Consider an Ergodic Markov Chain having transition probabilities Pij and stationary probabilities πi
A reversible Markov chain is like having a “time machine” for this little world. It considers the process to be “fair” in both directions.
We trace the sequence of states going backward in time, that is, starting at time n, consider the sequence of states Xn,Xn−1,Xn−2,...
This sequence of states is itself a Markov chain with transition probabilities Qij defined by Qij=P{Xm=j∣Xm+1=i}=πiπjPji
Opposite of Pij
The reverse process is also a Markov Chain
Markov chain is time reversible if Qij=Pij for all i,j
Equivalently πjPij=πiPji for all i,j
for all states i and j, the rate at which the process goes from i to j(πiPij) is equal to the rate at which it goes from j to i(πjPji)
We can model undirected connected graph with time reversible markov chain:
If at any time the particle resides at node i, then it will next move to node j with probability Pij where Pij=∑jwijwij
where wij is 1 if there is an arc, 0 otherwise
meaning probability from i to j is 1/number of arc connected from i
Using πiPji=πjPij=>πi∑jwijwij=πj∑iwjiwji combining with wij=wji and ∑iπi=1
we have πi=∑i∑jwij∑jwij
theorem A Stationary Markov Chain for which Pij=0 whenever Pji=0 is time reversible if and only if starting in state i, any path back to i has the same probability as the reversed path.
That is, if Pi,i1Pi1,i2...Pik,i=Pi,ikPik,ik−1...Pi2,i for all state i,i1,...,ik
Consider an irreducible Markov chain with transition probabilities Pij .
If we can find positive numbers πi,i≥0, summing to one, and a transition probability matrix Q=[Qij] such that πiPij=πjQji
then the Qij are the transition probabilities of the reversed chain and the πi are the stationary probabilities both for the original and reversed chain