Joint entropy: Difference between revisions
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{{Short description|Measure of information in probability and information theory}} |
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[[Image:Conditional_entropy.png|thumb|256px|right|Individual (H(X),H(Y)), joint (H(X,Y)), and conditional entropies for a pair of correlated subsystems X,Y with mutual information I(X; Y).]] |
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{{Information theory}} |
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[[Image:Entropy-mutual-information-relative-entropy-relation-diagram.svg|thumb|256px|right|A misleading<ref>{{Cite book|author=D.J.C. Mackay|title= Information theory, inferences, and learning algorithms|year= 2003|bibcode= 2003itil.book.....M}}{{rp|141}}</ref> [[Venn diagram]] showing additive, and subtractive relationships between various [[Quantities of information|information measures]] associated with correlated variables X and Y. The area contained by both circles is the joint entropy H(X,Y). The circle on the left (red and violet) is the [[Entropy (information theory)|individual entropy]] H(X), with the red being the [[conditional entropy]] H(X{{pipe}}Y). The circle on the right (blue and violet) is H(Y), with the blue being H(Y{{pipe}}X). The violet is the [[mutual information]] I(X;Y).]] |
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'''Joint [[entropy (information theory)|entropy]]''' is a measure of the uncertainty associated with a set of [[random variables|variables]]. |
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In [[information theory]], '''joint [[entropy (information theory)|entropy]]''' is a measure of the uncertainty associated with a set of [[random variables|variables]].<ref name=korn>{{cite book |author1=Theresa M. Korn|author1-link= Theresa M. Korn |author2=Korn, Granino Arthur |title=Mathematical Handbook for Scientists and Engineers: Definitions, Theorems, and Formulas for Reference and Review |date= January 2000 |publisher=Dover Publications |location=New York |isbn=0-486-41147-8 }}</ref> |
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==Definition== |
==Definition== |
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The joint [[Shannon entropy]] (in [[bit]]s) of two discrete [[random variable|random variables]] <math>X</math> and <math>Y</math> with images <math>\mathcal X</math> and <math>\mathcal Y</math> is defined as<ref name=cover1991>{{cite book |author1=Thomas M. Cover |author2=Joy A. Thomas |title=Elements of Information Theory |date=18 July 2006 |publisher=Wiley |location=Hoboken, New Jersey |isbn=0-471-24195-4}}</ref>{{rp|16}} |
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The joint entropy of two variables <math>X</math> and <math>Y</math> is defined as |
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{{Equation box 1 |
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where <math>x</math> and <math>y</math> are particular values of <math>X</math> and <math>Y</math>, respectively, <math>P(x,y)</math> is the probability of these values occurring together, and <math>P(x,y) \log_2[P(x,y)]</math> is defined to be 0 if <math>P(x,y)=0</math>. |
where <math>x</math> and <math>y</math> are particular values of <math>X</math> and <math>Y</math>, respectively, <math>P(x,y)</math> is the [[joint probability]] of these values occurring together, and <math>P(x,y) \log_2[P(x,y)]</math> is defined to be 0 if <math>P(x,y)=0</math>. |
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For more than two variables <math>X_1, ..., X_n</math> this expands to |
For more than two random variables <math>X_1, ..., X_n</math> this expands to |
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{{Equation box 1 |
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|equation = {{NumBlk||<math>\Eta(X_1, ..., X_n) = |
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where <math>x_1,...,x_n</math> are particular values of <math>X_1,...,X_n</math>, respectively, <math>P(x_1, ..., x_n)</math> is the probability of these values occurring together, and <math>P(x_1, ..., x_n) \log_2[P(x_1, ..., x_n)]</math> is defined to be 0 if <math>P(x_1, ..., x_n)=0</math>. |
where <math>x_1,...,x_n</math> are particular values of <math>X_1,...,X_n</math>, respectively, <math>P(x_1, ..., x_n)</math> is the probability of these values occurring together, and <math>P(x_1, ..., x_n) \log_2[P(x_1, ..., x_n)]</math> is defined to be 0 if <math>P(x_1, ..., x_n)=0</math>. |
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==Properties== |
==Properties== |
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===Nonnegativity=== |
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The joint entropy of a set of random variables is a nonnegative number. |
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:<math>\Eta(X,Y) \geq 0</math> |
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:<math>\Eta(X_1,\ldots, X_n) \geq 0</math> |
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===Greater than individual entropies=== |
===Greater than individual entropies=== |
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The joint entropy of a set of variables is greater than or equal to all of the individual entropies of the variables in the set. |
The joint entropy of a set of variables is greater than or equal to the maximum of all of the individual entropies of the variables in the set. |
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:<math> |
:<math>\Eta(X,Y) \geq \max \left[\Eta(X),\Eta(Y) \right]</math> |
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:<math> |
:<math>\Eta \bigl(X_1,\ldots, X_n \bigr) \geq \max_{1 \le i \le n} |
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\Bigl\{ \Eta\bigl(X_i\bigr) \Bigr\}</math> |
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===Less than sum of individual entropies=== |
===Less than or equal to the sum of individual entropies=== |
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The joint entropy of a set of variables is less than or equal to the sum of the individual entropies of the variables in the set. This is an example of [[subadditivity]]. This inequality is an equality if and only if <math>X</math> and <math>Y</math> are [[statistically independent]]. |
The joint entropy of a set of variables is less than or equal to the sum of the individual entropies of the variables in the set. This is an example of [[subadditivity]]. This inequality is an equality if and only if <math>X</math> and <math>Y</math> are [[statistically independent]].<ref name=cover1991 />{{rp|30}} |
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:<math> |
:<math>\Eta(X,Y) \leq \Eta(X) + \Eta(Y)</math> |
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:<math> |
:<math>\Eta(X_1,\ldots, X_n) \leq \Eta(X_1) + \ldots + \Eta(X_n)</math> |
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==Relations to |
==Relations to other entropy measures== |
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Joint entropy is used in the definition of [[conditional entropy]] |
Joint entropy is used in the definition of [[conditional entropy]]<ref name=cover1991 />{{rp|22}} |
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:<math> |
:<math>\Eta(X|Y) = \Eta(X,Y) - \Eta(Y)\,</math>, |
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and |
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-- and [[mutual information]]: |
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:<math> |
:<math>\Eta(X_1,\dots,X_n) = \sum_{k=1}^n \Eta(X_k|X_{k-1},\dots, X_1)</math>. |
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It is also used in the definition of [[mutual information]]<ref name=cover1991 />{{rp|21}} |
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:<math>\operatorname{I}(X;Y) = \Eta(X) + \Eta(Y) - \Eta(X,Y)\,</math>. |
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In [[quantum information theory]], the joint entropy is generalized into the [[joint quantum entropy]]. |
In [[quantum information theory]], the joint entropy is generalized into the [[joint quantum entropy]]. |
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==Joint differential entropy== |
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===Definition=== |
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The above definition is for discrete random variables and just as valid in the case of continuous random variables. The continuous version of discrete joint entropy is called ''joint differential (or continuous) entropy''. Let <math>X</math> and <math>Y</math> be a continuous random variables with a [[joint probability density function]] <math>f(x,y)</math>. The differential joint entropy <math>h(X,Y)</math> is defined as<ref name=cover1991 />{{rp|249}} |
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{{Equation box 1 |
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|equation = {{NumBlk||<math>h(X,Y) = -\int_{\mathcal X , \mathcal Y} f(x,y)\log f(x,y)\,dx dy</math>|{{EquationRef|Eq.3}}}} |
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For more than two continuous random variables <math>X_1, ..., X_n</math> the definition is generalized to: |
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{{Equation box 1 |
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|equation = {{NumBlk||<math>h(X_1, \ldots,X_n) = -\int f(x_1, \ldots,x_n)\log f(x_1, \ldots,x_n)\,dx_1 \ldots dx_n</math>|{{EquationRef|Eq.4}}}} |
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The [[integral]] is taken over the support of <math>f</math>. It is possible that the integral does not exist in which case we say that the differential entropy is not defined. |
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===Properties=== |
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As in the discrete case the joint differential entropy of a set of random variables is smaller or equal than the sum of the entropies of the individual random variables: |
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:<math>h(X_1,X_2, \ldots,X_n) \le \sum_{i=1}^n h(X_i)</math><ref name=cover1991 />{{rp|253}} |
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The following chain rule holds for two random variables: |
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:<math>h(X,Y) = h(X|Y) + h(Y)</math> |
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In the case of more than two random variables this generalizes to:<ref name=cover1991 />{{rp|253}} |
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:<math>h(X_1,X_2, \ldots,X_n) = \sum_{i=1}^n h(X_i|X_1,X_2, \ldots,X_{i-1})</math> |
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Joint differential entropy is also used in the definition of the [[mutual information]] between continuous random variables: |
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:<math>\operatorname{I}(X,Y)=h(X)+h(Y)-h(X,Y)</math> |
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== References == |
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{{Reflist}} |
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[[Category:Entropy and information]] |
[[Category:Entropy and information]] |
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[[de:Blockentropie]] |
[[de:Bedingte Entropie#Blockentropie]] |
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[[fr:Entropie conjointe]] |
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[[ja:結合エントロピー]] |
Latest revision as of 03:22, 10 November 2024
Information theory |
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In information theory, joint entropy is a measure of the uncertainty associated with a set of variables.[2]
Definition
[edit]The joint Shannon entropy (in bits) of two discrete random variables and with images and is defined as[3]: 16
(Eq.1) |
where and are particular values of and , respectively, is the joint probability of these values occurring together, and is defined to be 0 if .
For more than two random variables this expands to
(Eq.2) |
where are particular values of , respectively, is the probability of these values occurring together, and is defined to be 0 if .
Properties
[edit]Nonnegativity
[edit]The joint entropy of a set of random variables is a nonnegative number.
Greater than individual entropies
[edit]The joint entropy of a set of variables is greater than or equal to the maximum of all of the individual entropies of the variables in the set.
Less than or equal to the sum of individual entropies
[edit]The joint entropy of a set of variables is less than or equal to the sum of the individual entropies of the variables in the set. This is an example of subadditivity. This inequality is an equality if and only if and are statistically independent.[3]: 30
Relations to other entropy measures
[edit]Joint entropy is used in the definition of conditional entropy[3]: 22
- ,
and
- .
It is also used in the definition of mutual information[3]: 21
- .
In quantum information theory, the joint entropy is generalized into the joint quantum entropy.
Joint differential entropy
[edit]Definition
[edit]The above definition is for discrete random variables and just as valid in the case of continuous random variables. The continuous version of discrete joint entropy is called joint differential (or continuous) entropy. Let and be a continuous random variables with a joint probability density function . The differential joint entropy is defined as[3]: 249
(Eq.3) |
For more than two continuous random variables the definition is generalized to:
(Eq.4) |
The integral is taken over the support of . It is possible that the integral does not exist in which case we say that the differential entropy is not defined.
Properties
[edit]As in the discrete case the joint differential entropy of a set of random variables is smaller or equal than the sum of the entropies of the individual random variables:
- [3]: 253
The following chain rule holds for two random variables:
In the case of more than two random variables this generalizes to:[3]: 253
Joint differential entropy is also used in the definition of the mutual information between continuous random variables:
References
[edit]- ^ D.J.C. Mackay (2003). Information theory, inferences, and learning algorithms. Bibcode:2003itil.book.....M.: 141
- ^ Theresa M. Korn; Korn, Granino Arthur (January 2000). Mathematical Handbook for Scientists and Engineers: Definitions, Theorems, and Formulas for Reference and Review. New York: Dover Publications. ISBN 0-486-41147-8.
- ^ a b c d e f g Thomas M. Cover; Joy A. Thomas (18 July 2006). Elements of Information Theory. Hoboken, New Jersey: Wiley. ISBN 0-471-24195-4.