Conjugation by maps to . The phase-flip channel therefore acts on the Bloch vector as
In the computational basis,
At , the two opposite off-diagonal contributions cancel, giving
A computational-basis projective measurement has projections and . Discarding its result produces the nonselective projective measurement
Thus
Complete phase randomization and unread computational-basis measurement implement the same dephasing on this qubit.
The four index pairs give
The last global phase cancels under conjugation. Hence the Pauli channel probabilities are
Conjugation by one Pauli matrix preserves its parallel Bloch component and reverses the other two. Therefore

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