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dc.creatorBotey, Murieles
dc.creatorMolinos Gómez, Albertoes
dc.creatorDorado, Luis A.es
dc.creatorDepine, Ricardo A.es
dc.creatorLozano Barbero, Gabriel Sebastiánes
dc.creatorMartorell, Jordies
dc.creatorMihi, Agustínes
dc.creatorMaymó, Marces
dc.creatorMíguez García, Hernán Ruyes
dc.date.accessioned2018-04-19T08:59:19Z
dc.date.available2018-04-19T08:59:19Z
dc.date.issued2009
dc.identifier.citationBotey, M., Molinos Gómez, A., Dorado, L.A., Depine, R.A., Lozano Barbero, G. S., Martorell, J.,...,Míguez García, H.R. (2009). Light generation at the anomalous dispersion high energy range of a nonlinear opal film. Optics Express, 17 (15), 12210-12216.
dc.identifier.issn1094-4087es
dc.identifier.urihttps://hdl.handle.net/11441/73221
dc.description.abstractWe study experimentally and theoretically light propagation and generation at the high energy range of a close-packed fcc photonic crystal of polystyrene spheres coated with a nonlinear material. We observe an enhancement of the second harmonic generation of light that may be explained on the basis of amplification effects arising from propagation at anomalous group velocities. Theoretical calculations are performed to support this assumption. The vector KKR method we use allows us to determine, from the linear response of the crystal, the behavior of the group velocity in our finite photonic structures when losses introduced by absorption or scattering by defects are taken into account assuming a nonzero imaginary part for the dielectric constant. In such structures, we predict large variations of the group velocity for wavelengths on the order or smaller than the lattice constant of the structure, where an anomalous group velocity behavior is associated with the flat bands of the photonic band structure. We find that a direct relation may be established between the group velocity reduction and the enhancement of a light generation processes such as the second harmonic generation we consider. However, frequencies for which the enhancement is found, in the finite photonic crystals we use, do not necessarily coincide with the frequencies of flat high energy bands.es
dc.description.sponsorshipCONSOLIDER NANOLIGHT CSD2007-00046es
dc.description.sponsorshipEspaña Ministerio de Ciencia e Innovación MAT2008-00910/NAN MAT2008-02166es
dc.description.sponsorshipCONSOLIDER HOPE CSD2007- 00007es
dc.description.sponsorshipJunta de Andalucía FQM3579.es
dc.formatapplication/pdfes
dc.language.isoenges
dc.publisherOptical Society of Americaes
dc.relation.ispartofOptics Express, 17 (15), 12210-12216.
dc.rightsAttribution-NonCommercial-NoDerivatives 4.0 Internacional*
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/4.0/*
dc.titleLight generation at the anomalous dispersion high energy range of a nonlinear opal filmes
dc.typeinfo:eu-repo/semantics/articlees
dcterms.identifierhttps://ror.org/03yxnpp24
dc.type.versioninfo:eu-repo/semantics/publishedVersiones
dc.rights.accessRightsinfo:eu-repo/semantics/openAccesses
dc.relation.projectIDCSD2007-00046es
dc.relation.projectIDMAT2008-00910/NANes
dc.relation.projectIDMAT2008-02166es
dc.relation.projectIDCSD2007- 00007es
dc.relation.projectIDFQM3579.es
dc.relation.publisherversionhttp://dx.doi.org/10.1364/OE.17.012210/es
dc.identifier.doi10.1364/OE.17.012210es
idus.format.extent7 p.es
dc.journaltitleOptics Expresses
dc.publication.volumen17es
dc.publication.issue15es
dc.publication.initialPage12210es
dc.publication.endPage12216es

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