Open Access
Table C.1.
Molecular hydrogen lines detected.
| Transition | Notation | λ |
 |
Atot | Nucleus | Northeast Shock | North Lane | South Lane |
|---|---|---|---|---|---|---|---|---|
| (1) | (2) | (3) | (4) | (5) | (6) | (7) | (8) | (9) |
| ν = 0 → 0 | ||||||||
| J = 3 → 1 | S(1) | 17.035 | 1015 | 47.6 | 11.85 (0.51) | 4.60 (0.07) | 7.96 (0.03) | 10.46 (0.02) |
| J = 4 → 2 | S(2) | 12.279 | 1681 | 276 | 18.63 (0.85) | 6.37 (0.11) | 7.64 (0.03) | 9.06 (0.02) |
| J = 5 → 3 | S(3) | 9.665 | 2503 | 984 | 51.83 (1.57) | 19.90 (1.01) | 17.83 (0.38) | 20.41 (0.20) |
| J = 6 → 4 | S(4) | 8.025 | 3475 | 2643 | 35.33 (0.51) | 8.14 (0.08) | 6.18 (0.67) | 7.04 (0.40) |
| J = 7 → 5 | S(5) | 6.910 | 4586 | 5879 | 90.00 (0.79) | 23.00 (0.16) | 9.91 (0.96) | 15.33 (0.02) |
| J = 8 → 6 | S(6) | 6.109 | 5830 | 11400 | 23.10 (0.41) | 5.46 (0.14) | 2.43 (0.02) | 3.42 (0.08) |
| J = 9 → 7 | S(7) | 5.511 | 7197 | 20000 | 68.00 (1.38) | 13.15 (0.38) | 4.51 (0.12) | 7.32 (0.14) |
| J = 10 → 8 | S(8) | 5.053 | 8677 | 32360 | 18.24 (1.00) | 4.31 (0.37) | 1.51 (0.15) | 1.59 (0.11) |
| J = 11 → 9 | S(9) | 4.695 | 10261 | 49000 | 37.44 (0.92) | 7.62 (0.28) | 2.65 (0.15) | 3.01 (0.17) |
| J = 12 → 10 | S(10) | 4.410 | 11940 | 70290 | 8.22 (0.62) | 1.58 (0.49) | 0.48 (0.05) | 0.53 (0.05) |
| J = 13 → 11 | S(11) | 4.181 | 13703 | 96330 | 21.29 (0.92) | 3.88 (0.66) | 1.14 (0.03) | 1.31 (0.04) |
| J = 15 → 13 | S(13) | 3.846 | 17444 | 161700 | 11.79 (0.62) | 2.16 (0.11) | 0.51 (0.02) | 0.52 (0.03) |
| J = 16 → 14 | S(14) | 3.724 | 19403 | 199900 | 3.16 (0.89) | 0.67 (0.10) | 0.08 (0.01) | 0.12 (0.02) |
| J = 17 → 15 | S(15) | 3.626 | 21411 | 240700 | 5.59 (0.63) | 1.53 (0.14) | 0.27 (0.02) | 0.23 (0.02) |
| J = 18 → 16 | S(16) | 3.548 | 23459 | 283100 | < 2.71 | 0.59 (0.11) | 0.08 (0.02) | 0.07 (0.03) |
| J = 19 → 17 | S(17) | 3.486 | 25539 | 325900 | 2.71 (0.60) | 0.95 (0.13) | < 0.08 | 0.08 (0.02) |
| J = 20 → 18 | S(18) | 3.439 | 27643 | 368000 | 3.03 (0.55) | 1.10 (0.14) | 0.10 (0.02) | < 0.08 |
| ν = 1 → 0 | ||||||||
| J = 2 → 0 | 1-0 S(0) | 2.223 | 6471 | 84720 | 12.47 (2.54) | 2.01 (0.17) | 0.66 (0.06) | 1.57 (0.19) |
| J = 3 → 1 | 1-0 S(1) | 2.122 | 6951 | 83800 | 34.97 (1.53) | 7.03 (0.24) | 2.56 (0.07) | 2.89 (0.07) |
| J = 4 → 2 | 1-0 S(2) | 2.034 | 7584 | 82260 | 18.54 (2.52) | 3.11 (0.22) | 1.03 (0.06) | 1.02 (0.07) |
| J = 5 → 3 | 1-0 S(3) | 1.958 | 8365 | 80110 | 74.80 (28.11) | 8.15 (0.30) | 2.75 (0.09) | 2.96 (0.33) |
| J = 6 → 4 | 1-0 S(4) | 1.892 | 9286 | 77630 | 73.54 (15.23) | 2.95 (0.28) | 0.92 (0.07) | 3.12 (0.27) |
| J = 7 → 5 | 1-0 S(5) | 1.836 | 10341 | 75330 | 44.27 (3.70) | 6.22 (0.34) | 2.15 (0.09) | 2.42 (0.29) |
| J = 8 → 6 | 1-0 S(6) | 1.788 | 11521 | 73970 | < 22.76 | < 1.64 | < 0.46 | 0.86 (0.36) |
| J = 9 → 7 | 1-0 S(7) | 1.748 | 12817 | 74430 | 37.67 (6.73) | 3.18 (0.40) | 0.99 (0.12) | 1.92 (0.45) |
| J = 0 → 2 | 1-0 O(2) | 2.627 | 5987 | 85320 | 12.55 (1.60) | 1.58 (0.43) | 0.53 (0.04) | 0.47 (0.04) |
| J = 1 → 3 | 1-0 O(3) | 2.803 | 6149 | 85160 | 19.98 (0.98) | 4.92 (3.46) | 1.55 (0.06) | 1.31 (0.07) |
| J = 2 → 4 | 1-0 O(4) | 3.004 | 6471 | 84720 | 6.67 (0.61) | 2.01 (0.19) | 0.46 (0.03) | 0.63 (0.04) |
| J = 3 → 5 | 1-0 O(5) | 3.235 | 6951 | 83800 | 12.67 (0.60) | 2.47 (0.06) | 0.93 (0.02) | 1.04 (0.03) |
| J = 4 → 6 | 1-0 O(6) | 3.501 | 7584 | 82260 | 3.78 (0.56) | 0.68 (0.05) | 0.20 (0.02) | 0.23 (0.02) |
| J = 5 → 7 | 1-0 O(7) | 3.807 | 8365 | 80110 | 6.05 (0.57) | 1.44 (0.11) | 0.39 (0.02) | 0.35 (0.02) |
| J = 7 → 9 | 1-0 O(9) | 4.575 | 10341 | 75330 | 2.11 (0.72) | 0.49 (0.23) | 0.05 (0.06) | 0.29 (0.09) |
| J = 7 → 7 | 1-0 Q(7) | 2.500 | 10341 | 75330 | 11.24 (1.18) | 2.40 (0.16) | 0.86 (0.11) | 1.12 (0.28) |
| J = 8 → 8 | 1-0 Q(8) | 2.528 | 11521 | 73970 | < 14.85 | < 0.72 | 0.18 (0.07) | < 1.47 |
| J = 9 → 9 | 1-0 Q(9) | 2.560 | 12817 | 74430 | 9.34 (3.59) | 0.91 (0.26) | 0.49 (0.09) | 0.46 (0.09) |
| J = 11 → 11 | 1-0 Q(11) | 2.635 | 15722 | 84630 | 5.19 (0.74) | < 2.93 | 0.16 (0.03) | 0.27 (0.04) |
| ν = 1 → 1 | ||||||||
| J = 11 → 9 | 1-1 S(9) | 4.954 | 15722 | 84630 | 5.88 (0.93) | 0.60 (0.15) | 0.25 (0.10) | 0.42 (0.10) |
| J = 12 → 10 | 1-1 S(10) | 4.656 | 17311 | 95980 | < 7.32 | 0.23 (0.18) | < 0.45 | 0.13 (0.09) |
| J = 13 → 11 | 1-1 S(11) | 4.417 | 18979 | 112300 | 3.48 (0.68) | 0.44 (0.11) | < 0.26 | < 0.34 |
| ν = 2 → 1 | ||||||||
| J = 3 → 1 | 2-1 S(1) | 2.248 | 12550 | 162300 | 6.88 (3.72) | 1.18 (0.16) | 0.33 (0.05) | < 1.00 |
| J = 5 → 3 | 2-1 S(3) | 2.073 | 13890 | 157200 | 7.85 (2.59) | 1.52 (0.20) | 0.32 (0.05) | 0.46 (0.06) |
| J = 2 → 2 | 2-1 Q(2) | 2.559 | 12095 | 163000 | 5.06 (2.65) | 0.95 (0.23) | 0.13 (0.08) | < 0.42 |
| J = 3 → 3 | 2-1 Q(3) | 2.570 | 12550 | 162300 | 4.15 (2.38) | < 0.91 | 0.27 (0.19) | 0.20 (0.10) |
| J = 1 → 3 | 2-1 O(3) | 2.974 | 11789 | 163100 | < 5.31 | 0.44 (0.17) | 0.12 (0.04) | < 0.35 |
Notes. (1) Transition level, (2) Notation, (3) Vacuum wavelength in microns, (4) Excitation energy in K, (5) Einstein A coefficient in units of 10−11 s−1, (6-9) Fluxes and their 1-σ errors for different regions in unit of 10−16 erg cm−2 s−1. Upper limits are calculated at 5-σ. H2 transition data from Roueff et al. (2019).
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