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dc.contributor.authorALICE Collaboration
dc.date.accessioned2024-10-24T09:51:59Z
dc.date.available2024-10-24T09:51:59Z
dc.date.issued2024
dc.identifier.citationALICE Collaboration. (2024). Measurement of the impact-parameter dependent azimuthal anisotropy in coherent ρ0 photoproduction in Pb−Pb collisions at √sNN= 5.02 TeV. <i>Physics Letters B</i>, <i>858</i>, Article 139017. <a href="https://doi.org/10.1016/j.physletb.2024.139017" target="_blank">https://doi.org/10.1016/j.physletb.2024.139017</a>
dc.identifier.otherCONVID_243284273
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/97671
dc.description.abstractThe first measurement of the impact-parameter dependent angular anisotropy in the decay of coherently photoproduced ρ0 mesons is presented. The ρ0 mesons are reconstructed through their decay into a pion pair. The measured anisotropy corresponds to the amplitude of the cos(2ϕ) modulation, where ϕ is the angle between the two vectors formed by the sum and the difference of the transverse momenta of the pions, respectively. The measurement was performed by the ALICE Collaboration at the LHC using data from ultraperipheral Pb−Pb collisions at a center-of-mass energy of √sNN = 5.02 TeV per nucleon pair. Different impact-parameter regions are selected by classifying the events in nuclear-breakup classes. The amplitude of the cos(2ϕ) modulation is found to increase by about one order of magnitude from large to small impact parameters. Theoretical calculations, which describe the measurement, explain the cos(2ϕ) anisotropy as the result of a quantum interference effect at the femtometer scale that arises from the ambiguity as to which of the nuclei is the source of the photon in the interaction.en
dc.format.mimetypeapplication/pdf
dc.language.isoeng
dc.publisherElsevier
dc.relation.ispartofseriesPhysics Letters B
dc.rightsCC BY 4.0
dc.titleMeasurement of the impact-parameter dependent azimuthal anisotropy in coherent ρ0 photoproduction in Pb−Pb collisions at √sNN= 5.02 TeV
dc.typeresearch article
dc.identifier.urnURN:NBN:fi:jyu-202410246527
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.issn0370-2693
dc.relation.volume858
dc.type.versionpublishedVersion
dc.rights.copyright© 2024 CERN for the benefit of the ALICE Collaboration. Published by Elsevier B.V. Funded by SCOAP³
dc.rights.accesslevelopenAccessfi
dc.type.publicationarticle
dc.relation.grantnumber346328
dc.relation.grantnumber346327
dc.subject.ysoydinfysiikka
dc.subject.ysohiukkasfysiikka
dc.format.contentfulltext
jyx.subject.urihttp://www.yso.fi/onto/yso/p14759
jyx.subject.urihttp://www.yso.fi/onto/yso/p15576
dc.rights.urlhttps://creativecommons.org/licenses/by/4.0/
dc.relation.doi10.1016/j.physletb.2024.139017
dc.relation.funderResearch Council of Finlanden
dc.relation.funderResearch Council of Finlanden
dc.relation.funderSuomen Akatemiafi
dc.relation.funderSuomen Akatemiafi
jyx.fundingprogramCentre of Excellence, AoFen
jyx.fundingprogramCentre of Excellence, AoFen
jyx.fundingprogramHuippuyksikkörahoitus, SAfi
jyx.fundingprogramHuippuyksikkörahoitus, SAfi
jyx.fundinginformationAcademy of Finland (Center of Excellence in Quark Matter) (grant nos. 346327, 346328), Finland.
dc.type.okmA1


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