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Featured researches published by T. M. Crawford.


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 | 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.


Astroparticle Physics | 2015

Neutrino physics from the cosmic microwave background and large scale structure

K. N. Abazajian; K. Arnold; J. E. Austermann; B. A. Benson; C. Bischoff; J. Bock; J. R. Bond; J. Borrill; I. Buder; D. L. Burke; E. Calabrese; J. E. Carlstrom; C. S. Carvalho; C. L. Chang; H. C. Chiang; S. Church; A. Cooray; T. M. Crawford; B. P. Crill; Kyle S. Dawson; S. Das; M. J. Devlin; M. Dobbs; Scott Dodelson; O. Doré; Joanna Dunkley; J. L. Feng; A. Fraisse; J. Gallicchio; S. B. Giddings

This is a report on the status and prospects of the quantification of neutrino properties through the cosmological neutrino background for the Cosmic Frontier of the Division of Particles and Fields Community Summer Study long-term planning exercise. Experiments planned and underway are prepared to study the cosmological neutrino background in detail via its influence on distance-redshift relations and the growth of structure. The program for the next decade described in this document, including upcoming spectroscopic galaxy surveys eBOSS and DESI and a new Stage-IV CMB polarization experiment CMB-S4, will achieve σ(σmν) = 16 meV and σ(Neff) = 0.020. Such a mass measurement will produce a high significance detection of non-zero σmν, whose lower bound derived from atmospheric and solar neutrino oscillation data is about 58 meV. If neutrinos have a minimal normal mass hierarchy, this measurement will definitively rule out the inverted neutrino mass hierarchy, shedding light on one of the most puzzling aspects of the Standard Model of particle physics — the origin of mass. This precise a measurement of Neff will allow for high sensitivity to any light and dark degrees of freedom produced in the big bang and a precision test of the standard cosmological model prediction that Neff=3.046.


The Astrophysical Journal | 2013

ALMA REDSHIFTS OF MILLIMETER-SELECTED GALAXIES FROM THE SPT SURVEY: THE REDSHIFT DISTRIBUTION OF DUSTY STAR-FORMING GALAXIES

A. Weiß; C. De Breuck; D. P. Marrone; J. D. Vieira; James E. Aguirre; K. A. Aird; M. Aravena; M. L. N. Ashby; Matthew B. Bayliss; B. A. Benson; M. Béthermin; A. D. Biggs; L. E. Bleem; J. J. Bock; M. Bothwell; C. M. Bradford; M. Brodwin; J. E. Carlstrom; C. L. Chang; Sydney Chapman; T. M. Crawford; A. T. Crites; T. de Haan; M. Dobbs; Thomas P. Downes; C. D. Fassnacht; E. M. George; Michael D. Gladders; Anthony H. Gonzalez; T. R. Greve

Using the Atacama Large Millimeter/submillimeter Array, we have conducted a blind redshift survey in the 3 mm atmospheric transmission window for 26 strongly lensed dusty star-forming galaxies (DSFGs) selected with the South Pole Telescope. The sources were selected to have S_(1.4mm) > 20 mJy and a dust-like spectrum and, to remove low-z sources, not have bright radio (S_843MHz) 3. We discuss the effect of gravitational lensing on the redshift distribution and compare our measured redshift distribution to that of models in the literature.


arXiv: Cosmology and Nongalactic Astrophysics | 2016

CMB-S4 Science Book, First Edition

Kevork N. Abazajian; Peter Adshead; Z. Ahmed; S. W. Allen; David Alonso; K. Arnold; C. Baccigalupi; J. G. Bartlett; Nicholas Battaglia; B. A. Benson; C. Bischoff; J. Borrill; Victor Buza; Erminia Calabrese; Robert R. Caldwell; J. E. Carlstrom; C. L. Chang; T. M. Crawford; Francis-Yan Cyr-Racine; Francesco De Bernardis; Tijmen de Haan; Serego Alighieri Sperello di; Joanna Dunkley; Cora Dvorkin; J. Errard; Giulio Fabbian; Stephen M. Feeney; Simone Ferraro; Jeffrey P. Filippini; Raphael Flauger

This book lays out the scientific goals to be addressed by the next-generation ground-based cosmic microwave background experiment, CMB-S4, envisioned to consist of dedicated telescopes at the South Pole, the high Chilean Atacama plateau and possibly a northern hemisphere site, all equipped with new superconducting cameras. CMB-S4 will dramatically advance cosmological studies by crossing critical thresholds in the search for the B-mode polarization signature of primordial gravitational waves, in the determination of the number and masses of the neutrinos, in the search for evidence of new light relics, in constraining the nature of dark energy, and in testing general relativity on large scales.


Physical Review D | 2005

Spontaneous isotropy breaking: a mechanism for cmb multipole alignments

Christopher Gordon; Wayne Hu; Dragan Huterer; T. M. Crawford

We introduce a class of models in which statistical isotropy is broken spontaneously in the CMB by a nonlinear response to long-wavelength fluctuations in a mediating field. These fluctuations appear as a gradient locally and pick out a single preferred direction. The nonlinear response imprints this direction in a range of multipole moments. We consider two manifestations of isotropy breaking: additive contributions and multiplicative modulation of the intrinsic anisotropy. Since the Wilkinson microwave anisotropy probe (WMAP) exhibits an alignment of power deficits, an additive contribution is less likely to produce the observed alignments than the usual isotropic fluctuations, a fact which we illustrate with an explicit cosmological model of long-wavelength quintessence fluctuations. This problem applies to other models involving foregrounds or background anisotropy that seek to restore power to the CMB. Additive models that account directly for the observed power exacerbate the low power of the intrinsic fluctuations. Multiplicative models can overcome these difficulties. We construct a proof of principle model that significantly improves the likelihood and generates stronger alignments than WMAP in 30%-45% of realizations.


Proceedings of SPIE | 2014

SPT-3G: a next-generation cosmic microwave background polarization experiment on the South Pole telescope

B. A. Benson; Peter A. R. Ade; Z. Ahmed; S. W. Allen; K. Arnold; J. E. Austermann; A. N. Bender; L. E. Bleem; J. E. Carlstrom; C. L. Chang; H. M. Cho; Jean-François Cliche; T. M. Crawford; A. Cukierman; T. de Haan; M. Dobbs; D. Dutcher; W. Everett; A. Gilbert; N. W. Halverson; D. Hanson; N. L. Harrington; K. Hattori; J. W. Henning; G. C. Hilton; Gilbert P. Holder; W. L. Holzapfel; K. D. Irwin; R. Keisler; L. Knox

We describe the design of a new polarization sensitive receiver, spt-3g, for the 10-meter South Pole Telescope (spt). The spt-3g receiver will deliver a factor of ~20 improvement in mapping speed over the current receiver, spt-pol. The sensitivity of the spt-3g receiver will enable the advance from statistical detection of B-mode polarization anisotropy power to high signal-to-noise measurements of the individual modes, i.e., maps. This will lead to precise (~0.06 eV) constraints on the sum of neutrino masses with the potential to directly address the neutrino mass hierarchy. It will allow a separation of the lensing and inflationary B-mode power spectra, improving constraints on the amplitude and shape of the primordial signal, either through spt-3g data alone or in combination with bicep2/keck, which is observing the same area of sky. The measurement of small-scale temperature anisotropy will provide new constraints on the epoch of reionization. Additional science from the spt-3g survey will be significantly enhanced by the synergy with the ongoing optical Dark Energy Survey (des), including: a 1% constraint on the bias of optical tracers of large-scale structure, a measurement of the differential Doppler signal from pairs of galaxy clusters that will test General Relativity on ~200Mpc scales, and improved cosmological constraints from the abundance of clusters of galaxies


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.))


Review of Scientific Instruments | 2012

Frequency multiplexed superconducting quantum interference device readout of large bolometer arrays for cosmic microwave background measurements

M. Dobbs; M. Lueker; K. A. Aird; A. N. Bender; B. A. Benson; L. E. Bleem; J. E. Carlstrom; C. L. Chang; H. M. Cho; John Clarke; T. M. Crawford; A. T. Crites; D. Flanigan; T. de Haan; E. M. George; N. W. Halverson; W. L. Holzapfel; J. D. Hrubes; B. R. Johnson; John Joseph; R. Keisler; J. Kennedy; Z. Kermish; T. M. Lanting; A. T. Lee; E. M. Leitch; D. Luong-Van; J. J. McMahon; J. Mehl; S. S. Meyer

A technological milestone for experiments employing transition edge sensor bolometers operating at sub-Kelvin temperature is the deployment of detector arrays with 100s-1000s of bolometers. One key technology for such arrays is readout multiplexing: the ability to read out many sensors simultaneously on the same set of wires. This paper describes a frequency-domain multiplexed readout system which has been developed for and deployed on the APEX-SZ and South Pole Telescope millimeter wavelength receivers. In this system, the detector array is divided into modules of seven detectors, and each bolometer within the module is biased with a unique ∼MHz sinusoidal carrier such that the individual bolometer signals are well separated in frequency space. The currents from all bolometers in a module are summed together and pre-amplified with superconducting quantum interference devices operating at 4 K. Room temperature electronics demodulate the carriers to recover the bolometer signals, which are digitized separately and stored to disk. This readout system contributes little noise relative to the detectors themselves, is remarkably insensitive to unwanted microphonic excitations, and provides a technology pathway to multiplexing larger numbers of sensors.

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N. W. Halverson

University of Colorado Boulder

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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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