Symmetry-protected topological phases, generalized Laughlin argument, and orientifolds

Chang-Tse Hsieh, Olabode Mayodele Sule, Gil Young Cho, Shinsei Ryu, and Robert G. Leigh
Phys. Rev. B 90, 165134 – Published 27 October 2014

Abstract

We generalize Laughlin's flux insertion argument, originally discussed in the context of the quantum Hall effect, to topological phases protected by non-on-site unitary symmetries, in particular by parity symmetry or parity symmetry combined with an on-site unitary symmetry. As a model, we discuss fermionic or bosonic systems in two spatial dimensions with CP symmetry, which are, by the CPT theorem, related to time-reversal symmetric topological insulators (e.g., the quantum spin Hall effect). In particular, we develop the stability/instability (or “gappability”/“ingappablity”) criteria for nonchiral conformal field theories with parity symmetry that may emerge as an edge state of a symmetry-protected topological phase. A necessary ingredient, as it turns out, is to consider the edge conformal field theories on unoriented surfaces, such as the Klein bottle, which arises naturally from enforcing parity symmetry by a projection operation.

  • Received 9 April 2014
  • Revised 27 September 2014

DOI:https://doi.org/10.1103/PhysRevB.90.165134

©2014 American Physical Society

Authors & Affiliations

Chang-Tse Hsieh, Olabode Mayodele Sule, Gil Young Cho, Shinsei Ryu, and Robert G. Leigh

  • Department of Physics, University of Illinois at Urbana-Champaign, 1110 West Green St, Urbana, Illinois 61801, USA

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Issue

Vol. 90, Iss. 16 — 15 October 2014

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