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首页> 外文期刊>The Astrophysical journal >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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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

机译:用斯皮策和詹姆斯·克拉克·麦克斯韦望远镜观察到的边缘螺旋银河NGC 4631的粉尘排放的能谱分布

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We explore variations in dust emission within the edge-on Sd spiral galaxy NGC 4631 using 3.6-160 μm Spitzer Space Telescope data and 450-850 μm 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 submil-limeter emission compared to what is expected from dust models extrapolated from far-infrared wavelengths. The 8 μm PAH emission correlates best with 24 μm 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 μm PAH emission to 160 μm cool dust emission appears to vary as a function of radius. The 70 μm/160 μm and 160 μm/450 μm 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 μm emission relative to what would be predicted by dust models. The 850 μm excess is highest in regions with low 160 μm surface brightnesses, although the magnitude depends on the model fit to the data. We rule out variable emissivity functions or ~4 K dust as the possible origins of this 850 μm emission, but we do discuss the other possible mechanisms that could produce the emission.
机译:我们使用3.6-160μmSpitzer空间望远镜数据和450-850μmJCMT数据探索Sd旋涡星系NGC 4631边缘尘埃发射的变化,目的是了解PAHs和尘埃发射之间的关系,研究灰尘发射的颜色,并与从远红外波长推断出的灰尘模型所期望的相比,寻找可能的亚毫米级过量发射。 PAH的8μm发射与1.7 kpc尺度上的24μm的热尘埃发射最相关,但是该关系在650 pc尺度上破裂,这可能是由于激发PAH的光子与加热尘埃的光子之间的平均自由程不同。可能是因为PAH被某些恒星形成区域内的硬辐射场破坏了。 8μmPAH排放量与160μm冷尘排放量之比似乎随半径而变化。即使表面亮度的变化为25倍,70μm/ 160μm和160μm/ 450μm的通量密度比也显着恒定,这表明其发射来自几乎均匀的辐射场加热的灰尘。在全球范围内,我们发现与尘埃模型预测的排放相比,排放量超出了850-1230μm。 850μm的过剩在表面亮度低至160μm的区域最高,尽管幅度取决于适合数据的模型。我们排除了可变的发射率函数或〜4 K尘埃作为此850μm发射的可能起源,但我们确实讨论了可能产生发射的其他可能机制。

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