Table C.3.
Best E-type methanol fit parameters from our detailed two components modeling.
| Region | Component | N(Sp) | Tkin | FWHM | VLSR | ISO | nH2 |
|---|---|---|---|---|---|---|---|
| [cm−2] | [K] | [km s−1] | [km s−1] | [cm−3] | |||
| 4 | 1 | 7.67×1014±1.20×1013 | 26.68 ± 0.21 | 84.78 ± 0.32 | 252 | 1.516 ± 0.025 | – |
| 2 | 4.19×1014±1.19×1013 | 32.32 ± 0.39 | 30.66 ± 0.25 | 248 | 1.295 ± 0.061 | – | |
| 8 | 1 | 1.35×1014±1.29×1013 | 24.76 ± 0.80 | 75.59 ± 0.37 | 205 | 1.984 ± 0.121 | 2.777( ± 0.101)×108 |
| 2 | 1.34×1015±5.00×1013 | 14.84 ± 0.32 | 62.42 ± 0.68 | 200 | 3.141 ± 0.578 | 5.949(±0.279)×105 |
Notes. Uncertainties correspond to 3σ. Velocity uncertainties (not shown) correspond to less than 10% of the instrumental uncertainty (∼8–9 km s−1). Column density (N(Sp)) values for A-type methanol can be obtained dividing them by the ISO number (column density ratio of E- over A-type methanol, see Appendix C), while the rest of the parameters are the same for both methanol symmetric types. The minus symbol (-) indicates that no nH2 was derived as the model is in LTE.
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