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It is convenient to rewrite ( 7.151 ) in the following form:
t
t ) =
dt R
t )ψ(
t ),
ψ(
t
,
(
t
(7.154)
0
where we recall that
R
(
t
) =
0 ψ n (
t
).
(7.155)
n
=
The quantity R
is the number of events per unit time produced by the ensemble of
complex networks prepared at time t
(
t
)
=
0 and can easily be derived from
ψ(
t
)
for a
renewal process.
The double-indexed probability density
ψ t
t in ( 7.154 ) refers to a web that has
,
been prepared at time t
0 when an event occurs, say one generated by an external
excitation. For a renewal process the probability density of an event occurring at time t
given that the last event occurred at time t has the exact form [ 68 ]
=
t
0 ψ n (
t ) = ψ(
t )ψ(
t )
dt .
ψ(
t
,
t
) +
t
(7.156)
n
=
1
In the physics literature
ψ(
t
)
dt is the probability that an event occurs in the time inter-
. Since the observation process begins at time t >
,
+
val
0, the probability of
observing a new event after t depends on the last event occurring prior to t , at time
t as expressed by the distribution density
(
t
t
dt
)
t is
in general the last of a sequence of n events, occurring exactly at t , while the earlier
events can occur at any earlier time t
t )
. The event occurring at t <
ψ(
t
>
0. The probability for this last of n events is
t )
ψ n (
1; this is the first term in the integrand of ( 7.156 ). The renewal nature
of the process is adopted to define the function
, with n
ψ n (
t
)
through the hierarchy
t
0 ψ n 1 (
t 1 (
t )
dt
ψ n (
t
) =
t
(7.157)
starting at the preparation t
=
0, which is established by setting the condition
ψ 0 (
) = δ(
).
t
t
(7.158)
The hierarchy of ( 7.157 ) allows us to express the distribution densities
ψ n (
t
)
in terms
of
. The time-convolution structure of ( 7.157 )isa
consequence of the renewal nature of the process and makes it convenient for us to use
the Laplace-transform method. It is straightforward to prove that ( 7.157 )using( 7.158 )
yields the following relation among the Laplace-transformed functions:
ψ 1 (
t
)
, which is identified with
ψ(
t
)
ψ n (
) = ( ψ(
n
u
u
))
.
(7.159)
From this algebraic form of the Laplace transform of the probability density for n events
it is evident that the time intervals between events in a renewal process are independent
of one another.
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