Measurement of the $W+$ jets differential cross-sections in $$p\bar{p}$$ collisions at $$\sqrt{s} = 1.96$$ TeV using the CDF II Detector
In this thesis the measurements of differential cross sections for the production of themore »
The differential $$t\bar{t}$$ cross sections, measured as a function of the transverse momentum of the top quark and the invariant mass of the $$t\bar{t}$$ system, are employed to determine the pole mass of the top quark. The data corresponds to an integrated luminosity of 9.7 $$fb^{−1}$$, collected with the D0 detector of the Fermilab Tevatron. Precise calculations at next-to-next-to leading order in perturbative quantum chromodynamics provide the absolute differential cross sections that are employed to extract the pole mass of the top quark.We measure the pole mass of the top quark to be 169.1 ± 2.5 (tot.) GeV.
Czakon, M., Fiedler, P., Heymes, D., and Mitov, A. Measurement of the Pole Mass of the Top Quark using Differential $t\bar{t}$ Cross Sections in $p\bar{p}$ Collisions at $\sqrt{s}$ = 1.96 TeV. United States: N. p., 2016.
Web.
Czakon, M., Fiedler, P., Heymes, D., & Mitov, A. Measurement of the Pole Mass of the Top Quark using Differential $t\bar{t}$ Cross Sections in $p\bar{p}$ Collisions at $\sqrt{s}$ = 1.96 TeV. United States.
Czakon, M., Fiedler, P., Heymes, D., and Mitov, A. 2016.
"Measurement of the Pole Mass of the Top Quark using Differential $t\bar{t}$ Cross Sections in $p\bar{p}$ Collisions at $\sqrt{s}$ = 1.96 TeV". United States.
doi:. https://www.osti.gov/servlets/purl/1412098.
@article{osti_1412098,
title = {Measurement of the Pole Mass of the Top Quark using Differential $t\bar{t}$ Cross Sections in $p\bar{p}$ Collisions at $\sqrt{s}$ = 1.96 TeV},
author = {Czakon, M. and Fiedler, P. and Heymes, D. and Mitov, A.},
abstractNote = {The differential $t\bar{t}$ cross sections, measured as a function of the transverse momentum of the top quark and the invariant mass of the $t\bar{t}$ system, are employed to determine the pole mass of the top quark. The data corresponds to an integrated luminosity of 9.7 $fb^{−1}$, collected with the D0 detector of the Fermilab Tevatron. Precise calculations at next-to-next-to leading order in perturbative quantum chromodynamics provide the absolute differential cross sections that are employed to extract the pole mass of the top quark.We measure the pole mass of the top quark to be 169.1 ± 2.5 (tot.) GeV.},
doi = {},
journal = {},
number = ,
volume = ,
place = {United States},
year = 2016,
month = 9
}