Study of $b-$hadron decays to $\Lambda_c^+h^-h^{\prime -}$ final states
- Aaij, Roel et al
- arXiv:2405.12688CERN-EP-2024-116LHCb-PAPER-2024-013
| \small Examples of decay diagrams for the (left)~$\mathchar"7104_{b}^-\to\mathchar"7103_{c}^+ K^-\pi^-$, (centre)~$\mathchar"7104_{b}^-\to\mathchar"7103_{c}^+ K^- K^-$ and (right)~$\mathchar"710A_{b}^-\to\mathchar"7103_{c}^+ K^- K^-$ channels. |
| \small Examples of decay diagrams for the (left)~$\mathit{\Xi}_{b}^-\to\mathit{\Lambda}_{c}^+ K^-\pi^-$, (centre)~$\mathit{\Xi}_{b}^-\to\mathit{\Lambda}_{c}^+ K^- K^-$ and (right)~$\mathit{\Omega}_{b}^-\to\mathit{\Lambda}_{c}^+ K^- K^-$ channels. |
| \small Examples of decay diagrams for the (left)~$\mathchar"7104_{b}^-\to\mathchar"7103_{c}^+ K^-\pi^-$, (centre)~$\mathchar"7104_{b}^-\to\mathchar"7103_{c}^+ K^- K^-$ and (right)~$\mathchar"710A_{b}^-\to\mathchar"7103_{c}^+ K^- K^-$ channels. |
| \small Examples of decay diagrams for the (left)~$\mathit{\Xi}_{b}^-\to\mathit{\Lambda}_{c}^+ K^-\pi^-$, (centre)~$\mathit{\Xi}_{b}^-\to\mathit{\Lambda}_{c}^+ K^- K^-$ and (right)~$\mathit{\Omega}_{b}^-\to\mathit{\Lambda}_{c}^+ K^- K^-$ channels. |
| \small Examples of decay diagrams for the (left)~$\mathchar"7104_{b}^-\to\mathchar"7103_{c}^+ K^-\pi^-$, (centre)~$\mathchar"7104_{b}^-\to\mathchar"7103_{c}^+ K^- K^-$ and (right)~$\mathchar"710A_{b}^-\to\mathchar"7103_{c}^+ K^- K^-$ channels. |
| \small Examples of decay diagrams for the (left)~$\mathit{\Xi}_{b}^-\to\mathit{\Lambda}_{c}^+ K^-\pi^-$, (centre)~$\mathit{\Xi}_{b}^-\to\mathit{\Lambda}_{c}^+ K^- K^-$ and (right)~$\mathit{\Omega}_{b}^-\to\mathit{\Lambda}_{c}^+ K^- K^-$ channels. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+ K^- K^-$, (middle)~$\mathchar"7103_{c}^+ K^-\pi^-$ and (bottom)~$\mathchar"7103_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathchar"7104_{b}^-$ and $\mathchar"710A_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+ K^- K^-$, (middle)~$\mathit{\Lambda}_{c}^+ K^-\pi^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathit{\Xi}_{b}^-$ and $\mathit{\Omega}_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+ K^- K^-$, (middle)~$\mathchar"7103_{c}^+ K^-\pi^-$ and (bottom)~$\mathchar"7103_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathchar"7104_{b}^-$ and $\mathchar"710A_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+ K^- K^-$, (middle)~$\mathit{\Lambda}_{c}^+ K^-\pi^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathit{\Xi}_{b}^-$ and $\mathit{\Omega}_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+ K^- K^-$, (middle)~$\mathchar"7103_{c}^+ K^-\pi^-$ and (bottom)~$\mathchar"7103_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathchar"7104_{b}^-$ and $\mathchar"710A_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+ K^- K^-$, (middle)~$\mathit{\Lambda}_{c}^+ K^-\pi^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathit{\Xi}_{b}^-$ and $\mathit{\Omega}_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+ K^- K^-$, (middle)~$\mathchar"7103_{c}^+ K^-\pi^-$ and (bottom)~$\mathchar"7103_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathchar"7104_{b}^-$ and $\mathchar"710A_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+ K^- K^-$, (middle)~$\mathit{\Lambda}_{c}^+ K^-\pi^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathit{\Xi}_{b}^-$ and $\mathit{\Omega}_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+ K^- K^-$, (middle)~$\mathchar"7103_{c}^+ K^-\pi^-$ and (bottom)~$\mathchar"7103_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathchar"7104_{b}^-$ and $\mathchar"710A_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+ K^- K^-$, (middle)~$\mathit{\Lambda}_{c}^+ K^-\pi^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathit{\Xi}_{b}^-$ and $\mathit{\Omega}_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+ K^- K^-$, (middle)~$\mathchar"7103_{c}^+ K^-\pi^-$ and (bottom)~$\mathchar"7103_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathchar"7104_{b}^-$ and $\mathchar"710A_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+ K^- K^-$, (middle)~$\mathit{\Lambda}_{c}^+ K^-\pi^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathit{\Xi}_{b}^-$ and $\mathit{\Omega}_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+ K^- K^-$, (middle)~$\mathchar"7103_{c}^+ K^-\pi^-$ and (bottom)~$\mathchar"7103_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathchar"7104_{b}^-$ and $\mathchar"710A_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+ K^- K^-$, (middle)~$\mathit{\Lambda}_{c}^+ K^-\pi^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathit{\Xi}_{b}^-$ and $\mathit{\Omega}_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+ K^- K^-$, (middle)~$\mathchar"7103_{c}^+ K^-\pi^-$ and (bottom)~$\mathchar"7103_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathchar"7104_{b}^-$ and $\mathchar"710A_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+ K^- K^-$, (middle)~$\mathit{\Lambda}_{c}^+ K^-\pi^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathit{\Xi}_{b}^-$ and $\mathit{\Omega}_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+ K^- K^-$, (middle)~$\mathchar"7103_{c}^+ K^-\pi^-$ and (bottom)~$\mathchar"7103_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathchar"7104_{b}^-$ and $\mathchar"710A_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+ K^- K^-$, (middle)~$\mathit{\Lambda}_{c}^+ K^-\pi^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathit{\Xi}_{b}^-$ and $\mathit{\Omega}_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+ K^- K^-$, (middle)~$\mathchar"7103_{c}^+ K^-\pi^-$ and (bottom)~$\mathchar"7103_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathchar"7104_{b}^-$ and $\mathchar"710A_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+ K^- K^-$, (middle)~$\mathit{\Lambda}_{c}^+ K^-\pi^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathit{\Xi}_{b}^-$ and $\mathit{\Omega}_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+ K^- K^-$, (middle)~$\mathchar"7103_{c}^+ K^-\pi^-$ and (bottom)~$\mathchar"7103_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathchar"7104_{b}^-$ and $\mathchar"710A_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+ K^- K^-$, (middle)~$\mathit{\Lambda}_{c}^+ K^-\pi^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathit{\Xi}_{b}^-$ and $\mathit{\Omega}_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+ K^- K^-$, (middle)~$\mathchar"7103_{c}^+ K^-\pi^-$ and (bottom)~$\mathchar"7103_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathchar"7104_{b}^-$ and $\mathchar"710A_{b}^-$ decays. |
| \small Mass distributions of the signal channels with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+ K^- K^-$, (middle)~$\mathit{\Lambda}_{c}^+ K^-\pi^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\pi^-\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends, where the signal components include independent contributions from $\mathit{\Xi}_{b}^-$ and $\mathit{\Omega}_{b}^-$ decays. |
| \small Mass distributions of the $B^-$ modes with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+\overline{p} K^-$ and (bottom)~$\mathchar"7103_{c}^+\overline{p}\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends. |
| \small Mass distributions of the $B^-$ modes with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+\overline{p} K^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\overline{p}\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends. |
| \small Mass distributions of the $B^-$ modes with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+\overline{p} K^-$ and (bottom)~$\mathchar"7103_{c}^+\overline{p}\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends. |
| \small Mass distributions of the $B^-$ modes with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+\overline{p} K^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\overline{p}\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends. |
| \small Mass distributions of the $B^-$ modes with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+\overline{p} K^-$ and (bottom)~$\mathchar"7103_{c}^+\overline{p}\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends. |
| \small Mass distributions of the $B^-$ modes with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+\overline{p} K^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\overline{p}\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends. |
| \small Mass distributions of the $B^-$ modes with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+\overline{p} K^-$ and (bottom)~$\mathchar"7103_{c}^+\overline{p}\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends. |
| \small Mass distributions of the $B^-$ modes with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+\overline{p} K^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\overline{p}\pi^-$ final states for (left)~Run~1 and (right)~Run~2. The different components in the fit are shown as indicated in the legends. |
| \small Mass distributions of the $B^-$ modes with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+\overline{p} K^-$ and (bottom)~$\mathchar"7103_{c}^+\overline{p}\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends. |
| \small Mass distributions of the $B^-$ modes with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+\overline{p} K^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\overline{p}\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends. |
| \small Mass distributions of the $B^-$ modes with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+\overline{p} K^-$ and (bottom)~$\mathchar"7103_{c}^+\overline{p}\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends. |
| \small Mass distributions of the $B^-$ modes with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+\overline{p} K^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\overline{p}\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends. |
| \small Mass distributions of the $B^-$ modes with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+\overline{p} K^-$ and (bottom)~$\mathchar"7103_{c}^+\overline{p}\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends. |
| \small Mass distributions of the $B^-$ modes with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+\overline{p} K^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\overline{p}\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends. |
| \small Mass distributions of the $B^-$ modes with results of the fit superimposed: (top)~$\mathchar"7103_{c}^+\overline{p} K^-$ and (bottom)~$\mathchar"7103_{c}^+\overline{p}\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends. |
| \small Mass distributions of the $B^-$ modes with results of the fit superimposed: (top)~$\mathit{\Lambda}_{c}^+\overline{p} K^-$ and (bottom)~$\mathit{\Lambda}_{c}^+\overline{p}\pi^-$ final states for (left)~Run~1 and (right)~Run~2 (log scale). The different components in the fit are shown as indicated in the legends. |
| Distributions of (top)~$p_{\mathrm{T}}$ and (bottom)~$\eta$ for $B^- \to \mathchar"7103_{c}^+\overline{p}\pi^-$ decays in (left)~Run~1 and (right)~Run~2, obtained from background-subtracted data and compared to the uncorrected distributions from simulation. |
| Distributions of (top)~$p_{\mathrm{T}}$ and (bottom)~$\eta$ for $B^- \to \mathit{\Lambda}_{c}^+\overline{p}\pi^-$ decays in (left)~Run~1 and (right)~Run~2, obtained from background-subtracted data and compared to the uncorrected distributions from simulation. |
| Distributions of (top)~$p_{\mathrm{T}}$ and (bottom)~$\eta$ for $B^- \to \mathchar"7103_{c}^+\overline{p}\pi^-$ decays in (left)~Run~1 and (right)~Run~2, obtained from background-subtracted data and compared to the uncorrected distributions from simulation. |
| Distributions of (top)~$p_{\mathrm{T}}$ and (bottom)~$\eta$ for $B^- \to \mathit{\Lambda}_{c}^+\overline{p}\pi^-$ decays in (left)~Run~1 and (right)~Run~2, obtained from background-subtracted data and compared to the uncorrected distributions from simulation. |
| Distributions of (top)~$p_{\mathrm{T}}$ and (bottom)~$\eta$ for $B^- \to \mathchar"7103_{c}^+\overline{p}\pi^-$ decays in (left)~Run~1 and (right)~Run~2, obtained from background-subtracted data and compared to the uncorrected distributions from simulation. |
| Distributions of (top)~$p_{\mathrm{T}}$ and (bottom)~$\eta$ for $B^- \to \mathit{\Lambda}_{c}^+\overline{p}\pi^-$ decays in (left)~Run~1 and (right)~Run~2, obtained from background-subtracted data and compared to the uncorrected distributions from simulation. |
| Distributions of (top)~$p_{\mathrm{T}}$ and (bottom)~$\eta$ for $B^- \to \mathchar"7103_{c}^+\overline{p}\pi^-$ decays in (left)~Run~1 and (right)~Run~2, obtained from background-subtracted data and compared to the uncorrected distributions from simulation. |
| Distributions of (top)~$p_{\mathrm{T}}$ and (bottom)~$\eta$ for $B^- \to \mathit{\Lambda}_{c}^+\overline{p}\pi^-$ decays in (left)~Run~1 and (right)~Run~2, obtained from background-subtracted data and compared to the uncorrected distributions from simulation. |
| Distributions of (top)~$p_{\mathrm{T}}$ and (bottom)~$\eta$ for $\mathchar"7104_{b}^- \to \mathchar"7103_{c}^+ K^-\pi^-$ decays in (left)~Run~1 and (right)~Run~2, obtained from background-subtracted data and compared to the uncorrected distributions from simulation. |
| Distributions of (top)~$p_{\mathrm{T}}$ and (bottom)~$\eta$ for $\mathit{\Xi}_{b}^- \to \mathit{\Lambda}_{c}^+ K^-\pi^-$ decays in (left)~Run~1 and (right)~Run~2, obtained from background-subtracted data and compared to the uncorrected distributions from simulation. |
| Distributions of (top)~$p_{\mathrm{T}}$ and (bottom)~$\eta$ for $\mathchar"7104_{b}^- \to \mathchar"7103_{c}^+ K^-\pi^-$ decays in (left)~Run~1 and (right)~Run~2, obtained from background-subtracted data and compared to the uncorrected distributions from simulation. |
| Distributions of (top)~$p_{\mathrm{T}}$ and (bottom)~$\eta$ for $\mathit{\Xi}_{b}^- \to \mathit{\Lambda}_{c}^+ K^-\pi^-$ decays in (left)~Run~1 and (right)~Run~2, obtained from background-subtracted data and compared to the uncorrected distributions from simulation. |
| Distributions of (top)~$p_{\mathrm{T}}$ and (bottom)~$\eta$ for $\mathchar"7104_{b}^- \to \mathchar"7103_{c}^+ K^-\pi^-$ decays in (left)~Run~1 and (right)~Run~2, obtained from background-subtracted data and compared to the uncorrected distributions from simulation. |
| Distributions of (top)~$p_{\mathrm{T}}$ and (bottom)~$\eta$ for $\mathit{\Xi}_{b}^- \to \mathit{\Lambda}_{c}^+ K^-\pi^-$ decays in (left)~Run~1 and (right)~Run~2, obtained from background-subtracted data and compared to the uncorrected distributions from simulation. |
| Distributions of (top)~$p_{\mathrm{T}}$ and (bottom)~$\eta$ for $\mathchar"7104_{b}^- \to \mathchar"7103_{c}^+ K^-\pi^-$ decays in (left)~Run~1 and (right)~Run~2, obtained from background-subtracted data and compared to the uncorrected distributions from simulation. |
| Distributions of (top)~$p_{\mathrm{T}}$ and (bottom)~$\eta$ for $\mathit{\Xi}_{b}^- \to \mathit{\Lambda}_{c}^+ K^-\pi^-$ decays in (left)~Run~1 and (right)~Run~2, obtained from background-subtracted data and compared to the uncorrected distributions from simulation. |
| Background-subtracted and efficiency-corrected distributions of $B^-\to\mathchar"7103_{c}^+\overline{p}\pi^-$ decays: (top~left)~$m(\mathchar"7103_{c}^+\pi^-)$ at low mass, showing the $\mathchar"7106_{c}(2455)^0$ resonance peak; (top~right)~$m(\mathchar"7103_{c}^+\pi^-)$ at higher mass, showing additional $\mathchar"7106_{c}$ resonance structures; (bottom)~$m(\mathchar"7103_{c}^+\overline{p})$ at low mass, where $m(\mathchar"7103_{c}^+\pi^-)>2460\,\mathrm{Me\kern -0.1em V\!/}c^2$ has been required to remove contributions from the $\mathchar"7106_{c}(2455)^0$ resonance. |
| Background-subtracted and efficiency-corrected distributions of $B^-\to\mathit{\Lambda}_{c}^+\overline{p}\pi^-$ decays: (top~left)~$m(\mathit{\Lambda}_{c}^+\pi^-)$ at low mass, showing the $\mathit{\Sigma}_{c}(2455)^0$ resonance peak; (top~right)~$m(\mathit{\Lambda}_{c}^+\pi^-)$ at higher mass, showing additional $\mathit{\Sigma}_{c}$ resonance structures; (bottom)~$m(\mathit{\Lambda}_{c}^+\overline{p})$ at low mass, where $m(\mathit{\Lambda}_{c}^+\pi^-)>2460\,\mathrm{Me\kern -0.1em V\!/}c^2$ has been required to remove contributions from the $\mathit{\Sigma}_{c}(2455)^0$ resonance. |
| Background-subtracted and efficiency-corrected distributions of $B^-\to\mathchar"7103_{c}^+\overline{p}\pi^-$ decays: (top~left)~$m(\mathchar"7103_{c}^+\pi^-)$ at low mass, showing the $\mathchar"7106_{c}(2455)^0$ resonance peak; (top~right)~$m(\mathchar"7103_{c}^+\pi^-)$ at higher mass, showing additional $\mathchar"7106_{c}$ resonance structures; (bottom)~$m(\mathchar"7103_{c}^+\overline{p})$ at low mass, where $m(\mathchar"7103_{c}^+\pi^-)>2460\,\mathrm{Me\kern -0.1em V\!/}c^2$ has been required to remove contributions from the $\mathchar"7106_{c}(2455)^0$ resonance. |
| Background-subtracted and efficiency-corrected distributions of $B^-\to\mathit{\Lambda}_{c}^+\overline{p}\pi^-$ decays: (top~left)~$m(\mathit{\Lambda}_{c}^+\pi^-)$ at low mass, showing the $\mathit{\Sigma}_{c}(2455)^0$ resonance peak; (top~right)~$m(\mathit{\Lambda}_{c}^+\pi^-)$ at higher mass, showing additional $\mathit{\Sigma}_{c}$ resonance structures; (bottom)~$m(\mathit{\Lambda}_{c}^+\overline{p})$ at low mass, where $m(\mathit{\Lambda}_{c}^+\pi^-)>2460\,\mathrm{Me\kern -0.1em V\!/}c^2$ has been required to remove contributions from the $\mathit{\Sigma}_{c}(2455)^0$ resonance. |
| Background-subtracted and efficiency-corrected distributions of $B^-\to\mathchar"7103_{c}^+\overline{p}\pi^-$ decays: (top~left)~$m(\mathchar"7103_{c}^+\pi^-)$ at low mass, showing the $\mathchar"7106_{c}(2455)^0$ resonance peak; (top~right)~$m(\mathchar"7103_{c}^+\pi^-)$ at higher mass, showing additional $\mathchar"7106_{c}$ resonance structures; (bottom)~$m(\mathchar"7103_{c}^+\overline{p})$ at low mass, where $m(\mathchar"7103_{c}^+\pi^-)>2460\,\mathrm{Me\kern -0.1em V\!/}c^2$ has been required to remove contributions from the $\mathchar"7106_{c}(2455)^0$ resonance. |
| Background-subtracted and efficiency-corrected distributions of $B^-\to\mathit{\Lambda}_{c}^+\overline{p}\pi^-$ decays: (top~left)~$m(\mathit{\Lambda}_{c}^+\pi^-)$ at low mass, showing the $\mathit{\Sigma}_{c}(2455)^0$ resonance peak; (top~right)~$m(\mathit{\Lambda}_{c}^+\pi^-)$ at higher mass, showing additional $\mathit{\Sigma}_{c}$ resonance structures; (bottom)~$m(\mathit{\Lambda}_{c}^+\overline{p})$ at low mass, where $m(\mathit{\Lambda}_{c}^+\pi^-)>2460\,\mathrm{Me\kern -0.1em V\!/}c^2$ has been required to remove contributions from the $\mathit{\Sigma}_{c}(2455)^0$ resonance. |
| Background-subtracted and efficiency-corrected distributions of $B^-\to\mathchar"7103_{c}^+\overline{p} K^-$ decays: (left)~$m(\mathchar"7103_{c}^+\overline{p})$ at low mass; (right)~$m(\mathchar"7103_{c}^+ K^-)$ at low mass, where $m(\mathchar"7103_{c}^+\overline{p})>3500\,\mathrm{Me\kern -0.1em V\!/}c^2$ has been required to remove contributions from the $\mathchar"7103_{c}^+\overline{p}$ threshold enhancement. |
| Background-subtracted and efficiency-corrected distributions of $B^-\to\mathit{\Lambda}_{c}^+\overline{p} K^-$ decays: (left)~$m(\mathit{\Lambda}_{c}^+\overline{p})$ at low mass; (right)~$m(\mathit{\Lambda}_{c}^+ K^-)$ at low mass, where $m(\mathit{\Lambda}_{c}^+\overline{p})>3500\,\mathrm{Me\kern -0.1em V\!/}c^2$ has been required to remove contributions from the $\mathit{\Lambda}_{c}^+\overline{p}$ threshold enhancement. |
| Background-subtracted and efficiency-corrected distributions of $B^-\to\mathchar"7103_{c}^+\overline{p} K^-$ decays: (left)~$m(\mathchar"7103_{c}^+\overline{p})$ at low mass; (right)~$m(\mathchar"7103_{c}^+ K^-)$ at low mass, where $m(\mathchar"7103_{c}^+\overline{p})>3500\,\mathrm{Me\kern -0.1em V\!/}c^2$ has been required to remove contributions from the $\mathchar"7103_{c}^+\overline{p}$ threshold enhancement. |
| Background-subtracted and efficiency-corrected distributions of $B^-\to\mathit{\Lambda}_{c}^+\overline{p} K^-$ decays: (left)~$m(\mathit{\Lambda}_{c}^+\overline{p})$ at low mass; (right)~$m(\mathit{\Lambda}_{c}^+ K^-)$ at low mass, where $m(\mathit{\Lambda}_{c}^+\overline{p})>3500\,\mathrm{Me\kern -0.1em V\!/}c^2$ has been required to remove contributions from the $\mathit{\Lambda}_{c}^+\overline{p}$ threshold enhancement. |
| Background-subtracted and efficiency-corrected distributions of $\Xibm\to\mathchar"7103_{c}^+ K^-\pi^-$ decays: (left)~$m(\mathchar"7103_{c}^+ K^-)$ at low mass; (right)~$m(\mathchar"7103_{c}^+\pi^-)$ at low mass. |
| Background-subtracted and efficiency-corrected distributions of $\Xibm\to\mathit{\Lambda}_{c}^+ K^-\pi^-$ decays: (left)~$m(\mathit{\Lambda}_{c}^+ K^-)$ at low mass; (right)~$m(\mathit{\Lambda}_{c}^+\pi^-)$ at low mass. |
| Background-subtracted and efficiency-corrected distributions of $\Xibm\to\mathchar"7103_{c}^+ K^-\pi^-$ decays: (left)~$m(\mathchar"7103_{c}^+ K^-)$ at low mass; (right)~$m(\mathchar"7103_{c}^+\pi^-)$ at low mass. |
| Background-subtracted and efficiency-corrected distributions of $\Xibm\to\mathit{\Lambda}_{c}^+ K^-\pi^-$ decays: (left)~$m(\mathit{\Lambda}_{c}^+ K^-)$ at low mass; (right)~$m(\mathit{\Lambda}_{c}^+\pi^-)$ at low mass. |
| \small Variation of the ratio of fragmentation fractions times branching fractions of \mbox{$\mathchar"7104_{b}^- \to \mathchar"7103_{c}^+ K^-\pi^-$} and $B^- \to \mathchar"7103_{c}^+\overline{p}\pi^-$ decays with (left)~$b$-hadron transverse momentum and (right)~pseudorapidity, separately for Run~1 and Run~2, with statistical uncertainties only. |
| \small Variation of the ratio of fragmentation fractions times branching fractions of \mbox{$\mathit{\Xi}_{b}^- \to \mathit{\Lambda}_{c}^+ K^-\pi^-$} and $B^- \to \mathit{\Lambda}_{c}^+\overline{p}\pi^-$ decays with (left)~$b$-hadron transverse momentum and (right)~pseudorapidity, separately for Run~1 and Run~2, with statistical uncertainties only. |
| \small Variation of the ratio of fragmentation fractions times branching fractions of \mbox{$\mathchar"7104_{b}^- \to \mathchar"7103_{c}^+ K^-\pi^-$} and $B^- \to \mathchar"7103_{c}^+\overline{p}\pi^-$ decays with (left)~$b$-hadron transverse momentum and (right)~pseudorapidity, separately for Run~1 and Run~2, with statistical uncertainties only. |
| \small Variation of the ratio of fragmentation fractions times branching fractions of \mbox{$\mathit{\Xi}_{b}^- \to \mathit{\Lambda}_{c}^+ K^-\pi^-$} and $B^- \to \mathit{\Lambda}_{c}^+\overline{p}\pi^-$ decays with (left)~$b$-hadron transverse momentum and (right)~pseudorapidity, separately for Run~1 and Run~2, with statistical uncertainties only. |
| \small Variation of the ratio of branching fractions of $B^-\to\mathchar"7103_{c}^+\overline{p} K^-$ and $B^-\to\mathchar"7103_{c}^+\overline{p}\pi^-$ decays with (left)~$b$-hadron transverse momentum and (right)~pseudorapidity, separately for Run~1 and Run~2, with statistical uncertainties only. |
| \small Variation of the ratio of branching fractions of $B^-\to\mathit{\Lambda}_{c}^+\overline{p} K^-$ and $B^-\to\mathit{\Lambda}_{c}^+\overline{p}\pi^-$ decays with (left)~$b$-hadron transverse momentum and (right)~pseudorapidity, separately for Run~1 and Run~2, with statistical uncertainties only. |
| \small Variation of the ratio of branching fractions of $B^-\to\mathchar"7103_{c}^+\overline{p} K^-$ and $B^-\to\mathchar"7103_{c}^+\overline{p}\pi^-$ decays with (left)~$b$-hadron transverse momentum and (right)~pseudorapidity, separately for Run~1 and Run~2, with statistical uncertainties only. |
| \small Variation of the ratio of branching fractions of $B^-\to\mathit{\Lambda}_{c}^+\overline{p} K^-$ and $B^-\to\mathit{\Lambda}_{c}^+\overline{p}\pi^-$ decays with (left)~$b$-hadron transverse momentum and (right)~pseudorapidity, separately for Run~1 and Run~2, with statistical uncertainties only. |
| \small Variation of $\mathchar"7104_{b}^-$ production asymmetry with (left)~$\mathchar"7104_{b}^-$ transverse momentum and (right)~pseudorapidity determined with $\mathchar"7104_{b}^-\to\mathchar"7103_{c}^+ K^-\pi^-$ decays. |
| \small Variation of $\mathit{\Xi}_{b}^-$ production asymmetry with (left)~$\mathit{\Xi}_{b}^-$ transverse momentum and (right)~pseudorapidity determined with $\mathit{\Xi}_{b}^-\to\mathit{\Lambda}_{c}^+ K^-\pi^-$ decays. |
| \small Variation of $\mathchar"7104_{b}^-$ production asymmetry with (left)~$\mathchar"7104_{b}^-$ transverse momentum and (right)~pseudorapidity determined with $\mathchar"7104_{b}^-\to\mathchar"7103_{c}^+ K^-\pi^-$ decays. |
| \small Variation of $\mathit{\Xi}_{b}^-$ production asymmetry with (left)~$\mathit{\Xi}_{b}^-$ transverse momentum and (right)~pseudorapidity determined with $\mathit{\Xi}_{b}^-\to\mathit{\Lambda}_{c}^+ K^-\pi^-$ decays. |
| \small Variation of $B^-$ production asymmetry with (left)~$B^-$ transverse momentum and (right)~pseudorapidity determined with the $B^- \rightarrow \mathchar"7103_{c}^+ \overline{p} \pi^-$ control mode. |
| \small Variation of $B^-$ production asymmetry with (left)~$B^-$ transverse momentum and (right)~pseudorapidity determined with the $B^- \rightarrow \mathit{\Lambda}_{c}^+ \overline{p} \pi^-$ control mode. |
| \small Variation of $B^-$ production asymmetry with (left)~$B^-$ transverse momentum and (right)~pseudorapidity determined with the $B^- \rightarrow \mathchar"7103_{c}^+ \overline{p} \pi^-$ control mode. |
| \small Variation of $B^-$ production asymmetry with (left)~$B^-$ transverse momentum and (right)~pseudorapidity determined with the $B^- \rightarrow \mathit{\Lambda}_{c}^+ \overline{p} \pi^-$ control mode. |