A stationary distribution describes how probability is spread across the states of a Markov chain after a transition leaves that distribution unchanged. It also represents the long-run frequency of visits when the chain settles into such behavior. A time-invariant chain has transition probabilities that do not change over time; that is a property of the transitions, not the definition of a stationary distribution. section 7.1
Let A be a transition matrix whose rows sum to 1, and let π₀ be an initial row vector of state probabilities. After n transitions, the distribution is π₀Aⁿ. A stationary distribution π satisfies πA = π, with entries that sum to 1. Thus π is a left eigenvector of A with eigenvalue 1. Repeated transitions provide a way to approach it when the chain's behavior permits convergence. section 7.1
The two-state model makes each transition probability—and the requirement that probabilities leaving a state sum to 1—visible. section 7.1
Ranking web pages
Represent pages as states and links as possible transitions. The stationary probability πⱼ serves as page j's rank. Following links alone can leave pages unreachable or produce oscillation, so the transition rule also allows a uniformly chosen page; pages with no outgoing links use that random jump. For a large transition matrix, an iterative power method seeks the relevant eigenvector rather than treating ranking as a separate scoring rule. section 7.1.1
The same idea gives Markov chain Monte Carlo its target: construct a chain whose stationary distribution is the posterior p(θ|x). A random walk through parameter space then spends time in states in proportion to that posterior, supplying samples for Monte Carlo estimates. section 2.0 section 1.4.1
