English

Exclusive meson production at HERMES

High Energy Physics - Phenomenology 2016-07-11 v1

Abstract

The data were accumulated with the HERMES forward spectrometer using the 27.6 GeV longitudinally polarized electron or positron beam of HERA. Exclusive electroproduction of ω\omega mesons on unpolarized hydrogen and deuterium targets is studied in the kinematic region of Q2>1.0Q^2>1.0 GeV2^2, 3.0 GeV <W<< W < 6.3 GeV, and t<0.2-t'< 0.2 GeV2^{2}, while for ρ0\rho^0-meson production on a transversely polarized hydrogen target t<0.4-t'< 0.4 GeV2^{2} is used. Spin-density matrix elements for ω\omega production are presented in projections of Q2Q^2 or t-t', while the ratios of the helicity amplitudes for the reaction γ+pρ0+p\gamma^*+p \to \rho^0+p are obtained in the entire kinematic region. The usage of the transversely polarized target allows for the first time the extraction of the ratios of certain nucleon-helicity-flip amplitudes to the natural-parity exchange amplitude T012012T_{0\frac{1}{2}0\frac{1}{2}} without the nucleon-helicity flip describing the longitudinal ρ0\rho^0-meson production by the longitudinal virtual photon. Violation of ss-channel helicity conservation is observed for both mesons. A dominant contribution from unnatural-parity exchange (UPE) is established for special combinations of the ω\omega spin-density matrix elements. For ρ0\rho^0-meson production, the UPE amplitude without the nucleon-helicity flip, U112112U_{1\frac{1}{2}1\frac{1}{2}}, is shown to be the largest UPE amplitude. Good agreement is found between the HERMES data on ω\omega production on the proton and results of the perturbative QCD-inspired Goloskokov-Kroll model that includes pion-pole contribution.

Keywords

Cite

@article{arxiv.1607.02344,
  title  = {Exclusive meson production at HERMES},
  author = {Sergey Manaenkov},
  journal= {arXiv preprint arXiv:1607.02344},
  year   = {2016}
}

Comments

6 pages, 4 figures, XXIV International Workshop on Deep-Inelastic Scattering and Related Subjects, DESY Hamburg, Germany, 11-15 April, 2016

R2 v1 2026-06-22T14:49:12.350Z