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Elsevier eBooks

Many-Particle Lippmann–Schwinger Equations

Sadhan K. Adhikari, Kenneth L. Kowalski

Published Jan 1, 1991• 0 citations
Publisher
DOI
10.1016/b978-0-12-044273-7.50008-7

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Abstract The present work aims to obtain an exact solution for the Lippmann–Schwinger equation considering a scalar particle in three-dimensional hyperspherical and hyper-pseudospherical spaces. We analytically solve the Lippmann–Schwinger equation for a potential of the boundary-wall type, written as Dirac delta distributions over a two-dimensional single barrier. Our Lippmann–Schwinger equation in space representation is a second-kind Fredholm integral equation, where a bilinear form of the Green’s function leads to a separable kernel. The probability density for the particle, considering level surfaces in both spaces, and the differential cross-section in the hyper-pseudospherical space, are also presented graphically.

Physica Scripta•Jun 17, 2026•0 citations
Abstract The present work aims to obtain an exact solution for the Lippmann–Schwinger equation considering a scalar particle in three-dimensional hyperspherical and hyper-pseudospherical spaces. We analytically solve the Lippmann–Schwinger equation for a potential of the boundary-wall type, written as Dirac delta distributions over a two-dimensional single barrier. Our Lippmann–Schwinger equation in space representation is a second-kind Fredholm integral equation, where a bilinear form of the Green’s function leads to a separable kernel. The probability density for the particle, considering level surfaces in both spaces, and the differential cross-section in the hyper-pseudospherical space, are also presented graphically.