Duplicate of Centrality and system-size dependencies of temperatures of soft and hard components of pt distributions of negative pions in 4 He + 12C , 12C + 12C, and 12C + 181Ta collisions at

The partial inelasticity coefficients of the negative pions were determined in minimum bias p, d, α, 12C+12C and p, 12C+18Ta collisions at 4.2A GeV/c taking into account the average number of participant nucleons of a projectile nucleus. In nucleus–nucleus collisions, the average values of partial inelasticity coefficients (K(π−)) of the negative pions did not depend on the mass numbers of projectile and target nuclei. Increase of K(π−) in going from p+12C to d, α,12C+12C collisions was due to an additional source of production of fast negative pions in nucleus–nucleus collisions — a charge exchange conversion of one or more neutrons of a projectile nucleus into a proton and π−. Linking the experimental results of the present analysis at intermediate energy with those obtained at high and ultra-high energies, it was concluded that the average values of partial inelasticity coefficients of pions in nucleon–nucleus and nucleus–nucleus collisions manifest a transitive behavior. At intermediate energies, the values of K(π−) were smaller by a factor of two and more as compared to those at high energies, and they increased further with increasing incident energy, reaching a plateau at E0 > 100A GeV.

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