A^3COSMOS: Dust mass function and dust mass density at 0.5

A. Traina, B. Magnelli, C. Gruppioni, I. Delvecchio, M. Parente, F. Calura, L. Bisigello, A. Feltre, F. Pozzi, L. Vallini
{"title":"A^3COSMOS: Dust mass function and dust mass density at 0.5","authors":"A. Traina, B. Magnelli, C. Gruppioni, I. Delvecchio, M. Parente, F. Calura, L. Bisigello, A. Feltre, F. Pozzi, L. Vallini","doi":"10.1051/0004-6361/202451113","DOIUrl":null,"url":null,"abstract":"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","PeriodicalId":8585,"journal":{"name":"Astronomy & Astrophysics","volume":"50 9","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-07-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Astronomy & Astrophysics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1051/0004-6361/202451113","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0

Abstract

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
查看原文
分享 分享
微信好友 朋友圈 QQ好友 复制链接
本刊更多论文
A^3COSMOS: 0.5时的尘埃质量函数和尘埃质量密度
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。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
求助全文
约1分钟内获得全文 去求助
来源期刊
自引率
0.00%
发文量
0
期刊最新文献
X-ray polarisation in AGN circumnuclear media. Polarisation framework and 2D torus models COSMOS brightest group galaxies III. Evolution of stellar ages COSMOS brightest group galaxies III. Evolution of stellar ages X-ray polarisation in AGN circumnuclear media. Polarisation framework and 2D torus models Asteroid pairs: Survey of the inner main belt
×
引用
GB/T 7714-2015
复制
MLA
复制
APA
复制
导出至
BibTeX EndNote RefMan NoteFirst NoteExpress
×
×
提示
您的信息不完整,为了账户安全,请先补充。
现在去补充
×
提示
您因"违规操作"
具体请查看互助需知
我知道了
×
提示
现在去查看 取消
×
提示
确定
0
微信
客服QQ
Book学术公众号 扫码关注我们
反馈
×
意见反馈
请填写您的意见或建议
请填写您的手机或邮箱
已复制链接
已复制链接
快去分享给好友吧!
我知道了
×
扫码分享
扫码分享
Book学术官方微信
Book学术文献互助
Book学术文献互助群
群 号:481959085
Book学术
文献互助 智能选刊 最新文献 互助须知 联系我们:info@booksci.cn
Book学术提供免费学术资源搜索服务,方便国内外学者检索中英文文献。致力于提供最便捷和优质的服务体验。
Copyright © 2023 Book学术 All rights reserved.
ghs 京公网安备 11010802042870号 京ICP备2023020795号-1