The transitions between the firing of simple somatic spikes and the firing of dendritic spikes causes a break in the linearity of the frequency current (f - I) curve, with a second, shallower slope above this transition. Our f -I curves (Fig. 6A) were remarkably similar to those published by  (their Fig. 5). In the model, dendritic spike firing frequency remained relatively constant (16–19 Hz in both models) once the threshold was crossed and was rather insensitive to the current amplitude.
This paper principally concerns the simulation of Purkinje cell responses to current injection in the slice preparation [1, 3, 2, 4]. We believe that overall the model does a good job of simulating these experimental results.
As demonstrated in Figs. 3-7, both the somatic and dendritic firing patterns were reproduced well. In particular, at low-level current intensities the model fired only fast somatic spikes after a delay. At higher current amplitudes these fast Na+ spikes were interrupted by dendritic Ca2+ spikes that were caused by activation of the CaP channel. The model also replicated the experimental f - I curves well.
One aspect of Purkinje cells in slice preparations that we have not addressed explicitly is the tendency for Purkinje cells to become spontaneously active . This could be achieved in the model by introducing a bit of bias current. However, there are numerous ways in which this could be done. For example, increasing the amount of NaP or CaT channels would introduce such a current, as would decreasing any of the K+ currents or the leak in the model. In other words, there might be many ways in which Purkinje cells could become spontaneously firing cells, because modulating the conductivity of any of six different channels would be sufficient.
 RR Llinás and M Sugimori. The electrophysiology of the cerebellar Purkinje cell revisited. In RR Llinás and C Sotelo, editors, The Cerebellum Revisited, pages 167–181. Berlin: Springer-Verlag, 1992.