Math 2.0

Real functions Definition

Fractional calculus

Builds on Riemann–Liouville integralGamma functionHigher derivative

Definition

Let a∈ℝa \in \R and let ff be a locally integrable real function on [a,∞)[a, \infty). For a real number α>0\alpha > 0, the fractional integral of order α\alpha of ff is the Riemann–Liouville integral Iaαf(x)=1Γ(α)∫ax(x−t)α−1f(t) dt,x>a,I_a^\alpha f(x) = \frac{1}{\Gamma(\alpha)} \int_a^x (x - t)^{\alpha - 1} f(t) \, dt, \qquad x > a, where Γ\Gamma is the gamma function. For α>0\alpha > 0 let n=⌈α⌉n = \ceil{\alpha}. The Riemann–Liouville fractional derivative of order α\alpha is Daαf(x)=dndxn Ian−αf(x),D_a^\alpha f(x) = \frac{d^n}{dx^n} \, I_a^{n - \alpha} f(x), whenever the right side exists, with Ia0f=fI_a^0 f = f. Fractional calculus is the study of these operators and of their variants, for real or complex orders α\alpha.

Remarks

For a positive integer α=n\alpha = n, IanfI_a^n f is the nn-fold iterated integral of ff from aa, and DanfD_a^n f is the ordinary higher derivative f(n)f^{(n)}. Example: with a=0a = 0 and f(t)=1f(t) = 1, I01/2f(x)=1Γ(1/2)∫0x(x−t)−1/2 dt=2xπI_0^{1/2} f(x) = \frac{1}{\Gamma(1/2)} \int_0^x (x - t)^{-1/2} \, dt = \frac{2\sqrt{x}}{\sqrt{\pi}}. Non-example: for α=0\alpha = 0 the integral formula is not defined, since Γ(0)\Gamma(0) is not defined; the operator Ia0I_a^0 is set to be the identity by convention. The fractional integrals satisfy IaαIaβ=Iaα+βI_a^\alpha I_a^\beta = I_a^{\alpha + \beta} for α,β>0\alpha, \beta > 0. Other fractional derivatives, such as the Caputo derivative and the Grünwald–Letnikov derivative, agree with DaαD_a^\alpha on suitable classes of functions.

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Further reading

  1. Web https://en.wikipedia.org/wiki/Fractional_calculus
About this page
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WritingW0 stub
MSC26A33
DefinesFractional calculus
UsesRiemann–Liouville integral, Gamma function, Higher derivative
Changed2 November 2026

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