Improved conduction and orbital polarization in ultrathin LaNiO3 sublayer by modulating octahedron rotation in LaNiO3/CaTiO3 superlattices

Artificial oxide heterostructures have provided promising platforms for the exploration of emergent quantum phases with extraordinary properties. Here, we demonstrate an approach to stabilize a distinct oxygen octahedron rotation (OOR) characterized by <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup><mml:mrow><mml:mi>a</mml:mi></mml:mrow> <mml:mrow><mml:mo>-</mml:mo></mml:mrow> </mml:msup> <mml:msup><mml:mrow><mml:mi>a</mml:mi></mml:mrow> <mml:mrow><mml:mo>-</mml:mo></mml:mrow> </mml:msup> <mml:msup><mml:mrow><mml:mi>c</mml:mi></mml:mrow> <mml:mrow><mml:mo>+</mml:mo></mml:mrow> </mml:msup> </mml:math> in the ultrathin LaNiO<sub>3</sub> sublayers of the LaNiO<sub>3</sub>/CaTiO<sub>3</sub> superlattices. Unlike the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup><mml:mrow><mml:mi>a</mml:mi></mml:mrow> <mml:mrow><mml:mo>-</mml:mo></mml:mrow> </mml:msup> <mml:msup><mml:mrow><mml:mi>a</mml:mi></mml:mrow> <mml:mrow><mml:mo>-</mml:mo></mml:mrow> </mml:msup> <mml:msup><mml:mrow><mml:mi>c</mml:mi></mml:mrow> <mml:mrow><mml:mo>-</mml:mo></mml:mrow> </mml:msup> </mml:math> OOR in the LaNiO<sub>3</sub> bare film, the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup><mml:mrow><mml:mi>a</mml:mi></mml:mrow> <mml:mrow><mml:mo>-</mml:mo></mml:mrow> </mml:msup> <mml:msup><mml:mrow><mml:mi>a</mml:mi></mml:mrow> <mml:mrow><mml:mo>-</mml:mo></mml:mrow> </mml:msup> <mml:msup><mml:mrow><mml:mi>c</mml:mi></mml:mrow> <mml:mrow><mml:mo>+</mml:mo></mml:mrow> </mml:msup> </mml:math> OOR favors high conductivity, driving the LaNiO<sub>3</sub> sublayer to a metallic state of ~100 K even when the layer thickness is as thin as 2 unit cells (u.c.). Simultaneously, strongly preferred occupation of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub><mml:mrow><mml:mi>d</mml:mi></mml:mrow> <mml:mrow> <mml:msup><mml:mrow><mml:mi>x</mml:mi></mml:mrow> <mml:mrow><mml:mn>2</mml:mn></mml:mrow> </mml:msup> <mml:mo>-</mml:mo> <mml:msup><mml:mrow><mml:mi>y</mml:mi></mml:mrow> <mml:mrow><mml:mn>2</mml:mn></mml:mrow> </mml:msup> </mml:mrow> </mml:msub> </mml:math> orbital is achieved in LaNiO<sub>3</sub> sublayers. The largest change of occupancy is as high as 35%, observed in the 2 u.c.-thick LaNiO<sub>3</sub> sublayers sandwiched between 4 u.c.-thick CaTiO<sub>3</sub> sublayers. X-ray absorption spectra indicate that the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup><mml:mrow><mml:mi>a</mml:mi></mml:mrow> <mml:mrow><mml:mo>-</mml:mo></mml:mrow> </mml:msup> <mml:msup><mml:mrow><mml:mi>a</mml:mi></mml:mrow> <mml:mrow><mml:mo>-</mml:mo></mml:mrow> </mml:msup> <mml:msup><mml:mrow><mml:mi>c</mml:mi></mml:mrow> <mml:mrow><mml:mo>+</mml:mo></mml:mrow> </mml:msup> </mml:math> OOR pattern of LaNiO<sub>3</sub> achieved in the LaNiO<sub>3</sub>/CaTiO<sub>3</sub> heterostructures has significantly enhanced the Ni-3d/O-2p hybridization, stabilizing the metallic phase in ultrathin LaNiO<sub>3</sub> sublayers. The present work demonstrates that modulating the mode of OOR through heteroepitaxial synthesis can modify the orbital-lattice correlations in correlated perovskite oxides, revealing hidden properties of the materials.

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Journal
Nature Communications
Published
2024-11-15
DOI
https://doi.org/10.1038/s41467-024-54311-0
Citations
3
Primary Topic
Magnetic and transport properties of perovskites and related materials
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article
Field-Weighted Citation Impact
0.35

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article

Improved conduction and orbital polarization in ultrathin LaNiO3 sublayer by modulating octahedron rotation in LaNiO3/CaTiO3 superlattices

Jirong Sun, Bang‐Gui Liu, Fengxia Hu, Baogen Shen et al.
3 citations
Nature Communications
Magnetic and transport properties of perovskites and related materials
0.35
article

Improved conduction and orbital polarization in ultrathin LaNiO3 sublayer by modulating octahedron rotation in LaNiO3/CaTiO3 superlattices

Jirong Sun, Bang‐Gui Liu, Fengxia Hu, Baogen Shen, Jingying Zheng, Wenxiao Shi, Yuansha Chen, Yunzhong Chen, Mengqin Wang, Bo-Wen Yu, Jie Zheng, Jing Zhang, Zhe Li
article en
3 citations

Abstract

Artificial oxide heterostructures have provided promising platforms for the exploration of emergent quantum phases with extraordinary properties. Here, we demonstrate an approach to stabilize a distinct oxygen octahedron rotation (OOR) characterized by <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup><mml:mrow><mml:mi>a</mml:mi></mml:mrow> <mml:mrow><mml:mo>-</mml:mo></mml:mrow> </mml:msup> <mml:msup><mml:mrow><mml:mi>a</mml:mi></mml:mrow> <mml:mrow><mml:mo>-</mml:mo></mml:mrow> </mml:msup> <mml:msup><mml:mrow><mml:mi>c</mml:mi></mml:mrow> <mml:mrow><mml:mo>+</mml:mo></mml:mrow> </mml:msup> </mml:math> in the ultrathin LaNiO<sub>3</sub> sublayers of the LaNiO<sub>3</sub>/CaTiO<sub>3</sub> superlattices. Unlike the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup><mml:mrow><mml:mi>a</mml:mi></mml:mrow> <mml:mrow><mml:mo>-</mml:mo></mml:mrow> </mml:msup> <mml:msup><mml:mrow><mml:mi>a</mml:mi></mml:mrow> <mml:mrow><mml:mo>-</mml:mo></mml:mrow> </mml:msup> <mml:msup><mml:mrow><mml:mi>c</mml:mi></mml:mrow> <mml:mrow><mml:mo>-</mml:mo></mml:mrow> </mml:msup> </mml:math> OOR in the LaNiO<sub>3</sub> bare film, the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup><mml:mrow><mml:mi>a</mml:mi></mml:mrow> <mml:mrow><mml:mo>-</mml:mo></mml:mrow> </mml:msup> <mml:msup><mml:mrow><mml:mi>a</mml:mi></mml:mrow> <mml:mrow><mml:mo>-</mml:mo></mml:mrow> </mml:msup> <mml:msup><mml:mrow><mml:mi>c</mml:mi></mml:mrow> <mml:mrow><mml:mo>+</mml:mo></mml:mrow> </mml:msup> </mml:math> OOR favors high conductivity, driving the LaNiO<sub>3</sub> sublayer to a metallic state of ~100 K even when the layer thickness is as thin as 2 unit cells (u.c.). Simultaneously, strongly preferred occupation of <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub><mml:mrow><mml:mi>d</mml:mi></mml:mrow> <mml:mrow> <mml:msup><mml:mrow><mml:mi>x</mml:mi></mml:mrow> <mml:mrow><mml:mn>2</mml:mn></mml:mrow> </mml:msup> <mml:mo>-</mml:mo> <mml:msup><mml:mrow><mml:mi>y</mml:mi></mml:mrow> <mml:mrow><mml:mn>2</mml:mn></mml:mrow> </mml:msup> </mml:mrow> </mml:msub> </mml:math> orbital is achieved in LaNiO<sub>3</sub> sublayers. The largest change of occupancy is as high as 35%, observed in the 2 u.c.-thick LaNiO<sub>3</sub> sublayers sandwiched between 4 u.c.-thick CaTiO<sub>3</sub> sublayers. X-ray absorption spectra indicate that the <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msup><mml:mrow><mml:mi>a</mml:mi></mml:mrow> <mml:mrow><mml:mo>-</mml:mo></mml:mrow> </mml:msup> <mml:msup><mml:mrow><mml:mi>a</mml:mi></mml:mrow> <mml:mrow><mml:mo>-</mml:mo></mml:mrow> </mml:msup> <mml:msup><mml:mrow><mml:mi>c</mml:mi></mml:mrow> <mml:mrow><mml:mo>+</mml:mo></mml:mrow> </mml:msup> </mml:math> OOR pattern of LaNiO<sub>3</sub> achieved in the LaNiO<sub>3</sub>/CaTiO<sub>3</sub> heterostructures has significantly enhanced the Ni-3d/O-2p hybridization, stabilizing the metallic phase in ultrathin LaNiO<sub>3</sub> sublayers. The present work demonstrates that modulating the mode of OOR through heteroepitaxial synthesis can modify the orbital-lattice correlations in correlated perovskite oxides, revealing hidden properties of the materials.

Nature CommunicationsVol. 15(1)
Chinese Academy of Sciences (CN), Songshan Lake Materials Laboratory (CN), FZU ‒ Institute of Physics of the Academy of Sciences of the Czech Republic (CZ), Institute of Physics (CN), National Laboratory for Superconductivity (CN), University of Chinese Academy of Sciences (CN), Ningbo Institute of Industrial Technology (CN), Taiyuan University of Science and Technology (CN), Fuzhou University (CN)
National Science Foundation, Salt Science Research Foundation, National Natural Science Foundation of China, Chinese Academy of Sciences, Basic and Applied Basic Research Foundation of Guangdong Province
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Magnetic and transport properties of perovskites and related materials
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