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Local convex body and positive tangential Hessian in centered elliptic-hyperbolic coordinates

Proved
BirkhoffGlobalSection.eh_left_convex_body_local_subcritical

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

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 explicit centered-left elliptic-hyperbolic Hamiltonian Gμ,cG_{\mu,c}Gμ,c​ bounds a compact convex body B⊂R4B\subset\mathbb R^4B⊂R4 with

0∈int⁡B,∂B=Σμ,cEH.0\in\operatorname{int}B,\qquad \partial B=\Sigma^{\mathrm{EH}}_{\mu,c}.0∈intB,∂B=Σμ,cEH​.

The Hamiltonian is C2C^2C2 near every point of this boundary, and its tangential Hessian is strictly positive:

DGμ,c(y)v=0,v≠0⟹D2Gμ,c(y)[v,v]>0(y∈∂B).D G_{\mu,c}(y)v=0,\quad v\ne0\quad\Longrightarrow\quad D^2G_{\mu,c}(y)[v,v]>0\qquad(y\in\partial B).DGμ,c​(y)v=0,v=0⟹D2Gμ,c​(y)[v,v]>0(y∈∂B).

This is the local geometric persistence step at a regular equal-mass energy. It concerns the explicit elliptic-hyperbolic component only; identification with the Levi-Civita component and compatibility of their clocks are separate obligations.

Formalization Note. The assertion adapts Theorem 1.12 and the open parameter neighborhood in Section 10 to the centered-left component defined by a specified collision point. The hypothesis c0>2c_0>2c0​>2 excludes the singular critical surface.

Preamble
import Definitions.Def_BirkhoffGlobalSection_EHSubcritical

open BirkhoffGlobalSection
Formal statement
theorem BirkhoffGlobalSection.eh_left_convex_body_local_subcritical
    (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 ∧
          HasPositiveTangentialHessianOn (ehLeftHamiltonian 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.

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