Riemann-Liouville Fractional Derivative
📐 Definition
Section titled “📐 Definition”Let and let . The Riemann–Liouville fractional derivative of order of a function is defined by
where denotes the Gamma function. This definition generalizes integer-order differentiation by composing an ordinary derivative with a fractional integral.
Domain and Codomain
Section titled “Domain and Codomain”The Riemann–Liouville derivative is defined for functions that are locally integrable on and sufficiently regular for the integral and derivative to exist. The operator maps such functions to real- or complex-valued functions on .
⚙️ Key Properties
Section titled “⚙️ Key Properties”Linearity
Section titled “Linearity”The Riemann–Liouville derivative is linear:
for scalars .
Reduction to Integer-Order Derivatives
Section titled “Reduction to Integer-Order Derivatives”If , then
recovering the classical derivative.
Power Functions
Section titled “Power Functions”For ,
This identity highlights the central role of the Gamma function in fractional calculus.
Nonlocality
Section titled “Nonlocality”The value of depends on the values of for all . This nonlocality encodes memory effects absent in integer-order differentiation.
Semigroup Property (Restricted)
Section titled “Semigroup Property (Restricted)”For suitable functions and parameters,
holds under additional regularity assumptions. In general, the semigroup property does not hold without constraints.
🎯 Special Cases
Section titled “🎯 Special Cases”Fractional Integral
Section titled “Fractional Integral”For , the corresponding Riemann–Liouville fractional integral is
The fractional derivative is obtained by differentiating this integral.
Constant Functions
Section titled “Constant Functions”For a constant function ,
Unlike the Caputo derivative, the Riemann–Liouville derivative of a constant is generally nonzero.
🔗 Related Functions
Section titled “🔗 Related Functions”The Riemann–Liouville derivative is closely related to:
- the Riemann–Liouville fractional integral,
- the Caputo fractional derivative,
- convolution operators with power-law kernels.
These operators form the core of classical fractional calculus.
Usage in Oakfield
Section titled “Usage in Oakfield”Oakfield implements fractional-time behavior in two concrete places:
- Fractional memory operator:
fractional_memorymaintains a rolling history buffer and applies a finite-memory fractional-derivative approximation (Grünwald–Letnikov–style coefficients) with scaling like ; it operates component-wise even for complex fields (by treating storage as a flatdoublebuffer). - Subordination integrator: the
subordinationintegrator approximates fractional-time evolution by quadrature over a stretched-exponential kernel and repeatedly evaluating the context drift in a side-effect-free “drift mode”.
These implementations are practical, discrete approximations; they capture “long memory” effects without requiring an exact closed-form Riemann–Liouville integral kernel.
Historical Foundations
Section titled “Historical Foundations”📜 Origin (19th Century)
Section titled “📜 Origin (19th Century)”Bernhard Riemann introduced fractional integration while studying trigonometric series. Joseph Liouville later formalized fractional differentiation and extended the theory systematically.
🔬 Modern Development
Section titled “🔬 Modern Development”Riemann–Liouville operators became foundational tools in fractional calculus, influencing probability theory, viscoelasticity, and anomalous transport models.
🌍 Modern Perspective
Section titled “🌍 Modern Perspective”Today, the Riemann–Liouville derivative is viewed as a canonical fractional operator, particularly suited for analytic investigations and integral-equation formulations.
📚 References
Section titled “📚 References”- Riemann, Versuch einer allgemeinen Auffassung der Integration und Differentiation
- Liouville, Mémoire sur le calcul des différentielles à indices quelconques
- NIST Digital Library of Mathematical Functions (DLMF), §1.14