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 \begin{deluxetable}{lllcrrrrrrrrr}
\tablenum{2}
\tablewidth{566pt}
\tablecaption{Absolute transition probabilities and oscillator strengths of Fe II transitions.}
\tablehead{
 \multicolumn{1}{c}{$\lambda_{vac}$ } 
 & \multicolumn{1}{c}{$\lambda_{air}$ }
& \multicolumn{1}{c}{$\sigma$}      &
 \colhead{}
 & \colhead{BF}    &
 \multicolumn{1}{c}{Un.$_{BF}$}      &
\multicolumn{1}{c}{{\it A} (s$^{-1}$) }    &
 \multicolumn{1}{c}{(Un.$_{A}$)}  &
\multicolumn{1}{c}{log {\it gf}}  &
 \multicolumn{1}{c}{(Un.$_{log~{\it gf}}$)} &
 \colhead{log {\it gf}} & 
 \colhead{log {\it gf}} & \colhead{log {\it gf}} \\
\multicolumn{1}{c}{(\AA) }       &
\multicolumn{1}{c}{(\AA) }       &
\multicolumn{1}{c}{(cm$^{-1}$) }       &
\colhead{}      &
\colhead{}      &
\colhead{(\%)}    &  
\multicolumn{1}{c}{} &
 \multicolumn{1}{c}{($\pm$ \%)} 
 &  \multicolumn{1}{c}{}  &
\multicolumn{1}{c}{($\pm$ dex)}    & \multicolumn{1}{c}{Raassen} & 
 \multicolumn{1}{c}{Kurucz}  & \multicolumn{1}{c}{Nahar} }
\startdata
\multicolumn{12}{l}{Level 62065 cm$^{-1}$   $\;\;$  3d$^{6}$(a$^{3}$F)4p$\;$ y$^{4}$F$_{3.5}$           $\;\;$         3.50   ns   $\pm$ 0.3ns           $\;\;$       99.87 \% complete, 0.02 \% outside, 0.11 \% blended}             \nl
   3500.882 & 3499.881 & 28564.23  &   &  0.15 &   11 & .429E+06 & 14 & -2.20 & 0.06 &   -2.37 &  -2.38  &     -      \nl
   3496.622 & 3495.621 & 28599.03  &   &  0.09 &   13 & .262E+06 & 15 & -2.42 & 0.06 &   -2.46 &  -2.38  &     -      \nl
   3325.963 & 3325.006 & 30066.48  &   &  0.12 &   20 & .335E+06 & 22 & -2.35 & 0.09 &   -2.85 &  -2.51  &     -      \nl
   3305.379 & 3304.428 & 30253.71  &   &  0.07 &   25 & .203E+06 & 27 & -2.57 & 0.10 &   -2.71 &  -2.45  &     -      \nl
   3259.713 & 3258.773 & 30677.55  &   &  3.29 &    3 & .939E+07 &  9 & -0.92 & 0.04 &   -1.15 &  -1.08  &   -0.99   \nl
   3194.781 & 3193.857 & 31301.05  &   &  1.35 &    3 & .386E+07 &  9 & -1.33 & 0.04 &   -1.44 &  -1.42  &     -      \nl
   3156.867 & 3155.953 & 31676.98  &   &  0.15 &   12 & .417E+06 & 15 & -2.30 & 0.06 &   -2.61 &  -2.39  &     -      \nl
   2903.169 & 2902.318 & 34445.12  &   &  0.31 &   12 & .881E+06 & 15 & -2.05 & 0.06 &   -2.12 &  -2.27  &     -      \nl
   2877.647 & 2876.803 & 34750.61  &   &  3.35 &    3 & .956E+07 &  9 & -1.02 & 0.04 &   -1.10 &  -1.00  &     -      \nl
   2800.119 & 2799.294 & 35712.76  &   &  5.41 &    3 & .155E+08 &  9 & -0.84 & 0.04 &   -0.87 &  -0.84  &     -      \nl
   2776.998 & 2776.178 & 36010.11  &   &  0.93 &    5 & .266E+07 & 10 & -1.61 & 0.04 &   -1.62 &  -1.54  &   -3.56   \nl
   2757.845 & 2757.030 & 36260.20  &   &  2.83 &    3 & .807E+07 &  9 & -1.13 & 0.04 &   -1.24 &  -1.34  &   -1.07   \nl
   2555.834 & 2555.067 & 39126.18  &   &  6.87 &    3 & .196E+08 &  9 & -0.81 & 0.04 &    -0.82 &  -0.76  &   -0.61   \nl
   2547.434 & 2546.670 & 39255.18  &   & 27.94 &    3 & .798E+08 &  9 & -0.21 & 0.04 &    -0.21 &  -0.15  &    0.15   \nl
   2536.248 & 2535.486 & 39428.33  &   & 26.16 &    3 & .747E+08 &  9 & -0.24 & 0.04 &    -0.25 &  -0.24  &   -0.72   \nl
   2478.092 & 2477.343 & 40353.63  &   &  5.95 &    3 & .170E+08 &  9 & -0.90 & 0.04 &    -0.89 &  -0.80  &     -      \nl
   2470.117 & 2469.371 & 40483.91  &   &  0.78 &    8 & .223E+07 & 12 & -1.79 & 0.05 &   -1.81 &  -1.79  &     -      \nl
   2425.124 & 2424.390 & 41235.01  &   &  5.63 &    6 & .161E+08 & 10 & -0.95 & 0.04 &    -0.91 &  -1.05  &     -      \nl
   2423.669 & 2422.933 & 41259.76  &   &  1.03 &   14 & .294E+07 & 16 & -1.68 & 0.07 &   -1.96 &  -1.67  &     -      \nl
   2406.822 & 2406.090 & 41548.57  &   &  0.72 &   15 & .205E+07 & 17 & -1.85 & 0.07 &   -2.01 &  -1.75  &     -      \nl
   2188.370 & 2187.685 & 45696.12  &   &  1.00 &    5 & .287E+07 & 10 & -1.78 & 0.04 &   -1.64 &  -1.36  &     -      \nl
   2057.991 & 2057.332 & 48591.08  &   &  0.98 &   11 & .280E+07 & 14 & -1.85 & 0.06 &   -1.62 &  -1.44  &     -      \nl
   1688.404 &          & 59227.54  &   &  0.89 &   19 & .253E+07 & 20 & -2.06 & 0.08 &   -1.90 &  -1.59  &   -1.68   \nl
   1676.857 &          & 59635.39  &   &  2.36 &   11 & .675E+07 & 14 & -1.64 & 0.06 &   -1.64 &  -1.30  &   -0.92   \nl
   1611.200 &          & 62065.53  &   &  1.54 &   17 & .440E+07 & 19 & -1.86 & 0.08 &   -1.87 &  -2.56  &     -      \nl
   1863.114 &          & 53673.57  & x &  0.10 &      & .294E+06 &       & -2.91 &      &   -2.99 &  -2.80  &   -3.47   \nl
   1661.325 &          & 60192.93  & x &  0.34 &      & .964E+06 &       & -2.50 &      &   -2.38 &  -2.11  &   -1.78   \nl
   1621.252 &          & 61680.74  & x &  0.38 &      & .109E+07 &       & -2.46 &      &   -2.40 &  -3.11  &      -     \nl
   2771.321 & 2770.503 & 36083.88  & b &       &      &          &       &       &      &   -2.56 &  -2.57  &      -     \nl
           &          &              &   &        &        &       &       &      &          &       &         &            \nl
  \multicolumn{12}{l}{Level 63948 cm$^{-1}$   $\;\;$  3d$^{6}$(a$^{3}$F)4p$\;$ y$^{4}$G$_{4.5}$           $\;\;$         2.7   ns   $\pm$ 0.3ns           $\;\;$    99.97\% complete, 0.03\% outside}             \nl
   3280.592 & 3279.647 & 30482.30 &     &  0.16 &   13 & .575E+06 & 17 & -2.03 & 0.07 &   -2.23 &  -2.31 &      -     \nl
   3129.915 & 3129.008 & 31949.75 &     &  0.06 &   49 & .225E+06 & 50 & -2.48 & 0.18 &   -2.70 &  -2.53 &      -     \nl
   2979.715 & 2978.846 & 33560.25 &     &  0.19 &   17 & .717E+06 & 20 & -2.02 & 0.08 &   -2.29 &  -2.53 &      -     \nl
   2729.713 & 2728.905 & 36633.88 &     &  3.37 &    5 & .125E+08 & 12 & -0.86 & 0.05 &    -0.97 &  -0.96 &      -     \nl
   2647.000 & 2646.212 & 37778.62 &     &  0.39 &   10 & .144E+07 & 15 & -1.82 & 0.06 &   -1.90 &  -2.26 &      -     \nl
   2596.053 & 2595.277 & 38520.01 &     &  0.04 &   13 & .167E+06 & 17 & -2.77 & 0.07 &   -1.83 &  -1.65 &   -1.99   \nl
   2430.816 & 2430.078 & 41138.45 &     & 51.57 &    3 & .191E+09 & 12 &  0.23 & 0.05 &     0.23 &   0.24 &    0.26   \nl
   2420.628 & 2419.892 & 41311.60 &     &  0.60 &   29 & .222E+07 & 31 & -1.71 & 0.12 &   -1.90 &  -1.85 &   -0.78   \nl
   2367.598 & 2366.875 & 42236.90 &     &  0.95 &   10 & .351E+07 & 15 & -1.53 & 0.06 &   -1.67 &  -1.62 &   -3.19   \nl
   2360.317 & 2359.596 & 42367.18 &     &  6.08 &    3 & .225E+08 & 12 & -0.73 & 0.05 &    -0.70 &  -0.65 &   -1.41   \nl
   2351.921 & 2351.201 & 42518.44 &     & 19.41 &    3 & .719E+08 & 12 & -0.22 & 0.05 &    -0.20 &  -0.19 &   -0.29   \nl
   2293.128 & 2292.421 & 43608.55 &     &  0.23 &    8 & .842E+06 & 14 & -2.18 & 0.06 &   -2.25 &  -2.07 &      -     \nl
   2078.823 & 2078.160 & 48104.15 &     &  0.77 &   10 & .284E+07 & 15 & -1.74 & 0.06 &   -1.64 &  -1.46 &      -     \nl
   1625.523 &          & 61518.66 &     & 10.90 &    7 & .404E+08 & 13 & -0.80 & 0.05 &    -0.70 &  -0.52 &   -1.12   \nl
   1610.923 &          & 62076.20 &     &  5.25 &    8 & .194E+08 & 14 & -1.12 & 0.06 &   -1.04 &  -0.78 &   -2.16   \nl
   2659.855 & 2659.064 & 37596.03 &   x &  0.07 &      & .265E+06 &       & -2.55 &      &   -2.58 &  -2.48 &      -     \nl
   1785.922 &          & 55993.48 &   x &  0.34 &      & .126E+07 &       & -2.22 &      &   -2.77 &  -2.73 &      -     \nl
           &          &           &       &        &        &       &       &      &          &    &           &            \nl
  \multicolumn{12}{l}{Level 62945 cm$^{-1}$   $\;\;$  3d$^{6}$(a$^{3}$F)4p$\;$ x$^{4}$D$_{3.5}$   $\;\;$    2.8 ns   $\pm$ 0.3ns           $\;\;$     99.98 \% complete, 0.02 \% outside, 3.44 \% blended }             \nl
   3396.307 &  3395.332 & 29443.75 &    &  0.10 &   19 & .366E+06 & 22 & -2.30 & 0.09 &   -2.43 &  -2.24 &      -     \nl
   3212.002 &  3211.074 & 31133.23 &    &  0.06 &   38 & .211E+06 & 39 & -2.58 & 0.14 &   -2.85 &  -2.40 &      -     \nl
   3178.453 &  3177.534 & 31461.84 &    &  4.88 &    3 & .174E+08 & 11 & -0.68 & 0.05 &    -0.89 &  -0.87 &   -0.82   \nl
   3107.465 &  3106.564 & 32180.57 &    &  0.53 &    7 & .188E+07 & 13 & -1.66 & 0.05 &   -1.89 &  -1.76 &      -     \nl
   3071.584 &  3070.691 & 32556.49 &    &  0.36 &    7 & .128E+07 & 13 & -1.84 & 0.05 &   -2.01 &  -1.80 &      -     \nl
   2806.614 &  2805.787 & 35630.12 &    &  0.90 &    5 & .322E+07 & 12 & -1.52 & 0.05 &   -1.60 &  -1.42 &      -     \nl
   2732.817 &  2732.008 & 36592.28 &    &  1.97 &    4 & .705E+07 & 11 & -1.20 & 0.05 &   -1.31 &  -1.16 &      -     \nl
   2710.789 &  2709.986 & 36889.63 &    &  0.24 &   32 & .868E+06 & 33 & -2.12 & 0.13 &   -2.91 &  -2.87 &      -     \nl
   2705.379 &  2704.577 & 36963.39 &    &  0.46 &   12 & .166E+07 & 16 & -1.84 & 0.06 &   -2.00 &  -1.93 &      -     \nl
   2692.535 &  2691.736 & 37139.71 &    &  1.41 &    4 & .504E+07 & 11 & -1.36 & 0.05 &   -1.47 &  -1.55 &      -     \nl
   2491.610 &  2490.858 & 40134.70 &    & 24.70 &    3 & .882E+08 & 11 & -0.18 & 0.05 &    -0.20 &  -0.22 &   -0.68   \nl
   2480.907 &  2480.158 & 40307.84 &    & 43.47 &    3 & .155E+09 & 11 &  0.06 & 0.05 &     0.04 &   0.08 &    0.26   \nl
   2373.083 &  2372.359 & 42139.27 &    &  0.18 &   25 & .661E+06 & 27 & -2.35 & 0.10 &   -2.55 &  -2.15 &      -     \nl
   2356.929 &  2356.208 & 42428.09 &    &  0.20 &   37 & .710E+06 & 38 & -2.33 & 0.14 &   -2.48 &  -2.24 &      -     \nl
   2147.045 &  2146.370 & 46575.63 &    &  0.20 &   13 & .713E+06 & 17 & -2.40 & 0.07 &   -2.26 &  -1.85 &      -     \nl
   2123.125 &  2122.454 & 47100.39 &    &  0.13 &   23 & .480E+06 & 26 & -2.59 & 0.10 &   -2.55 &  -2.10 &      -     \nl
   2021.403 &  2020.751 & 49470.59 &    &  5.13 &    6 & .183E+08 & 12 & -1.05 & 0.05 &    -0.88 &  -0.64 &   -0.68   \nl
   1818.522 &          & 54989.72 &    &  1.60 &    7 & .570E+07 & 13 & -1.65 & 0.05 &   -1.60 &  -1.62  &   -1.48  \nl
   1637.400 &          & 61072.44 &    & 10.00 &    8 & .357E+08 & 14 & -0.94 & 0.06 &    -0.85 &  -0.58  &   -1.11   \nl
   2425.233 & 2424.497 & 41233.14 &  x &  0.24 &      & .840E+06 &       & -2.23 &      &   -2.68 &  -2.67  &      -     \nl
   1833.077 &          & 54553.08 &  x &  0.14 &      & .512E+06 &       & -2.69 &      &   -2.05 &  -2.05  &   -2.27   \nl
   1663.698 &          & 60107.06 &  x &  0.39 &      & .140E+07 &       & -2.33 &      &   -2.48 &  -2.24  &   -3.36   \nl
   1588.687 &          & 62945.04 &  x &  0.43 &      & .155E+07 &       & -2.33 &      &   -2.83 &  -2.93  &      -     \nl
   3168.863 & 3167.946 & 31557.06 &  b &       &       &         &       &       &      &   -2.66 &  -2.45  &   -1.60   \nl
   2499.644 & 2498.891 & 40005.69 &  b &       &      &          &       &       &      &   -1.14 &  -1.14  &   -1.98   \nl
   2374.480 & 2373.755 & 42114.49 &  b &         &       &          &       &       &   &   -1.80 &  -2.62  &   -2.08   \nl
           &          &             &        &        &       &       &      &          &    &         &       &            \nl
  \multicolumn{12}{l}{Level 64040 cm$^{-1}$   $\;\;$  3d$^{6}$(a$^{3}$F)4p$\;$ y$^{4}$G$_{3.5}$   $\;\;$    2.8 ns   $\pm$ 0.3ns           $\;\;$         99.96\% complete, 0.04\% outside}             \nl
   3274.438 &   3273.494 & 30539.59 &    &  0.23 &   12 & .848E+06 & 16 & -1.96 & 0.07 &   -2.22 &  -2.08&      -     \nl
   3270.711 &   3269.768 & 30574.39 &    &  0.14 &   17 & .520E+06 & 21 & -2.18 & 0.08 &   -2.42 &  -2.20&      -     \nl
   3102.788 &   3101.888 & 32229.08 &    &  0.24 &   24 & .905E+06 & 26 & -1.98 & 0.10 &   -2.57 &  -2.18&      -     \nl
   3005.132 &   3004.256 & 33276.41 &    &  0.23 &   13 & .860E+06 & 17 & -2.03 & 0.07 &   -2.16 &  -2.07&      -     \nl
   2971.561 &   2970.694 & 33652.34 &    &  1.12 &    6 & .415E+07 & 13 & -1.36 & 0.05 &   -1.60 &  -1.36&      -     \nl
   2745.708 &   2744.896 & 36420.48 &    &  0.98 &    7 & .362E+07 & 13 & -1.49 & 0.05 &   -1.60 &  -1.57&      -     \nl
   2722.869 &   2722.062 & 36725.97 &    &  3.83 &    5 & .142E+08 & 12 & -0.90 & 0.05 &   -1.11 &  -0.85&      -     \nl
   2653.356 &   2652.566 & 37688.12 &    &  1.20 &    7 & .445E+07 & 13 & -1.43 & 0.05 &   -1.56 &  -1.49&      -     \nl
   2627.483 &   2626.699 & 38059.24 &    &  0.52 &   10 & .194E+07 & 15 & -1.79 & 0.06 &   -2.14 &  -2.50&   -1.00   \nl
   2615.366 &   2614.586 & 38235.56 &    &  0.91 &   11 & .337E+07 & 16 & -1.56 & 0.06 &   -2.12 &  -1.77&   -1.88   \nl
   2432.999 &   2432.261 & 41101.54 &    & 42.27 &    3 & .157E+09 & 12 &  0.05 & 0.05 &     0.07 &   0.06&    0.13   \nl
   2425.386 &   2424.650 & 41230.54 &    &  1.77 &   10 & .655E+07 & 15 & -1.34 & 0.06 &   -1.40 &  -1.46&   -0.67   \nl
   2415.244 &   2414.510 & 41403.69 &    &  0.11 &   39 & .424E+06 & 40 & -2.53 & 0.15 &   -3.73 &  -2.63&   -2.31   \nl
   2362.447 &   2361.725 & 42328.99 &    &  6.49 &    3 & .240E+08 & 12 & -0.79 & 0.05 &    -0.85 &  -0.82&   -1.53   \nl
   2355.198 &   2354.478 & 42459.27 &    & 21.94 &    3 & .813E+08 & 12 & -0.27 & 0.05 &    -0.22 &  -0.23&   -0.38   \nl
   2312.935 &   2312.223 & 43235.12 &    &  0.25 &   14 & .931E+06 & 18 & -2.22 & 0.07 &   -2.52 &  -2.16&      -     \nl
   2297.587 &   2296.879 & 43523.93 &    &  0.49 &    7 & .182E+07 & 13 & -1.94 & 0.05 &   -2.13 &  -1.66&      -     \nl
   2097.690 &  2097.024 & 47671.48 &    &  0.29 &   20 & .107E+07 & 23 & -2.25 & 0.09 &   -2.14 &  -1.84 &      -     \nl
   2074.851 &  2074.189 & 48196.24 &    &  0.62 &   13 & .230E+07 & 17 & -1.93 & 0.07 &   -1.86 &  -1.42 &      -     \nl
   1633.909 &           & 61202.91 &    & 10.39 &    9 & .385E+08 & 14 & -0.91 & 0.06 &    -0.80 &  -0.65 &   -1.25   \nl
   1623.093 &           & 61610.75 &    &  5.37 &    9 & .199E+08 & 14 & -1.20 & 0.06 &   -1.09 &  -0.86 &   -2.05   \nl
   1608.537 &           & 62168.29 &    &  0.57 &   25 & .210E+07 & 27 & -2.19 & 0.10 &   -2.19 &  -1.86 &   -3.69   \nl
   1796.980 &           & 55648.93 &  x &  0.29 &      & .108E+07 &    & -2.38 &      &   -2.94 &  -2.86 &      -     \nl
\tablecomments{Columns are as follows 
$\lambda_{vac}$, vacuum wavelength;
$\lambda_{air}$, wavelength in air for $\lambda >$ 2000\AA;
$\sigma$, vacuum wavenumber (Ritz wavenumbers rounded down
to seven significant figures from Johansson (private communication));
BF, branching fraction; Un.$_{BF}$, \% relative uncertainty in BF; {\it A}, absolute transition
probability (s$^{-1}$), found by combining BF and the measured
lifetime; Un.$_{{\it A}}$,  \% uncertainty in {\it A}; log~{\it gf} measured in this work; 
uncertainty (dex) in log~{\it gf}, log~{\it gf} Raassen, calculated by Raassen (1999),
log~{\it gf} Kurucz, calculated by Kurucz (2000 private
communication).
Annotations to transitions indicate: x, transition not observed in this
work or in that of Johansson (private communication);  b, blended line.
 For lines
annotated with x, the maximum possible branching fraction has been estimated
and from this  the maximum value of {\it A} and maximum possible log~{\it gf} for that transition has
 also been estimated.
Since the values of  {\it A} and log~{\it gf} for lines annotated with x are maximum
values it may be preferable to use the theoretical values for these lines.
No uncertainty in
log~{\it gf} is given for these transitions annotated x  since it is
an approximate estimate.  } 
\enddata 
\end{deluxetable} 
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