出版社:SISSA, Scuola Internazionale Superiore di Studi Avanzati
摘要:The strong coupling limit (bgauge = 0) of lattice QCD with staggered fermions enjoys the same
non-perturbative properties as continuum QCD, namely confinement and chiral symmetry breaking.
In contrast to the situation at weak coupling, the sign problem which appears at finite density
can be brought under control for a determination of the full (μ,T) phase diagram by Monte Carlo
simulations. Further difficulties with efficiency and ergodicity of the simulations, especially at
the strongly first-order, low-T, finite-μ transition, are addressed respectively with a worm algorithm
and multicanonical sampling. Our simulations reveal sizeable corrections to the old results
of Karsch and Mütter [1]. Comparison with analytic mean-field determinations of the phase diagram
shows discrepancies of O(10) in the location of the QCD critical point.