Fast and slow domino regimes in transient network dynamics
Ashwin, P; Creaser, J; Tsaneva-Atanasova, K
Date: 8 November 2017
Journal
Physical Review E
Publisher
American Physical Society
Publisher DOI
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Abstract
It is well known that the addition of noise to a multistable dynamical system can induce random transitions from
one stable state to another. For low noise, the times between transitions have an exponential tail and Kramers’
formula gives an expression for the mean escape time in the asymptotic limit. If a number of multistable ...
It is well known that the addition of noise to a multistable dynamical system can induce random transitions from
one stable state to another. For low noise, the times between transitions have an exponential tail and Kramers’
formula gives an expression for the mean escape time in the asymptotic limit. If a number of multistable systems
are coupled into a network structure, a transition at one site may change the transition properties at other sites.
We study the case of escape from a “quiescent” attractor to an “active” attractor in which transitions back
can be ignored. There are qualitatively different regimes of transition, depending on coupling strength. For
small coupling strengths, the transition rates are simply modified but the transitions remain stochastic. For large
coupling strengths, transitions happen approximately in synchrony—we call this a “fast domino” regime. There
is also an intermediate coupling regime where some transitions happen inexorably but with a delay that may be
arbitrarily long—we call this a “slow domino” regime. We characterize these regimes in the low noise limit in
terms of bifurcations of the potential landscape of a coupled system. We demonstrate the effect of the coupling
on the distribution of timings and (in general) the sequences of escapes of the system.
Mathematics and Statistics
Faculty of Environment, Science and Economy
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