211 research outputs found

    Stacked phase-space density of galaxies around massive clusters: Comparison of dynamical and lensing masses

    Full text link
    We present a measurement of average histograms of line-of-sight velocities over pairs of galaxies and galaxy clusters. Since the histogram can be measured at different galaxy-cluster separations, this observable is commonly referred to as the stacked phase-space density. We formulate the stacked phase-space density based on a halo-model approach so that the model can be applied to real samples of galaxies and clusters. We examine our model by using an actual sample of massive clusters with known weak-lensing masses and spectroscopic observations of galaxies around the clusters. A likelihood analysis with our model enables us to infer the spherical-symmetric velocity dispersion of observed galaxies in massive clusters. We find the velocity dispersion of galaxies surrounding clusters with their lensing masses of 1.1Γ—1015 hβˆ’1MβŠ™1.1\times10^{15}\, h^{-1}M_{\odot} to be 1180βˆ’70+83 km/s1180^{+83}_{-70}\, \mathrm{km/s} at the 68\% confidence level. Our constraint confirms that the relation between the galaxy velocity dispersion and the host cluster mass in our sample is consistent with the prediction in dark-matter-only N-body simulations under General Relativity. Assuming that the Poisson equation in clusters can be altered by an effective gravitational constant of GeffG_\mathrm{eff}, our measurement of the velocity dispersion can place a tight constraint of 0.88<Geff/GN<1.29 (68%)0.88 < G_\mathrm{eff}/G_\mathrm{N} < 1.29\, (68\%) at length scales of a few Mpc about 2.52.5 Giga years ago, where GNG_\mathrm{N} is the Newton's constant.Comment: 22 pages, 8 figures, 3 tables. Accepted for publication in MNRA

    LoCuSS: Exploring the selection of faint blue background galaxies for cluster weak-lensing

    Get PDF
    Cosmological constraints from galaxy clusters rely on accurate measurements of the mass and internal structure of clusters. An important source of systematic uncertainty in cluster mass and structure measurements is the secure selection of background galaxies that are gravitationally lensed by clusters. This issue has been shown to be particular severe for faint blue galaxies. We therefore explore the selection of faint blue background galaxies, by reference to photometric redshift catalogs derived from the COSMOS survey and our own observations of massive galaxy clusters at z~0.2. We show that methods relying on photometric redshifts of galaxies in/behind clusters based on observations through five filters, and on deep 30-band COSMOS photometric redshifts are both inadequate to identify safely faint blue background galaxies. This is due to the small number of filters used by the former, and absence of massive galaxy clusters at redshifts of interest in the latter. We therefore develop a pragmatic method to combine both sets of photometric redshifts to select a population of blue galaxies based purely on photometric analysis. This sample yields stacked weak-lensing results consistent with our previously published results based on red galaxies. We also show that the stacked clustercentric number density profile of these faint blue galaxies is consistent with expectations from consideration of the lens magnification signal of the clusters. Indeed, the observed number density of blue background galaxies changes by ~10-30 per cent across the radial range over which other surveys assume it to be flat.Comment: submitted to MNRA

    PhoSim-NIRCam: Photon-by-photon image simulations of the James Webb Space Telescope's Near-Infrared Camera

    Full text link
    Recent instrumentation projects have allocated resources to develop codes for simulating astronomical images. Novel physics-based models are essential for understanding telescope, instrument, and environmental systematics in observations. A deep understanding of these systematics is especially important in the context of weak gravitational lensing, galaxy morphology, and other sensitive measurements. In this work, we present an adaptation of a physics-based ab initio image simulator: The Photon Simulator (PhoSim). We modify PhoSim for use with the Near-Infrared Camera (NIRCam) -- the primary imaging instrument aboard the James Webb Space Telescope (JWST). This photon Monte Carlo code replicates the observational catalog, telescope and camera optics, detector physics, and readout modes/electronics. Importantly, PhoSim-NIRCam simulates both geometric aberration and diffraction across the field of view. Full field- and wavelength-dependent point spread functions are presented. Simulated images of an extragalactic field are presented. Extensive validation is planned during in-orbit commissioning

    A high signal to noise ratio map of the Sunyaev-Zel'dovich increment at 1.1 mm wavelength in Abell 1835

    Full text link
    We present an analysis of an 8 arcminute diameter map of the area around the galaxy cluster Abell 1835 from jiggle map observations at a wavelength of 1.1 mm using the Bolometric Camera (Bolocam) mounted on the Caltech Submillimeter Observatory (CSO). The data is well described by a model including an extended Sunyaev-Zel'dovich (SZ) signal from the cluster gas plus emission from two bright background submm galaxies magnified by the gravitational lensing of the cluster. The best-fit values for the central Compton value for the cluster and the fluxes of the two main point sources in the field: SMM J140104+0252, and SMM J14009+0252 are found to be y0=(4.34Β±0.52Β±0.69)Γ—10βˆ’4y_{0}=(4.34\pm0.52\pm0.69)\times10^{-4}, 6.5Β±2.0Β±0.7\pm{2.0}\pm0.7 mJy and 11.3Β±1.9Β±1.1\pm{1.9}\pm1.1 mJy, where the first error represents the statistical measurement error and the second error represents the estimated systematic error in the result. This measurement assumes the presence of dust emission from the cluster's central cD galaxy of 1.8Β±0.51.8\pm0.5 mJy, based on higher frequency observations of Abell 1835. The cluster image represents one of the highest-significance SZ detections of a cluster in the positive region of the thermal SZ spectrum to date. The inferred central intensity is compared to other SZ measurements of Abell 1835 and this collection of results is used to obtain values for y0=(3.60Β±0.24)Γ—10βˆ’4y_{0} = (3.60\pm0.24)\times10^{-4} and the cluster peculiar velocity vz=βˆ’226Β±275v_{z} = -226\pm275 km/s.Comment: 9 pages, 5 figure

    LoCuSS: The Near-Infrared Luminosity and Weak-Lensing Mass Scaling Relation of Galaxy Clusters

    Full text link
    We present the first scaling relation between weak-lensing galaxy cluster mass, MWLM_{WL}, and near-infrared luminosity, LKL_K. Our results are based on 17 clusters observed with wide-field instruments on Subaru, the United Kingdom Infrared Telescope, the Mayall Telescope, and the MMT. We concentrate on the relation between projected 2D weak-lensing mass and spectroscopically confirmed luminosity within 1Mpc, modelled as MWL∝LKbM_{WL} \propto L_{K}^b, obtaining a power law slope of b=0.83βˆ’0.24+0.27b=0.83^{+0.27}_{-0.24} and an intrinsic scatter of ΟƒlnMWL∣LK=10βˆ’5+8%\sigma_{lnM_{WL}|L_{K}}=10^{+8}_{-5}\%. Intrinsic scatter of ~10% is a consistent feature of our results regardless of how we modify our approach to measuring the relationship between mass and light. For example, deprojecting the mass and measuring both quantities within r500r_{500}, that is itself obtained from the lensing analysis, yields ΟƒlnMWL∣LK=10βˆ’5+7%\sigma_{lnM_{WL}|L_{K}}=10^{+7}_{-5}\% and b=0.97βˆ’0.17+0.17b=0.97^{+0.17}_{-0.17}. We also find that selecting members based on their (J-K) colours instead of spectroscopic redshifts neither increases the scatter nor modifies the slope. Overall our results indicate that near-infrared luminosity measured on scales comparable with r500r_{500} (typically 1Mpc for our sample) is a low scatter and relatively inexpensive proxy for weak-lensing mass. Near-infrared luminosity may therefore be a useful mass proxy for cluster cosmology experiments.Comment: 9 Pages, 5 Figures, 3 Tables. Submitted to MNRA
    • …
    corecore