Mode-crystallography analysis and magnetic structures of SrLnFeRuO6 (Ln = La, Pr, Nd) disordered perovskites
The crystal and magnetic structures of SrLnFeRuO6 (Ln = La, Pr, Nd) double perovskites have been investigated. All compounds crystallize with an orthorhombic Pbnm structure at room temperature. These materials show complete chemical disorder of Fe and Ru cations for all compounds. The distortion of...
| Autores: | , , , |
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| Tipo de recurso: | artículo |
| Fecha de publicación: | 2012 |
| País: | España |
| Institución: | Consejo Superior de Investigaciones Científicas (CSIC) |
| Repositorio: | DIGITAL.CSIC. Repositorio Institucional del CSIC |
| OAI Identifier: | oai:digital.csic.es:10261/73854 |
| Acceso en línea: | http://hdl.handle.net/10261/73854 |
| Access Level: | acceso abierto |
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Mode-crystallography analysis and magnetic structures of SrLnFeRuO6 (Ln = La, Pr, Nd) disordered perovskitesIturbe-Zabalo, E.Fabelo, OscarGateshki, M.Igartua, J. M.The crystal and magnetic structures of SrLnFeRuO6 (Ln = La, Pr, Nd) double perovskites have been investigated. All compounds crystallize with an orthorhombic Pbnm structure at room temperature. These materials show complete chemical disorder of Fe and Ru cations for all compounds. The distortion of the structure, relative to the ideal cubic perovskite, has been decomposed into distortion modes. It has been found that the primary modes of the distortion are octahedral tilting modes: R + 4 and M + 3. The crystal structure of SrPrFeRuO6 has been studied from room temperature up to 1200 K by neutron powder diffraction. There is a structural phase transition from orthorhombic (space group Pbnm) to trigonal (space group ) at T = 1075 K. According to group theory no second-order transition is possible between these symmetries. Magnetic ordering for all the compounds is described by the magnetic propagation vector (0,0,0). SrPrFeRuO6 shows ferrimagnetic order below ca 475 K, while SrLaFeRuO6 (below ca 450 K) and SrNdFeRuO6 (below ca 430 K) exhibit canted-antiferromagnetic order. The magnetic moments at low temperatures are m(Fe/Ru) = 1.88 (3)B for SrLaFeRuO6 (2 K), m(Pr) = 0.46 (4)B and m(Fe/Ru) = 2.24B for SrPrFeRuO6 (2 K), and m(Fe/Ru) = 1.92B for SrNdFeRuO6 (10 K). © 2012 International Union of Crystallography.This work has been supported by ILL (grant MBR-GL/09-056 and MBR-GL/11-050), the Spanish Ministry of Science and Innovation (project MAT2008-05839) and the European Commission under the 7th Framework Program through the ‘Research Infrastructures’ action of the ‘Capacities’ Program, Contract No: CP-CSA_INFRA-2008-1.1.1 Number 226507- NMI3. The authors are grateful to FRMII (exp. 4456), ILL (exp. 5-24-458) and PSI (exp. 20101302) for the beamtime allocation and the instrument local contacts Dr Markus Hoelzel (SPODI, FRMII), Dr Gabriel Cuello (D2B, ILL) and Dr Vladimir Pumjakushin (HRPT, SINQ, PSI) for their kind help and technical assistance.Peer ReviewedInternational Union of Crystallography2013201320122013info:eu-repo/semantics/articlehttp://purl.org/coar/resource_type/c_6501http://hdl.handle.net/10261/73854reponame:DIGITAL.CSIC. Repositorio Institucional del CSICinstname:Consejo Superior de Investigaciones Científicas (CSIC)Inglés#PLACEHOLDER_PARENT_METADATA_VALUE#info:eu-repo/grantAgreement/EC/FP7/226507http://dx.doi.org/10.1107/S0108768112044217info:eu-repo/semantics/openAccessoai:digital.csic.es:10261/738542026-05-22T06:33:51Z |
| dc.title.none.fl_str_mv |
Mode-crystallography analysis and magnetic structures of SrLnFeRuO6 (Ln = La, Pr, Nd) disordered perovskites |
| title |
Mode-crystallography analysis and magnetic structures of SrLnFeRuO6 (Ln = La, Pr, Nd) disordered perovskites |
| spellingShingle |
Mode-crystallography analysis and magnetic structures of SrLnFeRuO6 (Ln = La, Pr, Nd) disordered perovskites Iturbe-Zabalo, E. |
| title_short |
Mode-crystallography analysis and magnetic structures of SrLnFeRuO6 (Ln = La, Pr, Nd) disordered perovskites |
| title_full |
Mode-crystallography analysis and magnetic structures of SrLnFeRuO6 (Ln = La, Pr, Nd) disordered perovskites |
| title_fullStr |
Mode-crystallography analysis and magnetic structures of SrLnFeRuO6 (Ln = La, Pr, Nd) disordered perovskites |
| title_full_unstemmed |
Mode-crystallography analysis and magnetic structures of SrLnFeRuO6 (Ln = La, Pr, Nd) disordered perovskites |
| title_sort |
Mode-crystallography analysis and magnetic structures of SrLnFeRuO6 (Ln = La, Pr, Nd) disordered perovskites |
| dc.creator.none.fl_str_mv |
Iturbe-Zabalo, E. Fabelo, Oscar Gateshki, M. Igartua, J. M. |
| author |
Iturbe-Zabalo, E. |
| author_facet |
Iturbe-Zabalo, E. Fabelo, Oscar Gateshki, M. Igartua, J. M. |
| author_role |
author |
| author2 |
Fabelo, Oscar Gateshki, M. Igartua, J. M. |
| author2_role |
author author author |
| description |
The crystal and magnetic structures of SrLnFeRuO6 (Ln = La, Pr, Nd) double perovskites have been investigated. All compounds crystallize with an orthorhombic Pbnm structure at room temperature. These materials show complete chemical disorder of Fe and Ru cations for all compounds. The distortion of the structure, relative to the ideal cubic perovskite, has been decomposed into distortion modes. It has been found that the primary modes of the distortion are octahedral tilting modes: R + 4 and M + 3. The crystal structure of SrPrFeRuO6 has been studied from room temperature up to 1200 K by neutron powder diffraction. There is a structural phase transition from orthorhombic (space group Pbnm) to trigonal (space group ) at T = 1075 K. According to group theory no second-order transition is possible between these symmetries. Magnetic ordering for all the compounds is described by the magnetic propagation vector (0,0,0). SrPrFeRuO6 shows ferrimagnetic order below ca 475 K, while SrLaFeRuO6 (below ca 450 K) and SrNdFeRuO6 (below ca 430 K) exhibit canted-antiferromagnetic order. The magnetic moments at low temperatures are m(Fe/Ru) = 1.88 (3)B for SrLaFeRuO6 (2 K), m(Pr) = 0.46 (4)B and m(Fe/Ru) = 2.24B for SrPrFeRuO6 (2 K), and m(Fe/Ru) = 1.92B for SrNdFeRuO6 (10 K). © 2012 International Union of Crystallography. |
| publishDate |
2012 |
| dc.date.none.fl_str_mv |
2012 2013 2013 2013 |
| dc.type.none.fl_str_mv |
info:eu-repo/semantics/article http://purl.org/coar/resource_type/c_6501 |
| format |
article |
| dc.identifier.none.fl_str_mv |
http://hdl.handle.net/10261/73854 |
| url |
http://hdl.handle.net/10261/73854 |
| dc.language.none.fl_str_mv |
Inglés |
| language_invalid_str_mv |
Inglés |
| dc.relation.none.fl_str_mv |
#PLACEHOLDER_PARENT_METADATA_VALUE# info:eu-repo/grantAgreement/EC/FP7/226507 http://dx.doi.org/10.1107/S0108768112044217 |
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info:eu-repo/semantics/openAccess |
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openAccess |
| dc.publisher.none.fl_str_mv |
International Union of Crystallography |
| publisher.none.fl_str_mv |
International Union of Crystallography |
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reponame:DIGITAL.CSIC. Repositorio Institucional del CSIC instname:Consejo Superior de Investigaciones Científicas (CSIC) |
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Consejo Superior de Investigaciones Científicas (CSIC) |
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DIGITAL.CSIC. Repositorio Institucional del CSIC |
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DIGITAL.CSIC. Repositorio Institucional del CSIC |
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15,811543 |