I-IV and marked in Figs. 1-2 correspond to the beam energies at SIS (2$A$ GeV), AGS (11.6$A$ GeV), SPS ($20A$, $30A$, $40A$, $80A$, and $158A$ GeV), colliding energies at RHIC ($\sqrt{s_{NN}}=62.4$ GeV, $130$ GeV, and $200$ GeV), and LHC ($\sqrt{s_{NN}}=5500$ GeV). Both the primordial and final state scaled variances are presented. To make a correspondence with real measurements, both strong and electromagnetic decays should be taken into account, while weak decays should be omitted.

Some features of the results should be mentioned. The values $\omega_{\pm}=\omega_{ch}=1$ are shown by the dashed-dotted lines in Figs. 1-2. They correspond to the primordial fluctuations in the ideal HG ($r=0$). The bump in $\omega_+$ for final state particles seen in Fig. \[omega\_pos\] at the small collision energies is due to a correlated production of proton and $\pi^+$ meson from $\Delta^{++}$ decays. This single resonance contribution dominates in $\omega_+$ at small collision energies (small temperatures), but becomes relatively unimportant at the high collision energies.

The number of negative particles is relatively small, $\langle
N_-\rangle \ll \langle N_+\rangle$, at low collision energies (see Fig. 2, right). For the hard-core radius $r=0.5$ fm, this region corresponds ’small’ particle number density, $vn_{tot}\ll 1$. It then follows, for the primordial 