Amplitude analysis of $B^\pm \to \pi^\pm K^+ K^-$ decays
- Aaij, Roel et al
- arXiv:1905.09244LHCb-PAPER-2018-051CERN-EP-2019-062
 | \small Distribution of \mmpik up to 3.5 \gevgevcccc. Data are represented by points for \Bp and \Bm candidates separately, with the result of the second solution overlaid. This is interpreted as an unphysical solution. The relative contribution of the individual components in the model is also shown, with the interference terms effects not included. |
 | \small Distribution of \mmpik up to 3.5 \gevgevcccc. Data are represented by points for \Bp and \Bm candidates separately, with the result of the second solution overlaid. This is interpreted as an unphysical solution. The relative contribution of the individual components in the model is also shown, with the interference terms effects not included. |
 | \small Distribution of \mmpik in the high mass region. Data are represented by points for (top) \Bp and (bottom) \Bm with the result of the second solution overlaid. This is interpreted as an unphysical solution. The relative contribution of the individual components in the model is also shown, with the interference terms effects not included. |
 | \small Distribution of \mmpik in the high mass region. Data are represented by points for (top) \Bp and (bottom) \Bm with the result of the second solution overlaid. This is interpreted as an unphysical solution. The relative contribution of the individual components in the model is also shown, with the interference terms effects not included. |
 | \small Distribution of \mmpik up to 3.5 \gevgevcccc. Data are represented by points for \Bp and \Bm candidates separately, with the result of the nominal solution overlaid. The relative contribution of the individual components in the model is also shown, with the interference terms effects not included. |
 | \small Distribution of \mmkk up to 3.5 \gevgevcccc. Data are represented by points for \Bp and \Bm candidates separately, with the result of the second solution overlaid. This is interpreted as an unphysical solution. The relative contribution of the individual components in the model is also shown, with the interference terms effects not included. |
 | \small Distribution of \mmkk up to 3.5 \gevgevcccc. Data are represented by points for \Bp and \Bm candidates separately, with the result of the second solution overlaid. This is interpreted as an unphysical solution. The relative contribution of the individual components in the model is also shown, with the interference terms effects not included. |
 | \small Distribution of \mmpik up to 3.5 \gevgevcccc. Data are represented by points for \Bp and \Bm candidates separately, with the result of the nominal solution overlaid. The relative contribution of the individual components in the model is also shown, with the interference terms effects not included. |
 | \small Dalitz plot for \kkpip and \kkpim candidates in the selected signal region. |
 | \small Distribution of \mmpik in the high mass region. Data are represented by points for (top) \Bp and (bottom) \Bm with the result of the nominal solution overlaid. The relative contribution of the individual components in the model is also shown, with the interference terms effects not included. |
 | \small Distribution of \mmkk up to 3.5 \gevgevcccc. Data are represented by points for \Bp and \Bm candidates separately, with the result of the nominal solution overlaid. The relative contribution of the individual components in the model is also shown, with the interference terms effects not included. |
 | \small Distribution of \mmkk up to 3.5 \gevgevcccc. Data are represented by points for \Bp and \Bm candidates separately, with the result of the nominal solution overlaid. The relative contribution of the individual components in the model is also shown, with the interference terms effects not included. |
 | \small Dalitz plot for \kkpip and \kkpim candidates in the selected signal region. |
 | \small Distribution of \mmpik in the high mass region. Data are represented by points for (top) \Bp and (bottom) \Bm with the result of the nominal solution overlaid. The relative contribution of the individual components in the model is also shown, with the interference terms effects not included. |
 | \small Distribution of \mmpik. Data are represented by points for \Bp and \Bm candidates separately, with the result of the fit overlaid. |
 | \small Distribution of \mmpik. Data are represented by points for \Bp and \Bm candidates separately, with the result of the fit overlaid. |
 | \small Distribution of \mmkk up to 3.5\gevgevcccc. Data are represented by points for \Bp and \Bm separately, with the result of the fit overlaid. |
 | \small Distribution of \mmkk up to 3.5\gevgevcccc. Data are represented by points for \Bp and \Bm separately, with the result of the fit overlaid. |