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Scaling of the superfluid density in high-temperature superconductors

C. C. Homes, S. V. Dordevic, T. Valla, M. Strongin

DOI 10.1103/PhysRevB.72.134517 · Physical Review B

T1

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Abstract

A scaling relation Nc≃4.4σdcTc has been observed in the copper-oxide superconductors, where Nc is the spectral weight associated with the formation of the superconducting condensate ρs=8Nc, Tc is the critical temperature, and σdc is the normal-state dc conductivity close to Tc. This scaling relation is examined within the context of a clean and dirty-limit BCS superconductor. These limits are well established for an isotropic BCS gap 2Δ and a normal-state scattering rate 1∕τ; in the clean limit 1∕τ⪡2Δ, and in the dirty limit 1∕τ>2Δ. The dirty limit may also be defined operationally as the regime where ρs varies with 1∕τ. It is shown that the scaling relation Nc or ρs∝σdcTc, which follows directly from the Ferell-Glover-Tinkham sum rule, is the hallmark of a BCS system in the dirty-limit. While the gap in the copper-oxide superconductors is considered to be d wave with nodes and a gap maximum Δ0, if 1∕τ>2Δ0 then the dirty-limit case is preserved. The scaling relation implies that the copper-oxide superconductors are likely to be in the dirty limit and, as a result, that the energy scale associated with the formation of the condensate scales linearly with Tc. The a−b planes and the c axis also follow the same scaling relation. It is observed that the scaling behavior for the dirty limit and the Josephson effect (assuming a BCS formalism) are essentially identical, suggesting that in some regime these two pictures may be viewed as equivalent.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
YBa2Cu3O6.95

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70Pressure not reportedunknown
YBa2Cu3O6.95

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80Pressure not reportedunknown
YBa2Cu3O6.95

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85Pressure not reportedunknown
YBa2Cu3O6.95

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93.5Pressure not reportedunknown
YBa2Cu3O6.60

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59Pressure not reportedunknown
YBa2Cu3O6.95

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93.2Pressure not reportedunknown
YBa2Cu3O7-δ

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92Pressure not reportedunknown
Pr-YBa2Cu3O7-δ

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40Pressure not reportedunknown
Pr-YBa2Cu3O7-δ

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75Pressure not reportedunknown
YBa2Cu4O8

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80Pressure not reportedunknown
Bi2Ca2SrCu2O8+δ

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90Pressure not reportedunknown
Bi2Ca2SrCu2O8+δ

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91Pressure not reportedunknown
Bi2Ca2SrCu2O8+δ

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85Pressure not reportedunknown
Y/Pb-Bi2Ca2SrCu2O8+δ

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35Pressure not reportedunknown
Y-Bi2Ca2SrCu2O8+δ

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40Pressure not reportedunknown
Y-Bi2Ca2SrCu2O8+δ

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43Pressure not reportedunknown
Tl2Ba2CuO6+δ

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88Pressure not reportedunknown
Nd1.85Ce0.15CuO4

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23Pressure not reportedunknown
Pr1.85Ce0.15CuO4

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19Pressure not reportedunknown
Pr1.85Ce0.15CuO4

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21Pressure not reportedunknown
Pr1.87Ce0.15CuO4

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16Pressure not reportedunknown
La1.87Sr0.13CuO4

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32Pressure not reportedunknown
La1.86Sr0.14CuO4

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36Pressure not reportedunknown
Ba0.62K0.38BiO3

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31Pressure not reportedunknown
Ba0.60K0.40BiO3

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28Pressure not reportedunknown
Ba0.54K0.46BiO3

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21Pressure not reportedunknown
Nb

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8.3Pressure not reportedunknown
Nb

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9.3Pressure not reportedunknown
Pb

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7.2Pressure not reportedunknown

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