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dc.contributor.authorNiemi, Harri
dc.contributor.authorEskola, Kari
dc.contributor.authorPaatelainen, R.
dc.contributor.authorTuominen, K.
dc.date.accessioned2019-02-11T06:23:27Z
dc.date.available2019-02-11T06:23:27Z
dc.date.issued2019fi
dc.identifier.citationNiemi, H., Eskola, K., Paatelainen, R., & Tuominen, K. (2019). Latest predictions from the EbyE NLO EKRT model. <em>Nuclear Physics A</em>, 982, 443-446. <a href="https://doi.org/10.1016/j.nuclphysa.2018.10.013">doi:10.1016/j.nuclphysa.2018.10.013</a>fi
dc.identifier.otherTUTKAID_80432
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/62730
dc.description.abstractWe present the latest results from the NLO pQCD + saturation + viscous hydrodynamics (EbyE NLO EKRT) model. The parameters in the EKRT saturation model are fixed by the charged hadron multiplicity in the 0-5 % 2.76 TeV Pb+Pb collisions. The √s, A and centrality dependence of the initial particle production follows then from the QCD dynamics of the model. This allows us to predict the √s and A dependence of the particle production. We show that our results are in an excellent agreement with the low-pT data from 2.76 TeV and 5.02 TeV Pb+Pb collisions at the LHC as well as with the data from the 200 GeV Au+Au collisions at RHIC. In particular, we study the centrality dependences of hadronic multiplicities, flow coefficients, and various flow correlations. Furthermore, the nuclear mass number dependence of the initial particle production and hydrodynamic evolution can be tested in the 5.44 TeV Xe+Xe collisions at the LHC. To this end, we show our predictions for charged particle multiplicities, and in particular, show how the deformations of the Xe nuclei reflect into the flow coefficients.fi
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherElsevier BV
dc.relation.ispartofseriesNuclear Physics A
dc.rightsCC BY-NC-ND 4.0
dc.subject.otherheavy-ion collisionsfi
dc.subject.otherperturbative QCD calculationsfi
dc.subject.othersaturationfi
dc.subject.otherdissipative fluid dynamicfi
dc.titleLatest predictions from the EbyE NLO EKRT modelfi
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-201901231280
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.type.urihttp://purl.org/eprint/type/JournalArticle
dc.identifier.doi10.1016/j.nuclphysa.2018.10.013
dc.date.updated2019-01-23T10:15:11Z
dc.description.reviewstatuspeerReviewed
dc.format.pagerange443-446
dc.relation.issn0375-9474
dc.relation.numberinseries0
dc.relation.volume982
dc.type.versionPublisher's PDF
dc.rights.copyright© 2018 Published by Elsevier B.V.
dc.rights.accesslevelopenAccessfi
dc.format.contentfulltext
dc.rights.urlhttps://creativecommons.org/licenses/by-nc-nd/4.0/


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