2004
DOI: 10.1103/physrevd.69.059903
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Erratum: Possible scenarios for soft and semihard component structure in central hadron-hadron collisions in the TeV region [Phys. Rev. D59, 094020 (1999)]

Abstract: Possible scenarios in hh collisions in the TeV region are discussed in full phase space. It is shown that at such high energies one should expect strong KNO scaling violation and a ln( √ s) increase of the average charged multiplicity of the semi-hard component, resulting in a huge mini-jet production. Dedication

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Cited by 53 publications
(140 citation statements)
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“…Apparently, the multiplicity increase in this analysis is dominated by increased frequency of events with a single hard scattering within a multiplicity class rather than bias toward more energetic partons. That scenario is consistent with the twocomponent model of [10].…”
Section: Discussionsupporting
confidence: 78%
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“…Apparently, the multiplicity increase in this analysis is dominated by increased frequency of events with a single hard scattering within a multiplicity class rather than bias toward more energetic partons. That scenario is consistent with the twocomponent model of [10].…”
Section: Discussionsupporting
confidence: 78%
“…The two-component model of nuclear collisions can be applied to (1) the event-frequency distribution on n ch (two or more negative-binomial distributions) [10,20], (2) the dependence of hp t i on n ch [8,16,26], (3) triggered jet correlations on ( , ) (correlations from soft and hard event classes) [21], and (4) the n ch dependence of the p t or y t spectrum shape [16]. The common theme is the relation of hard parton scattering to event multiplicity in the context of a ''soft'' underlying event.…”
Section: Discussionmentioning
confidence: 99%
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“…Possible scenarios for pp collisions in the TeV energy domain, based on extrapolations from data and fits in the GeV region to charged particle multiplicity distributions, P n , and on the weighted superposition mechanism of two classes of events, i.e., soft (without minijets) and semihard (with minijets), each described by a negative binomial multiplicity distribution (NBMD) with characteristic parameters (n soft , k soft andn sh , k sh , respectively) have been discussed both in full phase space [1] and rapidity intervals [2]. (For an experimental investigation of the substructures see Ref.…”
Section: Introductionmentioning
confidence: 99%