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Table 3
Our quantum Stark widths W for Br VI lines compared to the results of the Cowley formula WCow (Cowley 1971) at two electrons temperatures and at electron density N = 1017 cm−3.
| Line | λ (nm) | T(104 K) | W(nm) | WCow(nm) | WCow∕W |
|---|---|---|---|---|---|
4s2 1S0−4s4p 3P |
95.825 | 1 | 1.837E−03 | 6.688E−02 | 3.46 |
| 5 | 8.294E−04 | 6.688E−02 | 8.06 | ||
4s4p 1P 4p2 3P2 |
98.142 | 1 | 5.428E−03 | 1.625E−02 | 2.99 |
| 5 | 2.337E−03 | 1.625E−02 | 6.96 | ||
4s4p 1P 4p2 3P1 |
105.055 | 1 | 3.547E−03 | 1.837E−02 | 5.18 |
| 5 | 1.608E−03 | 1.837E−02 | 11.4 | ||
4s4p 3P 4s4d 3D1 |
50.1394 | 1 | 5.433E−03 | 3.768E−03 | 0.69 |
| 5 | 2.023E−03 | 3.768E−03 | 1.86 | ||
4s4p 3P 4s4d 3D2 |
50.6325 | 1 | 4.351E−03 | 3.849E−03 | 0.88 |
| 5 | 1.807E−03 | 3.849E−03 | 2.13 | ||
4s4p 3P 4s4d 3D1 |
50.7109 | 1 | 5.675E−03 | 3.855E−03 | 0.68 |
| 5 | 2.069E−03 | 3.855E−03 | 1.86 | ||
4s4p 3P 4s4d 3D3 |
51.8426 | 1 | 3.305E−03 | 4.045E−03 | 1.22 |
| 5 | 1.329E−03 | 4.045E−03 | 3.04 | ||
4s4p 3P 4s4d 3D2 |
51.9676 | 1 | 4.354E−03 | 4.064E−03 | 0.93 |
| 5 | 1.826E−03 | 4.064E−03 | 2.23 | ||
4s4p 3P 4s4d 3D1 |
52.0502 | 1 | 4.637E−03 | 4.061E−03 | 0.88 |
| 5 | 1.903E−03 | 4.061E−03 | 2.13 | ||
4s2 1S0−4s4p 1P |
61.7041 | 1 | 1.019E−03 | 2.983E−03 | 2.93 |
| 5 | 4.626E−04 | 2.983E−03 | 6.45 |
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