Representación modal de campos ópticos de auto-imágenes.

Optical fields that presents periodicity through the axis of propagation are called “self-imaging” fields. Such fields give rise to the well-known Talbot and Lau effects, which have had a lot of attention these last years due to the applications associated to them. Some authors define a partially co...

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Detalhes bibliográficos
Autor: ANGEL SINUE CRUZ FELIX
Formato: tesis de maestría
Estado:Versión aceptada para publicación
Fecha de publicación:2008
País:México
Recursos:Instituto Nacional de Astrofísica, Óptica y Electrónica
Repositorio:Repositorio Institucional del INAOE
Idioma:español
OAI Identifier:oai:inaoe.repositorioinstitucional.mx:1009/417
Acesso em linha:http://inaoe.repositorioinstitucional.mx/jspui/handle/1009/417
Access Level:acceso abierto
Palavra-chave:info:eu-repo/classification/Coherencia/Coherence
info:eu-repo/classification/Talbot efectos/Talbot effects
info:eu-repo/classification/Análisis modal/Modal analysis
info:eu-repo/classification/cti/1
info:eu-repo/classification/cti/22
info:eu-repo/classification/cti/2209
info:eu-repo/classification/cti/220990
Descrição
Resumo:Optical fields that presents periodicity through the axis of propagation are called “self-imaging” fields. Such fields give rise to the well-known Talbot and Lau effects, which have had a lot of attention these last years due to the applications associated to them. Some authors define a partially coherent self-imaging field as that which its cross-spectral density function is the same for two planes separated by a distance d. We have found the coherent mode-representation of self-imaging fields within the frame of the coherence spectral theory formulated by Wolf, we have proven that when we consider complete coherence of the field, we obtain the general expression for self-imaging fields and in the case when we have the superposition of an infinite numbers of coherent modes then we obtain the expression for the Lau effect.