--------------------------- 786 ------------------------------------------- Ref. "Relativistic fine structure oscillator strengths for Li-like ions: C IV - Si XII, S XIV, Ar XVI, Ca XVIII, Ti XX, Cr XXII, and Ni XXVI" Sultana N. Nahar, Astron. & Astrophys. 389, 716 (2002) -------------------------------------------------------------------------- Cr XXII : Fine structure levels The contents of the file: -------------------------- i) Target/Core info: Fine structure levels of the core/target included in the eigenfunction expansion of ion ii) Fine structure energy levels of the ion, with spectroscopic designation, ordered in energy and grouped as compoments of LS terms iii) Fine structure energy levels of the ion, with spectroscopic designation, ordered in J\pi and energy ----------------------------------------------------------------------- i) Target/Core info: Fine structure levels of the core/target included in the eigenfunction expansion of ion ------------------------------------------------------------ Z = 24, No. of core electrons = 2 Target levels: 17 Config SLp J E(Ry) 1 1s2 1Se 0 0.00000E+00 2 1s2s 3Se 1 4.13564E+02 3 1s2p 3Po 0 4.15493E+02 4 1s2p 3Po 1 4.15630E+02 5 1s2s 1Se 0 4.15669E+02 6 1s2p 3Po 2 4.16370E+02 7 1s2p 1Po 1 4.17607E+02 8 1s3s 3Se 1 4.89896E+02 9 1s3p 3Po 0 4.90429E+02 10 1s3s 1Se 0 4.90449E+02 11 1s3p 3Po 1 4.90463E+02 12 1s3p 3Po 2 4.90684E+02 13 1s3p 1Po 1 4.91024E+02 14 1s3d 3De 1 4.91631E+02 15 1s3d 3De 2 4.91638E+02 16 1s3d 3De 3 4.91727E+02 17 1s3d 1De 2 4.91739E+02 ------------------------------------------------------------------------ ii) Fine structure energy levels of the ion, with spectroscopic designation, ordered in energy and grouped as compoments of LS terms ------------------------------------------------------------------- Number of fine structure levels: J pi Nlv(c) 1 0 9 1 1 9 3 0 8 3 1 9 5 0 8 5 1 7 7 0 6 7 1 7 9 0 6 9 1 5 11 0 4 11 1 5 13 0 4 13 1 3 15 0 2 15 1 3 17 0 2 17 1 1 Total number of levels = 98 NOTE: Nlv=Number of levels expected Nlv(c)=Number of levels obtained Nlv=Nlv(c) -> set complete For Equivalent electron levels: (i) no EQN (effective qn) (ii) no check of set completeness Configuration J E(Ry) EQN LS terms Nlv= 1, 2Le: S ( 1 )/2 1s2 (1Se) 0 2s 1/2 -1.26565E+02 1.96 2 S e Nlv(c)= 1 : set complete Nlv= 2, 2Lo: P ( 3 1 )/2 1s2 (1Se) 0 2p 1/2 -1.23360E+02 1.98 2 P o 1s2 (1Se) 0 2p 3/2 -1.22422E+02 1.99 2 P o Nlv(c)= 2 : set complete Nlv= 1, 2Le: S ( 1 )/2 1s2 (1Se) 0 3s 1/2 -5.54020E+01 2.96 2 S e Nlv(c)= 1 : set complete Nlv= 2, 2Lo: P ( 3 1 )/2 1s2 (1Se) 0 3p 1/2 -5.45381E+01 2.98 2 P o 1s2 (1Se) 0 3p 3/2 -5.42612E+01 2.99 2 P o Nlv(c)= 2 : set complete Nlv= 2, 2Le: D ( 5 3 )/2 1s2 (1Se) 0 3d 3/2 -5.39292E+01 3.00 2 D e 1s2 (1Se) 0 3d 5/2 -5.38440E+01 3.00 2 D e Nlv(c)= 2 : set complete Nlv= 1, 2Le: S ( 1 )/2 1s2 (1Se) 0 4s 1/2 -3.14938E+01 3.92 2 S e Nlv(c)= 1 : set complete Nlv= 2, 2Lo: P ( 3 1 )/2 1s2 (1Se) 0 4p 1/2 -3.06592E+01 3.97 2 P o 1s2 (1Se) 0 4p 3/2 -3.05398E+01 3.98 2 P o Nlv(c)= 2 : set complete Nlv= 2, 2Le: D ( 5 3 )/2 1s2 (1Se) 0 4d 3/2 -3.03077E+01 4.00 2 D e 1s2 (1Se) 0 4d 5/2 -3.02716E+01 4.00 2 D e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: F ( 7 5 )/2 1s2 (1Se) 0 4f 5/2 -3.02660E+01 4.00 2 F o 1s2 (1Se) 0 4f 7/2 -3.02482E+01 4.00 2 F o Nlv(c)= 2 : set complete Nlv= 1, 2Le: S ( 1 )/2 1s2 (1Se) 0 5s 1/2 -1.99581E+01 4.92 2 S e Nlv(c)= 1 : set complete Nlv= 2, 2Lo: P ( 3 1 )/2 1s2 (1Se) 0 5p 1/2 -1.95540E+01 4.97 2 P o 1s2 (1Se) 0 5p 3/2 -1.94941E+01 4.98 2 P o Nlv(c)= 2 : set complete Nlv= 2, 2Le: D ( 5 3 )/2 1s2 (1Se) 0 5d 3/2 -1.93950E+01 4.99 2 D e 1s2 (1Se) 0 5d 5/2 -1.93765E+01 5.00 2 D e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: F ( 7 5 )/2 1s2 (1Se) 0 5f 5/2 -1.93733E+01 5.00 2 F o 1s2 (1Se) 0 5f 7/2 -1.93641E+01 5.00 2 F o Nlv(c)= 2 : set complete Nlv= 2, 2Le: G ( 9 7 )/2 1s2 (1Se) 0 5g 7/2 -1.93646E+01 5.00 2 G e 1s2 (1Se) 0 5g 9/2 -1.93592E+01 5.00 2 G e Nlv(c)= 2 : set complete Nlv= 1, 2Le: S ( 1 )/2 1s2 (1Se) 0 6s 1/2 -1.37766E+01 5.93 2 S e Nlv(c)= 1 : set complete Nlv= 2, 2Lo: P ( 3 1 )/2 1s2 (1Se) 0 6p 1/2 -1.35540E+01 5.98 2 P o 1s2 (1Se) 0 6p 3/2 -1.35196E+01 5.98 2 P o Nlv(c)= 2 : set complete Nlv= 2, 2Le: D ( 5 3 )/2 1s2 (1Se) 0 6d 3/2 -1.34668E+01 5.99 2 D e 1s2 (1Se) 0 6d 5/2 -1.34560E+01 6.00 2 D e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: F ( 7 5 )/2 1s2 (1Se) 0 6f 5/2 -1.34540E+01 6.00 2 F o 1s2 (1Se) 0 6f 7/2 -1.34488E+01 6.00 2 F o Nlv(c)= 2 : set complete Nlv= 2, 2Le: G ( 9 7 )/2 1s2 (1Se) 0 6g 7/2 -1.34491E+01 6.00 2 G e 1s2 (1Se) 0 6g 9/2 -1.34459E+01 6.00 2 G e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: H (11 9 )/2 1s2 (1Se) 0 6h 9/2 -1.34461E+01 6.00 2 H o 1s2 (1Se) 0 6h 11/2 -1.34440E+01 6.00 2 H o Nlv(c)= 2 : set complete Nlv= 1, 2Le: S ( 1 )/2 1s2 (1Se) 0 7s 1/2 -1.00818E+01 6.93 2 S e Nlv(c)= 1 : set complete Nlv= 2, 2Lo: P ( 3 1 )/2 1s2 (1Se) 0 7p 1/2 -9.94596E+00 6.98 2 P o 1s2 (1Se) 0 7p 3/2 -9.92437E+00 6.98 2 P o Nlv(c)= 2 : set complete Nlv= 2, 2Le: D ( 5 3 )/2 1s2 (1Se) 0 7d 3/2 -9.89252E+00 6.99 2 D e 1s2 (1Se) 0 7d 5/2 -9.88580E+00 7.00 2 D e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: F ( 7 5 )/2 1s2 (1Se) 0 7f 5/2 -9.88444E+00 7.00 2 F o 1s2 (1Se) 0 7f 7/2 -9.88110E+00 7.00 2 F o Nlv(c)= 2 : set complete Nlv= 2, 2Le: G ( 9 7 )/2 1s2 (1Se) 0 7g 7/2 -9.88130E+00 7.00 2 G e 1s2 (1Se) 0 7g 9/2 -9.87926E+00 7.00 2 G e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: H (11 9 )/2 1s2 (1Se) 0 7h 9/2 -9.87941E+00 7.00 2 H o 1s2 (1Se) 0 7h 11/2 -9.87810E+00 7.00 2 H o Nlv(c)= 2 : set complete Nlv= 2, 2Le: I (1311 )/2 1s2 (1Se) 0 7i 11/2 -9.87820E+00 7.00 2 I e 1s2 (1Se) 0 7i 13/2 -9.87723E+00 7.00 2 I e Nlv(c)= 2 : set complete Nlv= 1, 2Le: S ( 1 )/2 1s2 (1Se) 0 8s 1/2 -7.69758E+00 7.93 2 S e Nlv(c)= 1 : set complete Nlv= 2, 2Lo: P ( 3 1 )/2 1s2 (1Se) 0 8p 1/2 -7.60843E+00 7.98 2 P o 1s2 (1Se) 0 8p 3/2 -7.59401E+00 7.98 2 P o Nlv(c)= 2 : set complete Nlv= 2, 2Le: D ( 5 3 )/2 1s2 (1Se) 0 8d 3/2 -7.57324E+00 7.99 2 D e 1s2 (1Se) 0 8d 5/2 -7.56870E+00 8.00 2 D e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: F ( 7 5 )/2 1s2 (1Se) 0 8f 5/2 -7.56773E+00 8.00 2 F o 1s2 (1Se) 0 8f 7/2 -7.56550E+00 8.00 2 F o Nlv(c)= 2 : set complete Nlv= 2, 2Le: G ( 9 7 )/2 1s2 (1Se) 0 8g 7/2 -7.56555E+00 8.00 2 G e 1s2 (1Se) 0 8g 9/2 -7.56424E+00 8.00 2 G e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: H (11 9 )/2 1s2 (1Se) 0 8h 9/2 -7.56424E+00 8.00 2 H o 1s2 (1Se) 0 8h 11/2 -7.56337E+00 8.00 2 H o Nlv(c)= 2 : set complete Nlv= 2, 2Le: I (1311 )/2 1s2 (1Se) 0 8i 11/2 -7.56337E+00 8.00 2 I e 1s2 (1Se) 0 8i 13/2 -7.56274E+00 8.00 2 I e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: K (1513 )/2 1s2 (1Se) 0 8k 13/2 -7.56274E+00 8.00 2 K o 1s2 (1Se) 0 8k 15/2 -7.56226E+00 8.00 2 K o Nlv(c)= 2 : set complete Nlv= 1, 2Le: S ( 1 )/2 1s2 (1Se) 0 9s 1/2 -6.06941E+00 8.93 2 S e Nlv(c)= 1 : set complete Nlv= 2, 2Lo: P ( 3 1 )/2 1s2 (1Se) 0 9p 1/2 -6.00765E+00 8.98 2 P o 1s2 (1Se) 0 9p 3/2 -5.99758E+00 8.98 2 P o Nlv(c)= 2 : set complete Nlv= 2, 2Le: D ( 5 3 )/2 1s2 (1Se) 0 9d 3/2 -5.98326E+00 8.99 2 D e 1s2 (1Se) 0 9d 5/2 -5.98006E+00 9.00 2 D e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: F ( 7 5 )/2 1s2 (1Se) 0 9f 5/2 -5.97953E+00 9.00 2 F o 1s2 (1Se) 0 9f 7/2 -5.97793E+00 9.00 2 F o Nlv(c)= 2 : set complete Nlv= 2, 2Le: G ( 9 7 )/2 1s2 (1Se) 0 9g 7/2 -5.97803E+00 9.00 2 G e 1s2 (1Se) 0 9g 9/2 -5.97711E+00 9.00 2 G e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: H (11 9 )/2 1s2 (1Se) 0 9h 9/2 -5.97711E+00 9.00 2 H o 1s2 (1Se) 0 9h 11/2 -5.97653E+00 9.00 2 H o Nlv(c)= 2 : set complete Nlv= 2, 2Le: I (1311 )/2 1s2 (1Se) 0 9i 11/2 -5.97643E+00 9.00 2 I e 1s2 (1Se) 0 9i 13/2 -5.97600E+00 9.00 2 I e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: K (1513 )/2 1s2 (1Se) 0 9k 13/2 -5.97585E+00 9.00 2 K o 1s2 (1Se) 0 9k 15/2 -5.97556E+00 9.00 2 K o Nlv(c)= 2 : set complete Nlv= 2, 2Le: L (1715 )/2 1s2 (1Se) 0 9l 15/2 -5.97542E+00 9.00 2 L e 1s2 (1Se) 0 9l 17/2 -5.97517E+00 9.00 2 L e Nlv(c)= 2 : set complete Nlv= 1, 2Le: S ( 1 )/2 1s2 (1Se) 0 10s 1/2 -4.90820E+00 9.93 2 S e Nlv(c)= 1 : set complete Nlv= 2, 2Lo: P ( 3 1 )/2 1s2 (1Se) 0 10p 1/2 -4.86367E+00 9.98 2 P o 1s2 (1Se) 0 10p 3/2 -4.85631E+00 9.98 2 P o Nlv(c)= 2 : set complete Nlv= 2, 2Le: D ( 5 3 )/2 1s2 (1Se) 0 10d 3/2 -4.84600E+00 9.99 2 D e 1s2 (1Se) 0 10d 5/2 -4.84368E+00 10.00 2 D e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: F ( 7 5 )/2 1s2 (1Se) 0 10f 5/2 -4.84319E+00 10.00 2 F o 1s2 (1Se) 0 10f 7/2 -4.84208E+00 10.00 2 F o Nlv(c)= 2 : set complete Nlv= 2, 2Le: G ( 9 7 )/2 1s2 (1Se) 0 10g 7/2 -4.84208E+00 10.00 2 G e 1s2 (1Se) 0 10g 9/2 -4.84140E+00 10.00 2 G e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: H (11 9 )/2 1s2 (1Se) 0 10h 9/2 -4.84140E+00 10.00 2 H o 1s2 (1Se) 0 10h 11/2 -4.84097E+00 10.00 2 H o Nlv(c)= 2 : set complete Nlv= 2, 2Le: I (1311 )/2 1s2 (1Se) 0 10i 11/2 -4.84097E+00 10.00 2 I e 1s2 (1Se) 0 10i 13/2 -4.84063E+00 10.00 2 I e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: K (1513 )/2 1s2 (1Se) 0 10k 13/2 -4.84068E+00 10.00 2 K o 1s2 (1Se) 0 10k 15/2 -4.84048E+00 10.00 2 K o Nlv(c)= 2 : set complete Nlv= 2, 2Lo: M (1917 )/2 1s2 (1Se) 0 10m 17/2 -4.84048E+00 10.00 2 M o Nlv(c)= 1 , Nlv= 2 : set incomplete, level missing: 1/2( 19 Nlv= 2, 2Le: L (1715 )/2 1s2 (1Se) 0 10l 15/2 -4.84044E+00 10.00 2 L e 1s2 (1Se) 0 10l 17/2 -4.84029E+00 10.00 2 L e Nlv(c)= 2 : set complete Total number of levels processed= 98 ----------------------------------------------------------------------- iii) Fine structure energy levels of the ion, with spectroscopic designation, ordered in J\pi and energy --------------------------------------------------------- Table Explanation: T -> target (core) of the level Nlv=Number of levels nl = Principal and orbital quantum numbers of the outer electron EQN = Effective Quantum Number. ------------------------------------- Z = 24, No. of core electrons = 2 Target levels: 17 Config SLp J E(Ry) 1 1s2 1Se 0 0.00000E+00 2 1s2s 3Se 1 4.13564E+02 3 1s2p 3Po 0 4.15493E+02 4 1s2p 3Po 1 4.15630E+02 5 1s2s 1Se 0 4.15669E+02 6 1s2p 3Po 2 4.16370E+02 7 1s2p 1Po 1 4.17607E+02 8 1s3s 3Se 1 4.89896E+02 9 1s3p 3Po 0 4.90429E+02 10 1s3s 1Se 0 4.90449E+02 11 1s3p 3Po 1 4.90463E+02 12 1s3p 3Po 2 4.90684E+02 13 1s3p 1Po 1 4.91024E+02 14 1s3d 3De 1 4.91631E+02 15 1s3d 3De 2 4.91638E+02 16 1s3d 3De 3 4.91727E+02 17 1s3d 1De 2 4.91739E+02 i T(config SLpi Jt) nl J E(Ry) EQN Terms Nlv= 9 J pi = 1/2 e 1 1s2 1Se 0 2s 1/2 -1.26565E+02 1.96 2 S e 2 1s2 1Se 0 3s 1/2 -5.54020E+01 2.96 2 S e 3 1s2 1Se 0 4s 1/2 -3.14938E+01 3.92 2 S e 4 1s2 1Se 0 5s 1/2 -1.99581E+01 4.92 2 S e 5 1s2 1Se 0 6s 1/2 -1.37766E+01 5.93 2 S e 6 1s2 1Se 0 7s 1/2 -1.00818E+01 6.93 2 S e 7 1s2 1Se 0 8s 1/2 -7.69758E+00 7.93 2 S e 8 1s2 1Se 0 9s 1/2 -6.06941E+00 8.93 2 S e 9 1s2 1Se 0 10s 1/2 -4.90820E+00 9.93 2 S e Nlv= 9 J pi = 1/2 o 1 1s2 1Se 0 2p 1/2 -1.23360E+02 1.98 2 P o 2 1s2 1Se 0 3p 1/2 -5.45381E+01 2.98 2 P o 3 1s2 1Se 0 4p 1/2 -3.06592E+01 3.97 2 P o 4 1s2 1Se 0 5p 1/2 -1.95540E+01 4.97 2 P o 5 1s2 1Se 0 6p 1/2 -1.35540E+01 5.98 2 P o 6 1s2 1Se 0 7p 1/2 -9.94596E+00 6.98 2 P o 7 1s2 1Se 0 8p 1/2 -7.60843E+00 7.98 2 P o 8 1s2 1Se 0 9p 1/2 -6.00765E+00 8.98 2 P o 9 1s2 1Se 0 10p 1/2 -4.86367E+00 9.98 2 P o Nlv= 8 J pi = 3/2 e 1 1s2 1Se 0 3d 3/2 -5.39292E+01 3.00 2 D e 2 1s2 1Se 0 4d 3/2 -3.03077E+01 4.00 2 D e 3 1s2 1Se 0 5d 3/2 -1.93950E+01 4.99 2 D e 4 1s2 1Se 0 6d 3/2 -1.34668E+01 5.99 2 D e 5 1s2 1Se 0 7d 3/2 -9.89252E+00 6.99 2 D e 6 1s2 1Se 0 8d 3/2 -7.57324E+00 7.99 2 D e 7 1s2 1Se 0 9d 3/2 -5.98326E+00 8.99 2 D e 8 1s2 1Se 0 10d 3/2 -4.84600E+00 9.99 2 D e Nlv= 9 J pi = 3/2 o 1 1s2 1Se 0 2p 3/2 -1.22422E+02 1.99 2 P o 2 1s2 1Se 0 3p 3/2 -5.42612E+01 2.99 2 P o 3 1s2 1Se 0 4p 3/2 -3.05398E+01 3.98 2 P o 4 1s2 1Se 0 5p 3/2 -1.94941E+01 4.98 2 P o 5 1s2 1Se 0 6p 3/2 -1.35196E+01 5.98 2 P o 6 1s2 1Se 0 7p 3/2 -9.92437E+00 6.98 2 P o 7 1s2 1Se 0 8p 3/2 -7.59401E+00 7.98 2 P o 8 1s2 1Se 0 9p 3/2 -5.99758E+00 8.98 2 P o 9 1s2 1Se 0 10p 3/2 -4.85631E+00 9.98 2 P o Nlv= 8 J pi = 5/2 e 1 1s2 1Se 0 3d 5/2 -5.38440E+01 3.00 2 D e 2 1s2 1Se 0 4d 5/2 -3.02716E+01 4.00 2 D e 3 1s2 1Se 0 5d 5/2 -1.93765E+01 5.00 2 D e 4 1s2 1Se 0 6d 5/2 -1.34560E+01 6.00 2 D e 5 1s2 1Se 0 7d 5/2 -9.88580E+00 7.00 2 D e 6 1s2 1Se 0 8d 5/2 -7.56870E+00 8.00 2 D e 7 1s2 1Se 0 9d 5/2 -5.98006E+00 9.00 2 D e 8 1s2 1Se 0 10d 5/2 -4.84368E+00 10.00 2 D e Nlv= 7 J pi = 5/2 o 1 1s2 1Se 0 4f 5/2 -3.02660E+01 4.00 2 F o 2 1s2 1Se 0 5f 5/2 -1.93733E+01 5.00 2 F o 3 1s2 1Se 0 6f 5/2 -1.34540E+01 6.00 2 F o 4 1s2 1Se 0 7f 5/2 -9.88444E+00 7.00 2 F o 5 1s2 1Se 0 8f 5/2 -7.56773E+00 8.00 2 F o 6 1s2 1Se 0 9f 5/2 -5.97953E+00 9.00 2 F o 7 1s2 1Se 0 10f 5/2 -4.84319E+00 10.00 2 F o Nlv= 6 J pi = 7/2 e 1 1s2 1Se 0 5g 7/2 -1.93646E+01 5.00 2 G e 2 1s2 1Se 0 6g 7/2 -1.34491E+01 6.00 2 G e 3 1s2 1Se 0 7g 7/2 -9.88130E+00 7.00 2 G e 4 1s2 1Se 0 8g 7/2 -7.56555E+00 8.00 2 G e 5 1s2 1Se 0 9g 7/2 -5.97803E+00 9.00 2 G e 6 1s2 1Se 0 10g 7/2 -4.84208E+00 10.00 2 G e Nlv= 7 J pi = 7/2 o 1 1s2 1Se 0 4f 7/2 -3.02482E+01 4.00 2 F o 2 1s2 1Se 0 5f 7/2 -1.93641E+01 5.00 2 F o 3 1s2 1Se 0 6f 7/2 -1.34488E+01 6.00 2 F o 4 1s2 1Se 0 7f 7/2 -9.88110E+00 7.00 2 F o 5 1s2 1Se 0 8f 7/2 -7.56550E+00 8.00 2 F o 6 1s2 1Se 0 9f 7/2 -5.97793E+00 9.00 2 F o 7 1s2 1Se 0 10f 7/2 -4.84208E+00 10.00 2 F o Nlv= 6 J pi = 9/2 e 1 1s2 1Se 0 5g 9/2 -1.93592E+01 5.00 2 G e 2 1s2 1Se 0 6g 9/2 -1.34459E+01 6.00 2 G e 3 1s2 1Se 0 7g 9/2 -9.87926E+00 7.00 2 G e 4 1s2 1Se 0 8g 9/2 -7.56424E+00 8.00 2 G e 5 1s2 1Se 0 9g 9/2 -5.97711E+00 9.00 2 G e 6 1s2 1Se 0 10g 9/2 -4.84140E+00 10.00 2 G e Nlv= 5 J pi = 9/2 o 1 1s2 1Se 0 6h 9/2 -1.34461E+01 6.00 2 H o 2 1s2 1Se 0 7h 9/2 -9.87941E+00 7.00 2 H o 3 1s2 1Se 0 8h 9/2 -7.56424E+00 8.00 2 H o 4 1s2 1Se 0 9h 9/2 -5.97711E+00 9.00 2 H o 5 1s2 1Se 0 10h 9/2 -4.84140E+00 10.00 2 H o Nlv= 4 J pi = 11/2 e 1 1s2 1Se 0 7i 11/2 -9.87820E+00 7.00 2 I e 2 1s2 1Se 0 8i 11/2 -7.56337E+00 8.00 2 I e 3 1s2 1Se 0 9i 11/2 -5.97643E+00 9.00 2 I e 4 1s2 1Se 0 10i 11/2 -4.84097E+00 10.00 2 I e Nlv= 5 J pi = 11/2 o 1 1s2 1Se 0 6h 11/2 -1.34440E+01 6.00 2 H o 2 1s2 1Se 0 7h 11/2 -9.87810E+00 7.00 2 H o 3 1s2 1Se 0 8h 11/2 -7.56337E+00 8.00 2 H o 4 1s2 1Se 0 9h 11/2 -5.97653E+00 9.00 2 H o 5 1s2 1Se 0 10h 11/2 -4.84097E+00 10.00 2 H o Nlv= 4 J pi = 13/2 e 1 1s2 1Se 0 7i 13/2 -9.87723E+00 7.00 2 I e 2 1s2 1Se 0 8i 13/2 -7.56274E+00 8.00 2 I e 3 1s2 1Se 0 9i 13/2 -5.97600E+00 9.00 2 I e 4 1s2 1Se 0 10i 13/2 -4.84063E+00 10.00 2 I e Nlv= 3 J pi = 13/2 o 1 1s2 1Se 0 8k 13/2 -7.56274E+00 8.00 2 K o 2 1s2 1Se 0 9k 13/2 -5.97585E+00 9.00 2 K o 3 1s2 1Se 0 10k 13/2 -4.84068E+00 10.00 2 K o Nlv= 2 J pi = 15/2 e 1 1s2 1Se 0 9l 15/2 -5.97542E+00 9.00 2 L e 2 1s2 1Se 0 10l 15/2 -4.84044E+00 10.00 2 L e Nlv= 3 J pi = 15/2 o 1 1s2 1Se 0 8k 15/2 -7.56226E+00 8.00 2 K o 2 1s2 1Se 0 9k 15/2 -5.97556E+00 9.00 2 K o 3 1s2 1Se 0 10k 15/2 -4.84048E+00 10.00 2 K o Nlv= 2 J pi = 17/2 e 1 1s2 1Se 0 9l 17/2 -5.97517E+00 9.00 2 L e 2 1s2 1Se 0 10l 17/2 -4.84029E+00 10.00 2 L e Nlv= 1 J pi = 17/2 o 1 1s2 1Se 0 10m 17/2 -4.84048E+00 10.00 2 M o Nlv(cal) = 98