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Table 3

Comparison between the observed and CLOUDY model predicted line fluxes.

Lines Rest wavelength (μm) Observed line flux (10−18 Wm−2) Predicted line flux (10−18 W m−2) Ratio (Observed / Predicted)
This work(*) Neufeld et al. (2020) This work Neufeld et al. (2020)
HeH+ (υ, J) = (0,1 0,0) 149.091 163 ± 32 47.35 56 3.44 ± 0.68 2.86 ± 0.56
HeH+ (υ, J) = (1,0 → 0,1) [P(1)] 3.51532 1.55 ± 0.16 0.81 1.68 1.91 ± 0.20 0.92 ± 0.095

HeH+ (υ, J) = (1,1 → 0,2) [P(2)] 3.60677 2.08 ± 0.31 0.91 0.89 2.29 ± 0.34 2.33 ± 0.35
H I 19 − 6 3.64493 23.9 ± 0.22 20.44 34.6 1.17 ± 0.011 0.69 ± 0.006
He II 13 − 9 3.54328 53.7 ± 0.21 44.20 108 1 .22 ± 0.005 0.50 ± 0.002
He I 53 D − 43P0 3.70256 8.44 ± 0.48 11.35 12.8 0.74 ± 0.042 0.66 ± 0.038

Notes. (*)The line fluxes in CLOUDY are given in units of erg s−1 cm−2. To compare with the observations, we converted them to W m−2, accounting for the observational angular sizes tabulated in Table 4 (see notes) of Neufeld et al. (2020). The conversion formula used are: Predicted flux (W m−2) for HeH+(v,J)=(0,10,0)= CLOUDY flux (erg s1 cm2)×103×14π×π×(4.6×π180×3600)2${\rm{He}}{{\rm{H}}^ + }(v,J) = (0,1 \to 0,0) = {\rm{ CLOUDY flux }}\left( {{\rm{erg}}{{\rm{s}}^{ - 1}}{\rm{c}}{{\rm{m}}^{ - 2}}} \right) \times {10^{ - 3}} \times \frac{1}{{4\pi }} \times \pi \times {\left( {4.6 \times \frac{\pi }{{180 \times 3600}}} \right)^2}$. Predicted flux (W m−2) for HeH+ υ = 1 → 0 P(1), P(2), H i, He ii, and He I= CLOUDY flux (erg s1 cm2)×103×14π×(0.375×11)×(π180×3600)2${\text{He I}} = {\text{ CLOUDY flux }}\left( {{\text{erg}}{{\text{s}}^{ - 1}}{\text{c}}{{\text{m}}^{ - 2}}} \right) \times {10^{ - 3}} \times \frac{1} {{4\pi }} \times (0.375 \times 11) \times {\left( {\frac{\pi } {{180 \times 3600}}} \right)^2}$.

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