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Cartan identity for a one-form annihilating a vector field

Proved
ContactCalculus.lie_derivative_eq_exterior_of_annihilation

by Mazecto · Oct 6, 2026 · Mathlib 0df444a (Lean v4.33.1)

analysiscontact-geometrydifferential-geometry

Let VVV be a real normed vector space, let η:V→V∗\eta:V\to V^*η:V→V∗ be a differentiable one-form, and let X:V→VX:V\to VX:V→V be a differentiable vector field. Suppose ηy(X(y))=0\eta_y(X(y))=0ηy​(X(y))=0 at every point. For every y,v∈Vy,v\in Vy,v∈V,

Dη(y)[X(y)](v)+ηy(DX(y)[v])=Dη(y)[X(y)](v)−Dη(y)[v](X(y)).D\eta(y)[X(y)](v)+\eta_y(DX(y)[v])=D\eta(y)[X(y)](v)-D\eta(y)[v](X(y)).Dη(y)[X(y)](v)+ηy​(DX(y)[v])=Dη(y)[X(y)](v)−Dη(y)[v](X(y)).

Equivalently, LXη=iXdη\mathcal L_X\eta=i_Xd\etaLX​η=iX​dη. Here V∗V^*V∗ is the continuous real dual. This is the annihilation case of Cartan's formula used in the contact Moser equation. The annihilation hypothesis holds on the whole ambient space, so its derivative in every direction is zero.

Preamble
import Mathlib.Analysis.Calculus.FDeriv.Basic
Formal statement
theorem ContactCalculus.lie_derivative_eq_exterior_of_annihilation {V : Type*} [NormedAddCommGroup V] [NormedSpace ℝ V]
    (η : V → (V →L[ℝ] ℝ)) (X : V → V)
    (hη : Differentiable ℝ η) (hX : Differentiable ℝ X)
    (hz : ∀ y, η y (X y) = 0) (y v : V) :
    fderiv ℝ η y (X y) v + η y (fderiv ℝ X y v) =
      fderiv ℝ η y (X y) v - fderiv ℝ η y v (X y) := by sorry
Source
Geiges, Contact geometry, https://arxiv.org/abs/math/0307242, proof of Theorem 2.20, printed p. 15: Cartan formula and the choice X_t in ker α_t before equation (2.1). Ambient normed-space generalization under global annihilation; only first differentiability is used.

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