Triplet superconductivity in ferromagnets due to magnon exchange

Detalhes bibliográficos
Autor(a) principal: Bulaevskii, Lev
Data de Publicação: 2019
Outros Autores: Eneias, Ronivon, Ferraz Filho, Álvaro
Tipo de documento: Artigo
Idioma: eng
Título da fonte: Repositório Institucional da UFRN
Texto Completo: https://repositorio.ufrn.br/jspui/handle/123456789/28822
https://doi.org/10.1103/PhysRevB.99.064506
Resumo: We consider the superconducting pairing induced by spin-wave exchange in a ferromagnet with both conduction and localized electrons, the latter being described as spins. We use the microscopic Eliashberg theory to describe the pairing of conducting electrons and the random phase approximation approach to treat the localized spins assuming an exchange coupling between the conducting electrons and spins. In the framework of a nonrelativistic Hamiltonian, we found that the spin-wave exchange results in equal spin electron pairing described by the two components of the order parameter, Δ↑ (both spins up) and Δ↓ (both spins down). Due to the conservation of total spin projection on the axis of the spontaneous ferromagnetic moment, the spin-wave exchange at low temperatures includes an emission of magnons and an absorption of thermal magnons by the conduction electrons. The absorption and emission processes depend differently on the temperature, with the absorption being progressively suppressed as the temperature drops. As a result, the superconducting pairing exists only if the electron–spin-wave exchange parameter g exceeds some critical value gc. At g > gc, pairing vanishes if the temperature drops below the lowest point Tcl or increases above the upper critical point Tch ≈ Tm (the Curie temperature) where the spin waves cease to exist. This behavior inherent to the spin-carrying glue is in an obvious disagreement with the results of the conventional BCS approach, which assumes that the effective electron-electron attraction is simply proportional to the static magnetic susceptibility.
id UFRN_12f8e4805d3da348e583b6f7cdf2bc36
oai_identifier_str oai:https://repositorio.ufrn.br:123456789/28822
network_acronym_str UFRN
network_name_str Repositório Institucional da UFRN
repository_id_str
spelling Bulaevskii, LevEneias, RonivonFerraz Filho, Álvaro2020-04-20T19:54:42Z2020-04-20T19:54:42Z2019-02-13BULAEVSKII, Lev; ENEIAS, Ronivon; FERRAZ FILHO, Álvaro. Triplet superconductivity in ferromagnets due to magnon exchange. Physical Review B, [s.l.], v. 99, n. 6, p. 0645061-0645069, 13 fev. 2019. ISSN 2469-9950. DOI https://doi.org/10.1103/PhysRevB.99.064506. Disponível em: https://journals.aps.org/prb/abstract/10.1103/PhysRevB.99.064506. Acesso em: 20 abr. 2020.2469-9950 (print), 2469-9969 (online)https://repositorio.ufrn.br/jspui/handle/123456789/28822https://doi.org/10.1103/PhysRevB.99.064506We consider the superconducting pairing induced by spin-wave exchange in a ferromagnet with both conduction and localized electrons, the latter being described as spins. We use the microscopic Eliashberg theory to describe the pairing of conducting electrons and the random phase approximation approach to treat the localized spins assuming an exchange coupling between the conducting electrons and spins. In the framework of a nonrelativistic Hamiltonian, we found that the spin-wave exchange results in equal spin electron pairing described by the two components of the order parameter, Δ↑ (both spins up) and Δ↓ (both spins down). Due to the conservation of total spin projection on the axis of the spontaneous ferromagnetic moment, the spin-wave exchange at low temperatures includes an emission of magnons and an absorption of thermal magnons by the conduction electrons. The absorption and emission processes depend differently on the temperature, with the absorption being progressively suppressed as the temperature drops. As a result, the superconducting pairing exists only if the electron–spin-wave exchange parameter g exceeds some critical value gc. At g > gc, pairing vanishes if the temperature drops below the lowest point Tcl or increases above the upper critical point Tch ≈ Tm (the Curie temperature) where the spin waves cease to exist. This behavior inherent to the spin-carrying glue is in an obvious disagreement with the results of the conventional BCS approach, which assumes that the effective electron-electron attraction is simply proportional to the static magnetic susceptibility.We consider the superconducting pairing induced by spin-wave exchange in a ferromagnet with both conduction and localized electrons, the latter being described as spins. We use the microscopic Eliashberg theory to describe the pairing of conducting electrons and the random phase approximation approach to treat the localized spins assuming an exchange coupling between the conducting electrons and spins. In the framework of a nonrelativistic Hamiltonian, we found that the spin-wave exchange results in equal spin electron pairing described by the two components of the order parameter, Δ↑ (both spins up) and Δ↓ (both spins down). Due to the conservation of total spin projection on the axis of the spontaneous ferromagnetic moment, the spin-wave exchange at low temperatures includes an emission of magnons and an absorption of thermal magnons by the conduction electrons. The absorption and emission processes depend differently on the temperature, with the absorption being progressively suppressed as the temperature drops. As a result, the superconducting pairing exists only if the electron–spin-wave exchange parameter g exceeds some critical value gc. At g > gc, pairing vanishes if the temperature drops below the lowest point Tcl or increases above the upper critical point Tch ≈ Tm (the Curie temperature) where the spin waves cease to exist. This behavior inherent to the spin-carrying glue is in an obvious disagreement with the results of the conventional BCS approach, which assumes that the effective electron-electron attraction is simply proportional to the static magnetic susceptibility.American Physical SocietySuperconductivityFerromagnetsMagnonTriplet superconductivity in ferromagnets due to magnon exchangeinfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/articleengreponame:Repositório Institucional da UFRNinstname:Universidade Federal do Rio Grande do Norte (UFRN)instacron:UFRNinfo:eu-repo/semantics/openAccessORIGINALTriplet superconductivity in ferromagnets due to magnon exchange_2019.pdfTriplet superconductivity in ferromagnets due to magnon exchange_2019.pdfArtigoapplication/pdf361548https://repositorio.ufrn.br/bitstream/123456789/28822/1/Triplet%20superconductivity%20in%20ferromagnets%20due%20to%20magnon%20exchange_2019.pdffed8e503d86f7d6d34ad797aa36dd8acMD51LICENSElicense.txtlicense.txttext/plain; charset=utf-81484https://repositorio.ufrn.br/bitstream/123456789/28822/2/license.txte9597aa2854d128fd968be5edc8a28d9MD52TEXTTriplet superconductivity in ferromagnets due to magnon exchange_2019.pdf.txtTriplet superconductivity in ferromagnets due to magnon exchange_2019.pdf.txtExtracted texttext/plain44587https://repositorio.ufrn.br/bitstream/123456789/28822/3/Triplet%20superconductivity%20in%20ferromagnets%20due%20to%20magnon%20exchange_2019.pdf.txtacbab2988f2204e5556c959f5a600201MD53THUMBNAILTriplet superconductivity in ferromagnets due to magnon exchange_2019.pdf.jpgTriplet superconductivity in ferromagnets due to magnon exchange_2019.pdf.jpgGenerated Thumbnailimage/jpeg1797https://repositorio.ufrn.br/bitstream/123456789/28822/4/Triplet%20superconductivity%20in%20ferromagnets%20due%20to%20magnon%20exchange_2019.pdf.jpg11eaa40393eac0f3b2e969cdf986f197MD54123456789/288222020-05-05 00:08:15.605oai:https://repositorio.ufrn.br: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Repositório de PublicaçõesPUBhttp://repositorio.ufrn.br/oai/opendoar:2020-05-05T03:08:15Repositório Institucional da UFRN - Universidade Federal do Rio Grande do Norte (UFRN)false
dc.title.pt_BR.fl_str_mv Triplet superconductivity in ferromagnets due to magnon exchange
title Triplet superconductivity in ferromagnets due to magnon exchange
spellingShingle Triplet superconductivity in ferromagnets due to magnon exchange
Bulaevskii, Lev
Superconductivity
Ferromagnets
Magnon
title_short Triplet superconductivity in ferromagnets due to magnon exchange
title_full Triplet superconductivity in ferromagnets due to magnon exchange
title_fullStr Triplet superconductivity in ferromagnets due to magnon exchange
title_full_unstemmed Triplet superconductivity in ferromagnets due to magnon exchange
title_sort Triplet superconductivity in ferromagnets due to magnon exchange
author Bulaevskii, Lev
author_facet Bulaevskii, Lev
Eneias, Ronivon
Ferraz Filho, Álvaro
author_role author
author2 Eneias, Ronivon
Ferraz Filho, Álvaro
author2_role author
author
dc.contributor.author.fl_str_mv Bulaevskii, Lev
Eneias, Ronivon
Ferraz Filho, Álvaro
dc.subject.por.fl_str_mv Superconductivity
Ferromagnets
Magnon
topic Superconductivity
Ferromagnets
Magnon
description We consider the superconducting pairing induced by spin-wave exchange in a ferromagnet with both conduction and localized electrons, the latter being described as spins. We use the microscopic Eliashberg theory to describe the pairing of conducting electrons and the random phase approximation approach to treat the localized spins assuming an exchange coupling between the conducting electrons and spins. In the framework of a nonrelativistic Hamiltonian, we found that the spin-wave exchange results in equal spin electron pairing described by the two components of the order parameter, Δ↑ (both spins up) and Δ↓ (both spins down). Due to the conservation of total spin projection on the axis of the spontaneous ferromagnetic moment, the spin-wave exchange at low temperatures includes an emission of magnons and an absorption of thermal magnons by the conduction electrons. The absorption and emission processes depend differently on the temperature, with the absorption being progressively suppressed as the temperature drops. As a result, the superconducting pairing exists only if the electron–spin-wave exchange parameter g exceeds some critical value gc. At g > gc, pairing vanishes if the temperature drops below the lowest point Tcl or increases above the upper critical point Tch ≈ Tm (the Curie temperature) where the spin waves cease to exist. This behavior inherent to the spin-carrying glue is in an obvious disagreement with the results of the conventional BCS approach, which assumes that the effective electron-electron attraction is simply proportional to the static magnetic susceptibility.
publishDate 2019
dc.date.issued.fl_str_mv 2019-02-13
dc.date.accessioned.fl_str_mv 2020-04-20T19:54:42Z
dc.date.available.fl_str_mv 2020-04-20T19:54:42Z
dc.type.status.fl_str_mv info:eu-repo/semantics/publishedVersion
dc.type.driver.fl_str_mv info:eu-repo/semantics/article
format article
status_str publishedVersion
dc.identifier.citation.fl_str_mv BULAEVSKII, Lev; ENEIAS, Ronivon; FERRAZ FILHO, Álvaro. Triplet superconductivity in ferromagnets due to magnon exchange. Physical Review B, [s.l.], v. 99, n. 6, p. 0645061-0645069, 13 fev. 2019. ISSN 2469-9950. DOI https://doi.org/10.1103/PhysRevB.99.064506. Disponível em: https://journals.aps.org/prb/abstract/10.1103/PhysRevB.99.064506. Acesso em: 20 abr. 2020.
dc.identifier.uri.fl_str_mv https://repositorio.ufrn.br/jspui/handle/123456789/28822
dc.identifier.issn.none.fl_str_mv 2469-9950 (print), 2469-9969 (online)
dc.identifier.doi.none.fl_str_mv https://doi.org/10.1103/PhysRevB.99.064506
identifier_str_mv BULAEVSKII, Lev; ENEIAS, Ronivon; FERRAZ FILHO, Álvaro. Triplet superconductivity in ferromagnets due to magnon exchange. Physical Review B, [s.l.], v. 99, n. 6, p. 0645061-0645069, 13 fev. 2019. ISSN 2469-9950. DOI https://doi.org/10.1103/PhysRevB.99.064506. Disponível em: https://journals.aps.org/prb/abstract/10.1103/PhysRevB.99.064506. Acesso em: 20 abr. 2020.
2469-9950 (print), 2469-9969 (online)
url https://repositorio.ufrn.br/jspui/handle/123456789/28822
https://doi.org/10.1103/PhysRevB.99.064506
dc.language.iso.fl_str_mv eng
language eng
dc.rights.driver.fl_str_mv info:eu-repo/semantics/openAccess
eu_rights_str_mv openAccess
dc.publisher.none.fl_str_mv American Physical Society
publisher.none.fl_str_mv American Physical Society
dc.source.none.fl_str_mv reponame:Repositório Institucional da UFRN
instname:Universidade Federal do Rio Grande do Norte (UFRN)
instacron:UFRN
instname_str Universidade Federal do Rio Grande do Norte (UFRN)
instacron_str UFRN
institution UFRN
reponame_str Repositório Institucional da UFRN
collection Repositório Institucional da UFRN
bitstream.url.fl_str_mv https://repositorio.ufrn.br/bitstream/123456789/28822/1/Triplet%20superconductivity%20in%20ferromagnets%20due%20to%20magnon%20exchange_2019.pdf
https://repositorio.ufrn.br/bitstream/123456789/28822/2/license.txt
https://repositorio.ufrn.br/bitstream/123456789/28822/3/Triplet%20superconductivity%20in%20ferromagnets%20due%20to%20magnon%20exchange_2019.pdf.txt
https://repositorio.ufrn.br/bitstream/123456789/28822/4/Triplet%20superconductivity%20in%20ferromagnets%20due%20to%20magnon%20exchange_2019.pdf.jpg
bitstream.checksum.fl_str_mv fed8e503d86f7d6d34ad797aa36dd8ac
e9597aa2854d128fd968be5edc8a28d9
acbab2988f2204e5556c959f5a600201
11eaa40393eac0f3b2e969cdf986f197
bitstream.checksumAlgorithm.fl_str_mv MD5
MD5
MD5
MD5
repository.name.fl_str_mv Repositório Institucional da UFRN - Universidade Federal do Rio Grande do Norte (UFRN)
repository.mail.fl_str_mv
_version_ 1814832913038966784