K. A. Aird
University of Chicago
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Featured researches published by K. A. Aird.
The Astrophysical Journal | 2011
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
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.
The Astrophysical Journal | 2013
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.
Nature | 2012
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
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
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.
Proceedings of SPIE | 2012
J. E. Austermann; K. A. Aird; James A. Beall; D. Becker; A. N. Bender; B. A. Benson; L. E. Bleem; J. Britton; J. E. Carlstrom; C. L. Chang; H. C. Chiang; H. M. Cho; T. M. Crawford; A. T. Crites; A. Datesman; T. de Haan; M. Dobbs; E. M. George; N. W. Halverson; N. L. Harrington; J. W. Henning; G. C. Hilton; G. P. Holder; W. L. Holzapfel; S. Hoover; N. Huang; J. Hubmayr; K. D. Irwin; R. Keisler; J. Kennedy
SPTpol is a dual-frequency polarization-sensitive camera that was deployed on the 10-meter South Pole Telescope in January 2012. SPTpol will measure the polarization anisotropy of the cosmic microwave background (CMB) on angular scales spanning an arcminute to several degrees. The polarization sensitivity of SPTpol will enable a detection of the CMB “B-mode” polarization from the detection of the gravitational lensing of the CMB by large scale structure, and a detection or improved upper limit on a primordial signal due to inationary gravity waves. The two measurements can be used to constrain the sum of the neutrino masses and the energy scale of ination. These science goals can be achieved through the polarization sensitivity of the SPTpol camera and careful control of systematics. The SPTpol camera consists of 768 pixels, each containing two transition-edge sensor (TES) bolometers coupled to orthogonal polarizations, and a total of 1536 bolometers. The pixels are sensitive to light in one of two frequency bands centered at 90 and 150 GHz, with 180 pixels at 90 GHz and 588 pixels at 150 GHz. The SPTpol design has several features designed to control polarization systematics, including: singlemoded feedhorns with low cross-polarization, bolometer pairs well-matched to dfference atmospheric signals, an improved ground shield design based on far-sidelobe measurements of the SPT, and a small beam to reduce temperature to polarization leakage. We present an overview of the SPTpol instrument design, project status, and science projections.
The Astrophysical Journal | 2015
R. Keisler; S. Hoover; N. L. Harrington; J. W. Henning; Peter A. R. Ade; K. A. Aird; J. E. Austermann; J. A. Beall; A. N. Bender; B. A. Benson; L. E. Bleem; J. E. Carlstrom; C. L. Chang; H. C. Chiang; H. M. Cho; R. Citron; T. M. Crawford; A. T. Crites; T. de Haan; M. Dobbs; W. Everett; J. Gallicchio; J. Gao; E. M. George; A. Gilbert; N. W. Halverson; D. Hanson; G. C. Hilton; Gilbert P. Holder; W. L. Holzapfel
We present a measurement of the
The Astrophysical Journal | 2013
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
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The Astrophysical Journal | 2014
M. McDonald; B. A. Benson; A. Vikhlinin; K. A. Aird; S. W. Allen; Marshall W. Bautz; Matthew B. Bayliss; L. E. Bleem; S. Bocquet; M. Brodwin; J. E. Carlstrom; C. L. Chang; Hyunjii Cho; Alejandro Clocchiatti; T. M. Crawford; A. T. Crites; T. de Haan; M. Dobbs; Ryan J. Foley; W. Forman; E. M. George; Michael D. Gladders; Anthony H. Gonzalez; N. W. Halverson; J. Hlavacek-Larrondo; Gilbert P. Holder; W. L. Holzapfel; J. D. Hrubes; Christine M. Jones; R. Keisler
-mode polarization power spectrum (the