Refraction of a three-dimensional beam in uniaxial crystal-isotropic medium interfaces in presence of inhibited reflection

We propose a generalization of Artmann's method for three-dimensional beams. This generalization, that does not consider a symmetry coordinate for the incident beam, allows its use in non-isotropic interfaces. We apply it particularly to the study of the refraction of a beam that is limited in...

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Autores principales: Vanney, C.E., Perez, L.I., Marcano O. A., Paz J.L.
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Acceso en línea:http://hdl.handle.net/20.500.12110/paper_0277786X_v5622_nPART3_p1113_Vanney
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spelling todo:paper_0277786X_v5622_nPART3_p1113_Vanney2023-10-03T15:16:30Z Refraction of a three-dimensional beam in uniaxial crystal-isotropic medium interfaces in presence of inhibited reflection Vanney, C.E. Perez, L.I. Marcano O. A. Paz J.L. Inhibited reflection Lateral displacement Uniaxial crystal Anisotropy Approximation theory Interfaces (materials) Light interference Light reflection Vectors Wavefronts Inhibited reflection Lateral displacement Optical axis Uniaxial crystals Light refraction We propose a generalization of Artmann's method for three-dimensional beams. This generalization, that does not consider a symmetry coordinate for the incident beam, allows its use in non-isotropic interfaces. We apply it particularly to the study of the refraction of a beam that is limited in two directions and that impinges on a uniaxial crystal-isotropic medium interface in presence of inhibited reflection. As known, the direction of the energy flux of a three-dimensional incident beam can be obtained (to first order and considering paraxial approximation) from the interference patterns of two two-dimensional beams. Each beam can be obtained from the superposition of two plane waves. In the first beam, the normals to the wave fronts are contained in the same incidence plane and they impinge with different angles; in the second, they are contained in different planes of incidence but with the same angle. We show that the refracted ray, in presence of inhibited reflection, suffers a lateral displacement that is not contained in the plane of incidence. The refraction of the first two-dimensional wave packet takes into account the longitudinal displacement whereas the refraction of the second allows us to calculate the transversal displacement. CONF info:eu-repo/semantics/openAccess http://creativecommons.org/licenses/by/2.5/ar http://hdl.handle.net/20.500.12110/paper_0277786X_v5622_nPART3_p1113_Vanney
institution Universidad de Buenos Aires
institution_str I-28
repository_str R-134
collection Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA)
topic Inhibited reflection
Lateral displacement
Uniaxial crystal
Anisotropy
Approximation theory
Interfaces (materials)
Light interference
Light reflection
Vectors
Wavefronts
Inhibited reflection
Lateral displacement
Optical axis
Uniaxial crystals
Light refraction
spellingShingle Inhibited reflection
Lateral displacement
Uniaxial crystal
Anisotropy
Approximation theory
Interfaces (materials)
Light interference
Light reflection
Vectors
Wavefronts
Inhibited reflection
Lateral displacement
Optical axis
Uniaxial crystals
Light refraction
Vanney, C.E.
Perez, L.I.
Marcano O. A.
Paz J.L.
Refraction of a three-dimensional beam in uniaxial crystal-isotropic medium interfaces in presence of inhibited reflection
topic_facet Inhibited reflection
Lateral displacement
Uniaxial crystal
Anisotropy
Approximation theory
Interfaces (materials)
Light interference
Light reflection
Vectors
Wavefronts
Inhibited reflection
Lateral displacement
Optical axis
Uniaxial crystals
Light refraction
description We propose a generalization of Artmann's method for three-dimensional beams. This generalization, that does not consider a symmetry coordinate for the incident beam, allows its use in non-isotropic interfaces. We apply it particularly to the study of the refraction of a beam that is limited in two directions and that impinges on a uniaxial crystal-isotropic medium interface in presence of inhibited reflection. As known, the direction of the energy flux of a three-dimensional incident beam can be obtained (to first order and considering paraxial approximation) from the interference patterns of two two-dimensional beams. Each beam can be obtained from the superposition of two plane waves. In the first beam, the normals to the wave fronts are contained in the same incidence plane and they impinge with different angles; in the second, they are contained in different planes of incidence but with the same angle. We show that the refracted ray, in presence of inhibited reflection, suffers a lateral displacement that is not contained in the plane of incidence. The refraction of the first two-dimensional wave packet takes into account the longitudinal displacement whereas the refraction of the second allows us to calculate the transversal displacement.
format CONF
author Vanney, C.E.
Perez, L.I.
Marcano O. A.
Paz J.L.
author_facet Vanney, C.E.
Perez, L.I.
Marcano O. A.
Paz J.L.
author_sort Vanney, C.E.
title Refraction of a three-dimensional beam in uniaxial crystal-isotropic medium interfaces in presence of inhibited reflection
title_short Refraction of a three-dimensional beam in uniaxial crystal-isotropic medium interfaces in presence of inhibited reflection
title_full Refraction of a three-dimensional beam in uniaxial crystal-isotropic medium interfaces in presence of inhibited reflection
title_fullStr Refraction of a three-dimensional beam in uniaxial crystal-isotropic medium interfaces in presence of inhibited reflection
title_full_unstemmed Refraction of a three-dimensional beam in uniaxial crystal-isotropic medium interfaces in presence of inhibited reflection
title_sort refraction of a three-dimensional beam in uniaxial crystal-isotropic medium interfaces in presence of inhibited reflection
url http://hdl.handle.net/20.500.12110/paper_0277786X_v5622_nPART3_p1113_Vanney
work_keys_str_mv AT vanneyce refractionofathreedimensionalbeaminuniaxialcrystalisotropicmediuminterfacesinpresenceofinhibitedreflection
AT perezli refractionofathreedimensionalbeaminuniaxialcrystalisotropicmediuminterfacesinpresenceofinhibitedreflection
AT marcanooa refractionofathreedimensionalbeaminuniaxialcrystalisotropicmediuminterfacesinpresenceofinhibitedreflection
AT pazjl refractionofathreedimensionalbeaminuniaxialcrystalisotropicmediuminterfacesinpresenceofinhibitedreflection
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