Abstract
In this paper we discuss the Odderon contribution in our model[19] that gives a fairly good description of $\sigma_{\rm tot}$ $\sigma_{\rm el}$and $B_{\rm el}$ for proton-proton scattering. We show that the shadowing corrections are large, and induce considerable dependence on energy for the Odderon contribution, which in perturbative QCD does not depend on energy. This energy dependence is in agreement with the experimental data for $\rho = {\rm Re}/{\rm Im}$, assuming that the Odderon gives a contribution of about 1 mb at W = 7 TeV. This differs greatly with our estimates for a CGC based model. We reproduce the main features of the $ t$ -dependence that are measured experimentally: the slope of the elastic cross section at small $t$, the existence of the minima in $t$-dependence which is located at $|t|_{min}$ = 0.52 GeV 2 at W= 7 TeV; and the behaviour of the elastic cross section at $ |t| > |t|_{min}$.The real part of the elastic amplitude turns out to be much smaller than the experimental one. Consequently, to achieve a description of the data, it is necessary to add an odderon contribution.
Highlights
The new data of TOTEM collaboration [1,2,3,4] drew attention to the state with negative signature and with an intercept which is close to unity
We show that the shadowing corrections are large, and induce considerable dependence on energy for the odderon contribution, which in perturbative QCD does not depend on energy
We reproduce the main features of the t-dependence that are measured experimentally: the slope of the elastic cross section at small t, the existence of the minima in t-dependence which is located at jtjmin 1⁄4 0.52 GeV2 at W 1⁄4 7 TeV; and the behavior of the elastic cross section at jtj > jtjmin
Summary
The new data of TOTEM collaboration [1,2,3,4] drew attention to the state with negative signature and with an intercept which is close to unity (see Refs. [5,6,7,8,9,10,11,12,13,14]). In this paper we wish to study the shadowing corrections to the odderon contribution using the model that we proposed in Ref. [20], and (ii) on simple assumptions of hadron structure, related to the impact parameter dependence of the scattering amplitude. This parton model stems from QCD, assuming that the unknown. Our model includes three essential ingredients: (i) the new parton model for the dipole-dipole scattering amplitude that has been discussed above; (ii) the simplified one channel model that enables us to take into account diffractive production in the low mass region, and (iii) the assumptions for impact parameter dependence of the initial conditions
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