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Superconducting and Nonsuperconducting Ca-Free Single Crystals of Pb2Sr2RCu3O8 (R = La, Ce, Pr, Nd, Sm, Eu, Gd, Tb, Dy, Ho, and Y): Effect of Cation Vacancies and the Metal/Insulator Transition

โœ Scribed by J.S. Xue; M. Reedyk; J.E. Greedan; T. Timusk


Publisher
Elsevier Science
Year
1993
Tongue
English
Weight
354 KB
Volume
102
Category
Article
ISSN
0022-4596

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โœฆ Synopsis


Ci-free single erystal and polycrystalline samples of (\mathrm{Pb}{2} \mathrm{Sr}{2} \mathrm{RCu}{3} \mathrm{O}{k}) have been prepared by a (\mathrm{PbO} / \mathrm{NaCl}) flux growth method and a fast solid state reaction, respectively. The electronic character of the single crystals of this series can be roughly categorized into three groups: insulating (no carrier doping in the (\mathrm{CuO}_{2}) planes) for (R=\mathrm{La}, \mathrm{Ce}). (\mathrm{Pr}), and (\mathrm{Nd}), semiconducting for (R=\mathrm{Sm}), Eu, Gd, and (\mathrm{Tb}), and poorly metallic for (R=) Dy, Ho, and Y. Crystals with (R=) Eu to Ho are found to be superconducting with the exception of (\mathrm{Tb}). The metallic character in these crystals is likely promoted by a cation vacancy at the rare-earth sites which has been established by crystal structural and chemical analyses. The anomalous behavior of the (\mathrm{Tb}) crystals may originate from a lower dopant level as inferred from the structure determination or possibly from the presence of (\mathrm{Tb}^{4+}). The fact that metallic behavior is observed in nonstoichiometric polycrystalline samples and not in stoichiometric ones seems consistent with the cation vacancy carrier doping mechanism. 1993 Academic Press. Inc.


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Crystal Structures of Ca-Free Pb2Sr2RCu3
โœ J.S. Xue; J.E. Greedan; M. Maric ๐Ÿ“‚ Article ๐Ÿ“… 1993 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 612 KB

Structures of \(\mathrm{Pb}_{2} \mathrm{Sr}_{2} R \mathrm{Cu}_{3} \mathrm{O}_{8}\) have been determined by single crystal X-ray diffraction. A monoclinic symmetry \((C 2 / m, Z=2)\) was found for those crystals with \(R=\mathrm{Pr}, \mathrm{Nd}\), and \(\mathrm{Tb}\), orthorhombic \((\mathrm{Cmmm}\)