Why some interfaces cannot be sharp
By N. Nakagawa, H. Hwang, D. Muller. 2005
1,274 citations recorded by the source corpus.
A central goal of modern materials physics and nanoscience is the control of materials and their interfaces to atomic dimensions. For interfaces between polar and nonpolar layers, this goal is thwarted by a polar catastrophe that forces an interfacial reconstruction. In traditional semiconductors, this reconstruction is achieved by an atomic disordering and stoichiometry change at the interface, but a new option is available in multivalent oxides: if the electrons can move, the atoms do not have to. Using atomic-scale electron energy loss spectroscopy, we have examined the microscopic distribution of charge and ions across the (001) LaAlO3/SrTiO3 interface. We find that there is a fundamental asymmetry between the ionically compensated AlO2/SrO/TiO2 interface, and the electronically compensated AlO2/LaO/TiO2 interface, both in interfacial sharpness and charge density. This suggests a general strategy to design sharp interfaces, remove interfacial screening charges, control the band offset and, hence, markedly improve the performance of oxide devices.
Subfields: Electrical and Electronic Engineering, Electronic, Optical and Magnetic Materials, Materials Chemistry
View Paper: https://www.semanticscholar.org/paper/587abcd6b78c5df38f43cb302104a39003603b45
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In Electrical and Electronic Engineering
In Electronic, Optical and Magnetic Materials
In Materials Chemistry
- S. May
- A. Bhattacharya
- Ramamoorthy Ramesh
- J. Mannhart
- J. Coey
- Sayeef Salahuddin
- A. Hebard
- J. Triscone
Citations in the corpus
- Magnetic Oxide Heterostructures (2014, background): “Additionally, intermixing and interfacial roughness can depend on the specifics of interfacial termination (135, 136), producing asymmetries in the behavior of A/B and B/A interfaces (29).”
- Built-in and induced polarization across LaAlO3/SrTiO3 heterojunctions (2010, background): “comprise negatively charged AlO 2 and positively charged LaO end planes and are polar in the ionic limi”