The powers are
Thus the least positive period is .
The possible values are . Each occurs for four of the twelve equally weighted values of , so
The equality holds exactly for . Projecting onto the measured second-register value and normalizing gives
With , the quantum Fourier transform acts by
(The opposite phase convention gives the same measurement probabilities.)
Applying the transform to the coset state gives amplitude
for . The geometric sum vanishes unless , which means . For its magnitude is . Thus the quantum Fourier transform of a periodic coset state gives

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