Abstract
Some properties of angular distributions of jets of mesons produced in high-energy interactions are discussed in terms of the variable\(l = log\gamma _s tg\Theta _L \)(\(\gamma _s = Lorentz\) factor of the c.m. system,\(\Theta _L = emission\) angle in the laboratory system). Such distributions are called loquian distributions, because for a given distribution in the c.m. system, they are approximately independent of the primary energy. λ=logarithmicquasiinvariantangle. Loquian distributions for different c.m. system amplitudes are given and an analysis is discussed in terms of the moments of the loquian distributions. A fireball loquian distribution is approximately decomposed into one centre c.m. system amplitudes.
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