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Perturbed Divisible Sandpiles and Quadrature Surfaces

机译:扰动可分的砂浆和正交表面

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The main purpose of the present paper is to establish a link between quadrature surfaces (potential theoretic concept) and sandpile dynamics (Laplacian growth models). For this aim, we introduce a new model of Laplacian growth on the lattice DOUBLE-STRUCK CAPITAL Zd (d >= 2) which continuously deforms occupied regions of the divisible sandpile model of Levine and Peres (J. Anal. Math. 111(1), 151-219 2010), by redistributing the total mass of the system onto 1/m-sub-level sets of the odometer which is a function counting total emissions of mass from lattice vertices. In free boundary terminology this goes in parallel with singular perturbation, which is known to converge to a Bernoulli type free boundary. We prove that models, generated from a single source, have a scaling limit, if the threshold m is fixed. Moreover, this limit is a ball, and the entire mass of the system is being redistributed onto an annular ring of thickness 1/m. By compactness argument we show that when m tends to infinity sufficiently slowly with respect to the scale of the model, then in this case also there is scaling limit which is a ball, with the mass of the system being uniformly distributed onto the boundary of that ball, and hence we recover a quadrature surface in this case. Depending on the speed of decay of 1/m, the visited set of the sandpile interpolates between spherical and polygonal shapes. Finding a precise characterisation of this shape-transition phenomenon seems to be a considerable challenge, which we cannot address at this moment.
机译:本文的主要目的是建立正交表面(潜在理论概念)和SandPile动力学(Laplacian生长模型)之间的联系。为此目的,我们在格子双击资本ZD(D> = 2)上介绍了Laplacian生长的新模式,其连续地变形了Levine和Peres的可分地区的占用区域(J.肛门。数学。111(1 ),2010年151-219)通过将系统的总质量重新分配到1 / M级级组的里程表上,这是从格子顶点的总质量排放的函数。在自由边界术语中,这与奇异扰动并联,这已知已知为伯努利型自由边界。如果阈值M是固定的,我们证明了从单个源生成的模型具有缩放限制。此外,该限制是球,并且系统的整个质量被重新分配到厚度1 / m的环形环上。通过紧凑性论证,我们表明,当M倾向于相对于模型的规模速度充分慢慢地,在这种情况下也存在缩放限制,该缩放限制是球的缩放限制,系统的质量均匀地分布到该边界上球,因此我们在这种情况下恢复正交表面。根据1 / m的衰减速度,访问的砂堤组在球形和多边形形状之间插入。找到这种形状过渡现象的精确表征似乎是一个相当大的挑战,我们现在无法解决。

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