Characterizing bulk properties of gapped phases by smeared boundary conformal field theories: Role of duality in unusual ordering

TL;DR

This paper explores the classification of gapped phases via smeared boundary conformal field theories, revealing unusual structures and symmetry-breaking phenomena in duality contexts.

Contribution

It introduces a formalism combining SBCFTs with Higgs and Nambu-Goldstone arguments to characterize gapped phases with non-invertible symmetries.

Findings

Demonstrates duality between massive and massless RG flows in specific models

Reveals gapped phases can be outside boundary critical phenomena modules

Shows spontaneous breaking of non-invertible symmetries in gapped phases

Abstract

We study the classification of the gapped phases or massive renormalization group (RG) flows dual to the massless RG flows under changing the sign of the coupling constants. Whereas our formalism is based on combining Higgs- or Nambu-Goldstone-type arguments with Cardy's smeared boundary conformal field theories (SBCFTs), several puzzling structures arise. More specifically, the established Higgs or Nambu-Goldstone type arguments on the duality imply that the natural basis for the gapped states should be constructed from a set of smeared Ishibashi states, which are unphysical in boundary critical phenomena. Hence, the module of the gapped phases can be outside of that of boundary critical phenomena, whereas one can still calculate characterizing quantities by applying SBCFTs to the models. For example, we demonstrate that the massive RG flow dual to the massless RG flow from the tricritical Ising model to the Ising model, one of the simplest massless RG flows, has this unusual structure. This can be regarded as a quantum field-theoretic analogue of order-disorder coexistence in lattice models. More generally, the resultant gapped phases usually spontaneously break non-group-like symmetry (or noninvertible symmetry). Our work provides systematic quantum field theoretic descriptions of such unusual phases with spontaneous symmetry breaking of non-group-like (or noninvertible) symmetries.