Reconstruction of electrostatic field at the interface leads to formation of two-dimensional electron gas at multivalent (110)LaAlO3/SrTiO3 interfaces

Yin-Long Han, Yue-Wen Fang, Zhen-Zhong Yang, Cheng-Jian Li, Lin He, Sheng-Chun Shen, Zhong-Zhong Luo, Guo-Liang Qu, Chang-Min Xiong, Rui-Fen Dou, Xiao Wei, Lin Gu, Chun-Gang Duan, and Jia-Cai Nie
Phys. Rev. B 92, 115304 – Published 15 September 2015

Abstract

The interfacial atomic arrangement, which is different from that in the bulk form of the heterojunction, can induce a reconstruction of electrostatic field at the interface. For conventional semiconductor heterointerfaces, it is known that such reconstruction results in band bending, creating a quantum well in which the two-dimensional electron gas (2DEG) is formed. In this article, we show that this mechanism still works in a multivalent oxide heterojunction: for (110)LaAlO3/SrTiO3 (LAO/STO) heterojunctions, the coexistence of La and Ti in ABO3 perovskite unit cells at the interface reduces the valence of Ti, generating a local field leading to band bending in the interfacial STO layers. The extra free electrons are trapped in this bent conduction band forming a 2DEG. It unifies two independent mechanisms for 2DEG at LAO/STO interfaces, the “polar catastrophe” model and the “La1xSrxTiO3” layers model, and is expected to end the decade-old controversy. This study opens insight into atomic-scale band engineering to control the behavior of complex oxide heterojunctions.

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  • Received 20 January 2014
  • Revised 5 June 2015

DOI:https://doi.org/10.1103/PhysRevB.92.115304

©2015 American Physical Society

Authors & Affiliations

Yin-Long Han1,*, Yue-Wen Fang2,*, Zhen-Zhong Yang3,*, Cheng-Jian Li1, Lin He1, Sheng-Chun Shen1, Zhong-Zhong Luo1, Guo-Liang Qu1, Chang-Min Xiong1, Rui-Fen Dou1, Xiao Wei4,†, Lin Gu3,5,‡, Chun-Gang Duan2,§, and Jia-Cai Nie1,∥

  • 1Department of Physics, Beijing Normal University, Beijing 100875, People's Republic of China
  • 2Key Laboratory of Polar Materials and Devices, Ministry of Education, East China Normal University, Shanghai 200062, People's Republic of China
  • 3Laboratory for Advanced Materials & electron Microscopy, Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences, Beijing 100190, People's Republic of China
  • 4Department of Materials Science and Engineering, Zhejiang University, Hangzhou 310027, People's Republic of China
  • 5Collaborative Innovation Center of Quantum Matter, Beijing 100190, People's Republic of China

  • *These authors contributed equally to this paper.
  • mseweixiao@zju.edu.cn
  • l.gu@iphy.ac.cn
  • §wxbdcg@gmail.com
  • jcnie@bnu.edu.cn

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Vol. 92, Iss. 11 — 15 September 2015

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