*************************** 786 ******************************************* Ref. "Oscillator strengths and radiative transition rates for Kalpha lines in gold X-ray spectra: 1s-2p transitions", Sultana N. Nahar, Anil K. Pradhan, C. Sur, J. Quant. Spec. Rad. Transfer 109, 1951-1959 (2008) ************************************************************************** AU78+: 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: Au78+ + h\nu <-> Au78+* 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 = 79, 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 4680.783691 3 3 2Se 4680.786621 2 4 2De 5547.586914 6 5 2Se 5547.587891 4 6 2Po 5547.606934 5 7 2Fo 5850.968750 10 8 2Po 5850.969238 8 9 2Se 5850.969727 7 10 2De 5850.985352 9 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 4680.7837 2.441E+16 4.16E-01 4.16E-01 0.0E+00 1 2Se: 1 6 2Po: 5 0.0000 5547.6069 6.519E+15 7.91E-02 7.91E-02 1.3E-02 1 2Se: 1 8 2Po: 8 0.0000 5850.9692 2.657E+15 2.90E-02 2.90E-02 3.4E-02 2 2Po: 3 3 2Se: 2 4680.7837 4680.7866 2.516E-01 0.00E+00 0.00E+00 0.0E+00 2 2Po: 3 4 2De: 6 4680.7837 5547.5869 2.519E+15 6.96E-01 6.96E-01 4.8E-04 2 2Po: 3 5 2Se: 4 4680.7837 5547.5879 2.460E+14 1.36E-02 1.36E-02 2.5E-02 2 2Po: 3 9 2Se: 7 4680.7837 5850.9697 1.005E+14 3.04E-03 3.05E-03 1.6E-01 2 2Po: 3 10 2De: 9 4680.7837 5850.9854 8.040E+14 1.22E-01 1.22E-01 1.4E-03 3 2Se: 2 6 2Po: 5 4680.7866 5547.6069 8.750E+14 4.35E-01 4.35E-01 1.1E-03 3 2Se: 2 8 2Po: 8 4680.7866 5850.9692 3.766E+14 1.03E-01 1.03E-01 9.7E-03 4 2De: 6 6 2Po: 5 5547.5869 5547.6069 2.386E+02 4.00E-05 0.00E+00 1.0E+02 4 2De: 6 7 2Fo:10 5547.5869 5850.9688 5.373E+14 1.02E+00 1.02E+00 4.7E-06 4 2De: 6 8 2Po: 8 5547.5869 5850.9692 1.356E+13 1.10E-02 1.10E-02 4.5E-02 5 2Se: 4 6 2Po: 5 5547.5879 5547.6069 1.644E+02 1.70E-04 2.00E-04 8.1E+00 5 2Se: 4 8 2Po: 8 5547.5879 5850.9692 1.195E+14 4.85E-01 4.85E-01 1.9E-02 6 2Po: 5 9 2Se: 7 5547.6069 5850.9697 7.136E+13 3.22E-02 3.22E-02 1.1E-01 6 2Po: 5 10 2De: 9 5547.6069 5850.9854 2.741E+14 6.18E-01 6.18E-01 3.7E-02 7 2Fo:10 10 2De: 9 5850.9688 5850.9854 2.883E+02 9.00E-05 7.14E-06 8.5E+01 8 2Po: 8 10 2De: 9 5850.9692 5850.9854 2.866E+02 2.40E-04 6.67E-05 5.7E+01 LS transitions: Number of oscillator strengths = 19 ****************************************************************************** 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 554268032.0 5.05086E+03 3 2Se( 2) 2 556372352.0 5.07004E+03 4 2Po( 3) 4 569666496.0 5.19118E+03 5 2Po( 5) 2 662735424.0 6.03929E+03 6 2Se( 4) 2 663245952.0 6.04394E+03 7 2De( 6) 4 666291968.0 6.07170E+03 8 2Po( 5) 4 666370368.0 6.07241E+03 9 2De( 6) 6 667742784.0 6.08492E+03 10 2Po( 8) 2 699544064.0 6.37471E+03 11 2Se( 7) 2 699705728.0 6.37619E+03 12 2De( 9) 4 700694656.0 6.38520E+03 13 2Po( 8) 4 700729216.0 6.38551E+03 14 2Fo(10) 6 701229504.0 6.39007E+03 15 2De( 9) 6 701241728.0 6.39019E+03 16 2Fo(10) 8 701525888.0 6.39277E+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 5050.86 9.84E-02 1.169E-04 2.02E+16 2 3 2Po 3 2Se 2 2 2 47.52 5050.86 5070.04 8.16E-03 2.553E-03 2.41E+10 1 4 2Se 1 2Po 3 2 4 0.18 0.00 5191.18 1.94E-01 2.241E-04 2.10E+16 3 4 2Se 2 2Po 3 2 4 7.52 5070.04 5191.18 1.11E-01 5.489E-03 6.53E+12 1 5 2Se 1 2Po 5 2 2 0.15 0.00 6039.29 7.82E-03 7.766E-06 2.29E+15 3 5 2Se 2 2Po 5 2 2 0.94 5070.04 6039.29 1.12E-01 6.935E-04 8.45E+14 2 6 2Po 3 2Se 4 2 2 0.92 5050.86 6043.94 2.32E-03 1.403E-05 1.84E+13 4 6 2Po 3 2Se 4 4 2 1.07 5191.18 6043.94 1.83E-02 2.574E-04 2.14E+14 5 6 2Po 5 2Se 4 2 2 195.86 6039.29 6043.94 1.27E-02 1.644E-02 2.22E+09 2 7 2Po 3 2De 6 2 4 0.89 5050.86 6071.70 5.48E-01 3.220E-03 2.29E+15 4 7 2Po 3 2De 6 4 4 1.03 5191.18 6071.70 6.44E-02 8.774E-04 4.01E+14 5 7 2Po 5 2De 6 2 4 28.12 6039.29 6071.70 1.17E-01 2.174E-02 4.95E+11 1 8 2Se 1 2Po 5 2 4 0.15 0.00 6072.41 2.46E-02 2.429E-05 3.64E+15 3 8 2Se 2 2Po 5 2 4 0.91 5070.04 6072.41 1.68E-01 1.007E-03 6.79E+14 6 8 2Se 4 2Po 5 2 4 32.01 6043.94 6072.41 1.61E-01 3.384E-02 5.23E+11 7 8 2De 6 2Po 5 4 4 1276 6071.70 6072.41 2.47E-04 4.156E-03 1.01E+06 4 9 2Po 3 2De 6 4 6 1.02 5191.18 6084.92 5.79E-01 7.779E-03 2.48E+15 8 9 2Po 5 2De 6 4 6 72.86 6072.41 6084.92 4.02E-02 3.859E-02 3.37E+10 1 10 2Se 1 2Po 8 2 2 0.14 0.00 6374.71 8.69E-05 8.184E-08 2.84E+13 3 10 2Se 2 2Po 8 2 2 0.70 5070.04 6374.71 1.05E-02 4.844E-05 1.44E+14 6 10 2Se 4 2Po 8 2 2 2.76 6043.94 6374.71 1.14E-01 2.070E-03 1.00E+14 7 10 2De 6 2Po 8 4 2 3.01 6071.70 6374.71 8.56E-03 3.388E-04 1.26E+13 2 11 2Po 3 2Se 7 2 2 0.69 5050.86 6376.19 2.74E-03 1.240E-05 3.86E+13 4 11 2Po 3 2Se 7 4 2 0.77 5191.18 6376.19 9.63E-04 9.755E-06 2.17E+13 5 11 2Po 5 2Se 7 2 2 2.70 6039.29 6376.19 7.67E-03 1.367E-04 7.00E+12 8 11 2Po 5 2Se 7 4 2 3.00 6072.41 6376.19 3.34E-02 1.321E-03 4.96E+13 10 11 2Po 8 2Se 7 2 2 618.61 6374.71 6376.19 1.50E-02 6.113E-02 2.62E+08 2 12 2Po 3 2De 9 2 4 0.68 5050.86 6385.20 7.54E-02 3.391E-04 5.39E+14 4 12 2Po 3 2De 9 4 4 0.76 5191.18 6385.20 8.72E-03 8.767E-05 9.99E+13 5 12 2Po 5 2De 9 2 4 2.63 6039.29 6385.20 4.02E-01 6.981E-03 1.93E+14 8 12 2Po 5 2De 9 4 4 2.91 6072.41 6385.20 5.50E-02 2.109E-03 4.32E+13 10 12 2Po 8 2De 9 2 4 86.91 6374.71 6385.20 1.74E-01 9.931E-02 7.66E+10 1 13 2Se 1 2Po 8 2 4 0.14 0.00 6385.51 1.26E-03 1.181E-06 2.06E+14 3 13 2Se 2 2Po 8 2 4 0.69 5070.04 6385.51 2.08E-02 9.497E-05 1.45E+14 6 13 2Se 4 2Po 8 2 4 2.67 6043.94 6385.51 1.68E-01 2.943E-03 7.85E+13 7 13 2De 6 2Po 8 4 4 2.90 6071.70 6385.51 7.34E-04 2.806E-05 5.80E+11 9 13 2De 6 2Po 8 6 4 3.03 6084.92 6385.51 1.07E-02 6.408E-04 1.17E+13 11 13 2Se 7 2Po 8 2 4 97.70 6376.19 6385.51 1.88E-01 1.212E-01 6.58E+10 12 13 2De 9 2Po 8 4 4 2894 6385.20 6385.51 5.03E-04 1.920E-02 4.00E+05 7 14 2De 6 2Fo10 4 6 2.86 6071.70 6390.07 9.36E-01 3.528E-02 5.08E+14 9 14 2De 6 2Fo10 6 6 2.99 6084.92 6390.07 4.61E-02 2.718E-03 3.45E+13 12 14 2De 9 2Fo10 4 6 186.98 6385.20 6390.07 4.14E-02 1.019E-01 5.26E+09 4 15 2Po 3 2De 9 4 6 0.76 5191.18 6390.19 9.05E-02 9.061E-04 6.97E+14 8 15 2Po 5 2De 9 4 6 2.87 6072.41 6390.19 4.71E-01 1.778E-02 2.55E+14 13 15 2Po 8 2De 9 4 6 195.12 6385.51 6390.19 6.69E-02 1.718E-01 7.81E+09 14 15 2Fo10 2De 9 6 6 8173 6390.07 6390.19 4.40E-05 7.111E-03 4.38E+03 9 16 2De 6 2Fo10 6 8 2.96 6084.92 6392.77 9.30E-01 5.435E-02 5.31E+14 15 16 2De 9 2Fo10 6 8 351.96 6390.19 6392.77 2.04E-02 1.415E-01 8.22E+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 0.88 5.051E+03 6.085E+03 1.78E-07 4.52E+10 8.12E-02 3.80E+11 5 9 2Po 5 2De 6 2 6 19.97 6.039E+03 6.085E+03 1.02E-05 8.44E+02 5.71E-01 4.46E+05 9 10 2De 6 2Po 8 6 2 3.14 6.085E+03 6.375E+03 7.10E-06 7.35E+08 1.67E-02 4.06E+08 1 14 2Se 1 2Fo10 2 6 0.14 0.000E+00 6.390E+03 1.02E-08 8.89E+14 0.00E+00 0.00E+00 3 14 2Se 2 2Fo10 2 6 0.69 5.070E+03 6.390E+03 3.86E-07 5.42E+11 0.00E+00 0.00E+00 6 14 2Se 4 2Fo10 2 6 2.63 6.044E+03 6.390E+03 2.29E-05 2.73E+09 0.00E+00 0.00E+00 11 14 2Se 7 2Fo10 2 6 65.63 6.376E+03 6.390E+03 1.87E-04 3.74E+00 0.00E+00 0.00E+00 2 15 2Po 3 2De 9 2 6 0.68 5.051E+03 6.390E+03 3.73E-07 5.79E+11 9.93E-03 1.69E+11 5 15 2Po 5 2De 9 2 6 2.60 6.039E+03 6.390E+03 1.26E-05 1.66E+09 1.65E-01 3.46E+09 10 15 2Po 8 2De 9 2 6 58.90 6.375E+03 6.390E+03 6.05E-04 2.58E+01 2.53E+00 8.88E+03 1 16 2Se 1 2Fo10 2 8 0.14 0.000E+00 6.393E+03 1.36E-08 8.92E+14 0.00E+00 0.00E+00 3 16 2Se 2 2Fo10 2 8 0.69 5.070E+03 6.393E+03 5.15E-07 5.49E+11 0.00E+00 0.00E+00 6 16 2Se 4 2Fo10 2 8 2.61 6.044E+03 6.393E+03 3.05E-05 2.89E+09 0.00E+00 0.00E+00 7 16 2De 6 2Fo10 4 8 2.84 6.072E+03 6.393E+03 9.47E-06 5.02E+08 8.60E-01 8.71E+09 11 16 2Se 7 2Fo10 2 8 54.94 6.376E+03 6.393E+03 2.49E-04 1.30E+01 0.00E+00 0.00E+00 12 16 2De 9 2Fo10 4 8 120.31 6.385E+03 6.393E+03 1.63E-04 3.52E-02 2.48E+00 1.84E+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 5.070E+03 0.00E+00 0.00E+00 1.95E-02 4.53E+13 2 4 2Po 3 2Po 3 2 4 6.49 5.051E+03 5.191E+03 9.81E-06 3.57E+08 1.24E+00 3.05E+10 2 5 2Po 3 2Po 5 2 2 0.92 5.051E+03 6.039E+03 0.00E+00 0.00E+00 2.71E-04 4.67E+09 4 5 2Po 3 2Po 5 4 2 1.07 5.191E+03 6.039E+03 8.43E-06 4.95E+12 9.65E-03 1.05E+11 1 6 2Se 1 2Se 4 2 2 0.15 0.000E+00 6.044E+03 0.00E+00 0.00E+00 1.64E-02 6.46E+13 3 6 2Se 2 2Se 4 2 2 0.94 5.070E+03 6.044E+03 0.00E+00 0.00E+00 1.10E-03 1.81E+10 1 7 2Se 1 2De 6 2 4 0.15 0.000E+00 6.072E+03 6.46E-08 3.57E+14 1.14E-05 2.26E+10 3 7 2Se 2 2De 6 2 4 0.91 5.070E+03 6.072E+03 2.40E-05 1.61E+13 3.67E-04 3.29E+09 6 7 2Se 4 2De 6 2 4 32.83 6.044E+03 6.072E+03 2.52E-04 2.78E+06 2.38E-05 4.54E+03 2 8 2Po 3 2Po 5 2 4 0.89 5.051E+03 6.072E+03 2.74E-06 2.04E+12 3.12E-03 2.96E+10 4 8 2Po 3 2Po 5 4 4 1.03 5.191E+03 6.072E+03 7.16E-06 2.54E+12 6.14E-03 3.74E+10 5 8 2Po 5 2Po 5 2 4 27.51 6.039E+03 6.072E+03 3.86E-04 1.03E+07 1.30E+00 4.20E+08 1 9 2Se 1 2De 6 2 6 0.15 0.000E+00 6.085E+03 8.74E-08 3.25E+14 0.00E+00 0.00E+00 3 9 2Se 2 2De 6 2 6 0.90 5.070E+03 6.085E+03 3.59E-05 1.72E+13 0.00E+00 0.00E+00 6 9 2Se 4 2De 6 2 6 22.24 6.044E+03 6.085E+03 3.98E-04 2.05E+07 0.00E+00 0.00E+00 7 9 2De 6 2De 6 4 6 68.93 6.072E+03 6.085E+03 8.57E-05 1.54E+04 2.34E+00 3.21E+07 2 10 2Po 3 2Po 8 2 2 0.69 5.051E+03 6.375E+03 0.00E+00 0.00E+00 9.57E-06 3.96E+08 4 10 2Po 3 2Po 8 4 2 0.77 5.191E+03 6.375E+03 1.42E-08 4.40E+10 1.82E-03 5.37E+10 5 10 2Po 5 2Po 8 2 2 2.72 6.039E+03 6.375E+03 0.00E+00 0.00E+00 6.06E-05 4.08E+07 8 10 2Po 5 2Po 8 4 2 3.01 6.072E+03 6.375E+03 1.51E-04 5.11E+11 5.55E-03 2.73E+09 1 11 2Se 1 2Se 7 2 2 0.14 0.000E+00 6.376E+03 0.00E+00 0.00E+00 8.81E-02 4.07E+14 3 11 2Se 2 2Se 7 2 2 0.70 5.070E+03 6.376E+03 0.00E+00 0.00E+00 1.42E-03 5.64E+10 6 11 2Se 4 2Se 7 2 2 2.74 6.044E+03 6.376E+03 0.00E+00 0.00E+00 1.73E-04 1.13E+08 7 11 2De 6 2Se 7 4 2 2.99 6.072E+03 6.376E+03 1.67E-05 5.85E+10 2.82E-07 1.42E+05 9 11 2De 6 2Se 7 6 2 3.13 6.085E+03 6.376E+03 4.64E-05 1.30E+11 0.00E+00 0.00E+00 1 12 2Se 1 2De 9 2 4 0.14 0.000E+00 6.385E+03 3.18E-07 2.26E+15 1.07E-03 2.49E+12 3 12 2Se 2 2De 9 2 4 0.69 5.070E+03 6.385E+03 6.90E-09 1.81E+10 1.67E-04 3.38E+09 6 12 2Se 4 2De 9 2 4 2.67 6.044E+03 6.385E+03 3.16E-04 9.76E+11 2.53E-05 8.95E+06 7 12 2De 6 2De 9 4 4 2.91 6.072E+03 6.385E+03 8.16E-05 1.65E+11 6.31E-04 1.73E+08 9 12 2De 6 2De 9 6 4 3.04 6.085E+03 6.385E+03 4.63E-05 7.55E+10 2.08E-03 5.02E+08 11 12 2Se 7 2De 9 2 4 101.12 6.376E+03 6.385E+03 4.21E-03 1.67E+05 1.48E-05 9.66E+01 2 13 2Po 3 2Po 8 2 4 0.68 5.051E+03 6.386E+03 1.48E-06 4.19E+12 1.06E-04 2.25E+09 4 13 2Po 3 2Po 8 4 4 0.76 5.191E+03 6.386E+03 3.47E-08 5.64E+10 2.62E-03 3.98E+10 5 13 2Po 5 2Po 8 2 4 2.63 6.039E+03 6.386E+03 5.17E-05 1.72E+11 3.08E-03 1.14E+09 8 13 2Po 5 2Po 8 4 4 2.91 6.072E+03 6.386E+03 1.26E-04 2.54E+11 1.51E-03 4.14E+08 10 13 2Po 8 2Po 8 2 4 84.38 6.375E+03 6.386E+03 5.15E-03 5.06E+05 1.32E+00 1.48E+07 2 14 2Po 3 2Fo10 2 6 0.68 5.051E+03 6.390E+03 9.22E-06 1.77E+13 0.00E+00 0.00E+00 4 14 2Po 3 2Fo10 4 6 0.76 5.191E+03 6.390E+03 3.20E-06 3.53E+12 7.84E-05 8.02E+08 5 14 2Po 5 2Fo10 2 6 2.60 6.039E+03 6.390E+03 6.68E-04 1.58E+12 0.00E+00 0.00E+00 8 14 2Po 5 2Fo10 4 6 2.87 6.072E+03 6.390E+03 2.36E-04 3.40E+11 1.46E-04 2.78E+07 10 14 2Po 8 2Fo10 2 6 59.33 6.375E+03 6.390E+03 3.05E-03 1.16E+06 0.00E+00 0.00E+00 13 14 2Po 8 2Fo10 4 6 199.89 6.386E+03 6.390E+03 8.26E-04 7.25E+02 5.06E-06 2.85E+00 1 15 2Se 1 2De 9 2 6 0.14 0.000E+00 6.390E+03 4.87E-07 2.31E+15 0.00E+00 0.00E+00 3 15 2Se 2 2De 9 2 6 0.69 5.070E+03 6.390E+03 1.19E-09 2.12E+09 0.00E+00 0.00E+00 6 15 2Se 4 2De 9 2 6 2.63 6.044E+03 6.390E+03 4.54E-04 1.01E+12 0.00E+00 0.00E+00 7 15 2De 6 2De 9 4 6 2.86 6.072E+03 6.390E+03 3.26E-05 4.75E+10 5.82E-04 1.12E+08 9 15 2De 6 2De 9 6 6 2.98 6.085E+03 6.390E+03 1.74E-04 2.05E+11 3.48E-03 5.88E+08 11 15 2Se 7 2De 9 2 6 65.10 6.376E+03 6.390E+03 6.30E-03 1.51E+06 0.00E+00 0.00E+00 12 15 2De 9 2De 9 4 6 182.79 6.385E+03 6.390E+03 1.52E-03 2.08E+03 2.37E+00 1.74E+06 4 16 2Po 3 2Fo10 4 8 0.76 5.191E+03 6.393E+03 1.92E-05 1.61E+13 0.00E+00 0.00E+00 8 16 2Po 5 2Fo10 4 8 2.85 6.072E+03 6.393E+03 1.42E-03 1.60E+12 0.00E+00 0.00E+00 13 16 2Po 8 2Fo10 4 8 125.53 6.386E+03 6.393E+03 4.96E-03 3.34E+04 0.00E+00 0.00E+00 14 16 2Fo10 2Fo10 6 8 337.43 6.390E+03 6.393E+03 5.07E-04 2.43E+01 3.38E+00 2.97E+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