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TauCeti.Analysis.Calculus.DifferentialForm.Invariant

The Poincaré lemma for differential forms invariant under a linear action #

Let a group G act on a real normed space E through a continuous representation ρ, and let s ⊆ E be a ρ-invariant set. A differential k-form ω on E is invariant on s when (ρ g)^* ω = ω at every point of s, that is ω (ρ g x) (ρ g v₁, …, ρ g vₖ) = ω x (v₁, …, vₖ) for all g and all x ∈ s.

Pullback along a continuous linear map A intertwines the Poincaré homotopy operators centred at y₀ and at A y₀ (TauCeti.poincareHomotopy_pullback_apply). Hence the operator K centred at a point x₀ fixed by A sends A-invariant forms on a set star-convex with respect to x₀ to A-invariant forms (StarConvex.compContinuousLinearMap_poincareHomotopy_eq). When G is finite, a nonempty invariant convex set always contains a point fixed by G: the average |G|⁻¹ ∑ g, ρ g x of the orbit of any of its points (Convex.averageMap_mem). Centred there, the homotopy formula d K + K d = id restricts to invariant forms, so a closed invariant form of positive degree on an invariant convex set is the exterior derivative of an invariant form of the same regularity (Convex.exists_invariant_contDiffOn_forall_extDerivWithin_eq). The same holds on an invariant open set star-convex with respect to a fixed point (StarConvex.exists_invariant_contDiffOn_forall_extDeriv_eq), for any monoid.

This is the vanishing of the positive-degree cohomology of invariant forms on the linear local model of an orbifold: by Bochner linearization, a point with finite isotropy group G has a chart onto a G-invariant ball on which G acts linearly, possibly with a nontrivial kernel. No faithfulness of ρ is assumed, and every element of G, including those acting trivially, is taken into account in the average.

Main declarations #

References #

theorem StarConvex.exists_invariant_contDiffOn_forall_extDeriv_eq {E : Type u_1} {F : Type u_2} [NormedAddCommGroup E] [NormedSpace ℝ E] [NormedAddCommGroup F] [NormedSpace ℝ F] [CompleteSpace F] {n : ℕ} {x₀ : E} {s : Set E} {ω : E → E [⋀^Fin (n + 1)]→L[ℝ] F} {G : Type u_3} [Monoid G] {ρ : ContRepresentation ℝ G E} (hs : StarConvex ℝ x₀ s) (hso : IsOpen s) (hρx₀ : ∀ (g : G), (ρ g) x₀ = x₀) (hρs : ∀ (g : G), Set.MapsTo (⇑(ρ g)) s s) {r : ℕ∞} (hr : 1 ≤ r) (hωr : ContDiffOn ℝ (↑r) ω s) (hclosed : ∀ y ∈ s, extDeriv ω y = 0) (hω : ∀ (g : G), ∀ y ∈ s, (ω ((ρ g) y)).compContinuousLinearMap (ρ g) = ω y) :
∃ (α : E → E [⋀^Fin n]→L[ℝ] F), ContDiffOn ℝ (↑r) α s ∧ α x₀ = 0 ∧ (∀ (g : G), ∀ y ∈ s, (α ((ρ g) y)).compContinuousLinearMap (ρ g) = α y) ∧ ∀ y ∈ s, extDeriv α y = ω y

The Poincaré lemma for invariant forms. Let a monoid G act on E through a continuous representation ρ, fixing x₀ and preserving an open set s star-convex with respect to x₀. A closed C^r form of positive degree on s, r ≥ 1, invariant under every ρ g on s, is the exterior derivative on s of an invariant C^r form vanishing at x₀.

theorem Convex.exists_invariant_contDiffOn_forall_extDerivWithin_eq {E : Type u_1} {F : Type u_2} [NormedAddCommGroup E] [NormedSpace ℝ E] [NormedAddCommGroup F] [NormedSpace ℝ F] [CompleteSpace F] {n : ℕ} {G : Type u_3} [Group G] [Finite G] {ρ : ContRepresentation ℝ G E} {s : Set E} {ω : E → E [⋀^Fin (n + 1)]→L[ℝ] F} (hs : Convex ℝ s) (hsu : UniqueDiffOn ℝ s) (hsne : s.Nonempty) (hρs : ∀ (g : G), Set.MapsTo (⇑(ρ g)) s s) {r : ℕ∞} (hr : 1 ≤ r) (hωr : ContDiffOn ℝ (↑r) ω s) (hclosed : ∀ y ∈ s, extDerivWithin ω s y = 0) (hω : ∀ (g : G), ∀ y ∈ s, (ω ((ρ g) y)).compContinuousLinearMap (ρ g) = ω y) :
∃ (α : E → E [⋀^Fin n]→L[ℝ] F), ContDiffOn ℝ (↑r) α s ∧ (∀ (g : G), ∀ y ∈ s, (α ((ρ g) y)).compContinuousLinearMap (ρ g) = α y) ∧ ∀ y ∈ s, extDerivWithin α s y = ω y

The Poincaré lemma for forms invariant under a finite group. Let a finite group G act on E through a continuous representation ρ preserving a nonempty convex set s with unique derivatives, which need not be open. A C^r form of positive degree, r ≥ 1, closed within s and invariant under every ρ g on s, is the exterior derivative within s of an invariant C^r form. The primitive is the Poincaré homotopy operator centred at the average of an orbit in s, a point fixed by G.