1992
DOI: 10.1016/0920-5632(92)90265-t
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Full QCD and QED at finite temperature and chemical potential

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Cited by 70 publications
(64 citation statements)
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“…This theory retains many of the features of QCD and represents an approximation to the latter in the large mass, large chemical potential region (heavy dense QCD) [37,38]. For Wilson fermions, with hopping parameter κ, it is based on a resummed hopping parameter expansion, retaining only time-like Polyakov loops, which can formally be obtained from the limit κ → 0, µ → ∞, with κe µ fixed.…”
Section: Gauge Cooling For Qcd With Heavy Quarksmentioning
confidence: 99%
“…This theory retains many of the features of QCD and represents an approximation to the latter in the large mass, large chemical potential region (heavy dense QCD) [37,38]. For Wilson fermions, with hopping parameter κ, it is based on a resummed hopping parameter expansion, retaining only time-like Polyakov loops, which can formally be obtained from the limit κ → 0, µ → ∞, with κe µ fixed.…”
Section: Gauge Cooling For Qcd With Heavy Quarksmentioning
confidence: 99%
“…As a first application we consider QCD with static quarks at nonzero chemical potential, known as heavy dense QCD (HDQCD) [24,25]. Starting from Wilson quarks with hopping parameter κ, it can be obtained by discarding all spatial hopping terms, keeping only temporal hopping.…”
Section: Heavy Dense Qcdmentioning
confidence: 99%
“…Heavy-dense QCD (HDQCD) emerges in the limit in which the quark mass and chemical potential are simultaneously large [23,24]. This theory has a non-trivial phase diagram in the plane of temperature and chemical poten-tial, which qualitatively agrees with the one expected for real QCD: e.g., at vanishing chemical potential, there is a thermal deconfinement transition as the temperature is increased with the transition being first order for very heavy quarks and a crossover for slightly lighter but still heavy quarks [25].…”
Section: Introductionmentioning
confidence: 99%