A. Lodhia, S. Sheffield, Xin Sun, Samuel S. Watson
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引用次数: 86
摘要
我们讨论了一类以参数s∈R为索引的随机场,我们称之为分数阶高斯场,由fgf (R) =(-∆)- s/2W给出,其中W是Rd上的白噪声,(-∆)- s/2是分数阶拉普拉斯函数。这些字段也可以通过它们的Hurst参数H = s−d/2来参数化。在一维中,FGFs过程的例子包括布朗运动(s = 1)和分数布朗运动(1/2 < s < 3/2)。任意维度的例子包括白噪声(s = 0)、高斯自由场(s = 1)、双拉普拉斯高斯场(s = 2)、对数相关高斯场(s = d/2)、利维布朗运动(s = d/2 + 1/2)和多维分数布朗运动(d/2 < s < d/2 + 1)。这些领域在统计物理、早期宇宙宇宙学、金融、量子场论、图像处理等学科中都有应用。我们概述了分数阶高斯场,包括协方差公式、吉布斯性质、球坐标分解、线性子空间的限制、局部集定理和其他基本结果。我们还定义了一个离散分数高斯场,并解释了如何将s∈(0,1)的fgf理解为一个远程高斯自由场,其中布朗运动的势理论被各向同性2s稳定Levy过程的势理论所取代。*部分由NSF资助DMS 1209044。†由NSF GRFP奖号1122374支持。ar X iv:1 40 7。55 98 v1 [m at h. PR] 2 1 Ju 1 2 01 4
We discuss a family of random fields indexed by a parameter s ∈ R which we call the fractional Gaussian fields, given by FGFs(R) = (−∆)−s/2W, where W is a white noise on Rd and (−∆)−s/2 is the fractional Laplacian. These fields can also be parameterized by their Hurst parameter H = s − d/2. In one dimension, examples of FGFs processes include Brownian motion (s = 1) and fractional Brownian motion (1/2 < s < 3/2). Examples in arbitrary dimension include white noise (s = 0), the Gaussian free field (s = 1), the bi-Laplacian Gaussian field (s = 2), the log-correlated Gaussian field (s = d/2), Levy’s Brownian motion (s = d/2 + 1/2), and multidimensional fractional Brownian motion (d/2 < s < d/2 + 1). These fields have applications to statistical physics, early-universe cosmology, finance, quantum field theory, image processing, and other disciplines. We present an overview of fractional Gaussian fields including covariance formulas, Gibbs properties, spherical coordinate decompositions, restrictions to linear subspaces, local set theorems, and other basic results. We also define a discrete fractional Gaussian field and explain how the FGFs with s ∈ (0, 1) can be understood as a long range Gaussian free field in which the potential theory of Brownian motion is replaced by that of an isotropic 2s-stable Levy process. ∗Partially supported by NSF grant DMS 1209044. †Supported by NSF GRFP award number 1122374. ar X iv :1 40 7. 55 98 v1 [ m at h. PR ] 2 1 Ju l 2 01 4