\begin{table}%t3 \caption{\label{table:3}Abundances in the envelope of IRC+10216.} %\centerline { \begin{tabular}{lccccccccc} \noalign{\smallskip} \hline \hline \noalign{\smallskip} El. & Ion & $N$ & $C_{\rm i}$\tablefootmark{a} & $N$({\sc i}+{\sc ii}) & $N$({\sc i}+{\sc ii})/$N$(H) & $X_\odot$ & $\log_{10} \delta$ & $\log_{10} \delta_{7027}$ & $\log_{10} \delta_{\zeta~\rm{Oph}}$ \\ & & (cm$^{-2}$) & & (cm$^{-2}$) \\ \noalign{\smallskip} \hline \noalign{\smallskip} Na & \sc{i} & $\phantom{<}$4.6(14) & 1.22 & 5.6(14) & 4.2($-$7) & 2.00($-$6) & $-$0.68 & $-$0.06 & $-$0.95 \\ \noalign{\smallskip} Al & \sc{i} & $<$2.8(12) & 3.5(3)& $<$9.8(15) & $<$7.3($-$6) & 2.88($-$6) & $\ldots$\tablefootmark{c} & $\ldots$ & $\ldots$ \\ \noalign{\smallskip} K & \sc{i} & $\phantom{<}$4.6(12) & 1.60 & 7.4(12) & 5.5($-$9) & 1.29($-$7) & $-$1.37 & $-$0.17 & $-$1.09\\ \noalign{\smallskip} Ca & \sc{i} & $\phantom{<}$1.9(12) & 4.70 & 8.9(12)\tablefootmark{b} & 6.6($-$9) & 2.19($-$6) & $-$2.52 & $-$0.75 & $-$3.73 \\ & \sc{ii} & $\phantom{<}$7.0(12) & 1.27 & $\ldots$ & $\ldots$ & $\ldots$ & $\ldots$ & $\ldots$ & $\ldots$\\ \noalign{\smallskip} Ti & \sc{i} & $<$1.9(12) & 4.26 & $<$3.9(12)\tablefootmark{b} & $<$2.9($-$9) & 8.32($-$8) & $<$$-$1.45 & $\ldots$ & $-$3.02\\ & \sc{ii} & $<$2.0(12) & 1.31 & $\ldots$ & $\ldots$ & $\ldots$ & $\ldots$ & $\ldots$ & $\ldots$ \\ \noalign{\smallskip} Cr & \sc{i} & $\phantom{<}$1.4(12) & 10.6 & 1.5(13) & 1.1($-$8) & 4.47($-$7) & $-$1.60 & $\ldots$ & $-$2.28 \\ \noalign{\smallskip} Mn & \sc{i} & $<$3.1(12) & 2.21 & $<$6.9(12) & $<$5.1($-$9) & 3.16($-$7) & $<$~$-$1.79 & & $-$1.45 \\ \noalign{\smallskip} Fe & \sc{i} & $\phantom{<}$8.8(13) & 2.58 & 2.3(14) & 1.7($-$7) & 2.95($-$5) & $-$2.24 & $-$1.68 & $-$2.27 \\ \noalign{\smallskip} Sr & \sc{ii} & $<$2.7(11) & 3.82 & $<$1.0(12) & $<$7.6($-$10) & 8.13($-$10)& $\ldots$\tablefootmark{c} & $\ldots$ & $\ldots$ \\ \noalign{\smallskip} \hline \end{tabular}} \par \tablefoot {\tablefoottext{a} {Ionization correction $C_{\rm i} = N({\rm\sc I} + {\sc \rm II}) /N({\sc \rm i})$ for neutral species and $N({\sc\rm I} + {\sc \rm II}) /N({\sc\rm II})$ for singly ionized species.} \tablefoottext{b} {Based on observed values of $N$({\sc i}) + $N$({\sc ii}), independent of $C_{\rm i}$.} \tablefoottext{c} {Upper limit on $X > X_\odot$, no useful limit on~$\delta$. }} \par \end{table}