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\begin{document}
 
 \footnotesize
 
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  \begin{tabular}{l l r@{$\,\pm\,$}l l l l l l l l l l l l}
    Resonance & Var & \multicolumn{2}{c}{Baseline} & \makebox[9mm][l]{\rotatebox{60}{\makecell[c]{$d_{ D\xspace\xspace^0\xspace}, d_{ R\xspace}$}}} & \makebox[9mm][l]{\rotatebox{60}{\makecell[c]{ $ -2\log\mathcal{L}$ \xspace}}} & \makebox[9mm][l]{\rotatebox{60}{\makecell[c]{Efficiency}}} & \makebox[9mm][l]{\rotatebox{60}{\makecell[c]{$\max(|\cos|)$}}} & \makebox[9mm][l]{\rotatebox{60}{\makecell[c]{Weights}}} & \makebox[9mm][l]{\rotatebox{60}{\makecell[c]{Comb.}}} & \makebox[9mm][l]{\rotatebox{60}{\makecell[c]{Flatt\'{e}\xspace}}} & \makebox[9mm][l]{\rotatebox{60}{\makecell[c]{$T_{\rho\xspace\xspace^{\pm}}$}}} & \makebox[9mm][l]{\rotatebox{60}{\makecell[c]{$f_{\text{m}}, f_{\text{c}}$}}} & \makebox[9mm][l]{\rotatebox{60}{\makecell[c]{Joint}}} \\
    \midrule
    \multirow{1}{*}{ $ K\xspace\xspace^{*}_{{}}({892})^{{+}}$ \xspace} &FF [\%] & $56.9$ & $0.6\pm1.1$ & $0.03$ & $0.10$ & $0.40$ & $0.10$ & $0.19$ & $0.07$ & $0.06$ & $0.16$ & $0.17$ & $1.00$ &  \\
    \cmidrule{2-14}
    \multirow{3}{*}{ $ K\xspace\xspace^{*}_{{}}({1410})^{{+}}$ \xspace} & $ a_{ R\xspace}$ \xspace & $5.83$ & $0.29\pm0.29$ & $0.04$ & $0.02$ & $0.26$ & $0.05$ & $0.06$ & $0.02$ & $0.06$ & $0.02$ & $0.05$ & $0.06$ &  \\
     & $\phi_{ R\xspace}$ \xspace $(^{\circ})$ & $-143$ & $3\pm6$ & $1.9$ & $0.2$ & $3.7$ & $2.8$ & $1.6$ & $1.6$ & $0.7$ & $1.1$ & $0.1$ & $0.1$ &  \\
     &FF [\%] & $9.6$ & $1.1\pm2.9$ & $2.79$ & $0.06$ & $0.80$ & $0.22$ & $0.15$ & $0.14$ & $0.23$ & $0.02$ & $0.18$ & $0.21$ &  \\
    \cmidrule{2-14}
    \multirow{3}{*}{\mbox{$( K\xspace\xspace^0_{\rm\scriptscriptstyle S}\xspace\pi\xspace\xspace)^{+}_{S\text{-wave}}$}\xspace} & $ a_{ R\xspace}$ \xspace & $1.13$ & $0.09\pm0.21$ & $0.11$ & $0.11$ & $0.03$ & $0.09$ & $0.06$ & $0.06$ & $0.04$ & $0.04$ & $0.03$ & $0.02$ &  \\
     & $\phi_{ R\xspace}$ \xspace $(^{\circ})$ & $-59$ & $4\pm13$ & $10.6$ & $6.2$ & $3.2$ & $0.9$ & $0.6$ & $0.1$ & $1.3$ & $0.5$ & $0.8$ & $0.3$ &  \\
     &FF [\%] & $11.7$ & $1.0\pm2.3$ & $0.68$ & $0.53$ & $0.35$ & $1.35$ & $0.87$ & $0.90$ & $0.33$ & $0.71$ & $0.30$ & $0.56$ &  \\
    \cmidrule{2-14}
    \multirow{3}{*}{ $\overline{ K\xspace}{}\xspace^{*}_{{}}({892})^{{0}}$ \xspace} & $ a_{ R\xspace}$ \xspace & $0.210$ & $0.006\pm0.010$ & $0.01$ & $0.00$ & $0.00$ & $0.01$ & $0.00$ & $0.00$ & $0.00$ & $0.00$ & $0.00$ & $0.00$ &  \\
     & $\phi_{ R\xspace}$ \xspace $(^{\circ})$ & $-101.5$ & $2.0\pm2.8$ & $0.2$ & $1.8$ & $2.0$ & $0.0$ & $0.2$ & $0.4$ & $0.3$ & $0.4$ & $0.2$ & $0.1$ &  \\
     &FF [\%] & $2.47$ & $0.15\pm0.23$ & $0.16$ & $0.00$ & $0.06$ & $0.10$ & $0.03$ & $0.09$ & $0.03$ & $0.03$ & $0.04$ & $0.03$ &  \\
    \cmidrule{2-14}
    \multirow{3}{*}{ $\overline{ K\xspace}{}\xspace^{*}_{{}}({1410})^{{0}}$ \xspace} & $ a_{ R\xspace}$ \xspace & $3.9$ & $0.2\pm0.4$ & $0.13$ & $0.07$ & $0.24$ & $0.24$ & $0.17$ & $0.05$ & $0.07$ & $0.05$ & $0.05$ & $0.09$ &  \\
     & $\phi_{ R\xspace}$ \xspace $(^{\circ})$ & $-174$ & $4\pm7$ & $0.4$ & $3.5$ & $2.3$ & $3.3$ & $4.0$ & $1.9$ & $0.4$ & $0.4$ & $0.3$ & $0.2$ &  \\
     &FF [\%] & $3.8$ & $0.5\pm2.0$ & $1.75$ & $0.38$ & $0.70$ & $0.38$ & $0.08$ & $0.00$ & $0.15$ & $0.01$ & $0.10$ & $0.45$ &  \\
    \cmidrule{2-14}
    \multirow{3}{*}{\mbox{$( K\xspace\xspace\pi\xspace\xspace)^{0}_{S\text{-wave}}$}\xspace} & $ a_{ R\xspace}$ \xspace & $1.28$ & $0.12\pm0.23$ & $0.10$ & $0.07$ & $0.13$ & $0.07$ & $0.10$ & $0.06$ & $0.03$ & $0.03$ & $0.03$ & $0.01$ &  \\
     & $\phi_{ R\xspace}$ \xspace $(^{\circ})$ & $75$ & $3\pm8$ & $3.7$ & $3.7$ & $3.1$ & $2.5$ & $3.0$ & $1.6$ & $1.2$ & $1.4$ & $0.9$ & $0.0$ &  \\
     &FF [\%] & $18$ & $2\pm4$ & $2.36$ & $0.57$ & $1.97$ & $1.10$ & $1.08$ & $0.54$ & $0.30$ & $0.72$ & $0.22$ & $1.58$ &  \\
    \cmidrule{2-14}
    \multirow{3}{*}{ $ a\xspace_{0}(980)^{{-}}$ \xspace} & $ a_{ R\xspace}$ \xspace & $1.07$ & $0.09\pm0.14$ & $0.12$ & $0.02$ & $0.07$ & $0.02$ & $0.02$ & $0.01$ & $0.01$ & $0.02$ & $0.01$ & $0.02$ &  \\
     & $\phi_{ R\xspace}$ \xspace $(^{\circ})$ & $82$ & $5\pm7$ & $2.5$ & $2.1$ & $4.6$ & $1.2$ & $0.9$ & $0.9$ & $3.0$ & $0.6$ & $0.6$ & $0.5$ &  \\
     &FF [\%] & $4.0$ & $0.7\pm1.1$ & $0.91$ & $0.19$ & $0.50$ & $0.06$ & $0.20$ & $0.03$ & $0.17$ & $0.18$ & $0.14$ & $0.05$ &  \\
    \cmidrule{2-14}
    \multirow{3}{*}{ $ a\xspace_{2}(1320)^{{-}}$ \xspace} & $ a_{ R\xspace}$ \xspace & $0.17$ & $0.03\pm0.05$ & $0.02$ & $0.01$ & $0.04$ & $0.00$ & $0.01$ & $0.01$ & $0.00$ & $0.01$ & $0.00$ & $0.01$ &  \\
     & $\phi_{ R\xspace}$ \xspace $(^{\circ})$ & $-128$ & $10\pm8$ & $3.9$ & $3.9$ & $2.9$ & $2.8$ & $1.9$ & $2.5$ & $1.0$ & $0.5$ & $1.1$ & $1.4$ &  \\
     &FF [\%] & $0.15$ & $0.06\pm0.13$ & $0.09$ & $0.02$ & $0.08$ & $0.01$ & $0.02$ & $0.01$ & $0.01$ & $0.01$ & $0.01$ & $0.02$ &  \\
    \cmidrule{2-14}
    \multirow{3}{*}{ $ a\xspace_{0}(1450)^{{-}}$ \xspace} & $ a_{ R\xspace}$ \xspace & $0.43$ & $0.05\pm0.10$ & $0.07$ & $0.06$ & $0.03$ & $0.02$ & $0.02$ & $0.00$ & $0.00$ & $0.01$ & $0.01$ & $0.01$ &  \\
     & $\phi_{ R\xspace}$ \xspace $(^{\circ})$ & $-49$ & $11\pm19$ & $3.0$ & $12.5$ & $8.2$ & $5.7$ & $7.1$ & $1.2$ & $4.0$ & $2.2$ & $4.1$ & $0.5$ &  \\
     &FF [\%] & $0.74$ & $0.15\pm0.34$ & $0.25$ & $0.18$ & $0.10$ & $0.07$ & $0.08$ & $0.00$ & $0.00$ & $0.04$ & $0.01$ & $0.01$ &  \\
    \cmidrule{2-14}
    \multirow{3}{*}{ $\rho\xspace\xspace(1450)^{{-}}$ \xspace} & $ a_{ R\xspace}$ \xspace & $1.3$ & $0.1\pm0.4$ & $0.27$ & $0.05$ & $0.06$ & $0.01$ & $0.05$ & $0.01$ & $0.03$ & $0.24$ & $0.01$ & $0.00$ &  \\
     & $\phi_{ R\xspace}$ \xspace $(^{\circ})$ & $-144$ & $7\pm9$ & $1.5$ & $6.0$ & $3.2$ & $2.8$ & $2.2$ & $3.3$ & $1.0$ & $3.7$ & $1.0$ & $0.8$ &  \\
     &FF [\%] & $1.4$ & $0.2\pm0.7$ & $0.63$ & $0.21$ & $0.13$ & $0.06$ & $0.12$ & $0.05$ & $0.07$ & $0.10$ & $0.04$ & $0.07$ &  \\
    \midrule
     $\chi^2/\mathrm{bin}$ \xspace & & \multicolumn{2}{c}{1.10} & $1.11$ & $1.10$ & $-$ & $1.08$ & $-$ & $1.10$ & $1.10$ & $1.10$ & $1.10$ & $1.17$ \\
    DFF [\%] & & \multicolumn{2}{c}{109.1} & $114.1$ & $108.5$ & $-$ & $107.0$ & $-$ & $107.7$ & $108.7$ & $110.8$ & $109.4$ & $110.0$ \\
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