Discovery of a single topological Dirac fermion in the strong inversion asymmetric compound BiTeCl

  • Y. L. Chen
  • , M. Kanou
  • , Z. K. Liu
  • , H. J. Zhang
  • , J. A. Sobota
  • , D. Leuenberger
  • , S. K. Mo
  • , B. Zhou
  • , S. L. Yang
  • , P. S. Kirchmann
  • , D. H. Lu
  • , R. G. Moore
  • , Z. Hussain
  • , Z. X. Shen
  • , X. L. Qi
  • , T. Sasagawa

Research output: Contribution to journalArticlepeer-review

85 Scopus citations

Abstract

In the past few years, a new state of quantum matter known as the time-reversal-invariant topological insulator has been predicted theoretically and realized experimentally. All of the topological insulators discovered so far in experiment are inversion symmetric - except for strained HgTe, which has weak inversion asymmetry, a small bulk gap but no bulk charge polarization. Strong inversion asymmetry in topological insulators would not only lead to many interesting phenomena, such as crystalline-surface-dependent topological electronic states, pyroelectricity and intrinsic topological p-n junctions, but would also serve as an ideal platform for the realization of topological magneto-electric effects, which result from the modification of Maxwell equations in topological insulators. Here we report the discovery of a strong inversion asymmetric topological insulator phase in BiTeCl by angle-resolved photoemission spectroscopy, which reveals Dirac surface states and crystalline-surface-dependent electronic structures. Moreover, we observe a tenfold increase of the bulk energy gap in BiTeCl over the weak inversion asymmetric topological insulator HgTe, making it a promising platform for topological phenomena and possible applications at high temperature.

Original languageEnglish
Pages (from-to)704-708
Number of pages5
JournalNature Physics
Volume9
Issue number11
DOIs
StatePublished - Nov 2013
Externally publishedYes

Funding

We thank Z. Wang and C. X. Liu for the helpful discussion. Y.L.C. acknowledges support from a DARPA MESO project (No. N66001-11-1-4105) and the EPSRC First Grant (EP/K04074X/1). B.Z., Z.K.L., Z.X.S. and X.L.Q. acknowledge support from Department of Energy, Office of Basic Energy Science (contract DE-AC02-76SF00515). T.S. acknowledges support from MEXT, Japan (Grant-in-Aid for Scientific Research (B), No. 24340078). H.J.Z. acknowledges support from the Army Research Office (No. W911NF-09-1-0508). J.A.S. acknowledges support from the Stanford Graduate Fellowship. D.L. acknowledges the Swiss National Science Foundation.

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