High Magnetic Field Lattice Length Changes in URu2Si2

Autores
Correa, Víctor Félix; Francoual, S.; Jaime, M.; Harrison, N.; Murphy, T. P.; Palm, E. C.; Tozer, S. W.; Lacerda, A. H.; Sharma, P. A.; Mydosh, J. A.
Año de publicación
2012
Idioma
inglés
Tipo de recurso
artículo
Estado
versión publicada
Descripción
We report high-magnetic-field (up to 45 T)  c-axis thermal-expansion and magnetostriction experiments on URu2Si2 single crystals. The sample length change DeltaLc/Lc associated with the transition to the ??hidden order?? phase becomes increasingly discontinuous as the magnetic field is raised above 25 T. The reentrant ordered phase III is clearly observed in both the thermal expansion and magnetostriction above 36 T, in good agreement with previous results. The sample length is also discontinuous at the boundaries of this phase, mainly at the upper boundary. A change in the sign of the coefficient of thermal expansion  is observed at the metamagnetic transition (BM = 38 T), which is likely related to the existence of a quantum critical end point.
Fil: Correa, Víctor Félix. Comisión Nacional de Energía Atómica. Gerencia del Área de Energía Nuclear. Instituto Balseiro. Archivo Histórico del Centro Atómico Bariloche e Instituto Balseiro | Universidad Nacional de Cuyo. Instituto Balseiro. Archivo Histórico del Centro Atómico Bariloche e Instituto Balseiro; Argentina. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Patagonia Norte; Argentina
Fil: Francoual, S.. Los Alamos National High Magnetic Field Laboratory; Estados Unidos
Fil: Jaime, M.. Los Alamos National High Magnetic Field Laboratory; Estados Unidos
Fil: Harrison, N.. Los Alamos National High Magnetic Field Laboratory; Estados Unidos
Fil: Murphy, T. P.. National High Magnetic Field Laboratory; Estados Unidos
Fil: Palm, E. C.. National High Magnetic Field Laboratory; Estados Unidos
Fil: Tozer, S. W.. National High Magnetic Field Laboratory; Estados Unidos
Fil: Lacerda, A. H.. Los Alamos National High Magnetic Field Laboratory; Estados Unidos
Fil: Sharma, P. A.. Los Alamos National High Magnetic Field Laboratory; Estados Unidos
Fil: Mydosh, J. A.. Leiden University; Países Bajos
Materia
strongly correlated electron systems
magnetostriction
Nivel de accesibilidad
acceso abierto
Condiciones de uso
https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
Repositorio
CONICET Digital (CONICET)
Institución
Consejo Nacional de Investigaciones Científicas y Técnicas
OAI Identificador
oai:ri.conicet.gov.ar:11336/198948
Acceder
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oai_identifier_str oai:ri.conicet.gov.ar:11336/198948
network_acronym_str CONICETDig
repository_id_str 3498
network_name_str CONICET Digital (CONICET)
spelling High Magnetic Field Lattice Length Changes in URu2Si2Correa, Víctor FélixFrancoual, S.Jaime, M.Harrison, N.Murphy, T. P.Palm, E. C.Tozer, S. W.Lacerda, A. H.Sharma, P. A.Mydosh, J. A.strongly correlated electron systemsmagnetostrictionhttps://purl.org/becyt/ford/1.3https://purl.org/becyt/ford/1We report high-magnetic-field (up to 45 T)  c-axis thermal-expansion and magnetostriction experiments on URu2Si2 single crystals. The sample length change DeltaLc/Lc associated with the transition to the ??hidden order?? phase becomes increasingly discontinuous as the magnetic field is raised above 25 T. The reentrant ordered phase III is clearly observed in both the thermal expansion and magnetostriction above 36 T, in good agreement with previous results. The sample length is also discontinuous at the boundaries of this phase, mainly at the upper boundary. A change in the sign of the coefficient of thermal expansion  is observed at the metamagnetic transition (BM = 38 T), which is likely related to the existence of a quantum critical end point.Fil: Correa, Víctor Félix. Comisión Nacional de Energía Atómica. Gerencia del Área de Energía Nuclear. Instituto Balseiro. Archivo Histórico del Centro Atómico Bariloche e Instituto Balseiro | Universidad Nacional de Cuyo. Instituto Balseiro. Archivo Histórico del Centro Atómico Bariloche e Instituto Balseiro; Argentina. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Patagonia Norte; ArgentinaFil: Francoual, S.. Los Alamos National High Magnetic Field Laboratory; Estados UnidosFil: Jaime, M.. Los Alamos National High Magnetic Field Laboratory; Estados UnidosFil: Harrison, N.. Los Alamos National High Magnetic Field Laboratory; Estados UnidosFil: Murphy, T. P.. National High Magnetic Field Laboratory; Estados UnidosFil: Palm, E. C.. National High Magnetic Field Laboratory; Estados UnidosFil: Tozer, S. W.. National High Magnetic Field Laboratory; Estados UnidosFil: Lacerda, A. H.. Los Alamos National High Magnetic Field Laboratory; Estados UnidosFil: Sharma, P. A.. Los Alamos National High Magnetic Field Laboratory; Estados UnidosFil: Mydosh, J. A.. Leiden University; Países BajosAmerican Physical Society2012-12info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfapplication/pdfhttp://hdl.handle.net/11336/198948Correa, Víctor Félix; Francoual, S.; Jaime, M.; Harrison, N.; Murphy, T. P.; et al.; High Magnetic Field Lattice Length Changes in URu2Si2; American Physical Society; Physical Review Letters; 109; 24; 12-2012; 2464051-24640550031-9007CONICET DigitalCONICETenginfo:eu-repo/semantics/altIdentifier/url/http://link.aps.org/doi/10.1103/PhysRevLett.109.246405info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevLett.109.246405info:eu-repo/semantics/openAccesshttps://creativecommons.org/licenses/by-nc-sa/2.5/ar/reponame:CONICET Digital (CONICET)instname:Consejo Nacional de Investigaciones Científicas y Técnicas2025-09-29T09:50:42Zoai:ri.conicet.gov.ar:11336/198948instacron:CONICETInstitucionalhttp://ri.conicet.gov.ar/Organismo científico-tecnológicoNo correspondehttp://ri.conicet.gov.ar/oai/requestdasensio@conicet.gov.ar; lcarlino@conicet.gov.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:34982025-09-29 09:50:42.55CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicasfalse
dc.title.none.fl_str_mv High Magnetic Field Lattice Length Changes in URu2Si2
title High Magnetic Field Lattice Length Changes in URu2Si2
spellingShingle High Magnetic Field Lattice Length Changes in URu2Si2
Correa, Víctor Félix
strongly correlated electron systems
magnetostriction
title_short High Magnetic Field Lattice Length Changes in URu2Si2
title_full High Magnetic Field Lattice Length Changes in URu2Si2
title_fullStr High Magnetic Field Lattice Length Changes in URu2Si2
title_full_unstemmed High Magnetic Field Lattice Length Changes in URu2Si2
title_sort High Magnetic Field Lattice Length Changes in URu2Si2
dc.creator.none.fl_str_mv Correa, Víctor Félix
Francoual, S.
Jaime, M.
Harrison, N.
Murphy, T. P.
Palm, E. C.
Tozer, S. W.
Lacerda, A. H.
Sharma, P. A.
Mydosh, J. A.
author Correa, Víctor Félix
author_facet Correa, Víctor Félix
Francoual, S.
Jaime, M.
Harrison, N.
Murphy, T. P.
Palm, E. C.
Tozer, S. W.
Lacerda, A. H.
Sharma, P. A.
Mydosh, J. A.
author_role author
author2 Francoual, S.
Jaime, M.
Harrison, N.
Murphy, T. P.
Palm, E. C.
Tozer, S. W.
Lacerda, A. H.
Sharma, P. A.
Mydosh, J. A.
author2_role author
author
author
author
author
author
author
author
author
dc.subject.none.fl_str_mv strongly correlated electron systems
magnetostriction
topic strongly correlated electron systems
magnetostriction
purl_subject.fl_str_mv https://purl.org/becyt/ford/1.3
https://purl.org/becyt/ford/1
dc.description.none.fl_txt_mv We report high-magnetic-field (up to 45 T)  c-axis thermal-expansion and magnetostriction experiments on URu2Si2 single crystals. The sample length change DeltaLc/Lc associated with the transition to the ??hidden order?? phase becomes increasingly discontinuous as the magnetic field is raised above 25 T. The reentrant ordered phase III is clearly observed in both the thermal expansion and magnetostriction above 36 T, in good agreement with previous results. The sample length is also discontinuous at the boundaries of this phase, mainly at the upper boundary. A change in the sign of the coefficient of thermal expansion  is observed at the metamagnetic transition (BM = 38 T), which is likely related to the existence of a quantum critical end point.
Fil: Correa, Víctor Félix. Comisión Nacional de Energía Atómica. Gerencia del Área de Energía Nuclear. Instituto Balseiro. Archivo Histórico del Centro Atómico Bariloche e Instituto Balseiro | Universidad Nacional de Cuyo. Instituto Balseiro. Archivo Histórico del Centro Atómico Bariloche e Instituto Balseiro; Argentina. Consejo Nacional de Investigaciones Científicas y Técnicas. Centro Científico Tecnológico Conicet - Patagonia Norte; Argentina
Fil: Francoual, S.. Los Alamos National High Magnetic Field Laboratory; Estados Unidos
Fil: Jaime, M.. Los Alamos National High Magnetic Field Laboratory; Estados Unidos
Fil: Harrison, N.. Los Alamos National High Magnetic Field Laboratory; Estados Unidos
Fil: Murphy, T. P.. National High Magnetic Field Laboratory; Estados Unidos
Fil: Palm, E. C.. National High Magnetic Field Laboratory; Estados Unidos
Fil: Tozer, S. W.. National High Magnetic Field Laboratory; Estados Unidos
Fil: Lacerda, A. H.. Los Alamos National High Magnetic Field Laboratory; Estados Unidos
Fil: Sharma, P. A.. Los Alamos National High Magnetic Field Laboratory; Estados Unidos
Fil: Mydosh, J. A.. Leiden University; Países Bajos
description We report high-magnetic-field (up to 45 T)  c-axis thermal-expansion and magnetostriction experiments on URu2Si2 single crystals. The sample length change DeltaLc/Lc associated with the transition to the ??hidden order?? phase becomes increasingly discontinuous as the magnetic field is raised above 25 T. The reentrant ordered phase III is clearly observed in both the thermal expansion and magnetostriction above 36 T, in good agreement with previous results. The sample length is also discontinuous at the boundaries of this phase, mainly at the upper boundary. A change in the sign of the coefficient of thermal expansion  is observed at the metamagnetic transition (BM = 38 T), which is likely related to the existence of a quantum critical end point.
publishDate 2012
dc.date.none.fl_str_mv 2012-12
dc.type.none.fl_str_mv info:eu-repo/semantics/article
info:eu-repo/semantics/publishedVersion
http://purl.org/coar/resource_type/c_6501
info:ar-repo/semantics/articulo
format article
status_str publishedVersion
dc.identifier.none.fl_str_mv http://hdl.handle.net/11336/198948
Correa, Víctor Félix; Francoual, S.; Jaime, M.; Harrison, N.; Murphy, T. P.; et al.; High Magnetic Field Lattice Length Changes in URu2Si2; American Physical Society; Physical Review Letters; 109; 24; 12-2012; 2464051-2464055
0031-9007
CONICET Digital
CONICET
url http://hdl.handle.net/11336/198948
identifier_str_mv Correa, Víctor Félix; Francoual, S.; Jaime, M.; Harrison, N.; Murphy, T. P.; et al.; High Magnetic Field Lattice Length Changes in URu2Si2; American Physical Society; Physical Review Letters; 109; 24; 12-2012; 2464051-2464055
0031-9007
CONICET Digital
CONICET
dc.language.none.fl_str_mv eng
language eng
dc.relation.none.fl_str_mv info:eu-repo/semantics/altIdentifier/url/http://link.aps.org/doi/10.1103/PhysRevLett.109.246405
info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevLett.109.246405
dc.rights.none.fl_str_mv info:eu-repo/semantics/openAccess
https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
eu_rights_str_mv openAccess
rights_invalid_str_mv https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
dc.format.none.fl_str_mv application/pdf
application/pdf
dc.publisher.none.fl_str_mv American Physical Society
publisher.none.fl_str_mv American Physical Society
dc.source.none.fl_str_mv reponame:CONICET Digital (CONICET)
instname:Consejo Nacional de Investigaciones Científicas y Técnicas
reponame_str CONICET Digital (CONICET)
collection CONICET Digital (CONICET)
instname_str Consejo Nacional de Investigaciones Científicas y Técnicas
repository.name.fl_str_mv CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicas
repository.mail.fl_str_mv dasensio@conicet.gov.ar; lcarlino@conicet.gov.ar
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score 13.069144

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