The convolution of <math>f</math> and <math>g</math> is written <math>f * g</math>. It is defined as the integral of the product of the two functions while one is reversed and shifted.
The integration range depends on the domain on which the functions are defined. In case of a finite integration range, <math>f</math> and <math>g</math> are often considered as cyclically extended so that the term <math>g(\tau  t)</math> does not imply a range violation. Of course, extension with zeros is also possible.
If <math>X</math> and <math>Y</math> are two independent random variables with probability densities <math>f</math> and <math>g</math>, respectively, then the probability density of the sum <math>X + Y</math> is given by the convolution <math>f * g</math>.
For discrete functions, one can use a discrete version of the convolution. It is then given by
When multiplying two polynomials, the coefficients of the product are given by the convolution of the original coefficient sequences, in this sense (using extension with zeros as mentioned above).
Generalizing the above cases, the convolution can be defined for any two squareintegrable functions defined on a locally compact topological group. A different generalization is the convolution of distributions.
The various convolution operators all satisfy the following properties:
Symmetry:
Associativity:
Distributivity:
Associativity with scalar multiplication:
Derivation rule:
where Df denotes the derivative of f or, in the discrete case, the difference operator Df(n) = f(n+1)  f(n).
where F f denotes the Fourier transform of f. This theorem also holds for the Laplace transform.
Convolutions on Groups
If G is a suitable group endowed with a measure m (for instance, a locally compact Hausdorff topological group with the Haar measure) and if f and g are real or complex valued mintegrable functions of G, then we can define their convolution by
In this case, it is also possible to give, for instance, a Convolution Theorem, however it is much more difficult to phrase and requires representation theory for these types of groups and the peterweyl theorem[?] of Harmonic analysis. It is very difficult to do these calculations without more structure, and Lie groups turn out to be the setting in which these things are done.
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