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Large orbital polarization in nickelate-cuprate heterostructures by dimensional control of oxygen coordination.


ABSTRACT: Artificial heterostructures composed of dissimilar transition metal oxides provide unprecedented opportunities to create remarkable physical phenomena. Here, we report a means to deliberately control the orbital polarization in LaNiO3 (LNO) through interfacing with SrCuO2 (SCO), which has an infinite-layer structure for CuO2. Dimensional control of SCO results in a planar-type (P-SCO) to chain-type (C-SCO) structure transition depending on the SCO thickness. This transition is exploited to induce either a NiO5 pyramidal or a NiO6 octahedral structure at the SCO/LNO interface. Consequently, a large change in the Ni d orbital occupation up to ~30% is achieved in P-SCO/LNO superlattices, whereas the Ni eg orbital splitting is negligible in C-SCO/LNO superlattices. The engineered oxygen coordination triggers a metal-to-insulator transition in SCO/LNO superlattices. Our results demonstrate that interfacial oxygen coordination engineering provides an effective means to manipulate the orbital configuration and associated physical properties, paving a pathway towards the advancement of oxide electronics.

SUBMITTER: Liao Z 

PROVIDER: S-EPMC6362240 | biostudies-literature | 2019 Feb

REPOSITORIES: biostudies-literature

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Large orbital polarization in nickelate-cuprate heterostructures by dimensional control of oxygen coordination.

Liao Zhaoliang Z   Skoropata Elizabeth E   Freeland J W JW   Guo Er-Jia EJ   Desautels Ryan R   Gao Xiang X   Sohn Changhee C   Rastogi Ankur A   Ward T Zac TZ   Zou Tao T   Charlton Timothy T   Fitzsimmons Michael R MR   Lee Ho Nyung HN  

Nature communications 20190204 1


Artificial heterostructures composed of dissimilar transition metal oxides provide unprecedented opportunities to create remarkable physical phenomena. Here, we report a means to deliberately control the orbital polarization in LaNiO<sub>3</sub> (LNO) through interfacing with SrCuO<sub>2</sub> (SCO), which has an infinite-layer structure for CuO<sub>2</sub>. Dimensional control of SCO results in a planar-type (P-SCO) to chain-type (C-SCO) structure transition depending on the SCO thickness. This  ...[more]

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