In quantum information theory, quantum mutual information (QMI), or von Neumann mutual information, after John von Neumann, is a measure of correlation between subsystems of quantum state. It is the quantum mechanical analog of Shannon mutual information.
Motivation For simplicity, it will be assumed that all objects in the article are finite-dimensional. The definition of quantum mutual entropy is motivated by the classical case. For a probability distribution of two variables p(x, y), the two marginal distributions are
p ( x ) = ∑ y p ( x , y ) , p ( y ) = ∑ x p ( x , y ) . {\displaystyle p(x)=\sum _{y}p(x,y),\qquad p(y)=\sum _{x}p(x,y).}
The classical mutual information I(X:Y) is defined by
I ( X : Y ) = S ( p ( x ) ) + S ( p ( y ) ) − S ( p ( x , y ) ) {\displaystyle I(X:Y)=S(p(x))+S(p(y))-S(p(x,y))}
where S(q) denotes the Shannon entropy of the probability distribution q. One can calculate directly
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