************************** 786 ******************************************* Ref. "X-Rays of Heavy Elements for Nanotechnological Applications: W and Pb ions", S.N. Nahar, 4th international conference on Modern Trends in Physics Research (MTPR-010), Cairo University, Egypt, December 12 - 16 December 2010, Conference Proceedings, Vol 9910 (Ed. Lotfia El Nadi, World Scientific 2013),p.275 - 285 ************************************************************************** W73+: 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: W73+ (H-like) + h\nu <-> W73+* 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 = 74, 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 4107.028916 3 3 2Se 4107.034060 2 4 2De 4867.582615 6 5 2Se 4867.583279 4 6 2Po 4867.583658 5 7 2Fo 5133.776952 10 8 2De 5133.777147 9 9 2Po 5133.777532 8 10 2Se 5133.777544 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 4107.0289 1.880E+16 4.16E-01 4.16E-01 0.0E+00 1 2Se: 1 6 2Po: 5 0.0000 4867.5837 5.018E+15 7.91E-02 7.91E-02 0.0E+00 1 2Se: 1 9 2Po: 8 0.0000 5133.7775 2.046E+15 2.90E-02 2.90E-02 1.7E-02 2 2Po: 3 3 2Se: 2 4107.0289 4107.0341 1.797E+00 0.00E+00 0.00E+00 0.0E+00 2 2Po: 3 4 2De: 6 4107.0289 4867.5826 1.940E+15 6.96E-01 6.96E-01 4.8E-04 2 2Po: 3 5 2Se: 4 4107.0289 4867.5833 1.894E+14 1.36E-02 1.36E-02 2.5E-02 2 2Po: 3 8 2De: 9 4107.0289 5133.7771 6.188E+14 1.22E-01 1.22E-01 0.0E+00 2 2Po: 3 10 2Se: 7 4107.0289 5133.7775 7.735E+13 3.04E-03 3.05E-03 1.6E-01 3 2Se: 2 6 2Po: 5 4107.0341 4867.5837 6.735E+14 4.35E-01 4.35E-01 1.1E-03 3 2Se: 2 9 2Po: 8 4107.0341 5133.7775 2.901E+14 1.03E-01 1.03E-01 4.9E-03 4 2De: 6 6 2Po: 5 4867.5826 4867.5837 3.743E-02 0.00E+00 0.00E+00 0.0E+00 4 2De: 6 7 2Fo:10 4867.5826 5133.7770 4.137E+14 1.02E+00 1.02E+00 0.0E+00 4 2De: 6 9 2Po: 8 4867.5826 5133.7775 1.043E+13 1.10E-02 1.10E-02 0.0E+00 5 2Se: 4 9 2Po: 8 4867.5833 5133.7775 9.196E+13 4.85E-01 4.85E-01 2.1E-03 6 2Po: 5 8 2De: 9 4867.5837 5133.7771 2.111E+14 6.18E-01 6.18E-01 5.4E-04 6 2Po: 5 10 2Se: 7 4867.5837 5133.7775 5.507E+13 3.23E-02 3.23E-02 0.0E+00 LS transitions: Number of oscillator strengths = 16 ****************************************************************************** 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 481822739.0 4.39069E+03 3 2Se( 2) 2 483238206.0 4.40359E+03 4 2Po( 3) 4 493577372.0 4.49781E+03 5 2Po( 5) 2 575388797.0 5.24333E+03 6 2Se( 4) 2 575747066.0 5.24659E+03 7 2De( 6) 4 578191677.0 5.26887E+03 8 2Po( 5) 4 578243267.0 5.26934E+03 9 2De( 6) 6 579304398.0 5.27901E+03 10 2Po( 8) 2 607314863.0 5.53426E+03 11 2Se( 7) 2 607432105.0 5.53533E+03 12 2De( 9) 4 608246515.0 5.54275E+03 13 2Po( 8) 4 608271047.0 5.54297E+03 14 2Fo(10) 6 608664560.0 5.54656E+03 15 2De( 9) 6 608671742.0 5.54663E+03 16 2Fo(10) 8 608892717.0 5.54864E+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 0.21 0.00 4390.69 1.03E-01 1.414E-04 1.60E+16 2 3 2Po 3 2Se 2 2 2 70.65 4390.69 4403.59 6.32E-03 2.941E-03 8.45E+09 1 4 2Se 1 2Po 3 2 4 0.20 0.00 4497.81 2.03E-01 2.714E-04 1.65E+16 3 4 2Se 2 2Po 3 2 4 9.67 4403.59 4497.81 9.87E-02 6.288E-03 3.52E+12 1 5 2Se 1 2Po 5 2 2 0.17 0.00 5243.33 9.46E-03 1.082E-05 2.09E+15 3 5 2Se 2 2Po 5 2 2 1.08 4403.59 5243.33 1.15E-01 8.244E-04 6.54E+14 2 6 2Po 3 2Se 4 2 2 1.06 4390.69 5246.59 3.32E-03 2.330E-05 1.96E+13 4 6 2Po 3 2Se 4 4 2 1.22 4497.81 5246.59 1.81E-02 2.893E-04 1.63E+14 5 6 2Po 5 2Se 4 2 2 279.12 5243.33 5246.59 1.02E-02 1.881E-02 8.76E+08 2 7 2Po 3 2De 6 2 4 1.04 4390.69 5268.87 5.65E-01 3.858E-03 1.75E+15 4 7 2Po 3 2De 6 4 4 1.18 4497.81 5268.87 6.50E-02 1.012E-03 3.11E+14 5 7 2Po 5 2De 6 2 4 35.68 5243.33 5268.87 1.05E-01 2.476E-02 2.76E+11 1 8 2Se 1 2Po 5 2 4 0.17 0.00 5269.34 2.75E-02 3.134E-05 3.07E+15 3 8 2Se 2 2Po 5 2 4 1.05 4403.59 5269.34 1.80E-01 1.244E-03 5.40E+14 6 8 2Se 4 2Po 5 2 4 40.06 5246.59 5269.34 1.47E-01 3.866E-02 3.05E+11 7 8 2De 6 2Po 5 4 4 1938 5268.87 5269.34 1.86E-04 4.755E-03 3.31E+05 4 9 2Po 3 2De 6 4 6 1.17 4497.81 5279.01 5.85E-01 8.988E-03 1.91E+15 8 9 2Po 5 2De 6 4 6 94.24 5269.34 5279.01 3.55E-02 4.402E-02 1.78E+10 1 10 2Se 1 2Po 8 2 2 0.17 0.00 5534.26 3.52E-04 3.819E-07 8.67E+13 3 10 2Se 2 2Po 8 2 2 0.81 4403.59 5534.26 1.23E-02 6.506E-05 1.26E+14 6 10 2Se 4 2Po 8 2 2 3.17 5246.59 5534.26 1.18E-01 2.457E-03 7.83E+13 7 10 2De 6 2Po 8 4 2 3.43 5268.87 5534.26 8.85E-03 4.000E-04 1.00E+13 2 11 2Po 3 2Se 7 2 2 0.80 4390.69 5535.33 1.57E-03 8.244E-06 1.66E+13 4 11 2Po 3 2Se 7 4 2 0.88 4497.81 5535.33 1.17E-03 1.358E-05 2.03E+13 5 11 2Po 5 2Se 7 2 2 3.12 5243.33 5535.33 9.54E-03 1.961E-04 6.54E+12 8 11 2Po 5 2Se 7 4 2 3.43 5269.34 5535.33 3.40E-02 1.535E-03 3.87E+13 10 11 2Po 8 2Se 7 2 2 852.93 5534.26 5535.33 1.23E-02 6.934E-02 1.13E+08 2 12 2Po 3 2De 9 2 4 0.79 4390.69 5542.75 8.05E-02 4.193E-04 4.29E+14 4 12 2Po 3 2De 9 4 4 0.87 4497.81 5542.75 9.10E-03 1.045E-04 7.98E+13 5 12 2Po 5 2De 9 2 4 3.04 5243.33 5542.75 4.22E-01 8.460E-03 1.52E+14 8 12 2Po 5 2De 9 4 4 3.33 5269.34 5542.75 5.58E-02 2.447E-03 3.35E+13 10 12 2Po 8 2De 9 2 4 107.34 5534.26 5542.75 1.59E-01 1.125E-01 4.61E+10 1 13 2Se 1 2Po 8 2 4 0.16 0.00 5542.97 2.27E-03 2.459E-06 2.80E+14 3 13 2Se 2 2Po 8 2 4 0.80 4403.59 5542.97 2.46E-02 1.297E-04 1.28E+14 6 13 2Se 4 2Po 8 2 4 3.08 5246.59 5542.97 1.79E-01 3.626E-03 6.32E+13 7 13 2De 6 2Po 8 4 4 3.33 5268.87 5542.97 8.43E-04 3.691E-05 5.09E+11 9 13 2De 6 2Po 8 6 4 3.45 5279.01 5542.97 1.08E-02 7.340E-04 9.04E+12 11 13 2Se 7 2Po 8 2 4 119.20 5535.33 5542.97 1.75E-01 1.376E-01 4.12E+10 12 13 2De 9 2Po 8 4 4 4076 5542.75 5542.97 4.05E-04 2.172E-02 1.62E+05 7 14 2De 6 2Fo10 4 6 3.28 5268.87 5546.56 9.46E-01 4.088E-02 3.91E+14 9 14 2De 6 2Fo10 6 6 3.41 5279.01 5546.56 4.64E-02 3.118E-03 2.66E+13 12 14 2De 9 2Fo10 4 6 239.21 5542.75 5546.56 3.66E-02 1.154E-01 2.85E+09 4 15 2Po 3 2De 9 4 6 0.87 4497.81 5546.63 9.27E-02 1.061E-03 5.46E+14 8 15 2Po 5 2De 9 4 6 3.29 5269.34 5546.63 4.81E-01 2.080E-02 1.98E+14 13 15 2Po 8 2De 9 4 6 249.57 5542.97 5546.63 5.94E-02 1.951E-01 4.24E+09 14 15 2Fo10 2De 9 6 6 13923 5546.56 5546.63 2.93E-05 8.049E-03 1.01E+03 9 16 2De 6 2Fo10 6 8 3.38 5279.01 5548.64 9.34E-01 6.238E-02 4.09E+14 15 16 2De 9 2Fo10 6 8 452.54 5546.63 5548.64 1.80E-02 1.609E-01 4.40E+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 1.03 4.391E+03 5.279E+03 2.95E-07 2.58E+10 9.74E-02 2.13E+11 5 9 2Po 5 2De 6 2 6 25.54 5.243E+03 5.279E+03 1.54E-05 2.28E+02 6.48E-01 1.48E+05 9 10 2De 6 2Po 8 6 2 3.57 5.279E+03 5.534E+03 1.07E-05 4.55E+08 1.83E-02 2.35E+08 1 14 2Se 1 2Fo10 2 6 0.16 0.000E+00 5.547E+03 1.16E-08 3.78E+14 0.00E+00 0.00E+00 3 14 2Se 2 2Fo10 2 6 0.80 4.404E+03 5.547E+03 5.56E-07 2.85E+11 0.00E+00 0.00E+00 6 14 2Se 4 2Fo10 2 6 3.04 5.247E+03 5.547E+03 3.54E-05 1.56E+09 0.00E+00 0.00E+00 11 14 2Se 7 2Fo10 2 6 81.14 5.535E+03 5.547E+03 2.75E-04 1.25E+00 0.00E+00 0.00E+00 2 15 2Po 3 2De 9 2 6 0.79 4.391E+03 5.547E+03 4.30E-07 2.38E+11 1.21E-02 9.86E+10 5 15 2Po 5 2De 9 2 6 3.00 5.243E+03 5.547E+03 2.12E-05 1.00E+09 2.02E-01 2.05E+09 10 15 2Po 8 2De 9 2 6 73.70 5.534E+03 5.547E+03 8.93E-04 7.93E+00 2.87E+00 3.28E+03 1 16 2Se 1 2Fo10 2 8 0.16 0.000E+00 5.549E+03 1.55E-08 3.78E+14 0.00E+00 0.00E+00 3 16 2Se 2 2Fo10 2 8 0.80 4.404E+03 5.549E+03 7.41E-07 2.88E+11 0.00E+00 0.00E+00 6 16 2Se 4 2Fo10 2 8 3.02 5.247E+03 5.549E+03 4.72E-05 1.63E+09 0.00E+00 0.00E+00 7 16 2De 6 2Fo10 4 8 3.26 5.269E+03 5.549E+03 1.46E-05 2.95E+08 9.97E-01 5.07E+09 11 16 2Se 7 2Fo10 2 8 68.46 5.535E+03 5.549E+03 3.67E-04 4.09E+00 0.00E+00 0.00E+00 12 16 2De 9 2Fo10 4 8 154.75 5.543E+03 5.549E+03 2.41E-04 8.92E-03 2.81E+00 5.91E+01 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 0.21 0.000E+00 4.404E+03 0.00E+00 0.00E+00 1.41E-02 2.15E+13 2 4 2Po 3 2Po 3 2 4 8.51 4.391E+03 4.498E+03 1.30E-05 1.23E+08 1.25E+00 1.37E+10 2 5 2Po 3 2Po 5 2 2 1.07 4.391E+03 5.243E+03 0.00E+00 0.00E+00 2.22E-04 2.45E+09 4 5 2Po 3 2Po 5 4 2 1.22 4.498E+03 5.243E+03 1.11E-05 3.42E+12 7.63E-03 5.64E+10 1 6 2Se 1 2Se 4 2 2 0.17 0.000E+00 5.247E+03 0.00E+00 0.00E+00 1.06E-02 2.72E+13 3 6 2Se 2 2Se 4 2 2 1.08 4.404E+03 5.247E+03 0.00E+00 0.00E+00 8.75E-04 9.34E+09 1 7 2Se 1 2De 6 2 4 0.17 0.000E+00 5.269E+03 7.85E-08 2.13E+14 1.60E-05 2.09E+10 3 7 2Se 2 2De 6 2 4 1.05 4.404E+03 5.269E+03 3.28E-05 1.06E+13 2.79E-04 1.61E+09 6 7 2Se 4 2De 6 2 4 40.91 5.247E+03 5.269E+03 3.31E-04 1.21E+06 1.72E-05 1.69E+03 2 8 2Po 3 2Po 5 2 4 1.04 4.391E+03 5.269E+03 4.25E-06 1.49E+12 2.55E-03 1.54E+10 4 8 2Po 3 2Po 5 4 4 1.18 4.498E+03 5.269E+03 9.58E-06 1.75E+12 4.69E-03 1.92E+10 5 8 2Po 5 2Po 5 2 4 35.03 5.243E+03 5.269E+03 5.08E-04 4.05E+06 1.30E+00 2.04E+08 1 9 2Se 1 2De 6 2 6 0.17 0.000E+00 5.279E+03 1.08E-07 1.97E+14 0.00E+00 0.00E+00 3 9 2Se 2 2De 6 2 6 1.04 4.404E+03 5.279E+03 4.92E-05 1.13E+13 0.00E+00 0.00E+00 6 9 2Se 4 2De 6 2 6 28.11 5.247E+03 5.279E+03 5.19E-04 8.28E+06 0.00E+00 0.00E+00 7 9 2De 6 2De 6 4 6 89.87 5.269E+03 5.279E+03 1.12E-04 5.37E+03 2.35E+00 1.45E+07 2 10 2Po 3 2Po 8 2 2 0.80 4.391E+03 5.534E+03 0.00E+00 0.00E+00 1.31E-05 3.48E+08 4 10 2Po 3 2Po 8 4 2 0.88 4.498E+03 5.534E+03 5.84E-08 9.34E+10 1.46E-03 2.90E+10 5 10 2Po 5 2Po 8 2 2 3.13 5.243E+03 5.534E+03 0.00E+00 0.00E+00 5.06E-05 2.22E+07 8 10 2Po 5 2Po 8 4 2 3.44 5.269E+03 5.534E+03 2.02E-04 3.53E+11 4.62E-03 1.53E+09 1 11 2Se 1 2Se 7 2 2 0.17 0.000E+00 5.535E+03 0.00E+00 0.00E+00 5.28E-02 1.60E+14 3 11 2Se 2 2Se 7 2 2 0.81 4.404E+03 5.535E+03 0.00E+00 0.00E+00 9.76E-04 2.52E+10 6 11 2Se 4 2Se 7 2 2 3.16 5.247E+03 5.535E+03 0.00E+00 0.00E+00 1.44E-04 6.19E+07 7 11 2De 6 2Se 7 4 2 3.42 5.269E+03 5.535E+03 2.39E-05 4.28E+10 1.98E-07 6.68E+04 9 11 2De 6 2Se 7 6 2 3.56 5.279E+03 5.535E+03 6.07E-05 8.98E+10 0.00E+00 0.00E+00 1 12 2Se 1 2De 9 2 4 0.16 0.000E+00 5.543E+03 3.43E-07 1.20E+15 5.73E-04 8.69E+11 3 12 2Se 2 2De 9 2 4 0.80 4.404E+03 5.543E+03 9.51E-10 1.22E+09 1.20E-04 1.58E+09 6 12 2Se 4 2De 9 2 4 3.08 5.247E+03 5.543E+03 4.32E-04 6.57E+11 1.99E-05 4.61E+06 7 12 2De 6 2De 9 4 4 3.33 5.269E+03 5.543E+03 1.11E-04 1.15E+11 4.91E-04 9.00E+07 9 12 2De 6 2De 9 6 4 3.46 5.279E+03 5.543E+03 6.08E-05 5.18E+10 1.62E-03 2.64E+08 11 12 2Se 7 2De 9 2 4 122.79 5.535E+03 5.543E+03 5.44E-03 8.19E+04 1.08E-05 3.93E+01 2 13 2Po 3 2Po 8 2 4 0.79 4.391E+03 5.543E+03 1.22E-06 1.66E+12 1.32E-04 1.80E+09 4 13 2Po 3 2Po 8 4 4 0.87 4.498E+03 5.543E+03 9.86E-08 8.22E+10 1.94E-03 1.97E+10 5 13 2Po 5 2Po 8 2 4 3.04 5.243E+03 5.543E+03 7.89E-05 1.27E+11 2.62E-03 6.28E+08 8 13 2Po 5 2Po 8 4 4 3.33 5.269E+03 5.543E+03 1.72E-04 1.76E+11 1.19E-03 2.17E+08 10 13 2Po 8 2Po 8 2 4 104.58 5.534E+03 5.543E+03 6.67E-03 2.24E+05 1.32E+00 7.78E+06 2 14 2Po 3 2Fo10 2 6 0.79 4.391E+03 5.547E+03 1.23E-05 1.13E+13 0.00E+00 0.00E+00 4 14 2Po 3 2Fo10 4 6 0.87 4.498E+03 5.547E+03 4.19E-06 2.37E+12 6.16E-05 4.22E+08 5 14 2Po 5 2Fo10 2 6 3.00 5.243E+03 5.547E+03 9.03E-04 1.03E+12 0.00E+00 0.00E+00 8 14 2Po 5 2Fo10 4 6 3.29 5.269E+03 5.547E+03 3.12E-04 2.28E+11 1.12E-04 1.41E+07 10 14 2Po 8 2Fo10 2 6 74.09 5.534E+03 5.547E+03 3.93E-03 4.92E+05 0.00E+00 0.00E+00 13 14 2Po 8 2Fo10 4 6 254.12 5.543E+03 5.547E+03 1.07E-03 2.82E+02 3.69E-06 1.01E+00 1 15 2Se 1 2De 9 2 6 0.16 0.000E+00 5.547E+03 5.24E-07 1.22E+15 0.00E+00 0.00E+00 3 15 2Se 2 2De 9 2 6 0.80 4.404E+03 5.547E+03 3.19E-08 2.77E+10 0.00E+00 0.00E+00 6 15 2Se 4 2De 9 2 6 3.04 5.247E+03 5.547E+03 6.25E-04 6.77E+11 0.00E+00 0.00E+00 7 15 2De 6 2De 9 4 6 3.28 5.269E+03 5.547E+03 4.48E-05 3.30E+10 4.59E-04 5.84E+07 9 15 2De 6 2De 9 6 6 3.40 5.279E+03 5.547E+03 2.30E-04 1.41E+11 2.68E-03 3.05E+08 11 15 2Se 7 2De 9 2 6 80.67 5.535E+03 5.547E+03 8.14E-03 6.67E+05 0.00E+00 0.00E+00 12 15 2De 9 2De 9 4 6 235.17 5.543E+03 5.547E+03 1.97E-03 7.67E+02 2.37E+00 8.21E+05 4 16 2Po 3 2Fo10 4 8 0.87 4.498E+03 5.549E+03 2.52E-05 1.08E+13 0.00E+00 0.00E+00 8 16 2Po 5 2Fo10 4 8 3.26 5.269E+03 5.549E+03 1.87E-03 1.06E+12 0.00E+00 0.00E+00 13 16 2Po 8 2Fo10 4 8 160.86 5.543E+03 5.549E+03 6.41E-03 1.25E+04 0.00E+00 0.00E+00 14 16 2Fo10 2Fo10 6 8 438.30 5.547E+03 5.549E+03 6.59E-04 8.55E+00 3.39E+00 1.36E+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