Biomedical Engineering Reference
In-Depth Information
Therefore,
dw i (
t
)
dt
=
G 0 dt
(11.26)
dt K
t )
t )
j w j r i j (
t )
r in
i
t ) θ
(
P
(
t
(
t
+
r in (
A +
A ) .
For simplicity, let us assume that the scale of STDP is slow compared to the spiking
rate of the neurons, we can therefore replace r i j (
t )
r in
i
t )
t
(
t
+
with its average
r i j (
t )
r in
i
t ) > t ,or Q ij (
t
t )
t
t )
<
is stationary
for all subsequent calculations. We can now calculate the rate of change in synaptic
strengths for correlated inputs. From Section 11.1,
t
(
t
+
. We assume that Q ij (
C ij r in 2 e −| t |/ τ
r in 2
(
)=
+
+ δ (
)
,
Q ij
t
c
t
r in
(11.27)
ij
and
1
e t / τ
K
(
t
)=
.
(11.28)
m
m
Upon collecting terms,
dw i
r in w i A + τ + + τ
Hr in 2
r in 2
) )
dt =
G
(
j C ij w j (
A
A + )
j w j +
m
τ + τ
(11.29)
m
θ
r in (
A +
A ) ,
where
0
1
A +
τ + [
e t / τ
dt e t / τ + e ( t + t ) / τ
dt
=
{
H
m
c
t
0
m
t
A
τ
dt e t / τ + e t + t ) / τ
dt e t / τ e ( t + t ) / τ
+
]
}
c
c
0
c
A + τ
A + τ
τ +
A + τ
τ +
c
c
=
)
) +
( τ
τ + )( τ
+ τ
( τ
τ + )( τ + + τ
( τ
+ τ + )( τ + + τ
)
.
(11.30)
c
c
m
c
m
c
m
c
A τ
( τ
c + τ )( τ
c + τ
m )
c
A + ( τ
τ
A ( τ +
τ
=
+ τ ) [
A +
A +
c )
c )
( τ
+ τ
)( τ
+ τ + )( τ
c
m
c
c
2 A + τ
τ + ( τ
+ τ )
m
c
+
] .
c
( τ + + τ
)
m
The first term in the brackets in Equation (11.29) corresponds to the effect of corre-
lations in the inputs, the second term corresponds to the effect of the average input,
and the last term takes into account the correlation introduced by spiking. It is inter-
esting that STDP can switch from a Hebbian to an anti-Hebbian rule depending on
the time scale of the input correlation. In order for the rule to be Hebbian, H has to
be greater than zero. Otherwise, it is anti-Hebbian. Solving H
>
0 for
c yields
x 2
x
4
(
A
A + )
y
<
,
(11.31)
c
2
(
A
A + )
where
2 A + τ
τ +
m
x
=
A + τ
A τ + +
m ,
(11.32)
τ + + τ
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