Using a dataset corresponding to $9 \mathrm{fb}^{-1}$ of integrated luminosity collected with the LHCb detector between 2011 and 2018 in proton-proton collisions, the decay-time distributions of the decay modes $B_s^0 \rightarrow J/\psi \eta'$ and $B_s^0 \rightarrow J/\psi \pi^{+} \pi^{-}$ are studied. The decay-width difference between the light and heavy mass eigenstates of the $B_s^0$ meson is measured to be $\Delta \Gamma_s = 0.087 \pm 0.012 \pm 0.009 \mathrm{ps}^{-1}$, where the first uncertainty is statistical and the second systematic.
Decay-time binning scheme. |
Table_1.pdf [31 KiB] HiDef png [116 KiB] Thumbnail [48 KiB] tex code |
|
Values of $\Delta \Gamma_s$ and the $\chi^2$ probability obtained from the fits to $R$ for the four datasets. The uncertainties are statistical. |
Table_2.pdf [65 KiB] HiDef png [89 KiB] Thumbnail [38 KiB] tex code |
|
Systematic uncertainties on the measurement of $\Delta \Gamma_s$. |
Table_3.pdf [63 KiB] HiDef png [86 KiB] Thumbnail [39 KiB] tex code |
Created on 27 April 2024.