Study on the crystal structure of the high T-c superconductor (Hg,Re)-1223

dc.contributor.authorMARTINEZ, L.G.pt_BR
dc.contributor.authorROSSI, J.L.pt_BR
dc.contributor.authorCORREA, H.P.S.pt_BR
dc.contributor.authorPASSOS, C.A.C.pt_BR
dc.contributor.authorORLANDO, M.T.D.pt_BR
dc.coverageInternacionalpt_BR
dc.date.accessioned2014-07-15T13:43:17Zpt_BR
dc.date.accessioned2014-07-30T11:50:14Z
dc.date.available2014-07-15T13:43:17Zpt_BR
dc.date.available2014-07-30T11:50:14Z
dc.date.issued2008pt_BR
dc.description.abstractSamples of the superconducting compound (Hg,Re)–1223 of nominal composition Hg0.82Re0.18Ba2Ca2Cu3O8+δ and different oxygen contents were studied using X-ray absorption and diffraction techniques. In the synthesis process, treatments under different ratio oxygen/argon gas mixtures of 5%, 10%, and 15% O2 resulted in samples named as Sample A, Sample B, and Sample C, respectively. It was determined by using the XANES technique that in these compounds the Re cation has valence +7. The study by EXAFS determined that the octahedral coordination is distorted and the distances of Re–O bonds are of the order of 1.85 A˚ for equatorial oxygen and 2.10 A˚ for the apical ones. The Rietveld refinement of X-ray powder diffraction data revealed that the studied samples presented segregation of two superconducting phases with space group P4/mmm and distinct lattice parameters, also confirmed by anomalous X-ray scattering. The main phase was associated to the phase (Hg,Re)–1223 with higher oxygen content and the secondary superconducting phase was associated with the undoped Hg–1223 phase. Measurements of ac magnetic susceptibility showed that the sample treated under 10% O2 atmosphere presented the best superconducting properties.
dc.format.extentS23-S29pt_BR
dc.identifier.citationMARTINEZ, L.G.; ROSSI, J.L.; CORREA, H.P.S.; PASSOS, C.A.C.; ORLANDO, M.T.D. Study on the crystal structure of the high T-c superconductor (Hg,Re)-1223. <b>Powder Diffraction, Suppl</b>, v. 23, n. 2, p. S23-S29, 2008. DOI: <a href="https://dx.doi.org/10.1154/1.2903506">10.1154/1.2903506</a>. Disponível em: http://repositorio.ipen.br/handle/123456789/5017.
dc.identifier.doi10.1154/1.2903506
dc.identifier.fasciculo2pt_BR
dc.identifier.issn0885-7156pt_BR
dc.identifier.orcidhttps://orcid.org/0000-0002-8304-9939
dc.identifier.orcidhttps://orcid.org/0000-0001-7707-7821
dc.identifier.urihttp://repositorio.ipen.br/handle/123456789/5017pt_BR
dc.identifier.vol23pt_BR
dc.relation.ispartofPowder Diffraction, Supplpt_BR
dc.rightsopenAccessen
dc.subjectcrystal structurept_BR
dc.subjecthigh-tc superconductorspt_BR
dc.subjectx-ray diffractionpt_BR
dc.subjectabsorption spectrapt_BR
dc.subjectcrystallographypt_BR
dc.titleStudy on the crystal structure of the high T-c superconductor (Hg,Re)-1223pt_BR
dc.typeArtigo de periódicopt_BR
dspace.entity.typePublication
ipen.autorMARCOS TADEU D' AZEREDO ORLANDO
ipen.autorHAMILTON PEREZ SOARES CORREA
ipen.autorJESUALDO LUIZ ROSSI
ipen.autorLUIS GALLEGO MARTINEZ
ipen.codigoautor6087
ipen.codigoautor3906
ipen.codigoautor502
ipen.codigoautor397
ipen.contributor.ipenauthorMARCOS TADEU D' AZEREDO ORLANDO
ipen.contributor.ipenauthorHAMILTON PEREZ SOARES CORREA
ipen.contributor.ipenauthorJESUALDO LUIZ ROSSI
ipen.contributor.ipenauthorLUIS GALLEGO MARTINEZ
ipen.date.recebimento09-02pt_BR
ipen.identifier.fi0.602pt_BR
ipen.identifier.ipendoc13202pt_BR
ipen.identifier.iwosWoSpt_BR
ipen.range.fi0.001 - 1.499
ipen.type.genreArtigo
relation.isAuthorOfPublication703e052c-f00d-4753-b7ea-5ced9a48f7b4
relation.isAuthorOfPublicatione53899f9-d45d-4d75-999e-638b2a15fe8f
relation.isAuthorOfPublicationc30c7f95-0303-41bd-aa41-1fc8c12ec2ab
relation.isAuthorOfPublicationd024d136-878b-4d31-bb7e-c1cb06324cfb
relation.isAuthorOfPublication.latestForDiscoveryd024d136-878b-4d31-bb7e-c1cb06324cfb
sigepi.autor.atividadeMARTINEZ, L.G.:397:730:Spt_BR
sigepi.autor.atividadeROSSI, J.L.:502:730:Npt_BR
sigepi.autor.atividadeCORREA, H.P.S.:3906:610:Npt_BR
sigepi.autor.atividadeORLANDO, M.T.D.:6087:730:Npt_BR

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