\ \ \ \ \ \ \ 494^*$    $\ \ \ \ \ \ \ \ 477$       $\ \ \ \ \ \ \ \ \ 958^*$     $\ \ \ \ \ \ \ \ \ 92^*$    $\ \ \ \ \ \ \ \ \ 117^*$      $\ \ \ \ \ \ \ \ -14$                       $\ \ \ \ \ \ \ 235$                                  $\ \ \ \ \ \ \ 187\ \ $                 
   b    $\ \ \ \ \ \ \ \ \ \ \ \ \ 138^*$   $\ \ \ \ \ \ \ \ \ 494^*$    $\ \ \ \ \ \ \ \ 477$       $\ \ \ \ \ \ \ \ \ 958^*$     $\ \ \ \ \ \ \ \ \ 92^*$    $\ \ \ \ \ \ \ \ \ 117^*$      $\ \ \ \ \ \ \ \ -14$                       $\ \ \ \ \ \ \ 235$                                  $\ \ \ \ \ \ \ 187\ \ $                 

[TABLE III. The masses of the scalar nonet (in MeV), and the corresponding singlet-octet mixing angle $\theta_s$ (in degrees). ]{}

        $\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ 