Table 1
Column densities, rotational temperatures, and fractional abundances of all the observed molecules in the NE lobe of M 82.
Moleculea | Nmol (cm-2) | Trotb (K) | Nmol/NC34S | ||||||
|
|||||||||
C2H | (1.3 ± 0.6) × 1015 | 20.0 ± 10.0 | 118.2 ± 60.7 | ||||||
NO | (1.2 ± 0.1) × 1015 | 8.8 ± 4.4 | 109.1 ± 10.7 | ||||||
CH3CCHc | (1.2 ± 0.1) × 1015 | 31.6 ± 0.1 | 109.1 ± 10.7 | ||||||
CS (1)c | (2.0 ± 0.1) × 1014 | 5.9 ± 0.1 | 22.0 ± 1.7 | ||||||
CS (2)c | (4.2 ± 0.1) × 1013 | 14.7 ± 0.8 | ... | ||||||
CH3OH | (1.2 ± 1.1) × 1014 | 26.2 ± 11.7 | 10.9 ± 11.7 | ||||||
H2CO | (1.1 ± 0.2) × 1014 | 25.5 ± 3.0 | 10.0 ± 2.7 | ||||||
H2 S | (6.1 ± 4.5) × 1013 | 20.0 ± 10.0 | 5.5 ± 5.2 | ||||||
c-C3H2 | (4.8 ± 1.3) × 1013 | 10.1 ± 1.2 | 4.4 ± 2.0 | ||||||
HCO | (3.9 ± 2.8) × 1013 | 20.0 ± 10.0 | 3.5 ± 3.5 | ||||||
SO† | (3.7 ± 0.5) × 1013 | 20.0 ± 10.0 | 3.4 ± 1.2 | ||||||
H2CS | (3.1 ± 2.5) × 1013 | 20.0 ± 10.0 | 2.8 ± 3.2 | ||||||
HC3Nc | (2.5 ± 1.2) × 1013 | 24.2 ± 3.9 | 2.3 ± 1.9 | ||||||
SO2 | (1.2 ± 0.6) × 1013 | 20.0 ± 10.0 | 1.1 ± 1.3 | ||||||
NH2 CN | (1.2 ± 1.5) × 1013 | 80.3 ± 52.9 | 1.1 ± 2.2 | ||||||
C34S | (1.1 ± 0.7) × 1013 | 20.0 ± 10.0 | 1.0 ± 1.0 | ||||||
CH3 CN | (6.4 ± 1.2) × 1012 | 32.9 ± 1.6 | 0.6 ± 0.8 | ||||||
H13 CN | (1.7 ± 1.6) × 1012 | 20.0 ± 10.0 | 0.2 ± 0.9 | ||||||
H13CO+ | (1.3 ± 0.8) × 1012 | 20.0 ± 10.0 | 0.1 ± 0.8 | ||||||
|
|||||||||
C18Od | (3.5 ± 1.7) × 1016 | 20.0 ± 10.0 | 3181.8 ± 1700.7 | ||||||
CNe | (2.0 ± 0.5) × 1014 | ... | 18.2 ± 5.7 | ||||||
HCNe | (4.0 ± 0.5) × 1013 | ... | 3.6 ± 1.2 | ||||||
HNCf | 2.2 × 1013 | 10.0 | 2.0 | ||||||
CO+g | (6.6 ± 3.4) × 1012 | 20.0 ± 10.0 | 0.6 ± 1.0 | ||||||
HOC+h | (3.9 ± 1.9) × 1012 | 20.0 ± 10.0 | 0.4 ± 0.9 |
Notes.
Some molecules do not have a wide enough dynamic range in energy to calculate the rotational temperature with precision. For them, we assumed Trot = 20 ± 10 K (see Sect. 3.4 and Appendix A for details).
Some extra detections observed by Aladro et al. (2011) were used. CS shows two components with different column densities and rotational values corresponding to the two fits that result from its Boltzmann diagram. The fractional abundance value is in this case [NCS(1) + NCS(2)] /NC34S. The molecules shown at the bottom of the table were observed by:
Fuente et al. (2005) (averaged value for the galaxy disk);
Hüttemeister et al. (1995) (averaged value for the nuclear zone);
Only upper limits were reported until now: SO, and SO2 by Petuchowski & Bennett (1992), and H13CN by Wild et al. (1990).
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