Structure-property relationships in the layered cuprate La[sub 2-x]Sr[sub x]CuSnO[sub 6]
In an attempt to induce a metallic or superconductive state in the layered cuprate La[sub 2]CuSnO[sub 6], the series La[sub 2-x]Sr[sub x]CuSnO[sub 6-x/2+[delta]] (x = 0.00, 0.05, 0.10, 0.125, 0.15, 0.175, 0.20) was prepared. A solid solution forms for 0.00 < x < 0.175, the overall oxygen conte...
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Veröffentlicht in: | Journal of solid state chemistry 1993-01, Vol.102:1 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | In an attempt to induce a metallic or superconductive state in the layered cuprate La[sub 2]CuSnO[sub 6], the series La[sub 2-x]Sr[sub x]CuSnO[sub 6-x/2+[delta]] (x = 0.00, 0.05, 0.10, 0.125, 0.15, 0.175, 0.20) was prepared. A solid solution forms for 0.00 < x < 0.175, the overall oxygen content is 6.00 (3), and the samples are antiferromagnetic semiconductors. From neutron diffraction experiments, the compounds possess distinct copper-oxygen and tin-oxygen layers. There is a mismatch at the interface of the layers, which results in expansion of the copper-oxygen layers. There is a mismatch at the interface of the layers, which results in expansion of the copper-oxygen bond lengths (1.99 [angstrom] average). The copper is oxidized upon addition of strontium; however, in contrast to p-type cuprate superconductors, the in-plane copper-oxygen bond lengths increase and the axial bonds decrease. The interleaved tin-oxygen layers have a dramatic effect on the crystal chemistry, electronic structure, and properties. The electronic consequence is that empty upper and filled lower dx[sup 2] - y[sup 2] bands (upper and lower Hubbard bands) remain separated and narrow upon oxidation, which presumably prohibits superconductivity. |
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ISSN: | 0022-4596 1095-726X |
DOI: | 10.1006/jssc.1993.1019 |