Superconductivity of Bi-2201 (n=1) as influenced by the substitution of Pb and/or rare-earths (R=La, Nd and Pr)

Sastry, P. V. P. S. S. ; Yakhmi, J. V. ; Iyer, R. M. ; Subramanian, C. K. ; Srinivasan, R. (1991) Superconductivity of Bi-2201 (n=1) as influenced by the substitution of Pb and/or rare-earths (R=La, Nd and Pr) Physica C: Superconductivity, 178 (1-3). pp. 110-118. ISSN 0921-4534

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Official URL: http://www.sciencedirect.com/science/article/pii/0...

Related URL: http://dx.doi.org/10.1016/0921-4534(91)90165-U

Abstract

Preparation conditions for stabilizing the bulk superconductivity (Tc=9.5 K) in the nominal Bi2Sr2CuO ~6 composition corresponding to the n=1 phase in the Bi2Sr2Can-1CunO2n+4 system are described. The samples Bi2.1Sr1.9CuOy and Bi2.2Sr1.8CuOy become superconducting at 10 K and 12 K, respectively. Single-phase compounds (space group Amaa) could be synthesized for the range 0 x1.0 in the series Bi2Sr2-xLaxCuO6+y but the orthorhombicity decreased gradual ly with increase in x and the structure became tetragonal at x=1.0. The Tc (R=0) value increased to a maximum of 19 K for x=0.4, corresponding to a value of ~ 2.2 for the formal valence of copper. For x 0.5 a sudden loss of superconductivity is observed. Simultaneous substitution of Pb for Bi, and, La for Sr yields further improvement in superconducting characteristics, hitting a peak of 26 K (R=0) for x=0.4 in the series Bi2-xPbxSr2-xRxCuOy (R=La). The R=Nd- and and Pr-s ubstituting compounds showed lower values of Tc for the same extent of doping (x=0.4). Interestingly, doping of Pb alone (i.e., Bi2-xPbxSr2CuO y) results in suppression of superconductivity altogether. The electrical resistivity, magnetic susceptibility and the cell parameter data are presented for varying levels of different substituents and discussed.

Item Type:Article
Source:Copyright of this article belongs to Elsevier Science.
ID Code:57942
Deposited On:30 Aug 2011 09:08
Last Modified:30 Aug 2011 09:08

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