that for $\omega_{\pm}$ at high collision energies.

A comparison of the primordial scaled variances with those for final hadrons demonstrates that the fluctuations increase in GCE ideal HG for each hadron species (see Eq. (\[omega-id-1\])) for positive, as well as for negative, and all charged hadrons (see Figs. 1-2). In the VDW HG the behavior is more complicated. At high collision energies, as demonstrated in Fig. 1, they even decrease for $\omega_{\pm}$ after resonance decays. This unexpected behavior follows from Eqs. (\[VDW-corr\]) and (\[corr-VDW\]). Calculating (\[corr-VDW\]) one finds that only one term, $\sum_R\langle N_R\rangle \langle n_in_j\rangle$, coming from resonance decays gives a positive contribution to the $\langle \Delta N_j \Delta N_k\rangle$ correlator. Other terms in the right hand side of Eq. (\[corr-VDW\]) appear due to particle-resonance and resonance-resonance (anti)correlations in the VDW HG. As seen from Eq. (\[VDW-corr\]) these terms are negative and, thus, suppress the scaled variances for the final state particles. The resulting effect from resonance decays is defined by the competition of two effects: decays into more than one $j$th particle against particle-resonance and resonance-resonance anticorrelations. Multi-particle decays lead to increase the fluctuations, while the anticorrelations because of the excluded volume lead to decrease them. For all 