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TRANSIENT STATE PROBABILITIES                163

                variation over time with peaks at certain hours of the day. Equilibrium models
                are of no use in this kind of situation. The computation of transient solutions for
                Markov systems is a very important issue that arises in numerous problems in
                queueing, inventory and reliability. In this section we discuss two basic methods
                for the computation of the transient state probabilities of a continuous-time Markov
                chain. The next section deals with the computation of the transient distribution of
                the cumulative reward in a continuous-time Markov chain with a reward structure.
                  The transient probabilities of a continuous-time Markov chain {X(t), t ≥ 0} are
                defined by
                           p ij (t) = P {X(t) = j | X(0) = i},  i, j ∈ I and t > 0.

                In Section 4.5.1 we discuss the method of linear differential equations. The proba-
                bilistic method of uniformization will be discussed in Section 4.5.2. In Section 4.5.3
                we show that the computation of first passage time probabilities can be reduced to
                the computation of transient state probabilities by introducing an absorbing state.

                4.5.1 The Method of Linear Differential Equations
                This basic approach has a solid backing by tools from numerical analysis. We first
                prove the following theorem.

                Theorem 4.5.1 (Kolmogoroff’s forward differential equations) Suppose that
                the continuous-time Markov chain {X(t), t ≥ 0} satisfies Assumption 4.1.2. Then
                for any i ∈ I,


                             ′
                            p (t) =   q kj p ik (t) − ν j p ij (t),  j ∈ I and t > 0.  (4.5.1)
                             ij
                                   k =j
                Proof  We sketch the proof only for the case of a finite state space I. The proof
                of the validity of the forward equations for the case of an infinite state space is
                very intricate. Fix i ∈ I and t > 0. Let us consider what may happen in (t, t +  t]
                with  t very small. The number of transitions in any finite time interval is finite
                with probability 1, so we can condition on the state that will occur at time t:


                         p ij (t +  t) = P {X(t +  t) = j | X(0) = i}

                                   =    P {X(t +  t) = j | X(0) = i, X(t) = k}
                                     k∈I
                                     × P {X(t) = k | X(0) = i}

                                   =    P {X(t +  t) = j | X(t) = k}p ik (t)
                                     k∈I

                                   =    q kj  tp ik (t) + (1 − ν j  t)p ij (t) + o( t),
                                     k =j
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