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Seebeck Coefficient in a Cuprate Superconductor: Particle-Hole Asymmetry in the Strange Metal Phase and Fermi Surface Transformation in the Pseudogap Phase

A. Gourgout, G. Grissonnanche, F. Laliberté, A. Ataei, L. Chen, S. Verret, J.-S. Zhou, J. Mravlje, A. Georges, N. Doiron-Leyraud, Louis Taillefer

DOI 10.1103/PhysRevX.12.011037 · Physical Review X

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Abstract

We report measurements of the Seebeck effect in both the ab plane (Sa) and along the c axis (Sc) of the cuprate superconductor La1.6−xNd0.4SrxCuO4 (Nd-LSCO), performed in magnetic fields large enough to suppress superconductivity down to low temperature. We use the Seebeck coefficient as a probe of the particle-hole asymmetry of the electronic structure across the pseudogap critical doping p⋆=0.23. Outside the pseudogap phase, at p=0.24>p⋆, we observe a positive and essentially isotropic Seebeck coefficient as T→0. That S>0 at p=0.24 is at odds with expectations given the electronic band structure of Nd-LSCO above p⋆ and its known electronlike Fermi surface. We can reconcile this observation by invoking an energy-dependent scattering rate with a particle-hole asymmetry, possibly rooted in the non-Fermi-liquid nature of cuprates just above p⋆. Inside the pseudogap phase, for p<p⋆, Sa is seen to rise at low temperature as previously reported, consistent with the drop in carrier density n from n≃1+p to n≃p across p⋆ as inferred from other transport properties. In stark contrast, Sc at low temperature becomes negative below p⋆, a novel signature of the pseudogap phase. The sudden drop in Sc reveals a change in the electronic structure of Nd-LSCO upon crossing p⋆. We can exclude a profound change of the scattering across p⋆ and conclude that the change in the out-of-plane Seebeck coefficient originates from a transformation of the Fermi surface.

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

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—Pressure not reportedunknown

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