$e^+e^- \to b \bar{b} u \bar{d} μ^- \barν_μ$ with a $t\bar{t}$ production

Details $e^+e^- \to b \bar{b} u \bar{d} μ^- \barν_μ$ with a $t\bar{t}$ production $e^+e^- \to b \bar{b} u \bar{d} μ^- \barν_μ$ with a $t\bar{t}$ production

1997-06-03

arxiv.org/abs/hep-ph/9706225v2

Phys.Lett. B414 (1997) 178-186

Physics

High Energy Physics

High Energy Physics - Phenomenology

17 pages, 8 PostScript figures, LateX; To appear in Phys. Lett. B

Scientific paper

10.1016/S0370-2693(97)01117-9

The cross section of $e^+e^- \to b \bar{b} u \bar{d} \mu^- \bar{\nu}_\mu$ process with a complete set of tree diagrams, 232 diagrams in the unitary gauge, was calculated at the energy range of $\sqrt{s}$ = 340 - 500 GeV by using GRACE system. A main contribution to the cross section comes from $t\bar{t}$ production, where $t$ and $\bar{t}$ decay into $bu\bar{d}$ and $\bar{b} \mu^- \bar{\nu}_{\mu}$, respectively. It was found that the interference between the diagrams with $t\bar{t}$ production and those with single-$t$ through $ WW $ pair production amounts to 10% at the $t \bar{t}$ threshold energy region. In the energy region above twice of the top quark mass, more than 95% of the cross section comes from the $t\bar{t}$ diagrams.

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