Implications of a Froissart bound saturation of - deep inelastic scattering. Part I. Quark distributions at ultra small
arXiv:1302.6119 · doi:10.1103/PhysRevD.88.014006
Abstract
We argue that the deep inelastic structure function , regarded as a cross section for virtual scattering, is hadronic in nature. This implies that its growth is limited by the Froissart bound at high hadronic energies, giving a bound on as Bjorken . The same bound holds for the individual quark distributions. In earlier work, we obtained a very accurate global fit to the combined HERA data on using a fit function which respects the Froissart bound at small , and is equivalent in its dependence to the function used successfully to describe all high energy hadronic cross sections, including scattering. We extrapolate that fit by a factor of 3 beyond the HERA region in the natural variable to the values of down to and use the results to derive the quark distributions needed for the reliable calculation of neutrino cross sections at energies up to GeV. These distributions do not satisfy the Feynman "wee parton" assumption, that they all converge toward a common distribution at small and large . This was used in some past calculations to express the dominant neutrino structure function directly in terms of . We show that the correct distributions nevertheless give results for which differ only slightly from those obtained assuming that the wee parton limit holds. In two Appendices, we develop simple analytic results for the effects of QCD evolution and operator-product corrections on the distribution functions at small , and show that these effects amount mainly to shifting the values of in the initial distributions.
19 pages, 6 figures. The paper is now shorter with the new results clearly emphasized
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