Abstract

The $B^{\pm}$ meson production asymmetry in $pp$ collisions is measured using $B^+ \to \bar{D}^0 \pi^+$ decays. The data were recorded by the LHCb experiment during Run 1 of the LHC at centre-of-mass energies of $\sqrt{s}=$ 7 and 8 TeV. The production asymmetries, integrated over transverse momenta in the range $2 < p_{\rm T} < 30$ GeV/$c$, and rapidities in the range $2.1 < y < 4.5$, are measured to be \begin{align*} \mathcal{A}_{\rm prod}(B^+,\sqrt{s}=7~{\rm TeV}) &= (-0.41 \pm 0.49 \pm 0.10) \times 10^{-2},\\ \mathcal{A}_{\rm prod}(B^+,\sqrt{s}=8~{\rm TeV}) &= (-0.53 \pm 0.31 \pm 0.10) \times 10^{-2}, \end{align*} where the first uncertainties are statistical and the second are systematic. These production asymmetries are used to correct the raw asymmetries of $B^{+} \to J/\psi K^{+}$ decays, thus allowing a measurement of the $CP$ asymmetry, \begin{equation*} \mathcal{A}_{CP} = (0.09 \pm 0.27 \pm 0.07) \times 10^{-2}. \end{equation*}

Highlights

  • One of the primary goals of the LHCb experiment is to search for effects of physics beyond the Standard Model through measurements of CP-violating asymmetries in beauty- and charm-hadron decays

  • The Bþ production asymmetry is determined in the nine bins of pT and y according to AprodðBþÞ 1⁄4 ADrawπ − ADCPπ − AKdeπt − Aπdet − APdeIDt − ATdeISt ; ð5Þ

  • The Bþ meson production asymmetry is a crucial input in the measurement of CP asymmetries in Bþ decays

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Summary

INTRODUCTION

One of the primary goals of the LHCb experiment is to search for effects of physics beyond the Standard Model through measurements of CP-violating asymmetries in beauty- and charm-hadron decays. The current world average value of the CP asymmetry is ACPðBþ → J=ψKþÞ 1⁄4 ð0.3 Æ 0.6Þ% [4], and the uncertainty represents a limitation in many Bþ meson CP asymmetry measurements that use this channel as a reference This analysis exploits the decay Bþ → D 0πþ, which is dominated by a Cabibbo- and color-favored tree-level amplitude and is expected to have a CP asymmetry with a smaller value and uncertainty than for the Bþ → J=ψ Kþ mode. The high correlation of Adet between the two decay modes implies a partial cancellation in their difference This cancellation and the low level of CP violation in the Bþ → D 0πþ decay mode enable a precise measurement of ACPðBþ → J=ψKþÞ

LHCB DETECTOR
SELECTION OF
MEASUREMENT OF THE
Findings
SUMMARY AND CONCLUSIONS
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