Fractional Liouville Equation on Lattice Phase-Space
Vasily E. Tarasov

TL;DR
This paper introduces a lattice-based fractional Liouville equation that models nonlocal media, transforming into a continuum form with Riesz fractional derivatives, applicable to plasma-like systems.
Contribution
It proposes a novel lattice fractional Liouville equation and demonstrates its continuum limit involving Riesz fractional derivatives, extending phase-space dynamics modeling.
Findings
Lattice fractional Liouville equation derived for systems with long-range jumps.
Continuum limit yields Liouville equation with Riesz fractional derivatives.
Application to plasma-like nonlocal media demonstrates model relevance.
Abstract
In this paper we propose a lattice analog of phase-space fractional Liouville equation. The Liouville equation for phase-space lattice with long-range jumps of power-law types is suggested. We prove that the continuum limit transforms this lattice equation into Liouville equation with conjugate Riesz fractional derivatives of non-integer orders with respect to coordinates of continuum phase-space. An application of the fractional Liouville equation with these Riesz fractional derivatives to describe properties of plasma-like nonlocal media is considered.
Peer Reviews
No public reviews on file for this paper yet. If you reviewed it on a platform where reviews are public (OpenReview, ICLR, NeurIPS, ICML), you can paste yours below so the community can read it here.
Videos
No videos yet. Explain this paper in a talk, walkthrough, or lecture? Add one.
