Use the unitary position-to-momentum Fourier transform . Integration gives
where with its continuous value one at zero. The amplitude is real and even, with central maximum , zeros at for nonzero integer , and alternating-sign sidelobes decaying as .
Figure 1.
A finite rectangular position amplitude gives a sinc momentum amplitude and a sinc-squared momentum density
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The probability density is , not the signed Sinc function amplitude. Its integral is one by the unitarity of the Fourier transform.

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