In optics, jitter is used to refer to motion that has high temporal frequency relative to the integration/exposure time. This may result from vibration in an assembly or the unstable hand of a photographer. Jitter is typically differentiated from smear, which has a lower frequency relative to the integration time. Whereas smear refers to a relatively constant rate during the integration/exposure time, jitter refers to a relatively sinusoidal motion during the integration/exposure time.

The equation for the optical Modulation transfer function associated with jitter is

M T F j i t t e r ( k ) = e − 1 2 k 2 σ 2 {\displaystyle MTF_{jitter}(k)=e^{-{\frac {1}{2}}k^{2}\sigma ^{2}}}

where k is the spatial frequency and σ {\displaystyle \sigma } is the amplitude of the jitter. Note that this frequency is in radians of phase per cycle. The equivalent expression in Hz is

M T F j i t t e r ( u ) = e − 2 π 2 u 2 σ 2 {\displaystyle MTF_{jitter}(u)=e^{-2\pi ^{2}u^{2}\sigma ^{2}}}

where u is the spatial frequency and σ {\displaystyle \sigma } is again the amplitude of the jitter (note that as the jitter approaches infinity, the value of the function tends towards zero).

For spacecraft, operation in a vacuum often means low mechanical damping. Meanwhile, spacecraft are compact and rigid, to withstand high launch loads. Jitter, then, is transmitted easily and often a limiting factor for high-resolution optics.