(
A) Diagram of the site activation mechanism. Three states are introduced: [I], inactive, [D], delay, and [A], activated. SV fusion is only allowed from sites in state [A]. The rate from [I] to [D] is increased by Ca
2+, whereas the rate from [D] to [A] is slower and independent of Ca
2+, thereby introducing a delay. All (in)activation reactions are assumed to be reversible. (
B) Full site activation model. The Ca
2+ (un)binding of the SVs follow the same equations as in the single-sensor model and occurs independently of the site (in)activation. Replenishment is allowed into empty release sites regardless of activation status. (
C) Average, experimental eEJC traces (black) together with average simulated traces (red). (
D) eEJC
1 amplitudes of experiment (black) and simulation (red). Error bars and colored bands show standard deviation. Like with the three models described in the main text, simulations reproduce eEJC
1 amplitudes well. (
E) Average, normalized eEJC traces of experiment (black) and simulation (red). (
F) PPR values of experiment (gray) and simulation (blue). Error bars and colored bands show standard deviation. Like the unpriming model, simulations reproduce the experimentally observed facilitation. (
G) Average simulated traces (red) and examples of different outcomes of the stochastic simulation (colors). (
H) Plot of the mean synaptic variance vs. the mean eEJC
1 values, both from the experiment (black) and the simulation (red). The curves show the best fitted parabolas with forced intercept at (0,0) (simulation: Var = −0.0043*< eEJC
1>
2+0.5398 nA*< eEJC
1>, corresponding to n
sites = 233 and q = 0.54 nA when assuming a classical binomial model (
Clements and Silver, 2000), see Materials and methods). Like in experiments, simulations lead to decreasing variance at the highest Ca
2+ concentrations. (
I) The number of sites in state [I] and [A] (gray and red resp.) in simulations with extracellular Ca
2+ concentrations of 0.75 mM and 10 mM (solid and dashed resp.). The varying basal Ca
2+ concentration yield different initial amounts of site activation. The activation of sites mainly occurs between APs because of the delay state. Experimental data (example traces and means) depicted in panels C-F,H are replotted from
Figure 2A–D, F. Parameter values used for simulations can be found in
Tables 1–
3. Simulation scripts can be found in
Source code 1. Results from simulations (means and SDs) can be found in the accompanying source data file (
Figure 7—source data 1).