Lions (C. R. Acad. Sci. Paris Sér. I Math. 326 (1998) 1385–1390) identified the dual cone of the convex functions in L2(Ω)L^2(\Omega) for Ω⊂RN\Omega\subset\mathbb{R}^N smooth, bounded and strongly convex: a functional LL is nonpositive on all convex functions if and only if L=−∂ijμijL=-\partial_{ij}\mu_{ij} in the sense of distributions for some matrix (μij)(\mu_{ij}) of bounded Radon measures that is symmetric and positive semidefinite as a matrix. This representation yields the Euler–Lagrange equation for variational problems under a convexity constraint, the matrix measure μ\mu acting as the Lagrange multiplier for the constraint. The open problem is the regularity and structure one can expect for this matrix measure. In dimension one the multiplier is essentially a scalar nonnegative measure and the regularity theory is settled, but for N≥2N\ge 2 the representing measure is not unique in general, and the sharpness examples in Lions's note exhibit representing measures whose densities are merely L2L^2 (failing LpL^p for all p>2p>2) or that are singular with respect to Lebesgue measure. Whether one can always select a representing measure with improved regularity — absolute continuity, higher integrability, or Sobolev membership — or whether some LL force singular or minimally integrable representatives, and how the structure of μ\mu relates to the geometry of Ω\Omega and to LL, remains unresolved: literature up to 2024–2025 describes the structure of μ\mu as still mysterious and develops Abreu-equation approximations precisely to bypass it.

Background

Many variational problems in physics and economics are posed over classes of convex functions: Newton's problem of the minimal resistance of a body and the monopolist's (multidimensional screening) problem in economics both lead to minimizing an integral functional over the set of convex functions on a domain. Writing optimality conditions for such problems is obstructed by the fact that the convexity constraint is an inequality on the second derivatives of the unknown, not a standard pointwise or boundary constraint.

For a closed convex cone KK in a Hilbert space, the dual (polar) cone is the set K⊥K^\perp of all LL with ⟨L,u⟩≤0\langle L,u\rangle\le 0 for every u∈Ku\in K. When KK is the cone of convex functions, elements of K⊥K^\perp play the role of generalized Lagrange multipliers for the convexity constraint: the first-order condition of a constrained problem says that the ordinary Euler–Lagrange term of the variation must be balanced by some L∈K⊥L\in K^\perp evaluated on admissible perturbations. A usable optimality theory therefore requires an explicit description of K⊥K^\perp.

It is classical that the second distributional derivatives of a convex function are Radon measures (finite, regular Borel measures) and that the resulting Hessian matrix measure is symmetric positive semidefinite, meaning that ξT(D2u)ξ≥0\xi^T(D^2u)\xi\ge 0 as a measure for every constant vector ξ\xi. Lions's 1998 note identifies the dual cone in exactly this language: if Ω⊂RN\Omega\subset\mathbb{R}^N is smooth, bounded and strongly convex and KK is the set of convex functions in L2(Ω)L^2(\Omega), then L∈K⊥L\in K^\perp if and only if there exist bounded Radon measures μij\mu_{ij} on Ω\Omega, with the matrix (μij)(\mu_{ij}) symmetric and positive semidefinite as a matrix of measures, such that L=−∂ijμijL=-\partial_{ij}\mu_{ij} in the sense of distributions, the pairing being ∫ΩLv dx=−∫∂ijv dμij\int_\Omega Lv\,dx=-\int\partial_{ij}v\,d\mu_{ij} for every v∈C2(Ω‾)v\in C^2(\overline{\Omega}) (repeated indices are summed). The note also proves a priori estimates on μ\mu in terms of ∥L∥L2\|L\|_{L^2} — weighted integrability against powers of a convex defining function Φ\Phi of Ω\Omega (a smooth function with Ω={Φ<0}\Omega=\{\Phi<0\} and D2Φ>0D^2\Phi>0), a Morrey-type bound (after Morrey's classical estimates controlling a measure's mass in balls) on the total variation of μ\mu, and, when μ\mu is absolutely continuous, an LN/(N−1)L^{N/(N-1)} bound on (det⁡μ)1/N(\det\mu)^{1/N} reminiscent of Monge–Ampère regularity — together with analogous representations for the dual cones in H1H^1 and H−1H^{-1} (the Sobolev space with zero trace and its dual) and for cones combining convexity with positivity and coordinatewise monotonicity. As an application, the minimizer uu of a Dirichlet energy with linear forcing terms over convex functions in H01(Ω)H^1_0(\Omega) satisfies −Δu=f+∂ifi+∂ijμij-\Delta u=f+\partial_i f_i+\partial_{ij}\mu_{ij} together with a complementarity condition: the Lebesgue part of μ\mu is supported where the convexity of uu degenerates (Tr⁡(d2u⋅μ0)=0\operatorname{Tr}(d^2u\cdot\mu^0)=0 a.e., where d2ud^2u and μ0\mu^0 denote the Lebesgue parts of the Hessian of uu and of μ\mu). The matrix measure μ\mu is thus exactly the Lagrange multiplier of the convexity constraint.

What is missing is any real understanding of the regularity of μ\mu. In dimension N=1N=1 the multiplier reduces to a scalar nonnegative measure (L=−μ′′L=-\mu'' with μ≥0\mu\ge 0, determined up to an affine function by positivity), and regularity questions in one dimension — and in the radial case — were settled in subsequent work of Carlier (J. Nonlinear Convex Anal. 3 (2002) 125–143). For N≥2N\ge 2 the representing measure is not unique in general, and the sharpness examples in Lions's note show that representing measures with limited regularity genuinely occur: densities that belong to L2L^2 but to no LpL^p with p>2p>2, and measures singular with respect to Lebesgue measure. Whether these examples are the last word — that is, whether for every L∈K⊥L\in K^\perp one can select a representing μ\mu with better regularity, and what the structure of the admissible measures is in terms of Ω\Omega and LL — is the open problem. Its difficulty is underscored by the later literature: Le (Comm. Pure Appl. Math. 73 (2020) 2248–2283) writes that the structure of μ\mu is 'still mysterious', and Wang–Zhou (arXiv 2403.04235) note that 'very little is known about the measure μ\mu', which is why minimizer regularity via the Euler–Lagrange equation is 'still inaccessible'; instead, an entire research program approximates the constrained problems by fourth-order Abreu-type equations (equations of Monge–Ampère type involving the logarithm of the Hessian determinant, used as a barrier for the constraint) in order to bypass μ\mu.

Problem Statement

For Ω⊂RN\Omega\subset\mathbb{R}^N with N≥2N\ge 2 smooth, bounded and strongly convex, let KK denote the set of convex functions in L2(Ω)L^2(\Omega), and let K⊥K^\perp denote the set of all L∈L2(Ω)L\in L^2(\Omega) such that ∫ΩLu dx≤0\int_\Omega Lu\,dx\le 0 for every u∈Ku\in K. By Lions's theorem, every L∈K⊥L\in K^\perp is represented as L=−∂ijμijL=-\partial_{ij}\mu_{ij} in the sense of distributions by a matrix (μij)(\mu_{ij}) of bounded Radon measures on Ω\Omega that is symmetric and positive semidefinite as a matrix of measures. The problem is to determine the regularity and structure one can expect for this representing matrix measure, that is, to give a rigorous description of the admissible representing measures. The question encompasses the following interconnected aspects, which share this single objective:

(1) Selection and regularity. Since for N≥2N\ge 2 the representing measure is not uniquely determined by LL, determine whether one can always select a representing μ\mu with improved regularity — for instance absolutely continuous with respect to Lebesgue measure, with density in LpL^p for some p>2p>2, or in a Sobolev class — or whether there exist L∈K⊥L\in K^\perp for which every representing measure is singular with respect to Lebesgue measure or has minimal integrability. The sharpness examples in Lions's note (representing measures with densities in L2L^2 but in no LpL^p with p>2p>2, and singular representing measures) show that limited regularity occurs for the constructed representatives; whether the full class of representing measures for such LL — and for general LL — is necessarily of limited regularity, or can be improved by selection, is the question.

(2) Structure. Give a refined description of the class of representing measures for given LL (equivalently, of the admissible perturbations σ\sigma of a representing measure μ\mu, that is, of the symmetric matrices σ=(σij)\sigma=(\sigma_{ij}) of bounded Radon measures for which μ+σ\mu+\sigma is again positive semidefinite and represents the same LL; determining precisely the constraints defining this class — the divergence-type identity ∂ijσij=0\partial_{ij}\sigma_{ij}=0 and any further conditions imposed by the pairing in Lions's theorem — is part of the question), of its singular and absolutely continuous parts, of the boundary behavior relative to the defining function of Ω\Omega, and of how this structure depends on the geometry of Ω\Omega and on LL.

(3) Consequences for the multiplier. In the Euler–Lagrange equation −Δu=f+∂ifi+∂ijμij-\Delta u=f+\partial_i f_i+\partial_{ij}\mu_{ij} for convexity-constrained variational problems (with the complementarity condition tying the Lebesgue part of μ\mu to the degeneracy set of uu's convexity), determine the corresponding structure and regularity of the multiplier μ\mu.

The one-dimensional case is excluded (there the multiplier is essentially a scalar nonnegative measure and the regularity theory is settled); the problem concerns dimension N≥2N\ge 2. No restriction on LL, on Ω\Omega beyond the stated class, or on the form of the answer is intended: the target is a mathematically rigorous characterization — positive selection theorems, negative constructions, or structural descriptions — of the achievable regularity of the representing matrix measure.

References

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