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dc.contributor.authorALICE Collaboration
dc.date.accessioned2022-08-16T16:43:38Z
dc.date.available2022-08-16T16:43:38Z
dc.date.issued2022
dc.identifier.citationALICE Collaboration. (2022). Polarization of Λ and ¯Λ Hyperons along the Beam Direction in Pb-Pb Collisions at √sNN = 5.02 TeV. <i>Physical Review Letters</i>, <i>128</i>(17), Article 172005. <a href="https://doi.org/10.1103/PhysRevLett.128.172005" target="_blank">https://doi.org/10.1103/PhysRevLett.128.172005</a>
dc.identifier.otherCONVID_148934482
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/82595
dc.description.abstractThe polarization of the Λ and ¯Λ hyperons along the beam (z) direction, Pz, has been measured in Pb-Pb collisions at √sNN = 5.02TeV recorded with ALICE at the Large Hadron Collider (LHC). The largest contribution to Pz comes from elliptic flow induced vorticity and can be characterized by the second Fourier sine coefficient Pz,s2=⟨Pzsin(2φ−2Ψ2)⟩, where φ is the hyperon azimuthal emission angle, and Ψ2 is the elliptic flow plane angle. We report the measurement of Pz,s2 for different collision centralities, and in the 30-50% centrality interval as a function of the hyperon transverse momentum and rapidity. The Pz,s2 is positive similarly as measured by the STAR Collaboration in Au-Au collisions at √sNN = 200 GeV, with somewhat smaller amplitude in the semi-central collisions. This is the first experimental evidence of a non-zero hyperon Pz in Pb-Pb collisions at the LHC. The comparison of the measured Pz,s2 with the hydrodynamic model calculations shows sensitivity to the competing contributions from thermal and the recently found shear induced vorticity, as well as to whether the polarization is acquired at the quark-gluon plasma or the hadronic phase.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherAmerican Physical Society
dc.relation.ispartofseriesPhysical Review Letters
dc.rightsCC BY 4.0
dc.titlePolarization of Λ and ¯Λ Hyperons along the Beam Direction in Pb-Pb Collisions at √sNN = 5.02 TeV
dc.typeresearch article
dc.identifier.urnURN:NBN:fi:jyu-202208164139
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.type.urihttp://purl.org/eprint/type/JournalArticle
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1
dc.description.reviewstatuspeerReviewed
dc.relation.issn0031-9007
dc.relation.numberinseries17
dc.relation.volume128
dc.type.versionpublishedVersion
dc.rights.copyright© 2022 CERN, for the ALICE Collaboration
dc.rights.accesslevelopenAccessfi
dc.type.publicationarticle
dc.subject.ysohiukkasfysiikka
dc.subject.ysoydinfysiikka
dc.subject.ysokvarkki-gluoniplasma
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p15576
jyx.subject.urihttp://www.yso.fi/onto/yso/p14759
jyx.subject.urihttp://www.yso.fi/onto/yso/p38826
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1103/PhysRevLett.128.172005
dc.type.okmA1


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