Contents - Max-Planck-Institut für Physik komplexer Systeme
Contents - Max-Planck-Institut für Physik komplexer Systeme
Contents - Max-Planck-Institut für Physik komplexer Systeme
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Main results.<br />
probability density [kHz]<br />
1. In the case of deterministic adaptation we find<br />
that the ISI density can be well approximated<br />
by an inverse Gaussian probability density. This<br />
density is equal to the first-passage-time density<br />
of a Brownian motion with a drift corresponding<br />
to a base current that is reduced by the adaptation<br />
(Fig. 2A). Furthermore, we have derived an<br />
analytical formula for the serial correlation coefficient<br />
ρn, which shows that neighboring ISIs are<br />
negatively correlated (Fig. 3). This characteristic<br />
feature has been numerically found in other<br />
neuron models with deterministic adaptation and<br />
fast fluctuations (e.g. [2, 3]) and has been experimentally<br />
observed for a variety of neurons (for<br />
reviews see [4, 5]).<br />
2. A stochastic adaptation current can be approximated<br />
by a long-correlated colored noise process<br />
with effective parameters (reduced values<br />
of mean, noise variance, correlation time). As a<br />
consequence, the ISI densities become strongly<br />
skewed and peaked compared to an inverse<br />
Gaussian distribution (Fig. 2B) Another striking<br />
difference is, that the ISI correlations are positive<br />
and not negative as in the case of fast noise<br />
(Fig. 3). We have provided analytical formulas for<br />
the skewness, kurtosis and serial correlation coefficient<br />
of the ISIs that clearly explain these properties.<br />
0.20<br />
0.15<br />
0.10<br />
0.05<br />
0.00<br />
0 5 10 15 20 25 30<br />
A<br />
simulation<br />
inverse Gaussian<br />
0.20<br />
0.15<br />
0.10<br />
0.05<br />
0.00<br />
0 5 10 15 20 25 30<br />
interspike interval [ms]<br />
B<br />
channel model<br />
theory<br />
inv. Gaussian<br />
Figure 2: (A) Interspike interval (ISI) density for the case of deterministic<br />
adaptation. The gray bars display the result from a simulation of<br />
the model, the dashed line represents the inverse Gaussian distribution<br />
obtained from the theory. (B) ISI density in the case of stochastic<br />
adaptation. An inverse Gaussian distribution (dashed line) with the<br />
same mean ISI and the same variance does not fit the ISI density obtained<br />
from the simulation of the model with adaptation channels<br />
(gray bars). Circles depict simulation results of the diffusion approximation<br />
(Gaussian approximation) of the channel noise, the solid line<br />
shows our theoretical approximation.<br />
Conclusions. We have put forward several novel analytical<br />
results that characterize the non-renewal spiking<br />
behavior of neurons with noise and stochastic or<br />
deterministic adaptation. Our analysis has revealed<br />
a striking difference of the ISI statistics depending on<br />
whether slow adaptation noise or fast current noise is<br />
dominating. These findings suggest an indirect way to<br />
determine the dominant source of noise on the basis<br />
of the ISI statistics. As an application, we have used<br />
our theoretical results to understand the origin of neuronal<br />
response variability of auditory receptor cells of<br />
locusts (collaboration with J. Benda, Munich). Preliminary<br />
analysis indicates that slow adaptation currents<br />
may indeed contribute to neuronal variability of this<br />
primary sensory neuron.<br />
serial correlation coefficient<br />
0.8<br />
0.6<br />
0.4<br />
0.2<br />
0.0<br />
determ. adaptation<br />
stoch. adaptation<br />
theory<br />
0.2<br />
0 2 4 6 8 10<br />
lag<br />
Figure 3: Serial correlation coefficient ρn as a function of the lag n.<br />
In the case of deterministic adaptation interspike intervals (ISIs) are<br />
negatively correlated, whereas in the case of stochastic adaptation<br />
ISIs become positively correlated.<br />
[1] T. Schwalger, K. Fisch, J. Benda, and B. Lindner. PLoS Comp.<br />
Biol., 6(12):e1001026, 2010.<br />
[2] M. J. Chacron, K. Pakdaman, and A. Longtin. Neural Comp.,<br />
15:253, 2003.<br />
[3] Y.-H. Liu and X.-J. Wang. J. Comp. Neurosci., 10:25, 2001.<br />
[4] O. Avila-Akerberg and M. J. Chacron. Experimental Brain Research,<br />
2011.<br />
[5] F. Farkhooi, M. F. Strube-Bloss, and M. P. Nawrot. Phys. Rev. E,<br />
79(2):021905–10, 2009.<br />
2.9. How Stochastic Adaptation Currents Shape Neuronal Firing Statistics 59