Conditional quantum entropy: Difference between revisions

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The '''conditional quantum entropy''' is an [[entropy measure]] used in [[quantum information theory]]. It is a generalization of the [[conditional entropy]] of [[classical information theory]]. For a bipartite state <math>\rho^{AB}</math>, the conditional entropy is written <math>S(A|B)_\rho</math>, or <math>H(A|B)_\rho</math>, depending on the notation being used for the [[von Neumann entropy]]. The quantum conditional entropy was defined in terms of a conditional density operator <math> \rho_{A|B} </math> by [[Nicolas Cerf]] and [[Chris Adami]] <ref name="negent">{{cite journal | url=http://prl.aps.org/abstract/PRL/v79/i26/p5194_1 | title = Negative entropy and information in quantum mechanics| publisher = [[Physical Review Letters]]| year = 1997}}</ref><ref>{{cite journal | url=http://pra.aps.org/abstract/PRA/v60/i2/p893_1 | title = Quantum extension of conditional probability| publisher = [[Physical Review]]| year = 1999}}</ref>, who showed that quantum conditional entropies can be negative, something that is forbidden in classical physics. The negativity of quantum conditional entropy is a sufficient criterion for quantum [[Separable state|non-separability]].

ForIn the remainder of thewhat articlefollows, we use the notation <math>S(\cdot)</math> for the [[von Neumann entropy]], which wewill simply callbe called "entropy".

== Definition ==

Given a bipartite quantum state <math>\rho^{AB}</math>, the entropy of the entirejoint system AB is <math>S(AB)_\rho \ \stackrel{\mathrm{def}}{=}\ S(\rho^{AB})</math>, and the entropies of the subsystems are <math>S(A)_\rho \ \stackrel{\mathrm{def}}{=}\ S(\rho^A) = S(\mathrm{tr}_B\rho^{AB})</math> and <math>S(B)_\rho</math>. The von Neumann entropy measures howan uncertainobserver's we areuncertainty about the value of the state;, that is, how much the state is a [[mixed state (physics)|mixed state]].

By analogy with the classical conditional entropy, one defines the conditional quantum entropy as <math>S(A|B)_\rho \ \stackrel{\mathrm{def}}{=}\ S(AB)_\rho - S(B)_\rho</math>.

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==Properties==

Unlike the classical [[conditional entropy]], the conditional quantum entropy can be negative. This is true even though the (quantum) von Neumann entropy of single variable is never negative. The negative conditional entropy is also known as the [[coherent information]], and gives the additional number of bits above the classical limit that can be transmitted in a quantum dense coding protocol. Positive conditional entropy of a state thus means the state cannot reach even the classical limit, while the negative conditional entropy provides for additional information.

==References==

{{reflist}}

Nielsen, Michael A. and [[Isaac L. Chuang]] (2000). ''Quantum Computation and Quantum Information''. Cambridge University Press, ISBN 0-521-63503-9.

* Mark M. Wilde, [http://arxiv.org/abs/1106.1445 "From Classical to Quantum Shannon Theory", arXiv:1106.1445].

*{{cite book

| first = Mark

| last = Wilde

|

| title = Quantum Information Theory

| url= http://www.amazon.com/Quantum-Information-Theory-Mark-Wilde/dp/1107034256

| publisher = Cambridge University Press

| year = 2013

}}

[[Category:Quantum mechanical entropy]]