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Fragmentation of jets containing a prompt J$/\psi$ meson in PbPb and pp collisions at $\sqrt{s_\mathrm{NN}} =$ 5.02 TeV

The CMS collaboration
CMS-HIN-19-007, 2021.

Abstract
Jets containing a prompt J$/\psi$ meson are studied in lead-lead collisions at a nucleon-nucleon center-of-mass energy of 5.02 TeV, using the CMS detector at the LHC. Jets are selected to be in the transverse momentum range of 30 $\lt p_\mathrm{T} \lt$ 40 GeV. The J$/\psi$ yield in these jets is evaluated as a function of the jet fragmentation variable $z$, the ratio of the J$/\psi$$p_\mathrm{T} $ to the jet $p_\mathrm{T}$. The nuclear modification factor, $R_\mathrm{AA}$, is then derived by comparing the yield in lead-lead collisions to the corresponding expectation based on proton-proton data, at the same nucleon-nucleon center-of-mass energy. The suppression of the J$/\psi$ yield shows a dependence on $z$, indicating that the interaction of the J$/\psi$ with the quark-gluon plasma formed in heavy ion collisions depends on the fragmentation that gives rise to the J$/\psi$ meson.

  • Figure 4

    Data from Figure 4.

    10.17182/hepdata.95234.v1/t1

    Normalized $z$ distribution in pp collisions.

  • Figure 5-a

    Data from Figure 5-a.

    10.17182/hepdata.95234.v1/t2

    The J/$\psi$ differential cross section in pp and the $T_{AA}$-scaled yield in PbPb collisions, as a function of $z$.

  • Figure 5-b

    Data from Figure 5-b.

    10.17182/hepdata.95234.v1/t3

    The nuclear modification factor R$_{\rm AA}$, as a function of $z$.

  • Figure 6

    Data from Figure 6.

    10.17182/hepdata.95234.v1/t4

    The nuclear modification factor R$_{\rm AA}$, as a function of $z$ in the 0-20 and 20-30 collisions centrality ranges.

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