10 papers found.

Use AND, OR, NOT, +word, -word, "long phrase", (parentheses) to fine-tune your search.

Use AND, OR, NOT, +word, -word, "long phrase", (parentheses) to fine-tune your search.

neutrino
uxes, Astropart. Phys. 5 (1996) 309 [hep-ph/9505417] [INSPIRE].
[5] M.V. Garzelli, **S**. **Moch** and G. Sigl, Lepton
uxes from atmospheric charm revisited, JHEP
10 (2015) 115 [arXiv:1507.01570] [INSPIRE ...
(2015) 040 [arXiv:1410.8849] [INSPIRE].
(2016) 471 [arXiv:1603.08906] [INSPIRE].
[63] S. Alekhin, J. Blumlein and **S**. **Moch**, Parton Distribution Functions and Benchmark Cross
sections at NNLO, Phys. Rev

].
[14] **S**. **Moch**, J.A.M. Vermaseren and A. Vogt, The three loop splitting functions in QCD: the
nonsinglet case, Nucl. Phys. B 688 (2004) 101 [hep-ph/0403192] [INSPIRE].
[15] A. Vogt, **S**. **Moch** and J.A.M ...
production in QCD at three loops, Phys. Rev. Lett. 114 (2015) 212001 [arXiv:1503.06056]
[22] J.A.M. Vermaseren, A. Vogt and **S**. **Moch**, The third-order QCD corrections to
deep-inelastic scattering by photon

) 014504 [arXiv:1503.03656] [INSPIRE].
[6] **S**. **Moch**, J.A.M. Vermaseren and A. Vogt, The three loop splitting functions in QCD: The
nonsinglet case, Nucl. Phys. B 688 (2004) 101 [hep-ph/0403192] [INSPIRE].
[7 ... .
HJEP06(217)3
Lett. B 734 (2014) 137 [arXiv:1404.0863] [INSPIRE].
[16] V.M. Braun, A.N. Manashov, **S**. **Moch** and M. Strohmaier, Two-loop conformal generators
for leading-twist operators in QCD, JHEP 03 (2016

: Measuring atmospheric neutrino oscillations at the South Pole , EPJ Web Conf . 116 ( 2016 ) 11009 [5] KM3NeT collaboration, U.F. Katz, The ORCA Option for KM3NeT, PoS(NEUTEL [6] M.V. Garzelli , **S**. **Moch** and G ... . Aaron et al., Combined Measurement and QCD Analysis of [52] S. Alekhin , J. Blumlein and **S**. **Moch** , Parton Distribution Functions and Benchmark Cross [53] A. Accardi , L.T. Brady , W. Melnitchouk , J.F

We take a look at how the differential distributions for top-quark production are affected by changing to the running mass scheme. Specifically we consider the transverse momentum, rapidity and pair-invariant mass distributions at next-to-leading order for the top-quark mass in the \(\overline{\hbox {MS}}\) scheme. It is found that, similar to the total cross section, the...

. 114 (2015) 142002
[54] A. Buckley et al., LHAPDF6: parton density access in the LHC precision era, Eur. Phys. J.
[55] S. Alekhin, J. Blumlein and **S**. **Moch**, Parton distribution functions and benchmark ... to [56] S. Alekhin , J. Blumlein and **S**. **Moch** , The ABM parton distributions tuned to LHC data , [59] H.-L. Lai et al., New parton distributions for collider physics, Phys. Rev. D 82 (2010) 074024 [62

reproduction in
any medium, provided the original author(s) and source are credited.
References
[1] **S**. **Moch**, J.A.M. Vermaseren and A. Vogt, The three loop splitting functions in QCD: The
nonsinglet case, Nucl ... . Phys. B 688 (2004) 101 [hep-ph/0403192] [INSPIRE].
[2] A. Vogt, **S**. **Moch** and J.A.M. Vermaseren, The three-loop splitting functions in QCD: The
singlet case, Nucl. Phys. B 691 (2004) 129 [hep-ph/0404111

We review the present status of the determination of parton distribution functions (PDFs) in the light of the precision requirements for the LHC in Run 2 and other future hadron colliders. We provide brief reviews of all currently available PDF sets and use them to compute cross sections for a number of benchmark processes, including Higgs boson production in gluon–gluon fusion...

We analyse a tension between the D0 and CDF inclusive jet data and the perturbative QCD calculations, which are based on the ABKM09 and ABM11 parton distribution functions (PDFs) within the nuisance parameter framework. Particular attention is paid on the uncertainties in the nuisance parameters due to the data fluctuations and the PDF errors. We show that with account of these...

The single-logarithmic enhancement of the physical kernel for Higgs production by gluon-gluon fusion in the heavy top-quark limit is employed to derive the leading so far unknown contributions, ln 5, 4, 3(1−z), to the N3LO coefficient function in the threshold expansion. Also using knowledge from Higgs-exchange DIS to estimate the remaining terms not vanishing for z = m H 2...