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Band manipulation and spin texture in interacting moiré helical edges

Yang-Zhi Chou1,*, Jennifer Cano2,3, and J. H. Pixley4,3,5

  • 1Condensed Matter Theory Center and Joint Quantum Institute, Department of Physics, University of Maryland, College Park, Maryland 20742, USA
  • 2Department of Physics and Astronomy, Stony Brook University, Stony Brook, New York 11974, USA
  • 3Center for Computational Quantum Physics, Flatiron Institute, New York, New York 10010, USA
  • 4Department of Physics and Astronomy, Center for Materials Theory, Rutgers University, Piscataway, New Jersey 08854, USA
  • 5Physics Department, Princeton University, Princeton, New Jersey 08544, USA

  • *yzchou@umd.edu

Phys. Rev. B 104, L201113 – Published 23 November, 2021

DOI: https://doi.org/10.1103/PhysRevB.104.L201113

Abstract

We develop a theory for manipulating the effective band structure of interacting helical edge states realized on the boundary of two-dimensional time-reversal symmetric topological insulators. For a sufficiently strong interaction, an interacting edge band gap develops, spontaneously breaking time-reversal symmetry on the edge. The resulting spin texture, as well as the energy of the time-reversal breaking gaps, can be tuned by an external moiré potential (i.e., a superlattice potential). Remarkably, we establish that by tuning the strength and period of the potential, the interacting gaps can be fully suppressed and interacting Dirac points reemerge. In addition, nearly flat bands can be created by the moiré potential with a sufficiently long period. Our theory provides an unprecedented way to enhance the coherence length of interacting helical edges by suppressing the interacting gap. The implications of this finding for ongoing experiments on helical edge states is discussed.

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