Large-gap two-dimensional topological insulator in oxygen functionalized MXene

Hongming Weng, Ahmad Ranjbar, Yunye Liang, Zhida Song, Mohammad Khazaei, Seiji Yunoki, Masao Arai, Yoshiyuki Kawazoe, Zhong Fang, and Xi Dai
Phys. Rev. B 92, 075436 – Published 24 August 2015

Abstract

Two-dimensional (2D) topological insulators (TIs) have been recognized as a new class of quantum state of matter. They are distinguished from normal 2D insulators with their nontrivial band-structure topology identified by the Z2 number as protected by time-reversal symmetry (TRS). Two-dimensional TIs have intriguing spin-velocity locked conducting edge states and insulating properties in the bulk. In the edge states, the electrons with opposite spins propagate in opposite directions and the backscattering is fully prohibited when the TRS is conserved. This leads to a quantized dissipationless “two-lane highway” for charge and spin transportation and promises potential applications. Up to now, only very few 2D systems have been discovered to possess this property. The lack of suitable material obstructs further study and application. Here, by using first-principles calculations, we propose that functionalized MXenes with oxygen, M2CO2 (M=W, Mo, and Cr), are 2D TIs with the largest gap of 0.194 eV in the W case. They are dynamically stable and natively antioxidant. Most importantly, they are very likely to be easily synthesized by recently developed selective chemical etching of transition-metal carbides (the Mn+1AXn phase). This will pave the way to tremendous applications of 2D TIs, such as “ideal” conducting wire, multifunctional spintronic devices, and the realization of topological superconductivity and Majorana modes for quantum computing.

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  • Received 6 July 2015

DOI:https://doi.org/10.1103/PhysRevB.92.075436

©2015 American Physical Society

Authors & Affiliations

Hongming Weng1,2,*, Ahmad Ranjbar3, Yunye Liang4, Zhida Song1, Mohammad Khazaei5, Seiji Yunoki3,6,7, Masao Arai5, Yoshiyuki Kawazoe4,8, Zhong Fang1,2, and Xi Dai1,2

  • 1Beijing National Laboratory for Condensed Matter Physics, and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
  • 2Collaborative Innovation Center of Quantum Matter, Beijing, China
  • 3Computational Materials Science Research Team, RIKEN Advanced Institute for Computational Science, Kobe, Hyogo 650-0047, Japan
  • 4New Industry Creation Hatchery Center, Tohoku University, Sendai 980-8579, Japan
  • 5Computational Materials Science Unit, National Institute for Materials Science, 1-1 Namiki, Tsukuba 305-0044, Ibaraki, Japan
  • 6Computational Condensed Matter Physics Laboratory, RIKEN, Wako, Saitama 351-0198, Japan
  • 7Computational Quantum Matter Research Team, RIKEN Center for Emergent Matter Science, Wako, Saitama 351-0198, Japan
  • 8Thermophysics Institute, Siberian Branch, Russian Academy of Sciences, Russia

  • *hmweng@iphy.ac.cn

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Vol. 92, Iss. 7 — 15 August 2015

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