Hurst exponents, Markov processes, and fractional Brownian motion

被引:54
|
作者
McCauley, Joseph L. [1 ]
Gunaratne, Gemunu H.
Bassler, Kevin E.
机构
[1] Univ Houston, Dept Phys, Houston, TX 77204 USA
[2] NUI Galway, COBERA, Dept Econ, JE Cairnes Grad Sch Business & Publ Policy, Galway, Ireland
[3] Inst Fundamental Studies, Kandy, Sri Lanka
[4] Univ Houston, Texas Ctr Superconduct, Houston, TX USA
基金
美国国家科学基金会;
关键词
Markov processes; fractional Brownian motion; scaling; Hurst exponents; stationary and nonstationary increments; autocorrelations;
D O I
10.1016/j.physa.2006.12.028
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
There is much confusion in the literature over Hurst exponents. Recently, we took a step in the direction of eliminating some of the confusion. One purpose of this paper is to illustrate the difference between fractional Brownian motion (fBm) on the one hand and Gaussian Markov processes where H not equal 1/2 on the other. The difference lies in the increments, which are 2 stationary and correlated in one case and nonstationary and uncorrelated in the other. The two- and one-point densities of Min are constructed explicitly. The two-point density does not scale. The one-point density for a semi-infinite time interval is identical to that for a scaling Gaussian Markov process with H not equal 1/2 over a finite time interval. We conclude that both Hurst exponents and one-point densities are inadequate for deducing the underlying dynamics from empirical data. We apply these conclusions in the end to make a focused statement about 'nonlinear diffusion'. (c) 2007 Elsevier B.V. All rights reserved.
引用
收藏
页码:1 / 9
页数:9
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