Invariant mass distributions of (a) $ B ^0 \rightarrow D ^- \pi ^+ $ (b) $ B ^0 \rightarrow D ^- K ^+ $ and (c) $ B ^0_ s \rightarrow D ^-_ s \pi ^+ $ candidates. The solid line is the result of the fit and the dotted line indicates the signal. The stacked background shapes follow the same top-to-bottom order in the legend and the plot. The $ B ^0_ s $ and $\overline{\Lambda} ^0_ b $ backgrounds in the $ B ^0 \rightarrow D ^- \pi ^+ $ mass distribution are invisibly small. The resulting signal yields are listed in Table 1. For illustration purposes the figures include events from both magnet polarities, although they are fitted separately as described in the text.

Ratio of fragmentation fractions $ f_s/f_d$ as functions of (a) $p_{\rm T}$ and (b) $\eta$. The errors on the data points are the statistical and uncorrelated systematic uncertainties added in quadrature. The solid line is the result of a linear fit, and the dashed line corresponds to the fit for the no-dependence hypothesis. The average value of $p_{\rm T}$ or $\eta$ is determined for each bin and used as the center of the bin. The horizontal error bars indicate the bin size. Note that the scale is zero suppressed.

Animated gif made out of all figures.

Yields obtained from the fits to the invariant mass distributions.

Systematic uncertainties for the measurement of the corrected ratio of event yields used for the measurements of $ f_s/f_d$ and the relative branching fraction of $ B ^0 \rightarrow D ^- K ^+ $ . The systematic uncertainty in $p_{\rm T}$ and $\eta$ bins is shown as a range in the last column, and the total systematic uncertainty is the quadratic sum of the uncorrelated uncertainties. The systematic uncertainties on the ratio of $ B ^0 \rightarrow D ^- \pi ^+ $ and $ B ^0_ s \rightarrow D ^-_ s \pi ^+ $ yields that are correlated among the bins do not affect the dependence on $p_{\rm T}$ or $\eta$, and are not accounted for in the total systematic uncertainty.