66 research outputs found

    Swirling around filaments: are large-scale structure vortices spinning up dark halos?

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    The kinematic analysis of dark matter and hydrodynamical simulations suggests that the vorticity in large-scale structure is mostly confined to, and predominantly aligned with their filaments, with an excess of probability of 20 per cent to have the angle between vorticity and filaments direction lower than 60 degrees relative to random orientations. The cross sections of these filaments are typically partitioned into four quadrants with opposite vorticity sign, arising from multiple flows, originating from neighbouring walls. The spins of halos embedded within these filaments are consistently aligned with this vorticity for any halo mass, with a stronger alignment for the most massive structures up to an excess of probability of 165 per cent. On large scales, adiabatic/cooling hydrodynamical simulations display the same vorticity in the gas as in the dark matter. The global geometry of the flow within the cosmic web is therefore qualitatively consistent with a spin acquisition for smaller halos induced by this large-scale coherence, as argued in Codis et al. (2012). In effect, secondary anisotropic infall (originating from the vortex-rich filament within which these lower-mass halos form) dominates the angular momentum budget of these halos. The transition mass from alignment to orthogonality is related to the size of a given multi-flow region with a given polarity. This transition may be reconciled with the standard tidal torque theory if the latter is augmented so as to account for the larger scale anisotropic environment of walls and filaments.Comment: 17 pages, 19 figures, 3 tables. accepted for publication in MNRA

    Why do extremely massive disc galaxies exist today?

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    This article has been accepted for publication in Monthly Notices of the Royal Astronomical Society, Volume 494, Issue 4, June 2020, Pages 5568–5575, https://doi.org/10.1093/mnras/staa970. ©: 2020 The Author(s). Published by Oxford University Press on behalf of the Royal Astronomical Society. All rights reserved.Galaxy merger histories correlate strongly with stellar mass, largely regardless of morphology. Thus, at fixed stellar mass, spheroids and discs share similar assembly histories, both in terms of the frequency of mergers and the distribution of their mass ratios. Since mergers are the principal drivers of disc-to-spheroid morphological transformation, and the most massive galaxies typically have the richest merger histories, it is surprising that discs exist at all at the highest stellar masses (e.g. beyond the knee of the mass function). Using Horizon-AGN, a cosmological hydro-dynamical simulation, we show that extremely massive (M*> 10^11.4 MSun) discs are created via two channels. In the primary channel (accounting for ~70% of these systems and ~8% of massive galaxies) the most recent, significant merger (stellar mass ratio > 1:10) between a massive spheroid and a gas-rich satellite `spins up' the spheroid by creating a new rotational stellar component, leaving a massive disc as the remnant. In the secondary channel (accounting for ~30% of these systems and ~3% of massive galaxies), a system maintains a disc throughout its lifetime, due to an anomalously quiet merger history. Not unexpectedly, the fraction of massive discs is larger at higher redshift, due to the Universe being more gas-rich. The morphological mix of galaxies at the highest stellar masses is, therefore, a strong function of the gas fraction of the Universe. Finally, these massive discs have similar black-hole masses and accretion rates to massive spheroids, providing a natural explanation for why a minority of powerful AGN are surprisingly found in disc galaxies.Peer reviewedFinal Published versio

    Intrinsic alignments of galaxies in the Horizon-AGN cosmological hydrodynamical simulation

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    The intrinsic alignments of galaxies are recognised as a contaminant to weak gravitational lensing measurements. In this work, we study the alignment of galaxy shapes and spins at low redshift (z0.5z\sim 0.5) in Horizon-AGN, an adaptive-mesh-refinement hydrodynamical cosmological simulation box of 100 Mpc/h a side with AGN feedback implementation. We find that spheroidal galaxies in the simulation show a tendency to be aligned radially towards over-densities in the dark matter density field and other spheroidals. This trend is in agreement with observations, but the amplitude of the signal depends strongly on how shapes are measured and how galaxies are selected in the simulation. Disc galaxies show a tendency to be oriented tangentially around spheroidals in three-dimensions. While this signal seems suppressed in projection, this does not guarantee that disc alignments can be safely ignored in future weak lensing surveys. The shape alignments of luminous galaxies in Horizon-AGN are in agreement with observations and other simulation works, but we find less alignment for lower luminosity populations. We also characterize the systematics of galaxy shapes in the simulation and show that they can be safely neglected when measuring the correlation of the density field and galaxy ellipticities.Comment: 20 pages, 23 figure

    Low-Surface-Brightness Galaxies are missing in the observed Stellar Mass Function

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    We investigate the impact of the surface brightness (SB) limit on the galaxy stellar mass functions (GSMFs) using mock surveys generated from the Horizon Run 5 (HR5) simulation. We compare the stellar-to-halo-mass relation, GSMF, and size-stellar mass relation of the HR5 galaxies with empirical data and other cosmological simulations. The mean SB of simulated galaxies are computed using their effective radii, luminosities, and colors. To examine the cosmic SB dimming effect, we compute kk-corrections from the spectral energy distributions of individual simulated galaxy at each redshift, apply the kk-corrections to the galaxies, and conduct mock surveys based on the various SB limits. We find that the GSMFs are significantly affected by the SB limits at a low-mass end. This approach can ease the discrepancy between the GSMFs obtained from simulations and observations at 0.625z20.625\le z\le 2. We also find that a redshift survey with a SB selection limit of \left^e = 28 mag arcsec2{}^{-2} will miss 20% of galaxies with Mg=109 MM_\star^g=10^{9}~{\rm M_\odot} at z=0.625z=0.625. The missing fraction of low-surface-brightness galaxies increases to 50%, 70%, and 98% at z=0.9z=0.9, 1.1, and 1.9, respectively, at the SB limit.Comment: 27 pages, 30 figures, accepted for publication in Ap

    The Role of diapycnal mixing in coupled atmosphere-ocean general circulation models

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    The value of ocean diapycnal diffusivity (v) sets the rate at which dense bottom water can be mixedup through the stratified water column and thus plays an important role in the meridional overturningcirculation (MOC). Previous idealised experiments and simplified theory suggest that the strength ofthe MOC and the ocean heat transport scale with the v. This study investigates the dependence ofthe MOC and other parameters on v using atmosphere-ocean general circulation models (AOGCM).Firstly, the dependence of the MOC strength on v is studied using a low resolution AOGCM withrealistic geometry, FORTE, with spatially constant v values ranging from 0.1 cm2/s to an unrealistichigh value of 5 cm2/s. At the cyclostationary state, global MOC strength is found to scale with v(in agreement with previous studies) according to a power law of 0.5. No power law is found for theMOC in the individual basins. The increase in MOC strength in the Atlantic and Pacific Oceans isassociated with an increase in the ocean heat transport. The atmosphere responds to the change inthe ocean state by a decrease of its energy transport and surface winds. Only a partial compensationis found between the ocean and atmosphere energy transport. The strength of v is found to have astrong impact on coupled phenomena, such as a cessation of El Niño at high v.Secondly, similar experiments are conducted with a state-of-the-art AOGCM, ECHAM5/ MPIOM.In this model, v is derived from a constant background diapycnal diffusion (b), wind inducedmixing, the Richardson number and the convective adjustment. A set of 3 coupled experiments isconducted, with b = 0.1, 0.25 and 1 cm2/s. The scaling law from simple theory and the previousexperiments with FORTE is not observed with this coupled model. At the cyclostationary state, theMOC strength weakens by 16% as b increases from 0.1 to 1 cm2/s. This behavior is not foundwhen the experiments are repeated with an ocean-only model. The reduction in MOC in the coupledmodel is linked to a strong reduction in the convective mixing at high latitudes. The convectivemixing is reduced by a continuous strong freshening in the Arctic region due to an increase in surfaceair temperature and melting of the sea-ice in the coupled experiments, which is not observed in theocean-only experiments.The responses of the two coupled models show many similarities as b increases. Both modelsshow convection in the Pacific for high values of b. The main difference is the response of the MOCin the Atlantic is linked to the different locations of the deep convection and their relative changes inthe models.I conclude that the diapycnal mixing and the ocean-atmosphere interactions both control the strengthof the MOC, and their influences cannot be considered separately
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