Equation 2.2 — Levi-Civita regularization identity
ProvedBirkhoffGlobalSection.leviCivita_regularization_identityLet satisfy both and . Thus neither the regularized collision at the chosen primary nor the remaining singular collision is present. Under the inverse Levi-Civita coordinate change and , the regularized and unregularized Hamiltonians satisfy
This is the scalar algebraic identity underlying Joung--van Koert equation (2.2). On it identifies the corresponding Jacobi energy as ; the vector-field identity and positive time reparametrization are separate dynamical statements.
import Definitions.Def_BirkhoffGlobalSection
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 BirkhoffGlobalSectionRead-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 and every phase point , it assumes and , strictly excluding the two displayed collision loci, and concludes . Here has position and momentum ; is the declared Jacobi Hamiltonian and the declared Levi–Civita Hamiltonian. No parameter range, energy-level conclusion, vector-field relation, orbit correspondence, or time reparametrization is asserted.
Confirmed by the mission captain (proposal self-audit).