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Subcritical left EH component bounds a compact convex body

Proved
BirkhoffGlobalSection.eh_left_convex_body

by caleb · Oct 1, 2026 · Mathlib 0df444a (Lean v4.33.1)

celestial-mechanicsconvexityhamiltonian-dynamics

Fix c0>2c_0 > 2c0​>2. There are ε,η>0\varepsilon, \eta > 0ε,η>0 such that for every mass ratio and energy with

0<μ<1,∣μ−1/2∣<ε,∣c−c0∣<η,−c<h1(μ),0 < \mu < 1, \qquad |\mu - 1/2| < \varepsilon, \qquad |c - c_0| < \eta, \qquad -c < h_1(\mu),0<μ<1,∣μ−1/2∣<ε,∣c−c0​∣<η,−c<h1​(μ),

the selected zero-level component Σμ,cEH\Sigma^{\mathrm{EH}}_{\mu,c}Σμ,cEH​ of the centered-left elliptic-hyperbolic Hamiltonian Gμ,cG_{\mu,c}Gμ,c​ is the boundary of a compact convex body:

B⊂R4 compact and convex,0∈int B,∂B=Σμ,cEH.B \subset \mathbb{R}^4 \text{ compact and convex}, \qquad 0 \in \mathrm{int}\, B, \qquad \partial B = \Sigma^{\mathrm{EH}}_{\mu,c}.B⊂R4 compact and convex,0∈intB,∂B=Σμ,cEH​.

Here μ\muμ is the mass ratio (μ=1/2\mu = 1/2μ=1/2 is the equal-mass case), c=−hc = -hc=−h is the Jacobi energy parameter, −c<h1(μ)-c < h_1(\mu)−c<h1​(μ) says the energy lies below the first critical value, and the component Σμ,cEH\Sigma^{\mathrm{EH}}_{\mu,c}Σμ,cEH​ is the connected component of {Gμ,c=0}\{G_{\mu,c} = 0\}{Gμ,c​=0} through the designated left collision point.

This is the geometric half of the local subcritical convexity theorem: it provides the compact convex body whose boundary carries the regularized dynamics, while positivity of the tangential Hessian on that boundary is a separate obligation.

Formalization Note The statement adapts the parameter neighborhood of Theorem 1.12 to the centered-left component; the hypothesis c0>2c_0 > 2c0​>2 excludes the singular critical surface. No regularity or Hessian claim is made here.

Preamble
import Definitions.Def_BirkhoffGlobalSection_EHSubcritical

open BirkhoffGlobalSection
Formal statement
theorem BirkhoffGlobalSection.eh_left_convex_body
    (c₀ : ℝ) (hc₀ : 2 < c₀) :
    ∃ ε η : ℝ, 0 < ε ∧ 0 < η ∧
      ∀ μ c : ℝ, 0 < μ → μ < 1 →
        |μ - 1 / 2| < ε → |c - c₀| < η → belowFirstCriticalValue μ c →
        ∃ B : Set Phase, IsCompact B ∧ Convex ℝ B ∧
          (0 : Phase) ∈ interior B ∧
          ehLeftEnergyComponent μ c = frontier B := by sorry
Source
Liu--Salomao, https://arxiv.org/html/2506.17867v2#S9.SS3, Theorem 9.4(ii) and Section 9.4 (completion of Theorem 1.12); https://arxiv.org/html/2506.17867v2#S10, paragraph constructing an open neighborhood of {1/2} x (-infinity,-2) on which both regularized components are strictly convex. Adapted to the centered-left explicit Hamiltonian and designated component; this child is the convex-body half.

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