Perturbations both trigger and delay seizures due to generic properties of slow-fast relaxation oscillators
Fig 6
PRC of pulses A > 0 for relaxation oscillators.
Next we sketch the PRCs for pulses of amplitude A > 0 for the case . For phases θ < θ*, where θ* satisfies
, due to the slope of isochrons the effect of the pulses will be to delay trajectories. Since isochrons approach the unstable point P through
, the closer the phase θ to θ*, the larger the bending of the isochrons and thus the larger the corresponding delay value. For phases
, there is an advancement proportional to the fraction of cycle skipped. This prevalence of advancements is also seen for points in the upper branch. For phases in a neighbourhood of the fold point
, we expect a transition between advancement and delays not drawn because our analysis is only valid for normally hyperbolic points.