Let be as in i. Insert the explicit oracle from ii between the two pairs of Hadamard gates. The network identities
turn the entire network into
This is the last simplified circuit in i. On the designated input , its reversed control is certainly one, so
The global phase is unobservable. Measuring the first wire therefore determines the function class with certainty after one oracle query, while the second wire returns to . These circuit identities are the network form of quantum phase kickback: the answer state between the Hadamards is the eigenstate , on which an XOR acts as a phase.

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