Graphics Programs Reference
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for all A J S 0 , and also
X
η 0 J = 1
(A.62)
A J ∈S 0
where
X
η 0 J = lim n→∞ P { X n A J } =
j∈A J η j
(A.63)
X
X
p 0 IJ =
p ij ν i|I
(A.64)
i∈A I
j∈A J
η i
ν i|I =
(A.65)
P
k∈A I η k
Note that equations ( A.60) to (A.65) hold for all DTMCs, regardless of
the fulfillment of the lumpability condition, so that it is possible to evalu-
ate the steady-state distribution over macrostates from ( A.61) and ( A.62) ,
provided that we can evaluate the quantities p 0 IJ from (A.64) and ( A.65) .
Obviously, we do not want to evaluate the steady-state distribution of the
process { X n ,n 0 } and then plug the result into (A.64) and ( A.65) , since
the reason to aggregate states into macrostates is exactly to avoid the so-
lution of this problem due to the large number of states. In some cases,
however, it is possible to evaluate the p 0 IJ without solving for the η i .
The lumpability condition (A.59) is su cient to very simply obtain the p 0 IJ
without solving for the η i . In this case ( A.61) becomes
X
X
η 0 J
η 0 I
i A I
=
p ij
(A.66)
A I ∈S 0
j∈A J
A.5.2 Aggregation in Continuous Time Markov Chains
Consider a finite, ergodic CTMC { X(t),t 0 } with state space S = { 1, 2, ··· ,N } ,
infinitesimal generator Q, transition probability matrix P(t), state distri-
bution η(t), and equilibrium distribution η.
Define also in this case a partition of S by aggregating states into macrostates
A I such that ( A.55) holds.
A new stochastic process { Y (t),t 0 } can be defined on the set of macrostates,
with state space S 0 = { A 1 ,A 2 , ··· ,A M } . It can be shown that the condition
for this new process to be an ergodic CTMC is
X
q ij = q 0 IJ i A I
(A.67)
j∈A J
The q 0 IJ are the entries of the infinitesimal generator Q 0 of the process
{ Y (t),t 0 } . This equation represents the condition for the lumpability
of the CTMC { X(t),t 0 } with respect to the partition S 0 . This condition
also implies that
X
p ij (t) = p 0 IJ (t) i A I
(A.68)
j∈A J
 
 
 
 
 
 
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