Abstract
We propose a new quantum Monte Carlo algorithm to compute fermion ground-state properties. The ground state is projected from an initial wavefunction by a branching random walk in an over-complete basis space of Slater determinants. By constraining the determinants according to a trial wavefunction , we remove the exponential decay of signal-to-noise ratio characteristic of the sign problem. The method is variational and is exact if is exact. We report results on the two-dimensional Hubbard model up to size , for various electron fillings and interaction strengths.
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