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Doping dependence of the superconducting gap in Tl2Ba2CuO6+δ from heat transport

D. G. Hawthorn, S. Y. Li, M. Sutherland, Etienne Boaknin, R. W. Hill, C. Proust, F. Ronning, M. A. Tanatar, Johnpierre Paglione, Louis Taillefer, D. Peets, Ruixing Liang, D. A. Bonn, W. N. Hardy, N. N. Kolesnikov

DOI 10.1103/PhysRevB.75.104518 · Physical Review B

T1

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Abstract

We present low-temperature thermal conductivity measurements on the cuprate Tl2Ba2CuO6+δ throughout the overdoped regime. In the T→0 limit, the thermal conductivity due to d-wave nodal quasiparticles provides a bulk measurement of the superconducting gap Δ. We find Δ to decrease with increasing doping, with a magnitude consistent with spectroscopic measurements (photoemission and tunneling). This argues for a pure and simple d-wave superconducting state in the overdoped region of the phase diagram, which appears to extend into the underdoped regime down to a hole concentration of ≃0.1 hole/Cu. As hole concentration is decreased, the gap-to-Tc ratio increases, showing that the suppression of the superconducting transition temperature Tc (relative to the gap) begins in the overdoped regime.

Source-reported materials — not catalogue approval

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

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90Pressure not reportedzero_resistance
Tl2Ba2CuO6+δ

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

84Pressure not reportedzero_resistance
Tl2Ba2CuO6+δ

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

26Pressure not reportedzero_resistance
Bi2Sr2CaCu2O8+δ

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

—Pressure not reportedunknown
YBa2Cu3Oy

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—Pressure not reportedunknown
La2-xSrxCuO4

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

—Pressure not reportedunknown

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