Table 2:

Water and CO line emission toward NGC 7129 FIRS 2.

Transition
Component rmsa $T_{\rm MB}^{\rm peak}$b $\int T_{\rm MB}~{\rm d}\varv$ b $V_{\rm LSR}$c FWHMd
    (mK) (K) (K km s-1) (km s-1) (km s-1)

H216O 111-000
no Gaussian fit 16 0.59 8.4 -8.2  
202-111 narrow 20 0.36 2.3 -7.2 6.2
  broad 20 0.23 6.1 -12.4 24.6
211-202 narrow 16 0.21 1.5 -7.5 6.5
  broad 16 0.11 3.1 -13.7 26.8
312-303 narrow 16 0.14 1.7 -7.3 7.8
  broad 16 0.11 2.8 -14.5 24.4
H218O 110-101   5 0.015 0.071 -8.5 5.3
H218O 202-111 not seen 5   <0.010e    
C18O 5-4   5 0.16 0.49 -9.8 2.1
13CO  10-9   20 0.13 0.44 -9.8 5.5

Notes. (a) The rms measure is taken over a 1 km s-1 range.
(b) Uncertainties in the peak temperature and integrated line intensity are dominated by calibration issues. For H216O 111-000, 202-111, 312-303, and 13CO 10-9 the uncertainty is 32%. For all other lines the uncertainty is 16%.
(c) Velocity accuracy better than $\sim$0.5 km s-1.
(d) A 20% uncertainty in the line widths is due primarily to the component separation.
(e) The 3$\sigma$ detection limit, for data smoothed to the expected line width (5 km s-1), is 0.015 K.


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