Universe (Nov 2021)

A Fit to the Available <i>e</i><sup>+</sup><i>e</i><sup>−</sup> → <inline-formula><math display="inline"><semantics><mrow><msubsup><mi mathvariant="sans-serif">Λ</mi><mi>c</mi><mo>+</mo></msubsup><msubsup><mover accent="true"><mi mathvariant="sans-serif">Λ</mi><mo>¯</mo></mover><mi>c</mi><mo>−</mo></msubsup></mrow></semantics></math></inline-formula> Cross Section Data Nearby Production Threshold by Means of a Strong Correction to the Coulomb Enhancement Factor

  • Antonio Amoroso,
  • Stefano Bagnasco,
  • Rinaldo Baldini Ferroli,
  • Ilaria Balossino,
  • Monica Bertani,
  • Diego Bettoni,
  • Fabrizio Bianchi,
  • Alberto Bortone,
  • Alessandro Calcaterra,
  • Gianluigi Cibinetto,
  • Fabio Cossio,
  • Francesca De Mori,
  • Manuel Dioniso Da Rocha Rolo,
  • Marco Destefanis,
  • Riccardo Farinelli,
  • Luciano Fava,
  • Giulietto Felici,
  • Luciano Gaido,
  • Isabella Garzia,
  • Stefano Gramigna,
  • Michela Greco,
  • Lia Lavezzi,
  • Stefano Lusso,
  • Marco Maggiora,
  • Alessio Mangoni,
  • Simonetta Marcello,
  • Giulio Mezzadri,
  • Sara Morgante,
  • Elisabetta Pace,
  • Simone Pacetti,
  • Piero Patteri,
  • Angelo Rivetti,
  • Marco Scodeggio,
  • Stefano Sosio,
  • Stefano Spataro

DOI
https://doi.org/10.3390/universe7110436
Journal volume & issue
Vol. 7, no. 11
p. 436

Abstract

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There are two available sets of data on the e+e−→Λc+Λ¯c− cross section at energies close to the production threshold, collected by the Belle and by the BESIII Collaborations. The measurement of the former, performed by means of the initial state radiation technique, is compatible with the presence of a resonance, called ψ(4660), observed also in other final states. On the contrary, the latter is measured an almost flat and hence non-resonant cross section in the energy region just above the production threshold, but the data stop before the possible rise in the cross section for the resonant production. We propose an effective model to describe the behavior of the data near this threshold, which is based on a Coulomb-like enhancement factor due to the strong interaction among the final state particles. In the framework of this model, it is possible to describe both datasets.

Keywords