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Measurement of charged-pion production in deep-inelastic scattering off nuclei with the CLAS detector

S. MoránUniversidad Técnica Federico Santa María, Casilla 110-V Valparaíso, ChileR. DupréLaboratoire de Physique des 2 Infinis Irène Joliot-CurieH. HakobyanYerevan Physics Institute, 375036 Yerevan, ArmeniaM. ArratiaUniversity of California, Riverside, California, 92521, USAW. K. BrooksUniversidad Técnica Federico Santa María, Casilla 110-V Valparaíso, ChileA. BórquezUniversidad Técnica Federico Santa María, Casilla 110-V Valparaíso, ChileA. El AlaouiUniversidad Técnica Federico Santa María, Casilla 110-V Valparaíso, ChileL. El FassiMississippi State University, Mississippi State, Mississippi 39762-5167, USAK. HafidiArgonne National Laboratory, Argonne, Illinois 60439, USAR. A. MéndezUniversidad Técnica Federico Santa María, Casilla 110-V Valparaíso, ChileT. MineevaUniversidad Técnica Federico Santa María, Casilla 110-V Valparaíso, ChileSebouh J. PaulUniversity of California, Riverside, California, 92521, USAM. J. AmaryanOld Dominion University, Norfolk, Virginia 23529, USAGiovanni AngeliniThe George Washington University, Washington, D.C. 20052, USAW. ArmstrongArgonne National Laboratory, Argonne, Illinois 60439, USAH. AtaçTemple University, Philadelphia, Pennsylvania 19122, USAN. A. BaltzellThomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USAL. BarionINFN, Sezione di Ferrara, 44100 Ferrara, ItalyM. BashkanovUniversity of York, York YO10 5DD, United KingdomM. BattaglieriThomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USAI. BedlinskiyNational Research Centre Kurchatov Institute–ITEP, Moscow, 117259, RussiaF. BenmokhtarDuquesne University, Pittsburgh, Pennsylvania 15282, USAA. BianconiUniversità degli Studi di Brescia, 25123 Brescia, ItalyL. BiondoINFN, Sezione di Genova, 16146 Genova, ItalyA. S. BiselliCarnegie Mellon University, Pittsburgh, Pennsylvania 15213, USAF. BossùCEA Paris-SaclayS. BoiarinovThomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USAW. J. BriscoeThe George Washington University, Washington, D.C. 20052, USAD. BulumullaOld Dominion University, Norfolk, Virginia 23529, USAV. D. BurkertThomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USAD. S. CarmanThomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USAP. ChatagnonInstitut National de Physique Nucléaire et de Physique des ParticulesV. ChesnokovSkobeltsyn Institute of Nuclear Physics, Lomonosov Moscow State University, 119234 Moscow, RussiaT. ChetryMississippi State University, Mississippi State, Mississippi 39762-5167, USAG. CiulloINFN, Sezione di Ferrara, 44100 Ferrara, ItalyP. L. ColeCatholic University of America, Washington, D.C. 20064, USAM. ContalbrigoINFN, Sezione di Ferrara, 44100 Ferrara, ItalyG. CostantiniINFN, Sezione di Pavia, 27100 Pavia, ItalyA. D’AngeloINFN, Sezione di Roma Tor Vergata, 00133 Rome, ItalyN. DashyanYerevan Physics Institute, 375036 Yerevan, ArmeniaR. De VitaINFN, Sezione di Genova, 16146 Genova, ItalyM. DefurneIRFU, CEA, Université Paris-Saclay, F-91191 Gif-sur-Yvette, FranceA. DeurThomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USAS. DiehlII Physikalisches Institut der Universitaet Giessen, 35392 Giessen, GermanyC. DjalaliOhio University, Athens, Ohio 45701, USAH. EgiyanThomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USAL. ElouadrhiriThomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USAP. EugenioFlorida State University, Tallahassee, Florida 32306, USAR. FerschCollege of William and Mary, Williamsburg, Virginia 23187-8795, USAA. FilippiINFN, Sezione di Torino, 10125 Torino, ItalyG. GavalianThomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USAY. GhandilyanYerevan Physics Institute, 375036 Yerevan, ArmeniaG. P. GilfoyleUniversity of Richmond, Richmond, Virginia 23173, USAA. A. GolubenkoSkobeltsyn Institute of Nuclear Physics, Lomonosov Moscow State University, 119234 Moscow, RussiaR. W. GotheUniversity of South Carolina, Columbia, South Carolina 29208, USAK. A. GriffioenWilliams (United States)M. GuidalUniversit'e Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, FranceM. HattawyOld Dominion University, Norfolk, Virginia 23529, USAF. HauensteinOld Dominion University, Norfolk, Virginia 23529, USAT. B. HaywardUniversity of Connecticut, Storrs, Connecticut 06269, USAD. HeddleChristopher Newport University, Newport News, Virginia 23606, USAK. HicksOhio University, Athens, Ohio 45701, USAA. HobartUniversit'e Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, FranceM. HoltropUniversity of New Hampshire, Durham, New Hampshire 03824-3568, USAY. IlievaUniversity of South Carolina, Columbia, South Carolina 29208, USAD. G. IrelandUniversity of Glasgow, Glasgow G12 8QQ, United KingdomE. L. IsupovSkobeltsyn Institute of Nuclear Physics, Lomonosov Moscow State University, 119234 Moscow, RussiaH. S. JoKyungpook National University, Daegu 41566, Republic of KoreaD. KellerUniversity of Virginia, Charlottesville, Virginia 22901, USAA. KhanalFlorida International University, Miami, Florida 33199, USAM. KhandakerNorfolk State University, Norfolk, Virginia 23504, USAW. KimKyungpook National University, Daegu 41566, Republic of KoreaF. J. KleinCatholic University of AmericaÁ. KripkóII Physikalisches Institut der Universitaet Giessen, 35392 Giessen, GermanyV. KubarovskyRensselaer Polytechnic Institute, Troy, New York 12180-3590, USAS. E. KuhnOld Dominion University, Norfolk, Virginia 23529, USAL. LanzaINFN, Sezione di Roma Tor Vergata, 00133 Rome, ItalyM. LealiUniversità degli Studi di Brescia, 25123 Brescia, ItalyP. LenisaINFN, Sezione di Ferrara, 44100 Ferrara, ItalyK. LivingstonUniversity of Glasgow, Glasgow G12 8QQ, United KingdomI. J. D. MacGregorUniversity of Glasgow, Glasgow G12 8QQ, United KingdomD. MarchandUniversité Paris-SaclayL. MarsicanoINFN, Sezione di Genova, 16146 Genova, ItalyV. MascagnaINFN, Sezione di Pavia, 27100 Pavia, ItalyB. McKinnonUniversity of Glasgow, Glasgow G12 8QQ, United KingdomC. McLauchlinUniversity of South Carolina, Columbia, South Carolina 29208, USAZ.-E. MezianiArgonne National Laboratory, Argonne, Illinois 60439, USAS. MiglioratiINFN, Sezione di Pavia, 27100 Pavia, ItalyM. MirazitaINFN, Laboratori Nazionali di Frascati, 00044 Frascati, ItalyV. MokeevThomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USAC. Muñoz CamachoLaboratoire de Physique des 2 Infinis Irène Joliot-CurieP. Nadel-TurońskiThomas Jefferson National Accelerator Facility, Newport News, Virginia 23606, USAK. NeupaneUniversity of South Carolina, Columbia, South Carolina 29208, USAS. NiccolaiUniversit'e Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, FranceG. NiculescuJames Madison University, Harrisonburg, Virginia 22807, USAT. O׳ConnellUniversity of Connecticut, Storrs, Connecticut 06269, USAM. OsipenkoINFN, Sezione di Genova, 16146 Genova, ItalyA. OstrovidovFlorida State University, Tallahassee, Florida 32306, USAM. OuillonLaboratoire de Physique des 2 Infinis Irène Joliot-CurieP. PandeyOld Dominion University, Norfolk, Virginia 23529, USA
2022en
ABI

Annotatsiya

Background: Energetic quarks in nuclear deep-inelastic scattering propagate through the nuclear medium. Processes that are believed to occur inside nuclei include quark energy loss through medium-stimulated gluon bremsstrahlung and intranuclear interactions of forming hadrons. More data are required to gain a more complete understanding of these effects.Purpose: To test the theoretical models of parton transport and hadron formation, we compared their predictions for the nuclear and kinematic dependence of pion production in nuclei.Methods: We have measured charged-pion production in semi-inclusive deep-inelastic scattering off D, C, Fe, and Pb using the CLAS detector and the CEBAF 5.014-GeV electron beam. We report results on the nuclear-to-deuterium multiplicity ratio for ${\ensuremath{\pi}}^{+}$ and ${\ensuremath{\pi}}^{\ensuremath{-}}$ as a function of energy transfer, four-momentum transfer, and pion energy fraction or transverse momentum---the first three-dimensional study of its kind.Results: The ${\ensuremath{\pi}}^{+}$ multiplicity ratio is found to depend strongly on the pion fractional energy $z$ and reaches minimum values of $0.67\ifmmode\pm\else\textpm\fi{}0.03, 0.43\ifmmode\pm\else\textpm\fi{}0.02$, and $0.27\ifmmode\pm\else\textpm\fi{}0.01$ for the C, Fe, and Pb targets, respectively. The $z$ dependencies of the multiplicity ratios for ${\ensuremath{\pi}}^{+}$ and ${\ensuremath{\pi}}^{\ensuremath{-}}$ are equal within uncertainties for C and Fe targets but show differences at the level of $10%$ for the Pb-target data. The results are qualitatively described by the GiBUU transport model, as well as with a model based on hadron absorption, but are in tension with calculations based on nuclear fragmentation functions.Conclusions: These precise results will strongly constrain the kinematic and flavor dependence of nuclear effects in hadron production, probing an unexplored kinematic region. They will help to reveal how the nucleus reacts to a fast quark, thereby shedding light on its color structure and transport properties and on the mechanisms of the hadronization process.

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