Local Polya fluctuations of Riesz gravitational fields and the Cauchy problem

IF 1 Q1 MATHEMATICS
V. Litovchenko
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引用次数: 0

Abstract

We consider a pseudodifferential equation of parabolic type with a fractional power of the Laplace operator of order $\alpha\in(0;1)$ acting with respect to the spatial variable. This equation naturally generalizes the well-known fractal diffusion equation. It describes the local interaction of moving objects in the Riesz gravitational field. A simple example of such system of objects is stellar galaxies, in which interaction occurs according to Newton's gravitational law. The Cauchy problem for this equation is solved in the class of continuous bounded initial functions. The fundamental solution of this problem is the Polya distribution of probabilities $\mathcal{P}_\alpha(F)$ of the force $F$ of local interaction between these objects. With the help of obtained solution estimates the correct solvability of the Cauchy problem on the local field fluctuation coefficient under certain conditions is determined. In this case, the form of its classical solution is found and the properties of its smoothness and behavior at the infinity are studied. Also, it is studied the possibility of local strengthening of convergence in the initial condition. The obtained results are illustrated on the $\alpha$-wandering model of the Lévy particle in the Euclidean space $\mathbb{R}^3$ in the case when the particle starts its motion from the origin. The probability of this particle returning to its starting position is investigated. In particular, it established that this probability is a descending to zero function, and the particle "leaves" the space $\mathbb{R}^3$.
Riesz引力场的局部Polya涨落与Cauchy问题
我们考虑一个抛物型伪微分方程,其阶为$\alpha\in(0;1)$的拉普拉斯算子的分数次作用于空间变量。这个方程自然地推广了众所周知的分形扩散方程。它描述了在Riesz引力场中运动物体的局部相互作用。这种天体系统的一个简单例子是恒星星系,其中根据牛顿引力定律发生相互作用。该方程的柯西问题在连续有界初始函数中得到了求解。这个问题的基本解决方案是这些物体之间局部相互作用的力F的概率的Polya分布。利用得到的解估计,确定了柯西问题在一定条件下对局部场波动系数的正确可解性。在这种情况下,得到了它的经典解的形式,并研究了它在无穷远处的光滑性和行为。同时,研究了在初始条件下局部增强收敛的可能性。在欧几里得空间$\mathbb{R}^3$中,当粒子从原点开始运动时,用$\alpha$-漫游模型说明了所得到的结果。研究了该粒子返回起始位置的概率。特别地,它确定了这个概率是一个降至零的函数,并且粒子“离开”空间$\mathbb{R}^3$。
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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来源期刊
CiteScore
1.90
自引率
12.50%
发文量
31
审稿时长
25 weeks
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