Markov process, stationary

A Markov process which is a stationary stochastic process. There is a stationary Markov process associated with a homogeneous Markov transition function if and only if there is a stationary initial distribution $ \mu ( A) $ corresponding to this function, that is, $ \mu ( A) $ satisfies

$$ \mu ( A) = \int\limits _ { X } P ( x , t , A ) \mu ( d x ) . $$

If the phase space $ X $ is finite, then a stationary initial distribution always exists, independent of whether the process has discrete $ ( t= 0 , 1 ,\dots) $ or continuous time. For a process in discrete time and for a countable set $ X $, a condition for existence of a stationary distribution has been found by A.N. Kolmogorov [1]: It is necessary and sufficient that there is class of communicating states $ Y \subset X $ such that the mathematical expectation of the time for reaching $ y _ {2} \in Y $ from $ y _ {1} \in Y $ is finite for any $ y _ {1} \in Y $. This criterion has been generalized to strong Markov processes with an arbitrary phase space $ X $: For the existence of a stationary process it is sufficient that there is a compact set $ K \subset X $ such that the expectation of the time of reaching $ K $ from $ x $ is finite for all $ x \in X $. There is the following sufficient condition for the existence of a stationary Markov process in terms of Lyapunov stochastic functions (cf. Lyapunov stochastic function): If there is a function $ V ( x) \leq 0 $ for which $ L V ( x) \leq - 1 $ for $ x \notin K $, then there is a stationary Markov process associated with the Markov transition function $ P ( x , t , A ) $. Here $ L $ is the infinitesimal generator of the process.

When the stationary initial distribution $ \mu $ is unique, the corresponding stationary process is ergodic. In this case the Cesàro mean of the transition probabilities converges weakly to $ \mu $. Under certain additional conditions,

$$ \lim\limits _ {t \rightarrow \infty } P ( x , t , A ) = \ \mu ( A) \ ( \textrm{ weakly } ) . $$

A stationary initial distribution satisfies the Fokker–Planck(–Kolmogorov) equation $ L ^ {*} \mu = 0 $, where $ L ^ {*} $ is the adjoint operator to the infinitesimal operator of the process. For example, $ L ^ {*} $ is the adjoint operator to the generating differential operator of the process for diffusion processes. In this case $ \mu $ has a density $ p $ with respect to the Lebesgue measure which satisfies $ L ^ {*} p = 0 $. In the one-dimensional case this equation can be solved by quadrature.

#### References[edit]

[1] |  A.N. Kolmogorov, "Markov chains with a countable number of states" , Moscow (1937) (In Russian)

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[2] |  J.L. Doob, "Stochastic processes" , Wiley (1953)
[3] |  A.B. Sevast'yanov, "An ergodic theorem for Markov processes and its application to telephone systems with refusals" Theor. Probab. Appl. , 2 (1957) pp. 104–112 Teor. Veroyatnost. i Primenen. , 2 : 1 (1957) pp. 106–116

#### Comments[edit]

#### References[edit]

[a1] |  K.L. Chung, "Markov chains with stationary transition probabilities", Springer (1960)

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[a2] |  W. Feller, "An introduction to probability theory and its applications", 1–2, Wiley (1966)
[a3] |  P. Lévy, "Processus stochastiques et mouvement Brownien", Gauthier-Villars (1965)
[a4] |  E. Parzen, "Stochastic processes", Holden-Day (1962)
[a5] |  Yu.A. Rozanov, "Stationary random processes", Holden-Day (1967) (Translated from Russian)