Global entropy-admissible continuation of a finite solution segment
OpenBoltzmannContinuation.global_extensionLet be an initial density and let be an entropy-admissible evolution for the periodic hard-sphere Boltzmann equation on , where . Assume strong continuity and separate space-time integrability of the unrenormalized gain and loss on that interval. Then there exists a global entropy-admissible evolution with initial datum such that
The global evolution retains the supplied early strong continuity and collision integrability. Finite-interval admissibility includes finite entropy at every time, weak continuity, uniform entropy moments, collision-fiber integrability, separate renormalized collision integrability, terminal-trace weak renormalized and local-mass identities, total momentum conservation, and every-time energy and entropy-dissipation inequalities. The conclusion imposes all of the target definition of global admissibility. This continuation interface is independent of the particular nonuniqueness construction.
import Definitions.Def_BoltzmannFiniteInterval noncomputable section open MeasureTheory Set Filter open OAI.BoltzmannNonuniqueness
namespace BoltzmannContinuation
/-- Extend a finite entropy-admissible segment without changing its time sections.
The strong regularity remains confined to the supplied early interval. -/
theorem global_extension (f₀ : Density) (F : Evolution) (T : ℝ)
(hF : AdmissibleOn f₀ T F) (hstrong : StrongEarly T F) :
∃ G : Evolution, AdmissibleGlobal f₀ G ∧ StrongEarly T G ∧
∀ t ∈ Set.Icc 0 T, G t =ᵐ[volume] F t := by sorry
end BoltzmannContinuation