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Table 3
Transitions energies/wavelengths (λ in Å), radiative transition rates (A in s-1), absorption oscillator strengths (f, dimensionless) and line strengths (S in a.u.) for E1 transitions from the 3s2 and 3s3p levels, from the current work along with values from Christensen.
| Transition | Current | Christensen | |||
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| i − j | λij | Aji | fij | S | Aji |
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| 1−3 | 3.679E+02 | 7.823E+07 | 4.762E-03 | 5.768E-03 | 2.17E+07 |
| 1−5 | 2.461E+02 | 2.774E+10 | 7.554E-01 | 6.120E-01 | 2.75E+10 |
| 1−19 | 8.922E+01 | 5.251E+05 | 1.880E-06 | 5.521E-07 | – |
| 1−23 | 8.764E+01 | 4.017E+04 | 1.388E-07 | 4.003E-08 | – |
| 1−26 | 8.097E+01 | 4.607E+08 | 1.358E-03 | 3.620E-04 | – |
| 2−8 | 2.612E+02 | 8.763E+09 | 2.689E-01 | 2.312E-01 | 8.18E+09 |
| 2−11 | 1.958E+02 | 1.650E+10 | 2.846E-01 | 1.834E-01 | 1.62E+10 |
| 2−32 | 7.451E+01 | 5.246E+07 | 1.310E-04 | 3.213E-05 | – |
| 2−36 | 5.205E+01 | 5.545E+10 | 6.757E-02 | 1.158E-02 | 5.44E+10 |
| 3−6 | 2.785E+02 | 2.141E+10 | 8.297E-02 | 2.282E-01 | 2.19E+10 |
| 3−7 | 2.717E+02 | 1.684E+09 | 3.105E-02 | 8.332E-02 | 1.85E+09 |
| 3−8 | 2.669E+02 | 6.106E+09 | 6.522E-02 | 1.719E-01 | 5.74E+09 |
| 3−9 | 2.502E+02 | 5.461E+09 | 8.538E-02 | 2.109E-01 | 5.35E+09 |
| 3−10 | 2.041E+02 | 5.481E+08 | 1.141E-03 | 2.300E-03 | 4.63E+08 |
| 3−11 | 1.990E+02 | 1.161E+10 | 6.894E-02 | 1.355E-01 | 1.16E+10 |
| 3−12 | 1.984E+02 | 2.128E+10 | 2.093E-01 | 4.101E-01 | 2.09E+10 |
| 3−14 | 1.659E+02 | 6.710E+08 | 4.614E-03 | 7.558E-03 | 6.38E+07 |
| 3−27 | 7.746E+01 | 4.253E+04 | 6.376E-08 | 4.877E-08 | – |
| 3−30 | 7.513E+01 | 4.232E+07 | 5.968E-05 | 4.428E-05 | – |
| 3−31 | 7.502E+01 | 1.137E+08 | 3.197E-05 | 2.369E-05 | – |
| 3−32 | 7.497E+01 | 3.579E+07 | 3.015E-05 | 2.233E-05 | – |
| 3−33 | 7.480E+01 | 1.211E+07 | 1.693E-05 | 1.251E-05 | – |
| 3−35 | 6.974E+01 | 1.227E+07 | 2.983E-06 | 2.055E-06 | – |
| 3−36 | 5.228E+01 | 1.665E+11 | 6.820E-02 | 3.521E-02 | 1.64E+11 |
| 3−37 | 5.155E+01 | 2.568E+09 | 3.409E-04 | 1.736E-04 | 8.28E+09 |
| 4−7 | 2.880E+02 | 2.729E+09 | 3.394E-02 | 1.609E-01 | 3.03E+09 |
| 4−8 | 2.827E+02 | 8.535E+09 | 6.135E-02 | 2.855E-01 | 8.52E+09 |
| 4−9 | 2.639E+02 | 1.548E+10 | 1.617E-01 | 7.024E-01 | 1.51E+10 |
| 4−11 | 2.077E+02 | 6.818E+08 | 2.645E-03 | 9.041E-03 | 7.08E+08 |
| 4−12 | 2.070E+02 | 6.289E+09 | 4.039E-02 | 1.376E-01 | 6.46E+09 |
| 4−13 | 2.059E+02 | 2.550E+10 | 2.268E-01 | 7.688E-01 | 2.61E+10 |
| 4−14 | 1.718E+02 | 3.522E+07 | 1.559E-04 | 4.409E-04 | 2.73E+07 |
| 4−27 | 7.873E+01 | 2.434E+04 | 2.262E-08 | 2.931E-08 | – |
| 4−28 | 7.857E+01 | 2.117E+05 | 2.742E-07 | 3.547E-07 | – |
| 4−30 | 7.632E+01 | 1.326E+07 | 1.158E-05 | 1.455E-05 | – |
| 4−32 | 7.616E+01 | 3.571E+07 | 1.863E-05 | 2.335E-05 | – |
| 4−33 | 7.599E+01 | 7.908E+07 | 6.845E-05 | 8.562E-05 | – |
| 4−36 | 5.286E+01 | 2.871E+11 | 7.214E-02 | 6.276E-02 | 2.73E+11 |
| 5−6 | 4.455E+02 | 9.704E+07 | 9.622E-04 | 4.233E-03 | 8.84E+07 |
| 5−7 | 4.282E+02 | 1.710E+09 | 7.836E-02 | 3.314E-01 | 1.85E+09 |
| 5−8 | 4.166E+02 | 1.559E+07 | 4.055E-04 | 1.668E-03 | 4.50E+06 |
| 5−9 | 3.771E+02 | 6.870E+08 | 2.441E-02 | 9.091E-02 | 6.73E+08 |
| 5−10 | 2.814E+02 | 2.490E+10 | 9.850E-02 | 2.737E-01 | 2.46E+10 |
| 5−11 | 2.719E+02 | 4.629E+07 | 5.129E-04 | 1.377E-03 | 1.38E+07 |
| 5−12 | 2.707E+02 | 3.627E+07 | 6.639E-04 | 1.775E-03 | 3.45E+05 |
| 5−14 | 2.136E+02 | 5.036E+10 | 5.739E-01 | 1.210E+00 | 5.06E+10 |
| 5−27 | 8.647E+01 | 7.395E+04 | 1.382E-07 | 1.180E-07 | – |
| 5−30 | 8.358E+01 | 5.248E+08 | 9.160E-04 | 7.560E-04 | – |
| 5−31 | 8.345E+01 | 4.461E+06 | 1.552E-06 | 1.279E-06 | – |
| 5−32 | 8.338E+01 | 4.120E+04 | 4.294E-08 | 3.536E-08 | – |
| 5−33 | 8.318E+01 | 2.195E+08 | 3.795E-04 | 3.117E-04 | – |
| 5−35 | 7.697E+01 | 2.227E+09 | 6.591E-04 | 5.010E-04 | – |
| 5−36 | 5.623E+01 | 1.915E+09 | 9.080E-04 | 5.043E-04 | 4.95E+08 |
| 5−37 | 5.539E+01 | 3.403E+11 | 5.217E-02 | 2.854E-02 | 3.40E+11 |
Notes. See Table 2 for index of levels.
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