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相关论文: The Longitudinal Structure Function at the Third O…

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As a first step towards the complete calculation of deep-inelastic scattering at third order of massless perturbative QCD, we have computed the fermionic (nf) contributions to the flavour non-singlet structure functions in unpolarized…

高能物理 - 唯象学 · 物理学 2009-11-07 J. A. M. Vermaseren , S. Moch , A. Vogt

We have investigated the next-to-next-to-leading order (NNLO) corrections to inclusive hadron production in e^+e^- annihilation and the related parton fragmentation distributions, the `time-like' counterparts of the `space-like'…

高能物理 - 唯象学 · 物理学 2008-11-26 A. Mitov , S. Moch , A. Vogt

We compute the full three-loop coefficient functions for the structure functions F_2 and F_L in massless perturbative QCD. The results for F_L complete the next-to-next-to-leading order description of unpolarized electromagnetic…

高能物理 - 唯象学 · 物理学 2008-11-26 J. A. M. Vermaseren , A. Vogt , S. Moch

In this paper, we compute the first set of ${\cal O}(\alpha_s^2)$ corrections to semi-inclusive deep inelastic scattering structure functions. We start by studying the impact of the contribution of the partonic subprocesses that open at…

高能物理 - 唯象学 · 物理学 2017-03-01 Daniele Anderle , Daniel de Florian , Yamila Rotstein Habarnau

We present results for unpolarized and polarized semi-inclusive deep-inelastic scattering mediated by electroweak gauge bosons at next-to-next-to-leading order (NNLO) in perturbative quantum chromodynamics. The results include all relevant…

高能物理 - 唯象学 · 物理学 2026-04-01 Saurav Goyal , Sven-Olaf Moch , Vaibhav Pathak , V. Ravindran

We compute the next-to-next-to-leading order (NNLO) contributions to the splitting functions governing the evolution of the unpolarized flavour-singlet parton densities in perturbative QCD. The exact expressions are presented in both…

高能物理 - 唯象学 · 物理学 2010-04-05 A. Vogt , S. Moch , J. A. M. Vermaseren

We study the next-to-next-to-leading order (NNLO) evolution of flavour singlet parton densities and structure functions in massless perturbative QCD. Present information on the corresponding three-loop splitting functions is used to derive…

高能物理 - 唯象学 · 物理学 2009-10-31 W. L. van Neerven , A. Vogt

We summarize recent results on the evolution of unpolarized parton densities and deep-inelastic structure functions in massless perturbative QCD. Due to last year's extension of the integer-moment calculations of the three-loop splitting…

高能物理 - 唯象学 · 物理学 2008-11-26 W. L. van Neerven , A. Vogt

We study the next-to-next-to-leading order (NNLO) evolution of flavour non-singlet quark densities and structure functions in massless perturbative QCD. Present information on the corresponding three-loop splitting functions is used to…

高能物理 - 唯象学 · 物理学 2008-11-26 W. L. van Neerven , A. Vogt

We have calculated the coefficient functions for the structure functions F_2, F_L and F_3 in nu-nubar charged-current deep-inelastic scattering (DIS) at the third order in the strong coupling alpha_s, thus completing the description of…

高能物理 - 唯象学 · 物理学 2016-06-30 J. Davies , A. Vogt , S. Moch , J. A. M. Vermaseren

We have computed the complete next-to-next-to-leading order (NNLO) contributions to the splitting functions governing the evolution of unpolarized parton densities in perturbative QCD. Our results agree with all partial results available in…

高能物理 - 唯象学 · 物理学 2009-11-10 S. Moch , J. A. M. Vermaseren , A. Vogt

Using Laplace transform techniques, I calculate the longitudinal structure function $F_{L}(x,Q^{2})$ from the scaling violations of the proton structure function $F_{2}(x,Q^{2})$, and make a critical study of this relationship between the…

高能物理 - 唯象学 · 物理学 2018-01-31 G. R. Boroun

The next-to-next-to-leading order (NNLO) corrections in massless perturbative QCD are derived for the parton distributions of the photon and the deep inelastic structure functions F_1^gamma and F_2^gamma. We present the full photonic…

高能物理 - 唯象学 · 物理学 2009-11-07 S. Moch , J. A. M. Vermaseren , A. Vogt

We compute the fermionic (n_f) contributions to the flavour non-singlet structure functions in unpolarized electromagnetic deep-inelastic scattering at third order of massless perturbative QCD. Complete results are presented for the…

高能物理 - 唯象学 · 物理学 2010-04-05 S. Moch , J. A. M. Vermaseren , A. Vogt

The next-to-next-to-leading order (NNLO) non-singlet QCD analysis of the experimental data of the CCFR collaboration for the $xF_3$ and $F_2$ structure functions of the deep-inelastic scattering of neutrinos and antineutrinos on the nucleon…

高能物理 - 唯象学 · 物理学 2011-04-20 A. L. Kataev , A. V. Kotikov , G. Parente , A. V. Sidorov

We study the evolution of the flavour non-singlet deep-inelastic structure functions F_{2,NS} and F_3 at the next-to-next-to-next-to-leading order (N^3LO) of massless perturbative QCD. The present information on the corresponding three-loop…

高能物理 - 唯象学 · 物理学 2009-11-07 W. L. van Neerven , A. Vogt

We have calculated the n_f^2 and n_f^3 contributions to the flavour non-singlet structure functions F_2 and F_L in inclusive deep-inelastic scattering at the fourth order in the strong coupling alpha_s. The coefficient functions have been…

高能物理 - 唯象学 · 物理学 2023-04-12 A. Basdew-Sharma , A. Pelloni , Franz Herzog , A. Vogt

We report on the status of the calculation of deep-inelastic structure functions at three loops in perturbative QCD. The method employed allows to calculate the Mellin moments of structure functions analytically as a general function of N.…

高能物理 - 唯象学 · 物理学 2007-05-23 S. Moch , J. A. M. Vermaseren

We present the analytic calculation of the Mellin moments of the structure functions F_2, F_3 and F_L in perturbative QCD up to second order corrections and in leading twist approximation. We calculate the 2-loop contributions to the…

高能物理 - 唯象学 · 物理学 2009-10-31 S. Moch , J. A. M. Vermaseren

We compute the next-to-next-to-leading order (NNLO) contributions to the three splitting functions governing the evolution of unpolarized non-singlet combinations of quark densities in perturbative QCD. Our results agree with all partial…

高能物理 - 唯象学 · 物理学 2008-11-26 S. Moch , J. A. M. Vermaseren , A. Vogt
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