Generalized fractional approach to solving partial differential equations with arbitrary dispersion relations

TL;DR

This paper introduces a generalized fractional calculus method to solve partial differential equations with arbitrary dispersion relations, enabling analytical solutions for complex physical systems across various states of matter.

Contribution

It presents a novel fractional calculus approach that incorporates dispersion relations to fully describe system dynamics, applicable to diverse physical systems and extendable to higher dimensions.

Findings

Successfully applied to 1D ferromagnetic chain and modified KdV equations

Provides a unified analytical framework for systems with bounded and unbounded dispersion

Applicable to fluids, soft matter, and solid-state systems

Abstract

Fractional calculus has been used to describe physical systems with complexity. Here, we show that a fractional calculus approach can restore or include complexity in any physical systems that can be described by partial differential equations. We argue that the dispersion relation contains the required information relating the energy and momentum space of the system and thus fully describes their dynamics. The approach is demonstrated by two examples: the Landau-Lifshitz equation in a 1D ferromagnetic chain, an example of a periodic crystal system with a bounded dispersion relation; and a modified KdV equation supporting surface gravity waves or Euler dispersion, an example of an unbounded system in momentum space. The presented approach is applicable to fluids, soft matter, and solid-state matter and can be readily generalized to higher dimensions and more complex systems. While numerical calculations are needed to determine the fractional operator, the approach is analytical and can be utilized to determine analytical solutions and investigate nonlinear problems.