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Roberge-Weiss endpoint at the physical point of $N_f = 2+1$ QCD
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abstract
We study the phase diagram of $N_f = 2+1$ QCD in the $T - \mu_B$ plane and investigate the critical point corresponding to the onset of the Roberge-Weiss transition, which is found for imaginary values of $\mu_B$. We make use of stout improved staggered fermions and of the tree level Symanzik gauge action, and explore four different sets of lattice spacings, corresponding to $N_t = 4,6,8,10$, and different spatial sizes, in order to assess the universality class of the critical point. The continuum extrapolated value of the endpoint temperature is found to be $T_{\rm RW} = 208(5)$ MeV, i.e. $T_{\rm RW}/T_c \sim 1.34(7)$, where $T_c$ is the chiral pseudocritical temperature at zero chemical potential, while our finite size scaling analysis, performed on $N_t = 4$ and $N_t = 6$ lattices, provides evidence for a critical point in the $3d$ Ising universality class.
Forward citations
Cited by 3 Pith papers
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Critical point signatures in the cluster expansion in fugacities
In the trivirial model, cluster expansion coefficients b_k have asymptotics b_k ~ A e^{-k μ_R/T} k^{-α} sin(...), switching behavior at the critical temperature, and fitting the first four coefficients to lattice data...
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The Roberge-Weiss endpoint in $(2+1)$-flavor QCD with background magnetic fields
A background magnetic field lowers the Roberge-Weiss temperature in (2+1)-flavor QCD and turns the transition from second to first order between eB=1.0 and 2.5 GeV^2.
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First-order phase transition in dynamical 3-flavor QCD at imaginary isospin
Three-flavor QCD at imaginary isospin 4 pi T/3 has a first-order deconfinement transition, as shown by finite-size scaling of the rotated Polyakov loop.
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