\documentstyle{l-aa}
\begin{document}

\begin{table*}          %  Table 1.
\caption[ ]{Energy levels in Rydbergs for the Ni~III ion
relative to the $3d^8 ( ^3F)$ ground state. The present calculated 
energies are compared with experimentally determined 
energies and those calculated by Watts \& Burke (WB). 
The spectroscopic and
correlation configurations for Ni~III, and the values of the
scaling parameters $\lambda_{nl}$ for each orbital in the
Thomas-Fermi-Dirac
potential used in Superstructure, are also given}
\begin{flushleft}
\begin{tabular}{rllllllrlllll}     
            \hline\noalign{\smallskip}
  & Level      &     & Experimental & Present & WB &     
&  & Level      &     & Experimental & Present & WB \\   
            \hline\noalign{\smallskip}
  1&$ 3d^8               $&$^3F      $& 0.00000 & 0.00000 & 0.0000 &
&36&$ 3d^7 (^4P) 4p      $&$^3D^o    $&1.20764 & 1.17313 & 1.1591 \\
  2&$ 3d^8               $&$^1D      $& 0.11881 & 0.15138 & 0.1530 & 
&37&$ 3d^7 (^2G) 4p      $&$^3G^o    $&1.21295 & 1.19463 & 1.1521 \\
  3&$ 3d^8               $&$^3P      $& 0.14431 & 0.16910 & 0.1724  & 
&38&$ 3d^7 (^2G) 4p      $&$^1H^o    $&1.21402 & 1.15889 & 1.1499 \\
  4&$ 3d^8               $&$^1G      $& 0.20152 & 0.23027 & 0.2333  &
&39&$ 3d^7 (^2G) 4p      $&$^1F^o    $&1.22136 & 1.17331 & 1.1673 \\
  5&$ 3d^8               $&$^1S      $& 0.46965 & 0.56320 & 0.5693  & 
&40&$ 3d^7 (^4P) 4p      $&$^3P^o    $&1.22660 & 1.17770 & 1.1857 \\
  6&$ 3d^7 (^4F) 4s      $&$^5F      $&0.49063 & 0.43192 & 0.4345 &
&41&$ 3d^7 (^2P) 4p      $&$^3D^o    $&1.23933 & 1.21491 & 1.2093 \\
  7&$ 3d^7 (^4F) 4s      $&$^3F      $&0.55838 & 0.50696 & 0.5112  & 
&42&$ 3d^7 (^2P) 4p      $&$^1D^o    $&1.24510 & 1.21149 & 1.2057 \\
  8&$ 3d^7 (^4P) 4s      $&$^5P      $&0.64093 & 0.61541 & 0.6196 &
&43&$ 3d^7 (^2H) 4p      $&$^3I^o    $&1.24696 & 1.19688 & 1.1866 \\
  9&$ 3d^7 (^2G) 4s      $&$^3G      $&0.67974 & 0.64029 & 0.6533 & 
&44&$ 3d^7 (^2H) 4p      $&$^3G^o    $&1.24677 & 1.15834 & 1.1864 \\
 10&$ 3d^7 (^4P) 4s      $&$^3P      $&0.70540 & 0.69345 & 0.6985 &  
&45&$ 3d^7 (^2G) 4p      $&$^1S^o    $&1.24983 & 1.21895 & 1.2131 \\
 11&$ 3d^7 (^2G) 4s      $&$^1G      $&0.71312 & 0.67760 & 0.6911 &
&46&$ 3d^7 (^2G) 4p      $&$^3D^o    $&1.25616 & 1.22231 & 1.2161 \\
 12&$ 3d^7 (^2P) 4s      $&$^3P      $&0.71548 & 0.70220 & 0.7165 &  
&47&$ 3d^7 (^4P) 4p      $&$^1I^o    $&1.26338 & 1.20874 & 1.1989 \\
 13&$ 3d^7 (^2H) 4s      $&$^3H      $&0.73970 & 0.70229 & 0.7153 & 
&48&$ 3d^7 (^2P) 4p      $&$^3F^o    $&1.27101 & 1.23541 & 1.2299 \\
 14&$ 3d^7 (a ^2D) 4s    $&$^3D      $&0.64256 & 0.72358 & 0.7390 &  
&49&$ 3d^7 (^2H) 4p      $&$^3S^o    $&1.27478 & 1.25482 & 1.2557 \\
 15&$ 3d^7 (^2P) 4s      $&$^1P      $&0.76191 & 0.73984 & 0.7550 & 
&50&$ 3d^7 (^2H) 4p      $&$^1P^o    $&1.27960 & 1.27078 & 1.2486 \\
 16&$ 3d^7 (^2H) 4s      $&$^1H      $&0.77312 & 0.73884 & 0.7526 &  
&51&$ 3d^7 (^2G) 4p      $&$^1D^o    $&1.28890 & 1.26425 & 1.2598 \\
 17&$ 3d^7 (a ^2D) 4s    $&$^1D      $&0.78052 & 0.76212 & 0.7777 & 
&52&$ 3d^7 (^2G) 4p      $&$^3H^o    $&1.28986 & 1.24017 & 1.2364 \\
 18&$ 3d^7 (^2F) 4s      $&$^3F      $&0.88456 & 0.88604 & 0.9030 &  
&53&$ 3d^7(a^2D)4p   $&$^1F^o  $&1.30193 &1.26710 &1.2662     \\
 19&$ 3d^7 (^2F) 4s      $&$^1F      $&0.92002 & 0.92621 & 0.9430 & 
&54&$ 3d^7(a^2D)4p   $&$^3P^o  $&1.30394 &1.27065 &1.2702     \\
 20&$ 3d^7 (^4F) 4p      $&$^5F^o    $&1.00141 & 0.93138 & 0.9116 &  
&55&$ 3d^7(^2H)4p    $&$^1G^o  $&1.30456 &1.26040 &1.2616     \\
 21&$ 3d^7 (^4F) 4p      $&$^5D^o    $&1.01975 & 0.94546 & 0.9272 &   
&56&$ 3d^7(a^2D)4p   $&$^1P^o  $&1.32094 &1.29308 &1.2952     \\
 22&$ 3d^7 (^4F) 4p      $&$^5G^o    $&1.02468 & 0.94404 & 0.9341 &  
&57&$ 3d^7(^2H)4p    $&$^1H^o  $&1.32436 &1.28011 &1.2797     \\
 23&$ 3d^7 (^4F) 4p      $&$^3G^o    $&1.05115 & 0.98332 & 0.9650  & 
&58&$ 3d^6 4s^2      $&$^5D    $&1.39116 &1.67319 & ---       \\
 24&$ 3d^7 (^4F) 4p      $&$^3F^o    $&1.05715 & 0.99140 & 0.9758 &  
&59&$ 3d^7(^2F)4p    $&$^1D^o  $&1.40405 &1.39724 &1.3949     \\
 25&$ 3d^7 (^4F) 4p      $&$^3D^o    $&1.07862 & 1.01563 & 1.0032 & 
&60&$ 3d^7(^2F)4p    $&$^3G^o  $&1.41372 &1.40245 &1.4011     \\
 26&$ 3d^7 (^4F) 4s      $&$^3D      $&1.09859 & 1.13533 & 0.9272 &  
&61&$ 3d^7(^2F)4p    $&$^3F^o  $&1.41870 &1.40517 &1.4049     \\
 27&$ 3d^7 (^4P) 4p      $&$^5S^o    $&1.10526 & 1.06400 & 1.0416 &
&62&$ 3d^7(^2F)4p    $&$^3D^o  $&1.42190 &1.40991 &1.4100     \\
 28&$ 3d^7 (^4P) 4s      $&$^1D      $&1.13400 & 1.17534 & 1.2001 &
&63&$ 3d^7(^2F)4p    $&$^1G^o  $&1.42505 &1.41456 &1.4113     \\
 29&$ 3d^7 (^4P) 4p      $&$^5D^o    $&1.17636 & 1.13882 & 1.1239 &
&64&$ 3d^7(^2F)4p    $&$^1F^o  $&1.46496 &1.45926 &1.4607     \\
 30&$ 3d^7 (^4P) 4p      $&$^3S^o    $&1.18346 & 1.15889 & 1.1447 &
&65&$ 3d^7(b^2D)4p   $&$^3P^o  $&1.59975 &1.62133 &1.6258     \\
 31&$ 3d^7 (^2G) 4p      $&$^3H^o    $&1.19329 & 1.14180 & 1.1322 &
&66&$ 3d^7(b^2D)4p   $&$^3F^o  $&1.61895 &1.64261 &1.6492     \\
 32&$ 3d^7 (^2G) 4p      $&$^3F^o    $&1.20136 & 1.15002 & 1.1443 &
&67&$ 3d^7(b^2D)4p   $&$^1P^o  $&1.64219 &1.67025 &1.6795     \\
 33&$ 3d^7 (^4P) 4p      $&$^5P^o    $&1.20340 & 1.16800 & 1.1562 &
&68&$ 3d^7(b^2D)4p   $&$^1F^o  $&1.64633 &1.67426 &1.6796     \\
 34&$ 3d^7 (^2G) 4p      $&$^1G^o    $&1.20589 & 1.15878 & 1.1430 &
&69&$ 3d^7(b^2D)4p   $&$^3D^o  $&1.66984 &1.69755 &1.7097     \\
 35&$ 3d^7 (^2P) 4p      $&$^3P^o    $&1.20688 & 1.17770 & 1.1694 &
&70&$ 3d^7(b^2D)4p   $&$^1D^o  $&1.79860 &1.69812 &1.7088     \\
\noalign{\smallskip}
            \hline
         \end{tabular}
\end{flushleft}
Ni~III configurations

Spectroscopic:
$3p^6\ 3d^8$, $3p^6\ 3d^7\ 4s$, $3p^6\ 3d^7\ 4p$, $3p^6\ 3d^6\ 4s^2$

Correlation:
$3p^6\ 3d^6\ 4p^2$, $3p^6\ 3d^7\ 4d$, $3p^6\ 3d^6\ 4s\ 4p$,
$3p^5\ 3d^9$, $3p^5\ 3d^8\ 4s$, $3p^5\ 3d^8\ 4p$, $3p^5\ 3d^8\ 4d$

$\lambda_{nl}$: 1.43121(1s), 0.93950(2s), 1.28641(2p), 1.15714(3s),
1.02417(3p),

1.01626(3d), 0.97488(4s), 0.96711(4p), 1.26086(4d)

\end{table*}

\clearpage
\begin{table}        %  Table 2.
\caption[ ]{Comparison between present and NIST
radiative transition rates (A-values) for allowed transitions.
A-values are given in units of $10^8$ s$^{-1}$.}
\begin{flushleft}
\begin{tabular}{ccc}
            \hline\noalign{\smallskip}
Transition & NIST & Present \\
            \hline\noalign{\smallskip}
$ 3d^7(^4F)4s\ ^5F_5-3d^7(^4F)4p\ ^5G^o_4$& 0.038& 0.0269 \\
$ 3d^7(^4F)4s\ ^5F_5-3d^7(^4F)4p\ ^5G^o_6$&  7.9 & 8.28   \\
$ 3d^7(^4F)4s\ ^5F_4-3d^7(^4F)4p\ ^5G^o_5$&  6.3 & 7.76  \\
$ 3d^7(^4F)4s\ ^5F_2-3d^7(^4F)4p\ ^5G^o_3$&  6.0 & 7.25  \\
$ 3d^7(^4F)4s\ ^5F_1-3d^7(^4F)4p\ ^5G^o_2$&  5.9 & 7.08  \\
$ 3d^7(^4F)4s\ ^5F_1-3d^7(^4F)4p\ ^5D^o_0$&  6.7 & 7.63 \\
$ 3d^7(^4F)4s\ ^3F_4-3d^7(^4F)4p\ ^3D^o_3$&  5.7 & 5.75 \\
$ 3d^7(^4F)4s\ ^3F_3-3d^7(^4F)4p\ ^3D^o_2$&  5.5 & 5.75 \\
$ 3d^7(^4F)4s\ ^3F_2-3d^7(^4F)4p\ ^3D^o_1$&  6.5 & 7.28 \\
$ 3d^7(^4F)4s\ ^5F_5-3d^7(^4F)4p\ ^5F^o_5$&  6.2 & 7.38 \\
$ 3d^7(^4F)4s\ ^5F_1-3d^7(^4F)4p\ ^5F^o_1$&  3.8 & 4.05 \\
$ 3d^7(^4F)4s\ ^5F_2-3d^7(^4F)4p\ ^5F^o_2$&  2.5 & 2.84 \\
$ 3d^7(^4F)4s\ ^5F_3-3d^7(^4F)4p\ ^5F^o_3$&  2.5 & 2.93 \\
$ 3d^7(^4F)4s\ ^5F_4-3d^7(^4F)4p\ ^5F^o_4$&  2.7 & 3.46 \\
$ 3d^7(^4F)4s\ ^3F_4-3d^7(^4F)4p\ ^3F^o_4$&  5.6 & 5.30 \\
$ 3d^7(^4F)4s\ ^3F_3-3d^7(^4F)4p\ ^3F^o_3$&  4.6 & 4.27 \\
$ 3d^7(^4F)4s\ ^3F_2-3d^7(^4F)4p\ ^3F^o_2$&  5.0 & 5.03 \\
$ 3d^7(^4F)4s\ ^3F_3-3d^7(^4F)4p\ ^3G^o_4$&  5.3 & 5.04 \\
$ 3d^7(^4F)4s\ ^3F_4-3d^7(^4F)4p\ ^3G^o_5$&  5.4 & 6.09 \\
\noalign{\smallskip}
            \hline
         \end{tabular}
\end{flushleft}
\end{table}  


\clearpage
\begin{table}[Hh!]     %  Table 3.
\caption[ ]{Comparison of effective collision strengths in {\it LS} coupling
at T=10$^4$ K for excitations from the ground term to the first
51 excited terms.}
\begin{flushleft}
\begin{tabular}{rlccc}
            \hline\noalign{\smallskip}
 & Final state & $\Upsilon(52CC)$ & $\Upsilon(70CC)$&${\Upsilon(70CC)\over \Upsilon(52CC)}$\\
            \hline\noalign{\smallskip}
  2 & $3d^8\     ^1D  $ & 1.482& 1.804& 1.217 \\
  3 & $3d^8\ 4s\ ^3P  $ & 5.018& 5.064& 1.009 \\
  4 & $3d^8\ 4s\ ^1G  $ & 3.126& 3.115& 0.997 \\
  5 & $3d^8\ 4s\ ^1S  $ & 0.108& 0.149& 1.381 \\
  6 & $3d^7\ 4s\ ^5P  $ & 6.222& 6.109& 0.982 \\
  7 & $3d^7\ 4s\ ^3F  $ & 8.026& 9.237& 1.151 \\
  8 & $3d^7\ 4s\ ^5P  $ & 1.434& 1.571& 1.096 \\
  9 & $3d^7\ 4s\ ^3G  $ & 6.246& 7.212& 1.155 \\
 10 & $3d^7\ 4s\ ^3P  $ & 1.387& 1.612& 1.163 \\        
 11 & $3d^7\ 4s\ ^1G  $ & 0.822& 0.946& 1.151 \\
 12 & $3d^7\ 4s\ ^3P  $ & 1.560& 1.748& 1.121 \\
 13 & $3d^7\ 4s\ ^3H  $ & 6.193& 6.611& 1.068 \\
 14 & $3d^7\ 4s\ ^3D  $ & 2.787& 2.752& 0.987 \\
 15 & $3d^7\ 4s\ ^1P  $ & 0.458& 0.457& 0.998 \\
 16 & $3d^7\ 4s\ ^1H  $ & 1.030& 0.789& 0.766 \\
 17 & $3d^7\ 4s\ ^1D  $ & 0.608& 0.554& 0.911 \\
 18 & $3d^7\ 4s\ ^3F  $ & 1.221& 0.874& 0.715 \\
 19 & $3d^7\ 4s\ ^1F  $ & 0.272& 0.079& 0.292 \\
 20 & $3d^7\ 4p\ ^5F^o$ & 1.968& 2.016& 1.024 \\
 21 & $3d^7\ 4p\ ^5D^o$ & 1.032& 1.111& 1.076 \\
 22 & $3d^7\ 4p\ ^5G^o$ & 1.777& 1.871& 1.053 \\
 23 & $3d^7\ 4p\ ^3G^o$ & 2.058& 2.055& 0.998 \\
 24 & $3d^7\ 4p\ ^3F^o$ & 6.761& 6.880& 1.018 \\
 25 & $3d^7\ 4p\ ^3D^o$ & 3.932& 4.034& 1.026 \\
 26 & $3d^7\ 4s\ ^3D  $ & 0.381& 0.248& 0.650 \\
 27 & $3d^7\ 4p\ ^5S^o$ & 0.241& 0.245& 1.019 \\
 28 & $3d^7\ 4s\ ^1D  $ & 0.094& 0.027& 0.292 \\
 29 & $3d^7\ 4p\ ^5D^o$ & 0.466& 0.457& 0.979 \\
 30 & $3d^7\ 4p\ ^3S^o$ & 0.108& 0.100& 0.924 \\
 31 & $3d^7\ 4p\ ^3H^o$ & 0.756& 0.777& 1.028 \\         
 32 & $3d^7\ 4p\ ^3F^o$ & 4.698& 4.784& 1.018 \\
 33 & $3d^7\ 4p\ ^5P^o$ & 0.273& 0.259& 0.949 \\
 34 & $3d^7\ 4p\ ^1G^o$ & 0.258& 0.268& 1.037 \\
 35 & $3d^7\ 4p\ ^3P^o$ & 0.270& 0.243& 0.902 \\
 36 & $3d^7\ 4p\ ^3D^o$ & 0.800& 0.774& 0.969 \\
 37 & $3d^7\ 4p\ ^3G^o$ & 1.325& 1.317& 0.993 \\
 38 & $3d^7\ 4p\ ^1H^o$ & 0.193& 0.183& 0.947 \\
 39 & $3d^7\ 4p\ ^1F^o$ & 0.146& 0.139& 0.955 \\
 40 & $3d^7\ 4p\ ^3P^o$ & 0.222& 0.208& 0.937 \\
 41 & $3d^7\ 4p\ ^3D^o$ & 0.527& 0.736& 1.398 \\
 42 & $3d^7\ 4p\ ^1D^o$ & 0.072& 0.065& 0.910 \\
 43 & $3d^7\ 4p\ ^3I^o$ & 0.693& 0.650& 0.938 \\
 44 & $3d^7\ 4p\ ^3G^o$ & 5.617& 5.648& 1.005 \\
 45 & $3d^7\ 4p\ ^1S^o$ & 0.010& 0.009& 0.889 \\
 46 & $3d^7\ 4p\ ^3D^o$ & 3.308& 3.332& 1.007 \\
 47 & $3d^7\ 4p\ ^1I^o$ & 0.214& 0.214& 0.997 \\
 48 & $3d^7\ 4p\ ^3F^o$ & 0.863& 0.887& 1.028 \\
 49 & $3d^7\ 4p\ ^3S^o$ & 0.038& 0.031& 0.823 \\
 50 & $3d^7\ 4p\ ^1P^o$ & 0.022& 0.019& 0.860 \\
 51 & $3d^7\ 4p\ ^1D^o$ & 0.062& 0.061& 0.986 \\
 52 & $3d^7\ 4p\ ^3H^o$ & 0.369& 0.363& 0.985 \\     
\noalign{\smallskip}
            \hline
         \end{tabular}
\end{flushleft}
\end{table}  



\clearpage
\begin{table}[ht]      % Table 4
\caption[]{Comparison of effective collision strengths
in {\it LS} coupling
from the present calculation and those of WB. The level indices refer 
to the entries in Table 1.}
\begin{flushleft}
\begin{tabular}{lllllll}
\hline
Trans. & \multicolumn{2}{c}{5000K} & \multicolumn{2}{c}{10~000K} & \multicolumn{2}{c}{20~000K} \cr
 & Present & WB & Present & BW & Present & WB \cr
\hline
1-2 & 1.25 & 1.37 & 1.48 & 1.48 & 1.70 & 1.56 \cr
1-3 & 5.17 & 4.03 & 5.02 & 4.19 & 4.69 & 4.19 \cr
1-4 & 2.80 & 2.24 & 3.13 & 2.52 & 3.30 & 2.71 \cr
1-5 & 0.l26& 0.137& 0.110& 0.118& 0.109& 0.112\cr
1-6 & 6.29 & 5.49 & 6.14 & 5.83 & 5.60 & 5.52 \cr
1-7 & 8.09 & 7.75 & 7.99 & 7.86 & 7.65 & 7.54 \cr
1-8 & 1.47 & 1.43 & 1.38 & 1.32 & 1.28 & 1.22 \cr
1-9 & 7.05 & 5.25 & 6.21 & 5.08 & 5.31 & 4.59 \cr
1-10& 1.34 & 1.68 & 1.39 & 1.54 & 1.34 & 1.40 \cr
1-11& 0.830& 1.03 & 0.814&0.972 & 0.774& 0.876\cr
1-12& 1.67 & 1.23 & 1.54 & 1.27 & 1.32 & 1.17 \cr
1-13& 7.03 & 6.39 & 6.24 & 6.00 & 5.37 & 5.13 \cr
1-14& 2.82 & 2.28 & 2.86 & 2.45 & 2.57 & 2.31 \cr
1-15& 0.589& 0.504& 0.442& 0.413& 0.329&0.320 \cr
1-16& 0.967& 1.03 & 1.03 & 1.09 & 0.978& 1.03 \cr
1-17& 0.682& 0.677& 0.615& 0.624& 0.520& 0.531\cr
1-18& 1.01 & 0.843& 1.21 & 1.13 & 1.27 & 1.25 \cr
1-19&0.262 & 0.292&0.266 & 0.302&0.240 & 0.270\cr
1-26& 0.337& 0.374& 0.389& 0.416& 0.375& 0.392\cr
1-28& 0.105&0.096&0.096&0.091&0.079&0.078\cr
\hline
\end{tabular}
\end{flushleft}
\end{table}
                                     

\clearpage
\begin{table*}       %  Table 5.
\caption[ ]{Line emissivities for the strongest optical and IR Ni~III lines. 
The emissivity per Ni$^{2+}$ ion of the $\lambda$6000 line is given in
erg/s. The emissivity of other lines is relative to that of 
$\lambda$6000.}  
\begin{flushleft}
\begin{tabular}{rrrrrrrrrrr}   
            \hline\noalign{\smallskip}
$T$ & $N_e$ & $j(\lambda6000)$ &$I(7.3\mu m)$&$I(11\mu
m)$&$I(\lambda7889)$&$I(\lambda8499)$&$I(\lambda6533)$&$I(\lambda6401)$&
$I(\lambda4326)$&$I(\lambda4596)$\cr
\hline
\noalign{\smallskip}
 5.0E+3 & 1.E+02 & 1.03E-20 & 8.46E+1 & 1.05E+1 & 3.53E+0 &
 1.43E+0 & 2.19E+0 & 7.84E-1 & 6.18E-1 & 2.99E-1\\
          & 1.E+04 & 1.02E-18 & 8.35E+1 & 1.04E+1 & 3.54E+0 &
 1.44E+0 & 2.19E+0 & 7.96E-1 & 6.22E-1 & 3.01E-1\\
          & 1.E+06 & 8.19E-17 & 3.96E+1 & 5.73E+0 & 4.54E+0 &
 1.84E+0 & 2.19E+0 & 1.21E+0 & 8.51E-1 & 4.12E-1\\
          & 1.E+08 & 3.98E-16 & 1.26E+1 & 1.92E+0 & 1.36E+1 &
 5.52E+0 & 2.19E+0 & 1.23E+0 & 2.49E+0 & 1.21E+0\\
          & 1.E+10 & 4.14E-16 & 1.22E+1 & 1.86E+0 & 1.57E+1 &
 6.37E+0 & 2.19E+0 & 1.22E+0 & 2.73E+0 & 1.32E+0\\
 1.0E+4 & 1.E+02 & 7.67E-20 & 1.12E+1 & 1.56E+0 & 3.23E+0 &
 1.31E+0 & 2.19E+0 & 8.61E-1 & 1.82E+0 & 8.82E-1\\
          & 1.E+04 & 7.64E-18 & 1.11E+1 & 1.55E+0 & 3.25E+0 &
 1.32E+0 & 2.19E+0 & 8.71E-1 & 1.83E+0 & 8.86E-1\\
          & 1.E+06 & 6.07E-16 & 5.63E+0 & 9.03E-1 & 3.93E+0 &
 1.60E+0 & 2.19E+0 & 1.27E+0 & 2.35E+0 & 1.14E+0\\
          & 1.E+08 & 3.55E-15 & 1.42E+0 & 2.47E-1 & 9.38E+0 &
 3.81E+0 & 2.19E+0 & 1.29E+0 & 6.24E+0 & 3.02E+0\\
          & 1.E+10 & 3.73E-15 & 1.35E+0 & 2.34E-1 & 1.08E+1 &
 4.36E+0 & 2.19E+0 & 1.28E+0 & 6.90E+0 & 3.34E+0\\
 1.5E+4 & 1.E+02 & 1.34E-19 & 6.14E+0 & 8.77E-1 & 3.26E+0 &
 1.32E+0 & 2.19E+0 & 8.91E-1 & 2.69E+0 & 1.30E+0\\
          & 1.E+04 & 1.34E-17 & 6.08E+0 & 8.72E-1 & 3.27E+0 &
 1.33E+0 & 2.19E+0 & 9.00E-1 & 2.70E+0 & 1.31E+0\\
          & 1.E+06 & 1.06E-15 & 3.22E+0 & 5.23E-1 & 3.88E+0 &
 1.58E+0 & 2.19E+0 & 1.29E+0 & 3.37E+0 & 1.63E+0\\
          & 1.E+08 & 6.76E-15 & 6.98E-1 & 1.26E-1 & 8.35E+0 &
 3.39E+0 & 2.19E+0 & 1.31E+0 & 8.46E+0 & 4.09E+0\\
          & 1.E+10 & 7.11E-15 & 6.46E-1 & 1.17E-1 & 9.48E+0 &
 3.85E+0 & 2.19E+0 & 1.30E+0 & 9.40E+0 & 4.55E+0\\
 2.0E+4 & 1.E+02 & 1.68E-19 & 4.68E+0 & 6.76E-1 & 3.31E+0 &
 1.34E+0 & 2.19E+0 & 9.09E-1 & 3.30E+0 & 1.60E+0\\
          & 1.E+04 & 1.67E-17 & 4.64E+0 & 6.72E-1 & 3.32E+0 &
 1.35E+0 & 2.19E+0 & 9.17E-1 & 3.32E+0 & 1.60E+0\\
          & 1.E+06 & 1.33E-15 & 2.54E+0 & 4.11E-1 & 3.90E+0 &
 1.58E+0 & 2.19E+0 & 1.30E+0 & 4.07E+0 & 1.97E+0\\
          & 1.E+08 & 8.86E-15 & 4.94E-1 & 9.05E-2 & 7.90E+0 &
 3.21E+0 & 2.19E+0 & 1.33E+0 & 9.85E+0 & 4.77E+0\\
          & 1.E+10 & 9.25E-15 & 4.48E-1 & 8.32E-2 & 8.91E+0 &
 3.62E+0 & 2.19E+0 & 1.31E+0 & 1.10E+1 & 5.31E+0\\
 3.0E+4 & 1.E+02 & 1.95E-19 & 3.66E+0 & 5.36E-1 & 3.40E+0 &
 1.38E+0 & 2.19E+0 & 9.29E-1 & 4.05E+0 & 1.96E+0\\
          & 1.E+04 & 1.94E-17 & 3.63E+0 & 5.33E-1 & 3.41E+0 &
 1.38E+0 & 2.19E+0 & 9.36E-1 & 4.07E+0 & 1.97E+0\\
          & 1.E+06 & 1.55E-15 & 2.09E+0 & 3.34E-1 & 3.94E+0 &
 1.60E+0 & 2.19E+0 & 1.30E+0 & 4.89E+0 & 2.36E+0\\
          & 1.E+08 & 1.08E-14 & 3.62E-1 & 6.70E-2 & 7.55E+0 &
 3.06E+0 & 2.19E+0 & 1.34E+0 & 1.15E+1 & 5.54E+0\\
          & 1.E+10 & 1.07E-14 & 3.14E-1 & 5.96E-2 & 8.40E+0 &
 3.41E+0 & 2.19E+0 & 1.32E+0 & 1.28E+1 & 6.20E+0\\
 4.0E+4  & 1.E+02 & 2.01E-19 & 3.27E+0 & 4.86E-1 & 3.46E+0 &
 1.41E+0 & 2.19E+0 & 9.40E-1 & 4.44E+0 & 2.15E+0\\
          & 1.E+04 & 2.01E-17 & 3.25E+0 & 4.83E-1 & 3.47E+0 &
 1.41E+0 & 2.19E+0 & 9.47E-1 & 4.45E+0 & 2.15E+0\\
          & 1.E+06 & 1.60E-15 & 1.94E+0 & 3.09E-1 & 3.99E+0 &
 1.62E+0 & 2.19E+0 & 1.29E+0 & 5.28E+0 & 2.56E+0\\
          & 1.E+08 & 1.13E-14 & 3.22E-1 & 5.99E-2 & 7.46E+0 &
 3.03E+0 & 2.19E+0 & 1.35E+0 & 1.23E+1 & 5.97E+0\\
          & 1.E+10 & 1.06E-14 & 2.68E-1 & 5.14E-2 & 8.20E+0 &
 3.33E+0 & 2.19E+0 & 1.32E+0 & 1.38E+1 & 6.67E+0\\
 5.0E+4 & 1.E+02 & 2.01E-19 & 3.07E+0 & 4.61E-1 & 3.50E+0 &
 1.42E+0 & 2.19E+0 & 9.43E-1 & 4.61E+0 & 2.23E+0\\
          & 1.E+04 & 2.00E-17 & 3.05E+0 & 4.58E-1 & 3.51E+0 &
 1.42E+0 & 2.19E+0 & 9.50E-1 & 4.63E+0 & 2.24E+0\\
          & 1.E+06 & 1.60E-15 & 1.88E+0 & 2.98E-1 & 4.01E+0 &
 1.63E+0 & 2.19E+0 & 1.29E+0 & 5.45E+0 & 2.64E+0\\
          & 1.E+08 & 1.14E-14 & 3.09E-1 & 5.76E-2 & 7.47E+0 &
 3.03E+0 & 2.19E+0 & 1.36E+0 & 1.28E+1 & 6.21E+0\\
          & 1.E+10 & 1.01E-14 & 2.49E-1 & 4.79E-2 & 8.13E+0 &
 3.30E+0 & 2.19E+0 & 1.32E+0 & 1.44E+1 & 6.95E+0\\
 6.0E+4 & 1.E+02 & 1.98E-19 & 2.96E+0 & 4.47E-1 & 3.53E+0 &
 1.43E+0 & 2.19E+0 & 9.43E-1 & 4.71E+0 & 2.28E+0\\
          & 1.E+04 & 1.97E-17 & 2.94E+0 & 4.45E-1 & 3.54E+0 &
 1.44E+0 & 2.19E+0 & 9.49E-1 & 4.72E+0 & 2.28E+0\\
          & 1.E+06 & 1.57E-15 & 1.85E+0 & 2.94E-1 & 4.04E+0 &
 1.64E+0 & 2.19E+0 & 1.28E+0 & 5.54E+0 & 2.68E+0\\
          & 1.E+08 & 1.12E-14 & 3.07E-1 & 5.74E-2 & 7.53E+0 &
 3.06E+0 & 2.19E+0 & 1.36E+0 & 1.32E+1 & 6.38E+0\\
          & 1.E+10 & 9.56E-15 & 2.41E-1 & 4.64E-2 & 8.11E+0 &
 3.29E+0 & 2.19E+0 & 1.32E+0 & 1.47E+1 & 7.13E+0\\
            \hline
         \end{tabular}
\end{flushleft}
\end{table*}

\end{document}
