From Stellar Halos to Intracluster Light: the physics of the Intra-Halo Stellar Component in cosmological hydrodynamical simulations

Abstract

We study the Intra-Halo Stellar Component (IHSC) of Milky Way-mass systems up to galaxy clusters in the Horizon-AGN cosmological hydrodynamical simulation. We identify the IHSC using an improved phase-space galaxy finder algorithm which provides an adaptive, physically motivated and shape-independent definition of this stellar component, that can be applied to halos of arbitrary masses. We explore the IHSC mass fraction-total halo's stellar mass, fM*,IHSC-M*, relation and the physical drivers of its scatter. We find that on average the fM*,IHSC increases with M*,tot, with the scatter decreasing strongly with mass from 2 dex at M*,tot1011M to 0.3 dex at group masses. At high masses, M*,tot>1011.5M, fM*,IHSC increases with the number of substructures, and with the mass ratio between the central galaxy and largest satellite, at fixed M*,tot. From mid-size groups and systems below M*,tot<1012M, we find that the central galaxy's stellar rotation-to-dispersion velocity ratio, V/σ, displays the strongest (anti)-correlation with fM*,IHSC at fixed M*,tot of all the galaxy and halo properties explored, transitioning from fM*,IHSC<0.1% for high V/σ, to fM*,IHSC5% for low V/σ galaxies. By studying the fM*,IHSC temporal evolution, we find that, in the former, mergers not always take place, but if they did, they happened early (z>1), while the high fM*,IHSC population displays a much more active merger history. In the case of massive groups and galaxy clusters, M*,tot>1012M, a fraction fM*,IHSC10-20% is reached at z1 and then they evolve across lines of constant fM*,IHSC modulo some small perturbations. Because of the limited simulation's volume, the latter is only tentative and requires a larger sample of simulated galaxy clusters to confirm.

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