Burkert, A. and Förster Schreiber, N.M. and Genzel, R. and Lang, P. and Tacconi, L.J. and Wisnioski, E. and Wuyts, S. and Bandara, K. and Beifiori, A. and Bender, R. and Brammer, G. and Chan, J. and Davies, R. and Dekel, A. and Fabricius, M. and Fossati, M. and Kulkarni, S. and Lutz, D. and Mendel, J.T. and Momcheva, I. and Nelson, E.J. and Naab, T. and Renzini, A. and Saglia, R. and Sharples, R.M. and Sternberg, A. and Wilman, D. and Wuyts, E. (2016) 'The angular momentum distribution and baryon content of star forming galaxies at z~1-3.', Astrophysical journal., 826 (2). p. 214.
We analyze the angular momenta of massive star-forming galaxies (SFGs) at the peak of the cosmic star formation epoch (z ~ 0.8–2.6). Our sample of ~360 log(M */M ⊙) ~ 9.3–11.8 SFGs is mainly based on the KMOS3D and SINS/zC-SINF surveys of Hα kinematics, and collectively provides a representative subset of the massive star-forming population. The inferred halo scale angular momentum distribution is broadly consistent with that theoretically predicted for their dark matter halos, in terms of mean spin parameter $\langle \lambda \rangle $ ~ 0.037 and its dispersion (σ logλ ~ 0.2). Spin parameters correlate with the disk radial scale and with their stellar surface density, but do not depend significantly on halo mass, stellar mass, or redshift. Our data thus support the long-standing assumption that on average, even at high redshifts, the specific angular momentum of disk galaxies reflects that of their dark matter halos (j d = j DM). The lack of correlation between λ × (j d /j DM) and the nuclear stellar density Σ*(1 kpc) favors a scenario where disk-internal angular momentum redistribution leads to "compaction" inside massive high-redshift disks. For our sample, the inferred average stellar to dark matter mass ratio is ~2%, consistent with abundance matching results. Including the molecular gas, the total baryonic disk to dark matter mass ratio is ~5% for halos near 1012 M ⊙, which corresponds to 31% of the cosmologically available baryons, implying that high-redshift disks are strongly baryon dominated.
|Full text:||(AM) Accepted Manuscript|
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|Publisher Web site:||https://doi.org/10.3847/0004-637x/826/2/214|
|Publisher statement:||© 2016. The American Astronomical Society. All rights reserved.|
|Date accepted:||15 May 2016|
|Date deposited:||03 November 2016|
|Date of first online publication:||01 August 2016|
|Date first made open access:||03 November 2016|
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