Table A.2.
Measure differences (Δ(fJPL- fOBS)) and corresponding uncertainty (σΔ) between predicted (fJPL) and observed (fOBS) line frequencies.
| Star | fJPL | v, NJ | F′−F″ | Δ(fJPL- fOBS) | σΔ | Channel width |
|---|---|---|---|---|---|---|
| (MHz) | (MHz) | (MHz) | (MHz) | |||
| W Hya | ||||||
| 130078.430 |  |
13− − 13+ | -0.163 | 0.680 | 0.977 | |
| 130113.648 |  |
12− − 12+ | -0.141 | 0.667 | 0.977 | |
| 265734.656 |  |
18+ − 18− | 1.359 | 1.379 | 0.977 | |
| 265765.312 |  |
17+ − 17− | 1.600 | 1.367 | 0.977 | |
| 333394.344 |  |
17− − 17+ | 7.751 | 1.705 | 0.977 | |
| 333411.688 |  |
18− − 18+ | 6.448 | 1.873 | 0.977 | |
| 130639.219 |  |
10+ − 10− | -0.619 | 0.816 | 0.977 | |
| 130654.695 |  |
11+ − 11− | 0.754 | 0.738 | 0.977 | |
| R Dor | ||||||
| 107036.922 |  |
12+ − 12− | -0.190 | 0.721 | 0.717 | |
| 107073.172 |  |
11+ − 11− | -0.273 | 0.812 | 0.717 | |
| 252127.094 |  |
14+ − 14− | 2.605 | 1.650 | 0.977 | |
| 252145.359 |  |
15+ − 15− | 2.345 | 1.645 | 0.977 | |
| 317396.750 |  |
16+ − 16− | 5.941 | 1.854 | 1.953 | |
| 317415.312 |  |
17+ − 17− | 6.636 | 1.598 | 1.953 | |
| 351593.094 |  |
17− − 17+ | 9.528 | 1.783 | 0.488 | |
| 351611.656 |  |
18− − 18+ | 9.161 | 1.769 | 0.488 | |
| IK Tau | ||||||
| 252127.094 |  |
14+ − 14− | 2.988 | 1.633 | 1.953 | |
| 252145.359 |  |
15+ − 15− | 2.109 | 1.660 | 1.953 |
Notes. These values are also displayed in Fig. 3. In Cols. 3 and 4 we indicate the transitions specifying the quantum numbers described in the text and the positive or negative parity of the energy levels involved. In the last column we give the channel width of the different spectra.
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