Perturbations both trigger and delay seizures due to generic properties of slow-fast relaxation oscillators
Fig 4
The slow vector field shapes the isochrons for relaxation oscillators.
In the limit ϵ → 0 isochrons are lines of y constant denoted by . However, since ϵ ≠ 0 but small, the isochrons are
perturbations of
. As we show in the right panel, the sign of the
corrections depends on the difference of speeds between the converging point
and the base point z during the convergence time th. In this case, to approach Γϵ,
has to cross layers of x whose values are smaller than the ones surrounding Γϵ. For this reason
travels slower than z. Since
and z have to meet after a time th at the same point on Γϵ, but
travels slower than z, then
needs to travel a short distance. This determines the sign of the
correction. Furthermore, if the slow vector field is monotonous along the fast direction, the farther the point
, the slower (faster) it travels, so the slope of the isochrons will have the same sign for all the points
satisfying fast convergence, thus determining the effect of perturbations in the fast direction.