The Whittaker–Shannon interpolation formula dates back to works of E. Borel in 1898, and E. T. Whittaker in 1915, and was cited from works of J. M. Whittaker in 1935 in the formulation of the Nyquist–Shannon sampling theorem by C. E. Shannon in 1949. It is most commonly called Shannon's interpolation formula, and is sometimes called Whittaker's interpolation formula. E. T. Whittaker, who published it in 1915, called it the Cardinal series. It is even more commonly called simply the interpolation formula.
The interpolation formula states that, under certain limiting conditions, a function can be recovered exactly from its samples, , by the formula:
where is the sampling interval, is the sampling rate, and is the normalized sinc function.
There are two limiting conditions that the function must satisfy:
The interpolation formula reconstructs the original signal, , as long as these two conditions are met. Otherwise, aliasing occurs; that is, frequencies at or above are erroneously reconstructed at or below . See Aliasing for further discussion on this point.
The interpolation formula is derived in the Nyquist-Shannon sampling theorem article, which points out that it can be also be expressed as the convolution of an infinite impulse train with a sinc function:
This is equivalent to filtering the impulse train with an ideal (brick-wall) low-pass filter.
By the Hölder inequality this is satisfied if the sequence belongs to any of the spaces with
If
Since a random process does not have a Fourier transform, the condition under which the sum converges to the original function must also be different. A stationary random process does have an autocorrelation function and hence a spectral density according to the Wiener–Khinchin theorem. A suitable condition for convergence to a sample function from the process is that the spectral density of the process be zero at all frequencies equal to and above half the sample rate.
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