1992
DOI: 10.1016/0378-4371(92)90256-p
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Propagation failure and multiple steady states in an array of diffusion coupled flow reactors

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Cited by 46 publications
(22 citation statements)
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“…[23] Such elements can have local or diffusive connections between them. For regular lattices and linear chains (i.e., for relatively simple networks), it is known that, under sufficiently weak coupling, the fronts fail to propagate, and thus stationary domains can be formed, [24,25,26,27] whereas at strong coupling the fronts spread [27,28] and a uniform state is eventually established. Recently, analogues phenomena were theoretically investigated for complex networks and the formation of stationary domains, sensitive to the network topology, was predicted based on a simple model of regular trees and onecomponent bistable elements.…”
mentioning
confidence: 99%
“…[23] Such elements can have local or diffusive connections between them. For regular lattices and linear chains (i.e., for relatively simple networks), it is known that, under sufficiently weak coupling, the fronts fail to propagate, and thus stationary domains can be formed, [24,25,26,27] whereas at strong coupling the fronts spread [27,28] and a uniform state is eventually established. Recently, analogues phenomena were theoretically investigated for complex networks and the formation of stationary domains, sensitive to the network topology, was predicted based on a simple model of regular trees and onecomponent bistable elements.…”
mentioning
confidence: 99%
“…In continuous bistable media, traveling fronts, representing waves of transition from one stable state into another can be observed [29,30]. Traveling fronts can become pinned if coupling is sufficiently weak [34][35][36][37][38], forming stationary patterns, in chains and lattices of diffusively coupled bistable elements. Complex tree networks of coupled bistable units, both regular and irregular, exhibit the spreading, retreating or stationary patterns dependent on the coupling strength and the degree distribution of the nodes [5,6,28].…”
Section: Introductionmentioning
confidence: 99%
“…The discreteness effects may modify severely the dynamics of the front propagation even in the framework of the simplest models (see the pioneering works of Ishimori & Munakata [14] and Peyrard & Kruskal [15]). The relevant physical contexts can be quite diverse, including hydrogen-bonded chains [16], calcium release waves in living cells [17][18][19], reaction fronts in chains of coupled chemical reactors [20][21][22], arrays of coupled diode resonators [23], semiconductor superlattices [24], discontinuous propagation of action potential in cardiac tissue [25][26][27], arrays of autocrine cells [28], superconductivity in Josephson junctions [29], nonlinear optics and waveguide arrays [30] and the dynamics of neuron chains [31] to mention a few. The dynamics of all these systems is mainly driven by their inherently discrete nature.…”
Section: Introductionmentioning
confidence: 99%