← Back to search

Wiedemann-Franz Law and Abrupt Change in Conductivity across the Pseudogap Critical Point of a Cuprate Superconductor

B. Michon, A. Ataei, P. Bourgeois-Hope, C. Collignon, S. Y. Li, S. Badoux, A. Gourgout, F. Laliberté, J.-S. Zhou, Nicolas Doiron-Leyraud, Louis Taillefer

DOI 10.1103/PhysRevX.8.041010 · Physical Review X

T1

Active bibliographic source — not scientific approval

Bibliographic access preserves source history; it does not approve extracted materials or validate reported claims. Review warnings on each occurrence separately.

Abstract

The thermal conductivity κ of the cuprate superconductor La1.6−xNd0.4SrxCuO4 was measured down to 50 mK in seven crystals with doping from p=0.12 to p=0.24, both in the superconducting state and in the magnetic field-induced normal state. We obtain the electronic residual linear term κ0/T as T→0 across the pseudogap critical point p⋆=0.23. In the normal state, we observe an abrupt drop in κ0/T upon crossing below p⋆, consistent with a drop in carrier density n from 1+p to p, the signature of the pseudogap phase inferred from the Hall coefficient. A similar drop in κ0/T is observed at H=0, showing that the pseudogap critical point and its signatures are unaffected by the magnetic field. In the normal state, the Wiedemann-Franz law, κ0/T=L0/ρ(0), is obeyed at all dopings, including at the critical point where the electrical resistivity ρ(T) is T linear down to T→0. We conclude that the nonsuperconducting ground state of the pseudogap phase at T=0 is a metal whose fermionic excitations carry heat and charge as conventional electrons do.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
La1.6-xNd0.4SrxCuO4

Archive — visibility unverified

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

5Pressure not reportedunknown
La1.6-xNd0.4SrxCuO4

Archive — visibility unverified

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

14.5Pressure not reportedunknown
La1.6-xNd0.4SrxCuO4

Archive — visibility unverified

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

15.5Pressure not reportedunknown
La1.6-xNd0.4SrxCuO4

Archive — visibility unverified

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

15Pressure not reportedunknown
La1.6-xNd0.4SrxCuO4

Archive — visibility unverified

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

14.7Pressure not reportedunknown
La1.6-xNd0.4SrxCuO4

Archive — visibility unverified

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

12.4Pressure not reportedunknown
La1.6-xNd0.4SrxCuO4

Archive — visibility unverified

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

10.7Pressure not reportedunknown

Similar papers