Cargando…
Terahertz Broadband Polarization Conversion for Transmitted Waves Based on Graphene Plasmon Resonances
We applied the harmonic oscillator model combined with the transfer matrix method to study the polarization conversion for transmitted waves in metallic grating/plasmon-excitation layer/metallic grating structure in the terahertz (THz) region. By comparing the calculated spectra and the simulated (b...
Autores principales: | , , , , , , , , |
---|---|
Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2020
|
Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7823980/ https://www.ncbi.nlm.nih.gov/pubmed/33379402 http://dx.doi.org/10.3390/nano11010056 |
_version_ | 1783639965797711872 |
---|---|
author | Yu, Anqi Yu, Dahai Yang, Zhenyu Guo, Xuguang Ren, Yuxiang Zang, Xiaofei Balakin, Alexei V. Shkurinov, Alexander P. Zhu, YiMing |
author_facet | Yu, Anqi Yu, Dahai Yang, Zhenyu Guo, Xuguang Ren, Yuxiang Zang, Xiaofei Balakin, Alexei V. Shkurinov, Alexander P. Zhu, YiMing |
author_sort | Yu, Anqi |
collection | PubMed |
description | We applied the harmonic oscillator model combined with the transfer matrix method to study the polarization conversion for transmitted waves in metallic grating/plasmon-excitation layer/metallic grating structure in the terahertz (THz) region. By comparing the calculated spectra and the simulated (by the finite-difference-time-domain method) ones, we found that they correspond well with each other. Both methods show that the Drude background absorption and the excited plasmon resonances are responsible for polarization conversion. The transmission is close to 0 when the distance between the top/bottom metallic gratings and gated graphene is an integer multiple of half the wavelength of the incident wave (in the dielectrics), at which points the plasmon resonances are greatly suppressed by the destructive interference between the backward/forward electromagnetic waves and that reflected by the top/bottom metallic gratings. Away from these points, the transmission can be higher than 80%. The electron density and the excitation efficiency of the plasmon-excitation layer were found to be important for the bandwidth of the polarization conversion window, while the scattering rate was found to influence mainly the polarization conversion rate. Multi-broadband polarization conversion is realized by exciting plasmon modes between the 0 transmission points in the THz region. |
format | Online Article Text |
id | pubmed-7823980 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2020 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-78239802021-01-24 Terahertz Broadband Polarization Conversion for Transmitted Waves Based on Graphene Plasmon Resonances Yu, Anqi Yu, Dahai Yang, Zhenyu Guo, Xuguang Ren, Yuxiang Zang, Xiaofei Balakin, Alexei V. Shkurinov, Alexander P. Zhu, YiMing Nanomaterials (Basel) Article We applied the harmonic oscillator model combined with the transfer matrix method to study the polarization conversion for transmitted waves in metallic grating/plasmon-excitation layer/metallic grating structure in the terahertz (THz) region. By comparing the calculated spectra and the simulated (by the finite-difference-time-domain method) ones, we found that they correspond well with each other. Both methods show that the Drude background absorption and the excited plasmon resonances are responsible for polarization conversion. The transmission is close to 0 when the distance between the top/bottom metallic gratings and gated graphene is an integer multiple of half the wavelength of the incident wave (in the dielectrics), at which points the plasmon resonances are greatly suppressed by the destructive interference between the backward/forward electromagnetic waves and that reflected by the top/bottom metallic gratings. Away from these points, the transmission can be higher than 80%. The electron density and the excitation efficiency of the plasmon-excitation layer were found to be important for the bandwidth of the polarization conversion window, while the scattering rate was found to influence mainly the polarization conversion rate. Multi-broadband polarization conversion is realized by exciting plasmon modes between the 0 transmission points in the THz region. MDPI 2020-12-28 /pmc/articles/PMC7823980/ /pubmed/33379402 http://dx.doi.org/10.3390/nano11010056 Text en © 2020 by the authors. Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (http://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Article Yu, Anqi Yu, Dahai Yang, Zhenyu Guo, Xuguang Ren, Yuxiang Zang, Xiaofei Balakin, Alexei V. Shkurinov, Alexander P. Zhu, YiMing Terahertz Broadband Polarization Conversion for Transmitted Waves Based on Graphene Plasmon Resonances |
title | Terahertz Broadband Polarization Conversion for Transmitted Waves Based on Graphene Plasmon Resonances |
title_full | Terahertz Broadband Polarization Conversion for Transmitted Waves Based on Graphene Plasmon Resonances |
title_fullStr | Terahertz Broadband Polarization Conversion for Transmitted Waves Based on Graphene Plasmon Resonances |
title_full_unstemmed | Terahertz Broadband Polarization Conversion for Transmitted Waves Based on Graphene Plasmon Resonances |
title_short | Terahertz Broadband Polarization Conversion for Transmitted Waves Based on Graphene Plasmon Resonances |
title_sort | terahertz broadband polarization conversion for transmitted waves based on graphene plasmon resonances |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7823980/ https://www.ncbi.nlm.nih.gov/pubmed/33379402 http://dx.doi.org/10.3390/nano11010056 |
work_keys_str_mv | AT yuanqi terahertzbroadbandpolarizationconversionfortransmittedwavesbasedongrapheneplasmonresonances AT yudahai terahertzbroadbandpolarizationconversionfortransmittedwavesbasedongrapheneplasmonresonances AT yangzhenyu terahertzbroadbandpolarizationconversionfortransmittedwavesbasedongrapheneplasmonresonances AT guoxuguang terahertzbroadbandpolarizationconversionfortransmittedwavesbasedongrapheneplasmonresonances AT renyuxiang terahertzbroadbandpolarizationconversionfortransmittedwavesbasedongrapheneplasmonresonances AT zangxiaofei terahertzbroadbandpolarizationconversionfortransmittedwavesbasedongrapheneplasmonresonances AT balakinalexeiv terahertzbroadbandpolarizationconversionfortransmittedwavesbasedongrapheneplasmonresonances AT shkurinovalexanderp terahertzbroadbandpolarizationconversionfortransmittedwavesbasedongrapheneplasmonresonances AT zhuyiming terahertzbroadbandpolarizationconversionfortransmittedwavesbasedongrapheneplasmonresonances |