The $γ^* \lowercase{p}$ total cross section at low x

Details The $γ^* \lowercase{p}$ total cross section at low x The $γ^* \lowercase{p}$ total cross section at low x

2001-10-24

arxiv.org/abs/hep-ph/0110311v2

Acta Phys.Polon. B32 (2001) 3745-3754

Physics

High Energy Physics

High Energy Physics - Phenomenology

8 pages, Latex using psfig, 5 figures Invited Talk presented at the XXXVth Internat. School of Theoretical Physics, Ustron, Po

Scientific paper

The scaling in $\sigma_{\gamma^*p}(W^2, Q^2)$ cross sections (for $Q^2/W^2 << 1$) in terms of the scaling variable $\eta = (Q^2 + m^2_0)/\Lambda^2 (W^2)$ is interpreted in the generalized vector dominance/color-dipole picture (GVD/CDP). The quantity $\Lambda^2 (W^2)$ is identified as the average gluon transverse momentum absorbed by the $q \bar q$ state, $<\vec l_\bot^{~2}> = (1/6) \Lambda^2 (W^2)$. At any $Q^2$, for $W^2 \to \infty$, the cross sections for virtual and real photons become universal,$\sigma_{\gamma^*p}(W^2,Q^2)/ \sigma_{\gamma p} (W^2) \to 1$. The gluon density corresponding to the color-dipole cross section in the appropriate limit is found to be consistent with the results from QCD fits.

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