Abstract

We calculate second- and fourth-order cumulants of conserved charges in a temperature range stretching from the QCD transition region towards the realm of (resummed) perturbation theory. We perform lattice simulations with staggered quarks; the continuum extrapolation is based on Nt=10…24N_t=10\dots24 in the crossover-region and Nt=8…16N_t=8\dots16 at higher temperatures. We find that the Hadron Resonance Gas model predictions describe the lattice data rather well in the confined phase. At high temperatures (above ∼\sim250 MeV) we find agreement with the three-loop Hard Thermal Loop results.

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