Controlling the Sign Problem in Finite Density Quantum Field Theory
arXiv:1703.04649 · doi:10.1140/epjc/s10052-017-5039-7
Abstract
Quantum field theories at finite matter densities generically possess a partition function that is exponentially suppressed with the volume compared to that of the phase quenched analogue. The smallness arises from an almost uniform distribution for the phase of the fermion determinant. Large cancellations upon integration is the origin of a poor signal to noise ratio. We study three alternatives for this integration: the Gaussian approximation, the "telegraphic" approximation, and a novel expansion in terms of theory-dependent moments and universal coefficients. We have tested the methods for QCD at finite densities of heavy quarks. We find that for two of the approximations the results are extremely close - if not identical - to the full answer in the strong sign problem regime.
13 pages, 10 figures
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- Free energy of the self-interacting relativistic lattice Bose gas at finite density
- New DoS approaches to finite density lattice QCD
- Density of states approach for lattice gauge theory with a -term
- Reduced critical slowing down for statistical physics simulations
- Real Time Simulations of Quantum Spin Chains: Density-of-States and Reweighting approaches
- Anatomy of a strong residual sign problem on the thimbles
- New canonical and grand canonical DoS techniques for finite density lattice QCD
- Efficient computations of continuous action densities of states for lattice models
- The density of states approach to the sign problem
- Nonanalyticity, sign problem and Polyakov line in Z3-symmetric heavy quark model at low temperature: Phenomenological model analyses