Strontium substitution for barium in mercury superconductors
HgBa sub(2-x)Sr sub(x)CuO sub(4+ delta ) (x identical with 0.06 - 0.45) and Hg sub(1-y)V sub(y)Ba sub(2-x)Sr sub(x)CuO sub(4+ delta ) (x identical with 0.16 - 1.1, y identical with 0.2 - 0.35) series were prepared by the encapsulation method. In the former series the optimum doping level is achieved...
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Veröffentlicht in: | Journal of low temperature physics 1999-11, Vol.117 (3), p.879-883 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | HgBa sub(2-x)Sr sub(x)CuO sub(4+ delta ) (x identical with 0.06 - 0.45) and Hg sub(1-y)V sub(y)Ba sub(2-x)Sr sub(x)CuO sub(4+ delta ) (x identical with 0.16 - 1.1, y identical with 0.2 - 0.35) series were prepared by the encapsulation method. In the former series the optimum doping level is achieved by annealing under oxygen for x identical with 0.06 and by annealing under nitrogen for x identical with 0.45. This behaviour is explained by different equilibrium oxygen pressures over phases with different Sr content. The decrease of T sub(c) is approx. -8K/x. The latter series is doped by replacing (HgO sub(2)) super(2-) groups by (VO sub(4)) super(3-) tetrahedra and optimum doping is achieved by argon annealing. |
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ISSN: | 0022-2291 1573-7357 |
DOI: | 10.1023/a:1022594606304 |