Bulletin of the American Physical Society
APS March Meeting 2020
Volume 65, Number 1
Monday–Friday, March 2–6, 2020; Denver, Colorado
Session U48: Superconductivity: Nickelates II (Theory and Models)
2:30 PM–4:54 PM,
Thursday, March 5, 2020
Room: Mile High Ballroom 1A
Sponsoring
Unit:
DCMP
Chair: B. Moritz
Abstract: U48.00007 : Superconductivity in trilayer Nickelates*
Presenter:
Emilian Nica
(Department of Physics, Arizona State Univ)
Authors:
Emilian Nica
(Department of Physics, Arizona State Univ)
Jyoti Krishna
(Department of Physics, Arizona State Univ)
Rong Yu
(Department of Physics and Beijing Key Laboratory of Opto-electronic Functional Materials and Micro-nano Devices, Renmin University of China)
Qimiao Si
(Department of Physics and Astronomy, Rice University)
Antia S. Botana
(Department of Physics, Arizona State Univ)
Onur Erten
(Department of Physics, Arizona State Univ)
For doped NdNiO2, it is believed that pairing in the superconducting phase occurs mainly in the Ni dx2-y2 band [2]. In contrast to the Cu-based high-Tc superconductors, the parent RNiO2 (R=La, Nd) phases are not insulating-in spite of containing Ni1+: d9 ions-due to the appearance of rare-earth 5d-bands in the Fermi surface (FS) [2]. RNiO2 materials are members of a larger family of layered nickelates Rn+1(NiO2)nO2 with n= 2, 3, ... ∞ determining the number of NiO2 planes along the c-axis. Here, we consider alternate trilayer compounds [3] where the rare-earth bands are pushed away from the FS which only includes three Ni- dx2-y2 sheets. We study superconductivity in these compounds in several doping regimes using a t-J model. We compare and contrast the pairing instabilities in the tri- and infinite-layer cases.
[1] D. Li, K. et al, Nature 572, 624 (2019).
[2] X. Wu et al, arXiv:1909.03015.
[3] J. Zhang et al, Nature Physics 13, 864 (2017).
*Supported by the DOE BES Award \# DE-SC0018197 and the Robert A. Welch Foundation Grant No. C-1411 (Q.S.)
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