Convexity of level sets for solutions to nonlinear elliptic problems in convex rings. Paola Cuoghi and Paolo Salani

Similar documents
Brunn-Minkowski inequality for the 1-Riesz capacity and level set convexity for the 1/2-Laplacian

Asymptotic behavior of infinity harmonic functions near an isolated singularity

Brunn-Minkowski inequalities for two functionals involving the p-laplace operator

VISCOSITY SOLUTIONS OF ELLIPTIC EQUATIONS

Brunn-Minkowski inequality for the 1-Riesz capacity and level set convexity for the 1/2-Laplacian

Convex Functions and Optimization

Numerical Solutions of Geometric Partial Differential Equations. Adam Oberman McGill University

Asymptotic Behavior of Infinity Harmonic Functions Near an Isolated Singularity

VISCOSITY SOLUTIONS. We follow Han and Lin, Elliptic Partial Differential Equations, 5.

On a Fractional Monge Ampère Operator

SYMMETRY OF POSITIVE SOLUTIONS OF SOME NONLINEAR EQUATIONS. M. Grossi S. Kesavan F. Pacella M. Ramaswamy. 1. Introduction

Gradient Estimate of Mean Curvature Equations and Hessian Equations with Neumann Boundary Condition

Example 1. Hamilton-Jacobi equation. In particular, the eikonal equation. for some n( x) > 0 in Ω. Here 1 / 2

COINCIDENCE SETS IN THE OBSTACLE PROBLEM FOR THE p-harmonic OPERATOR

Asymptotic behavior of the degenerate p Laplacian equation on bounded domains

The general programming problem is the nonlinear programming problem where a given function is maximized subject to a set of inequality constraints.

A LOCALIZATION PROPERTY AT THE BOUNDARY FOR MONGE-AMPERE EQUATION

Centre for Mathematics and Its Applications The Australian National University Canberra, ACT 0200 Australia. 1. Introduction

On Generalized and Viscosity Solutions of Nonlinear Elliptic Equations

On John type ellipsoids

Local strong convexity and local Lipschitz continuity of the gradient of convex functions

Eigenfunctions for versions of the p-laplacian

TOPICS IN NONLINEAR ANALYSIS AND APPLICATIONS. Dipartimento di Matematica e Applicazioni Università di Milano Bicocca March 15-16, 2017

MEAN VALUE PROPERTY FOR p-harmonic FUNCTIONS

REGULARITY RESULTS FOR THE EQUATION u 11 u 22 = Introduction

A VARIATIONAL METHOD FOR THE ANALYSIS OF A MONOTONE SCHEME FOR THE MONGE-AMPÈRE EQUATION 1. INTRODUCTION

Class Meeting # 1: Introduction to PDEs

SHARP BOUNDARY TRACE INEQUALITIES. 1. Introduction

Hausdorff Continuous Viscosity Solutions of Hamilton-Jacobi Equations

Obstacle Problems Involving The Fractional Laplacian

Dedicated to Professor Linda Rothchild on the occasion of her 60th birthday

arxiv: v1 [math.ap] 18 Jan 2019

1 Convexity, concavity and quasi-concavity. (SB )

A Brunn Minkowski inequality for the Hessian eigenvalue in three-dimensional convex domain

Degenerate Monge-Ampère equations and the smoothness of the eigenfunction

HESSIAN MEASURES III. Centre for Mathematics and Its Applications Australian National University Canberra, ACT 0200 Australia

On a weighted total variation minimization problem

Written Examination

COMPARISON PRINCIPLES FOR CONSTRAINED SUBHARMONICS PH.D. COURSE - SPRING 2019 UNIVERSITÀ DI MILANO

AN INTRODUCTION TO VISCOSITY SOLUTION THEORY. In this note, we study the general second-order fully nonlinear equations arising in various fields:

Integro-differential equations: Regularity theory and Pohozaev identities

PROD. TYPE: COM ARTICLE IN PRESS. Andrea Colesanti. Received 4 August 2003; accepted 8 June 2004 Communicated by Michael Hopkins

GERARD AWANOU. i 1< <i k

On the second differentiability of convex surfaces

Applications of the periodic unfolding method to multi-scale problems

EQUAZIONI A DERIVATE PARZIALI. STEKLOV EIGENVALUES FOR THE -LAPLACIAN

Fast convergent finite difference solvers for the elliptic Monge-Ampère equation

Lecture No 2 Degenerate Diffusion Free boundary problems

Convex analysis and profit/cost/support functions

On the spectrum of the Hodge Laplacian and the John ellipsoid

1. Introduction Boundary estimates for the second derivatives of the solution to the Dirichlet problem for the Monge-Ampere equation

Convex Optimization. Convex Analysis - Functions

Appeared in Commun. Contemp. Math. 11 (1) (2009) ZERO ORDER PERTURBATIONS TO FULLY NONLINEAR EQUATIONS: COMPARISON, EXISTENCE AND UNIQUENESS

GENERALIZED CONVEXITY AND OPTIMALITY CONDITIONS IN SCALAR AND VECTOR OPTIMIZATION

Lecture Introduction

AN ASYMPTOTIC MEAN VALUE CHARACTERIZATION FOR p-harmonic FUNCTIONS

INTERIOR CURVATURE BOUNDS FOR A CLASS OF CURVATURE EQUATIONS

The location of the hot spot in a grounded convex conductor

CONVEX SOLUTIONS OF ELLIPTIC DIFFERENTIAL EQUATIONS IN CLASSICAL DIFFERENTIAL GEOMETRY. 1. Introduction

MATH Final Project Mean Curvature Flows

N. L. P. NONLINEAR PROGRAMMING (NLP) deals with optimization models with at least one nonlinear function. NLP. Optimization. Models of following form:

Fifth Abel Conference : Celebrating the Mathematical Impact of John F. Nash Jr. and Louis Nirenberg

Comparison Results for Semilinear Elliptic Equations in Equimeasurable Domains

ALEKSANDROV-TYPE ESTIMATES FOR A PARABOLIC MONGE-AMPÈRE EQUATION

Math 328 Course Notes

On the definition and properties of p-harmonious functions

Lecture 2: Convex functions

Lecture Unconstrained optimization. In this lecture we will study the unconstrained problem. minimize f(x), (2.1)

PERTURBATION THEORY FOR NONLINEAR DIRICHLET PROBLEMS

SOLUTIONS OF NONLINEAR PDES IN THE SENSE OF AVERAGES

Differentiable Functions

AN ASYMPTOTIC MEAN VALUE CHARACTERIZATION FOR p-harmonic FUNCTIONS. To the memory of our friend and colleague Fuensanta Andreu

Math (P)Review Part II:

Murat Akman. The Brunn-Minkowski Inequality and a Minkowski Problem for Nonlinear Capacities. March 10

Flux-limited solutions for quasi-convex Hamilton-Jacobi equations on networks

A BOUNDARY VALUE PROBLEM FOR MINIMAL LAGRANGIAN GRAPHS. Simon Brendle & Micah Warren. Abstract. The associated symplectic structure is given by

Sébastien Chaumont a a Institut Élie Cartan, Université Henri Poincaré Nancy I, B. P. 239, Vandoeuvre-lès-Nancy Cedex, France. 1.

Constrained Optimal Stopping Problems

Parabolic quasi-concavity for solutions to parabolic problems in convex rings

ON THE REGULARITY OF SAMPLE PATHS OF SUB-ELLIPTIC DIFFUSIONS ON MANIFOLDS

A Geometric Approach to Free Boundary Problems

Fractional convexity maximum principle

Lecture Notes (Math 90): Week IX (Thursday)

A CONNECTION BETWEEN A GENERAL CLASS OF SUPERPARABOLIC FUNCTIONS AND SUPERSOLUTIONS

Linear vector spaces and subspaces.

THE DIRICHLET PROBLEM FOR THE CONVEX ENVELOPE

EXISTENCE AND REGULARITY RESULTS FOR SOME NONLINEAR PARABOLIC EQUATIONS

U.C. Berkeley CS294: Spectral Methods and Expanders Handout 11 Luca Trevisan February 29, 2016

Around the Brunn-Minkowski inequality

SYMMETRY RESULTS FOR PERTURBED PROBLEMS AND RELATED QUESTIONS. Massimo Grosi Filomena Pacella S. L. Yadava. 1. Introduction

Motivation Power curvature flow Large exponent limit Analogues & applications. Qing Liu. Fukuoka University. Joint work with Prof.

Boundary value problems for the infinity Laplacian. regularity and geometric results

Elliptic stability for stationary Schrödinger equations by Emmanuel Hebey. Part III/VI A priori blow-up theories March 2015

Multiple positive solutions for a class of quasilinear elliptic boundary-value problems

Regularity of flat level sets in phase transitions

Landesman-Lazer type results for second order Hamilton-Jacobi-Bellman equations

PHASE TRANSITIONS: REGULARITY OF FLAT LEVEL SETS

arxiv: v1 [math.ap] 10 Apr 2013

REGULARITY OF SUBELLIPTIC MONGE-AMPÈRE EQUATIONS IN THE PLANE

A note on W 1,p estimates for quasilinear parabolic equations

Transcription:

Convexity of level sets for solutions to nonlinear elliptic problems in convex rings Paola Cuoghi and Paolo Salani Dip.to di Matematica U. Dini - Firenze - Italy 1

Let u be a solution of a Dirichlet problem of elliptic type in a domain Ω: { F (x, u, u, D 2 u) = 0 in Ω u = g on Ω - F is degenerate elliptic, i.e. F (x, t, p, A) F (x, t, p, B), for every A, B Γ such that A B, where A B means that B A is positive semidefinite. - F is proper, i.e. F (x, t, p, A) F (x, s, p, A) if s t. A quite natural question is the following: is there any relationship between the geometry of the domain Ω and the geometry of the solution u? Is it possible to find assumptions on the elliptic operator F which ensure that some geometric property of the domain is inherited, in some sense, by the solution? For instance, if the domain Ω is convex and the Dirichlet data is a constant, we may ask whether the function u must be convex too. 2

Precisely, the problem we are here involved with is the following: Ω is a convex ring, i.e. Ω = Ω 0 \ Ω 1 where Ω 0 and Ω 1 are convex, bounded and open subsets of R n such that Ω 1 Ω 0. u is a solution of the following Dirichlet problem F (x, u, u, D 2 u) = 0 in Ω u = 0 on Ω 0 u = 1 on Ω 1. (1) Hence, two level sets of the solution, are convex surfaces: namely, {u = 0} = Ω 0 and {u = 1} = Ω 1. MAIN QUESTION: Is it possible to find suitable assumptions on F which ensure that all the level sets of u are convex? 3

This problem and related questions have been faced by many authors; we recall, for instance, the classic work of Gabriel (1957) and more recent important contributions by Acker, Caffarelli, Korevaar, Lewis, Spruck, as well as many papers and a well-known monograph by Kawohl. The method here adopted is a generalization of the method introduced in [CS] - A. Colesanti & P. S. Quasi-concave Envelope of a Function and Convexity of Level Sets of Solutions to Elliptic Equations Math. Nach. 258 (2003), 3 15. It makes use of the quasi-concave envelope u of a function u. Roughly speaking, u is the function whose superlevel sets are the convex hulls of the corresponding superlevel sets of u (we sistematically extend u 1 in Ω 1 ), i.e. {u t} = conv({u t}. 4

Ω t = { u t } Ω t = { u t } Ω1= { u 1} Ω 0 = { u 0} More explicitely, we can define u in the following way: { u (x) = max min {u(x 1 ),..., u(x n+1 )} : x 1,..., x n+1 Ω, x = n+1 i=1 λ ix i, λ 1 0,..., λ n+1 0, } n+1 i=1 λ i = 1. 5

We look for conditions that imply u = u. Notice that u u by definition (to obtain u we enlarge the superlevel sets of u), then it suffices to prove the reverse inequality; the latter can be obtained by a suitable Comparison Principle, if u is a viscosity subsolution of problem (1). In this way we reduce ourselves to the following question: Can we find suitable assumptions on F that force u to be a viscosity subsolution of (1)? A positive answer was given in [CS], but only for operators whose principal can be decomposed in a normal and a tangential part (normal and tangential with respect to level sets of the solution, we mean). 6

Basically, the operators which share such a structure are: - the laplacian u = f(x, u, u ); - the p-laplacian p u = div( u p 2 u) = f(x, u, u ); - the mean curvature operator Mu = n(1 + u 2 ) 3/2 H = f(x, u, u ). There, we proved that under suitable concavity assumption on f, the solutions to Dirichlet problems in convex rings for these equations have convex level sets. Now we are able to treat much more general operator! In particular, we are able to treat the Hessian operators, defined, for k = 1,..., n, as the k-th elementary symmetric function of the eigenvalues of the Hessian matrix of u, i.e. for k = 1,..., n S k (D 2 u) = S k (λ 1,..., λ n ) = λ i1 λ ik 1 i 1 < <i k n where λ 1,..., λ n are the eigenvalues of D 2 u. 7

MAIN THEOREM. Let Ω = Ω 0 \Ω 1 be a convex ring and let F (x, u, θ, A) be a proper, continuous and degenerate elliptic operator in Ω (0, 1) R n Γ F. Assume that there exists p < 0 such that, for every p p and for every θ R n, the application ( ) (x, t, A) F x, tp, 1 tp 1 1 θ, tp 1 3 A (2) is concave in Ω (1, + ) Γ F. If u C 2 (Ω) C(Ω) is an admissible classical solution of (1) such that u > 0 in Ω, then u is a viscosity subsolution of (1). Remarks 1. The above theorem holds also for viscosity solutions. 2. The assumption u > 0 is typical for this kind of investigation; in fact, we can relax it a little bit, but not in an essential way. To prove geometric properties of solutions to elliptic problems without this assumption it is a difficult task. In fact, this assumption is often automatically satisfied by classical solutions, thanks to some maximum principle applied to u. 3. Admissible solution means that D 2 u(x) Γ F for every x Ω, i.e. u is an elliptic solution. 8

To prove the main theorem, we need some preliminaries. First of all we recall the notion of p-means of m nonnegative real numbers. Given a = (a 1,..., a m ) > 0, λ Λ m and p [, + ], the quantity [λ 1 a p 1 + + λ ma p m] 1/p for p, 0, + M p (a, λ) = max{a 1,..., a m } p = + a λ 1 1 aλ m m p = 0 min{a 1, a 2,..., a m } p = is the p-(weighted) mean of a. For a 0, we define M p (a, λ) as above if p 0 and we set M p (a, λ) = 0 if p < 0 and a i = 0, for some i = 1,..., m. Let us fix λ Λ n+1 and consider p [, + ]. Definition 0.1 The (p, λ) envelope of u is the function u p,λ : Ω [0, 1] defined as follows { u p,λ (x) = sup M p (u(x 1 ),..., u(x n+1 ), λ) : x i Ω, x = n+1 i=1 λ (3) ix i }. Notice that, as Ω is compact and M p is continuous, the supremum of the definition is in fact a maximum. 9

Hence, for every x Ω, there exist (x 1,p,..., x n+1,p ) Ω n+1 such that x = n+1 i=1 λ i x i,p, u p,λ (x) = M p (u(x 1 ),..., u(x n+1 ), λ). An immediate consequence of the definition is that u p,λ (x) u(x), x Ω, p [,, + ]; moreover, from the monotonicity of means, we have u p,λ (x) u q,λ (x), for p q, x Ω. For convenience, we will refer to u,λ as u λ. Notice that u (x) = sup {u λ(x) : λ Λ n+1 } (4) and the above supremum is in fact a maximum as Λ n+1 is compact. Theorem. u p,λ converge uniformly to u λ as p. 10

Sketch of the proof of the main thm. i. We fix λ Λ n+1 and we prove that, for every compact subset K of Ω, u p,λ is a viscosity subsolution, for p large enough (depending on K). ii. Then passing to the limit for p, thanks to uniform convergence, we obtain that u λ is a subsolution. iii. Thanks to (4) and since the supremum of subsolutions is a subsolution, the proof is concluded. How do we prove the first item? By definition, u p,λ is a viscosity subsolution of F = 0 if, for every C 2 function φ touching u p,λ from above at any point x Ω, it holds F (x, φ(x), φ(x), D 2 φ(x)) 0. If u is an admissible classical solution, this task is somewhat simplified, since u can be used as a test function. 11

Indeed, for every point x Ω, we can use u to construct a C 2 function ϕ p,λ that touches u p,λ from below at x. This function is defined as follows: [ n+1 ] 1/p ϕ p,λ (x) = λ i u (x i,p + a i,p (x x)) p, (5) where i=1 a i,p = u(x i,p) p u p,λ (x) p, for i = 1,..., n + 1, (6) and the points x i,p are the ones which realize the maximum in the definition of u p,λ (x). If all the points x 1,p,..., x n+1,p belong to Ω, we can write the gradient and the Hessian matrix of φ p,λ at the point x as a convex combination of the gradients and the Hessian matrices of u at these points and our concavity assumption on F makes the rest. But we cannot be sure, in general, that any one of these points belongs to Ω; notice that, if for some p we could be able to prove this, we would obtain that u coincide with its p-concave envelope and finally it is p-concave, which is of course much more than quasi-concave. On the other hand, it is easily seen that this actually happens for p =, hence restricting to any compact subset of Ω, we can prove that it must also happen for p enough large and this conclude the proof. 12