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The main sequence of star-forming galaxies across cosmic times

P. PopessoEuropean Southern Observatory , Karl Schwarzschildstrasse 2, D-85748 Garching bei München, GermanyAlice ConcasEuropean Southern Observatory , Karl Schwarzschildstrasse 2, D-85748 Garching bei München, GermanyG. CresciINAF-Osservatorio Astronomico di Arcetri , Largo Enrico Fermi 5, I-50125 Firenze, ItalySirio BelliDipartimento di Fisica e Astronomia “Augusto Righi”, Università di Bologna , Viale Berti Pichat 6/2, Bologna, ItalyL. BisigelloDipartimento di Fisica e Astronomia, Universitá di Padova , Vicolo dell’ Osservatorio 3, I-35122 Padova, ItalyHanae InamiMark DickinsonNOIRLab , 950 N. Cherry Ave. Tucson, AZ 85719, USAO. IlbertLaboratoire d’Astrophysique de Marseille , 38 rue Frederic Joliot Curie, F-13388 Marseille, FranceM. PannellaDipartimento di Fisica e Astronomia, Universitá di Trieste , Via Valerio, 2, I-34127 Trieste, ItalyD. ElbazLaboratoire AIM-Paris-Saclay, CEA/DRF/Irfu - CNRS - Université Paris Diderot , CEA-Saclay, F-91191 Gif-sur-Yvette, France
2022en
ABI

Аннотация

ABSTRACT By compiling a comprehensive census of literature studies, we investigate the evolution of the main sequence (MS) of star-forming galaxies (SFGs) in the widest range of redshift (0 < z < 6) and stellar mass (108.5–1011.5 M⊙) ever probed. We convert all observations to a common calibration and find a remarkable consensus on the variation of the MS shape and normalization across cosmic time. The relation exhibits a curvature towards the high stellar masses at all redshifts. The best functional form is governed by two parameters: the evolution of the normalization and the turnover mass (M0(t)), which both evolve as a power law of the Universe age. The turn-over mass determines the MS shape. It marginally evolves with time, making the MS slightly steeper towards z ∼ 4–6. At stellar masses below M0(t), SFGs have a constant specific SFR (sSFR), while above M0(t) the sSFR is suppressed. We find that the MS is dominated by central galaxies. This allows to turn M0(t) into the corresponding host halo mass. This evolves as the halo mass threshold between cold and hot accretion regimes, as predicted by the theory of accretion, where the central galaxy is fed or starved of cold gas supply, respectively. We, thus, argue that the progressive MS bending as a function of the Universe age is caused by the lower availability of cold gas in haloes entering the hot accretion phase, in addition to black hole feedback. We also find qualitatively the same trend in the largest sample of star-forming galaxies provided by the IllustrisTNG simulation. Nevertheless, we still note large quantitative discrepancies with respect to observations, in particular at the high-mass end. These can not be easily ascribed to biases or systematics in the observed SFRs and the derived MS.

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