QCD analysis of the structure function F2 in muon nucleon scattering
✍ Scribed by J.J. Aubert; G. Bassompierre; K.H. Becks; C. Best; E. Böhm; X. de Bouard; F.W. Brasse; C. Broll; S. Brown; J. Carr; R.W. Clifft; J.H. Cobb; G. Coignet; F. Combley; G.R. Court; J.M. Crespo; G. D'Agostini; P.F. Dalpiaz; P. Dalpiaz; W.D. Dau; J.K. Davies; Y. Déclais; R.W. Dobinson; U. Dosselli; J. Drees; A. Edwards; M. Edwards; J. Favier; M.I. Ferrero; W. Flauger; E. Gabathuler; R. Gamet; J. Gayler; V. Gerhardt; C. Gössling; P. Gregory; J. Haas; K. Hamacher; P. Hayman; M. Henckes; J.R. Holt; H. Jokisch; V. Korbel; G. Krikonis; U. Landgraf; M. Leenen; M. Maire; L. Massonnet; H. Minssieux; W. Mohr; H.E. Montgomery; K. Moser; R.P. Mount; P.R. Norton; J. McNicholas; A.M. Osborne; P. Payre; C. Peroni; H. Pessard; U. Pietrzyk; K. Rith; M. Schneegans; T. Sloan; H.E. Stier; W. Stockhausen; J.M. Thénard; J.C. Thompson; L. Urban; M. Villers; H. Wahlen; M. Whalley; D. Williams; W.S.C. Williams; J. Williamson; S.J. Wimpenny
- Book ID
- 113344928
- Publisher
- Elsevier Science
- Year
- 1982
- Tongue
- English
- Weight
- 454 KB
- Volume
- 114
- Category
- Article
- ISSN
- 0370-2693
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📜 SIMILAR VOLUMES
The difference between NLO and NNLO is small with respect to uncertainties of the data 2 , (1) where LT n is the leading, twist-2 moment, α S is the running coupling constant, μ 2 is an arbitrary scale (taken to be 10 (GeV/c) 2 ), a τ n is the matrix element of corresponding QCD operators, γ τ n i