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Table 2:

Observations and model calculations for the narrow PDR component in the RADEX homogeneous modela.
Species Transition Frequency Observations Ref. Model calculations
    $\nu$ $T_{\rm b}$ $4\pi I$ $\Delta \upsilon$   $T_{\rm ex}$ $\tau$ $T_{\rm b}$ $4\pi I$
    [GHz] [K] [erg s-1 cm-2] [km s-1]   [K]   [K] [erg s-1 cm-2]
H2O 11,0-10,1 556.936 0.92 ... 3.1 c 8.2 6.6 0.92 $6.8\times 10^{-6}$
H218O 11,0-10,1 547.676 <0.051 ... (3.1)b c 6.3 0.2 <0.05 < $3.5\times 10^{-7}$
NH3 10-0 0 572.498 1.1 ... 3.3 c 9.0 6.1 1.1 $9.2\times 10^{-6}$
  (1, 1) 23.695 2.9 ... ... d 54 0.02 0.87 $2.5\times 10^{-10}$
  (2, 2) 23.723 2.0 ... ... d 47 0.01 0.50 $1.7\times 10^{-10}$
  (3, 3) 23.870 1.4 ... ... d -5.1 -0.25 2.2 $9.0\times 10^{-10}$
  (4, 4) 24.139 0.15 ... ... d 46 0.001 0.06 $3.8\times 10^{-11}$
13CO 2-1 220.399 12 ... 3.3 e 55 0.2 9.1 $4.3\times 10^{-6}$
  5-4 550.926 14.7 ... 3.2 c 51 0.5 14.7 $1.1\times 10^{-4}$
CS 2-1 97.981 8.6 ... 3.0 f 47 0.2 9.1 $3.5\times 10^{-7}$
  3-2 146.969 10.2 ... 3.0 f 20 1.0 10.0 $1.3\times 10^{-6}$
  5-4 244.936 5.4 ... 3.0 f 13 1.3 5.5 $3.3\times 10^{-6}$
  6-5 293.912 3.3 ... 2.2 f 12 0.7 3.1 $3.3\times 10^{-6}$
[C I] 1-0 492.161 3.7 ... 3.5 g 54 0.1 3.7 $2.1\times 10^{-5}$
[C II] 3/2-1/2 1900.537 ... $4.4\times 10^{-3}$ ... h 55 1.0 13.4 $4.4\times 10^{-3}$
[O I] 1-2 4744.778 ... $4.1\times 10^{-3}$ ... h 46 0.9 0.88 $4.5\times 10^{-3}$
a All results for $T_{\rm K}$ = 55 K, $n({\rm H}_2)$ = 4 $\times $ 105 cm-3. $T_{\rm b}$ = Rayleigh-Jeans brightness temperature, $4\pi I$ = flux, $\Delta \upsilon$ = line width, $T_{\rm ex}$ = excitation temperature, $\tau$ = line-centre peak opacity; b from H2O; c this work; d Ungerechts et al. (1986); e Minchin et al. (1993); f Snell et al. (1984a); g Plume et al. (1994); h Emery et al. (1996).

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