Enriched string-net models and their excitations
- URL: http://arxiv.org/abs/2305.14068v2
- Date: Tue, 19 Mar 2024 15:36:12 GMT
- Title: Enriched string-net models and their excitations
- Authors: David Green, Peter Huston, Kyle Kawagoe, David Penneys, Anup Poudel, Sean Sanford,
- Abstract summary: Boundaries of Walker-Wang models have been used to construct commuting projector models.
This article gives a rigorous treatment of this 2D boundary model.
We also use TQFT techniques to show the 3D bulk point excitations of the Walker-Wang bulk are given by the M"uger center.
- Score: 0.0
- License: http://creativecommons.org/licenses/by/4.0/
- Abstract: Boundaries of Walker-Wang models have been used to construct commuting projector models which realize chiral unitary modular tensor categories (UMTCs) as boundary excitations. Given a UMTC $\mathcal{A}$ representing the Witt class of an anomaly, the article [arXiv:2208.14018] gave a commuting projector model associated to an $\mathcal{A}$-enriched unitary fusion category $\mathcal{X}$ on a 2D boundary of the 3D Walker-Wang model associated to $\mathcal{A}$. That article claimed that the boundary excitations were given by the enriched center/M\"uger centralizer $Z^\mathcal{A}(\mathcal{X})$ of $\mathcal{A}$ in $Z(\mathcal{X})$. In this article, we give a rigorous treatment of this 2D boundary model, and we verify this assertion using topological quantum field theory (TQFT) techniques, including skein modules and a certain semisimple algebra whose representation category describes boundary excitations. We also use TQFT techniques to show the 3D bulk point excitations of the Walker-Wang bulk are given by the M\"uger center $Z_2(\mathcal{A})$, and we construct bulk-to-boundary hopping operators $Z_2(\mathcal{A})\to Z^{\mathcal{A}}(\mathcal{X})$ reflecting how the UMTC of boundary excitations $Z^{\mathcal{A}}(\mathcal{X})$ is symmetric-braided enriched in $Z_2(\mathcal{A})$. This article also includes a self-contained comprehensive review of the Levin-Wen string net model from a unitary tensor category viewpoint, as opposed to the skeletal $6j$ symbol viewpoint.
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