A^3COSMOS: 0.5时的尘埃质量函数和尘埃质量密度

A. Traina, B. Magnelli, C. Gruppioni, I. Delvecchio, M. Parente, F. Calura, L. Bisigello, A. Feltre, F. Pozzi, L. Vallini
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引用次数: 0

摘要

虽然星系中的尘埃只占重子总质量的百分之几,但它在星系中发生的物理过程中却起着至关重要的作用。因此,研究星系中的尘埃含量,特别是在高 $z$ 的情况下,对于理解尘埃产生、遮蔽恒星形成和星系恒星质量积累之间的联系至关重要。我们研究了最大的阿塔卡马大型毫米波/亚毫米波阵列(ALMA)样本(A$^3$COSMOS)的尘埃特性(质量和温度),并推导出了$z=0.5\,-\,6$星系的尘埃质量函数和尘埃质量密度。我们用 CIGALE 代码拟合了光谱能量分布(SED),根据每个星系的紫外-近红外光度覆盖范围,结合 ALMA(如果有的话,还有 Herschel)对其尘埃-连续发射的 Rayleigh-Jeans 尾部的覆盖范围,确定了 A$^3$COSMOS 星系样本的尘埃质量和温度。然后,我们结合 A$^3$COSMOS 和最新的 Herschel 样本,计算并拟合了尘埃质量函数,以获得高达 $z 的综合尘埃质量密度的最佳估计值。 从 SED 拟合中,我们还可以得出尘埃温度。尘埃温度的分布峰值为 $30-35$K。在$z=0.5\,-\,6$的尘埃质量函数随着$M^*$的增加和数量密度($ ^*$)的减小而变化,与文献估计值吻合得很好。在从 $z 0.5$ 到 $z 6$ 的演化过程中,尘埃质量密度平稳地下降,这比在 $z 0.5$ 和 $z 6$ 时的模型更陡峭。
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A^3COSMOS: Dust mass function and dust mass density at 0.5
Although dust in galaxies represents only a few percent of the total baryonic mass, it plays a crucial role in the physical processes occurring in galaxies. Studying the dust content of galaxies, particularly at high $z$, is therefore crucial for understanding the link between dust production, obscured star formation, and the build-up of galaxy stellar mass. We study the dust properties (mass and temperature) of the largest Atacama Large Millimeter/submillimeter Array (ALMA)-selected sample of star-forming galaxies available from the archive (A$^3$COSMOS), and we derive the dust mass function and dust mass density of galaxies from $z=0.5\,-\,6$. We fit the spectral energy distribution (SED) with the CIGALE code to constrain the dust mass and temperature of the A$^3$COSMOS galaxy sample based on the UV-to-near-infrared photometric coverage of each galaxy combined with the ALMA (and Herschel when available) coverage of the Rayleigh-Jeans tail of their dust-continuum emission. We then computed and fit the dust mass function by combining the A$^3$COSMOS and the most recent Herschel samples in order to obtain the best estimate of the integrated dust mass density up to $z The dust masses in galaxies in lie between $ 10^8$ and $ $ M$_ odot $. From the SED fitting, we were also able to derive a dust temperature. The distribution of the dust temperature peaks at $ 30-35$K. The dust mass function at $z=0.5\,-\,6$ evolves with an increase in $M^*$ and a decrease in the number density ($ ^*$), and it agrees well with literature estimates. The dust mass density decreases smoothly in its evolution from $z 0.5$ to $z 6$, which is steeper than what is found by models at $z
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