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Fragile Topology Protected by Inversion Symmetry: Diagnosis, Bulk-Boundary Correspondence, and Wilson Loop (1905.08128v3)

Published 20 May 2019 in cond-mat.mes-hall

Abstract: We study the bulk and boundary properties of fragile topological insulators (TIs) protected by inversion symmetry, mostly focusing on the class A of the Altland-Zirnbauer classification. First, we propose an efficient method for diagnosing fragile band topology by using the symmetry data in momentum space. Using this method, we show that among all the possible parity configurations of inversion-symmetric insulators, at least 17 percent of them have fragile topology in 2D while fragile TIs are less than 3 percent in 3D. Second, we study the bulk-boundary correspondence of fragile TIs protected by inversion symmetry. In particular, we generalize the notion of $d$-dimensional ($d$D) $k$th-order TIs, which is normally defined for $0<k\le d$, to the cases with $k>d$, and show that they all have fragile topology. In terms of the Dirac Hamiltonian, a $d$D $k$th-order TI has $(k-1)$ boundary mass terms. We show that a minimal fragile TI with the filling anomaly can be considered as the $d$D $(d+1)$th-order TI, and all the other $d$D $k$th-order TIs with $k>(d+1)$ can be constructed by stacking $d$D $(d+1)$th-order TIs. Although $d$D $(d+1)$th-order TIs have no in-gap states, the boundary mass terms carry an odd winding number along the boundary, which induces localized charges on the boundary at the positions where the boundary mass terms change abruptly. In the cases with $k>(d+1)$, we show that the net parity of the system with boundaries can distinguish topological insulators and trivial insulators. Also, by studying the (nested) Wilson loop spectra, we determine the minimal number of bands to resolve the Wannier obstruction, which is consistent with the prediction from our diagnosis method of fragile topology. Finally, we show that a $(d+1)$D $(k-1)$th-order TI can be obtained by an adiabatic pumping of $d$D $k$th-order TI, which generalizes the previous study of the 2D 3rd-order TI.

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