Abstract
The distribution over the number of prongs in inelastic hadronic collisions can be calculated by assuming (i) that the multiplicities of produced pions form a Poisson distribution, and (ii) that all the isospin final states are equally probable. The set of distributions for ${\ensuremath{\pi}}^{\ensuremath{-}}p$ inelastic collisions have been calculated, and agree well with experiments for all energies.
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