Diffraction by a grating made of a uniaxial dielectric-magnetic medium exhibiting negative refraction

Diffraction of linearly polarized plane electromagnetic waves at the periodically corrugated boundary of vacuum and a linear, homogeneous, uniaxial, dielectric-magnetic medium is formulated as a boundary-value problem and solved using the Rayleigh method. The focus is on situations where the diffrac...

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Detalles Bibliográficos
Autores principales:	Depine, R.A., Lakhtakia, A.
Formato:	JOUR
Materias:	Dielectric-magnetic medium Negative refraction Permeability tensors Boundary value problems Electromagnetic waves Permittivity Polarization Rayleigh fading Tensors Diffraction gratings
Acceso en línea:	http://hdl.handle.net/20.500.12110/paper_13672630_v7_n_p_Depine
Aporte de:	Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA) de Universidad de Buenos Aires

id	todo:paper_13672630_v7_n_p_Depine
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spelling	todo:paper_13672630_v7_n_p_Depine2023-10-03T16:11:31Z Diffraction by a grating made of a uniaxial dielectric-magnetic medium exhibiting negative refraction Depine, R.A. Lakhtakia, A. Dielectric-magnetic medium Negative refraction Permeability tensors Boundary value problems Electromagnetic waves Permittivity Polarization Rayleigh fading Tensors Diffraction gratings Diffraction of linearly polarized plane electromagnetic waves at the periodically corrugated boundary of vacuum and a linear, homogeneous, uniaxial, dielectric-magnetic medium is formulated as a boundary-value problem and solved using the Rayleigh method. The focus is on situations where the diffracted fields maintain the same polarization state as the s- or p-polarized incident plane wave. Attention is paid to two classes of diffracting media: those with negative definite permittivity and permeability tensors, and those with indefinite permittivity and permeability tensors. For the situations investigated, whereas the dispersion equations in the diffracting medium turn out to be elliptic for the first class of diffracting media, they are hyperbolic for the second class. Examples are reported with the first class of diffracting media of instances when the grating acts either as a positively refracting interface or as a negatively refracting interface. For the second class of diffracting media, hyperbolic dispersion equations imply the possibility of an infinite number of refraction channels. © lOP Publishing Ltd and Deutsche Physikalische Gesellschaft. JOUR info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by/2.5/ar http://hdl.handle.net/20.500.12110/paper_13672630_v7_n_p_Depine
institution	Universidad de Buenos Aires
institution_str	I-28
repository_str	R-134
collection	Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA)
topic	Dielectric-magnetic medium Negative refraction Permeability tensors Boundary value problems Electromagnetic waves Permittivity Polarization Rayleigh fading Tensors Diffraction gratings
spellingShingle	Dielectric-magnetic medium Negative refraction Permeability tensors Boundary value problems Electromagnetic waves Permittivity Polarization Rayleigh fading Tensors Diffraction gratings Depine, R.A. Lakhtakia, A. Diffraction by a grating made of a uniaxial dielectric-magnetic medium exhibiting negative refraction
topic_facet	Dielectric-magnetic medium Negative refraction Permeability tensors Boundary value problems Electromagnetic waves Permittivity Polarization Rayleigh fading Tensors Diffraction gratings
description	Diffraction of linearly polarized plane electromagnetic waves at the periodically corrugated boundary of vacuum and a linear, homogeneous, uniaxial, dielectric-magnetic medium is formulated as a boundary-value problem and solved using the Rayleigh method. The focus is on situations where the diffracted fields maintain the same polarization state as the s- or p-polarized incident plane wave. Attention is paid to two classes of diffracting media: those with negative definite permittivity and permeability tensors, and those with indefinite permittivity and permeability tensors. For the situations investigated, whereas the dispersion equations in the diffracting medium turn out to be elliptic for the first class of diffracting media, they are hyperbolic for the second class. Examples are reported with the first class of diffracting media of instances when the grating acts either as a positively refracting interface or as a negatively refracting interface. For the second class of diffracting media, hyperbolic dispersion equations imply the possibility of an infinite number of refraction channels. © lOP Publishing Ltd and Deutsche Physikalische Gesellschaft.
format	JOUR
author	Depine, R.A. Lakhtakia, A.
author_facet	Depine, R.A. Lakhtakia, A.
author_sort	Depine, R.A.
title	Diffraction by a grating made of a uniaxial dielectric-magnetic medium exhibiting negative refraction
title_short	Diffraction by a grating made of a uniaxial dielectric-magnetic medium exhibiting negative refraction
title_full	Diffraction by a grating made of a uniaxial dielectric-magnetic medium exhibiting negative refraction
title_fullStr	Diffraction by a grating made of a uniaxial dielectric-magnetic medium exhibiting negative refraction
title_full_unstemmed	Diffraction by a grating made of a uniaxial dielectric-magnetic medium exhibiting negative refraction
title_sort	diffraction by a grating made of a uniaxial dielectric-magnetic medium exhibiting negative refraction
url	http://hdl.handle.net/20.500.12110/paper_13672630_v7_n_p_Depine
work_keys_str_mv	AT depinera diffractionbyagratingmadeofauniaxialdielectricmagneticmediumexhibitingnegativerefraction AT lakhtakiaa diffractionbyagratingmadeofauniaxialdielectricmagneticmediumexhibitingnegativerefraction
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Diffraction by a grating made of a uniaxial dielectric-magnetic medium exhibiting negative refraction

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