Strong Superexchange in a d^{9-δ} Nickelate Revealed by Resonant Inelastic X-Ray Scattering.


Journal

Physical review letters
ISSN: 1079-7114
Titre abrégé: Phys Rev Lett
Pays: United States
ID NLM: 0401141

Informations de publication

Date de publication:
26 Feb 2021
Historique:
received: 06 08 2020
accepted: 15 01 2021
entrez: 12 3 2021
pubmed: 13 3 2021
medline: 13 3 2021
Statut: ppublish

Résumé

The discovery of superconductivity in a d^{9-δ} nickelate has inspired disparate theoretical perspectives regarding the essential physics of this class of materials. A key issue is the magnitude of the magnetic superexchange, which relates to whether cuprate-like high-temperature nickelate superconductivity could be realized. We address this question using Ni L-edge and O K-edge spectroscopy of the reduced d^{9-1/3} trilayer nickelates R_{4}Ni_{3}O_{8} (where R=La, Pr) and associated theoretical modeling. A magnon energy scale of ∼80  meV resulting from a nearest-neighbor magnetic exchange of J=69(4)  meV is observed, proving that d^{9-δ} nickelates can host a large superexchange. This value, along with that of the Ni-O hybridization estimated from our O K-edge data, implies that trilayer nickelates represent an intermediate case between the infinite-layer nickelates and the cuprates. Layered nickelates thus provide a route to testing the relevance of superexchange to nickelate superconductivity.

Identifiants

pubmed: 33709756
doi: 10.1103/PhysRevLett.126.087001
doi:

Types de publication

Journal Article

Langues

eng

Sous-ensembles de citation

IM

Pagination

087001

Auteurs

J Q Lin (JQ)

Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA.
School of Physical Science and Technology, ShanghaiTech University, Shanghai 201210, China.
Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China.
University of Chinese Academy of Sciences, Beijing 100049, China.

P Villar Arribi (P)

Materials Science Division, Argonne National Laboratory, Lemont, Illinois 60439, USA.

G Fabbris (G)

Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA.
Advanced Photon Source, Argonne National Laboratory, Lemont, Illinois 60439, USA.

A S Botana (AS)

Department of Physics, Arizona State University, Tempe, Arizona 85287, USA.

D Meyers (D)

Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA.
Department of Physics, Oklahoma State University, Stillwater, Oklahoma 74078, USA.

H Miao (H)

Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA.
Material Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37830, USA.

Y Shen (Y)

Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA.

D G Mazzone (DG)

Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA.
Laboratory for Neutron Scattering and Imaging, Paul Scherrer Institut, 5232 Villigen PSI, Switzerland.

J Feng (J)

Sorbonne Université, CNRS, Laboratoire de Chimie Physique-Matière et Rayonnement, UMR 7614, 4 place Jussieu, 75252 Paris Cedex 05, France.

S G Chiuzbăian (SG)

Sorbonne Université, CNRS, Laboratoire de Chimie Physique-Matière et Rayonnement, UMR 7614, 4 place Jussieu, 75252 Paris Cedex 05, France.
Synchrotron SOLEIL, L'Orme des Merisiers, Saint-Aubin, BP 48, 91192 Gif-sur-Yvette, France.

A Nag (A)

Diamond Light Source, Harwell Science and Innovation Campus, Didcot, Oxfordshire OX11 0DE, United Kingdom.

A C Walters (AC)

Diamond Light Source, Harwell Science and Innovation Campus, Didcot, Oxfordshire OX11 0DE, United Kingdom.

M García-Fernández (M)

Diamond Light Source, Harwell Science and Innovation Campus, Didcot, Oxfordshire OX11 0DE, United Kingdom.

Ke-Jin Zhou (KJ)

Diamond Light Source, Harwell Science and Innovation Campus, Didcot, Oxfordshire OX11 0DE, United Kingdom.

J Pelliciari (J)

National Synchrotron Light Source II, Brookhaven National Laboratory, Upton, New York 11973, USA.

I Jarrige (I)

National Synchrotron Light Source II, Brookhaven National Laboratory, Upton, New York 11973, USA.

J W Freeland (JW)

Advanced Photon Source, Argonne National Laboratory, Lemont, Illinois 60439, USA.

Junjie Zhang (J)

Materials Science Division, Argonne National Laboratory, Lemont, Illinois 60439, USA.
Institute of Crystal Materials, Shandong University, Jinan, Shandong 250100, China.

J F Mitchell (JF)

Materials Science Division, Argonne National Laboratory, Lemont, Illinois 60439, USA.

V Bisogni (V)

National Synchrotron Light Source II, Brookhaven National Laboratory, Upton, New York 11973, USA.

X Liu (X)

School of Physical Science and Technology, ShanghaiTech University, Shanghai 201210, China.

M R Norman (MR)

Materials Science Division, Argonne National Laboratory, Lemont, Illinois 60439, USA.

M P M Dean (MPM)

Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA.

Classifications MeSH