Bimodal gas accretion in the Horizon-MareNostrum galaxy formation simulation

Astronomy and Astrophysics – Astrophysics

Scientific paper

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15 pages, 6 figures, accepted for publication in MNRAS, 29th of july 2008

Scientific paper

10.1111/j.1365-2966.2008.13763.x

(abridged) The physics of diffuse gas accretion and the properties of the cold and hot modes of accretion onto proto-galaxies between z=2 and z=5.4 is investigated using the large cosmological simulation performed with the RAMSES code on the MareNostrum supercomputing facility. Galactic winds, chemical enrichment, UV background heating and radiative cooling are taken into account in this very high resolution simulation. Using accretion--weighted temperature histograms, we have perfomed two different measurements of the thermal state of the gas accreted towards the central galaxy. The first measurement, performed using accretion--weighted histograms on a spherical surface of radius 0.2 Rvir centred on the densest gas structure near the halo centre of mass, is a good indicator of the presence of an accretion shock in the vicinity of the galactic disc. We define the hot shock mass, Mshock, as the typical halo mass separating cold dominated from hot dominated accretion in the vicinity of the galaxy. The second measurement is performed by radially averaging histograms between 0.2 Rvir and Rvir, in order to detect radially extended structures such as gas filaments: this is a good proxy for detecting cold streams feeding the central galaxy. We define Mstream as the transition mass separating cold dominated from hot dominated accretion in the outer halo, marking the disappearance of these cold streams. We find a hot shock transition mass of Mshock=10^{11.6} Msun (dark matter), with no significant evolution with redshift. Conversely, we find that Mstream increases sharply with z. Our measurements are in agreement with the analytical predictions of Birnboim & Dekel (2003) and Dekel & Birnboim (2006), if we correct their model by assuming low metallicity (< 10^{-3} Zsun) for the filaments, correspondingly to our measurements.

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