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Pauli-complementary qubit recovery fidelity inequality

PDF p. 9: Optimality argument after Eq. (S1.9)

Statement

Let H=C2 with standard ordered basis, and let R:L(H)→L(H) be a quantum channel, meaning a complex-linear, completely positive, trace-preserving map. Let U be a unitary matrix, let Z=diag⁡(1,−1), and write Ad⁡V(X)=VXV†. For entanglement fidelity Fe at the maximally mixed input I/2,

Fe(R∘Ad⁡U)+Fe(R∘Ad⁡ZU)≤1.

Here V† is the conjugate transpose, and composition applies the right-hand channel first.

Facts & Assumptions

Given: The qubit space, channel R, unitary U, and matrix Z in the Statement.

Goal: Prove that the displayed sum of entanglement fidelities is at most one.

[F1]

The finite operator conventions use the standard basis and conjugate-transpose adjoints. Finite operator and ket conventions

[F2]

A quantum channel is complex-linear, completely positive and trace-preserving; Fe is the maximally entangled-state overlap for the specified maximally mixed input. Finite-dimensional quantum channel Entanglement fidelity on a finite logical space

[F3]

For a qubit channel R, unitary U, and Z=diag⁡(1,−1), the sum Fe(R∘Ad⁡U)+Fe(R∘Ad⁡ZU) is at most one, with fidelities evaluated at I/2. Two orthogonal Pauli alternatives bound recovery fidelity

Proof

1.1givenF1F2F3

The given H, R, U, and Z satisfy the hypotheses of [F3]: the space is a qubit, R is a quantum channel, U is unitary, and Z has the required diagonal entries. The adjoint and fidelity conventions are those in [F1] and [F2].

2.1step 1.1F3∎

Applying [F3] to these data gives the displayed inequality, with both fidelities evaluated at I/2, as required.

Depends on

Used by · 1

Dependency tree · 2 levels

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Sources