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The Cauchy formula for repeated integration, named after Augustin-Louis Cauchy, allows one to compress n antiderivatives of a function into a single integral (cf. Cauchy's formula). For non-integer n it yields the definition of fractional integrals and (with n < 0) fractional derivatives.
Let f be a continuous function on the real line. Then the nth repeated integral of f with base-point a, is given by single integration
A proof is given by induction. The base case with n = 1 is trivial, since it is equivalent to
Now, suppose this is true for n, and let us prove it for n + 1. Firstly, using the Leibniz integral rule, note that Then, applying the induction hypothesis, Note that the term within square bracket has n-times successive integration, and upper limit of outermost integral inside the square bracket is . Thus, comparing with the case for n = n and replacing of the formula at induction step n = n with respectively leads to Putting this expression inside the square bracket results in
This completes the proof.
The Cauchy formula is generalized to non-integer parameters by the Riemann–Liouville integral, where is replaced by , and the factorial is replaced by the gamma function. The two formulas agree when .
Both the Cauchy formula and the Riemann–Liouville integral are generalized to arbitrary dimensions by the Riesz potential.
In fractional calculus, these formulae can be used to construct a differintegral, allowing one to differentiate or integrate a fractional number of times. Differentiating a fractional number of times can be accomplished by fractional integration, then differentiating the result.