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Il Nuovo cimento della Società italiana di fisica. B/Il Nuovo cimento B

A new method for solving the many-body boson problem. I

K. W. Wong, P. C. W. Fung

Published Feb 1, 1975• 9 citations
Publisher
DOI
10.1007/bf02724741

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A general method of a quasi-linear canonical transformation is introduced as an approach to the many-body problems. In this method the n-body problem can be solved if the (n-1)-body problem is assumed to be solved. In the application of this method to the system of N bosons, there appears no logarithmic divergent term in the physical quantities which correspond to the self-energy operators Σ11 and Σ02 appearing in the method of Green's function.

Progress of Theoretical Physics•Apr 1, 1969•0 citations

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The resources required to solve the general interacting quantum N-body problem scale exponentially with N, making the solution of this problem very difficult when N is large. In a previous series of papers we develop an approach for a fully-interacting wave function with a general two-body interaction which tames the N-scaling by developing a perturbation series that is order-by-order invariant under a point group isomorphic with S_N . Group theory and graphical techniques are then used to solve for the wave function exactly and analytically at each order. Recently this formalism has been used to obtain the first-order, fully-interacting wave function for a system of harmonically-confined bosons interacting harmonically. In this paper, we report the first application of this N-body wave function to a system of N fully-interacting bosons in three dimensions. We determine the density profile for a confined system of harmonically-interacting bosons. Choosing this simple interaction is not necessary or even advantageous for our method, however this choice allows a direct comparison of our exact results through first order with exact results obtained in an independent solution. Our density profile through first-order in three dimensions is indistinguishable from the first-order exact result obtained independently and shows strong convergence to the exact result to all orders.

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Solution of a Quantum Mechanical N-Body Problem

Lecture notes in physics. M, Monographs•Jan 1, 1992•0 citations
The resources required to solve the general interacting quantum N-body problem scale exponentially with N, making the solution of this problem very difficult when N is large. In a previous series of papers we develop an approach for a fully-interacting wave function with a general two-body interaction which tames the N-scaling by developing a perturbation series that is order-by-order invariant under a point group isomorphic with S_N . Group theory and graphical techniques are then used to solve for the wave function exactly and analytically at each order. Recently this formalism has been used to obtain the first-order, fully-interacting wave function for a system of harmonically-confined bosons interacting harmonically. In this paper, we report the first application of this N-body wave function to a system of N fully-interacting bosons in three dimensions. We determine the density profile for a confined system of harmonically-interacting bosons. Choosing this simple interaction is not necessary or even advantageous for our method, however this choice allows a direct comparison of our exact results through first order with exact results obtained in an independent solution. Our density profile through first-order in three dimensions is indistinguishable from the first-order exact result obtained independently and shows strong convergence to the exact result to all orders.