Please use this identifier to cite or link to this item: https://elib.belstu.by/handle/123456789/36197
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dc.contributor.authorKlyndyuk, A. I.-
dc.date.accessioned2020-11-02T11:55:09Z-
dc.date.available2020-11-02T11:55:09Z-
dc.date.issued2009-
dc.identifier.citationThermoelectric Properties of Layered Ferrocuprates LnBaCuFeO5 + d (Ln = La, Pr, Nd, Sm, Gd–Lu) / A. I. Klyndyuk // Physics of the Solid State. - 2009. - Vol. 51, № 2. - P. 250–254ru
dc.identifier.urihttps://elib.belstu.by/handle/123456789/36197-
dc.description.abstractThe electrical resistivity ρ and the thermopower S of ceramic materials LnBaCuFeO5 + δ (Ln = La, Pr, Nd, Sm, Gd–Lu) are measured in air at temperatures in the range from 300 to 1100 K. All the studied ferrocuprates are p-type semiconductors. The electrical resistivity ρ and the thermopower S of these compounds increase with a decrease in the radius of the Ln3+ cation (with an increase in the number of 4f electrons n in Ln3+). The nonmonotonic behavior of the dependences ρ = f(n) and S = f(n) indicates that the electrical properties of the layered ferrocuprates LnBaCuFeO5 + δ depend on the electronic configuration of the Ln3+ cation. The power factors P calculated for the LnBaCuFeO5 + δ ceramic materials from the experimental values of ρ and S increase with increasing temperature and, at T = 1000 K, reach the maximum values P = 102.0 and 54.1 µW m–1 K–2 for Ln = Pr (4f 2 ) and Sm (4f 5 ), respectively, and become close to each other and equal to 30– 35 µW m–1 K–2 for Ln = Gd (4f 7 ), Dy (4f 9 ), and Ho (4f 10).ru
dc.format.mimetypeapplication/pdfru
dc.language.isoenru
dc.subjectceramic materialsru
dc.subjectthe electrical resistivityru
dc.subjectp-type semiconductorsru
dc.subjectthe electrical propertiesru
dc.subjectthe layered ferrocupratesru
dc.titleThermoelectric Properties of Layered Ferrocuprates LnBaCuFeO5 + d (Ln = La, Pr, Nd, Sm, Gd–Lu)ru
dc.typeArticleru
dc.identifier.DOI10.1134/S1063783409020073-
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