Fig. 1. Statistics dependence of κσ2 of net-proton (a) and net-charge (b) multiplicity distributions calculated by the CBWC method at various centrality bin width

Fig. 2. The centrality dependency of κσ2 of original (a) and mixed (b) samples, dynamical (c) and formula corrected (d) for three values of efficiency 100%, 80% and 60%

Fig. 3. χ2vs.T/Tpt at h= 0.000 5 (a), 0.000 775 (b), 0.002 (c) with the system sizes of L = 40, 50, 60, 70

Fig. 4. The scaled order parameter mLλ/νvs. the scaled variabletL1/ν (a, c) and T (b, d)(a, b) 2D Ising model with external field h=0, (c, d) 3D three-state Potts model with h=0.000 5

Fig. 5. Contour plot of D(T,a) for three different external fields (a) h = 0.000 775, (b) h = 0.000 5, (c) h = 0.002

Fig. 6. The evolution of |m| with time at L = 60 for random initial configuration at temperatures T/T_c = 0.93 (a), 0.99 (b), 1.00 (c) and 1.03 (d), respectively

Fig. 7. Average relaxation time as a function of temperature (a) System sizes L = 50 and 60 starting from random initial configuration, (b) Random initial configurations and polarized initial configurations at a fixed system size L=60

Fig. 8. The time evolution of cumulants of |m| at a given system size L=60 at T/T_c=0.99 (a~d) and 1.01 (e~h)