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Heavy quark photoproduction in proton-proton collisions
High Energy Physics - Phenomenology · Submitted 13 Oct 2004
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The integrated cross section and the rapidity distributions for open charm and bottom production are computed employing sound high energy QCD formalisms.
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We calculate the photoproduction of heavy quarks in proton-proton collisions at RHIC, Tevatron and LHC energies. The integrated cross section and the rapidity distributions for open charm and bottom production are computed employing sound high energy QCD formalisms. For the linear pQCD approaches we consider both the usual collinear factorization and the k_T-factorization formalisms, whereas for the nonlinear QCD (saturation) calculations one considers the Golec-Biernat-Wuesthoff and the Iancu-Itakura-Munier parameterizations for the dipole cross section within the color dipole picture.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We calculate the photoproduction of heavy quarks in proton-proton collisions at RHIC, Tevatron and LHC energies. | contribution 1.00 | 0.94 | 0.07 | asserted 0.98 |
| s1 | The integrated cross section and the rapidity distributions for open charm and bottom production are computed employing sound high energy QCD formalisms. | contribution 0.59 | 0.93 | 0.10 | asserted 1.00 |
| s2 | For the linear pQCD approaches we consider both the usual collinear factorization and the k_T-factorization formalisms, whereas for the nonlinear QCD (saturation) calculations one considers the Golec-Biernat-Wuesthoff and the Iancu-Itakura-Munier parameterizations for the dipole cross section within the color dipole picture. | method 0.99 | 0.54 | 0.04 | asserted 0.98 |
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Original abstract
We calculate the photoproduction of heavy quarks in proton-proton collisions at RHIC, Tevatron and LHC energies. The integrated cross section and the rapidity distributions for open charm and bottom production are computed employing sound high energy QCD formalisms. For the linear pQCD approaches we consider both the usual collinear factorization and the k_T-factorization formalisms, whereas for the nonlinear QCD (saturation) calculations one considers the Golec-Biernat-Wuesthoff and the Iancu-Itakura-Munier parameterizations for the dipole cross section within the color dipole picture.
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