Table of Contents
Fetching ...

Search for Fermion-Pair Decays $Q\Qbar \to (\t\Wmp)(\tbar\Wpm)$ in Same-Charge Dilepton Events

The CDF Collaboration

Abstract

We report the most restrictive direct limits on masses of fourth-generation down-type quarks $b^{\prime}$, and quark-like composite fermions ($B$ or $T_{5/3}$), decaying promptly to $t W^{\mp}$. We search for a significant excess of events with two same-charge leptons ($e$, $μ$), several hadronic jets, and missing transverse energy. An analysis of data from $p\overline{p}$ collisions with an integrated luminosity of 2.7 fb$^{-1}$ collected with the CDF II detector at Fermilab yields no evidence for such a signal, setting mass limits $m_{b^{\prime}}, m_{B} >$ 338 $\mathrm{GeV}/c^2$ and $m_{T_{5/3}} >$ 365 $\mathrm{GeV}/c^2$ at 95% confidence level.

Search for Fermion-Pair Decays $Q\Qbar \to (\t\Wmp)(\tbar\Wpm)$ in Same-Charge Dilepton Events

Abstract

We report the most restrictive direct limits on masses of fourth-generation down-type quarks , and quark-like composite fermions ( or ), decaying promptly to . We search for a significant excess of events with two same-charge leptons (, ), several hadronic jets, and missing transverse energy. An analysis of data from collisions with an integrated luminosity of 2.7 fb collected with the CDF II detector at Fermilab yields no evidence for such a signal, setting mass limits 338 and 365 at 95% confidence level.

Paper Structure

This paper contains 4 figures, 3 tables.

Figures (4)

  • Figure 1: Missing transverse energy in events with same-charge leptons in 2.7$\hbox{,fb}^{-1}$ . The right outer-most bin includes overflow events with ${\not\!\! E_T} > 160$ GeV.
  • Figure 2: Number of reconstructed jets for the expected backgrounds. The observed data and the $b^{\prime}$ (or $B$) signal are shown at the best-fit rate for $m_Q=330$ GeV/$c^2$. The fitted size and shape for the $T_{5/3}\xspace+B$ signal is nearly identical.
  • Figure 3: Event displays for the observed three-jet, $\mu\mu$ event (a,b) and the five-jet, $e\mu$ event (c,d). Shown in (a) and (c) are views of the events along the beam axis; jets shown as cones, electrons as solid lines, muons as dotted lines and missing transverse energy as an arrow; lengths are proportional to $p_T$ (see Table \ref{['table:evdetails']}). Shown in (b) and (d) are views of the events in $\eta-\phi$; jets shown as open circles, electrons as filled circles and muons as dashed circles; radii are proportional to $p_T$.
  • Figure 4: Theoretical cross sections for $b^{\prime}$ (or $B$) and $T_{5/3}\xspace+B$ with expected and observed 95% C.L. limits overlaid.