Alphabeta Math
PropositionStatement: AI-adaptedProof: AI-adaptedPipeline-generatedjudge pass (gpt-5.6-terra)audited 2026-09-07
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Orientation identifies top forms with signed densities

Statement

A chosen orientation on Mn determines a smooth real-linear bundle isomorphism from top forms to signed densities. In a signed chart it is Jo(fdx1dxn)=σϕfdx. For n=0 it sends f(p) to ε(p)f(p). It preserves support and, assuming ACω, preserves the integral for compact support. Reversing orientation negates Jo.

Facts & Assumptions

[F1]

Orientation-free density integration and its properties: Compactly supported smooth density integration is independent of charts and partition, linear, local, nonnegative on nonnegative densities and strictly positive for a nonzero nonnegative density. It is invariant under every diffeomorphism, without choosing an orientation. The finite-parametrization formula holds under the hypotheses of prop-integration-of-top-forms-by-finite-parametrizations, with orientation preservation omitted and absolute Jacobians used.

[F2]

Integral of a compactly supported top form: Assume ACω. For an oriented smooth manifold Mn, possibly with boundary, and ωΩcn(M), choose a smooth partition (ρi) subordinate to connected interior or boundary charts (Ui,ϕi). For n1 set Mω=iIϕi(ρiω). Each product has compact support in its chart and only finitely many are nonzero, by lem-a-locally-finite-sum-is-finite-near-the-compact-support-of-a-form. For n=0 set Mω=psuppωε(p)ω(p). Λ0TpMR has two orientations; define ε(p)=+1 when 1 is positive in the chosen orientation and ε(p)=1 when 1 is positive. A zero-manifold is discrete; the singleton open cover of a compact subset has a finite subcover. Thus this sum too is finite. Empty support or empty M gives zero. Independence of the choices is discharged by thm-global-form-integration-is-independent-of-the-atlas-partition-and-refinement.

Proof

Given: The objects and hypotheses in the statement above.

1.1

On a coordinate overlap with transition G, fx=(fyG)detDG and σxsgndetDG=σy. Therefore σxfx=(σyfy)GdetDG, exactly the density gluing law. Local multiplication by σx is smooth, linear, and invertible with inverse the same sign.

F1F2
2.1

The coefficient vanishes exactly when its image does, so the support is unchanged. Under ACω, each weighted density integral equals its signed form chart integral, and the finite sums agree. In zero dimension the same equality is the signed scalar formula. Changing the orientation changes all signs and hence negates the map, including at a single point or on the zero form.

F1F2step 1.1

Depends on

Used by

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Sources