--------------------------- 786 ------------------------------------------- Ref. "A comprehensive set of UV and X-Ray Radiative Transition Rates for Fe~XVI", S.N. Nahar, W. Eissner, C. Sur, A.K. Pradhan, Phys. Scr. 79, 035401 (2009) -------------------------------------------------------------------------- Fe XVI : 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 - (Table 3 in the paper) iii) Fine structure energy levels of the ion, with spectroscopic designation, ordered in J\pi and energy - (Table 4 in the paper) --------------------------------------------------------------------------- i) Target/Core info: Fine structure levels of the core/target included in the eigenfunction expansion of ion --------------------------------------------------------------- Z = 26, No. of core electrons = 10 Target levels: 1 Config SLp J E(Ry) 1 2s22p6 1Se 0 0.00000E+00 ------------------------------------------------------------------- ii) Fine structure energy levels of the ion, with spectroscopic designation, ordered in energy and grouped as compoments of LS terms - (Table 3 in the paper) ----------------------------------------------------------------------- Number of fine structure levels: J pi Nlv(c) 1 0 8 1 1 8 3 0 8 3 1 8 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 19 0 0 19 1 1 21 0 0 21 1 0 Total number of levels = 96 NOTE: Nlv=Number of levels expected Nlv(c)=Number of levels obtained Nlv=Nlv(c) -> set complete For Equivalent electron levels: no EQN (effective qn) Configuration J E(Ry) EQN LS terms Nlv= 1, 2Le: S ( 1 )/2 2s22p6 (1Se) 0 3s 1/2 -3.59570E+01 2.67 2 S e Nlv(c)= 1 : set complete Nlv= 2, 2Lo: P ( 3 1 )/2 2s22p6 (1Se) 0 3p 1/2 -3.34269E+01 2.77 2 P o 2s22p6 (1Se) 0 3p 3/2 -3.32342E+01 2.78 2 P o Nlv(c)= 2 : set complete Nlv= 2, 2Le: D ( 5 3 )/2 2s22p6 (1Se) 0 3d 3/2 -2.97853E+01 2.93 2 D e 2s22p6 (1Se) 0 3d 5/2 -2.97436E+01 2.93 2 D e Nlv(c)= 2 : set complete Nlv= 1, 2Le: S ( 1 )/2 2s22p6 (1Se) 0 4s 1/2 -1.89363E+01 3.68 2 S e Nlv(c)= 1 : set complete Nlv= 2, 2Lo: P ( 3 1 )/2 2s22p6 (1Se) 0 4p 1/2 -1.79324E+01 3.78 2 P o 2s22p6 (1Se) 0 4p 3/2 -1.78566E+01 3.79 2 P o Nlv(c)= 2 : set complete Nlv= 2, 2Le: D ( 5 3 )/2 2s22p6 (1Se) 0 4d 3/2 -1.65879E+01 3.93 2 D e 2s22p6 (1Se) 0 4d 5/2 -1.65695E+01 3.93 2 D e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: F ( 7 5 )/2 2s22p6 (1Se) 0 4f 5/2 -1.60544E+01 3.99 2 F o 2s22p6 (1Se) 0 4f 7/2 -1.60472E+01 3.99 2 F o Nlv(c)= 2 : set complete Nlv= 1, 2Le: S ( 1 )/2 2s22p6 (1Se) 0 5s 1/2 -1.16932E+01 4.68 2 S e Nlv(c)= 1 : set complete Nlv= 2, 2Lo: P ( 3 1 )/2 2s22p6 (1Se) 0 5p 1/2 -1.11997E+01 4.78 2 P o 2s22p6 (1Se) 0 5p 3/2 -1.11648E+01 4.79 2 P o Nlv(c)= 2 : set complete Nlv= 2, 2Le: D ( 5 3 )/2 2s22p6 (1Se) 0 5d 3/2 -1.05538E+01 4.93 2 D e 2s22p6 (1Se) 0 5d 5/2 -1.05448E+01 4.93 2 D e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: F ( 7 5 )/2 2s22p6 (1Se) 0 5f 5/2 -1.02754E+01 4.99 2 F o 2s22p6 (1Se) 0 5f 7/2 -1.02719E+01 4.99 2 F o Nlv(c)= 2 : set complete Nlv= 2, 2Le: G ( 9 7 )/2 2s22p6 (1Se) 0 5g 7/2 -1.02428E+01 5.00 2 G e 2s22p6 (1Se) 0 5g 9/2 -1.02407E+01 5.00 2 G e Nlv(c)= 2 : set complete Nlv= 1, 2Le: S ( 1 )/2 2s22p6 (1Se) 0 6s 1/2 -7.92865E+00 5.68 2 S e Nlv(c)= 1 : set complete Nlv= 2, 2Lo: P ( 3 1 )/2 2s22p6 (1Se) 0 6p 1/2 -7.64675E+00 5.79 2 P o 2s22p6 (1Se) 0 6p 3/2 -7.62529E+00 5.79 2 P o Nlv(c)= 2 : set complete Nlv= 2, 2Le: D ( 5 3 )/2 2s22p6 (1Se) 0 6d 3/2 -7.28069E+00 5.93 2 D e 2s22p6 (1Se) 0 6d 5/2 -7.27514E+00 5.93 2 D e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: F ( 7 5 )/2 2s22p6 (1Se) 0 6f 5/2 -7.12755E+00 5.99 2 F o 2s22p6 (1Se) 0 6f 7/2 -7.12545E+00 5.99 2 F o Nlv(c)= 2 : set complete Nlv= 2, 2Le: G ( 9 7 )/2 2s22p6 (1Se) 0 6g 7/2 -7.11393E+00 6.00 2 G e 2s22p6 (1Se) 0 6g 9/2 -7.11281E+00 6.00 2 G e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: H (11 9 )/2 2s22p6 (1Se) 0 6h 9/2 -7.11171E+00 6.00 2 H o 2s22p6 (1Se) 0 6h 11/2 -7.11096E+00 6.00 2 H o Nlv(c)= 2 : set complete Nlv= 1, 2Le: S ( 1 )/2 2s22p6 (1Se) 0 7s 1/2 -5.73268E+00 6.68 2 S e Nlv(c)= 1 : set complete Nlv= 2, 2Lo: P ( 3 1 )/2 2s22p6 (1Se) 0 7p 1/2 -5.55871E+00 6.79 2 P o 2s22p6 (1Se) 0 7p 3/2 -5.54563E+00 6.79 2 P o Nlv(c)= 2 : set complete Nlv= 2, 2Le: D ( 5 3 )/2 2s22p6 (1Se) 0 7d 3/2 -5.33325E+00 6.93 2 D e 2s22p6 (1Se) 0 7d 5/2 -5.32979E+00 6.93 2 D e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: F ( 7 5 )/2 2s22p6 (1Se) 0 7f 5/2 -5.23727E+00 6.99 2 F o 2s22p6 (1Se) 0 7f 7/2 -5.23597E+00 6.99 2 F o Nlv(c)= 2 : set complete Nlv= 2, 2Le: G ( 9 7 )/2 2s22p6 (1Se) 0 7g 7/2 -5.22655E+00 7.00 2 G e 2s22p6 (1Se) 0 7g 9/2 -5.22583E+00 7.00 2 G e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: H (11 9 )/2 2s22p6 (1Se) 0 7h 9/2 -5.22532E+00 7.00 2 H o 2s22p6 (1Se) 0 7h 11/2 -5.22488E+00 7.00 2 H o Nlv(c)= 2 : set complete Nlv= 2, 2Le: I (1311 )/2 2s22p6 (1Se) 0 7i 11/2 -5.22483E+00 7.00 2 I e 2s22p6 (1Se) 0 7i 13/2 -5.22460E+00 7.00 2 I e Nlv(c)= 2 : set complete Nlv= 1, 2Le: S ( 1 )/2 2s22p6 (1Se) 0 8s 1/2 -4.33725E+00 7.68 2 S e Nlv(c)= 1 : set complete Nlv= 2, 2Lo: P ( 3 1 )/2 2s22p6 (1Se) 0 8p 1/2 -4.22249E+00 7.79 2 P o 2s22p6 (1Se) 0 8p 3/2 -4.21396E+00 7.79 2 P o Nlv(c)= 2 : set complete Nlv= 2, 2Le: D ( 5 3 )/2 2s22p6 (1Se) 0 8d 3/2 -4.07386E+00 7.93 2 D e 2s22p6 (1Se) 0 8d 5/2 -4.07158E+00 7.93 2 D e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: F ( 7 5 )/2 2s22p6 (1Se) 0 8f 5/2 -4.00965E+00 7.99 2 F o 2s22p6 (1Se) 0 8f 7/2 -4.00876E+00 7.99 2 F o Nlv(c)= 2 : set complete Nlv= 2, 2Le: G ( 9 7 )/2 2s22p6 (1Se) 0 8g 7/2 -4.00156E+00 8.00 2 G e 2s22p6 (1Se) 0 8g 9/2 -4.00108E+00 8.00 2 G e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: H (11 9 )/2 2s22p6 (1Se) 0 8h 9/2 -4.00069E+00 8.00 2 H o 2s22p6 (1Se) 0 8h 11/2 -4.00041E+00 8.00 2 H o Nlv(c)= 2 : set complete Nlv= 2, 2Le: I (1311 )/2 2s22p6 (1Se) 0 8i 11/2 -4.00033E+00 8.00 2 I e 2s22p6 (1Se) 0 8i 13/2 -4.00013E+00 8.00 2 I e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: K (1513 )/2 2s22p6 (1Se) 0 8k 13/2 -4.00010E+00 8.00 2 K o 2s22p6 (1Se) 0 8k 15/2 -4.00008E+00 8.00 2 K o Nlv(c)= 2 : set complete Nlv= 1, 2Le: S ( 1 )/2 2s22p6 (1Se) 0 9s 1/2 -3.39566E+00 8.68 2 S e Nlv(c)= 1 : set complete Nlv= 2, 2Lo: P ( 3 1 )/2 2s22p6 (1Se) 0 9p 1/2 -3.31599E+00 8.79 2 P o 2s22p6 (1Se) 0 9p 3/2 -3.31016E+00 8.79 2 P o Nlv(c)= 2 : set complete Nlv= 2, 2Le: D ( 5 3 )/2 2s22p6 (1Se) 0 9d 3/2 -3.21283E+00 8.93 2 D e 2s22p6 (1Se) 0 9d 5/2 -3.21126E+00 8.93 2 D e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: F ( 7 5 )/2 2s22p6 (1Se) 0 9f 5/2 -3.16774E+00 8.99 2 F o 2s22p6 (1Se) 0 9f 7/2 -3.16713E+00 8.99 2 F o Nlv(c)= 2 : set complete Nlv= 2, 2Le: G ( 9 7 )/2 2s22p6 (1Se) 0 9g 7/2 -3.16168E+00 9.00 2 G e 2s22p6 (1Se) 0 9g 9/2 -3.16134E+00 9.00 2 G e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: H (11 9 )/2 2s22p6 (1Se) 0 9h 9/2 -3.16101E+00 9.00 2 H o 2s22p6 (1Se) 0 9h 11/2 -3.16081E+00 9.00 2 H o Nlv(c)= 2 : set complete Nlv= 2, 2Le: I (1311 )/2 2s22p6 (1Se) 0 9i 11/2 -3.16078E+00 9.00 2 I e 2s22p6 (1Se) 0 9i 13/2 -3.16063E+00 9.00 2 I e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: K (1513 )/2 2s22p6 (1Se) 0 9k 13/2 -3.16063E+00 9.00 2 K o 2s22p6 (1Se) 0 9k 15/2 -3.16058E+00 9.00 2 K o Nlv(c)= 2 : set complete Nlv= 2, 2Le: L (1715 )/2 2s22p6 (1Se) 0 9l 15/2 -3.16052E+00 9.00 2 L e 2s22p6 (1Se) 0 9l 17/2 -3.16050E+00 9.00 2 L e Nlv(c)= 2 : set complete Nlv= 1, 2Le: S ( 1 )/2 2s22p6 (1Se) 0 10s 1/2 -2.73047E+00 9.68 2 S e Nlv(c)= 1 : set complete Nlv= 2, 2Lo: P ( 3 1 )/2 2s22p6 (1Se) 0 10p 1/2 -2.67295E+00 9.79 2 P o 2s22p6 (1Se) 0 10p 3/2 -2.66875E+00 9.79 2 P o Nlv(c)= 2 : set complete Nlv= 2, 2Le: D ( 5 3 )/2 2s22p6 (1Se) 0 10d 3/2 -2.59837E+00 9.93 2 D e 2s22p6 (1Se) 0 10d 5/2 -2.59725E+00 9.93 2 D e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: F ( 7 5 )/2 2s22p6 (1Se) 0 10f 5/2 -2.56550E+00 9.99 2 F o 2s22p6 (1Se) 0 10f 7/2 -2.56507E+00 9.99 2 F o Nlv(c)= 2 : set complete Nlv= 2, 2Le: G ( 9 7 )/2 2s22p6 (1Se) 0 10g 7/2 -2.56090E+00 10.00 2 G e 2s22p6 (1Se) 0 10g 9/2 -2.56067E+00 10.00 2 G e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: H (11 9 )/2 2s22p6 (1Se) 0 10h 9/2 -2.56038E+00 10.00 2 H o 2s22p6 (1Se) 0 10h 11/2 -2.56023E+00 10.00 2 H o Nlv(c)= 2 : set complete Nlv= 2, 2Le: I (1311 )/2 2s22p6 (1Se) 0 10i 11/2 -2.56023E+00 10.00 2 I e 2s22p6 (1Se) 0 10i 13/2 -2.56013E+00 10.00 2 I e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: K (1513 )/2 2s22p6 (1Se) 0 10k 13/2 -2.56013E+00 10.00 2 K o 2s22p6 (1Se) 0 10k 15/2 -2.56008E+00 10.00 2 K o Nlv(c)= 2 : set complete Nlv= 2, 2Le: L (1715 )/2 2s22p6 (1Se) 0 10l 15/2 -2.56003E+00 10.00 2 L e 2s22p6 (1Se) 0 10l 17/2 -2.56003E+00 10.00 2 L e Nlv(c)= 2 : set complete Nlv= 2, 2Lo: M (1917 )/2 2s22p6 (1Se) 0 10m 17/2 -2.56000E+00 10.00 2 M o 2s22p6 (1Se) 0 10m 19/2 -2.56000E+00 10.00 2 M o Nlv(c)= 2 : set complete Total number of levels processed= 96 ------------------------------------------------------------------------ iii) Fine structure energy levels of the ion, with spectroscopic designation, ordered in J\pi and energy - (Table 4 in the paper) ------------------------------------------------------------------- Table Explanation: Energy levels with ids: jjpiiii jj= 2 x total angular momentum j, p=parity (0=even, 1=odd), iii=level position Note: There may be more than one possible LS term for some j-levels. Assumption made: higher L -> lower energy ----------------------------------------------------------------- nz = 26 , No. of core electrons= 10 96 = number of energies (Ecalc are replaced by available' Eobs) i j p iiii E(Ry) conf LS term jjpiiii 1 0.5 e 1 -3.59611E+01 2p63s 2Se 100001 2 0.5 e 2 -1.89410E+01 2p64s 2Se 100002 3 0.5 e 3 -1.17032E+01 2p65s 2Se 100003 4 0.5 e 4 -7.93052E+00 2p66s 2Se 100004 5 0.5 e 5 -5.67969E+00 2p67s 2Se 100005 6 0.5 e 6 -4.33725E+00 2s22p6 1Se 8s 2 S e 100006 7 0.5 e 7 -3.39566E+00 2s22p6 1Se 9s 2 S e 100007 8 0.5 e 8 -2.73047E+00 2s22p6 1Se10s 2 S e 100008 9 0.5 o 1 -3.34351E+01 2p63p 2Po 110001 10 0.5 o 2 -1.79394E+01 2p64p 2Po 110002 11 0.5 o 3 -1.12004E+01 2p65p 2Po 110003 12 0.5 o 4 -7.65350E+00 2p66p 2Po 110004 13 0.5 o 5 -5.55871E+00 2s22p6 1Se 7p 2 P o 110005 14 0.5 o 6 -4.22249E+00 2s22p6 1Se 8p 2 P o 110006 15 0.5 o 7 -3.31599E+00 2s22p6 1Se 9p 2 P o 110007 16 0.5 o 8 -2.67295E+00 2s22p6 1Se10p 2 P o 110008 17 1.5 e 1 -2.98055E+01 2p63d 2De 300001 18 1.5 e 2 -1.65992E+01 2p64d 2De 300002 19 1.5 e 3 -1.05545E+01 2p65d 2De 300003 20 1.5 e 4 -7.29200E+00 2p66d 2De 300004 21 1.5 e 5 -5.33797E+00 2p67d 2De 300005 22 1.5 e 6 -4.07768E+00 2p68d 2De 300006 23 1.5 e 7 -3.16460E+00 2p69d 2De 300007 24 1.5 e 8 -2.59837E+00 2s22p6 1Se10d 2 D e 300008 25 1.5 o 1 -3.32442E+01 2p63p 2Po 310001 26 1.5 o 2 -1.78665E+01 2p64p 2Po 310002 27 1.5 o 3 -1.11641E+01 2p65p 2Po 310003 28 1.5 o 4 -7.63071E+00 2p66p 2Po 310004 29 1.5 o 5 -5.51567E+00 2p67p 2Po 310005 30 1.5 o 6 -4.17610E+00 2p68p 2Po 310006 31 1.5 o 7 -3.27395E+00 2p69p 2Po 310007 32 1.5 o 8 -2.66875E+00 2s22p6 1Se10p 2 P o 310008 33 2.5 e 1 -2.97790E+01 2p63d 2De 500001 34 2.5 e 2 -1.65879E+01 2p64d 2De 500002 35 2.5 e 3 -1.05494E+01 2p65d 2De 500003 36 2.5 e 4 -7.28653E+00 2p66d 2De 500004 37 2.5 e 5 -5.33523E+00 2p67d 2De 500005 38 2.5 e 6 -4.07586E+00 2p68d 2De 500006 39 2.5 e 7 -3.20105E+00 2p69d 2De 500007 40 2.5 e 8 -2.59725E+00 2s22p6 1Se10d 2 D e 500008 41 2.5 o 1 -1.60503E+01 2p64f 2Fo 510001 42 2.5 o 2 -1.02761E+01 2p65f 2Fo 510002 43 2.5 o 3 -7.13654E+00 2p66f 2Fo 510003 44 2.5 o 4 -5.24037E+00 2p67f 2Fo 510004 45 2.5 o 5 -4.01481E+00 2p68f 2Fo 510005 46 2.5 o 6 -3.15548E+00 2p69f 2Fo 510006 47 2.5 o 7 -2.56550E+00 2s22p6 1Se10f 2 F o 510007 48 3.5 e 1 -1.02388E+01 2p65g 2Ge 700001 49 3.5 e 2 -7.11393E+00 2s22p6 1Se 6g 2 G e 700002 50 3.5 e 3 -5.22655E+00 2s22p6 1Se 7g 2 G e 700003 51 3.5 e 4 -4.00156E+00 2s22p6 1Se 8g 2 G e 700004 52 3.5 e 5 -3.16168E+00 2s22p6 1Se 9g 2 G e 700005 53 3.5 e 6 -2.56090E+00 2s22p6 1Se10g 2 G e 700006 54 3.5 o 1 -1.60462E+01 2p64f 2Fo 710001 55 3.5 o 2 -1.02734E+01 2p65f 2Fo 710002 56 3.5 o 3 -7.13599E+00 2p66f 2Fo 710003 57 3.5 o 4 -5.24165E+00 2p67f 2Fo 710004 58 3.5 o 5 -4.01390E+00 2p68f 2Fo 710005 59 3.5 o 6 -3.15548E+00 2p69f 2Fo 710006 60 3.5 o 7 -2.56507E+00 2s22p6 1Se10f 2 F o 710007 61 4.5 e 1 -1.02379E+01 2p65g 2Ge 900001 62 4.5 e 2 -7.11281E+00 2s22p6 1Se 6g 2 G e 900002 63 4.5 e 3 -5.22583E+00 2s22p6 1Se 7g 2 G e 900003 64 4.5 e 4 -4.00108E+00 2s22p6 1Se 8g 2 G e 900004 65 4.5 e 5 -3.16134E+00 2s22p6 1Se 9g 2 G e 900005 66 4.5 e 6 -2.56067E+00 2s22p6 1Se10g 2 G e 900006 67 4.5 o 1 -7.11171E+00 2s22p6 1Se 6h 2 H o 910001 68 4.5 o 2 -5.22532E+00 2s22p6 1Se 7h 2 H o 910002 69 4.5 o 3 -4.00069E+00 2s22p6 1Se 8h 2 H o 910003 70 4.5 o 4 -3.16101E+00 2s22p6 1Se 9h 2 H o 910004 71 4.5 o 5 -2.56038E+00 2s22p6 1Se10h 2 H o 910005 72 5.5 e 1 -5.22483E+00 2s22p6 1Se 7i 2 I e 1100001 73 5.5 e 2 -4.00033E+00 2s22p6 1Se 8i 2 I e 1100002 74 5.5 e 3 -3.16078E+00 2s22p6 1Se 9i 2 I e 1100003 75 5.5 e 4 -2.56023E+00 2s22p6 1Se10i 2 I e 1100004 76 5.5 o 1 -7.11096E+00 2s22p6 1Se 6h 2 H o 1110001 77 5.5 o 2 -5.22488E+00 2s22p6 1Se 7h 2 H o 1110002 78 5.5 o 3 -4.00041E+00 2s22p6 1Se 8h 2 H o 1110003 79 5.5 o 4 -3.16081E+00 2s22p6 1Se 9h 2 H o 1110004 80 5.5 o 5 -2.56023E+00 2s22p6 1Se10h 2 H o 1110005 81 6.5 e 1 -5.22460E+00 2s22p6 1Se 7i 2 I e 1300001 82 6.5 e 2 -4.00013E+00 2s22p6 1Se 8i 2 I e 1300002 83 6.5 e 3 -3.16063E+00 2s22p6 1Se 9i 2 I e 1300003 84 6.5 e 4 -2.56013E+00 2s22p6 1Se10i 2 I e 1300004 85 6.5 o 1 -4.00010E+00 2s22p6 1Se 8k 2 K o 1310001 86 6.5 o 2 -3.16063E+00 2s22p6 1Se 9k 2 K o 1310002 87 6.5 o 3 -2.56013E+00 2s22p6 1Se10k 2 K o 1310003 88 7.5 e 1 -3.16052E+00 2s22p6 1Se 9l 2 L e 1500001 89 7.5 e 2 -2.56003E+00 2s22p6 1Se10l 2 L e 1500002 90 7.5 o 1 -4.00008E+00 2s22p6 1Se 8k 2 K o 1510001 91 7.5 o 2 -3.16058E+00 2s22p6 1Se 9k 2 K o 1510002 92 7.5 o 3 -2.56008E+00 2s22p6 1Se10k 2 K o 1510003 93 8.5 e 1 -3.16050E+00 2s22p6 1Se 9l 2 L e 1700001 94 8.5 e 2 -2.56003E+00 2s22p6 1Se10l 2 L e 1700002 95 8.5 o 1 -2.56000E+00 2s22p6 1Se10m 2 M o 1710001 96 9.5 o 1 -2.56000E+00 2s22p6 1Se10m 2 M o 1910001 Total number of energies 96