Corrected coupled-wave theory for non-slanted reflection gratings

Please use this identifier to cite or link to this item: http://hdl.handle.net/10045/19879
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dc.contributorHolografía y Procesado Ópticoen
dc.contributor.authorEstepa Espada, Luis Alberto-
dc.contributor.authorNeipp, Cristian-
dc.contributor.authorFrancés, Jorge-
dc.contributor.authorMárquez, Andrés-
dc.contributor.authorBleda, Sergio-
dc.contributor.authorPérez Molina, Manuel-
dc.contributor.authorOrtuño, Manuel-
dc.contributor.authorGallego, Sergi-
dc.contributor.otherUniversidad de Alicante. Departamento de Física, Ingeniería de Sistemas y Teoría de la Señalen
dc.contributor.otherUniversidad de Alicante. Instituto Universitario de Física Aplicada a las Ciencias y las Tecnologíasen
dc.date.accessioned2011-12-09T10:39:29Z-
dc.date.available2011-12-09T10:39:29Z-
dc.date.created2011-07-
dc.date.issued2011-10-05-
dc.identifier.citationESTEPA ESPADA, Luis Alberto, et al. "Corrected coupled-wave theory for non-slanted reflection gratings". En: Physical Optics / edited by Daniel G. Smith, Frank Wyrowski, Andreas Erdmann. Bellingham, Wash. : SPIE, 2011. (Proceedings of SPIE; Vol. 8171). ISBN 978-0-81948-797-1, pp. 81710R-1/10en
dc.identifier.isbn978-0-81948-797-1-
dc.identifier.issn0277-786X-
dc.identifier.urihttp://hdl.handle.net/10045/19879-
dc.description.abstractIn this work we present an analysis of non-slanted reflection gratings by using a corrected Coupled Wave Theory which takes into account boundary conditions. It is well known that Kogelnik's Coupled Wave Theory predicts with great accuracy the response of the efficiency of the zero and first order for volume phase gratings, for both reflection and transmission gratings. Nonetheless, since this theory disregard the second derivatives in the coupled wave equations derived from Maxwell equations, it doesn't account for boundary conditions. Moreover only two orders are supposed, so when either the thickness is low or when high refractive index high are recorded in the element Kogelnik's Theory deviates from the expected results. In Addition, for non-slanted reflection gratings, the natural reflected wave superimpose the reflection order predicted by Coupled Wave theories, so the reflectance cannot be obtained by the classical expression of Kogelnik's Theory for reflection gratings. In this work we correct Kogelnik's Coupled Wave Theory to take into account these issues, the results are compared to those obtained by a Matrix Method, showing good agreement between both theories.en
dc.description.sponsorshipThis work was supported by the “Ministerio de Ciencia e Innovación" of Spain under projects FIS2008-05856-C02-01 and FIS2008-05856-C02-02, and by the “Generalitat Valenciana" of Spain under project PROMETEO/2011/021.en
dc.languageengen
dc.publisherSPIE, The International Society for Optical Engineeringen
dc.rightsCopyright 2011 Society of Photo-Optical Instrumentation Engineers. This paper was published in Proceedings of SPIE, vol. 8171, and is made available as an electronic reprint with permission of SPIE. One print or electronic copy may be made for personal use only. Systematic or multiple reproduction, distribution to multiple locations via electronic or other means, duplication of any material in this paper for a fee or for commercial purposes, or modification of the content of the paper are prohibited.en
dc.subjectHolographyen
dc.subjectMatrix methoden
dc.subjectCoupled wave theoryen
dc.subjectVolume phase gratingen
dc.subjectDiffraction gratingen
dc.subjectDiffraction efficiencyen
dc.subject.otherFísica Aplicadaen
dc.subject.otherÓpticaen
dc.subject.otherElectromagnetismoen
dc.titleCorrected coupled-wave theory for non-slanted reflection gratingsen
dc.typeinfo:eu-repo/semantics/articleen
dc.peerreviewedsien
dc.identifier.doi10.1117/12.896877-
dc.relation.publisherversionhttp://dx.doi.org/10.1117/12.896877en
dc.rights.accessRightsinfo:eu-repo/semantics/openAccessen
dc.relation.projectIDinfo:eu-repo/grantAgreement/MICINN//FIS2008-05856-C02-01-
dc.relation.projectIDinfo:eu-repo/grantAgreement/MICINN//FIS2008-05856-C02-02-
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