\begin{table}
%\centering
\par
\caption{Atomic lines detected in the \fuse\ spectrum of
HD~141569A. The velocities are in the pipeline's rest frame (observed
spectrum) and are heliocentric. For the saturated lines, we measured
the velocity of the centroid; for those lines the error bars on the
velocity are symetric (not calculated by a $\chi ^2$ minimization).
The radial velocities and line widths have been determined using
respectively all the unsaturated and saturated lines of a given
ion. "sat'' and "unsat'' are respectively for saturated and
unsaturated lines. --$^a$ line not fitted because of the
very low $S/N$ ratio of the data; --$^b$ Doppler parameter
{\it b} not measured because of the unsaturated state of the line.}
\label{tab1}
\begin{tabular}{lcccccc}
\hline
\hline
Element & Wavelength & Energy level & Line              & Radial velocity                 &         $N$                         &    $b$    \\
        &  \AA\      & (cm$^{-1}$)  & State             &    (\kms)                 &  (cm$^{-2}$)                      &   (\kms)   \\
\hline
 Ar I   & 1048.2198  &  0.00        & --$^a$ & --$27.0\pm3$              &  $>$$7.30\times10^{14}$               & $\rm 5.6_{-0.25}^{+0.42}$ \\
        & 1066.6599  &  0.00        & sat               &                           &                                   &  \\
\noalign{\medskip}
 FeII   & 1063.1764  &  0.00        & unsat             & $\rm -24.28_{-2.75}^{+1.89}$ & $\rm 9.77_{-0.94}^{+4.56}\times10^{15}$  & $\rm 2.34_{-0.79}^{+0.25}$ \\
        & 1096.8770  &  0.00        & sat               &                           &                                   &  \\
        & 1121.9749  &  0.00        & unsat             &                           &                                   & \\
        & 1143.2260  &  0.00        & unsat             &                           &                                   & \\
        & 1144.9379  &  0.00        & sat               &                           &                                   &  \\
\noalign{\medskip}
 FeII*  & 1068.3456  & 384.79       & unsat             & $\rm -24.28_{-2.75}^{+1.89}$ & $\rm 5.21_{-1.25}^{+3.65}\times10^{13}$ & $\rm 2.34_{-0.79}^{+0.25}$  \\
        & 1096.6073  & 384.79       & unsat             &                           &                                   & \\
        & 1147.4092  & 384.79       & unsat             &                           &                                   & \\
        & 1148.2773  & 384.79       & unsat             &                           &                                   & \\
\noalign{\medskip}
 FeII** & 1071.5842  & 667.68       & unsat             & $\rm -24.28_{-2.75}^{+1.89}$ & $4.25_{-2.65}^{+4.36}\times10^{13}$ & $\rm 2.34_{-0.79}^{+0.25}$  \\ 
        & 1151.1458  & 667.68       & unsat             &                           &                                   & \\
\noalign{\medskip}
FeII*** & 1148.0789  & 862.61       & unsat             & --24.28$_{-2.75}^{+1.89}$ & $2.77_{-0.89}^{+1.12}\times10^{13}$ & $\rm 2.34_{-0.79}^{+0.25}$  \\
        & 1153.2719  & 862.61       & unsat             &                           &                                   & \\
\noalign{\medskip}
N I     & 1134.1653  &  0.00        & sat               & --$24.0\pm2$              & $>$$3.16\times10^{14}$                & $\rm 6.80_{-3.05}^{+2.11}$ \\
        & 1134.4149  &  0.00        & sat               &                           &                                   &  \\ 
        & 1134.9803  &  0.00        & sat               &                           &                                   &  \\ 
\noalign{\medskip}
N II    & 1083.9937  &  0.00        & --$^a$ & --$22.0\pm4 $             &                                   &  --$^a$ \\
\noalign{\medskip}
N II*   & 1084.5659  &  48.67       & --$^a$ & --$22.0\pm4 $             &                                   &  --$^a$ \\
        & 1084.5841  &  48.67       & --$^a$ &                           &                                   &  \\
\noalign{\medskip}
N II**  & 1085.5511  &  130.80      & --$^a$ & --$22.0\pm4 $             &                                   & --$^a$ \\
        & 1085.7096  &  130.80      & --$^a$ &                           &                                   & \\
\noalign{\medskip}
P II    & 1152.8180  &  0.00        & unsat             & $\rm -25.37_{-1.25}^{+1.56}$ & $1.00_{-0.67}^{+0.65}\times10^{13}$  &  --$^b$ \\
\noalign{\medskip}
P II*   & 1149.9580  & 164.90       & unsat             & $\rm -25.37_{-1.25}^{+1.56}$ & $1.03_{-0.56}^{+0.74}\times10^{13}$  &  --$^b$ \\
\noalign{\medskip}
P II**  & 1153.9951  & 469.12       & unsat             & $\rm -25.37_{-1.25}^{+1.56}$ & $1.24_{-0.81}^{+0.70}\times10^{13}$  &  --$^b$ \\
\noalign{\medskip}
Cl I    & 1097.3691  &  0.00        & unsat             & $\rm -25.12_{-1.13}^{+1.64}$ & $3.12_{-1.53}^{+0.82}\times10^{14}$  &  --$^b$ \\
        & 1099.5229  &  0.00        & unsat             &                           &                                          & --$^b$ \\
\hline
\end{tabular}
\end{table}