A gamma-function growth model using parameters fixed by the cosmic star formation history reproduces the observed galaxy stellar mass function from z=0 to z=8 for low and intermediate mass galaxies, but not for massive galaxies at high redshift.
On the signature of black holes on the quenched stellar mass function
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abstract
As star-forming galaxies approach or exceed a stellar mass around $10^{11} M_\odot$, they are increasingly likely to be quenched in a process generically called mass quenching. Central galaxies, which are quenched via mass rather than environmental quenching, therefore accumulate in a peak around this characteristic mass. While a number of processes may influence the shape of the quenched central stellar mass function (QCSMF), we find that its low-mass slope is strongly affected by the scatter in the mass of black holes at a given stellar mass, with higher scatters in the black hole population yielding shallower slopes. Higher scatters in the black hole mass spread out the stellar mass range over which quenching occurs, leading to shallower slopes. This trend holds across a variety of semi-analytic models and cosmological hydrodynamic simulations. A comparison with observations provides indirect evidence for a large scatter in black hole mass $\sigma(\log_{10}(M_\mathrm{BH})|M_*) \gtrsim 0.5$ dex, and a joint constraint on AGN feedback physics and the co-evolution of galaxies and black holes.
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Gamma Analytical Modeling Evolution (GAME) I: The physical implications of deriving the stellar mass functions from z=0 to z=8
A gamma-function growth model using parameters fixed by the cosmic star formation history reproduces the observed galaxy stellar mass function from z=0 to z=8 for low and intermediate mass galaxies, but not for massive galaxies at high redshift.