Band diagrams and field distribution of squarely-modulated slab metallic gratings

The optical transmission properties of squarely-modulated metallic gratings has been widely investigated. This study used rigorous-coupled wave analysis (RCWA) to re-examine in detail the band structure of a laminated metal film with squarely-modulated metallic gratings located at the top. The top s...

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Main Authors: Jih-Yin Lee, Yu-Ju Hung
Format: Article
Language:English
Published: AIP Publishing LLC 2016-12-01
Series:AIP Advances
Online Access:http://dx.doi.org/10.1063/1.4973336
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spelling doaj-341c251c853947f5894151bea9ad62872020-11-24T22:10:03ZengAIP Publishing LLCAIP Advances2158-32262016-12-01612125117125117-710.1063/1.4973336064612ADVBand diagrams and field distribution of squarely-modulated slab metallic gratingsJih-Yin Lee0Yu-Ju Hung1Department of Photonics, National Sun Yat-Sen University, Kaohsiung, Taiwan 80424, R.O.C.Department of Photonics, National Sun Yat-Sen University, Kaohsiung, Taiwan 80424, R.O.C.The optical transmission properties of squarely-modulated metallic gratings has been widely investigated. This study used rigorous-coupled wave analysis (RCWA) to re-examine in detail the band structure of a laminated metal film with squarely-modulated metallic gratings located at the top. The top structure was shown to modify the long-range surface plasmon polariton modes (LRSPP) at both interfaces of the thin metal film. When the thickness of the intact metal film was altered, the coupling between the two interfaces presented intriguing behavior. If the thickness of the metallic film was 30nm, the field achieved strong coupling similar to that of a two-level system. When the thickness was decreased to 10nm, the band branch possessing negative group velocity was dominant. Our results also verify that the first-order Fourier expansion of the gratings determined the energy position of bands at k||=0, whereas the second-order term caused band gap opening. Introducing an asymmetrical component to the grating profile intensified the opening effect at k||=0 due to an increase in the amplitude of the second-order Fourier component.http://dx.doi.org/10.1063/1.4973336
collection DOAJ
language English
format Article
sources DOAJ
author Jih-Yin Lee
Yu-Ju Hung
spellingShingle Jih-Yin Lee
Yu-Ju Hung
Band diagrams and field distribution of squarely-modulated slab metallic gratings
AIP Advances
author_facet Jih-Yin Lee
Yu-Ju Hung
author_sort Jih-Yin Lee
title Band diagrams and field distribution of squarely-modulated slab metallic gratings
title_short Band diagrams and field distribution of squarely-modulated slab metallic gratings
title_full Band diagrams and field distribution of squarely-modulated slab metallic gratings
title_fullStr Band diagrams and field distribution of squarely-modulated slab metallic gratings
title_full_unstemmed Band diagrams and field distribution of squarely-modulated slab metallic gratings
title_sort band diagrams and field distribution of squarely-modulated slab metallic gratings
publisher AIP Publishing LLC
series AIP Advances
issn 2158-3226
publishDate 2016-12-01
description The optical transmission properties of squarely-modulated metallic gratings has been widely investigated. This study used rigorous-coupled wave analysis (RCWA) to re-examine in detail the band structure of a laminated metal film with squarely-modulated metallic gratings located at the top. The top structure was shown to modify the long-range surface plasmon polariton modes (LRSPP) at both interfaces of the thin metal film. When the thickness of the intact metal film was altered, the coupling between the two interfaces presented intriguing behavior. If the thickness of the metallic film was 30nm, the field achieved strong coupling similar to that of a two-level system. When the thickness was decreased to 10nm, the band branch possessing negative group velocity was dominant. Our results also verify that the first-order Fourier expansion of the gratings determined the energy position of bands at k||=0, whereas the second-order term caused band gap opening. Introducing an asymmetrical component to the grating profile intensified the opening effect at k||=0 due to an increase in the amplitude of the second-order Fourier component.
url http://dx.doi.org/10.1063/1.4973336
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AT yujuhung banddiagramsandfielddistributionofsquarelymodulatedslabmetallicgratings
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