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Oakfield Operator Calculus Function Reference Site

Fractional Integrals

For α>0\alpha > 0 and locally integrable ff on [0,T][0,T], the Riemann–Liouville fractional integral is

Itαf(t)=1Γ(α)0t(tτ)α1f(τ)dτI_t^{\alpha} f(t) = \frac{1}{\Gamma(\alpha)} \int_{0}^{t} (t-\tau)^{\alpha-1} f(\tau)\,d\tau

Defined for fLloc1([0,T])f \in L^1_{\text{loc}}([0,T]); output is continuous on (0,T](0,T] and inherits weak singularity near t=0t=0 depending on α\alpha.


ItαItβf=Itα+βfI_t^{\alpha} I_t^{\beta} f = I_t^{\alpha+\beta} f

For suitable ff,

L{Itαf}(s)=sαL{f}(s)\mathcal{L}\{I_t^{\alpha} f\}(s) = s^{-\alpha}\,\mathcal{L}\{f\}(s)

  • As α0+\alpha\to 0^+, ItαffI_t^{\alpha} f \to f (in an appropriate sense).
  • For integer nn, ItnI_t^{n} reduces to nn-fold integration.
  • The kernel (tτ)α1(t-\tau)^{\alpha-1} decays algebraically in time difference, producing long memory effects.

Fractional derivatives invert fractional integrals (up to boundary conditions). Temporal memory kernels generalize the weighting beyond pure power laws.


Oakfield’s current fractional-time support is implemented via discrete approximations:

  • fractional_memory operator applies a finite-history fractional derivative/integral-style accumulator using Grünwald–Letnikov-like coefficients and a rolling history buffer.
  • subordination integrator implements a quadrature-based subordination scheme (time-change) that produces fractional-time behavior without an explicit convolution kernel.

Fractional integration and differentiation extend integer-order calculus to non-integer orders. Riemann–Liouville definitions provide one of the classical analytic formulations used in PDEs and memory models.

Fractional integrals serve as canonical power-law memory operators, connecting convolution kernels, Laplace multipliers, and anomalous transport models.


  • Podlubny, Fractional Differential Equations
  • Kilbas, Srivastava, Trujillo, Theory and Applications of Fractional Differential Equations