Abstract
Even though the dark-matter power spectrum in the absence of biasing predicts a number density of haloes n(M) ∝M-2 (i.e. a Schechter α value of -2) at the low-mass end (M < 1010M⊙), hydrodynamic simulations have typically produced values for stellar systems in good agreement with the observed value α≃-1. We explain this with a simple physical argument and show that an efficient external gas-heating mechanism (such as the UV background included in all hydro codes) will produce a critical halo mass below which haloes cannot retain their gas and form stars. We test this conclusion with gadget-2-based simulations using various UV backgrounds, and for the first time we also investigate the effect of an X-ray background. We show that at the present epoch α depends primarily on the mean gas temperature at the star-formation epoch for low-mass systems (z≲ 3): with no background we find α≃-1.5, with UV only α≃-1.0 and with UV and X-rays α≃-0.75. We find the critical final halo mass for star formation to be ∼4 × 108M⊙ with a UV background and ∼7 × 108M⊙ with UV and X-rays. © 2011 The Authors Monthly Notices of the Royal Astronomical Society © 2011 RAS.
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Hambrick, D. C., Ostriker, J. P., Johansson, P. H., & Naab, T. (2011). The effects of X-ray and UV background radiation on the low-mass slope of the galaxy mass function. Monthly Notices of the Royal Astronomical Society, 413(4), 2421–2428. https://doi.org/10.1111/j.1365-2966.2011.18312.x
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