Please use this identifier to cite or link to this item: https://dspace.iiti.ac.in/handle/123456789/11953
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dc.contributor.authorBailung, Yoshinien_US
dc.contributor.authorBehera, Debadattaen_US
dc.contributor.authorDeb, Soumenen_US
dc.date.accessioned2023-06-24T13:02:14Z-
dc.date.available2023-06-24T13:02:14Z-
dc.date.issued2023-
dc.identifier.citationAcharya, S., Adamová, D., Adler, A., Aglieri Rinella, G., Agnello, M., Agrawal, N., . . . Zurlo, N. (2023). Σ (1385) ± resonance production in Pb–Pb collisions at √sNN=5.02 TeV. European Physical Journal C, 83(5) doi:10.1140/epjc/s10052-023-11475-1en_US
dc.identifier.issn1434-6044-
dc.identifier.otherEID(2-s2.0-85159950234)-
dc.identifier.urihttps://doi.org/10.1140/epjc/s10052-023-11475-1-
dc.identifier.urihttps://dspace.iiti.ac.in/handle/123456789/11953-
dc.description.abstractHadronic resonances are used to probe the hadron gas produced in the late stage of heavy-ion collisions since they decay on the same timescale, of the order of 1–10 fm/c, as the decoupling time of the system. In the hadron gas, (pseudo)elastic scatterings among the products of resonances that decayed before the kinetic freeze-out and regeneration processes counteract each other, the net effect depending on the resonance lifetime, the duration of the hadronic phase, and the hadronic cross sections at play. In this context, the Σ (1385) ± particle is of particular interest as models predict that regeneration dominates over rescattering despite its relatively short lifetime of about 5.5 fm/c. The first measurement of the Σ (1385) ± resonance production at midrapidity in Pb–Pb collisions at sNN=5.02 TeV with the ALICE detector is presented in this Letter. The resonances are reconstructed via their hadronic decay channel, Λ π , as a function of the transverse momentum (pT) and the collision centrality. The results are discussed in comparison with the measured yield of pions and with expectations from the statistical hadronization model as well as commonly employed event generators, including PYTHIA8/Angantyr and EPOS3 coupled to the UrQMD hadronic cascade afterburner. None of the models can describe the data. For Σ (1385) ± , a similar behaviour as K ∗(892) is observed in data unlike the predictions of EPOS3 with afterburner. © 2023, CERN for the benefit of the ALICE Collaboration.en_US
dc.language.isoenen_US
dc.publisherInstitute for Ionicsen_US
dc.sourceEuropean Physical Journal Cen_US
dc.titleΣ (1385) ± resonance production in Pb–Pb collisions at √sNN=5.02 TeVen_US
dc.typeJournal Articleen_US
dc.rights.licenseAll Open Access, Gold-
Appears in Collections:Department of Physics

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