Talbot effect for periodical objects limited by finite apertures : a new interpretation

ABSTRACT: The paper presents a new interpretation of the Talbot effect for periodical objects limited by finite apertures. According to the proposed approach, a self-image of a real, finite object is a superposition of deformed images of an elementary cell. The singular elementary cell image is equi...

Full description

Autores:
Barrera Ramírez, John Fredy
Henao Henao, Rodrigo
Jaroszewicz, Zbigniew
Kolodziejczyk, Andrzej
Tipo de recurso:
Article of investigation
Fecha de publicación:
2005
Institución:
Universidad de Antioquia
Repositorio:
Repositorio UdeA
Idioma:
eng
OAI Identifier:
oai:bibliotecadigital.udea.edu.co:10495/9331
Acceso en línea:
http://hdl.handle.net/10495/9331
Palabra clave:
Diferencias finitas
Finite differences
Procesamiento de imágenes
Image processing
Efecto talbot
Talbot effect
Difracción
Diffraction
Imagen
Rights
openAccess
License
Atribución-NoComercial-SinDerivadas 2.5 Colombia
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oai_identifier_str oai:bibliotecadigital.udea.edu.co:10495/9331
network_acronym_str UDEA2
network_name_str Repositorio UdeA
repository_id_str
dc.title.spa.fl_str_mv Talbot effect for periodical objects limited by finite apertures : a new interpretation
title Talbot effect for periodical objects limited by finite apertures : a new interpretation
spellingShingle Talbot effect for periodical objects limited by finite apertures : a new interpretation
Diferencias finitas
Finite differences
Procesamiento de imágenes
Image processing
Efecto talbot
Talbot effect
Difracción
Diffraction
Imagen
title_short Talbot effect for periodical objects limited by finite apertures : a new interpretation
title_full Talbot effect for periodical objects limited by finite apertures : a new interpretation
title_fullStr Talbot effect for periodical objects limited by finite apertures : a new interpretation
title_full_unstemmed Talbot effect for periodical objects limited by finite apertures : a new interpretation
title_sort Talbot effect for periodical objects limited by finite apertures : a new interpretation
dc.creator.fl_str_mv Barrera Ramírez, John Fredy
Henao Henao, Rodrigo
Jaroszewicz, Zbigniew
Kolodziejczyk, Andrzej
dc.contributor.author.none.fl_str_mv Barrera Ramírez, John Fredy
Henao Henao, Rodrigo
Jaroszewicz, Zbigniew
Kolodziejczyk, Andrzej
dc.subject.none.fl_str_mv Diferencias finitas
Finite differences
Procesamiento de imágenes
Image processing
Efecto talbot
Talbot effect
Difracción
Diffraction
Imagen
topic Diferencias finitas
Finite differences
Procesamiento de imágenes
Image processing
Efecto talbot
Talbot effect
Difracción
Diffraction
Imagen
description ABSTRACT: The paper presents a new interpretation of the Talbot effect for periodical objects limited by finite apertures. According to the proposed approach, a self-image of a real, finite object is a superposition of deformed images of an elementary cell. The singular elementary cell image is equivalent to that formed in a proper optical system. Two possible optical arrangements are discussed. The theoretical description makes possible to define a structure of selfimages. Particularly, the approach enables a determination of apertures’ dimensions, which lead to self-images of a reasonable quality in a desired region of an image plane. The theory is illustrated and verified by numerical simulations.
publishDate 2005
dc.date.issued.none.fl_str_mv 2005
dc.date.accessioned.none.fl_str_mv 2018-04-05T21:12:13Z
dc.date.available.none.fl_str_mv 2018-04-05T21:12:13Z
dc.type.spa.fl_str_mv info:eu-repo/semantics/article
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dc.type.local.spa.fl_str_mv Artículo de investigación
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dc.identifier.citation.spa.fl_str_mv Barrera Ramírez, J. F., Henao Henao, R., Jaroszewicz, Z., & Kolodziejczyk, A. (2005). Talbot effect for periodical objects limited by finite apertures: a new interpretation. Optik. 116(3), 144-148. DOI:10.1016/j.ijleo.2004.12.008
dc.identifier.issn.none.fl_str_mv 1618-1336
dc.identifier.uri.none.fl_str_mv http://hdl.handle.net/10495/9331
dc.identifier.doi.none.fl_str_mv 10.1016/j.ijleo.2004.12.008
identifier_str_mv Barrera Ramírez, J. F., Henao Henao, R., Jaroszewicz, Z., & Kolodziejczyk, A. (2005). Talbot effect for periodical objects limited by finite apertures: a new interpretation. Optik. 116(3), 144-148. DOI:10.1016/j.ijleo.2004.12.008
1618-1336
10.1016/j.ijleo.2004.12.008
url http://hdl.handle.net/10495/9331
dc.language.iso.spa.fl_str_mv eng
language eng
dc.rights.*.fl_str_mv Atribución-NoComercial-SinDerivadas 2.5 Colombia
dc.rights.spa.fl_str_mv info:eu-repo/semantics/openAccess
dc.rights.uri.*.fl_str_mv http://creativecommons.org/licenses/by-nc-nd/2.5/co/
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dc.rights.creativecommons.spa.fl_str_mv https://creativecommons.org/licenses/by-nc-nd/4.0/
rights_invalid_str_mv Atribución-NoComercial-SinDerivadas 2.5 Colombia
http://creativecommons.org/licenses/by-nc-nd/2.5/co/
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eu_rights_str_mv openAccess
dc.format.mimetype.spa.fl_str_mv application/pdf
dc.publisher.spa.fl_str_mv Elsevier
dc.publisher.group.spa.fl_str_mv Grupo de Optica y Fotónica
dc.publisher.place.spa.fl_str_mv Alemania
institution Universidad de Antioquia
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spelling Barrera Ramírez, John FredyHenao Henao, RodrigoJaroszewicz, ZbigniewKolodziejczyk, Andrzej2018-04-05T21:12:13Z2018-04-05T21:12:13Z2005Barrera Ramírez, J. F., Henao Henao, R., Jaroszewicz, Z., & Kolodziejczyk, A. (2005). Talbot effect for periodical objects limited by finite apertures: a new interpretation. Optik. 116(3), 144-148. DOI:10.1016/j.ijleo.2004.12.0081618-1336http://hdl.handle.net/10495/933110.1016/j.ijleo.2004.12.008ABSTRACT: The paper presents a new interpretation of the Talbot effect for periodical objects limited by finite apertures. According to the proposed approach, a self-image of a real, finite object is a superposition of deformed images of an elementary cell. The singular elementary cell image is equivalent to that formed in a proper optical system. Two possible optical arrangements are discussed. The theoretical description makes possible to define a structure of selfimages. Particularly, the approach enables a determination of apertures’ dimensions, which lead to self-images of a reasonable quality in a desired region of an image plane. The theory is illustrated and verified by numerical simulations.application/pdfengElsevierGrupo de Optica y FotónicaAlemaniainfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/articlehttp://purl.org/coar/resource_type/c_2df8fbb1https://purl.org/redcol/resource_type/ARTArtículo de investigaciónhttp://purl.org/coar/version/c_970fb48d4fbd8a85Atribución-NoComercial-SinDerivadas 2.5 Colombiainfo:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by-nc-nd/2.5/co/http://purl.org/coar/access_right/c_abf2https://creativecommons.org/licenses/by-nc-nd/4.0/Diferencias finitasFinite differencesProcesamiento de imágenesImage processingEfecto talbotTalbot effectDifracciónDiffractionImagenTalbot effect for periodical objects limited by finite apertures : a new interpretationOptik1441481163CC-LICENSElicense_urllicense_urlArtículo de investigacióntext/plain; charset=utf-849http://bibliotecadigital.udea.edu.co/bitstream/10495/9331/2/license_url4afdbb8c545fd630ea7db775da747b2fMD52license_textlicense_texttext/html; charset=utf-80http://bibliotecadigital.udea.edu.co/bitstream/10495/9331/3/license_textd41d8cd98f00b204e9800998ecf8427eMD53license_rdflicense_rdfLicenciaapplication/rdf+xml; charset=utf-80http://bibliotecadigital.udea.edu.co/bitstream/10495/9331/4/license_rdfd41d8cd98f00b204e9800998ecf8427eMD54ORIGINALBarreraJohn_2005_TalbotEffectObjects.pdfBarreraJohn_2005_TalbotEffectObjects.pdfArtículo de investigaciónapplication/pdf444470http://bibliotecadigital.udea.edu.co/bitstream/10495/9331/1/BarreraJohn_2005_TalbotEffectObjects.pdf7116a83fa7952807f6a913badfaaaffaMD51LICENSElicense.txtlicense.txttext/plain; charset=utf-81748http://bibliotecadigital.udea.edu.co/bitstream/10495/9331/5/license.txt8a4605be74aa9ea9d79846c1fba20a33MD5510495/9331oai:bibliotecadigital.udea.edu.co:10495/93312021-05-16 11:44:03.528Repositorio Institucional Universidad de Antioquiaandres.perez@udea.edu.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