Crossing with the circle in Dijkgraaf–Witten theory and applications to topological phases of matter

Author:

Bullivant Alex1,Delcamp Clement23ORCID

Affiliation:

1. Department of Theoretical Physics, University of Maynooth, Maynooth, Ireland

2. Max-Planck-Institut für Quantenoptik, Hans-Kopfermann-Str. 1, 85748 Garching, Germany

3. Munich Center for Quantum Science and Technology (MCQST), Schellingstr. 4, D-80799 München, Germany

Abstract

Given a fully extended topological quantum field theory, the “crossing with the circle” conditions establish that the dimension, or categorification thereof, of the quantum invariant assigned to a closed k-manifold Σ is equivalent to that assigned to the ( k + 1)-manifold [Formula: see text]. We compute in this paper these conditions for the 4-3-2-1 Dijkgraaf–Witten theory. In the context of the lattice Hamiltonian realization of the theory, the quantum invariants assigned to the circle and the torus encode the defect open string-like and bulk loop-like excitations, respectively. The corresponding “crossing with the circle” condition, thus, formalizes the process by which loop-like excitations are formed out of string-like ones. Exploiting this result, we revisit the statement that loop-like excitations define representations of the linear necklace group as well as the loop braid group.

Funder

Deutsche Forschungsgemeinschaft

Science Foundation Ireland

Publisher

AIP Publishing

Subject

Mathematical Physics,Statistical and Nonlinear Physics

Reference59 articles.

1. Topological quantum field theories

2. Higher‐dimensional algebra and topological quantum field theory

3. Higher Topos Theory (AM-170)

4. J. Lurie, “On the classification of topological field theories,” arXiv:0905.0465 [math.CT] (2009).

5. B. Bartlett, “On unitary 2-representations of finite groups and topological quantum field theory,” arXiv:0901.3975 (2009).

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