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DC Field | Value | Language |
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dc.contributor.author | Bailung, Yoshini | en_US |
dc.contributor.author | Behera, Debadatta | en_US |
dc.contributor.author | Deb, Soumen | en_US |
dc.date.accessioned | 2023-11-03T12:30:22Z | - |
dc.date.available | 2023-11-03T12:30:22Z | - |
dc.date.issued | 2023 | - |
dc.identifier.citation | Acharya, S., Adamová, D., Adler, A., Aglieri Rinella, G., Agnello, M., Agrawal, N., Ahammed, Z., Ahmad, S., Ahn, S. U., Ahuja, I., Akindinov, A., Al-Turany, M., Aleksandrov, D., Alessandro, B., Alfanda, H. M., Alfaro Molina, R., Ali, B., Ali, Y., Alici, A., … The ALICE collaboration. (2023c). Measurement of ψ (2S) production as a function of charged-particle pseudorapidity density in pp collisions at √s = 13 TeV and p–Pb collisions at √sNN = 8.16 TeV with ALICE at the LHC. Journal of High Energy Physics. Scopus. https://doi.org/10.1007/JHEP06(2023)147 | en_US |
dc.identifier.issn | 1029-8479 | - |
dc.identifier.other | EID(2-s2.0-85163024333) | - |
dc.identifier.uri | https://doi.org/10.1007/JHEP06(2023)147 | - |
dc.identifier.uri | https://dspace.iiti.ac.in/handle/123456789/12416 | - |
dc.description.abstract | Production of inclusive charmonia in pp collisions at center-of-mass energy of s = 13 TeV and p–Pb collisions at center-of-mass energy per nucleon pair of sNN = 8.16 TeV is studied as a function of charged-particle pseudorapidity density with ALICE. Ground and excited charmonium states (J/ψ, ψ(2S)) are measured from their dimuon decays in the interval of rapidity in the center-of-mass frame 2.5 < | en_US |
dc.description.abstract | y cms < | en_US |
dc.description.abstract | 4.0 for pp collisions, and 2.03 < | en_US |
dc.description.abstract | y cms < | en_US |
dc.description.abstract | 3.53 and −4.46 < | en_US |
dc.description.abstract | y cms < | en_US |
dc.description.abstract | −2.96 for p–Pb collisions. The charged-particle pseudorapidity density is measured around midrapidity (|η| < | en_US |
dc.description.abstract | 1.0). In pp collisions, the measured charged-particle multiplicity extends to about six times the average value, while in p-Pb collisions at forward (backward) rapidity a multiplicity corresponding to about three (four) times the average is reached. The ψ(2S) yield increases with the charged-particle pseudorapidity density. The ratio of ψ(2S) over J/ψ yield does not show a significant multiplicity dependence in either colliding system, suggesting a similar behavior of J/ψ and ψ(2S) yields with respect to charged-particle pseudorapidity density. Results for the ψ(2S) yield and its ratio with respect to J/ψ agree with available model calculations. [Figure not available: see fulltext.]. © 2023, The Author(s). | en_US |
dc.language.iso | en | en_US |
dc.publisher | Springer Science and Business Media Deutschland GmbH | en_US |
dc.source | Journal of High Energy Physics | en_US |
dc.subject | Jets and Jet Substructure | en_US |
dc.subject | Properties of Hadrons | en_US |
dc.title | Measurement of ψ (2S) production as a function of charged-particle pseudorapidity density in pp collisions at √s = 13 TeV and p–Pb collisions at √sNN = 8.16 TeV with ALICE at the LHC | en_US |
dc.type | Journal Article | en_US |
dc.rights.license | All Open Access, Gold, Green | - |
Appears in Collections: | Department of Physics |
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