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Zastosuj identyfikator do podlinkowania lub zacytowania tej pozycji: http://hdl.handle.net/20.500.12128/7959
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dc.contributor.authorGroń, Tadeusz-
dc.contributor.authorFilipek, E.-
dc.contributor.authorPacześna, A.-
dc.contributor.authorUrbanowicz, Piotr-
dc.contributor.authorSawicki, Bogdan-
dc.contributor.authorDuda, Henryk-
dc.date.accessioned2019-01-25T07:03:42Z-
dc.date.available2019-01-25T07:03:42Z-
dc.date.issued2016-
dc.identifier.citationActa Physica Polonica. A, Vol. 130, nr 5 (2016), s. 1239-1241pl_PL
dc.identifier.issn0587-4246-
dc.identifier.urihttp://hdl.handle.net/20.500.12128/7959-
dc.description.abstractThe electrical conductivity (T) and thermoelectric power S(T) measurements of Sr2InV3O11 showed the insulating state and the change of sign of thermopower from p to n at Tn􀀀p = 400 K. The I–V characteristics provided the evidence of symmetrical and non-linear behaviour typical of strong emission of charge carriers induced by temperature and voltage. Relative dielectric permittivity "r as well as loss tangent (tan ) strongly depend both on the temperature in the range of 295–400 K and the frequency in the range of 5 102 to 1 106 Hz, showing the broad maximum at 320 K. These effects are considered as a relaxation process like in the Maxwell–Wagner or Jonscher model as well as the conduction of electric current, as determined by the Joule–Lenz law[…]pl_PL
dc.language.isoenpl_PL
dc.rightsUznanie autorstwa-Użycie niekomercyjne-Bez utworów zależnych 3.0 Polska*
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/3.0/pl/*
dc.subjectelectric conductivitypl_PL
dc.subjectthermoelectric powerpl_PL
dc.subjectelectric currentspl_PL
dc.titleElectrical properties of Sr2InV3O11pl_PL
dc.typeinfo:eu-repo/semantics/articlepl_PL
dc.relation.journalActa Physica Polonica. Apl_PL
dc.identifier.doi10.12693/APhysPolA.130.1239-
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