Highly-resonant two-polarization transmission guided-mode resonance filter
We theoretically demonstrate a mid-infrared polarization-independent guided-mode-resonance transmission filter. We designed a structure based on a deeply-etched 2D grating above a thin slab of the same material respectively supporting transverse magnetic and transverse electric fundamental modes wit...
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2018-11-01
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Online Access: | http://dx.doi.org/10.1063/1.5051621 |
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doaj-a787eca6b038437186f6afdd2259cc232020-11-24T20:58:44ZengAIP Publishing LLCAIP Advances2158-32262018-11-01811115228115228-710.1063/1.5051621117811ADVHighly-resonant two-polarization transmission guided-mode resonance filterLéopold Macé0Olivier Gauthier-Lafaye1Antoine Monmayrant2Stéphane Calvez3Henri Camon4Hervé Leplan5SAFRAN REOSC, Avenue de la Tour Maury, 91280 Saint-Pierre-du-Perray, FranceLAAS-CNRS, Université de Toulouse, CNRS, 31400 Toulouse, FranceLAAS-CNRS, Université de Toulouse, CNRS, 31400 Toulouse, FranceLAAS-CNRS, Université de Toulouse, CNRS, 31400 Toulouse, FranceLAAS-CNRS, Université de Toulouse, CNRS, 31400 Toulouse, FranceSAFRAN REOSC, Avenue de la Tour Maury, 91280 Saint-Pierre-du-Perray, FranceWe theoretically demonstrate a mid-infrared polarization-independent guided-mode-resonance transmission filter. We designed a structure based on a deeply-etched 2D grating above a thin slab of the same material respectively supporting transverse magnetic and transverse electric fundamental modes with identical effective index, which propagate along orthogonal directions. This device relates to multi-resonant guided-mode-resonance filters, and more particularly to the concept of zero-contrast gratings (ZCG), which can operate either as wideband reflectors [R. Magnusson, Optics Letters 39, 4337 (2014)] or bandpass filters [M. Niraula, J. W. Yoon, and R. Magnusson, Optics Letters 40, 5062 (2015)]. However, contrary to the latter, this new generation of filters is not bound by stringent material requirements inherent to conventional ZCGs. In particular, ZCGs are demonstrated with high to low refractive index ratio below 2, using germanium as high-index material over a low-index zinc sulfide substrate. These filters exhibit a transmission peak with a full-width at half-maximum of about 30 pm, and a maximum transmission close to 100 % lying in a 46-nm-wide rejection window.http://dx.doi.org/10.1063/1.5051621 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Léopold Macé Olivier Gauthier-Lafaye Antoine Monmayrant Stéphane Calvez Henri Camon Hervé Leplan |
spellingShingle |
Léopold Macé Olivier Gauthier-Lafaye Antoine Monmayrant Stéphane Calvez Henri Camon Hervé Leplan Highly-resonant two-polarization transmission guided-mode resonance filter AIP Advances |
author_facet |
Léopold Macé Olivier Gauthier-Lafaye Antoine Monmayrant Stéphane Calvez Henri Camon Hervé Leplan |
author_sort |
Léopold Macé |
title |
Highly-resonant two-polarization transmission guided-mode resonance filter |
title_short |
Highly-resonant two-polarization transmission guided-mode resonance filter |
title_full |
Highly-resonant two-polarization transmission guided-mode resonance filter |
title_fullStr |
Highly-resonant two-polarization transmission guided-mode resonance filter |
title_full_unstemmed |
Highly-resonant two-polarization transmission guided-mode resonance filter |
title_sort |
highly-resonant two-polarization transmission guided-mode resonance filter |
publisher |
AIP Publishing LLC |
series |
AIP Advances |
issn |
2158-3226 |
publishDate |
2018-11-01 |
description |
We theoretically demonstrate a mid-infrared polarization-independent guided-mode-resonance transmission filter. We designed a structure based on a deeply-etched 2D grating above a thin slab of the same material respectively supporting transverse magnetic and transverse electric fundamental modes with identical effective index, which propagate along orthogonal directions. This device relates to multi-resonant guided-mode-resonance filters, and more particularly to the concept of zero-contrast gratings (ZCG), which can operate either as wideband reflectors [R. Magnusson, Optics Letters 39, 4337 (2014)] or bandpass filters [M. Niraula, J. W. Yoon, and R. Magnusson, Optics Letters 40, 5062 (2015)]. However, contrary to the latter, this new generation of filters is not bound by stringent material requirements inherent to conventional ZCGs. In particular, ZCGs are demonstrated with high to low refractive index ratio below 2, using germanium as high-index material over a low-index zinc sulfide substrate. These filters exhibit a transmission peak with a full-width at half-maximum of about 30 pm, and a maximum transmission close to 100 % lying in a 46-nm-wide rejection window. |
url |
http://dx.doi.org/10.1063/1.5051621 |
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