\begin{table}%T2
\caption{\label{tab:lines}List of the strongest \ion{Fe}{vii} EUV~lines in the 160--295~\AA\ range. 
} 
\small%\centerline
{
\begin{tabular}[c]{@{}ccccrllllll@{}}
\hline \hline\noalign{\smallskip}  
 $i-j$ & Levels   &   Int  & $gf$ & $gf^*$  &  $A_{ji}$(s$^{-1}$) &   $\lambda_{\rm exp}$(\AA) & $\lambda_{\rm th}$(\AA)   &  $\lambda_{\rm NIST}$(\AA) & ID \\   
\noalign{\smallskip}\hline\noalign{\smallskip} 
3--135 & 3d$^2$ $^3$F$_{4}$--3d$^3$ $^3$F$_{4}$ & 1.0 & 7.15 & 7.4 & 1.7 $\times$ 10$^{11}$ & 176.745 & 176.81&      176.745 &    FC73 \\ 
3--148 & 3d$^2$ $^3$F$_{4}$--3d$^3$ $^3$D$_{3}$ & 0.78 & 8.55 & 8.8 & 2.9 $\times$ 10$^{11}$ & 166.365 & 166.38&      166.365 &    FC73 \\ 
3--110 & 3d$^2$ $^3$F$_{4}$--3d$^3$ $^3$G$_{5}$ & 0.86 & 2.90 & 3.0 & 4.6 $\times$ 10$^{10}$ & 196.046 & 196.13&      195.388 &    N \\ 
8--150 & 3d$^2$ $^1$G$_{4}$--3d$^3$ $^1$G$_{4}$ & 0.73 & 8.52 & 8.6 & 2.2 $\times$ 10$^{11}$ & 171.070 & 171.10&      173.442 &   T N  \\ 
2--133 & 3d$^2$ $^3$F$_{3}$--3d$^3$ $^3$F$_{3}$ & 0.71 & 5.03 & 5.2 & 1.5 $\times$ 10$^{11}$ & 176.927 & 176.97&      176.927 &    FC73 \\ 
8--153 & 3d$^2$ $^1$G$_{4}$--3d$^3$ $^1$F$_{3}$ & 0.61 & 9.82 & 10. & 3.5 $\times$ 10$^{11}$ & 165.087   & 164.34& --  &   T N \\ 
2--147 & 3d$^2$ $^3$F$_{3}$--3d$^3$ $^3$D$_{2}$ & 0.53 & 5.85 & 6.0 & 2.8 $\times$ 10$^{11}$ & 165.919 & 166.00&      165.919 &    FC73 \\ 
2--108 & 3d$^2$ $^3$F$_{3}$--3d$^3$ $^3$G$_{4}$ & 0.61 & 1.24 & 2.1 & 2.4 $\times$ 10$^{10}$ & 196.210 & 196.16&      196.423 &    N \\ 
1--131 & 3d$^2$ $^3$F$_{2}$--3d$^3$ $^3$F$_{2}$ & 0.47 & 3.19 & 3.8 & 1.4 $\times$ 10$^{11}$ & 177.171 & 177.06&      177.171 &    FC73 \\ 
8--116 & 3d$^2$ $^1$G$_{4}$--3d$^3$ $^1$H$_{5}$ & 0.47 & 2.22 & 2.3 & 3.5 $\times$ 10$^{10}$ & 196.209 & 196.22& --  &    N  \\ 
7--120 & 3d$^2$ $^3$P$_{2}$--3d$^3$ $^1$F$_{3}$ & 0.34 & 2.00 & 2.3 & 5.5 $\times$ 10$^{10}$ & 186.600 & 186.60&      188.576 &    N  \\ 
1--149 & 3d$^2$ $^3$F$_{2}$--3d$^3$ $^3$D$_{1}$ & 0.30 & 3.44 & 3.5 & 2.8 $\times$ 10$^{11}$ & 165.489 & 165.57&      165.489 &    E81 \\ 
4--119 & 3d$^2$ $^1$D$_{2}$--3d$^3$ $^3$D$_{3}$ & 0.34 & 2.01 & 2.3 & 5.5 $\times$ 10$^{10}$ & 186.852 & 186.80&      185.547 &    N \\ 
7--134 & 3d$^2$ $^3$P$_{2}$--3d$^3$ $^3$P$_{2}$ & 0.32 & 2.26 & 2.3 & 9.1 $\times$ 10$^{10}$ & 182.133 & 182.32&      183.825 &    N \\ 
4--121 & 3d$^2$ $^1$D$_{2}$--3d$^3$ $^1$D$_{2}$ & 0.32 & 2.24 & 2.3 & 8.8 $\times$ 10$^{10}$ & 183.823 & 183.99&      186.656 &    N \\ 
1--106 & 3d$^2$ $^3$F$_{2}$--3d$^3$ $^3$G$_{3}$ & 0.33 & 1.36 & 1.1 & 3.3 $\times$ 10$^{10}$ & 197.358 & 196.96&      196.045 &    N \\ 
2--98 & 3d$^2$ $^3$F$_{3}$--3d$^3$ $^3$G$_{4}$ & 0.35 & 0.73 & 0.74 & 1.2 $\times$ 10$^{10}$ & 208.823 & 209.52&      211.931 &    N \\ 
3--97 & 3d$^2$ $^3$F$_{4}$--3d$^3$ $^3$G$_{5}$ & 0.34 & 0.62 & 0.60 & 8.5 $\times$ 10$^{9}$ & 209.731 & 210.59&      212.663 &     N \\ 
3--43 & 3d$^2$ $^3$F$_{4}$--3d$^3$ $^3$F$_{4}$ & 0.35 & 6.2 $\times$ 10$^{-2}$ & 0.13 & 8.0 $\times$ 10$^{8}$ &  --  & 239.24& --  &   \\ 
3--52 & 3d$^2$ $^3$F$_{4}$--3d$^3$ $^3$G$_{5}$ & 0.31 & 9.2 $\times$ 10$^{-2}$ & 9.5 $\times$ 10$^{-2}$ & 1.0 $\times$ 10$^{9}$ & 235.630 & 235.83& --  &    T N \\ 
3--20 & 3d$^2$ $^3$F$_{4}$--3d$^3$ $^5$F$_{5}$ & 0.34 & 1.7 $\times$ 10$^{-5}$ & 1.4 $\times$ 10$^{-5}$ & 1.6 $\times$ 10$^{5}$ & 254.051 & 254.26& --  &    N \\ 
3--19 & 3d$^2$ $^3$F$_{4}$--3d$^3$ $^5$D$_{4}$ & 0.29 & 8.5 $\times$ 10$^{-4}$ & 2.9 $\times$ 10$^{-4}$ & 9.3 $\times$ 10$^{6}$ & 260.676 & 260.83& --  &    N \\ 
1--101 & 3d$^2$ $^3$F$_{2}$--3d$^3$ $^3$G$_{3}$ & 0.31 & 0.75 & 0.75 & 1.7 $\times$ 10$^{10}$ & 206.754 & 207.69&      207.712 &     N \\ 
1--37 & 3d$^2$ $^3$F$_{2}$--3d$^3$ $^3$F$_{2}$ & 0.26 & 2.1 $\times$ 10$^{-2}$ & 8.7 $\times$ 10$^{-4}$ & 4.8 $\times$ 10$^{8}$ & 241.021 & 238.76& --  &   T N\\ 
2--42 & 3d$^2$ $^3$F$_{3}$--3d$^3$ $^3$F$_{3}$ & 0.23 & 3.7 $\times$ 10$^{-2}$ & 1.8 $\times$ 10$^{-3}$ & 6.2 $\times$ 10$^{8}$ &  --  & 239.53& --  &   \\ 
3--29 & 3d$^2$ $^3$F$_{4}$--3d$^3$ $^5$G$_{5}$ & 0.24 & 5.2 $\times$ 10$^{-5}$ & 7.4 $\times$ 10$^{-5}$ & 5.2 $\times$ 10$^{5}$ &  --  & 245.00& --  &   \\ 
2--51 & 3d$^2$ $^3$F$_{3}$--3d$^3$ $^3$G$_{4}$ & 0.23 & 0.11 & 9.0 $\times$ 10$^{-2}$ & 1.5 $\times$ 10$^{9}$ & 235.180 & 235.28& --  &    T N \\ 
2--30 & 3d$^2$ $^3$F$_{3}$--3d$^3$ $^3$D$_{2}$ & 0.22 & 4.1 $\times$ 10$^{-2}$ & 0.16 & 9.4 $\times$ 10$^{8}$ & 243.830 & 241.02& --  &    T N \\ 
3--22 & 3d$^2$ $^3$F$_{4}$--3d$^3$ $^5$F$_{4}$ & 0.22 & 1.0 $\times$ 10$^{-3}$ & 2.0 $\times$ 10$^{-4}$ & 1.2 $\times$ 10$^{7}$ &  253.520  & 253.71& --  & T N  \\ 
6--118 & 3d$^2$ $^3$P$_{1}$--3d$^3$ $^3$D$_{2}$ & 0.24 & 1.35 & 1.2 & 5.1 $\times$ 10$^{10}$ & 188.170 & 188.18&      189.450 &     N \\ 
4--152 & 3d$^2$ $^1$D$_{2}$--3d$^3$ $^1$P$_{1}$ & 0.18 & 2.84 & 3.0 & 2.4 $\times$ 10$^{11}$ & 163.183 & 163.17&      163.183 &    E81 \\ 
7--151 & 3d$^2$ $^3$P$_{2}$--3d$^3$ $^3$S$_{1}$ & 0.17 & 2.30 & 2.4 & 1.9 $\times$ 10$^{11}$ & 165.997 & 166.02&      165.997 &    E81 \\ 
3--93 & 3d$^2$ $^3$F$_{4}$--3d$^3$ $^3$H$_{5}$ & 0.20 & 0.16 & 0.28 & 2.1 $\times$ 10$^{9}$ & 212.664 & 213.54&      216.590 &  T  N \\ 
4--120 & 3d$^2$ $^1$D$_{2}$--3d$^3$ $^1$F$_{3}$ & 0.14 & 0.78 & 0.56 & 2.2 $\times$ 10$^{10}$ & 185.285 & 185.24&      187.233 &    N \\ 
6--151 & 3d$^2$ $^3$P$_{1}$--3d$^3$ $^3$S$_{1}$ & 0.11 & 1.49 & 1.5 & 1.2 $\times$ 10$^{11}$ & 165.764 & 165.75&      165.764 &    E81 \\ 
7--119 & 3d$^2$ $^3$P$_{2}$--3d$^3$ $^3$D$_{3}$ & 0.12 & 0.73 & 0.52 & 2.0 $\times$ 10$^{10}$ & 188.189 & 188.19&      186.866 &    N \\ 
\noalign{\smallskip}
%1-121 & 3d$^2$ $^3$F$_{2}$--3d$^3$ $^1$D$_{2}$ & 0.11 & 0.72 & 0.18 & 3.0 $\times$ 10$^{10}$ & 178.102 & 178.27&      180.760 &    N \\ 
% 
% 160.001-230 \AA 
% 
8--46 & 3d$^2$ $^1$G$_{4}$--4p $^1$F$_{3}$ & 1.2 & 1.71 & 1.7 & 2.8 $\times$ 10$^{10}$ & 243.378 & 243.37&      243.378 &    E81 \\ 
3--31 & 3d$^2$ $^3$F$_{4}$--4p $^3$D$_{3}$ & 0.78 & 0.90 & 0.80 & 1.6 $\times$ 10$^{10}$ & 233.308 & 233.53&      233.308 &     E81 \\ 
3--36 & 3d$^2$ $^3$F$_{4}$--4p $^3$F$_{4}$ & 0.70 & 0.48 & 0.46 & 6.6 $\times$ 10$^{9}$ & 231.728 & 231.97&      231.728 &    E81 \\ 
4--25 & 3d$^2$ $^1$D$_{2}$--4p $^1$D$_{2}$ & 0.59 & 0.37 & 0.39 & 8.3 $\times$ 10$^{9}$ & 245.152 & 244.51&      245.152 &    E81 \\ 
2--28 & 3d$^2$ $^3$F$_{3}$--4p $^3$D$_{2}$ & 0.48 & 0.46 & 0.59 & 1.1 $\times$ 10$^{10}$ & 234.338 & 233.20&      234.338 &    E81 \\ 
1--27 & 3d$^2$ $^3$F$_{2}$--4p $^3$D$_{1}$ & 0.46 & 0.45 & 0.51 & 1.9 $\times$ 10$^{10}$ & 235.223 & 233.04&      235.223 &    E81 \\ 
7--44 & 3d$^2$ $^3$P$_{2}$--4p $^3$P$_{2}$ & 0.33 & 0.54 & 0.32 & 1.2 $\times$ 10$^{10}$ & 240.223 & 240.62&      240.223 &    E81 \\ 
3--32 & 3d$^2$ $^3$F$_{4}$--4p $^3$F$_{3}$ & 0.28 & 0.27 & 0.25 & 4.7 $\times$ 10$^{9}$ & 232.949 & 232.78&      232.949 &    E81 \\ 
4--53 & 3d$^2$ $^1$D$_{2}$--4p $^1$P$_{1}$ & 0.25 & 0.29 & 0.30 & 1.2 $\times$ 10$^{10}$ & 234.757 & 234.71&      234.757 &     E81 \\ 
2--32 & 3d$^2$ $^3$F$_{3}$--4p $^3$F$_{3}$ & 0.24 & 0.23 & 0.11 & 4.1 $\times$ 10$^{9}$ & 232.257 & 232.00&      232.257 &    E81 \\ 
2--35 & 3d$^2$ $^3$F$_{3}$--4p $^3$F$_{2}$ & 0.23 & 0.29 & 1.8 $\times$ 10$^{-2}$ & 7.1 $\times$ 10$^{9}$ & 233.012 & 232.96&      233.012 &    E81 \\ 
1--28 & 3d$^2$ $^3$F$_{2}$--4p $^3$D$_{2}$ & 0.20 & 0.19 & 0.12 & 4.7 $\times$ 10$^{9}$ & 233.762 & 232.55&      233.762 &    E81 \\ 
2--31 & 3d$^2$ $^3$F$_{3}$--4p $^3$D$_{3}$ & 0.19 & 0.22 & 0.21 & 3.9 $\times$ 10$^{9}$ & 232.614 & 232.74&      232.614 &     E81 \\ 
\noalign{\smallskip}
% 
% 230.001-250 \AA 
% 
3--12 & 3d$^2$ $^3$F$_{4}$--4s $^3$D$_{3}$ & 1.3  & -- & -- & 1.6 $\times$ 10$^{5}$ & 290.756 & 290.97&      290.756 &    N \\ 
2--11 & 3d$^2$ $^3$F$_{3}$--4s $^3$D$_{2}$ & 0.61 & -- & -- & 1.0 $\times$ 10$^{5}$ & 290.717 & 290.87&      290.717 &    N \\ 
1--10 & 3d$^2$ $^3$F$_{2}$--4s $^3$D$_{1}$ & 0.53 & -- & -- & 1.4 $\times$ 10$^{5}$ & 290.307 & 290.36&      290.307 &    N \\ 
1--11 & 3d$^2$ $^3$F$_{2}$--4s $^3$D$_{2}$ & 0.37 & -- & -- & 6.2 $\times$ 10$^{4}$ & 289.831 & 289.86&      289.831 &    N \\ 
2--12 & 3d$^2$ $^3$F$_{3}$--4s $^3$D$_{3}$ & 0.37 & -- & -- & 4.6 $\times$ 10$^{4}$ & 289.678 & 289.76&      289.678 &    N \\ 
3-11 & 3d$^2$ $^3$F$_{4}$--4s $^3$D$_{2}$ & 0.27 & -- & -- & 4.5 $\times$ 10$^{4}$ & 291.803 & 292.09&      291.803 &   N \\ 
2--10 & 3d$^2$ $^3$F$_{3}$--4s $^3$D$_{1}$ & 0.26 & -- & -- & 7.1 $\times$ 10$^{4}$ & 291.196 & 291.37&      291.196 &   N  \\ 
% 
% 250.001-295 \AA 
\noalign{\smallskip} \hline                                   %inserts single line
\end{tabular}}
\smallskip
Note: the relative intensities  (photons)  ${\rm Int}=N_{j} A_{ji}/N_{\rm e}$ are normalised to 
the strongest transition and were calculated at an electron density of~10$^{9}$~cm$^{-3}$
and a temperature of $2.5\times 10^{5}$~K.
Weighted  oscillator strengths $gf$ and A-values (s$^{-1}$) are from  the benchmark calculation.
The $gf$ values from WB08 are also listed ($gf^*$).
 $\lambda_{\rm exp}$ are our experimental wavelengths, while 
$\lambda_{\rm th}$  are the theoretical ones from the benchmark calculation. 
 $\lambda_{\rm NIST}$ are the NIST wavelengths.
The last column (ID) provides a key to previous identifications.
N~indicates a new one proposed here. T N a tentative new one.
FC73: \cite{fawcett_cowan:73}; E81: \cite{ekberg:81}.
\end{table}