Elements Of Applied Probability For Engineering, Mathematics And Systems Science

5.2: Steady-State Markov Chains

5.2 Steady-State Markov Chains

Consider a probability transition kernel K ij on a state space S. We say a state j is accessible from state i if for some n ? 0, K ij n > 0. We say two states i and j communicate if each is accessible from the other.

Proposition 5.10

The state space may be divided into disjoint sets called communication classes. States within a communication class all communicate.

Proof: Suppose k communicates with both i and j. Therefore there exist n and m such that K ik m > 0 and K kj n > 0. Now by the Chapman-Kolmogorov equation

Hence j is accessible from i. Similarly i is accessible from j, so i and j communicate. Communicating states form an equivalence class so sets of communicating states are necessarily equal or disjoint. (The notion of equivalence class is reviewed in the Appendix.)

Example 5.11: A reducible chain

Consider the probability kernel

Clearly K has two communication classes, the first two states and the last two.

Definition 5.12

We say a Markov chain is irreducible if there is only one communication class.

Definition 5.13

We say a positive measure ? on S is stationary if

and is a stationary probability measure if in addition ? i ?( i) = 1.

If the initial distribution of a Markov...

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