Tailoring the breathing-mode distortions in nickelate/ferroelectric heterostructures

G Guillaume Krieger (Department of Applied Physics, Eindhoven University of Technology 1 , P. O. Box 513, 5600MB Eindhoven,) C Chia-Ping Su (Laboratoire de Physique des Solides, CNRS, Université Paris-Saclay 2 , Orsay 91405,) H Hoshang Sahib (Université de Strasbourg, CNRS, IPCMS UMR 7504 1 Département de Chimie de la Matière Inorganique, , Strasbourg F-67034,) R Raymond Fan (Diamond Light Source, Diamond House, Harwell Science and Innovation Campus 3 , Didcot, Oxfordshire OX11 0DE,) P Paul Steadman (Diamond Light Source 4 , Didcot OX11 0DE,) A Alexandre Gloter N Nathalie Viart (Université de Strasbourg, CNRS, IPCMS UMR 7504 1 Département de Chimie de la Matière Inorganique, , Strasbourg F-67034,) D Daniele Preziosi (Université de Strasbourg, CNRS, IPCMS UMR 7504 1 Département de Chimie de la Matière Inorganique, , Strasbourg F-67034,)

Abstract

In transition metal oxides, electron–electron interaction and lattice degree of freedom are basic ingredients of emergent phenomena, such as metal-to-insulator transition (MIT) and superconductivity. Perovskite rare-earth nickelates are largely studied for their temperature-driven MIT, which is accompanied by a breathing-mode distortion and associated with a bond-disproportionation of the expanded (3d8L0) and compressed (3d8L2) NiO6 octahedra. Steric effects control the onset temperature of the MIT, the latter being concomitant or not with a complex antiferromagnetic spin arrangement depending upon the choice of the rare-earth ion (TMIT ≥ TNéel). Interface engineering of oxygen octahedra tilting, as imposed by the symmetry and orientation of the substrate, has resulted in an efficient pathway to modify both TMIT and TNéel, hence suggesting a key role of the electron–phonon coupling for both transport and magnetic properties in nickelate thin films. Here, via a combination of resonant elastic x-ray scattering and transport experiments, we show control over both TMIT and TNéel in heteroepitaxial PbZr0.2Ti0.8O3(d)/NdNiO3(7 nm)//SrTiO3 heterostructures, which are characterized by different strains and polarization states of the PbZr0.2Ti0.8O3 layer grown at different thicknesses d. We found the expected NdNiO3 bulk behavior (TMIT = TNéel), for a fully relaxed PbZr0.2Ti0.8O3 layer showing a monodomain polarization state. On the other side, an almost 30 K difference (TMIT > TNéel), is found for a fully strained PbZr0.2Ti0.8O3 characterized by a multidomain texture of the polarization state. We discuss our results in terms of an altered breathing distortion pattern of the underlying nickelate layer as supported by x-ray absorption spectroscopy measurements. We infer that locally different polar distortions controlled by a combination of polarization direction and strength of the strain state play the main role in the observed TMIT and TNéel variations.

Article Details

Volume / Issue Vol. 137, Issue 12
Published March 28, 2025
ISSN 0021-8979
Publisher American Institute of Physics

Journal Info

Journal of Applied Physics

American Institute of Physics

ISSN: 0021-8979 Physical Sciences

Authors (8)

G

Guillaume Krieger

Department of Applied Physics, Eindhoven University of Technology 1 , P. O. Box 513, 5600MB Eindhoven,

C

Chia-Ping Su

Laboratoire de Physique des Solides, CNRS, Université Paris-Saclay 2 , Orsay 91405,

H

Hoshang Sahib

Université de Strasbourg, CNRS, IPCMS UMR 7504 1 Département de Chimie de la Matière Inorganique, , Strasbourg F-67034,

R

Raymond Fan

Diamond Light Source, Diamond House, Harwell Science and Innovation Campus 3 , Didcot, Oxfordshire OX11 0DE,

P

Paul Steadman

Diamond Light Source 4 , Didcot OX11 0DE,

A

Alexandre Gloter

N

Nathalie Viart

Université de Strasbourg, CNRS, IPCMS UMR 7504 1 Département de Chimie de la Matière Inorganique, , Strasbourg F-67034,

D

Daniele Preziosi

Université de Strasbourg, CNRS, IPCMS UMR 7504 1 Département de Chimie de la Matière Inorganique, , Strasbourg F-67034,