The tensor pomeron and low-x deep inelastic scattering

The tensor-pomeron model is applied to low-x deep-inelastic lepton-nucleon scattering and photoproduction. We consider c.m. energies in the range 6 - 318 GeV and Q^2 < 50 GeV^2. In addition to the soft tensor pomeron, which has proven quite successful for the description of soft hadronic high-ene...

Full description

Saved in:
Bibliographic Details
Main Authors: Britzger, Daniel (Author) , Ewerz, Carlo (Author) , Glazov, S. (Author) , Nachtmann, Otto (Author) , Schmitt, Stefan (Author)
Format: Article (Journal)
Language:English
Published: 24 Jan 2019
In: Physical review
Year: 2019, Volume: 100, Issue: 11
ISSN:2470-0029
DOI:10.1103/PhysRevD.100.114007
Online Access:Verlag, Volltext: https://doi.org/10.1103/PhysRevD.100.114007
Verlag: http://arxiv.org/abs/1901.08524
Get full text
Author Notes:Daniel Britzger, Carlo Ewerz, Sasha Glazov, Otto Nachtmann, Stefan Schmitt
Description
Summary:The tensor-pomeron model is applied to low-x deep-inelastic lepton-nucleon scattering and photoproduction. We consider c.m. energies in the range 6 - 318 GeV and Q^2 < 50 GeV^2. In addition to the soft tensor pomeron, which has proven quite successful for the description of soft hadronic high-energy reactions, we include a hard tensor pomeron. We also include f_2-reggeon exchange which turns out to be particularly relevant for real-photon-proton scattering at c.m. energies in the range up to 30 GeV. The combination of these exchanges permits a description of the absorption cross sections of real and virtual photons on the proton in the same framework. In particular, a detailed comparison of this two-tensor-pomeron model with the latest HERA data for x < 0.01 is made. Our model gives a very good description of the transition from the small-Q^2 regime where the real or virtual photon behaves hadron-like to the large-Q^2 regime where hard scattering dominates. Our fit allows us, for instance, a determination of the intercepts of the hard pomeron as 1.3008(+73,-84), of the soft pomeron as 1.0935(+76,-64), and of the f_2 reggeon. We find that in photoproduction the hard pomeron does not contribute within the errors of the fit. We show that assuming a vector instead of a tensor character for the pomeron leads to the conclusion that it must decouple in real photoproduction.
Item Description:Gesehen am 21.02.2020
Physical Description:Online Resource
ISSN:2470-0029
DOI:10.1103/PhysRevD.100.114007