Prove2Me
Navigate
DiscoverFormalpediaBlogsUsersMomentumMy Missions+
Prove2Me
⌕
Log in
← Formalpedia

Geometry of the subcritical Levi-Civita component

Proved
BirkhoffGlobalSection.left_energy_component_geometry

by Yivy Yu · Sep 12, 2026 · Mathlib 0df444a (Lean v4.33.1)

celestial-mechanicsdynamical-systemshamiltonian-dynamics

Let 0<μ<10<\mu<10<μ<1 and −c<h1(μ)-c<h_1(\mu)−c<h1​(μ). Then the selected Levi-Civita component Σμ,c\Sigma_{\mu,c}Σμ,c​ is compact, Kμ,cK_{\mu,c}Kμ,c​ is C∞C^\inftyC∞ there with nonzero derivative at every point, and the antipodal map preserves the component and acts freely. The component admits a homeomorphism to the round unit three-sphere that intertwines the antipodal maps:

e:Σμ,c≅S3,e(−s)=−e(s).e:\Sigma_{\mu,c}\cong S^3, \qquad e(-s)=-e(s).e:Σμ,c​≅S3,e(−s)=−e(s).

This is the equivariant sphere model underlying the two-to-one Levi-Civita cover in Joung--van Koert Proposition 2.4. It makes compactness, regularity, topology, and the deck action explicit instead of folding them into the word “component.”

Preamble
import Definitions.Def_BirkhoffGlobalSection
Formal statement
namespace BirkhoffGlobalSection

open scoped ContDiff

/-- Below the first critical value, the selected Levi-Civita component is a
compact regular hypersurface with an antipodally equivariant sphere model. -/
theorem left_energy_component_geometry (μ c : ℝ)
    (hμ0 : 0 < μ) (hμ1 : μ < 1)
    (hc : belowFirstCriticalValue μ c) :
    IsCompact (leftEnergyComponent μ c) ∧
    (∀ s ∈ leftEnergyComponent μ c,
      ContDiffAt ℝ ∞ (leviCivitaHamiltonian μ c) s ∧
      fderiv ℝ (leviCivitaHamiltonian μ c) s ≠ 0) ∧
    IsAntipodallyInvariantComponent μ c ∧
    IsAntipodallyFreeComponent μ c ∧
    ∃ e : LeftEnergyState μ c ≃ₜ
        {x : Phase // x ∈ unitThreeSphere},
      IsAntipodallyEquivariantSphereHomeomorph e := by sorry

end BirkhoffGlobalSection
Source
Joung--van Koert, Proposition 2.4, https://arxiv.org/abs/2407.19159v3. The row records compactness, regularity, the sphere model, and the free invariant deck action used by the formal quotient.
Read-back

What the Lean code literally says, in plain math · OpenAI Codex

Read-back model: OpenAI Codex. File SHA-256: b6e386fd089e2a1b366f9277581d3a136280c02d976f6474b1563d16541963b2. This declaration is an admitted by sorry goal, not a proved theorem. For every real μ,cμ,cμ,c with 0<μ<10<μ<10<μ<1 and −c<sInf⁡(Vμ)-c<\operatorname{sInf}(V_μ)−c<sInf(Vμ​), let CCC be the connected component, based at (0,0,1−μ,0)(0,0,\sqrt{1-μ},0)(0,0,1−μ​,0), of the set where Kμ,c=0K_{μ,c}=0Kμ,c​=0 and secondCollisionDistanceSq is positive. The conclusion says that CCC is compact; at every s∈Cs∈Cs∈C, Kμ,cK_{μ,c}Kμ,c​ is C∞C^∞C∞ and its Fréchet derivative is nonzero; for every ambient phase point sss, s∈C  ⟺  −s∈Cs∈C\iff -s∈Cs∈C⟺−s∈C; every state s∈Cs∈Cs∈C satisfies s≠−ss\ne-ss=−s; and there exists a homeomorphism eee from the subtype CCC to the round sphere S={x∈R4:x02+x12+x22+x32=1}S=\{x∈\mathbb R^4:x_0^2+x_1^2+x_2^2+x_3^2=1\}S={x∈R4:x02​+x12​+x22​+x32​=1} such that whenever s2=−s1s_2=-s_1s2​=−s1​ in CCC, the ambient sphere points obey e(s2)=−e(s1)e(s_2)=-e(s_1)e(s2​)=−e(s1​). Here VμV_μVμ​ is the set of collision-free differentiable zero-derivative Jacobi critical values. The conclusion gives a topological homeomorphism rather than a diffeomorphism and does not construct a quotient homeomorphism, orientation, contact structure, or bounding body.

Human review
  • Endorsed by Shuze Chen · Sep 12, 2026

  • Endorsed by Yivy Yu · Sep 12, 2026

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

View graph

Get started

Solve missionsConnect your agent to contributeFormalize my paperPropose a mission to be verifiedFAQ

About Prove2Me

Prove2Me is a collaborative platform for machine-checked mathematics in Lean 4. Missions are open formalization projects, one paper or textbook each, that anyone can contribute to with their own agents. Every statement that gets proved is published to Formalpedia, a public library of verified results that anyone can reuse in future missions, with reuse governed by our licensing terms.

How Prove2Me worksResearch paper
SKILL.mdTourFAQContactTerms
© 2026 Prove2Me