Complex spectrum of finite-density lattice QCD with static quarks at strong coupling
arXiv:1512.09131 · doi:10.1103/PhysRevD.93.094501
Abstract
We calculate the spectrum of transfer matrix eigenvalues associated with Polyakov loops in finite-density lattice QCD with static quarks. These eigenvalues determine the spatial behavior of Polyakov loop correlations functions. Our results are valid for all values of the gauge coupling in dimensions, and valid in the strong-coupling region for any number of dimensions. When the quark chemical potential is nonzero, the spatial transfer matrix is non-Hermitian. The appearance of complex eigenvalues in is a manifestation of the sign problem in finite-density QCD. The invariance of finite-density QCD under the combined action of charge conjugation and complex conjugation implies that the eigenvalues of are either real or part of a complex pair. Calculation of the spectrum confirms the existence of complex pairs in much of the temperature-chemical potential plane. Many features of the spectrum for static quarks are determined by a particle-hole symmetry. For small compared to the quark mass , we typically find real eigenvalues for the lowest lying states. At somewhat larger values of pairs of eigenvalues may form complex-conjugate pairs, leading to damped oscillatory behavior in Polyakov loop correlation functions. However, near , the low-lying spectrum becomes real again. This is a direct consequence of the approximate particle-hole symmetry at for heavy quarks. This behavior of the eigenvalues should be observable in lattice simulations and can be used as a test of lattice algorithms. Our results provide independent confirmation of results we have previously obtained in PNJL models using complex saddle points.
14 pages, 11 figures. Figure 1 fixed, references added, minor editing and typos corrected
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