“…and n F , n B the numbers of charged particles lying respectively in the forward and backward hemispheres, andn F andn B their corresponding average charged multiplicities [1,7,8,9]. It should be pointed out that the qualifying assumption of the WSM is that P n is described for each class of events in terms of the Pascal, i.e., negative binomial (NB), MD with the average charged particle multiplicity,n, and k (linked to the variance D 2 ≡ n 2 −n 2 by the relation k =n 2 /(D 2 −n)) as characteristic parameters, and this fact leads to a sound description of the experimental data [1,10,11].…”