Table 3
Kinetic temperatures, hydrogen nuclei number densities, and column densities of the species resulting from the multi-transition analysis described in Sect. 4.
TMC 1-C | TMC 1-C (P) | TMC 1-CP | TMC 1-CP (P1) | TMC 1-CP (P2) | ||
---|---|---|---|---|---|---|
Tk (K)(a) | 7.4 ± 2.1 | 8.7 ± 1.9 | 9.0 ± 2.1 | 9.3 ± 1.8 | 9.1 ± 1.6 | |
CS | nH (cm−3) | (1.4 ± 0.8) × 105 | (8.8 ± 6.0) × 104 | (6.2 ± 2.0) × 104 | (6.7 ± 2.5) × 104 | (7.0 ± 4.6) × 104 |
N (cm−2) | (1.0 ± 0.5) × 1014 | (1.2 ± 0.9) × 1014 | (2.9 ± 1.8) × 1014 | (1.6 ± 1.2) × 1014 | (2.5 ± 0.9) × 1014 | |
DNC | nH (cm−3) | (1.8 ± 0.5) × 105 | (2.4 ± 0.5) × 105 | (4.0 ± 1.0) × 105 | (3.0 ± 0.6) × 105 | (4.0 ± 0.8) × 105 |
N (cm−2) | (3.0 ± 0.9) × 1012 | (3.2 ± 0.7) × 1012 | (2.0 ± 0.5) × 1012 | (2.8 ± 0.5) × 1012 | (2.5 ± 0.4) × 1012 | |
DN13C | nH (cm−3) | (4.1 ± 1.2) × 105 | − | − | − | − |
N (cm−2) | (8.5 ± 2.4) × 1010 | |||||
DCN | N (cm−2) | (2.5 ± 0.7) × 1012 | (5.0 ± 1.1) × 1012 | (2.3 ± 0.5) × 1012 | (3.5 ± 0.7) × 1012 | (3.5 ± 0.6) × 1012 |
N2H+ | Nupp (cm−2) (b) | (1.2 ± 0.3) × 1013 | (1.0 ± 0.2) × 1013 | (6.0 ± 1.4) × 1012 | (6.0 ± 1.2) × 1012 | (5.0 ± 0.9) × 1012 |
Nlow (cm−2) (c) | (8.0 ± 2.0) × 1012 | (5.0 ± 1.0) × 1012 | (3.5 ± 0.8) × 1012 | (4.2 ± 0.8) × 1012 | (3.0 ± 0.6) × 1012 | |
N2D+ | N (cm−2) | (1.8 ± 0.5) × 1012 | (1.5 ± 0.3) × 1012 | <3.5 × 1011 | <3.0 × 1011 | <3.0 × 1011 |
N(DNC)/N(DCN) | 2.04 ± 0.82 | 0.64 ± 0.20 | 0.87 ± 0.29 | 0.80 ± 0.22 | 0.71 ± 0.18 | |
N(N2D+)/N(N2H+)upp | 0.15 ± 0.06 | 0.15 ± 0.04 | <0.06 | <0.05 | < 0.06 | |
N(N2D+)/N(N2H+)low | 0.23 ± 0.08 | 0.30 ± 0.08 | <0.10 | <0.07 | <0.10 | |
N(N2H+)upp/N(CS) | 0.09 ± 0.05 | 0.08 ± 0.06 | 0.02 ± 0.01 | 0.04 ± 0.03 | 0.02 ± 0.01 |
Notes. (a) We assume the kinetic temperatureTk and the hydrogen nuclei number densities nH obtained from CS and DNC multi-transition fitting (in bold) to derive the DCN, N2H+, and N2D+ column densities. (b)Upper bound value for the column density obtained assuming the Tk and n(H2) values in bold and fitting the opacity of the main component and the brightness of the weakest hyperfine component as explained in Sect. 4.2. (c) Lower bound value for the column density obtained in the low excitation temperature scenario discussed in Sect. 6.
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