Table 2a: Sample table of fine structure energy levels of Fe  XVII as sets of LS term components; $C_{\rm t}$ is the core configuration, $\nu $ is the effective quantum number.

$C_{\rm t}(S_{\rm t}L_{\rm t}\pi_{\rm t})$		 $J_{\rm t}$nl J E/Ry $\nu $ $SL\pi$
Eqv electron/unidentified levels, parity: e
2s22p6     0 -92.8398   1  S e

Nlv(c) =  1: set complete
Nlv =  3,   $^3\!L^{\rm o}$: P ( 2 1 0 )

2s22p5		(2Po)3/2 3s 2 -39.4577 2.71 3  P o
2s22p5(2Po)3/2 3s 1 -39.3187 2.71 3  P o
2s22p5(2Po)1/2 3s 0 -38.5208 2.71 3  P o

Nlv(c) =  3: set complete
Nlv =  1,   $^1\!L^{\rm o}$: P ( 1 )

2s22p5		(2Po)1/2 3s 1 -38.4324 2.71 1  P o

Nlv(c) =  1: set complete
Nlv =  7,   $^3\!L^{{\rm e}}$: S ( 1 ) P ( 2 1 0 ) D ( 3 2 1 )

2s22p5		(2Po)3/2 3p 1 -37.2397 2.79 3  SPD e
2s22p5(2Po)1/2 3p 2 -36.9744 2.80 3  PD e
2s22p5(2Po)3/2 3p 3 -36.8541 2.80 3  D e
2s22p5(2Po)3/2 3p 2 -36.6391 2.81 3  PD e
2s22p5(2Po)1/2 3p 0 -36.2221 2.82 3  P e
2s22p5(2Po)1/2 3p 1 -36.0724 2.79 3  SPD e
2s22p5(2Po)3/2 3p 1 -35.8374 2.80 3  SPD e

Nlv(c) =  7: set complete
Nlv =  3,   $^1\!L^{{\rm e}}$: S ( 0 ) P ( 1 ) D ( 2 )

2s22p5		(2Po)3/2 3p 1 -36.7729 2.80 1  P e
2s22p5(2Po)3/2 3p 2 -35.8059 2.80 1  D e
2s22p5(2Po)1/2 3p 0 -34.8040 2.84 1  S e

Nlv(c) =  3: set complete


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