Kelvin functions: Difference between revisions

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In the mathematical theory of [[probability]], the '''entropy rate''' or '''source information rate''' of a [[stochastic process]] is, informally, the time density of the average information in a stochastic process. For stochastic processes with a [[countable]] index, the entropy rate ''H''(''X'') is the limit of the [[joint entropy]] of ''n'' members of the process ''X''<sub>''k''</sub> divided by ''n'', as ''n'' [[Limit (mathematics)|tends to]] [[infinity]]:
 
:<math>H(X) = \lim_{n \to \infty} \frac{1}{n} H(X_1, X_2, \dots X_n)</math>
 
when the limit exists. An alternative, related quantity is:
 
:<math>H'(X) = \lim_{n \to \infty} H(X_n|X_{n-1}, X_{n-2}, \dots X_1)</math>
 
For [[strongly stationary]] stochastic processes, <math>H(X) = H'(X)</math>.  The entropy rate can be thought of as a general property of stochastic sources; this is the [[asymptotic equipartition property]].
 
== Entropy rates for Markov chains ==
Since a stochastic process defined by a [[Markov chain]] that is [[irreducible]] and [[aperiodic]] has a [[stationary distribution]], the entropy rate is independent of the initial distribution.
 
For example, for such a Markov chain ''Y''<sub>''k''</sub> defined on a [[countable]] number of states, given the [[transition matrix]] ''P''<sub>''ij''</sub>, ''H''(''Y'') is given by:
 
:<math>\displaystyle H(Y) = - \sum_{ij} \mu_i P_{ij} \log P_{ij}</math>
 
where ''&mu;''<sub>''i''</sub> is the [[stationary distribution]] of the chain.
 
A simple consequence of this definition is that the entropy rate of an [[independent and identically distributed|i.i.d.]] [[stochastic process]] has an entropy rate that is the same as the [[entropy]] of any individual member of the process.
 
==See also==
* [[Information source (mathematics)]]
* [[Markov information source]]
* [[Asymptotic equipartition property]]
 
==References==
 
* Cover, T. and Thomas, J. (1991) Elements of Information Theory, John Wiley and Sons, Inc., ISBN 0-471-06259-6 [http://www3.interscience.wiley.com/cgi-bin/bookhome/110438582?CRETRY=1&SRETRY=0]
 
== External links ==
* [http://www.eng.ox.ac.uk/samp Systems Analysis, Modelling and Prediction (SAMP), University of Oxford] [[MATLAB]] code for estimating information-theoretic quantities for stochastic processes.
 
[[Category:Information theory]]
[[Category:Entropy]]
[[Category:Markov models]]

Revision as of 06:43, 23 January 2014

In the mathematical theory of probability, the entropy rate or source information rate of a stochastic process is, informally, the time density of the average information in a stochastic process. For stochastic processes with a countable index, the entropy rate H(X) is the limit of the joint entropy of n members of the process Xk divided by n, as n tends to infinity:

H(X)=limn1nH(X1,X2,Xn)

when the limit exists. An alternative, related quantity is:

H(X)=limnH(Xn|Xn1,Xn2,X1)

For strongly stationary stochastic processes, H(X)=H(X). The entropy rate can be thought of as a general property of stochastic sources; this is the asymptotic equipartition property.

Entropy rates for Markov chains

Since a stochastic process defined by a Markov chain that is irreducible and aperiodic has a stationary distribution, the entropy rate is independent of the initial distribution.

For example, for such a Markov chain Yk defined on a countable number of states, given the transition matrix Pij, H(Y) is given by:

H(Y)=ijμiPijlogPij

where μi is the stationary distribution of the chain.

A simple consequence of this definition is that the entropy rate of an i.i.d. stochastic process has an entropy rate that is the same as the entropy of any individual member of the process.

See also

References

  • Cover, T. and Thomas, J. (1991) Elements of Information Theory, John Wiley and Sons, Inc., ISBN 0-471-06259-6 [1]

External links