Table 2
Observed sources.
RA (J2000.0) | Dec (J2000.0) | vLSR | Distance | ηmb | ηmb | ηmb | |
Source | (h m s) | (° ′ ″) | (km s-1) | (kpc) | (CH3OH) | (12C18O) | (13C18O) |
|
|||||||
W51 e1/e2 | 19 23 44.0 | + 14 30 29 | + 57 | 7 a | 0.43 | - | - |
NGC 2264 IRS1 | 06 41 10.1 | + 09 29 36 | + 8 | 0.9 b | 0.42 | - | - |
DR21 (OH) | 20 39 00.9 | + 42 22 38 | −3 | 3 c | 0.51 | - | - |
NGC 7538 IRS9 | 23 14 01.7 | + 61 27 20 | −57 | 2.7 d | 0.52 | 0.46 | 0.48 |
S140 IRS1 | 22 19 18.2 | + 63 18 47 | −7 | 0.9 e | 0.52 | 0.46 | 0.48 |
NGC 7538 IRS1 | 23 13 45.4 | + 61 28 11 | −57 | 2.7 d | 0.40 | - | - |
AFGL 2591 | 20 29 24.7 | + 40 11 19 | −6 | 1f | 0.47 | - | - |
|
|||||||
NGC 2024 IRS2 | 05 41 45.8 | −01 54 34 | + 12 | ||||
W3 IRS5 | 02 25 40.6 | + 62 05 51 | −39 |
Notes. The sources in the second part of the table, below the line, did not have strong enough methanol emission to be includedin the analysis, and therefore the parameters relevant for the analysis have been omitted.
References. .
Very uncertain, see Pipenbrink & Wendker (1988);
Very uncertain, see van der Tak et al. (1999)
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