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dc.date.accessioned2018-09-27T14:31:48Z
dc.date.available2018-09-27T14:31:48Z
dc.date.created2018-02-16T16:02:11Z
dc.date.issued2017
dc.identifier.citationAcharya, Shreyasi Adam, Jaroslav Adamová, Dagmar Adolfsson, Jonatan Aggarwal, Madan M. Aglieri Rinella, G Agnello, Michelangelo Agrawal, Nikita Ahammed, Zubayer Ahmad, N Ahn, SU Aiola, Salvatore Akindinov, Alexander Alam, Sk Noor Alba, José Luis Bazo Aleksandrov, Dimitry Allesandro, B. Alme, Johan Altenkaemper, Lucas Arsene, Ionut Christian Bätzing, Paul Christoph Djuvsland, Øystein Dordic, Olja Helstrup, Håvard Hetland, Kristin Fanebust Kileng, Bjarte Langøy, Rune Lardeux, Antoine Xavier Lien, Jørgen André Lindal, Svein Lønne, Per-Ivar Mahmood, Sohail Musa Milosevic, Jovan Nesbø, Simon Voigt Nystrand, Joakim Rehman, Attiq Ur Richter, Matthias Rudolph Røed, Ketil Røhrich, Dieter Skaali, Toralf Bernhard Tambave, Ganesh Jagannath Tveter, Trine Spedstad Ullaland, Kjetil Velure, Arild Wagner, Boris Wikne, Jon Christopher Zhang, Hui Zhao, Chengxin Zhou, Zhuo Zhu, Hongsheng ALICE, Collaboration . Azimuthally differential pion femtoscopy relative to the second and thrid harmonic in Pb-Pb 2.76 TeV collisions from ALICE. Nuclear Physics A. 2017, 967, 468-471
dc.identifier.urihttp://hdl.handle.net/10852/64990
dc.description.abstractAzimuthally differential femtoscopic measurements, being sensitive to spatio-temporal characteristics of the source as well as to the collective velocity fields at freeze-out, provide very important information on the nature and dynamics of the system evolution. While the HBT radii modulations relative to the second harmonic event plane reflect mostly the spatial geometry of the source, the third harmonic results are mostly defined by the velocity fields [1]. Radii variations with respect to the third harmonic event plane unambiguously signal a collective expansion and anisotropy in the flow fields. Event shape engineering (ESE) is a technique proposed to select events corresponding to a particular shape. Azimuthally differential HBT combined with ESE allows for a detailed analysis of the relation between initial geometry, anisotropic flow and the deformation of source shape. We present azimuthally differential pion femtoscopy with respect to second and third harmonic event planes as a function of the pion transverse momentum for different collision centralities in Pb–Pb collisions at √sNN = 2.76 TeV. All these results are compared to existing models. The effects of the selection of the events with high elliptic or triangular flow are also presented.en_US
dc.languageEN
dc.rightsAttribution-NonCommercial-NoDerivatives 4.0 International
dc.rights.urihttps://creativecommons.org/licenses/by-nc-nd/4.0/
dc.titleAzimuthally differential pion femtoscopy relative to the second and thrid harmonic in Pb-Pb 2.76 TeV collisions from ALICEen_US
dc.typeJournal articleen_US
dc.creator.authorAcharya, Shreyasi
dc.creator.authorAdam, Jaroslav
dc.creator.authorAdamová, Dagmar
dc.creator.authorAdolfsson, Jonatan
dc.creator.authorAggarwal, Madan M.
dc.creator.authorAglieri Rinella, G
dc.creator.authorAgnello, Michelangelo
dc.creator.authorAgrawal, Nikita
dc.creator.authorAhammed, Zubayer
dc.creator.authorAhmad, N
dc.creator.authorAhn, SU
dc.creator.authorAiola, Salvatore
dc.creator.authorAkindinov, Alexander
dc.creator.authorAlam, Sk Noor
dc.creator.authorAlba, José Luis Bazo
dc.creator.authorAleksandrov, Dimitry
dc.creator.authorAllesandro, B.
dc.creator.authorAlme, Johan
dc.creator.authorAltenkaemper, Lucas
dc.creator.authorArsene, Ionut Christian
dc.creator.authorBätzing, Paul Christoph
dc.creator.authorDjuvsland, Øystein
dc.creator.authorDordic, Olja
dc.creator.authorHelstrup, Håvard
dc.creator.authorHetland, Kristin Fanebust
dc.creator.authorKileng, Bjarte
dc.creator.authorLangøy, Rune
dc.creator.authorLardeux, Antoine Xavier
dc.creator.authorLien, Jørgen André
dc.creator.authorLindal, Svein
dc.creator.authorLønne, Per-Ivar
dc.creator.authorMahmood, Sohail Musa
dc.creator.authorMilosevic, Jovan
dc.creator.authorNesbø, Simon Voigt
dc.creator.authorNystrand, Joakim
dc.creator.authorRehman, Attiq Ur
dc.creator.authorRichter, Matthias Rudolph
dc.creator.authorRøed, Ketil
dc.creator.authorRøhrich, Dieter
dc.creator.authorSkaali, Toralf Bernhard
dc.creator.authorTambave, Ganesh Jagannath
dc.creator.authorTveter, Trine Spedstad
dc.creator.authorUllaland, Kjetil
dc.creator.authorVelure, Arild
dc.creator.authorWagner, Boris
dc.creator.authorWikne, Jon Christopher
dc.creator.authorZhang, Hui
dc.creator.authorZhao, Chengxin
dc.creator.authorZhou, Zhuo
dc.creator.authorZhu, Hongsheng
dc.creator.authorALICE, Collaboration
cristin.unitcode185,15,4,0
cristin.unitnameFysisk institutt
cristin.ispublishedtrue
cristin.fulltextoriginal
cristin.qualitycode1
dc.identifier.cristin1566106
dc.identifier.bibliographiccitationinfo:ofi/fmt:kev:mtx:ctx&ctx_ver=Z39.88-2004&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.jtitle=Nuclear Physics A&rft.volume=967&rft.spage=468&rft.date=2017
dc.identifier.jtitleNuclear Physics A
dc.identifier.volume967
dc.identifier.startpage468
dc.identifier.endpage471
dc.identifier.doihttp://dx.doi.org/10.1016/j.nuclphysa.2017.07.011
dc.identifier.urnURN:NBN:no-67520
dc.type.documentTidsskriftartikkelen_US
dc.type.peerreviewedPeer reviewed
dc.source.issn0375-9474
dc.identifier.fulltextFulltext https://www.duo.uio.no/bitstream/handle/10852/64990/2/1-s2.0-S0375947417303299-main_HVL.pdf
dc.type.versionPublishedVersion


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