The extra Pauli gate on the control is removed by . Conjugating the target by a Hadamard gate then gives
Thus, from left to right in the network, apply , then , then and ; the last two gates commute.
Figure 1.
Synthesis of a CNOT gate from the ion gate , and preparation of a Bell pair
. Details.
For a direct proof, the control-zero block of is and its control-one block is . Multiplication by changes the latter into . Since and , the result is
which is exactly the CNOT gate on all inputs, including quantum superpositions.

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