Table 4
Conjugate inversion and anti-inversion of satellite lines.
| Name | 1612 | 1720 | v |
|---|---|---|---|
| [km s−1] | |||
| G18.303−0.390 | E | A | 31.5 |
| G19.075−0.288 | A | E | 58.5 |
| R | R | 67.5 | |
| E | A | 70.0 | |
| G25.396+0.033 | E | A | −12.0 |
| G25.397−0.141 | E | A | 96.0 |
| G29.935−0.053 | A | – | 97.0 |
| R | – | 98.5 | |
| E | A | 100.0 | |
| G29.957−0.018 | E | A | 100.5 |
| G30.535+0.021 | E | A | 45.0 |
| G30.535+0.021 | A | E | 92.0 |
| G30.720−0.083 | E | A | 93.0 |
| G30.783−0.028 | E | A | 82.0 |
| G32.151+0.132 | E | A | 94.5 |
| G32.798+0.190 | A | E | 12.0 |
| R | R | 14.0 | |
| E | A | 18.0 | |
| G32.798+0.190 | A | E | 90.0 |
| G33.915+0.110 | E | A | 105.0 |
| G37.764−0.215 | A | – | 62.5 |
| R | R | 65.0 | |
| – | A | 67.5 | |
| G37.874−0.399 | E | A | 58.5 |
| G38.876+0.308 | E | A | −16.5 |
| G39.883−0.346 | E | A | 57.0 |
| G41.741+0.097 | E | A | 14.0 |
| G49.206−0.342 | A | – | 65.0 |
| R | – | 66.0 | |
| E | A | 68.0 | |
| G49.369−0.302 | A | – | 49.0 |
| R | – | 49.5 | |
| E | A | 53.0 | |
| G49.369−0.302 | A | E | 62.5 |
| R | R | 63.5 | |
| E | A | 65.0 | |
| G49.459−0.353 | A | E | 69.0 |
| G60.882−0.132 | E | A | 22.5 |
Notes. Cols. 2 and 3 indicate conjugate absorption (A) and emission (E) of the OH 1612 MHz and OH 1720 MHz transitions. The corresponding velocity is given in Col. 4. In some cases, 1612 MHz absorption and 1720 MHz emission transform into 1612 MHz emission and 1720 MHz absorption at higher velocities. For this kind of profile we give three entries: the central velocities of absorption and emission as well as the velocity, at which the reversal (R) of the line profile occurs. This is defined here as the velocity at which the satellite lines are equal. Components of the reversal profile that are not detected significantly are indicated by a horizontal dash.
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