Joint quantum entropy

The joint quantum entropy generalizes the classical joint entropy to the context of quantum information theory. Intuitively, given two quantum states formula_1 and formula_2, represented as density operators that are subparts of a quantum system, the joint quantum entropy is a measure of the total uncertainty or entropy of the joint system. It is written formula_3 or formula_4, depending on the notation being used for the von Neumann entropy. Like other entropies, the joint quantum entropy is measured in bits, i.e. the logarithm is taken in base 2.
In this article, we will use formula_3 for the joint quantum entropy.
Background.
In information theory, for any classical random variable formula_6, the classical Shannon entropy formula_7 is a measure of how uncertain we are about the outcome of formula_6. For example, if formula_6 is a probability distribution concentrated at one point, the outcome of formula_6 is certain and therefore its entropy formula_11. At the other extreme, if formula_6 is the uniform probability distribution with formula_13 possible values, intuitively one would expect formula_6 is associated with the most uncertainty. Indeed such uniform probability distributions have maximum possible entropy formula_15.
In quantum information theory, the notion of entropy is extended from probability distributions to quantum states, or density matrices. For a state formula_1, the von Neumann entropy is defined by
Applying the spectral theorem, or Borel functional calculus for infinite dimensional systems, we see that it generalizes the classical entropy. The physical meaning remains the same. A maximally mixed state, the quantum analog of the uniform probability distribution, has maximum von Neumann entropy. On the other hand, a pure state, or a rank one projection, will have zero von Neumann entropy. We write the von Neumann entropy formula_18 (or sometimes formula_19.
Definition.
Given a quantum system with two subsystems "A" and "B", the term joint quantum entropy simply refers to the von Neumann entropy of the combined system. This is to distinguish from the entropy of the subsystems.
In symbols, if the combined system is in state formula_20,
the joint quantum entropy is then
Each subsystem has its own entropy. The state of the subsystems are given by the partial trace operation.
Properties.
The classical joint entropy is always at least equal to the entropy of each individual system. This is not the case for the joint quantum entropy. If the quantum state formula_20 exhibits quantum entanglement, then the entropy of each subsystem may be larger than the joint entropy. This is equivalent to the fact that the conditional quantum entropy may be negative, while the classical conditional entropy may never be.
Consider a maximally entangled state such as a Bell state. If formula_20 is a Bell state, say,
then the total system is a pure state, with entropy 0, while each individual subsystem is a maximally mixed state, with maximum von Neumann entropy formula_25. Thus the joint entropy of the combined system is less than that of subsystems. This is because for entangled states, definite states cannot be assigned to subsystems, resulting in positive entropy.
Notice that the above phenomenon cannot occur if a state is a separable pure state. In that case, the reduced states of the subsystems are also pure. Therefore all entropies are zero.
Relations to other entropy measures.
The joint quantum entropy formula_26 can be used to define of the conditional quantum entropy:
and the quantum mutual information:
These definitions parallel the use of the classical joint entropy to define the conditional entropy and mutual information.