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dc.contributor.authorALICE Collaboration
dc.date.accessioned2018-04-25T10:51:03Z
dc.date.available2018-04-25T10:51:03Z
dc.date.issued2018
dc.identifier.citationALICE Collaboration. (2018). π0 and η meson production in proton-proton collisions at √s = 8 TeV. <i>European Physical Journal C</i>, <i>78</i>(3), Article 263. <a href="https://doi.org/10.1140/epjc/s10052-018-5612-8" target="_blank">https://doi.org/10.1140/epjc/s10052-018-5612-8</a>
dc.identifier.otherCONVID_28001722
dc.identifier.otherTUTKAID_77365
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/57755
dc.description.abstractAn invariant differential cross section measurement of inclusive π0 and η meson production at mid-rapidity in pp collisions at s√=8 TeV was carried out by the ALICE experiment at the LHC. The spectra of π0 and η mesons were measured in transverse momentum ranges of 0.3<p T <35 GeV/c and 0.5<p T <35 GeV/c , respectively. Next-to-leading order perturbative QCD calculations using fragmentation functions DSS14 for the π0 and AESSS for the η overestimate the cross sections of both neutral mesons, although such calculations agree with the measured η/π0 ratio within uncertainties. The results were also compared with PYTHIA 8.2 predictions for which the Monash 2013 tune yields the best agreement with the measured neutral meson spectra. The measurements confirm a universal behavior of the η/π0 ratio seen for NA27, PHENIX and ALICE data for pp collisions from s√=27.5 GeV to s√=8 TeV within experimental uncertainties. A relation between the π0 and η production cross sections for pp collisions at s√=8 TeV is given by m T scaling for p T >3.5 GeV/c . However, a deviation from this empirical scaling rule is observed for transverse momenta below p T <3.5 GeV/c in the η/π0 ratio with a significance of 6.2σ.
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherSpringer Berlin Heidelberg
dc.relation.ispartofseriesEuropean Physical Journal C
dc.subject.otherp-Pb collisions
dc.titleπ0 and η meson production in proton-proton collisions at √s = 8 TeV
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-201804192130
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.type.urihttp://purl.org/eprint/type/JournalArticle
dc.date.updated2018-04-19T12:15:15Z
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1
dc.description.reviewstatuspeerReviewed
dc.relation.issn1434-6044
dc.relation.numberinseries3
dc.relation.volume78
dc.type.versionpublishedVersion
dc.rights.copyright© the Authors, 2018. This is an open access article distributed under the terms of the Creative Commons License.
dc.rights.accesslevelopenAccessfi
dc.subject.ysohiukkasfysiikka
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p15576
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1140/epjc/s10052-018-5612-8
dc.type.okmA1


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© the Authors, 2018. This is an open access article distributed under the terms of the Creative Commons License.
Ellei muuten mainita, aineiston lisenssi on © the Authors, 2018. This is an open access article distributed under the terms of the Creative Commons License.