QCD at finite chemical potential with six time slices
By R. Gavai, Sourendu Gupta. 2008
169 citations recorded by the source corpus.
We investigate the Taylor expansion of the baryon number susceptibility, and hence, pressure, in a series in the baryon chemical potential ({mu}{sub B}) through a lattice simulation with two flavors of light dynamical staggered quarks at a finer lattice cutoff a=1/6T. We determine the QCD cross over coupling at {mu}{sub B}=0. We find the radius of convergence of the series at various temperatures, and bound the location of the QCD critical point to be T{sup E}/T{sub c}{approx_equal}0.94 and {mu}{sub B}{sup E}/T<1.8. We also investigate the extrapolation of various susceptibilities and linkages to finite chemical potential.
Subfields: Atomic and Molecular Physics, and Optics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/64be78e2cbeb7b8c15df3679b1ceacd775028b37
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In Atomic and Molecular Physics, and Optics
In Nuclear and High Energy Physics
- C. Fischer
- Zoltán Fodor
- Kenji Fukushima
- Sándor D. Katz
- Kálmán K. Szabó
- T. Hatsuda
- S. Borsányi
- V. Koch
Citations in the corpus
- Properties of hot and dense matter from relativistic heavy ion collisions (2015, methodology): “Therefore, the above Taylor expansion for the pressure is employed in order to determine the QCD equation of state for small chemical potentials [64,67,241].”
- Higher order fluctuations and correlations of conserved charges from lattice QCD (2018, background): “Finally, higher order fluctuations of conserved charges are proportional to powers of the correlation length and are expected to diverge at the critical point, thus providing an important signature for its experimental detection [9, 24, 25].”
- The QCD phase diagram from analytic continuation (2015, methodology): “Attempts to reach non-vanishing μB on the lattice include reweighting of the generated configurations [9–13], Taylor expansion in μ [14–18], analytic continuation from imaginary μ [19–26], use of the canonical ensemble [27–29] and density of state methods [30,31].”
- The phase diagram of dense QCD (2010, background): “In [116] it was reported that coefficients up to sixth order yield TE/Tpc = 0.”