Sampling theory

In signal processing, sampling is the reduction of a continuous-time signal to a discrete-time signal. A common example is the conversion of a sound wave to a sequence of "samples". A sample is a value of the signal at a point in time and/or space; this definition differs from the term's usage in statistics, which refers to a set of such values. A sampler is a subsystem or operation that extracts samples from a continuous signal. A theoretical ideal sampler produces samples equivalent to the instantaneous value of the continuous signal at the desired points. The original signal can be reconstructed from a sequence of samples, up to the Nyquist limit, by passing the sequence of samples through a type of low-pass filter called a reconstruction filter. Nyquist–Shannon sampling theorem Functions of space, time, or any other dimension can be sampled, and similarly in two or more dimensions. For functions that vary with time, let S(t) be a continuous function (or "signal") to be sampled, and let sampling be performed by measuring the value of the continuous function every T seconds, which is called the sampling interval or sampling period. Then the sampled function is given by the sequence: S(nT), for integer values of n. The sampling frequency or sampling rate, fs, is the number of samples divided by the interval length over in which occur, thus fs = 1/T, with the unit sample per second, sometimes referred to as hertz, for example e.g. 48 kHz is 48,000 samples per second. Reconstructing a continuous function from samples is done by interpolation algorithms. The Whittaker–Shannon interpolation formula is mathematically equivalent to an ideal low-pass filter whose input is a sequence of Dirac delta functions that are modulated (multiplied) by the sample values. When the time interval between adjacent samples is a constant (T), the sequence of delta functions is called a Dirac comb. Mathematically, the modulated Dirac comb is equivalent to the product of the comb function with s(t).

A 1-GS/s 6-8-b Cryo-CMOS SAR ADC for Quantum Computing

Vibrational NDT with Under-sampled Data through Physics-informed Neural Networks

Architecture for integrated RF photonic downconversion of electronic signals

A 1-GS/s 6-8-b Cryo-CMOS SAR ADC for Quantum Computing

Architecture for integrated RF photonic downconversion of electronic signals

Vibrational NDT with Under-sampled Data through Physics-informed Neural Networks