We review briefly the ``analog interpretation'' of sampling rate conversion
[1] on which the present method is based. Suppose we have
samples x(nT_{s}) of a continuous absolutely integrable signal x(t),
where t is time in seconds (real), n ranges over the integers, and
T_{s} is the sampling period. We assume x(t) is bandlimited to
, where F_{s}=1/T_{s} is the sampling rate. If
denotes the Fourier transform of x(t), i.e.,
, then we assume for
. Consequently, Shannon's sampling
theorem gives us that x(t) can be uniquely reconstructed from the
samples x(nT_{s}) via
where
(2) 
When the new sampling rate is less than the original rate F_{s}, the lowpass cutoff must be placed below half the new lower sampling rate. Thus, in the case of an ideal lowpass, , where the scale factor maintains unity gain in the passband.
A plot of the sinc function to the left and right of the origin t=0 is shown in Fig.1. Note that peak is at amplitude 1, and zerocrossings occur at all nonzero integers. The sinc function can be seen as a hyperbolically weighted sine function with its zero at the origin canceled out. The name sinc function derives from its classical name as the sine cardinal (or cardinal sine) function.
If ``'' denotes the convolution operation for digital signals, then the summation in Eq.(1) can be written as .
Equation Eq.(1) can be interpreted as a superpositon of shifted and scaled sinc functions h_{s}. A sinc function instance is translated to each signal sample and scaled by that sample, and the instances are all added together. Note that zerocrossings of occur at all integers except z=0. That means at time t=nT_{s}, (i.e., on a sample instant), the only contribution to the sum is the single sample x(nT_{s}). All other samples contribute sinc functions which have a zerocrossing at time t=nT_{s}. Thus, the interpolation goes precisely through the existing samples, as it should.
A plot indicating how sinc functions sum together to reconstruct bandlimited signals is shown in Fig.2. The figure shows a superposition of five sinc functions, each at unit amplitude, and displaced by onesample intervals. These sinc functions would be used to reconstruct the bandlimited interpolation of the discretetime signal . Note that at each sampling instant t=nT_{s}, the solid line passes exactly through the tip of the sinc function for that sample; this is just a restatement of the fact that the interpolation passes through the existing samples. Since the nonzero samples of the digital signal are all 1, we might expect the interpolated signal to be very close to 1 over the nonzero interval; however, this is far from being the case. The deviation from unity between samples can be thought of as ``overshoot'' or ``ringing'' of the lowpass filter which cuts off at half the sampling rate, or it can be considered a ``Gibbs phenomenon'' associated with bandlimiting.

A second interpretation of Eq.(1) is as follows: to obtain the interpolation at time t, shift the signal samples under one sinc function so that time t in the signal is translated under the peak of the sinc function, then create the output as a linear combination of signal samples where the coefficient of each signal sample is given by the value of the sinc function at the location of each sample. That this interpretation is equivalent to the first can be seen as a result of the fact that convolution is commutative; in the first interpretation, all signal samples are used to form a linear combination of shifted sinc functions, while in the second interpretation, samples from one sinc function are used to form a linear combination of samples of the shifted input signal. The practical bandlimited interpolation algorithm presented below is based on the second interpretation.