Doping dependence of the superconducting gap in Tl_2Ba_2CuO_{6+delta} 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

TL;DR
This study measures the superconducting gap in Tl_2Ba_2CuO_{6+delta} across doping levels using heat transport, revealing a decreasing gap with doping and supporting a pure d-wave superconducting state.
Contribution
It provides the first bulk thermal conductivity measurements of the superconducting gap across the overdoped regime in Tl_2Ba_2CuO_{6+delta}, confirming the d-wave symmetry and its doping dependence.
Findings
Superconducting gap decreases with increased doping.
Gap-to-Tc ratio increases as hole concentration decreases.
Superconducting state remains pure d-wave into the underdoped regime.
Abstract
We present low-temperature thermal conductivity measurements on the cuprate Tl_2Ba_2CuO_{6+delta} 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, Delta. We find Delta 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.
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Taxonomy
TopicsSuperconducting Materials and Applications · Physics of Superconductivity and Magnetism · Particle accelerators and beam dynamics
