2014Journal of Physics A Mathematical and TheoreticalOpen access

Integrable dispersive chains and energy dependent Schrödinger operator

M. V. Pavlov

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Abstract

In this paper we consider integrable dispersive chains associated with the so-called ‘energy dependent’ Schrödinger operator. In a general case multi-component reductions of these dispersive chains are new integrable systems, which are characterized by two arbitrary natural numbers. Also we show that integrable three-dimensional linearly degenerate quasilinear equations of a second order possess infinitely many differential constraints. Corresponding dispersive reductions are integrable systems associated with the ‘energy dependent’ Schrödinger operator.

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In this paper we consider integrable dispersive chains associated with the so-called ‘energy dependent’ Schrödinger operator. In a general case multi-component reductions of these dispersive chains are new integrable systems, which are characterized by two arbitrary natural numbers. Also we show that integrable three-dimensional linearly degenerate quasilinear equations of a second order possess infinitely many differential constraints. Corresponding dispersive reductions are integrable systems associated with the ‘energy dependent’ Schrödinger operator.

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Available abstract

In this paper we consider integrable dispersive chains associated with the so-called ‘energy dependent’ Schrödinger operator. In a general case multi-component reductions of these dispersive chains are new integrable systems, which are characterized by two arbitrary natural numbers. Also we show that integrable three-dimensional linearly degenerate quasilinear equations of a second order possess infinitely many differential constraints. Corresponding dispersive reductions are integrable systems associated with the ‘energy dependent’ Schrödinger operator.

Key concepts: Integrable system, Degenerate energy levels, Operator (biology), Schrödinger's cat, Mathematical physics, Differential operator, Mathematics, Energy (signal processing)

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