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Table 4

Comparison between predicted (for i = 60°) and observed intensities (erg cm−2 s−1 sr−1).

I[H2 S(1)] I([S I] 25.249 µm) I([SI]25.249μm)I[ H2S(1) ]${{I([{\rm{SI}}]25.249\mu {\rm{m}})} \over {I\left[ {{{\rm{H}}_2}{\rm{S}}(1)} \right]}}$ Models
1.16(−3)(*) 3.72(−6) 0.003 Model 1 (P = 2.8 × 107 K cm−3)
7.61(−4) 2.80(−5) 0.04 Model 2 (p = 2.8 × 108 K cm−3)
4.86(−4) 4.58(−4) 0.94 Model 3 (p = 2.8 × 109 K cm−3)
1.98(−4) 1.37(−5) 0.07 Model 4 (G0 = 3.1 × 103 Mathis field)
1.12(−3) 2.44(−4) 0.21 Model 5 (G0 = 3.1 × 105 Mathis field)
7.57(−4) 2.69(−5) 0.03 Model 6 (ζH2=5×10−16 s−1${\zeta _{{H_2}}} = 5 \times {10^{ - 16}}{\rm{ }}{{\rm{s}}^{ - 1}}$)
1.11(−3) 4.65(-5) 0.04 Model 8 (NH/E(B − V) = 1.6 × 1022 cm−2 mag−1)
7.23(−4) 2.00(−7) 0.0004 Reference (S/H = 1.86 × 10−7)
8.95(−4) 4.23(−5) 0.05 Reference (S/H = 1.86 × 10−5)
8.62(−4) 1.19(−4) 0.14 DF3

Notes. In this table, only the model parameters relevant for the discussion in Sect. 6.3 are shown. The complete set of input parameters are given in Table 3 and Table A.4.(*) 1.16(−3) = 1.16 × 10−3.

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