*************************** 786 ******************************************* Ref. "K$_{\alpha}$ Transition Probabilities for Platinum and Uranium Ions for possible X-ray Biomedical Applications", S.N. Nahar, A.K. Pradhan, S. Lim, Can. J. Phys. 89, 483-494 (2011, doi: 10.1139/p11-020) ************************************************************************** Pt77+: 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: Pt77+ + h\nu <-> Pt77+* 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 = 78, 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) LS term energies ------------------- LS energies: i SLP E(Rel,Ry) cfg# 1 2Se 0.000000 1 2 2Po 4563.032826 3 3 2Se 4563.035980 2 4 2De 5408.030500 6 5 2Se 5408.031409 4 6 2Po 5408.031892 5 7 2Fo 5703.780370 10 8 2De 5703.780555 9 9 2Po 5703.781080 8 10 2Se 5703.781130 7 Number of first LS terms optimized = 10 ************************************************************************* 3) 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 4563.0328 2.320E+16 4.16E-01 4.16E-01 0.0E+00 1 2Se: 1 6 2Po: 5 0.0000 5408.0319 6.194E+15 7.91E-02 7.91E-02 0.0E+00 1 2Se: 1 9 2Po: 8 0.0000 5703.7811 2.525E+15 2.90E-02 2.90E-02 1.7E-02 2 2Po: 3 3 2Se: 2 4563.0328 4563.0360 3.729E-01 0.00E+00 0.00E+00 0.0E+00 2 2Po: 3 4 2De: 6 4563.0328 5408.0305 2.394E+15 6.96E-01 6.96E-01 4.8E-04 2 2Po: 3 5 2Se: 4 4563.0328 5408.0314 2.338E+14 1.36E-02 1.36E-02 2.5E-02 2 2Po: 3 8 2De: 9 4563.0328 5703.7806 7.638E+14 1.22E-01 1.22E-01 0.0E+00 2 2Po: 3 10 2Se: 7 4563.0328 5703.7811 9.548E+13 3.04E-03 3.05E-03 1.6E-01 3 2Se: 2 6 2Po: 5 4563.0360 5408.0319 8.313E+14 4.35E-01 4.35E-01 1.1E-03 3 2Se: 2 9 2Po: 8 4563.0360 5703.7811 3.580E+14 1.03E-01 1.03E-01 4.9E-03 4 2De: 6 6 2Po: 5 5408.0305 5408.0319 8.001E-02 0.00E+00 0.00E+00 0.0E+00 4 2De: 6 7 2Fo:10 5408.0305 5703.7804 5.106E+14 1.02E+00 1.02E+00 0.0E+00 4 2De: 6 9 2Po: 8 5408.0305 5703.7811 1.287E+13 1.10E-02 1.10E-02 0.0E+00 5 2Se: 4 9 2Po: 8 5408.0314 5703.7811 1.135E+14 4.85E-01 4.85E-01 2.1E-03 6 2Po: 5 8 2De: 9 5408.0319 5703.7806 2.606E+14 6.18E-01 6.18E-01 5.4E-04 6 2Po: 5 10 2Se: 7 5408.0319 5703.7811 6.797E+13 3.23E-02 3.23E-02 0.0E+00 8 2De: 9 9 2Po: 8 5703.7806 5703.7811 1.835E-02 0.00E+00 0.00E+00 0.0E+00 LS transitions: Number of oscillator strengths = 17 ****************************************************************************** 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 539294261.0 4.91441E+03 3 2Se( 2) 2 541242051.0 4.93216E+03 4 2Po( 3) 4 553902536.0 5.04753E+03 5 2Po( 5) 2 644662144.0 5.87459E+03 6 2Se( 4) 2 645139451.0 5.87894E+03 7 2De( 6) 4 648059060.0 5.90555E+03 8 2Po( 5) 4 648130130.0 5.90620E+03 9 2De( 6) 6 649436692.0 5.91810E+03 10 2Po( 8) 2 680461002.0 6.20082E+03 11 2Se( 7) 2 680613351.0 6.20221E+03 12 2De( 9) 4 681565074.0 6.21088E+03 13 2Po( 8) 4 681598334.0 6.21118E+03 14 2Fo(10) 6 682076031.0 6.21553E+03 15 2De( 9) 6 682085867.0 6.21562E+03 16 2Fo(10) 8 682357665.0 6.21810E+03 ****************************************************************************** 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 0.18 0.00 4914.41 9.94E-02 1.214E-04 1.93E+16 2 3 2Po 3 2Se 2 2 2 51.34 4914.41 4932.16 7.77E-03 2.625E-03 1.96E+10 1 4 2Se 1 2Po 3 2 4 0.18 0.00 5047.53 1.96E-01 2.328E-04 2.00E+16 3 4 2Se 2 2Po 3 2 4 7.90 4932.16 5047.53 1.08E-01 5.636E-03 5.79E+12 1 5 2Se 1 2Po 5 2 2 0.15 0.00 5874.59 8.14E-03 8.309E-06 2.26E+15 3 5 2Se 2 2Po 5 2 2 0.97 4932.16 5874.59 1.13E-01 7.173E-04 8.04E+14 2 6 2Po 3 2Se 4 2 2 0.94 4914.41 5878.94 2.52E-03 1.565E-05 1.88E+13 4 6 2Po 3 2Se 4 4 2 1.10 5047.53 5878.94 1.83E-02 2.635E-04 2.03E+14 5 6 2Po 5 2Se 4 2 2 209.51 5874.59 5878.94 1.22E-02 1.688E-02 1.86E+09 2 7 2Po 3 2De 6 2 4 0.92 4914.41 5905.55 5.51E-01 3.337E-03 2.18E+15 4 7 2Po 3 2De 6 4 4 1.06 5047.53 5905.55 6.45E-02 9.023E-04 3.82E+14 5 7 2Po 5 2De 6 2 4 29.44 5874.59 5905.55 1.15E-01 2.229E-02 4.43E+11 1 8 2Se 1 2Po 5 2 4 0.15 0.00 5906.20 2.52E-02 2.557E-05 3.53E+15 3 8 2Se 2 2Po 5 2 4 0.94 4932.16 5906.20 1.70E-01 1.050E-03 6.49E+14 6 8 2Se 4 2Po 5 2 4 33.44 5878.94 5906.20 1.58E-01 3.473E-02 4.71E+11 7 8 2De 6 2Po 5 4 4 1407 5905.55 5906.20 2.30E-04 4.265E-03 7.75E+05 4 9 2Po 3 2De 6 4 6 1.05 5047.53 5918.10 5.81E-01 8.002E-03 2.36E+15 8 9 2Po 5 2De 6 4 6 76.54 5906.20 5918.10 3.93E-02 3.958E-02 2.98E+10 1 10 2Se 1 2Po 8 2 2 0.15 0.00 6200.82 1.26E-04 1.223E-07 3.90E+13 3 10 2Se 2 2Po 8 2 2 0.72 4932.16 6200.82 1.09E-02 5.144E-05 1.41E+14 6 10 2Se 4 2Po 8 2 2 2.83 5878.94 6200.82 1.15E-01 2.140E-03 9.56E+13 7 10 2De 6 2Po 8 4 2 3.09 5905.55 6200.82 8.61E-03 3.500E-04 1.21E+13 2 11 2Po 3 2Se 7 2 2 0.71 4914.41 6202.21 2.47E-03 1.152E-05 3.29E+13 4 11 2Po 3 2Se 7 4 2 0.79 5047.53 6202.21 1.01E-03 1.045E-05 2.15E+13 5 11 2Po 5 2Se 7 2 2 2.78 5874.59 6202.21 8.06E-03 1.477E-04 6.95E+12 8 11 2Po 5 2Se 7 4 2 3.08 5906.20 6202.21 3.36E-02 1.363E-03 4.73E+13 10 11 2Po 8 2Se 7 2 2 656.39 6200.82 6202.21 1.45E-02 6.265E-02 2.24E+08 2 12 2Po 3 2De 9 2 4 0.70 4914.41 6210.88 7.64E-02 3.536E-04 5.16E+14 4 12 2Po 3 2De 9 4 4 0.78 5047.53 6210.88 8.80E-03 9.075E-05 9.56E+13 5 12 2Po 5 2De 9 2 4 2.71 5874.59 6210.88 4.07E-01 7.256E-03 1.85E+14 8 12 2Po 5 2De 9 4 4 2.99 5906.20 6210.88 5.52E-02 2.173E-03 4.11E+13 10 12 2Po 8 2De 9 2 4 90.57 6200.82 6210.88 1.71E-01 1.018E-01 6.94E+10 1 13 2Se 1 2Po 8 2 4 0.15 0.00 6211.18 1.44E-03 1.392E-06 2.23E+14 3 13 2Se 2 2Po 8 2 4 0.71 4932.16 6211.18 2.16E-02 1.012E-04 1.42E+14 6 13 2Se 4 2Po 8 2 4 2.74 5878.94 6211.18 1.70E-01 3.065E-03 7.52E+13 7 13 2De 6 2Po 8 4 4 2.98 5905.55 6211.18 7.54E-04 2.962E-05 5.66E+11 9 13 2De 6 2Po 8 6 4 3.11 5918.10 6211.18 1.07E-02 6.576E-04 1.11E+13 11 13 2Se 7 2Po 8 2 4 101.52 6202.21 6211.18 1.86E-01 1.242E-01 6.01E+10 12 13 2De 9 2Po 8 4 4 3006 6210.88 6211.18 4.95E-04 1.961E-02 3.66E+05 7 14 2De 6 2Fo10 4 6 2.94 5905.55 6215.53 9.38E-01 3.632E-02 4.83E+14 9 14 2De 6 2Fo10 6 6 3.06 5918.10 6215.53 4.61E-02 2.792E-03 3.28E+13 12 14 2De 9 2Fo10 4 6 195.71 6210.88 6215.53 4.05E-02 1.044E-01 4.70E+09 4 15 2Po 3 2De 9 4 6 0.78 5047.53 6215.62 9.10E-02 9.345E-04 6.65E+14 8 15 2Po 5 2De 9 4 6 2.94 5906.20 6215.62 4.73E-01 1.835E-02 2.43E+14 13 15 2Po 8 2De 9 4 6 205.11 6211.18 6215.62 6.52E-02 1.761E-01 6.89E+09 14 15 2Fo10 2De 9 6 6 10167 6215.53 6215.62 3.61E-05 7.258E-03 2.33E+03 9 16 2De 6 2Fo10 6 8 3.04 5918.10 6218.10 9.31E-01 5.583E-02 5.04E+14 15 16 2De 9 2Fo10 6 8 367.92 6215.62 6218.10 2.00E-02 1.452E-01 7.38E+08 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 0.91 4.914E+03 5.918E+03 1.97E-07 4.05E+10 8.42E-02 3.39E+11 5 9 2Po 5 2De 6 2 6 20.94 5.875E+03 5.918E+03 1.11E-05 6.56E+02 5.85E-01 3.61E+05 9 10 2De 6 2Po 8 6 2 3.22 5.918E+03 6.201E+03 7.70E-06 6.69E+08 1.70E-02 3.64E+08 1 14 2Se 1 2Fo10 2 6 0.15 0.000E+00 6.216E+03 1.04E-08 7.52E+14 0.00E+00 0.00E+00 3 14 2Se 2 2Fo10 2 6 0.71 4.932E+03 6.216E+03 4.14E-07 4.77E+11 0.00E+00 0.00E+00 6 14 2Se 4 2Fo10 2 6 2.71 5.879E+03 6.216E+03 2.49E-05 2.45E+09 0.00E+00 0.00E+00 11 14 2Se 7 2Fo10 2 6 68.37 6.202E+03 6.216E+03 2.02E-04 3.02E+00 0.00E+00 0.00E+00 2 15 2Po 3 2De 9 2 6 0.70 4.914E+03 6.216E+03 3.83E-07 4.86E+11 1.03E-02 1.52E+11 5 15 2Po 5 2De 9 2 6 2.67 5.875E+03 6.216E+03 1.40E-05 1.51E+09 1.71E-01 3.13E+09 10 15 2Po 8 2De 9 2 6 61.54 6.201E+03 6.216E+03 6.53E-04 2.05E+01 2.60E+00 7.31E+03 1 16 2Se 1 2Fo10 2 8 0.15 0.000E+00 6.218E+03 1.39E-08 7.54E+14 0.00E+00 0.00E+00 3 16 2Se 2 2Fo10 2 8 0.71 4.932E+03 6.218E+03 5.53E-07 4.84E+11 0.00E+00 0.00E+00 6 16 2Se 4 2Fo10 2 8 2.69 5.879E+03 6.218E+03 3.32E-05 2.58E+09 0.00E+00 0.00E+00 7 16 2De 6 2Fo10 4 8 2.92 5.906E+03 6.218E+03 1.03E-05 4.52E+08 8.85E-01 7.83E+09 11 16 2Se 7 2Fo10 2 8 57.33 6.202E+03 6.218E+03 2.69E-04 1.04E+01 0.00E+00 0.00E+00 12 16 2De 9 2Fo10 4 8 126.17 6.211E+03 6.218E+03 1.76E-04 2.72E-02 2.54E+00 1.48E+02 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 0.18 0.000E+00 4.932E+03 0.00E+00 0.00E+00 1.83E-02 3.91E+13 2 4 2Po 3 2Po 3 2 4 6.84 4.914E+03 5.048E+03 1.04E-05 2.90E+08 1.24E+00 2.61E+10 2 5 2Po 3 2Po 5 2 2 0.95 4.914E+03 5.875E+03 0.00E+00 0.00E+00 2.61E-04 4.12E+09 4 5 2Po 3 2Po 5 4 2 1.10 5.048E+03 5.875E+03 8.90E-06 4.60E+12 9.22E-03 9.30E+10 1 6 2Se 1 2Se 4 2 2 0.15 0.000E+00 5.879E+03 0.00E+00 0.00E+00 1.50E-02 5.45E+13 3 6 2Se 2 2Se 4 2 2 0.96 4.932E+03 5.879E+03 0.00E+00 0.00E+00 1.05E-03 1.59E+10 1 7 2Se 1 2De 6 2 4 0.15 0.000E+00 5.906E+03 6.71E-08 3.22E+14 1.25E-05 2.29E+10 3 7 2Se 2 2De 6 2 4 0.94 4.932E+03 5.906E+03 2.55E-05 1.49E+13 3.48E-04 2.86E+09 6 7 2Se 4 2De 6 2 4 34.25 5.879E+03 5.906E+03 2.66E-04 2.37E+06 2.23E-05 3.75E+03 2 8 2Po 3 2Po 5 2 4 0.92 4.914E+03 5.906E+03 2.99E-06 1.92E+12 3.00E-03 2.61E+10 4 8 2Po 3 2Po 5 4 4 1.06 5.048E+03 5.906E+03 7.58E-06 2.36E+12 5.82E-03 3.29E+10 5 8 2Po 5 2Po 5 2 4 28.84 5.875E+03 5.906E+03 4.08E-04 8.59E+06 1.30E+00 3.65E+08 1 9 2Se 1 2De 6 2 6 0.15 0.000E+00 5.918E+03 9.10E-08 2.94E+14 0.00E+00 0.00E+00 3 9 2Se 2 2De 6 2 6 0.92 4.932E+03 5.918E+03 3.82E-05 1.59E+13 0.00E+00 0.00E+00 6 9 2Se 4 2De 6 2 6 23.27 5.879E+03 5.918E+03 4.19E-04 1.72E+07 0.00E+00 0.00E+00 7 9 2De 6 2De 6 4 6 72.59 5.906E+03 5.918E+03 9.03E-05 1.26E+04 2.34E+00 2.75E+07 2 10 2Po 3 2Po 8 2 2 0.71 4.914E+03 6.201E+03 0.00E+00 0.00E+00 1.04E-05 3.94E+08 4 10 2Po 3 2Po 8 4 2 0.79 5.048E+03 6.201E+03 2.01E-08 5.48E+10 1.74E-03 4.76E+10 5 10 2Po 5 2Po 8 2 2 2.79 5.875E+03 6.201E+03 0.00E+00 0.00E+00 5.86E-05 3.62E+07 8 10 2Po 5 2Po 8 4 2 3.09 5.906E+03 6.201E+03 1.60E-04 4.76E+11 5.36E-03 2.44E+09 1 11 2Se 1 2Se 7 2 2 0.15 0.000E+00 6.202E+03 0.00E+00 0.00E+00 7.97E-02 3.39E+14 3 11 2Se 2 2Se 7 2 2 0.72 4.932E+03 6.202E+03 0.00E+00 0.00E+00 1.32E-03 4.82E+10 6 11 2Se 4 2Se 7 2 2 2.82 5.879E+03 6.202E+03 0.00E+00 0.00E+00 1.67E-04 1.00E+08 7 11 2De 6 2Se 7 4 2 3.07 5.906E+03 6.202E+03 1.79E-05 5.51E+10 2.63E-07 1.23E+05 9 11 2De 6 2Se 7 6 2 3.21 5.918E+03 6.202E+03 4.89E-05 1.21E+11 0.00E+00 0.00E+00 1 12 2Se 1 2De 9 2 4 0.15 0.000E+00 6.211E+03 3.23E-07 2.00E+15 9.53E-04 2.03E+12 3 12 2Se 2 2De 9 2 4 0.71 4.932E+03 6.211E+03 3.96E-09 9.04E+09 1.56E-04 2.91E+09 6 12 2Se 4 2De 9 2 4 2.75 5.879E+03 6.211E+03 3.35E-04 9.03E+11 2.41E-05 7.86E+06 7 12 2De 6 2De 9 4 4 2.98 5.906E+03 6.211E+03 8.67E-05 1.54E+11 6.01E-04 1.52E+08 9 12 2De 6 2De 9 6 4 3.11 5.918E+03 6.211E+03 4.88E-05 7.02E+10 1.98E-03 4.43E+08 11 12 2Se 7 2De 9 2 4 105.07 6.202E+03 6.211E+03 4.43E-03 1.45E+05 1.39E-05 8.10E+01 2 13 2Po 3 2Po 8 2 4 0.70 4.914E+03 6.211E+03 1.43E-06 3.51E+12 1.12E-04 2.19E+09 4 13 2Po 3 2Po 8 4 4 0.78 5.048E+03 6.211E+03 4.42E-08 6.30E+10 2.47E-03 3.47E+10 5 13 2Po 5 2Po 8 2 4 2.71 5.875E+03 6.211E+03 5.63E-05 1.63E+11 2.99E-03 1.02E+09 8 13 2Po 5 2Po 8 4 4 2.99 5.906E+03 6.211E+03 1.34E-04 2.37E+11 1.44E-03 3.65E+08 10 13 2Po 8 2Po 8 2 4 87.93 6.201E+03 6.211E+03 5.42E-03 4.33E+05 1.32E+00 1.31E+07 2 14 2Po 3 2Fo10 2 6 0.70 4.914E+03 6.216E+03 9.75E-06 1.62E+13 0.00E+00 0.00E+00 4 14 2Po 3 2Fo10 4 6 0.78 5.048E+03 6.216E+03 3.38E-06 3.27E+12 7.48E-05 7.08E+08 5 14 2Po 5 2Fo10 2 6 2.67 5.875E+03 6.216E+03 7.09E-04 1.46E+12 0.00E+00 0.00E+00 8 14 2Po 5 2Fo10 4 6 2.95 5.906E+03 6.216E+03 2.49E-04 3.15E+11 1.39E-04 2.44E+07 10 14 2Po 8 2Fo10 2 6 61.92 6.201E+03 6.216E+03 3.20E-03 9.86E+05 0.00E+00 0.00E+00 13 14 2Po 8 2Fo10 4 6 209.34 6.211E+03 6.216E+03 8.68E-04 6.05E+02 4.75E-06 2.33E+00 1 15 2Se 1 2De 9 2 6 0.15 0.000E+00 6.216E+03 4.94E-07 2.04E+15 0.00E+00 0.00E+00 3 15 2Se 2 2De 9 2 6 0.71 4.932E+03 6.216E+03 3.61E-09 5.60E+09 0.00E+00 0.00E+00 6 15 2Se 4 2De 9 2 6 2.71 5.879E+03 6.216E+03 4.83E-04 9.31E+11 0.00E+00 0.00E+00 7 15 2De 6 2De 9 4 6 2.94 5.906E+03 6.216E+03 3.47E-05 4.43E+10 5.56E-04 9.84E+07 9 15 2De 6 2De 9 6 6 3.06 5.918E+03 6.216E+03 1.84E-04 1.91E+11 3.31E-03 5.17E+08 11 15 2Se 7 2De 9 2 6 67.91 6.202E+03 6.216E+03 6.62E-03 1.28E+06 0.00E+00 0.00E+00 12 15 2De 9 2De 9 4 6 192.01 6.211E+03 6.216E+03 1.60E-03 1.72E+03 2.37E+00 1.51E+06 4 16 2Po 3 2Fo10 4 8 0.78 5.048E+03 6.218E+03 2.02E-05 1.49E+13 0.00E+00 0.00E+00 8 16 2Po 5 2Fo10 4 8 2.92 5.906E+03 6.218E+03 1.50E-03 1.48E+12 0.00E+00 0.00E+00 13 16 2Po 8 2Fo10 4 8 131.69 6.211E+03 6.218E+03 5.21E-03 2.76E+04 0.00E+00 0.00E+00 14 16 2Fo10 2Fo10 6 8 355.07 6.216E+03 6.218E+03 5.34E-04 1.99E+01 3.39E+00 2.55E+05 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