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Influence of a dynamical gluon mass in the pp and p¯p forward scattering

E. G. S. Luna, A. F. Martini, M. J. Menon, A. Mihara, and A. A. Natale
Phys. Rev. D 72, 034019 – Published 23 August 2005

Abstract

We compute the tree level cross section for gluon-gluon elastic scattering taking into account a dynamical gluon mass, and show that this mass scale is a natural regulator for this subprocess cross section. Using an eikonal approach in order to examine the relationship between this gluon-gluon scattering and the elastic pp and p¯p channels, we found that the dynamical gluon mass is of the same order of magnitude as the ad hoc infrared mass scale m0 underlying eikonalized QCD-inspired models. We argue that this correspondence is not an accidental result, and that this dynamical scale indeed represents the onset of nonperturbative contributions to the elastic hadron-hadron scattering. We apply the eikonal model with a dynamical infrared mass scale to obtain predictions for σtotpp,p¯p, ρpp,p¯p, slope Bpp,p¯p, and differential elastic scattering cross section dσp¯p/dt at Tevatron and CERN-LHC energies.

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  • Received 7 July 2005

DOI:https://doi.org/10.1103/PhysRevD.72.034019

©2005 American Physical Society

Authors & Affiliations

E. G. S. Luna1,2, A. F. Martini2, M. J. Menon2, A. Mihara3, and A. A. Natale1

  • 1Instituto de Física Teórica, Universidade Estadual Paulista, 01405-900, São Paulo, SP, Brazil
  • 2Instituto de Física Gleb Wataghin, Universidade Estadual de Campinas, 13083-970, Campinas, SP, Brazil
  • 3Instituto de Física de São Carlos, Universidade de São Paulo, 13560-970, São Carlos, SP, Brazil

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Issue

Vol. 72, Iss. 3 — 1 August 2005

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Images

  • Figure 1
    Figure 1
    The χ2/DOF as a function of dynamical gluon mass mg.Reuse & Permissions
  • Figure 2
    Figure 2
    Total cross section for pp (solid curve) and p¯p (dashed curve) scattering.Reuse & Permissions
  • Figure 3
    Figure 3
    Ratio of the real to imaginary part of the forward scattering amplitude for pp (solid curve) and p¯p (dashed curve) scattering.Reuse & Permissions
  • Figure 4
    Figure 4
    Nuclear slope parameter for elastic pp (solid curve) and p¯p (dashed curve) scattering.Reuse & Permissions
  • Figure 5
    Figure 5
    Predictions for the elastic differential scattering cross sections at s=1.8,1.96 and 14 TeV. In our model the channels pp and p¯p are not distinguished at high energies. The data points are from E710 [28].Reuse & Permissions
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