9 research outputs found

    The Cosmic Mach Number as an Environment Measure for the Underlying Dark Matter Density Field

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    Using cosmological dark matter only simulations of a (1.6(1.6 Gpc/h)3/h)^3 volume from the Legacy simulation project, we calculate Cosmic Mach Numbers (CMN) and perform a theoretical investigation of their relation with halo properties and features of the density field to gauge their use as an measure of the environment. CMNs calculated on individual spheres show correlations with both the overdensity in a region and the density gradient in the direction of the bulk flow around that region. To reduce the scatter around the median of these correlations, we introduce a new measure, the rank ordered Cosmic Mach number (M^g\hat{\mathcal{M}}_g), which shows a tight correlations with the overdensity ÎŽ=ρ−ρˉρˉ\delta=\frac{\rho-\bar{\rho}}{\bar{\rho}}. Measures of the large scale density gradient as well as other average properties of the halo population in a region show tight correlations with M^g\hat{\mathcal{M}}_g as well. Our results in this first empirical study suggest that M^g\hat{\mathcal{M}}_g is an excellent proxy for the underlying density field and hence environment that can circumvent reliance on number density counts in a region. For scales between 1010 and 100Mpc100 Mpc/h, Mach numbers calculated using dark matter halos (>1012(> 10^{12} M⊙)_{\odot}) that would typically host massive galaxies are consistent with theoretical predictions of the linear matter power spectrum at a level of 10%10\% due to non-linear effects of gravity. At redshifts z≄3z\geq 3, these deviations disappear. We also quantify errors due to missing large scale modes in simulations. Simulations of box size ≀1\leq 1 Gpc/hh typically predict CMNs 10-30\% too small on scales of∌100\sim 100 Mpc/h/h.Comment: 16 pages, 20 figures. Accepted for publication in MNRAS on 08/02/2022. Typos correcte

    Sterile neutrino dark matter bounds from galaxies of the Local Group

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    We show that the canonical oscillation-based (non-resonant) production of sterile neutrino dark matter is inconsistent at >99>99% confidence with observations of galaxies in the Local Group. We set lower limits on the non-resonant sterile neutrino mass of 2.52.5 keV (equivalent to 0.70.7 keV thermal mass) using phase-space densities derived for dwarf satellite galaxies of the Milky Way, as well as limits of 8.88.8 keV (equivalent to 1.81.8 keV thermal mass) based on subhalo counts of NN-body simulations of M 31 analogues. Combined with improved upper mass limits derived from significantly deeper X-ray data of M 31 with full consideration for background variations, we show that there remains little room for non-resonant production if sterile neutrinos are to explain 100100% of the dark matter abundance. Resonant and non-oscillation sterile neutrino production remain viable mechanisms for generating sufficient dark matter sterile neutrinos.Comment: 10 pages, 4 figures, 2 tables. Submitted to PR

    Sweating the small stuff: simulating dwarf galaxies, ultra-faint dwarf galaxies, and their own tiny satellites

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    We present FIRE/Gizmo hydrodynamic zoom-in simulations of isolated dark matter halos, two each at the mass of classical dwarf galaxies (Mvir≃1010M⊙M_{\rm vir} \simeq 10^{10} M_{\odot}) and ultra-faint galaxies (Mvir≃109M⊙M_{\rm vir} \simeq 10^9 M_{\odot}), and with two feedback implementations. The resultant central galaxies lie on an extrapolated abundance matching relation from M⋆≃106M_{\star} \simeq 10^6 to 104M⊙10^4 M_{\odot} without a break. Every host is filled with subhalos, many of which form stars. Our dwarfs with M⋆≃106M⊙M_{\star} \simeq 10^6 M_{\odot} each have 1-2 well-resolved satellites with M⋆=3−200×103M⊙M_{\star} = 3-200 \times 10^3 M_{\odot}. Even our isolated ultra-faint galaxies have star-forming subhalos. If this is representative, dwarf galaxies throughout the universe should commonly host tiny satellite galaxies of their own. We combine our results with the ELVIS simulations to show that targeting ∌50 kpc\sim 50~ \rm kpc regions around nearby isolated dwarfs could increase the chances of discovering ultra-faint galaxies by ∌35%\sim 35\% compared to random halo pointings, and specifically identify the region around the Phoenix dwarf galaxy as a good potential target. The well-resolved ultra-faint galaxies in our simulations (M⋆≃3−30×103M⊙M_{\star} \simeq 3 - 30 \times 10^3 M_{\odot}) form within Mpeak≃0.5−3×109M⊙M_{\rm peak} \simeq 0.5 - 3 \times 10^9 M_{\odot} halos. Each has a uniformly ancient stellar population (>10 Gyr > 10~ \rm Gyr) owing to reionization-related quenching. More massive systems, in contrast, all have late-time star formation. Our results suggest that Mhalo≃5×109M⊙M_{\rm halo} \simeq 5 \times 10^9 M_{\odot} is a probable dividing line between halos hosting reionization "fossils" and those hosting dwarfs that can continue to form stars in isolation after reionization.Comment: 12 pages, 6 figures, 1 table, submitted to MNRA

    The agora high-resolution galaxy simulations comparison project

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    We introduce the Assembling Galaxies Of Resolved Anatomy (AGORA) project, a comprehensive numerical study of well-resolved galaxies within the ΛCDM cosmology. Cosmological hydrodynamic simulations with force resolutions of ~100 proper pc or better will be run with a variety of code platforms to follow the hierarchical growth, star formation history, morphological transformation, and the cycle of baryons in and out of eight galaxies with halo masses Mvir 1010, 1011, 1012, and 1013 M☉ at z = 0 and two different ("violent" and "quiescent") assembly histories. The numerical techniques and implementations used in this project include the smoothed particle hydrodynamics codes GADGET and GASOLINE, and the adaptive mesh refinement codes ART, ENZO, and RAMSES. The codes share common initial conditions and common astrophysics packages including UV background, metal-dependent radiative cooling, metal and energy yields of supernovae, and stellar initial mass function. These are described in detail in the present paper. Subgrid star formation and feedback prescriptions will be tuned to provide a realistic interstellar and circumgalactic medium using a non-cosmological disk galaxy simulation. Cosmological runs will be systematically compared with each other using a common analysis toolkit and validated against observations to verify that the solutions are robust—i.e., that the astrophysical assumptions are responsible for any success, rather than artifacts of particular implementations. The goals of the AGORA project are, broadly speaking, to raise the realism and predictive power of galaxy simulations and the understanding of the feedback processes that regulate galaxy "metabolism." The initial conditions for the AGORA galaxies as well as simulation outputs at various epochs will be made publicly available to the community. The proof-of-concept dark-matter-only test of the formation of a galactic halo with a z = 0 mass of Mvir 1.7 × 1011 M☉ by nine different versions of the participating codes is also presented to validate the infrastructure of the project

    The wide-field, multiplexed, spectroscopic facility WEAVE: Survey design, overview, and simulated implementation

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    International audienceWEAVE, the new wide-field, massively multiplexed spectroscopic survey facility for the William Herschel Telescope, will see first light in late 2022. WEAVE comprises a new 2-degree field-of-view prime-focus corrector system, a nearly 1000-multiplex fibre positioner, 20 individually deployable 'mini' integral field units (IFUs), and a single large IFU. These fibre systems feed a dual-beam spectrograph covering the wavelength range 366-959 nm at R ~ 5000, or two shorter ranges at R ~ 20 000. After summarising the design and implementation of WEAVE and its data systems, we present the organisation, science drivers and design of a five- to seven-year programme of eight individual surveys to: (i) study our Galaxy's origins by completing Gaia's phase-space information, providing metallicities to its limiting magnitude for ~3 million stars and detailed abundances for ~1.5 million brighter field and open-cluster stars; (ii) survey ~0.4 million Galactic-plane OBA stars, young stellar objects and nearby gas to understand the evolution of young stars and their environments; (iii) perform an extensive spectral survey of white dwarfs; (iv) survey ~400 neutral-hydrogen-selected galaxies with the IFUs; (v) study properties and kinematics of stellar populations and ionised gas in z 1 million spectra of LOFAR-selected radio sources; (viii) trace structures using intergalactic/circumgalactic gas at z > 2. Finally, we describe the WEAVE Operational Rehearsals using the WEAVE Simulator
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