Skewness and kurtosis of net-strangeness, net-baryon number and net-electric charge distributions at non-zero $\mu_B$.

6 Nov 2019, 17:20
20m
Ball Room1 (Wanda Reign Wuhan Hotel)

Ball Room1

Wanda Reign Wuhan Hotel

Oral Presentation QCD at finite temperature and baryon density Parallel Session - QCD at finite temperature III

Speaker

Dennis Bollweg (Bielefeld University)

Description

Using recent results on higher order cumulants of conserved charge fluctuations from lattice QCD, we construct mean, variance, skewness and kurtosis of net-strangeness, net-baryon number and net-electric charge distributions at next-to-leading order in $\mu_B$. For the strangeness neutral case ($\mu_S=0$) at fixed ratio of electric charge to baryon number density ($\frac{n_Q}{n_B}=0.4$), which is appropriate for a comparison with heavy ion collisions, we present results for $\kappa_X \sigma_X^2$ and $S_X \sigma_X$ and $S_X \sigma_X^3/M_X, (X=B,Q,S)$ on the crossover line for the chiral transition ($T_{pc}(\mu_B)$). Continuum extrapolations for this pseudo-critical transition line have recently been reported by HotQCD up to baryon chemical potentials $\mu_B\simeq 300$ MeV (arXiv:1812.08235). These cumulant ratios thus are of direct relevance for comparisons with corresponding ratios measured by STAR in the BES-I and II runs at beam energies $\sqrt{s_{NN}}\ge 20$ GeV. In particular, we point out that recent high statistics results on skewness and kurtosis of net-baryon number distributions obtained by STAR at $\sqrt{s_{NN}} = 54.4$ GeV put strong constraints on freeze-out parameters and are consistent with predictions from thermal QCD. Additionally, we show that, unlike in the case of net-baryon number fluctuations, the kurtosis ratios for strangeness and electric charge are only weakly dependent on $\mu_B$.

Furthermore, we also construct Taylor series for baryon-strangeness and baryon-charge correlations up to $\mathcal{O}(\mu_B^4)$ and present results for these observables on the crossover transition line. We point out that these correlations are dominated by correlations in the baryon sector of QCD, which is consistent with recent findings of the STAR collaboration (arXiv:1903.05370). Correlations of proton fluctuations with kaon or pion fluctuations, respectively, thus are poor proxies for studying such correlations on the freeze-out line in heavy ion collisions.

Primary authors

Dennis Bollweg (Bielefeld University) Frithjof Karsch (Brookhaven National Laboratory) Swagato Mukherjee (Brookhaven National Laboratory) Christian Schmidt (University of Bielefeld)

Presentation materials