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.
regularity implies classical or H"older regularity when is large
Statement
Assume the Axiom of Choice. Let , , and let be a bounded -extension domain (the extension property is for this displayed and exponent ). (i) If , every has a representative in for every , with the norm controlled by . (ii) If , every such has a representative in for every , with the corresponding norm bound; in particular . For any nondivergence expression with , this gives ; whenever also holds distributionally for some , the equality then holds almost everywhere. (iii) If for , the representative is . No finite gives regularity in general: on a ball, the function belongs to for every finite , while has no continuous representative.
Facts & Assumptions
Given: the Axiom of Choice, , , the bounded -extension domain , and .
The Axiom of Choice is the standing hypothesis, used through the extension operator and the embedding theorem below. (The Axiom of Choice)
By the extension property there is a bounded linear with almost everywhere and . (Sobolev extension domains and extension operators)
Higher-order Sobolev embedding (Higher-order Sobolev embedding): for a bounded extension domain and , , (a) if then for every ; (b) if then for every finite ; (c) if then every has a representative in for every integer and with , with the norm bounded by a constant times . Applied with and , the three cases are , , ; the case is exactly . (Higher-order Sobolev embedding)
The witness on the unit ball : for , the weak derivatives are , and otherwise. Thus for every finite . On the disk section the one-sided values of differ, so this weak derivative has no continuous representative; consequently for every . (Integer-order Sobolev spaces and their norms)
The unit ball is a bounded domain and hence a -extension domain for every (Bounded C^k domains and boundary charts, Bounded C^k domains admit integer-order Sobolev extension).
If two locally integrable functions represent the same distribution on , they agree almost everywhere; this is the uniqueness of the zeroth weak derivative (Uniqueness of a weak derivative as an almost-everywhere class).
Proof
Domain hypothesis. By the definition of a -extension domain [F1], satisfies the bounded-domain premise of [F2] for and exponent . The embedding conclusion of [F2] is already on ; no embedding on the unbounded space is used.
The ball witness: no finite gives . On let . The function is with , and integration by parts on the two sides of gives the weak derivative ; the interface term vanishes because is continuous there. All second derivatives are bounded, so for every finite . If had a continuous representative, it would equal on the negative open half-ball and on the positive open half-ball: the almost-everywhere equalities force these values on each open side by continuity. They cannot extend continuously across the interior disk . Thus has no representative for any . The ball is in the stated extension-domain class by [F4].
Part (i): . Then . For every the embedding [F2] with , , gives a representative and . If , the same strict inequality allows every .
Part (ii): . Then . For each , one has , so [F2] with , , gives a representative and the stated norm bound. The weak derivatives with are classes by the definition of . Thus for with bounded coefficients, is an class. If also distributionally with , then [F5] gives equality of the represented classes almost everywhere.
Part (iii): . Then , so [F2] with , , and exponent gives a representative in with norm bounded by . Parts (i), (ii), (iii) are direct applications of the bounded-domain higher-order embedding.
Conclusion. The higher-order embedding gives the asserted representatives when , representatives when , and representatives when . The ball witness of step 1.2 shows that no finite forces regularity in general, so the Sobolev and Schauder scales differ at the top order.
Remarks
- The hypothesis is indexed by : a domain that is an extension domain for one pair need not be for another, and the statement uses only the displayed pair. The counterexample on the ball shows that the extension property alone, or any finite , cannot produce two H"older derivatives.
- The strict exponent ranges in the statement are sufficient, rather than an assertion of optimality. For , the endpoint clause of Higher-order Sobolev embedding also gives , since is nonintegral; for example gives . The ball witness shows that no finite forces two Hölder derivatives.
Depends on
Used by
Dependency tree · two levels
42 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- John Villavert, Elementary Theory and Methods for Elliptic Partial Differential Equations (2017; complete 220-page lecture notes) (standard reference, not scraped)
- Armin Schikorra, Partial Differential Equations I & II (version October 1, 2025; complete 281-page graduate lecture notes) (standard reference, not scraped)