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Table 5

Normalized spectral line emission distribution.

Transition Obs. BNF a F em b F abs c L cor d
(Jy   km   s-1) (104  L)

The   12CO ladder

J = 1–0 SEST 0.53 583 ± 87 340 0.16 ± 0.05
J = 2–1 SEST 0.99 1705 ± 256 410 0.72 ± 0.20
J = 3–2 JCMT 2.13 3151 ± 473 220 1.71 ± 0.29
J = 4–3 APEX 2.13 3513 ± 703 195 2.83 ± 0.61
SPIRE 0.57 4208 ± 365
J = 5–4 SPIRE 0.66 3441 ± 155 170 2.87 ± 0.20
HIFI 0.60 2803 ± 280
J = 6–5 SPIRE 0.75 2066 ± 66 145 2.30 ± 0.15
HIFI 0.66 2291 ± 380
J = 7–6 SPIRE 0.63 1267 ± 46 140 1.58 ± 0.13
HIFI 0.79 1229 ± 185
J = 8–7 SPIRE 0.62 961 ± 63 1.48 ± 0.20
HIFI 0.89 1477 ± 370
J = 9–8 SPIRE 1.25 790 ± 89 1.44 ± 0.16
HIFI 0.99 1246 ± 210
J = 10–9 SPIRE 1.45 494 ± 90 0.76 ± 0.15
HIFI 1.14 319 ± 106
J = 11–10 SPIRE 1.39 425 ± 120 0.79 ± 0.22
J = 12–11 SPIRE 1.47 269 ± 90 0.55 ± 0.18

The   13CO ladder

J = 1–0 0.017 ± 0.007
J = 2–1 0.065 ± 0.019
J = 3–2 0.122 ± 0.027
J = 4–3
J = 5–4 0.16 ± 0.0.04

The carbon and C+ lines

[CI](1–0) APEX 2.17 6149 ± 922 655 4.2 ± 0.8
SPIRE 0.63 4418 ± 207
HIFI 0.58 5360 ± 804
[CI](2–1) APEX 7: 1782 11.1 ± 2.4
SPIRE 0.68 7613 ± 761
HIFI 0.81 7408 ± 1111
[CII] HIFI 2.8 140 773 ± 21 115 1436 397 ± 60
[NII] SPIRE 1.47 14 832 ± 2000 31 ± 5

Notes.

(a)

Beam normalisation factor (BNF) to reduce observed emission line fluxes from Tables 2, 3, 4 to those enclosed by a 22′′ beam; for line fluxes expressed in   K   km   s-1, multiply BNF by (θb/22)2, where θb is the observing FWHM beam-size from Tables 2 and 4.

(b)

Emission line fluxes normalised to the response of a 22′′ beam by application of the BNF.

(c)

Beam-independent absorption line flux derived from the estimated difference between integrated and Gaussian-fitted line intensities in Table 2; adopted error: 50%. Note that this is the total amount of absorption over the whole profile, not just the prominently visible deep absorption at systemic velocities.

(d)

Final adopted emission line luminosity in a 22′′ beam, corrected for absorption line losses. For   13CO we did not determine line fluxes, but derived corrected luminosities directly from the more accurate   12CO values using the mean of the   12CO/   13CO ratios in Table 3.

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