Biomedical Engineering Reference
In-Depth Information
A
B
80
g Low
tot
0.8
60
0.6
g High
tot
40
0.4
20
0.2
0
10
20
30
40
10
20
30
40
g tot s NMDA (nS)
g tot s NMDA (nS)
C
D
60
2
gain < g Low
tot
40
1
0
0.05
0.1
20
0
0
−1
0.025
−2
gain > g High
tot
−0.025
0
2
4
6
8
0
0.25
0.5
0.75
1
s NMDA
Time (s)
Figure 15.5
Bistability in a simple, one-population recurrent network. (A) . Mean synaptic ac-
tivity as a function of the total recurrent synaptic input ˜ s
g tot s NMDA (sigmoid; thick
solid line) and same quantity when s is interpreted as the total recurrent network
feedback (thin dashed lines). g High
=
50 nS and g Low
34 nS correspond to the
highest and lowest values of the network gain in which the network is bistable for
this network parameters. The crossings of a straight line corresponding to an in-
termediate value of g tot
=
=
tot
tot
=
40 nS with the sigmoid, correspond to the 3 steady state
solutions in the bistable regime. Stable (unstable) solutions are marked with a filled
(open) circle. (B) . Mean firing rate of the neurons as a function of the total recur-
rent synaptic input. The fixed point solutions in A are shown. Note the low rate
(
40 Hz) of the stable high activity state, and the non-zero rate (
1Hz)ofthe
7 KHz, g ext
AMPA
stable low activity state. Network parameters are: C ext n ext =
1
nS. Parameters for the single cells are like in Figure 15.1. Synaptic parameters are
given in Section 15.2.6.2. (C) . Time course of activity (top) in the network when
g tot =
0
.
=
3
.
40 nS. Brief current pulses (bottom) switch the network between its two stable
states. (D) . Potential function associated to the dynamics of Equation (15.92) for
three different values of g tot , corresponding to the situations where there is only one
low activity steady-state (upper curve), one high activity steady-state (lower curve)
and for a bistable network (middle curve). The values of s NMDA at the steady states
are given by the minima of the potential function. Inset : blown-up version of the
low activity region of U shows the disappearance of the low activity minimum of the
potential as g tot increases.
 
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