

摘要

双曲线材料可用于在特定频段激发双曲线声子极化激元,这会导致出现介电常数波动的突变界面以及在不同入射波长下具有不同的传输特性。本文利用准静态近似研究了六方氮化硼(h-BN)的滤波特性以及声子极化激元波在介质-h-BN-介质结构上的传输特性。结果表明,h-BN上下材料的相对介电常数较小且h-BN较厚(ε = 1(空气),ε = 3.9(SiO),d = 100 nm)会导致对不同波数的入射波(传播长度从0.0028μm到1.9756μm)具有更好的滤波特性。COMSOL中的模拟结果验证了先前的理论计算。此外,还计算了不同结构宽度下II型波段的透射率和3dB带宽。在宽度为100 nm时出现约99%的最大透射率,在结构宽度为1300 nm时最小3dB带宽达到86.35 cm。当结构宽度达到或超过1700 nm时,3dB带宽等于0,其结构长度是滤波器应用的极限。这些特性揭示了介质-h-BN-介质结构优异的滤波特性,并揭示了利用介质-h-BN-介质结构设计在中红外波段具有优异性能的光学滤波器件的巨大潜力。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/689e/7279279/7902a48ed551/nanomaterials-10-00878-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/689e/7279279/6d2d25f75e8e/nanomaterials-10-00878-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/689e/7279279/2022d5428b69/nanomaterials-10-00878-g002.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/689e/7279279/3498299a31b3/nanomaterials-10-00878-g004.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/689e/7279279/a80fd26e878f/nanomaterials-10-00878-g008a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/689e/7279279/7902a48ed551/nanomaterials-10-00878-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/689e/7279279/6d2d25f75e8e/nanomaterials-10-00878-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/689e/7279279/2022d5428b69/nanomaterials-10-00878-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/689e/7279279/6f50878c56a7/nanomaterials-10-00878-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/689e/7279279/3498299a31b3/nanomaterials-10-00878-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/689e/7279279/df92426b57fd/nanomaterials-10-00878-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/689e/7279279/dbca3df096b9/nanomaterials-10-00878-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/689e/7279279/05c1ef119cc7/nanomaterials-10-00878-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/689e/7279279/a80fd26e878f/nanomaterials-10-00878-g008a.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/689e/7279279/7902a48ed551/nanomaterials-10-00878-g009.jpg

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