Übler, H.Genzel, RWisnioski, EmilyFörster Schreiber, Natascha M FShimizu, TPrice, S. H.Tacconi, L JBelli, S.Wilman, David JFossati, M.Mendel, JonDavies, Roger L2022-03-090004-637Xhttp://hdl.handle.net/1885/261936We present the 0.6 < z < 2.6 evolution of the ionized gas velocity dispersion in 175 star-forming disk galaxies based on data from the full KMOS3D integral field spectroscopic survey. In a forward-modeling Bayesian framework including instrumental effects and beam-smearing, we fit simultaneously the observed galaxy velocity and velocity dispersion along the kinematic major axis to derive the intrinsic velocity dispersion σ0. We find a reduction of the average intrinsic velocity dispersion of disk galaxies as a function of cosmic time, from σ0 ∼ 45 km s−1 at z ∼ 2.3 to σ0 ∼ 30 km s−1 at z ∼ 0.9. There is substantial intrinsic scatter (ss » - ,int 10 km s 1 0 ) around the best-fit σ0–z relation beyond what can be accounted for from the typical measurement uncertainties (δσ0 ≈ 12 km s−1 ), independent of other identifiable galaxy parameters. This potentially suggests a dynamic mechanism such as minor mergers or variation in accretion being responsible for the scatter. Putting our data into the broader literature context, we find that ionized and atomic+molecular velocity dispersions evolve similarly with redshift, with the ionized gas dispersion being ∼10–15 km s−1 higher on average. We investigate the physical driver of the on average elevated velocity dispersions at higher redshift and find that our galaxies are at most marginally Toomre-stable, suggesting that their turbulent velocities are powered by gravitational instabilities, while stellar feedback as a driver alone is insufficient. This picture is supported through comparison with a state-of-theart analytical model of galaxy evolution.application/pdfen-AU© 2019. The American Astronomical Society.galaxies: evolutiongalaxies: high-redshiftgalaxies: ISMgalaxies: kinematics and dynamics201910.3847/1538-4357/ab27cc2020-12-20