Quantum nonlinear Schrödinger equation: two solutions
E Gutkin - Physics reports, 1988 - Elsevier
Physics reports, 1988•Elsevier
The quantum nonlinear Schrödinger equation (QNLS) has attracted much attention recently
as a simplest exactly soluble nonlinear model of the quantum field theory in 1+ 1 space-time.
There are two approaches in the literature to solution of QNLS. One is a quantization
prescription for the solution of classical nonlinear Schrödinger equation by the inverse
scattering method. It is called the quantum inverse method (QIM). The other is an elaboration
of the Bethe Ansatz technique. It is called the method of intertwining operators (MIO). The …
as a simplest exactly soluble nonlinear model of the quantum field theory in 1+ 1 space-time.
There are two approaches in the literature to solution of QNLS. One is a quantization
prescription for the solution of classical nonlinear Schrödinger equation by the inverse
scattering method. It is called the quantum inverse method (QIM). The other is an elaboration
of the Bethe Ansatz technique. It is called the method of intertwining operators (MIO). The …
Abstract
The quantum nonlinear Schrödinger equation (QNLS) has attracted much attention recently as a simplest exactly soluble nonlinear model of the quantum field theory in 1 + 1 space-time. There are two approaches in the literature to solution of QNLS. One is a quantization prescription for the solution of classical nonlinear Schrödinger equation by the inverse scattering method. It is called the quantum inverse method (QIM). The other is an elaboration of the Bethe Ansatz technique. It is called the method of intertwining operators (MIO). The two approaches produce formally different expansions for the QNLS field and for certain Fock space operators associated with it. In this work we give a comparative exposition of both methods. We then show that the QIM expansions and the MIO expansions define the same operators on Fock space.
Elsevier
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