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We show that very accurate ground-state energies and correlation functions can be obtained from an approximate, variational form of the widely used auxiliary-field simulation method. It is derived by recasting this method as a diffusion problem, and does not exhibit the poor statistical behavior due to vanishing normalization or ``sign'' common to exact fermion simulations. We give illustrative results for two-dimensional Hubbard models.
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Fahy et al. (1990) studied this question.
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