Bulletin of the American Physical Society
APS March Meeting 2020
Volume 65, Number 1
Monday–Friday, March 2–6, 2020; Denver, Colorado
Session J48: Superconductivity: Nickelates
2:30 PM–5:30 PM,
Tuesday, March 3, 2020
Room: Mile High Ballroom 1A
Sponsoring
Unit:
DCMP
Chair: Bing Lv, University of Texas at Dallas
Abstract: J48.00006 : In Situ Synchrotron X-ray Studies of Nickelate Growth and Reduction*
Presenter:
YAN LI
(Materials Science Division, Argonne National Laboratory)
Authors:
YAN LI
(Materials Science Division, Argonne National Laboratory)
XI YAN
(Materials Science Division, Argonne National Laboratory)
Zhan Zhang
(Advanced Photon Source, Argonne National Laboratory)
Hua Huan Wang
(Institute of High Energy Physics, Chinese Academy of Sciences)
Hua Zhou
(Advanced Photon Source, Argonne National Laboratory)
Dillon Fong
(Materials Science Division, Argonne National Laboratory)
Long-sought non-cuprate superconductivity has recently been discovered in epitaxial thin films of alloyed neodymium nickelate (Nd0.8Sr0.2NiO2) [1]. Interestingly, the superconducting phase is only observed in the infinite layer A1B1O2 or ‘112’ phase, and not the more typical A1B1O3 (‘113’) perovskite phase. Reduction of the 113 to the 112 phase generally requires use of a strong reducing agent like hydrides. However, the topotactic transition process involving significant oxygen loss is intrinsically non-trivial and remains elusive for precise synthesis control. Here we present the results of in situ synchrotron X-ray studies on the growth of nickelate heterostructures by pulsed laser deposition (PLD). We employ a Nd0.8Sr0.2NiO3 target for the growth of Nd0.8Sr0.2NiO3 / SrTiO3 (001) heterostructures and NdNiO3 and SrNiOx targets for the growth of nickelate superlattices. We will discuss the relationships between phase stability and the oxygen concentration for different deposition parameters prior to CaH2 reduction. The results of in situ studies of the reduction process to realize square-planar nickelates will also be described.
*Work supported by the Department of Energy, Office of Science, Basic Energy Sciences under contract no. DE-AC02-06CH11357.
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