Assume Alice independently chooses X or Z with equal probabilities and that bit labels identify the corresponding positive and negative eigenstates. If Daisy measures Z, she reads a Z-encoded bit correctly with probability one and an X-encoded bit correctly with probability one half. Therefore
The probability to read the entire independently encoded -bit check number correctly by this strategy is .
Daisy's random choice of X or Z agrees with Alice's independent random basis with probability . Agreement gives the correct label with certainty and disagreement gives it with probability . Hence
the same result as a fixed Z measurement. Randomizing her basis does not supply the missing information about Alice's choice. These are the probabilities for the two specified strategies, rather than an assertion that they are optimal among all possible quantum measurements.

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