*************************** 786 ******************************************* Ref. "K$_{\alpha}$ resonance fluorescence in Al, Ti, Cu and potential applications for X-ray sources", Sultana N. Nahar and Anil K. Pradhan, JQSRT 155, 32-48 (2015) ************************************************************************** Ti21+: 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: Ti21+ + h\nu <-> Ti21+* 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 = 22, 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) Table of LS term energies ------------------- LS energies: i SLP E(Rel,Ry) cfg# 1 2Se 0.000000 1 2 2Po 363.000476 3 3 2Se 363.000482 2 4 2De 430.222670 6 5 2Po 430.222685 5 6 2Se 430.222694 4 7 2Fo 453.750444 10 8 2De 453.750452 9 9 2Po 453.750465 8 10 2Se 453.750471 7 Number of first LS terms optimized = 10 ************************************************************************* 3) Table of 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 363.0005 1.468E+14 4.16E-01 4.16E-01 0.0E+00 1 2Se: 1 5 2Po: 5 0.0000 430.2227 3.920E+13 7.91E-02 7.91E-02 0.0E+00 1 2Se: 1 9 2Po: 8 0.0000 453.7505 1.598E+13 2.90E-02 2.90E-02 1.7E-02 2 2Po: 3 4 2De: 6 363.0005 430.2227 1.515E+13 6.96E-01 6.96E-01 4.8E-04 2 2Po: 3 6 2Se: 4 363.0005 430.2227 1.480E+12 1.36E-02 1.36E-02 2.5E-02 2 2Po: 3 8 2De: 9 363.0005 453.7505 4.834E+12 1.22E-01 1.22E-01 0.0E+00 2 2Po: 3 10 2Se: 7 363.0005 453.7505 6.043E+11 3.04E-03 3.05E-03 1.6E-01 3 2Se: 2 5 2Po: 5 363.0005 430.2227 5.261E+12 4.35E-01 4.35E-01 2.3E-03 3 2Se: 2 9 2Po: 8 363.0005 453.7505 2.266E+12 1.03E-01 1.03E-01 9.7E-03 4 2De: 6 7 2Fo:10 430.2227 453.7504 3.232E+12 1.02E+00 1.02E+00 0.0E+00 4 2De: 6 9 2Po: 8 430.2227 453.7505 8.145E+10 1.10E-02 1.10E-02 0.0E+00 5 2Po: 5 8 2De: 9 430.2227 453.7505 1.649E+12 6.18E-01 6.18E-01 5.4E-04 5 2Po: 5 10 2Se: 7 430.2227 453.7505 4.302E+11 3.23E-02 3.23E-02 0.0E+00 6 2Se: 4 9 2Po: 8 430.2227 453.7505 7.184E+11 4.85E-01 4.85E-01 1.0E-03 LS transitions: Number of oscillator strengths = 14 Comparison of LS term energies: relativistic(r) & pure LS: Expt theory %diff config term E(Ry) term E(LSr) CF term E(LS) CF 1 2Se 0.0000 1 2Se 0.0000 1 2 2Se 365.1594 2 2Po 363.0005 3 3 2Po 365.6744 3 2Se 363.0005 2 4 2Se 433.0123 4 2De 430.2227 6 5 2Po 433.1620 5 2Po 430.2227 5 6 2De 433.2842 6 2Se 430.2227 4 7 2Se 456.7279 7 2Fo 453.7504 10 8 2Po 456.7895 8 2De 453.7505 9 9 2De 456.8401 9 2Po 453.7505 8 10 2Fo 456.8623 10 2Se 453.7505 7 ****************************************************************************** 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 40070685.0 3.65151E+02 3 2Se( 2) 2 40071611.0 3.65159E+02 4 2Po( 3) 4 40156840.0 3.65936E+02 5 2Po( 5) 2 47517298.0 4.33009E+02 6 2Se( 4) 2 47517609.0 4.33012E+02 7 2De( 6) 4 47542363.0 4.33238E+02 8 2Po( 5) 4 47542398.0 4.33238E+02 9 2De( 6) 6 47550835.0 4.33315E+02 10 2Po( 8) 2 50119962.0 4.56727E+02 11 2Se( 7) 2 50120095.0 4.56728E+02 12 2De( 9) 4 50130283.0 4.56821E+02 13 2Po( 8) 4 50130303.0 4.56821E+02 14 2Fo(10) 6 50133820.0 4.56853E+02 15 2De( 9) 6 50133826.0 4.56853E+02 16 2Fo(10) 8 50135602.0 4.56869E+02 ****************************************************************************** 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 2.50 0.00 365.15 1.36E-01 2.231E-03 1.45E+14 2 3 2Po 3 2Se 2 2 2 107903 365.15 365.16 5.17E-05 3.673E-02 2.96E+01 1 4 2Se 1 2Po 3 2 4 2.49 0.00 365.94 2.71E-01 4.436E-03 1.46E+14 3 4 2Se 2 2Po 3 2 4 1173 365.16 365.94 9.59E-03 7.405E-02 2.32E+07 1 5 2Se 1 2Po 5 2 2 2.10 0.00 433.01 2.45E-02 3.401E-04 3.70E+13 3 5 2Se 2 2Po 5 2 2 13.43 365.16 433.01 1.42E-01 1.256E-02 5.25E+12 2 6 2Po 3 2Se 4 2 2 13.43 365.15 433.01 1.26E-02 1.115E-03 4.66E+11 4 6 2Po 3 2Se 4 4 2 13.59 365.94 433.01 1.42E-02 2.537E-03 1.02E+12 5 6 2Po 5 2Se 4 2 2 321877 433.01 433.01 1.05E-04 2.217E-01 6.74E+00 2 7 2Po 3 2De 6 2 4 13.38 365.15 433.24 6.84E-01 6.026E-02 1.27E+13 4 7 2Po 3 2De 6 4 4 13.54 365.94 433.24 6.92E-02 1.234E-02 2.52E+12 5 7 2Po 5 2De 6 2 4 3989 433.01 433.24 1.06E-02 2.790E-01 2.22E+06 1 8 2Se 1 2Po 5 2 4 2.10 0.00 433.24 5.03E-02 6.960E-04 3.79E+13 3 8 2Se 2 2Po 5 2 4 13.39 365.16 433.24 2.78E-01 2.449E-02 5.17E+12 6 8 2Se 4 2Po 5 2 4 4034 433.01 433.24 1.68E-02 4.453E-01 3.44E+06 4 9 2Po 3 2De 6 4 6 13.52 365.94 433.32 6.23E-01 1.109E-01 1.51E+13 8 9 2Po 5 2De 6 4 6 11853 433.24 433.32 3.21E-03 5.016E-01 1.02E+05 1 10 2Se 1 2Po 8 2 2 2.00 0.00 456.73 8.15E-03 1.071E-04 1.37E+13 3 10 2Se 2 2Po 8 2 2 9.95 365.16 456.73 3.14E-02 2.056E-03 2.11E+12 6 10 2Se 4 2Po 8 2 2 38.43 433.01 456.73 1.56E-01 3.946E-02 7.04E+11 7 10 2De 6 2Po 8 4 2 38.80 433.24 456.73 9.30E-03 4.749E-03 8.24E+10 2 11 2Po 3 2Se 7 2 2 9.95 365.15 456.73 2.16E-03 1.416E-04 1.46E+11 4 11 2Po 3 2Se 7 4 2 10.04 365.94 456.73 2.87E-03 3.791E-04 3.80E+11 5 11 2Po 5 2Se 7 2 2 38.42 433.01 456.73 2.95E-02 7.452E-03 1.33E+11 8 11 2Po 5 2Se 7 4 2 38.79 433.24 456.73 3.29E-02 1.681E-02 2.92E+11 10 11 2Po 8 2Se 7 2 2 749785 456.73 456.73 1.52E-04 7.497E-01 1.80E+00 2 12 2Po 3 2De 9 2 4 9.94 365.15 456.82 1.18E-01 7.717E-03 3.98E+12 4 12 2Po 3 2De 9 4 4 10.03 365.94 456.82 1.19E-02 1.569E-03 7.88E+11 5 12 2Po 5 2De 9 2 4 38.27 433.01 456.82 5.96E-01 1.502E-01 1.36E+12 8 12 2Po 5 2De 9 4 4 38.64 433.24 456.82 6.13E-02 3.117E-02 2.74E+11 10 12 2Po 8 2De 9 2 4 9688 456.73 456.82 1.88E-02 1.200E+00 6.68E+05 1 13 2Se 1 2Po 8 2 4 2.00 0.00 456.82 1.71E-02 2.243E-04 1.43E+13 3 13 2Se 2 2Po 8 2 4 9.94 365.16 456.82 6.32E-02 4.140E-03 2.13E+12 6 13 2Se 4 2Po 8 2 4 38.27 433.01 456.82 3.04E-01 7.673E-02 6.93E+11 7 13 2De 6 2Po 8 4 4 38.64 433.24 456.82 1.73E-03 8.812E-04 7.74E+09 9 13 2De 6 2Po 8 6 4 38.77 433.32 456.82 1.10E-02 8.421E-03 7.32E+10 11 13 2Se 7 2Po 8 2 4 9796 456.73 456.82 2.32E-02 1.496E+00 8.06E+05 7 14 2De 6 2Fo10 4 6 38.59 433.24 456.85 1.01E+00 5.137E-01 3.02E+12 9 14 2De 6 2Fo10 6 6 38.71 433.32 456.85 4.83E-02 3.691E-02 2.15E+11 12 14 2De 9 2Fo10 4 6 28274 456.82 456.85 3.37E-03 1.255E+00 1.88E+04 4 15 2Po 3 2De 9 4 6 10.02 365.94 456.85 1.08E-01 1.426E-02 4.78E+12 8 15 2Po 5 2De 9 4 6 38.59 433.24 456.85 5.49E-01 2.791E-01 1.64E+12 13 15 2Po 8 2De 9 4 6 28387 456.82 456.85 5.75E-03 2.148E+00 3.17E+04 9 16 2De 6 2Fo10 6 8 38.69 433.32 456.87 9.66E-01 7.381E-01 3.23E+12 15 16 2De 9 2Fo10 6 8 56290 456.85 456.87 1.61E-03 1.788E+00 2.54E+03 Number of non-zero E1 transitions = 45 Number of dipole transitions, E1d = 45 Number of lines in the table = 68 ************************************************************************* 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 = 45 Number of intercombination transitions, E1i = 0 Number of lines in the table = 68 *******************************************************************************" 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 13.37 3.652E+02 4.333E+02 8.15E-04 1.12E+06 1.54E+00 8.96E+06 5 9 2Po 5 2De 6 2 6 2981 4.330E+02 4.333E+02 2.58E-02 1.29E-09 7.16E+00 7.55E-05 9 10 2De 6 2Po 8 6 2 38.92 4.333E+02 4.567E+02 1.66E-02 3.87E+04 1.29E-01 1.08E+04 1 14 2Se 1 2Fo10 2 6 1.99 0.000E+00 4.569E+02 5.89E-08 4.91E+07 0.00E+00 0.00E+00 3 14 2Se 2 2Fo10 2 6 9.94 3.652E+02 4.569E+02 6.71E-04 7.34E+06 0.00E+00 0.00E+00 6 14 2Se 4 2Fo10 2 6 38.22 4.330E+02 4.569E+02 7.35E-02 6.46E+04 0.00E+00 0.00E+00 11 14 2Se 7 2Fo10 2 6 7285 4.567E+02 4.569E+02 3.77E-01 3.62E-11 0.00E+00 0.00E+00 2 15 2Po 3 2De 9 2 6 9.94 3.652E+02 4.569E+02 5.06E-06 5.55E+04 2.00E-01 5.12E+06 5 15 2Po 5 2De 9 2 6 38.22 4.330E+02 4.569E+02 6.88E-02 6.05E+04 3.83E+00 1.17E+05 10 15 2Po 8 2De 9 2 6 7212 4.567E+02 4.569E+02 1.25E+00 1.29E-10 3.07E+01 3.91E-06 1 16 2Se 1 2Fo10 2 8 1.99 0.000E+00 4.569E+02 7.85E-08 4.92E+07 0.00E+00 0.00E+00 3 16 2Se 2 2Fo10 2 8 9.94 3.652E+02 4.569E+02 8.95E-04 7.35E+06 0.00E+00 0.00E+00 6 16 2Se 4 2Fo10 2 8 38.20 4.330E+02 4.569E+02 9.80E-02 6.49E+04 0.00E+00 0.00E+00 7 16 2De 6 2Fo10 4 8 38.56 4.332E+02 4.569E+02 2.71E-02 1.68E+04 1.25E+01 2.74E+05 11 16 2Se 7 2Fo10 2 8 6448 4.567E+02 4.569E+02 5.02E-01 8.51E-11 0.00E+00 0.00E+00 12 16 2De 9 2Fo10 4 8 18800 4.568E+02 4.569E+02 3.44E-01 3.25E-14 3.06E+01 2.43E-08 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 2.50 0.000E+00 3.652E+02 0.00E+00 0.00E+00 7.96E-05 6.91E+07 2 4 2Po 3 2Po 3 2 4 1160 3.652E+02 3.659E+02 2.01E-03 4.00E-01 1.33E+00 5.72E+03 2 5 2Po 3 2Po 5 2 2 13.43 3.652E+02 4.330E+02 0.00E+00 0.00E+00 2.36E-06 1.31E+04 4 5 2Po 3 2Po 5 4 2 13.59 3.659E+02 4.330E+02 1.48E-03 2.69E+09 6.88E-05 3.70E+05 1 6 2Se 1 2Se 4 2 2 2.10 0.000E+00 4.330E+02 0.00E+00 0.00E+00 2.33E-05 3.37E+07 3 6 2Se 2 2Se 4 2 2 13.43 3.652E+02 4.330E+02 0.00E+00 0.00E+00 8.96E-06 4.99E+04 1 7 2Se 1 2De 6 2 4 2.10 0.000E+00 4.332E+02 7.00E-06 7.14E+10 6.67E-07 4.83E+05 3 7 2Se 2 2De 6 2 4 13.39 3.652E+02 4.332E+02 6.07E-03 5.94E+09 2.00E-06 5.62E+03 6 7 2Se 4 2De 6 2 4 4039 4.330E+02 4.332E+02 4.57E-02 1.78E-02 7.40E-08 7.57E-06 2 8 2Po 3 2Po 5 2 4 13.38 3.652E+02 4.332E+02 1.37E-03 1.34E+09 2.81E-05 7.91E+04 4 8 2Po 3 2Po 5 4 4 13.54 3.659E+02 4.332E+02 1.46E-03 1.34E+09 3.48E-05 9.47E+04 5 8 2Po 5 2Po 5 2 4 3984 4.330E+02 4.332E+02 7.28E-02 3.04E-02 1.33E+00 1.42E+02 1 9 2Se 1 2De 6 2 6 2.10 0.000E+00 4.333E+02 1.05E-05 7.13E+10 0.00E+00 0.00E+00 3 9 2Se 2 2De 6 2 6 13.37 3.652E+02 4.333E+02 9.11E-03 5.97E+09 0.00E+00 0.00E+00 6 9 2Se 4 2De 6 2 6 3009 4.330E+02 4.333E+02 6.89E-02 7.81E-02 0.00E+00 0.00E+00 7 9 2De 6 2De 6 4 6 11803 4.332E+02 4.333E+02 1.54E-02 1.88E-05 2.40E+00 6.55E+00 2 10 2Po 3 2Po 8 2 2 9.95 3.652E+02 4.567E+02 0.00E+00 0.00E+00 6.84E-07 9.36E+03 4 10 2Po 3 2Po 8 4 2 10.04 3.659E+02 4.567E+02 1.22E-04 1.01E+09 1.62E-05 2.16E+05 5 10 2Po 5 2Po 8 2 2 38.42 4.330E+02 4.567E+02 0.00E+00 0.00E+00 6.93E-07 1.65E+02 8 10 2Po 5 2Po 8 4 2 38.80 4.332E+02 4.567E+02 2.97E-02 2.84E+08 6.07E-05 1.40E+04 1 11 2Se 1 2Se 7 2 2 2.00 0.000E+00 4.567E+02 0.00E+00 0.00E+00 1.86E-05 3.15E+07 3 11 2Se 2 2Se 7 2 2 9.95 3.652E+02 4.567E+02 0.00E+00 0.00E+00 3.48E-06 4.76E+04 6 11 2Se 4 2Se 7 2 2 38.42 4.330E+02 4.567E+02 0.00E+00 0.00E+00 2.17E-06 5.17E+02 7 11 2De 6 2Se 7 4 2 38.79 4.332E+02 4.567E+02 4.72E-03 4.51E+07 3.61E-10 8.34E-02 9 11 2De 6 2Se 7 6 2 38.92 4.333E+02 4.567E+02 7.39E-03 6.95E+07 0.00E+00 0.00E+00 1 12 2Se 1 2De 9 2 4 2.00 0.000E+00 4.568E+02 4.61E-06 6.13E+10 1.66E-07 1.41E+05 3 12 2Se 2 2De 9 2 4 9.94 3.652E+02 4.568E+02 1.17E-04 5.05E+08 5.53E-07 3.80E+03 6 12 2Se 4 2De 9 2 4 38.27 4.330E+02 4.568E+02 8.43E-02 4.31E+08 1.92E-07 2.31E+01 7 12 2De 6 2De 9 4 4 38.64 4.332E+02 4.568E+02 1.91E-02 9.31E+07 4.14E-06 4.84E+02 9 12 2De 6 2De 9 6 4 38.77 4.333E+02 4.568E+02 8.35E-03 4.00E+07 1.35E-05 1.56E+03 11 12 2Se 7 2De 9 2 4 9815 4.567E+02 4.568E+02 6.61E-01 3.05E-03 4.73E-08 3.37E-07 2 13 2Po 3 2Po 8 2 4 9.94 3.652E+02 4.568E+02 9.31E-05 4.03E+08 5.25E-06 3.60E+04 4 13 2Po 3 2Po 8 4 4 10.03 3.659E+02 4.568E+02 1.25E-04 5.17E+08 1.14E-05 7.61E+04 5 13 2Po 5 2Po 8 2 4 38.27 4.330E+02 4.568E+02 2.73E-02 1.40E+08 3.94E-05 4.74E+03 8 13 2Po 5 2Po 8 4 4 38.64 4.332E+02 4.568E+02 2.92E-02 1.42E+08 1.04E-05 1.22E+03 10 13 2Po 8 2Po 8 2 4 9669 4.567E+02 4.568E+02 8.24E-01 4.09E-03 1.33E+00 9.93E+00 2 14 2Po 3 2Fo10 2 6 9.94 3.652E+02 4.569E+02 1.94E-03 5.60E+09 0.00E+00 0.00E+00 4 14 2Po 3 2Fo10 4 6 10.02 3.659E+02 4.569E+02 5.65E-04 1.56E+09 5.43E-07 2.42E+03 5 14 2Po 5 2Fo10 2 6 38.22 4.330E+02 4.569E+02 1.54E-01 5.29E+08 0.00E+00 0.00E+00 8 14 2Po 5 2Fo10 4 6 38.59 4.332E+02 4.569E+02 4.49E-02 1.47E+08 8.28E-07 6.48E+01 10 14 2Po 8 2Fo10 2 6 7215 4.567E+02 4.569E+02 4.64E-01 6.64E-03 0.00E+00 0.00E+00 13 14 2Po 8 2Fo10 4 6 28434 4.568E+02 4.569E+02 1.32E-01 1.98E-06 1.94E-08 3.79E-09 1 15 2Se 1 2De 9 2 6 2.00 0.000E+00 4.569E+02 6.95E-06 6.16E+10 0.00E+00 0.00E+00 3 15 2Se 2 2De 9 2 6 9.94 3.652E+02 4.569E+02 1.80E-04 5.20E+08 0.00E+00 0.00E+00 6 15 2Se 4 2De 9 2 6 38.22 4.330E+02 4.569E+02 1.26E-01 4.33E+08 0.00E+00 0.00E+00 7 15 2De 6 2De 9 4 6 38.59 4.332E+02 4.569E+02 8.14E-03 2.66E+07 4.17E-06 3.26E+02 9 15 2De 6 2De 9 6 6 38.71 4.333E+02 4.569E+02 3.32E-02 1.07E+08 2.08E-05 1.61E+03 11 15 2Se 7 2De 9 2 6 7282 4.567E+02 4.569E+02 9.91E-01 1.35E-02 0.00E+00 0.00E+00 12 15 2De 9 2De 9 4 6 28227 4.568E+02 4.569E+02 2.48E-01 3.88E-06 2.40E+00 4.79E-01 4 16 2Po 3 2Fo10 4 8 10.02 3.659E+02 4.569E+02 3.39E-03 7.04E+09 0.00E+00 0.00E+00 8 16 2Po 5 2Fo10 4 8 38.56 4.332E+02 4.569E+02 2.69E-01 6.63E+08 0.00E+00 0.00E+00 13 16 2Po 8 2Fo10 4 8 18870 4.568E+02 4.569E+02 7.90E-01 6.93E-05 0.00E+00 0.00E+00 14 16 2Fo10 2Fo10 6 8 56105 4.569E+02 4.569E+02 8.43E-02 3.18E-08 3.43E+00 6.54E-02 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 = = 45 + 107 = 152