We present spatially resolved ALMA observations of the CO J = 3 - 2 emission line in two massive galaxies at z = 2.5 on the star-forming main sequence. Both galaxies have compact dusty star-forming cores with effective radii of Re = 1.3 ± 0.1 kpc and Re = 1.2 ± 0.1 kpc in the 870 μm continuum emission. The spatial extent of starforming molecular gas is also compact with Re = 1.9 ± 0.4 kpc and Re = 2.3 ± 0.4 kpc, but more extended than the dust emission. Interpreting the observed position-velocity diagrams with dynamical models, we find the starburst cores to be rotation dominated with the ratio of the maximum rotation velocity to the local velocity dispersion of Vmax/σ0 = 7.0+2.5-2.8 (Vmax = 386+36-32 km s-1) and Vmax/σ0 = 4.1+1.7-1.5 (Vmax = 391+54-41 km s-1). Given that the descendants of these massive galaxies in the local universe are likely ellipticals with v/σ nearly an order of magnitude lower, the rapidly rotating galaxies would lose significant net angular momentum in the intervening time. The comparisons among dynamical, stellar, gas, and dust mass suggest that the starburst CO-to-H2 conversion factor of αCO = 0.8 M⊙ (K km s-1 pc-2)-1 is appropriate in the spatially resolved cores. The dense cores are likely to be formed in extreme environments similar to the central regions of local ultraluminous infrared galaxies. Our work also demonstrates that a combination of medium-resolution CO and high-resolution dust continuum observations is a powerful tool for characterizing the dynamical state of molecular gas in distant galaxies.
Tadaki K.-I., Kodama T., Nelson E.J., Belli S., Schreiber N.M.F., Genzel R., et al. (2017). Rotating Starburst Cores in Massive Galaxies at z = 2.5. THE ASTROPHYSICAL JOURNAL LETTERS, 841(2), 1-6 [10.3847/2041-8213/aa7338].
Rotating Starburst Cores in Massive Galaxies at z = 2.5
Belli S.;
2017
Abstract
We present spatially resolved ALMA observations of the CO J = 3 - 2 emission line in two massive galaxies at z = 2.5 on the star-forming main sequence. Both galaxies have compact dusty star-forming cores with effective radii of Re = 1.3 ± 0.1 kpc and Re = 1.2 ± 0.1 kpc in the 870 μm continuum emission. The spatial extent of starforming molecular gas is also compact with Re = 1.9 ± 0.4 kpc and Re = 2.3 ± 0.4 kpc, but more extended than the dust emission. Interpreting the observed position-velocity diagrams with dynamical models, we find the starburst cores to be rotation dominated with the ratio of the maximum rotation velocity to the local velocity dispersion of Vmax/σ0 = 7.0+2.5-2.8 (Vmax = 386+36-32 km s-1) and Vmax/σ0 = 4.1+1.7-1.5 (Vmax = 391+54-41 km s-1). Given that the descendants of these massive galaxies in the local universe are likely ellipticals with v/σ nearly an order of magnitude lower, the rapidly rotating galaxies would lose significant net angular momentum in the intervening time. The comparisons among dynamical, stellar, gas, and dust mass suggest that the starburst CO-to-H2 conversion factor of αCO = 0.8 M⊙ (K km s-1 pc-2)-1 is appropriate in the spatially resolved cores. The dense cores are likely to be formed in extreme environments similar to the central regions of local ultraluminous infrared galaxies. Our work also demonstrates that a combination of medium-resolution CO and high-resolution dust continuum observations is a powerful tool for characterizing the dynamical state of molecular gas in distant galaxies.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.