\begin{table}%t3
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\caption{\label{Table3a} Truncated {\tt STGBB} output "{\tt FVALUE}'':
$gf$-values and Einstein coefficients $A$ for [{\tt 0 0 0   0 2 1}]
$=~(0^\re - 1^\ro)$ transitions of~\Fedisept\ [{\tt Z=26, \mbox{\rm core-}Nel=9}],
as function of bound state energies~{\tt RE}($n_1l_1~0^\re$)
and {\tt Re}($n_2l_2~1^{\ro}$) in units of~$z^2~$Ry, $z$~={\tt~26-9}.
The line strength column $S$(E1) has been added by hand
(see Eqs.~(7), (8)) for the first transition array.}
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        26         9    IPERT= 0     AC,IBUT= 1.0E-5 1  06/25/01  15:06:37     
    0    0    0         0    2    1 
   20   47    RE1          RE2     GFL  -  E1  -  GFV    A(E1)*s      S(E1)    
  1  1 -3.212451E-1 -1.360506E-1 -1.225E-01 -1.232E-01  9.396E+11   6.866E-3  
  1  2 -3.212451E-1 -1.329843E-1 -1.010E-01 -1.020E-01  8.005E+11   5.569E-3  
  1  3 -3.212451E-1 -1.167997E-1 -8.149E-03 -8.015E-03  7.617E+10   4.138E-4  
  1  4 -3.212451E-1 -1.141704E-1 -6.222E-01 -5.940E-01  5.967E+12   3.119E-2  
  1  5 -3.212451E-1 -1.107050E-1 -2.321E+00 -2.214E+00  2.301E+13   1.144E-1  
  1  6 -3.212451E-1 -9.354728E-2 -3.511E-02 -3.404E-02  4.070E+11   1.601E-3  
  1  7 -3.212451E-1 -9.243291E-2 -2.843E-01 -2.989E-01  3.328E+12   1.290E-2  
  1  8 -3.212451E-1 -7.222739E-2 -2.289E-02 -2.328E-02  3.175E+11   9.542E-4  
  1  9 -3.212451E-1 -6.907663E-2 -1.761E-02 -1.707E-02  2.504E+11   7.249E-4  
  1 10 -3.212451E-1 -6.480154E-2 -3.289E-03 -3.310E-03  4.837E+10   1.331E-4  
  1 11 -3.212451E-1 -6.369437E-2 -3.601E-01 -3.275E-01  5.341E+12   1.451E-2  
  1 12 -3.212451E-1 -6.072860E-2 -3.993E-01 -3.613E-01  6.059E+12   1.591E-2  
  1 13 -3.212451E-1 -4.488317E-2 -1.004E-02 -1.027E-02  1.715E+11   3.771E-4  
  1 14 -3.212451E-1 -4.170278E-2 -1.220E-02 -1.168E-02  2.133E+11   4.530E-4  
  1 15 -3.212451E-1 -4.121385E-2 -1.138E-03 -1.113E-03  1.996E+10   4.219E-5  
  1 16 -3.212451E-1 -4.063208E-2 -1.935E-01 -1.755E-01  3.407E+12   7.158E-3  
  1 17 -3.212451E-1 -3.760452E-2 -1.488E-01 -1.349E-01  2.678E+12   5.446E-3  
  1 18 -3.212451E-1 -3.522922E-2 -1.075E-02 -1.194E-02  1.967E+11   3.902E-4  
  1 19 -3.212451E-1 -3.483027E-2 -9.202E-02 -9.137E-02  1.688E+12   3.335E-3  
 ..... 
  1 45 -3.212451E-1 -8.686647E-3 -2.118E-04 -2.123E-04  4.628E+09   7.034E-6  
  1 46 -3.212451E-1 -8.368791E-3 -1.125E-04 -1.082E-04  2.464E+09   3.733E-6  
  1 47 -3.212451E-1 -8.321573E-3 -1.418E-02 -1.271E-02  3.105E+11   4.704E-4  
  2  1 -1.253358E-1 -1.360506E-1  1.012E-01  9.828E-02  7.797E+09   9.804E-2  
  2  2 -1.253358E-1 -1.329843E-1  2.878E-02  2.541E-02  1.129E+09   3.906E-2  
  2  3 -1.253358E-1 -1.167997E-1 -9.562E-03 -7.884E-03  1.558E+08   1.163E-2  
  2  4 -1.253358E-1 -1.141704E-1 -2.041E-01 -2.001E-01  5.689E+09   1.898E-1    
 ..... 
 20 45 -8.486569E-3 -8.686647E-3  7.494E-05  5.519E-05  2.012E+03   3.822E-3 
 20 46 -8.486569E-3 -8.368791E-3 -4.901E+00 -4.929E+00  1.520E+07   4.319E+2 
 20 47 -8.486569E-3 -8.321573E-3 -3.850E-01 -3.826E-01  2.344E+06   2.422E+1 
    0    2    0         0    0    1    
   45   19    RE1          RE2     GFL  -  E1  -  GFV    A(E1)*S   
  1  1 -1.288567E-1 -1.332897E-1  2.198E-03  9.246E-04  9.659E+06  
  1  2 -1.288567E-1 -1.170725E-1 -1.226E-01 -1.213E-01  1.142E+10  
  1  3 -1.288567E-1 -9.365835E-2 -5.438E-02 -3.476E-02  4.520E+10  
 .....   
    0    0    0         0    0    0    
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\end{table}