Non-monotonic relations of galaxy star formation, radius, and structure at fixed stellar mass

Author:

Stephenson Jimena1,Rodríguez-Puebla Aldo2ORCID,Faber S M3,Primack Joel R4,Avila-Reese Vladimir2ORCID,Calette A R5ORCID,Cannarozzo Carlo267ORCID,Kakos James4ORCID,Cano-Díaz Mariana8ORCID,Koo David C3,Shankar Francesco9ORCID,Morell D F2ORCID

Affiliation:

1. University of Arizona , Tucson, Arizona 85721 , USA

2. Universidad Nacional Autónoma de México, Instituto de Astronomía , A. P. 70-264, 04510, Ciudad de México , México

3. UCO/Lick Observatory, Department of Astronomy and Astrophysics, University of California , Santa Cruz, CA 95064 , USA

4. Department of Physics, University of California , Santa Cruz, CA 95064 , USA

5. Center for Astronomy and Astrophysics, Shanghai Jiao Tong University , Shanghai 200240 , China

6. New York University Abu Dhabi , PO Box 129188, Abu Dhabi , United Arab Emirates

7. Center for Astrophysics and Space Science (CASS), New York University Abu Dhabi , Abu Dhabi, PO Box 129188, Abu Dhabi , United Arab Emirates

8. CONACYT Research Fellow – Universidad Nacional Autónoma de México, Instituto de Astronomía , A.P. 70-264, 04510, Ciudad de México , México

9. Department of Physics and Astronomy, University of Southampton , High Field SO17 1BJ , UK

Abstract

ABSTRACT We investigate the relation between galaxy structure and star formation rate (SFR) in a sample of $\sim 2.9\times 10^{4}$ central galaxies with $z\lt 0.0674$ and axial ratios $b/a\gt 0.5$. The star-forming main sequence (SFMS) shows a bend around the stellar mass of $M_\ast \le {}M_c=2\times 10^{10}{}{\rm M}_{\odot }$. At $M_\ast \le {}M_c$, the SFMS follows a power-law $\text{SFR}\propto {}M_\ast ^{0.85}$, while at higher masses it flattens. $M_c$ corresponds to a dark matter halo mass of $M_\text{vir}\sim {}10^{11.8}{\rm M}_{\odot }$ where virial shocks occurs. Some galaxy structure (e.g. half-light radius, $R_e$) exhibits a non-monotonic dependence across the SFMS at a fixed $M_\ast$. We find $\text{SFR}\propto {R_e^{-0.28}}$ at fixed $M_\ast$, consistent with the global Kennicutt–Schmidt (KS) law. This finding suggests that galaxy sizes contribute to the scatter of the SFMS. However, at $M_\ast \gt M_c$ the relationship between SFR and $R_e$ diminishes. Low-mass galaxies above the mean of the SFMS have smaller radii, exhibit compact and centrally concentrated profiles resembling green valley (GV) and quiescent galaxies at the same mass, and have higher $M_{\text{H}_2}{/}M_\rm{H\,{\small I}}$. Conversely, those below the SFMS exhibit larger radii, lower densities, have no GV or quiescent counterparts at their mass and have lower $M_{\text{H}_2}/M_\rm{H\,{\small I}}$. The above data suggest two pathways for quenching low-mass galaxies, $M_\ast \le {}M_c$: a fast one that changes the morphology on the SFMS and a slow one that does not. Above $M_c$, galaxies below the SFMS resemble GV and quiescent galaxies structurally, implying that they undergo a structural transformation already within the SFMS. For these massive galaxies, CG are strongly bimodal, with SFMS galaxies exhibiting negative colour gradients, suggesting most star formation occurs in their outskirts, maintaining them within the SFMS.

Funder

CONACYT

Publisher

Oxford University Press (OUP)

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