Search for $C\!P$ violation and observation of $P$ violation in $\Lambda_b^0 \to p \pi^- \pi^+ \pi^-$ decays
- Aaij, Roel et al
- arXiv:1912.10741LHCB-PAPER-2019-028CERN-EP-2019-256
| Invariant-mass distribution for \LbToppipipi candidates with the result of the fit overlaid. The solid and dotted lines describe the projections of the fit results for various components as listed in the legend. |
| Invariant-mass distribution for \LbToppipipi candidates with the result of the fit overlaid. The solid and dotted lines describe the projections of the fit results for various components as listed in the legend. |
| \small Measured asymmetries for the binning scheme (left) $A_1$ and $A_2$ and (right) $B_1$ and $B_2$. The error bars represent the sum in quadrature of the statistical and systematic uncertainties. The \chisq per ndof is calculated with respect to the null hypothesis and includes statistical and systematic uncertainties. |
| \small Measured asymmetries for the binning scheme (left) $A_1$ and $A_2$ and (right) $B_1$ and $B_2$. The error bars represent the sum in quadrature of the statistical and systematic uncertainties. The \chisq per ndof is calculated with respect to the null hypothesis and includes statistical and systematic uncertainties. |
| \small Measured asymmetries for the binning scheme (left) $A_1$ and $A_2$ and (right) $B_1$ and $B_2$. The error bars represent the sum in quadrature of the statistical and systematic uncertainties. The \chisq per ndof is calculated with respect to the null hypothesis and includes statistical and systematic uncertainties. |
| \small Measured asymmetries for the binning scheme (left) $A_1$ and $A_2$ and (right) $B_1$ and $B_2$. The error bars represent the sum in quadrature of the statistical and systematic uncertainties. The \chisq per ndof is calculated with respect to the null hypothesis and includes statistical and systematic uncertainties. |