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<> Thermodynamics of largeN_{f} QCD at Finite Chemical Potential
1/2*Susceptibility at mu_q=0
(T=1, mubar=\pi T, mu_q=0, g_eff^2=0 .. 40. First column is g_eff^2, second column is the pressure. Data give the second derivative of the pressure with respect to mu_q. To get the susceptibility multiply by 2.) 1/12*Higher Susceptibility at mu_q=0
(T=1, mubar=\pi T, mu_q=0, g_eff^2=0 .. 40. First column is g_eff^2, second column is the pressure. Data give the forth derivative of the pressure with respect to mu_q. To get the higher susceptibility multiply by 12.) Further data tables from the paper will be available soon. <> Comment on and erratum to "Pressure of Hot QCD at Large N_{f}"
Tables: The data tables give the pressure over the free pressure. The first column is the effective coupling g_eff^2 from 0 to 35 in steps of 0.25. The second column gives the normalized pressure with different cutoffs. In the combined tables, the second column shows a=1/4, the third column a=1/2 and the last column a=0.81. Graphs: The graphs show the combined plots for different cutoffs. In the pressure plots, green corresponds to a=1/4, blue to a=1/2, and black to a=0.81. Computational details: For values of g_eff^2 > 22.5, the cutoff is chosen at Lambda_Landau / 2 (a=1/4), Lambda_Landau / sqrt(2) (a=1/2), and 0.9 Lambda_Landau (a=0.81). For smaller values of g_eff^2, a constant cutoff is chosen at 28.2, 39.9, and 50.7 (which is the cutoff for g_eff^2=22.5). This cutoff affects the spatial qintegration in Minkowski space, and the 4dimensional Qintegration in Euclidean space. In Minkowski space omega is integrated up to 40 for all g_eff^2. The lower bounds for q and omega in Minkowski space are chosen at 10^8, and the range closer than 10^9 to the lightcone q=omega is taken out of Minkowski integration. The results given are accurate to at least 4 or 5 digits.
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