具有慢势垒的远距离对称不相容的流体力学行为:超扩散状态

P. Cardoso, P. Gonccalves, Byron Jim'enez-Oviedo
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引用次数: 5

摘要

在本文中,我们分析了在有慢势垒存在的情况下,具有长跳跃的对称不相容过程的流体动力学行为。快速键的跳跃率由一个过渡概率$p(\cdot)$给出,它是对称的,具有有限的方差,而对于慢键,跳跃率给出$p(\cdot)\alpha n^{-\beta}$(与$\alpha>0$和$\beta\geq 0$),并对应于从$\mathbb{Z}_{-}^{*}$到$\mathbb N$的跳跃。证明了:如果在$\mathbb{Z}_{-}^{*}$和$\mathbb N$之间存在一个快键,则流体动力极限由无边界条件的热方程给出;否则,由上式给出,如果$0\leq \beta1$。
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Hydrodynamic behavior of long-range symmetric exclusion with a slow barrier: superdiffusive regime
In this article we analyse the hydrodynamical behavior of the symmetric exclusion process with long jumps and in the presence of a slow barrier. The jump rates for fast bonds are given by a transition probability $p(\cdot)$ which is symmetric and has finite variance, while for slow bonds the jump rates are given $p(\cdot)\alpha n^{-\beta}$ (with $\alpha>0$ and $\beta\geq 0$), and correspond to jumps from $\mathbb{Z}_{-}^{*}$ to $\mathbb N$. We prove that: if there is a fast bond from $\mathbb{Z}_{-}^{*}$ and $\mathbb N$, then the hydrodynamic limit is given by the heat equation with no boundary conditions; otherwise, it is given by the previous equation if $0\leq \beta<1$, but for $\beta\geq 1$ boundary conditions appear, namely, we get Robin (linear) boundary conditions if $\beta=1$ and Neumann boundary conditions if $\beta>1$.
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