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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) Navthin (b)[cm2]$\[\begin{gathered}N_{\mathrm{av}}^{\text {thin }(b)} \\{\left[\mathrm{cm}^{-2}\right]}\end{gathered}\]$
C18O 2–1 15.81 −6.22 5 7.461 14.57 28.81 1.10.1+0.4$\[1.1_{-0.1}^{+0.4}\]$
H2CO 30,3−20,2 21.0 −3.55 7 44.68 128.7 361.7 2.30.6+1.5$\[2.3_{-0.6}^{+1.5}\]$ × 1013
H2CO 32,1−22,0 68.1 −3.80 7 44.68 128.7 361.7 1.60.4+1.3$\[1.6_{-0.4}^{+1.3}\]$ × 1013
C2H 37/2,4−25/2,3 25.16 −4.3 9 37.14 72.91 144.7 7.50.1+1.5$\[7.5_{-0.1}^{+1.5}\]$ × 1013
C2H 37/2,3−25/2,2 25.15 −4.3 7 37.14 72.91 144.7 7.70.1+1.6$\[7.7_{-0.1}^{+1.6}\]$ × 1013
H13CN 3–2 24.86 −3.11 21 28.17 55.31 109.6 7.80.2+1.7$\[7.8_{-0.2}^{+1.7}\]$ × 1011
HC15N 3–2 24.78 −3.11 7 9.421 18.50 36.66 3.90.2+0.9$\[3.9_{-0.2}^{+0.9}\]$ × 1011
DCN 3–2 20.85 −3.33 21 33.39 65.75 130.5 8.72.6+2.5$\[8.7_{-2.6}^{+2.5}\]$ × 1011
H13CO+ 3–2 24.98 −2.87 7 9.348 18.35 36.37 4.70.1+0.9$\[4.7_{-0.1}^{+0.9}\]$ × 1011
CS 5–4 35.27 −3.53 11 16.29 32.24 64.15 3.90.1+0.9$\[3.9_{-0.1}^{+0.9}\]$ × 1012
c-C3H2 ortho 321−212 18.17 −4.23 21 201.8 566.9 1598 5.92.1+5.0$\[5.9_{-2.1}^{+5.0}\]$ × 1012
c-C3H2 ortho 71,6−70,7 61.17 −4.05 45 201.8(c) 566.9(c) 1598(c) 2.00.7+1.9$\[2.0_{-0.7}^{+1.9}\]$ × 1012
c-C3H2 para 72,6−71,7 61.17 −4.05 15 201.8(c) 566.9(c) 1598(c) 3.61.2+3.3$\[3.6_{-1.2}^{+3.3}\]$ × 1012
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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