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Anisotropic Seebeck coefficient of Sr2RuO4 in the incoherent regime

Ramzy Daou1, Sylvie Hébert1, Gaël Grissonnanche2, Elena Hassinger2, Louis Taillefer2, Haruka Taniguchi3,4, Yoshiteru Maeno3,5, Alexandra S. Gibbs6, and Andrew P. Mackenzie6

  • 1Normandie Univ, ENSICAEN, UNICAEN, CNRS, CRISMAT, 14000 Caen, France
  • 2Département de physique & RQMP, Université de Sherbrooke, Sherbrooke, Québec J1K 2R1, Canada
  • 3Department of Physics, Kyoto University, Kyoto 606-8502, Japan
  • 4Department of Applied Physics, Graduate School of Engineering, Nagoya University, Nagoya, 464-8603, Japan
  • 5Toyota Riken - Kyoto Univ. Research Center (TRiKUC), Kyoto 606-8501, Japan
  • 6Max Planck Institute for Chemical Physics of Solids, Nöthnitzer Str. 40, 01187 Dresden, Germany

Phys. Rev. B 108, L121106 – Published 13 September, 2023

DOI: https://doi.org/10.1103/PhysRevB.108.L121106

Abstract

Intuitive entropic interpretations of the thermoelectric effect in metals predict an isotropic Seebeck coefficient at high temperatures in the incoherent regime even in anisotropic metals since entropy is not directional. Sr2RuO4 is an enigmatic material known for a wellcharacterized anisotropic normal state and unconventional superconductivity. Recent ab initio transport calculations of Sr2RuO4 that include the effect of strong electronic correlations predicted an enhanced high-temperature anisotropy of the Seebeck coefficient at temperatures above 300 K, but experimental evidence is missing. From measurements on clean Sr2RuO4 single crystals along both crystallographic directions, we find that the Seebeck coefficient becomes increasingly isotropic upon heating towards room temperature as generally expected. Above 300 K, however, S acquires a new anisotropy which rises up to the highest temperatures measured (750 K), in qualitative agreement with calculations. This is a challenge to entropic interpretations and highlights the lack of an intuitive framework to understand the anisotropy of thermopower at high temperatures.

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