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    The Evolution of the Interstellar Medium in Post-starburst Galaxies

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    Li_2019_ApJ_879_131.pdf
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    Final Published Version
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    Author
    Li, Zhihui
    French, K. Decker cc
    Zabludoff, Ann I.
    Ho, Luis C. cc
    Affiliation
    Univ Arizona, Steward Observ
    Issue Date
    2019-07-16
    Keywords
    galaxies: evolution
    galaxies: ISM
    galaxies: starburst
    infrared: galaxies
    
    Metadata
    Show full item record
    Publisher
    IOP PUBLISHING LTD
    Citation
    Zhihui Li et al 2019 ApJ 879 131
    Journal
    ASTROPHYSICAL JOURNAL
    Rights
    Copyright © 2019. The American Astronomical Society. All rights reserved.
    Collection Information
    This item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at repository@u.library.arizona.edu.
    Abstract
    We derive dust masses (M-dust) from the spectral energy distributions of 58 post-starburst galaxies (PSBs). There is an anticorrelation between specific dust mass (M-dust/M-star) and the time elapsed since the starburst ended, indicating that dust was either destroyed, expelled, or rendered undetectable over the similar to 1 Gyr after the burst. The M-dust/M-star depletion timescale, 205(-37)(+58) Myr, is consistent with that of the CO-traced M-H2/M-star, suggesting that dust and gas are altered via the same process. Extrapolating these trends leads to the M-dust/M-star and M-H2/M-star values of early-type galaxies (ETGs) within 1-2 Gyr, a timescale consistent with the evolution of other PSB properties into ETGs. Comparing M-dust and M-H2 for PSBs yields a calibration, log M-H2 = 0.45 log M-dust + 6.02, that allows us to place 33 PSBs on the Kennicutt-Schmidt (KS) plane, Sigma SFR-Sigma M-H2. Over the first similar to 200-300 Myr, the PSBs evolve down and off of the KS relation, as their star formation rate (SFR) decreases more rapidly than M-H2. Afterwards, M-H2 continues to decline whereas the SFR levels off. These trends suggest that the star formation efficiency bottoms out at 10-11 yr(-1) and will rise to ETG levels within 0.5-1.1 Gyr afterwards. The SFR decline after the burst is likely due to the absence of gas denser than the CO-traced H-2. The mechanism of the M-dust/M-star and M-H2/M-star decline, whose timescale suggests active galactic nucleus/low-ionization nuclear emission-line region feedback, may also be preventing the large CO-traced molecular gas reservoirs from collapsing and forming denser star-forming clouds.
    ISSN
    0004-637X
    EISSN
    1538-4357
    DOI
    10.3847/1538-4357/ab1f68
    Version
    Final published version
    Sponsors
    Study Abroad Scholarship for Excellent Students by China Scholarship Council for undergraduate research [HST-HF2-51391.001-A]; NASA [ADP-NNX10AE88G]; Space Telescope Science Institute; National Key R&D Program of China [2016YFA0400702]; National Science Foundation of China [11721303]; Alfred P. Sloan Foundation; U.S. Department of Energy Office of Science; Center for High-Performance Computing at the University of Utah; Carnegie Institution for Science; Chilean Participation Group; French Participation Group; Harvard-Smithsonian Center for Astrophysics; Johns Hopkins University; Kavli Institute for the Physics and Mathematics of the Universe (IPMU)/University of Tokyo; Max-Planck-Institut fur Astrophysik (MPA Garching); Max-Planck-Institut fur Extraterrestrische Physik (MPE); New Mexico State University, New York University, University of Notre Dame, Observatario Nacional/MCTI; Shanghai Astronomical Observatory, United Kingdom Participation Group; Yale University - National Aeronautics and Space Administration; National Science Foundation - National Aeronautics and Space Administration
    ae974a485f413a2113503eed53cd6c53
    10.3847/1538-4357/ab1f68
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