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Quarkonia production as a function of charged-particle multiplicity in pp collisions at $\sqrt{s}=13$ TeV with ALICE
In pp collisions at LHC energies, heavy quarks are produced in initial hard scatterings and then these quarks hadronize in either open heavy-flavor hadrons or quarkonia (e.g. J/$\psi$, $\psi(2S)$, $\Upsilon$). The study of quarkonium production as a function of charged-particle multiplicity links so...
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Lenguaje: | eng |
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SISSA
2021
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Acceso en línea: | https://dx.doi.org/10.22323/1.382.0224 http://cds.cern.ch/record/2732997 |
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author | Ding, Yanchun |
author_facet | Ding, Yanchun |
author_sort | Ding, Yanchun |
collection | CERN |
description | In pp collisions at LHC energies, heavy quarks are produced in initial hard scatterings and then these quarks hadronize in either open heavy-flavor hadrons or quarkonia (e.g. J/$\psi$, $\psi(2S)$, $\Upsilon$). The study of quarkonium production as a function of charged-particle multiplicity links soft and hard processes and allows one to study their interplay. While a linear increase of quarkonium production as a function of charged-particle multiplicity can be reasonably well understood in the context of multi-parton interactions, the observation of deviations with respect to a linear increase requires a more detailed description of the collision. In this contribution, we will present the latest ALICE measurements at forward rapidity for J/$\psi$ and $\Upsilon$ production as a function of charged-particle multiplicity in pp collisions at $\sqrt{s}=13$ TeV. The first measurement of the double ratios of relative yield of $\Upsilon(2S)$ over $\Upsilon(1S)$ and J/$\psi$ over $\Upsilon(1S)$ as a function of charged-particle multiplicity will also be shown. |
id | cern-2732997 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2021 |
publisher | SISSA |
record_format | invenio |
spelling | cern-27329972021-10-11T10:04:24Zdoi:10.22323/1.382.0224http://cds.cern.ch/record/2732997engDing, YanchunQuarkonia production as a function of charged-particle multiplicity in pp collisions at $\sqrt{s}=13$ TeV with ALICEhep-exParticle Physics - Experimentnucl-exNuclear Physics - ExperimentIn pp collisions at LHC energies, heavy quarks are produced in initial hard scatterings and then these quarks hadronize in either open heavy-flavor hadrons or quarkonia (e.g. J/$\psi$, $\psi(2S)$, $\Upsilon$). The study of quarkonium production as a function of charged-particle multiplicity links soft and hard processes and allows one to study their interplay. While a linear increase of quarkonium production as a function of charged-particle multiplicity can be reasonably well understood in the context of multi-parton interactions, the observation of deviations with respect to a linear increase requires a more detailed description of the collision. In this contribution, we will present the latest ALICE measurements at forward rapidity for J/$\psi$ and $\Upsilon$ production as a function of charged-particle multiplicity in pp collisions at $\sqrt{s}=13$ TeV. The first measurement of the double ratios of relative yield of $\Upsilon(2S)$ over $\Upsilon(1S)$ and J/$\psi$ over $\Upsilon(1S)$ as a function of charged-particle multiplicity will also be shown.In pp collisions at LHC energies, heavy quarks are produced in initial hard scatterings and then these quarks hadronize in either open heavy-flavor hadrons or quarkonia (e.g. J/$\psi$, $\psi(2S)$, $\Upsilon$). The study of quarkonium production as a function of charged-particle multiplicity links soft and hard processes and allows one to study their interplay. While a linear increase of quarkonium production as a function of charged-particle multiplicity can be reasonably well understood in the context of multi-parton interactions, the observation of deviations with respect to a linear increase requires a more detailed description of the collision.In this contribution, we will present the latest ALICE measurements at forward rapidity for J/$\psi$ and $\Upsilon$ production as a function of charged-particle multiplicity in pp collisions at $\sqrt{s}=13$ TeV. The first measurement of the double ratios of relative yield of $\Upsilon(2S)$ over $\Upsilon(1S)$ and J/$\psi$ over $\Upsilon(1S)$ as a function of charged-particle multiplicity will also be shown.SISSAarXiv:2009.10782oai:cds.cern.ch:27329972021 |
spellingShingle | hep-ex Particle Physics - Experiment nucl-ex Nuclear Physics - Experiment Ding, Yanchun Quarkonia production as a function of charged-particle multiplicity in pp collisions at $\sqrt{s}=13$ TeV with ALICE |
title | Quarkonia production as a function of charged-particle multiplicity in pp collisions at $\sqrt{s}=13$ TeV with ALICE |
title_full | Quarkonia production as a function of charged-particle multiplicity in pp collisions at $\sqrt{s}=13$ TeV with ALICE |
title_fullStr | Quarkonia production as a function of charged-particle multiplicity in pp collisions at $\sqrt{s}=13$ TeV with ALICE |
title_full_unstemmed | Quarkonia production as a function of charged-particle multiplicity in pp collisions at $\sqrt{s}=13$ TeV with ALICE |
title_short | Quarkonia production as a function of charged-particle multiplicity in pp collisions at $\sqrt{s}=13$ TeV with ALICE |
title_sort | quarkonia production as a function of charged-particle multiplicity in pp collisions at $\sqrt{s}=13$ tev with alice |
topic | hep-ex Particle Physics - Experiment nucl-ex Nuclear Physics - Experiment |
url | https://dx.doi.org/10.22323/1.382.0224 http://cds.cern.ch/record/2732997 |
work_keys_str_mv | AT dingyanchun quarkoniaproductionasafunctionofchargedparticlemultiplicityinppcollisionsatsqrts13tevwithalice |