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On the continuity of Pickands constants

Published 21 May 2021 in math.PR | (2105.10435v1)

Abstract: For a non-negative separable random field Z(t),tR<sup>dZ(t), t\in \mathbb{R}<sup>d satisfying some mild assumptions we show that \begin{eqnarray*} H_Z\delta = \lim_{T\to\infty} \frac{1}{Td} E {\sup_{ t\in [0,T]d \cap \delta \mathbb{Z}d } Z(t) } <\infty \end{eqnarray*} for δ0\delta \ge 0 where 0Z<sup>d</sup>:=R<sup>d0 \mathbb{Z}<sup>d</sup> := \mathbb{R}<sup>d and prove that HZ<sup>0H_Z<sup>0 can be approximated by HZ<sup>δH_Z<sup>\delta if δ\delta tends to 0. These results extend the classical findings for the Pickands constants HZ<sup>δH_{Z}<sup>\delta, defined for Z(t)=exp(2Bα(t)t<sup>2α</sup>),tRZ(t)= \exp\left( \sqrt{ 2} B_\alpha (t)- |t|<sup>{2\alpha</sup> }\right), t\in \mathbb{R} with BαB_\alpha a standard fractional Brownian motion with Hurst parameter α(0,1]\alpha \in (0,1]. The continuity of HZ<sup>δH_{Z}<sup>\delta at δ=0\delta=0 is additionally shown for two particular extensions of Pickands constants.

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