Study of the production of $Λ_b^0$ and $\overline{B}^0$ hadrons in $pp$ collisions and first measurement of the $Λ_b^0\rightarrow J/ψ pK^-$ branching fraction
Abstract: The product of the $\Lambda_b0$ ($\overline{B}0$) differential production cross-section and the branching fraction of the decay $\Lambda_b0\rightarrow J/\psi pK-$ ($\overline{B}0\rightarrow J/\psi\overline{K}*(892)0$) is measured as a function of the beauty hadron transverse momentum, $p_{\rm T}$, and rapidity, $y$. The kinematic region of the measurements is $p_{\rm T}<20~{\rm GeV}/c$ and $2.0<y<4.5$. The measurements use a data sample corresponding to an integrated luminosity of $3~{\rm fb}{-1}$ collected by the LHCb detector in $pp$ collisions at centre-of-mass energies $\sqrt{s}=7~{\rm TeV}$ in 2011 and $\sqrt{s}=8~{\rm TeV}$ in 2012. Based on previous LHCb results of the fragmentation fraction ratio, $f_{\Lambda_B0}/f_d$, the branching fraction of the decay $\Lambda_b0\rightarrow J/\psi pK-$ is measured to be \begin{equation*} \mathcal{B}(\Lambda_b0\rightarrow J/\psi pK-)= (3.17\pm0.04\pm0.07\pm0.34{+0.45}_{-0.28})\times10{-4}, \end{equation*} where the first uncertainty is statistical, the second is systematic, the third is due to the uncertainty on the branching fraction of the decay $\overline{B}0\rightarrow J/\psi\overline{K}*(892)0$, and the fourth is due to the knowledge of $f_{\Lambda_b0}/f_d$. The sum of the asymmetries in the production and decay between $\Lambda_b0$ and $\overline{\Lambda}b0$ is also measured as a function of $p{\rm T}$ and $y$. The previously published branching fraction of $\Lambda_b0\rightarrow J/\psi p\pi-$, relative to that of $\Lambda_b0\rightarrow J/\psi pK-$, is updated. The branching fractions of $\Lambda_b0\rightarrow P_c+(\rightarrow J/\psi p)K-$ are determined.
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