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QuantumInfo.Finite.Distance.Fidelity

8 declarations

definition

Fidelity F(ρ,σ)F(\rho, \sigma) of two quantum states

#fidelity

Given two quantum states ρ\rho and σ\sigma represented as density matrices in a dd-dimensional Hilbert space, their fidelity is defined as F(ρ,σ)=tr(ρσρ)F(\rho, \sigma) = \text{tr}\left( \sqrt{\sqrt{\rho} \sigma \sqrt{\rho}} \right) where \sqrt{\cdot} denotes the unique positive semi-definite square root of a matrix, and tr\text{tr} is the trace operator. This quantity represents the quantum version of the Bhattacharyya coefficient between two states.

theorem

Fidelity F(ρ,σ)F(\rho, \sigma) is Non-negative

#fidelity_ge_zero

For any two quantum states ρ\rho and σ\sigma in a dd-dimensional Hilbert space, their fidelity F(ρ,σ)F(\rho, \sigma) is non-negative, i.e., 0F(ρ,σ)0 \le F(\rho, \sigma).

theorem

Fidelity of Mixed States is at Most 1

#fidelity_le_one

For any mixed states ρ\rho and σ\sigma in a dd-dimensional Hilbert space, the fidelity F(ρ,σ)F(\rho, \sigma) satisfies the inequality F(ρ,σ)1F(\rho, \sigma) \le 1.

definition

Fidelity of mixed states ρ\rho and σ\sigma as a probability value F(ρ,σ)[0,1]F(\rho, \sigma) \in [0, 1]

#fidelity_prob

The fidelity between two mixed states ρ\rho and σ\sigma in a dd-dimensional Hilbert space, denoted as F(ρ,σ)F(\rho, \sigma), defined as a probability value in the interval [0,1][0, 1]. This is implemented by bundling the real-valued fidelity function `MState.fidelity` with the proofs that 0F(ρ,σ)0 \le F(\rho, \sigma) and F(ρ,σ)1F(\rho, \sigma) \le 1.

theorem

F(ρ,ρ)=1F(\rho, \rho) = 1

#fidelity_self_eq_one

For any quantum state ρ\rho represented as a density matrix in a dd-dimensional Hilbert space, the fidelity of the state with itself is equal to 1, i.e., F(ρ,ρ)=1F(\rho, \rho) = 1.

theorem

F(ρ,σ)=1    ρ=σF(\rho, \sigma) = 1 \iff \rho = \sigma

#fidelity_eq_one_iff_self

Let ρ\rho and σ\sigma be two quantum states represented as density matrices in a dd-dimensional Hilbert space. The fidelity between these states, defined as F(ρ,σ)=tr(ρσρ)F(\rho, \sigma) = \text{tr}\left( \sqrt{\sqrt{\rho} \sigma \sqrt{\rho}} \right), is equal to 11 if and only if the two states are identical, i.e., F(ρ,σ)=1    ρ=σF(\rho, \sigma) = 1 \iff \rho = \sigma.

theorem

Symmetry of fidelity F(ρ,σ)=F(σ,ρ)F(\rho, \sigma) = F(\sigma, \rho)

#fidelity_symm

For any two mixed states ρ\rho and σ\sigma in a Hilbert space of dimension dd, the fidelity between them is symmetric, such that F(ρ,σ)=F(σ,ρ)F(\rho, \sigma) = F(\sigma, \rho).

theorem

Monotonicity of Fidelity under CPTP Maps

#fidelity_channel_nondecreasing

For any two quantum states ρ\rho and σ\sigma represented as matrix states in Md\mathcal{M}_d, and for any completely positive trace-preserving (CPTP) map Λ:MdMd2\Lambda: \mathcal{M}_d \to \mathcal{M}_{d_2}, the fidelity FF satisfies the inequality F(Λ(ρ),Λ(σ))F(ρ,σ)F(\Lambda(\rho), \Lambda(\sigma)) \geq F(\rho, \sigma).