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An operator algebraic approach to fusion category symmetry on the lattice

David E. Evans, Corey Jones

TL;DR

This work develops an operator-algebraic framework for fusion category symmetry in (1+1)D lattice systems via SymTFT, by embedding the physical boundary content into a quasi-local algebra $A$ and extracting a symmetry category $\mathcal{C}$ from a boundary subalgebra $B\subseteq A$. It shows that $\text{DHR}(B) \cong \mathcal{Z}(\mathcal{C})$, that $\mathcal{C}$ embeds into $\text{Bim}(A)$ and acts on $A$ via unital completely positive channels whose fixed points recover $B$, and that realizability on a tensor-product algebra requires integrality of $\mathcal{C}$ with on-site actions equivalent to the existence of a fiber functor. The paper then characterizes local extensions through Q-systems in $\text{DHR}(B)$, defines physical boundary subalgebras, and formulates symmetry channels $\text{Ch}(A|B)$, culminating in an equivalence $\text{Ch}(A|B) \cong S(\mathcal{C})$. It also proves two anomaly-enforced gaplessness theorems for symmetric states and analyzes dualities (e.g. Kramers-Wannier) as obstructions to fixing Lagrangian algebras, thereby linking categorical data to spectral properties. Overall, the work provides a rigorous lattice realization of SymTFT and a deep connection between boundary subalgebras, DHR categories, and bulk topological order with concrete criteria for when and how non-invertible symmetries can act on tensor-product lattice systems.

Abstract

We propose a framework for fusion category symmetry on the (1+1)D lattice in the thermodynamic limit by giving a formal interpretation of SymTFT decompositions. Our approach is based on axiomatizing physical boundary subalgebra of quasi-local observables, and applying ideas from algebraic quantum field theory to derive the expected categorical structures. We show that given a physical boundary subalgebra $B$ of a quasi-local algebra $A$, there is a canonical fusion category $\mathcal{C}$ that acts on $A$ by bimodules and whose fusion ring acts by locality preserving quantum channels on the quasi-local algebra such that $B$ is recovered as the fixed point operators. We show that a fusion category can be realized as symmetries on a tensor product quasi-local algebra if and only if all of its objects have integer dimensions, and that it admits an ``on-site" action on a tensor product spin chain if and only if it admits a fiber functor. We give a formal definition of a topological symmetric state, and prove two anomaly enforced gaplessness theorems, one for internal categorical symmetries and one for anomalous duality channels. Using the first, we show that for any fusion category $\mathcal{C}$ with no fiber functor there always exist gapless pure symmetric states on an anyon chain.

An operator algebraic approach to fusion category symmetry on the lattice

TL;DR

This work develops an operator-algebraic framework for fusion category symmetry in (1+1)D lattice systems via SymTFT, by embedding the physical boundary content into a quasi-local algebra and extracting a symmetry category from a boundary subalgebra . It shows that , that embeds into and acts on via unital completely positive channels whose fixed points recover , and that realizability on a tensor-product algebra requires integrality of with on-site actions equivalent to the existence of a fiber functor. The paper then characterizes local extensions through Q-systems in , defines physical boundary subalgebras, and formulates symmetry channels , culminating in an equivalence . It also proves two anomaly-enforced gaplessness theorems for symmetric states and analyzes dualities (e.g. Kramers-Wannier) as obstructions to fixing Lagrangian algebras, thereby linking categorical data to spectral properties. Overall, the work provides a rigorous lattice realization of SymTFT and a deep connection between boundary subalgebras, DHR categories, and bulk topological order with concrete criteria for when and how non-invertible symmetries can act on tensor-product lattice systems.

Abstract

We propose a framework for fusion category symmetry on the (1+1)D lattice in the thermodynamic limit by giving a formal interpretation of SymTFT decompositions. Our approach is based on axiomatizing physical boundary subalgebra of quasi-local observables, and applying ideas from algebraic quantum field theory to derive the expected categorical structures. We show that given a physical boundary subalgebra of a quasi-local algebra , there is a canonical fusion category that acts on by bimodules and whose fusion ring acts by locality preserving quantum channels on the quasi-local algebra such that is recovered as the fixed point operators. We show that a fusion category can be realized as symmetries on a tensor product quasi-local algebra if and only if all of its objects have integer dimensions, and that it admits an ``on-site" action on a tensor product spin chain if and only if it admits a fiber functor. We give a formal definition of a topological symmetric state, and prove two anomaly enforced gaplessness theorems, one for internal categorical symmetries and one for anomalous duality channels. Using the first, we show that for any fusion category with no fiber functor there always exist gapless pure symmetric states on an anyon chain.

Paper Structure

This paper contains 20 sections, 31 theorems, 124 equations.

Key Result

Theorem A

Symmetry from SymTFT. Let $B\subseteq A$ be a physical boundary subalgebra of a quasi-local algebra $A$ over $\mathbbm{Z}$. We say $\mathcal{C}$ is the symmetry fusion category of the physical boundary subalgebra.

Theorems & Definitions (100)

  • Definition 1.1
  • Theorem A
  • Theorem B
  • Theorem C
  • Theorem D
  • Theorem E
  • Theorem F
  • Definition 2.1
  • Definition 2.2
  • Definition 2.3
  • ...and 90 more