Searching for a Quantum Critical Point in Rh doped ferromagnetic Ce2.15Pd1.95In0.9
- Autores
- Sereni, Julian Gustavo Renzo; Giovannini, M.; Gomez Berisso, Mariano; Saccone, A.
- Año de publicación
- 2012
- Idioma
- inglés
- Tipo de recurso
- artículo
- Estado
- versión publicada
- Descripción
- Low temperature magnetic and thermal ( C m ) properties of the ferromagnetic (FM) alloys Ce 2.15 (Pd 1− x Rh x ) 1.95 In 0.9 were investigated in order to explore the possibility for tuning towards a quantum critical point (QCP) by doping Pd with Rh. As expected, the magnetic transition decreases from T = 4.1K at x = 0 with increasing Rh concentration. However, the phase boundary splits into two transitions, the upper being antiferromagnetic (AF) whereas the lower FM. The AF phase boundary extrapolates to T N = 0 for x cr ≈ 0.65 whereas the first order FM transition vanishes at x ≈ 0.3. The quantum critical character of the T N → 0 point is inferred from the divergent T dependence of the tail of C m /T observed in the x = 0.5 and 0.55 alloys, and the tendency to saturation of the maximum of C m ( T N )/ T currently observed in exemplary Ce compounds when T N → 0. Beyond the critical concentration the unit cell volume deviates from the Vegard´s law in coincidence with a strong increase of the Kondo temperature.
Fil: Sereni, Julian Gustavo Renzo. Consejo Nacional de Investigaciones Científicas y Técnicas; Argentina. Comisión Nacional de Energía Atómica. Gerencia del Area de Investigación y Aplicaciones No Nucleares. Gerencia de Física (Centro Atómico Bariloche). División Bajas Temperaturas; Argentina
Fil: Giovannini, M.. Università di Genova; Italia
Fil: Gomez Berisso, Mariano. Consejo Nacional de Investigaciones Científicas y Técnicas; Argentina. Comisión Nacional de Energía Atómica. Gerencia del Area de Investigación y Aplicaciones No Nucleares. Gerencia de Física (Centro Atómico Bariloche). División Bajas Temperaturas; Argentina
Fil: Saccone, A.. Università di Genova; Italia - Materia
-
Critical-Point Effects
Magnetic Phase Boundaries
Antiferromagnetics
Ferromagnetic Metals And Alloys
Specific Heats
Short-Range Order - Nivel de accesibilidad
- acceso abierto
- Condiciones de uso
- https://creativecommons.org/licenses/by-nc-sa/2.5/ar/
- Repositorio
- Institución
- Consejo Nacional de Investigaciones Científicas y Técnicas
- OAI Identificador
- oai:ri.conicet.gov.ar:11336/11215
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Searching for a Quantum Critical Point in Rh doped ferromagnetic Ce2.15Pd1.95In0.9Sereni, Julian Gustavo RenzoGiovannini, M.Gomez Berisso, MarianoSaccone, A.Critical-Point EffectsMagnetic Phase BoundariesAntiferromagneticsFerromagnetic Metals And AlloysSpecific HeatsShort-Range Orderhttps://purl.org/becyt/ford/1.3https://purl.org/becyt/ford/1Low temperature magnetic and thermal ( C m ) properties of the ferromagnetic (FM) alloys Ce 2.15 (Pd 1− x Rh x ) 1.95 In 0.9 were investigated in order to explore the possibility for tuning towards a quantum critical point (QCP) by doping Pd with Rh. As expected, the magnetic transition decreases from T = 4.1K at x = 0 with increasing Rh concentration. However, the phase boundary splits into two transitions, the upper being antiferromagnetic (AF) whereas the lower FM. The AF phase boundary extrapolates to T N = 0 for x cr ≈ 0.65 whereas the first order FM transition vanishes at x ≈ 0.3. The quantum critical character of the T N → 0 point is inferred from the divergent T dependence of the tail of C m /T observed in the x = 0.5 and 0.55 alloys, and the tendency to saturation of the maximum of C m ( T N )/ T currently observed in exemplary Ce compounds when T N → 0. Beyond the critical concentration the unit cell volume deviates from the Vegard´s law in coincidence with a strong increase of the Kondo temperature.Fil: Sereni, Julian Gustavo Renzo. Consejo Nacional de Investigaciones Científicas y Técnicas; Argentina. Comisión Nacional de Energía Atómica. Gerencia del Area de Investigación y Aplicaciones No Nucleares. Gerencia de Física (Centro Atómico Bariloche). División Bajas Temperaturas; ArgentinaFil: Giovannini, M.. Università di Genova; ItaliaFil: Gomez Berisso, Mariano. Consejo Nacional de Investigaciones Científicas y Técnicas; Argentina. Comisión Nacional de Energía Atómica. Gerencia del Area de Investigación y Aplicaciones No Nucleares. Gerencia de Física (Centro Atómico Bariloche). División Bajas Temperaturas; ArgentinaFil: Saccone, A.. Università di Genova; ItaliaIOP Publishing2012-01info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfapplication/pdfhttp://hdl.handle.net/11336/11215Sereni, Julian Gustavo Renzo; Giovannini, M.; Gomez Berisso, Mariano; Saccone, A.; Searching for a Quantum Critical Point in Rh doped ferromagnetic Ce2.15Pd1.95In0.9; IOP Publishing; Journal of Physics: Conference Series; 391; 1; 1-2012; 12062-120661742-6596enginfo:eu-repo/semantics/altIdentifier/url/http://iopscience.iop.org/1742-6596/391/1/012062/info:eu-repo/semantics/altIdentifier/doi/10.1088/1742-6596/391/1/012062info:eu-repo/semantics/openAccesshttps://creativecommons.org/licenses/by-nc-sa/2.5/ar/reponame:CONICET Digital (CONICET)instname:Consejo Nacional de Investigaciones Científicas y Técnicas2025-10-15T15:01:09Zoai:ri.conicet.gov.ar:11336/11215instacron: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:34982025-10-15 15:01:10.172CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicasfalse |
dc.title.none.fl_str_mv |
Searching for a Quantum Critical Point in Rh doped ferromagnetic Ce2.15Pd1.95In0.9 |
title |
Searching for a Quantum Critical Point in Rh doped ferromagnetic Ce2.15Pd1.95In0.9 |
spellingShingle |
Searching for a Quantum Critical Point in Rh doped ferromagnetic Ce2.15Pd1.95In0.9 Sereni, Julian Gustavo Renzo Critical-Point Effects Magnetic Phase Boundaries Antiferromagnetics Ferromagnetic Metals And Alloys Specific Heats Short-Range Order |
title_short |
Searching for a Quantum Critical Point in Rh doped ferromagnetic Ce2.15Pd1.95In0.9 |
title_full |
Searching for a Quantum Critical Point in Rh doped ferromagnetic Ce2.15Pd1.95In0.9 |
title_fullStr |
Searching for a Quantum Critical Point in Rh doped ferromagnetic Ce2.15Pd1.95In0.9 |
title_full_unstemmed |
Searching for a Quantum Critical Point in Rh doped ferromagnetic Ce2.15Pd1.95In0.9 |
title_sort |
Searching for a Quantum Critical Point in Rh doped ferromagnetic Ce2.15Pd1.95In0.9 |
dc.creator.none.fl_str_mv |
Sereni, Julian Gustavo Renzo Giovannini, M. Gomez Berisso, Mariano Saccone, A. |
author |
Sereni, Julian Gustavo Renzo |
author_facet |
Sereni, Julian Gustavo Renzo Giovannini, M. Gomez Berisso, Mariano Saccone, A. |
author_role |
author |
author2 |
Giovannini, M. Gomez Berisso, Mariano Saccone, A. |
author2_role |
author author author |
dc.subject.none.fl_str_mv |
Critical-Point Effects Magnetic Phase Boundaries Antiferromagnetics Ferromagnetic Metals And Alloys Specific Heats Short-Range Order |
topic |
Critical-Point Effects Magnetic Phase Boundaries Antiferromagnetics Ferromagnetic Metals And Alloys Specific Heats Short-Range Order |
purl_subject.fl_str_mv |
https://purl.org/becyt/ford/1.3 https://purl.org/becyt/ford/1 |
dc.description.none.fl_txt_mv |
Low temperature magnetic and thermal ( C m ) properties of the ferromagnetic (FM) alloys Ce 2.15 (Pd 1− x Rh x ) 1.95 In 0.9 were investigated in order to explore the possibility for tuning towards a quantum critical point (QCP) by doping Pd with Rh. As expected, the magnetic transition decreases from T = 4.1K at x = 0 with increasing Rh concentration. However, the phase boundary splits into two transitions, the upper being antiferromagnetic (AF) whereas the lower FM. The AF phase boundary extrapolates to T N = 0 for x cr ≈ 0.65 whereas the first order FM transition vanishes at x ≈ 0.3. The quantum critical character of the T N → 0 point is inferred from the divergent T dependence of the tail of C m /T observed in the x = 0.5 and 0.55 alloys, and the tendency to saturation of the maximum of C m ( T N )/ T currently observed in exemplary Ce compounds when T N → 0. Beyond the critical concentration the unit cell volume deviates from the Vegard´s law in coincidence with a strong increase of the Kondo temperature. Fil: Sereni, Julian Gustavo Renzo. Consejo Nacional de Investigaciones Científicas y Técnicas; Argentina. Comisión Nacional de Energía Atómica. Gerencia del Area de Investigación y Aplicaciones No Nucleares. Gerencia de Física (Centro Atómico Bariloche). División Bajas Temperaturas; Argentina Fil: Giovannini, M.. Università di Genova; Italia Fil: Gomez Berisso, Mariano. Consejo Nacional de Investigaciones Científicas y Técnicas; Argentina. Comisión Nacional de Energía Atómica. Gerencia del Area de Investigación y Aplicaciones No Nucleares. Gerencia de Física (Centro Atómico Bariloche). División Bajas Temperaturas; Argentina Fil: Saccone, A.. Università di Genova; Italia |
description |
Low temperature magnetic and thermal ( C m ) properties of the ferromagnetic (FM) alloys Ce 2.15 (Pd 1− x Rh x ) 1.95 In 0.9 were investigated in order to explore the possibility for tuning towards a quantum critical point (QCP) by doping Pd with Rh. As expected, the magnetic transition decreases from T = 4.1K at x = 0 with increasing Rh concentration. However, the phase boundary splits into two transitions, the upper being antiferromagnetic (AF) whereas the lower FM. The AF phase boundary extrapolates to T N = 0 for x cr ≈ 0.65 whereas the first order FM transition vanishes at x ≈ 0.3. The quantum critical character of the T N → 0 point is inferred from the divergent T dependence of the tail of C m /T observed in the x = 0.5 and 0.55 alloys, and the tendency to saturation of the maximum of C m ( T N )/ T currently observed in exemplary Ce compounds when T N → 0. Beyond the critical concentration the unit cell volume deviates from the Vegard´s law in coincidence with a strong increase of the Kondo temperature. |
publishDate |
2012 |
dc.date.none.fl_str_mv |
2012-01 |
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/11336/11215 Sereni, Julian Gustavo Renzo; Giovannini, M.; Gomez Berisso, Mariano; Saccone, A.; Searching for a Quantum Critical Point in Rh doped ferromagnetic Ce2.15Pd1.95In0.9; IOP Publishing; Journal of Physics: Conference Series; 391; 1; 1-2012; 12062-12066 1742-6596 |
url |
http://hdl.handle.net/11336/11215 |
identifier_str_mv |
Sereni, Julian Gustavo Renzo; Giovannini, M.; Gomez Berisso, Mariano; Saccone, A.; Searching for a Quantum Critical Point in Rh doped ferromagnetic Ce2.15Pd1.95In0.9; IOP Publishing; Journal of Physics: Conference Series; 391; 1; 1-2012; 12062-12066 1742-6596 |
dc.language.none.fl_str_mv |
eng |
language |
eng |
dc.relation.none.fl_str_mv |
info:eu-repo/semantics/altIdentifier/url/http://iopscience.iop.org/1742-6596/391/1/012062/ info:eu-repo/semantics/altIdentifier/doi/10.1088/1742-6596/391/1/012062 |
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 |
IOP Publishing |
publisher.none.fl_str_mv |
IOP Publishing |
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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1846083151589277696 |
score |
13.22299 |