\begin{table}%t2
\caption{\label{Tab:tar-rad}Dominant radiative transition data from the ground state of the
recombining ion $3p^6\;({}^1S_{0})\to 3p^53d\;({}^1P_{1}^{{\rm o}})$, where $v_{(u)}^{\rm [\pm p]}$ denotes $v(u)\times 10^{\pm p}$.}
 %\centering
$$
\begin{tabular}{c l l l l c l l l l}    
\hline
\hline
\multicolumn{10}{c}{\vspace*{-2mm}} \\
$\begin{array}{c} {\rm Ion} \\  \end{array}$ &
$\begin{array}{c} A^{r} \\ ({\rm ns}^{-1}) \end{array}$ &
$\begin{array}{c} S \\ ({\rm a.u.}) \end{array}$ &
$\begin{array}{c} f \\  \hfill \end{array}$ &
$\begin{array}{c} {\rm Ref.} \\ \hfill \end{array}$ &
$\begin{array}{c} {\rm Ion} \\  \end{array}$ &
$\begin{array}{c} A^{r} \\ ({\rm ns}^{-1}) \end{array}$ &
$\begin{array}{c} S \\ ({\rm a.u.}) \end{array}$ &
$\begin{array}{c} f \\  \hfill \end{array}$ &
$\begin{array}{c} {\rm Ref.} \\ \hfill \end{array}$ \\
\hline
\multicolumn{10}{c}{\vspace*{-2mm}} \\
\multirow{2}{*}{${\rm K}^{+}$}&$0.2785^{\rm [+2]}$&$5.004$&$3.070$& 
Present\tablefootmark{a}&\multirow{4}{*}{${\rm Ca}^{2+}$}&$0.836^{\rm [+2]}$&$5.678$&$4.818$&
 Present\tablefootmark{a}\\
               & $0.2224^{\rm [+2]}$ & $4.147$ & $2.513$ & MCHF$^{{\rm c}}    $ &   &$0.83^{\rm [+2]}_{(15)}$&$5.64$&$4.75_{(88)}$&NIST$^{{\rm b},~\S}$\\
\cline{2-5}
\multirow{3}{*}{${\rm V}^{5+}$}&$1.4610^{\rm [+2]}$&$2.448$&$3.313$&Present\tablefootmark{a}&        &$0.638^{\rm [+2]}$&$4.614$&$3.834$&MCHF$^{{\rm c}}    $\\
               &$1.46  ^{\rm [+2]} $ & $2.45 $ & $3.31 $ & NIST$^{{\rm b}\dag}$ &               &$0.682^{\rm [+2]}$&$4.210$&$3.688$&CIV3$^{{\rm j}}    $\\
\cline{7-10}
               &$1.8447^{\rm [+2]}$&$2.968$&$4.070$&MCHF\tablefootmark{c}&\multirow{3}{*}{${\rm Cr}^{6+}$}&$1.65^{\rm [+2]}$&$2.04$&$3.05$&Present\tablefootmark{a}\\
\cline{2-5}
%ion           & Ar              &     S   &      f  & Refs                 & %ion          & Ar          &     S  &    f  & Refs
\multirow{3}{*}{${\rm Mn}^{7+}$}&$1.858^{\rm [+2]}$&$1.754$&$2.874$&Present\tablefootmark{a}&        &$1.67^{\rm [+2]}$&$2.06 $ &$ 3.09$&NIST\tablefootmark{b}\tablefootmark{\S}\\
               &$1.85 ^{\rm [+2]}  $ &$1.75 $  &$2.86 $  &NIST\tablefootmark{b,}\tablefootmark{\S} &               &$2.05^{\rm [+2]}$&$2.43 $ &$ 3.69$&MCHF\tablefootmark{c}      \\
\cline{7-10}
         &$1.963^{\rm [+2]}$ &$2.033$ &$3.229$ &MCHF\tablefootmark{c} &\multirow{8}{*}{${\rm Fe}^{8+}$}&$2.009^{\rm [+2]}$&$1.489$&$2.645$&Present\tablefootmark{a}\\
\cline{2-5}
\multirow{4}{*}{${\rm Co}^{9+}$}&$2.190^{\rm [+2]}$&$1.300$&$2.486$&Present\tablefootmark{a}&        &$2.01 ^{\rm [+2]}$&$1.49 $&$2.65 $&NIST\tablefootmark{b},\tablefootmark{\S}\\
               &$2.200^{\rm [+2]}  $ &$1.300 $ &$2.500 $ &NIST\tablefootmark{b} \tablefootmark{\ddag}  &               &$2.097^{\rm [+2]}$&$1.724$&$2.958$&MCHF\tablefootmark{c}      \\
               &$2.224^{\rm [+2]}  $ &$1.482 $ &$2.726 $ &MCHF\tablefootmark{c}       &               &$2.438^{\rm [+2]}$&$1.678$&$3.054$&FAC4\tablefootmark{d}     \\
               &$1.448^{\rm [+2]}  $ &$1.409 $ &$2.628 $ &TDCHF\tablefootmark{f}  &               &$2.266^{\rm [+2]}$&$1.680$&$2.983$&CIV3\tablefootmark{e}    \\
\cline{2-5}
\multirow{6}{*}{${\rm Ni}^{10+}$}&$2.339^{\rm [+2]}$&$1.132$&$2.317$&Present\tablefootmark{a}&       &$1.356^{\rm [+2]}$&$1.073$&$2.843$&TDCHF\tablefootmark{f}      \\
                &$2.340^{\rm [+2]} $ &$1.130 $ &$2.320 $ &NIST\tablefootmark{b}\tablefootmark{\dag} &               &$2.889^{\rm [+2]}$&       &       &SELT \tablefootmark{g}    \\
                &$2.345^{\rm [+2]} $ &$1.288 $ &$2.528 $ &MCHF\tablefootmark{c} &               &$2.404^{\rm [+2]}$&$1.637$&$2.99 $&IRON\tablefootmark{h}     \\
\cline{7-10}
            &$1.537^{\rm [+2]}$&$0.808$&$2.444$&TDCHF\tablefootmark{f}&\multirow{4}{*}{${\rm Cu}^{11+}$}&$2.530^{\rm [+2]}$&$1.01$&$2.204$&Present\tablefootmark{a}\\
                &$2.786^{\rm [+2]} $ &$1.274 $ &$2.657 $ &FAC3\tablefootmark{h}    &  &$2.501^{\rm [+2]}_{(30)}$&$1.07_{(11)}$&$2.29_{(7)}$&NIST\tablefootmark{b},\tablefootmark{\S}\\
                &$2.841^{\rm [+2]} $ &$1.204 $ &$2.575 $ &CIV3\tablefootmark{i}       &                &$2.462^{\rm [+2]}$&$1.13$&$2.355  $&MCHF\tablefootmark{c}\\
\cline{2-5}
\multirow{4}{*}{${\rm Zn}^{12+}$}&$2.720^{\rm [+2]}$&$0.906$&$2.101$&Present\tablefootmark{a}&        &$1.624^{\rm [+2]}$&$1.08$&$2.285  $&TDCHF\tablefootmark{f} \\
    &$2.653^{\rm [+2]}_{(33)}$&$0.99_{(11)}$&$2.21_{(7)}$&NIST\tablefootmark{b},\tablefootmark{\S}&                &              &      &            &                   \\
                &$2.576^{\rm [+2]} $ &$1.001 $ &$2.204 $ &MCHF\tablefootmark{c}      &                &              &	&            &	             \\
                &$1.708^{\rm [+2]} $ &$0.958 $ &$2.145 $ &TDCHF\tablefootmark{f}     &                &              &	&            &	             \\
\hline
\end{tabular}
$$
\tablefoot {In the case of ${\rm Sc}^{3+}$ and ${\rm Ti}^{4+}$ ions, refer to \cite{Nikolic:2010} and \cite{Nikolic:2009}, respectively.} \vspace*{-4mm}
\tablebib {Assigned uncertainties:  \tablefoottext{\dag}{$<$18\%,}
\tablefoottext{\ddag}{~$<$25\%;} 
\tablefoottext{a}{present work: 2894-level MCBP results;}
    \tablefoottext{b}{critically compiled experimental data of \cite{Shirai:2000};}
    \tablefoottext{c}{MCHF results of \cite{Irimia:2003};}
    \tablefoottext{d}{6284-level FAC results of \cite{Aggarwal:2006};}
    \tablefoottext{e}{CIV3 results of \cite{Verma:2006};}
    \tablefoottext{f}{single-config. TDCHF results\ of \cite{Ghosh:1997};}
    \tablefoottext{g}{semiempirical results of \cite{Loginov:2002};}
    \tablefoottext{h}{6164-level FAC results of \cite{Aggarwal:2008};}
    \tablefoottext{i}{restricted CIV3 results of \cite{Verma:2007};}
    \tablefoottext{j}{18-config. CIV3 LS results of \cite{Baluja:1986};}
    \tablefoottext{\S}{extrapolated along the isoelectronic sequence.}}
\end{table}