Quantifying Scatter in Galaxy Formation at the Lowest Masses
We predict the stellar mass–halo mass (SMHM) relationship for dwarf galaxies, using simulated galaxies with peak halo masses of M peak = 10 11 M ⊙ down into the ultra-faint dwarf range to M peak = 10 7 M ⊙ . Our simulated dwarfs have stellar masses of M star = 790 M ⊙ to 8.2 × 10 8 M ⊙ , with corres...
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Veröffentlicht in: | The Astrophysical journal 2021-12, Vol.923 (1), p.35 |
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Sprache: | eng |
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Zusammenfassung: | We predict the stellar mass–halo mass (SMHM) relationship for dwarf galaxies, using simulated galaxies with peak halo masses of
M
peak
= 10
11
M
⊙
down into the ultra-faint dwarf range to
M
peak
= 10
7
M
⊙
. Our simulated dwarfs have stellar masses of
M
star
= 790
M
⊙
to 8.2 × 10
8
M
⊙
, with corresponding
V
-band magnitudes from −2 to −18.5. For
M
peak
> 10
10
M
⊙
, the simulated SMHM relationship agrees with literature determinations, including exhibiting a small scatter of 0.3 dex. However, the scatter in the SMHM relation increases for lower-mass halos. We first present results for well-resolved halos that contain a simulated stellar population, but recognize that whether a halo hosts a galaxy is inherently mass resolution dependent. We thus adopt a probabilistic model to populate “dark” halos below our resolution limit to predict an “intrinsic” slope and scatter for the SMHM relation. We fit linearly growing log-normal scatter in stellar mass, which grows to more than 1 dex at
M
peak
= 10
8
M
⊙
. At the faintest end of the SMHM relation probed by our simulations, a galaxy cannot be assigned a unique halo mass based solely on its luminosity. Instead, we provide a formula to stochastically populate low-mass halos following our results. Finally, we show that our growing log-normal scatter steepens the faint-end slope of the predicted stellar mass function. |
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ISSN: | 0004-637X 1538-4357 |
DOI: | 10.3847/1538-4357/ac0db6 |