************************** 786 ******************************************* Ref. "X-Rays of Heavy Elements for Nanotechnological Applications: W and Pb", S. 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 ************************************************************************** Pb81+: 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: Pb81+(H-like) + h\nu <-> Pb81+* File contents : -------------- 1) Table of Configurations and Thomas-Fermi scaling parameters 2) Table of LS term energies 3) LS Multiplets 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 = 82, 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 5043.036577 3 3 2Se 5043.038520 2 4 2De 5976.922576 6 5 2Se 5976.923797 4 6 2Po 5976.937654 5 7 2Fo 6303.783536 10 8 2Po 6303.784382 8 9 2Se 6303.784481 7 10 2De 6303.799638 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 5043.0366 2.834E+16 4.16E-01 4.16E-01 0.0E+00 1 2Se: 1 6 2Po: 5 0.0000 5976.9377 7.567E+15 7.91E-02 7.91E-02 6.3E-03 1 2Se: 1 8 2Po: 8 0.0000 6303.7844 3.084E+15 2.90E-02 2.90E-02 1.7E-02 2 2Po: 3 3 2Se: 2 5043.0366 5043.0385 7.889E-02 0.00E+00 0.00E+00 0.0E+00 2 2Po: 3 4 2De: 6 5043.0366 5976.9226 2.924E+15 6.96E-01 6.96E-01 4.8E-04 2 2Po: 3 5 2Se: 4 5043.0366 5976.9238 2.856E+14 1.36E-02 1.36E-02 2.5E-02 2 2Po: 3 9 2Se: 7 5043.0366 6303.7845 1.166E+14 3.04E-03 3.05E-03 1.6E-01 2 2Po: 3 10 2De: 9 5043.0366 6303.7996 9.332E+14 1.22E-01 1.22E-01 1.4E-03 3 2Se: 2 6 2Po: 5 5043.0385 5976.9377 1.016E+15 4.35E-01 4.35E-01 1.1E-03 3 2Se: 2 8 2Po: 8 5043.0385 6303.7844 4.372E+14 1.03E-01 1.03E-01 4.9E-03 4 2De: 6 6 2Po: 5 5976.9226 5976.9377 9.212E+01 3.00E-05 0.00E+00 1.0E+02 4 2De: 6 7 2Fo:10 5976.9226 6303.7835 6.237E+14 1.02E+00 1.02E+00 0.0E+00 4 2De: 6 8 2Po: 8 5976.9226 6303.7844 1.573E+13 1.10E-02 1.10E-02 4.5E-02 5 2Se: 4 6 2Po: 5 5976.9238 5976.9377 5.720E+01 1.10E-04 1.50E-04 1.5E+01 5 2Se: 4 8 2Po: 8 5976.9238 6303.7844 1.387E+14 4.85E-01 4.85E-01 1.3E-02 6 2Po: 5 9 2Se: 7 5976.9377 6303.7845 8.289E+13 3.22E-02 3.23E-02 7.8E-02 6 2Po: 5 10 2De: 9 5976.9377 6303.7996 3.183E+14 6.18E-01 6.18E-01 2.5E-02 7 2Fo:10 10 2De: 9 6303.7835 6303.7996 2.513E+02 9.00E-05 7.14E-06 8.5E+01 8 2Po: 8 10 2De: 9 6303.7844 6303.7996 2.443E+02 2.20E-04 1.00E-04 3.8E+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 600679730.0 5.47380E+03 3 2Se( 2) 2 603317425.0 5.49783E+03 4 2Po( 3) 4 618646792.0 5.63752E+03 5 2Po( 5) 2 718813024.0 6.55031E+03 6 2Se( 4) 2 719437413.0 6.55600E+03 7 2De( 6) 4 722880886.0 6.58738E+03 8 2Po( 5) 4 722978341.0 6.58826E+03 9 2De( 6) 6 724568840.0 6.60276E+03 10 2Po( 8) 2 758754716.0 6.91428E+03 11 2Se( 7) 2 758948868.0 6.91605E+03 12 2De( 9) 4 760048131.0 6.92607E+03 13 2Po( 8) 4 760091242.0 6.92646E+03 14 2Fo(10) 6 760664347.0 6.93168E+03 15 2De( 9) 6 760679184.0 6.93182E+03 16 2Fo(10) 8 761008350.0 6.93482E+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 0.17 0.00 5473.80 9.53E-02 1.044E-04 2.29E+16 2 3 2Po 3 2Se 2 2 2 37.91 5473.80 5497.83 9.43E-03 2.355E-03 4.38E+10 1 4 2Se 1 2Po 3 2 4 0.16 0.00 5637.52 1.88E-01 2.000E-04 2.40E+16 3 4 2Se 2 2Po 3 2 4 6.52 5497.83 5637.52 1.18E-01 5.079E-03 9.27E+12 1 5 2Se 1 2Po 5 2 2 0.14 0.00 6550.31 6.87E-03 6.294E-06 2.37E+15 3 5 2Se 2 2Po 5 2 2 0.87 5497.83 6550.31 1.10E-01 6.270E-04 9.78E+14 2 6 2Po 3 2Se 4 2 2 0.84 5473.80 6556.00 1.78E-03 9.849E-06 1.67E+13 4 6 2Po 3 2Se 4 4 2 0.99 5637.52 6556.00 1.84E-02 2.405E-04 2.49E+14 5 6 2Po 5 2Se 4 2 2 160.16 6550.31 6556.00 1.44E-02 1.522E-02 3.75E+09 2 7 2Po 3 2De 6 2 4 0.82 5473.80 6587.38 5.38E-01 2.896E-03 2.68E+15 4 7 2Po 3 2De 6 4 4 0.96 5637.52 6587.38 6.40E-02 8.082E-04 4.64E+14 5 7 2Po 5 2De 6 2 4 24.58 6550.31 6587.38 1.25E-01 2.018E-02 6.88E+11 1 8 2Se 1 2Po 5 2 4 0.14 0.00 6588.26 2.28E-02 2.076E-05 3.97E+15 3 8 2Se 2 2Po 5 2 4 0.84 5497.83 6588.26 1.61E-01 8.882E-04 7.71E+14 6 8 2Se 4 2Po 5 2 4 28.24 6556.00 6588.26 1.69E-01 3.137E-02 7.05E+11 7 8 2De 6 2Po 5 4 4 1026 6587.38 6588.26 2.84E-04 3.844E-03 1.80E+06 4 9 2Po 3 2De 6 4 6 0.94 5637.52 6602.76 5.76E-01 7.160E-03 2.87E+15 8 9 2Po 5 2De 6 4 6 62.87 6588.26 6602.76 4.32E-02 3.579E-02 4.86E+10 1 10 2Se 1 2Po 8 2 2 0.13 0.00 6914.28 1.25E-05 1.088E-08 4.82E+12 3 10 2Se 2 2Po 8 2 2 0.64 5497.83 6914.28 9.56E-03 4.051E-05 1.54E+14 6 10 2Se 4 2Po 8 2 2 2.54 6556.00 6914.28 1.12E-01 1.876E-03 1.16E+14 7 10 2De 6 2Po 8 4 2 2.79 6587.38 6914.28 8.34E-03 3.062E-04 1.43E+13 2 11 2Po 3 2Se 7 2 2 0.63 5473.80 6916.05 3.63E-03 1.509E-05 6.06E+13 4 11 2Po 3 2Se 7 4 2 0.71 5637.52 6916.05 8.40E-04 7.881E-06 2.20E+13 5 11 2Po 5 2Se 7 2 2 2.49 6550.31 6916.05 6.66E-03 1.093E-04 7.16E+12 8 11 2Po 5 2Se 7 4 2 2.78 6588.26 6916.05 3.31E-02 1.212E-03 5.71E+13 10 11 2Po 8 2Se 7 2 2 515.06 6914.28 6916.05 1.68E-02 5.687E-02 4.22E+08 2 12 2Po 3 2De 9 2 4 0.63 5473.80 6926.07 7.23E-02 2.985E-04 6.12E+14 4 12 2Po 3 2De 9 4 4 0.71 5637.52 6926.07 8.49E-03 7.905E-05 1.13E+14 5 12 2Po 5 2De 9 2 4 2.42 6550.31 6926.07 3.91E-01 6.249E-03 2.22E+14 8 12 2Po 5 2De 9 4 4 2.70 6588.26 6926.07 5.45E-02 1.937E-03 5.00E+13 10 12 2Po 8 2De 9 2 4 77.31 6914.28 6926.07 1.82E-01 9.252E-02 1.01E+11 1 13 2Se 1 2Po 8 2 4 0.13 0.00 6926.46 7.74E-04 6.708E-07 1.49E+14 3 13 2Se 2 2Po 8 2 4 0.64 5497.83 6926.46 1.87E-02 7.834E-05 1.53E+14 6 13 2Se 4 2Po 8 2 4 2.46 6556.00 6926.46 1.61E-01 2.604E-03 8.86E+13 7 13 2De 6 2Po 8 4 4 2.69 6587.38 6926.46 6.67E-04 2.360E-05 6.16E+11 9 13 2De 6 2Po 8 6 4 2.81 6602.76 6926.46 1.06E-02 5.915E-04 1.34E+13 11 13 2Se 7 2Po 8 2 4 87.54 6916.05 6926.46 1.96E-01 1.128E-01 8.52E+10 12 13 2De 9 2Po 8 4 4 2319 6926.07 6926.46 5.83E-04 1.780E-02 7.22E+05 7 14 2De 6 2Fo10 4 6 2.65 6587.38 6931.68 9.30E-01 3.242E-02 5.90E+14 9 14 2De 6 2Fo10 6 6 2.77 6602.76 6931.68 4.59E-02 2.511E-03 3.99E+13 12 14 2De 9 2Fo10 4 6 162.28 6926.07 6931.68 4.44E-02 9.489E-02 7.50E+09 4 15 2Po 3 2De 9 4 6 0.70 5637.52 6931.82 8.91E-02 8.264E-04 8.00E+14 8 15 2Po 5 2De 9 4 6 2.65 6588.26 6931.82 4.65E-01 1.624E-02 2.94E+14 13 15 2Po 8 2De 9 4 6 170.08 6926.46 6931.82 7.14E-02 1.599E-01 1.10E+10 14 15 2Fo10 2De 9 6 6 6739 6931.68 6931.82 4.94E-05 6.582E-03 7.26E+03 9 16 2De 6 2Fo10 6 8 2.74 6602.76 6934.82 9.26E-01 5.022E-02 6.15E+14 15 16 2De 9 2Fo10 6 8 303.80 6931.82 6934.82 2.19E-02 1.316E-01 1.19E+09 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 0.81 5.474E+03 6.603E+03 1.32E-07 6.21E+10 7.29E-02 5.29E+11 5 9 2Po 5 2De 6 2 6 17.37 6.550E+03 6.603E+03 8.07E-06 1.77E+03 5.30E-01 8.33E+05 9 10 2De 6 2Po 8 6 2 2.93 6.603E+03 6.914E+03 5.61E-06 9.63E+08 1.59E-02 5.53E+08 1 14 2Se 1 2Fo10 2 6 0.13 0.000E+00 6.932E+03 9.41E-09 1.45E+15 0.00E+00 0.00E+00 3 14 2Se 2 2Fo10 2 6 0.64 5.498E+03 6.932E+03 3.14E-07 7.86E+11 0.00E+00 0.00E+00 6 14 2Se 4 2Fo10 2 6 2.43 6.556E+03 6.932E+03 1.78E-05 3.77E+09 0.00E+00 0.00E+00 11 14 2Se 7 2Fo10 2 6 58.29 6.916E+03 6.932E+03 1.50E-04 6.87E+00 0.00E+00 0.00E+00 2 15 2Po 3 2De 9 2 6 0.63 5.474E+03 6.932E+03 3.43E-07 9.66E+11 8.84E-03 2.30E+11 5 15 2Po 5 2De 9 2 6 2.39 6.550E+03 6.932E+03 9.33E-06 2.20E+09 1.46E-01 4.67E+09 10 15 2Po 8 2De 9 2 6 51.96 6.914E+03 6.932E+03 4.85E-04 4.96E+01 2.36E+00 1.55E+04 1 16 2Se 1 2Fo10 2 8 0.13 0.000E+00 6.935E+03 1.25E-08 1.46E+15 0.00E+00 0.00E+00 3 16 2Se 2 2Fo10 2 8 0.63 5.498E+03 6.935E+03 4.19E-07 7.98E+11 0.00E+00 0.00E+00 6 16 2Se 4 2Fo10 2 8 2.41 6.556E+03 6.935E+03 2.37E-05 4.00E+09 0.00E+00 0.00E+00 7 16 2De 6 2Fo10 4 8 2.62 6.587E+03 6.935E+03 7.39E-06 6.80E+08 7.90E-01 1.19E+10 11 16 2Se 7 2Fo10 2 8 48.56 6.916E+03 6.935E+03 2.00E-04 2.47E+01 0.00E+00 0.00E+00 12 16 2De 9 2Fo10 4 8 104.14 6.926E+03 6.935E+03 1.31E-04 7.74E-02 2.31E+00 3.52E+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 0.17 0.000E+00 5.498E+03 0.00E+00 0.00E+00 2.36E-02 6.98E+13 2 4 2Po 3 2Po 3 2 4 5.57 5.474E+03 5.638E+03 8.33E-06 6.55E+08 1.23E+00 4.81E+10 2 5 2Po 3 2Po 5 2 2 0.85 5.474E+03 6.550E+03 0.00E+00 0.00E+00 3.03E-04 6.74E+09 4 5 2Po 3 2Po 5 4 2 1.00 5.638E+03 6.550E+03 7.19E-06 6.09E+12 1.10E-02 1.49E+11 1 6 2Se 1 2Se 4 2 2 0.14 0.000E+00 6.556E+03 0.00E+00 0.00E+00 2.13E-02 1.07E+14 3 6 2Se 2 2Se 4 2 2 0.86 5.498E+03 6.556E+03 0.00E+00 0.00E+00 1.25E-03 2.63E+10 1 7 2Se 1 2De 6 2 4 0.14 0.000E+00 6.587E+03 5.82E-08 4.82E+14 7.69E-06 1.96E+10 3 7 2Se 2 2De 6 2 4 0.84 5.498E+03 6.587E+03 2.00E-05 2.05E+13 4.30E-04 4.96E+09 6 7 2Se 4 2De 6 2 4 29.04 6.556E+03 6.587E+03 2.16E-04 4.40E+06 2.87E-05 7.91E+03 2 8 2Po 3 2Po 5 2 4 0.82 5.474E+03 6.588E+03 2.09E-06 2.41E+12 3.48E-03 4.29E+10 4 8 2Po 3 2Po 5 4 4 0.96 5.638E+03 6.588E+03 6.05E-06 3.14E+12 7.16E-03 5.48E+10 5 8 2Po 5 2Po 5 2 4 24.01 6.550E+03 6.588E+03 3.30E-04 1.74E+07 1.29E+00 6.30E+08 1 9 2Se 1 2De 6 2 6 0.14 0.000E+00 6.603E+03 7.77E-08 4.34E+14 0.00E+00 0.00E+00 3 9 2Se 2 2De 6 2 6 0.82 5.498E+03 6.603E+03 3.00E-05 2.20E+13 0.00E+00 0.00E+00 6 9 2Se 4 2De 6 2 6 19.49 6.556E+03 6.603E+03 3.42E-04 3.40E+07 0.00E+00 0.00E+00 7 9 2De 6 2De 6 4 6 59.24 6.587E+03 6.603E+03 7.34E-05 2.82E+04 2.33E+00 5.04E+07 2 10 2Po 3 2Po 8 2 2 0.63 5.474E+03 6.914E+03 0.00E+00 0.00E+00 6.93E-06 3.69E+08 4 10 2Po 3 2Po 8 4 2 0.71 5.638E+03 6.914E+03 3.25E-09 1.47E+10 2.05E-03 7.62E+10 5 10 2Po 5 2Po 8 2 2 2.50 6.550E+03 6.914E+03 0.00E+00 0.00E+00 6.69E-05 5.75E+07 8 10 2Po 5 2Po 8 4 2 2.79 6.588E+03 6.914E+03 1.28E-04 6.31E+11 6.14E-03 3.79E+09 1 11 2Se 1 2Se 7 2 2 0.13 0.000E+00 6.916E+03 0.00E+00 0.00E+00 1.18E-01 6.98E+14 3 11 2Se 2 2Se 7 2 2 0.64 5.498E+03 6.916E+03 0.00E+00 0.00E+00 1.77E-03 8.98E+10 6 11 2Se 4 2Se 7 2 2 2.53 6.556E+03 6.916E+03 0.00E+00 0.00E+00 1.91E-04 1.58E+08 7 11 2De 6 2Se 7 4 2 2.77 6.587E+03 6.916E+03 1.35E-05 6.93E+10 3.44E-07 2.18E+05 9 11 2De 6 2Se 7 6 2 2.91 6.603E+03 6.916E+03 3.97E-05 1.60E+11 0.00E+00 0.00E+00 1 12 2Se 1 2De 9 2 4 0.13 0.000E+00 6.926E+03 3.06E-07 3.26E+15 1.53E-03 4.54E+12 3 12 2Se 2 2De 9 2 4 0.64 5.498E+03 6.926E+03 1.97E-08 7.81E+10 2.02E-04 5.24E+09 6 12 2Se 4 2De 9 2 4 2.46 6.556E+03 6.926E+03 2.63E-04 1.22E+12 2.89E-05 1.31E+07 7 12 2De 6 2De 9 4 4 2.69 6.587E+03 6.926E+03 6.82E-05 2.03E+11 7.26E-04 2.52E+08 9 12 2De 6 2De 9 6 4 2.82 6.603E+03 6.926E+03 3.96E-05 9.34E+10 2.40E-03 7.22E+08 11 12 2Se 7 2De 9 2 4 90.97 6.916E+03 6.926E+03 3.64E-03 2.45E+05 1.78E-05 1.59E+02 2 13 2Po 3 2Po 8 2 4 0.63 5.474E+03 6.926E+03 1.61E-06 6.98E+12 8.38E-05 2.29E+09 4 13 2Po 3 2Po 8 4 4 0.71 5.638E+03 6.926E+03 1.47E-08 3.49E+10 3.13E-03 5.97E+10 5 13 2Po 5 2Po 8 2 4 2.42 6.550E+03 6.926E+03 4.03E-05 2.03E+11 3.35E-03 1.59E+09 8 13 2Po 5 2Po 8 4 4 2.69 6.588E+03 6.926E+03 1.06E-04 3.12E+11 1.74E-03 5.99E+08 10 13 2Po 8 2Po 8 2 4 74.82 6.914E+03 6.926E+03 4.45E-03 7.97E+05 1.32E+00 2.12E+07 2 14 2Po 3 2Fo10 2 6 0.62 5.474E+03 6.932E+03 7.83E-06 2.30E+13 0.00E+00 0.00E+00 4 14 2Po 3 2Fo10 4 6 0.70 5.638E+03 6.932E+03 2.75E-06 4.44E+12 8.98E-05 1.16E+09 5 14 2Po 5 2Fo10 2 6 2.39 6.550E+03 6.932E+03 5.62E-04 2.02E+12 0.00E+00 0.00E+00 8 14 2Po 5 2Fo10 4 6 2.65 6.588E+03 6.932E+03 2.01E-04 4.28E+11 1.71E-04 4.10E+07 10 14 2Po 8 2Fo10 2 6 52.37 6.914E+03 6.932E+03 2.64E-03 1.88E+06 0.00E+00 0.00E+00 13 14 2Po 8 2Fo10 4 6 174.49 6.926E+03 6.932E+03 7.13E-04 1.24E+03 6.06E-06 5.13E+00 1 15 2Se 1 2De 9 2 6 0.13 0.000E+00 6.932E+03 4.69E-07 3.34E+15 0.00E+00 0.00E+00 3 15 2Se 2 2De 9 2 6 0.64 5.498E+03 6.932E+03 1.47E-09 3.98E+09 0.00E+00 0.00E+00 6 15 2Se 4 2De 9 2 6 2.42 6.556E+03 6.932E+03 3.77E-04 1.26E+12 0.00E+00 0.00E+00 7 15 2De 6 2De 9 4 6 2.65 6.587E+03 6.932E+03 2.70E-05 5.84E+10 6.64E-04 1.61E+08 9 15 2De 6 2De 9 6 6 2.77 6.603E+03 6.932E+03 1.48E-04 2.54E+11 4.04E-03 8.55E+08 11 15 2Se 7 2De 9 2 6 57.79 6.916E+03 6.932E+03 5.44E-03 2.36E+06 0.00E+00 0.00E+00 12 15 2De 9 2De 9 4 6 158.47 6.926E+03 6.932E+03 1.31E-03 3.67E+03 2.37E+00 2.68E+06 4 16 2Po 3 2Fo10 4 8 0.70 5.638E+03 6.935E+03 1.65E-05 2.02E+13 0.00E+00 0.00E+00 8 16 2Po 5 2Fo10 4 8 2.63 6.588E+03 6.935E+03 1.21E-03 2.02E+12 0.00E+00 0.00E+00 13 16 2Po 8 2Fo10 4 8 109.04 6.926E+03 6.935E+03 4.28E-03 5.83E+04 0.00E+00 0.00E+00 14 16 2Fo10 2Fo10 6 8 290.70 6.932E+03 6.935E+03 4.37E-04 4.42E+01 3.38E+00 4.64E+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