The SAMI galaxy survey: gas velocity dispersions in low-z star-forming galaxies and the drivers of turbulence

ABSTRACT We infer the intrinsic ionized gas kinematics for 383 star-forming galaxies across a range of integrated star formation rates (SFR ∈ [10−3, 102] M⊙ yr−1) at z ≲ 0.1 using a consistent 3D forward-modelling technique. The total sample is a combination of galaxies from the Sydney-AAO Multiobje...

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Bibliographic Details
Published in:Monthly Notices of the Royal Astronomical Society
Main Authors: Varidel, Mathew R, Croom, Scott M, Lewis, Geraint F, Fisher, Deanne B, Glazebrook, Karl, Catinella, Barbara, Cortese, Luca, Krumholz, Mark R, Bland-Hawthorn, Joss, Bryant, Julia J, Groves, Brent, Brough, Sarah, Federrath, Christoph, Lawrence, Jon S, Lorente, Nuria P, Owers, Matt S, Richards, Samuel N, López-Sánchez, Ángel R, Sweet, Sarah M, van de Sande, Jesse, Vaughan, Sam P
Other Authors: Australian Research Council
Format: Article in Journal/Newspaper
Language:English
Published: Oxford University Press (OUP) 2020
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Online Access:http://dx.doi.org/10.1093/mnras/staa1272
http://academic.oup.com/mnras/advance-article-pdf/doi/10.1093/mnras/staa1272/33242714/staa1272.pdf
http://academic.oup.com/mnras/article-pdf/495/2/2265/33323115/staa1272.pdf
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Summary:ABSTRACT We infer the intrinsic ionized gas kinematics for 383 star-forming galaxies across a range of integrated star formation rates (SFR ∈ [10−3, 102] M⊙ yr−1) at z ≲ 0.1 using a consistent 3D forward-modelling technique. The total sample is a combination of galaxies from the Sydney-AAO Multiobject Integral field Spectrograph (SAMI) Galaxy survey and DYnamics of Newly Assembled Massive Objects survey. For typical low-z galaxies taken from the SAMI Galaxy Survey, we find the vertical velocity dispersion (σv,z) to be positively correlated with measures of SFR, stellar mass, H i gas mass, and rotational velocity. The greatest correlation is with SFR surface density (ΣSFR). Using the total sample, we find σv,z increases slowly as a function of integrated SFR in the range SFR ∈ [10−3, 1] M⊙ yr−1 from 17 ± 3 to 24 ± 5 km s−1 followed by a steeper increase up to σv,z ∼80 km s−1 for SFR ≳ 1 M⊙ yr−1. This is consistent with recent theoretical models that suggest a σv,z floor driven by star formation feedback processes with an upturn in σv,z at higher SFR driven by gravitational transport of gas through the disc.