H α emission in local galaxies: star formation, time variability, and the diffuse ionized gas

Author:

Tacchella Sandro1234ORCID,Smith Aaron5ORCID,Kannan Rahul2ORCID,Marinacci Federico6ORCID,Hernquist Lars2,Vogelsberger Mark5ORCID,Torrey Paul7ORCID,Sales Laura8ORCID,Li Hui9ORCID

Affiliation:

1. Department of Physics, Ulsan National Institute of Science and Technology (UNIST) , Ulsan 44919, Republic of Korea

2. Center for Astrophysics | Harvard & Smithsonian , 60 Garden St, Cambridge, MA 02138, USA

3. Kavli Institute for Cosmology, University of Cambridge , Madingley Road, Cambridge, CB3 0HA, UK

4. Cavendish Laboratory, University of Cambridge , 19 JJ Thomson Avenue, Cambridge, CB3 0HE, UK

5. Department of Physics, Massachusetts Institute of Technology , Cambridge, MA 02139, USA

6. Department of Physics and Astronomy ‘Augusto Righi’, University of Bologna , via Gobetti 93/2, I-40129 Bologna, Italy

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

8. Department of Physics and Astronomy, University of California , Riverside, 900 University Avenue, Riverside, CA 92521, USA

9. Department of Astronomy, Columbia University , New York, NY 10027, USA

Abstract

ABSTRACT The nebular recombination line H α is widely used as a star formation rate (SFR) indicator in the local and high-redshift Universe. We present a detailed H α radiative transfer study of high-resolution isolated Milky-Way and Large Magellanic Cloud simulations that include radiative transfer, non-equilibrium thermochemistry, and dust evolution. We focus on the spatial morphology and temporal variability of the H α emission, and its connection to the underlying gas and star formation properties. The H α and H β radial and vertical surface brightness profiles are in excellent agreement with observations of nearby galaxies. We find that the fraction of H α emission from collisional excitation amounts to fcol ∼ 5–$10{{\ \rm per\ cent}}$, only weakly dependent on radius and vertical height, and that scattering boosts the H α luminosity by $\sim 40{{\ \rm per\ cent}}$. The dust correction via the Balmer decrement works well (intrinsic H α emission recoverable within 25 per cent), though the dust attenuation law depends on the amount of attenuation itself both on spatially resolved and integrated scales. Important for the understanding of the H α–SFR connection is the dust and helium absorption of ionizing radiation (Lyman continuum [LyC] photons), which are about $f_{\rm abs}\approx 28{{\ \rm per\ cent}}$ and $f_{\rm He}\approx 9{{\ \rm per\ cent}}$, respectively. Together with an escape fraction of $f_{\rm esc}\approx 6{{\ \rm per\ cent}}$, this reduces the available budget for hydrogen line emission by nearly half ($f_{\rm H}\approx 57{{\ \rm per\ cent}}$). We discuss the impact of the diffuse ionized gas, showing – among other things – that the extraplanar H α emission is powered by LyC photons escaping the disc. Future applications of this framework to cosmological (zoom-in) simulations will assist in the interpretation of spectroscopy of high-redshift galaxies with the upcoming James Webb Space Telescope.

Funder

ST

UNIST

Ulsan National Institute of Science and Technology

Smithsonian Astrophysical Observatory

CFA

NASA

Space Telescope Science Institute

NSF

NAS

Alfred P. Sloan Foundation

U.S. Department of Energy

University of Utah

Carnegie Mellon University

Johns Hopkins University

University of Tokyo

Lawrence Berkeley National Laboratory

Leibniz Institute for Astrophysics Potsdam

New Mexico State University

New York University

University of Notre Dame

MCTI

Ohio State University

Pennsylvania State University

Universidad Nacional Autónoma de México

University of Arizona

University of Colorado Boulder

Oxford University

University of Portsmouth

University of Virginia

University of Washington

Vanderbilt University

Yale University

Publisher

Oxford University Press (OUP)

Subject

Space and Planetary Science,Astronomy and Astrophysics

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