Position-Momentum Duality, Geometrical Description and Ideal Host Lattices for Fractional Chern Insulators

ORAL

Abstract

The recent discovery of fractional quantum Hall (FQH) physics in flat-band Chern insulators without external magnetic field presents a profound theoretical challenge to understand the interplay of universal long-wavelength physics of the FQH effect and short-wavelength physics determined by the host lattice. Here, we present a first quantization description of fractional Chern insulators that is the dual of the anisotropic FQH problem, with the roles of position and momentum interchanged. The fundamental guiding-center geometry of the problem emerges from the interplay of lattice and interaction metrics that act as momentum-space duals of Haldane's geometrical description of the anisotropic FQH effect. We introduce a novel broad class of ideal C>1 Chern insulator lattice models that are duals of the isotropic limit of the conventional FQH effect. These models afford a particularly elegant analytical framework and act as parent Hamiltonians for lattice FQH states with emergent guiding-center and SU(C) symmetry. Resulting microscopic insight into stabilization of FQH states on the lattice provides a foundation for future analyses of non-Abelian phases and fractional topological insulators.

Authors

  • Martin Claassen

    Department of Applied Physics, Stanford University

  • Ching-Hua Lee

    Stanford Univ, Department of Physics, Stanford University

  • Ronny Thomale

    University of Wurzburg, University of Wuerzburg, Institute for Theoretical Physics, W\"urzburg University, Institute for Theoretical Physics, University of Wuerzburg, Wuerzburg University

  • Xiaoliang Qi

    Stanford Univ, Stanford University, Department of Physics, Stanford University

  • Thomas Devereaux

    Stanford Institute for Materials \& Energy Sciences, Stanford University, SLAC National Accelerator Laboratory, Stanford University/ Stanford Institute for Materials and Energy Sciences, SLAC National Accelerator Laboratory, SLAC National Lab and Stanford University, SLAC National Accelerator Laboratory, Stanford Institute for Materials and Energy Sciences