*************************** 786 ******************************************* Ref. "K$_{\alpha}$ resonance fluorescence in Al, Ti, Cu and potential applications for X-ray sources", Sultana N. Nahar and Anil K. Pradhan, JQSRT 155, 32-48 (2015) ************************************************************************** Cu28+: Energy levels, Oscillator strengths f, S, A-values for allowed (E1) and forbidden (E2,E3,M1,M2) fine structure transitions in Breit-Pauli approximation Process: Cu28+ + h\nu <-> Cu28+* File contents : -------------- 1) Table of Configurations and Thomas-Fermi scaling parameters 2) Table of LS term energies 3) LS Multiplets 4) Fine Structure energies : 5) Allowed E1 transitions with same spin multiplicity - E1d 6) Allowed E1 transitions with intercombination spin multiplicity - E1i 7) Forbidden E3 and M2 transitions in Breit-Pauli approximation 8) Forbidden E2 and M1 transitions in Breit-Pauli approximation **************************************************************************** i) Table of Configurations and Thomas-Fermi scaling parameters --------------------------------------------------------------- Ion: nz = 29, 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) **************************************************************************** 2) Table of LS term energies ------------------- LS energies: i SLP E(Rel,Ry) cfg# 1 2Se 0.000000 1 2 2Po 630.751248 3 3 2Se 630.751262 2 4 2De 747.556734 6 5 2Po 747.556777 5 6 2Se 747.556805 4 7 2Fo 788.438676 10 8 2Po 788.438711 8 9 2Se 788.438733 7 10 2De 788.440668 9 Number of first LS terms optimized = 10 ************************************************************************* 3) Table of LS Multiplets: ------------------ Transitions in pure LS coupling - Oscillator Strengths: Ni LSi:CFi Nf LSf:CFf Ei Ef aji(s-1) fL fV %diff 1 2Se: 1 2 2Po: 3 0.0000 630.7512 4.433E+14 4.16E-01 4.16E-01 0.0E+00 1 2Se: 1 5 2Po: 5 0.0000 747.5568 1.184E+14 7.91E-02 7.91E-02 0.0E+00 1 2Se: 1 8 2Po: 8 0.0000 788.4387 4.825E+13 2.90E-02 2.90E-02 1.7E-02 2 2Po: 3 4 2De: 6 630.7512 747.5567 4.575E+13 6.96E-01 6.96E-01 4.8E-04 2 2Po: 3 6 2Se: 4 630.7512 747.5568 4.468E+12 1.36E-02 1.36E-02 2.5E-02 2 2Po: 3 9 2Se: 7 630.7512 788.4387 1.824E+12 3.04E-03 3.05E-03 1.6E-01 2 2Po: 3 10 2De: 9 630.7512 788.4407 1.460E+13 1.22E-01 1.22E-01 1.4E-03 3 2Se: 2 5 2Po: 5 630.7513 747.5568 1.589E+13 4.35E-01 4.35E-01 2.3E-03 3 2Se: 2 8 2Po: 8 630.7513 788.4387 6.842E+12 1.03E-01 1.03E-01 9.7E-03 4 2De: 6 7 2Fo:10 747.5567 788.4387 9.757E+12 1.02E+00 1.02E+00 0.0E+00 4 2De: 6 8 2Po: 8 747.5567 788.4387 2.459E+11 1.10E-02 1.10E-02 0.0E+00 5 2Po: 5 9 2Se: 7 747.5568 788.4387 1.299E+12 3.23E-02 3.23E-02 0.0E+00 5 2Po: 5 10 2De: 9 747.5568 788.4407 4.982E+12 6.18E-01 6.18E-01 2.2E-03 6 2Se: 4 8 2Po: 8 747.5568 788.4387 2.169E+12 4.85E-01 4.85E-01 1.0E-03 7 2Fo:10 10 2De: 9 788.4387 788.4407 3.804E+00 9.00E-05 7.14E-06 8.5E+01 8 2Po: 8 10 2De: 9 788.4387 788.4407 4.120E+00 2.20E-04 2.17E-04 7.6E-01 LS transitions: Number of oscillator strengths = 16 Comparison of LS term energies: relativistic(r) & pure LS: Expt theory %diff config term E(Ry) term E(LSr) CF term E(LS) CF 1 2Se 0.0000 1 2Se 0.0000 1 2 2Se 637.3031 2 2Po 630.7512 3 3 2Po 638.8469 3 2Se 630.7513 2 4 2Se 756.0184 4 2De 747.5567 6 5 2Po 756.4607 5 2Po 747.5568 5 6 2De 756.8277 6 2Se 747.5568 4 7 2Se 797.4663 7 2Fo 788.4387 10 8 2Po 797.6452 8 2Po 788.4387 8 9 2De 797.7971 9 2Se 788.4387 7 10 2Fo 797.8617 10 2De 788.4407 9 ****************************************************************************** 4) Fine Structure energies : --------------------------- ie -> energy position number SLP (cf) -> SLpi symmetry belonging to configuration 1 of Table i Fine structure energy levels of Fe~XV for which forbidden (E2,E3,M1,M2) transitions are presented. The indices (cf) correspond to cofigurations numbers 2J -> 2 times total angular momentum k*cm -> k momentum in cm (ignore the column) Ec(Ry) -> calculated energies (relative) cfg -> configuration only for observed levels given in NIST compilation (if available) SLP -> Symmetry in numerical notation (sllp: s=2S+1, ll=L, p=parity, 0=even 1=odd) if the level has been observed E(Ry) -> Final energies (relative) that were used in the transitions df -> percent difference between calculated and available experimental energies ----------------------------------------------------- Number of fine structure levels = 16 Number of default fine structure levels = 16 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 69931042.0 6.37259E+02 3 2Se( 2) 2 69935929.0 6.37303E+02 4 2Po( 3) 4 70192491.0 6.39641E+02 5 2Po( 5) 2 82961823.0 7.56004E+02 6 2Se( 4) 2 82963427.0 7.56018E+02 7 2De( 6) 4 83036856.0 7.56688E+02 8 2Po( 5) 4 83037039.0 7.56689E+02 9 2De( 6) 6 83062483.0 7.56921E+02 10 2Po( 8) 2 87511134.0 7.97460E+02 11 2Se( 7) 2 87511806.0 7.97466E+02 12 2Po( 8) 4 87541602.0 7.97738E+02 13 2De( 9) 4 87541714.0 7.97739E+02 14 2Fo(10) 6 87552122.0 7.97834E+02 15 2De( 9) 6 87552364.0 7.97836E+02 16 2Fo(10) 8 87557504.0 7.97883E+02 ****************************************************************************** 5) Allowed E1 transitions with same spin multiplicity - E1d ------------------------------------------------------------------------ (ignore the negative signs, for internal purpose, in linestrengths S): Explanantion: ------------- Ni, Nj -> energy level number in Table ii SLpC -> symmetry SLpi of configuration C wl -> Transition wavelength Ei, Ej -> Energies of levels in Rydberg fij -> oscillator strength S -> line strength for E1 transitions aij -> Radiative decay rate/ Transition probability ---------------------------------------------------------- Dipole allowed E1d fine structure transitions in Breit-Pauli approx: 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 1.43 0.00 637.26 1.34E-01 1.258E-03 4.36E+14 2 3 2Po 3 2Se 2 2 2 20460 637.26 637.30 1.55E-04 2.095E-02 2.48E+03 1 4 2Se 1 2Po 3 2 4 1.43 0.00 639.64 2.66E-01 2.491E-03 4.36E+14 3 4 2Se 2 2Po 3 2 4 389.77 637.30 639.64 1.65E-02 4.247E-02 3.63E+08 1 5 2Se 1 2Po 5 2 2 1.21 0.00 756.00 2.32E-02 1.843E-04 1.07E+14 3 5 2Se 2 2Po 5 2 2 7.68 637.30 756.00 1.40E-01 7.070E-03 1.58E+13 2 6 2Po 3 2Se 4 2 2 7.67 637.26 756.02 1.19E-02 5.998E-04 1.34E+12 4 6 2Po 3 2Se 4 4 2 7.83 639.64 756.02 1.46E-02 1.506E-03 3.18E+12 5 6 2Po 5 2Se 4 2 2 62340 756.00 756.02 3.10E-04 1.271E-01 5.31E+02 2 7 2Po 3 2De 6 2 4 7.63 637.26 756.69 6.75E-01 3.390E-02 3.86E+13 4 7 2Po 3 2De 6 4 4 7.79 639.64 756.69 6.89E-02 7.064E-03 7.58E+12 5 7 2Po 5 2De 6 2 4 1332 756.00 756.69 1.83E-02 1.606E-01 3.44E+07 1 8 2Se 1 2Po 5 2 4 1.20 0.00 756.69 4.84E-02 3.841E-04 1.11E+14 3 8 2Se 2 2Po 5 2 4 7.63 637.30 756.69 2.69E-01 1.353E-02 1.54E+13 6 8 2Se 4 2Po 5 2 4 1358 756.02 756.69 2.86E-02 2.559E-01 5.17E+07 7 8 2De 6 2Po 5 4 4 544345 756.69 756.69 4.45E-06 3.191E-02 1.00E-01 4 9 2Po 3 2De 6 4 6 7.77 639.64 756.92 6.20E-01 6.343E-02 4.57E+13 8 9 2Po 5 2De 6 4 6 3930 756.69 756.92 5.58E-03 2.886E-01 1.60E+06 1 10 2Se 1 2Po 8 2 2 1.14 0.00 797.46 7.14E-03 5.372E-05 3.65E+13 3 10 2Se 2 2Po 8 2 2 5.69 637.30 797.46 2.94E-02 1.102E-03 6.06E+12 6 10 2Se 4 2Po 8 2 2 21.99 756.02 797.46 1.52E-01 2.202E-02 2.10E+12 7 10 2De 6 2Po 8 4 2 22.35 756.69 797.46 9.37E-03 2.759E-03 2.50E+11 2 11 2Po 3 2Se 7 2 2 5.69 637.26 797.47 1.61E-03 6.030E-05 3.32E+11 4 11 2Po 3 2Se 7 4 2 5.77 639.64 797.47 2.74E-03 2.081E-04 1.10E+12 5 11 2Po 5 2Se 7 2 2 21.98 756.00 797.47 2.75E-02 3.981E-03 3.80E+11 8 11 2Po 5 2Se 7 4 2 22.35 756.69 797.47 3.33E-02 9.804E-03 8.90E+11 10 11 2Po 8 2Se 7 2 2 148722 797.46 797.47 4.42E-04 4.333E-01 1.33E+02 1 12 2Se 1 2Po 8 2 4 1.14 0.00 797.74 1.55E-02 1.167E-04 3.97E+13 3 12 2Se 2 2Po 8 2 4 5.68 637.30 797.74 5.95E-02 2.227E-03 6.16E+12 6 12 2Se 4 2Po 8 2 4 21.84 756.02 797.74 2.92E-01 4.195E-02 2.04E+12 7 12 2De 6 2Po 8 4 4 22.20 756.69 797.74 1.66E-03 4.851E-04 2.25E+10 9 12 2De 6 2Po 8 6 4 22.33 756.92 797.74 1.10E-02 4.851E-03 2.21E+11 11 12 2Se 7 2Po 8 2 4 3356 797.47 797.74 3.91E-02 8.643E-01 1.16E+07 2 13 2Po 3 2De 9 2 4 5.68 637.26 797.74 1.15E-01 4.302E-03 1.19E+13 4 13 2Po 3 2De 9 4 4 5.76 639.64 797.74 1.17E-02 8.855E-04 2.34E+12 5 13 2Po 5 2De 9 2 4 21.83 756.00 797.74 5.81E-01 8.346E-02 4.06E+12 8 13 2Po 5 2De 9 4 4 22.20 756.69 797.74 6.08E-02 1.778E-02 8.23E+11 10 13 2Po 8 2De 9 2 4 3270 797.46 797.74 3.22E-02 6.938E-01 1.00E+07 12 13 2Po 8 2De 9 4 4 888211 797.74 797.74 1.18E-05 1.377E-01 9.95E-02 7 14 2De 6 2Fo10 4 6 22.15 756.69 797.83 1.01E+00 2.935E-01 9.12E+12 9 14 2De 6 2Fo10 6 6 22.27 756.92 797.83 4.81E-02 2.118E-02 6.47E+11 13 14 2De 9 2Fo10 4 6 9608 797.74 797.83 5.73E-03 7.245E-01 2.76E+05 4 15 2Po 3 2De 9 4 6 5.76 639.64 797.84 1.07E-01 8.112E-03 1.43E+13 8 15 2Po 5 2De 9 4 6 22.15 756.69 797.84 5.44E-01 1.587E-01 4.93E+12 12 15 2Po 8 2De 9 4 6 9291 797.74 797.84 1.01E-02 1.239E+00 5.22E+05 14 15 2Fo10 2De 9 6 6 413454 797.83 797.84 6.31E-06 5.153E-02 2.46E-01 9 16 2De 6 2Fo10 6 8 22.25 756.92 797.88 9.64E-01 4.235E-01 9.74E+12 15 16 2De 9 2Fo10 6 8 19456 797.84 797.88 2.68E-03 1.030E+00 3.54E+04 Number of non-zero E1 transitions = 48 Number of dipole transitions, E1d = 48 Number of lines in the table = 71 ************************************************************************ 6) Allowed E1 transitions with intercombination spin multiplicity - E1i Explanantion: ------------- Ni, Nj -> energy level number in Table ii SLpC -> symmetry SLpi of configuration C wl -> Transition wavelength Ei, Ej -> Energies of levels in Rydberg fij -> oscillator strength S -> line strength for E1 transitions aij -> Radiative decay rate/ Transition probability ---------------------------------------------------------- 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 = 48 Number of intercombination transitions, E1i = 0 Number of lines in the table = 71 *******************************************************************************" 7) Forbidden E3 and M2 transitions in Breit-Pauli approximation ------------------------------------------------------------------------ (ignore the negative signs, for internal purpose, in linestrengths S): Explanantion: ------------- Ni, Nj -> energy level number in Table ii SLpC -> symmetry SLpi of configuration C gi,gj -> statistical weight factors of initial and final states wl = Transition wavelengths Ei,Ej -> level energies of initial and final state SE3, SM2 -> line strengths for E3, M2 transitions AE3, AM2 -> Radiative Decay Rates for E3, M2 transitions ---------------------------------------------------------- Forbidden octu E3 and quadrupole M2 transitions in Breit-Pauli approximation: 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 7.62 6.373E+02 7.569E+02 1.49E-04 1.05E+07 8.66E-01 8.40E+07 5 9 2Po 5 2De 6 2 6 993.44 7.560E+02 7.569E+02 4.86E-03 5.33E-07 4.13E+00 1.06E-02 9 10 2De 6 2Po 8 6 2 22.48 7.569E+02 7.975E+02 3.17E-03 3.43E+05 7.80E-02 1.01E+05 1 14 2Se 1 2Fo10 2 6 1.14 0.000E+00 7.978E+02 5.32E-08 2.20E+09 0.00E+00 0.00E+00 3 14 2Se 2 2Fo10 2 6 5.68 6.373E+02 7.978E+02 1.29E-04 7.14E+07 0.00E+00 0.00E+00 6 14 2Se 4 2Fo10 2 6 21.79 7.560E+02 7.978E+02 1.36E-02 6.10E+05 0.00E+00 0.00E+00 11 14 2Se 7 2Fo10 2 6 2480 7.975E+02 7.978E+02 7.22E-02 1.31E-08 0.00E+00 0.00E+00 2 15 2Po 3 2De 9 2 6 5.67 6.373E+02 7.978E+02 2.91E-06 1.61E+06 1.12E-01 4.73E+07 5 15 2Po 5 2De 9 2 6 21.78 7.560E+02 7.978E+02 1.24E-02 5.57E+05 2.12E+00 1.07E+06 10 15 2Po 8 2De 9 2 6 2425 7.975E+02 7.978E+02 2.39E-01 5.08E-08 1.78E+01 5.26E-04 1 16 2Se 1 2Fo10 2 8 1.14 0.000E+00 7.979E+02 7.09E-08 2.20E+09 0.00E+00 0.00E+00 3 16 2Se 2 2Fo10 2 8 5.67 6.373E+02 7.979E+02 1.73E-04 7.16E+07 0.00E+00 0.00E+00 6 16 2Se 4 2Fo10 2 8 21.77 7.560E+02 7.979E+02 1.81E-02 6.15E+05 0.00E+00 0.00E+00 7 16 2De 6 2Fo10 4 8 22.12 7.567E+02 7.979E+02 5.07E-03 1.54E+05 7.16E+00 2.52E+06 11 16 2Se 7 2Fo10 2 8 2188 7.975E+02 7.979E+02 9.62E-02 3.15E-08 0.00E+00 0.00E+00 13 16 2De 9 2Fo10 4 8 6333 7.977E+02 7.979E+02 6.56E-02 1.26E-11 1.77E+01 3.23E-06 Number of transitions: E3 = 16, M2 = 8, Total E3+M2 = 24 Total number of lines of M2/E3 transitions = 16 ***************************************************************************** 8) Forbidden E2 and M1 transitions in Breit-Pauli approximation ------------------------------------------------------------------------ (ignore the negative signs, for internal purpose, in linestrengths S): Explanantion: ------------- Ni, Nj -> energy level number in Table ii SLpC -> symmetry SLpi of configuration C gi,gj -> statistical weight factors of initial and final states wl = Transition wavelengths Ei,Ej -> level energies of initial and final state SE2, SM1 -> line strengths for E2, M1 transitions AE2, AM1 -> radiative decay rates for E2, M1 transitions ---------------------------------------------------------- Forbidden quad E2 and dipoe M1 transitions in Breit-Pauli approximation: 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 1.43 0.000E+00 6.373E+02 0.00E+00 0.00E+00 2.45E-04 1.13E+09 2 4 2Po 3 2Po 3 2 4 382.48 6.373E+02 6.396E+02 6.55E-04 3.36E+01 1.32E+00 1.59E+05 2 5 2Po 3 2Po 5 2 2 7.67 6.373E+02 7.560E+02 0.00E+00 0.00E+00 6.99E-06 2.09E+05 4 5 2Po 3 2Po 5 4 2 7.83 6.396E+02 7.560E+02 4.92E-04 1.40E+10 2.06E-04 5.79E+06 1 6 2Se 1 2Se 4 2 2 1.21 0.000E+00 7.560E+02 0.00E+00 0.00E+00 7.68E-05 5.91E+08 3 6 2Se 2 2Se 4 2 2 7.68 6.373E+02 7.560E+02 0.00E+00 0.00E+00 2.65E-05 7.90E+05 1 7 2Se 1 2De 6 2 4 1.20 0.000E+00 7.567E+02 2.36E-06 3.92E+11 1.89E-06 7.29E+06 3 7 2Se 2 2De 6 2 4 7.63 6.373E+02 7.567E+02 1.96E-03 3.17E+10 6.07E-06 9.20E+04 6 7 2Se 4 2De 6 2 4 1361 7.560E+02 7.567E+02 1.50E-02 1.35E+00 2.36E-07 6.30E-04 2 8 2Po 3 2Po 5 2 4 7.63 6.373E+02 7.567E+02 4.30E-04 6.98E+09 8.32E-05 1.26E+06 4 8 2Po 3 2Po 5 4 4 7.79 6.396E+02 7.567E+02 4.77E-04 7.01E+09 1.06E-04 1.51E+06 5 8 2Po 5 2Po 5 2 4 1329 7.560E+02 7.567E+02 2.39E-02 2.41E+00 1.33E+00 3.81E+03 1 9 2Se 1 2De 6 2 6 1.20 0.000E+00 7.569E+02 3.53E-06 3.90E+11 0.00E+00 0.00E+00 3 9 2Se 2 2De 6 2 6 7.62 6.373E+02 7.569E+02 2.93E-03 3.20E+10 0.00E+00 0.00E+00 6 9 2Se 4 2De 6 2 6 1009 7.560E+02 7.569E+02 2.27E-02 6.07E+00 0.00E+00 0.00E+00 7 9 2De 6 2De 6 4 6 3902 7.567E+02 7.569E+02 5.07E-03 1.57E-03 2.39E+00 1.81E+02 2 10 2Po 3 2Po 8 2 2 5.69 6.373E+02 7.975E+02 0.00E+00 0.00E+00 1.89E-06 1.38E+05 4 10 2Po 3 2Po 8 4 2 5.77 6.396E+02 7.975E+02 3.60E-05 4.71E+09 4.76E-05 3.33E+06 5 10 2Po 5 2Po 8 2 2 21.98 7.560E+02 7.975E+02 0.00E+00 0.00E+00 2.01E-06 2.55E+03 8 10 2Po 5 2Po 8 4 2 22.35 7.567E+02 7.975E+02 9.78E-03 1.47E+09 1.76E-04 2.13E+05 1 11 2Se 1 2Se 7 2 2 1.14 0.000E+00 7.975E+02 0.00E+00 0.00E+00 8.66E-05 7.83E+08 3 11 2Se 2 2Se 7 2 2 5.69 6.373E+02 7.975E+02 0.00E+00 0.00E+00 1.11E-05 8.13E+05 6 11 2Se 4 2Se 7 2 2 21.99 7.560E+02 7.975E+02 0.00E+00 0.00E+00 6.22E-06 7.90E+03 7 11 2De 6 2Se 7 4 2 22.35 7.567E+02 7.975E+02 1.53E-03 2.31E+08 1.34E-09 1.61E+00 9 11 2De 6 2Se 7 6 2 22.48 7.569E+02 7.975E+02 2.48E-03 3.63E+08 0.00E+00 0.00E+00 2 12 2Po 3 2Po 8 2 4 5.68 6.373E+02 7.977E+02 2.11E-05 1.50E+09 1.47E-05 5.42E+05 4 12 2Po 3 2Po 8 4 4 5.76 6.396E+02 7.977E+02 3.73E-05 2.46E+09 3.51E-05 1.24E+06 5 12 2Po 5 2Po 8 2 4 21.84 7.560E+02 7.977E+02 8.45E-03 7.15E+08 1.14E-04 7.36E+04 8 12 2Po 5 2Po 8 4 4 22.20 7.567E+02 7.977E+02 9.49E-03 7.39E+08 3.13E-05 1.93E+04 10 12 2Po 8 2Po 8 2 4 3282 7.975E+02 7.977E+02 2.74E-01 3.02E-01 1.33E+00 2.54E+02 1 13 2Se 1 2De 9 2 4 1.14 0.000E+00 7.977E+02 2.03E-06 4.39E+11 1.78E-07 8.06E+05 3 13 2Se 2 2De 9 2 4 5.68 6.373E+02 7.977E+02 3.32E-05 2.36E+09 1.74E-06 6.41E+04 6 13 2Se 4 2De 9 2 4 21.84 7.560E+02 7.977E+02 2.69E-02 2.28E+09 5.69E-07 3.68E+02 7 13 2De 6 2De 9 4 4 22.20 7.567E+02 7.977E+02 6.20E-03 4.83E+08 1.25E-05 7.68E+03 9 13 2De 6 2De 9 6 4 22.33 7.569E+02 7.977E+02 2.75E-03 2.08E+08 4.07E-05 2.46E+04 11 13 2Se 7 2De 9 2 4 3343 7.975E+02 7.977E+02 2.20E-01 2.21E-01 1.52E-07 2.74E-05 2 14 2Po 3 2Fo10 2 6 5.67 6.373E+02 7.978E+02 6.30E-04 3.00E+10 0.00E+00 0.00E+00 4 14 2Po 3 2Fo10 4 6 5.76 6.396E+02 7.978E+02 1.86E-04 8.23E+09 1.63E-06 3.82E+04 5 14 2Po 5 2Fo10 2 6 21.79 7.560E+02 7.978E+02 4.99E-02 2.84E+09 0.00E+00 0.00E+00 8 14 2Po 5 2Fo10 4 6 22.15 7.567E+02 7.978E+02 1.47E-02 7.74E+08 2.51E-06 1.04E+03 10 14 2Po 8 2Fo10 2 6 2439 7.975E+02 7.978E+02 1.55E-01 5.01E-01 0.00E+00 0.00E+00 12 14 2Po 8 2Fo10 4 6 9505 7.977E+02 7.978E+02 4.37E-02 1.58E-04 6.05E-08 3.17E-07 1 15 2Se 1 2De 9 2 6 1.14 0.000E+00 7.978E+02 3.07E-06 4.42E+11 0.00E+00 0.00E+00 3 15 2Se 2 2De 9 2 6 5.68 6.373E+02 7.978E+02 5.22E-05 2.48E+09 0.00E+00 0.00E+00 6 15 2Se 4 2De 9 2 6 21.79 7.560E+02 7.978E+02 4.02E-02 2.29E+09 0.00E+00 0.00E+00 7 15 2De 6 2De 9 4 6 22.15 7.567E+02 7.978E+02 2.63E-03 1.38E+08 1.25E-05 5.16E+03 9 15 2De 6 2De 9 6 6 22.27 7.569E+02 7.978E+02 1.09E-02 5.58E+08 6.29E-05 2.56E+04 11 15 2Se 7 2De 9 2 6 2465 7.975E+02 7.978E+02 3.30E-01 1.01E+00 0.00E+00 0.00E+00 13 15 2De 9 2De 9 4 6 9389 7.977E+02 7.978E+02 8.23E-02 3.16E-04 2.40E+00 1.30E+01 4 16 2Po 3 2Fo10 4 8 5.76 6.396E+02 7.979E+02 1.12E-03 3.71E+10 0.00E+00 0.00E+00 8 16 2Po 5 2Fo10 4 8 22.12 7.567E+02 7.979E+02 8.84E-02 3.50E+09 0.00E+00 0.00E+00 12 16 2Po 8 2Fo10 4 8 6288 7.977E+02 7.979E+02 2.62E-01 5.60E-03 0.00E+00 0.00E+00 14 16 2Fo10 2Fo10 6 8 18582 7.978E+02 7.979E+02 2.79E-02 2.65E-06 3.42E+00 1.80E+00 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 = = 48 + 107 = 155