2008
DOI: 10.1142/6813
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Universality in Nonequilibrium Lattice Systems

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Cited by 146 publications
(174 citation statements)
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“…The first one is the probability that there will be at least one active node at time t. This probability is then averaged over the position of the initial active seed. For the contact process, it scales in the same way as the order parameter [12,13] so we have…”
Section: Scaling Theory In An Irfpmentioning
confidence: 99%
“…The first one is the probability that there will be at least one active node at time t. This probability is then averaged over the position of the initial active seed. For the contact process, it scales in the same way as the order parameter [12,13] so we have…”
Section: Scaling Theory In An Irfpmentioning
confidence: 99%
“…For larger values of ν, however, generic, continuously changing power laws can be observed. In particular for ν = 1.5 simulations We have also performed spreading simulations, starting from a very small initial seed of active sites [9]. These simulations were performed on networks with N = 10 5 nodes up to t = 4 × 10 5 MC time steps.…”
Section: Weighted Ba Trees With Multiplicative Weights: Wbat-i Modelmentioning
confidence: 99%
“…On the other hand, occupied vertices become empty with a unitary rate. On a regular lattice the CP experiences a nonequilibrium phase transition at a critical point λ c , separating an absorbing phase from an active one [8][9][10], whose order parameter is the density of occupied sites ρ in the steady state. Thus, for λ < λ c , an absorbing phase with ρ = 0 is observed, while for λ > λ c the system reaches an active phase, with ρ > 0 in the thermodynamic limit.…”
Section: Introductionmentioning
confidence: 99%
“…The research of nonequilibrium models has been a central topic of statistical mechanics [1][2][3]. A fundamental dynamical model to understand them is the contact process (CP) [4,5], in which sites can be either active (infected) or inactive (susceptible).…”
Section: Introductionmentioning
confidence: 99%