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@ARTICLE{Acharya:250925,
      author       = {Acharya, Shreyasi and others},
      title        = {{N}uclear modification factor of light neutral-meson
                      spectra up to high transverse momentum in p–{P}b
                      collisions at $\sqrt{s_{\rm {NN}}}$ = 8.16 {T}e{V}},
      journal      = {Physics letters / B},
      volume       = {827},
      issn         = {0031-9163},
      address      = {Amsterdam},
      publisher    = {North-Holland Publ.},
      reportid     = {GSI-2023-00137, arXiv:2104.03116. CERN-EP-2021-053},
      pages        = {136943},
      year         = {2022},
      note         = {Phys. Lett. B 827 (2022) 136943. 19 pages, 4 captioned
                      figures, 2 tables, authors from page 14, published version,
                      figures at this
                      http://alice-publications.web.cern.ch/node/7044SCOAP3 . This
                      article is licensed under a Creative Commons Attribution 4.0
                      International License},
      abstract     = {Neutral pion (π$^0$) and η meson production cross
                      sections were measured up to unprecedentedly high transverse
                      momenta (p$_T$) in p–Pb collisions at $\sqrt{s_{\rm NN}}$
                      = 8.16TeV. The mesons were reconstructed via their
                      two-photon decay channel in the rapidity interval −1.3 < y
                      < 0.3 in the ranges of 0.4 < p$_T$ < 200 GeV/c and 1.0 <
                      p$_T$ < 50 GeV/c, respectively. The respective nuclear
                      modification factor (R$_{pPb}$) is presented for p$_T$ up to
                      of 200 and 30 GeV/c, where the former was achieved by
                      extending the π$^0$ measurement in pp collisions at
                      $\sqrt{s}$ = 8TeV using the merged cluster technique. The
                      values of R$_{pPb}$ are below unity for p$_T$ < 10 GeV/c,
                      while they are consistent with unity for p$_T$ > 10 GeV/c,
                      leaving essentially no room for final state energy loss. The
                      new data provide strong constraints for nuclear parton
                      distribution and fragmentation functions over a broad
                      kinematic range and are compared to model predictions as
                      well as previous results at $\sqrt{s_{\rm NN}}$ = 5.02TeV.},
      keywords     = {experimental results (INSPIRE) / p nucleus: scattering
                      (INSPIRE) / transverse momentum: momentum spectrum (INSPIRE)
                      / transverse momentum: high (INSPIRE) / pi0: production
                      (INSPIRE) / eta: production (INSPIRE) / parton: distribution
                      function (INSPIRE) / photon: pair production (INSPIRE) /
                      fragmentation function (INSPIRE) / meson: radiative decay
                      (INSPIRE) / kinematics (INSPIRE) / rapidity (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       = {2104.03116},
      howpublished = {arXiv:2104.03116},
      archivePrefix = {arXiv},
      SLACcitation = {$\%\%CITATION$ = $arXiv:2104.03116;\%\%$},
      UT           = {WOS:000820935000012},
      doi          = {10.1016/j.physletb.2022.136943},
      url          = {https://repository.gsi.de/record/250925},
}