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Second-order contributions to the structure functions in deep inelastic scattering III The singlet
For pt.II see ibid., vol.159, p.512 (1979). Pointlike QCD predictions for the singlet part of the structure functions are given up to next- to-leading order of perturbation theory. This generalises the result obtained in pt.I (see ibid., vol.153, p.161, 1979) which deals with the non-singlet case. A...
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
1980
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/0550-3213(80)90207-2 http://cds.cern.ch/record/879363 |
Sumario: | For pt.II see ibid., vol.159, p.512 (1979). Pointlike QCD predictions for the singlet part of the structure functions are given up to next- to-leading order of perturbation theory. This generalises the result obtained in pt.I (see ibid., vol.153, p.161, 1979) which deals with the non-singlet case. An interesting by-product is an exact and simple analytical expression for the anomalous dimension matrix to second non-trivial order in the QCD coupling constant. (18 refs). |
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