At the last step, and . Ignoring the recorded outcome, the final density matrix isFor large , the Taylor expansion givesThus , and the final state tends to , or as a pure-state representative. In fact , and its trace distance from is exactly . With records retained, the final conditional state is with probability tending to one. These are compatible descriptions, not a coherent sum of the two outcome branches. This quantum Zeno effect guides a known preparation through slowly rotating measurement bases; it is not a unitary Pauli X gate acting coherently on an arbitrary unknown input.
Total probability of the final target outcome versus the uninterrupted measurement record, and the asymptotic target-error probability in measurement-guided Zeno transfer
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