\begin{table}%t5
\caption{Finding list of new experimental log($gf$)-values for the Os I and Ir I
transitions in Tables~\ref{osibf1} and~\ref{iribf1}.}
\label{findlist}
%\centerline
{\begin{tabular}{rr@{}c@{}lrrr} \hline \hline \noalign{\smallskip}
\multicolumn{1}{c}{$\lambda_{\rm air}$} & \multicolumn{3}{c}{Transition}
&\multicolumn{3}{c}{log($gf$)} \\ %&\multicolumn{1}{c}{Th. log($gf$)}\\
\cline{5-7}
\multicolumn{1}{c}{(\AA)}               &&&& \multicolumn{1}{c}{Exp}
&\multicolumn{1}{c}{Unc.$^{a}$}& \multicolumn{1}{c}{Kurucz} \\
%\multicolumn{1}{c}{Theory} \\
\noalign{\smallskip} \hline \noalign{\smallskip}
& \multicolumn{3}{c}{\hspace{-4mm}Os I}\\
2909.057     &5d$^{6}$6s$^{2}$                           
a$^{5}$D$_{4}$& $-$& 5d$^{6}$6s($^{6}$D)6p
z$^{5}$F$_{5}$     &    --0.25&7   &--0.32$^{b}$ \\ %& -0.112\\
3058.652     &5d$^{6}$6s$^{2}$
a$^{5}$D$_{4}$& $-$& 5d$^{6}$6s($^{6}$D)6p
z$^{7}$F$_{4}$     &    --0.45& 7  &--0.43$^{c}$ \\ %& -0.331\\
3301.567     &5d$^{6}$6s$^{2}$
a$^{5}$D$_{4}$& $-$& 5d$^{6}$6s($^{6}$D)6p
z$^{7}$F$_{5}$     &    --0.74& 7   &--0.75$^{c}$ \\ %& -0.585\\
3421.160     &5d$^{7}$($^{4}$F)6s
a$^{5}$F$_{5}$& $-$& 5d$^{6}$6s($^{6}$D)6p
z$^{5}$F$_{5}$     &    --2.57&17   &--1.33$^{b}$ \\ %& -2.839\\
3504.662     &5d$^{6}$6s$^{2}$
a$^{5}$D$_{3}$& $-$& 5d$^{6}$6s($^{6}$D)6p
z$^{7}$F$_{4}$     &    --1.64&13   &--1.39$^{c}$ \\ %& -1.642\\
3528.602     &5d$^{6}$6s$^{2}$
a$^{5}$D$_{4}$& $-$& 5d$^{5}$6s$^{2}$($^{6}$S)6p
z$^{7}$P$_{4}$     &    --1.74&11   &             \\ %& -1.572\\
3629.958     &5d$^{7}$($^{4}$F)6s
a$^{5}$F$_{5}$& $-$& 5d$^{6}$6s($^{6}$D)6p
z$^{7}$F$_{4}$     &    --2.91&14   &--2.32$^{c}$ \\ %& -1.814\\
3901.698     &5d$^{7}$($^{4}$F)6s
a$^{5}$F$_{4}$& $-$& 5d$^{6}$6s($^{6}$D)6p
z$^{5}$F$_{5}$     &    --2.15&17   &--1.66$^{b}$ \\ %& -1.854\\
3977.225     &5d$^{7}$($^{4}$F)6s
a$^{5}$F$_{5}$& $-$& 5d$^{6}$6s($^{6}$D)6p
z$^{7}$F$_{5}$     &    --1.77&17   &--1.43$^{b}$ \\ %& -1.684\\
4135.781     &5d$^{6}$6s$^{2}$
a$^{5}$D$_{3}$& $-$& 5d$^{5}$6s$^{2}$($^{6}$S)6p
z$^{7}$P$_{4}$&    --1.35&9    &--1.26$^{c}$ \\ %& -1.103\\
4175.612     &5d$^{7}$($^{4}$F)6s
a$^{5}$F$_{4}$& $-$& 5d$^{6}$6s($^{6}$D)6p
z$^{7}$F$_{4}$     &    --1.50&13   &--1.24$^{c}$ \\ %& -1.483\\
4260.849     &5d$^{6}$6s$^{2}$
a$^{5}$D$_{4}$& $-$& 5d$^{6}$6s($^{6}$D)6p
z$^{7}$D$_{5}$     &    --1.47& 9   &--1.44$^{c}$ \\ %&-1.089\\
4284.248     &5d$^{7}$($^{4}$F)6s
a$^{3}$F$_{4}$& $-$& 5d$^{6}$6s($^{6}$D)6p
z$^{5}$F$_{5}$     &    --1.91&17   &--1.67$^{c}$ \\ %&-2.681\\
4311.393     &5d$^{7}$($^{4}$F)6s
a$^{5}$F$_{5}$& $-$& 5d$^{5}$6s$^{2}$($^{6}$S)6p
z$^{7}$P$_{4}$&    --1.74&11    &--1.85$^{c}$ \\ %&-2.474\\
4616.769     &5d$^{7}$($^{4}$F)6s
a$^{3}$F$_{4}$& $-$& 5d$^{6}$6s($^{6}$D)6p
z$^{7}$F$_{4}$     &    --1.82&14   &--1.67$^{c}$ \\ %&-1.913\\
4641.833     &5d$^{7}$($^{4}$F)6s
a$^{5}$F$_{4}$& $-$& 5d$^{6}$6s($^{6}$D)6p
z$^{7}$F$_{5}$     &    --2.96&14   &--2.73$^{c}$ \\ %&-3.343\\
4692.056     &5d$^{7}$($^{4}$F)6s
a$^{5}$F$_{3}$& $-$& 5d$^{6}$6s($^{6}$D)6p
z$^{7}$F$_{4}$     &    --2.18& 14  &--2.05$^{c}$ \\ %&-2.388\\
5103.497     &5d$^{7}$($^{4}$F)6s
a$^{5}$F$_{4}$& $-$& 5d$^{5}$6s$^{2}$($^{6}$S)6p
z$^{7}$P$_{4}$&    --3.50& 13    &--2.43$^{c}$ \\ %&-2.536\\
\\
& \multicolumn{3}{c}{ Ir I}\\
3513.647     &5d$^{7}$6s$^{2}$ a$^{4}$F$_{9/2}$
&$-$& 5d$^{7}$6s($^{5}$F)6p z$^{6}$F$_{11/2}$ &
--1.246&9    &--1.260$^{b}$ \\ %& -0.669\\
3800.124     &5d$^{7}$6s$^{2}$ a$^{4}$F$_{9/2}$
&$-$& 5d$^{7}$6s($^{5}$F)6p z$^{6}$D$_{9/2}$  &
--1.489&2    &--1.450$^{b}$ \\ %& -1.065\\
3902.501     &5d$^{8}$($^{3}$F)6s
b$^{4}$F$_{9/2}$& $-$& 5d$^{7}$6s($^{5}$F)6p
z$^{6}$F$_{11/2}$  &    --2.077&11   &--1.930$^{b}$ \\ %&-2.144\\
4259.108     &5d$^{8}$($^{3}$F)6s
b$^{4}$F$_{9/2}$& $-$& 5d$^{7}$6s($^{5}$F)6p
z$^{6}$D$_{9/2}$   &    --2.882&7   &--2.900$^{b}$ \\ %&-4.104\\
 \hline
\end{tabular}}
{$^{a}$ One-$\sigma$ uncertainty of $gf$, in \%}.\\
{$^{b}$ Experimental values rescaled by Kurucz \citep{K93}.}\\
{$^{c}$ Unscaled values from \citet{Kwiatkowski84}}.
\end{table}