lumpability
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.
{{cite book
| first = John G.
| last = Kemeny
| author-link = John George Kemeny
| first2 = J. Laurie
| last2 = Snell
| editor-first = F. W.
| editor-last = Gehring
| editor2-first = P. R.
| editor2-last = Halmos
| title = Finite Markov Chains
| edition = Second
| orig-year = 1960
|date=July 1976
| publisher = Springer-Verlag
| location = New York Berlin Heidelberg Tokyo
| isbn = 978-0-387-90192-3
| pages = 124
}}
Definition
Suppose that the complete state-space of a Markov chain is divided into disjoint subsets of states, where these subsets are denoted by ti. This forms a partition of the states. Both the state-space and the collection of subsets may be either finite or countably infinite.
A continuous-time Markov chain is lumpable with respect to the partition T if and only if, for any subsets ti and tj in the partition, and for any states n,n’ in subset ti,
:
where q(i,j) is the transition rate from state i to state j.Jane Hillston, [http://www.dcs.ed.ac.uk/pepa/compositional.ps.gz Compositional Markovian Modelling Using A Process Algebra] in the Proceedings of the Second International Workshop on Numerical Solution of Markov Chains: Computations with Markov Chains, Raleigh, North Carolina, January 1995. Kluwer Academic Press
Similarly, for a stochastic matrix P, P is a lumpable matrix on a partition T if and only if, for any subsets ti and tj in the partition, and for any states n,n’ in subset ti,
:
where p(i,j) is the probability of moving from state i to state j.Peter G. Harrison and Naresh M. Patel, Performance Modelling of Communication Networks and Computer Architectures Addison-Wesley 1992
Example
Consider the matrix
:
\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
:
\frac{7}{8} & \frac{1}{8} \\
\frac{1}{16} & \frac{15}{16} \end{pmatrix}
and call Pt the lumped matrix of P on t.
Successively lumpable processes
In 2012, Katehakis and Smit discovered the Successively Lumpable processes for which the stationary probabilities can be obtained by successively computing the stationary probabilities of a propitiously constructed sequence of Markov chains. Each of the latter chains has a (typically much) smaller state space and this yields significant computational improvements. These results have many applications reliability and queueing models and problems.{{Cite journal | last1 = Katehakis | first1 = M. N. | author-link1 = Michael Katehakis| last2 = Smit | first2 = L. C. | doi = 10.1017/S0269964812000150 | title = A Successive Lumping Procedure for a Class of Markov Chains | journal = Probability in the Engineering and Informational Sciences | volume = 26 | issue = 4 | pages = 483 | year = 2012 }}
Quasi–lumpability
Franceschinis and Muntz introduced quasi-lumpability, a property whereby a small change in the rate matrix makes the chain lumpable.{{cite journal |last1=Franceschinis |first1=G. |last2=Muntz |first2=Richard R. |year=1993 |title=Bounds for quasi-lumpable Markov chains |journal=Performance Evaluation |publisher=Elsevier B.V. |volume=20 |issue=1–3 |pages=223–243 |doi=10.1016/0166-5316(94)90015-9}}
See also
References
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