Strong Superexchange in a d9δ Nickelate Revealed by Resonant Inelastic X-Ray Scattering

J. Q. Lin, P. Villar Arribi, G. Fabbris, A. S. Botana, D. Meyers, H. Miao, Y. Shen, D. G. Mazzone, J. Feng, S. G. Chiuzbăian, A. Nag, A. C. Walters, M. García-Fernández, Ke-Jin Zhou, J. Pelliciari, I. Jarrige, J. W. Freeland, Junjie Zhang, J. F. Mitchell, V. Bisogni, X. Liu, M. R. Norman, and M. P. M. Dean
Phys. Rev. Lett. 126, 087001 – Published 22 February 2021
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Abstract

The discovery of superconductivity in a d9δ 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 d91/3 trilayer nickelates R4Ni3O8 (where R=La, Pr) and associated theoretical modeling. A magnon energy scale of 80meV resulting from a nearest-neighbor magnetic exchange of J=69(4)meV is observed, proving that d9δ 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.

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  • Received 6 August 2020
  • Accepted 15 January 2021

DOI:https://doi.org/10.1103/PhysRevLett.126.087001

© 2021 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

J. Q. Lin1,2,3,4, P. Villar Arribi5, G. Fabbris1,6, A. S. Botana7, D. Meyers1,8, H. Miao1,9, Y. Shen1, D. G. Mazzone1,10, J. Feng11,*, S. G. Chiuzbăian11,12, A. Nag13, A. C. Walters13, M. García-Fernández13, Ke-Jin Zhou13, J. Pelliciari14, I. Jarrige14, J. W. Freeland6, Junjie Zhang5,15, J. F. Mitchell5, V. Bisogni14, X. Liu2,†, M. R. Norman5,‡, and M. P. M. Dean1,§

  • 1Condensed Matter Physics and Materials Science Department, Brookhaven National Laboratory, Upton, New York 11973, USA
  • 2School of Physical Science and Technology, ShanghaiTech University, Shanghai 201210, China
  • 3Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
  • 4University of Chinese Academy of Sciences, Beijing 100049, China
  • 5Materials Science Division, Argonne National Laboratory, Lemont, Illinois 60439, USA
  • 6Advanced Photon Source, Argonne National Laboratory, Lemont, Illinois 60439, USA
  • 7Department of Physics, Arizona State University, Tempe, Arizona 85287, USA
  • 8Department of Physics, Oklahoma State University, Stillwater, Oklahoma 74078, USA
  • 9Material Science and Technology Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37830, USA
  • 10Laboratory for Neutron Scattering and Imaging, Paul Scherrer Institut, 5232 Villigen PSI, Switzerland
  • 11Sorbonne Université, CNRS, Laboratoire de Chimie Physique-Matière et Rayonnement, UMR 7614, 4 place Jussieu, 75252 Paris Cedex 05, France
  • 12Synchrotron SOLEIL, L’Orme des Merisiers, Saint-Aubin, BP 48, 91192 Gif-sur-Yvette, France
  • 13Diamond Light Source, Harwell Science and Innovation Campus, Didcot, Oxfordshire OX11 0DE, United Kingdom
  • 14National Synchrotron Light Source II, Brookhaven National Laboratory, Upton, New York 11973, USA
  • 15Institute of Crystal Materials, Shandong University, Jinan, Shandong 250100, China

  • *CAS Key Laboratory of Magnetic Materials and Devices, Ningbo Institute of Materials Technology and Engineering, Chinese Academy of Sciences, Ningbo 315201, China, and Zhejiang Province Key Laboratory of Magnetic Materials and Application Technology, Ningbo Institute of Materials Technology and Engineering, Chinese Academy of Sciences, Ningbo 315201, China.
  • liuxr@shanghaitech.edu.cn
  • norman@anl.gov
  • §mdean@bnl.gov

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Issue

Vol. 126, Iss. 8 — 26 February 2021

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