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First measurement of massive virtual photon emission from N* baryon resonances

  • R. Abou Yassine
  • , J. Adamczewski-Musch
  • , O. Arnold
  • , E. T. Atomssa
  • , M. Becker
  • , C. Behnke
  • , J. C. Berger-Chen
  • , A. Blanco
  • , C. Blume
  • , M. Böhmer
  • , L. Chlad
  • , I. Ciepał
  • , S. Deb
  • , C. Deveaux
  • , D. Dittert
  • , J. Dreyer
  • , E. Epple
  • , L. Fabbietti
  • , J. Förtsch
  • , P. Fonte
  • C. Franco, J. Friese, I. Fröhlich, T. Galatyuk, J. A. Garzón, R. Gernhäuser, R. Greifenhagen, M. Grunwald, M. Gumberidze, S. Harabasz, T. Heinz, T. Hennino, C. Höhne, F. Hojeij, R. Holzmann, M. Idzik, B. Kämpfer, K. H. Kampert, B. Kardan, V. Kedych, S. Kim, I. Koenig, W. Koenig, M. Kohls, J. Kolas, B. W. Kolb, G. Korcyl, G. Kornakov, R. Kotte, W. Krueger, A. Kugler, T. Kunz, R. Lalik, K. Lapidus, S. Linev, F. Linz, L. Lopes, M. Lorenz, T. Mahmoud, L. Maier, A. Malige, J. Markert, S. Maurus, V. Metag, J. Michel, D. M. Mihaylov, A. Molenda, C. Müntz, R. Münzer, M. Nabroth, L. Naumann, K. Nowakowski, A. Opíchal, J. Orliński, J. H. Otto, Y. Parpottas, M. Parschau, C. Pauly, V. Pechenov, O. Pechenova, K. Piasecki, J. Pietraszko, T. Povar, K. Prościński, A. Prozorov, W. Przygoda, K. Pysz, B. Ramstein, N. Rathod, P. Rodriguez-Ramos, A. Rost, A. Rustamov, P. Salabura, K. Scharmann, T. Scheib, N. Schild, K. Schmidt-Sommerfeld, H. Schuldes, E. Schwab, F. Scozzi, F. Seck, P. Sellheim, J. Siebenson, L. Silva, U. Singh, J. Smyrski, S. Spataro, S. Spies, A. Sreejith, H. Ströbele, J. Stroth, C. Sturm, K. Sumara, O. Svoboda, M. Szala, P. Tlusty, M. Traxler, S. Treliński, H. Tsertos, I. C. Udrea, O. Vazquez-Doce, V. Wagner, A. A. Weber, C. Wendisch, M. G. Wiebusch, J. Wirth, A. Władyszewska, H. P. Zbroszczyk, M. Zieliński, P. Zumbruch
  • Technische Universität Darmstadt
  • University Paris-Sud
  • GSI Helmholtz Center
  • Excellence Cluster’Origin and Structure of the Universe’
  • Technical University of Munich
  • Justus-Liebig-Universität Gießen
  • Johann Wolfgang Goethe University
  • LIP-Laboratorio de Instrumentacao e Fisica Experimental de Particulas
  • Helmholtz Research Academy Hesse for FAIR (HFHF)
  • Nuclear Physics Institute of the Cas
  • Czech Technical University in Prague
  • Henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of Sciences
  • HelmholtzZentrum Dresden-Rossendorf
  • Bergische Universität Wuppertal
  • Coimbra Polytechnic - ISEC
  • Helmholtz Research Academy Hesse for FAIR (HFHF)
  • Universidad de Santiago de Compostela
  • Technische Universität Dresden
  • Warsaw Institute of Technology
  • Univ of Mining and Metallurgy
  • Jagiellonian University
  • Palacky University
  • University of Warsaw
  • Frederick University
  • Charles University in Prague
  • INFN Sez. di Torino

Research output: Contribution to journalArticlepeer-review

1 Scopus citations

Abstract

First information on the timelike electromagnetic structure of baryons in the second resonance region has been obtained from measurements of the dielectron (e+e) invariant mass and angular distributions with the High Acceptance Di-Electron Spectrometer (HADES) at GSI, using a secondary pion beam impinging on CH2 and C targets. The quasi-free reaction π+ p → n e+e at sπp = 1.49 GeV is isolated in several analysis steps. The data set provides a crucial test for the description of baryon timelike transitions. Close to the kinematical limit the meassured e+e mass distribution shows deviations by up to a factor 8 from the Dalitz decay of a point-like baryon. Various theoretical approaches connecting information from hadronic and electromagnetic channels in the spacelike and timelike regime compare well with the measured e+e invariant mass distribution, including (i) a Vector Meson Dominance amplitude containing direct photon and vector meson (ρ) couplings to the baryon, (ii) electromagnetic timelike baryon transition form factors in a covariant spectator-quark model, where meson cloud effects dominate, and (iii) application of dispersion theory, which demonstrates the importance of the pion electromagnetic form factors. The dielectron angular distributions exhibit contributions of virtual photons (γ *) with longitudinal polarization, in contrast to real photons. The γ * angular dependence supports the dominance of J=3/2, I=1/2 contributions in both the γ n and the ππ N channels.

Original languageEnglish
Article number140338
JournalPhysics Letters B
Volume875
DOIs
StatePublished - Apr 2026

Keywords

  • Baryon Dalitz decay
  • Dilepton
  • Electromagnetic timelike transitions
  • Off-shell ρ meson
  • Pion-nucleon interaction

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