A. Traina, B. Magnelli, C. Gruppioni, I. Delvecchio, M. Parente, F. Calura, L. Bisigello, A. Feltre, F. Pozzi, L. Vallini
{"title":"A^3COSMOS: 0.5时的尘埃质量函数和尘埃质量密度","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":"{\"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}","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}
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