1992
DOI: 10.1142/s0217732392003839
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A Connection of Inelasticity With Multiplicity Distribution at High Energies

Abstract: The widely known experimental value of the mean coefficient of the inelasticity <K>~0.5 is calculated by the investigation of a connection of the inelasticity with KNO scaling invariant multiplicity distributions of secondary particles.

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Cited by 8 publications
(6 citation statements)
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“…It is well established experimentally that at very high energies ( √ s 3 GeV) the incoming particles lose only one-half their energy via pion photoproduction independently of the number of pions produced, i.e., y ∼ 1/2 [267]. This leading particle effect is consistent with (126).…”
Section: Opacity Of the Cmb To Uhecr Protonssupporting
confidence: 58%
“…It is well established experimentally that at very high energies ( √ s 3 GeV) the incoming particles lose only one-half their energy via pion photoproduction independently of the number of pions produced, i.e., y ∼ 1/2 [267]. This leading particle effect is consistent with (126).…”
Section: Opacity Of the Cmb To Uhecr Protonssupporting
confidence: 58%
“…However, it is well established experimentally [247] that, at very high energies ( √ s > ∼ 3 GeV), the incoming particles lose only one-half their energy via pion photoproduction independently of the number of pions produced. This is the "leading particle effect".…”
Section: A the Gzk Cutoffmentioning
confidence: 99%
“…For multi-pion production the case is much more complicated because of the non-trivial final state kinematics. However, it is well established experimentally [109] that, at very high energies ( √ s 3 GeV), the incoming particles lose only one-half their energy via pion photoproduction independently of the number of pions produced, y π ∼ 1/2. This is the "leading particle effect".…”
Section: Opacity Of the Cmb To Uhecr Protonsmentioning
confidence: 99%