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dc.contributor.authorALICE Collaboration
dc.date.accessioned2015-07-14T08:11:10Z
dc.date.available2015-07-14T08:11:10Z
dc.date.issued2015
dc.identifier.citationALICE Collaboration. (2015). Measurement of jet suppression in central Pb–Pb collisions at √sNN = 2.76 TeV. <i>Physics Letters B</i>, <i>746</i>, 1-14. <a href="https://doi.org/10.1016/j.physletb.2015.04.039" target="_blank">https://doi.org/10.1016/j.physletb.2015.04.039</a>
dc.identifier.otherCONVID_24781327
dc.identifier.otherTUTKAID_66540
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/46503
dc.description.abstractThe transverse momentum (pT) spectrum and nuclear modification factor (RAA) of reconstructed jets in 0–10% and 10–30% central Pb–Pb collisions at √sNN = 2.76 TeV were measured. Jets were reconstructed using the anti-kT jet algorithm with a resolution parameter of R = 0.2 from charged and neutral particles, utilizing the ALICE tracking detectors and Electromagnetic Calorimeter (EMCal). The jet pT spectra are reported in the pseudorapidity interval of |ηjet| < 0.5 for 40 < pT, jet < 120 GeV/c in 0–10% and for 30 < pT, jet < 100 GeV/c in 10–30% collisions. Reconstructed jets were required to contain a leading charged particle with pT > 5 GeV/c to suppress jets constructed from the combinatorial background in Pb–Pb collisions. The leading charged particle requirement applied to jet spectra both in pp and Pb– Pb collisions had a negligible effect on the RAA. The nuclear modification factor RAA was found to be 0.28 ± 0.04 in 0–10% and 0.35 ± 0.04 in 10–30% collisions, independent of pT, jet within the uncertainties of the measurement. The observed suppression is in fair agreement with expectations from two model calculations with different approaches to jet quenching.fi
dc.language.isoeng
dc.publisherElsevier BV * North-Holland
dc.relation.ispartofseriesPhysics Letters B
dc.subject.otherjet spectra
dc.subject.otherjet suppression
dc.subject.otherPb–Pb collisions
dc.titleMeasurement of jet suppression in central Pb–Pb collisions at √sNN = 2.76 TeV
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-201507072544
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.type.urihttp://purl.org/eprint/type/JournalArticle
dc.date.updated2015-07-07T12:15:02Z
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1
dc.description.reviewstatuspeerReviewed
dc.format.pagerange1–14
dc.relation.issn0370-2693
dc.relation.numberinseries0
dc.relation.volume746
dc.type.versionpublishedVersion
dc.rights.copyright© 2015 CERN for the benefit of the ALICE Collaboration. Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP3.
dc.rights.accesslevelopenAccessfi
dc.rights.urlhttp://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1016/j.physletb.2015.04.039
dc.type.okmA1


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© 2015 CERN for the benefit of the ALICE Collaboration. Published by Elsevier B.V. This is an open
access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP3.
Except where otherwise noted, this item's license is described as © 2015 CERN for the benefit of the ALICE Collaboration. Published by Elsevier B.V. This is an open access article under the CC BY license (http://creativecommons.org/licenses/by/4.0/). Funded by SCOAP3.