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Equation 2.2 — Levi-Civita regularization identity

Proved
BirkhoffGlobalSection.leviCivita_regularization_identity

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

celestial-mechanicsdynamical-systemshamiltonian-dynamics

Let s=(z1,z2,w1,w2)s=(z_1,z_2,w_1,w_2)s=(z1​,z2​,w1​,w2​) satisfy both ∣z∣2>0|z|^2>0∣z∣2>0 and D(z)>0D(z)>0D(z)>0. Thus neither the regularized collision at the chosen primary nor the remaining singular collision is present. Under the inverse Levi-Civita coordinate change q+μ=2z2q+\mu=2z^2q+μ=2z2 and p=w/zˉp=w/\bar zp=w/zˉ, the regularized and unregularized Hamiltonians satisfy

Kμ,c(s)=∣z∣2(Hμ(q,p)+c).K_{\mu,c}(s)=|z|^2\bigl(H_\mu(q,p)+c\bigr).Kμ,c​(s)=∣z∣2(Hμ​(q,p)+c).

This is the scalar algebraic identity underlying Joung--van Koert equation (2.2). On Kμ,c=0K_{\mu,c}=0Kμ,c​=0 it identifies the corresponding Jacobi energy as Hμ=−cH_\mu=-cHμ​=−c; the vector-field identity and positive time reparametrization are separate dynamical statements.

Preamble
import Definitions.Def_BirkhoffGlobalSection
Formal statement
namespace BirkhoffGlobalSection

/-- Equation (2.2): away from both collision loci, the Levi-Civita Hamiltonian
is the shifted Jacobi Hamiltonian multiplied by `|z|²`. -/
theorem leviCivita_regularization_identity (μ c : ℝ) (s : Phase)
    (hz : 0 < zNormSq s) (hD : 0 < secondCollisionDistanceSq s) :
    leviCivitaHamiltonian μ c s =
      zNormSq s * (jacobiHamiltonian μ (leviCivitaToJacobi μ s) + c) := by sorry

end BirkhoffGlobalSection
Source
Joung--van Koert, equation (2.2) and the immediately following scalar/vector-field relation, https://arxiv.org/abs/2407.19159v3.
Read-back

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

Read-back model: OpenAI Codex. File SHA-256: 2ca660b2ee0a25bd29b71f88545eb354e5149464a5fb51a707806595497decec. This declaration is an admitted by sorry goal, not a proved theorem. For every real μ,cμ,cμ,c and every phase point s=(z1,z2,w1,w2)s=(z_1,z_2,w_1,w_2)s=(z1​,z2​,w1​,w2​), it assumes z12+z22>0z_1^2+z_2^2>0z12​+z22​>0 and (2(z12−z22)−1)2+(4z1z2)2>0(2(z_1^2-z_2^2)-1)^2+(4z_1z_2)^2>0(2(z12​−z22​)−1)2+(4z1​z2​)2>0, strictly excluding the two displayed collision loci, and concludes Kμ,c(s)=(z12+z22)(Hμ(Lμ(s))+c)K_{μ,c}(s)=(z_1^2+z_2^2)(H_μ(L_μ(s))+c)Kμ,c​(s)=(z12​+z22​)(Hμ​(Lμ​(s))+c). Here Lμ(s)L_μ(s)Lμ​(s) has position (2(z12−z22)−μ,4z1z2)(2(z_1^2-z_2^2)-μ,4z_1z_2)(2(z12​−z22​)−μ,4z1​z2​) and momentum ((w1z1−w2z2)/(z12+z22),(w1z2+w2z1)/(z12+z22))((w_1z_1-w_2z_2)/(z_1^2+z_2^2),(w_1z_2+w_2z_1)/(z_1^2+z_2^2))((w1​z1​−w2​z2​)/(z12​+z22​),(w1​z2​+w2​z1​)/(z12​+z22​)); HμH_μHμ​ is the declared Jacobi Hamiltonian and Kμ,cK_{μ,c}Kμ,c​ the declared Levi–Civita Hamiltonian. No parameter range, energy-level conclusion, vector-field relation, orbit correspondence, or time reparametrization is asserted.

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

  • Endorsed by Yivy Yu · Sep 12, 2026

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

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