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- Deprecated function: TYPO3\PharStreamWrapper\Manager::initialize(): Implicitly marking parameter $resolver as nullable is deprecated, the explicit nullable type must be used instead in include_once() (line 19 of includes/file.phar.inc).
- Deprecated function: TYPO3\PharStreamWrapper\Manager::initialize(): Implicitly marking parameter $collection as nullable is deprecated, the explicit nullable type must be used instead in include_once() (line 19 of includes/file.phar.inc).
- Deprecated function: TYPO3\PharStreamWrapper\Manager::__construct(): Implicitly marking parameter $resolver as nullable is deprecated, the explicit nullable type must be used instead in include_once() (line 19 of includes/file.phar.inc).
- Deprecated function: TYPO3\PharStreamWrapper\Manager::__construct(): Implicitly marking parameter $collection as nullable is deprecated, the explicit nullable type must be used instead in include_once() (line 19 of includes/file.phar.inc).
Superfidelity is a measure of similarity between
density
operators. It is defined as
G(ρ,σ)=trρσ+√1−tr(ρ2)√1−tr(σ2),
where σ and ρ are density matrices.
Superfidelity was introduced inmiszczak09sub as an upper bound for
fidelity.
Properties
Super-fidelity has also properties which make it useful for
quantifying distance between quantum states. In particular we have:
- Bounds: 0 ≤ G(ρ1, ρ2) ≤ 1.
- Symmetry: G(ρ1, ρ2) = G(ρ2, ρ1).
- Unitary invariance: for any unitary operator U, we have G(ρ1, ρ2) = G(Uρ1U†, Uρ2U†).
- Concavity:
-
G(ρ1, αρ2 + (1 − α)ρ3) ≥ αG(ρ1, ρ2) + (1 − α)G(ρ1, ρ3)
for any ρ1, ρ2, ρ3 ∈ ΩN
and α ∈ [0, 1].
- Supermultiplicativity: for ρ1, ρ2, ρ3, ρ4 ∈ ΩN
we have
-
G(ρ1 ⊗ ρ2, ρ3 ⊗ ρ4) ≥ G(ρ1, ρ3)G(ρ2, ρ4).
See also
References
Category:Handbook
of Quantum Information
Category:Mathematical
Structure
Category:Linear
Algebra
Last modified:
Monday, October 26, 2015 - 17:56