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Direct observation of strong surface reconstruction in partially reduced nickelate films

Physics

Direct observation of strong surface reconstruction in partially reduced nickelate films

C. Yang, R. Pons, et al.

This groundbreaking study by Chao Yang and colleagues explores the surface structure of Pr0.8Sr0.2NiO2+x films, revealing intriguing insights into surface polarity and atomic-level phenomena, including the effects of oxygen vacancies from topochemical reduction.

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~3 min • Beginner • English
Abstract
The polarity of a surface can affect the electronic and structural properties of oxide thin films through electrostatic effects. Understanding the mechanism behind these effects requires knowledge of the atomic structure and electrostatic characteristics at the surface. In this study, we use annular bright-field imaging to investigate the surface structure of a Pr0.8Sr0.2NiO2+x (0 < x < 1) film. We observe a polar distortion coupled with octahedral rotations in a fully oxidized Pr0.8Sr0.2NiO3 sample, and a stronger polar distortion in a partially reduced sample. Its spatial depth extent is about three unit cells from the surface. Additionally, we use four-dimensional scanning transmission electron microscopy (4D-STEM) to directly image the local atomic electric field surrounding Ni atoms near the surface and discover distinct valence variations of Ni atoms, which are confirmed by atomic-resolution electron energy-loss spectroscopy (EELS). Our results suggest that the strong surface reconstruction in the reduced sample is closely related to the formation of oxygen vacancies from topochemical reduction. These findings provide insights into the understanding and evolution of surface polarity at the atomic level.
Publisher
Nature Communications
Published On
Jan 09, 2024
Authors
Chao Yang, Rebecca Pons, Wilfried Sigle, Hongguang Wang, Eva Benckiser, Gennady Logvenov, Bernhard Keimer, Peter A. van Aken
Tags
Pr0.8Sr0.2NiO2+x
surface structure
4D-STEM
polar distortion
oxygen vacancy
electron energy-loss spectroscopy
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