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Journal ArticleDOI

The crystal structure of the 1212 nonsuperconductor phase (Pb0.71Cu0.29)Sr2(Y0.73Ca0.27)Cu2O7

TLDR
In this article, the crystal structure of a single crystal, selected from the reaction product, was determined from three-dimensional x-ray diffraction data, and the stoichiometry was found to be Pb 0.71 Cu 0.29 Sr 2 (Y 0.73 Ca 0.27 )Cu 2 O 7.
Abstract
The reaction product from an oxide mixture of 1Pb:2Sr:0.75Y:25Ca:2Cu at 960 °C was nearly single phase. The crystal structure of a single crystal, selected from the reaction product, was determined from three-dimensional x-ray diffraction data. The stoichiometry was found to be Pb 0.71 Cu 0.29 Sr 2 (Y 0.73 Ca 0.27 )Cu 2 O 7 . The tetragonal lattice constants are a = 3.8207(4) A, c = 11.826(1) A, space group P 4/ mmm , M r = 655.6, Z = 1, D x , = 6.31 g cm −3 , λ(MoK α ) = 0.71069 A. R = 0.0269 for 179 unique observed reflections. The crystal structure is isomorphous with the 1212 phases. The Pb ion at the origin has an occupancy of 0.705 (8) and a Cu ion is located at 0.221, 0, 0 with an occupancy of 0.295. The oxygen ion in the plane of the Pb ions is disordered over a fourfold site with an occupancy of one. An ordered arrangement of this oxygen ion results in a distorted environment for periodically repeated Pb ions. The Pb–O bond lengths to the two oxygen ions above and below the Pb plane are 1.968(14) A. The Cu ion, displaced from the origin, can be considered as tetrahedrally coordinated. The four Cu–O bond distances in the CuO 2 plane are 1.917(6) A and the bond length to a fifth oxygen atom is 2.304(14) A at the apex of the square pyramid. A valence sum calculation for Cu in square coplanar coordination yields a value of 2.01. A similar calculation for Cu in the tetrahedral site yields 1.5. Sr is in a monocapped square antiprism coordination polyhedron. Y and Ca atoms occupy statistically the same site and are in cubic coordination. The structure can be described as consisting of CuO 2 –(Y, Ca)–CuO 2 layers with PbO 6 octahedra flanking the layers and Sr in the oxygen interstice. The compound is metallic at room temperature and shows no superconducting transition to 20 K.

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Citations
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Structures of High‐Temperature Cuprate Superconductors

TL;DR: Most of the known cuprate superconductors are shown to belong structurally to a single family and are closely related to each other as discussed by the authors, which leads to three significant insights into the nature of, and requirements for, superconductivity in these phases: (1) a nearly planar sheet of CuO{sub 2} supports the supercurrent; (2) as the distance between the n ACuO{ sub 2} blocks in a crystal structure increases, the critical current density decreases at high reduced temperatures due to the magnetic flux lines becoming unpinned; (
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Synthesis and structural characterisation of YSr2Cu3−xMxO7±y (M = Fe, Ti, Al, Co, Ga, Pb; 0.5 < x < 1), and the non-existence of the parent phase YSr2Cu3O7

TL;DR: The possibility of synthesizing phases of general composition YSr 2 Cu 3− x M x O 7± y has been examined for a wide variety of metals M.
Journal ArticleDOI

A new mercury-based superconductor: (Hg, Cr)Sr2CuOy

TL;DR: In this paper, a new mercury-based cuprate superconductor, (Hg 1- x Cr x )Sr 2 CuO y (0⩽ x ⩽0.8), having T c of 58 K ( x = 0.3 and 0.4), was synthesized.
Journal ArticleDOI

Structural changes accompanying oxygen incorporation in (Pb0.65Cu0.35Sr2(Y0.7Ca0.3)Cu2O7+δ

TL;DR: The structure parameters of superconducting (Pb 0.65 Cu 0.35 )Sr 2 (Y 0.7 Ca 0.3 )Cu 2 O 7.1 were refined by the Rietveld analysis of their TOF neutron powder diffraction data as mentioned in this paper.
Journal ArticleDOI

New families of layered cuprates containing double-MO2-unit fluorite blocks: (Ho, Ce)3Sr2Cu3O11 and (Ho, Ce)3Sr2Cu2 (Cu, M)O11 (M = Pb, Fe, Al)

TL;DR: Two new families of layered cuprates, (Ho, Ce)3Sr2Cu2(Cu, Pb)O11 and (Ho and Ce), have been synthesized as mentioned in this paper, which have tetragonal unit cells with lattice constants approximately equal to 3.8A and 17 A.
References
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Journal ArticleDOI

Possible high Tc superconductivity in the Ba-La-Cu-O system

TL;DR: In this paper, Ba−La−Cu−O system, with the composition BaxLa5−xCu5O5(3−y) have been prepared in polycrystalline form, and samples with x=1 and 0.75,y>0, annealed below 900°C under reducing conditions, consist of three phases, one of them a perovskite-like mixed-valent copper compound.
Journal ArticleDOI

Empirical bond-strength–bond-length curves for oxides

TL;DR: In this article, it was shown that all ions with an isoelectronic core can be fitted by a single pair of parameters, R0 and N, that are independent of the ionic character of the bond and the coordination number of the cation.
Journal ArticleDOI

A New High-Temperature Superconductor: Bi2Sr3-x Cax Cu2O8+y.

TL;DR: A new superconductor that displays onset behavior near 120 K has been identified as Bi2Sr3-xCaxCu2O8+y, with x ranging from about 0.4 to 0.9, and electron microscopy studies show an incommensurate superstructure along the a axis that can be approximated by an increase of a factor of 5 over the subcell dimension.
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