Abstract
A more powerful version of a numerical method published before is given which permits the integration of the Schrödinger equation for a large ensemble of particles. A new method for obtaining quantum expectation values is outlined. Numerical results are tabulated for the energy of the ground state of a system of 32 bosons interacting by Lennard-Jones potentials and with periodic boundary conditions. This is a commonly used model of liquid He4. The present results are substantially lower and closer to experiment than variational estimates based on a Jastrow-type wave function.

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