Quantum and CircuitsReading edition

The typed mathematical target

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A.2 The typed mathematical target

The complex matrices act on vectors indexed by \(\operatorname{Fin}(12)\). The Fourier convention is

\[ F_{nk}=\frac{1}{\sqrt{12}}\exp\!\left(\frac{2\pi i nk}{12}\right), \qquad n,k\in\{0,\ldots,11\}. \]

The adjoint \(F^*\) therefore carries the negative exponential sign. The selector \(D\) is diagonal with value one precisely at the residues \(U=\{1,5,7,11\}\). The transported operator is \(P=FDF^*\).

Write

\[ c=(4,0,2,0,-2,0,-4,0,-2,0,2,0),\qquad \psi=\frac{c}{\sqrt{48}},\qquad \chi=\frac{|c|}{\sqrt{48}}. \]

Both vectors have norm one. Their initial probability histograms are identical, but their inner product is zero. The vector \(u\) has entry \(1/2\) on \(U\) and zero elsewhere. Lean proves the actual complex identities \(Fu=\psi\) and \(F^*\psi=u\), as well as transformed coprime probability one for \(\psi\) and zero for \(\chi\).

The statements are finite and exact. No parameterized arbitrary-modulus theorem, general circuit construction, physical phase-removal process, or quantum speedup is included in these formal claims.

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