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Crystal substructure and physical properties of the superconducting phase<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Bi</mml:mi></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mo>(</mml:mo><mml:mi mathvariant="normal">S</mml:mi><mml:mi mathvariant="normal">r</mml:mi><mml:mo>,</mml:mo><mml:mi mathvariant="normal">C</mml:mi><mml:mi mathvariant="normal">a</mml:mi><mml:mo>)</mml:mo></mml:mrow><mml:mrow><mml:mn>6</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">Cu</mml:mi></mml:mrow><mml:mrow><mml:mn>4</mml:mn></mml:mrow></mml:msub></mml:mrow><mml:mrow><mml:msub><mml:mrow><mml:mi mathvariant="normal">O</mml:mi></mml:mrow><mml:mrow><mml:mn>1</mml:mn><mml:mn>6</mml:mn><mml:mo>+</mml:mo><mml:mi>x</mml:mi></mml:mrow></mml:msub></mml:mrow></mml:math>

Jean‐Marie TarasconY. Le PageBellcore, 331 Newman Springs Road, Red Bank, New Jersey 07701P. BarbouxB. G. BagleyL. H. GreeneW. R. McKinnonBellcore, 331 Newman Springs Road, Red Bank, New Jersey 07701G. W. HullM. GiroudD. M. Hwang
1988lv
ABI

Annotatsiya

We have isolated a high-${T}_{c}$ phase in the Bi-Sr-Ca-Cu-O system of composition ${\mathrm{Bi}}_{4}{(\mathrm{S}\mathrm{r},\mathrm{C}\mathrm{a})}_{6}{\mathrm{Cu}}_{4}{\mathrm{O}}_{16+x}$. The crystal substructure has a tetragonal unit cell $a=3.817$ \AA{}, $c=30.5$ \AA{}) with similarities to both the oxygen-defect perovskites $\mathrm{Y}{\mathrm{Ba}}_{2}{\mathrm{Cu}}_{3}{\mathrm{O}}_{7\ensuremath{-}x}$ and the ${\mathrm{K}}_{2}$Ni${\mathrm{F}}_{4}$ structure of ${\mathrm{La}}_{2}$Cu${\mathrm{O}}_{4}$. The oxygen content, determined by titration and thermogravimetric analysis experiments, corresponds to a formal oxidation state Cu(2.15). Oxygen can be reversibly depleted in an argon ambient in an amount corresponding to the reduction of the Cu(III) into Cu(II). The compound has a metalliclike resistance above its ${T}_{c}$ near 85 K. Processing this precursor compound by heating to temperatures near its melting point (885 \ifmmode^\circ\else\textdegree\fi{}C) produces a sharp resistivity drop near 110 K that we show by ac susceptibility and Meissner effect is due to a superconducting transition.

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