\begin{table}%t4
\caption{Targets with $T_{\rm C}$ slopes more than 2$\sigma$ below the fit. The atmospheric parameters are taken from Santos et~al. (\cite{San04b}, \cite{San05}) and the metallic abundances are from Ecuvillon et~al. (\cite{Ecu04a},b, \cite{Ecu05a}) and Gilli et~al. (\cite{Gil05}). The Li and Be~abundances are those published by Israelian et~al. (\cite{Isr04b}) and Santos et~al. (\cite{San04c}).}
\label{twosigmaminus}
%\centering
\par
\begin{tabular}{lccc}
\hline
\hline
 & \object{HD~114783} & \object{HD~169830} \\
\hline
Type & plan & plan \\
$T_{\rm C}$ slope (10$^{-5}$~K$^{-1}$) & $-$9.07 & $-$7.00 \\
$T_{\rm eff}$ (K)& 5098 $\pm$ 36 & 6299 $\pm$ 41 \\
$\log{g}$ & 4.45 $\pm$ 0.11 & 4.10 $\pm$ 0.02 \\
$\rm [Fe/H]$ & 0.09 $\pm$ 0.04 & 0.21 $\pm$ 0.05 \\
$\rm [C/H]$ & 0.33 $\pm$ 0.13 & 0.19 $\pm$ 0.04 \\
$\rm [N/H]$ & $-$ & 0.38 $\pm$ 0.12 \\
$\rm [O/H]$ & 0.08 $\pm$ 0.18 & 0.22 $\pm$ 0.12 \\
$\rm [S/H]$ & 0.10 $\pm$ 0.07 & $-$0.10 $\pm$ 0.06 \\ 
$\rm [Zn/H]$ & 0.27 $\pm$ 0.07 & $-$ \\ 
$\rm [Cu/H]$ & 0.21 $\pm$ 0.07 & $-$ \\
$\rm [Si/H]$ & 0.02 $\pm$ 0.06 & 0.12 $\pm$ 0.05 \\
$\rm [Ca/H]$ & $-$0.28 $\pm$ 0.07 & 0.11 $\pm$ 0.07 \\
$\rm [Sc/H]$ & 0.11 $\pm$ 0.08 & 0.18 $\pm$ 0.07\\
$\rm [Ti/H]$ & 0.16 $\pm$ 0.08 & 0.08 $\pm$ 0.04 \\
$\rm [V/H]$  & 0.29 $\pm$ 0.10 & 0.17 $\pm$ 0.13 \\
$\rm [Cr/H]$ & $-$0.01 $\pm$ 0.04 & 0.03 $\pm$ 0.03 \\
$\rm [Mn/H]$ & 0.21 $\pm$ 0.06 & 0.17 $\pm$ 0.10 \\
$\rm [Co/H]$ & 0.27 $\pm$ 0.10 & 0.15 $\pm$ 0.08 \\
$\rm [Ni/H]$ & 0.05 $\pm$ 0.09 & 0.09 $\pm$  0.05 \\
$\rm [Na/H]$ &$-$0.11 $\pm$ 0.04 & 0.41 $\pm$ 0.02 \\
$\rm [Mg/H]$ & 0.16 $\pm$ 0.04 & 0.18 $\pm$ 0.06 \\
$\rm [Al/H]$ & 0.18 $\pm$ 0.06 & 0.18 $\pm$ 0.03 \\
$\log{\epsilon}$(Li) & $-$0.12 & 1.16 \\
$\log{\epsilon}$(Be) & $-$ & $<$$-$0.40 \\
\hline  	    
\end{tabular} 	    
\end{table}