Table 3:

Parameters of the narrow absorption features seen in the two ground-state H216O transitions.

Line
$v\rm _{\rm lsr}$ $T\rm _{\rm MB}$ $\int T_{\rm MB} {\rm d}v$ Cont. level
  km s-1 K Kkm s-1 K
  - $6.2\pm 0.3$ $0.21\pm0.17$ $6.2\pm0.31$ $7.7\pm0.4$
111-000 $-0.34\pm 0.1$ $1.87\pm0.17$ $7.8\pm0.39$ $7.7\pm0.4$
  $+6.1\pm 0.10$ $0.33\pm0.17$ $7.8\pm0.39$ $9.0\pm0.45$
  $-6.8\pm 1.0$ 0.22$\pm0.024$ $2.04\pm0.10$ $1.54\pm0.08$
110-101 $-0.25\pm 0.1$ $0.81\pm0.024$ $2.69\pm0.13$ $1.53\pm0.08$
  +6.3$\pm 0.10$ 0.19$\pm0.024$ $2.36\pm0.76$ $1.51\pm0.08$

Notes.  $\int T_{\rm MB} {\rm d}v$ is the intensity integrated over the velocity ranges of the individual components (Table 1). The continuum level given is an average value for the individual components.


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