Notes. ^(a)COMs and vibrational states used to derive population diagrams.^(b) Assumed size of the emitting region.^(c)Rotational temperature used for the Weeds model.^(d)Rotational temperature derived from the population diagram.^(e)Column density used for the Weeds model.^(f)Vibrational state correction at temperature T_rot,W applied to the column density N_W when the partition function does not account for higher-excited vibrational states, where C_vib,W = C_vib,W(T_rot,W).^(g)Column density derived from the population diagram.^(h)Vibrational state correction at temperature T_rot,pd applied to N_pd, where C_vib,pd = C_vib,pd (T_rot,pd).⁽ⁱ⁾Linewidths (FWHM) of the transitions^(j) Offset from the source systemic velocity, which was set to 62 km s⁻¹.

Values in parentheses show the decimal power, where x(z) = x × 10^z or (x ± y)(z) = (x ± y) × 10^z.

Upper limits on N_W indicate that a population diagram could not be derived, either because too many transitions are contaminated or the molecule is not detected. Then, the temperature, FWHM, and offset velocity values used in Weeds correspond to medians derived from other molecules at this position. Upper limits on T_rot,pd indicate when upper limits on integrated intensity for non-detected transitions are used in the population diagrams.