Spontaneous symmetry breaking on surface defects

Abstract

Coleman’s theorem states that continuous internal symmetries cannot be spontaneously broken in two-dimensional quantum field theories (QFTs). In this work we consider surface (i.e. two-dimensional) defects in d-dimensional conformal field theories (CFTs) invariant under a continuous internal symmetry group G. We study under which conditions it is possible for a surface defect to break spontaneously a continuous internal symmetry. We find that spontaneous symmetry breaking (SSB) is impossible under reasonable assumptions on the defect Renormalization Group (RG) flow. Counterexamples are possible only for exotic RG flows, that do not terminate at a fixed-point. We discuss an example of this kind. We also illustrate our no-go result with an effective field theory analysis of generic defect RG flows. We find a generic weakly coupled defect universality class (with no SSB), where correlation functions decay logarithmically. Our analysis generalizes the recent discovery by Metlitski of the extraordinary-log boundary universality class in the O(N) model.

Casimir Forces in CFT with Defects and Boundaries

“…Here, ⟨O(x α , z)O(x α , z)⟩ J is the CFT 2-point function dressed by the membrane at z = 0. This correlator is computed in Equation (26). Going to the position-momentum space, one has…”

“…[11][12][13][14][15] for some seminal papers, Refs. [16][17][18][19][20][21][22][23][24][25][26][27] for recent progresses, and Refs. [28,29] for recent reviews.…”