Novikov–Veselov equation


In mathematics, the Novikov–Veselov equation is a natural -dimensional analogue of the Korteweg–de Vries equation. Unlike another -dimensional analogue of KdV, the Kadomtsev–Petviashvili equation, it is integrable via the inverse scattering transform for the 2-dimensional stationary Schrödinger equation. Similarly, the Korteweg–de Vries equation is integrable via the inverse scattering transform for the 1-dimensional Schrödinger equation. The equation is named after S.P. Novikov and A.P. Veselov who published it in.

Definition

The Novikov–Veselov equation is most commonly written as
where and the following standard notation of complex analysis is used: is the real part,
The function is generally considered to be real-valued. The function is an auxiliary function defined via up to a holomorphic summand, is a real parameter corresponding to the energy level of the related 2-dimensional Schrödinger equation

Relation to other nonlinear integrable equations

When the functions and in the Novikov–Veselov equation depend only on one spatial variable, e.g.,, then the equation is reduced to the classical Korteweg–de Vries equation. If in the Novikov–Veselov equation, then the equation reduces to another -dimensional analogue of the KdV equation, the Kadomtsev–Petviashvili equation .

History

The inverse scattering transform method for solving nonlinear partial differential equations begins with the discovery of C.S. Gardner, J.M. Greene, M.D. Kruskal, R.M. Miura, who demonstrated that the Korteweg–de Vries equation can be integrated via the inverse scattering problem for the 1-dimensional stationary Schrödinger equation. The algebraic nature of this discovery was revealed by Lax who showed that the Korteweg–de Vries equation can be written in the following operator form :
where, and is a commutator. Equation is a compatibility condition for the equations
for all values of.
Afterwards, a representation of the form was found for many other physically interesting nonlinear equations, like the Kadomtsev–Petviashvili equation, sine-Gordon equation, nonlinear Schrödinger equation and others. This led to an extensive development of the theory of inverse scattering transform for integrating nonlinear partial differential equations.
When trying to generalize representation to two dimensions, one obtains that it holds only for trivial cases. However, S.V. Manakov showed that in the two-dimensional case it is more correct to consider the following representation :
or, equivalently, to search for the condition of compatibility of the equations
at one fixed value of parameter .
Representation for the 2-dimensional Schrödinger operator was found by S.P. Novikov and A.P. Veselov in. The authors also constructed a hierarchy of evolution equations integrable via the inverse scattering transform for the 2-dimensional Schrödinger equation at fixed energy. This set of evolution equations contains, in particular, the equation.

Physical applications

The dispersionless version of the Novikov–Veselov equation was derived in a model of nonlinear geometrical optics.

Behavior of solutions

The behavior of solutions to the Novikov–Veselov equation depends essentially on the regularity of the scattering data for this solution. If the scattering data are regular, then the solution vanishes uniformly with time. If the scattering data have singularities, then the solution may develop solitons. For example, the scattering data of the Grinevich–Zakharov soliton solutions of the Novikov–Veselov equation have singular points.
Solitons are traditionally a key object of study in the theory of nonlinear integrable equations. The solitons of the Novikov–Veselov equation at positive energy are transparent potentials, similarly to the one-dimensional case. However, unlike the one-dimensional case where there exist well-known exponentially decaying solitons, the Novikov–Veselov equation does not possess exponentially localized solitons.