Pressure-induced metal-insulator transition and absence of magnetic order in FeGa3 from a first-principles study

ABSTRACT: The intermetallic compound FeGa3 is a narrow-gap semiconductor with a measured gap between 0.2 and 0.6 eV. The presence of iron d states on the top of the valence band and on the bottom of the conduction band, together with its moderate electronic correlation (U/W ∼ 0.6), have led to the q...

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Autores:
Osorio Guillén, Jorge Mario
Larrauri Pizarro, Yohel D.
Dalpian, Gustavo Martini
Tipo de recurso:
Article of investigation
Fecha de publicación:
2012
Institución:
Universidad de Antioquia
Repositorio:
Repositorio UdeA
Idioma:
eng
OAI Identifier:
oai:bibliotecadigital.udea.edu.co:10495/8635
Acceso en línea:
http://hdl.handle.net/10495/8635
Palabra clave:
Transición metal-aislante
Orden magnético
Estructura electrónica
Teoría Funcional de la Densidad
Rights
openAccess
License
Atribución-NoComercial-SinDerivadas 2.5 Colombia
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network_acronym_str UDEA2
network_name_str Repositorio UdeA
repository_id_str
dc.title.spa.fl_str_mv Pressure-induced metal-insulator transition and absence of magnetic order in FeGa3 from a first-principles study
title Pressure-induced metal-insulator transition and absence of magnetic order in FeGa3 from a first-principles study
spellingShingle Pressure-induced metal-insulator transition and absence of magnetic order in FeGa3 from a first-principles study
Transición metal-aislante
Orden magnético
Estructura electrónica
Teoría Funcional de la Densidad
title_short Pressure-induced metal-insulator transition and absence of magnetic order in FeGa3 from a first-principles study
title_full Pressure-induced metal-insulator transition and absence of magnetic order in FeGa3 from a first-principles study
title_fullStr Pressure-induced metal-insulator transition and absence of magnetic order in FeGa3 from a first-principles study
title_full_unstemmed Pressure-induced metal-insulator transition and absence of magnetic order in FeGa3 from a first-principles study
title_sort Pressure-induced metal-insulator transition and absence of magnetic order in FeGa3 from a first-principles study
dc.creator.fl_str_mv Osorio Guillén, Jorge Mario
Larrauri Pizarro, Yohel D.
Dalpian, Gustavo Martini
dc.contributor.author.none.fl_str_mv Osorio Guillén, Jorge Mario
Larrauri Pizarro, Yohel D.
Dalpian, Gustavo Martini
dc.subject.none.fl_str_mv Transición metal-aislante
Orden magnético
Estructura electrónica
Teoría Funcional de la Densidad
topic Transición metal-aislante
Orden magnético
Estructura electrónica
Teoría Funcional de la Densidad
description ABSTRACT: The intermetallic compound FeGa3 is a narrow-gap semiconductor with a measured gap between 0.2 and 0.6 eV. The presence of iron d states on the top of the valence band and on the bottom of the conduction band, together with its moderate electronic correlation (U/W ∼ 0.6), have led to the question of whether there is magnetic order in this compound. We have examined the possible presence of magnetism in FeGa3 as well as its electronic structure at high pressures, using the density functional theory (DFT) + U method with the intermediated double-counting scheme. We have found that for an optimized value of the Yukawa screening length λ, there is no magnetic moment on the iron ions (μ = 0), implying that FeGa3 is nonmagnetic. We have also found that around a pressure of 25 GPa a metal-insulator transition takes place.
publishDate 2012
dc.date.issued.none.fl_str_mv 2012
dc.date.accessioned.none.fl_str_mv 2017-10-24T16:13:38Z
dc.date.available.none.fl_str_mv 2017-10-24T16:13:38Z
dc.type.spa.fl_str_mv info:eu-repo/semantics/article
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dc.type.local.spa.fl_str_mv Artículo de investigación
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dc.identifier.citation.spa.fl_str_mv Osorio Guillén, J. M., Larrauri Pizarro, Y. D., & Dalpian, G. M. (2012). Pressure-induced metal-insulator transition and absence of magnetic order in FeGa3 from a first-principles study. Physical Review B: Condensed Matter. 86(235202), 1-6.
dc.identifier.issn.none.fl_str_mv 0163-1829
dc.identifier.uri.none.fl_str_mv http://hdl.handle.net/10495/8635
dc.identifier.doi.none.fl_str_mv 10.1103/PhysRevB.90.035213
dc.identifier.eissn.none.fl_str_mv 2469-9969
identifier_str_mv Osorio Guillén, J. M., Larrauri Pizarro, Y. D., & Dalpian, G. M. (2012). Pressure-induced metal-insulator transition and absence of magnetic order in FeGa3 from a first-principles study. Physical Review B: Condensed Matter. 86(235202), 1-6.
0163-1829
10.1103/PhysRevB.90.035213
2469-9969
url http://hdl.handle.net/10495/8635
dc.language.iso.spa.fl_str_mv eng
language eng
dc.relation.ispartofjournalabbrev.spa.fl_str_mv Phys Rev B
dc.rights.*.fl_str_mv Atribución-NoComercial-SinDerivadas 2.5 Colombia
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eu_rights_str_mv openAccess
dc.format.mimetype.spa.fl_str_mv application/pdf
dc.publisher.spa.fl_str_mv The American Physical Society
dc.publisher.group.spa.fl_str_mv Ciencia de los Materiales
institution Universidad de Antioquia
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spelling Osorio Guillén, Jorge MarioLarrauri Pizarro, Yohel D.Dalpian, Gustavo Martini2017-10-24T16:13:38Z2017-10-24T16:13:38Z2012Osorio Guillén, J. M., Larrauri Pizarro, Y. D., & Dalpian, G. M. (2012). Pressure-induced metal-insulator transition and absence of magnetic order in FeGa3 from a first-principles study. Physical Review B: Condensed Matter. 86(235202), 1-6.0163-1829http://hdl.handle.net/10495/863510.1103/PhysRevB.90.0352132469-9969ABSTRACT: The intermetallic compound FeGa3 is a narrow-gap semiconductor with a measured gap between 0.2 and 0.6 eV. The presence of iron d states on the top of the valence band and on the bottom of the conduction band, together with its moderate electronic correlation (U/W ∼ 0.6), have led to the question of whether there is magnetic order in this compound. We have examined the possible presence of magnetism in FeGa3 as well as its electronic structure at high pressures, using the density functional theory (DFT) + U method with the intermediated double-counting scheme. We have found that for an optimized value of the Yukawa screening length λ, there is no magnetic moment on the iron ions (μ = 0), implying that FeGa3 is nonmagnetic. We have also found that around a pressure of 25 GPa a metal-insulator transition takes place.application/pdfengThe American Physical SocietyCiencia de los Materialesinfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/articlehttp://purl.org/coar/resource_type/c_2df8fbb1https://purl.org/redcol/resource_type/ARTArtículo de investigaciónhttp://purl.org/coar/version/c_970fb48d4fbd8a85Atribución-NoComercial-SinDerivadas 2.5 Colombiainfo:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by-nc-nd/2.5/co/http://purl.org/coar/access_right/c_abf2https://creativecommons.org/licenses/by-nc-nd/4.0/Transición metal-aislanteOrden magnéticoEstructura electrónicaTeoría Funcional de la DensidadPressure-induced metal-insulator transition and absence of magnetic order in FeGa3 from a first-principles studyPhys Rev BPhysical Review B: Condensed Matter1686235202CC-LICENSElicense_urllicense_urlArtículo de investigacióntext/plain; charset=utf-849http://bibliotecadigital.udea.edu.co/bitstream/10495/8635/2/license_url4afdbb8c545fd630ea7db775da747b2fMD52license_textlicense_texttext/html; charset=utf-80http://bibliotecadigital.udea.edu.co/bitstream/10495/8635/3/license_textd41d8cd98f00b204e9800998ecf8427eMD53license_rdflicense_rdfapplication/rdf+xml; charset=utf-80http://bibliotecadigital.udea.edu.co/bitstream/10495/8635/4/license_rdfd41d8cd98f00b204e9800998ecf8427eMD54LICENSElicense.txtlicense.txttext/plain; charset=utf-81748http://bibliotecadigital.udea.edu.co/bitstream/10495/8635/5/license.txt8a4605be74aa9ea9d79846c1fba20a33MD55ORIGINALOsorioJorge_2012_PressureInducedMetal.pdfOsorioJorge_2012_PressureInducedMetal.pdfArtículo de investigaciónapplication/pdf1967542http://bibliotecadigital.udea.edu.co/bitstream/10495/8635/1/OsorioJorge_2012_PressureInducedMetal.pdfa9da873426ab2a7968e4837f238db58cMD5110495/8635oai:bibliotecadigital.udea.edu.co:10495/86352021-05-16 11:45:03.388Repositorio Institucional Universidad de Antioquiaandres.perez@udea.edu.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