\begin{table}   %t5
\caption{\label{tab5}Electric quadrupole transition rates (in s$^{-1}$) for levels
within the 3d$^7$ ground state configuration of \nifour.
The table shows the results computed with neither TEC nor 2-body relativistic operators (w/o T + w/o 2-body), with
2-body relativistic operators (w/o T + 2-body), with TECs and 2-body relativistic operators (T + 2-body)
and with TECs, LEVs and  2-body relativistic operators (T + L + 2-body). The rates previously
reported by Hansen et~al. (\cite{Hansen1984}) and Garstang (1969) are also given.}
%\centering
\par
\begin{tabular}{cccccccc}
            \hline \hline 
 & & \multispan{5}{\ $A_{ij}(E2)$}   \\
Term $i$&Term $j$& w/o T + w/o 2-body  & w/o T + 2-body   & T + 2-body & T + L + 2-body &Hansen &Garstang\\
            \hline
$\rm ^4F_{7/2}$&$\rm ^4F_{9/2}$&5.65E$-$09&4.41E$-$09&4.49E$-$09&4.16E$-$09&3.40E$-$09&2.50E$-$09\\
$\rm ^4F_{5/2}$&$\rm ^4F_{7/2}$&1.61E$-$09&1.25E$-$09&1.25E$-$09&1.15E$-$09&9.40E$-$10&7.40E$-$10\\
$\rm ^4F_{3/2}$&$\rm ^4F_{5/2}$&2.67E$-$10&2.11E$-$10&2.09E$-$10&1.93E$-$10&1.60E$-$10&1.20E$-$10\\
$\rm ^4P_{5/2}$&$\rm ^4F_{9/2}$&1.16E$-$01&1.18E$-$01&8.65E$-$02&8.57E$-$02&6.80E$-$02&6.20E$-$02\\
$\rm ^4P_{5/2}$&$\rm ^4F_{7/2}$&2.66E$-$02&2.74E$-$02&1.97E$-$02&1.96E$-$02&1.50E$-$02&1.50E$-$02\\
$\rm ^4P_{5/2}$&$\rm ^4F_{5/2}$&4.57E$-$03&4.76E$-$03&3.36E$-$03&3.36E$-$03&2.70E$-$03&2.50E$-$03\\
$\rm ^4P_{5/2}$&$\rm ^4F_{3/2}$&4.23E$-$04&4.44E$-$04&3.09E$-$04&3.11E$-$04&2.50E$-$04&2.40E$-$04\\
$\rm ^4P_{3/2}$&$\rm ^4F_{7/2}$&5.78E$-$02&6.05E$-$02&4.44E$-$02&4.42E$-$02&3.50E$-$02&3.40E$-$02\\
$\rm ^4P_{3/2}$&$\rm ^4F_{5/2}$&3.28E$-$02&3.47E$-$02&2.50E$-$02&2.50E$-$02&2.00E$-$02&1.90E$-$02\\
$\rm ^4P_{3/2}$&$\rm ^4F_{3/2}$&9.08E$-$03&9.67E$-$03&6.89E$-$03&6.91E$-$03&5.40E$-$03&5.40E$-$03\\
$\rm ^4P_{3/2}$&$\rm ^4P_{5/2}$&1.51E$-$11&1.99E$-$11&3.42E$-$11&3.14E$-$11&2.40E$-$11&8.10E$-$11\\
$\rm ^4P_{1/2}$&$\rm ^4F_{5/2}$&4.45E$-$02&4.54E$-$02&3.28E$-$02&3.28E$-$02&2.60E$-$02&2.50E$-$02\\
$\rm ^4P_{1/2}$&$\rm ^4F_{3/2}$&5.79E$-$02&5.93E$-$02&4.23E$-$02&4.24E$-$02&3.30E$-$02&3.20E$-$02\\
$\rm ^4P_{1/2}$&$\rm ^4P_{3/2}$&9.97E$-$10&4.49E$-$10&3.92E$-$10&3.89E$-$10&3.00E$-$10&2.40E$-$10\\
$\rm ^2G_{9/2}$&$\rm ^4F_{9/2}$&2.47E$-$04&1.97E$-$04&1.43E$-$04&1.42E$-$04&1.30E$-$04&1.20E$-$04\\
$\rm ^2G_{9/2}$&$\rm ^4F_{7/2}$&1.12E$-$05&9.16E$-$06&7.06E$-$06&7.09E$-$06&6.60E$-$06&5.70E$-$06\\
$\rm ^2G_{9/2}$&$\rm ^4F_{5/2}$&1.98E$-$05&1.56E$-$05&9.65E$-$06&9.73E$-$06&8.90E$-$06&7.70E$-$06\\
$\rm ^2G_{7/2}$&$\rm ^4F_{9/2}$&4.30E$-$05&3.23E$-$05&2.53E$-$05&2.52E$-$05&2.40E$-$05&2.00E$-$05\\
$\rm ^2G_{7/2}$&$\rm ^4F_{7/2}$&5.42E$-$05&4.21E$-$05&3.07E$-$05&3.07E$-$05&2.90E$-$05&2.60E$-$05\\
$\rm ^2G_{7/2}$&$\rm ^4F_{5/2}$&5.30E$-$06&4.35E$-$06&2.83E$-$06&2.84E$-$06&2.60E$-$06&2.30E$-$06\\
$\rm ^2G_{7/2}$&$\rm ^4F_{3/2}$&3.32E$-$05&2.70E$-$05&1.62E$-$05&1.64E$-$05&1.60E$-$05&1.30E$-$05\\
$\rm ^2G_{7/2}$&$\rm ^2G_{9/2}$&2.05E$-$09&1.29E$-$09&1.72E$-$09&1.67E$-$09&1.60E$-$09&1.20E$-$09\\
$\rm ^2P_{3/2}$&$\rm ^4F_{7/2}$&1.89E$-$02&1.61E$-$02&1.18E$-$02&1.18E$-$02&9.90E$-$03&7.20E$-$03\\
$\rm ^2P_{3/2}$&$\rm ^4F_{5/2}$&8.24E$-$03&7.11E$-$03&5.01E$-$03&5.03E$-$03&4.30E$-$03&2.90E$-$03\\
$\rm ^2P_{3/2}$&$\rm ^4F_{3/2}$&2.00E$-$03&1.73E$-$03&1.19E$-$03&1.20E$-$03&1.10E$-$03&7.40E$-$04\\
$\rm ^2P_{3/2}$&$\rm ^4P_{5/2}$&6.73E$-$06&5.56E$-$06&6.58E$-$06&6.68E$-$06&5.80E$-$06&5.60E$-$06\\
$\rm ^2P_{3/2}$&$\rm ^4P_{3/2}$&3.88E$-$06&3.06E$-$06&3.56E$-$06&3.63E$-$06&2.60E$-$06&2.90E$-$06\\
$\rm ^2P_{3/2}$&$\rm ^4P_{1/2}$&5.45E$-$08&5.23E$-$08&7.48E$-$08&7.66E$-$08&4.40E$-$08&5.60E$-$08\\
$\rm ^2P_{1/2}$&$\rm ^4F_{5/2}$&8.20E$-$03&6.78E$-$03&5.10E$-$03&5.14E$-$03&4.20E$-$03&3.40E$-$03\\
$\rm ^2P_{1/2}$&$\rm ^4F_{3/2}$&4.65E$-$03&3.89E$-$03&2.68E$-$03&2.70E$-$03&2.40E$-$03&1.70E$-$03\\
$\rm ^2P_{1/2}$&$\rm ^4P_{5/2}$&1.07E$-$05&7.94E$-$06&9.01E$-$06&9.21E$-$06&8.00E$-$06&8.40E$-$06\\
$\rm ^2P_{1/2}$&$\rm ^4P_{3/2}$&3.43E$-$07&2.14E$-$07&2.04E$-$07&2.10E$-$07&4.30E$-$07&3.90E$-$07\\
$\rm ^2P_{1/2}$&$\rm ^2P_{3/2}$&1.64E$-$08&8.66E$-$09&8.65E$-$09&9.20E$-$09&8.10E$-$09&1.50E$-$08\\
            \hline
         \end{tabular}
       \end{table}