Alphabeta Math
RemarkRemark: AI-adaptedProof: AI-generatedPipeline-generatedprecheck pendingverified 2026-10-23 (gpt-6.1-sol)
How statement and proof provenance work

The first chip identifies the source of the statement or construction; the second identifies the source of its local proof or verification.

  • Literature-sourced: the exact statement appears in a cited source; only wording and notation differ.
  • AI-adapted: a semantically identical restatement of literature-sourced material, modulo indexing, notation, and boundary cases adopted by the library.
  • AI-generated: a genuinely novel statement formulated by AI, with no source for the claim itself.

These labels describe origin, not correctness: citations and verification chips remain separate evidence.

Scope of the kinetic-to-fluid limit results

Remark

The Euler-passage theorem in this collection assumes weighted strong convergence to local Maxwellians and proves only the resulting conservation-law passage. The separate homogeneous BGK theorem gives an explicit relaxation solution and its limit. Neither result proves convergence for general inhomogeneous Boltzmann solutions, a Boltzmann–Grad limit from deterministic many-particle dynamics, or a Navier–Stokes–Fourier limit. Those questions require additional hypotheses and separate theorem chains.

Facts & Assumptions

Given: The statements and hypotheses of the conditional Euler-passage theorem and homogeneous BGK relaxation theorem.

[F1]

Euler equations under weighted local-equilibrium convergence: The Euler conclusion assumes weighted strong convergence and does not assert that such convergence occurs.

[F2]

Exact homogeneous BGK fast relaxation: The explicit convergence result concerns the spatially homogeneous BGK relaxation model.

Verification

1.1F1

The first scope statement follows directly from the convergence hypotheses and conclusion of [F1]; its proof is a conditional passage of already assumed moments and fluxes.

2.1F1F2∎

The second theorem [F2] has no spatial dependence and uses the BGK operator, so its exact solution does not supply an existence or convergence argument for inhomogeneous Boltzmann dynamics. Neither supplier states a many-particle Boltzmann–Grad or Navier–Stokes–Fourier result; this remark records only the limits of these two carriers.

Depends on

Dependency tree · 2 levels

Sources