Bulletin of the American Physical Society
APS March Meeting 2021
Volume 66, Number 1
Monday–Friday, March 15–19, 2021; Virtual; Time Zone: Central Daylight Time, USA
Session S48: Superconductivity: Transport Properties
11:30 AM–2:30 PM,
Thursday, March 18, 2021
Sponsoring
Unit:
DCMP
Chair: Timir Datta, Univ of South Carolina
Abstract: S48.00003 : Linear-in-field magnetoresistance in cuprates
11:54 AM–12:06 PM
Live
Presenter:
Amirreza Ataei
(Institut Quantique, Département de physique & RQMP, Université de Sherbrooke)
Authors:
Amirreza Ataei
(Institut Quantique, Département de physique & RQMP, Université de Sherbrooke)
Adrien Gourgout
(Institut Quantique, Département de physique & RQMP, Université de Sherbrooke)
Francis Laliberte
(Institut Quantique, Département de physique & RQMP, Université de Sherbrooke)
Sven Badoux
(Institut Quantique, Département de physique & RQMP, Université de Sherbrooke)
Gael Grissonnanche
(Institut Quantique, Département de physique & RQMP, Université de Sherbrooke)
siham benhabib
(Laboratoire National des Champs Magnétiques Intenses)
David Vignolles
(Laboratoire National des Champs Magnétiques Intenses)
Jianshi Zhou
(Materials Science and Engineering Program, Department of Mechanical Engineering, University of Texas at Austin)
Nicolas Doiron-Leyraud
(Institut Quantique, Département de physique & RQMP, Université de Sherbrooke)
Cyril Proust
(Laboratoire National des Champs Magnétiques Intenses)
Louis Taillefer
(Institut Quantique, Département de physique & RQMP, Université de Sherbrooke)
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)
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