Table 1
Spectral lines and dust continuum emission in our study.
Species | Transition | Rest wavelengtha |
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FWHMc |
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Luminosityf,g |
(μm) | (K) | (cm-3) | (′′) | (10-11 W m-2 sr-1) | (10-11 W m-2 sr-1) | (L⊙) | ||
|
||||||||
12CO | J = 1–0 | 2600.8 | 6 | 4.7 × 102 | 45 | 0.1 | 0.8 | 0.9±0.1 |
12CO | J = 3–2 | 867.0 | 33 | 1.5 × 104 | 22 | 1.4 | 25.1 | 33.5±1.9 |
12CO | J = 4–3 | 650.3 | 55 | 3.7 × 104 | 42 | 15.3 | 29.4 | 67.8±2.2 |
12CO | J = 5–4 | 520.2 | 83 | 7.2 × 104 | 34 | 11.6 | 34.6 | 88.5±2.6 |
12CO | J = 6–5 | 433.6 | 116 | 1.3 × 105 | 29 | 6.6 | 36.9 | 101.5±3.0 |
12CO | J = 7–6 | 371.7 | 155 | 2.0 × 105 | 33 | 6.3 | 32.5 | 86.5±2.6 |
12CO | J = 8–7 | 325.2 | 199 | 2.9 × 105 | 33 | 17.2 | 29.4 | 71.5±2.6 |
12CO | J = 9–8 | 289.1 | 249 | 4.0 × 105 | 19 | 14.7 | 22.6 | 48.7±1.7 |
12CO | J = 10–9 | 260.2 | 304 | 5.3 × 105 | 18 | 18.3 | 22.7 | 33.4±1.5 |
12CO | J = 11–10 | 236.6 | 365 | 7.0 × 105 | 17 | 20.6 | 23.2 | 24.3±1.3 |
12CO | J = 12–11 | 216.9 | 431 | 9.0 × 105 | 17 | 17.9 | 23.2 | 18.9±1.1 |
12CO | J = 13–12 | 200.3 | 503 | 1.1 × 106 | 17 | 27.1 | 27.9 | – |
[CI] | 3P1–3P0 | 609.1 | 24 | 4.9 × 102 | 38 | 17.9 | 20.0 | 18.8±1.2 |
[CI] | 3P2–3P1 | 370.4 | 62 | 9.3 × 102 | 33 | 6.3 | 17.4 | 48.8±1.5 |
[CII] | 2P3/2–2P1/2 | 157.7 | 91 | 2.7 × 103 | 12 | 368.8 | 9439.1 | 3907.2±399.9 |
[OI] | 3P0–3P1 | 145.5 | 327 | 1.5 × 105 | 12 | 88.1 | 622.7 | 250.3±25.4 |
[OI] | 3P1–3P2 | 63.2 | 228 | 9.7 × 105 | 10 | 354.5 | 6444.5 | 2435.1±248.9 |
[OIII] | 3P1–3P0 | 88.4 | 163 | 5.0 × 102 | 10 | 544.8 | 1.1 × 104 | 5460.5±600.8 |
[NII] | 3P1–3P0 | 205.2 | 70 | 4.5 × 101 | 17 | 27.5 | 42.5 | 99.2±3.5 |
LFIR | – | 60–200 | – | – | 42 | – | 3.9 × 104 | (3.3±0.1) × 105 |
LTIR | – | 3–1000 | – | – | 42 | – | 8.1 × 104 | (7.5±0.1) × 105 |
Notes.
Data from Leiden Atomic and Molecular Database (except for [NII] and [OIII], whose data come from Carilli & Walter 2013).
Critical density (CO data from Walker et al. 2015 and the rest from Tielens 2005). For the CO, [CI], [CII], and [OI] lines, the critical densities are evaluated at the kinetic temperature of 100 K.
Median σf in the integrated intensity at 42′′ resolution (σf = final 1σ uncertainty; statistical and calibration errors added in quadrature).
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