Abstract (deu)
Future linear colliders will be able to measure the top quark mass with unprecedented accuracy
using a threshold scan of the top quark pair production cross section. At threshold, the inclusive
production cross section is known from non-relativistic QCD (NRQCD), while in the continuum
it is calculated with usual fixed-order QCD. In the region between threshold and continuum the
exact form of the inclusive cross section has been unknown up to now.
The aim of this thesis is to fill this gap by matching the velocity-NRQCD (vNRQCD) next-to-
next-to-leading-logarithm (NNLL) threshold cross section to the next-to-next-to-next-to-leading-
order (NNNLO) QCD continuum cross section. We perform the matching for two cases: with the
resummation of large logarithms of the velocity at threshold and without it. Apart from QCD
effects, we include leading-order electroweak effects at threshold by shifting the center-of-mass
energy into the complex plane. This gives the bulk of all contributions to the top quark pair
production cross section at threshold. Furthermore, we use the MSR mass with an adjustable scale
R in order to have a consistent mass scheme in the matching. This avoids the renormalon problem
of the pole mass as well as the power counting breaking effects of the MS mass at threshold. In
the continuum, we employ a switch-off function to turn off the non-relativistic contributions. By
varying the switch-off function, we estimate the error in our matching.
Our results show that the matched cross section differs from both the vNRQCD and the QCD cross
section in a region starting directly above the threshold peak to about 20 GeV above the threshold.
In this region the matched cross section should be used instead of the QCD and vNRQCD cross
section. On the other hand, the matched cross section is practically identical with the vNRQCD
at threshold and with the QCD cross section for energies more than 20 GeV above the threshold,
and they replace the matched cross section in these regions. Furthermore, the dependence of the
matched cross section on the switch-off function decreases when going to higher orders, showing
the consistency of the matching.