{"title":"A phenomenological model for bright galaxies in the high-redshift Universe","authors":"Georgios Panagiotis Nikopoulos, Pratika Dayal","doi":"arxiv-2409.10613","DOIUrl":null,"url":null,"abstract":"Recent observations by the James Webb Telescope (JWST) have unveiled numerous\ngalaxy candidates between $z \\sim 9 - 16.5$, hinting at an over-abundance of\nthe bright-end of the UV Luminosity Function (UV LF) $z \\gtrsim 11$. Possible\nsolutions require extremely bursty star formation, these systems being\ndust-free, an evolving initial mass function or even cosmic variance. In this\nwork, we develop an analytic formalism to study dust enrichment and its impact\non the UV luminosity of both main-sequence early galaxies and extremely bursty\nstar formers. Our dust model, including the key processes of dust production in\ntype II Supernovae, dust destruction, ejection, growth and sputtering, is\ncalibrated against the latest datasets from the Atacama Large Millimeter Array\n(ALMA) at $z \\sim 4-7$. The model has only 3 free parameters: (i) the star\nformation efficiency; (ii) the dust growth timescale; and (iii) the dust\ndistribution radius. Our key results are: (i) explaining the observed UV LF\nrequires an average star formation efficiency that increases with redshift as\n$f_*(z) = 10^{0.13z-3.5}$ at $z \\sim 5-13$ with a number of observations\nhinting at objects lying a factor 10 above this main-sequence. (ii) The dust\nenrichment of early systems is driven by dust production in SNII ejecta; growth\nand sputtering are the second and third most crucial processes, impacting the\ndust mass by 60% and 40% respectively at $z \\sim 7$. (iii) In our model,\ngalaxies at $z \\gtrsim 9$ can still host significant amounts of dust reaching\naverage dust-to-stellar mass ratios of 0.19% (0.14%) at $z \\sim 9$ ($z \\sim\n11$). Dust attenuation decreases with redshift due to dust being increasingly\nmore dispersed within the halo. (iv) the galaxies observed by ALMA at $z \\sim\n7$ comprise a biased sample that is not representative of the average\npopulation that makes up the UV LF.","PeriodicalId":501187,"journal":{"name":"arXiv - PHYS - Astrophysics of Galaxies","volume":"49 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Astrophysics of Galaxies","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.10613","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
Recent observations by the James Webb Telescope (JWST) have unveiled numerous
galaxy candidates between $z \sim 9 - 16.5$, hinting at an over-abundance of
the bright-end of the UV Luminosity Function (UV LF) $z \gtrsim 11$. Possible
solutions require extremely bursty star formation, these systems being
dust-free, an evolving initial mass function or even cosmic variance. In this
work, we develop an analytic formalism to study dust enrichment and its impact
on the UV luminosity of both main-sequence early galaxies and extremely bursty
star formers. Our dust model, including the key processes of dust production in
type II Supernovae, dust destruction, ejection, growth and sputtering, is
calibrated against the latest datasets from the Atacama Large Millimeter Array
(ALMA) at $z \sim 4-7$. The model has only 3 free parameters: (i) the star
formation efficiency; (ii) the dust growth timescale; and (iii) the dust
distribution radius. Our key results are: (i) explaining the observed UV LF
requires an average star formation efficiency that increases with redshift as
$f_*(z) = 10^{0.13z-3.5}$ at $z \sim 5-13$ with a number of observations
hinting at objects lying a factor 10 above this main-sequence. (ii) The dust
enrichment of early systems is driven by dust production in SNII ejecta; growth
and sputtering are the second and third most crucial processes, impacting the
dust mass by 60% and 40% respectively at $z \sim 7$. (iii) In our model,
galaxies at $z \gtrsim 9$ can still host significant amounts of dust reaching
average dust-to-stellar mass ratios of 0.19% (0.14%) at $z \sim 9$ ($z \sim
11$). Dust attenuation decreases with redshift due to dust being increasingly
more dispersed within the halo. (iv) the galaxies observed by ALMA at $z \sim
7$ comprise a biased sample that is not representative of the average
population that makes up the UV LF.