Absorbing phase transitions with memory in critical scaling
arXiv:2106.14865 · doi:10.1103/jcby-h3pw
Abstract
Many driven systems alternate between bursts of activity and quiescence and can become trapped in an absorbing state, such as complete inactivity in reaction-diffusion processes or extinction in predator-prey dynamics. It is generally assumed that, conditioned on survival, their long-lived (quasi-stationary) behavior is unique and independent of the initial condition. We show this need not hold, even for memoryless Markov dynamics. When the configuration space fractures into multiple macroscopic communicating classes, where configurations can be reach from one another within a class but not across classes, the system retains a measurable memory of its preparation, which can directly affect the critical exponents near absorbing transitions. Using a minimal birth-death-diffusion model, we demonstrate that the quasi-stationary state is unique when birth processes are present, but becomes nonunique and initial-condition dependent when they are suppressed. This mechanism, arising from vanishing of inter-class escape-rate ratios in thermodynamic limit, challenges the conventional universality hypothesis and suggests possibility of history-dependent critical scaling in controlled lattice or colloidal systems with tunable particle-number.
References in corpus (9)
- Directed percolation criticality in turbulent liquid crystals
- Quasi-stationary distributions and population processes
- Universality in the three-dimensional random-field Ising model
- Experimental realization of directed percolation criticality in turbulent liquid crystals
- Specific-Heat Exponent of Random-Field Systems via Ground-State Calculations
- Strong Violation of Critical Phenomena Universality: Wang-Landau Study of the 2d Blume-Capel Model under Bond Randomness
- Fixed-Energy Sandpiles Belong Generically to Directed Percolation
- The Oslo model, hyperuniformity, and the quenched Edwards-Wilkinson model
- Hidden superuniversality in systems with continuous variation of critical exponents