93 research outputs found
On the Assembly Bias of Cool Core Clusters Traced by H Nebulae
Do cool-core (CC) and noncool-core (NCC) clusters live in different
environments? We make novel use of H emission lines in the central
galaxies of redMaPPer clusters as proxies to construct large (1,000's) samples
of CC and NCC clusters, and measure their relative assembly bias using both
clustering and weak lensing. We increase the statistical significance of the
bias measurements from clustering by cross-correlating the clusters with an
external galaxy redshift catalog from the Sloan Digital Sky Survey III, the
LOWZ sample. Our cross-correlations can constrain assembly bias up to a
statistical uncertainty of 6%. Given our H criteria for CC and NCC, we
find no significant differences in their clustering amplitude. Interpreting
this difference as the absence of halo assembly bias, our results rule out the
possibility of having different large-scale (tens of Mpc) environments as the
source of diversity observed in cluster cores. Combined with recent
observations of the overall mild evolution of CC and NCC properties, such as
central density and CC fraction, this would suggest that either the cooling
properties of the cluster core are determined early on solely by the local
(<200 kpc) gas properties at formation or that local merging leads to
stochastic CC relaxation and disruption in a periodic way, preserving the
average population properties over time. Studying the small-scale clustering in
clusters at high redshift would help shed light on the exact scenario.Comment: 17 pages, 9 figures, 2 tables, to be submitted to ApJ; comments
welcom
Discovery of a new fundamental plane dictating galaxy cluster evolution from gravitational lensing
In cold dark matter (CDM) cosmology, objects in the Universe have grown under
the effect of gravity of dark matter. The intracluster gas in a galaxy cluster
was heated when the dark-matter halo formed through gravitational collapse. The
potential energy of the gas was converted to thermal energy through this
process. However, this process and the thermodynamic history of the gas have
not been clearly characterized in connection with with the formation and
evolution of the internal structure of dark-matter halos. Here, we show that
observational CLASH data of high-mass galaxy clusters lie on a plane in the
three-dimensional logarithmic space of their characteristic radius , mass
, and X-ray temperature with a very small orthogonal scatter. The
tight correlation indicates that the gas temperature was determined at a
specific cluster formation time, which is encoded in and . The plane
is tilted with respect to , which is the plane expected in
case of simplified virial equilibrium. We show that this tilt can be explained
by a similarity solution, which indicates that clusters are not isolated but
continuously growing through matter accretion from their outer environments.
Numerical simulations reproduce the observed plane and its angle. This result
holds independently of the gas physics implemented in the code, revealing the
fundamental origin of this plane.Comment: Replaced with a revised version to match the ApJ accepted versio
Halo Concentrations and the Fundamental Plane of Galaxy Clusters
According to the standard cold dark matter (CDM) cosmology, the structure of
dark halos including those of galaxy clusters reflects their mass accretion
history. Older clusters tend to be more concentrated than younger clusters.
Their structure, represented by the characteristic radius and mass
of the Navarro--Frenk--White (NFW) density profile, is related to their
formation time. In~this study, we showed that , , and the X-ray
temperature of the intracluster medium (ICM), , form a thin plane in the
space of . This tight correlation indicates
that the ICM temperature is also determined by the formation time of individual
clusters. Numerical simulations showed that clusters move along the fundamental
plane as they evolve. The plane and the cluster evolution within the plane
could be explained by a similarity solution of structure formation of the
universe. The angle of the plane shows that clusters have not achieved "virial
equilibrium" in the sense that mass/size growth and pressure at the boundaries
cannot be ignored. The distribution of clusters on the plane was related to the
intrinsic scatter in the halo concentration--mass relation, which originated
from the variety of cluster ages. The well-known mass--temperature relation of
clusters () can be explained by the fundamental
plane and the mass dependence of the halo concentration without the assumption
of virial equilibrium. The fundamental plane could also be used for calibration
of cluster masses.Comment: Invited review article, to be published in "From Dark Haloes to
Visible Galaxies", special issue of Galaxie
Three-dimensional Multi-probe Analysis of the Galaxy Cluster A1689
We perform a 3D multi-probe analysis of the rich galaxy cluster A1689 by
combining improved weak-lensing data from new BVRi'z' Subaru/Suprime-Cam
observations with strong-lensing, X-ray, and Sunyaev-Zel'dovich effect (SZE)
data sets. We reconstruct the projected matter distribution from a joint
weak-lensing analysis of 2D shear and azimuthally integrated magnification
constraints, the combination of which allows us to break the mass-sheet
degeneracy. The resulting mass distribution reveals elongation with axis ratio
~0.7 in projection. When assuming a spherical halo, our full weak-lensing
analysis yields a projected concentration of
(), consistent with and improved from earlier weak-lensing
work. We find excellent consistency between weak and strong lensing in the
region of overlap. In a parametric triaxial framework, we constrain the
intrinsic structure and geometry of the matter and gas distributions, by
combining weak/strong lensing and X-ray/SZE data with minimal geometric
assumptions. We show that the data favor a triaxial geometry with minor-major
axis ratio 0.39+/-0.15 and major axis closely aligned with the line of sight
(22+/-10 deg). We obtain and
, which overlaps with the tail of the predicted
distribution. The shape of the gas is rounder than the underlying matter but
quite elongated with minor-major axis ratio 0.60+/-0.14. The gas mass fraction
within 0.9Mpc is 10^{+3}_{-2}%. The thermal gas pressure contributes to ~60% of
the equilibrium pressure, indicating a significant level of non-thermal
pressure support. When compared to Planck's hydrostatic mass estimate, our
lensing measurements yield a spherical mass ratio of and with and without corrections for lensing projection
effects, respectively.Comment: Accepted by ApJ. Minor textual changes to improve clarity (e.g., 5.
HST STRONG-LENSING ANALYSIS). 26 pages, 17 figures. A version with
high-resolution figures is available at
http://www.asiaa.sinica.edu.tw/~keiichi/upfiles/Umetsu15/umetsu15.pd
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Weak-lensing Mass Calibration of ACTPol Sunyaev–Zel’dovich Clusters with the Hyper Suprime-Cam Survey
We present weak-lensing measurements using the first-year data from the Hyper Suprime-Cam Strategic Survey Program on the Subaru telescope for eight galaxy clusters selected through their thermal Sunyaev–Zel'dovich (SZ) signal measured at 148 GHz with the Atacama Cosmology Telescope Polarimeter experiment. The overlap between the two surveys in this work is 33.8 square degrees, before masking bright stars. The signal-to-noise ratio of individual cluster lensing measurements ranges from 2.2 to 8.7, with a total of 11.1 for the stacked cluster weak-lensing signal. We fit for an average weak-lensing mass distribution using three different profiles, a Navarro–Frenk–White profile, a dark-matter-only emulated profile, and a full cosmological hydrodynamic emulated profile. We interpret the differences among the masses inferred by these models as a systematic error of 10%, which is currently smaller than the statistical error. We obtain the ratio of the SZ-estimated mass to the lensing-estimated mass (the so-called hydrostatic mass bias 1−b) of , which is comparable to previous SZ-selected clusters from the Atacama Cosmology Telescope and from the Planck Satellite. We conclude with a discussion of the implications for cosmological parameters inferred from cluster abundances compared to cosmic microwave background primary anisotropy measurements.U.S. National Science Foundation [AST-1440226, AST-0965625, AST-0408698, PHY-1214379, PHY-0855887]; Princeton University; University of Pennsylvania; Canada Foundation for Innovation (CFI) award; Comision Nacional de Investigacion Cientifica y Tecnologica de Chile (CONICYT); CFI under Compute Canada; Government of Ontario; Ontario Research Fund Research Excellence; University of Toronto; NASA [NNX13AE56G, NNX14AB58G]; FIRST program from Japanese Cabinet Office; Ministry of Education, Culture, Sports, Science and Technology (MEXT); Japan Society for the Promotion of Science (JSPS); Japan Science and Technology Agency (JST); Toray Science Foundation; NAOJ; Kavli IPMU; KEK; ASIAA; National Aeronautics and Space Administration [NNX08AR22G]; National Science Foundation [AST-1238877]; Jet Propulsion Laboratory, California Institute of Technology; National Aeronautics and Space Administration; Japan Society for the Promotion of Science (JSPS) KAKENHI [JP17H06600, JP18H04350]; Simons Foundation; JSPS KAKENHI [JP16H01089]; STFC Ernest Rutherford Fellowship [ST/M004856/2]; National Research Foundation of South Africa [93565]; CONICYT FONDECYT grant [3170846]; JSPS KAKENHI grant [JP17K14273, JP15H03654, JP15H05893, JP15K21733, JP15H05892]; Japan Science and Technology Agency (JST) CREST [JPMJCR1414]; Ministry of Science and Technology of Taiwan [MOST 103-2628-M-001-003-MY3]; Academia Sinica Investigator Award; Vincent and Beatrice Tremaine Fellowship; [Anillo ACT-1417]; [QUIMAL-160009]This item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at [email protected]
Comparison of Cluster Lensing Profiles with Lambda CDM Predictions
We derive lens distortion and magnification profiles of four well known
clusters observed with Subaru. Each cluster is very well fitted by the general
form predicted for Cold Dark Matter (CDM) dominated halos, with good
consistency found between the independent distortion and magnification
measurements. The inferred level of mass concentration is surprisingly high,
8 = 10.4 \pm 0.9), compared to the relatively shallow
profiles predicted by the Lambda CDM model, c_{vir}=5.1 \pm 1.1 (for
=1.25\times 10^{15}M_{\odot}/h). This represents a 4sigma discrepancy, and
includes the relatively modest effects of projection bias and profile evolution
derived from N-body simulations, which oppose each other with little residual
effect. In the context of CDM based cosmologies, this discrepancy implies
clusters collapse earlier (z\geq 1) than predicted (z<0.5), when the Universe
was correspondingly denser.Comment: Accepted version in ApJL, minor change
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