Squaring the diagonal gate gives
Thus the T gate is available up to a global phase. Reading the supplied W columns in order , it sends to , to , and fixes the other two vectors: it is CNOT with the second wire controlling the first. Conjugating both wires by the Hadamard gate reverses that orientation:
For instance, write . Conjugation uses and , , yielding . Expanding the first-wire Z eigenspaces gives , as required.
We have H directly and finite constructions of CNOT and T up to physically irrelevant global phase. By universality transfer by exact gate synthesis, the assumed universality of proves that is universal under the phase-insensitive convention. There is no assertion of arbitrary strict operator-norm phases: on a fixed register these generators have only a finite set of possible determinants, which would obstruct density in the entire unitary group if global phase were treated as an observable target.
Let . Since the Hadamard gate maps the standard basis to , the given gate is . Because ,
Next, use on the target wire of the Controlled-Z gate:
The control-zero block remains the identity, and the control-one block becomes , proving the identity with the stated control convention. We have therefore constructed each gate in the assumed universal quantum gate set using only .
Replacing every gate of a circuit by its displayed finite construction reproduces that circuit exactly. Thus is universal under the usual arbitrary-accuracy convention: it can perform every approximation obtainable from the given universal set. The claim concerns approximation of arbitrary unitary operators; it does not assert that finitely many circuits exactly represent an uncountable continuum of gates. This is universality transfer by exact gate synthesis.