*************************** 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) ************************************************************************** U91+: 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: U91+ + h\nu <-> U91+* 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 = 92, 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 6348.043945 3 3 2Se 6348.045898 2 4 2De 7523.594727 6 5 2Po 7523.601562 5 6 2Se 7523.611816 4 7 2Fo 7935.039062 10 8 2Po 7935.040039 8 9 2Se 7935.040527 7 10 2De 7935.054199 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 6348.0439 4.491E+16 4.16E-01 4.16E-01 0.0E+00 1 2Se: 1 5 2Po: 5 0.0000 7523.6016 1.199E+16 7.91E-02 7.91E-02 6.3E-03 1 2Se: 1 8 2Po: 8 0.0000 7935.0400 4.887E+15 2.90E-02 2.90E-02 1.7E-02 2 2Po: 3 3 2Se: 2 6348.0439 6348.0459 7.003E-02 0.00E+00 0.00E+00 0.0E+00 2 2Po: 3 4 2De: 6 6348.0439 7523.5947 4.634E+15 6.96E-01 6.96E-01 4.8E-04 2 2Po: 3 6 2Se: 4 6348.0439 7523.6118 4.526E+14 1.36E-02 1.36E-02 2.5E-02 2 2Po: 3 9 2Se: 7 6348.0439 7935.0405 1.848E+14 3.04E-03 3.05E-03 1.6E-01 2 2Po: 3 10 2De: 9 6348.0439 7935.0542 1.479E+15 1.22E-01 1.22E-01 2.7E-03 3 2Se: 2 5 2Po: 5 6348.0459 7523.6016 1.609E+15 4.35E-01 4.35E-01 2.3E-03 3 2Se: 2 8 2Po: 8 6348.0459 7935.0400 6.929E+14 1.03E-01 1.03E-01 4.9E-03 4 2De: 6 5 2Po: 5 7523.5947 7523.6016 6.440E+00 1.00E-05 0.00E+00 1.0E+02 4 2De: 6 7 2Fo:10 7523.5947 7935.0391 9.883E+14 1.02E+00 1.02E+00 4.7E-06 4 2De: 6 8 2Po: 8 7523.5947 7935.0400 2.491E+13 1.10E-02 1.10E-02 2.5E-06 5 2Po: 5 6 2Se: 4 7523.6016 7523.6118 5.681E+01 2.00E-05 0.00E+00 1.0E+02 5 2Po: 5 9 2Se: 7 7523.6016 7935.0405 1.315E+14 3.22E-02 3.22E-02 1.9E-06 5 2Po: 5 10 2De: 9 7523.6016 7935.0542 5.045E+14 6.18E-01 6.18E-01 5.4E-03 6 2Se: 4 8 2Po: 8 7523.6118 7935.0400 2.196E+14 4.85E-01 4.85E-01 1.7E-02 7 2Fo:10 10 2De: 9 7935.0391 7935.0542 1.667E+02 6.00E-05 0.00E+00 1.0E+02 8 2Po: 8 10 2De: 9 7935.0400 7935.0542 1.488E+02 1.60E-04 1.33E-04 9.1E+00 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 772250560.0 7.03727E+03 3 2Se( 2) 2 777542848.0 7.08549E+03 4 2Po( 3) 4 801227776.0 7.30133E+03 5 2Po( 5) 2 926934080.0 8.44684E+03 6 2Se( 4) 2 928081344.0 8.45730E+03 7 2De( 6) 4 933035072.0 8.50244E+03 8 2Po( 5) 4 933229824.0 8.50422E+03 9 2De( 6) 6 935731840.0 8.52702E+03 10 2Po( 8) 2 978468480.0 8.91646E+03 11 2Se( 7) 2 978804736.0 8.91953E+03 12 2De( 9) 4 980297344.0 8.93313E+03 13 2Po( 8) 4 980381760.0 8.93390E+03 14 2Fo(10) 6 981247168.0 8.94178E+03 15 2De( 9) 6 981275008.0 8.94204E+03 16 2Fo(10) 8 981792256.0 8.94675E+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 0.13 0.00 7037.27 8.41E-02 7.168E-05 3.34E+16 2 3 2Po 3 2Se 2 2 2 18.90 7037.27 7085.49 1.47E-02 1.834E-03 2.75E+11 1 4 2Se 1 2Po 3 2 4 0.12 0.00 7301.33 1.67E-01 1.375E-04 3.58E+16 3 4 2Se 2 2Po 3 2 4 4.22 7085.49 7301.33 1.44E-01 3.993E-03 2.69E+13 1 5 2Se 1 2Po 5 2 2 0.11 0.00 8446.84 4.03E-03 2.864E-06 2.31E+15 3 5 2Se 2 2Po 5 2 2 0.67 7085.49 8446.84 1.03E-01 4.548E-04 1.54E+15 2 6 2Po 3 2Se 4 2 2 0.64 7037.27 8457.30 3.98E-04 1.680E-06 6.44E+12 4 6 2Po 3 2Se 4 4 2 0.79 7301.33 8457.30 1.85E-02 1.923E-04 3.98E+14 5 6 2Po 5 2Se 4 2 2 87.16 8446.84 8457.30 2.09E-02 1.201E-02 1.84E+10 2 7 2Po 3 2De 6 2 4 0.62 7037.27 8502.44 5.01E-01 2.052E-03 4.32E+15 4 7 2Po 3 2De 6 4 4 0.76 7301.33 8502.44 6.25E-02 6.241E-04 7.24E+14 5 7 2Po 5 2De 6 2 4 16.39 8446.84 8502.44 1.49E-01 1.605E-02 1.85E+12 1 8 2Se 1 2Po 5 2 4 0.11 0.00 8504.22 1.69E-02 1.192E-05 4.91E+15 3 8 2Se 2 2Po 5 2 4 0.64 7085.49 8504.22 1.40E-01 5.902E-04 1.13E+15 6 8 2Se 4 2Po 5 2 4 19.42 8457.30 8504.22 1.94E-01 2.481E-02 1.72E+12 7 8 2De 6 2Po 5 4 4 513.40 8502.44 8504.22 4.48E-04 3.030E-03 1.13E+07 4 9 2Po 3 2De 6 4 6 0.74 7301.33 8527.02 5.63E-01 5.510E-03 4.53E+15 8 9 2Po 5 2De 6 4 6 39.97 8504.22 8527.02 5.39E-02 2.838E-02 1.50E+11 1 10 2Se 1 2Po 8 2 2 0.10 0.00 8916.46 2.65E-04 1.785E-07 1.69E+14 3 10 2Se 2 2Po 8 2 2 0.50 7085.49 8916.46 6.67E-03 2.187E-05 1.80E+14 6 10 2Se 4 2Po 8 2 2 1.99 8457.30 8916.46 1.05E-01 1.377E-03 1.78E+14 7 10 2De 6 2Po 8 4 2 2.20 8502.44 8916.46 7.46E-03 2.162E-04 2.05E+13 2 11 2Po 3 2Se 7 2 2 0.48 7037.27 8919.53 7.78E-03 2.480E-05 2.21E+14 4 11 2Po 3 2Se 7 4 2 0.56 7301.33 8919.53 4.60E-04 3.408E-06 1.93E+13 5 11 2Po 5 2Se 7 2 2 1.93 8446.84 8919.53 3.76E-03 4.767E-05 6.74E+12 8 11 2Po 5 2Se 7 4 2 2.19 8504.22 8919.53 3.15E-02 9.109E-04 8.73E+13 10 11 2Po 8 2Se 7 2 2 297.39 8916.46 8919.53 2.32E-02 4.550E-02 1.75E+09 2 12 2Po 3 2De 9 2 4 0.48 7037.27 8933.13 6.15E-02 1.946E-04 8.88E+14 4 12 2Po 3 2De 9 4 4 0.56 7301.33 8933.13 7.69E-03 5.656E-05 1.64E+14 5 12 2Po 5 2De 9 2 4 1.87 8446.84 8933.13 3.55E-01 4.378E-03 3.37E+14 8 12 2Po 5 2De 9 4 4 2.12 8504.22 8933.13 5.29E-02 1.480E-03 7.82E+13 10 12 2Po 8 2De 9 2 4 54.68 8916.46 8933.13 2.07E-01 7.439E-02 2.31E+11 1 13 2Se 1 2Po 8 2 4 0.10 0.00 8933.90 7.09E-07 4.765E-10 2.27E+11 3 13 2Se 2 2Po 8 2 4 0.49 7085.49 8933.90 1.22E-02 3.960E-05 1.67E+14 6 13 2Se 4 2Po 8 2 4 1.91 8457.30 8933.90 1.40E-01 1.767E-03 1.28E+14 7 13 2De 6 2Po 8 4 4 2.11 8502.44 8933.90 4.52E-04 1.258E-05 6.76E+11 9 13 2De 6 2Po 8 6 4 2.24 8527.02 8933.90 1.04E-02 4.602E-04 2.07E+13 11 13 2Se 7 2Po 8 2 4 63.41 8919.53 8933.90 2.16E-01 9.025E-02 1.79E+11 12 13 2De 9 2Po 8 4 4 1185 8933.13 8933.90 9.12E-04 1.423E-02 4.34E+06 7 14 2De 6 2Fo10 4 6 2.07 8502.44 8941.78 9.08E-01 2.481E-02 9.39E+14 9 14 2De 6 2Fo10 6 6 2.20 8527.02 8941.78 4.52E-02 1.963E-03 6.25E+13 12 14 2De 9 2Fo10 4 6 105.28 8933.13 8941.78 5.50E-02 7.631E-02 2.21E+10 4 15 2Po 3 2De 9 4 6 0.56 7301.33 8942.04 8.42E-02 6.155E-04 1.21E+15 8 15 2Po 5 2De 9 4 6 2.08 8504.22 8942.04 4.45E-01 1.218E-02 4.56E+14 13 15 2Po 8 2De 9 4 6 111.95 8933.90 8942.04 8.68E-02 1.280E-01 3.08E+10 14 15 2Fo10 2De 9 6 6 3592 8941.78 8942.04 7.40E-05 5.244E-03 3.83E+04 9 16 2De 6 2Fo10 6 8 2.17 8527.02 8946.75 9.16E-01 3.926E-02 9.72E+14 15 16 2De 9 2Fo10 6 8 193.33 8942.04 8946.75 2.75E-02 1.052E-01 3.69E+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 0.61 7.037E+03 8.527E+03 5.03E-08 1.64E+11 5.15E-02 1.50E+12 5 9 2Po 5 2De 6 2 6 11.37 8.447E+03 8.527E+03 3.90E-06 1.67E+04 4.24E-01 5.55E+06 9 10 2De 6 2Po 8 6 2 2.34 8.527E+03 8.916E+03 2.68E-06 2.19E+09 1.35E-02 1.43E+09 1 14 2Se 1 2Fo10 2 6 0.10 0.000E+00 8.942E+03 7.35E-09 6.74E+15 0.00E+00 0.00E+00 3 14 2Se 2 2Fo10 2 6 0.49 7.085E+03 8.942E+03 1.67E-07 2.55E+12 0.00E+00 0.00E+00 6 14 2Se 4 2Fo10 2 6 1.88 8.457E+03 8.942E+03 8.13E-06 1.02E+10 0.00E+00 0.00E+00 11 14 2Se 7 2Fo10 2 6 40.94 8.920E+03 8.942E+03 7.60E-05 4.13E+01 0.00E+00 0.00E+00 2 15 2Po 3 2De 9 2 6 0.48 7.037E+03 8.942E+03 2.65E-07 4.84E+12 6.00E-03 5.95E+11 5 15 2Po 5 2De 9 2 6 1.84 8.447E+03 8.942E+03 3.53E-06 5.18E+09 9.94E-02 1.17E+10 10 15 2Po 8 2De 9 2 6 35.63 8.916E+03 8.942E+03 2.44E-04 3.51E+02 1.90E+00 8.21E+04 1 16 2Se 1 2Fo10 2 8 0.10 0.000E+00 8.947E+03 9.79E-09 6.77E+15 0.00E+00 0.00E+00 3 16 2Se 2 2Fo10 2 8 0.49 7.085E+03 8.947E+03 2.23E-07 2.60E+12 0.00E+00 0.00E+00 6 16 2Se 4 2Fo10 2 8 1.86 8.457E+03 8.947E+03 1.08E-05 1.10E+10 0.00E+00 0.00E+00 7 16 2De 6 2Fo10 4 8 2.05 8.502E+03 8.947E+03 3.38E-06 1.74E+09 6.05E-01 3.11E+10 11 16 2Se 7 2Fo10 2 8 33.47 8.920E+03 8.947E+03 1.01E-04 1.69E+02 0.00E+00 0.00E+00 12 16 2De 9 2Fo10 4 8 66.89 8.933E+03 8.947E+03 6.59E-05 8.64E-01 1.86E+00 2.59E+03 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 0.13 0.000E+00 7.085E+03 0.00E+00 0.00E+00 4.33E-02 2.75E+14 2 4 2Po 3 2Po 3 2 4 3.45 7.037E+03 7.301E+03 5.02E-06 4.31E+09 1.20E+00 1.97E+11 2 5 2Po 3 2Po 5 2 2 0.65 7.037E+03 8.447E+03 0.00E+00 0.00E+00 4.12E-04 2.06E+10 4 5 2Po 3 2Po 5 4 2 0.80 7.301E+03 8.447E+03 4.33E-06 1.14E+13 1.63E-02 4.37E+11 1 6 2Se 1 2Se 4 2 2 0.11 0.000E+00 8.457E+03 0.00E+00 0.00E+00 4.94E-02 5.33E+14 3 6 2Se 2 2Se 4 2 2 0.66 7.085E+03 8.457E+03 0.00E+00 0.00E+00 1.85E-03 8.50E+10 1 7 2Se 1 2De 6 2 4 0.11 0.000E+00 8.502E+03 4.31E-08 1.28E+15 5.77E-07 3.16E+09 3 7 2Se 2 2De 6 2 4 0.64 7.085E+03 8.502E+03 1.12E-05 4.28E+13 7.05E-04 1.79E+10 6 7 2Se 4 2De 6 2 4 20.19 8.457E+03 8.502E+03 1.34E-04 1.68E+07 5.15E-05 4.22E+04 2 8 2Po 3 2Po 5 2 4 0.62 7.037E+03 8.504E+03 8.15E-07 3.70E+12 4.71E-03 1.33E+11 4 8 2Po 3 2Po 5 4 4 0.76 7.301E+03 8.504E+03 3.54E-06 5.96E+12 1.15E-02 1.79E+11 5 8 2Po 5 2Po 5 2 4 15.88 8.447E+03 8.504E+03 2.03E-04 8.44E+07 1.28E+00 2.16E+09 1 9 2Se 1 2De 6 2 6 0.11 0.000E+00 8.527E+03 5.52E-08 1.11E+15 0.00E+00 0.00E+00 3 9 2Se 2 2De 6 2 6 0.63 7.085E+03 8.527E+03 1.69E-05 4.68E+13 0.00E+00 0.00E+00 6 9 2Se 4 2De 6 2 6 13.07 8.457E+03 8.527E+03 2.13E-04 1.57E+08 0.00E+00 0.00E+00 7 9 2De 6 2De 6 4 6 37.08 8.502E+03 8.527E+03 4.53E-05 1.81E+05 2.31E+00 2.04E+08 2 10 2Po 3 2Po 8 2 2 0.49 7.037E+03 8.916E+03 0.00E+00 0.00E+00 8.93E-09 1.06E+06 4 10 2Po 3 2Po 8 4 2 0.56 7.301E+03 8.916E+03 1.10E-08 1.61E+11 2.98E-03 2.24E+11 5 10 2Po 5 2Po 8 2 2 1.94 8.447E+03 8.916E+03 0.00E+00 0.00E+00 8.88E-05 1.64E+08 8 10 2Po 5 2Po 8 4 2 2.21 8.504E+03 8.916E+03 7.56E-05 1.20E+12 8.18E-03 1.02E+10 1 11 2Se 1 2Se 7 2 2 0.10 0.000E+00 8.920E+03 0.00E+00 0.00E+00 3.00E-01 3.79E+15 3 11 2Se 2 2Se 7 2 2 0.50 7.085E+03 8.920E+03 0.00E+00 0.00E+00 3.55E-03 3.91E+11 6 11 2Se 4 2Se 7 2 2 1.97 8.457E+03 8.920E+03 0.00E+00 0.00E+00 2.57E-04 4.52E+08 7 11 2De 6 2Se 7 4 2 2.18 8.502E+03 8.920E+03 6.60E-06 1.11E+11 6.22E-07 8.05E+05 9 11 2De 6 2Se 7 6 2 2.32 8.527E+03 8.920E+03 2.43E-05 3.02E+11 0.00E+00 0.00E+00 1 12 2Se 1 2De 9 2 4 0.10 0.000E+00 8.933E+03 2.73E-07 1.04E+16 4.54E-03 2.88E+13 3 12 2Se 2 2De 9 2 4 0.49 7.085E+03 8.933E+03 8.02E-08 1.15E+12 3.71E-04 2.08E+10 6 12 2Se 4 2De 9 2 4 1.91 8.457E+03 8.933E+03 1.49E-04 2.44E+12 4.38E-05 4.20E+07 7 12 2De 6 2De 9 4 4 2.12 8.502E+03 8.933E+03 3.84E-05 3.80E+11 1.12E-03 7.96E+08 9 12 2De 6 2De 9 6 4 2.24 8.527E+03 8.933E+03 2.43E-05 1.79E+11 3.70E-03 2.21E+09 11 12 2Se 7 2De 9 2 4 67.00 8.920E+03 8.933E+03 2.32E-03 7.22E+05 3.11E-05 6.98E+02 2 13 2Po 3 2Po 8 2 4 0.48 7.037E+03 8.934E+03 1.96E-06 3.22E+13 5.87E-06 3.57E+08 4 13 2Po 3 2Po 8 4 4 0.56 7.301E+03 8.934E+03 2.60E-09 2.01E+10 5.45E-03 2.11E+11 5 13 2Po 5 2Po 8 2 4 1.87 8.447E+03 8.934E+03 1.75E-05 3.20E+11 4.24E-03 4.36E+09 8 13 2Po 5 2Po 8 4 4 2.12 8.504E+03 8.934E+03 6.01E-05 5.88E+11 2.64E-03 1.87E+09 10 13 2Po 8 2Po 8 2 4 52.27 8.916E+03 8.934E+03 2.83E-03 3.04E+06 1.31E+00 6.20E+07 2 14 2Po 3 2Fo10 2 6 0.48 7.037E+03 8.942E+03 4.73E-06 5.29E+13 0.00E+00 0.00E+00 4 14 2Po 3 2Fo10 4 6 0.56 7.301E+03 8.942E+03 1.70E-06 9.02E+12 1.36E-04 3.55E+09 5 14 2Po 5 2Fo10 2 6 1.84 8.447E+03 8.942E+03 3.27E-04 4.33E+12 0.00E+00 0.00E+00 8 14 2Po 5 2Fo10 4 6 2.08 8.504E+03 8.942E+03 1.22E-04 8.72E+11 2.75E-04 1.37E+08 10 14 2Po 8 2Fo10 2 6 35.99 8.916E+03 8.942E+03 1.69E-03 7.86E+06 0.00E+00 0.00E+00 13 14 2Po 8 2Fo10 4 6 115.55 8.934E+03 8.942E+03 4.56E-04 6.19E+03 1.07E-05 3.11E+01 1 15 2Se 1 2De 9 2 6 0.10 0.000E+00 8.942E+03 4.18E-07 1.07E+16 0.00E+00 0.00E+00 3 15 2Se 2 2De 9 2 6 0.49 7.085E+03 8.942E+03 4.97E-08 4.88E+11 0.00E+00 0.00E+00 6 15 2Se 4 2De 9 2 6 1.88 8.457E+03 8.942E+03 2.11E-04 2.52E+12 0.00E+00 0.00E+00 7 15 2De 6 2De 9 4 6 2.07 8.502E+03 8.942E+03 1.48E-05 1.09E+11 9.92E-04 5.01E+08 9 15 2De 6 2De 9 6 6 2.20 8.527E+03 8.942E+03 8.92E-05 4.89E+11 6.40E-03 2.72E+09 11 15 2Se 7 2De 9 2 6 40.48 8.920E+03 8.942E+03 3.46E-03 8.92E+06 0.00E+00 0.00E+00 12 15 2De 9 2De 9 4 6 102.29 8.933E+03 8.942E+03 8.31E-04 2.08E+04 2.36E+00 9.92E+06 4 16 2Po 3 2Fo10 4 8 0.55 7.301E+03 8.947E+03 1.02E-05 4.12E+13 0.00E+00 0.00E+00 8 16 2Po 5 2Fo10 4 8 2.06 8.504E+03 8.947E+03 7.32E-04 4.15E+12 0.00E+00 0.00E+00 13 16 2Po 8 2Fo10 4 8 70.90 8.934E+03 8.947E+03 2.73E-03 3.20E+05 0.00E+00 0.00E+00 14 16 2Fo10 2Fo10 6 8 183.46 8.942E+03 8.947E+03 2.75E-04 2.78E+02 3.37E+00 1.84E+06 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