. | . | . | . | Dust scattering‡ . | |
---|---|---|---|---|---|
. | Observed 3 σ upper limit . | Case A* . | Case B† . | Silicate . | Graphite . |
Paβ/Hα | <3.5 × 10−2 (Main southwest) | 7.6 × 10−2 | 5.7 × 10−2 | (3.0 ± 0.3) × 10−2 | (5.2 ± 0.4) × 10−2 |
. | . | . | . | Dust scattering‡ . | |
---|---|---|---|---|---|
. | Observed 3 σ upper limit . | Case A* . | Case B† . | Silicate . | Graphite . |
Paβ/Hα | <3.5 × 10−2 (Main southwest) | 7.6 × 10−2 | 5.7 × 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.
. | . | . | . | Dust scattering‡ . | |
---|---|---|---|---|---|
. | Observed 3 σ upper limit . | Case A* . | Case B† . | Silicate . | Graphite . |
Paβ/Hα | <3.5 × 10−2 (Main southwest) | 7.6 × 10−2 | 5.7 × 10−2 | (3.0 ± 0.3) × 10−2 | (5.2 ± 0.4) × 10−2 |
. | . | . | . | Dust scattering‡ . | |
---|---|---|---|---|---|
. | Observed 3 σ upper limit . | Case A* . | Case B† . | Silicate . | Graphite . |
Paβ/Hα | <3.5 × 10−2 (Main southwest) | 7.6 × 10−2 | 5.7 × 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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