Graphics Programs Reference
In-Depth Information
where the p 0 IJ (t) are the elements of the transition probability matrix P 0 (t)
of the process { Y (t),t 0 } .
If we are only interested in the analysis of the steady-state probabilities of
macrostates defined as
η 0 I
X
t→∞ P { X(t) A I } =
=
lim
η i
(A.69)
i∈A I
we can, as in the discrete-time case, write the following equation for the
process { X(t),t 0 }
X
η i q ij = 0
(A.70)
i∈S
for all j S, and
X
η i = 1
(A.71)
i∈S
Summing (A.70) over all states j A J we obtain
X
η 0 I q 0 IJ = 0
(A.72)
A I ∈S 0
for all A J S 0 , and
X
η 0 I
= 1
(A.73)
A I ∈S 0
where
X
X
q 0 IJ =
q ij ν i|I
(A.74)
i∈A I
j∈A J
and ν i|I is as in (A.65) . Also in this case equations ( A.69) - ( A.74) hold,
regardless of the fulfillment of the lumpability condition, so that we can
directly evaluate the steady-state distribution of macrostates from ( A.72)
provided that we can evaluate the q 0 IJ from ( A.74) without solving for the
steady-state distribution of the CTMC { X(t),t 0 } .
If the CTMC { X(t),t 0 } is lumpable with respect to the partition S 0 , then
( A.67) holds, and ( A.72) reduces to
X
X
η 0 I
i A I
q ij
= 0
(A.75)
A I ∈S 0
j∈A J
A.6
Semi-Markov Processes
Consider the stochastic process sample function shown in Fig. A.4. Assume
that the process { X(t),t 0 } is a finite-state continuous-time homogeneous
process which changes state at instants θ n , n = 0, 1, ··· and assumes the
value Y n in the interval [θ n n+1 ), and such that
P { Y n+1 = j,θ n+1 θ n τ | Y 0 = k, ··· ,Y n = i,θ 0 = t 0 , ··· θ n = t n }
= P { Y n+1 = j,θ n+1 θ n τ | Y n = i } = H ij (τ)
(A.76)
 
 
 
 
 
 
 
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