A key ingredient to searches for physics beyond the Standard Model in $B^{0}_{s}$ mixing phenomena is the measurement of the $B^{0}_{s}$-$\bar{B}^{0}_{s}$ oscillation frequency, which is equivalent to the mass difference $\Delta m_{s}$ of the $B^{0}_{s}$ mass eigenstates. Using the world's largest $B^{0}_{s}$ meson sample accumulated in a dataset, corresponding to an integrated luminosity of 1.0 fb$^{-1}$, collected by the LHCb experiment at the CERN LHC in 2011, a measurement of $\Delta m_{s}$ is presented. A total of about 34,000 $B^{0}_{s}\rightarrowD^{-}_{s}\pi^{+}$ signal decays are reconstructed, with an average decay time resolution of 44 fs. The oscillation frequency is measured to be $\Delta m_{s}$ = 17.768 $\pm$ 0.023 (stat) $\pm$ 0.006 (syst) ps$^{-1}$, which is the most precise measurement to date.
Invariant mass distributions for $ B ^0_ s \rightarrow D ^-_ s \pi ^+ $ candidates with the $ D ^-_ s $ meson decaying as a) $ D ^-_ s \rightarrow \phi( K ^+ K ^- )\pi ^- $ , b) $ D ^-_ s \rightarrow K ^{*0} ( K ^+ \pi ^- ) K ^- $ , c) $ D ^-_ s \rightarrow K ^+ K ^- \pi ^- $ nonresonant, d) $ D ^-_ s \rightarrow K ^- \pi ^+ \pi ^- $ , and e) $ D ^-_ s \rightarrow \pi ^- \pi ^+ \pi ^- $ . The fits and the various background components are described in the text. Misidentified backgrounds refer to background from $ B ^0$ and $\Lambda ^0_ b $ decays with one misidentified daughter particle. |
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Decay time distribution for the sum of the five decay modes for candidates tagged as mixed (different flavour at decay and production; red, continuous line) or unmixed (same flavour at decay and production; blue, dotted line). The data and the fit projections are plotted in a signal window around the reconstructed $ B ^0_ s $ mass of 5.32 -- 5.55 $ {\mathrm{ Ge V /}c^2}$ . |
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Animated gif made out of all figures. |
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Number of candidates and $ B ^0_ s $ signal fractions in the mass range 5.32 -- 5.98 $ {\mathrm{ Ge V /}c^2}$ . |
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Systematic uncertainties on the $\Delta m_{ s }$ measurement. The total systematic uncertainty is calculated as the quadratic sum of the individual contributions. |
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Created on 02 May 2024.