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and consequently the convolution form of ( 7.40 ) reduces to the product of Laplace
transforms
ψ n (
) = ψ n 1 (
1 (
u
u
u
),
so that substituting from ( 7.42 ) and carrying out the iteration yields ( 3.193 )
= ψ(
) n
ψ n (
u
)
u
.
(7.43)
The Laplace transform of the survival probability
(
t
)
is
ψ(
1
u
)
(
u
) =
,
(7.44)
u
so that inserting ( 7.43 ) and ( 7.44 ) into the Laplace transform of ( 7.39 ) and again using
the convolution theorem yields
ψ(
ψ(
) n p
1
u
)
p
(
u
) =
u
)(
I
+
K
(
0
).
(7.45)
u
n
=
0
1 and ψ(
1, having the value ψ(
The eigenvalues of the matrix
(
I
+
K
)
are
u
)<
u
) =
1
only in the limiting case u
0. Thus, we evaluate the geometric sum appearing in ( 7.45 )
according to the well-known rule
=
ψ(
) n
1
u
)(
I
+
K
=
) .
(7.46)
ψ(
1
u
)(
I
+
K
n
=
0
Consequently, inserting this form of the series into ( 7.45 ) gives us for the Laplace
transform of the probability density
ψ(
ψ(
1
u
)
1
u
)
p
(
u
) =
p
(
0
) =
p
(
0
)
u ψ(
ψ(
u ψ(
u ψ(
u
u
)(
I
+
K
)
u
(
1
u
)) +
u
)
u
)(
I
+
K
)
and, using the form of the unit matrix, this reduces to
ψ(
1
u
)
p
(
u
) =
K p
(
0
).
(7.47)
ψ(
u ψ(
u
(
1
u
))
u
)
ψ(
By dividing both the numerator and the denominator of ( 7.47 )by
(
1
u
))
we obtain
1
p
(
u
) =
K p
(
0
),
(7.48)
(
u
u
)
where
u ψ(
u
)
(
u
) =
) ,
(7.49)
ψ(
1
u
namely the typical memory kernel that emerged in CTRW theory discussed previously.
With a little algebra ( 7.48 ) can be rewritten as
) = (
u
p
(
u
)
p
(
0
u
)
K
p
(
u
),
(7.50)
 
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