2019
DOI: 10.1016/j.physletb.2019.135049
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Pseudorapidity distributions of charged hadrons in xenon-xenon collisions at sNN=5.44 TeV

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Cited by 12 publications
(5 citation statements)
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“…It has been noted by ALICE [23], that the charged multiplicity per participant nucleon, defined by 2 dN ch /dη/ N part , shows an 'uptick' for limiting (high) values of N part , breaking participant scaling. The same effect has been measured by CMS [24] and PHOBOS [25], but without giving it too much attention. The effect can be reproduced by some, but not all, models.…”
Section: Multiplicity Distributionssupporting
confidence: 70%
“…It has been noted by ALICE [23], that the charged multiplicity per participant nucleon, defined by 2 dN ch /dη/ N part , shows an 'uptick' for limiting (high) values of N part , breaking participant scaling. The same effect has been measured by CMS [24] and PHOBOS [25], but without giving it too much attention. The effect can be reproduced by some, but not all, models.…”
Section: Multiplicity Distributionssupporting
confidence: 70%
“…Historically, heavy ion collisions have been considered an overly complicated environment, therefore unsuitable for precise measurements of particle properties or searches of rare phenomena, because of their large final-state particle multiplicity, as opposed to pp collisions. However, due to the high pileup during Run 4 in pp collisions, the track multiplicity is expected to become comparable for pp and PbPb collisions while it is smaller for lighter ion collisions [29].…”
Section: Track and Vertex Multiplicitiesmentioning
confidence: 99%
“…To determine the value n, we must use data. Pseudorapidity distributions have been measured extensively in the ATLAS [42][43][44][45], CMS [46][47][48][49][50][51][52] and ALICE [53][54][55][56][57][58][59][60][61][62] experiments at the LHC, in both pp and heavy ion collisions. From those data, we can determine the parameter n by noting the following.…”
Section: Jhep10(2021)094mentioning
confidence: 99%