Abstract

In the present paper, we extend the Froissaron-Maximal Odderon (FMO) approach at t different from 0. Our extended FMO approach gives an excellent description of the 3266 experimental points considered in a wide range of energies and momentum transferred. We show that the very interesting TOTEM results for proton–proton differential cross-section in the range 2.76–13 TeV, together with the Tevatron data for antiproton–proton at 1.8 and 1.96 TeV give further experimental evidence for the existence of the Odderon. One spectacular theoretical result is the fact that the difference in the dip-bump region between {bar{p}}p and pp differential cross-sections is diminishing with increasing energies and for very high energies (say 100 TeV), the difference between {bar{p}}p and pp in the dip-bump region is changing its sign: pp becomes bigger than {bar{p}}p at |t| about 1 GeV^2. This is a typical Odderon effect. Another important – phenomenological – result of our approach is that the slope in pp scattering has a different behavior in t than the slope in {bar{p}}p scattering. This is also a clear Odderon effect.

Highlights

  • In the present paper, we extend the FroissaronMaximal Odderon (FMO) approach at t different from 0

  • We show that the very interesting TOTEM results for proton–proton differential crosssection in the range 2.76–13 TeV, together with the Tevatron data for antiproton–proton at 1.8 and 1.96 TeV give further experimental evidence for the existence of the Odderon

  • One spectacular theoretical result is the fact that the difference in the dip-bump region between pp and pp differential crosssections is diminishing with increasing energies and for very high energies, the difference between pp and pp in the dip-bump region is changing its sign: pp becomes bigger than pp at |t| about 1 GeV2

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Summary

Introduction

We extend the FMO approach at t different from 0. We show that the very interesting TOTEM results for proton–proton differential cross-section in the range 2.76–13 TeV, together with the D0 data for antiproton– proton at 1.96 TeV give further experimental evidence for the existence of the Odderon

Extension of the FMO approach at t different from zero: general definitions
Regge poles and their double rescatterings
Partial amplitudes for Froissaron and Odderon
Comparison of the FMO model with the data
Comparison with other approaches
Conclusion
General constraints
Findings
Partial amplitudes
Full Text
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