CERN Accelerating science

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002779925 005__ 20240817063418.0
002779925 0248_ $$aoai:cds.cern.ch:2779925$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
002779925 0247_ $$2DOI$$9arXiv$$a10.1007/JHEP11(2021)181$$qpublication
002779925 037__ $$9arXiv$$aarXiv:2109.00220$$chep-ex
002779925 037__ $$9arXiv:reportnumber$$aLHCb-PAPER-2021-020
002779925 037__ $$aCERN-EP-2021-156
002779925 035__ $$9arXiv$$aoai:arXiv.org:2109.00220
002779925 035__ $$9Inspire$$aoai:inspirehep.net:1915030$$d2024-08-16T08:58:10Z$$h2024-08-17T02:58:57Z$$mmarcxml$$ttrue$$uhttps://inspirehep.net/api/oai2d
002779925 035__ $$9Inspire$$a1915030
002779925 041__ $$aeng
002779925 088__ $$9LHCB-PAPER-2021-020-003
002779925 088__ $$aLHCB-PAPER-2021-020
002779925 100__ $$aAaij, R.$$iINSPIRE-00258707$$jORCID:0000-0003-0533-1952
002779925 245__ $$aMeasurement of $J/\psi$ production cross-sections in $pp$ collisions at $\sqrt{s}=5$ TeV
002779925 260__ $$c2021
002779925 269__ $$aGeneva$$bCERN$$c02 Sep 2021
002779925 300__ $$a34 p
002779925 500__ $$9arXiv$$aAll figures and tables, along with any supplementary material and
 additional information, are available at
 https://cern.ch/lhcbproject/Publications/p/LHCb-PAPER-2021-020.html (LHCb
 public pages)
002779925 520__ $$aThe production cross-sections of $J/\psi$ mesons in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}=5$ TeV are measured using a data sample corresponding to an integrated luminosity of $9.13\pm0.18~\text{pb}^{-1}$, collected by the LHCb experiment. The cross-sections are measured differentially as a function of transverse momentum, $p_{\text{T}}$, and rapidity, $y$, and separately for $J/\psi$ mesons produced promptly and from beauty hadron decays (nonprompt). With the assumption of unpolarised $J/\psi$ mesons, the production cross-sections integrated over the kinematic range $0 < p_{\text{T}}<20~\text{GeV}/c$ and $2.0 < y<4.5$ are $$^{\sigma} \text{prompt} \ J/\psi = 8.154\pm0.010\pm0.283~\mu\text{b},$$  $$^{\sigma} \text{nonprompt} \ J/\psi = 0.820\pm0.003\pm0.034~\mu\text{b},$$  where the first uncertainties are statistical and the second systematic. These cross-sections are compared with those at $\sqrt{s}=8$ TeV and $13$ TeV, and are used to update the measurement of the nuclear modification factor in proton-lead collisions for $J/\psi$ mesons at a centre-of-mass energy per nucleon pair of $\sqrt{s_{\text{NN}}}=5$ TeV. The results are compared with theoretical predictions.
002779925 520__ $$9arXiv$$aThe production cross-sections of $J/\psi$ mesons in proton-proton collisions at a centre-of-mass energy of $\sqrt{s}=5$ TeV are measured using a data sample corresponding to an integrated luminosity of $9.13\pm0.18~\text{pb}^{-1}$, collected by the LHCb experiment. The cross-sections are measured differentially as a function of transverse momentum, $p_{\text{T}}$, and rapidity, $y$, and separately for $J/\psi$ mesons produced promptly and from beauty hadron decays (nonprompt). With the assumption of unpolarised $J/\psi$ mesons, the production cross-sections integrated over the kinematic range $0<p_{\text{T}}<20~\text{GeV}/c$ and $2.0<y<4.5$ are $8.154\pm0.010\pm0.283~\mu\text{b}$ for prompt $J/\psi$ mesons and $0.820\pm0.003\pm0.034~\mu\text{b}$ for nonprompt $J/\psi$ mesons, where the first uncertainties are statistical and the second systematic. These cross-sections are compared with those at $\sqrt{s}=8$ TeV and $13$ TeV, and are used to update the measurement of the nuclear modification factor in proton-lead collisions for $J/\psi$ mesons at a centre-of-mass energy per nucleon pair of $\sqrt{s_{\text{NN}}}=5$ TeV. The results are compared with theoretical predictions.
002779925 540__ $$3Preprint$$aCC-BY-4.0$$uhttp://creativecommons.org/licenses/by/4.0/
002779925 540__ $$3Publication$$aCC-BY-4.0$$fSCOAP3$$uhttp://creativecommons.org/licenses/by/4.0/
002779925 542__ $$3Preprint$$dCERN$$g2021
002779925 542__ $$3Publication$$dCERN$$g2021
002779925 595__ $$aFor annual report
002779925 65017 $$2SzGeCERN$$aParticle Physics - Experiment
002779925 6531_ $$9CERN$$aQCD
002779925 6531_ $$9CERN$$aquarkonium
002779925 6531_ $$9CERN$$aheavy quark production
002779925 693__ $$aCERN LHC$$eLHCb
002779925 690C_ $$aLHCb_Papers
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002779925 700__ $$aSierra, C. Vázquez$$iINSPIRE-00392390
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002779925 700__ $$aVelthuis, J.J.$$iINSPIRE-00318722
002779925 700__ $$aVeltri, M.$$iINSPIRE-00258261$$jORCID:0000-0001-7917-9661
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002779925 700__ $$aVesterinen, M.$$iINSPIRE-00014030$$jORCID:0000-0001-7717-2765
002779925 700__ $$aVieira, D.$$iINSPIRE-00341866$$jORCID:0000-0001-9511-2846
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002779925 700__ $$aWang, Jianchun$$iINSPIRE-00262940$$uBeijing, Inst. High Energy Phys.
002779925 700__ $$aWang, Jianqiao$$uTsinghua U., Beijing, CHEP
002779925 700__ $$aWang, Jike$$jORCID:0000-0001-6711-4465$$uWuhan U.
002779925 700__ $$aWang, M.
002779925 700__ $$aWang, R.$$jORCID:0000-0002-2629-4735
002779925 700__ $$aWang, Y.
002779925 700__ $$aWang, Zhenzi$$uZurich U.
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002779925 700__ $$aWard, J.A.
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002779925 700__ $$aWatson, N.K.$$iINSPIRE-00146172$$jORCID:0000-0002-8142-4678
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002779925 700__ $$aWilson, F.F.$$iINSPIRE-00136130$$jORCID:0000-0002-5552-0842
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002779925 700__ $$aXu, Q.
002779925 700__ $$aXu, Zehua$$uPeking U., SKLNPT
002779925 700__ $$aXu, Zhihao$$uBeijing, GUCAS
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002779925 700__ $$aYang, S.$$jORCID:0000-0003-2505-0365
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002779925 700__ $$aYang, Zishuo$$uMaryland U., College Park
002779925 700__ $$aYao, Y.$$iINSPIRE-00582891
002779925 700__ $$aYeomans, L.E.
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002779925 700__ $$aZhang, L.$$iINSPIRE-00043581
002779925 700__ $$aZhang, Shulei$$jORCID:0000-0002-9794-4088$$uHunan U.
002779925 700__ $$aZhang, Shunan$$jORCID:0000-0002-2385-0767$$uPeking U., SKLNPT
002779925 700__ $$aZhang, Yanxi$$iINSPIRE-00257306$$uPeking U., SKLNPT
002779925 700__ $$aZhang, Yu$$iINSPIRE-00469638$$uOxford U.
002779925 700__ $$aZharkova, A.
002779925 700__ $$aZhelezov, A.$$iINSPIRE-00217483
002779925 700__ $$aZheng, Y.$$iINSPIRE-00138380
002779925 700__ $$aZhou, T.
002779925 700__ $$aZhou, X.
002779925 700__ $$aZhou, Y.
002779925 700__ $$aZhovkovska, V.$$jORCID:0000-0002-9812-4508
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002779925 700__ $$aZhu, Z.$$jORCID:0000-0002-9211-3867
002779925 700__ $$aZhukov, V.$$iINSPIRE-00170284
002779925 700__ $$aZonneveld, J.B.
002779925 700__ $$aZou, Q.$$jORCID:0000-0003-0038-5038
002779925 700__ $$aZucchelli, S.$$iINSPIRE-00040570
002779925 700__ $$aZuliani, D.$$jORCID:0000-0002-1478-4593
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002779925 710__ $$gLHCb Collaboration
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002779925 8564_ $$82320024$$s957423$$uhttps://cds.cern.ch/record/2779925/files/LHCb-PAPER-2021-020.pdf$$yFulltext$$zStamped by WebSubmit: 02/09/2021
002779925 8564_ $$82320023$$s977784$$uhttps://cds.cern.ch/record/2779925/files/LHCb-PAPER-2021-020-figures.zip$$yRelated data file(s)
002779925 8564_ $$82320052$$s236390$$uhttps://cds.cern.ch/record/2779925/files/LHCb-PAPER-2021-020-supplementary.zip$$ySupplementary information
002779925 8564_ $$82320144$$s13125$$uhttps://cds.cern.ch/record/2779925/files/Fig7a.png$$y00011 Ratios of differential cross-sections between 13\tev and 5\tev measurements as a function of (left) \pt and (right) $y$ for prompt \jpsi mesons compared with NRQCD and CGC calculations~\cite{Ma:2010yw,Ma:2014mri}. Uncertainties due to the LDMEs determination, renormalisation scales, and factorisation scales are included in the NRQCD and CGC calculations.
002779925 8564_ $$82320145$$s77860$$uhttps://cds.cern.ch/record/2779925/files/Fig4b.png$$y00007 Differential cross-sections (left) $\deriv\sigma/\deriv\pt$ and (right) $\deriv\sigma/\deriv y$ for nonprompt \jpsi mesons compared with FONLL calculations~\cite{Cacciari:2012ny,Cacciari:2015fta}. The orange band shows the total FONLL calculation uncertainty; the violet band shows the uncertainties of PDFs and that due to \bquark-quark mass added in quadrature; the blue band shows only the uncertainties on PDFs.
002779925 8564_ $$82320146$$s47401$$uhttps://cds.cern.ch/record/2779925/files/Fig4a.png$$y00006 Differential cross-sections (left) $\deriv\sigma/\deriv\pt$ and (right) $\deriv\sigma/\deriv y$ for nonprompt \jpsi mesons compared with FONLL calculations~\cite{Cacciari:2012ny,Cacciari:2015fta}. The orange band shows the total FONLL calculation uncertainty; the violet band shows the uncertainties of PDFs and that due to \bquark-quark mass added in quadrature; the blue band shows only the uncertainties on PDFs.
002779925 8564_ $$82320147$$s46709$$uhttps://cds.cern.ch/record/2779925/files/Fig8b.png$$y00014 Ratios of differential cross-sections between 8\tev and 5\tev measurements as a function of (left) \pt and (right) $y$ for nonprompt \jpsi mesons compared with FONLL calculations~\cite{Cacciari:2012ny,Cacciari:2015fta}. The orange band shows the total FONLL calculation uncertainty; the violet band shows the uncertainties on PDFs and that due to \bquark-quark mass added in quadrature; the red band shows only the uncertainty due to the \bquark-quark mass.
002779925 8564_ $$82320148$$s885102$$uhttps://cds.cern.ch/record/2779925/files/2109.00220.pdf$$yFulltext
002779925 8564_ $$82320149$$s12980$$uhttps://cds.cern.ch/record/2779925/files/Fig2b.png$$y00003 Differential cross-sections for (left) prompt and (right) nonprompt \jpsi mesons as a function of \pt in intervals of $y$. The error bars represent the total uncertainties, which are partially correlated between intervals.
002779925 8564_ $$82320150$$s11400$$uhttps://cds.cern.ch/record/2779925/files/Fig7b.png$$y00012 Ratios of differential cross-sections between 13\tev and 5\tev measurements as a function of (left) \pt and (right) $y$ for prompt \jpsi mesons compared with NRQCD and CGC calculations~\cite{Ma:2010yw,Ma:2014mri}. Uncertainties due to the LDMEs determination, renormalisation scales, and factorisation scales are included in the NRQCD and CGC calculations.
002779925 8564_ $$82320151$$s45519$$uhttps://cds.cern.ch/record/2779925/files/Fig8a.png$$y00013 Ratios of differential cross-sections between 8\tev and 5\tev measurements as a function of (left) \pt and (right) $y$ for nonprompt \jpsi mesons compared with FONLL calculations~\cite{Cacciari:2012ny,Cacciari:2015fta}. The orange band shows the total FONLL calculation uncertainty; the violet band shows the uncertainties on PDFs and that due to \bquark-quark mass added in quadrature; the red band shows only the uncertainty due to the \bquark-quark mass.
002779925 8564_ $$82320152$$s31587$$uhttps://cds.cern.ch/record/2779925/files/Fig5.png$$y00008 Fraction of nonprompt \jpsi mesons as a function of \pt in intervals of $y$. The error bars represent the total uncertainties, which are partially correlated between intervals.
002779925 8564_ $$82320153$$s12937$$uhttps://cds.cern.ch/record/2779925/files/Fig2a.png$$y00002 Differential cross-sections for (left) prompt and (right) nonprompt \jpsi mesons as a function of \pt in intervals of $y$. The error bars represent the total uncertainties, which are partially correlated between intervals.
002779925 8564_ $$82320154$$s57707$$uhttps://cds.cern.ch/record/2779925/files/Fig9a.png$$y00015 Ratios of differential cross-sections between 13\tev and 5\tev measurements as a function of (left) \pt and (right) $y$ for nonprompt \jpsi mesons compared with FONLL calculations~\cite{Cacciari:2012ny,Cacciari:2015fta}. The orange band shows the total FONLL calculation uncertainty; the violet band shows the uncertainties on PDFs and that due to \bquark-quark mass added in quadrature; the red band shows only the uncertainty due to \bquark-quark mass.
002779925 8564_ $$82320155$$s69500$$uhttps://cds.cern.ch/record/2779925/files/Fig9b.png$$y00016 Ratios of differential cross-sections between 13\tev and 5\tev measurements as a function of (left) \pt and (right) $y$ for nonprompt \jpsi mesons compared with FONLL calculations~\cite{Cacciari:2012ny,Cacciari:2015fta}. The orange band shows the total FONLL calculation uncertainty; the violet band shows the uncertainties on PDFs and that due to \bquark-quark mass added in quadrature; the red band shows only the uncertainty due to \bquark-quark mass.
002779925 8564_ $$82320156$$s36927$$uhttps://cds.cern.ch/record/2779925/files/Fig3a.png$$y00004 Differential cross-sections (left) $\deriv\sigma/\deriv\pt$ and (right) $\deriv\sigma/\deriv y$ for prompt \jpsi mesons compared with NRQCD and CGC calculations~\cite{Ma:2010yw,Ma:2014mri}. Uncertainties due to LDMEs determination, renormalisation scales, and factorisation scales are included in the NRQCD and CGC predictions.
002779925 8564_ $$82320157$$s12505$$uhttps://cds.cern.ch/record/2779925/files/Fig6a.png$$y00009 Ratios of differential cross-sections between 8\tev and 5\tev measurements as a function of (left) \pt and (right) $y$ for prompt \jpsi mesons compared with NRQCD and CGC calculations~\cite{Ma:2010yw,Ma:2014mri}. Uncertainties due to the LDMEs determination, renormalisation scales, and factorisation scales are included in the NRQCD and CGC calculations.
002779925 8564_ $$82320158$$s77390$$uhttps://cds.cern.ch/record/2779925/files/Fig3b.png$$y00005 Differential cross-sections (left) $\deriv\sigma/\deriv\pt$ and (right) $\deriv\sigma/\deriv y$ for prompt \jpsi mesons compared with NRQCD and CGC calculations~\cite{Ma:2010yw,Ma:2014mri}. Uncertainties due to LDMEs determination, renormalisation scales, and factorisation scales are included in the NRQCD and CGC predictions.
002779925 8564_ $$82320159$$s10851$$uhttps://cds.cern.ch/record/2779925/files/Fig6b.png$$y00010 Ratios of differential cross-sections between 8\tev and 5\tev measurements as a function of (left) \pt and (right) $y$ for prompt \jpsi mesons compared with NRQCD and CGC calculations~\cite{Ma:2010yw,Ma:2014mri}. Uncertainties due to the LDMEs determination, renormalisation scales, and factorisation scales are included in the NRQCD and CGC calculations.
002779925 8564_ $$82320160$$s53968$$uhttps://cds.cern.ch/record/2779925/files/Fig10a.png$$y00017 Nuclear modification factor $R_{p\text{Pb}}$ as a function of $y$ for (left) prompt and (right) nonprompt \jpsi mesons, together with the theoretical predictions from (yellow dashed line and brown band) Ref.~\cite{Ferreiro:2013pua}, (blue band) Ref.~\cite{Albacete:2013ei}, and (violet solid line with band) Ref.~\cite{Arleo:2012rs,Arleo:2012hn}. In the data points the full error bars represent the statistical and systematic uncertainties added in quadrature, while the smaller ones represent the statistical uncertainties.
002779925 8564_ $$82320161$$s47327$$uhttps://cds.cern.ch/record/2779925/files/Fig1a.png$$y00000 Distributions of (left) invariant mass and (right) pseudoproper time of the \jpsi candidate for an example interval corresponding to $2<\pt<3\gevc$ and $3.0<y<3.5$. Projections of the two-dimensional fit are also shown.
002779925 8564_ $$82320162$$s54224$$uhttps://cds.cern.ch/record/2779925/files/Fig1b.png$$y00001 Distributions of (left) invariant mass and (right) pseudoproper time of the \jpsi candidate for an example interval corresponding to $2<\pt<3\gevc$ and $3.0<y<3.5$. Projections of the two-dimensional fit are also shown.
002779925 8564_ $$82320163$$s12046$$uhttps://cds.cern.ch/record/2779925/files/Fig10b.png$$y00018 Nuclear modification factor $R_{p\text{Pb}}$ as a function of $y$ for (left) prompt and (right) nonprompt \jpsi mesons, together with the theoretical predictions from (yellow dashed line and brown band) Ref.~\cite{Ferreiro:2013pua}, (blue band) Ref.~\cite{Albacete:2013ei}, and (violet solid line with band) Ref.~\cite{Arleo:2012rs,Arleo:2012hn}. In the data points the full error bars represent the statistical and systematic uncertainties added in quadrature, while the smaller ones represent the statistical uncertainties.
002779925 8564_ $$82402302$$s756913$$uhttps://cds.cern.ch/record/2779925/files/JHEP11(2021)181.pdf$$yFulltext from publisher
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