Dependences of the chemical potential shift and superconducting transitiontemperature on the hole concentration in La2-xSrxCuO4 and Bi2Sr2Ca1-xYxCu2O8+delta

Citation
P. Konsin et B. Sorkin, Dependences of the chemical potential shift and superconducting transitiontemperature on the hole concentration in La2-xSrxCuO4 and Bi2Sr2Ca1-xYxCu2O8+delta, SUPERCOND S, 13(3), 2000, pp. 301-306
Citations number
51
Categorie Soggetti
Apllied Physucs/Condensed Matter/Materiales Science
Journal title
SUPERCONDUCTOR SCIENCE & TECHNOLOGY
ISSN journal
09532048 → ACNP
Volume
13
Issue
3
Year of publication
2000
Pages
301 - 306
Database
ISI
SICI code
0953-2048(200003)13:3<301:DOTCPS>2.0.ZU;2-B
Abstract
Dependences of the superconducting transition temperature (T-c) on the hole concentration (n(h)) in La2-xSrxCuO4 and Bi2Sr2Ca1-xYxCu2O8+delta have bee n calculated using the interband model. The phase space for pair-transfer s cattering between the overlapping bands is governed by the position of the chemical potential. Downward shifts (Delta mu) of the electron chemical pot ential (mu) with n(h) have been found. The slope is partial derivative mu/p artial derivative n(h) approximate to 8 eV/hole in under-doped Bi2Sr2Ca1-xY xCu2O8+delta and it becomes smaller in optimally-doped and over-doped sampl es (similar to 1.2 eV/hole). In La2-xSrxCuO4 partial derivative mu/partial derivative n(h) is equal to 1.25 eV/hole in over-doped samples and similar to 0.4 eV/hole in under-doped samples at T = 80 K. The pseudogap leads to t he suppression of Delta mu(n(h)) up to n(h) approximate to 0.17 holes per C uO2 plane at T = 80 K. The shift of the chemical potential mu leads to the curve T-c(n(h)) with a maximum. The dependences Delta mu(n(h)) and T-c(n(h) ) for the systems considered agree with the experimental data.