18 research outputs found
Multimessenger study of merging massive black holes in the Obelisk simulation: gravitational waves, electromagnetic counterparts, and their link to galaxy and black hole populations
Massive black hole (BH) mergers are predicted to be powerful sources of
low-frequency gravitational waves (GWs). Coupling the detection of GWs with
electromagnetic (EM) detection can provide key information about merging BHs
and their environments. We study the high-resolution cosmological
radiation-hydrodynamics simulation Obelisk, run to redshift , to assess
the GW and EM detectability of high-redshift BH mergers, modelling spectral
energy distribution and obscuration. For EM detectability we further consider
sub-grid dynamical delays in postprocessing. We find that most of the merger
events can be detected by LISA, except for high-mass mergers with very unequal
mass ratios. Intrinsic binary parameters are accurately measured, but the sky
localisation is poor generally. Only of these high-redshift sources
have sky localisation better than . Merging BHs are hard to
detect in the restframe UV since they are fainter than the host galaxies, which
at high are star-forming. A significant fraction, , of BH mergers
instead outshines the galaxy in X-rays, and about are sufficiently
bright to be detected with sensitive X-ray instruments. If mergers induce an
Eddington-limited brightening, up to of sources can become observable.
The transient flux change originating from such a brightening is often large,
allowing of mergers to be detected as EM counterparts. A fraction
of mergers is also detectable at radio frequencies. Observable merging
BHs tend to have higher accretion rates and masses and are overmassive at fixed
galaxy mass with respect to the full population. Most EM-observable mergers can
also be GW-detected with LISA, but their sky localisation is generally poorer.
This has to be considered when using EM counterparts to obtain information
about the properties of merging BHs and their environment.Comment: 17 pages, 11 figures, submitted to A&
Population statistics of intermediate mass black holes in dwarf galaxies using the NewHorizon simulation
While it is well established that supermassive black holes (SMBHs) co-evolve
with their host galaxy, it is currently less clear how lower mass black holes,
so-called intermediate mass black holes (IMBHs), evolve within their dwarf
galaxy hosts. In this paper, we present results on the evolution of a large
sample of IMBHs from the NewHorizon simulation. We show that occupation
fractions of IMBHs in dwarf galaxies are at least 50 percent for galaxies with
stellar masses down to 1E6 Msun, but BH growth is very limited in dwarf
galaxies. In NewHorizon, IMBH growth is somewhat more efficient at high
redshift z = 3 but in general IMBH do not grow significantly until their host
galaxy leaves the dwarf regime. As a result, NewHorizon under-predicts observed
AGN luminosity function and AGN fractions. We show that the difficulties of
IMBH to remain attached to the centres of their host galaxies plays an
important role in limiting their mass growth, and that this dynamic evolution
away from galactic centres becomes stronger at lower redshift.Comment: 15 pages, submitted to MNRA
The DESI One-Percent Survey: Modelling the clustering and halo occupation of all four DESI tracers with Uchuu
We present results from a set of high-fidelity simulated lightcones for the
DESI One-Percent Survey, created from the Uchuu simulation. This 8 (Gpc/h)^3
N-body simulation comprises 2.1 trillion particles and provides high-resolution
dark matter (sub)haloes in the framework of the Planck base-LCDM cosmology.
Employing the subhalo abundance matching (SHAM) technique, we populate the
Uchuu (sub)haloes with all four DESI tracers (BGS, LRG, ELG and QSO) to z =
2.1. Our method accounts for redshift evolution as well as the clustering
dependence on luminosity and stellar mass. The two-point clustering statistics
of the DESI One-Percent Survey align reasonably well with our predictions from
Uchuu across scales ranging from 0.1 Mpc/h to 100 Mpc/h. Some discrepancies
arise due to cosmic variance, incompleteness in the massive end of the stellar
mass function, and a simplified galaxy-halo connection model. We find that the
Uchuu BGS and LRG samples are adequately described using the standard
5-parameter halo occupation distribution model, while the ELGs and QSOs show
agreement with an adopted Gaussian distribution for central halos with a power
law for satellites. We observe a fair agreement in the large-scale bias
measurements between data and mock samples, although the data exhibits smaller
bias values, likely due to cosmic variance. The bias dependence on absolute
magnitude, stellar mass and redshift aligns with that of previous surveys.
These results improve simulated lightcone construction from cosmological models
and enhance our understanding of the galaxy-halo connection, with pivotal
insights from the first DESI data for the success of the final survey.Comment: 23 pages, 15 figures, 5 tables, submitted to MNRAS. The Uchuu-DESI
lightcones will be available at https://data.desi.lbl.go
The Uchuu-SDSS galaxy lightcones: a clustering, RSD and BAO study
We present the data release of the Uchuu-SDSS galaxies: a set of 32 high-fidelity galaxy lightcones constructed from the large Uchuu 2.1 trillion particle -body simulation using Planck cosmology. We adopt subhalo abundance matching to populate the Uchuu-box halo catalogues with SDSS galaxy luminosities. These cubic box galaxy catalogues generated at several redshifts are combined to create the set of lightcones with redshift-evolving galaxy properties. The Uchuu-SDSS galaxy lightcones are built to reproduce the footprint and statistical properties of the SDSS main galaxy survey, along with stellar masses and star formation rates. This facilitates direct comparison of the observed SDSS and simulated Uchuu-SDSS data. Our lightcones reproduce a large number of observational results, such as the distribution of galaxy properties, the galaxy clustering, the stellar mass functions, and the halo occupation distributions. Using the simulated and real data we select samples of bright red galaxies at to explore Redshift Space Distortions and Baryon Acoustic Oscillations (BAO) utilizing a full-shape analytical model of the two-point correlation function. We create a set of 5100 galaxy lightcones using GLAM N-body simulations to compute covariance errors. We report a precision increase on , due to our better estimate of the covariance matrix. From our BAO-inferred and parameters, we obtain the first SDSS measurements of the Hubble and angular diameter distances , . Overall, we conclude that the Planck LCDM cosmology nicely explains the observed large-scale structure statistics of SDSS. All data sets are made publicly available
Hydrogenation, Hydrogenolysis, and Desulfurization of Thiophenes by Soluble Metal Complexes: Recent Achievements and Future Directions
Structural basis for tRNA modification by Elp3 from Dehalococcoides mccartyi
International audienceDuring translation elongation, decoding is based on the recognition of codons by corresponding tRNA anticodon triplets. Molecular mechanisms that regulate global protein synthesis via specific base modifications in tRNA anticodons are receiving increasing attention. The conserved eukaryotic Elongator complex specifically modifies uridines located in the wobble base position of tRNAs. Mutations in Elongator subunits are associated with certain neurodegenerative diseases and cancer. Here we present the crystal structure of D. mccartyi Elp3 (DmcElp3) at 2.15-Å resolution. Our results reveal an unexpected arrangement of Elp3 lysine acetyltransferase (KAT) and radical S-adenosyl methionine (SAM) domains, which share a large interface and form a composite active site and tRNA-binding pocket, with an iron–sulfur cluster located in the dimerization interface of two DmcElp3 molecules. Structure-guided mutagenesis studies of yeast Elp3 confirmed the relevance of our findings for eukaryotic Elp3s and should aid in understanding the cellular functions and pathophysiological roles of Elongator