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hal.structure.identifierInstitut für Anorganische und Analytische Chemie
dc.contributor.authorHERMES, Wilfried
hal.structure.identifierInstitut für Anorganische und Analytische Chemie
dc.contributor.authorRODEWALD, Ute Ch.
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorCHEVALIER, Bernard
hal.structure.identifierInstitut de Chimie de la Matière Condensée de Bordeaux [ICMCB]
dc.contributor.authorMATAR, Samir F.
hal.structure.identifierInstitut für Physik
dc.contributor.authorEYERT, Volker
hal.structure.identifierAnorganische Chemie
dc.contributor.authorPÖTTGEN, Rainer
dc.date.issued2010
dc.identifier.issn1293-2558
dc.description.abstractEnThe plumbide CeZnPb was synthesized from the elements in a sealed tantalum ampoule. Its YPtAs-type structure was refined on the basis of single-crystal X-ray diffraction data: <i>P</i>6<sub>3</sub>/<i>mmc</i>, <i>a</i> = 463.7(2) and <i>c</i> = 1669.6(6) pm, w<i>R</i>2 = 0.1161, 189 <i>F</i><sup>2</sup> values, and 12 variables. CeZnPb crystallizes with a superstructure of AlB<sub>2</sub>. The zinc and lead atoms form puckered [Zn<sub>3</sub>Pb<sub>3</sub>] hexagons, which are stacked in a sequence <i>ABB</i>′<i>A</i>′. The Zn–Pb distances within the layers are 278 pm. The shortest interlayer distance occurs between the zinc atoms of adjacent layers (305 pm). Susceptibility measurements of CeZnPb show Curie–Weiss behavior with an experimental magnetic moment of 2.47(1) <i>μ</i><sub>B</sub>/mol CeZnPb. CeZnPb shows two antiferromagnetic transitions at <i>T</i><sub>N1</sub> = 3.8 K and <i>T</i><sub>N2</sub> = 2.6 K. Magnetization measurements at 2 K show two metamagnetic transitions at critical fields of approximately 1.1 and 7.0 kOe, underlining the antiparallel spin alignment at zero field. The electronic and magnetic structure is discussed based on scalar relativistic computations using the augmented spherical wave (ASW) method within density functional theory (DFT). As a result, our calculations employing the generalized gradient approximation (GGA) reveal a delicate competition of ferro and antiferromagnetic interactions. Only after properly taking into account the electronic correlations present in CeZnPb via a GGA + <i>U</i> treatment we are able to correctly describe the antiferromagnetic ground state. In addition, our calculations give a clue to the metamagnetic transitions as being due to the inherent geometric frustration of the cerium spin system.
dc.language.isoen
dc.publisherElsevier
dc.subject.enIntermetallic compounds
dc.subject.enCrystal chemistry
dc.subject.enCeZnPb
dc.subject.enMagnetic properties
dc.subject.enElectronic structure
dc.title.enThe plumbide CeZnPb – Structure, magnetism, and chemical bonding
dc.typeArticle de revue
dc.identifier.doi10.1016/j.solidstatesciences.2010.01.029
dc.subject.halChimie/Matériaux
bordeaux.journalSolid State Sciences
bordeaux.page929-937
bordeaux.volume12
bordeaux.issue5
bordeaux.peerReviewedoui
hal.identifierhal-00482379
hal.version1
hal.popularnon
hal.audienceInternationale
hal.origin.linkhttps://hal.archives-ouvertes.fr//hal-00482379v1
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