Notes on Partial Differential Equations VI: Interior Regularity of Weak Solutions via Difference QuotientsTextbook
Motivation
A second-order elliptic equation in divergence form, , is usually solved in a weak sense: the Lax–Milgram theorem or the Fredholm alternative produces a function , which has only first-order weak derivatives, and the equation holds after one integration by parts against every test function. The phrase "solution of a PDE" then covers objects for which the second derivatives appearing in need not exist. Regularity theory closes this gap: under smoothness of the coefficients and the data, weak solutions have exactly as many derivatives as the equation suggests. It is used throughout the calculus of variations, spectral theory and nonlinear PDE.
The interior estimate for divergence-form operators with coefficients goes back to the difference-quotient technique of L. Nirenberg (1955) and is standard in textbooks such as Evans, Partial Differential Equations, §6.3, and Gilbarg–Trudinger, Chapter 8. This mission follows the treatment in J. K. Hunter's lecture notes, §4.11 and Appendix 4.C.
Setting
Points of are written , and is the th standard unit vector. Let be an open set. A set is compactly contained in , written , if is nonempty and open, its closure is compact, and .
A test function is an infinitely differentiable with compact support inside (the space ). A function is the weak derivative of a locally integrable (multi-index ) if for all test functions . The Sobolev space consists of the functions whose weak derivatives of order at most exist and lie in , with norm ; more generally uses . The space is the closure of in .
The coefficients are functions , , which are bounded (), symmetric () and uniformly elliptic: for some ,
Given , a function is a weak solution of if
No boundary condition is imposed on .
For the th difference quotient of is , and with pointwise length .
Formalization targets
Goal: interior regularity (Theorem 4.27)
If moreover , then for every there is a constant , depending only on , , and the coefficients, such that every weak solution of with satisfies and
Milestones: difference quotients (Appendix 4.C)
- Proposition 4.52 (1): if and its weak derivative are locally integrable on , then .
- Proposition 4.52 (2): for , , , .
- Theorem 4.53 (1): with , and , for each .
- Theorem 4.53 (2): if , , and for all , then and .
Stronger targets
- Theorem 4.28: if and , then with , depending only on and the coefficients.
- Corollary 4.29: if , then agrees a.e. in with a function.
Significance
The goal theorem shows that weak solutions of divergence-form equations with coefficients are strong solutions: their second weak derivatives are square integrable on compact subsets, so the equation holds pointwise almost everywhere. The iterated version (Theorem 4.28) and its corollary turn the existence theory for weak solutions into existence of smooth solutions whenever the coefficients and data are smooth; in combination with Sobolev embedding this is how one proves that eigenfunctions of the Dirichlet Laplacian on an open set are smooth in its interior.
All of these results are classical and fully proved in the literature. To the best of the platform's records, none is formalized: Mathlib has Lebesgue spaces, Fréchet derivatives and Hilbert-space tools, but neither weak derivatives nor Sobolev spaces on open sets, and there is no elliptic regularity result in any proof assistant known to the maintainers. A complete development would therefore also deliver reusable infrastructure: weak derivatives, and its norm, difference quotients and their calculus, and cut-off functions subordinate to .
Difficulty
The formal computation behind the estimate — testing the equation against for a cut-off and using ellipticity — is illegitimate for a weak solution, because the test function involves second derivatives of that are not yet known to exist. Replacing derivatives by difference quotients makes every step meaningful but requires a separate theory: commuting difference quotients with weak derivatives, a discrete product rule and integration by parts, and a compactness argument in (reflexivity) that turns an -uniform bound into a weak derivative. The error terms involve difference quotients of the coefficients, which is where enters, and the final estimate has to be closed with a Cauchy inequality and a second localization to replace by .
Formalization scope
Space is = EuclideanSpace ℝ (Fin n) with Lebesgue measure volume; coordinates are 0-based (i : Fin n), so the book's are EuclideanSpace.single 0 1, …. Functions are real-valued on all of and only their values on the relevant open set matter. Weak derivatives (HasWeakDeriv, weakDeriv), (MemW), its norm (sobolevNorm, valued in ℝ≥0∞) and (MemW0) are defined in the mission; weakDeriv is a chosen representative and is only used under hypotheses guaranteeing existence. Exponents are p : ℝ≥0∞; conjugate exponents use ENNReal.HolderConjugate. and are ContDiffOn ℝ k and ContDiffOn ℝ ∞ on (smooth, not analytic); "" for a Sobolev function means a.e. equality on with such a function.
Conventions committed to:
- The standing assumptions of §4.6 on the operator — , , uniform ellipticity — are explicit hypotheses of Theorems 4.27–4.29, and (the setting (4.34)) is a hypothesis of Corollary 4.29.
- Theorem 4.27 assumes as printed, not .
- Constants:
∃ C : ℝis quantified after , the coefficients, the ellipticity constant and (and ), and before and . - in Theorem 4.53 is modelled by any with for all ; the largest such is the book's distance (and when ), so this is the book's condition and avoids Lean's convention that the distance to the empty set is .
- Two corrections of the printed statements: Proposition 4.52 (2) is stated with on the right, as the book's proof derives; Theorem 4.53 (1) is stated componentwise, , which is what its proof establishes and what the proof of Theorem 4.27 uses (the printed vector form with Euclidean lengths fails for large , e.g. for ).
The theorems are not trivialized by junk values: the difference quotient is only used at , the weak formulation's Bochner integrals are integrable under the stated and hypotheses, and the conclusion asserts existence of all weak derivatives of order at most two, not merely a bound on a norm that could be computed from junk representatives.
Contributions welcome: a library of weak derivatives and Sobolev spaces on open subsets of compatible with these definitions, cut-off functions for (Mathlib's ContDiffBump and exists_smooth_tsupport_subset are natural starting points), and Banach–Alaoglu for , .
Selected references
- J. K. Hunter, Notes on Partial Differential Equations, UC Davis lecture notes, revised 6/18/2014, §4.11 and Appendix 4.C. https://www.math.ucdavis.edu/~hunter/pdes/pde_notes.pdf
- L. C. Evans, Partial Differential Equations, 2nd ed., Graduate Studies in Mathematics 19, American Mathematical Society, 2010, §5.8.2 and §6.3. https://doi.org/10.1090/gsm/019
- D. Gilbarg and N. S. Trudinger, Elliptic Partial Differential Equations of Second Order, Classics in Mathematics, Springer, 2001, §7.11 and §8.3. https://doi.org/10.1007/978-3-642-61798-0
- L. Nirenberg, Remarks on strongly elliptic partial differential equations, Communications on Pure and Applied Mathematics 8 (1955), 649–675. https://doi.org/10.1002/cpa.3160080414