Enriched string-net models and their excitations
1The Ohio State University
2Vanderbilt University
| Published: | 2024-03-28, volume 8, page 1301 |
| Eprint: | arXiv:2305.14068v2 |
| Doi: | https://doi.org/10.22331/q-2024-03-28-1301 |
| Citation: | Quantum 8, 1301 (2024). |
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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 [10] 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/Müger 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 Müger 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.

Featured image: An $\mathcal{A}$-enriched fusion category $\mathcal{X}$ is the data necessary to attach the (2+1)D Levin-Wen string net model associated to the fusion category $\mathcal{X}$ to the (3+1)D Walker-Wang string net model associated to the modular tensor category $\mathcal{A}$.
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