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Concentration of mean exit times

G. Pacelli Bessa, Vicent Gimeno i Garcia, Vicente Palmer

Abstract

The mean exit time function defined on the $δ$-tube around any equator $\mathbb{S}^{n-1} \subseteq \mathbb{S}^{n}$ of the sphere $\mathbb{S}^{n}$, ($0<δ<π/2$), goes to infinity with the dimension, so that when we consider a Brownian particle that begins its motion at one equator of the sphere, this particle will remain near this equator for an almost infinite amount of time when the dimension of the sphere goes to infinity. On the other hand, if the Brownian particle begins its motion at the North pole, then this particle will leave quickly, when the dimension of the sphere goes to infinity, any geodesic ball with radius $δ<π/2$, centered at this point. Namely, the mean exit time function defined on the equatorial tubes presents a kind of {\em concentration} phenomenon or {\em fat equator} effect, as it has been described in the book \cite{MS}. Moreover, the same concentration phenomenon occurs when we consider this mean exit time function defined on tubes around closed and minimal hypersurfaces of a compact Riemannian $n$-manifold $M$ with Ricci curvature bounded from below, ${\rm Ric}_{M}\geq (n-1)$. Namely, a Brownian particle that begins its random movement around a closed embedded minimal hypersurface of a compact $n$-manifold $M$ with ${\rm Ric}_{M}\geq (n-1)$ will wanders arbitrarily close to the hypersurface for a time that approaches infinity as the dimension of the ambient manifold does so as well.

Concentration of mean exit times

Abstract

The mean exit time function defined on the -tube around any equator of the sphere , (), goes to infinity with the dimension, so that when we consider a Brownian particle that begins its motion at one equator of the sphere, this particle will remain near this equator for an almost infinite amount of time when the dimension of the sphere goes to infinity. On the other hand, if the Brownian particle begins its motion at the North pole, then this particle will leave quickly, when the dimension of the sphere goes to infinity, any geodesic ball with radius , centered at this point. Namely, the mean exit time function defined on the equatorial tubes presents a kind of {\em concentration} phenomenon or {\em fat equator} effect, as it has been described in the book \cite{MS}. Moreover, the same concentration phenomenon occurs when we consider this mean exit time function defined on tubes around closed and minimal hypersurfaces of a compact Riemannian -manifold with Ricci curvature bounded from below, . Namely, a Brownian particle that begins its random movement around a closed embedded minimal hypersurface of a compact -manifold with will wanders arbitrarily close to the hypersurface for a time that approaches infinity as the dimension of the ambient manifold does so as well.
Paper Structure (7 sections, 7 theorems, 98 equations, 1 figure)

This paper contains 7 sections, 7 theorems, 98 equations, 1 figure.

Table of Contents

  1. Introduction
  2. Tubes around submanifolds
  3. Proof of Theorem \ref{['thmmain']}
  4. Proof of Corollary \ref{['thmmain2']}
  5. Proof of Theorem \ref{['thmmain3']}
  6. Proof of Corollary \ref{['cor:moments']}
  7. Proof of Corollary \ref{['teo:Shiohama']}

Key Result

Theorem 1.1

Let us consider the tube $T_\delta(\mathbb{S}^{n-1}) \subseteq \mathbb{S}^{n}$, of radius $\delta \in (0,\pi/2)$, around the totally geodesic submanifold $\varphi: \mathbb{S}^{n-1} \rightarrow \mathbb{S}^{n}$, and the geodesic ball $B_{\pi/2-\delta}(p_N) \subseteq \mathbb{S}^{n}$ centered at the nor

Figures (1)

  • Figure 1: Tube $T_\delta(\mathbb{S}^{n-1})$ of radius $\delta$ around the equator $\mathbb{S}^{n-1}$ and geodesic balls $B_{\pi/2-\delta}(p_N)$, $B_{\pi/2-\delta}(p_S)$ of radius $\pi/2-\delta$ centered at the north ans south pole respectively.

Theorems & Definitions (11)

  • Theorem 1.1
  • Corollary 1.1
  • Theorem 1.2
  • Remark 1.2
  • Corollary 1.3
  • Corollary 1.4
  • Definition 2.1
  • Remark 2.2
  • Proposition 3.1
  • proof
  • ...and 1 more