“…Here we define a phase space X corresponding to P 0 as X = X (1) ∪ X (2) , where X (1) = {1, 2, 3, 4} and X (2) = {5, 6, 7, 8}. The corresponding matrices of transition probabilities for the two ergodic classes are, respectively, P 0,1 and P 0,2 , where P 0,1 = 0 1 0 0 We are going to get the second order asymptotic expansion for stationary probabilities π ε,k , k ∈ X given by relation (59).…”