Published October 1, 2020 | Version v1
Journal article

The Evolution of the Baryons Associated with Galaxies Averaged over Cosmic Time and Space

  • 1. Max Planck Institute for Astronomy, Königstuhl 17, D-69117 Heidelberg (Germany)
  • 2. National Radio Astronomy Observatory, Pete V. Domenici Array Science Center, P.O. Box O, Socorro, NM 87801 (United States)
  • 3. INAFOsservatorio di Astrofisica e Scienza dello Spazio, via Gobetti 93/3, I-40129, Bologna (Italy)
  • 4. European Southern Observatory, Karl-Schwarzschild-Strasse 2, D-85748, Garching (Germany)
  • 5. Rutgers University, 136 Frelinghuysen Road, Piscataway, NJ 08854-8019 (United States)
  • 6. Núcleo de Astronomía, Facultad de Ingeniería y Ciencias, Universidad Diego Portales, Av. Ejército 441, Santiago (Chile)
  • 7. Argelander-Institut für Astronomie, Universität Bonn, Auf dem Hügel 71, D-53121 Bonn (Germany)
  • 8. Leiden Observatory, Leiden University, P.O. Box 9513, NL-2300 RA Leiden (Netherlands)
  • 9. Institut d'Astrophysique de Paris, Sorbonne Université, CNRS, UMR 7095, 98 bis Blvd. Arago, F-75014 Paris (France)
  • 10. International Centre for Radio Astronomy Research, The University of Western Australia, 35 Stirling Highway, Crawley WA 6009 (Australia)
  • 11. Cornell University, 220 Space Sciences Building, Ithaca, NY 14853 (United States)
  • 12. Centre for Extragalactic Astronomy, Durham University, Department of Physics, South Road, Durham DH1 3LE (United Kingdom)

Description

We combine the recent determination of the evolution of the cosmic density of molecular gas (H2) using deep, volumetric surveys, with previous estimates of the cosmic density of stellar mass, star formation rate and atomic gas (H i), to constrain the evolution of baryons associated with galaxies averaged over cosmic time and space. The cosmic H i and H2 densities are roughly equal at z ∼ 1.5. The H2 density then decreases by a factor 6 2 + 3 to today's value, whereas the H i density stays approximately constant. The stellar mass density is increasing continuously with time and surpasses that of the total gas density (H i and H2) at redshift z ∼ 1.5. The growth in stellar mass cannot be accounted for by the decrease in cosmic H2 density, necessitating significant accretion of additional gas onto galaxies. With the new H2 constraints, we postulate and put observational constraints on a two-step gas accretion process: (i) a net infall of ionized gas from the intergalactic/circumgalactic medium to refuel the extended H i reservoirs, and (ii) a net inflow of H i and subsequent conversion to H2 in the galaxy centers. Both the infall and inflow rate densities have decreased by almost an order of magnitude since z ∼ 2. Assuming that the current trends continue, the cosmic molecular gas density will further decrease by about a factor of two over the next 5 Gyr, the stellar mass will increase by approximately 10%, and cosmic star formation activity will decline steadily toward zero, as the gas infall and accretion shut down.

Availability note (English)

Available from http://dx.doi.org/10.3847/1538-4357/abb82e

Additional details

Identifiers

Publishing Information

Journal Title
Astrophysical Journal
Journal Volume
902
Journal Issue
2
Journal Page Range
[15 p.]
ISSN
0004-637X
CODEN
ASJOAB

INIS

Country of Publication
United Kingdom
Country of Input or Organization
International Atomic Energy Agency (IAEA)
INIS RN
52071878
Subject category
S79: ASTROPHYSICS, COSMOLOGY AND ASTRONOMY;
Descriptors DEI
DENSITY; GALAXIES; GALAXY NUCLEI; HYDROGEN; INTERGALACTIC SPACE; LIMITING VALUES; MASS; RED SHIFT; STARS
Descriptors DEC
ELEMENTS; NONMETALS; PHYSICAL PROPERTIES; SPACE