Abstract
The experimental multiplicity and angular distribution of the secondary particles of high-energy nuclear interactions are analysed. The manner in which the estimate of dispersion σ of the log tg θ representation of the angular distribution of the secondaries varies with the energy of the primary, is studied. Based on the observed results, a distribution function which explains both the σ and multiplicity distributions is suggested. By appropriate application of that empirical relation to the «fireball model», the distributions of the mass and Lorentz factor of the fireball are derived.
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