Table 4
Best-fit 1D gas-grain modelled column densities compared to the observed values in MM1−MM3.
MM3f | MM2f | MM1f | |||||
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Moleculed,e | N Observed g | N Modeled h | N Observed g | N Modeled h | N Observed g | N Modeled h | Notes on the observed values |
(cm-2) | (cm-2) | (cm-2) | (cm-2) | (cm-2) | (cm-2) | ||
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H2 | 5.25± 0.23(24) | 9.9(24) | 1.70± 0.22(24) | 3.1(24) | 1.69± 0.27(24) | 2.7(24) | derived from dust continuum |
CO | 2.39± 0.06(18) | 2.6(18) | 2.21± 0.16(19) | 2.2(19) | 1.35± 0.16(20) | 5.6(19) | derived from C18O with 16O /18O = 607a |
H2CO | ≤4.95(14) | 7.0(14) | 4.50± 0.51(16) | 3.3(16) | 2.22± 0.34(16) | 1.6(16) | derived from ![]() |
CH2CO † | ≤3.67(13) | 2.6(14) | 1.43± 0.12(15) | 1.0(15) | 4.66± 0.37(14) | 1.3(15) | |
CH3OH † | 2.25± 0.02(15) | 4.5(14) | 4.33± 0.58(16) | 2.2(16) | 4.61± 0.88(16) | 7.2(16) | |
HCOOCH3 † | ≤4.95(14) | 2.4(09) × | 1.33± 0.13(16) | 1.2(14) × | 2.91± 0.39(16) | 1.2(13) × | |
CH3OCH3 *, † | ≤1.96(17) | 4.8(11) × | 1.97± 0.19(17) | 5.3(14) × | 7.62± 0.57(17) | 1.1(14) × | |
HNCO † | ≤2.44(13) | 9.1(12) | 1.89 ± 1.01(15) | 1.8(16) | 2.64 ± 1.35(15) | 2.4(17) × | |
HC3N † | ≤6.60(12) | 2.8(13) | 2.11± 0.03(14) | 6.1(14) | 6.33± 0.12(14) | 8.7(15) × | |
CH3CN | ≤ 1.18(15) | 1.3(13) × | 2.64 ± 0.96(15) | 1.3(14) × | 4.58 ± 1.97(16) | 3.8(15) | derived from opacity corrected CH3CN in Sect. 5.2.1 |
CH3CH2CN † | ≤8.43(13) | 1.3(10) × | ≤3.77(13) | 1.5(11) × | 1.70± 0.13(15) | 6.3(12) × | |
NH2CHO † | ≤7.11(12) | 2.3(13) | 5.46± 0.50(14) | 1.8(14) | 2.91± 0.13(14) | 2.9(14) | |
OCS | 8.25± 0.11(16) | 1.3(16) | 5.39± 1.71(16) | 2.5(17) | 6.79± 0.14(16) | 4.6(16) | derived from O13CS with 12C /13C = 73a |
SO2 | ≤ 4.29(14) | 1.2(16) × | ≤1.58(15) | 1.6(16) | 3.05± 0.43(17) | 2.7(16) × | derived from 34SO2 with 32S /34S = 22b |
SO | ≤ 1.93(15) | 1.8(16) | 3.29± 0.58(16) | 3.5(16) | 3.57± 0.38(17) | 3.4(17) | derived from 33SO with 32S /33S = 127b |
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Agreement | 10/15 = 67% | 11/15 = 73% | 9/15 = 60% | ||||
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Agec | 11 200 yr | 11 210 yr | 11 660 yr |
Notes.
Derived from galactic local isotope ratio (Giannetti et al. 2014).
Derived from isotope ratio in solar system (Lodders 2003).
The physical time moment when our chemical code describes the observed column densities most accurately in our assumed physical structures.
“†” denote the species which do not have rare isotopologues, so we derive their values by assuming they are optically thin.
“×” denote the model predicted column densities inconsistent to the observation (NModeled/NObserved< 0.1 or >10).
Uncertainties of the observed value are determined from Trot, partition function Q(Trot), and Gaussian fit to .
The values listed were obtained at the end of each evolutionary stage, corresponding to the values used in Fig. 6.
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