Stationary Distributions (Continuous Time)

We quickly recap the results known for discrete time that also hold in continuous time. (The slight advantage from a modeling perspective is that in continuous time, transitions occur distinctly, which gives more chances for reversibility to hold)

Stationary Distributions

The stationary distribution of an irreducible continuous-time Markov chain is the unique probability distribution \pi satisfying the full balance equation

\displaystyle \pi Q = 0

That is,

\displaystyle \sum_{y \ne x} \pi(y)\, q(y,x) = \sum_{y \ne x} \pi(x)\, q(x,y) \quad \forall x \in \mathcal{X}

and, since \pi is a probability distribution, we require

\displaystyle \sum_{x \in \mathcal{X}} \pi(x) = 1

Theorem. An irreducible continuous-time Markov chain is positive recurrent if and only if there exists a solution to the balance equations.


Time Reversal

If X = (X(t) : t \in \mathbb{R}) is a continuous-time Markov chain with X(0) \sim \pi, we define its time reversal by

\displaystyle X^R = (X(-t) : t \in \mathbb{R})

Theorem. If X is a continuous-time Markov chain with Q-matrix Q = (q(x,y) : x,y \in \mathcal{X}) and stationary distribution \pi, then the reversed process X^R is also a continuous-time Markov chain with Q-matrix

\displaystyle q^R(x,y) = \frac{\pi(y)}{\pi(x)}\, q(x,y)

and the same stationary distribution \pi.

If X^R \overset{\mathcal{D}}{=} X, then the chain is called reversible. In this case, it satisfies the detailed balance equations:

\displaystyle \pi(x)\, q(x,y) = \pi(y)\, q(y,x) \quad \forall x,y \in \mathcal{X}

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