The effects of X-ray and UV background radiation on the low-mass slope of the galaxy mass function
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 v...
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Published in | Monthly notices of the Royal Astronomical Society Vol. 413; no. 4; pp. 2421 - 2428 |
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Main Authors | , , , |
Format | Journal Article |
Language | English |
Published |
Oxford, UK
Blackwell Publishing Ltd
01.06.2011
Wiley-Blackwell Oxford University Press |
Subjects | |
Online Access | Get full text |
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Summary: | 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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Bibliography: | istex:9BC034714394FAA5651FC49929EE667BBE54F0CE ArticleID:MNR18312 ark:/67375/WNG-SDMM3T2R-J ObjectType-Article-1 SourceType-Scholarly Journals-1 ObjectType-Feature-2 content type line 23 |
ISSN: | 0035-8711 1365-2966 |
DOI: | 10.1111/j.1365-2966.2011.18312.x |