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  • 1
    In: Astronomy & Astrophysics, EDP Sciences, Vol. 661 ( 2022-5), p. A46-
    Abstract: Context. Galaxy clusters grow through mergers and the accretion of substructures along large-scale filaments. Many of the missing baryons in the local Universe may reside in such filaments as the warm-hot intergalactic medium (WHIM). Aims. SRG/eROSITA performance verification observations revealed that the binary cluster Abell 3391/3395 and the Northern Clump (the MCXC J0621.7–5242 galaxy cluster) are aligning along a cosmic filament in soft X-rays, similarly to what has been seen in simulations before. We aim to understand the dynamical state of the Northern Clump as it enters the atmosphere (3 × R 200 ) of Abell 3391. Methods. We analyzed joint eROSITA, XMM-Newton , and Chandra observations to probe the morphological, thermal, and chemical properties of the Northern Clump from its center out to a radius of 988 kpc ( R 200 ). We utilized the ASKAP/EMU radio data, the DECam optical image, and the Planck y -map to study the influence of the wide-angle tail (WAT) radio source on the Northern Clump’s central intracluster medium. Using eROSITA data, we also analyzed the gas properties of the Northern Filament, the region between the virial radii of the Northern Clump and the A3391 cluster. From the Magneticum simulation, we identified an analog of the A3391/95 system along with an infalling group resembling the Northern Clump. Results. The Northern Clump is a weak cool-core cluster centered on a WAT radio galaxy. The gas temperature over 0.2–0.5 R 500 is k B T 500 = 1.99 ± 0.04 keV. We employed the mass-temperature (M – T ) scaling relation and obtained a mass estimate of M 500 = (7.68 ± 0.43) × 10 13 M ⊙ and R 500 = (63 6 ± 12) kpc. Its X-ray atmosphere has a boxy shape and deviates from spherical symmetry. We identify a southern surface brightness edge, likely caused by subsonic motion relative to the filament gas in the southern direction. At ~ R 500 , the southern atmosphere (infalling head) appears to be 42% hotter than its northern atmosphere. We detect a downstream tail pointing toward the north with a projected length of ~318 kpc, plausibly the result of ram pressure stripping. Through a two-temperature fit, we identify a cooler component in the Northern Filament with k B T = 0.68 - 0.64 + 0.38 keV and n e = 1.99 -1.24 +0.88 × 10 -5 cm -3 , which are consistent within the expected ranges of WHIM properties. The analog group in the Magneticum simulation is experiencing changes in its gas properties and a shift between the position of the halo center and that of the bound gas, while approaching the main cluster pair. Conclusions. The Northern Clump is a dynamically active system and far from being relaxed. Its atmosphere is affected by an interaction with the WAT and by gas sloshing or its infall toward Abell 3391 along the filament, consistent with the analog group-size halo in the Magneticum simulation.
    Type of Medium: Online Resource
    ISSN: 0004-6361 , 1432-0746
    RVK:
    RVK:
    Language: English
    Publisher: EDP Sciences
    Publication Date: 2022
    detail.hit.zdb_id: 1458466-9
    SSG: 16,12
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  • 2
    In: Astronomy & Astrophysics, EDP Sciences, Vol. 667 ( 2022-11), p. A125-
    Abstract: We demonstrate how to use persistent homology for cosmological parameter inference in a tomographic cosmic shear survey. We obtain the first cosmological parameter constraints from persistent homology by applying our method to the first-year data of the Dark Energy Survey. To obtain these constraints, we analyse the topological structure of the matter distribution by extracting persistence diagrams from signal-to-noise maps of aperture masses. This presents a natural extension to the widely used peak count statistics. Extracting the persistence diagrams from the cosmo-SLICS, a suite of N -body simulations with variable cosmological parameters, we interpolate the signal using Gaussian processes and marginalise over the most relevant systematic effects, including intrinsic alignments and baryonic effects. For the structure growth parameter, we find S 8  = 0.747 −0.031 +0.025 , which is in full agreement with other late-time probes. We also constrain the intrinsic alignment parameter to A  = 1.54 ± 0.52, which constitutes a detection of the intrinsic alignment effect at almost 3 σ .
    Type of Medium: Online Resource
    ISSN: 0004-6361 , 1432-0746
    RVK:
    RVK:
    Language: English
    Publisher: EDP Sciences
    Publication Date: 2022
    detail.hit.zdb_id: 1458466-9
    SSG: 16,12
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  • 3
    Online Resource
    Online Resource
    EDP Sciences ; 2023
    In:  Astronomy & Astrophysics Vol. 670 ( 2023-02), p. A33-
    In: Astronomy & Astrophysics, EDP Sciences, Vol. 670 ( 2023-02), p. A33-
    Abstract: Context. To assume hydrostatic equilibrium between the intracluster medium and the gravitational potential of galaxy clusters is an extensively used method to investigate their total masses. Aims. We want to test hydrostatic masses obtained with an observational code in the context of the Spectrum-Roentgen-Gamma/eROSITA survey. Methods. We used the hydrostatic modeling code MBProj2 to fit surface-brightness profiles to simulated clusters with idealized properties as well as to a sample of 93 clusters taken from the Magneticum Pathfinder simulations. We investigated the latter under the assumption of idealized observational conditions and also for realistic eROSITA data quality. The comparison of the fitted cumulative total mass profiles and the true mass profiles provided by the simulations allows us to gain knowledge both about the validity of hydrostatic equilibrium in each cluster and the reliability of our approach. Furthermore, we used the true profiles for gas density and pressure to compute hydrostatic mass profiles based on theory for every cluster. Results. For an idealized cluster that was simulated to fulfill perfect hydrostatic equilibrium, we find that the cumulative total mass at the true r 500 and r 200 can be reproduced with deviations of less than 7%. For the clusters from the Magneticum Pathfinder simulations under idealized observational conditions, the median values of the fitted cumulative total masses at the true r 500 and r 200 are in agreement with our expectations, taking into account the hydrostatic mass bias. Nevertheless, we find a tendency towards steeper cumulative total mass profiles in the outskirts than expected. For realistic eROSITA data quality, this steepness problem intensifies for clusters with high redshifts and leads to excessive cumulative total masses at r 200 . For the hydrostatic masses based on the true profiles known from the simulations, we find good agreement with our expectations concerning the hydrostatic mass.
    Type of Medium: Online Resource
    ISSN: 0004-6361 , 1432-0746
    RVK:
    RVK:
    Language: English
    Publisher: EDP Sciences
    Publication Date: 2023
    detail.hit.zdb_id: 1458466-9
    SSG: 16,12
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  • 4
    Online Resource
    Online Resource
    World Scientific Pub Co Pte Ltd ; 2004
    In:  Modern Physics Letters A Vol. 19, No. 13n16 ( 2004-05-30), p. 1083-1087
    In: Modern Physics Letters A, World Scientific Pub Co Pte Ltd, Vol. 19, No. 13n16 ( 2004-05-30), p. 1083-1087
    Abstract: We perform a set of ray-tracing simulations, using numerical cluster models, aiming at evaluating how the galaxy cluster efficiency for producing strong lensing events changes in different cosmological models with dark energy. The sample of investigated clusters for which we present our results here is composed by 7 dark matter halos. Each of them was simulated in 8 different cosmological models with constant and time-variable equation of state of dark energy. For all the clusters in the sample, we have measured the lensing cross sections for producing giant arcs, i.e. arcs having a minimum length-to-width ratio. We find that the lensing cross section for giant arcs is sensitive to the equation of state of quintessence. Indeed, the optical depth, which can be translated into a number of arcs by multiplying by the correct density of source galaxy on the sky, spans more than one order of magnitude among different cosmological models.
    Type of Medium: Online Resource
    ISSN: 0217-7323 , 1793-6632
    Language: English
    Publisher: World Scientific Pub Co Pte Ltd
    Publication Date: 2004
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  • 5
    Online Resource
    Online Resource
    World Scientific Pub Co Pte Ltd ; 2004
    In:  Modern Physics Letters A Vol. 19, No. 13n16 ( 2004-05-30), p. 1079-1082
    In: Modern Physics Letters A, World Scientific Pub Co Pte Ltd, Vol. 19, No. 13n16 ( 2004-05-30), p. 1079-1082
    Abstract: We study the concentration parameters, their mass dependence and redshift evolution, of dark-matter halos in different dark-energy cosmologies with constant and time-variable equation of state, and compare them with "standard" ΛCDM and OCDM models. The dependence of averaged halo concentrations on mass and redshift permits a simple fit of the form (1+z)c=c 0 (M/M 0 ) α , with α≈-0.1 throughout. We find that the cluster concentration depends on the dark energy equation of state at the cluster formation redshift z coll through the linear growth factor D + (z coll ). As a simple correction accounting for dark-energy cosmologies, we propose scaling c 0 from ΛCDM with the ratio of linear growth factors, c 0 →c 0 D + (z coll )/D + , ΛCDM (z coll ).
    Type of Medium: Online Resource
    ISSN: 0217-7323 , 1793-6632
    Language: English
    Publisher: World Scientific Pub Co Pte Ltd
    Publication Date: 2004
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  • 6
    In: Astronomy & Astrophysics, EDP Sciences, Vol. 665 ( 2022-09), p. A16-
    Abstract: Context. Recent observations found that observed cluster member galaxies are more compact than their counterparts in ΛCDM hydrodynamic simulations, as indicated by the difference in their strong gravitational lensing properties, and they reported that measured and simulated galaxy–galaxy strong lensing events on small scales are discrepant by one order of magnitude. Among the possible explanations for this discrepancy, some studies suggest that simulations with better resolution and implementing different schemes for galaxy formation could produce simulations that are in better agreement with the observations. Aims. In this work, we aim to assess the impact of numerical resolution and of the implementation of energy input from AGN feedback models on the inner structure of cluster sub-haloes in hydrodynamic simulations. Methods. We compared several zoom-in re-simulations of a sub-sample of cluster-sized haloes obtained by varying mass resolution and softening the length and AGN energy feedback scheme. We studied the impact of these different setups on the sub-halo (SH) abundances, their radial distribution, their density and mass profiles, and the relation between the maximum circular velocity, which is a proxy for SH compactness Results. Regardless of the adopted numerical resolution and feedback model, SHs with masses of M SH  ≲ 10 11   h −1   M ⊙ , the most relevant mass range for galaxy–galaxy strong lensing, have maximum circular velocities ∼30% smaller than those measured from strong lensing observations. We also find that simulations with less effective AGN energy feedback produce massive SHs ( M SH  ≳ 10 11   h −1   M ⊙ ) with higher maximum circular velocity and that their V max  −  M SH relation approaches the observed one. However, the stellar-mass number count of these objects exceeds the one found in observations, and we find that the compactness of these simulated SHs is the result of an extremely over-efficient star formation in their cores, also leading to larger than observed SH stellar mass. Conclusions. Regardless of the resolution and galaxy formation model adopted, simulations are unable to simultaneously reproduce the observed stellar masses and compactness (or maximum circular velocities) of cluster galaxies. Thus, the discrepancy between theory and observations that emerged previous works. It remains an open question as to whether such a discrepancy reflects limitations of the current implementation of galaxy formation models or the ΛCDM paradigm.
    Type of Medium: Online Resource
    ISSN: 0004-6361 , 1432-0746
    RVK:
    RVK:
    Language: English
    Publisher: EDP Sciences
    Publication Date: 2022
    detail.hit.zdb_id: 1458466-9
    SSG: 16,12
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  • 7
    In: Frontiers in Astronomy and Space Sciences, Frontiers Media SA, Vol. 6 ( 2019-6-4)
    Type of Medium: Online Resource
    ISSN: 2296-987X
    Language: Unknown
    Publisher: Frontiers Media SA
    Publication Date: 2019
    detail.hit.zdb_id: 2778829-5
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  • 8
    Online Resource
    Online Resource
    MDPI AG ; 2017
    In:  Galaxies Vol. 5, No. 3 ( 2017-09-01), p. 49-
    In: Galaxies, MDPI AG, Vol. 5, No. 3 ( 2017-09-01), p. 49-
    Type of Medium: Online Resource
    ISSN: 2075-4434
    Language: English
    Publisher: MDPI AG
    Publication Date: 2017
    detail.hit.zdb_id: 2691049-4
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  • 9
    Online Resource
    Online Resource
    American Astronomical Society ; 2012
    In:  The Astrophysical Journal Vol. 749, No. 2 ( 2012-04-20), p. L34-
    In: The Astrophysical Journal, American Astronomical Society, Vol. 749, No. 2 ( 2012-04-20), p. L34-
    Type of Medium: Online Resource
    ISSN: 2041-8205 , 2041-8213
    Language: Unknown
    Publisher: American Astronomical Society
    Publication Date: 2012
    detail.hit.zdb_id: 2207648-7
    detail.hit.zdb_id: 2006858-X
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  • 10
    Online Resource
    Online Resource
    Oxford University Press (OUP) ; 2019
    In:  Monthly Notices of the Royal Astronomical Society Vol. 488, No. 4 ( 2019-10-01), p. 5370-5389
    In: Monthly Notices of the Royal Astronomical Society, Oxford University Press (OUP), Vol. 488, No. 4 ( 2019-10-01), p. 5370-5389
    Abstract: The effect of galactic orbits on a galaxy’s internal evolution within a galaxy cluster environment has been the focus of heated debate in recent years. To understand this connection, we use both the $(0.5 \,$Gpc)3 and the Gpc3 boxes from the cosmological hydrodynamical simulation set Magneticum Pathfinder. We investigate the velocity anisotropy, phase space, and the orbital evolution of up to ∼5 × 105 resolved satellite galaxies within our sample of 6776 clusters with $M_{\mathrm{vir}}\,\, \gt\,\, 10^{14} \, \mathrm{M_{\odot }}$ at low redshift, which we also trace back in time. In agreement with observations, we find that star-forming satellite galaxies inside galaxy clusters are characterized by more radially dominated orbits, independent of cluster mass. Furthermore, the vast majority of star-forming satellite galaxies stop forming stars during their first passage. We find a strong dichotomy both in line-of-sight and radial phase space between star-forming and quiescent galaxies, in line with observations. The tracking of individual orbits shows that the star formation of almost all satellite galaxies drops to zero within $1 \, \mathrm{Gyr}$ after infall. Satellite galaxies that are able to remain star forming longer are characterized by tangential orbits and high stellar mass. All this indicates that in galaxy clusters the dominant quenching mechanism is ram-pressure stripping.
    Type of Medium: Online Resource
    ISSN: 0035-8711 , 1365-2966
    Language: English
    Publisher: Oxford University Press (OUP)
    Publication Date: 2019
    detail.hit.zdb_id: 2016084-7
    SSG: 16,12
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