Bak-Tang-Wiesenfeld model in the finite range random link lattice

被引:9
作者
Najafi, M. N. [1 ]
机构
[1] Univ Mohaghegh Ardabili, Dept Phys, Ardebil, Iran
关键词
AVALANCHES;
D O I
10.1016/j.physleta.2014.05.051
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
We consider the BTW model in random link lattices with finite range interaction (RLFRI). The degree distribution of nodes is considered to be uniform in the interval (0, n(0)). We tune the topology of the lattices by two parameters (no, R) in which R is the range of interactions. We numerically calculate the exponents of the statistical distribution functions in terms of these parameters. Dijkstra radius is utilized to calculate the fractal dimension of the avalanches. Our analysis shows that for a fixed no value there are two intervals of R, namely (1, R-0) and (R-0, L) each of which has a distinct behavior. In the first interval the fractal dimension monotonically grows from D (f) (R = 1) similar or equal to D-f(BTw) = 1.25, up to D (f) similar or equal to 5.0 +/- 0.4. We found however that in the second interval there is a length scale r(0)(n(0), R) in which the behaviors are changed. For the scales smaller than r(0)(n(0), R), which is typically one decade, the fractal dimension is nearly independent of no and R and is nearly equal to 2.0 +/- 0.2. We retrieve the BTW-type behaviors in the limit R -> 1 and find some new behaviors in the random scaleless lattice limit, i.e. R -> L. We also numerically calculate the explicit form of the number of unstable nodes (NUN) as a time-dependent process and show that for regular lattice, it is (up to a normalization) proportional to a one-dimensional Weiner process and for RLFRI it acquires a drift term. Our analytical analysis shows that the relaxation time (exit time) for NUN process for RLFRI is related to a fitting parameter of NUN and is shorter than the regular one. (C) 2014 Elsevier B.V. All rights reserved.
引用
收藏
页码:2008 / 2015
页数:8
相关论文
共 19 条
[1]   SELF-ORGANIZED CRITICALITY - AN EXPLANATION OF 1/F NOISE [J].
BAK, P ;
TANG, C ;
WIESENFELD, K .
PHYSICAL REVIEW LETTERS, 1987, 59 (04) :381-384
[2]  
Beggs JM, 2003, J NEUROSCI, V23, P11167
[3]   FRACTAL STRUCTURE OF ISING AND POTTS CLUSTERS - EXACT RESULTS [J].
CONIGLIO, A .
PHYSICAL REVIEW LETTERS, 1989, 62 (26) :3054-3057
[4]   Self-organized criticality model for brain plasticity [J].
de Arcangelis, L ;
Perrone-Capano, C ;
Herrmann, HJ .
PHYSICAL REVIEW LETTERS, 2006, 96 (02)
[5]   INVERSE AVALANCHES IN THE ABELIAN SANDPILE MODEL [J].
DHAR, D ;
MANNA, SS .
PHYSICAL REVIEW E, 1994, 49 (04) :2684-2687
[6]   Theoretical studies of self-organized criticality [J].
Dhar, Deepak .
PHYSICA A-STATISTICAL MECHANICS AND ITS APPLICATIONS, 2006, 369 (01) :29-70
[7]  
Dijkstra E. W., 1959, NUMER MATH, V1, P269
[8]   Universal Critical Dynamics in High Resolution Neuronal Avalanche Data [J].
Friedman, Nir ;
Ito, Shinya ;
Brinkman, Braden A. W. ;
Shimono, Masanori ;
DeVille, R. E. Lee ;
Dahmen, Karin A. ;
Beggs, John M. ;
Butler, Thomas C. .
PHYSICAL REVIEW LETTERS, 2012, 108 (20)
[9]   Self-organized criticality and coevolution of network structure and dynamics [J].
Fronczak, P ;
Fronczak, A ;
Holyst, JA .
PHYSICAL REVIEW E, 2006, 73 (04)
[10]   Sandpile on scale-free networks [J].
Goh, KI ;
Lee, DS ;
Kahng, B ;
Kim, D .
PHYSICAL REVIEW LETTERS, 2003, 91 (14)