A phenomenological model for bright galaxies in the high-redshift Universe

Georgios Panagiotis Nikopoulos, Pratika Dayal
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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.
高红移宇宙中明亮星系的现象学模型
詹姆斯-韦伯望远镜(JWST)最近的观测揭示了大量介于$z \sim 9 - 16.5$之间的候选星系,暗示了紫外亮度函数(UV LF)$z \gtrsim 11$的亮端过度丰富。可能的解决方案需要极强的爆发性恒星形成、这些系统是无尘的、不断演化的初始质量函数,甚至是宇宙变异。在这项工作中,我们建立了一个分析形式来研究尘埃富集及其对主序早期星系和极迸发恒星形成者紫外光度的影响。我们的尘埃模型包括了II型超新星中尘埃产生、尘埃破坏、抛射、生长和溅射等关键过程,并根据阿塔卡马大型毫米波阵列(ALMA)在$z \sim 4-7$的最新数据集进行了校准。该模型只有三个自由参数:(i)恒星形成效率;(ii)尘埃生长时间尺度;(iii)尘埃分布半径。我们的主要结果是(i) 解释观测到的紫外低频需要一个平均恒星形成效率,这个效率随着红移的增加而增加,在$z \sim 5-13$时为$f_*(z)=10^{0.13z-3.5}$,一些观测结果提示位于这个主序之上10倍的天体。(ii) 早期系统的尘埃富集是由SNII喷出物中的尘埃生成驱动的;生长和溅射是第二和第三大关键过程,在$z \sim 7$时分别影响了60%和40%的尘埃质量。 (iii) 在我们的模型中,$z \gtrsim 9$的星系仍然可以容纳大量的尘埃,在$z \sim 9$($z \sim11$)时,平均尘埃与恒星质量比达到0.19%(0.14%)。尘埃衰减随红移而减小,这是因为尘埃在光环内越来越分散。(iv) ALMA 在 $z \sim7$ 观测到的星系是一个有偏差的样本,不能代表构成紫外低频的平均群体。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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