Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/10424
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dc.contributor.authorCMS Collaborationen_US
dc.contributor.authorChekhovsky, V.en_US
dc.contributor.authorACHARYA, S.en_US
dc.contributor.authorALPANA, A.en_US
dc.contributor.authorDUBE, SOURABHen_US
dc.contributor.authorGOMBER, B.en_US
dc.contributor.authorHAZARIKA, P.en_US
dc.contributor.authorKANSAL, B.en_US
dc.contributor.authorLAHA, A.en_US
dc.contributor.authorSAHU, B.en_US
dc.contributor.authorSHARMA, SEEMAen_US
dc.contributor.authorVAISH, K. Y. et al.en_US
dc.date.accessioned2025-09-25T05:36:42Z-
dc.date.available2025-09-25T05:36:42Z-
dc.date.issued2025-07en_US
dc.identifier.citationJournal of High Energy Physics, 2025(07), 118.en_US
dc.identifier.issn1029-8479en_US
dc.identifier.urihttps://doi.org/10.1007/JHEP07(2025)118en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/10424-
dc.description.abstractThe first measurement of the dijet transverse momentum balance xj in proton-lead (pPb) collisions at a nucleon-nucleon center-of-mass energy of = 8.16 TeV is presented. The xj observable, defined as the ratio of the subleading over leading jet transverse momentum in a dijet pair, is used to search for jet quenching effects. The data, corresponding to an integrated luminosity of 174.6 nb−1, were collected with the CMS detector in 2016. The xj distributions and their average values are studied as functions of the charged-particle multiplicity of the events and for various dijet rapidity selections. The latter enables probing hard scattering of partons carrying distinct nucleon momentum fractions x in the proton- and lead-going directions. The former, aided by the high-multiplicity triggers, allows probing for potential jet quenching effects in high-multiplicity events (with up to 400 charged particles), for which collective phenomena consistent with quark-gluon plasma (QGP) droplet formation were previously observed. The ratios of xj distributions for high- to low-multiplicity events are used to quantify the possible medium effects. These ratios are consistent with simulations of the hard-scattering process that do not include QGP production. These measurements set an upper limit on medium-induced energy loss of the subleading jet of 1.26% of its transverse momentum at the 90% confidence level in high multiplicity pPb events.en_US
dc.language.isoenen_US
dc.publisherSpringer Natureen_US
dc.subjectHeavy Ion Experimentsen_US
dc.subjectJetsen_US
dc.subject2025-SEP-WEEK3en_US
dc.subjectTOC-SEP-2025en_US
dc.subject2025en_US
dc.titleSearch for jet quenching with dijets from high-multiplicity pPb collisions at √sNN=8.16 TeVen_US
dc.typeArticleen_US
dc.contributor.departmentDept. of Physicsen_US
dc.identifier.sourcetitleJournal of High Energy Physicsen_US
dc.publication.originofpublisherForeignen_US
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