Multiplicities of secondary hadrons in the fragmentation region of a projectile are computed as a function of the atomic number of the target, A. The calculation is based on the notion of a nucleon (meson) composed of three (two) spatially discrete constituent quarks. For an incident proton, yields of secondary nucleons near x = 23(as well as π− or K+ mesons near x = 13) are determined solely by the magnitude of the quark-nucleon cross section, assumed to be ∼ 13 of the inelastic proton-proton cross section, and the distribution of nuclear matter. Our results agree well with the data on A dependence of the p, π− and K+ yields in proton-nucleus collisions. Predictions are given for the A dependence of the projectile fragment yields in the cases of π, K and hyperon beams.
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Anisovich et al. (1978) studied this question.
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