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Featured researches published by J. J. Mohr.


The Astrophysical Journal | 2011

A measurement of the damping tail of the cosmic microwave background power spectrum with the South Pole Telescope

R. Keisler; C. L. Reichardt; K. A. Aird; B. A. Benson; L. E. Bleem; J. E. Carlstrom; C. L. Chang; H. M. Cho; T. M. Crawford; A. T. Crites; T. de Haan; M. Dobbs; J. P. Dudley; E. M. George; N. W. Halverson; G. P. Holder; W. L. Holzapfel; S. Hoover; Z. Hou; J. D. Hrubes; M. Joy; L. Knox; A. T. Lee; E. M. Leitch; M. Lueker; D. Luong-Van; J. J. McMahon; J. Mehl; S. S. Meyer; M. Millea

We present a measurement of the angular power spectrum of the cosmic microwave background (CMB) using data from the South Pole Telescope (SPT). The data consist of 790 square degrees of sky observed at 150 GHz during 2008 and 2009. Here we present the power spectrum over the multipole range 650 < ‘ < 3000, where it is dominated by primary CMB anisotropy. We combine this power spectrum with the power spectra from the seven-year Wilkinson Microwave Anisotropy Probe (WMAP) data release to constrain cosmological models. We nd that the SPT and WMAP data are consistent with each other and, when combined, are well t by a spatially at, CDM cosmological model. The SPT+WMAP constraint on the spectral index of scalar uctuations is ns = 0:9663 0:0112. We detect, at 5 signicance, the eect of gravitational lensing on the CMB power spectrum, and nd its amplitude to be consistent with the CDM cosmological model. We explore a number of extensions beyond the CDM model. Each extension is tested independently, although there are degeneracies between some of the extension parameters. We constrain the tensorto-scalar ratio to be r < 0:21 (95% CL) and constrain the running of the scalar spectral index to be dns=d lnk = 0:024 0:013. We strongly detect the eects of primordial helium and neutrinos on the CMB; a model without helium is rejected at 7.7 , while a model without neutrinos is rejected at 7.5 . The primordial helium abundance is measured to be Yp = 0:296 0:030, and the eective number of relativistic species is measured to be Ne = 3:85 0:62. The constraints on these models are strengthened when the CMB data are combined with measurements of the Hubble constant and the baryon acoustic oscillation feature. Notable improvements include ns = 0:9668 0:0093, r < 0:17 (95% CL), and Ne = 3:86 0:42. The SPT+WMAP data show a mild preference for low power in the CMB damping tail, and while this preference may be accommodated by models that have a negative spectral running, a high primordial helium abundance, or a high eective number of relativistic species, such models are disfavored by the abundance of low-redshift galaxy clusters. Subject headings: cosmology { cosmology:cosmic microwave background { cosmology: observations { large-scale structure of universe


The Astrophysical Journal | 2015

EIGHT NEW MILKY WAY COMPANIONS DISCOVERED IN FIRST-YEAR DARK ENERGY SURVEY DATA

K. Bechtol; A. Drlica-Wagner; E. Balbinot; A. Pieres; J. D. Simon; Brian Yanny; B. Santiago; Risa H. Wechsler; Joshua A. Frieman; Alistair R. Walker; P. Williams; Eduardo Rozo; Eli S. Rykoff; A. Queiroz; E. Luque; A. Benoit-Lévy; Douglas L. Tucker; I. Sevilla; Robert A. Gruendl; L. N. da Costa; A. Fausti Neto; M. A. G. Maia; T. D. Abbott; S. Allam; R. Armstrong; A. Bauer; G. M. Bernstein; R. A. Bernstein; E. Bertin; David J. Brooks

We report the discovery of eight new Milky Way companions in ~1,800 deg^2 of optical imaging data collected during the first year of the Dark Energy Survey (DES). Each system is identified as a statistically significant over-density of individual stars consistent with the expected isochrone and luminosity function of an old and metal-poor stellar population. The objects span a wide range of absolute magnitudes (M_V from -2.2 mag to -7.4 mag), physical sizes (10 pc to 170 pc), and heliocentric distances (30 kpc to 330 kpc). Based on the low surface brightnesses, large physical sizes, and/or large Galactocentric distances of these objects, several are likely to be new ultra-faint satellite galaxies of the Milky Way and/or Magellanic Clouds. We introduce a likelihood-based algorithm to search for and characterize stellar over-densities, as well as identify stars with high satellite membership probabilities. We also present completeness estimates for detecting ultra-faint galaxies of varying luminosities, sizes, and heliocentric distances in the first-year DES data.


The Astrophysical Journal | 2014

Constraints on cosmology from the cosmic microwave background power spectrum of the 2500 deg2 SPT-SZ survey

Z. Hou; C. L. Reichardt; K. Story; B. Follin; R. Keisler; K. A. Aird; B. A. Benson; L. E. Bleem; J. E. Carlstrom; C. L. Chang; H. M. Cho; T. M. Crawford; A. T. Crites; T. de Haan; R. de Putter; M. Dobbs; Scott Dodelson; J. P. Dudley; E. M. George; N. W. Halverson; G. P. Holder; W. L. Holzapfel; S. Hoover; J. D. Hrubes; M. Joy; L. Knox; A. T. Lee; E. M. Leitch; M. Lueker; D. Luong-Van

We explore extensions to the ΛCDM cosmology using measurements of the cosmic microwave background (CMB) from the recent SPT-SZ survey, along with data from WMAP7 and measurements of H_0 and baryon acoustic oscillation (BAO). We check for consistency within ΛCDM between these data sets, and find some tension. The CMB alone gives weak support to physics beyond ΛCDM, due to a slight trend relative to ΛCDM of decreasing power toward smaller angular scales. While it may be due to statistical fluctuation, this trend could also be explained by several extensions. We consider running of the primordial spectral index (dn_s /d ln k), as well as two extensions that modify the damping tail power (the primordial helium abundance Y_p and the effective number of neutrino species N_(eff)) and one that modifies the large-scale power due to the integrated Sachs-Wolfe effect (the sum of neutrino masses ∑m_ν). These extensions have similar observational consequences and are partially degenerate when considered simultaneously. Of the six one-parameter extensions considered, we find CMB to have the largest preference for dn_s/d ln k with –0.046 0 from CMB+BAO+H_0 + SPT_(CL). The median value is (0.32 ± 0.11) eV, a factor of six above the lower bound set by neutrino oscillation observations. All data sets except H_0 show some preference for massive neutrinos; data combinations including H_0 favor nonzero masses only if BAO data are also included. We also constrain the two-parameter extensions N_(eff) + ∑m_ν and N_(eff) + Y_p to explore constraints on additional light species and big bang nucleosynthesis, respectively.


Nature | 2012

A massive, cooling-flow-induced starburst in the core of a luminous cluster of galaxies

M. McDonald; Matthew B. Bayliss; B. A. Benson; Ryan J. Foley; J. Ruel; Peter W. Sullivan; Sylvain Veilleux; K. A. Aird; M. L. N. Ashby; Marshall W. Bautz; G. Bazin; L. E. Bleem; M. Brodwin; J. E. Carlstrom; C. L. Chang; H. M. Cho; Alejandro Clocchiatti; T. M. Crawford; A. T. Crites; T. de Haan; S. Desai; M. Dobbs; J. P. Dudley; E. Egami; W. Forman; Gordon Garmire; E. M. George; Michael D. Gladders; Anthony H. Gonzalez; N. W. Halverson

In the cores of some clusters of galaxies the hot intracluster plasma is dense enough that it should cool radiatively in the cluster’s lifetime, leading to continuous ‘cooling flows’ of gas sinking towards the cluster centre, yet no such cooling flow has been observed. The low observed star-formation rates and cool gas masses for these ‘cool-core’ clusters suggest that much of the cooling must be offset by feedback to prevent the formation of a runaway cooling flow. Here we report X-ray, optical and infrared observations of the galaxy cluster SPT-CLJ2344-4243 (ref. 11) at redshift z = 0.596. These observations reveal an exceptionally luminous (8.2 × 1045 erg s−1) galaxy cluster that hosts an extremely strong cooling flow (around 3,820 solar masses a year). Further, the central galaxy in this cluster appears to be experiencing a massive starburst (formation of around 740 solar masses a year), which suggests that the feedback source responsible for preventing runaway cooling in nearby cool-core clusters may not yet be fully established in SPT-CLJ2344-4243. This large star-formation rate implies that a significant fraction of the stars in the central galaxy of this cluster may form through accretion of the intracluster medium, rather than (as is currently thought) assembling entirely via mergers.


The Astrophysical Journal | 2010

SPT-CL J0546-5345: A Massive z > 1 Galaxy Cluster Selected Via the Sunyaev-Zel'dovich Effect with the South Pole Telescope

Mark Brodwin; J. Ruel; Peter A. R. Ade; K. A. Aird; K. Andersson; M. L. N. Ashby; Marshall W. Bautz; G. Bazin; B. A. Benson; L. E. Bleem; J. E. Carlstrom; C. L. Chang; T. M. Crawford; A. T. Crites; T. de Haan; S. Desai; M. Dobbs; J. P. Dudley; G. G. Fazio; Ryan J. Foley; W. Forman; Gordon Garmire; E. M. George; Michael D. Gladders; Anthony H. Gonzalez; N. W. Halverson; F. W. High; G. P. Holder; W. L. Holzapfel; J. D. Hrubes

United States. National Aeronautics and Space Administration (Jet Propulsion Laboratory (U.S.))


Monthly Notices of the Royal Astronomical Society | 2016

The DES Science Verification weak lensing shear catalogues

M. Jarvis; E. Sheldon; J. Zuntz; Tomasz Kacprzak; Sarah Bridle; Adam Amara; Robert Armstrong; M. R. Becker; G. M. Bernstein; C. Bonnett; C. L. Chang; Ritanjan Das; J. P. Dietrich; A. Drlica-Wagner; T. F. Eifler; C. Gangkofner; D. Gruen; Michael Hirsch; Eric Huff; Bhuvnesh Jain; S. Kent; D. Kirk; N. MacCrann; P. Melchior; A. A. Plazas; Alexandre Refregier; Barnaby Rowe; E. S. Rykoff; S. Samuroff; C. Sanchez

We present weak lensing shear catalogues for 139 square degrees of data taken during the Science Verification (SV) time for the new Dark Energy Camera (DECam) being used for the Dark Energy Survey (DES). We describe our object selection, point spread function estimation and shear measurement procedures using two independent shear pipelines, IM3SHAPE and NGMIX, which produce catalogues of 2.12 million and 3.44 million galaxies respectively. We detail a set of null tests for the shear measurements and find that they pass the requirements for systematic errors at the level necessary for weak lensing science applications using the SV data. We also discuss some of the planned algorithmic improvements that will be necessary to produce sufficiently accurate shear catalogues for the full 5-year DES, which is expected to cover 5000 square degrees.


Astronomy and Astrophysics | 2011

The X-ray luminous galaxy cluster XMMU J1007.4+1237 at z = 1.56 - the dawn of starburst activity in cluster cores

R. Fassbender; A. Nastasi; H. Böhringer; R. Suhada; J. S. Santos; P. Rosati; D. Pierini; M. Mühlegger; H. Quintana; A. D. Schwope; G. Lamer; A. de Hoon; J. Kohnert; G. W. Pratt; J. J. Mohr

Context. Observational galaxy cluster studies at z > 1.5 probe the formation of the first massive M > 10 14 M ⊙ dark matter halos, the early thermal history of the hot ICM, and the emergence of the red-sequence population of quenched early-type galaxies. Aims. We present first results for the newly discovered X-ray luminous galaxy cluster XMMUJ1007.4+1237 at z = 1.555, detected and confirmed by the XMM-Newton Distant Cluster Project (XDCP) survey. Methods. We selected the system as a serendipitous weak extended X-ray source in XMM-Newton archival data and followed it up with two-band near-infrared imaging and deep optical spectroscopy. Results. We can establish XMMU J 1007.4+1237 as a spectroscopically confirmed, massive, bona fide galaxy cluster with a bolometric X-ray luminosity of L bol X,500 ≃ (2.1 ± 0.4) x 10 44 erg/s, a red galaxy population centered on the X-ray emission, and a central radio-loud brightest cluster galaxy. However, we see evidence for the first time that the massive end of the galaxy population and the cluster red-sequence are not yet fully in place. In particular, we find ongoing starburst activity for the third ranked galaxy close to the center and another slightly fainter object. Conclusions. At a lookback time of 9.4 Gyr, the cluster galaxy population appears to be caught in an important evolutionary phase, prior to full star-formation quenching and mass assembly in the core region. X-ray selection techniques are an efficient means of identifying and probing the most distant clusters without any prior assumptions about their galaxy content.


The Astrophysical Journal | 2013

TOWARD UNBIASED GALAXY CLUSTER MASSES FROM LINE-OF-SIGHT VELOCITY DISPERSIONS

A. Saro; J. J. Mohr; G. Bazin; K. Dolag

We study the use of red-sequence-selected galaxy spectroscopy for unbiased estimation of galaxy cluster masses by using a publicly available simulated galaxy catalog. We explore the impact of selection using galaxy color, projected separation from the cluster center, galaxy luminosity, and spectroscopic redshift. We identify and characterize each of the following sources of bias and scatter in velocity dispersion at fixed mass: the intrinsic properties of halos in the form of halo triaxiality, sampling noise, the presence of multiple kinematic populations within the cluster, and the effect of interlopers. We show that even in red-sequence and spectroscopically selected galaxy samples, the interloper fraction is significant, and that the variations in the interloper population from cluster to cluster provide the dominant contribution to the velocity dispersion scatter at fixed mass. We present measurements of the total scatter in dispersion at fixed mass as a function of the number of redshifts. Results indicate that improvements in scatter are modest beyond samples of ~30 redshifts per cluster. Our results show that while cluster velocity dispersions extracted from a few dozen red-sequence-selected galaxies do not provide precise masses on a single cluster basis, an ensemble of cluster velocity dispersions can be combined to produce a precise calibration of a cluster survey-mass-observable relation. Currently, disagreements in the literature on simulated subhalo velocity dispersion-mass relations place a systematic floor on velocity dispersion mass calibration at the 5% level in dispersion.


The Astrophysical Journal | 2013

A DIRECT MEASUREMENT OF THE LINEAR BIAS OF MID-INFRARED-SELECTED QUASARS AT z ≈ 1 USING COSMIC MICROWAVE BACKGROUND LENSING

J. E. Geach; R. C. Hickox; L. E. Bleem; M. Brodwin; Gilbert P. Holder; K. A. Aird; B. A. Benson; Suman Bhattacharya; J. E. Carlstrom; C. L. Chang; H. M. Cho; T. M. Crawford; A. T. Crites; T. de Haan; M. Dobbs; J. P. Dudley; E. M. George; Kevin N. Hainline; N. W. Halverson; W. L. Holzapfel; S. Hoover; Z. Hou; J. D. Hrubes; R. Keisler; L. Knox; A. T. Lee; E. M. Leitch; M. Lueker; D. Luong-Van; D. P. Marrone

We measure the cross-power spectrum of the projected mass density as traced by the convergence of the cosmic microwave background lensing field from the South Pole Telescope (SPT) and a sample of Type 1 and 2 (unobscured and obscured) quasars at 〈z〉 ~ 1 selected with the Wide-field Infrared Survey Explorer, over 2500 deg^2. The cross-power spectrum is detected at ≈7σ, and we measure a linear bias b = 1.61 ± 0.22, consistent with clustering analyses. Using an independent lensing map, derived from Planck observations, to measure the cross-spectrum, we find excellent agreement with the SPT analysis. The bias of the combined sample of Type 1 and 2 quasars determined in this work is similar to that previously determined for Type 1 quasars alone; we conclude that obscured and unobscured quasars trace the matter field in a similar way. This result has implications for our understanding of quasar unification and evolution schemes.


Monthly Notices of the Royal Astronomical Society | 2016

Halo mass function: baryon impact, fitting formulae, and implications for cluster cosmology

S. Bocquet; A. Saro; K. Dolag; J. J. Mohr

We use a set of hydrodynamical and dark matter-only (DMonly) simulations to calibrate the halo mass function (HMF). We explore the impact of baryons, propose an improved parametrization for spherical overdensity masses, and identify differences between our DMonly HMF and previously published HMFs. We use the Magneticum simulations, which are well suited because of their accurate treatment of baryons, high resolution, and large cosmological volumes of up to (3818 Mpc)(3). Baryonic effects globally decrease the masses of galaxy clusters, which, at a given mass, results in a decrease of their number density. This effect vanishes at high redshift z similar to 2 and for high masses M-200m greater than or similar to 10(14)M(circle dot). We perform cosmological analyses of three idealized approximations to the cluster surveys by the South Pole Telescope (SPT), Planck, and eROSITA. We pursue two main questions. (1) What is the impact of baryons? - for the SPT-like and the Planck-like samples, the impact of baryons on cosmological results is negligible. In the eROSITA-like case, however, neglecting the baryonic impact leads to an underestimate of Omega(m) by about 0.01, which is comparable to the expected uncertainty from eROSITA. (2) How does our DMonly HMF compare with previous work? - for the Planck-like sample, results obtained using our DMonly HMF are shifted by Delta(sigma(8)) similar or equal to (sigma(8)(Omega(m)/0.27)(0.3)) similar or equal to 0.02 with respect to results obtained using the Tinker et al. fit. This suggests that using our HMF would shift results from Planck clusters towards better agreement with cosmic-microwave-background anisotropy measurements. Finally, we discuss biases that can be introduced through inadequate HMF parametrizations that introduce false cosmological sensitivity.

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T. de Haan

University of California

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A. T. Crites

California Institute of Technology

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E. M. George

University of California

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N. W. Halverson

University of Colorado Boulder

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