Table 3b: Sample table for calculated fine structure energy levels of Fe XX in $J\pi $ energy order. Nlv is the total number of levels of the symmetry.
  Level E (Ry) $\nu $ $SL\pi$

Nlv=127,     $J\pi=1/2$ e

1		 $\rm 2s2p4 $   1/2 -1.08024E+02   $\rm ^4P e $
2 $\rm 2s2p4 $   1/2 -1.04752E+02   $\rm ^2S e $
3 $\rm 2s2p4 $   1/2 -1.03421E+02   $\rm ^2P e $
4 $\rm 2s22p2 (^3P^e_0)$ $\rm 3s$ 1/2 -5.04616E+01 2.80 $\rm ^4P e $
5 $\rm 2s22p2 (^3P^e_0)$ $\rm 3s$ 1/2 -4.95776E+01 2.84 $\rm ^2P e $
6 $\rm 2s22p2 (^1S^e_0)$ $\rm 3s$ 1/2 -4.69768E+01 2.82 $\rm ^2S e $
7 $\rm 2s22p2 (^3P^e_0)$ $\rm 3d$ 1/2 -4.53140E+01 2.95 $\rm ^4PD e $
8 $\rm 2s22p2 (^3P^e_0)$ $\rm 3d$ 1/2 -4.45636E+01 2.96 $\rm ^4PD e $
9 $\rm 2s22p2 (^3P^e_0)$ $\rm 3d$ 1/2 -4.44980E+01 2.96 $\rm ^2P e $
10 $\rm 2s22p2 (^1D^e_0)$ $\rm 3d$ 1/2 -4.33144E+01 2.96 $\rm ^2SP e $
11 $\rm 2s2p3 (^5S^o_0)$ $\rm 3p$ 1/2 -4.31856E+01 2.90 $\rm ^4P e $
12 $\rm 2s22p2 (^1D^e_0)$ $\rm 3d$ 1/2 -4.30172E+01 2.97 $\rm ^2SP e $
13 $\rm 2s2p3 (^3D^o_0)$ $\rm 3p$ 1/2 -4.14220E+01 2.87 $\rm ^4PD e $
14 $\rm 2s2p3 (^3D^o_0)$ $\rm 3p$ 1/2 -4.08576E+01 2.89 $\rm ^4PD e $
15 $\rm 2s2p3 (^3D^o_0)$ $\rm 3p$ 1/2 -4.04084E+01 2.90 $\rm ^2P e $
16 $\rm 2s2p3 (^3P^o_0)$ $\rm 3p$ 1/2 -3.99518E+01 2.88 $\rm ^4PD e $
17 $\rm 2s2p3 (^3P^o_0)$ $\rm 3p$ 1/2 -3.95238E+01 2.89 $\rm ^2SP e $
18 $\rm 2s2p3 (^3P^o_0)$ $\rm 3p$ 1/2 -3.94558E+01 2.89 $\rm ^4PD e $
19 $\rm 2s2p3 (^3P^o_0)$ $\rm 3p$ 1/2 -3.86848E+01 2.91 $\rm ^2SP e $
20 $\rm 2s2p3 (^3S^o_0)$ $\rm 3p$ 1/2 -3.83062E+01 2.89 $\rm ^4P e $


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