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Parton distribution functions, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msub><mml:mi>α</mml:mi><mml:mi>s</mml:mi></mml:msub></mml:math>, and heavy-quark masses for LHC Run II

S. AlekhinInstitute for High Energy Physics, 142281 Protvino, Moscow region, RussiaJ. BlümleinDeutsches Elektronensynchrotron DESY, Platanenallee 6, D–15738 Zeuthen, GermanyS. MochII. Institut für Theoretische Physik, Universität Hamburg Luruper Chaussee 149, D–22761 Hamburg, GermanyR. PlačakytėII. Institut für Theoretische Physik, Universität Hamburg Luruper Chaussee 149, D–22761 Hamburg, Germany
2017lv
ABI

Аннотация

We determine a new set of parton distribution functions (ABMP16), the strong coupling constant $\alpha_s$ and the quark masses $m_c$, $m_b$ and $m_t$ in a global fit to next-to-next-to-leading order (NNLO) in QCD. The analysis uses the $\overline{\mathrm{MS}}$ scheme for $\alpha_s$ and all quark masses and is performed in the fixed-flavor number scheme for $n_f=3, 4, 5$. Essential new elements of the fit are the combined data from HERA for inclusive deep-inelastic scattering (DIS), data from the fixed-target experiments NOMAD and CHORUS for neutrino-induced DIS, and data from Tevatron and the LHC for the Drell-Yan process and the hadro-production of single-top and top-quark pairs. The theory predictions include new improved approximations at NNLO for the production of heavy quarks in DIS and for the hadro-production of single-top quarks. The description of higher twist effects relevant beyond the leading twist collinear factorization approximation is refined. At NNLO we obtain the value $\alpha_s^{(n_f=5)}(M_Z) = 0.1147 \pm 0.0008$.

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