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Theoretical and Mathematical Physics

New variants of many-particle Faddeev equations

B.E. Grinyuk

Published Jun 1, 1980• 0 citations
Publisher
DOI
10.1007/bf01029129

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We use the assumption that the potential for the AAA-boson system can be written as a sum of pairwise acting forces to decompose the wave function into Faddeev components that fulfill a Faddeev type equation. Expanding these components in terms of potential harmonic (PH) polynomials and projecting on the potential basis for a specific pair of particles results in a two-variable integro-differential equations suitable for AAA-boson bound-state studies. The solution of the equation requires the evaluation of Jacobi polynomials ${P}_{K}^{\ensuremath{\alpha},\ensuremath{\beta}}(x)$ and of the weight function W(z)W(z)W(z) which give severe numerical problems for very large AAA. However, using appropriate limits for $A\ensuremath{\rightarrow}\ensuremath{\infty}$ we obtain a variant equation which depends only on the input two-body interaction, and the kernel in the integral part has a simple analytic form. This equation can be readily applied to a variety of bosonic systems such as microclusters of noble gasses. We employ it to obtain results for $A\ensuremath{\in}(10\ensuremath{-}100)$ 87Rb^{87}\mathrm{Rb}87Rb atoms interacting via interatomic interactions and confined by an externally applied trapping potential Vtrap(r){V}_{\mathrm{trap}}(r)Vtrap​(r). Our results are in excellent agreement with those previously obtained using the potential harmonic expansion method (PHEM) and the diffusion Monte Carlo (DMC) method.