In spiral wave chimera states the incoherent core radius scales linearly with phase lag α near zero while the average positive winding number grows exponentially with α and defect statistics transition from binomial-like to Poisson-like at a critical α*.
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Spatially extended relaxation oscillations near SNIPER bifurcations undergo long-wavelength instabilities producing nonuniform oscillations such as chimeras and chaotic spiking that persist across the bifurcation.
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Topological defects in spiral wave chimera states
In spiral wave chimera states the incoherent core radius scales linearly with phase lag α near zero while the average positive winding number grows exponentially with α and defect statistics transition from binomial-like to Poisson-like at a critical α*.
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Nonuniform relaxation oscillations near SNIPER bifurcations
Spatially extended relaxation oscillations near SNIPER bifurcations undergo long-wavelength instabilities producing nonuniform oscillations such as chimeras and chaotic spiking that persist across the bifurcation.