Complete Hamiltonian time change to a convex regularization model
ProvedBirkhoffGlobalSection.convex_regularization_model_dynamicscelestial-mechanicsdynamical-systemshamiltonian-dynamics
Assume and . Let be a convex regularization model and suppose its regularized time factor satisfies
Every complete LC Hamiltonian flow then admits complete model dynamics: a Hamiltonian flow on and increasing onto clocks with
This is the analytic time-change obligation. It is independent of any chosen periodic orbit or spanning page. It asserts joint continuity and the flow law for the model dynamics, not merely the existence of a separate scalar clock along each orbit.
Formalization Note. The model dynamics are the structure ConvexModelDynamics; the formal hypotheses state finite real upper and lower clock bounds.
Preamble
import Definitions.Def_BirkhoffGlobalSection_ConvexModelDynamics
Formal statement
namespace BirkhoffGlobalSection
/-- A uniformly positive bounded regularized clock transports a complete
LC Hamiltonian flow to a complete Hamiltonian flow on the convex model. -/
theorem convex_regularization_model_dynamics
(μ c : ℝ) (hμ0 : 0 < μ) (hμ1 : μ < 1)
(hc : belowFirstCriticalValue μ c)
(M : ConvexRegularizationModel μ c)
(a b : ℝ) (ha : 0 < a)
(hclock : ∀ s ∈ leftEnergyComponent μ c,
a ≤ M.timeScale s ∧ M.timeScale s ≤ b)
(φ : Flow ℝ (LeftEnergyState μ c))
(hφ : IsLeviCivitaHamiltonianFlow μ c φ) :
Nonempty (ConvexModelDynamics M φ) := by sorry
end BirkhoffGlobalSection
Source
Standard positive time-change construction specialized to the explicit convex regularization interface: C_s(t)=integral from 0 to t of tau(phi_u(s)) du, with inverse clocks defining the model flow. The regularized coordinate/time-change setting is Liu--Salomao, https://arxiv.org/html/2506.17867v2, Section 4. This is an auxiliary analytic theorem formulated for this decomposition, not a verbatim theorem in that paper.