\begin{table}%t2 \caption{Determined atmospheric parameters for \corots, the Sun, and \acenb.}\label{tab:vwa} \par %%\centerline {\small \begin{tabular}{lcclclllccc} \hline \hline & \multicolumn{4}{c}{$\langle$\feonetwo$\rangle$} & $\langle$Mg~1b$\rangle$ & $\langle$Ca6122$\rangle$ & $\langle$Ca6162$\rangle$ & $\langle$Ca6439$\rangle$ & \multicolumn{2}{c}{$\langle$Isol.\ lines$\rangle$} \\ % [\kms]} \\ Spec. & \teff\ [K] & \logg & \multicolumn{1}{c}{\feh} & \vmicro\ [\kms] & \multicolumn{1}{c}{\logg} & \multicolumn{1}{c}{\logg} & \multicolumn{1}{c}{\logg} & \multicolumn{1}{c}{\logg} & \vsini & \vmacro \\ % & [\kms] & [\kms] \\ \hline \hline H1 & $ 5180\pm67$ & $ 4.30\pm0.08$ & $+0.11\pm0.13$ & $ 0.98\pm0.07$ & $3.89\pm0.46 $ &$4.44\pm0.08$ & $4.43\pm0.10 $ &$4.34\pm0.19 $ & 1.3 & 1.2 \\ % HARPS, spec1 H1~\sme& $ 5280\pm44$ & $ 4.44\pm0.06$ & $+0.13\pm0.06$ & $ 0.80\pm0.07$ & $4.62 $ &$4.66 $ & $4.53 $ & & & \\ % HARPS, spec1 - SME analysis H2 & $ 5300\pm41$ & $ 4.46\pm0.08$ & $+0.14\pm0.13$ & $ 0.80\pm0.09$ & $4.02\pm0.47 $ &$4.43\pm0.05$ & $4.56\pm0.06 $ &$4.13\pm0.35 $ & 1.1 & 1.2 \\ % HARPS, spec2 H3 & $ 5350\pm31$ & $ 4.57\pm0.06$ & $+0.15\pm0.09$ & $ 0.76\pm0.07$ & $4.14\pm0.44 $ &$4.50\pm0.09$ & $4.77\pm0.07 $ &$4.72\pm0.26 $ & 1.1 & 1.2 \\ \hline % HARPS,spec3 H1-7 & $ 5280\pm35$ & $ 4.48\pm0.06$ & $+0.13\pm0.09$ & $ 0.80\pm0.05$ & $3.94\pm0.52 $ &$4.47\pm0.06$ & $4.60\pm0.08 $ &$4.32\pm0.27 $ & 0.9 & 1.4 \\ % HARPS, spec1-7=comb. H1-107 & $ 5300\pm25$ & $ 4.54\pm0.05$ & $+0.13\pm0.08$ & $ 0.77\pm0.05$ & $3.91\pm0.55 $ &$4.51\pm0.06$ & $4.58\pm0.05 $ &$4.45\pm0.18 $ & & \\ % HARPS = 107 spe. H1-107~\sme&$5290\pm44$ & $ 4.49\pm0.06$ & $+0.13\pm0.06$ & $ 0.80\pm0.05$ & $4.43 $ &$4.49 $ & $4.49 $ & & & \\ % HARPS = 107 spe. -- SME analysis U1 & $ 5300\pm17$ & $ 4.50\pm0.03$ & $+0.11\pm0.06$ & $ 0.70\pm0.08$ & $3.94\pm0.49 $ &$4.42\pm0.05$ & $4.46\pm0.06 $ &$4.41\pm0.19 $ & $ $ & $ $ \\ \hline % UVES spec Ceres & $ 5767\pm17$ & $ 4.44\pm0.03$ & $-0.01\pm0.03$ & $ 1.01\pm0.03$ & $4.50\pm0.08 $ &$4.46\pm0.20$ & $4.43\pm0.10 $ &$4.43\pm0.42$ & 1.4 & 2.1 \\ % Solar Ganymede& $ 5757\pm17$ & $ 4.43\pm0.04$ & $-0.00\pm0.04$ & $ 0.93\pm0.03$ & $4.51\pm0.10 $ &$4.33\pm0.17$ & $4.38\pm0.08 $ &$4.47\pm0.37$ & 1.1 & 2.3 \\ % Solar Moon & $ 5775\pm25$ & $ 4.48\pm0.03$ & $+0.02\pm0.04$ & $ 0.91\pm0.04$ & $4.41\pm0.08 $ &$4.53\pm0.20$ & $4.41\pm0.14 $ &$4.50\pm0.33$ & 2.1 & 2.2 \\ % Solar \hline \acenb & $ 5185\pm25$ & $ 4.50\pm0.03$ & $+0.31\pm0.05$ & $ 0.83\pm0.04$ & $4.01\pm0.50 $ &$4.53\pm0.07$ & $4.51\pm0.05 $ &$4.65\pm0.16$ & 1.0 & 0.8 \\ % Alpha Cen B \hline \end{tabular}} \tablefoot{Results are from \vwa\ except H1 and H1-107, which are also given for the \sme\ analysis. The 1-$\sigma$ uncertainties are internal errors.} %% We find $T_{\rm eff}=5185\pm25$~K, $\log g = 4.50\pm0.03$, ${\rm [Fe/H] = +0.31 \pm 0.05$ \par % Results from \sme\ is given for the H1-107 spectrum. % The method is indicated in angled brackets. % The 1-$\sigma$ uncertainties stated here are internal errors. % The \vsini\ and \vmacro\ are determined from isolated spectral lines; % the $1$-$\sigma$ uncertainty range for each parameter is $(+1.0, -0.5)$ ~\kms. \end{table}