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@ARTICLE{Acharya:250889,
      author       = {Acharya, Shreyasi and others},
      title        = {{P}roduction of {K}$^{*}(892)^{0}$ and $\phi(1020)$ in pp
                      and {P}b-{P}b collisions at $\sqrt{s_{\rm {NN}}} = 5.02$
                      {T}e{V}},
      journal      = {Physical review / C},
      volume       = {106},
      number       = {3},
      issn         = {2469-9985},
      address      = {Woodbury, NY},
      publisher    = {Inst.},
      reportid     = {GSI-2023-00115, arXiv:2106.13113. CERN-EP-2021-101},
      pages        = {034907},
      year         = {2022},
      note         = {ISSN 2469-9993 not unique: **2 hits**.figures at
                      http://alice-publications.web.cern.ch/node/7203SCOAP3
                      ccby4.0},
      abstract     = {The production of K$^{*}(892)^{0}$ and $\phi(1020)$ mesons
                      in proton-proton (pp) and lead-lead (Pb-Pb) collisions at
                      $\sqrt{s_\mathrm{NN}} = 5.02$ TeV has been measured using
                      the ALICE detector at the Large Hadron Collider (LHC). The
                      transverse momentum ($p_{\mathrm{T}}$) distributions of
                      K$^{*}(892)^{0}$ and $\phi(1020)$ mesons have been measured
                      at midrapidity $(|y|<0.5)$ up to $p_{\mathrm{T}} = 20$
                      GeV$/c$ in inelastic pp collisions and for several Pb-Pb
                      collision centralities. The collision centrality and
                      collision energy dependence of the average transverse
                      momenta agree with the radial flow scenario observed with
                      stable hadrons, showing that the effect is stronger for more
                      central collisions and higher collision energies. The
                      $\mathrm{K^{*0}/K}$ ratio is found to be suppressed in Pb-Pb
                      collisions relative to pp collisions: this indicates a loss
                      of the measured K$^{*}(892)^{0}$ signal due to rescattering
                      of its decay products in the hadronic phase. In contrast,
                      for the longer-lived $\phi(1020)$ mesons, no such
                      suppression is observed. The nuclear modification factors
                      ($R_{\rm AA}$) of K$^{*}(892)^{0}$ and $\phi(1020)$ mesons
                      are calculated using pp reference spectra at the same
                      collision energy. In central Pb-Pb collisions for $p_{\rm T}
                      > 8$ GeV$/c$, the $R_{\rm AA}$ values of K$^{*}(892)^{0}$
                      and $\phi(1020)$ are below unity and observed to be similar
                      to those of pions, kaons, and (anti)protons. The $R_{\rm
                      AA}$ values at high $p_{\mathrm T}$ for K$^{*}(892)^{0}$ and
                      $\phi(1020)$ mesons are in agreement within uncertainties
                      for $\sqrt{s_\mathrm{NN}} = 5.02$ and 2.76 TeV.},
      keywords     = {K*(892)0: production (INSPIRE) / Phi(1020): production
                      (INSPIRE) / heavy ion: scattering (INSPIRE) / hadron:
                      stability (INSPIRE) / p p: scattering (INSPIRE) / heavy ion,
                      scattering (INSPIRE) / hadron, stability (INSPIRE) / meson
                      (INSPIRE) / GeV (INSPIRE) / TeV (INSPIRE) / transverse
                      momentum (INSPIRE) / CERN LHC Coll (INSPIRE) / suppression
                      (INSPIRE) / flow (INSPIRE) / ALICE (INSPIRE) / nucleus
                      (INSPIRE) / energy dependence (INSPIRE) / impact parameter
                      (INSPIRE) / experimental results (INSPIRE) / 2760
                      GeV-cms/nucleon (INSPIRE) / 5020 GeV-cms/nucleon (INSPIRE)},
      cin          = {ALI / DTL / CIT / EXM / ALICE@CERN},
      ddc          = {530},
      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)},
      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},
      experiment   = {EXP:(DE-H253)LHC-Exp-ALICE-20150101},
      typ          = {PUB:(DE-HGF)16},
      eprint       = {2106.13113},
      howpublished = {arXiv:2106.13113},
      archivePrefix = {arXiv},
      SLACcitation = {$\%\%CITATION$ = $arXiv:2106.13113;\%\%$},
      UT           = {WOS:000890202900004},
      doi          = {10.1103/PhysRevC.106.034907},
      url          = {https://repository.gsi.de/record/250889},
}