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Observation of the Production of a W Boson in Association with a Single Charm Quark

CDF Collaboration

TL;DR

The first observation of the production of a W boson with a single charm quark (c) jet in pp[over ¯] collisions at √s=1.96  TeV is reported, and the magnitude of the quark-mixing matrix element V(cs) is derived.

Abstract

The first observation of the production of a $W$ boson with a single charm quark ($c$) jet in $p\bar{p}$ collisions at $\sqrt{s}=1.96 {\rm TeV}$ is reported. The analysis uses data corresponding to 4.3 fb$^{-1}$, recorded with the CDF II detector at the Fermilab Tevatron. Charm quark candidates are selected through the identification of an electron or muon from charm-hadron semileptonic decay within a hadronic jet, and a $Wc$ signal is observed with a significance of 5.7 standard deviations. The production cross section $σ_{Wc}(p_{Tc}>20 {\rm GeV}/c, |η_c|<1.5)\times B(W\rightarrow \ellν)$ is measured to be $13.6^{+3.4}_{-3.1} {\rm pb}$ and is in agreement with theoretical expectations. From this result the magnitude of the quark-mixing matrix element $V_{cs}$ is derived, $|V_{cs}|=1.08\pm0.16$ along with a lower limit of $|V_{cs}|>0.71$ at the 95% confidence level, assuming that the $Wc$ production through $c$ to $s$ quark coupling is dominant.

Observation of the Production of a W Boson in Association with a Single Charm Quark

TL;DR

The first observation of the production of a W boson with a single charm quark (c) jet in pp[over ¯] collisions at √s=1.96  TeV is reported, and the magnitude of the quark-mixing matrix element V(cs) is derived.

Abstract

The first observation of the production of a boson with a single charm quark () jet in collisions at is reported. The analysis uses data corresponding to 4.3 fb, recorded with the CDF II detector at the Fermilab Tevatron. Charm quark candidates are selected through the identification of an electron or muon from charm-hadron semileptonic decay within a hadronic jet, and a signal is observed with a significance of 5.7 standard deviations. The production cross section is measured to be and is in agreement with theoretical expectations. From this result the magnitude of the quark-mixing matrix element is derived, along with a lower limit of at the 95% confidence level, assuming that the production through to quark coupling is dominant.

Paper Structure

This paper contains 1 equation, 1 figure, 2 tables.

Figures (1)

  • Figure 1: (color online) The soft muon and soft electron $p_T$ distributions. The $Wc$ contribution is normalized to the measured cross section.