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Neutral-Boson Photoproduction on Hydrogen at High Energies

R. Anderson, D. Gustavson, J. Johnson, D. Ritson, and B. H. Wiik

W. G. Jones* and D. Kreinick

F. Murphy

R. Weinstein

  • Stanford Linear Accelerator Center, Stanford University, Stanford, California 94305

  • California Institute of Technology, Pasadena, California 91109

  • University of California, Santa Barbara, California

  • Northeastern University, Boston, Massachusetts 02115

  • *On leave of absence from Imperial College, London, England.

Phys. Rev. D 1, 27 – Published 1 January, 1970

DOI: https://doi.org/10.1103/PhysRevD.1.27

Abstract

Photoproduction cross sections for neutral π, η, ρ, and φ mesons have been measured at the Stanford Linear Accelerator Center for photon energies between 5 and 17.8 GeV, and t (four-momentum transfer squared) between -0.12 and -1.4 (GeV/c)2, using a missing-mass technique. The pion production at lower energies is characterized by a fast falloff with increasing |t| at small |t| values, with a dip at t=0.5 (GeV/c)2 followed by a secondary maximum around t=0.9 (GeV/c)2 and a smooth falloff at larger |t| values. As the incident photon energy increases, the dip becomes less pronounced, in contradiction to the expectations of simple Regge theories based only on the exchange of the ω and B trajectories. η photo-production was measured around 6 GeV and at 9 GeV. The cross section decreases smoothly with t and shows no dip at t=0.5 (GeV/c)2, in disagreement with predictions based on Reggeized ρ exchange. ρ production rates agree well with predictions assuming diffraction production. The differential cross section varies approximately as e8.5t. The total cross section decreases from 16.0 μb at 5.5 GeV to 12.3 μb at 17.8 GeV incident photon energy. A quark-model relation between πp elastic scattering and ρ photoproduction gives a good representation of the data. φ production also appears consistent with the predictions of the diffraction-dissociation model. We also searched for evidence of photoproduction of other particles with mass up to 2 GeV. Production of one particle of mass 1240±20 MeV and width around 100 MeV was observed. No particles with mass between 1300 and 2000 MeV were found. Any particle with cross section larger than 4% of the ρ cross section would have been visible.

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