Direct imaging of the electron liquid at oxide interfaces

被引:0
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作者
Kyung Song
Sangwoo Ryu
Hyungwoo Lee
Tula R. Paudel
Christoph T. Koch
Bumsu Park
Ja Kyung Lee
Si-Young Choi
Young-Min Kim
Jong Chan Kim
Hu Young Jeong
Mark S. Rzchowski
Evgeny Y. Tsymbal
Chang-Beom Eom
Sang Ho Oh
机构
[1] Pohang University of Science and Technology (POSTECH),Department of Materials Science and Engineering
[2] Korea Institute of Materials Science (KIMS),Materials Modeling and Characterization Department
[3] University of Wisconsin-Madison,Department of Materials Science and Engineering
[4] University of Nebraska,Department of Physics and Astronomy & Nebraska Center for Materials and Nanoscience
[5] Humboldt University of Berlin,Department of Physics
[6] Sungkyunkwan University (SKKU),Department of Energy Science
[7] Institute for Basic Science (IBS),Center for Integrated Nanostructure Physics
[8] Ulsan National Institute of Science and Engineering (UNIST),School of Materials Science and Engineering
[9] Ulsan National Institute of Science and Engineering (UNIST),UNIST Central Research Facilities (UCRF)
[10] University of Wisconsin-Madison,Department of Physics
来源
Nature Nanotechnology | 2018年 / 13卷
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摘要
The breaking of symmetry across an oxide heterostructure causes the electronic orbitals to be reconstructed at the interface into energy states that are different from their bulk counterparts1. The detailed nature of the orbital reconstruction critically affects the spatial confinement and the physical properties of the electrons occupying the interfacial orbitals2–4. Using an example of two-dimensional electron liquids forming at LaAlO3/SrTiO3 interfaces5,6 with different crystal symmetry, we show that the selective orbital occupation and spatial quantum confinement of electrons can be resolved with subnanometre resolution using inline electron holography. For the standard (001) interface, the charge density map obtained by inline electron holography shows that the two-dimensional electron liquid is confined to the interface with narrow spatial extension (~1.0 ± 0.3 nm in the half width). On the other hand, the two-dimensional electron liquid formed at the (111) interface shows a much broader spatial extension (~3.3 ± 0.3 nm) with the maximum density located ~2.4 nm away from the interface, in excellent agreement with density functional theory calculations.
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页码:198 / 203
页数:5
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