Absorbing phase transitions in a non-conserving sandpile model

被引:3
|
作者
Goebel, Marvin [1 ]
Gros, Claudius [1 ]
机构
[1] Goethe Univ Frankfurt, Inst Theoret Phys, Frankfurt, Germany
关键词
absorbing phase transition; self-organization; Manna model; sandpile model; non-conserving; SELF-ORGANIZED CRITICALITY; UNIVERSAL SCALING BEHAVIOR; LOGARITHMIC CORRECTIONS;
D O I
10.1088/1751-8121/ab59ad
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
We introduce and study a non-conserving sandpile model, the autonomously adapting sandpile (AAS) model, for which a site topples whenever it has two or more grains, distributing three or two grains randomly on its neighboring sites, respectively with probability p and . The toppling process is independent of the actual number of grains z(i) of the toppling site, as long as . For a periodic lattice the model evolves into an inactive state for small p , with the number of active sites becoming stationary for larger values of p . In one and two dimensions we find that the absorbing phase transition occurs for and . The symmetry of bipartite lattices allows states in which all active sites are located alternatingly on one of the two sublattices, A and B, respectively for even and odd times. We show that the AB-sublattice symmetry is spontaneously broken for the AAS model, an observation that holds also for the Manna model. One finds that a metastable AB-symmetry conserving state is transiently observable and that it has the potential to influence the width of the scaling regime, in particular in two dimensions. The AAS model mimics the behavior of integrate-and-fire neurons which propagate activity independently of the input received, as long as the threshold is crossed. ing from regular lattices, one can identify sites with neurons and consider quenched networks of neurons connected to a fixed number G of other neurons, with G being drawn from a suitable distribution. The neuronal activity is then propagated to G other neurons. The AAS model is hence well suited for theoretical studies of nearly critical brain dynamics. We also point out that the waiting-time distribution allows an avalanche-free experimental access to criticality.
引用
收藏
页数:17
相关论文
共 50 条
  • [1] A non-conserving coagulation model with extremal dynamics
    Juhasz, Robert
    JOURNAL OF STATISTICAL MECHANICS-THEORY AND EXPERIMENT, 2009,
  • [2] Phase transition in a non-conserving driven diffusive system
    Evans, MR
    Kafri, Y
    Levine, E
    Mukamel, D
    JOURNAL OF PHYSICS A-MATHEMATICAL AND GENERAL, 2002, 35 (29): : L433 - L438
  • [3] Simple sandpile model of active-absorbing state transitions
    Jain, K
    PHYSICAL REVIEW E, 2005, 72 (01):
  • [5] INTERACTION CURRENT CONTRIBUTIONS TO PARITY NON-CONSERVING NUCLEAR GGAMMA-TRANSITIONS
    GARI, M
    HUFFMAN, AH
    PHYSICS LETTERS B, 1971, B 36 (05) : 442 - &
  • [6] LEPTON NUMBER CONSERVING AND NON-CONSERVING WEAK INTERACTIONS
    FREUND, PGO
    NUCLEAR PHYSICS B, 1972, 47 (01) : 200 - &
  • [7] RENORMALIZATION OF A PARITY NON-CONSERVING THEORY
    ALBRIGHT, CH
    HAAG, R
    TREIMAN, SB
    NUOVO CIMENTO, 1959, 13 (06): : 1282 - 1284
  • [8] ON THE RENORMALIZATION OF A PARITY NON-CONSERVING INTERACTION
    SEKINE, K
    NUOVO CIMENTO, 1959, 11 (01): : 87 - 101
  • [9] NONEQUILIBRIUM PHASE-TRANSITIONS IN A DRIVEN SANDPILE MODEL
    DHAR, SK
    PANDIT, R
    RAMASWAMY, S
    JOURNAL OF PHYSICS A-MATHEMATICAL AND GENERAL, 1995, 28 (22): : L563 - L569
  • [10] PARITY NON-CONSERVING NEUTRON SPIN ROTATION
    HECKEL, B
    FORTE, M
    RAMSEY, NF
    GREENE, GL
    GREEN, K
    BYRNE, J
    PENDLEBURY, JM
    JOURNAL DE PHYSIQUE, 1984, 45 (NC-3): : 89 - 92