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dc.contributor.authorFetisov, A. V.en
dc.contributor.authorEstemirova, S. K.en
dc.date.accessioned2021-08-31T15:01:54Z-
dc.date.available2021-08-31T15:01:54Z-
dc.date.issued2018-
dc.identifier.citationFetisov A. V. Relationship Between Electronic and Crystal Structure in Nd1 + xBa2 − xCu3O6 + δ / A. V. Fetisov, S. K. Estemirova. — DOI 10.1007/s10948-017-4188-0 // Journal of Superconductivity and Novel Magnetism. — 2018. — Vol. 31. — Iss. 1. — P. 203-208.en
dc.identifier.issn15571939-
dc.identifier.otherFinal2
dc.identifier.otherAll Open Access, Green3
dc.identifier.otherhttps://www.scopus.com/inward/record.uri?eid=2-s2.0-85020285309&doi=10.1007%2fs10948-017-4188-0&partnerID=40&md5=cf6650903e06b014e6d171b7c25f1e42
dc.identifier.otherhttp://arxiv.org/pdf/1701.01397m
dc.identifier.urihttp://elar.urfu.ru/handle/10995/102120-
dc.description.abstractIn accordance with a relation between the lattice parameter c and the concentration of holes p, which has been found earlier for the YBa2Cu3O6+δcompound, we obtain the p parameter in the same manner for the solid solution Nd1.2Ba1.8Cu3O6+δwith substitution of Nd3+for Ba2+in barium sites. For this, structural and superconducting properties of the Nd1.2Ba1.8Cu3O6+δsamples stored for specified times τ after quenching from annealing temperatures have been studied. The investigation shows that Nd1.2Ba1.8Cu3O6+δstored for a long time has quite a low critical temperature Tcextending only to Tconset = 55 K for the most oxidized sample with δ = 0.953. We find that the δ-dependence of the lattice parameter c significantly changes with time τ. When using the relation between c and p, the existence of electron doping of 0.045 per Cu in Nd1.2Ba1.8Cu3O6+δcan be inferred. This doping explains well-reduced Tcin Nd1.2Ba1.8Cu3O6+δ. In addition, we observe a local drop of Tcby up to 20 K for the samples with p˜0.095 (δ˜0.8) similar to decreasing Tcknown as “anomaly 1/8”. © 2017, Springer Science+Business Media New York.en
dc.format.mimetypeapplication/pdfen
dc.language.isoenen
dc.publisherSpringer New York LLCen
dc.rightsinfo:eu-repo/semantics/openAccessen
dc.sourceJ Supercond Novel Magn2
dc.sourceJournal of Superconductivity and Novel Magnetismen
dc.subjectMAGNETIC PROPERTIESen
dc.subjectPEROVSKITESen
dc.subjectSUPERCONDUCTIVITYen
dc.subjectX-RAY METHODSen
dc.subjectBARIUM COMPOUNDSen
dc.subjectCRYSTAL STRUCTUREen
dc.subjectLATTICE CONSTANTSen
dc.subjectMAGNETIC PROPERTIESen
dc.subjectPEROVSKITEen
dc.subjectSUPERCONDUCTIVITYen
dc.subjectANNEALING TEMPERATURESen
dc.subjectBARIUM SITESen
dc.subjectCRITICAL TEMPERATURESen
dc.subjectELECTRON-DOPINGen
dc.subjectSTRUCTURAL AND SUPERCONDUCTING PROPERTIESen
dc.subjectX RAY METHODSen
dc.subjectCOPPER COMPOUNDSen
dc.titleRelationship Between Electronic and Crystal Structure in Nd1 + xBa2 − xCu3O6 + δen
dc.typeArticleen
dc.typeinfo:eu-repo/semantics/articleen
dc.typeinfo:eu-repo/semantics/publishedVersionen
dc.identifier.rsi35502906-
dc.identifier.doi10.1007/s10948-017-4188-0-
dc.identifier.scopus85020285309-
local.contributor.employeeFetisov, A.V., Institute of Metallurgy, Ural Branch of the Russian Academy of Sciences, 101 Amundsen Str., Ekaterinburg, 620016, Russian Federation
local.contributor.employeeEstemirova, S.K., Institute of Metallurgy, Ural Branch of the Russian Academy of Sciences, 101 Amundsen Str., Ekaterinburg, 620016, Russian Federation, Ural Federal University, 19 Mira St., Ekaterinburg, 620002, Russian Federation
local.description.firstpage203-
local.description.lastpage208-
local.issue1-
local.volume31-
local.contributor.departmentInstitute of Metallurgy, Ural Branch of the Russian Academy of Sciences, 101 Amundsen Str., Ekaterinburg, 620016, Russian Federation
local.contributor.departmentUral Federal University, 19 Mira St., Ekaterinburg, 620002, Russian Federation
local.identifier.pure6253142-
local.identifier.pure53f24561-e56e-45d3-bd54-3e6a81a589d2uuid
local.identifier.eid2-s2.0-85020285309-
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