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Gray stability (Theorem 2.20): contact structures on closed manifolds have no deformations

Proved
GrayStability.gray_stability

by Mazecto · Oct 5, 2026 · Mathlib 0df444a (Lean v4.33.1)

contact-geometrydifferential-geometrysymplectic-geometry

Let F:Rn→RcF:\mathbb{R}^n\to\mathbb{R}^cF:Rn→Rc be smooth with M=F−1(0)M=F^{-1}(0)M=F−1(0) compact and DFDFDF surjective along MMM, and let αt\alpha_tαt​, t∈[0,1]t\in[0,1]t∈[0,1], be a smooth family of contact forms on MMM, with contact structures ξt=ker⁡αt\xi_t=\ker\alpha_tξt​=kerαt​. Then there is an isotopy ψt\psi_tψt​ of MMM such that

Tψt(ξ0)=ξtfor each t∈[0,1],T\psi_t(\xi_0)=\xi_t\qquad\text{for each } t\in[0,1],Tψt​(ξ0​)=ξt​for each t∈[0,1],

that is, for every y∈My\in My∈M and v∈TyMv\in T_yMv∈Ty​M: α0(v)=0\alpha_0(v)=0α0​(v)=0 if and only if αt(Dψt(y)v)=0\alpha_t(D\psi_t(y)v)=0αt​(Dψt​(y)v)=0.

Gray's theorem says that contact structures on closed manifolds have discrete moduli: a smooth deformation of a contact structure is induced by an isotopy.

Formalization Note Geiges states the theorem on an abstract closed manifold. Here MMM is a compact regular level set in Rn\mathbb{R}^nRn, a special case covering every closed manifold with trivial normal bundle in some Rn\mathbb{R}^nRn (all spheres, all star-shaped hypersurfaces). Contact structures are cooriented, given by the global forms αt\alpha_tαt​, as in Geiges' standing assumption.

Preamble
import Definitions.Def_GrayStability_Basic
Formal statement
namespace GrayStability

/-- Gray stability (Geiges, Theorem 2.20): for a smooth family of contact structures
`ξ_t = ker α_t`, `t ∈ [0, 1]`, on a closed submanifold `M ⊂ ℝⁿ` there is an isotopy
`ψ_t` of `M` with `Tψ_t(ξ_0) = ξ_t`. -/
theorem gray_stability {n c : ℕ} (F : E n → (Fin c → ℝ))
    (hF : IsCompactRegularLevel F) (α : ℝ → OneForm n) (hα : IsContactFamilyOn F α) :
    ∃ ψ : ℝ → E n → E n, IsIsotopyOf F ψ ∧
      ∀ t ∈ Set.Icc (0 : ℝ) 1, ∀ y ∈ levelSet F, ∀ v ∈ tangentSpace F y,
        (α 0 y v = 0 ↔ pullback (ψ t) (α t) y v = 0) := by sorry

end GrayStability
Source
Geiges, Contact geometry, Handbook of Differential Geometry Vol. II (2006) 315-382, https://arxiv.org/abs/math/0307242, Theorem 2.20, p. 14
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What the Lean code literally says, in plain math · claude-opus-5-5

Read-back: gray_stability

Statement. For all natural numbers n,cn, cn,c, every map F:Rn→RcF : \mathbb{R}^n \to \mathbb{R}^cF:Rn→Rc, and every map t↦αtt \mapsto \alpha_tt↦αt​ from R\mathbb{R}R to one-forms on Rn\mathbb{R}^nRn: if

  • (hypothesis on FFF) FFF is a compact regular level, i.e. F∈C∞F \in C^\inftyF∈C∞, M=F−1(0)M = F^{-1}(0)M=F−1(0) is compact, and DF(y)DF(y)DF(y) is surjective for all y∈My \in My∈M; and
  • (hypothesis on α\alphaα) α\alphaα is a contact family on MMM, i.e. (t,y)↦αt(y)(t,y) \mapsto \alpha_t(y)(t,y)↦αt​(y) is C∞C^\inftyC∞ on R×Rn\mathbb{R} \times \mathbb{R}^nR×Rn and αt\alpha_tαt​ is contact at yyy for all t∈[0,1]t \in [0,1]t∈[0,1] and all y∈My \in My∈M,

then there exists ψ:R×Rn→Rn\psi : \mathbb{R} \times \mathbb{R}^n \to \mathbb{R}^nψ:R×Rn→Rn which is an isotopy of MMM (definition below) such that for every t∈[0,1]t \in [0,1]t∈[0,1], every y∈My \in My∈M and every v∈Ty=ker⁡DF(y)v \in T_y = \ker DF(y)v∈Ty​=kerDF(y),

α0(y)(v)=0  ⟺  αt(ψt(y))(Dψt(y) v)=0.\alpha_0(y)(v) = 0 \iff \alpha_t\big(\psi_t(y)\big)\big(D\psi_t(y)\,v\big) = 0 .α0​(y)(v)=0⟺αt​(ψt​(y))(Dψt​(y)v)=0.

That is, for t∈[0,1]t \in [0,1]t∈[0,1] and y∈My \in My∈M, the vectors of TyT_yTy​ annihilated by α0(y)\alpha_0(y)α0​(y) are exactly those annihilated by the pullback (ψt∗αt)y(\psi_t^*\alpha_t)_y(ψt∗​αt​)y​. The conclusion is only this equality of zero sets inside TyT_yTy​; it does not assert any proportionality factor, sign or positivity relation between α0\alpha_0α0​ and ψt∗αt\psi_t^*\alpha_tψt∗​αt​, nor anything for t∉[0,1]t \notin [0,1]t∈/[0,1] or y∉My \notin My∈/M. The isotopy is required to satisfy ψ0=id\psi_0 = \mathrm{id}ψ0​=id only on MMM.

Setting and unfolded definitions. Throughout, n,c∈Nn, c \in \mathbb{N}n,c∈N are arbitrary natural numbers (both may be 000), and Rn\mathbb{R}^nRn means the space of functions {0,…,n−1}→R\{0,\dots,n-1\} \to \mathbb{R}{0,…,n−1}→R with the sup norm. A one-form α\alphaα is any map Rn→(Rn)∗\mathbb{R}^n \to (\mathbb{R}^n)^*Rn→(Rn)∗, y↦αyy \mapsto \alpha_yy↦αy​ (a continuous linear functional at each point; no regularity is built in). Derivatives DDD are Fréchet derivatives of maps on the ambient space Rn\mathbb{R}^nRn (or R×Rn\mathbb{R} \times \mathbb{R}^nR×Rn), with the convention that a derivative is 000 at any point where the map is not differentiable. For F:Rn→RcF : \mathbb{R}^n \to \mathbb{R}^cF:Rn→Rc and a one-form α\alphaα:

  • Level set: M:=F−1(0)={y∈Rn:F(y)=0}M := F^{-1}(0) = \{ y \in \mathbb{R}^n : F(y) = 0 \}M:=F−1(0)={y∈Rn:F(y)=0}.

  • Compact regular level (hypothesis on FFF): FFF is C∞C^\inftyC∞ on all of Rn\mathbb{R}^nRn, MMM is compact, and for every y∈My \in My∈M the derivative DF(y):Rn→RcDF(y) : \mathbb{R}^n \to \mathbb{R}^cDF(y):Rn→Rc is surjective.

  • Tangent space: Ty:=ker⁡DF(y)={v∈Rn:DF(y) v=0}T_y := \ker DF(y) = \{ v \in \mathbb{R}^n : DF(y)\,v = 0 \}Ty​:=kerDF(y)={v∈Rn:DF(y)v=0} (defined for every yyy, used only for y∈My \in My∈M).

  • Exterior derivative: dαy(u,v):=(Dα(y) u)(v)−(Dα(y) v)(u)d\alpha_y(u,v) := \big(D\alpha(y)\,u\big)(v) - \big(D\alpha(y)\,v\big)(u)dαy​(u,v):=(Dα(y)u)(v)−(Dα(y)v)(u), where Dα(y):Rn→(Rn)∗D\alpha(y) : \mathbb{R}^n \to (\mathbb{R}^n)^*Dα(y):Rn→(Rn)∗ is the ambient derivative of y↦αyy \mapsto \alpha_yy↦αy​ (equal to 000 if α\alphaα is not differentiable at yyy).

  • Contact plane: ξy:={v∈Ty:αy(v)=0}\xi_y := \{ v \in T_y : \alpha_y(v) = 0 \}ξy​:={v∈Ty​:αy​(v)=0}.

  • Contact at yyy: (i) there exists v∈Tyv \in T_yv∈Ty​ with αy(v)≠0\alpha_y(v) \neq 0αy​(v)=0, and (ii) for every u∈ξyu \in \xi_yu∈ξy​ with u≠0u \neq 0u=0 there exists v∈ξyv \in \xi_yv∈ξy​ with dαy(u,v)≠0d\alpha_y(u,v) \neq 0dαy​(u,v)=0 (i.e. dαyd\alpha_ydαy​ restricted to ξy×ξy\xi_y \times \xi_yξy​×ξy​ is nondegenerate; condition (ii) is vacuous when ξy={0}\xi_y = \{0\}ξy​={0}). No orientation, sign, or dimension-parity condition is imposed explicitly.

  • Smooth family: a map t↦αtt \mapsto \alpha_tt↦αt​ from R\mathbb{R}R to one-forms such that (t,y)↦αt(y)∈(Rn)∗(t,y) \mapsto \alpha_t(y) \in (\mathbb{R}^n)^*(t,y)↦αt​(y)∈(Rn)∗ is C∞C^\inftyC∞ on all of R×Rn\mathbb{R} \times \mathbb{R}^nR×Rn.

  • Contact family on MMM (hypothesis on α\alphaα): α\alphaα is a smooth family, and for every t∈[0,1]t \in [0,1]t∈[0,1] and every y∈My \in My∈M, αt\alpha_tαt​ is contact at yyy in the above sense. Nothing is required of αt\alpha_tαt​ for t∉[0,1]t \notin [0,1]t∈/[0,1] beyond smoothness, nor off MMM beyond smoothness.

  • Isotopy of MMM: a map ψ:R×Rn→Rn\psi : \mathbb{R} \times \mathbb{R}^n \to \mathbb{R}^nψ:R×Rn→Rn, (t,y)↦ψt(y)(t,y) \mapsto \psi_t(y)(t,y)↦ψt​(y), such that

    1. (t,y)↦ψt(y)(t,y) \mapsto \psi_t(y)(t,y)↦ψt​(y) is C∞C^\inftyC∞ on all of R×Rn\mathbb{R} \times \mathbb{R}^nR×Rn;
    2. ψ0(y)=y\psi_0(y) = yψ0​(y)=y for every y∈My \in My∈M (only on MMM, not on all of Rn\mathbb{R}^nRn);
    3. for every t∈[0,1]t \in [0,1]t∈[0,1]: ψt\psi_tψt​ maps MMM into MMM, is injective on MMM, and maps MMM onto MMM; and for every y∈My \in My∈M, the linear map Dψt(y)D\psi_t(y)Dψt​(y) is injective on TyT_yTy​.

    Nothing is required of ψt\psi_tψt​ for t∉[0,1]t \notin [0,1]t∈/[0,1] other than smoothness, and nothing off MMM other than smoothness. The definition does not state separately that Dψt(y)D\psi_t(y)Dψt​(y) maps TyT_yTy​ into Tψt(y)T_{\psi_t(y)}Tψt​(y)​.

  • Pullback: (ψt∗αt)y(v):=αt(ψt(y))(Dψt(y) v)(\psi_t^*\alpha_t)_y(v) := \alpha_t\big(\psi_t(y)\big)\big(D\psi_t(y)\,v\big)(ψt∗​αt​)y​(v):=αt​(ψt​(y))(Dψt​(y)v), where Dψt(y)D\psi_t(y)Dψt​(y) is the ambient derivative of ψt:Rn→Rn\psi_t : \mathbb{R}^n \to \mathbb{R}^nψt​:Rn→Rn at yyy. Edge cases of the hypotheses.

  • Surjectivity of DF(y)DF(y)DF(y) at points of MMM forces dim⁡Ty=n−c\dim T_y = n - cdimTy​=n−c there; if c>nc > nc>n then MMM must be empty.

  • If M=∅M = \emptysetM=∅ (e.g. c>nc > nc>n; or n=0n = 0n=0 and c≥1c \ge 1c≥1; or FFF a nonzero constant with c≥1c \ge 1c≥1), every condition quantified over MMM is vacuous: both hypotheses reduce to smoothness of FFF and of α\alphaα, and the conclusion only asks for smooth objects with no constraint coming from MMM.

  • Contact condition (i) requires Ty≠{0}T_y \neq \{0\}Ty​={0} at each y∈My \in My∈M, so a nonempty MMM needs n−c≥1n - c \ge 1n−c≥1. For c=0c = 0c=0 the target R0\mathbb{R}^0R0 is a point, so F≡0F \equiv 0F≡0 and M=RnM = \mathbb{R}^nM=Rn; compactness forces n=0n = 0n=0, and then Ty={0}T_y = \{0\}Ty​={0} violates (i). Hence for c=0c = 0c=0 the two hypotheses cannot hold simultaneously.

  • If n−c=1n - c = 1n−c=1, then ξy={0}\xi_y = \{0\}ξy​={0} and contact condition (ii) is vacuous; "contact" then only means that αt(y)\alpha_t(y)αt​(y) does not vanish identically on TyT_yTy​.

  • The contact condition and dαd\alphadα use the ambient derivative of αt\alpha_tαt​ on Rn\mathbb{R}^nRn, evaluated at points of MMM on vectors of ξy\xi_yξy​.

Human review
  • Endorsed by Shuze Chen · Oct 6, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Mazecto · Oct 6, 2026

    Confirmed by the mission captain (proposal self-audit).

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