The largest fragment in self-similar fragmentation processes of positive index

Piotr Dyszewski, Samuel G. G. Johnston, Sandra Palau, Joscha Prochno
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Abstract

Take a self-similar fragmentation process with dislocation measure $\nu$ and index of self-similarity $\alpha > 0$. Let $e^{-m_t}$ denote the size of the largest fragment in the system at time $t\geq 0$. We prove fine results for the asymptotics of the stochastic process $(s_{t \geq 0}$ for a broad class of dislocation measures. In the case where the process has finite activity (i.e.\ $\nu$ is a finite measure with total mass $\lambda>0$), we show that setting \begin{equation*} g(t) :=\frac{1}{\alpha}\left(\log t - \log \log t + \log(\alpha \lambda)\right), \qquad t\geq 0, \end{equation*} we have $\lim_{t \to \infty} (m_t - g(t)) = 0$ almost-surely. In the case where the process has infinite activity, we impose the mild regularity condition that the dislocation measure satisfies \begin{equation*} \nu(1-s_1 > \delta ) = \delta^{-\theta} \ell(1/\delta), \end{equation*} for some $\theta \in (0,1)$ and $\ell:(0,\infty) \to (0,\infty)$ slowly varying at infinity. Under this regularity condition, we find that if \begin{equation*} g(t) :=\frac{1}{\alpha}\left( \log t - (1-\theta) \log \log t - \log \ell \left( \log t ~\ell\left( \log t \right)^{\frac{1}{1-\theta}} \right) + c(\alpha,\theta) \right), \qquad t\geq 0, \end{equation*} then $\lim_{t \to \infty} (m_t - g(t)) = 0$ almost-surely. Here $c(\alpha,\theta) := \log \alpha -(1-\theta)\log(1-\theta) - \log \Gamma(1-\theta)$. Our results sharpen significantly the best prior result on general self-similar fragmentation processes, due to Bertoin, which states that $m_t = (1+o(1)) \frac{1}{\alpha} \log t$.
正指数自相似破碎过程中的最大碎片
取一个自相似分裂过程,其错位度量为 $\nu$,自相似度指数为 $\alpha > 0$。让 $e^{-m_t}$ 表示时间 $t\geq 0$ 时系统中最大碎片的大小。我们证明了随机过程$(s_{t \geq 0}$对于一类广泛的位移度量的渐近性的精细结果。在过程具有有限活动的情况下(即\nu$是总质量为$\lambda>0$的有限度量)的情况下,我们证明 setting\begin{equation*} g(t) :=frac{1}\{alpha}\left(\log t -\log \log t +\log(\alpha \lambda)\right), \qquad t\geq 0, \end{equation*} 我们几乎可以肯定 $\lim_{t\to \infty} (m_t - g(t)) = 0$。在过程具有无限活动的情况下,我们施加了一个温和的规则性条件,即位错度量满足 \begin{equation*}\nu(1-s_1 > \delta ) = \delta^{-\theta}\ell(1/\delta), \end{equation*} for some $\theta \in (0,1)$ and$ell:(0,\infty) \to (0,\infty)$ slowly varying at infinity.在这个正则条件下,我们会发现如果g(t):=\frac{1}{alpha}\left((log t - (1-\theta) \log \log t - \log \ell \left(\log t ~\ell\left( (log t (right)^{\frac{1}{1-\theta}})\right) +c(\alpha,\theta) \right), \qquad t\geq 0, \end{equation*} 那么 $\lim_{t \to\infty} (m_t - g(t)) = 0$ 几乎是肯定的。这里 $c(\alpha,\theta) := \log \alpha-(1-\theta)\log(1-\theta) - \log \Gamma(1-\theta)$.我们的结果极大地改进了贝托因提出的关于一般自相似分裂过程的最佳先验结果,即 $m_t = (1+o(1)) \frac{1}\{alpha}\log t$。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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