Mutual information

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In probability theory and information theory, the mutual information, or transinformation, of two random variables is a quantity that measures the mutual dependence of the two variables. The most common unit of measurement of mutual information is the bit, when logarithms to the base 2 are used.

Definition of mutual information

Formally, the mutual information of two discrete random variables X and Y can be defined as:

<math> I(X;Y) = \sum_{y \in Y} \sum_{x \in X}
                p(x,y) \log{ \left( \frac{p(x,y)}{p_1(x)\,p_2(y)}
                             \right) }, \,\!

</math>

where p(x,y) is the joint probability distribution function of X and Y, and <math>p_1(x)</math> and <math>p_2(y)</math> are the marginal probability distribution functions of X and Y respectively.

In the continuous case, we replace summation by a definite double integral:

<math> I(X;Y) = \int_Y \int_X
                p(x,y) \log{ \left( \frac{p(x,y)}{p_1(x)\,p_2(y)}
                             \right) } \; dx \,dy, \,\!dsf

</math>

where p(x,y) is now the joint probability density function of X and Y, and <math>p_1(x)</math> and <math>p_2(y)</math> are the marginal probability density functions of X and Y respectively.

These definitions are ambiguous because the base of the log function is not specified. To disambiguate, the function I could be parameterized as I(X,Y,b) where b is the base. Alternatively, since the most common unit of measurement of mutual information is the bit, a base of 2 could be specified.

Intuitively, mutual information measures the information that X and Y share: it measures how much knowing one of these variables reduces our uncertainty about the other. For example, if X and Y are independent, then knowing X does not give any information about Y and vice versa, so their mutual information is zero. At the other extreme, if X and Y are identical then all information conveyed by X is shared with Y: knowing X determines the value of Y and vice versa. As a result, the mutual information is the same as the uncertainty contained in Y (or X) alone, namely the entropy of Y (or X: clearly if X and Y are identical they have equal entropy).

Mutual information quantifies the distance between the joint distribution of X and Y and what the joint distribution would be if X and Y were independent. Mutual information is a measure of dependence in the following sense: I(X; Y) = 0 if and only if X and Y are independent random variables. This is easy to see in one direction: if X and Y are independent, then p(x,y) = p(x) × p(y), and therefore:

<math> \log{ \left( \frac{p(x,y)}{p(x)\,p(y)} \right) } = \log 1 = 0. \,\!
</math>

Moreover, mutual information is nonnegative (i.e. I(X;Y) ≥ 0; see below) and symmetric (i.e. I(X;Y) = I(Y;X)).

Relation to other quantities

Mutual information can be equivalently expressed as

<math>

\begin{align} I(X;Y) & {} = H(X) - H(X|Y) \\ & {} = H(Y) - H(Y|X) \\ & {} = H(X) + H(Y) - H(X,Y) \end{align} </math>

where H(X) and H(Y) are the marginal entropies, H(X|Y) and H(Y|X) are the conditional entropies, and H(X,Y) is the joint entropy of X and Y. Since H(X) ≥ H(X|Y), this characterization is consistent with the nonnegativity property stated above.

Intuitively, if entropy H(X) is regarded as a measure of uncertainty about a random variable, then H(X|Y) is a measure of what Y does not say about X. This is "the amount of uncertainty remaining about X after Y is known", and thus the right side of the first of these equalities can be read as "the amount of uncertainty in X, minus the amount of uncertainty in X which remains after Y is known", which is equivalent to "the amount of uncertainty in X which is removed by knowing Y". This corroborates the intuitive meaning of mutual information as the amount of information (that is, reduction in uncertainty) that knowing either variable provides about the other.

Note that in the discrete case H(X|X) = 0 and therefore H(X) = I(X;X). Thus I(X;X) ≥ I(X;Y), and one can formulate the basic principle that a variable contains more information about itself than any other variable can provide.

Mutual information can also be expressed as a Kullback-Leibler divergence, of the product p(x) × p(y) of the marginal distributions of the two random variables X and Y, from p(x,y) the random variables' joint distribution:

<math> I(X;Y) = D_{\mathrm{KL}}(p(x,y)\|p(x)p(y)). </math>

Furthermore, let p(x|y) = p(x, y) / p(y). Then

<math>

\begin{align} I(X;Y) & {} = \sum_y p(y) \sum_x p(x|y) \log_2 \frac{p(x|y)}{p(x)} \\ & {} = \sum_y p(y) \; D_{\mathrm{KL}}(p(x|y)\|p(x)) \\ & {} = \mathbb{E}_Y\{D_{\mathrm{KL}}(p(x|y)\|p(x))\}. \end{align} </math>

Thus mutual information can thus also be understood as the expectation of the Kullback-Leibler divergence of the univariate distribution p(x) of X from the conditional distribution p(x|y) of X given Y: the more different the distributions p(x|y) and p(x), the greater the information gain.

Variations of the mutual information

Several variations on the mutual information have been proposed to suit various needs. Among these are normalized variants and generalizations to more than two variables.

Normalized variants

Normalized variants of the mutual information are provided by the coefficients of constraint (Coombs, Dawes & Tversky 1970) or uncertainty coefficient (Press & Flannery 1988)

<math>

C_{XY}=\frac{I(X;Y)}{H(Y)} WikiBot 07:58, 10 August 2012 (UTC)\mbox{and}WikiBot 07:58, 10 August 2012 (UTC) C_{YX}=\frac{I(X;Y)}{H(X)} </math>

The two coefficients are not necessarily equal. A more useful and symmetric scaled information measure is the redundancy

<math>R= \frac{I(X;Y)}{H(X)+H(Y)}</math>

which obtains a minimum of zero when the variables are independent and a maximum value of

<math>R_{\max }=\frac{\min (H(X),H(Y))}{H(X)+H(Y)} </math>

when one variable becomes completely redundant with the knowledge of the other. Another symmetrical measure is the symmetric uncertainty (Witten & Frank 2005), given by

<math>U(X,Y) = 2R = 2 \frac{I(X;Y)}{H(X)+H(Y)}</math>

which represents a weighted average of the two uncertainty coefficients (Press & Flannery 1988).

Other normalized versions are provided by the following expressions (Yao 2003, Strehl & Ghosh 2002).

<math>

\frac{I(X;Y)}{\mbox{min}(H(X),H(Y))}, 07:58, 10 August 2012 (UTC)~~ \frac{I(X;Y)}{H(X,Y)}, 07:58, 10 August 2012 (UTC)~~ \frac{I(X;Y)}{\sqrt{H(X)H(Y)}} </math>

Weighted variants

In the traditional formulation of the mutual information,

<math> I(X;Y) = \sum_{y \in Y} \sum_{x \in X} p(x,y) \log \frac{p(x,y)}{p(x)\,p(y)}, </math>

each event or object specified by <math>(x,y)</math> is weighted by the corresponding probability <math>p(x,y)</math>. This assumes that all objects or events are equivalent apart from their probability of occurrence. However, in some applications it may be the case that certain objects or events are more significant than others, or that certain patterns of association are more semantically important than others.

For example, the deterministic mapping <math>\{(1,1),(2,2),(3,3)\}</math> may be viewed as stronger (by some standard) than the deterministic mapping <math>\{(1,3),(2,1),(3,2)\}</math>, although these relationships would yield the same mutual information. This is because the mutual information is not sensitive at all to any inherent ordering in the variable values (Cronbach 1954, Coombs & Dawes 1970, Lockhead 1970), and is therefore not sensitive at all to the form of the relational mapping between the associated variables. If it is desired that the former relation — showing agreement on all variable values — be judged stronger than the later relation, then it is possible to use the following weighted mutual information (Guiasu 1977)

<math> I(X;Y) = \sum_{y \in Y} \sum_{x \in X} w(x,y) p(x,y) \log \frac{p(x,y)}{p(x)\,p(y)}, </math>

which places a weight <math>w(x,y)</math> on the probability of each variable value co-occurrence, <math>p(x,y)</math>. This allows that certain probabilities may carry more or less significance than others, thereby allowing the quantification of relevant holistic or prägnanz factors. In the above example, using larger relative weights for <math>w(1,1)</math>, <math>w(2,2)</math>, and <math>w(3,3)</math> would have the effect of assessing greater informativeness for the relation <math>\{(1,1),(2,2),(3,3)\}</math> than for the relation <math>\{(1,3),(2,1),(3,2)\}</math>, which may be desirable in some cases of pattern recognition, and the like. There has been little mathematical work done on the weighted mutual information and its properties, however.

Multiple-variable variants

Several generalizations of mutual information to more than two random variables have been proposed, such as total correlation and interaction information, but a widely agreed on definition has not yet emerged. One high-dimensional generalization scheme that maximizes the mutual information between the joint distribution and other target variables is found be useful in feature selection.

Absolute mutual information

Using the ideas of Kolmogorov complexity, one can consider the mutual information of two sequences independent of any probability distribution:

<math>

I_K(X;Y) = K(X) - K(X|Y). </math>

To establish that this quantity is symmetric up to a logarithmic factor (<math>I_K(X;Y) \approx I_K(Y;X)</math>) requires the chain rule for Kolmogorov complexity Template:Harvard citation. Approximations of this quantity via compression can be used to define a distance measure to perform a hierarchical clustering of sequences without having any domain knowledge of the sequences Template:Harvard citation.

Applications of mutual information

In many applications, one wants to maximize mutual information (thus increasing dependencies), which is often equivalent to minimizing conditional entropy. Examples include:

See also

References

  • Cilibrasi, R. (2005). "Clustering by compression" (PDF). IEEE Transactions on Information Theory. 51 (4): 1523–1545. Unknown parameter |coauthors= ignored (help)
  • Coombs, C. H., Dawes, R. M. & Tversky, A. (1970), Mathematical Psychology: An Elementary Introduction, Prentice-Hall, Englewood Cliffs, NJ.
  • Cronbach L. J. (1954). On the non-rational application of information measures in psychology, in H Quastler, ed., Information Theory in Psychology: Problems and Methods, Free Press, Glencoe, Illinois, pp. 14—30.
  • Kenneth Ward Church and Patrick Hanks. Word association norms, mutual information, and lexicography, Proceedings of the 27th Annual Meeting of the Association for Computational Linguistics, 1989.
  • Guiasu, Silviu (1977), Information Theory with Applications, McGraw-Hill, New York.
  • Li, Ming (1997). An introduction to Kolmogorov complexity and its applications. New York: Springer-Verlag. ISBN 0387948686. Unknown parameter |coauthors= ignored (help); Unknown parameter |month= ignored (help)
  • Lockhead G. R. (1970). Identification and the form of multidimensional discrimination space, Journal of Experimental Psychology 85(1), 1-10.
  • Athanasios Papoulis. Probability, Random Variables, and Stochastic Processes, second edition. New York: McGraw-Hill, 1984. (See Chapter 15.)
  • Press, W. H., Flannery, B. P., Teukolsky, S. A. & Vetterling, W. T. (1988), Numerical Recipes in C: The Art of Scientific Computing, Cambridge University Press, Cambridge, p. 634
  • Witten, Ian H. & Frank, Eibe (2005), Data Mining: Practical Machine Learning Tools and Techniques, Morgan Kaufmann, Amsterdam.
  • Yao, Y. Y. (2003) Information-theoretic measures for knowledge discovery and data mining, in Entropy Measures, Maximum Entropy Principle and Emerging Applications , Karmeshu (ed.), Springer, pp. 115-136.
  • Peng, H.C., Long, F., and Ding, C., "Feature selection based on mutual information: criteria of max-dependency, max-relevance, and min-redundancy," IEEE Transactions on Pattern Analysis and Machine Intelligence, Vol. 27, No. 8, pp.1226-1238, 2005. Program
  • Andre S. Ribeiro, Stuart A. Kauffman, Jason Lloyd-Price, Bjorn Samuelsson, and Joshua Socolar, (2008) "Mutual Information in Random Boolean models of regulatory networks", Physical Review E, Vol.77, No.1. arXiv:0707.3642.

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