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Determination of quadrupole strengths in the γ* p → Δ (1232) transition at Q2 = 0.20 (GeV / c)2

  • N. F. Sparveris
  • , P. Achenbach
  • , C. Ayerbe Gayoso
  • , D. Baumann
  • , J. Bernauer
  • , A. M. Bernstein
  • , R. Böhm
  • , D. Bosnar
  • , T. Botto
  • , A. Christopoulou
  • , D. Dale
  • , M. Ding
  • , M. O. Distler
  • , L. Doria
  • , J. Friedrich
  • , A. Karabarbounis
  • , M. Makek
  • , H. Merkel
  • , U. Müller
  • , I. Nakagawa
  • R. Neuhausen, L. Nungesser, C. N. Papanicolas, A. Piegsa, J. Pochodzalla, M. Potokar, M. Seimetz, S. Širca, S. Stave, S. Stiliaris, Th Walcher, M. Weis
  • National and Kapodistrian University of Athens
  • Johannes Gutenberg University Mainz
  • Massachusetts Institute of Technology
  • University of Zagreb
  • University of Kentucky
  • RIKEN
  • University of Ljubljana

Research output: Contribution to journalArticlepeer-review

46 Scopus citations

Abstract

We report new precise p (over(e, →), e p) π0 measurements at the peak of the Δ+ (1232) resonance at Q2 = 0.20 (GeV / c)2 performed at the Mainz Microtron (MAMI). The new data are sensitive to both the electric (E2) and the Coulomb (C2) quadrupole amplitudes of the γ* N → Δ transition. They yield precise quadrupole to dipole amplitude ratios: CMR = (- 5.09 ± 0.28stat + sys ± 0.30model) % and EMR = (- 1.96 ± 0.68stat + sys ± 0.41model) % for M1 +3 / 2 = (39.57 ± 0.75stat + sys ± 0.40model) (10-3 / mπ+). The new results are in disagreement with Constituent Quark Model predictions and in qualitative agreement with models that account for mesonic contributions, including recent Lattice calculations. They thus give further credence to the conjecture of deformation in hadronic systems favoring the attribution of the origin of deformation to the dominance of mesonic effects.

Original languageEnglish
Pages (from-to)102-107
Number of pages6
JournalPhysics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics
Volume651
Issue number2-3
DOIs
StatePublished - Jul 26 2007

Keywords

  • CMR
  • Electro-pion production
  • EMR
  • Nucleon deformation

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