1996
DOI: 10.1103/physreve.54.175
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Percolation and cluster Monte Carlo dynamics for spin models

Abstract: A general scheme for devising efficient cluster dynamics proposed in a previous paper ͓Phys. Rev. Lett. 72, 1541 ͑1994͔͒ is extensively discussed. In particular, the strong connection among equilibrium properties of clusters and dynamic properties as the correlation time for magnetization is emphasized. The general scheme is applied to a number of frustrated spin models and the results discussed. ͓S1063-651X͑96͒08406-1͔

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Cited by 31 publications
(29 citation statements)
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“…To each molecules we associate a cell on a square lattice. The Wolff algorithm is based on the definition of a cluster of variables chosen in such a way to be thermodynamically correlated [18,19]. To define the Wolff cluster, a bond index (arm) of a molecule is randomly selected; this is the initial element of a stack.…”
Section: The Simulation With the Wolff's Clusters Monte Carlo Algorithmmentioning
confidence: 99%
“…To each molecules we associate a cell on a square lattice. The Wolff algorithm is based on the definition of a cluster of variables chosen in such a way to be thermodynamically correlated [18,19]. To define the Wolff cluster, a bond index (arm) of a molecule is randomly selected; this is the initial element of a stack.…”
Section: The Simulation With the Wolff's Clusters Monte Carlo Algorithmmentioning
confidence: 99%
“…Different algorithms have been developed to optimize the MC simulation of spin models and cell models [56,57]. The Wolff cluster algorithm [58] has become a particularly useful tool for the simulation of water when coarse-grained or cell models are utilized [53,[59][60][61].…”
Section: Simulations Of a Coarse-grained Model Of Water Confined Imentioning
confidence: 99%
“…To each molecules we associate a cell on a square lattice. The Wolff's algorithm is based on the definition of a cluster of 41,42 To selected; this is the initial element of a stack. The cluster is grown by first same Potts state, then they are added to the stack with probability p same ≡ min σ 43 where β ≡ (k B T) −1 .…”
Section: K Stokely Et Almentioning
confidence: 99%
“…This choice for the probability p same σ guarantees that the connected arms are thermodynamically correlated. 41 Next, guarantee that connected facing arms correspond to thermodynamically correlated variables, is necessary 42 proposed in 10 which gives rise to the SF scenario (Fig. 3a).…”
Section: K Stokely Et Almentioning
confidence: 99%