2004/12/31 by Abdel Nasser Tawfik, A. Tawfik · 2 citations
Physics and Astronomy · #Diffraction #Hadron #High-Energy Particle Collisions Research #Lattice (music) #Lattice QCD #Lattice constant #Lattice field theory #Mathematical physics #Particle physics #Particle physics theoretical and experimental studies #Phase (matter) #Phase diagram #Physics #Quantum Chromodynamics and Particle Interactions #Quantum chromodynamics #Quantum mechanics #Strangeness #hep-ph
paper · pdf · doi:10.1103/physrevd.71.054502
published as Phys.Rev. D71 (2005) 054502 · 25 pages, 8 eps figures
arxiv created 2005/02/19 · openalex publication_date 2005/03/08 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We compare the lattice results on QCD phase diagram for two and three flavors with the hadron resonance gas model (HRGM) calculations. Lines of constant energy density ϵ have been determined at different baryo-chemical potentials \ensuremathμB. For the strangeness chemical potentials \ensuremathμS, we use two models. In one model, we explicitly set \ensuremathμS=0 for all temperatures and baryo-chemical potentials. This assignment is used in lattice calculations. In the other model, \ensuremathμS is calculated in dependence on T and \ensuremathμB according to the condition of vanishing strangeness. We also derive an analytical expression for the dependence of Tc on \ensuremathμB/T by applying Taylor expansion of ϵ. In both cases, we compare HRGM results on Tc\ensuremath-\ensuremathμB diagram with the lattice calculations. The agreement is excellent, especially when the trigonometric function of ϵ is truncated up to the same order as done in lattice simulations. For studying the efficiency of the truncated Taylor expansion, we calculate the radius of convergence. For zero- and second-order radii, the agreement with lattice is convincing. Furthermore, we make predictions for QCD phase diagram for nontruncated expressions and physical masses. These predictions are to be confirmed by heavy-ion experiments and future lattice calculations with very small lattice spacing and physical quark masses.