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Table 7.

Line parameter results derived using MADCUBA.

Line vLSR Δv1/2 Area Notes
(km s−1) (km s−1) (K) (K km s−1)
(1) (2) (3) (4) (5) (6)
CO(3–2) 451; 566; 706 90; 109 (20); 90 3.05; 3.58; 2.28 294; 456 (75); 220 a
CO(5–4) 0.19; 0.26; 0.13 18; 33 (6); 13 a
CO(6–5) 0.052; 0.08; 0.035 5; 10 (3); 3 a
CO(9–8) a, d
CO(3–2) 455; 578; 683 90; 119 (16); 90 0.64; 0.32; 0.64 57.4; 34.4 (5); 57.4 b
CO(5–4) 0.35; 0.18; 0.35 33.4; 21.1 (3); 33.4 b
CO(6–5) 0.44; 0.24; 0.44 42.4; 27.7 (4); 42.3 b
CO(9–8) 0.344; 0.21; 0.34 33.0; 24.4 (4); 32.6 b

13CO(3–2) 446; 566; 685 90; 148 (21); 90 0.36; 0.31; 0.30 35; 48 (9); 29
13CO(6–5) 0.028; 0.015; 0.020 2.7; 2.4 (0.40); 1.9
13CO(9–8) <0.06 <8 c

HCN(4–3) 446; 574; 683 90; 169 (19); 90 0.12; 0.095 ; 0.13 11.33; 17.04 (3); 12.39
HCN(6–5) 0.008; 0.004 ; 0.008 0.90; 0.84 (0.3); 0.90
HCN(7–6) 0.0035; 0.0012; 0.0035 0.34; 0.22; 0.34
HCN(12–11) <0.1 <1 c

HNC(3–2) 448; 572; 683 90; 138 (18); 90 0.064; 0.043; 0.063 6.2; 6.4 (0.9); 6.0
HNC(4–3) 0.056; 0.04; 0.059 5.4; 5.9 (0.96); 5.7
HNC(6–5) 0.002; 0.002; 0.002 0.22; 0.34 (0.09); 0.22
HNC(7–6) <0.06 <6 c

HCO+(4–3) 450; 580; 685 90; 176; 90 0.13; 0.11; 0.14 12.2; 21.3; 12.4
HCO+(6–5) 0.004; 0.004; 0.004 034; 0.66; 0.34
HCO+(7–6) <0.02 <2 c

CS(6–5) 444; 564; 671 90; 129 (28); 90 0.023; 0.029; 0.027 2.24; 3.92 (1.07); 2.61
CS(7–6) 0.021; 0.028; 0.027 2.03; 3.82 (0.97); 2.54
CS(10–9) <0.02 <2 c
CS(12–11) <0.02 <3 c
CS(13–12) <0.03 <4 c

[CI] 3P13P0 448; 568; 688 90; 152 (23); 90 0.24; 0.24; 0.20 23; 39 (8); 20
[CI] 3P23P1 0.33; 0.32; 0.38 33; 52 (10); 37

CH(3/2–1/2) 438; 556; 698 90; 150 (18); 90 0.041; 0.023; 0.037 4.59; 4.29; 4.14
CH(3/2–1/2) 0.041; 0.024; 0.037 4.59; 3.13; 4.14
CH(5/2–3/2) <0.06 <5 c

Notes. Column (1): molecule and rotational transition (J); Col. (2): centroid of the Gaussian component (local standard of rest velocity, vLSR) in km s−1; Col. (3): FWHM of the Gaussian in km s−1. The error values were computed only for the central component for which the FWHM has been let free to vary. For the blue and red components, the FWHM was fixed to 90 km s−1; Col. (4): main beam peak temperature of each Gaussian in kelvin; Col. (5): area of the Gaussian component in K km s−1; Col. (6): notes with the following code: (a) cold component; (b) hot component; (c) 3σ upper limit; (d) the cold component does not exist for this transition.

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