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X-ray single crystal structure analysis of the 1245 type superconductor Hg0.5Pb0.5Ba2Ca4Cu5O12+δ

✍ Scribed by H. Schwer; J. Karpinski; L. Lesne; C. Rossel; A. Morawski; T. Lada; A. Paszewin


Publisher
Elsevier Science
Year
1995
Tongue
English
Weight
603 KB
Volume
254
Category
Article
ISSN
0921-4534

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✦ Synopsis


Crystals of Hgo.sPbo.sBa2Ca4CusO12+ 8 were measured on an X-ray four-circle single-crystal diffractometer and the crystal structure was refined to R -0.033. The onset of the superconducting transition of the crystals ranges from 101 K-115 K. The space group is P4/mmm and lattice parameters of the five-layer material are a = 3.8529(3) ~,, and c = 22.172(2) ,~. Hg is partially substituted for Pb and heavy atoms are shifted away from the origin by ~ 0.38 A. Stacking faults of 1234 or 1256 material are manifest in the Fourier maps, and the amount was refined to 4.4%. These stacking faults induce an additional electron density at the ideal 0(4) site and mask a possible oxygen occupancy at (½, ½, 0). However, electron density is observed at a distance of 0.6 ,~ from (½, -~, 0), suggesting a shift of the excess oxygen atom from its ideal position. Bondlengths and distances show systematic changes with increasing number n of CuO 2 layers. Changes occur mainly in the rock-salt type layer, whereas the CaCuO 2 units remain stable over the whole Hg-12(n -1)n series.


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## Crystals of Hgo.sPbo.zBa2Ca3Cu4OloA4 were measured on an X-ray four-circle single-crystal diffractometer and the crystal structure was refined to R = 0.023. The space group is P4/mmm and the lattice parameters are a = 3.8530 (5) .A, and c = 18.968 (3) /~. Lead is incorporated at the Hg site, b