The physical connection between central stellar surface density and stellar spin in SAMI and MaNGA nearby galaxies

Author:

Cortese L12ORCID,Fraser-McKelvie A12ORCID,Woo J3,Catinella B12ORCID,Harborne K E12ORCID,van de Sande J24ORCID,Bland-Hawthorn J24,Brough S25ORCID,Bryant J J246,Croom S24ORCID,Sweet S27ORCID

Affiliation:

1. International Centre for Radio Astronomy Research, The University of Western Australia , 35 Stirling Highway, Crawley, Perth, WA 6009, Australia

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

3. Department of Physics, Simon Fraser University , 8888 University Drive, Burnaby, BC V5A 1S6, Canada

4. Sydney Institute for Astronomy (SIfA), School of Physics, The University of Sydney , Sydney, NSW 2006, Australia

5. School of Physics, University of New South Wales , Kensington, Sydney, NSW 2052, Australia

6. Australian Astronomical Optics, AAO-USydney, School of Physics, University of Sydney , North Ryde, Sydney, NSW 2006, Australia

7. School of Mathematics and Physics, University of Queensland , Brisbane, QLD 4072, Australia

Abstract

ABSTRACT The stellar surface density within the inner 1 kpc (Σ1) has become a popular tool for understanding the growth of galaxies and its connection with the quenching of star formation. The emerging picture suggests that building a central dense core is a necessary condition for quenching. However, it is not clear whether changes in Σ1 trace changes in stellar kinematics and the growth of dispersion-dominated bulges. In this paper, we combine imaging from the Sloan Digital Sky Survey with stellar kinematics from the Sydney-AAO Multi-object Integral-field unit and Mapping Nearby Galaxies at Apache Point Observatory surveys to quantify the correlation between Σ1 and the proxy for stellar spin parameter within one effective radius (λre) for 1599 nearby galaxies. We show that, on the star-forming main sequence and at fixed stellar mass, changes in Σ1 are mirrored by changes in λre. While forming stars, main-sequence galaxies remain rotationally-dominated systems, with their Σ1 increasing but their stellar spin staying either constant or slightly increasing. The picture changes below the main sequence, where Σ1 and λre are no longer correlated. Passive systems show a narrower range of Σ1, but a wider range of λre compared to star-forming galaxies. Our results indicate that, from a structural point of view, passive galaxies are a more heterogeneous population than star-forming systems, and may have followed a variety of evolutionary paths. This also suggests that, if dispersion-dominated bulges still grow significantly at z ∼ 0, this generally takes place during, or after, the quenching phase.

Funder

Australian Research Council

Australian Government

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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