Origin of the 110-K superconducting transition in the Bi-Sr-Ca-Cu-O system

J. M. Tarascon, Y. LePage, L. H. Greene, B. G. Bagley, P. Barboux, D. M. Hwang, G. W. Hull, W. R. McKinnon, and M. Giroud
Phys. Rev. B 38, 2504 – Published 1 August 1988
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Abstract

Superconducting critical transitions with an onset at 112 K and zero resistance at 107 K are obtained within the Bi-Sr-Ca-Cu-O system. The synthesis and formation of the 110-K superconducting phase using the 85-K material as a precursor is explained. The 110-K phase grows from the 85-K phase such that the resulting faceted crystal (a pseudomorph) can contain some of the 85-K phase in the core. With such a microstructure our magnetic data can be simply explained. A major structural difference between the 85- and 110-K materials is that the 85-K material can grow (relatively) large single crystals having long-range order whereas the 110-K material has only intermediate-range order (cryptocrystalline) of about 100-200 Å.

  • Received 29 February 1988

DOI:https://doi.org/10.1103/PhysRevB.38.2504

©1988 American Physical Society

Authors & Affiliations

J. M. Tarascon

  • Bell Communications Research, Inc., 331 Newman Springs Road, Red Bank, New Jersey 07701

Y. LePage

  • National Research Council of Canada, Ottawa K1A0R6

L. H. Greene, B. G. Bagley, P. Barboux, D. M. Hwang, and G. W. Hull

  • Bell Communications Research, Inc., 331 Newman Springs Road, Red Bank, New Jersey 07701

W. R. McKinnon

  • National Research Council of Canada, Ottawa K1A0R6

M. Giroud

  • Bell Communications Research, Inc., 331 Newman Springs Road, Red Bank, New Jersey 07701

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Vol. 38, Iss. 4 — 1 August 1988

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