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Universal Heat Conduction in the Iron Arsenide Superconductor KFe2As2: Evidence of a d-Wave State

J.-Ph. Reid, M. A. Tanatar, A. Juneau-Fecteau, R. T. Gordon, S. René de Cotret, N. Doiron-Leyraud, T. Saito, H. Fukazawa, Y. Kohori, K. Kihou, C. H. Lee, A. Iyo, H. Eisaki, R. Prozorov, Louis Taillefer

DOI 10.1103/PhysRevLett.109.087001 · Physical Review Letters

T1

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Abstract

The thermal conductivity κ of the iron arsenide superconductor KFe2As2 was measured down to 50 mK for a heat current parallel and perpendicular to the tetragonal c axis. A residual linear term at T→0, κ0/T is observed for both current directions, confirming the presence of nodes in the superconducting gap. Our value of κ0/T in the plane is equal to that reported by Dong et al. [Phys. Rev. Lett. 104, 087005 (2010)] for a sample whose residual resistivity ρ0 was 10 times larger. This independence of κ0/T on impurity scattering is the signature of universal heat transport, a property of superconducting states with symmetry-imposed line nodes. This argues against an s-wave state with accidental nodes. It favors instead a d-wave state, an assignment consistent with five additional properties: the magnitude of the critical scattering rate Γc for suppressing Tc to zero; the magnitude of κ0/T, and its dependence on current direction and on magnetic field; the temperature dependence of κ(T).

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
KFe2As2

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3.8Pressure not reportedzero_resistance
KFe2As2

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3.65Pressure not reportedzero_resistance
KFe2As2

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2.45Pressure not reportedunknown
YBa2Cu3O7

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—Pressure not reportedunknown
Ba2Sr2CaCu2O8+δ

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—Pressure not reportedunknown
Tl2Ba2CuO6+δ

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—Pressure not reportedunknown

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