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Heat Transport in a Strongly Overdoped Cuprate: Fermi Liquid and a Pure d-Wave BCS Superconductor

Cyril Proust, Etienne Boaknin, R. W. Hill, Louis Taillefer, A. P. Mackenzie

DOI 10.1103/PhysRevLett.89.147003 · Physical Review Letters

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Abstract

The transport of heat and charge in the overdoped cuprate superconductor Tl2Ba2CuO6+δ was measured down to low temperature. In the normal state, obtained by applying a magnetic field greater than the upper critical field, the Wiedemann-Franz law is verified to hold perfectly. In the superconducting state, a large residual linear term is observed in the thermal conductivity, in quantitative agreement with BCS theory for a d-wave superconductor. This is compelling evidence that the electrons in overdoped cuprates form a Fermi liquid, with no indication of spin-charge separation.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
Tl2Ba2CuO6+δ

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15Pressure not reportedunknown
Tl2Ba2CuO6+δ

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

15Pressure not reportedunknown
Tl2Ba2CuO6+δ

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

90Pressure not reportedunknown
YBa2Cu3O7-δ

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

93Pressure not reportedunknown
Bi2Sr2CaCu2O8

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

90Pressure not reportedunknown

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