The 16th Moment of the Non--Singlet Structure Functions $F_2(x,Q^2)$ and $F_L(x,Q^2)$ to $O(α_s^3)$

Details The 16th Moment of the Non--Singlet Structure Functions $F_2(x,Q^2)$ and $F_L(x,Q^2)$ to $O(α_s^3)$ The 16th Moment of the Non--Singlet Structure Functions $F_2(x,Q^2)$ and $F_L(x,Q^2)$ to $O(α_s^3)$

2004-11-08

arxiv.org/abs/hep-ph/0411111v1

Phys.Lett. B606 (2005) 130-138

Physics

High Energy Physics

High Energy Physics - Phenomenology

11 pages, 1 style file, 1 figure

Scientific paper

10.1016/j.physletb.2004.11.059

We present the results of an analytic next--to--next--to leading order QCD
calculation of the non--singlet anomalous dimension $\gamma_{\rm NS}^+(N)$ and
the coefficient functions $C_{2,L}(N)$ associated to the deeply inelastic
structure functions $F_2(x,Q^2)$ and $F_L(x,Q^2)$ for the Mellin moment N=16.
Comparisons are made with results in the literature.

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