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Pauli-complementary qubit recovery fidelity inequality
PDF p. 9: Optimality argument after Eq. (S1.9)
Statement
Let with standard ordered basis, and let be a quantum channel, meaning a complex-linear, completely positive, trace-preserving map. Let be a unitary matrix, let , and write . For entanglement fidelity at the maximally mixed input ,
Here is the conjugate transpose, and composition applies the right-hand channel first.
Statement references
Facts & Assumptions
Given: The qubit space, channel , unitary , and matrix in the Statement.
Goal: Prove that the displayed sum of entanglement fidelities is at most one.
The finite operator conventions use the standard basis and conjugate-transpose adjoints. Finite operator and ket conventions
A quantum channel is complex-linear, completely positive and trace-preserving; is the maximally entangled-state overlap for the specified maximally mixed input. Finite-dimensional quantum channel Entanglement fidelity on a finite logical space
For a qubit channel , unitary , and , the sum is at most one, with fidelities evaluated at . Two orthogonal Pauli alternatives bound recovery fidelity
Proof
The given , , , and satisfy the hypotheses of [F3]: the space is a qubit, is a quantum channel, is unitary, and has the required diagonal entries. The adjoint and fidelity conventions are those in [F1] and [F2].
Applying [F3] to these data gives the displayed inequality, with both fidelities evaluated at , as required.
Depends on
Used by · 1
Dependency tree · 2 levels
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Sources
- Monolithic Quantum Error Correction in the Presence of Distinguishability · PDF p. 9, Comparison of Recoveries and Fidelity Measures, paragraph after Eq. (S1.9)