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Fermi-surface transformation across the pseudogap critical point of the cuprate superconductor La1.6−xNd0.4SrxCuO4

C. Collignon, S. Badoux, S. A. A. Afshar, B. Michon, F. Laliberté, O. Cyr-Choinière, J.-S. Zhou, S. Licciardello, S. Wiedmann, N. Doiron-Leyraud, Louis Taillefer

DOI 10.1103/PhysRevB.95.224517 · Physical Review B

T1

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Abstract

The electrical resistivity ρ and Hall coefficient RH of the tetragonal single-layer cuprate La1.6−xNd0.4SrxCuO4 were measured in magnetic fields up to H=37.5 T, large enough to access the normal state at T→0, for closely spaced dopings p across the pseudogap critical point at p☆=0.23. Below p☆, both coefficients exhibit an upturn at low temperature, which gets more pronounced with decreasing p. Taken together, these upturns show that the normal-state carrier density n at T=0 drops upon entering the pseudogap phase. Quantitatively, it goes from n=1+p at p=0.24 to n=p at p=0.20. By contrast, the mobility does not change appreciably, as revealed by the magnetoresistance. Our data are in excellent agreement with recent high-field data on YBa2Cu3Oy and La2−xSrxCuO4. The quantitative consistency across three different cuprates shows that a drop in carrier density from 1+p to p is a universal signature of the pseudogap transition at T=0. We discuss the implication of these findings for the nature of the pseudogap phase.

Source-reported materials — not catalogue approval

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

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—Pressure not reportedunknown
La2-xSrxCuO4

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—Pressure not reportedunknown
Bi2La2-xSrxCuO6+δ

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—Pressure not reportedunknown
YBa2Cu3Oy

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—Pressure not reportedunknown

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