c ******************* 786 **************************** c Ref: "Electron-Ion Recombination Rate Coefficients and Photoionization Cross Sections for Astrophysically Abundant Elements. V. Relativistic calculations for Fe~XXIV and Fe~XXV for X-ray modeling", Sultana N. Nahar, Anil K. Pradhan, Hong Lin Zhang, Astro. Phys. J. Suppl. 133, 375 (2000) c **************************************************** c Fe XXVI : Energies, Oscillator strengths and decay rates for allowed (E1) and forbidden (E2,E3,M1,m2) transitions (1s to 4f) Process: Fe XXVI + h\nu <-> Fe XXVI* Contents of the file (contains both LS and fine structure transitions): --------------------- i) Table 1 - Ion Information and Configuration Set: ii) LS Term Energies (Relative to the ground) iii) Transitions in pure LS coupling - Oscillator Strengths: iv) Fine Structure energies: relativistic(BP): v-a) Same Spin-Multiplicity Dipole allowed E1 (E1d) fine structure transitions v-b) Fine structure intercombination (E1i) transitions vi) Forbidden Electric Octupole E3 & Magnetic Quadrupole M2 transitions: vii) Forbidden Electric Quadrupole E2 & Magnetic Dipole M1 transitions: --------------------------------------------------------------------------- i) Table 1 - Ion Information and Configuration Set: --------------------------------------------------- Ion: nz = 26, nelc = 1 Total Number of LS terms= 10 Configuration set: ------------------ 10 configurations: first 10 spectroscopic, rest 0 correlation 1 1s 2 2s 3 2p 4 3s 5 3p 6 3d 7 4s 8 4p 9 4d 10 4f Number of orbitals = 10 Scaling parameters of the orbitals: 1.00000(1s) 1.00000(2s) 1.00000(2p) 1.00000(3s) 0.00000(3p) 1.00000(3d) 1.00000(4s) 1.00000(4p) 1.00000(4d) 1.00000(4f) -------------------------------------------------------------------------- ii) LS Term Energies (Relative to the ground) ---------------------------------------------- Note: Configuration numbers are as in Table 1. LS energies: i SLP E(Rel,Ry) cfg# 1 2Se 0.000000 1 2 2Po 507.000824 3 3 2Se 507.002380 2 4 2De 600.889648 6 5 2Se 600.889709 4 6 2Po 600.890808 5 7 2Fo 633.750793 10 8 2De 633.750793 9 9 2Po 633.750793 8 10 2Se 633.750793 7 Number of first LS terms optimized = 10 -------------------------------------------------------------------------- iii) Transitions in pure LS coupling - Oscillator Strengths: ------------------------------------------------------------ Table Explanation: ------------------ LSi:CFi -> Initial LS term & configuration number as in Table 1 LSf:CFf -> Final LS term & configuration number as in Table 1 fL, fV -> oscillator strengths in length and velocity forms -------------------- Ni LSi:CFi Nf LSf:CFf Ei Ef aji(s-1) fL fV %diff 1 2Se: 1 2 2Po: 3 0.0000 507.0008 2.864E+14 4.16E-01 4.16E-01 0.0E+00 1 2Se: 1 6 2Po: 5 0.0000 600.8908 7.648E+13 7.91E-02 7.91E-02 6.3E-03 1 2Se: 1 9 2Po: 8 0.0000 633.7508 3.117E+13 2.90E-02 2.90E-02 1.7E-02 2 2Po: 3 3 2Se: 2 507.0008 507.0024 4.109E-01 1.00E-05 0.00E+00 1.0E+02 2 2Po: 3 4 2De: 6 507.0008 600.8896 2.956E+13 6.96E-01 6.96E-01 4.8E-04 2 2Po: 3 5 2Se: 4 507.0008 600.8897 2.887E+12 1.36E-02 1.36E-02 2.5E-02 2 2Po: 3 8 2De: 9 507.0008 633.7508 9.430E+12 1.22E-01 1.22E-01 1.0E-06 2 2Po: 3 10 2Se: 7 507.0008 633.7508 1.179E+12 3.04E-03 3.05E-03 1.6E-01 3 2Se: 2 6 2Po: 5 507.0024 600.8908 1.026E+13 4.35E-01 4.35E-01 1.1E-03 3 2Se: 2 9 2Po: 8 507.0024 633.7508 4.419E+12 1.03E-01 1.03E-01 4.9E-03 4 2De: 6 6 2Po: 5 600.8896 600.8908 4.128E-01 2.00E-05 0.00E+00 1.0E+02 4 2De: 6 7 2Fo:10 600.8896 633.7508 6.304E+12 1.02E+00 1.02E+00 4.7E-06 4 2De: 6 9 2Po: 8 600.8896 633.7508 1.590E+11 1.10E-02 1.10E-02 4.5E-02 5 2Se: 4 6 2Po: 5 600.8897 600.8908 2.911E-01 9.00E-05 1.00E-04 5.3E+00 5 2Se: 4 9 2Po: 8 600.8897 633.7508 1.402E+12 4.85E-01 4.85E-01 1.1E-02 6 2Po: 5 8 2De: 9 600.8908 633.7508 3.216E+12 6.18E-01 6.18E-01 2.1E-02 6 2Po: 5 10 2Se: 7 600.8908 633.7508 8.381E+11 3.22E-02 3.22E-02 6.2E-02 LS transitions: Number of oscillator strengths = 17 ----------------------------------------------------------------------------- iv) Fine Structure energies: relativistic(BP): ----------------------------------------------- Theory Expt(+Theo with 0% diff) ie SLp(cf#) 2J k*cm E(Ry) cfg SLP E(Ry) %df 1 2Se( 1) 2 0.0 0.00000E+00 2 2Po( 3) 2 56097812.0 5.11201E+02 3 2Se( 2) 2 56100508.0 5.11225E+02 4 2Po( 3) 4 56266344.0 5.12737E+02 5 2Po( 5) 2 66537964.0 6.06339E+02 6 2Se( 4) 2 66538688.0 6.06345E+02 7 2De( 6) 4 66586520.0 6.06781E+02 8 2Po( 5) 4 66586736.0 6.06783E+02 9 2De( 6) 6 66603064.0 6.06932E+02 10 2Po( 8) 2 70184592.0 6.39569E+02 11 2Se( 7) 2 70184944.0 6.39572E+02 12 2De( 9) 4 70204448.0 6.39750E+02 13 2Po( 8) 4 70204496.0 6.39750E+02 14 2Fo(10) 6 70211328.0 6.39813E+02 15 2De( 9) 6 70211336.0 6.39813E+02 16 2Fo(10) 8 70214800.0 6.39844E+02 ------------------------------------------------------------------------ v-a) Same Spin-Multiplicity Dipole allowed E1 (E1d) fine structure transitions -------------------------------------------------------- Table Explanation: ----------------- SLpCi -> initial symmetry (2S+1)Lpi(parity) & configuration number as in Table 1 SLpCi -> final symmetry (2S+1)Lpi(parity) & configuration number as in Table 1 fij, S, aji -> Oscillator strength fij, line strengh S & transition probability aji for electic dipole E1 same-spin transition ------------------------ Ni Nj SLpCi SLpCj gi gj wl(A) Ei(Ry) Ej(Ry) fij S aji(s-1) 1 2 2Se 1 2Po 3 2 2 1.78 0.00 511.20 1.35E-01 1.580E-03 2.82E+14 2 3 2Po 3 2Se 2 2 2 37093 511.20 511.23 1.07E-04 2.616E-02 5.19E+02 1 4 2Se 1 2Po 3 2 4 1.78 0.00 512.74 2.68E-01 3.134E-03 2.83E+14 3 4 2Se 2 2Po 3 2 4 603.02 511.23 512.74 1.33E-02 5.290E-02 1.22E+08 1 5 2Se 1 2Po 5 2 2 1.50 0.00 606.34 2.38E-02 2.358E-04 7.04E+13 3 5 2Se 2 2Po 5 2 2 9.58 511.23 606.34 1.41E-01 8.881E-03 1.02E+13 2 6 2Po 3 2Se 4 2 2 9.58 511.20 606.35 1.22E-02 7.704E-04 8.88E+11 4 6 2Po 3 2Se 4 4 2 9.73 512.74 606.35 1.44E-02 1.848E-03 2.03E+12 5 6 2Po 5 2Se 4 2 2 137768 606.34 606.35 1.76E-04 1.600E-01 6.13E+01 2 7 2Po 3 2De 6 2 4 9.53 511.20 606.78 6.79E-01 4.260E-02 2.49E+13 4 7 2Po 3 2De 6 4 4 9.69 512.74 606.78 6.90E-02 8.809E-03 4.90E+12 5 7 2Po 5 2De 6 2 4 2059 606.34 606.78 1.47E-02 1.999E-01 1.16E+07 1 8 2Se 1 2Po 5 2 4 1.50 0.00 606.78 4.93E-02 4.874E-04 7.29E+13 3 8 2Se 2 2Po 5 2 4 9.54 511.23 606.78 2.73E-01 1.716E-02 1.00E+13 6 8 2Se 4 2Po 5 2 4 2081 606.35 606.78 2.32E-02 3.186E-01 1.79E+07 7 8 2De 6 2Po 5 4 4 462196 606.78 606.78 6.26E-06 3.728E-02 2.04E-01 4 9 2Po 3 2De 6 4 6 9.67 512.74 606.93 6.21E-01 7.913E-02 2.95E+13 8 9 2Po 5 2De 6 4 6 6124 606.78 606.93 4.45E-03 3.594E-01 5.28E+05 1 10 2Se 1 2Po 8 2 2 1.42 0.00 639.57 7.59E-03 7.124E-05 2.49E+13 3 10 2Se 2 2Po 8 2 2 7.10 511.23 639.57 3.03E-02 1.417E-03 4.01E+12 6 10 2Se 4 2Po 8 2 2 27.43 606.35 639.57 1.54E-01 2.778E-02 1.36E+12 7 10 2De 6 2Po 8 4 2 27.79 606.78 639.57 9.35E-03 3.420E-03 1.61E+11 2 11 2Po 3 2Se 7 2 2 7.10 511.20 639.57 1.85E-03 8.669E-05 2.46E+11 4 11 2Po 3 2Se 7 4 2 7.18 512.74 639.57 2.80E-03 2.647E-04 7.23E+11 5 11 2Po 5 2Se 7 2 2 27.42 606.34 639.57 2.84E-02 5.120E-03 2.52E+11 8 11 2Po 5 2Se 7 4 2 27.79 606.78 639.57 3.31E-02 1.211E-02 5.72E+11 10 11 2Po 8 2Se 7 2 2 284034 639.57 639.57 2.94E-04 5.554E-01 2.38E+01 2 12 2Po 3 2De 9 2 4 7.09 511.20 639.75 1.16E-01 5.431E-03 7.72E+12 4 12 2Po 3 2De 9 4 4 7.18 512.74 639.75 1.18E-02 1.111E-03 1.52E+12 5 12 2Po 5 2De 9 2 4 27.27 606.34 639.75 5.87E-01 1.055E-01 2.63E+12 8 12 2Po 5 2De 9 4 4 27.64 606.78 639.75 6.10E-02 2.220E-02 5.32E+11 10 12 2Po 8 2De 9 2 4 5037 639.57 639.75 2.60E-02 8.615E-01 3.41E+06 1 13 2Se 1 2Po 8 2 4 1.42 0.00 639.75 1.62E-02 1.522E-04 2.67E+13 3 13 2Se 2 2Po 8 2 4 7.09 511.23 639.75 6.12E-02 2.858E-03 4.06E+12 6 13 2Se 4 2Po 8 2 4 27.28 606.35 639.75 2.97E-01 5.342E-02 1.33E+12 7 13 2De 6 2Po 8 4 4 27.64 606.78 639.75 1.69E-03 6.166E-04 1.48E+10 9 13 2De 6 2Po 8 6 4 27.77 606.93 639.75 1.10E-02 6.036E-03 1.43E+11 11 13 2Se 7 2Po 8 2 4 5113 639.57 639.75 3.19E-02 1.073E+00 4.07E+06 7 14 2De 6 2Fo10 4 6 27.59 606.78 639.81 1.01E+00 3.664E-01 5.89E+12 9 14 2De 6 2Fo10 6 6 27.71 606.93 639.81 4.82E-02 2.638E-02 4.18E+11 12 14 2De 9 2Fo10 4 6 14536 639.75 639.81 4.70E-03 9.001E-01 9.89E+04 4 15 2Po 3 2De 9 4 6 7.17 512.74 639.81 1.07E-01 1.015E-02 9.29E+12 8 15 2Po 5 2De 9 4 6 27.59 606.78 639.81 5.46E-01 1.985E-01 3.19E+12 13 15 2Po 8 2De 9 4 6 14620 639.75 639.81 8.00E-03 1.541E+00 1.66E+05 9 16 2De 6 2Fo10 6 8 27.69 606.93 639.84 9.65E-01 5.277E-01 6.30E+12 15 16 2De 9 2Fo10 6 8 28882 639.81 639.84 2.25E-03 1.281E+00 1.35E+04 Number of non-zero E1 transitions = 46 Number of dipole transitions, E1d = 46 Number of lines in the table = 69 v-b) Fine structure intercombination (E1i) transitions ------------------------------------------------------ Fine structure E1i intercombination transitions in Breit-Pauli approx: Ni Nj SLpCi SLpCj gi gj wl(A) Ei(Ry) Ej(Ry) fij S aji(s-1) Number of non-zero E1 transitions = 46 Number of intercombination transitions, E1i = 0 Number of lines in the table = 69 ------------------------------------------------------------------------------ vi) Forbidden Electric Octupole E3 & Magnetic Quadrupole M2 transitions: ------------------------------------------------------ Table Explanation: ----------------- SLpCi -> initial symmetry (2S+1)Lpi(parity) & configuration number as in Table 1 SLpCi -> final symmetry (2S+1)Lpi(parity) & configuration number as in Table 1 SE3, AE3 -> line strengh S & transition probability A for electic octupole E3 transition SM2, AM2 -> line strengh S & transition probability A for magnetic quadrupole M2 transition ------------------------ Ni Nj SLpCi SLpCj gi gj wl(A) Ei(Ry) Ej(Ry) SE3 AE3(s-1) SM2 AM2(s-1) 2 9 2Po 3 2De 6 2 6 9.52 5.112E+02 6.069E+02 2.92E-04 4.33E+06 1.09E+00 3.46E+07 5 9 2Po 5 2De 6 2 6 1536 6.063E+02 6.069E+02 9.41E-03 4.89E-08 5.14E+00 1.49E-03 9 10 2De 6 2Po 8 6 2 27.92 6.069E+02 6.396E+02 6.10E-03 1.45E+05 9.49E-02 4.17E+04 1 14 2Se 1 2Fo10 2 6 1.42 0.000E+00 6.398E+02 5.77E-08 5.08E+08 0.00E+00 0.00E+00 3 14 2Se 2 2Fo10 2 6 7.09 5.112E+02 6.398E+02 2.48E-04 2.89E+07 0.00E+00 0.00E+00 6 14 2Se 4 2Fo10 2 6 27.23 6.063E+02 6.398E+02 2.65E-02 2.51E+05 0.00E+00 0.00E+00 11 14 2Se 7 2Fo10 2 6 3790 6.396E+02 6.398E+02 1.38E-01 1.29E-09 0.00E+00 0.00E+00 2 15 2Po 3 2De 9 2 6 7.09 5.112E+02 6.398E+02 3.63E-06 4.24E+05 1.41E-01 1.96E+07 5 15 2Po 5 2De 9 2 6 27.22 6.063E+02 6.398E+02 2.45E-02 2.31E+05 2.68E+00 4.46E+05 10 15 2Po 8 2De 9 2 6 3738 6.396E+02 6.398E+02 4.60E-01 4.72E-09 2.21E+01 7.50E-05 1 16 2Se 1 2Fo10 2 8 1.42 0.000E+00 6.398E+02 7.69E-08 5.09E+08 0.00E+00 0.00E+00 3 16 2Se 2 2Fo10 2 8 7.09 5.112E+02 6.398E+02 3.30E-04 2.90E+07 0.00E+00 0.00E+00 6 16 2Se 4 2Fo10 2 8 27.20 6.063E+02 6.398E+02 3.54E-02 2.52E+05 0.00E+00 0.00E+00 7 16 2De 6 2Fo10 4 8 27.56 6.068E+02 6.398E+02 9.84E-03 6.40E+04 8.93E+00 1.05E+06 11 16 2Se 7 2Fo10 2 8 3349 6.396E+02 6.398E+02 1.85E-01 3.07E-09 0.00E+00 0.00E+00 12 16 2De 9 2Fo10 4 8 9656 6.398E+02 6.398E+02 1.26E-01 1.27E-12 2.20E+01 4.87E-07 Number of transitions: E3 = 16, M2 = 8, Total E3+M2 = 24 Total number of lines of M2/E3 transitions = 16 ---------------------------------------------------------------------------- vii) Forbidden Electric Quadrupole E2 & Magnetic Dipole M1 transitions: ----------------------------------------------------- Table Explanation: ----------------- SLpCi -> initial symmetry (2S+1)Lpi(parity) & configuration number as in Table 1 SLpCi -> final symmetry (2S+1)Lpi(parity) & configuration number as in Table 1 SE2, AE2 -> line strengh S & transition probability A for electric quadrupole E2 transition SM1, AM1 -> line strengh S & transition probability A for magnetic dipole M1 transition ------------------------ Ni Nj SLpCi SLpCj gi gj wl(A) Ei(Ry) Ej(Ry) SE2 AE2(s-1) SM1 AM1(s-1) 1 3 2Se 1 2Se 2 2 2 1.78 0.000E+00 5.112E+02 0.00E+00 0.00E+00 1.57E-04 3.73E+08 2 4 2Po 3 2Po 3 2 4 593.37 5.112E+02 5.127E+02 1.02E-03 5.83E+00 1.32E+00 4.27E+04 2 5 2Po 3 2Po 5 2 2 9.58 5.112E+02 6.063E+02 0.00E+00 0.00E+00 4.55E-06 6.99E+04 4 5 2Po 3 2Po 5 4 2 9.74 5.127E+02 6.063E+02 7.61E-04 7.30E+09 1.34E-04 1.95E+06 1 6 2Se 1 2Se 4 2 2 1.50 0.000E+00 6.063E+02 0.00E+00 0.00E+00 4.76E-05 1.89E+08 3 6 2Se 2 2Se 4 2 2 9.58 5.112E+02 6.063E+02 0.00E+00 0.00E+00 1.73E-05 2.65E+05 1 7 2Se 1 2De 6 2 4 1.50 0.000E+00 6.068E+02 3.63E-06 1.99E+11 1.26E-06 2.50E+06 3 7 2Se 2 2De 6 2 4 9.54 5.112E+02 6.068E+02 3.07E-03 1.63E+10 3.91E-06 3.04E+04 6 7 2Se 4 2De 6 2 4 2090 6.063E+02 6.068E+02 2.33E-02 2.45E-01 1.49E-07 1.10E-04 2 8 2Po 3 2Po 5 2 4 9.53 5.112E+02 6.068E+02 6.83E-04 3.64E+09 5.43E-05 4.22E+05 4 8 2Po 3 2Po 5 4 4 9.69 5.127E+02 6.068E+02 7.43E-04 3.65E+09 6.81E-05 5.05E+05 5 8 2Po 5 2Po 5 2 4 2050 6.063E+02 6.068E+02 3.71E-02 4.30E-01 1.33E+00 1.04E+03 1 9 2Se 1 2De 6 2 6 1.50 0.000E+00 6.069E+02 5.42E-06 1.99E+11 0.00E+00 0.00E+00 3 9 2Se 2 2De 6 2 6 9.52 5.112E+02 6.069E+02 4.60E-03 1.64E+10 0.00E+00 0.00E+00 6 9 2Se 4 2De 6 2 6 1553 6.063E+02 6.069E+02 3.53E-02 1.09E+00 0.00E+00 0.00E+00 7 9 2De 6 2De 6 4 6 6044 6.068E+02 6.069E+02 7.87E-03 2.73E-04 2.39E+00 4.87E+01 2 10 2Po 3 2Po 8 2 2 7.10 5.112E+02 6.396E+02 0.00E+00 0.00E+00 1.27E-06 4.80E+04 4 10 2Po 3 2Po 8 4 2 7.18 5.127E+02 6.396E+02 5.89E-05 2.58E+09 3.11E-05 1.13E+06 5 10 2Po 5 2Po 8 2 2 27.42 6.063E+02 6.396E+02 0.00E+00 0.00E+00 1.32E-06 8.65E+02 8 10 2Po 5 2Po 8 4 2 27.79 6.068E+02 6.396E+02 1.52E-02 7.69E+08 1.16E-04 7.29E+04 1 11 2Se 1 2Se 7 2 2 1.42 0.000E+00 6.396E+02 0.00E+00 0.00E+00 4.63E-05 2.16E+08 3 11 2Se 2 2Se 7 2 2 7.10 5.112E+02 6.396E+02 0.00E+00 0.00E+00 6.99E-06 2.63E+05 6 11 2Se 4 2Se 7 2 2 27.43 6.063E+02 6.396E+02 0.00E+00 0.00E+00 4.12E-06 2.69E+03 7 11 2De 6 2Se 7 4 2 27.79 6.068E+02 6.396E+02 2.39E-03 1.21E+08 7.89E-10 4.96E-01 9 11 2De 6 2Se 7 6 2 27.92 6.069E+02 6.396E+02 3.81E-03 1.89E+08 0.00E+00 0.00E+00 1 12 2Se 1 2De 9 2 4 1.42 0.000E+00 6.398E+02 2.77E-06 1.98E+11 1.99E-07 4.64E+05 3 12 2Se 2 2De 9 2 4 7.09 5.112E+02 6.398E+02 5.52E-05 1.29E+09 1.10E-06 2.09E+04 6 12 2Se 4 2De 9 2 4 27.28 6.063E+02 6.398E+02 4.24E-02 1.18E+09 3.71E-07 1.23E+02 7 12 2De 6 2De 9 4 4 27.64 6.068E+02 6.398E+02 9.68E-03 2.52E+08 8.06E-06 2.58E+03 9 12 2De 6 2De 9 6 4 27.77 6.069E+02 6.398E+02 4.27E-03 1.09E+08 2.63E-05 8.29E+03 11 12 2Se 7 2De 9 2 4 5128 6.396E+02 6.398E+02 3.39E-01 4.02E-02 9.53E-08 4.77E-06 2 13 2Po 3 2Po 8 2 4 7.09 5.112E+02 6.398E+02 3.93E-05 9.22E+08 9.84E-06 1.86E+05 4 13 2Po 3 2Po 8 4 4 7.18 5.127E+02 6.398E+02 6.05E-05 1.34E+09 2.24E-05 4.10E+05 5 13 2Po 5 2Po 8 2 4 27.27 6.063E+02 6.398E+02 1.35E-02 3.76E+08 7.50E-05 2.49E+04 8 13 2Po 5 2Po 8 4 4 27.64 6.068E+02 6.398E+02 1.48E-02 3.86E+08 2.03E-05 6.48E+03 10 13 2Po 8 2Po 8 2 4 5023 6.396E+02 6.398E+02 4.23E-01 5.55E-02 1.33E+00 7.08E+01 2 14 2Po 3 2Fo10 2 6 7.09 5.112E+02 6.398E+02 9.84E-04 1.54E+10 0.00E+00 0.00E+00 4 14 2Po 3 2Fo10 4 6 7.17 5.127E+02 6.398E+02 2.89E-04 4.27E+09 1.05E-06 1.28E+04 5 14 2Po 5 2Fo10 2 6 27.22 6.063E+02 6.398E+02 7.80E-02 1.46E+09 0.00E+00 0.00E+00 8 14 2Po 5 2Fo10 4 6 27.59 6.068E+02 6.398E+02 2.29E-02 4.01E+08 1.62E-06 3.46E+02 10 14 2Po 8 2Fo10 2 6 3740 6.396E+02 6.398E+02 2.39E-01 9.13E-02 0.00E+00 0.00E+00 13 14 2Po 8 2Fo10 4 6 14651 6.398E+02 6.398E+02 6.76E-02 2.80E-05 3.85E-08 5.51E-08 1 15 2Se 1 2De 9 2 6 1.42 0.000E+00 6.398E+02 4.18E-06 2.00E+11 0.00E+00 0.00E+00 3 15 2Se 2 2De 9 2 6 7.09 5.112E+02 6.398E+02 8.60E-05 1.35E+09 0.00E+00 0.00E+00 6 15 2Se 4 2De 9 2 6 27.23 6.063E+02 6.398E+02 6.33E-02 1.18E+09 0.00E+00 0.00E+00 7 15 2De 6 2De 9 4 6 27.59 6.068E+02 6.398E+02 4.12E-03 7.22E+07 8.09E-06 1.73E+03 9 15 2De 6 2De 9 6 6 27.71 6.069E+02 6.398E+02 1.70E-02 2.90E+08 4.06E-05 8.58E+03 11 15 2Se 7 2De 9 2 6 3788 6.396E+02 6.398E+02 5.09E-01 1.83E-01 0.00E+00 0.00E+00 12 15 2De 9 2De 9 4 6 14505 6.398E+02 6.398E+02 1.28E-01 5.55E-05 2.40E+00 3.53E+00 4 16 2Po 3 2Fo10 4 8 7.17 5.127E+02 6.398E+02 1.73E-03 1.92E+10 0.00E+00 0.00E+00 8 16 2Po 5 2Fo10 4 8 27.56 6.068E+02 6.398E+02 1.37E-01 1.81E+09 0.00E+00 0.00E+00 13 16 2Po 8 2Fo10 4 8 9706 6.398E+02 6.398E+02 4.06E-01 9.88E-04 0.00E+00 0.00E+00 14 16 2Fo10 2Fo10 6 8 28760 6.398E+02 6.398E+02 4.33E-02 4.61E-07 3.43E+00 4.85E-01 Number of transitions: E2 = 44, M1 = 39, Total E2+M1 = 83 Total number of transitions lines (including non-spectroscopic) = 53 NT= total number of forbidden (E2,M1,E3,M2) transitions = 83 + 24 = 107 Net allowed (E1) and forbidden (E2,M1,E3,M2) transitions = = 46 + 107 = 153