Wave Propagation in Spatially Distributed Excitable Media

Consider wave propagation through regions of no excitability (gaps) in an otherwise excitable medium. Propagation in the gaps takes place via simple diffusion. We extend the geometric method for a one-gap system developed by Lewis and Keener to the case of two and three gaps, and we obtain conditions for successful wave propagation and failure. We show that, like the one-gap system, steady-state multiplicity for the case of two gaps arises via a limit point bifurcation. We also demonstrate that in some cases the presence of a large number of gaps promotes wavefront propagation.

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