Abstract

We investigate the phase of the quark determinant with finite chemical potential in lattice QCD using both analytic and numerical methods. Applying the winding expansion and the hopping parameter expansion to the logarithm of the determinant, we show that the absolute value of the phase has an upper bound that grows with the spatial volume but decreases exponentially with an increase in the temporal extent of the lattice. This analytic but approximate result is confirmed with a numerical study in four-flavor QCD in which the phase is calculated exactly. Since the phase is well controlled on lattices with larger time extents, we try the phase reweighting method in a region beyond $\ensuremath{\mu}/T=1$ where the Taylor expansion method cannot be applied. Working in four-flavor QCD, we find a first-order like behavior on a ${6}^{3}\ifmmode\times\else\texttimes\fi{}4$ lattice at $\ensuremath{\mu}/T\ensuremath{\approx}0.8$ which was previously observed by the Kentucky group with the canonical method. We also show that the winding expansion has a nice convergence property beyond $\ensuremath{\mu}/T=1$. We expect that this expansion is useful to study the high density region of the QCD phase diagram at low temperatures.

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