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Pfaffian groupoids Lie-Prolongations Spencer Operators Compatible S.O. Maurer-Cartan Pfaffian groupoids Mar a Amelia Salazar CRM, Barcelona December 10, 2013 Mar a Amelia Salazar Pfaffian groupoids Pfaffian groupoids


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Pfaffian groupoids Lie-Prolongations Spencer Operators Compatible S.O. Maurer-Cartan

Pfaffian groupoids

Mar´ ıa Amelia Salazar

CRM, Barcelona

December 10, 2013

Mar´ ıa Amelia Salazar Pfaffian groupoids

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Pfaffian groupoids Lie-Prolongations Spencer Operators Compatible S.O. Maurer-Cartan

Motivation

Understand the work of Cartan on Lie Pseudogroups, and the theory of PDE’s using the language of Lie groupoids and Lie algebroids.

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Definition of Pfaffian groupoid

Definition A Pfaffian groupoid (G, θ) consists of: G ⇒ M Lie groupoid, θ ∈ Ω1(G, t∗E) point-wise surjective, E → M ∈ Rep(G), with ker θ ∩ ker ds involutive,

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Definition of Pfaffian groupoid

Definition A Pfaffian groupoid (G, θ) consists of: G ⇒ M Lie groupoid, θ ∈ Ω1(G, t∗E) point-wise surjective, E → M ∈ Rep(G), with ker θ ∩ ker ds involutive, with the property that θ is multiplicative: m∗θ(g,h) = g · pr∗

1 θ(g,h) + pr∗ 2 θ(g,h),

m, pr1, pr2 : G2 ⊂ G × G → G.

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Pfaffian groupoids Lie-Prolongations Spencer Operators Compatible S.O. Maurer-Cartan

Examples

Example (Rotations on the plane) For the standard action of S1 on R2 by rotations, we have the action groupoid over R2 G := S1 ⋉ R2, s(α, z) = z, t(α, z) = α · z, and θ = dα ∈ Ω1(G).

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Examples

Example (Rotations on the plane) For the standard action of S1 on R2 by rotations, we have the action groupoid over R2 G := S1 ⋉ R2, s(α, z) = z, t(α, z) = α · z, and θ = dα ∈ Ω1(G). A bisection β of G (i.e. β : R2 → G, s ◦ β = id and t ◦ β-diffeo) belongs to Sol(G, θ) = {β | β∗θ = 0} iff α : R2 → S1 is constant. Diff(R2) ⊃ Γnaive = t ◦ Sol(G, θ) = {rotations of the plane}

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Pfaffian groupoids Lie-Prolongations Spencer Operators Compatible S.O. Maurer-Cartan

Examples

Example (Jet groupoids and the Cartan form) For M a manifold, consider the pair groupoid M × M ⇒ M.

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Examples

Example (Jet groupoids and the Cartan form) For M a manifold, consider the pair groupoid M × M ⇒ M. G = J1(M × M) = { first jets of local diffeos (= bisections)}. The Cartan form θ1 ∈ Ω1(G; t∗TM) at X ∈ Tj1

x φJ1(M × M) is:

dpr1(X) − dxφ(dpr2(X)).

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Examples

Example (Jet groupoids and the Cartan form) For M a manifold, consider the pair groupoid M × M ⇒ M. G = J1(M × M) = { first jets of local diffeos (= bisections)}. The Cartan form θ1 ∈ Ω1(G; t∗TM) at X ∈ Tj1

x φJ1(M × M) is:

dpr1(X) − dxφ(dpr2(X)). Sol(G, θ1) = {β : M → J1(M × M) | β = j1f , f a local diffeo} correspond to VB-iso F : TM → TM over f s.t Fx = dxf .

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Definition of Lie-Prolongation

Definition Let (G, θ) be a Pfaffian groupoid. A Lie-prolongation of (G, θ) is a Pfaffian groupoid (G′, θ′) together with a Lie groupoid morphism p : (G′, θ′) → (G, θ), p surjective

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Pfaffian groupoids Lie-Prolongations Spencer Operators Compatible S.O. Maurer-Cartan

Definition of Lie-Prolongation

Definition Let (G, θ) be a Pfaffian groupoid. A Lie-prolongation of (G, θ) is a Pfaffian groupoid (G′, θ′) together with a Lie groupoid morphism p : (G′, θ′) → (G, θ), p surjective satisfying: θ′ takes values in the Lie algebroid A of G, and it is of Lie-type: ker θ′ ∩ ker ds′ = ker θ′ ∩ ker dt′,

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Pfaffian groupoids Lie-Prolongations Spencer Operators Compatible S.O. Maurer-Cartan

Definition of Lie-Prolongation

Definition Let (G, θ) be a Pfaffian groupoid. A Lie-prolongation of (G, θ) is a Pfaffian groupoid (G′, θ′) together with a Lie groupoid morphism p : (G′, θ′) → (G, θ), p surjective satisfying: θ′ takes values in the Lie algebroid A of G, and it is of Lie-type: ker θ′ ∩ ker ds′ = ker θ′ ∩ ker dt′, Lie(p) = θ′|A′, A′ = Lie(G′),

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Definition of Lie-Prolongation

Definition Let (G, θ) be a Pfaffian groupoid. A Lie-prolongation of (G, θ) is a Pfaffian groupoid (G′, θ′) together with a Lie groupoid morphism p : (G′, θ′) → (G, θ), p surjective satisfying: θ′ takes values in the Lie algebroid A of G, and it is of Lie-type: ker θ′ ∩ ker ds′ = ker θ′ ∩ ker dt′, Lie(p) = θ′|A′, A′ = Lie(G′), dp(ker θ′) ⊂ ker θ, for X, Y ∈ ker θ′, δθ(dp(X), dp(Y )) = 0,

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Definition of the Classical Lie-prolongation

Definition The classical Lie-prolongation space P(G, θ) of (G, θ) consists of j1

x β ∈ J1G with the property that for any X, Y ∈ TxM

θ(dxβ(X)) = 0 and δθ(dxβ(X), dxβ(Y )) = 0.

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Definition of the Classical Lie-prolongation

Definition The classical Lie-prolongation space P(G, θ) of (G, θ) consists of j1

x β ∈ J1G with the property that for any X, Y ∈ TxM

θ(dxβ(X)) = 0 and δθ(dxβ(X), dxβ(Y )) = 0. Proposition Whenever P(G, θ) ⊂ J1G smooth and pr : P(G, θ) → G is a submersion, (P(G, θ), θ(1) = θ1|P(G,θ)) is a Lie-prolongation of (G, θ).

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Examples

Example (Rotations on the plane) For G = S1 ⋉ R2, a bisection β : R2 → G is of the form β = (α, id), with (x, y) → α · (x, y) a diffeo.

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Pfaffian groupoids Lie-Prolongations Spencer Operators Compatible S.O. Maurer-Cartan

Examples

Example (Rotations on the plane) For G = S1 ⋉ R2, a bisection β : R2 → G is of the form β = (α, id), with (x, y) → α · (x, y) a diffeo. For θ = dα, P(G, θ) = {j1

(x,y)β | ∂α

∂x |(x,y) = ∂α ∂y |(x,y) = 0}

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Pfaffian groupoids Lie-Prolongations Spencer Operators Compatible S.O. Maurer-Cartan

Examples

Example (Rotations on the plane) For G = S1 ⋉ R2, a bisection β : R2 → G is of the form β = (α, id), with (x, y) → α · (x, y) a diffeo. For θ = dα, P(G, θ) = {j1

(x,y)β | ∂α

∂x |(x,y) = ∂α ∂y |(x,y) = 0} Example (Jet groupoid and the Cartan form) For J1(M × M) and the Cartan form θ1, P(J1(M × M), θ1) = J2(M × M), and (θ1)(1) = θ2, where J2(M × M) is the second jets of local diffeos, and θ2 is the Cartan form.

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Definition of Spencer operator

Definition Let A → M be a Lie algebroid and let E ∈ Rep(A) with associated connection denoted by ∇.

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Definition of Spencer operator

Definition Let A → M be a Lie algebroid and let E ∈ Rep(A) with associated connection denoted by ∇. A Spencer operator is a bilinear operator D : X(M) × Γ(A) → Γ(E), (X, α) → DX(α) together with a surjective V.B-map l : A → E, which is C ∞(M)-linear in X, satisfies the Leibniz identity relative to l: DX(f α) = fDX(α) + LX(f )l(α),

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Definition of Spencer operator

Definition Let A → M be a Lie algebroid and let E ∈ Rep(A) with associated connection denoted by ∇. A Spencer operator is a bilinear operator D : X(M) × Γ(A) → Γ(E), (X, α) → DX(α) together with a surjective V.B-map l : A → E, which is C ∞(M)-linear in X, satisfies the Leibniz identity relative to l: DX(f α) = fDX(α) + LX(f )l(α), and the following two compatibility conditions: Dρ(α)(α′) = ∇α′(l(α)) + l([α, α′]) DX[α, α′] = ∇α(DXα′)−D[ρ(α),X]α′−∇α′(DXα)+D[ρ(α′),X]α.

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Integrability result for Pfaffian groupoids

Theorem Let E ∈ Rep(G) and A = Lie(G). Then any multiplicative form θ ∈ Ω1(G, t∗E), making (G, θ) Pfaffian, induces a Spencer operator

  • n A with coefficient on E, given by

DX(α) = “Lαr θ(X)′′, and l(α) = θ(α), with the property that ker l ⊂ A is a Lie subalgebroid.

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Integrability result for Pfaffian groupoids

Theorem Let E ∈ Rep(G) and A = Lie(G). Then any multiplicative form θ ∈ Ω1(G, t∗E), making (G, θ) Pfaffian, induces a Spencer operator

  • n A with coefficient on E, given by

DX(α) = “Lαr θ(X)′′, and l(α) = θ(α), with the property that ker l ⊂ A is a Lie subalgebroid. If G is source simply connected, then this construction defines a 1-1 correspondence.

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Examples

Example (Rotations on the plane) The infinitesimal action of S1 R2 is defined by a : R → X(R2), 1 → a(1)(x,y) = x ∂

∂y − y ∂ ∂x .

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Examples

Example (Rotations on the plane) The infinitesimal action of S1 R2 is defined by a : R → X(R2), 1 → a(1)(x,y) = x ∂

∂y − y ∂ ∂x .The induced action

algebroid is Lie(S1 ⋉ R2) = R ⋉ R2.

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Examples

Example (Rotations on the plane) The infinitesimal action of S1 R2 is defined by a : R → X(R2), 1 → a(1)(x,y) = x ∂

∂y − y ∂ ∂x .The induced action

algebroid is Lie(S1 ⋉ R2) = R ⋉ R2. The associated Spencer operator D : R2 × Γ(R ⋉ R2) → C ∞(R2), l : R ⋉ R2 → R × R2 of dα ∈ Ω1(S1 ⋉ R2) is then l(r) = r, and DX(f ) = fdf (X).

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Examples

Example (Jet algebroids and the classical Spencer Operator) For a V.B A → M, one has a decomposition of vector spaces Γ(J1A) ≃ Γ(A) ⊕ Ω1(M, A), coming from the exact sequence 0 → T ∗M ⊗ A → J1A

pr

→ A → 0.

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Examples

Example (Jet algebroids and the classical Spencer Operator) For a V.B A → M, one has a decomposition of vector spaces Γ(J1A) ≃ Γ(A) ⊕ Ω1(M, A), coming from the exact sequence 0 → T ∗M ⊗ A → J1A

pr

→ A → 0. The classical Spencer operator Dclas : Γ(J1A) → Ω1(M, A), l = pr : J1A → A is the projection to the 2nd component.

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Examples

Example (Jet algebroids and the classical Spencer Operator) For a V.B A → M, one has a decomposition of vector spaces Γ(J1A) ≃ Γ(A) ⊕ Ω1(M, A), coming from the exact sequence 0 → T ∗M ⊗ A → J1A

pr

→ A → 0. The classical Spencer operator Dclas : Γ(J1A) → Ω1(M, A), l = pr : J1A → A is the projection to the 2nd component. If A is a Lie algebroid Dclas is a Spencer Operator, if A = Lie(G), Dclas is the Spencer Operator of the Cartan form θ1 ∈ Ω1(G, t∗A).

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Definition of compatible Spencer Operators

Definition Let ˜ D : X(M) × Γ(A′) → Γ(A), D : X(M) × Γ(A) → Γ(E) ˜ l : A′ → A l : A → E be two Spencer Operators. (D′, D) are compatible if

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Definition of compatible Spencer Operators

Definition Let ˜ D : X(M) × Γ(A′) → Γ(A), D : X(M) × Γ(A) → Γ(E) ˜ l : A′ → A l : A → E be two Spencer Operators. (D′, D) are compatible if D ◦˜ l − l ◦ ˜ D = 0 DX ˜ DY − DY ˜ DX − l ◦ ˜ D[X,Y ] = 0

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Definition of compatible Spencer Operators

Definition Let ˜ D : X(M) × Γ(A′) → Γ(A), D : X(M) × Γ(A) → Γ(E) ˜ l : A′ → A l : A → E be two Spencer Operators. (D′, D) are compatible if D ◦˜ l − l ◦ ˜ D = 0 DX ˜ DY − DY ˜ DX − l ◦ ˜ D[X,Y ] = 0 l′ is a Lie algebroid map.

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Definition of the classical Lie prolongation

Definition The classical Lie prolongation space PD(A) of D : X × Γ(A) → Γ(E), l : A → E, consists of elements (α, ω)x ∈ J1A with the property that for any X, Y ∈ X(M), D(α)(x) = l(ωx) DX(ω(Y ))(x) − DY (ω(X))(x) − l ◦ ω[X, Y ]x = 0.

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Proposition Whenever PD(A) smooth and pr : PD(A) → A surjective, (PD(A), D(1) = Dclas|PD(A)) is compatible with D.

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Proposition Whenever PD(A) smooth and pr : PD(A) → A surjective, (PD(A), D(1) = Dclas|PD(A)) is compatible with D. If D is the Spencer operator of (G, θ), then P(G, θ) is smooth iff PD(A) is smooth, and Lie(P(G, θ)) = PD(A).

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Integrability result for Lie-Prolongations

Theorem Let G′ be Lie groupoid, and (G, θ) a Pfaffian groupoid, and let D : X(M) × Γ(A) → Γ(E) be the Spencer Operator of (G, θ).

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Integrability result for Lie-Prolongations

Theorem Let G′ be Lie groupoid, and (G, θ) a Pfaffian groupoid, and let D : X(M) × Γ(A) → Γ(E) be the Spencer Operator of (G, θ). If G′ is s-simply connected and G s-connected, then there is a 1-1 correspondence Lie prolongations p : (G′, θ′) → (G, θ), and Spencer operators D : X(M) × Γ(A′) → Γ(A) compatible with D. In this correspondence D′ is the Spencer Operator of θ′.

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Maurer-Cartan equation

Out of D : X(M) × Γ(A) → Γ(E), one has an antysimmetric bilinear map {·, ·}D : A × A → E, 1 2{α, β}D = Dρ(α)(β) − Dρ(β)(α) − l[α, β]

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Maurer-Cartan equation

Out of D : X(M) × Γ(A) → Γ(E), one has an antysimmetric bilinear map {·, ·}D : A × A → E, 1 2{α, β}D = Dρ(α)(β) − Dρ(β)(α) − l[α, β] and a differential operator dD : Ω1(G′, t∗A) → Ω2(G′, t∗E), dDθ′(X, Y ) = Dt

X(θ′(Y )) − Dt Y (θ′(X)) − l(θ′[X, Y ]), where Dt is

the pullback of D via t : G′ → M.

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Maurer-Cartan equation

Out of D : X(M) × Γ(A) → Γ(E), one has an antysimmetric bilinear map {·, ·}D : A × A → E, 1 2{α, β}D = Dρ(α)(β) − Dρ(β)(α) − l[α, β] and a differential operator dD : Ω1(G′, t∗A) → Ω2(G′, t∗E), dDθ′(X, Y ) = Dt

X(θ′(Y )) − Dt Y (θ′(X)) − l(θ′[X, Y ]), where Dt is

the pullback of D via t : G′ → M. MC(θ′, θ) := dDθ′ − 1 2{θ′, θ′}D.

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Lie Prolongations and MC

Theorem If p : (G′, θ′) → (G, θ) is a Lie Prolongation then MC(θ′, θ) = 0.

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Lie Prolongations and MC

Theorem If p : (G′, θ′) → (G, θ) is a Lie Prolongation then MC(θ′, θ) = 0. If G′ is s-connected and p is a submersion with Lie(p) = θ′|A′, then the converse also holds.

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Thank you

Thank you for your attention.

Mar´ ıa Amelia Salazar Pfaffian groupoids