1        0.860         0.691              0.454            1.605       1.356         1.056              0.634
        $ 5500 $          1        0.860         0.691              0.454            1.605       1.356         1.056              0.634
  -------------------- ------- ------------- ------------- ----------------------- --------- ------------- ------------- -----------------------

  : The same as in Table II, but for all charged hadrons (see also Fig. 2, left). \[Table4\]

The excluded volume corrections, i.e. the factors $ \exp \left( -
vp/T \right)$ and $\left( 1+ v\sum_i x_i \right)^{-1}$, are calculated using the THERMUS package [@Thermus]. Numerical optimization functions allow to solve the transcendental equation (\[pvdw\]) for the pressure and, thus, find the hadron yields and fluctuations of the VDW HG. The thermodynamical parameters $T,~\mu_B$, and $\gamma_S$, the VDW suppression factor $R=\exp(-vp/T)[1+v\sum_ix_i]$, and the particle number ratios $n_i/n_{tot}=n_i^{id}/n_{tot}^{id}$ (see also Fig. 2, right) along the chemical freeze-out line are presented in Table I. Once a suitable set of thermodynamical parameters is determined for each collision energy, the scaled variance of negatively, positively, and all charged particles can be calculated using Eq. (\[omega-plus-VDW\]) for $\omega_+$ and similar equations for $\omega_-$, $\omega_{ch}$, with the correlators taken from Eq. (\[corr-VDW\]). The resulting scaled variances are presented in Tables II-IV and Figs. 1 and 2 (left) as a function of $\sqrt{s_{NN}}$. The values of $\sqrt{s_{NN}}$ quoted in Tables 