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\begin{document}
  \footnotesize
  \resizebox{\textwidth}{!}{
  \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]{Comb.}}} & \makebox[9mm][l]{\rotatebox{60}{\makecell[c]{$\max(|\cos|)$}}} & \makebox[9mm][l]{\rotatebox{60}{\makecell[c]{$T_{\rho\xspace\xspace^{\pm}}$}}} & \makebox[9mm][l]{\rotatebox{60}{\makecell[c]{Joint}}} & \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]{Weights}}} & \makebox[9mm][l]{\rotatebox{60}{\makecell[c]{Flatt\'{e}\xspace}}} & \makebox[9mm][l]{\rotatebox{60}{\makecell[c]{$f_{\text{m}}, f_{\text{c}}$}}} \\
    \midrule
    \multirow{3}{*}{Coherence} &$R_{ K\xspace\xspace^0_{\rm\scriptscriptstyle S}\xspace K\xspace\xspace\pi\xspace\xspace\xspace}$ & $0.573$ & $0.007\pm0.019$ & $0.000$ & $0.004$ & $0.001$ & $0.003$ & $0.017$ & $0.004$ & $0.002$ & $0.004$ & $0.002$ & $0.004$ &  \\
     &$\delta_{ K\xspace\xspace^0_{\rm\scriptscriptstyle S}\xspace K\xspace\xspace\pi\xspace\xspace\xspace} - \delta_{ K\xspace\xspace^*\xspace K\xspace\xspace}$ & $0.2$ & $0.6\pm1.1$ & $0.03$ & $0.32$ & $0.45$ & $0.39$ & $0.69$ & $0.35$ & $0.23$ & $0.21$ & $0.09$ & $0.22$ & $(^{\circ})$ \\
     &$R_{ K\xspace\xspace^*\xspace K\xspace\xspace}$ & $0.831$ & $0.004\pm0.011$ & $0.002$ & $0.004$ & $0.002$ & $0.002$ & $0.007$ & $0.002$ & $0.004$ & $0.003$ & $0.001$ & $0.002$ &  \\
    \cmidrule{2-14}
    \multirow{2}{*}{ $\cal B$ \xspace} &$\cal B\xspace_{ K\xspace\xspace^*\xspace K\xspace\xspace}$ & $0.372$ & $0.001\pm0.009$ & $0.001$ & $0.001$ & $0.000$ & $0.001$ & $0.008$ & $0.000$ & $0.002$ & $0.001$ & $0.001$ & $0.001$ &  \\
     &$\cal B\xspace_{ K\xspace\xspace^0_{\rm\scriptscriptstyle S}\xspace K\xspace\xspace\pi\xspace\xspace\xspace}$ & $0.655$ & $0.001\pm0.006$ & $0.001$ & $0.002$ & $0.003$ & $0.001$ & $0.002$ & $0.000$ & $0.003$ & $0.003$ & $0.000$ & $0.000$ &  \\
    \cmidrule{2-14}
    \multirow{1}{*}{ $ C\!P$ \xspace-even fraction} &$F_+$ & $0.777$ & $0.003\pm0.009$ & $0.000$ & $0.002$ & $0.000$ & $0.001$ & $0.008$ & $0.002$ & $0.001$ & $0.002$ & $0.001$ & $0.002$ &  \\
    \cmidrule{2-14}
    \multirow{2}{*}{ $ K\xspace\xspace^{*}_{{}}({892})^{{\pm}}$ \xspace} &$m_{ R\xspace}$ & $893.1$ & $0.1\pm0.9$ & $0.3$ & $0.1$ & $0.1$ & $0.1$ & $0.9$ & $0.0$ & $0.1$ & $0.0$ & $0.0$ & $0.0$ &  $ {\mathrm{\,Me\kern -0.1em V\!/}c^2}$ \xspace \\
     &$\Gamma_{ R\xspace}$ & $46.9$ & $0.3\pm2.5$ & $0.5$ & $0.4$ & $0.5$ & $0.4$ & $2.2$ & $0.1$ & $0.2$ & $0.2$ & $0.1$ & $0.1$ &  $ {\mathrm{\,Me\kern -0.1em V\!/}c^2}$ \xspace \\
    \cmidrule{2-14}
    \multirow{1}{*}{ $ K\xspace\xspace^{*}_{{}}({1410})^{{\pm}}$ \xspace} &$\Gamma_{ R\xspace}$ & $210$ & $20\pm60$ & $8.8$ & $41.0$ & $27.0$ & $36.2$ & $11.0$ & $4.1$ & $12.5$ & $2.9$ & $7.1$ & $5.9$ &  $ {\mathrm{\,Me\kern -0.1em V\!/}c^2}$ \xspace \\
    \cmidrule{2-14}
    \multirow{4}{*}{\mbox{$( K\xspace\xspace^0_{\rm\scriptscriptstyle S}\xspace\pi\xspace\xspace)^{\pm}_{S\text{-wave}}$}\xspace} &$a$ & $4.7$ & $0.4\pm1.0$ & $0.209$ & $0.168$ & $0.606$ & $0.311$ & $0.092$ & $0.470$ & $0.095$ & $0.360$ & $0.114$ & $0.150$ &  $ {\,(\mathrm{Ge\kern -0.1em V\!/}c)^{-1}}$ \xspace \\
     &$\phi_F$ & $0.28$ & $0.05\pm0.19$ & $0.1$ & $0.0$ & $0.1$ & $0.0$ & $0.0$ & $0.0$ & $0.0$ & $0.0$ & $0.0$ & $0.0$ &  $\rm \,rad$ \xspace \\
     &$\phi_S$ & $-3.5$ & $0.2\pm0.5$ & $0.2$ & $0.1$ & $0.0$ & $0.4$ & $0.1$ & $0.1$ & $0.1$ & $0.1$ & $0.1$ & $0.1$ &  $\rm \,rad$ \xspace \\
     &$r$ & $-5.3$ & $0.4\pm1.9$ & $0.68$ & $0.84$ & $0.87$ & $1.08$ & $0.15$ & $0.49$ & $0.37$ & $0.29$ & $0.19$ & $0.24$ &  $ {\,(\mathrm{Ge\kern -0.1em V\!/}c)^{-1}}$ \xspace \\
    \cmidrule{2-14}
    \multirow{2}{*}{ $ K\xspace\xspace^{*}_{{}}({1410})^{{0}}$ \xspace} &$m_{ R\xspace}$ & $1426$ & $8\pm24$ & $2.3$ & $11.8$ & $5.8$ & $13.0$ & $10.6$ & --- & $7.4$ & $5.6$ & $2.9$ & $2.0$ &  $ {\mathrm{\,Me\kern -0.1em V\!/}c^2}$ \xspace \\
     &$\Gamma_{ R\xspace}$ & $270$ & $20\pm40$ & $26.2$ & $5.4$ & $17.6$ & $1.4$ & $23.6$ & $8.2$ & $4.6$ & $3.0$ & $4.9$ & $0.9$ &  $ {\mathrm{\,Me\kern -0.1em V\!/}c^2}$ \xspace \\
    \cmidrule{2-14}
    \multirow{5}{*}{\mbox{$( K\xspace\xspace\pi\xspace\xspace)^{0}_{S\text{-wave}}$}\xspace} &$F$ & $0.15$ & $0.03\pm0.14$ & $0.06$ & $0.02$ & $0.06$ & $0.03$ & $0.02$ & $0.08$ & $0.05$ & $0.03$ & $0.00$ & $0.00$ &  \\
     &$a$ & $4.2$ & $0.3\pm2.8$ & $1.074$ & $1.563$ & $1.092$ & $1.548$ & $0.649$ & $0.260$ & $0.607$ & $0.143$ & $0.090$ & $0.030$ &  $ {\,(\mathrm{Ge\kern -0.1em V\!/}c)^{-1}}$ \xspace \\
     &$\phi_F$ & $-2.5$ & $0.2\pm1.0$ & $0.8$ & $0.2$ & $0.2$ & $0.2$ & $0.0$ & $0.1$ & $0.3$ & $0.2$ & $0.1$ & $0.1$ &  $\rm \,rad$ \xspace \\
     &$\phi_S$ & $-1.1$ & $0.6\pm1.3$ & $0.7$ & $0.3$ & $0.8$ & $0.4$ & $0.2$ & $0.3$ & $0.5$ & $0.3$ & $0.0$ & $0.0$ &  $\rm \,rad$ \xspace \\
     &$r$ & $-3.0$ & $0.4\pm1.7$ & $1.51$ & $0.34$ & $0.33$ & $0.30$ & $0.02$ & $0.45$ & $0.17$ & $0.11$ & $0.05$ & $0.04$ &  $ {\,(\mathrm{Ge\kern -0.1em V\!/}c)^{-1}}$ \xspace \\
    \cmidrule{2-14}
    \multirow{1}{*}{ $ a\xspace_{0}(1450)^{{\pm}}$ \xspace} &$m_{ R\xspace}$ & $1430$ & $10\pm40$ & $4.1$ & $26.9$ & $16.6$ & $23.8$ & $12.6$ & $1.8$ & $7.1$ & $3.1$ & $0.8$ & $0.9$ &  $ {\mathrm{\,Me\kern -0.1em V\!/}c^2}$ \xspace \\
    \cmidrule{2-14}
    \multirow{1}{*}{ $\rho\xspace\xspace(1450)^{{\pm}}$ \xspace} &$\Gamma_{ R\xspace}$ & $410$ & $19\pm35$ & $11.1$ & $1.6$ & $4.1$ & $2.2$ & $31.3$ & --- & $8.1$ & $2.7$ & $2.6$ & $1.5$ &  $ {\mathrm{\,Me\kern -0.1em V\!/}c^2}$ \xspace \\
    \cmidrule{2-14}
    \multirow{1}{*}{ $\rho\xspace\xspace(1700)^{{\pm}}$ \xspace} &$m_{ R\xspace}$ & $1530$ & $10\pm40$ & $6.4$ & $2.6$ & $4.0$ & $0.8$ & $36.3$ & $14.7$ & $3.0$ & $4.3$ & $2.4$ & $2.6$ &  $ {\mathrm{\,Me\kern -0.1em V\!/}c^2}$ \xspace \\
  \end{tabular}}
  
\end{document}
