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Quantum Fidelity
Fidelity is a popular measure of distance between density operators. It is not a metric, but has some useful properties and it can be used to defined a metric on this space of density matrices, known as Bures metric.
Fidelity as a distance measure between pure states used to be called "transition probability". For two states given by unit vectors φ,ψ it is
.
For a pure state (vector ψ) and a mixed state (density matrix ρ) this generalizes to
, and for two density matrices ρ,σ it is generalized as the largest fidelity between any two purifications of the given states. According to a theorem by Uhlmann, this leads to the expression
This is precisely the expression used by Richard Jozsa in<bibref>Jozsa94</bibref>, where the term fidelity appears to have been used first.
However, one can also start from
, leading to the alternative
used in<bibref>NielsenChuang</bibref>. This second quantity is sometimes denoted as
and called square root fidelity. It has no interpretation as a probability, but appears in some estimates in a simpler way.
Basic properties
If
is pure, then
and if both states are pure i.e.
and
, then
.
Other properties:
Bures distance
Fidelity can be used to define metric on the set of quantum states, so called Bures distance<bibref>fuchs96phd</bibref> DB
and the angle<bibref>NielsenChuang</bibref>
The quantity DB(ρ,σ) is the minimal distance between purifications of ρ and σ using a common environment.
Classical fidelity
Fidelity is also defined for classical probability distributions. Let {pi} and {qi} where i = 1,2,...,n be probability distributions. The fidelity between p and q is defined as

References
<bibreferences/>