pith. sign in

arxiv: 1210.6363 · v4 · pith:3XPAPMISnew · submitted 2012-10-23 · 🧮 math.QA · hep-th· math.CT

Orbifold completion of defect bicategories

classification 🧮 math.QA hep-thmath.CT
keywords completiondefectsorbifoldorbifoldstheoriesbicategoryequivalencesfield
0
0 comments X p. Extension
pith:3XPAPMIS Add to your LaTeX paper What is a Pith Number?
\usepackage{pith}
\pithnumber{3XPAPMIS}

Prints a linked pith:3XPAPMIS badge after your title and writes the identifier into PDF metadata. Compiles on arXiv with no extra files. Learn more

read the original abstract

Orbifolds of two-dimensional quantum field theories have a natural formulation in terms of defects or domain walls. This perspective allows for a rich generalisation of the orbifolding procedure, which we study in detail for the case of topological field theories. Namely, a TFT with defects gives rise to a pivotal bicategory of "worldsheet phases" and defects between them. We develop a general framework which takes such a bicategory B as input and returns its "orbifold completion" B_orb. The completion satisfies the natural properties B \subset B_orb and (B_orb)_orb = B_orb, and it gives rise to various new equivalences and nondegeneracy results. When applied to TFTs, the objects in B_orb correspond to generalised orbifolds of the theories in B. In the example of Landau-Ginzburg models we recover and unify conventional equivariant matrix factorisations, prove when and how (generalised) orbifolds again produce open/closed TFTs, and give nontrivial examples of new orbifold equivalences.

This paper has not been read by Pith yet.

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Forward citations

Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. From gauging to duality in one-dimensional quantum lattice models

    cond-mat.str-el 2025-09 unverdicted novelty 6.0

    Gauging and duality transformations are equivalent up to constant depth quantum circuits in one-dimensional quantum lattice models, demonstrated via matrix product operators.