Please use this identifier to cite or link to this item: http://ricaxcan.uaz.edu.mx/jspui/handle/20.500.11845/613
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dc.contributor39945es_ES
dc.contributor.otherhttps://orcid.org/0000-0003-0087-8991-
dc.contributor.otherhttps://orcid.org/0000-0002-6232-9958-
dc.coverage.spatialGlobales_ES
dc.creatorMartínez Orozco, Juan Carlos-
dc.creatorRojas Briseño, J. G.-
dc.creatorRodríguez Magdaleno, Karla Arely-
dc.creatorRodríguez Vargas, Isaac-
dc.creatorMora Ramos, Miguel Eduardo-
dc.creatorRestrepo Arango, Ricardo León-
dc.creatorUngan, Fatih-
dc.creatorKasapoǧlu, Esin-
dc.creatorDuque, Carlos Alberto-
dc.date.accessioned2018-08-08T16:34:03Z-
dc.date.available2018-08-08T16:34:03Z-
dc.date.issued2017-11-
dc.identifierinfo:eu-repo/semantics/publishedVersiones_ES
dc.identifier.issn0921-4526es_ES
dc.identifier.urihttp://hdl.handle.net/20.500.11845/613-
dc.identifier.urihttps://doi.org/10.48779/mbxx-rq44-
dc.description.abstractIn this paper we are reporting the computation for the Nonlinear Optical Rectification (NOR) and the Second and Third Harmonic Generation (SHG and THG) related with electronic states of asymmetric double Si-δ-doped quantum well in a GaAs matrix when this is subjected to an in-plane (x-oriented) constant magnetic field effect. The work is performed in the effective mass and parabolic band approximations in order to compute the electronic structure for the system by a diagonalization procedure. The expressions for the nonlinear optical susceptibilities, χ0 (2), χ2ω (2), and χ 3ω (3), are those arising from the compact matrix density formulation and stand for the NOR, SHG, and THG, respectively. This asymmetric double δ-doped quantum well potential profile actually exhibits nonzero NOR, SHG, and THG responses which can be easily controlled by the in-plane (x-direction) externally applied magnetic field. In particular we find that for the chosen configuration the harmonic generation is in the far-infrared/THz region, thus and becoming suitable building blocks for photodetectors in this range of the electromagnetic spectra.es_ES
dc.language.isoenges_ES
dc.publisherElsevieres_ES
dc.relationhttps://reader.elsevier.com/reader/sd/2B62B65AB4CD9317A3F21FFF86C70A438A1126944DABDB9B14DD92F8D0B9A6D08F21030DE0F09CDBC9E7FBBDC129D51A#pf1es_ES
dc.relation.ispartofhttps://www.sciencedirect.com/science/article/pii/S0921452617305756?via%3Dihub#!es_ES
dc.relation.urigeneralPublices_ES
dc.rightsAtribución-NoComercial-CompartirIgual 3.0 Estados Unidos de América*
dc.rights.urihttp://creativecommons.org/licenses/by-nc-sa/3.0/us/*
dc.sourcePhysica B: Condensed Matter Volume 525, 15 November 2017, Pages 30-35es_ES
dc.subject.classificationCIENCIAS FISICO MATEMATICAS Y CIENCIAS DE LA TIERRA [1]es_ES
dc.subject.otherδ-doped QWes_ES
dc.subject.otherNonlinear optical rectificationes_ES
dc.subject.otherSecond Harmonic Generationes_ES
dc.subject.otherThird Harmonic Generationes_ES
dc.titleEffect of the magnetic field on the nonlinear optical rectification and second and third harmonic generation in double δ-doped GaAs quantum wellses_ES
dc.typeinfo:eu-repo/semantics/conferenceObjectes_ES
Appears in Collections:*Documentos Académicos*-- UA Física

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