Abstract
I discuss algorithms for simulating many-fermion systems via global updatings of auxiliary fields followed by an accept-reject stage which eliminates finite-step-size errors. When the system size is larger than the correlation length, these procedures should require computer time growing only slightly faster than linearly with the system volume V. A corrected Langevin scheme should asymptotically display a ${V}^{4/3}$ behavior, while the hybrid Monte Carlo scheme can behave as ${V}^{5/4}$. I present some tests of the latter algorithm on a simple model of interacting electrons on a two-dimensional lattice.
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Publication Info
- Year
- 1988
- Type
- article
- Volume
- 38
- Issue
- 4
- Pages
- 1228-1238
- Citations
- 146
- Access
- Closed
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Identifiers
- DOI
- 10.1103/physrevd.38.1228