Bulletin of the American Physical Society
APS March Meeting 2022
Volume 67, Number 3
Monday–Friday, March 14–18, 2022; Chicago
Session T61: Copper Oxide and Related Systems-II
11:30 AM–2:18 PM,
Thursday, March 17, 2022
Room: Hyatt Regency Hotel -Field
Sponsoring
Unit:
DCMP
Chair: Eduardo Fradkin, University of Illinois
Abstract: T61.00001 : Hidden strange metallic state in underdoped electron-doped cuprates*
11:30 AM–11:42 AM
Presenter:
Tarapada Sarkar
(University of Maryland, College Park)
Authors:
Tarapada Sarkar
(University of Maryland, College Park)
Nicholas R Poniatowski
(University of Maryland, College Park)
Joshua S Higgins
(University of Maryland, College Park)
Pampa R Mandal Sarkar
(University of Maryland, College Park)
Mun K Chan
(Los Alamos National Laboratory)
Richard L Greene
(University of Maryland -College Park)
The low-temperature linear-in-T resistivity of “strange metals,” such as the metallic state of the cuprate high-temperature superconductors, has long been thought to be associated with a quantum critical point. However, recent transport studies of the cuprates have found this behavior persists over a wide range of overdoping. In this work [1], we report magnetoresistance and Hall effect results for electron-doped cuprate La2− xCexCuO4 for temperatures from 0.7 to 45 K and magnetic fields up to 65 T. For x= 0.12 and 0.13, just below the Fermi surface reconstruction (FSR) at x= 0.14, the normal state in-plane resistivity exhibits a well-known upturn at low temperature. Our new results show that this resistivity upturn is eliminated at a high magnetic field and the resistivity becomes linear-in-temperature. The magnitude of the linear coefficient scales with Tc and doping, as found previously [2,3] for dopings above the FSR. This finding suggests that the strange metal is not confined to a single “critical point” in the phase diagram, but rather is a robust universal feature of the metallic ground state of the cuprates.
1. T. Sarkar, et al., Phys. Rev. B 103, 224501 (2021).
2. K. Jin, et al.,Nature(London) 476, 73 (2011).
3. T. Sarkar, et al., Sci. Adv. 5, eaav6753 (2019).
*This work was supported by the NSF under grants DMR-1708334 and DMR-2002658 and the Maryland Quantum Materials Center (QMC). The National High Magnetic Field Laboratory research was supported by the NSF Cooperative agreements DMR-1157490 and DMR1644779.
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