Abstract
The relationship between the already formed stellar mass in a galaxy and the gas reservoir of neutral atomic hydrogen, is a key element in our understanding of how gas is turned into stars in galaxy haloes. In this paper, we measure the MHI − M* relation based on a stellar-mass selected sample at 0.25 < z < 0.5 and the MeerKAT International GHz Tiered Extragalactic Exploration-H I Data Release 1 spectral data. Using a powerful Bayesian stacking technique, for the first time we are also able to measure the underlying bivariate distribution of H I mass and stellar mass of galaxies with M* > 109.5 M, finding that an asymmetric underlying H I distribution is strongly preferred by our complete samples. We define the concepts of the average of the logarithmic H I mass, ⟨log10(MH I)⟩, and the logarithmic average of the H I mass, log10(⟨MH I⟩), and find that the difference between ⟨log10(MH I)⟩ and log10(⟨MH I⟩) can be as large as ∼0.5 dex for the preferred asymmetric H I distribution. We observe shallow slopes in the underlying MH I − M* scaling relations, suggesting the presence of an upper H I mass limit beyond which a galaxy can no longer retain further H I gas. From our bivariate distribution we also infer the H I mass function at this redshift and find tentative evidence for a decrease of 2–10 times in the comoving space density of the most H I massive galaxies up to z ∼ 0.5.K
| Original language | English |
|---|---|
| Pages (from-to) | 1710-1731 |
| Number of pages | 22 |
| Journal | Monthly Notices of the Royal Astronomical Society |
| Volume | 544 |
| Issue number | 2 |
| Early online date | 29 Oct 2025 |
| DOIs | |
| Publication status | Published - 31 Dec 2025 |
Keywords
- radio lines: galaxies
- methods: statistical
- galaxies: fundamental parameters
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