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Thermal transport measurements through the charge density wave transition in CsV3Sb5

Erik D. Kountz1,2,3, Chaitanya R. Murthy1,2,3, Dong Chen4,5, Linda Ye2,6, Mark P. Zic2,3, Claudia Felser4, Ian R. Fisher1,2,6, Steven A. Kivelson1,2,3, and Aharon Kapitulnik1,2,3,6

  • 1Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, 2575 Sand Hill Road, Menlo Park, California 94025, USA
  • 2Geballe Laboratory for Advanced Materials, Stanford University, Stanford, California 94305, USA
  • 3Department of Physics, Stanford University, Stanford, California 94305, USA
  • 4Max Planck Institute for Chemical Physics of Solids, 01187 Dresden, Germany
  • 5College of Physics, Qingdao University, Qingdao 266071, China
  • 6Department of Applied Physics, Stanford University, Stanford, California 94305, USA

Phys. Rev. B 109, L201120 – Published 17 May, 2024

DOI: https://doi.org/10.1103/PhysRevB.109.L201120

Abstract

We study thermal transport and thermalization in single crystals of CsV3Sb5 through the CDW transition by directly measuring thermal diffusivity (D), thermal conductivity (κ), specific heat (c), and resistivity (ρ). Commensurate with previous reports, we observe a sharp, narrow anomaly in specific heat associated with a first-order transition that results in a CDW state below ∼94 K. While a corresponding sharp anomaly in thermal diffusivity is also observed, resistivity and thermal conductivity only exhibit small steps at the transition, where the feature is sharp for resistivity and broader for thermal conductivity. Scrutinizing the thermal Einstein relation κ=cD, we find that this relation is generally satisfied, except in the narrow two-phase regime of the putative first-order transition. The Wiedemann-Franz law as well seems to work outside the two-phase regime, where strong resemblance between the specific heat and the resistivity derivative below the transition may point to a concurrent emergence of a secondary electronic order parameter.

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