Gas-phase metallicity break radii of star-forming galaxies in IllustrisTNG

Author:

Garcia Alex M1ORCID,Torrey Paul1ORCID,Hemler Z S2ORCID,Hernquist Lars3,Kewley Lisa J345,Nelson Erica J6,Grasha Kathryn45ORCID,Zovaro Henry R M4ORCID,Chen Qian-Hui45ORCID

Affiliation:

1. Department of Astronomy, University of Florida , 211 Bryant Space Sciences Center, Gainesville, FL 32611, USA

2. Department of Astrophysical Sciences, Princeton University , Peyton Hall, Princeton, NJ 08544, USA

3. Institute for Theory and Computation, Harvard-Smithsonian Center for Astrophysics , Cambridge, MA 02138, USA

4. Research School of Astronomy & Astrophysics, Australian National University , Canberra 2611, Australia

5. ARC Centre of Excellence for All Sky Astrophysics in 3 Dimensions (ASTRO 3D)

6. Department for Astrophysical and Planetary Science, University of Colorado , Boulder, CO 80309, USA

Abstract

ABSTRACT We present radial gas-phase metallicity profiles, gradients, and break radii at redshift z = 0–3 from the TNG50-1 star-forming galaxy population. These metallicity profiles are characterized by an emphasis on identifying the steep inner gradient and flat outer gradient. From this, the break radius, Rbreak, is defined as the region where the transition occurs. We observe the break radius having a positive trend with mass that weakens with redshift. When normalized by the stellar half-mass radius, the break radius has a weaker relation with both mass and redshift. To test if our results are dependent on the resolution or adopted physics of TNG50-1, the same analysis is performed in TNG50-2 and Illustris-1. We find general agreement between each of the simulations in their qualitative trends; however, the adopted physics between TNG and Illustris differ and therefore the breaks, normalized by galaxy size, deviate by a factor of ∼2. In order to understand where the break comes from, we define two relevant time-scales: an enrichment time-scale and a radial gas mixing time-scale. We find that Rbreak occurs where the gas mixing time-scale is ∼10 times as long as the enrichment time-scale in all three simulation runs, with some weak mass and redshift dependence. This implies that galactic discs can be thought of in two-parts: a star-forming inner disc with a steep gradient and a mixing-dominated outer disc with a flat gradient, with the break radius marking the region of transition between them.

Funder

NSF

NASA

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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