2013
DOI: 10.1103/physreve.88.062817
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Critical properties of a dissipative sandpile model on small-world networks

Abstract: A dissipative sandpile model (DSM) is constructed and studied on small world networks (SWN). SWNs are generated adding extra links between two arbitrary sites of a two dimensional square lattice with different shortcut densities φ. Three different regimes are identified as regular lattice (RL) for φ 2 −12 , SWN for 2 −12 < φ < 0.1 and random network (RN) for φ ≥ 0.1. In the RL regime, the sandpile dynamics is characterized by usual Bak, Tang, Weisenfeld (BTW) type correlated scaling whereas in the RN regime it… Show more

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Cited by 13 publications
(27 citation statements)
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References 77 publications
(94 reference statements)
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“…scale-free networks [36] or small-world networks [43]. More recently, the existence of two scaling regimes, one of mean-field-like and one of regular-lattice-like have also been reported [44,45]. We note that in all such studies definitive mean-field behavior has been observed for the value of shortcut link probability (long range connections) equal or greater than p ∼ 10 −1 .…”
Section: Discussionmentioning
confidence: 88%
“…scale-free networks [36] or small-world networks [43]. More recently, the existence of two scaling regimes, one of mean-field-like and one of regular-lattice-like have also been reported [44,45]. We note that in all such studies definitive mean-field behavior has been observed for the value of shortcut link probability (long range connections) equal or greater than p ∼ 10 −1 .…”
Section: Discussionmentioning
confidence: 88%
“…x for x ≫ 1 [21]. Noting that for large enough αs F is a decreasing function, we see that the average shortest distance decreases with increasing α.…”
Section: The Btw Model On the Small World Networkmentioning
confidence: 68%
“…2a. It is worth mentioning that it is well-known in the literature that in the IR limit the BTW model on the random network phase (in which α 10) should have the same exponents as the mean field (MF) results [20,21,31,32]. Two points should be noted in this regard: Firstly we have not entered this phase.…”
Section: Three Dimensionsmentioning
confidence: 96%
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“…The probability of dissipation ǫ φ is taken as the inverse of the average number of steps n φ required for a random walker to reach the lattice boundary starting from any lattice point [27,19]. The dissipation factor ǫ φ = 1/ n φ for a given φ is then determined using the numerically estimated values of n φ .…”
Section: The Model: Dssm On Swnmentioning
confidence: 99%