首页> 外文期刊>PASJ: Publications of the Astronomical Society of Japan >Deep 15 μm AKARI Observations in the CDFS:Estimating Dust Luminosities for a MIR-Selected Sample and for Lyman Break Galaxies and the Evolution of L _(dust) /L_(UV) with the Redshift
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Deep 15 μm AKARI Observations in the CDFS:Estimating Dust Luminosities for a MIR-Selected Sample and for Lyman Break Galaxies and the Evolution of L _(dust) /L_(UV) with the Redshift

机译:CDFS中深15μm的AKARI观测值:估算MIR选定样品和莱曼断裂星系的尘埃光度,以及红移引起的L _(尘埃)/ L_(UV)演化

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Deep observations of the Chandra Deep Field South have been secured at 15 Am with AKARI/RC infrared space telescope. From these observations, we define a sample of mid infrared-selected galaxies at 15 /μm and we also obtain 15 μm flux densities for a sample of Lyman Break Galaxies at z 1 already observed at 24 Am with Spitzer/MIPS. Number counts for the mid infrared-selected sample show a bump around a 15 Am flux density of 0.2 mJy that can be attributed to galaxies at z > 0.4 and at z > 0.8 for the fainter part of the bump. This bump seems to be shifted as compared to other works and a possible origin can be the Cosmic variance. On the two above samples at z~1 we have tested the validity of the conversions from luminosities vf_v at 8 Am to total dust luminosities by comparing with luminosities estimated from 12 μm data used as a reference. Some calibrations seem better when compared to Ldust evaluated from longer wavelength luminosities. We also find that the rest-frame 8 μm luminosities provide good estimates of L_(dust). By comparing our data to several libraries of spectral energy distributions, we find that models can explain the diversity of the observed f_(24)/f_(15) ratio quite reasonably. However, when we analyse the luminosity dependence of this ratio, we find important discrepancies. Finally, we revisit the evolution of L_(dust) /L_(UV) ratio with the redshift z by re-calibrating previous L_(dust) at z ~ 2 based on our results and added new data points at higher redshifts. The decreasing trend is amplified as compared to the previous estimate.
机译:AKARI / RC红外太空望远镜已于上午15点对Chandra Deep Field South进行了深入观测。从这些观察中,我们将样本定义为15 /μm的中红外选择星系样本,并且使用Spitzer / MIPS在z 1处获得的莱曼断裂星系样本的通量密度也为15μm。中红外选择样品的计数表明在15 Am的通量密度为0.2 mJy附近有一个凸起,这可以归因于凸起的较弱部分的z> 0.4和z> 0.8的星系。与其他作品相比,这种颠簸似乎已转移,可能的起源可能是宇宙方差。通过比较从12μm数据估计的光度,在z〜1处的上述两个样本中,我们测试了8 am的光度vf_v转换为总尘埃光度的有效性。与从较长波长的光度评估的Ldust相比,某些校准似乎更好。我们还发现,其余帧的8μm发光度可很好地估计L_(灰尘)。通过将我们的数据与几个光谱能量分布库进行比较,我们发现模型可以相当合理地解释观测到的f_(24)/ f_(15)比的多样性。但是,当我们分析此比率的光度依赖性时,我们发现了重要的差异。最后,根据我们的结果,通过在z〜2处重新校准先前的L_(灰尘),并在更高的红移处添加新的数据点,来重新考察具有红移z的L_(灰尘)/ L_(UV)比的变化。与先前的估计相比,下降趋势被放大了。

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