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Suppression of neutral-pion production in deep-inelastic scattering off nuclei with the CLAS detector

T. MineevaCenter for Science and Technology of ValparaísoW. K. BrooksCenter for Science and Technology of ValparaísoA. El AlaouiCenter for Science and Technology of ValparaísoH. HakobyanCenter for Science and Technology of ValparaísoK. JooUniversity of ConnecticutJ. A. LópezUniversidad Técnica Federico Santa MaríaOrlando Javier Soto SandovalUniversidad de La SerenaP. AchenbachThomas Jefferson National Accelerator FacilityZ. AkbarNational Research and Innovation Agency (BRIN)J. S. AlvaradoUniversit'e Paris-SaclayW. R. ArmstrongArgonne National LaboratoryM. ArratiaUniversity of California RiversideH. AtaçTemple UniversityHarutyun AvagyanThomas Jefferson National Accelerator FacilityC. Ayerbe GayosoCollege of William and MaryL. BaashenFlorida International UniversityL. BarionINFNM. BashkanovUniversity of YorkI. BedlinskiyNational Research Centre Kurchatov Institute - ITEPBruno BenkelUniversidad Técnica Federico Santa MaríaF. BenmokhtarDuquesne UniversityA. BianconiINFNA. S. BiselliFairfield UniversityF. BossúIRFUS. BoiarinovThomas Jefferson National Accelerator FacilityKai-Thomas BrinkmannII Physikalisches Institut der Universitaet GiessenW. J. BriscoeThe George Washington UniversityV. D. BurkertThomas Jefferson National Accelerator FacilityT. CaoThomas Jefferson National Accelerator FacilityR. CapobiancoUniversity of ConnecticutD. S. CarmanThomas Jefferson National Accelerator FacilityJ. C. CarvajalFlorida International UniversityA. CelentanoINFNP. ChatagnonThomas Jefferson National Accelerator FacilityV. ChesnokovSkobeltsyn Institute of Nuclear PhysicsT. ChetryFlorida International UniversityG. CiulloINFNP. L. ColeLamar UniversityM. ContalbrigoINFNG. CostantiniINFNA. D’AngeloINFNN. DashyanYerevan Physics InstituteR. De VitaINFNM. DefurneIRFUA. DeurThomas Jefferson National Accelerator FacilityS. DiehlII Physikalisches Institut der Universitaet GiessenC. DjalaliOhio UniversityR. DupréUniversit'e Paris-SaclayH. EgiyanThomas Jefferson National Accelerator FacilityL. El FassiMississippi State UniversityP. EugenioFlorida State UniversityS. FeganUniversity of YorkA. FilippiINFNG. GavalianThomas Jefferson National Accelerator FacilityG. P. GilfoyleUniversity of RichmondF. X. GirodThomas Jefferson National Accelerator FacilityA. A. GolubenkoSkobeltsyn Institute of Nuclear PhysicsG. GostaINFNR. W. GotheUniversity of South CarolinaK. A. GriffioenCollege of William and MaryL. GuoFlorida International UniversityK. HafidiArgonne National LaboratoryM. HattawyArgonne National LaboratoryF. HauensteinOld Dominion UniversityT. B. HaywardUniversity of ConnecticutD. HeddleChristopher Newport UniversityA. HobartUniversit'e Paris-SaclayM. HoltropUniversity of New HampshireYing‐Chao HungOld Dominion UniversityY. IlievaUniversity of South CarolinaD. G. IrelandUniversity of GlasgowE. L. IsupovSkobeltsyn Institute of Nuclear PhysicsH. S. JoKyungpook National UniversityD. KellerUniversity of VirginiaA. KhanalFlorida International UniversityMd. Al-Amin KhandakerIdaho State UniversityW. KimKyungpook National UniversityF. J. KleinCatholic University of AmericaV. KlimenkoUniversity of ConnecticutÁ. KripkóII Physikalisches Institut der Universitaet GiessenV. KubarovskyThomas Jefferson National Accelerator FacilityS. E. KuhnOld Dominion UniversityL. LanzaINFNM. LealiINFNS. LeeArgonne National LaboratoryP. LenisaINFNX. LiMassachusetts Institute of TechnologyI. J. D. MacGregorUniversity of GlasgowD. MarchandUniversit'e Paris-SaclayD MatamorosINFNB. McKinnonUniversity of GlasgowS. MiglioratiINFNR. G. MilnerMassachusetts Institute of TechnologyM. MirazitaINFNV. MokeevThomas Jefferson National Accelerator FacilityP. MoranMassachusetts Institute of TechnologyC. Muñoz CamachoUniversit'e Paris-SaclayP. Nadel-TuronskiThomas Jefferson National Accelerator FacilityK. NeupaneUniversity of South CarolinaD. NguyenThomas Jefferson National Accelerator Facility
Physical review. Cjournal2025en
ABI

Annotatsiya

We present the first threefold differential measurement for neutral-pion multiplicity ratios produced in semi-inclusive deep-inelastic electron scattering on carbon, iron, and lead nuclei normalized to deuterium from CLAS at Jefferson Lab. We found that the neutral-pion multiplicity ratio is maximally suppressed for the leading hadrons (energy fraction <a:math xmlns:a="http://www.w3.org/1998/Math/MathML"><a:mrow><a:mi>z</a:mi><a:mo>→</a:mo></a:mrow></a:math> 1), suppression varying from 25% in carbon up to 75% in lead. An enhancement of the multiplicity ratio at low <b:math xmlns:b="http://www.w3.org/1998/Math/MathML"><b:mi>z</b:mi></b:math> and high <c:math xmlns:c="http://www.w3.org/1998/Math/MathML"><c:msubsup><c:mi>p</c:mi><c:mrow><c:mi>T</c:mi></c:mrow><c:mn>2</c:mn></c:msubsup></c:math> is observed, suggesting an interconnection between these two variables. This behavior is qualitatively similar to the previous twofold differential measurement of charged pions by the HERMES Collaboration and, recently, by CLAS Collaboration. The largest enhancement was observed at high <d:math xmlns:d="http://www.w3.org/1998/Math/MathML"><d:msubsup><d:mi>p</d:mi><d:mrow><d:mi>T</d:mi></d:mrow><d:mn>2</d:mn></d:msubsup></d:math> for heavier nuclei, namely, iron and lead, while the smallest enhancement was observed for the lightest nucleus, carbon. This behavior suggests a competition between partonic multiple scattering, which causes enhancement, and hadronic inelastic scattering, which causes suppression.

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