Volume 413, Issue 4 pp. 2421-2428

The effects of X-ray and UV background radiation on the low-mass slope of the galaxy mass function

D. C. Hambrick

Corresponding Author

D. C. Hambrick

Princeton University Observatory, Princeton, NJ 08544, USA

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J. P. Ostriker

J. P. Ostriker

Princeton University Observatory, Princeton, NJ 08544, USA

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P. H. Johansson

P. H. Johansson

Finnish Centre for Astronomy with ESO, University of Turku, Väisäläntie 20, FI-21500 Piikkiö, Finland

Division of Geophysics and Astronomy, Department of Physics, University of Helsinki, PO Box 64, FI-00014 Helsinki, Finland

University Observatory Munich, Scheinerstr. 1, 81679 Munich, Germany

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T. Naab

T. Naab

University Observatory Munich, Scheinerstr. 1, 81679 Munich, Germany

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First published: 06 April 2011
Citations: 1

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 < 1010 M), 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 × 108 M with a UV background and ∼7 × 108 M with UV and X-rays.

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