Evolution of the Crystal and Electronic Structures of the RBa2Cu3O6 + δ Cuprates in Annealing
- Authors: Fetisov A.V.1, Estemirova S.K.1,2, Mitrofanov V.Y.1, Uporov S.A.1
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Affiliations:
- Institute of Metallurgy, Ural Branch, Russian Academy of Sciences
- El’tsin Ural Federal University
- Issue: Vol 127, No 6 (2018)
- Pages: 1033-1039
- Section: Order, Disorder, and Phase Transition in Condensed System
- URL: https://journals.rcsi.science/1063-7761/article/view/193935
- DOI: https://doi.org/10.1134/S1063776118120051
- ID: 193935
Cite item
Abstract
The crystal structure and the magnetic properties of the HTSC cuprates YBa2Cu3O6 + δ, Y1 ‒ xCaxBa2Cu3O6 + δ, and Nd1 +xBa2 –xCu3O6 + δ (x = 0.2) with the structure of a layered perovskite are studied. The well-known aging effect detected in these HTSC materials during storage under standard conditions, namely, an increase in their critical temperature Tc and a decrease in lattice parameter c in time, is investigated. Using YBa2Cu3O6 + δ as an example, we show that the dependence of c on the oxygen content undergoes the following changes in time: (1) the negative slope of the dependence with respect to axis δ increases and (2) nonlinearity appears and grows in time according to a quadratic law. The first type of changes is explained by an increase in the valence of copper ions, which is accompanied by a decrease in their radius. The second type is explained by the electrostatic interaction of structural CuO2 planes due to the accumulation of electron holes, which come from CuOδ planes, in them. The calculation of the second type of changes in parameter c in the YBa2Cu3O6 + δ cuprate exhibits good quantitative agreement with the experimental data. The second-type changes in the Y1 –xCaxBa2Cu3O6 + δ compound (hole doping of CuO2 planes) turn out to be identical to those in YBa2Cu3O6 + δ. However, the differently directed (in time) changes in lattice parameter c in Nd1 +xBa2 –xCu3O6 + δ indicate that the CuO2 planes in the neodymium cuprate are doped by electrons at the initial stage of aging. However, when these planes are saturated with holes in time, the type of doping changes from n to p without a noticeable change in the crystal structure, which has been considered to be impossible for layered cuprates to date.
About the authors
A. V. Fetisov
Institute of Metallurgy, Ural Branch, Russian Academy of Sciences
Author for correspondence.
Email: fetisovav@mail.ru
Russian Federation, ul. Amundsena 101, Yekaterinburg, 620016
S. Kh. Estemirova
Institute of Metallurgy, Ural Branch, Russian Academy of Sciences; El’tsin Ural Federal University
Email: fetisovav@mail.ru
Russian Federation, ul. Amundsena 101, Yekaterinburg, 620016; ul. Mira 19, Yekaterinburg, 620000
V. Ya. Mitrofanov
Institute of Metallurgy, Ural Branch, Russian Academy of Sciences
Email: fetisovav@mail.ru
Russian Federation, ul. Amundsena 101, Yekaterinburg, 620016
S. A. Uporov
Institute of Metallurgy, Ural Branch, Russian Academy of Sciences
Email: fetisovav@mail.ru
Russian Federation, ul. Amundsena 101, Yekaterinburg, 620016
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