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

We report measurements of the Seebeck effect in both the ab plane (S-a) 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*, S-a is seen to rise at low temperature as previously reported, consistent with the drop in carrier density n from n similar or equal to 1 + p to n similar or equal to p across p* as inferred from other transport properties. In stark contrast, S-c at low temperature becomes negative below p*, a novel signature of the pseudogap phase. The sudden drop in S-c 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.

Automated summary

This study reports on the measurements of the Seebeck effect in La1.6-xNd0.4SrxCuO4, a cuprate superconductor. The Seebeck coefficient is used to investigate the particle-hole asymmetry of the electronic structure across the pseudogap critical doping p* = 0.23. The results show that the Seebeck coefficient is positive and isotropic outside the pseudogap phase, contradicting the expected behavior based on the electronic band structure. Inside the pseudogap phase, the Seebeck coefficient along the c axis becomes negative at low temperature, indicating a novel signature of the pseudogap phase.