
arXiv: 2103.12717
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 Σ×S1. 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.
High Energy Physics - Theory, Condensed Matter - Strongly Correlated Electrons, Quantum Physics, High Energy Physics - Theory (hep-th), Strongly Correlated Electrons (cond-mat.str-el), FOS: Physical sciences, Mathematical Physics (math-ph), Topological field theories in quantum mechanics, Quantum Physics (quant-ph), Topological quantum field theories (aspects of differential topology), Mathematical Physics
High Energy Physics - Theory, Condensed Matter - Strongly Correlated Electrons, Quantum Physics, High Energy Physics - Theory (hep-th), Strongly Correlated Electrons (cond-mat.str-el), FOS: Physical sciences, Mathematical Physics (math-ph), Topological field theories in quantum mechanics, Quantum Physics (quant-ph), Topological quantum field theories (aspects of differential topology), Mathematical Physics
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