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hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorTENCÉ, Sophie
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorGAUDIN, Etienne
hal.structure.identifierLaboratoire Léon Brillouin [LLB - UMR 12]
dc.contributor.authorANDRÉ, Gilles
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorCHEVALIER, Bernard
dc.date.issued2009
dc.identifier.issn0022-3727
dc.description.abstractEnNeutron powder diffraction experiments have been carried out on the hexagonal ternary silicides Nd<sub>6</sub>Co<sub>1.67</sub>Si<sub>3</sub> and Tb<sub>6</sub>Co<sub>1.67</sub>Si<sub>3</sub> in order to determine their magnetic structures. These compounds exhibit two successive ferromagnetic transitions at <i>T</i><sub>C</sub> = 84 K and <i>T</i><sub>1</sub> = 40 K for Nd<sub>6</sub>Co<sub>1.67</sub>Si<sub>3</sub> and at <i>T</i><sub>C</sub> = 186 K and <i>T</i><sub>1</sub> = 171 K for Tb<sub>6</sub>Co<sub>1.67</sub>Si<sub>3</sub>. Single-crystal x-ray diffraction and specific heat measurements have been realized on Tb<sub>6</sub>Co<sub>1.67</sub>Si<sub>3</sub> in order to complete its characterization. Neutron diffraction investigation at 1.5 K reveals for both compounds a canted ferromagnetic structure with a propagation vector <b><i>k</i></b> = (0 0 0). The Nd moment values are, respectively, equal to μ<sub>1</sub> = 2.06(10)μ<sub>B</sub> and μ<sub>2</sub> = 3.14(9)μ<sub>B</sub> for Nd1 and Nd2 atoms whereas Tb1 and Tb2 atoms carry a magnetic moment of μ<sub>1</sub> = 7.9(2)μ<sub>B</sub> and μ<sub>2</sub> = 8.9(2)μ<sub>B</sub> in Tb<sub>6</sub>Co<sub>1.67</sub>Si<sub>3</sub>. Moreover, a transition from a canted ferromagnet to a pure ferromagnet occurs at <i>T</i><sub>1</sub> = 40 K in Nd<sub>6</sub>Co<sub>1.67</sub>Si<sub>3</sub> while a spin reorientation of the non-collinear ferromagnetic structure occurs at <i>T</i><sub>1</sub> = 171 K for Tb<sub>6</sub>Co<sub>1.67</sub>Si<sub>3</sub>. These magnetic structures are discussed on the basis of the atomic disorder existing for Co atoms in these ternary silicides around the Nd1 and Tb1 atoms.
dc.language.isoen
dc.publisherIOP Publishing
dc.subject.enSpin
dc.subject.enNeutron diffraction
dc.subject.enNonmetallic ferromagnetic materials
dc.subject.enMagnetic phase boundaries
dc.subject.enX-ray diffraction
dc.subject.enMagnetic susceptibilities
dc.title.enMulti-magnetic phases in the ferromagnetic ternary silicides Nd<sub>6</sub>Co<sub>1.67</sub>Si<sub>3</sub> and Tb<sub>6</sub>Co<sub>1.67</sub>Si<sub>3</sub>
dc.typeArticle de revue
dc.identifier.doi10.1088/0022-3727/42/16/165003
dc.subject.halChimie/Matériaux
bordeaux.journalJournal of Physics D: Applied Physics
bordeaux.page165003 (10 p.)
bordeaux.volume42
bordeaux.issue16
bordeaux.peerReviewedoui
hal.identifierhal-00418906
hal.version1
hal.popularnon
hal.audienceInternationale
hal.origin.linkhttps://hal.archives-ouvertes.fr//hal-00418906v1
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