In signal processing, the Nyquist rate is a value equal to twice the highest frequency (bandwidth) of a given function or signal. It is named after Harry Nyquist. It has units of samples per unit time, conventionally expressed as samples per second, or hertz (Hz). When the signal is sampled at a higher sample rate (see § Critical frequency), the resulting discrete-time sequence is said to be free of the distortion known as aliasing. Conversely, for a given sample rate the corresponding Nyquist frequency is one-half the sample rate. Note that the Nyquist rate is a property of a continuous-time signal, whereas Nyquist frequency is a property of a discrete-time system. The term Nyquist rate is also used in a different context with units of symbols per second, which is actually the field in which Harry Nyquist was working. In that context it is an upper bound for the symbol rate across a bandwidth-limited baseband channel such as a telegraph line or passband channel such as a limited radio frequency band or a frequency division multiplex channel.
Relative to sampling
When a continuous function, x ( t ) , {\displaystyle x(t),} is sampled at a constant rate, f s {\displaystyle f_{s}} samples/second, there is always an unlimited number of other continuous functions that fit the same set of samples. But only one of them is bandlimited to 1 2 f s {\displaystyle {\tfrac {1}{2}}f_{s}} cycles/second (hertz), which means that its Fourier transform, X ( f ) , {\displaystyle X(f),} is 0 {\displaystyle 0} for all | f | ≥ 1 2 f s . {\displaystyle |f|\geq {\tfrac {1}{2}}f_{s}.} The mathematical algorithms that are typically used to recreate a continuous function from samples create arbitrarily good approximations to this theoretical, but infinitely long, function. It follows that if the original function, x ( t ) , {\displaystyle x(t),} is bandlimited to 1 2 f s , {\displaystyle {\tfrac {1}{2}}f_{s},} which is called the Nyquist criterion, then it is the one unique function the interpolation algorithms are approximating. In terms of a function's own bandwidth ( B ) , {\displaystyle (B),} as depicted here, the Nyquist criterion is often stated as f s > 2 B . {\displaystyle f_{s}>2B.} And 2 B {\displaystyle 2B} is called the Nyquist rate for functions with bandwidth B . {\displaystyle B.} When the Nyquist criterion is not met ( {\displaystyle (} say, B > 1 2 f s ) , {\displaystyle B>{\tfrac {1}{2}}f_{s}),} a condition called aliasing occurs, which results in some inevitable differences between x ( t ) {\displaystyle x(t)} and a reconstructed function that has less bandwidth. In most cases, the differences are viewed as distortion.
Intentional aliasing
Figure 3 depicts a type of function called baseband or lowpass, because its positive-frequency range of significant energy is [0, B). When instead, the frequency range is (A, A+B), for some A > B, it is called bandpass, and a common desire (for various reasons) is to convert it to baseband. One way to do that is frequency-mixing (heterodyne) the bandpass function down to the frequency range (0, B). One of the possible reasons is to reduce the Nyquist rate for more efficient storage. And it turns out that one can directly achieve the same result by sampling the bandpass function at a sub-Nyquist sample-rate that is the smallest integer-sub-multiple of frequency A that meets the baseband Nyquist criterion: fs > 2B. For a more general discussion, see bandpass sampling.
Relative to signaling Long before Harry Nyquist had his name associated with sampling, the term Nyquist rate was used differently, with a meaning closer to what Nyquist actually studied. Quoting Harold S. Black's 1953 book Modulation Theory, in the section Nyquist Interval of the opening chapter Historical Background:
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