Write the stationary distribution as a row vector . For the first transition matrix, gives , , and . Hence and . Normalization yieldsBy the stated common-stationary distribution property, this is also the answer for the second transition matrix.
The first Markov chain is a finite irreducible Markov chain: its positive-probability directed cycle reaches all four states. The self-loop at state 1 makes it an aperiodic Markov chain. Convergence to an invariant distribution therefore givesThe second chain alternates between the sets and . It is a periodic Markov chain with period two, so . From either state 2 or state 4 the next-step probability of entering state 1 is . Therefore for every . The subsequences have different limits, so the second return-probability sequence does not converge.
Start the Markov chain at a state and define the strictly positive first return time . A recurrent state satisfies ; a transient state has this probability strictly below one. Equivalently a recurrent state is visited infinitely often almost surely when started there, whereas a transient state receives finitely many visits almost surely. The recurrence criterion by return probabilities gives the equivalent testStates in a communicating class share this classification. In an irreducible Markov chain all states communicate, so the chain is called a recurrent Markov chain if all its states are recurrent and a transient Markov chain if all are transient.
Represent the simple random walk by , where the increments are independent and identically distributed and satisfy , . They are integrable and have expectation , so the strong law of large numbers givesIf , this nonzero drift implies that eventually leaves every fixed finite interval and tends to the appropriate infinity. Hence it visits zero only finitely many times almost surely, so zero is a transient state. By translation of the starting state, every state is transient: the chain is transient for . This also covers the deterministic endpoint cases , without assuming Markov chain irreducibility at those endpoints.
For the symmetric simple random walk on the integer line, odd return times are impossible. A return after steps requires exactly positive increments, soby Stirling's approximation. The resulting sum diverges by the p-series criterion. The recurrence criterion by return probabilities therefore makes zero a recurrent state. The simple random walk is an irreducible Markov chain on , so the symmetric chain is recurrent.
This is the synchronous product of simple symmetric random walks, rather than a walk that changes only one coordinate at a time. Independence of the three coordinate processes givesOdd-time return probabilities vanish. The p-series with exponent converges, so the sum of all return probabilities is finite. By the recurrence criterion by return probabilities, the origin is a transient state: the three-dimensional process is transient. From the origin its communicating class consists of integer triples whose coordinates have the same parity; translation gives the same classification for every other class.
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