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Fusion of a normalized finite-group gauging wall with its reverse

Physical scope

Conditional finite-state fusion rule for the normalized gauging interface of an anomaly-free finite abelian symmetry in a two-dimensional CFT.

Statement

Let a finite abelian group G act on a two-dimensional CFT C by normalized, anomaly-free topological symmetry lines, with action and wall conventions as specified below. Let WG:C→C/G be the endpoint-framed gauging interface. Assume the full C-linear subcategory generated from the Lg by fusion, orientation reversal, and finite direct sums, with topological junctions as morphisms, unit 1C, and tensor product defect fusion, is a finite semisimple fusion category. Also assume the Lg are pairwise non-isomorphic simple objects. Fuse WG with its orientation reverse using the framed finite-groupoid-cardinality convention. Then, as a direct sum of topological lines on C, WG⊗WˉG=⨁g∈GLg. Each Lg occurs once as a simple summand. This is a finite-gauge counting statement under the stated line-sector hypothesis and makes no assertion about continuous groups.

Facts & Assumptions

Given: A finite abelian anomaly-free group G, its normalized symmetry lines Lg, and the gauging interface WG with the endpoint convention in the statement.

[F1]

Finite-group gauging wall conventions: G acts through normalized lines and coherent multiplication junctions; the sum is untwisted and uses the endpoint-framed flat-bundle weight 1/∣Aut⁡∣, so each relative-holonomy sector with trivial framed automorphism group has weight one.

[F2]

Fusion and multifusion categories: the assumed topological-line category is a finite semisimple fusion category; each Lg is a pairwise distinct simple object, so a finite direct-sum decomposition has a well-defined simple-summand multiplicity.

Proof

1.1givenF1algebra

Let I=[0,1] be the interval transverse to the fused wall. A flat principal G-bundle on I with chosen endpoint trivializations has relative parallel transport g∈G. Since G is finite and discrete and I is contractible, an endpoint-preserving gauge transformation cannot change this transport; conversely, each g∈G is realized by a framed flat bundle. Thus the isomorphism classes in the framed groupoid are in bijection with G.

2.1givenF1F2step 1.1algebra∎

By the oriented-strip convention in [F1], the sector with relative transport g contributes the action line Lg on the C side. Its coefficient is 1/∣Aut⁡∣=1 because its framed automorphism group is trivial. There is exactly one such sector for each g by step 1.1. The assumed finite semisimple line category and pairwise non-isomorphic simplicity in [F2] therefore give one copy of each Lg and no identifications between distinct summands, proving the displayed fusion rule.

Remarks

The proof uses only finite flat connections on an interval, where a fixed endpoint framing removes conjugacy ambiguity. It does not justify the analogous manipulation for an R-valued gauge field or its continuous measure.

Depends on

Dependency tree · 2 levels

Sources