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The Spectral Energy Distribution of Dust Emission in the Edge-on Spiral Galaxy NGC 4631 as Seen with Spitzer and the James Clerk Maxwell Telescope
We explore variations in dust emission within the edge-on Sd spiral galaxy NGC 4631 using 3.6-160 km Spitzer Space Telescope data and 450-850 km JCMT data with the goals of understanding the relation between PAHs and dust emission, studying the variations in the colors of the dust emission, and sear...
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Published in: | The Astrophysical journal 2006-11, Vol.652 (1), p.283-305 |
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creator | Bendo, George J Dale, Daniel A Draine, Bruce T Engelbracht, Charles W Kennicutt, Jr., Robert C Calzetti, Daniela Gordon, Karl D Helou, George Hollenbach, David Li, Aigen Murphy, Eric J Prescott, Moire K. M Smith, John-David T |
description | We explore variations in dust emission within the edge-on Sd spiral galaxy NGC 4631 using 3.6-160 km Spitzer Space Telescope data and 450-850 km JCMT data with the goals of understanding the relation between PAHs and dust emission, studying the variations in the colors of the dust emission, and searching for possible excess submillimeter emission compared to what is expected from dust models extrapolated from far-infrared wavelengths. The 8 km PAH emission correlates best with 24 km hot dust emission on 1.7 kpc scales, but the relation breaks down on 650 pc scales, possibly because of differences in the mean free paths between photons that excite the PAHs and photons that heat the dust and possibly because the PAHs are destroyed by the hard radiation fields within some star formation regions. The ratio of 8 km PAH emission to 160 km cool dust emission appears to vary as a function of radius. The 70 km/160 km and 160 km/450 km flux density ratios are remarkably constant even though the surface brightnesses vary by factors of 25, which suggests that the emission is from dust heated by a nearly uniform radiation field. Globally, we find an excess of 850-1230 km emission relative to what would be predicted by dust models. The 850 km excess is highest in regions with low 160 km surface brightnesses, although the magnitude depends on the model fit to the data. We rule out variable emissivity functions or 64 K dust as the possible origins of this 850 km emission, but we do discuss the other possible mechanisms that could produce the emission. |
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The 8 km PAH emission correlates best with 24 km hot dust emission on 1.7 kpc scales, but the relation breaks down on 650 pc scales, possibly because of differences in the mean free paths between photons that excite the PAHs and photons that heat the dust and possibly because the PAHs are destroyed by the hard radiation fields within some star formation regions. The ratio of 8 km PAH emission to 160 km cool dust emission appears to vary as a function of radius. The 70 km/160 km and 160 km/450 km flux density ratios are remarkably constant even though the surface brightnesses vary by factors of 25, which suggests that the emission is from dust heated by a nearly uniform radiation field. Globally, we find an excess of 850-1230 km emission relative to what would be predicted by dust models. The 850 km excess is highest in regions with low 160 km surface brightnesses, although the magnitude depends on the model fit to the data. 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title | The Spectral Energy Distribution of Dust Emission in the Edge-on Spiral Galaxy NGC 4631 as Seen with Spitzer and the James Clerk Maxwell Telescope |
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