How to discriminate easily between Directed-percolation and Manna scaling
arXiv:cond-mat/0703209 · doi:10.1016/j.physa.2007.04.110
Abstract
Here we compare critical properties of systems in the directed-percolation (DP) universality class with those of absorbing-state phase transitions occurring in the presence of a non-diffusive conserved field, i.e. transitions in the so-called Manna or C-DP class. Even if it is clearly established that these constitute two different universality classes, most of their universal features (exponents, moment ratios, scaling functions,...) are very similar, making it difficult to discriminate numerically between them. Nevertheless, as illustrated here, the two classes behave in a rather different way upon introducing a physical boundary or wall. Taking advantage of this, we propose a simple and fast method to discriminate between these two universality classes. This is particularly helpful in solving some existing discrepancies in self-organized critical systems as sandpiles.
7 Pages, 4 Figures
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- Confirming and extending the hypothesis of universality in sandpiles
- Abelian Manna model on various lattices in one and two dimensions
- Quasi-Neutral theory of epidemic outbreaks
- Continuous and discontinuous absorbing-state phase transitions on Voronoi-Delaunay random lattices
- Steady state of Stochastic Sandpile Models
- Phase transition in an exactly solvable reaction-diffusion process
- Connecting the Micro-dynamics to the Emergent Macro-variables: Self-Organized Criticality and Absorbing Phase Transitions in the Deterministic Lattice Gas
- Crossover from rotational to stochastic sandpile universality in the random rotational sandpile model
- Self-organised criticality in stochastic sandpiles: Connection to directed percolation
- Absorbing boundaries in the conserved Manna model