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@MISC{Collaboration:356816,
      author       = {{ALICE Collaboration}},
      title        = {{P}rompt and non-prompt {J}$/\psi$ production at
                      midrapidity in {P}b$-${P}b collisions at
                      $\sqrt{s_{\mathrm{{NN}}}}$ = 5.02 {T}e{V}},
      reportid     = {GSI-2025-00199},
      year         = {2024},
      note         = {Journal Article GSI record: GSI-2025-00198},
      abstract     = {The transverse momentum ($p_T$) and centrality dependence
                      of the nuclear modification factor $R_{AA}$ of prompt and
                      non-prompt J/$\psi$, the latter originating from the weak
                      decays of beauty hadrons, have been measured by the ALICE
                      collaboration in Pb--Pb collisions at 5.02 TeV. The
                      measurements are carried out through the e^+e^- decay
                      channel at midrapidity ($|y| $ 5~\GeVc, which becomes
                      stronger with increasing collision centrality. The results
                      are consistent with similar LHC measurements in the
                      overlapping $p_T$ intervals, and cover the kinematic region
                      down to $p_T$ = 1.5 \GeVc at midrapidity, not accessible by
                      other LHC experiments. The suppression of prompt J/$\psi$ in
                      central and semicentral collisions exhibits a decreasing
                      trend towards lower transverse momentum, described within
                      uncertainties by models implementing J/$\psi$ production
                      from recombination of c and $\overline{\rm c}$ quarks
                      produced independently in different partonic scatterings. At
                      high transverse momentum, transport models including
                      quarkonium dissociation are able to describe the suppression
                      for prompt J/$\psi$. For non-prompt J/$\psi$, the
                      suppression predicted by models including both collisional
                      and radiative processes for the computation of the
                      beauty-quark energy loss inside the quark--gluon plasma is
                      consistent with measurements within uncertainties.},
      cin          = {ALI / DTL / CIT / EXM / ALICE@CERN},
      cid          = {I:(DE-Ds200)ALI-20080822OR105 /
                      I:(DE-Ds200)DTL-20051214OR031 /
                      I:(DE-Ds200)CIT-20110310OR121 /
                      I:(DE-Ds200)EXM-20080818OR100 / I:(DE-Ds200)Coll-CERN-ALICE},
      pnm          = {612 - Cosmic Matter in the Laboratory (POF4-612) / HGS-HIRe
                      - HGS-HIRe for FAIR (HGS-HIRe) / SUC-GSI-Heidelberg -
                      Strategic university cooperation GSI-U Heidelberg
                      (SUC-GSI-HE) / SUC-GSI-Frankfurt - Strategic university
                      cooperation GSI-U Frankfurt/M (SUC-GSI-FR) /
                      SUC-GSI-Darmstadt - Strategic university cooperation GSI-TU
                      Darmstadt (SUC-GSI-DA) / STRONG-2020 - The strong
                      interaction at the frontier of knowledge: fundamental
                      research and applications (824093)},
      pid          = {G:(DE-HGF)POF4-612 / G:(DE-Ds200)HGS-HIRe /
                      G:(DE-Ds200)SUC-GSI-HE / G:(DE-Ds200)SUC-GSI-FR /
                      G:(DE-Ds200)SUC-GSI-DA / G:(EU-Grant)824093},
      experiment   = {EXP:(DE-H253)LHC-Exp-ALICE-20150101},
      typ          = {PUB:(DE-HGF)32},
      doi          = {10.17182/HEPDATA.146723},
      url          = {https://repository.gsi.de/record/356816},
}