Lumpability
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In probability theory, lumpability is a method for reducing the size of the state space of some continuous-time Markov chains, first published by Kemeny and Snell.
In probability theory, lumpability is a method for reducing the size of the state space of some continuous-time Markov chains, first published by Kemeny and Snell. ==Definition== Suppose that the complete state-space of a Markov chain is divided into disjoint subsets of states, where these subsets are denoted by t i . This forms a partition \scriptstyle{T = \{ t_1, t_2, \ldots \}} of the states. Both the state-space and the collection of subsets may be either finite or countably infinite. A continuous-time Markov chain \{ X_i \} is lumpable with respect to the partition T if and only if, for any subsets t i and t j in the partition, and for any states n,n’ in subset t i , \sum_{m \in t_j} q(n,m) = \sum_{m \in t_j} q(n',m) , where q(i,j) is the transition rate from state i to state j. Similarly, for a stochastic matrix P, P is a lumpable matrix on a partition T if and only if, for any subsets t i and t j in the partition, and for any states n,n’ in subset t i , \sum_{m \in t_j} p(n,m) = \sum_{m \in t_j} p(n',m) , where p(i,j) is the probability of moving from state i to state j. ==Example== Consider the matrix P = \begin{pmatrix} \frac{1}{2} & \frac{3}{8} & \frac{1}{16} & \frac{1}{16} \\ \frac{7}{16} & \frac{7}{16} & 0 & \frac{1}{8} \\ \frac{1}{16} & 0 & \frac{1}{2} & \frac{7}{16} \\ 0 & \frac{1}{16} & \frac{3}{8} & \frac{9}{16} \end{pmatrix} and notice it is lumpable on the partition t = {(1,2),(3,4)} so we write P_t = \begin{pmatrix} \frac{7}{8} & \frac{1}{8} \\ \frac{1}{16} & \frac{15}{16} \end{pmatrix} and call P t the lumped matrix of P on t. ==Quasi–lumpability== Franceschinis and Muntz introduced quasi-lumpability, a property whereby a small change in the rate matrix makes the chain lumpable. ==See also== Nearly completely decomposable Markov chain ==References==
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