Abstract

The dependence of the one-dimensional Bose–Einstein correlation R1D derived from proton–proton collisions is examined in terms of energy, hadron multiplicity and number of emerging hadronic jets. It is argued that the observed rise of R1D with energy is the result of the increase of the average number of hadronic jets. It is further shown that by the relatively straightforward measurements of R1D and its chaoticity parameter λ one should be able to estimate the average number of outgoing hadronic jets emitted over the entire final state phase space without the need to rely on a particular jet finding algorithm and its associated parameters.

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