paper

Quantized charge polarization as a many-body invariant in (2+1)D crystalline topological states and Hofstadter butterflies

arXiv:2211.09127 · doi:10.1103/PhysRevX.13.031005

Abstract

We show how to define a quantized many-body charge polarization for (2+1)D topological phases of matter, even in the presence of non-zero Chern number and magnetic field. For invertible topological states, is a , , , or topological invariant in the presence of , , , or -fold rotational symmetry, lattice (magnetic) translational symmetry, and charge conservation. manifests in the bulk of the system as (i) a fractional quantized contribution of to the charge bound to lattice disclinations and dislocations with Burgers vector , (ii) a linear momentum for magnetic flux, and (iii) an oscillatory system size dependent contribution to the effective 1d polarization on a cylinder. We study in lattice models of spinless free fermions in a magnetic field. We derive predictions from topological field theory, which we match to numerical calculations for the effects (i)-(iii), demonstrating that these can be used to extract from microscopic models in an intrinsically many-body way. We show how, given a high symmetry point , there is a topological invariant, the discrete shift , such that specifies the dependence of on . We derive colored Hofstadter butterflies, corresponding to the quantized value of , which further refine the colored butterflies from the Chern number and discrete shift.

25+16 pages, 10+11 figures, minor edits to the main text and the appendix

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