Elliptic geometric variational problems


Opportunities

Team members

Papers

Project description

Introduction

In the theory of optimisation one studies configurations of objects which are optimal in some predefined sense. If the set of competitors is closed under smooth deformations and optimality is expressed in terms of an energy functional, then one can use methods of calculus of variations to find a minimiser, or just a critical point, of the energy. I am mainly interested in optimising shapes of subsets of Rn. A typical example is the Plateau problem where one is interested in finding a surface in R3 of smallest possible area among all surfaces with a given boundary curve. Another example is the isoperimetric problem which is about describing an open set in Rn which minimises the perimeter (i.e. (n1) dimensional area of the boundary) among all open sets of volume equal one. These two classical and well understood problems give rise to many others, e.g., by considering arbitrary dimension and co-dimension, modelling the notions of surface and boundary with various objects, or by changing the way area is defined. Of course, studying the structure and regularity of critical points is a lot harder than the same for minimisers. The ultimate tool, tailored to tackle these kind of problems, is the theory of varifolds (cf. [Allard1972]) which can be thought of as currents deprived of orientation.

If TG(n,k) is a k-dimensional linear subspace of Rn, a non-zero translation invariant (inside T) Radon measure over T must be a constant multiple of the Lebesgue measure which coincides with HkT, where Hk is the k-Hausdorff measure over Rn; hence, a choice of a positive constant for each TG(n,k) gives rise to a k-dimensional measure over Rn. More precisely, let F:G(n,k)(0,) be continuous. The measure ΦF is defined first for k-dimensional “polyhedral surfaces” S=i=1Si, where each Si is a Borel subset of some TiG(n,k), by ΦF(S)=i=1F(Ti)Hk(Si). Next, one extends ΦF to all k-submanifolds of Rn by approximation and to all countably k-rectifiable sets by countable additivity. For purely k-unrectifiable sets S one can set ΦF(S)=0. This motivates the study of anisotropic energies of the form ΦF(M)=MF(Tan(M,x))θ(x)dHk(x), where MRn is countably k-rectifiable and θ:M[0,) is a Borel multiplicity (or density) function.

Assume URn is open and MU is as above and has locally finite Hk-measure. Adopting the viewpoint that ΦF defines an action of the Radon measure V over U×G(n,k), given for Borel sets AU×G(n,k) by V(A)=1{x:(x,T)A,T=Tan(M,x)}θdHk, on the function [U×G(n,k)(x,T)F(T)], we arrive at the definition of a rectifiable k-varifold in U. If imθZ, we say that V is integral. The weight measure, denoted V, is the projection of V onto U.

Let us emphasise that some very classical measures may be expressed as ΦF for an appropriate choice of F, e.g., given a non-euclidean norm on Rn the corresponding anisotropic k-Hausdorff measure coincides (on countably k-rectifiable sets) with ΦF provided F is the Busemann-Hausdorff integrand and the anisotropic symplectic measure is produced by the Holmes-Thompson integrand; see [APT2004].

Scientific goal of the project

Almost everywhere regularity of minima of ΦF has been proven by Almgren under the assumption that F is elliptic; cf. [Almgren1968 §1.6(2) and §1.4]. His ellipticity condition is a natural counterpart of quasi-convexity of Morrey; cf. [Morrey1966 p. 18] and [DRT2022 Proposition 3.13]. However, it is rather hard to check so that no examples of elliptic integrands in high co-dimension are known apart from the area integrand and its class 2 neighbourhood. Regularity of critical points is still an open problem. Recently the atomic condition (abbreviated AC) was introduced in [DPDRG2018] as a necessary and sufficient condition for rectifiability of critical points. It is stronger than Almgren’s ellipticity as we showed in [DRK2022]. Some partial results in high co-dimension concerning existence of non-trivial AC integrands and regularity of critical points were obtained by De Rosa and Tione [DT2022] but the most important questions remain still open.

The main goal of the project is to expand the regularity theory for critical points of ΦF in any co-dimension by exploiting the atomic condition. In co-dimension one (uniform) ellipticity is the same as strict (uniform) convexity (see [DPDRG2018 Theorem 1.3]) but focusing on convexity distracts attention from the true nature of ellipticity, which is a more subtle notion. I am strongly convinced that AC reveals the hidden geometric structure of ellipticity and deep understanding of this condition will lead to solving (at least partially) some of the big questions mentioned in the next section.

Significance of the project

The regularity theory for critical points of the area integrand (i.e. F1) rests on the monotonicity formula which implies Ahlfors regularity; cf. [Allard1972 5.1]. For anisotropic integrands this formula is inaccessible; cf. [Allard1974]. Ellipticity for F was defined by Almgren [Almgren1968] so to prove partial regularity for minimisers of ΦF. His proof employs a form of the isoperimetric inequality, which is provable for minimisers and acts as replacement for monotonicity. Allard [Allard1986] showed partial regularity for critical points V assuming nk=1, the integrand is uniformly convex, and the set of points of positive V-density is closed. The last condition is crucial and would follow from monotonicity.

The essential question, that is now open for more than 50 years and that prevents any substantial progress, is how to derive density ratio bounds for F-stationary varifolds under an ellipticity condition on F? The most promising route seems to lead via the isoperimetric inequality.

According to Almgren’s definition, F is elliptic if any flat k-disc D minimises ΦF among all countably k-rectifiable surfaces that cannot be retracted onto the relative boundary of D. Another, great problem is the very existence of elliptic integrands which are not just perturbations of the area integrand. In particular, it is not known whether the anisotropic k-Hausdorff measure constructed from some non-euclidean norm is elliptic. In case k=2 and surfaces are understood as Lipschitz integral chains, this has been resolved by Burago and Ivanov [BI2012]. Note that ellipticity heavily depends on the precise definition of a surface. In case we are considering only integral currents, then uniform convexity of the integrand (now being a norm on kRn) is sufficient for uniform ellipticity in any co-dimension but an analogous fact is not yet proven in case surfaces are allowed to be more general objects; cf. [Federer1969 §5.1.2].

In co-dimension one (uniform) ellipticity is equivalent to (uniform) strict convexity of the norm naturally associate with F; cf. [DPDRG2018 Theorem 1.3] and [Almgren1968 §5.7]. In case F is of class 2 critical points of the associated isoperimetric functional are then classified as finite sums of Wulff shapes; cf. [HLMG2009] and also our recent work [DRKS2020]. In this context, however, the most interesting are crystalline energies, where the integrand is only Lipschitz continuous; cf. [Taylor2002]. Characterisation of critical points of these kind of energies is yet another outstanding problem; cf. [DMv1]. We call it the anisotropic Alexandrov’s problem.

Assume F is of class 2. In this case one can define the principal F-curvatures of a hypersurface; cf. [DRKS2020 Definition 2.26]. If the total F-variation measure of a varifold V is Radon, then one defines the mean F-curvature vector of V using the Radon-Nikodym and a Riesz-type representation theorems. Assume U is an open set with smooth boundary M. We say that a maximum principle holds if any k-varifold in U that touches M at a point a has mean F-curvature at a bigger than the sum of k greatest principle F-curvatures of M at a. This holds in co-dimension one given F is smooth and uniformly convex; cf. [SW1989]. In higher co-dimension this is resolved only for the area integrand; cf. [White2010]. Maximum principle for other integrands and high co-dimension is still an open problem. Proving it could potentially lead to a generalisation of Allard’s co-dimension one theory [Allard1986]; in particular, the part where he is using barriers to prove a local height bound.

Bibliography