\begin{table}%t6
\caption{\label{tab6}\ion{Fe}{ii} lines in the 3800--8000~\AA\ region  
with $\log~gf$~$\ge$~$-$1.5  and 3d$^{6}$($^{3}$P)4f 
energy levels as upper levels. } 
\small%\centering
\par
\begin{tabular}{llllllllllll}
\hline\hline\noalign{\smallskip}
\multicolumn{4}{c}{Upper level}&
\multicolumn{2}{c}{Lower level}&
\multicolumn{1}{c}{$\lambda$(calc)}&
\multicolumn{1}{c}{$\log~gf$}&
\multicolumn{1}{c}{$\lambda$(obs)}&
\multicolumn{1}{c}{Notes}
\\
\noalign{\smallskip} 
\multicolumn{1}{c}{cm$^{-1}$}&
\multicolumn{1}{c}{} &
\multicolumn{1}{c}{} &
\multicolumn{1}{c}{$J$} &
\multicolumn{1}{c}{cm$^{-1}$}&
\multicolumn{1}{c}{} &
\multicolumn{1}{c}{\AA} &
\multicolumn{1}{c}{KUR} &
\multicolumn{1}{c}{\AA} 
\\
\hline\noalign{\smallskip}
 122~351.810 & ($^{3}$P)4f & 2[5] & 11/2 & 103~165.320 & ($^{3}$P)4d $^{4}$F$_{9/2}$ & 5210.550 & $+$0.795& 5210.55 & good agreement \\   
               &          &      &      & 103~683.070 & ($^{5}$D)5d $^{4}$F$_{9/2}$ & 5355.059 & $+$0.164& 5355.06 & computed too strong\\  
               &          &      &      & 103~771.320 & ($^{3}$H)4d $^{4}$G$_{9/2}$ & 5380.493 & $-$1.047&    & at the noise level\\  
               &          &      &      & 104~807.210 & ($^{3}$H)4d $^{2}$G$_{9/2}$ & 5698.178 & $-$0.539&    & blend with a telluric line \\  
               &          &      &      & 104~916.550 & ($^{3}$H)4d $^{4}$F$_{9/2}$ & 5733.913 & $-$0.635& 5733.90 & computed too weak\\  
               &          &      &      & 106~722.170 & ($^{3}$F)4d $^{4}$F$_{9/2}$ & 6396.332 & $-$0.741& 6396.32 & computed too weak\\  
               &          &      &      & 109~811.920 & ($^{3}$G)4d $^{4}$F$_{9/2}$ & 7972.359 & $-$0.985&         & at the noise level\\  
\\
 122~324.142    & ($^{3}$P)4f & 2[5] & 9/2 & 103~102.860 & ($^{3}$P)4d $^{4}$D$_{7/2}$ & 5201.118 & $-$0.056&  & wrong,not observed \\ 
               &             &      &      & 103~191.917 & ($^{3}$P)4d $^{2}$F$_{7/2}$ & 5225.329 & $+$0.634& & blend, good agreement \\  
               &             &      &      & 103~986.330 & ($^{3}$H)4d $^{4}$H$_{7/2}$ & 5451.698 & $-$1.133& & blend, good agreement\\  
               &             &      &      & 104~107.950 & ($^{3}$P)4d $^{4}$F$_{7/2}$ & 5488.097 & $-$0.362& & blend, good agreement\\  
               &             &      &      & 104~481.590 & ($^{3}$H)4d $^{2}$F$_{7/2}$ & 5603.024 & $-$0.170& 5603.05 & \\
               &             &      &      & 105~123.000 & ($^{3}$H)4d $^{2}$G$_{7/2}$ & 5811.956 & $-$1.441& &blend,good agreement \\  
               &             &      &      & 105~775.491 & ($^{3}$F)4d $^{2}$F$_{7/2}$ & 6041.116 & $-$0.837&6041.1 & weak,good agreement \\  
  \\
122~355.116 & ($^{3}$P)4f & 2[4] & 9/2      & 102~394.718 & ($^{5}$D)6s $^{4}$D$_{7/2}$ & 5008.523 & $-$0.809&  &weak, computed too strong  \\ 
           &             &      &          & 103~102.860 & ($^{3}$P)4d $^{4}$D$_{7/2}$ & 5192.750 & $+$0.657& 5192.75& lab, good agreement  \\ 
           &             &      &          & 103~165.320 & ($^{3}$P)4d $^{4}$F$_{9/2}$ & 5209.652 & $-$0.035& 5209.66& lab, good agreement \\ 
           &             &      &          & 103~191.917 & ($^{3}$P)4d $^{2}$F$_{7/2}$ & 5216.883 & $-$0.404&  & blend \\ 
           &             &      &          & 103~683.070 & ($^{5}$D)5d $^{4}$F$_{9/2}$ & 5354.110 & $-$0.637& 5354.1 & weak  \\ 
           &             &      &          & 104~107.950 & ($^{3}$P)4d $^{4}$F$_{7/2}$ & 5478.781 & $-$1.319&  & at the continuum level \\ 
           &             &      &          & 104~807.210 & ($^{3}$H)4d $^{2}$G$_{9/2}$ & 5697.105 & $-$1.443&  & at the continuum level  \\
           &             &      &          & 106~767.210 & ($^{3}$F)4d $^{4}$F$_{7/2}$ & 6413.457 & $-$1.407&  & blend \\ 
\par
\\ 
122~355.550     & ($^{3}$P)4f & 2[4] & 7/2 & 102~394.718 & ($^{5}$D)6s $^{4}$D$_{7/2}$ & 5008.414 & $-$1.258&     & good agreement\\  
               &             &      &     & 102~802.312 & ($^{5}$D)6s $^{4}$D$_{5/2}$ & 5112.818 & $-$0.959& 5112.82 & computed too weak\\  
               &             &      &     & 103~002.670 & ($^{3}$P)4d $^{4}$D$_{5/2}$ & 5165.751 & $+$0.441& 5165.75 & lab, good agreement\\
               &             &      &    & 103~102.860 & ($^{3}$P)4d $^{4}$D$_{7/2}$ & 5192.633 & $+$0.155& 5192.62&lab, computed too weak\\
               &             &      &    & 103~165.320 & ($^{3}$P)4d $^{4}$F$_{9/2}$ & 5209.534 & $-$1.105& & blend, good agreement\\
               &             &      &    & 103~191.917 & ($^{3}$P)4d $^{2}$F$_{7/2}$ & 5216.765 & $-$0.764& &blend \\
               &             &      &     & 106~796.660 & ($^{3}$F)4d $^{4}$P$_{5/2}$ & 6425.418 & $-$1.436&    & at the continuum level\\
\\
122~351.488 & ($^{3}$P)4f & 2[3] & 7/2    & 103~102.860 & ($^{3}$P)4d $^{4}$D$_{7/2}$ & 5193.729 & $-$1.320& &blend\\
           &             &      &        & 103~191.917 & ($^{3}$P)4d $^{2}$F$_{7/2}$ & 5217.871 & $-$0.250& 5217.870 & lab \\                  
           &             &      &        & 103~597.402 & ($^{3}$P)4d $^{2}$D$_{5/2}$ & 5330.689 & $+$0.525& 5330.680 & lab\\                  
           &             &      &        & 104~023.910 & ($^{3}$H)4d $^{4}$G$_{5/2}$ & 5454.742 & $-$1.327&          &at the continuum level\\                  
           &             &      &        & 104~107.950 & ($^{3}$P)4d $^{4}$F$_{7/2}$ & 5479.870 & $-$1.320&          &at the continuum level\\
           &             &      &        & 104~481.590 & ($^{3}$H)4d $^{2}$F$_{7/2}$ & 5594.450 & $-$1.116& 5594.42  & computed too weak?\\ 
           &             &      &        & 104~569.230 & ($^{3}$P)4d $^{4}$F$_{5/2}$ & 5622.022 & $-$0.573& 5622.02  & computed too weak? \\                  
           &             &      &        & 105~234.237 & ($^{3}$H)4d $^{4}$F$_{5/2}$ & 5840.440 & $-$1.282&          & at the continuum level\\
           &             &      &        & 107~407.800 & ($^{3}$F)4d $^{2}$D$_{5/2}$ & 6689.941 & $-$0.330& 6689.91  & \\                  
\\                 
123~629.520     & ($^{3}$P)4f & 1[4] & 9/2 & 103~102.860 & ($^{3}$P)4d $^{4}$D$_{7/2}$ & 4870.353 & $-$1.402& & at the continuum level \\   
               &             &      &     & 104~000.810 & ($^{5}$D)5d $^{6}$P$_{7/2}$ & 5093.159 & $-$0.981&  &blend \\  
               &             &      &     & 104~107.950 & ($^{3}$P)4d $^{4}$F$_{7/2}$ & 5121.112 & $+$0.327& 5121.1    & lab, good agreement\\  
               &             &      &     & 104~481.590 & ($^{3}$H)4d $^{2}$F$_{7/2}$ & 5221.043 & $+$0.408& 5221.04    & lab, good agreement\\  
               &             &      &     & 104~873.230 & ($^{5}$D)5d $^{4}$D$_{7/2}$ & 5330.062 & $-$1.183&     & blend\\  
               &             &      &     & 104~993.860 & ($^{3}$F)4d $^{4}$D$_{7/2}$ & 5364.564 & $-$0.118&5364.55& computed too strong\\
               &             &      &     & 105~123.000 & ($^{3}$H)4d $^{2}$G$_{7/2}$ & 5401.999 & $-$0.418&     &blend\\  
               &             &      &     & 105~220.600 & ($^{3}$H)4d $^{4}$F$_{7/2}$ & 5430.640 & $-$1.066&5430.64 & computed too weak\\  
               &             &      &     & 105~775.491 & ($^{3}$F)4d $^{2}$F$_{7/2}$ & 5599.422 & $-$0.624& 5599.42 & good agreement\\  
               &             &      &     & 106~767.210 & ($^{3}$F)4d $^{4}$F$_{7/2}$ & 5928.743 & $-$0.677& 5928.72 & at the noise level\\ 
               &             &      &     & 110~167.280 & ($^{3}$G)4d $^{4}$F$_{7/2}$ & 7426.139 & $-$1.173&     &\\  
\par
\hline 
123~637.833 & ($^{3}$P)4f & 1[4] & 7/2     & 102~802.312 & ($^{5}$D)6s $^{4}$D$_{5/2}$ & 4798.155 & $-$1.297&  &at the continuum level \\
           &             &      &         & 103~002.670 & ($^{3}$P)4d $^{4}$D$_{5/2}$ & 4844.743 & $-$0.954&  &computed too strong\\  
           &             &      &         & 103~597.402 & ($^{3}$P)4d $^{2}$D$_{5/2}$ & 4988.521 & $-$0.339& 4988.51 & lab \\  
           &             &      &         & 104~107.950 & ($^{3}$P)4d $^{4}$F$_{7/2}$ & 5118.932 & $-$0.819& 5118.95 & lab, computed too weak\\  
           &             &      &         & 104~120.270 & ($^{5}$D)5d $^{6}$P$_{5/2}$ & 5122.163 & $-$1.282&         & \\  
           &             &      &         & 104~481.590 & ($^{3}$H)4d $^{2}$F$_{7/2}$ & 5218.777 & $-$0.644&         &blend\\  
           &             &      &         & 104~569.230 & ($^{3}$P)4d $^{4}$F$_{5/2}$ & 5242.763 & $+$0.180& 5242.775 & lab\\  
           &             &      &         & 104~993.860 & ($^{3}$F)4d $^{4}$D$_{7/2}$ & 5362.172 & $-$1.268&        & at the continuum level \\  
           &             &      &         & 105~127.770 & ($^{5}$D)5d $^{4}$D$_{5/2}$ & 5400.965 & $-$1.143&        & at the continuum level\\  
           &             &      &         & 105~234.237 & ($^{3}$H)4d $^{4}$F$_{5/2}$ & 5432.211 & $-$0.531&        & wrong, not observed\\  
           &             &      &         & 105~379.430 & ($^{3}$F)4d $^{4}$D$_{5/2}$ & 5475.409 & $-$0.552& 5475.42 & computed too strong\\  
           &             &      &         & 105~711.730 & ($^{5}$D)5d $^{6}$S$_{5/2}$ & 5576.909 & $-$1.432&         &at the continuum level\\  
           &             &      &         & 106~208.560 & ($^{3}$F)4d $^{2}$F$_{5/2}$ & 5735.883 & $-$1.221&         &at the continuum level\\  
           &             &      &         & 106~796.660 & ($^{3}$F)4d $^{4}$P$_{5/2}$ & 5936.184 & $-$1.317&         & at the level of the noise\\  
           &             &      &         & 106~866.760 & ($^{3}$F)4d $^{4}$F$_{5/2}$ & 5960.996 & $-$0.565& 5961.00 &\\  
           &             &      &         & 107~407.800 & ($^{3}$F)4d $^{2}$D$_{5/2}$ & 6159.712 & $-$0.665& 6179.75 & blend?\\
           &             &      &         & 110~428.280 & ($^{3}$G)4d $^{4}$F$_{5/2}$ & 7568.195 & $-$1.229&         & no spectrum\\  
\\      
123~615.875 & ($^{3}$P)4f & 1[3] & 7/2    & 103~597.402 & ($^{3}$P)4d $^{2}$D$_{5/2}$ & 4993.993 & $-$1.435&   &  \\  
           &             &      &        & 104~023.910 & ($^{3}$H)4d $^{4}$G$_{5/2}$ & 5102.711 & $-$0.526& 5102.7  & lab, good agreement \\  
           &             &      &        & 104~107.950 & ($^{3}$P)4d $^{4}$F$_{7/2}$ & 5124.694 & $-$1.046& 5124.69 & good agreement\\  
           &             &      &        & 104~120.270 & ($^{5}$D)5d $^{6}$P$_{5/2}$ & 5127.932 & $-$0.244&     &wrong, not obs\\
           &             &      &        & 104~209.610 & ($^{3}$H)4d $^{2}$F$_{5/2}$ & 5151.540 & $-$0.081 & 5151.52 & J78, lab, computed too weak\\
           &             &      &        & 104~481.590 & ($^{3}$H)4d $^{2}$F$_{7/2}$ & 5224.766 & $-$0.973& 5227.77  & good agreement\\  
           &             &      &        & 104~569.230 & ($^{3}$P)4d $^{4}$F$_{5/2}$ & 5248.807 & $-$0.232& 5248.801 & computed too strong\\  
           &             &      &        & 105~127.770 & ($^{5}$D)5d $^{4}$D$_{5/2}$ & 5407.380 & $-$1.391& 5407.37 & computed too weak\\
           &             &      &        & 105~234.237 & ($^{3}$H)4d $^{4}$F$_{5/2}$ & 5438.700 & $-$0.416& 5438.70 & computed too strong\\  
           &             &      &        & 106~208.560 & ($^{3}$F)4d $^{2}$F$_{5/2}$ & 5743.118 & $-$0.454& 5743.10 & good agreement\\  
\\
123~649.493 & ($^{3}$P)4f & 1[3] & 5/2    & 104~209.610 & ($^{3}$H)4d $^{2}$F$_{5/2}$ & 5142.631 & $-$1.288&     & at the continuum level\\   
           &             &      &        & 104~569.230 & ($^{3}$P)4d $^{4}$F$_{5/2}$ & 5239.559 & $-$1.150& 5239.56 & good agreement\\  
           &             &      &        & 104~572.920 & ($^{3}$P)4d $^{4}$F$_{3/2}$ & 5240.573 & $+$0.071& 5240.587 & lab, good agreement\\  
           &             &      &        & 104~588.710 & ($^{5}$D)5d $^{6}$D$_{3/2}$ & 5244.914 & $-$1.288&     & blend\\  
           &             &      &        & 104~839.998 & ($^{3}$P)4d $^{2}$D$_{3/2}$ & 5314.985 & $-$0.441&     & blend,computed too strong\\  
           &             &      &        & 105~234.237 & ($^{3}$H)4d $^{4}$F$_{5/2}$ & 5428.771 & $-$1.471&     & blend\\  
           &             &      &        & 105~317.440 & ($^{3}$P)4d $^{2}$P$_{3/2}$ & 5453.411 & $+$0.082& 5453.42 & lab, computed too strong \\  
           &             &      &        & 105~518.140 & ($^{3}$H)4d $^{4}$F$_{3/2}$ & 5513.777 & $-$0.591&    & wrong, not observed\\  
           &             &      &        & 106~846.650 & ($^{3}$F)4d $^{4}$F$_{3/2}$ & 5949.725 & $-$1.358&    & at the continuum level\\  
           &             &      &        & 107~430.250 & ($^{3}$F)4d $^{2}$D$_{3/2}$ & 6163.810 & $-$0.253&    & wrong, not observed\\  
           &             &      &        & 108~105.900 & ($^{3}$F)4d $^{2}$P$_{3/2}$ & 6431.741 & $-$0.724&    & blend\\  
\par
\\
124~157.060 & ($^{3}$P)4f & 0[3] & 5/2     & 104~569.230 & ($^{3}$P)4d $^{4}$F$_{5/2}$ & 5103.788 & $-$1.191& 5103.8 & good agreement\\  
           &             &      &         & 104~572.920 & ($^{3}$P)4d $^{4}$F$_{3/2}$ & 5104.750 & $+$0.094& 5104.75  & lab, good agreement \\  
           &             &      &         & 104~588.710 & ($^{5}$D)5d $^{6}$D$_{3/2}$ & 5108.869 & $-$1.369&   &  \\  
           &             &      &         & 104~839.998 & ($^{3}$P)4d $^{2}$D$_{3/2}$ & 5175.329 & $-$1.125&  &blend \\  
           &             &      &         & 105~234.237 & ($^{3}$H)4d $^{4}$F$_{5/2}$ & 5283.154 & $-$0.937&     &blend\\  
           &             &      &         & 105~317.440 & ($^{3}$P)4d $^{2}$P$_{3/2}$ & 5306.486 & $-$1.020& 5306.49 & computed too weak \\ 
           &             &      &         & 105~460.230 & ($^{3}$F)4d $^{4}$D$_{3/2}$ & 5347.013 & $-$0.482& 5347.05 & blend  \\  
           &             &      &         & 105~518.140 & ($^{3}$H)4d $^{4}$F$_{3/2}$ & 5363.626 & $+$0.082& 5363.61 &computed too strong  \\  
           &             &      &         & 106~846.650 & ($^{3}$F)4d $^{4}$F$_{3/2}$ & 5775.269 & $-$0.286& 5775.25 & good agreement\\  
           &             &      &         & 107~430.250 & ($^{3}$F)4d $^{2}$D$_{3/2}$ & 5976.771 & $-$0.922&    & blend\\  
           &             &      &         & 108~105.900 & ($^{3}$F)4d $^{2}$P$_{3/2}$ & 6228.356 & $-$0.686& 6228.34 & good agreement\\  
           &             &      &         & 110~609.540 & ($^{3}$G)4d $^{4}$F$_{3/2}$ & 7379.392 & $-$1.370&    &at the continuum level \\  
\par
\hline 
\end{tabular} 
\end{table}