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LemmaStatement: Literature-sourcedProof: AI-adaptedPipeline-generatedjudge pass (gpt-5.6-terra)audited 2026-09-22
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An invariant horizontal form on a free proper quotient descends uniquely

Statement

Assume ACω. Let a Lie group G act smoothly, freely and properly on a smooth manifold M with quotient map π:MM/G. A smooth k-form σ on M is the pullback σ=πσˉ of a smooth k-form on M/G if and only if

  • σ is G-invariant: agσ=σ for all gG, where ag(x)=gx; and
  • σ is horizontal: σx(v1,,vk)=0 whenever some vi is tangent to the orbit Gx; equivalently ιξMσ=0 for every fundamental field ξM.

The form σˉ is then unique.

Facts & Assumptions

Given: ACω, a smooth free proper action of G on M, the quotient map π, and a smooth k-form σ on M.

[A1]

ACω is countable choice; it is used only through the quotient and slice suppliers cited below.

[F1]

M/G is a smooth manifold and π is a smooth surjective submersion. Free proper action quotient manifold.

[F2]

kerdπx=Tx(Gx), and πag=π for all g. Tangent space of a free proper quotient, Free proper action quotient manifold.

[F3]

Every x has a slice S such that G×SGS is a diffeomorphism onto an open saturated neighbourhood and qS is a diffeomorphism onto its image. Local slice for a free proper action, Free proper action quotient manifold.

[F4]

A submersion admits smooth local sections, and a surjective submersion is a quotient map; a form on the base that pulls back to zero is zero because dπ is pointwise onto. The constant-rank theorem for manifolds, For a quotient map q:XY, a map out of Y is continuous iff its composite with q is; a continuous map on X constant on the fibres of q factors uniquely through q; and a composite of quotient maps is a quotient map.

Proof

technique · direct
1.1

The conditions are necessary. If σ=πσˉ, then agσ=agπσˉ=(πag)σˉ=πσˉ=σ by [F2], so σ is G-invariant. If v=ξM(x) is vertical, then dπxv=0 by [F2] and therefore σx(v,w2,,wk)=σˉπ(x)(0,dπw2,,dπwk)=0, so σ is horizontal.

F1F2
1.2

For the converse, fix x0M and let V:=π(GS) for a slice S through x0 from [F3]; V is open in M/G. For π(x)V and v1,,vkTπ(x)(M/G), choose lifts v~iTxM with dπxv~i=vi and set σˉπ(x)(v1,,vk):=σx(v~1,,v~k).

F1F3given
2.1

The prescription of step 1.2 does not depend on the lifts: two lifts of the same vi differ by an element of kerdπx=Tx(Gx) by [F2], and expanding multilinearly every resulting difference term contains a vertical entry, hence vanishes by horizontality.

step 1.2F2
2.2

It does not depend on the chosen point in the fibre: if x=hx and v~i are lifts at x, then d(ah)v~i are lifts of the same vi at x by [F2], and G-invariance of σ gives σx(d(ah)v~1,)=σx(v~1,).

step 1.2F2
3.1

Hence σˉ is well defined on all of M/G. It is smooth: near any point of M/G the submersion π admits a smooth local section s by [F4], and there σˉ=sσ because ds provides the lifts; the local definitions agree on overlaps since both pull back to σ, and forms on the base with equal pullback are equal by [F4].

step 2.1step 2.2F4
4.1

By construction πσˉ=σ. If σˉ is another such form, then π(σˉσˉ)=0, so σˉσˉ=0 by [F4]; the descended form is therefore unique.

step 3.1F4A1

Depends on

Used by

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Sources