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Near-critical EH component lies in the convexity box off the saddle-centers

Proved
BirkhoffGlobalSection.eh_left_component_near_critical_in_box

by Mazecto · Oct 3, 2026 · Mathlib 0df444a (Lean v4.33.1)

celestial-mechanicsconvexityrestricted-three-body

Localization of the selected EH component near the equal-mass critical energy.

Let WWW be any open set containing the EH saddle-centers σ±=(0,±π2,0,0)\sigma_\pm=(0,\pm\tfrac{\pi}{2},0,0)σ±​=(0,±2π​,0,0). Then there are ε,η>0\varepsilon,\eta>0ε,η>0 with the following property. Whenever

0<μ<1,∣μ−12∣<ε,c<2+η,−c<h1(μ),0<\mu<1,\qquad |\mu-\tfrac12|<\varepsilon,\qquad c<2+\eta,\qquad -c<h_1(\mu),0<μ<1,∣μ−21​∣<ε,c<2+η,−c<h1​(μ),

every point of the selected EH component Σμ,cEH\Sigma^{EH}_{\mu,c}Σμ,cEH​ outside WWW lies in the compact box

cosh⁡2x1≤4,∣x2∣≤π2,∣y1∣,∣y2∣≤12.\cosh^2x_1\le 4,\qquad |x_2|\le\tfrac{\pi}{2},\qquad |y_1|,|y_2|\le 12 .cosh2x1​≤4,∣x2​∣≤2π​,∣y1​∣,∣y2​∣≤12.

Below the first critical value the left Hill region is separated from the right one. As (μ,c)→(12,2)(\mu,c)\to(\tfrac12,2)(μ,c)→(21​,2) the component converges to the left lobe of the critical surface, and it leaves the region ∣x2∣≤π/2|x_2|\le\pi/2∣x2​∣≤π/2 only through a small neck around σ±\sigma_\pmσ±​. The box is the one on which the critical convexity estimate holds.

Formalization Note ehLeftEnergyComponent is the connected component of the EH zero set through the collision point; it is the image of the Levi-Civita component under the EH regularization (accepted eh_left_regularization_subcritical).

Preamble
import Definitions.Def_BirkhoffGlobalSection_EHSubcritical
Formal statement
namespace BirkhoffGlobalSection

/-- Localization of the selected EH component near the equal-mass critical energy: given any
open set containing the two EH saddle-centers `(0, ±π/2, 0, 0)`, for subcritical parameters
in a small strip around `(1/2, 2)` every point of the selected EH component outside the set
lies in the compact box `cosh² x₁ ≤ 4`, `|x₂| ≤ π/2`, `|y₁|, |y₂| ≤ 12`. -/
theorem eh_left_component_near_critical_in_box (W : Set Phase) (hW : IsOpen W)
    (hplus : (![0, Real.pi / 2, 0, 0] : Phase) ∈ W)
    (hminus : (![0, -(Real.pi / 2), 0, 0] : Phase) ∈ W) :
    ∃ ε η : ℝ, 0 < ε ∧ 0 < η ∧
      ∀ μ c : ℝ, 0 < μ → μ < 1 →
        |μ - 1 / 2| < ε → c < 2 + η → belowFirstCriticalValue μ c →
        ∀ y ∈ ehLeftEnergyComponent μ c, y ∉ W →
          Real.cosh (y 0) ^ 2 ≤ 4 ∧ |y 1| ≤ Real.pi / 2 ∧ |y 2| ≤ 12 ∧ |y 3| ≤ 12 := by sorry

end BirkhoffGlobalSection
Source
Liu--Salomao, https://arxiv.org/html/2506.17867v2 (Theorem 1.12, Sections 9.2-9.3 and 10); reduction of regularization_model_convex_away_from_saddle_center.

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