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Next-to-leading order QCD corrections to $bg \to t W^-$ at the CERN Large Hadron Collider

Shou-hua Zhu

Abstract

The next-to-leading order QCD corrections to the Standard Model process of single top production, $bg \to t W^-$, for the CERN Large Hadron Collider with $\sqrt{s}=14$ TeV have been calculated. For renormalization and factorization scales $μ=μ_0$ ($μ_0=m_t+m_W$), the NLO hadronic cross section is $\sim 37 $ pb, while $\sim 25 $ pb for tree level. The NLO QCD corrections can enhance the cross section by a factor from 1.33 to 1.66 for $\frac{μ_0}{2} < μ< 2 μ_0$.

Next-to-leading order QCD corrections to $bg \to t W^-$ at the CERN Large Hadron Collider

Abstract

The next-to-leading order QCD corrections to the Standard Model process of single top production, , for the CERN Large Hadron Collider with TeV have been calculated. For renormalization and factorization scales (), the NLO hadronic cross section is pb, while pb for tree level. The NLO QCD corrections can enhance the cross section by a factor from 1.33 to 1.66 for .

Paper Structure

This paper contains 16 equations, 3 figures.

Figures (3)

  • Figure 1: Feynmann diagrams for $bg \rightarrow t W^-$: the Born level (a), the virtual gluon exchange (b) and the gluon radiation (c).
  • Figure 2: Cross sections of NLO (dashed) and LO (solid) for $pp \rightarrow b g \rightarrow t W^-$ as functions of $\mu/\mu_0$ at the LHC with $\sqrt{s}=14$ TeV, where $\mu_0=m_t+m_W$.
  • Figure 3: K factor for $pp \rightarrow bg \rightarrow t W^-$ as functions of $\mu/\mu_0$ at the LHC.