\begin{table}%t1
   %\centering
\par
   \caption{{Parameters for two "Hot Jupiters''.  The values used for the calculation of
   the magnetic moments are given in units normalized to Jupiter, while
   the relative core radius, resulting from Eqs.~(\ref{scaleRc}) and (\ref{scaleRc2}), is normalized to the
   planetary radius.
   The magnetic moment is given
   for two cases: "tidal locking'' (using the value of~$\omega$ given above), and "fast rotation''
   (for the hypothetical case $\omega=\omega_{\rm J}$).}\label{table}}
      \begin{tabular}{l|cc}\hline\hline
         & \hspace{0.05cm} HD~209458b \hspace{0.05cm} & OGLE-TR-56b \\[4pt] \hline
        Semimajor axis $r$ [AU] & 0.045 & 0.0225 \\[4pt] \hline
        Radius $R$ [$R_{\rm J}$] & 1.42 & 1.23 \\[4pt] \hline
        Mass $M$ [$M_{\rm J}$] & 0.69 & 1.45 \\[4pt] \hline
        Rotation rate $\omega$ [$\omega_{\rm J}$] & 0.12 & 0.34 \\[4pt] \hline
        Core density $\rho_{\rm c}$ [$\rho_{\rm c, J}$]& 0.24 & 0.78 \\[4pt] \hline 
        Relative core radius $r_{\rm c}/R$ (\ref{scaleRc})& 0.54 & 0.86 \\[4pt] \hline
        Relative core radius $r_{\rm c}/R$ (\ref{scaleRc2})& 0.34 & 0.79 \\[4pt] \hline
        $\mathcal{M}$ [$\mathcal{M}_{\rm J}$] (for tidal locking) & 0.005 \ldots 0.10 & 0.40
	\ldots 0.84 \\[4pt] \hline
        $\mathcal{M}$ [$\mathcal{M}_{\rm J}$] (for fast rotation) & 0.042 \ldots 0.30 & 1.1 \ldots 1.7 \\[4pt] \hline
   \end{tabular}
  \end{table}