Journal
ASTROPHYSICAL JOURNAL
Volume 854, Issue 2, Pages -Publisher
IOP PUBLISHING LTD
DOI: 10.3847/1538-4357/aaa9bc
Keywords
galaxies: evolution; galaxies: formation; galaxies: star formation
Categories
Funding
- Ministry of Science and Technology of Taiwan [MOST 103-2112-M-001-031-MY3, 106-2112-M-001-034-]
- CONACyt [CB-180125, DGAPA-PAPIIT IA101217]
- MINEDUC-UA project [ANT 1655]
- Alfred P. Sloan Foundation
- U.S. Department of Energy Office of Science
- Brazilian Participation Group
- Carnegie Institution for Science
- Carnegie Mellon University
- Chilean Participation Group
- French Participation Group
- Harvard-Smithsonian Center for Astrophysics
- Instituto de Astrofisica de Canarias
- Johns Hopkins University
- Kavli Institute for the Physics and Mathematics of the Universe (IPMU)/University of Tokyo
- Lawrence Berkeley National Laboratory
- Leibniz Institut fur Astrophysik Potsdam (AIP)
- Max-Planck-Institut fur Astronomie (MPIA Heidelberg)
- Max-Planck-Institut fur Astrophysik (MPA Garching)
- Max-Planck-Institut fur Extraterrestrische Physik (MPE)
- National Astronomical Observatories of China
- New Mexico State University
- New York University
- University of Notre Dame
- Observatario Nacional/MCTI
- Ohio State University
- Pennsylvania State University
- Shanghai Astronomical Observatory
- United Kingdom Participation Group
- Universidad Nacional Autonoma de Mexico
- University of Arizona
- University of Colorado Boulder
- University of Oxford
- University of Portsmouth
- University of Utah
- University of Virginia
- University of Washington
- University of Wisconsin
- Vanderbilt University
- Yale University
- [ConaCyt-180125]
Ask authors/readers for more resources
The galaxy integrated Ha star formation rate-stellar mass relation, or SFR(global)-M-*((global) relation, is crucial for understanding star formation history and evolution of galaxies. However, many studies have dealt with SFR using unresolved measurements, which makes it difficult to separate out the contamination from other ionizing sources, such as active galactic nuclei and evolved stars. Using the integral field spectroscopic observations from SDSS-IV MaNGA, we spatially disentangle the contribution from different Ha powering sources for similar to 1000 galaxies. We find that, when including regions dominated by all ionizing sources in galaxies, the spatially resolved relation between Ha surface density (Sigma(H alpha) (all)) and stellar mass surface density (Sigma(*)(all)) progressively turns over at the high Sigma(*)(all) end for increasing M-*((global) and/or bulge dominance (bulge-to-total light ratio, B/T). This in turn leads to the flattening of the integrated Ha(global)-M-*((global) relation in the literature. By contrast, there is no noticeable flattening in both integrated Ha(H II)-M-*((H II) and spatially resolved Sigma(H alpha) (H II)-Sigma(*)(H II) relations when only regions where star formation dominates the ionization are considered. In other words, the flattening can be attributed to the increasing regions powered by non-star-formation sources, which generally have lower ionizing ability than star formation. An analysis of the fractional contribution of non-star-formation sources to total Ha luminosity of a galaxy suggests a decreasing role of star formation as an ionizing source toward high-mass, high-B/T galaxies and bulge regions. This result indicates that the appearance of the galaxy integrated SFR-M-*( relation critically depends on their global properties (M-*((global) and B/T) and relative abundances of various ionizing sources within the galaxies.
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