Convex model normalized variation energy tangent
ProvedBirkhoffGlobalSection.convex_model_normalized_variation_energy_tangentconvex-geometryreal-analysis
For supplied normalized model trajectories and variational solutions on the boundary, an initially energy-tangent variation remains energy tangent.
All displayed regularity, tangency, normalization and supplied-data hypotheses of the exact formal statement are retained. This is a conditional result for the defined convex regularization model, not a global-section or index-existence theorem.
Preamble
import Theorems.Thm_BirkhoffGlobalSection_reverse_radial_variation_bundle open BirkhoffGlobalSection Set Filter SignType open scoped ContDiff Topology set_option linter.unusedVariables false set_option autoImplicit false set_option maxHeartbeats 800000
Formal statement
theorem BirkhoffGlobalSection.convex_model_normalized_variation_energy_tangent :
∀ {μ c : ℝ}
(M : ConvexRegularizationModel μ c) (x v : ℝ → Phase)
(hs : ∀ t, x t ∈ frontier M.body)
(hx : ∀ t, HasDerivAt x
((phaseRadialContact (x t) (hamiltonianVectorField M.modelHamiltonian (x t)))⁻¹ •
hamiltonianVectorField M.modelHamiltonian (x t)) t)
(hv : ∀ t, HasDerivAt v
(fderiv ℝ (fun y =>
(phaseRadialContact y (hamiltonianVectorField M.modelHamiltonian y))⁻¹ •
hamiltonianVectorField M.modelHamiltonian y) (x t) (v t)) t)
(h0 : fderiv ℝ M.modelHamiltonian (x 0) (v 0) = 0),
∀ t, fderiv ℝ M.modelHamiltonian (x t) (v t) = 0 := by sorrySource
Independent extraction of component 3 of the Proved theorem BirkhoffGlobalSection.reverse_radial_variation_bundle. Original verified source: Solutions/Sol_BirkhoffGlobalSection_reverse_radial_variation_bundle.lean. Exact original component retained.