Crystal Structure of Tl <sub>2</sub> Ba <sub>2</sub> Ca <sub>2</sub> Cu <sub>3</sub> O <sub>10</sub> , a 125 K Superconductor

C.C. Torardi(DuPont (United States)), M.A. Subramanian(DuPont (United States)), J. C. CALABRESE(DuPont (United States)), J. Gopalakrishnan(DuPont (United States)), K. J. Morrissey(DuPont (United States)), T.R. Askew(DuPont (United States)), R. B. Flippen(DuPont (United States)), U. Chowdhry(DuPont (United States)), A.W. Sleight(DuPont (United States))
Science
April 29, 1988
Cited by 443

Abstract

There is now a new series of high-temperature superconductors that may be represented as (A(III)O)(2)A(2)(II)Can-1CunO2+2n where A(III) is Bi or Tl, A(II) is Ba or Sr, and n is the number of Cu-O sheets stacked consecutively. There is a general trend toward higher transition temperatures as n increases. The highest n value for a bulk phase is three and is found when A(III) is Tl. This compound, Tl(2)Ba(2)Ca(2)Cu(3)O(10), has the highest transition temperature( approximately 125 K) of any presently known bulk superconductor. The structure of Tl(2)Ba(2)Ca(2)Cu(3)O(10) has been determined from single-crystal x-ray diffraction data and is tetragonal, with a = 3.85 A and c = 35.9 A. No superstructure is observed, and the material is essentially twin-free. Electron microscopy in the Tl/Ba/Ca/Cu/O system has revealed intergrowths where n = 5; such regions may well be responsible for the superconducting onset behavior observed in this system at about 140 K.


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