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Cosmic Evolution of Gas and Star Formation

  • Nick Scoville
  • , Andreas Faisst
  • , John Weaver
  • , Sune Toft
  • , Henry J. McCracken
  • , Olivier Ilbert
  • , Tanio Diaz-Santos
  • , Johannes Staguhn
  • , Jin Koda
  • , Caitlin Casey
  • , David Sanders
  • , Bahram Mobasher
  • , Nima Chartab
  • , Zahra Sattari
  • , Peter Capak
  • , Paul Vanden Bout
  • , Angela Bongiorno
  • , Catherine Vlahakis
  • , Kartik Sheth
  • , Min Yun
  • Herve Aussel, Clotilde Laigle, Dan Masters
  • California Institute of Technology
  • Cosmic Dawn Center
  • University of Copenhagen
  • Institut d'Astrophysique de Paris
  • LAM
  • Foundation for Research and Technology-Hellas
  • Johns Hopkins University
  • NASA Goddard Space Flight Center
  • University of Texas at Austin
  • University of Hawai'i at Mānoa
  • University of California at Riverside
  • Carnegie Institution of Washington
  • National Science Foundation
  • Osservatorio Astronomico Roma
  • National Aeronautics and Space Administration
  • University of Massachusetts
  • Université Paris VII
  • CNRS
  • Sorbonne Université

Research output: Contribution to journalArticlepeer-review

24 Scopus citations

Abstract

Atacama Large Millimeter/submillimeter Array (ALMA) observations of the long-wavelength dust continuum are used to estimate the gas masses in a sample of 708 star-forming galaxies at z = 0.3−4.5. We determine the dependence of gas masses and star formation efficiencies (SFEs; SFR per unit gas mass) on redshift (z), M *, and star formation rate (SFR) relative to the main sequence (MS). We find that 70% of the increase in SFRs of the MS is due to the increased gas masses at earlier epochs, while 30% is due to increased efficiency of star formation (SF). For galaxies above the MS this is reversed—with 70% of the increased SFR relative to the MS being due to elevated SFEs. Thus, the major evolution of star formation activity at early epochs is driven by increased gas masses, while the starburst activity taking galaxies above the MS is due to enhanced triggering of star formation (likely due to galactic merging). The interstellar gas peaks at z = 2 and dominates the stellar mass down to z = 1.2. Accretion rates needed to maintain continuity of the MS evolution reach >100 M yr−1 at z > 2. The galactic gas contents are likely the driving determinant for both the rise in SF and AGN activity from z = 5 to their peak at z = 2 and subsequent fall at lower z. We suggest that for self-gravitating clouds with supersonic turbulence, cloud collisions and the filamentary structure of the clouds regulate the star formation activity.

Original languageEnglish
Article number82
JournalAstrophysical Journal
Volume943
Issue number2
DOIs
StatePublished - Feb 1 2023

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