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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 perturbativeâ€¦ (More)

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 exactâ€¦ (More)

- H.-J. Stolberg, Susan D Moch, +4 authors Peter Pirsch
- 2004 IEEE International Solid-State Circuitsâ€¦
- 2004

An SoC is comprised of a 16-way SIMD DSP core with a 2D matrix memory, a 64b VLIW DSP core with subword parallelism, and a 32b RISC core. The 81mm/sup 2/ chip is implemented in a 0.18/spl mu/m 6Mâ€¦ (More)

- M. Aliev, H. Lacker, U. Langenfeld, Susan D Moch, Peter Uwer, M. Wiedermann
- Computer Physics Communications
- 2011

Required libraries: The code uses the FF library [3] to calculate scalar one-loop integrals and the dilogarithm. Random numbers for the Monte Carlo integration are generated using the Ranlux libraryâ€¦ (More)

- Susan D Moch, Peter Uwer
- 2008

We present updated predictions for the total cross section of top-quark pair production at Tevatron and LHC. For the LHC we also provide results at âˆš s = 10 TeV, in view of the anticipated run inâ€¦ (More)

We compute the fermionic (nf ) contributions to the flavour non-singlet structure functions in unpolarized electromagnetic deep-inelastic scattering at third order of massless perturbative QCD.â€¦ (More)

- Susan D Moch, C. Schneider
- 2008

We report on the calculation of multi-loop Feynman integrals for single-scale problems by means of difference equations in Mellin space. The solution to these difference equations in terms ofâ€¦ (More)

- Susan D Moch, Annika Vogt
- 2006

Utilizing recent three-loop results on the quark and gluon splitting functions and form factors, we derive the complete threshold-enhanced third-order (N 3 LO) QCD corrections to the total crossâ€¦ (More)

We present the first direct determination of the running top-quark mass based on the total cross section of top-quark pair-production as measured at the Tevatron. Our theory prediction for the crossâ€¦ (More)

We compute the complete third-order contributions to the coefficient functions for the longitudinal structure function F L , thus completing the next-to-next-to-leading order (NNLO) description ofâ€¦ (More)