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Linear-in-field magnetoresistance in cuprates

ORAL

Abstract

The normal state of cuprate superconductors near the pseudogap critical point p* has been investigated by various measurements in high magnetic fields [1]. Resistivity shows a T-linear regime near p* whose magnitude appears to be controlled by a scattering rate in the Planckian limit [2].

A T-linear resistivity is observed, for example, in Nd-LSCO at a doping p = 0.24 (p* = 0.23) [3] and in LSCO at p = 0.19 (p* ≈ 0.18) [4]. In the latter material, a linear-in-field dependence of the resistivity is also reported, whose relation to the Planckian dissipation remains to be understood.

Here we report measurements of the resistivity in Nd-LSCO and LSCO near p* in magnetic fields H up to 85 T. The magnetoresistance (MR) is found to evolve from H-linear at low T to H-quadratic at high T, much as reported for LSCO at p = 0.19 [4]. We investigate this behaviour with calculations based on the Fermi surface geometry and scattering rate anisotropy deduced from a study of angle-dependent magnetoresistance (ADMR) in Nd-LSCO at p = 0.24 [5]. We also explore the MR of Nd-LSCO at p < p*.

[1] Proust & Taillefer, ARCMP.10,409 (2019)
[2] Legros et al., Nat. Phys.15,142 (2019)
[3] Daou et al., Nat. Phys.5,31 (2019)
[4] Giraldo-Gallo et al., Science 361,479 (2018)
[5] Fang et al., arXiv:2004.01725 (2020)

Presenters

  • Amirreza Ataei

    Institut Quantique, Département de physique & RQMP, Université de Sherbrooke, Universite de Sherbrooke (Canada), Universite de Sherbrooke, Université de Sherbrooke

Authors

  • Amirreza Ataei

    Institut Quantique, Département de physique & RQMP, Université de Sherbrooke, Universite de Sherbrooke (Canada), Universite de Sherbrooke, Université de Sherbrooke

  • Adrien Gourgout

    Institut Quantique, Département de physique & RQMP, Université de Sherbrooke, Universite de Sherbrooke (Canada), Universite de Sherbrooke

  • Francis Laliberte

    Institut Quantique, Département de physique & RQMP, Université de Sherbrooke, Universite de Sherbrooke (Canada), Universite de Sherbrooke, Université de Sherbrooke

  • Sven Badoux

    Institut Quantique, Département de physique & RQMP, Université de Sherbrooke, Universite de Sherbrooke

  • Gael Grissonnanche

    Institut Quantique, Département de physique & RQMP, Université de Sherbrooke, Universite de Sherbrooke (Canada), Universite de Sherbrooke, Cornell University

  • siham benhabib

    Laboratoire National des Champs Magnétiques Intenses, Laboratoire National des Champs Magnetiques Intenses

  • David Vignolles

    Laboratoire National des Champs Magnétiques Intenses

  • Jianshi Zhou

    University of Texas at Austin, Materials Science and Engineering Program, Department of Mechanical Engineering, University of Texas at Austin, University of Texas (Austin, USA), University of Texas, Texas Materials Institute, University of Texas at Austin, Materials Science and Engineering Program, Mechanical Engineering, University of Texas at Austin

  • Nicolas Doiron-Leyraud

    Institut Quantique, Département de physique & RQMP, Université de Sherbrooke, Universite de Sherbrooke

  • Cyril Proust

    Laboratoire National des Champs Magnétiques Intenses, Laboratoire National des Champs Magnetiques Intenses

  • Louis Taillefer

    Institut Quantique, Département de physique & RQMP, Université de Sherbrooke, Universite de Sherbrooke (Canada), Universite de Sherbrooke, Université de Sherbrooke