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Lettere al nuovo cimento della societa italiana di fisica/Lettere al nuovo cimento

On the three-body problem in quantum mechanics. — III. Case of potentials with hard cores

V. S. Olkhovsky

Published May 1, 1971• 0 citations
Publisher
DOI
10.1007/bf02770122

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The treatment of hard-core potentials in quantum mechanics is described. Known techniques and results are collected and discussed here so that they may be readily available. Two-body bound-state and scattering problems are considered in some detail. The use of hard-core potentials in analyses of more complicated systems is indicated.

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We present a mathematically rigorous method suitable for solving three-body bound-state and scattering problems when the inter-particle interaction is of a hard-core nature. The proposed method is a variant of the boundary condition model and it has been employed to calculate the binding energies for a system consisting of three atoms. Two realistic He-He interactions of Aziz and collaborators have been used for this purpose. The results obtained compare favourably with those previously obtained by other methods. We further used the model to calculate, for the first time, the ultralow-energy scattering phase shifts. This study revealed that our method is ideally suited for three-body molecular calculations where the practically hard-core of the inter-atomic potential gives rise to strong numerical inaccuracies that make calculations for these molecules cumbersome.

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Equivalence of the δ′ and the Hard Core Potentials

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The introduction of the hard core potential into the two-body problem forces the system wave function to vanish, if the interacting particles approach each other more closely than the hard core radius. In this paper it is shown that this “hard core effect” can also be obtained in the two-body problem by replacing the hard core potential with a δ′ interaction of suitable strength.

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REMARKS ON THE THREE BODY PROBLEM IN QUANTUM MECHANICS.

Endre Makai

•Jan 1, 1971•0 citations
We present a mathematically rigorous method suitable for solving three-body bound-state and scattering problems when the inter-particle interaction is of a hard-core nature. The proposed method is a variant of the boundary condition model and it has been employed to calculate the binding energies for a system consisting of three atoms. Two realistic He-He interactions of Aziz and collaborators have been used for this purpose. The results obtained compare favourably with those previously obtained by other methods. We further used the model to calculate, for the first time, the ultralow-energy scattering phase shifts. This study revealed that our method is ideally suited for three-body molecular calculations where the practically hard-core of the inter-atomic potential gives rise to strong numerical inaccuracies that make calculations for these molecules cumbersome.