Article ID | Journal | Published Year | Pages | File Type |
---|---|---|---|---|
9854854 | Nuclear Physics B | 2005 | 180 Pages |
Abstract
We compute the full three-loop coefficient functions for the structure functions F2 and FL in massless perturbative QCD. The results for FL complete the next-to-next-to-leading order description of unpolarized electromagnetic deep-inelastic scattering. The third-order coefficient functions for F2 form, at not too small values of the Bjorken variable x, the dominant part of the next-to-next-to-next-to-leading order corrections, thus facilitating improved determinations of the strong coupling αs from scaling violations. The three-loop corrections to FL are larger than those for F2. Especially for the latter quantity the expansion in powers of αs is very stable, for photon virtualities Q2â«1GeV2, over the full x-range accessible to fixed-target and collider measurements.
Related Topics
Physical Sciences and Engineering
Mathematics
Mathematical Physics
Authors
J.A.M. Vermaseren, A. Vogt, S. Moch,