Triplet superconductivity in ferromagnets due to magnon exchange
Autor(a) principal: | |
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Data de Publicação: | 2019 |
Outros Autores: | , |
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. |
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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 |
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eng |
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eng |
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openAccess |
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American Physical Society |
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American Physical Society |
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Universidade Federal do Rio Grande do Norte (UFRN) |
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UFRN |
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UFRN |
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Repositório Institucional da UFRN |
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