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.
Weak existence and smooth regularity scope
Remark
Under Countable Choice, the periodic existence theorem gives a global weak solution for every stated initial datum and positive viscosity; it does not prove global smoothness or uniqueness among all three-dimensional weak solutions. Under Countable Choice and Dependent Choice, the weak–smooth theorem yields uniqueness only on an interval where a smooth solution with the same data is already given. The finite-mode compactness lemma assumes Countable Choice, and the Galerkin compactness argument uses a positive-viscosity gradient bound; that proof does not apply at . These are limits of the claims proved on this page and are not assertions about empirical fluid behavior.
Remark references
Facts & Assumptions
Given: Only the theorem statements and proof hypotheses on this page are being summarized.
Global periodic weak viscous existence: the conclusion is global unforced weak existence for , , , and contains no uniqueness or smoothness assertion.
Fourier compactness with coefficient time control: under Countable Choice, the compactness statement uses an integrated gradient bound, which in the Galerkin energy estimate is supplied by the positive factor .
Weak–smooth uniqueness on a smooth interval: under Countable Choice and Dependent Choice, uniqueness is conditional on a smooth comparison solution on the interval.
Proof
The first sentences restate the exact scope, assumptions, and quantifiers of [F1] and [F3]; neither theorem's conclusion contains global regularity or unrestricted three-dimensional uniqueness.
The compactness lemma requires the bound ; in the viscous Galerkin energy identity this is obtained after dividing by . At that step supplies no gradient control, so the stated compactness proof gives no inviscid conclusion. This is a proof-scope observation only.