A fractional generalization of the classical lattice dynamics approach
T.M. Michelitsch (IJLRA), B.A. Collet (IJLRA), A.P. Riascos (UNAM),, A.F. Nowakowski, F.C.G.A. Nicolleau

TL;DR
This paper introduces a fractional lattice model based on Hamilton's principle that generalizes classical difference operators to fractional powers, capturing nonlocal effects and describing anomalous transport phenomena in discrete and continuous systems.
Contribution
It develops a physically admissible fractional lattice model using Hamilton's variational principle, extending difference operators to fractional powers and connecting discrete models with continuous fractional Laplacians.
Findings
Explicit fractional Laplacian matrices for 1D chains derived
Model captures nonlocal long-range interactions in lattice systems
Continuum limit yields Riesz fractional derivative kernels
Abstract
We develop physically admissible lattice models in the harmonic approximation which define by Hamilton's variational principle fractional Laplacian matrices of the forms of power law matrix functions on the n -dimensional periodic and infinite lattice in n=1,2,3,..n=1,2,3,.. dimensions. The present model which is based on Hamilton's variational principle is confined to conservative non-dissipative isolated systems. The present approach yields the discrete analogue of the continuous space fractional Laplacian kernel. As continuous fractional calculus generalizes differential operators such as the Laplacian to non-integer powers of Laplacian operators, the fractional lattice approach developed in this paper generalized difference operators such as second difference operators to their fractional (non-integer) powers. Whereas differential operators and difference operators constitute local…
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