QCD NLO predictions to $W$-pair production in association with a massive (anti)bottom-jet at the LHC

Details QCD NLO predictions to $W$-pair production in association with a massive (anti)bottom-jet at the LHC QCD NLO predictions to $W$-pair production in association with a massive (anti)bottom-jet at the LHC

2011-06-15

arxiv.org/abs/1106.2890v2

Phys.Rev.D84:014009,2011

Physics

High Energy Physics

High Energy Physics - Phenomenology

Published version in PRD

Scientific paper

10.1103/PhysRevD.84.014009

The $W$-pair production in association with a massive (anti)bottom jet is not only an important background to a number of interesting processes, such as the single top production associated with a W boson, but also a potential background to new physics searches. We present the calculations of the total and differential cross sections for the $W^+W^-+ b(\bar{b})$ jet productions at the LHC up to the QCD next-to-leading order (NLO). Our results by adopting the QCD NLO contribution collection scheme-I show that the K factors can be 1.66 and 1.21 with the inclusive and exclusive two-jet event selection schemes respectively, when we set $m_H=120 GeV$, $\mu=m_W+m_b/2$ and take the constraints of $p_{T,b(\bar{b})}>25 GeV$, $|y_{b(\bar{b})}|<2.5$ for $b(\bar{b})$ jet. We find that the stabilization of the theoretical prediction for the integrated cross section for the $pp \to W^+W^-b(\bar b)+X$ up to the QCD NLO requires a veto on a second isolated hard jet and the inclusion of the QCD NLO contribution from the $W^+W^-b\bar{b}(bb, \bar{b}\bar{b})$ production with the final two $b(\bar{b})$ quarks being merged as one jet.

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