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. Author manuscript; available in PMC: 2011 Nov 1.
Published in final edited form as: Prog Nucl Magn Reson Spectrosc. 2010 Jul 30;57(4):381–419. doi: 10.1016/j.pnmrs.2010.07.001

Figure 3. Point Responses, Convolution and Discrete Sampling.

Figure 3

The consequences of discretely sampling a continuous signal can be understood through the convolution theorem of the Fourier transform. In the time domain, the sampling process can be written mathematically as a multiplication of the continuous signal with functions describing the sampling—in this case, one function specifying evenly distributed samples, and a second function specifying the limited duration of the sampling interval. Each of these sampling functions has a Fourier transform, shown below, which is called its point response. According to the convolution theorem, the effects of sampling in the frequency domain are described by convolving (in the commonly-accepted convention of Bracewell, indicated by the operator “*”) the continuous spectrum with the point responses from the two sampling functions, yielding the discrete spectrum, with its aliasing and truncation artifacts.