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Table 3

Best-fit slab model parameters for the molecules detected in Sz28.

Molecules T (K) log10 N (cm−2) Rem (au) N$\[\mathcal{N}\]$
  C2H2 425225+175$\[425_{-225}^{+175}\]$ 20.67−2.17 0.0150.005+0.015$\[0.015_{-0.005}^{+0.015}\]$
18.331.03+1.67$\[18.33_{-1.03}^{+1.67}\]$ 0.030.02+0.07$\[0.03_{-0.02}^{+0.07}\]$
C6H6 225115+325$\[225_{-115}^{+325}\]$ 18.170.67+1.33$\[18.17_{-0.67}^{+1.33}\]$ 0.070.06+0.53$\[0.07_{-0.06}^{+0.53}\]$ 5 × 1042
C3H4 25050+200$\[250_{-50}^{+200}\]$ 15.830.83+1.67$\[15.83_{-0.83}^{+1.67}\]$ 0.380.33+0.62$\[0.38_{-0.33}^{+0.62}\]$ 1.2 × 1041
C4H2 25050+200$\[250_{-50}^{+200}\]$ 16.330.83+1.67$\[16.33_{-0.83}^{+1.67}\]$ 0.0670.017+0.93$\[0.067_{-0.017}^{+0.93}\]$ 6.7 × 1040

HCN detected
CO2 detected
HC3N detected
C2H6 detected
CH3 detected
CH4 detected

Notes. For optically thin emission, N$\[\mathcal{N}\]$ represents the number of molecules obtained as a product of N×πRem2$\[N \times \pi R_{\mathrm{em}}^2\]$. The values for the optically thick and thin component of C2H2 are provided. The fitting procedure did not yield a well-constrained solution for the molecules labelled as “detected”.

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