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Flat-connection groupoids satisfy boundary descent

Statement

Let M1 and M2 be compact triangulated d-bordisms glued along an identified closed triangulated boundary Σ, with collars and compatible triangulations. The finite flat-connection groupoid on the glued manifold is equivalent to the homotopy pullback groupoid

CG(M2∪ΣM1)≃CG(M2)×CG(Σ)hCG(M1).

Writing ri:CG(Mi)→CG(Σ) for restriction, a pullback object is (A2,A1,α:r2(A2)≅r1(A1)). A morphism (u2,u1) to (A2′,A1′,α′) satisfies r1(u1)∘α=α′∘r2(u2).

Facts & Assumptions

Given: The compatible triangulated bordisms M1,M2, their common boundary Σ, and the finite flat-connection groupoids from Finite flat connection groupoid on a cell complex.

[F1]

Finite flat connection groupoid on a cell complex: objects are flat edge labels and arrows are vertex gauge transformations; gauge transformations preserve flatness.

[F2]

Finite gauge state spaces and bordism spans: boundary restriction is a functor of finite flat-connection groupoids.

[F3]

Homotopy pullback of finite groupoids: a homotopy-pullback object includes an isomorphism α between the two images, and its arrows satisfy q(v)∘α=α′∘p(u).

Proof

1.1givenF1F2F3construct

A global flat labeling on M2∪ΣM1 restricts to flat labelings on both pieces whose boundary labels agree. The identity boundary isomorphism makes this a triple in the homotopy pullback defined by [F3]. Restriction of a global vertex gauge transformation gives a compatible pair, so restriction defines a functor from the global groupoid.

2.1givenF1F3step 1.1construct

Conversely, let (A2,A1,α) be a homotopy-pullback object as in [F3], where α:r2(A2)→r1(A1) is a boundary gauge isomorphism. Its finite vertex values on the boundary extend to the vertices of M2 by setting every non-boundary value to the identity. Applying this gauge transformation to A2 makes its boundary edge labels equal to those of A1. The two edge labelings then glue to a unique labeling on the union; every 2-cell lies in one of the pieces or their common boundary, so each flatness equation remains satisfied. This proves essential surjectivity.

3.1F1F2F3step 2.1construct

By [F3], a morphism in the homotopy pullback is a pair of gauge transformations on M2 and M1 satisfying the boundary compatibility equation. After the boundary representatives are aligned as in step 2.1, this equation says exactly that the two vertex gauge values agree at every identified boundary vertex. They therefore glue to a unique gauge transformation on M2∪ΣM1. Conversely, every global gauge transformation restricts to such a compatible pair. Thus the restriction functor is fully faithful and, with step 2.1, an equivalence.

4.1givenF1F2F3algebra∎

The boundary isomorphism α is load-bearing. For the one-object groupoid BG of a finite group G, an object of the homotopy pullback of two identity functors is an element α∈G. By [F3], a morphism (u,v):α→α′ satisfies vα=α′u, so every α is isomorphic to 1 and the automorphisms of 1 are the diagonal pairs (u,u). Thus the homotopy pullback has one isomorphism class with automorphism group isomorphic to G and cardinality 1/∣G∣. The ordinary set-theoretic fiber product has one object with trivial automorphism group and cardinality 1. Omitting α therefore discards the stabilizer factor required by the gluing measure.

Gluing diagram

Write ri:CG(Mi)→CG(Σ) for restriction to the common boundary and resi for restriction from the glued manifold to Mi. The restriction square below commutes with the identity boundary isomorphism. It is a homotopy pullback: the comparison functor to CG(M2)×CG(Σ)hCG(M1), sending a global field to its two restrictions and their identity boundary isomorphism, is the equivalence proved by descent. The proof is independent of the drawing.

\mathcal C_G(M_2\cup_\Sigma M_1) \arrow[r,"\mathrm{res}_1"] \arrow[d,"\mathrm{res}_2"'] &
\mathcal C_G(M_1) \arrow[d,"r_1"] \\
\mathcal C_G(M_2) \arrow[r,"r_2"'] & \mathcal C_G(\Sigma)

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