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Fusion of a normalized finite-group gauging wall with its reverse
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 act on a two-dimensional CFT by normalized, anomaly-free topological symmetry lines, with action and wall conventions as specified below. Let be the endpoint-framed gauging interface. Assume the full -linear subcategory generated from the by fusion, orientation reversal, and finite direct sums, with topological junctions as morphisms, unit , and tensor product defect fusion, is a finite semisimple fusion category. Also assume the are pairwise non-isomorphic simple objects. Fuse with its orientation reverse using the framed finite-groupoid-cardinality convention. Then, as a direct sum of topological lines on , Each 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.
Statement references
Facts & Assumptions
Given: A finite abelian anomaly-free group , its normalized symmetry lines , and the gauging interface with the endpoint convention in the statement.
Finite-group gauging wall conventions: acts through normalized lines and coherent multiplication junctions; the sum is untwisted and uses the endpoint-framed flat-bundle weight , so each relative-holonomy sector with trivial framed automorphism group has weight one.
Fusion and multifusion categories: the assumed topological-line category is a finite semisimple fusion category; each is a pairwise distinct simple object, so a finite direct-sum decomposition has a well-defined simple-summand multiplicity.
Proof
Let be the interval transverse to the fused wall. A flat principal -bundle on with chosen endpoint trivializations has relative parallel transport . Since is finite and discrete and is contractible, an endpoint-preserving gauge transformation cannot change this transport; conversely, each is realized by a framed flat bundle. Thus the isomorphism classes in the framed groupoid are in bijection with .
By the oriented-strip convention in [F1], the sector with relative transport contributes the action line on the side. Its coefficient is because its framed automorphism group is trivial. There is exactly one such sector for each by step 1.1. The assumed finite semisimple line category and pairwise non-isomorphic simplicity in [F2] therefore give one copy of each 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 -valued gauge field or its continuous measure.