Open Access

Table 2

Fluxes and velocity dispersion of the 12CO and 13CO v = 1−0 bands.

Transition Wavelength Region
μm N1 N2 N3 N4 N5 S1 S2 S3
12CO v = 1−0
σ1/(km s−1) (a) 34 ± 1 36 ± 1 55 ± 2 45 ± 2 51 ± 3 86±3 67 ± 3 52 ± 2
σ2/(km s−1) (a) 78 ± 3 105±4

R(9) 4.5876 0.80 ± 0.64
R(8) 4.5950 2.68 ± 0.64
R(7) 4.6024 5.98 ± 0.64 0.93 ± 0.28 0.52 ± 0.10 0.41 ± 0.11 0.00 ± 0.09 0.78 ± 0.14 0.63 ± 0.10 0.23 ± 0.11
R(6) 4.6100 9.53 ± 0.64 2.05 ± 0.28 0.54 ± 0.10 0.34 ± 0.11 0.00 ± 0.08 1.14 ± 0.14 0.76 ± 0.10 0.24 ± 0.11
R(5) 4.6177 15.1 ± 0.6 3.51 ± 0.28 1.01 ± 0.10 1.22 ± 0.21 0.50 ± 0.10 1.18 ± 0.14 0.76 ± 0.10 0.44 ± 0.26
R(4) 4.6254 19.0 ± 0.6 4.79 ± 0.28 1.11 ± 0.10 0.94 ± 0.11 0.21 ± 0.10 1.52 ± 0.14 1.16 ± 0.10 0.93 ± 0.15
R(3) 4.6333 27.7 ± 0.7 7.06 ± 0.28 1.72 ± 0.11 1.54 ± 0.12 0.68 ± 0.11 2.64 ± 0.17 1.94 ± 0.10 1.73 ± 0.11
R(2) 4.6412 36.8 ± 0.7 10.0 ± 0.3 1.80 ± 0.19 1.78 ± 0.20 0.76 ± 0.12 2.69 ± 0.20 2.64 ± 0.12 2.13 ± 0.12
R(1) 4.6493 46.6 ± 1.1 14.8 ± 0.4 2.97 ± 0.27 3.07 ± 0.21 2.04 ± 0.12 3.91 ± 0.31 3.74 ± 0.12 3.82 ± 0.22
R(0) 4.6575 52.5±1.3 18.8 ± 0.5 4.77 ± 0.25 4.45 ± 0.26 3.07 ± 0.12 6.28 ± 0.29 3.86 ± 0.11 5.53 ± 0.23
P(1) 4.6742 60.7 ± 1.1 24.8 ± 0.6 6.91 ± 0.16 6.86 ± 0.14 4.91 ± 0.12 7.25 ± 0.18 5.60 ± 0.15 5.69 ± 0.13
P(2) 4.6826 85.2±1.6 37.2 ± 0.8 13.0 ± 0.2 12.1 ± 0.2 9.18 ± 0.12 11.3 ± 0.3 8.92 ± 0.16 9.01 ± 0.16
P(3) 4.6912 105.6 ± 2.1 46.0 ± 0.9 16.5 ± 0.2 16.0 ± 0.3 13.4 ± 0.3 15.7 ± 0.5 13.7 ± 0.3 12.6 ± 0.3
P(4) 4.6999 112.1 ± 2.5 45.4±1.2 15.0 ± 0.2 16.0 ± 0.4 11.8 ± 0.4 14.3 ± 0.5 12.8 ± 0.2 11.4 ± 0.3
P(5) 4.7088 105.4 ± 2.1 39.0 ± 0.8 11.0 ± 0.1 13.0 ± 0.1 9.98 ± 0.15 12.8 ± 0.2 10.3 ± 0.1 9.55 ± 0.12
P(6) 4.7177 86.3±1.7 27.0 ± 0.6 6.36 ± 0.12 8.84 ± 0.14 6.31 ± 0.15 8.75 ± 0.18 7.45 ± 0.11 6.28 ± 0.11
P(7) 4.7267 62.0±1.3 15.7 ± 0.3 3.40 ± 0.13 6.34 ± 0.12 3.50 ± 0.11 5.72 ± 0.19 4.77 ± 0.10 4.44 ± 0.11
P(8) 4.7359 35.8 ± 0.7 6.86 ± 0.27 1.27 ± 0.10 2.46 ± 0.11 1.35 ± 0.10 3.19 ± 0.19 2.30 ± 0.13 2.17 ± 0.10
P(9) 4.7451 17.4 ± 0.6 2.20 ± 0.26 0.35 ± 0.10 0.84 ± 0.17 0.25 ± 0.15 2.12 ± 0.14 0.66 ± 0.13 1.31 ± 0.10
P(10) 4.7545 6.32 ± 0.61
P(11) 4.7640 3.73 ± 0.61

13CO v = 1−0
σ/(km s−1) (a) 39±6 50±4 100 ± 20 30±5 45 ± 6 130 ± 20 63 ± 5 90 ± 15

R(0) 4.7626 7.66 ± 0.62 (b) 3.26 ± 0.16 1.31 ± 0.16 0.62 ± 0.08 0.62 ± 0.10 1.25 ± 0.21 (b) 0.50 ± 0.09 1.63 ± 0.20
P(1) 4.7792 6.61 ± 0.38 4.07 ± 0.15 1.27 ± 0.15 0.85 ± 0.08 0.48 ± 0.10 0.75 ± 0.13 0.47 ± 0.06 1.69 ± 0.14
P(2) 4.7877 9.34 ± 0.42 5.66 ± 0.18 1.97 ± 0.14 1.32 ± 0.09 1.34 ± 0.13 0.99 ± 0.14 0.86 ± 0.06 2.06 ± 0.17
P(3) 4.7963 11.1 ± 0.5 5.49 ± 0.19 1.76 ± 0.13 1.44 ± 0.10 1.39 ± 0.14 1.61 ± 0.16 1.05 ± 0.07 1.77 ± 0.17
P(4) 4.8050 9.54 ± 0.43 3.53 ± 0.16 1.26 ± 0.14 1.13 ± 0.09 0.89 ± 0.11 0.71 ± 0.07 1.26 ± 0.16
P(5) 4.8138 5.04 ± 0.37 1.64 ± 0.14 0.39 ± 0.06
P(6) 4.8227 2.22 ± 0.35 0.74 ± 0.13
P(7) 4.8317 1.12 ± 0.34

Notes. The fluxes are in 10−17 erg cm−2 s−1 units. These fluxes include both the narrow and broad velocity components for the regions where two Gaussians were used. (a)Intrinsic velocity dispersion after subtracting the instrumental width (σinst = 39 km s−1 at λobs = 4.7 μm; Jakobsen et al. 2022). For 12CO, the dispersions of the narrow (σ1) and broad (σ2) components are reported when two Gaussians were used for the fit.(b)The listed 13CO R(0) flux is likely contaminated by the 12CO P(11) transition.

Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.

Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.

Initial download of the metrics may take a while.