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hal.structure.identifierDepartment of Chemistry [Waterloo]
dc.contributor.authorNANDIHALLI, Nagaraj
hal.structure.identifierDepartment of Physics and Astronomy [Clemson]
dc.contributor.authorLAHWAL, Ali
hal.structure.identifierDepartment of Physics and Astronomy [Clemson]
dc.contributor.authorTHOMPSON, Daniel
hal.structure.identifierDepartment of Physics and Astronomy [Clemson]
dc.contributor.authorHOLGATE, Tim C.
hal.structure.identifierDepartment of Physics and Astronomy [Clemson]
dc.contributor.authorTRITT, Terry M.
hal.structure.identifierDépartement des Sciences Appliqués
dc.contributor.authorDASSYLVA-RAYMOND, Véronique
hal.structure.identifierDépartement des Sciences Appliqués
dc.contributor.authorKISS, László I.
hal.structure.identifierCentre de Ressources en Microscopie Electronique et Microanalyse [CREMEN]
dc.contributor.authorSELLIER, Elisabeth
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorGORSSE, Stéphane
hal.structure.identifierDepartment of Chemistry [Waterloo]
dc.contributor.authorKLEINKE, Holger
dc.date.issued2013
dc.identifier.issn0022-4596
dc.description.abstractEnAbout 18 g of Ni0.05Mo3Sb5.4Te1.6 were prepared by heating the elements in the stoichiometric ratio at 1000 K. The product was divided into four parts, and then C60 was added to three of these four parts at 1, 2, and 3 mass%, respectively. Each part was hot-pressed at 150 MPa and 923 K. The sample with 1% C60 was characterized via a Rietveld refinement and TEM analyses. Measurements of the three thermoelectric key properties revealed that the Seebeck coefficient barely depends on the carbon amount added, while both the electrical and the thermal conductivity decrease with increasing amount of carbon. Depending on the amount of C60 used and on the temperature, the thermoelectric performance was either enhanced or decreased, depending on whether the electrical conductivity decreased less or more than the thermal conductivity. At the highest temperature measured, all carbon-containing samples performed better than the unmodified bulk sample, namely up to 14%. These improvements are within the error margin, however.
dc.language.isoen
dc.publisherElsevier
dc.subject.enZintl phases
dc.subject.enThermoelectrics
dc.subject.enComposite
dc.subject.enAntimony
dc.subject.enTellurium
dc.title.enThermoelectric properties of composites made of Ni0.05Mo3Sb5.4Te1.6 and fullerene
dc.typeArticle de revue
dc.identifier.doi10.1016/j.jssc.2013.03.061
dc.subject.halChimie/Matériaux
bordeaux.journalJournal of Solid State Chemistry
bordeaux.page25-30
bordeaux.volume203
bordeaux.peerReviewedoui
hal.identifierhal-00833443
hal.version1
hal.popularnon
hal.audienceInternationale
hal.origin.linkhttps://hal.archives-ouvertes.fr//hal-00833443v1
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