Abstract:We comment on the reweighting method for the study of finite density lattice QCD. We discuss the applicable parameter range of the reweighting method for models which have more than one simulation parameter. The applicability range is determined by the fluctuations of the modification factor of the Boltzmann weight. In some models having a first order phase transition, the fluctuations are minimized along the phase transition line if we assume that the pressure in the hot and the cold phase is balanced at the … Show more
The expectation value of the complex phase factor of the fermion determinant is computed to leading order in the p-expansion of the chiral Lagrangian. The computation is valid for µ < mπ/2 and determines the dependence of the sign problem on the volume and on the geometric shape of the volume. In the thermodynamic limit with Li → ∞ at fixed temperature 1/L0, the average phase factor vanishes. In the low temperature limit where Li/L0 is fixed as Li becomes large the average phase factor approaches one. The results for a finite volume compare well with lattice results obtained by Allton et al.. After taking appropriate limits, we reproduce previously derived results for the ǫ-regime and for 1-dimensional QCD. The distribution of the phase itself is also computed.
The expectation value of the complex phase factor of the fermion determinant is computed to leading order in the p-expansion of the chiral Lagrangian. The computation is valid for µ < mπ/2 and determines the dependence of the sign problem on the volume and on the geometric shape of the volume. In the thermodynamic limit with Li → ∞ at fixed temperature 1/L0, the average phase factor vanishes. In the low temperature limit where Li/L0 is fixed as Li becomes large the average phase factor approaches one. The results for a finite volume compare well with lattice results obtained by Allton et al.. After taking appropriate limits, we reproduce previously derived results for the ǫ-regime and for 1-dimensional QCD. The distribution of the phase itself is also computed.
“…The origin of the sign problem are the fluctuations of the complex phase θ, defined by detM ≡ |detM| exp{iθ}. In case those fluctuations ( (θ − θ ) 2 ) become considerably larger than π/2 [2], the problem becomes serious. For a detailed discussion of the phase of the fermion determinant see also [3].…”
Abstract:We study the QCD phase diagram by first principle lattice calculations at so far unreached high densities. For this purpose we employ the density of states method. Unimproved staggered fermions, which describe four quark flavors in the continuum are used in this analysis. Though the method is quite expensive, small lattices show an indication for a triple-point connecting three different phases on the phase diagram.
“…When µ = 0, the complex nature of the fermion determinant makes the matter much worse. While finite-µ results, including the location of the QCD critical point, have been obtained by reweighting µ = 0 data [3], assessing the reliability of these results is a challenge in itself [4]. It appears that the only information that can be obtained reliably (i.e.…”
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