Structural, optoelectronic, and thermodynamic properties of YxAl1-xN semiconducting alloys

The structural, electronic, optical, and thermodynamic properties of YxAl1-xN alloys were computed using first-principles calculations. The effects of exchange and correlation have been considered by means of the generalized gradient approximation (GGA) with the Perdew–Burke–Ernzerhof parametrizatio...

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Autores:
López Pérez, William
González García, Alvaro
González Hernández, Rafael J.
Ramirez Montes, Luz Mery
Tipo de recurso:
Article of journal
Fecha de publicación:
2016
Institución:
Corporación Universidad de la Costa
Repositorio:
REDICUC - Repositorio CUC
Idioma:
eng
OAI Identifier:
oai:repositorio.cuc.edu.co:11323/3262
Acceso en línea:
https://hdl.handle.net/11323/3262
https://repositorio.cuc.edu.co/
Palabra clave:
Wurtzite
Dielectric function
Bulk modulus
Wurtzite phase
Yttrium concentration
Función dieléctrica
Módulo de volumen
Fase de Wurtzite
Concentración de itrio
Rights
openAccess
License
Attribution-NonCommercial-ShareAlike 4.0 International
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dc.title.spa.fl_str_mv Structural, optoelectronic, and thermodynamic properties of YxAl1-xN semiconducting alloys
dc.title.translated.spa.fl_str_mv Propiedades estructurales, optoelectrónicas y termodinámicas de las aleaciones semiconductoras YxAl1-xN.
title Structural, optoelectronic, and thermodynamic properties of YxAl1-xN semiconducting alloys
spellingShingle Structural, optoelectronic, and thermodynamic properties of YxAl1-xN semiconducting alloys
Wurtzite
Dielectric function
Bulk modulus
Wurtzite phase
Yttrium concentration
Función dieléctrica
Módulo de volumen
Fase de Wurtzite
Concentración de itrio
title_short Structural, optoelectronic, and thermodynamic properties of YxAl1-xN semiconducting alloys
title_full Structural, optoelectronic, and thermodynamic properties of YxAl1-xN semiconducting alloys
title_fullStr Structural, optoelectronic, and thermodynamic properties of YxAl1-xN semiconducting alloys
title_full_unstemmed Structural, optoelectronic, and thermodynamic properties of YxAl1-xN semiconducting alloys
title_sort Structural, optoelectronic, and thermodynamic properties of YxAl1-xN semiconducting alloys
dc.creator.fl_str_mv López Pérez, William
González García, Alvaro
González Hernández, Rafael J.
Ramirez Montes, Luz Mery
dc.contributor.author.spa.fl_str_mv López Pérez, William
González García, Alvaro
González Hernández, Rafael J.
Ramirez Montes, Luz Mery
dc.subject.spa.fl_str_mv Wurtzite
Dielectric function
Bulk modulus
Wurtzite phase
Yttrium concentration
Función dieléctrica
Módulo de volumen
Fase de Wurtzite
Concentración de itrio
topic Wurtzite
Dielectric function
Bulk modulus
Wurtzite phase
Yttrium concentration
Función dieléctrica
Módulo de volumen
Fase de Wurtzite
Concentración de itrio
description The structural, electronic, optical, and thermodynamic properties of YxAl1-xN alloys were computed using first-principles calculations. The effects of exchange and correlation have been considered by means of the generalized gradient approximation (GGA) with the Perdew–Burke–Ernzerhof parametrization. In addition, the Tran–Blaha-modified Becke–Johnson potential (TB-mBJ) was applied to give a better description of the band-gap energies and optical spectra. The lattice parameters, bulk modulus, and band-gap energy show nonlinear dependence on concentration x. Results for rock-salt YxAl1-xN alloys show that the band gap undergoes an indirect (Γ→X)-to-direct (Γ→Γ) transition at a given yttrium composition, followed by a direct (Γ→Γ)-to-indirect (Γ→X) transition in a higher yttrium concentration. For wurtzite YxAl1-xN alloys, the band gap presents a direct (Γ→Γ)-to-indirect (→Γ) transition at a given yttrium composition, followed by an indirect (→Γ)-to-indirect (M→Σ) transition in a higher yttrium concentration. The real dielectric function, imaginary dielectric function, refractive index, and extinction coefficient were calculated using the TB-mBJ potential. Using a regular solution model, slightly lower mixing enthalpies for wurtzite YxAl1-xN alloys were found. The mixing enthalpy for a given concentration differs depending on structures, and on the interaction between atoms of constituents. The effect of temperature on the volume, bulk modulus, Debye temperature, and the heat capacity for YxAl1-xN alloys was analyzed using the quasi-harmonic Debye model. Results show that the heat capacity is fairly sensitive to composition as temperature increases.
publishDate 2016
dc.date.issued.none.fl_str_mv 2016-04-05
dc.date.accessioned.none.fl_str_mv 2019-05-08T15:53:43Z
dc.date.available.none.fl_str_mv 2019-05-08T15:53:43Z
dc.type.spa.fl_str_mv Artículo de revista
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dc.identifier.issn.spa.fl_str_mv 00222461
dc.identifier.uri.spa.fl_str_mv https://hdl.handle.net/11323/3262
dc.identifier.instname.spa.fl_str_mv Corporación Universidad de la Costa
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identifier_str_mv 00222461
Corporación Universidad de la Costa
REDICUC - Repositorio CUC
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https://repositorio.cuc.edu.co/
dc.language.iso.none.fl_str_mv eng
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dc.publisher.spa.fl_str_mv Universidad De La Costa
institution Corporación Universidad de la Costa
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spelling López Pérez, WilliamGonzález García, AlvaroGonzález Hernández, Rafael J.Ramirez Montes, Luz Mery2019-05-08T15:53:43Z2019-05-08T15:53:43Z2016-04-0500222461https://hdl.handle.net/11323/3262Corporación Universidad de la CostaREDICUC - Repositorio CUChttps://repositorio.cuc.edu.co/The structural, electronic, optical, and thermodynamic properties of YxAl1-xN alloys were computed using first-principles calculations. The effects of exchange and correlation have been considered by means of the generalized gradient approximation (GGA) with the Perdew–Burke–Ernzerhof parametrization. In addition, the Tran–Blaha-modified Becke–Johnson potential (TB-mBJ) was applied to give a better description of the band-gap energies and optical spectra. The lattice parameters, bulk modulus, and band-gap energy show nonlinear dependence on concentration x. Results for rock-salt YxAl1-xN alloys show that the band gap undergoes an indirect (Γ→X)-to-direct (Γ→Γ) transition at a given yttrium composition, followed by a direct (Γ→Γ)-to-indirect (Γ→X) transition in a higher yttrium concentration. For wurtzite YxAl1-xN alloys, the band gap presents a direct (Γ→Γ)-to-indirect (→Γ) transition at a given yttrium composition, followed by an indirect (→Γ)-to-indirect (M→Σ) transition in a higher yttrium concentration. The real dielectric function, imaginary dielectric function, refractive index, and extinction coefficient were calculated using the TB-mBJ potential. Using a regular solution model, slightly lower mixing enthalpies for wurtzite YxAl1-xN alloys were found. The mixing enthalpy for a given concentration differs depending on structures, and on the interaction between atoms of constituents. The effect of temperature on the volume, bulk modulus, Debye temperature, and the heat capacity for YxAl1-xN alloys was analyzed using the quasi-harmonic Debye model. Results show that the heat capacity is fairly sensitive to composition as temperature increases.Las propiedades estructurales, electrónicas, ópticas y termodinámicas de las aleaciones YxAl1-xN se calcularon utilizando cálculos de primeros principios. Los efectos del intercambio y la correlación se han considerado mediante la aproximación generalizada del gradiente (GGA) con la parametrización Perdew-Burke-Ernzerhof. Además, se aplicó el potencial de Becke-Johnson modificado por Tran-Blaha (TB-mBJ) para proporcionar una mejor descripción de las energías de banda ancha y los espectros ópticos. Los parámetros de red, el módulo de volumen y la energía de la banda prohibida muestran una dependencia no lineal de la concentración x. Los resultados de las aleaciones YxAl1-xN de sal de roca muestran que la brecha de banda experimenta una transición indirecta (Γ → X) a directa (Γ → Γ) en una composición de itrio determinada, seguida de una directa (Γ → Γ) a Transición indirecta (Γ → X) en una mayor concentración de itrio. Para las aleaciones wurtzite YxAl1-xN, el espacio entre bandas presenta una transición directa (Γ → Γ) a indirecta (→ Γ) en una composición de itrio dada, seguida de una indirecta (→ Γ) a indirecta (M → Σ) Transición en una mayor concentración de itrio. La función dieléctrica real, la función dieléctrica imaginaria, el índice de refracción y el coeficiente de extinción se calcularon utilizando el potencial TB-mBJ. Usando un modelo de solución regular, se encontraron entalpías de mezcla ligeramente más bajas para las aleaciones de wurtzita YxAl1-xN. La entalpía de mezcla para una concentración dada difiere dependiendo de las estructuras y de la interacción entre los átomos de los constituyentes. El efecto de la temperatura en el volumen, el módulo de volumen, la temperatura de Debye y la capacidad de calor de las aleaciones YxAl1-xN se analizó mediante el modelo de Debye cuasi-armónico. Los resultados muestran que la capacidad de calor es bastante sensible a la composición a medida que aumenta la temperatura.López Pérez, William-4357fa0d-5aec-4610-a554-3231f7337f5b-600González García, Alvaro-577111cf-cbe5-4fa5-8fd1-503c4bbf040e-600González Hernández, Rafael J.-47836a79-8a31-4ba4-b27a-d1e0ef4dbcf2-600Ramirez Montes, Luz Mery-9bae5494-21b5-4a6f-a73f-6245f843f738-600engUniversidad De La CostaAttribution-NonCommercial-ShareAlike 4.0 Internationalhttp://creativecommons.org/licenses/by-nc-sa/4.0/info:eu-repo/semantics/openAccesshttp://purl.org/coar/access_right/c_abf2WurtziteDielectric functionBulk modulusWurtzite phaseYttrium concentrationFunción dieléctricaMódulo de volumenFase de WurtziteConcentración de itrioStructural, optoelectronic, and thermodynamic properties of YxAl1-xN semiconducting alloysPropiedades estructurales, optoelectrónicas y termodinámicas de las aleaciones semiconductoras YxAl1-xN.Artículo de revistahttp://purl.org/coar/resource_type/c_6501http://purl.org/coar/resource_type/c_2df8fbb1Textinfo:eu-repo/semantics/articlehttp://purl.org/redcol/resource_type/ARTinfo:eu-repo/semantics/acceptedVersionPublicationORIGINALStructural, optoelectronic, and thermodynamic.pdfStructural, optoelectronic, and thermodynamic.pdfapplication/pdf245118https://repositorio.cuc.edu.co/bitstreams/dcef7f62-f6a4-4248-bd91-9489b3ef89b0/download3f5cc986b900ee01c92182c940b050efMD51CC-LICENSElicense_rdflicense_rdfapplication/rdf+xml; charset=utf-81031https://repositorio.cuc.edu.co/bitstreams/5778bee0-92a5-4661-be60-bdc419edc8fe/download934f4ca17e109e0a05eaeaba504d7ce4MD52LICENSElicense.txtlicense.txttext/plain; charset=utf-81748https://repositorio.cuc.edu.co/bitstreams/4cf371c4-f5fc-4558-b0c0-1bad1adae228/download8a4605be74aa9ea9d79846c1fba20a33MD53THUMBNAILStructural, optoelectronic, and thermodynamic.pdf.jpgStructural, optoelectronic, and thermodynamic.pdf.jpgimage/jpeg51989https://repositorio.cuc.edu.co/bitstreams/716a67db-50c2-408c-8cf8-6a24dccce662/download62afe45e3376637ac2f48e6b85cc5365MD55TEXTStructural, optoelectronic, and thermodynamic.pdf.txtStructural, optoelectronic, and thermodynamic.pdf.txttext/plain2044https://repositorio.cuc.edu.co/bitstreams/5b174a03-4d81-4bb7-9396-5018eb7d5227/downloadb5131f5513a910a47f04e498657ce2deMD5611323/3262oai:repositorio.cuc.edu.co:11323/32622024-09-17 14:19:29.112http://creativecommons.org/licenses/by-nc-sa/4.0/Attribution-NonCommercial-ShareAlike 4.0 Internationalopen.accesshttps://repositorio.cuc.edu.coRepositorio de la Universidad de la Costa CUCrepdigital@cuc.edu.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