Table B.5
Excitation temperatures (in K) derived with MADCUBA.
source | SO | CCS | HCS+ | OCS | SO2 |
---|---|---|---|---|---|
HMSCs | |||||
00117b | 11.9(0.4) | 12(3) | 13(3) | – | – |
AFGLa | 11(1) | 18(3) | 12.8(0.7) | 73(b) | |
05358a | 24.2(1.0) | 17(3) | 22.0(1.0) | 76(3) | 68(3) |
20293a | 12.6(0.4) | 12(3) | 12.1(0.9) | – | – |
22134b | 10.7(0.4) | 12(4) | 12(2) | – | – |
HMPOs | |||||
00117a | 16.7(0.4) | 13(3) | 19(2) | 21 | – |
05358b | 20.9(0.5) | 26(4) | 16.6(0.6) | 66(5) | 63(5) |
18517 | 25.8(0.6) | 21(3) | 26.4(0.9) | 60(3) | 48(4) |
21307 | 16.5(0.9) | 16(4) | 25(2) | 21 | 17(2) |
23385 | 33.0(0.6) | 22(3) | 27.8(1.0) | 48(2) | 56(5) |
UCHIIs | |||||
G75 | 18.4(0.9) | 29(5) | 27.3(0.5) | 54(4) | 47(5) |
19410 | 23.4(0.4) | 25(2) | 21.5(0.3) | 85(8) | 42(5) |
22134 | 23.9(0.6) | 25(5) | 14.3(1.2) | – | 62(6) |
23033 | 21.3(0.4) | 13(2) | 14.4(0.6) | 105(8) | 50(4) |
NGC7538 | 49.7(1.0) | 21(3) | 22.3(0.5) | 90(6) | 93(7) |
Notes. The values without uncertainty are the temperatures we assumed to derive the upper limits on the total column densities. (a)the J = 18 17 line is too strong with respect to the LTE predictions. It is unlikely that the discrepancy in intensity between this line and the LTE prediction is due to contamination with nearby lines because no reliable candidates have been found around it; (b) Tex needs to be fixed to 73 K to obtain a reasonable fit, but the J(Ka, Kb) = 11(1,11) − 10(0,10) intensity is largely underestimated probably due to contamination with methyl formate J(Ka, Kb) = 11(5,6) − 11(3,9) at 221.969 GHz.
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