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The effect of gas physics on the halo mass function

dc.contributor.authorStanek, R. M. (Rebecca M.)en_US
dc.contributor.authorRudd, D.en_US
dc.contributor.authorEvrard, August E.en_US
dc.date.accessioned2010-04-01T15:38:40Z
dc.date.available2010-04-01T15:38:40Z
dc.date.issued2009-03-21en_US
dc.identifier.citationStanek, R.; Rudd, D.; Evrard, A. E. (2009). "The effect of gas physics on the halo mass function." Monthly Notices of the Royal Astronomical Society: Letters 394(1): L11-L15. <http://hdl.handle.net/2027.42/66132>en_US
dc.identifier.issn1745-3925en_US
dc.identifier.issn1745-3933en_US
dc.identifier.urihttps://hdl.handle.net/2027.42/66132
dc.description.abstractCosmological tests based on cluster counts require accurate calibration of the space density of massive haloes, but most calibrations to date have ignored complex gas physics associated with halo baryons. We explore the sensitivity of the halo mass function to baryon physics using two pairs of gas-dynamic simulations that are likely to bracket the true behaviour. Each pair consists of a baseline model involving only gravity and shock heating, and a refined physics model aimed at reproducing the observed scaling of the hot, intracluster gas phase. One pair consists of billion-particle resimulations of the original 500  h −1  Mpc Millennium Simulation of Springel et al., run with the smoothed particle hydrodynamics (SPH) code gadget-2 and using a refined physics treatment approximated by pre-heating (PH) at high redshift. The other pair are high-resolution simulations from the adaptive-mesh refinement code art, for which the refined treatment includes cooling, star formation and supernova feedback (CSF). We find that, although the mass functions of the gravity-only (GO) treatments are consistent with the recent calibration of Tinker et al. (2008) , both pairs of simulations with refined baryon physics show significant deviations. Relative to the GO case, the masses of ∼10 14   h −1  M haloes in the PH and CSF treatments are shifted by the averages of −15 ± 1 and +16 ± 2 per cent, respectively. These mass shifts cause ∼30 per cent deviations in number density relative to the Tinker function, significantly larger than the 5 per cent statistical uncertainty of that calibration.en_US
dc.format.extent246649 bytes
dc.format.extent3110 bytes
dc.format.mimetypeapplication/pdf
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dc.publisherBlackwell Publishing Ltden_US
dc.rightsJournal compilation © 2009 RASen_US
dc.subject.otherGalaxies: Clusters: Generalen_US
dc.subject.otherCosmology: Theoryen_US
dc.titleThe effect of gas physics on the halo mass functionen_US
dc.typeArticleen_US
dc.rights.robotsIndexNoFollowen_US
dc.subject.hlbsecondlevelAstronomyen_US
dc.subject.hlbtoplevelScienceen_US
dc.description.peerreviewedPeer Revieweden_US
dc.contributor.affiliationumDepartment of Astronomy, University of Michigan, 500 Church St, Ann Arbor, MI 48109, USAen_US
dc.contributor.affiliationumDepartment of Physics and Michigan Center for Theoretical Physics, University of Michigan, 450 Church St, Ann Arbor, MI 48109, USAen_US
dc.contributor.affiliationotherSchool of Natural Sciences, Institute for Advanced Study, Einstein Drive, Princeton, NJ 08540, USAen_US
dc.description.bitstreamurlhttp://deepblue.lib.umich.edu/bitstream/2027.42/66132/1/j.1745-3933.2008.00597.x.pdf
dc.identifier.doi10.1111/j.1745-3933.2008.00597.xen_US
dc.identifier.sourceMonthly Notices of the Royal Astronomical Society: Lettersen_US
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dc.owningcollnameInterdisciplinary and Peer-Reviewed


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