Cauchy formula for repeated integration explained

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).

Scalar case

Let f be a continuous function on the real line. Then the nth repeated integral of f with base-point a,f^(x) = \int_a^x \int_a^ \cdots \int_a^ f(\sigma_) \, \mathrm\sigma_ \cdots \, \mathrm\sigma_2 \, \mathrm\sigma_1,is given by single integrationf^(x) = \frac \int_a^x\left(x-t\right)^ f(t)\,\mathrmt.

Proof

A proof is given by induction. The base case with n = 1 is trivial, since it is equivalent to f^(x) = \frac1 \int_a^x f(t)\,\mathrmt = \int_a^x f(t)\,\mathrmt.

Now, suppose this is true for n, and let us prove it for n + 1. Firstly, using the Leibniz integral rule, note that \frac \left[\frac{1}{n!} \int_a^x (x - t)^n f(t)\,\mathrm{d}t \right] = \frac \int_a^x (x - t)^ f(t)\,\mathrmt.Then, applying the induction hypothesis,\begin f^(x) &= \int_a^x \int_a^ \cdots \int_a^ f(\sigma_) \,\mathrm\sigma_ \cdots \,\mathrm\sigma_2 \,\mathrm\sigma_1 \\ &= \int_a^x \left[\int_a^{\sigma_1} \cdots \int_a^{\sigma_n} f(\sigma_{n+1}) \,\mathrm{d}\sigma_{n+1} \cdots \,\mathrm{d}\sigma_2 \right] \,\mathrm\sigma_1.\endNote that the term within square bracket has n-times successive integration, and upper limit of outermost integral inside the square bracket is

\sigma1

. Thus, comparing with the case for n = n and replacing

x,\sigma1,,\sigman

of the formula at induction step n = n with

\sigma1,\sigma2,,\sigman+1

respectively leads to \int_a^ \cdots \int_a^ f(\sigma_) \,\mathrm\sigma_ \cdots \,\mathrm\sigma_2 = \frac \int_a^ (\sigma_1 - t)^ f(t)\,\mathrmt.Putting this expression inside the square bracket results in\begin &= \int_a^x \frac \int_a^ (\sigma_1 - t)^ f(t)\,\mathrmt\,\mathrm\sigma_1 \\ &= \int_a^x \frac \left[\frac{1}{n!} \int_a^{\sigma_1} (\sigma_1 - t)^n f(t)\,\mathrm{d}t\right] \,\mathrm\sigma_1 \\ &= \frac \int_a^x (x - t)^n f(t)\,\mathrmt.\end

n=1

.

n=k

, then it has been shown that the statement holds true for

n=k+1

.

This completes the proof.

Generalizations and applications

The Cauchy formula is generalized to non-integer parameters by the Riemann–Liouville integral, where

n\in\Z\geq

is replaced by

\alpha\in\Complex,\Re(\alpha)>0

, and the factorial is replaced by the gamma function. The two formulas agree when

\alpha\in\Z\geq

.

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.

References

External links