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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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