Table 2
Line parameters for the various species for which we estimated the column density.
Species | Transition(a) | Eu [K] | log10(Auls−1) | gu | Q(18.75 K) | Q(37.50 K) | Q(75 K) | ![]() |
---|---|---|---|---|---|---|---|---|
C18O | 2–1 | 15.81 | −6.22 | 5 | 7.461 | 14.57 | 28.81 | ![]() |
H2CO | 30,3−20,2 | 21.0 | −3.55 | 7 | 44.68 | 128.7 | 361.7 | ![]() |
H2CO | 32,1−22,0 | 68.1 | −3.80 | 7 | 44.68 | 128.7 | 361.7 | ![]() |
C2H | 37/2,4−25/2,3 | 25.16 | −4.3 | 9 | 37.14 | 72.91 | 144.7 | ![]() |
C2H | 37/2,3−25/2,2 | 25.15 | −4.3 | 7 | 37.14 | 72.91 | 144.7 | ![]() |
H13CN | 3–2 | 24.86 | −3.11 | 21 | 28.17 | 55.31 | 109.6 | ![]() |
HC15N | 3–2 | 24.78 | −3.11 | 7 | 9.421 | 18.50 | 36.66 | ![]() |
DCN | 3–2 | 20.85 | −3.33 | 21 | 33.39 | 65.75 | 130.5 | ![]() |
H13CO+ | 3–2 | 24.98 | −2.87 | 7 | 9.348 | 18.35 | 36.37 | ![]() |
CS | 5–4 | 35.27 | −3.53 | 11 | 16.29 | 32.24 | 64.15 | ![]() |
c-C3H2 | ortho 321−212 | 18.17 | −4.23 | 21 | 201.8 | 566.9 | 1598 | ![]() |
c-C3H2 | ortho 71,6−70,7 | 61.17 | −4.05 | 45 | 201.8(c) | 566.9(c) | 1598(c) | ![]() |
c-C3H2 | para 72,6−71,7 | 61.17 | −4.05 | 15 | 201.8(c) | 566.9(c) | 1598(c) | ![]() |
SO | 67−56 | 47.55 | −3.64 | 15 | 38.88 | 90.34 | 197.51 | <3.0×1012 (d) |
SO | 66−55 | 56.5 | −3.67 | 13 | 38.88 | 90.34 | 197.51 | <8.0×1012 (d) |
CH3OH | 51,4,0−41,3,0 | 49.66 | −4.22 | 44 | 275.0 | 920.9 | 2924 | <4×1013 (d) |
Notes. (a)See Table 1 for quantum numbers formatting. (b) Average column density within the integration area of the flux estimate, for an excitation temperature of 30 K. The uncertainties on the column density include the propagated uncertainty on the flux and the systematic uncertainty on the excitation temperature. (c)The calculation of the partition functions includes all lines of both ortho and para isomers. (d)For the undetected lines we present an upper limit on the column density from the upper limit on the flux.
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