Universal <i>T</i>-linear resistivity and Planckian dissipation in cuprates

ORAL

Abstract

The perfectly linear temperature dependence of the electrical resistivity observed as T→0 in a variety of metals close to a quantum critical point is a major puzzle of condensed matter physics. Here we show that T-linear resistivity as T→0 is a generic property of cuprates, associated with a universal scattering rate [1]. We measured the low-temperature resistivity of the bi-layer cuprate Bi2212 and found that it exhibits a T-linear dependence with the same slope as in the single-layer cuprates Bi2201, Nd-LSCO and LSCO, despite their very different Fermi surfaces and structural, superconducting and magnetic properties. We then show that the T-linear coefficient (per CuO2 plane), A, is given by the universal relation A TF = h / 2e2, where e is the electron charge, h is the Planck constant and TF is the Fermi temperature. This relation, obtained by assuming that the scattering rate 1 /τ of charge carriers reaches the Planckian limit [2], whereby h /τ = 2π kBT, works not only for hole-doped cuprates but also for electron-doped cuprates, despite the different nature of their quantum critical point and strength of their electron correlations.

[1] Legros et al., Nature Physics (in press); arXiv:1805.02512 (2018).
[2] Bruin et al., Science 339, 804 (2013).

Presenters

  • Louis Taillefer

    • University of Sherbrooke (Canada)
    • Université de Sherbrooke, Canada
    • Physics, Université de Sherbrooke
    • Universite de Sherbrooke
    • Universite de Sherbrooke (Canada)

Authors

  • Louis Taillefer

    • University of Sherbrooke (Canada)
    • Université de Sherbrooke, Canada
    • Physics, Université de Sherbrooke
    • Universite de Sherbrooke
    • Universite de Sherbrooke (Canada)
  • Anaelle Legros

    • Université de Sherbrooke, Canada
    • Physics, Université de Sherbrooke
    • Universite de Sherbrooke (Canada)
  • Siham Benhabib

    • LNCMI
    • LNCMI Toulouse, France
    • LNCMI - CNRS
  • Wojciech Tabis

    • LNCMI Toulouse, France
  • Francis Laliberte

    • Université de Sherbrooke, Canada
    • Physics, Université de Sherbrooke
    • Universite de Sherbrooke (Canada)
  • Maxime Dion

    • Université de Sherbrooke, Canada
  • Maude Lizaire

    • Université de Sherbrooke, Canada
  • Baptiste Vignolle

    • LNCMI Toulouse, France
    • Institut de Chimie de la Matière Condensée de Bordeaux
  • David Vignolles

    • LNCMI Toulouse, France
  • Hélène Raffy

    • Université Paris-Sud, France
  • ZZ Li

    • Université Paris-Sud, France
  • Pascale Auban-Senzier

    • Université Paris-Sud, France
  • Nicolas Doiron-Leyraud

    • Université de Sherbrooke, Canada
    • Universite de Sherbrooke
    • Universite de Sherbrooke (Canada)
  • Patrick Fournier

    • Universite de Sherbrooke
    • Université de Sherbrooke, Canada
    • Université de Sherbrooke
  • Dorothée Colson

    • CEA Saclay, France
    • Service de Physique de l'Etat Condensée, CEA Saclay
  • cyril proust

    • LNCMI
    • LNCMI Toulouse, France
    • LNCMI - CNRS