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Circle gluing, curvature and connection variations

Statement

Let M be a smooth, Hausdorff, second-countable oriented four-manifold, and let (Ui,gij,ai;κ0) be a normalized circle-connection datum as in Local potentials and smooth circle-bundle connection data. Use the set-sized-object and quotient convention of Set-sized objects and definable-class schemas. Then the chart data construct a smooth Hausdorff second-countable right principal U(1)-bundle π:P→M and a global smooth real connection one-form ω on P. Its curvature is basic: there is a smooth closed two-form f∈Ω2(M) with dω=π∗f and f∣Ui=dai. The local potentials Ai=κ0ai satisfy dAi=F, where F=κ0f is global. For two connections on the same fixed bundle with the same transition functions, their local-form differences are restrictions of one global base one-form; adding a global one-form to all local representatives stays in that bundle sector.

Facts & Assumptions

Given: The smooth base, countable cover, circle cocycle, local real one-forms, fixed scale κ0>0, and the set-sized data stated above.

[F1]

Local potentials and smooth circle-bundle connection data: U(1) is the unit circle in R2 with the four explicit smooth charts and polynomial group operations stated there. Every smooth transition map has a smooth local real phase f with g=eif; any two such lifts differ by a locally constant element of 2πZ, and the complex-exponential derivative and chain rule give the real one-form identity λ(g):=−i g−1dg=df. The transitions obey gijgjk=gik, and the local forms obey aj=ai+λ(gij).

[F2]

Principal g bundle and associated fiber bundle: a right principal bundle is locally a product with equivariant charts, and the right group action is free and transitive on each fibre.

[F3]

Lorentzian exterior calculus and Hodge star: the exterior derivative satisfies d2=0 and the usual coordinate formula on smooth forms.

[F4]

Set-sized objects and definable-class schemas constructs the tagged union as a subset of I×M×U(1) and the equivalence-class quotient as a separated subset of its power set; no representatives are chosen.

Proof

1.1givenF1F4construct

Form the set-sized disjoint union ∐i(Ui×U(1)) and identify (x,zi) with (x,gij−1(x)zi) in chart j. Reflexivity follows from gii=1; the cocycle gives gji=gij−1 and shows that transfer from i to j to k equals direct transfer from i to k. Hence these identifications define an equivalence relation and a well-defined projection π:P→M.

2.1givenF1step 1.1algebra

For fixed i, the quotient map restricts to a bijection from Ui×U(1) onto π−1(Ui): every representative over x∈Ui transfers uniquely to chart i, and a transition loop acts as the identity by the cocycle. On overlaps the chart changes are (x,zi)↦(x,gij−1(x)zi), smooth diffeomorphisms with smooth inverse. The quotient map is open because the saturation of any open set is a union of its images under these overlap diffeomorphisms; therefore the bijections are homeomorphisms and form a smooth atlas.

3.1givenF1step 2.1algebra

Distinct base points have disjoint preimage neighborhoods because M is Hausdorff. For two distinct points over the same base point, choose a chart containing that base point and disjoint fibre neighborhoods in U(1); their products with a common base neighborhood separate the total-space points. Thus P is Hausdorff. Fix one countable base (Bn) of M and the explicit countable base (Cm) of circle arcs obtained by intersecting U(1)⊂R2 with rational open rectangles. In chart i, the products (Bn∩Ui)×Cm form a base. Their images under the open charts form a base of P indexed by the countable set I×N×N, which has an explicit finite-product enumeration. Thus P is second countable, without selecting separate bases for a countable family of spaces.

3.2F2step 2.1construct

Define the right action by [x,zi]⋅ζ=[x,ziζ]. It is well-defined because the chart transition is left multiplication by gij−1 and hence commutes with right multiplication. In each chart it is smooth; it is free and transitive on every fibre. The charts in step 2.1 are equivariant, so P→M satisfies the principal-bundle definition in [F2].

3.3F1F2step 2.1algebra

Let η=−iz−1dz be the real invariant one-form on U(1), normalized by η(∂θ)=1 for the local angle z=eiθ. In chart i set ωi=η+ai. If zj=gij−1zi, then ηj=ηi−λ(gij), while [F1] gives aj=ai+λ(gij); thus ωj=ωi on every overlap and the local forms define a global smooth one-form ω. Its value on the vertical generator is 1, it is right invariant, and in every chart ker⁡ωi is a complement to the vertical line, since for each base tangent vector there is a unique circle tangent vector cancelling ai. Hence ω is a principal connection.

4.1F1F3step 3.3algebra

In chart i, dω=dai because dη=0. On overlaps daj=dai+dλ(gij)=dai, since locally λ(gij)=dfij and d2fij=0 by [F3]. The forms dai therefore glue to a global two-form f, and the local identity dω=π∗f proves the curvature is basic and closed. Multiplication by the fixed constant κ0 gives Ai=κ0ai and F=κ0f with dAi=F.

5.1F1step 4.1algebra∎

If (ai′) is another compatible family for the same transition maps, then (aj′−aj)−(ai′−ai)=0 on each overlap. Thus the differences patch to a global one-form α on M. Conversely, adding any global one-form α to every ai preserves aj=ai+λ(gij) and changes curvature from f to f+dα without changing the transition data. This proves the fixed-bundle variation claim.

Remarks

The set-size convention is used for the tagged disjoint union and quotient. All seven typed foundational carriers now occur earlier on this page; their exact domains remain in force. The construction assumes no global real phase lift or bundle-classification theorem and makes no arbitrary choice of representatives or countable family of bases.

Depends on

Dependency tree · 2 levels

Sources