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Extremals for Poincaré-Sobolev sharp constants in Steiner symmetric sets

Lorenzo Brasco, Luca Briani, Francesca Prinari

TL;DR

We prove that open Steiner symmetric sets $\Omega\subset \mathbb{R}^N$, possibly unbounded, admit minimizers for the sharp Poincaré-Sobolev constant $\lambda_{p,q}(\Omega)$ and that the corresponding extremals solve the Lane-Emden equation $-\Delta_p u=\lambda_{p,q}(\Omega)|u|^{q-2}u$. Existence is obtained via an elementary Direct Method using a vanishing confinement perturbation and Steiner symmetrization to regain compactness, together with a uniform Harnack principle and Brézis–Lieb arguments to pass to the limit; minimizers exhibit exponential decay with rates determined by the underlying geometry, notably the inradius $r_\Omega$. A sharp geometric lower bound $\lambda_{p,q}(\Omega)\ge c(1/r_\Omega)^{N-p-\frac{p}{q}N}$ is established, and the results are illustrated with concrete examples and counterexamples highlighting the necessity of Steiner symmetry and convexity assumptions. Additionally, decay at infinity is developed for general nonnegative Lane-Emden subsolutions, with a Steiner-symmetric refinement yielding geometry-dependent, uniform decay constants for extremals.

Abstract

We prove existence of minimizers for the sharp Poincaré-Sobolev constant in general Steiner symmetric sets, in the subcritical and superhomogeneous regime. The sets considered are not necessarily bounded, thus the relevant embeddings may suffer from a lack of compactness. We prove existence by means of an elementary compactness method. We also prove an exponential decay at infinity for minimizers, showing that in the case of Steiner symmetric sets the relevant estimates only depend on the underlying geometry. Finally, we illustrate the optimality of the existence result, by means of some examples.

Extremals for Poincaré-Sobolev sharp constants in Steiner symmetric sets

TL;DR

We prove that open Steiner symmetric sets , possibly unbounded, admit minimizers for the sharp Poincaré-Sobolev constant and that the corresponding extremals solve the Lane-Emden equation . Existence is obtained via an elementary Direct Method using a vanishing confinement perturbation and Steiner symmetrization to regain compactness, together with a uniform Harnack principle and Brézis–Lieb arguments to pass to the limit; minimizers exhibit exponential decay with rates determined by the underlying geometry, notably the inradius . A sharp geometric lower bound is established, and the results are illustrated with concrete examples and counterexamples highlighting the necessity of Steiner symmetry and convexity assumptions. Additionally, decay at infinity is developed for general nonnegative Lane-Emden subsolutions, with a Steiner-symmetric refinement yielding geometry-dependent, uniform decay constants for extremals.

Abstract

We prove existence of minimizers for the sharp Poincaré-Sobolev constant in general Steiner symmetric sets, in the subcritical and superhomogeneous regime. The sets considered are not necessarily bounded, thus the relevant embeddings may suffer from a lack of compactness. We prove existence by means of an elementary compactness method. We also prove an exponential decay at infinity for minimizers, showing that in the case of Steiner symmetric sets the relevant estimates only depend on the underlying geometry. Finally, we illustrate the optimality of the existence result, by means of some examples.
Paper Structure (19 sections, 20 theorems, 301 equations, 4 figures)

This paper contains 19 sections, 20 theorems, 301 equations, 4 figures.

Key Result

Lemma 2.1

Let $0<\alpha<1$, for every $A,B>0$ we have

Figures (4)

  • Figure 1: The pinched slab $\Omega^-_\varepsilon$ of Example \ref{['exa:pinchedslab']}, with inward pinching. The constant $\lambda_{p,q}(\Omega^-_\varepsilon)$ is not attained.
  • Figure 2: The pinched slab $\Omega^+_\varepsilon$ of Example \ref{['exa:pinchedslab']}, with outward pinching. This is a Steiner symmetric set and the constant $\lambda_{p,q}(\Omega^+_\varepsilon)$ is attained, thanks to Theorems \ref{['teo:main']} and \ref{['teo:maininfty']}.
  • Figure 3: An unbounded Steiner symmetric set in $\mathbb{R}^3$, exhibiting three different behaviours "at infinity", according to the coordinate directions. In particular, we have that $\Omega$ shrinks at infinity in direction $\mathbf{e}_1$; it is bounded in direction $\mathbf{e}_2$ and it is tubular at infinity in direction $\mathbf{e}_3$.
  • Figure 4: The set $E$ in Remark \ref{['rem:nolip']}. Near the boundary point marked by a black dot, the gradient of the solution blows-up.

Theorems & Definitions (55)

  • Remark 1.1: The case $q\le p$
  • Remark 1.2: Breaking Steiner symmetry
  • Remark 1.3: Uniqueness
  • Lemma 2.1
  • proof
  • Proposition 2.2
  • proof
  • Lemma 2.3
  • proof
  • Definition 3.1: The class $\mathfrak{S}^N$
  • ...and 45 more