Misplaced Pages

Volterra lattice

Article snapshot taken from Wikipedia with creative commons attribution-sharealike license. Give it a read and then ask your questions in the chat. We can research this topic together.

In mathematics, the Volterra lattice, also known as the discrete KdV equation, the Kac–van Moerbeke lattice, and the Langmuir lattice, is a system of ordinary differential equations with variables indexed by some of the points of a 1-dimensional lattice. It was introduced by Marc Kac and Pierre van Moerbeke (1975) and Jürgen Moser (1975) and is named after Vito Volterra. The Volterra lattice is a special case of the generalized Lotka–Volterra equation describing predator–prey interactions, for a sequence of species with each species preying on the next in the sequence. The Volterra lattice also behaves like a discrete version of the KdV equation. The Volterra lattice is an integrable system, and is related to the Toda lattice. It is also used as a model for Langmuir waves in plasmas.

Definition

The Volterra lattice is the set of ordinary differential equations for functions an:

a n = a n ( a n + 1 a n 1 ) {\displaystyle a_{n}'=a_{n}(a_{n+1}-a_{n-1})}

where n is an integer. Usually one adds boundary conditions: for example, the functions an could be periodic: an = an+N for some N, or could vanish for n ≤ 0 and n ≥ N.

The Volterra lattice was originally stated in terms of the variables Rn = -log an in which case the equations are

R n = e R n 1 e R n + 1 {\displaystyle R_{n}'=e^{R_{n-1}}-e^{R_{n+1}}}

References


Stub icon

This article about theoretical physics is a stub. You can help Misplaced Pages by expanding it.

Categories:
Volterra lattice Add topic