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Published August 2022 | Supplemental Material + Submitted + Published
Journal Article Open

Hot-mode accretion and the physics of thin-disc galaxy formation

Abstract

We use FIRE simulations to study disc formation in z ∼ 0, Milky Way-mass galaxies, and conclude that a key ingredient for the formation of thin stellar discs is the ability for accreting gas to develop an aligned angular momentum distribution via internal cancellation prior to joining the galaxy. Among galaxies with a high fraction (⁠>70 per cent⁠) of their young stars in a thin disc (h/R ∼ 0.1), we find that: (i) hot, virial-temperature gas dominates the inflowing gas mass on halo scales (≳20 kpc), with radiative losses offset by compression heating; (ii) this hot accretion proceeds until angular momentum support slows inward motion, at which point the gas cools to ≲10⁴K⁠; (iii) prior to cooling, the accreting gas develops an angular momentum distribution that is aligned with the galaxy disc, and while cooling transitions from a quasi-spherical spatial configuration to a more-flattened, disc-like configuration. We show that the existence of this 'rotating cooling flow' accretion mode is strongly correlated with the fraction of stars forming in a thin disc, using a sample of 17 z ∼ 0 galaxies spanning a halo mass range of 10^(10.5) M⊙ ≲ M_h ≲ 10¹² M⊙ and stellar mass range of 10⁸ M⊙ ≲ M⋆ ≲ 10¹¹ M⊙. Notably, galaxies with a thick disc or irregular morphology do not undergo significant angular momentum alignment of gas prior to accretion and show no correspondence between halo gas cooling and flattening. Our results suggest that rotating cooling flows (or, more generally, rotating subsonic flows) that become coherent and angular momentum-supported prior to accretion on to the galaxy are likely a necessary condition for the formation of thin, star-forming disc galaxies in a ΛCDM universe.

Additional Information

© 2022 The Author(s). Published by Oxford University Press on behalf of Royal Astronomical Society. This article is published and distributed under the terms of the Oxford University Press, Standard Journals Publication Model (https://academic.oup.com/journals/pages/open_access/funder_policies/chorus/standard_publication_model). Accepted 2022 June 8. Received 2022 June 6; in original form 2022 January 19. Published: 14 June 2022. ZH was supported by a Gary A. McCue postdoctoral fellowship at UC Irvine. JS was supported by the Israel Science Foundation (grant no. 2584/21) and by the German Science Foundation via DIP grant STE 1869/2-1 GE 625/17-1. JSB was supported by NSF grant AST-1910346. ABG was supported by an NSF-GRFP under grant DGE-1842165 and was additionally supported by NSF grants DGE-0948017 and DGE-145000. SY was supported by NSF grant AST-1910346. CAFG was supported by NSF through grants AST-1715216, AST-2108230, and CAREER award AST-1652522; by NASA through grant 17-ATP17-0067; by STScI through grant HST-AR-16124.001-A; and by the Research Corporation for Science Advancement through a Cottrell Scholar Award. DBF is supported by the Simons Foundation through the Flatiron Institute. DAA was supported in part by NSF grants AST-2009687 and AST-2108944 and by the Flatiron Institute, which is supported by the Simons Foundation. EQ was supported in part by a Simons Investigator grant from the Simons Foundation and NSF grant 2107872. AW received support from: NSF grants CAREER 2045928 and 2107772; NASA ATP grant 80NSSC20K0513; HST grants AR-15809 and GO-15902 from STScI; a Scialog Award from the Heising-Simons Foundation; and a Hellman Fellowship. MBK acknowledges support from NSF CAREER award AST-1752913, NSF grants AST-1910346 and AST-2108962, NASA grant NNX17AG29G, and HST-AR-15006, HST-AR-15809, HST-GO-15658, HST-GO-15901, HST-GO-15902, HST-AR-16159, and HST-GO-16226 from the Space Telescope Science Institute, which is operated by AURA, Inc., under NASA contract NAS5-26555. JM gratefully acknowledges sabbatical leave support from Pomona College and the Harry and Grace Steele Foundation. RF acknowledges financial support from the Swiss National Science Foundation (grant no. PP00P2_194814 and 200021_188552). TKC is supported by Science and Technology Facilities Council (STFC) astronomy consolidated grant ST/P000541/1 and ST/T000244/1. CT and DK were supported by NSF grants AST-1715101 and AST-2108314. Numerical calculations were performed on the Quest computing cluster at Northwestern University, the Wheeler computing cluster at Caltech, XSEDE allocations TG-AST130039, TG-AST120025, TG-AST140064, and TG-AST140023, Blue Waters PRAC allocation NSF.1713353, NASA HEC allocation SMD16-7592, and allocations AST21010 and AST20016 supported by the NSF and TACC. This research benefited from the Halo21 KITP workshop, which was supported in part by the National Science Foundation under grant no. NSF PHY-1748958. This research used the PYTHON programming language and the following modules: FIREFLY (Geller & Gurvich 2018), NUMPY (Harris et al. 2020), MATPLOTLIB (Hunter 2007), PYTEST (Krekel et al. 2004), JUG (Coelho 2017), H5PY (Collette 2013), SCIPY (Virtanen et al. 2020), PANDAS (McKinney 2010; Reback et al. 2020), PALETTABLE (https://github.com/jiffyclub/palettable), and NUMBA (Lam, Pitrou & Seibert 2015). Data Availability: The data underlying this article will be shared on reasonable request to the corresponding author (ZH). The simulation initial conditions, snapshot files, and visualization can be found in https://fire.northwestern.edu/data/. A public version of the GIZMO simulation code is available http://www.tapir.caltech.edu/phopkins/Site/GIZMO.html.

Attached Files

Published - stac1603.pdf

Submitted - 2201.07235.pdf

Supplemental Material - stac1603_supplemental_files.zip

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Additional details

Created:
August 20, 2023
Modified:
October 23, 2023