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Global entropy-admissible continuation of a finite solution segment

Open
BoltzmannContinuation.global_extension

by Mazecto · Oct 7, 2026 · Mathlib 0df444a (Lean v4.33.1)

entropykinetic-theorypartial-differential-equations

Let f0f_0f0​ be an initial density and let FFF be an entropy-admissible evolution for the periodic hard-sphere Boltzmann equation on [0,T][0,T][0,T], where T>0T>0T>0. Assume strong L1L^1L1 continuity and separate space-time integrability of the unrenormalized gain and loss on that interval. Then there exists a global entropy-admissible evolution GGG with initial datum f0f_0f0​ such that

G(t)=F(t)a.e. on phase space for every t∈[0,T].G(t)=F(t)\quad\text{a.e. on phase space for every }t\in[0,T].G(t)=F(t)a.e. on phase space for every t∈[0,T].

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.

Preamble
import Definitions.Def_BoltzmannFiniteInterval

noncomputable section
open MeasureTheory Set Filter
open OAI.BoltzmannNonuniqueness

Formal statement
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
Source
https://github.com/openai/math/blob/adc7f1241b42e322a6451854ab7e4b4c146bf78a/preprints/Nonuniqueness-for-the-periodic-hard-sphere-Boltzmann-equation-September-23-2026/build/sections/06-admissibility.tex; Section 6, subsection “Continuation and inherited bounds”, concatenation at time T using the periodic DiPerna–Lions theorem. See also Levermore–Masmoudi 2010, Section 4.1, Theorem 4.1, https://doi.org/10.1007/s00205-009-0254-5.

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