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Displacive Jahn--Teller transition in NaNiO₂

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Peer-reviewed

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Authors

Nagle-Cocco, Liam AV  ORCID logo  https://orcid.org/0000-0001-9265-1588
Genreith-Schriever, Annalena R  ORCID logo  https://orcid.org/0000-0001-5626-2438

Abstract

Below its Jahn--Teller transition temperature, $T_\mathrm{JT}$, NaNiO$_2$ has a monoclinic layered structure consisting of alternating layers of edge-sharing NaO$_6$ and Jahn--Teller-distorted NiO$6$ octahedra. Above $T\mathrm{JT}$ where NaNiO$2$ is rhombohedral, diffraction measurements show the absence of a cooperative Jahn--Teller distortion, accompanied by an increase in the unit cell volume. Using neutron total scattering, solid-state Nuclear Magnetic Resonance (NMR), and extended X-ray absorption fine structure (EXAFS) experiments as local probes of the structure we find direct evidence for a displacive, as opposed to order-disorder Jahn--Teller transition at $T\mathrm{JT}$. This is supported by \textit{ab initio} molecular dynamics (AIMD) simulations. To our knowledge this study is the first to show a displacive Jahn--Teller transition in any material using direct observations with local probe techniques.

Description

Publication status: Published

Journal Title

Journal of the American Chemical Society

Conference Name

Journal ISSN

0002-7863
1520-5126

Volume Title

146

Publisher

American Chemical Society

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Except where otherwised noted, this item's license is described as Attribution 4.0 International
Sponsorship
Engineering and Physical Sciences Research Council (2275821)
Engineering and Physical Sciences Research Council (EP/L015978/1)
EPSRC (EP/R513180/1)
This work was supported by the Faraday Institution (FIRG001, FIRG017, FIRG024, FIRG060). L.A.V.N-C acknowledges a scholarship EP/R513180/1 to pursue doctoral research from the UK Engineering and Physical Sciences Research Council (EPSRC) and additional funding from the Cambridge Philosophical Society. J.M.A.S. acknowledges support from the EPSRC Cambridge NanoCDT, EP/L015978/1. A.L.G. acknowledges European Research Council (ERC) funding under grant 788144. The authors acknowledge Oak Ridge National Laboratory, a United States Department of Energy Office of Science User Facility, for use of the NOMAD instrument at the Spallation Neutron Source (experiment IPTS25164). We acknowledge the European Synchrotron Radiation Facility for provision of beam time on BM23 (experiment CH6437). We acknowledge I11 beamline at the Diamond Light Source, UK, for the synchrotron XRD measurement done under BAG proposal (the data presented in this work under CY34243; essential preliminary data from CY28349). Calculations were performed using the Sulis Tier 2 HPC platform hosted by the Scientific Computing Research Technology Platform at the University of Warwick (EP/T022108/1).