The convex envelope Γv\Gamma_v of a continuous function — the largest convex function lying below it — is the central object behind the Aleksandrov–Bakelman–Pucci estimate, the Dirichlet problem for the degenerate Monge–Ampère equation, Hamilton–Jacobi theory, and obstacle formulations. De Philippis and Figalli (Trans. AMS, 2015) proved that Γv∈Cloc1,min⁡{α,β}(Ω)\Gamma_v\in C^{1,\min\{\alpha,\beta\}}_{\mathrm{loc}}(\Omega) when vv is globally Lipschitz and (1+α)(1+\alpha)-semiconcave and ∂Ω\partial\Omega is of class C1,βC^{1,\beta}, and that Γv∈C1,1(Ω‾)\Gamma_v\in C^{1,1}(\overline{\Omega}) when Ω\Omega is uniformly convex with C3,1C^{3,1} boundary and v∈C3,1(Ω‾)v\in C^{3,1}(\overline{\Omega}), with both hypothesis sets shown sharp by explicit two-dimensional examples. The unresolved problem, identified by the authors as arising exactly when the contact points supporting the envelope lie close to the boundary, is the matching up-to-boundary theory: characterize the minimal geometric hypotheses on Ω\Omega — weaker than uniform convexity and than C3,1C^{3,1} boundary smoothness — and the minimal analytic hypotheses on vv that still guarantee C1,αC^{1,\alpha} or C1,1C^{1,1} regularity of Γv\Gamma_v up to ∂Ω\partial\Omega; and classify, for general moduli of continuity, when boundary-induced contacts force a loss of regularity, quantifying how boundary regularity trades against semiconcavity of vv. Caffarelli–Tang–Wang (2022) settled the C1,αC^{1,\alpha} scale on uniformly convex domains under optimal conditions, and Han–Liu–Zhou (2025) proved global C1,β/kC^{1,\beta/k} bounds on planar domains with a finite-order degenerate boundary point; the general-dimensional, non-uniformly-convex, general-moduli regime and the sharp modulus trade-off remain open.

Background

Given an open set Ω⊂Rn\Omega\subset\mathbb{R}^n and a continuous function v:Ω‾→Rv:\overline{\Omega}\to\mathbb{R}, the convex envelope of vv in Ω\Omega is

Γv(x):=sup⁡{ℓ(x): ℓ≤v in Ω, ℓ affine},\Gamma_v(x):=\sup\{\ell(x):\ \ell\le v \text{ in }\Omega,\ \ell \text{ affine}\},

the largest convex function lying below vv. Convex functions are automatically locally Lipschitz, but applications need quantitative control of derivatives, so the central question of this literature is when ∇Γv\nabla\Gamma_v is Hölder continuous (Γv∈C1,α\Gamma_v\in C^{1,\alpha} for some α∈(0,1]\alpha\in(0,1]) or Lipschitz (Γv∈C1,1\Gamma_v\in C^{1,1}), and up to which sets. The envelope appears throughout analysis and geometry: in the Aleksandrov–Bakelman–Pucci maximum principle for fully nonlinear elliptic equations, in the Dirichlet problem for the degenerate Monge–Ampère equation — where the solution of det⁡D2u=f≥0\det D^2u=f\ge 0 with boundary datum vv is precisely the envelope of vv weighted by ff — in Hamilton–Jacobi theory, where viscosity solutions are semiconcave and their singular sets are governed by contact geometry, and as a nonlinear obstacle problem studied numerically by Oberman and Silvestre.

A function vv is (1+α)(1+\alpha)-semiconcave in Ω‾\overline{\Omega}, α∈(0,1]\alpha\in(0,1], if for every x0∈Ω‾x_0\in\overline{\Omega} there is a slope px0p_{x_0} with v(x)≤v(x0)+px0⋅(x−x0)+C∣x−x0∣1+αv(x)\le v(x_0)+p_{x_0}\cdot(x-x_0)+C|x-x_0|^{1+\alpha} near x0x_0: semiconcave functions are 'differentiable from above' with a controlled defect, which is the natural one-sided regularity of Hamilton–Jacobi solutions. A contact (or touching) point is a point where v=Γvv=\Gamma_v; a supporting slope is the gradient of an affine function touching vv from below at such a point. A convex domain Ω\Omega is uniformly convex if for some fixed radius RR it is enclosed in balls of radius RR tangent to ∂Ω\partial\Omega at each boundary point — a quantitative lower bound on boundary curvature, strictly stronger than smooth strict convexity.

Earlier work treated either the Dirichlet case, where Γv\Gamma_v is determined by boundary data (Caffarelli–Nirenberg–Spruck; Griewank–Rabier; Kirchheim–Kristensen; Oberman–Silvestre), or imposed strong global assumptions on vv. De Philippis–Figalli (2015) treated the general problem and proved: (a) [Theorem 1.2] if Ω\Omega is bounded convex with ∂Ω\partial\Omega of class C1,βC^{1,\beta} and vv is globally Lipschitz and (1+α)(1+\alpha)-semiconcave in Ω‾\overline{\Omega}, then Γv∈Cloc1,min⁡{α,β}(Ω)\Gamma_v\in C^{1,\min\{\alpha,\beta\}}_{\mathrm{loc}}(\Omega) — an interior result only; (b) [Theorem 1.3] if Ω\Omega is uniformly convex with ∂Ω\partial\Omega of class C3,1C^{3,1} and v∈C3,1(Ω‾)v\in C^{3,1}(\overline{\Omega}), then Γv∈C1,1(Ω‾)\Gamma_v\in C^{1,1}(\overline{\Omega}); (c) both hypothesis sets are sharp, via explicit two-dimensional examples in which the envelope is computed exactly — e.g. a harmonic function equal to ∣x∣|x| on the boundary of the disk has Γv=∣x∣\Gamma_v=|x|, which is not C1C^1; on the non-uniformly-convex domain {∣x∣p+∣y∣p≤1}\{|x|^p+|y|^p\le 1\}, 1<p<21<p<2, the envelope is no better than C1,p−1C^{1,p-1}, so high-order semiconcavity cannot compensate a degenerate boundary; (d) for general moduli of continuity — vv being ω1\omega_1-semiconcave and ∂Ω\partial\Omega being C1C^1 with modulus ω2\omega_2 — the gradient ∇Γv\nabla\Gamma_v has modulus of continuity controlled by max⁡{ω1,ω2}\max\{\omega_1,\omega_2\} (up to rescaling) on compact subsets of Ω\Omega, again an interior statement; (e) if v=0v=0 on ∂Ω\partial\Omega and inf⁡Ωv<0\inf_{\Omega}v<0, no regularity of ∂Ω\partial\Omega whatsoever is needed for interior C1,αC^{1,\alpha} regularity [Theorem 4.1], showing the entire difficulty is genuinely a boundary-contact phenomenon.

The proofs expose the structural reason for the gap between (a) and (b): by Carathéodory's theorem, any point of the convex hull of a set in Rn\mathbb{R}^n is a convex combination of at most n+1n+1 points of the set, so the regularity of Γv\Gamma_v at a point is controlled by the contact points in its supporting simplex; the authors state that 'the main difficulty when proving the regularity of Γv\Gamma_v arises when [these contact points] are close to the boundary'. Interior contact points transfer the semiconcavity of vv to the envelope directly; boundary contact points instead couple the envelope to the fine geometry of ∂Ω\partial\Omega, and the only known mechanism to control them — geometric barrier constructions around boundary-flat regions — required uniform convexity and C3,1C^{3,1} smoothness. What is missing is the matching theory at the boundary: which geometric assumptions on ∂Ω\partial\Omega, weaker than uniform convexity and than high-order smoothness, and which analytic assumptions on vv, control Γv\Gamma_v up to ∂Ω\partial\Omega — and how the boundary's modulus of continuity trades against the semiconcavity of vv.

Problem Statement

Determine the up-to-boundary regularity of the convex envelope Γv\Gamma_v in the regime where the supporting contact points of Γv\Gamma_v may lie arbitrarily close to ∂Ω\partial\Omega. The single objective is a sharp characterization of this boundary regularity, in the two independent components below: neither component is a prerequisite for the other, and the general-moduli classification (ii) also settles the modulus part of (i).

(i) [Positive direction, minimal hypotheses] Find minimal geometric hypotheses on the bounded convex domain Ω\Omega — strictly weaker in each respect than uniform convexity of Ω\Omega and than C3,1C^{3,1}-smoothness of ∂Ω\partial\Omega, so that neither of these two properties is assumed — and minimal analytic hypotheses on vv (in the scale of global Lipschitz continuity and semiconcavity-type moduli) under which Γv∈C1,α(Ω‾)\Gamma_v\in C^{1,\alpha}(\overline{\Omega}) with its optimal exponent α∈(0,1)\alpha\in(0,1), or else Γv∈C1,1(Ω‾)\Gamma_v\in C^{1,1}(\overline{\Omega}), with quantitative estimates on the modulus of continuity of ∇Γv\nabla\Gamma_v; minimality is measured in the two scales these hypotheses live in, compared pointwise in each — the analytic hypotheses in the semiconcavity modulus ω1\omega_1 of vv, and the geometric hypotheses in the pair formed by the smoothness modulus ω2\omega_2 of ∂Ω\partial\Omega (the C1C^1 boundary modulus of (ii)) and a curvature modulus ω3\omega_3 of ∂Ω\partial\Omega, a pointwise lower bound on the boundary curvature for which uniform convexity is the case of ω3\omega_3 bounded below by a positive constant and strict convexity the case of a finite but possibly degenerating ω3\omega_3 — and prove the matching necessity of the hypotheses by explicit examples, as De Philippis–Figalli did for theirs.

(ii) [Classification and trade-off direction] For general moduli of continuity — vv being ω1\omega_1-semiconcave and ∂Ω\partial\Omega being C1C^1 with modulus ω2\omega_2 — classify when boundary-induced contacts force a loss of up-to-boundary regularity, and quantify how much boundary regularity can be traded against improved semiconcavity hypotheses on vv; equivalently, extend the interior modulus estimate max⁡{ω1,ω2}\max\{\omega_1,\omega_2\} of De Philippis–Figalli up to the boundary in a sharp form, identifying the pairs (ω1,ω2)(\omega_1,\omega_2) for which ∇Γv\nabla\Gamma_v has a controlled modulus on Ω‾\overline{\Omega}.

Literature-status note (this describes the state of knowledge, not a restriction of the question): the uniformly convex case in the Hölder scale has been resolved by Caffarelli–Tang–Wang, who proved global C1,αC^{1,\alpha} regularity for the envelope under optimal conditions on uniformly convex domains, and Han–Liu–Zhou proved global C1,β/kC^{1,\beta/k} gradient bounds for planar domains whose boundary is strictly convex but only finitely flat at a distinguished point. The problem above is therefore posed in its original generality; its presently open core is the general-dimensional, non-uniformly-convex, general-moduli regime of (i), and the sharp trade-off classification of (ii).

References

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