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The Longitudinal Structure Function at the Third Order
S. Moch, J. A. M. Vermaseren, A. Vogt
We compute the complete third-order contributions to the coefficient functions for the longitudinal structure function F_L, thus completing the next-to-next-to-leading order (NNLO)…
The QCD Splitting Functions at Three Loops: Methods and Results
S. Moch, J. A. M. Vermaseren, A. Vogt
We have computed the complete next-to-next-to-leading order (NNLO) contributions to the splitting functions governing the evolution of unpolarized parton densities in perturbative…
The Three-Loop Splitting Functions in QCD
A. Vogt, S. Moch, J. Vermaseren
We have computed the next-to-next-to-leading-order (NNLO) contributions to the evolution of unpolarized parton distributions in perturbative QCD. In this talk, we briefly recall wh…
The Three-Loop Splitting Functions in QCD: The Singlet Case
A. Vogt, S. Moch, J. A. M. Vermaseren
We compute the next-to-next-to-leading order (NNLO) contributions to the splitting functions governing the evolution of the unpolarized flavour-singlet parton densities in perturba…
The Three-Loop Splitting Functions in QCD: The Non-Singlet Case
S. Moch, J. A. M. Vermaseren, A. Vogt
We compute the next-to-next-to-leading order (NNLO) contributions to the three splitting functions governing the evolution of unpolarized non-singlet combinations of quark densitie…