Problem in solving the long run behavior of a Markov chain. (Exercise 1.3 Georgy F.Lawler )

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Exercise 1.3 Introduction to Stochastic Processes Georgy.F Lawler :

Consider a Markov chain with state space {1,2,3} and transition matrix
$$ P= \begin{pmatrix} .4 & .2 & .4 \\ .6 & 0 & .4 \\ .2 & .5 & .3 \\ \end{pmatrix} $$ what is the probability in the long run that the chain is in state 1?

My Answer: I want to use the invariant probability vector as a left eigenvector. But according to Perron-Frobenius Theorem, The matrix P ( Markov matrix) doesn't satisfy the condition to use the invariant probability distribution.( all of entries must be strictly positive, one of them is zero ), so I am thinking to use the square of the matrix P instead of P .

My question: How can I use the invariant probability distribution here?

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The solution of the following system of equations will give the left eigenvector (assuming that there is a corresponding eigenvalue: $1$)

$$ \begin{pmatrix} P_1& P_2& P_3 \end{pmatrix}= \begin{pmatrix} P_1& P_2& P_3 \end{pmatrix} \begin{pmatrix} .4 & .2 & .4 \\ .6 & 0 & .4 \\ .2 & .5 & .3 \\ \end{pmatrix} .$$

If we want he eigenvector(s) to be long run state probabilites the we have to add the equation that

$$P_1+P_2+P_3=1.$$

So, we have

$$0.4P_1+0.6P_2+0.2P_3=P_1$$ $$0.2P_1+0.5P_3=P_2$$ $$0.4P_1+0.4P_2+0.5P_3=P_3$$ $$P_1+P_2+P_3=1.$$

This system of equations happens to have a unique solution:

$$P=\left(\frac{25}{66} \ \frac{17}{66}\ \frac{4}{11 }\right).$$

The long run probability that the process is in state $1$ is then

$$\frac{25}{66}.$$

The mere existence of this solution shows that there is an eigenvalue: $1$.