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=== Translational equivariance === The convolution commutes with translations, meaning that : <math>\tau_x (f * g) = (\tau_x f) * g = f * (\tau_x g)</math> where Ο<sub>''x''</sub>f is the translation of the function ''f'' by ''x'' defined by : <math>(\tau_x f)(y) = f(y - x).</math> If ''f'' is a [[Schwartz function]], then ''Ο<sub>x</sub>f'' is the convolution with a translated Dirac delta function ''Ο''<sub>''x''</sub>''f'' = ''f'' β ''Ο''<sub>''x''</sub> ''Ξ΄''. So translation invariance of the convolution of Schwartz functions is a consequence of the associativity of convolution. Furthermore, under certain conditions, convolution is the most general translation invariant operation. Informally speaking, the following holds : Suppose that ''S'' is a bounded [[linear operator]] acting on functions which commutes with translations: ''S''(''Ο<sub>x</sub>f'') = ''Ο<sub>x</sub>''(''Sf'') for all ''x''. Then ''S'' is given as convolution with a function (or distribution) ''g''<sub>''S''</sub>; that is ''Sf'' = ''g''<sub>''S''</sub> β ''f''. Thus some translation invariant operations can be represented as convolution. Convolutions play an important role in the study of [[time-invariant system]]s, and especially [[LTI system theory]]. The representing function ''g''<sub>''S''</sub> is the [[impulse response]] of the transformation ''S''. A more precise version of the theorem quoted above requires specifying the class of functions on which the convolution is defined, and also requires assuming in addition that ''S'' must be a [[continuous linear operator]] with respect to the appropriate [[topology]]. It is known, for instance, that every continuous translation invariant continuous linear operator on ''L''<sup>1</sup> is the convolution with a finite [[Borel measure]]. More generally, every continuous translation invariant continuous linear operator on ''L''<sup>''p''</sup> for 1 β€ ''p'' < β is the convolution with a [[Distribution (mathematics)#Tempered distributions and Fourier transform|tempered distribution]] whose [[Fourier transform]] is bounded. To wit, they are all given by bounded [[Fourier multiplier]]s.
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