From: Computation of hyperfine multiplet oscillator strengths in Tantalum atom
Upper level | Lower level | Wave number (cm−1) | Intensity | Log hf gh | ||
---|---|---|---|---|---|---|
Energy (cm−1) | F | Energy (cm−1) | F | |||
30664.684 | 1 | 0 | 1 | 30664.51 | 3.750 | − 3.8352 |
1 | 2 | 30664.45 | 8.750 | − 3.4845 | ||
2 | 1 | 30664.64 | 8.750 | − 3.4845 | ||
2 | 2 | 30664.58 | 0.231 | − 4.7351 | ||
2 | 3 | 30664.52 | 11.852 | − 3.3562 | ||
3 | 2 | 30664.75 | 11.852 | − 3.3562 | ||
3 | 3 | 30664.68 | 7.940 | − 3.5254 | ||
3 | 4 | 30664.64 | 9.375 | − 3.4555 | ||
4 | 3 | 30664.84 | 9.375 | − 3.4555 | ||
4 | 4 | 30664.80 | 28.125 | − 2.9867 | ||
30664.684 | 1 | 2010.134 | 0 | 28654.38 | 2.778 | − 3.8075 |
1 | 1 | 28654.36 | 5.833 | − 3.5001 | ||
1 | 2 | 28654.33 | 3.889 | − 3.6694 | ||
2 | 1 | 28654.49 | 2.500 | − 3.8502 | ||
2 | 2 | 28654.46 | 8.333 | − 3.3494 | ||
2 | 3 | 28654.42 | 10.000 | − 3.2718 | ||
3 | 2 | 28654.62 | 1.667 | − 4.0111 | ||
3 | 3 | 28654.58 | 8.750 | − 3.3286 | ||
3 | 4 | 28654.54 | 18.750 | − 3.0026 | ||
4 | 3 | 28654.74 | 0.694 | − 4.3331 | ||
4 | 4 | 28654.70 | 6.250 | − 3.4711 | ||
4 | 5 | 28654.66 | 30.556 | − 2.7922 | ||
30664.684 | 1 | 6068.956 | 0 | 24595.59 | 2.778 | − 2.9920 |
1 | 1 | 24595.56 | 5.833 | − 2.6720 | ||
1 | 2 | 24595.52 | 3.889 | − 2.8471 | ||
2 | 1 | 24595.69 | 2.500 | − 3.0373 | ||
2 | 2 | 24595.65 | 8.333 | − 2.5177 | ||
2 | 3 | 24595.60 | 10.000 | − 2.4388 | ||
3 | 2 | 24595.81 | 1.667 | − 3.2110 | ||
3 | 3 | 24595.76 | 8.750 | − 2.4966 | ||
3 | 4 | 24595.71 | 18.750 | − 2.1664 | ||
4 | 3 | 24595.92 | 0.694 | − 3.5815 | ||
4 | 4 | 24595.87 | 6.250 | − 2.6422 | ||
4 | 5 | 24595.83 | 30.556 | − 1.9545 | ||
30664.684 | 1 | 11243.656 | 1 | 19420.93 | 3.750 | − 3.2875 |
1 | 2 | 19420.88 | 8.750 | − 2.9243 | ||
2 | 1 | 19421.06 | 8.750 | − 2.9243 | ||
2 | 2 | 19421.01 | 0.231 | − 4.3848 | ||
2 | 3 | 19420.90 | 11.852 | − 2.7935 | ||
3 | 2 | 19421.17 | 11.852 | − 2.7935 | ||
3 | 3 | 19421.07 | 7.940 | − 2.9662 | ||
3 | 4 | 19420.88 | 9.375 | − 2.8946 | ||
4 | 3 | 19421.23 | 9.375 | − 2.8946 | ||
4 | 4 | 19421.04 | 28.125 | − 2.4198 |