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arXiv 2203.06003math.PRmath-phmath.APmath.MP
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一个奇异两相 Stefan 问题及通过其到达时间相互作用的粒子

A singular two-phase Stefan problem and particles interacting through their hitting times

Graeme Baker, Mykhaylo Shkolnikov

AI总结:

本文将一维奇异两相 Stefan 问题表述为耦合的 McKean-Vlasov SDE,并用有限粒子系统在 Skorokhod M1 拓扑下的大系统极限,在自由边界非单调条件下证明满足物理性条件的解存在。

摘要:

我们考虑一维空间中一个奇异两相 Stefan 问题的概率表述,它等价于两个 McKean-Vlasov 随机微分方程的耦合系统。在系统性风险的金融背景下,该系统模拟两个相互竞争的区域,其中包含大量面临违约风险的相互关联银行或公司。我们的主要结果证明了一个解的存在性,该解的间断点满足当前问题的自然物理性条件。因此,本工作扩展了文献 [DIRT15a]、[NS19a]、[HLS18]、[CRS20] 中关于一维奇异单相 Stefan 问题的一系列近期存在性结果。与这些工作相同,我们的存在性结果是通过有限粒子系统逼近在 Skorokhod M1 拓扑下的大系统极限获得的。但与此前研究的单相情形不同,此处的自由边界不是单调的,因此大系统极限需要通过一种新的论证来获得。

英文摘要:

We consider a probabilistic formulation of a singular two-phase Stefan problem in one space dimension, which amounts to a coupled system of two McKean-Vlasov stochastic differential equations. In the financial context of systemic risk, this system models two competing regions with a large number of interconnected banks or firms at risk of default. Our main result shows the existence of a solution whose discontinuities obey the natural physicality condition for the problem at hand. Thus, this work extends the recent series of existence results for singular one-phase Stefan problems in one space dimension that can be found in [DIRT15a], [NS19a], [HLS18], [CRS20]. As therein, our existence result is obtained via a large system limit of a finite particle system approximation in the Skorokhod M1 topology. But, unlike for the previously studied one-phase case, the free boundary herein is not monotone, so that the large system limit is obtained by a novel argument.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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