Table 3.

Comparison of the observed and model-predicted Paβ/Hα ratios.

Dust scattering
Observed 3 σ upper limitCase A*Case BSilicateGraphite
Paβ/Hα<3.5 × 10−2 (Main southwest)7.6 × 10−25.7 × 10−2(3.0 ± 0.3) × 10−2(5.2 ± 0.4) × 10−2
Dust scattering
Observed 3 σ upper limitCase A*Case BSilicateGraphite
Paβ/Hα<3.5 × 10−2 (Main southwest)7.6 × 10−25.7 × 10−2(3.0 ± 0.3) × 10−2(5.2 ± 0.4) × 10−2
*

Low density limit, |$T_{\rm e}=10^4\rm \, K$| (Osterbrock & Ferland 2006).

|$n_{\rm e} = 10^2\rm \, cm^{-3}$|⁠, |$T_{\rm e} = 10^4\rm \, K$| (Osterbrock & Ferland 2006).

Scattering efficiency from Laor and Draine (1993). A single dust size of 0.35 μm is assumed. The scattered Paβ/Hα photons originate from the Case B recombination lines from the host galaxy.

Table 3.

Comparison of the observed and model-predicted Paβ/Hα ratios.

Dust scattering
Observed 3 σ upper limitCase A*Case BSilicateGraphite
Paβ/Hα<3.5 × 10−2 (Main southwest)7.6 × 10−25.7 × 10−2(3.0 ± 0.3) × 10−2(5.2 ± 0.4) × 10−2
Dust scattering
Observed 3 σ upper limitCase A*Case BSilicateGraphite
Paβ/Hα<3.5 × 10−2 (Main southwest)7.6 × 10−25.7 × 10−2(3.0 ± 0.3) × 10−2(5.2 ± 0.4) × 10−2
*

Low density limit, |$T_{\rm e}=10^4\rm \, K$| (Osterbrock & Ferland 2006).

|$n_{\rm e} = 10^2\rm \, cm^{-3}$|⁠, |$T_{\rm e} = 10^4\rm \, K$| (Osterbrock & Ferland 2006).

Scattering efficiency from Laor and Draine (1993). A single dust size of 0.35 μm is assumed. The scattered Paβ/Hα photons originate from the Case B recombination lines from the host galaxy.

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