Abstract
Abstract
In cosmological simulations without baryons, the relation between the specific angular momentum j
h and mass M
h of galactic dark matter halos has the well-established form
j
h
∝
M
h
2
/
3
. This is invariably adopted as the starting point in efforts to understand the analogous relation between the specific angular momentum j
* and mass M
* of the stellar parts of galaxies, which are often re-expressed relative to the corresponding halo properties through the retention fractions f
j
= j
*/j
h and f
M
= M
*/M
h. An important caveat here is that the adopted
j
h
∝
M
h
2
/
3
relation could, in principle, be modified by the gravitational back-reaction of baryons on dark matter (DM). We have tested for this possibility by comparing the j
h–M
h relations in the IllustrisTNG100 and TNG50 simulations that include baryons (full-physics runs) with their counterparts that do not (DM-only runs). In all cases, we find scaling relations of the form
j
h
∝
M
h
α
, with α ≈ 2/3 over the ranges of mass and redshift studied here: M
h ≥ 1010
M
⊙ and 0 ≤ z ≤ 2. The values of α are virtually identical in the full-physics and DM-only runs at the same redshift. The only detectable effect of baryons on the j
h–M
h relation is a slightly higher normalization, by 12%–15% at z = 0 and by 5% at z = 2. This implies that existing estimates of f
j
based on DM-only simulations should be adjusted downward by similar amounts. Finally, we discuss briefly some implications of this work for studies of galaxy formation.
Publisher
American Astronomical Society
Subject
Space and Planetary Science,Astronomy and Astrophysics
Cited by
1 articles.
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