2006
DOI: 10.1021/cm061856r
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Chemical Control of Hole Distribution and Superconductivity in (Cu,Mo)Sr2(Ce,R)sCu2O5+2s+δ (s = 2, 3; R = Y, La−Yb)

Abstract: In the crystal structure of members of the (Cu,Mo)Sr2(Ce,R) s Cu2O5+2 s + δ or (Cu,Mo)-12s2 homologous series of superconductive copper oxides, adjacent CuO2 planes are separated by a fluorite-structured (Ce,R)-[O2-(Ce,R)] s -1 blocking block. Here we utilize the fluorite block as a “chemical-pressure medium” for the s = 2 and 3 members of the series. The (Ce,R) sites readily accommodate rare earth elements (R) ranging in size from La down to Yb. With decreasing size of the R constituent, T c first monotoni… Show more

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Cited by 1 publication
(4 citation statements)
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“…This has been checked by combined O K and Cu L XAS and Mo K XAFS for YSCO-Mo [60]. The XAFS indicated the Mo to be Mo(VI).…”
Section: The Phase Diagram Of High-pressure Oxygenized Compoundsmentioning
confidence: 98%
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“…This has been checked by combined O K and Cu L XAS and Mo K XAFS for YSCO-Mo [60]. The XAFS indicated the Mo to be Mo(VI).…”
Section: The Phase Diagram Of High-pressure Oxygenized Compoundsmentioning
confidence: 98%
“…The superconductivity is much more sensitive to substitutions in the CuO 2 planes than in other sites [59], with many substituting metals quenching it at only a few percent. In contrast, the Cu chains in the charge reservoir block remain stable with substitution and the materials remain superconducting; for example Cr, Ga, Ge, Fe and Mo have been incorporated, often at ratios around 10-20% [23,54,56] and as high as 25% for Mo [26,28,32,44,60]. The Mo solubility limit of 25% could be explained by a bond strain model: the differing bonding preferences of Mo and Cu drive nanoscale domain formation, which might be shifting into grain-level phase separation due to nanodomain percolation.…”
Section: Figurementioning
confidence: 99%
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