Color-Dipole Picture versus Hard Pomeron in Deep Inelastic Scattering
arXiv:2011.09934 · doi:10.1103/PhysRevD.104.014009
Abstract
For photon virtualities of $Q^2 \gsim 20 {\rm GeV}^2$, the results of the (hard Pomeron) fit in the tensor-Pomeron model in terms of the variables and the virtual-photon-proton energy squared, , provide empirical evidence for the validity of the Color Dipole Picture (CDP). Consistency of the CDP with the perturbative QCD (pQCD) improved parton model implies the prediction of for the exponent of the energy-squared dependence in agreement with the results of the fits. For $Q^2 \lsim 20 GeV^2$, the CDP yields a parameter-free smooth transition from $Q^2 \gsim 20 {\rm GeV}^2$ to photoproduction, in distinction from the tensor-Pomeron model that relies on the additional parameter quantifying the intercept of the soft-Pomeron trajectory.
7 pages, 1 figure
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Cited by in corpus (6)
- Asymptotic gluon density within the color dipole picture in the light of HERA high-precision data
- Top cross section in the LHeC and FCC-he energy range
- Nuclear transverse momentum imbalance in the color dipole approach at the LHC regime
- Color dipole cross-section from unifying the color dipole picture and improved saturation models
- The Proton Gluon Distribution from the Color Dipole Picture
- One-to-One correspondence of soft and hard Pomeron with the CDP of the gluon density at low