The Universe at 148 & 218 Gigahertz
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Measurement of the Cosmic Microwave Background Polarization with the BICEP Telescope at the South Pole
UC Berkeley UC Berkeley Electronic Theses and Dissertations Title Measurement of the Cosmic Microwave Background Polarization with the BICEP Telescope at the South Pole Permalink https://escholarship.org/uc/item/6b98h32b Author Takahashi, Yuki David Publication Date 2010 Peer reviewed|Thesis/dissertation eScholarship.org Powered by the California Digital Library University of California Measurement of the Cosmic Microwave Background Polarization with the Bicep Telescope at the South Pole by Yuki David Takahashi A dissertation submitted in partial satisfaction of the requirements for the degree of Doctor of Philosophy in Physics in the Graduate Division of the University of California, Berkeley Committee in charge: Professor William L. Holzapfel, Chair Professor Adrian T. Lee Professor Chung-Pei Ma Fall 2010 Measurement of the Cosmic Microwave Background Polarization with the Bicep Telescope at the South Pole Copyright 2010 by Yuki David Takahashi 1 Abstract Measurement of the Cosmic Microwave Background Polarization with the Bicep Telescope at the South Pole by Yuki David Takahashi Doctor of Philosophy in Physics University of California, Berkeley Professor William L. Holzapfel, Chair The question of how exactly the universe began is the motivation for this work. Based on the discoveries of the cosmic expansion and of the cosmic microwave background (CMB) ra- diation, humans have learned of the Big Bang origin of the universe. However, what exactly happened in the first moments of the Big Bang? A scenario of initial exponential expansion called “inflation” was proposed in the 1980s, explaining several important mysteries about the universe. Inflation would have generated gravitational waves that would have left a unique imprint in the polarization of the CMB. -
Analysis and Measurement of Horn Antennas for CMB Experiments
Analysis and Measurement of Horn Antennas for CMB Experiments Ian Mc Auley (M.Sc. B.Sc.) A thesis submitted for the Degree of Doctor of Philosophy Maynooth University Department of Experimental Physics, Maynooth University, National University of Ireland Maynooth, Maynooth, Co. Kildare, Ireland. October 2015 Head of Department Professor J.A. Murphy Research Supervisor Professor J.A. Murphy Abstract In this thesis the author's work on the computational modelling and the experimental measurement of millimetre and sub-millimetre wave horn antennas for Cosmic Microwave Background (CMB) experiments is presented. This computational work particularly concerns the analysis of the multimode channels of the High Frequency Instrument (HFI) of the European Space Agency (ESA) Planck satellite using mode matching techniques to model their farfield beam patterns. To undertake this analysis the existing in-house software was upgraded to address issues associated with the stability of the simulations and to introduce additional functionality through the application of Single Value Decomposition in order to recover the true hybrid eigenfields for complex corrugated waveguide and horn structures. The farfield beam patterns of the two highest frequency channels of HFI (857 GHz and 545 GHz) were computed at a large number of spot frequencies across their operational bands in order to extract the broadband beams. The attributes of the multimode nature of these channels are discussed including the number of propagating modes as a function of frequency. A detailed analysis of the possible effects of manufacturing tolerances of the long corrugated triple horn structures on the farfield beam patterns of the 857 GHz horn antennas is described in the context of the higher than expected sidelobe levels detected in some of the 857 GHz channels during flight. -
Integrated Sachs Wolfe Effect and Rees Sciama Effect
Prog. Theor. Exp. Phys. 2012, 00000 (24 pages) DOI: 10.1093/ptep/0000000000 Integrated Sachs Wolfe Effect and Rees Sciama Effect Atsushi J. Nishizawa1 1 Kavli Institute for the Physics and Mathematics of the Universe (Kavli IPMU, WPI), The University of Tokyo, Chiba 277-8582, Japan ∗E-mail: [email protected] ............................................................................... It has been around fifty years since R. K. Sachs and A. M. Wolfe predicted the existence of anisotropy in the Cosmic Microwave Background (CMB) and ten years since the integrated Sachs Wolfe effect (ISW) was first detected observationally. The ISW effect provides us with a unique probe of the accelerating expansion of the Universe. The cross-correlation between the large-scale structure and CMB has been the most promising way to extract the ISW effect from the data. In this article, we review the physics of the ISW effect and summarize recent observational results and interpretations. ................................................................................................. Subject Index Cosmological perturbation theory, Cosmic background radiations, Dark energy and dark matter 1. Overview After the discovery of the isotropic radiation of the Cosmic Microwave Background (CMB) of the Universe by A. A. Penzias and R. W. Wilson in 1965 [100], R. K. Sachs and A. M Wolfe predict the existence of anisotropy in the CMB associated with the gravitational redshift in 1967 [116]. They fully integrate the geodesic equation in a perturbed Friedman-Robertson-Walker (FRW) metric in the fully general relativistic framework. The Sachs-Wolfe (SW) is the first paper that predicts the presence of the anisotropy in the CMB which now plays an important role for constraining cosmo- logical models, the nature of dark energy, modified gravity, and non-Gaussianity of the primordial fluctuation. -
19 International Workshop on Low Temperature Detectors
19th International Workshop on Low Temperature Detectors Program version 1.24 - British Summer Time 1 Date Time Session Monday 19 July 14:00 - 14:15 Introduction and Welcome 14:15 - 15:15 Oral O1: Devices 1 15:15 - 15:25 Break 15:25 - 16:55 Oral O1: Devices 1 (continued) 16:55 - 17:05 Break 17:05 - 18:00 Poster P1: MKIDs and TESs 1 Tuesday 20 July 14:00 - 15:15 Oral O2: Cold Readout 15:15 - 15:25 Break 15:25 - 16:55 Oral O2: Cold Readout (continued) 16:55 - 17:05 Break 17:05 - 18:30 Poster P2: Readout, Other Devices, Supporting Science 1 20:00 - 21:00 Virtual Tour of NIST Quantum Sensor Group Labs Wednesday 21 July 14:00 - 15:15 Oral O3: Instruments 15:15 - 15:25 Break 15:25 - 16:55 Oral O3: Instruments (continued) 16:55 - 17:05 Break 17:05 - 18:30 Poster P3: Instruments, Astrophysics and Cosmology 1 18:00 - 19:00 Vendor Exhibitor Hour Thursday 22 July 14:00 - 15:15 Oral O4A: Rare Events 1 Oral O4B: Material Analysis, Metrology, Other 15:15 - 15:25 Break 15:25 - 16:55 Oral O4A: Rare Events 1 (continued) Oral O4B: Material Analysis, Metrology, Other (continued) 16:55 - 17:05 Break 17:05 - 18:30 Poster P4: Rare Events, Materials Analysis, Metrology, Other Applications 20:00 - 21:00 Virtual Tour of NIST Cleanoom Monday 26 July 23:00 - 00:15 Oral O5: Devices 2 00:15 - 00:25 Break 00:25 - 01:55 Oral O5: Devices 2 (continued) 01:55 - 02:05 Break 02:05 - 03:30 Poster P5: MMCs, SNSPDs, more TESs Tuesday 27 July 23:00 - 00:15 Oral O6: Warm Readout and Supporting Science 00:15 - 00:25 Break 00:25 - 01:55 Oral O6: Warm Readout and Supporting Science -
An Analysis Including the Latest Local Measurement of the Hubble Constant
Eur. Phys. J. C (2017) 77:882 https://doi.org/10.1140/epjc/s10052-017-5454-9 Regular Article - Theoretical Physics Constraints on inflation revisited: an analysis including the latest local measurement of the Hubble constant Rui-Yun Guo1, Xin Zhang1,2,a 1 Department of Physics, College of Sciences, Northeastern University, Shenyang 110004, China 2 Center for High Energy Physics, Peking University, Beijing 100080, China Received: 21 June 2017 / Accepted: 8 December 2017 / Published online: 18 December 2017 © The Author(s) 2017. This article is an open access publication Abstract We revisit the constraints on inflation models by current cosmological observations can be used to explore using the current cosmological observations involving the the nature of inflation. For example, the measurements of latest local measurement of the Hubble constant (H0 = CMB anisotropies have confirmed that inflation can provide 73.00 ± 1.75 km s −1 Mpc−1). We constrain the primordial a nearly scale-invariant primordial power spectrum [5–8]. power spectra of both scalar and tensor perturbations with the Although inflation took place at energy scale as high as observational data including the Planck 2015 CMB full data, 1016 GeV, where particle physics remains elusive, hundreds the BICEP2 and Keck Array CMB B-mode data, the BAO of different theoretical scenarios have been proposed. Thus data, and the direct measurement of H0. In order to relieve the selecting an actual version of inflation has become a major tension between the local determination of the Hubble con- issue in the current study. As mentioned above, the primor- stant and the other astrophysical observations, we consider dial perturbations can lead to the CMB anisotropies and LSS the additional parameter Neff in the cosmological model. -
CMB Telescopes and Optical Systems to Appear In: Planets, Stars and Stellar Systems (PSSS) Volume 1: Telescopes and Instrumentation
CMB Telescopes and Optical Systems To appear in: Planets, Stars and Stellar Systems (PSSS) Volume 1: Telescopes and Instrumentation Shaul Hanany ([email protected]) University of Minnesota, School of Physics and Astronomy, Minneapolis, MN, USA, Michael Niemack ([email protected]) National Institute of Standards and Technology and University of Colorado, Boulder, CO, USA, and Lyman Page ([email protected]) Princeton University, Department of Physics, Princeton NJ, USA. March 26, 2012 Abstract The cosmic microwave background radiation (CMB) is now firmly established as a funda- mental and essential probe of the geometry, constituents, and birth of the Universe. The CMB is a potent observable because it can be measured with precision and accuracy. Just as importantly, theoretical models of the Universe can predict the characteristics of the CMB to high accuracy, and those predictions can be directly compared to observations. There are multiple aspects associated with making a precise measurement. In this review, we focus on optical components for the instrumentation used to measure the CMB polarization and temperature anisotropy. We begin with an overview of general considerations for CMB ob- servations and discuss common concepts used in the community. We next consider a variety of alternatives available for a designer of a CMB telescope. Our discussion is guided by arXiv:1206.2402v1 [astro-ph.IM] 11 Jun 2012 the ground and balloon-based instruments that have been implemented over the years. In the same vein, we compare the arc-minute resolution Atacama Cosmology Telescope (ACT) and the South Pole Telescope (SPT). CMB interferometers are presented briefly. We con- clude with a comparison of the four CMB satellites, Relikt, COBE, WMAP, and Planck, to demonstrate a remarkable evolution in design, sensitivity, resolution, and complexity over the past thirty years. -
The Design of the Ali CMB Polarization Telescope Receiver
The design of the Ali CMB Polarization Telescope receiver M. Salatinoa,b, J.E. Austermannc, K.L. Thompsona,b, P.A.R. Aded, X. Baia,b, J.A. Beallc, D.T. Beckerc, Y. Caie, Z. Changf, D. Cheng, P. Chenh, J. Connorsc,i, J. Delabrouillej,k,e, B. Doberc, S.M. Duffc, G. Gaof, S. Ghoshe, R.C. Givhana,b, G.C. Hiltonc, B. Hul, J. Hubmayrc, E.D. Karpela,b, C.-L. Kuoa,b, H. Lif, M. Lie, S.-Y. Lif, X. Lif, Y. Lif, M. Linkc, H. Liuf,m, L. Liug, Y. Liuf, F. Luf, X. Luf, T. Lukasc, J.A.B. Matesc, J. Mathewsonn, P. Mauskopfn, J. Meinken, J.A. Montana-Lopeza,b, J. Mooren, J. Shif, A.K. Sinclairn, R. Stephensonn, W. Sunh, Y.-H. Tsengh, C. Tuckerd, J.N. Ullomc, L.R. Valec, J. van Lanenc, M.R. Vissersc, S. Walkerc,i, B. Wange, G. Wangf, J. Wango, E. Weeksn, D. Wuf, Y.-H. Wua,b, J. Xial, H. Xuf, J. Yaoo, Y. Yaog, K.W. Yoona,b, B. Yueg, H. Zhaif, A. Zhangf, Laiyu Zhangf, Le Zhango,p, P. Zhango, T. Zhangf, Xinmin Zhangf, Yifei Zhangf, Yongjie Zhangf, G.-B. Zhaog, and W. Zhaoe aStanford University, Stanford, CA 94305, USA bKavli Institute for Particle Astrophysics and Cosmology, Stanford, CA 94305, USA cNational Institute of Standards and Technology, Boulder, CO 80305, USA dCardiff University, Cardiff CF24 3AA, United Kingdom eUniversity of Science and Technology of China, Hefei 230026 fInstitute of High Energy Physics, Chinese Academy of Sciences, Beijing 100049 gNational Astronomical Observatories, Chinese Academy of Sciences, Beijing 100012 hNational Taiwan University, Taipei 10617 iUniversity of Colorado Boulder, Boulder, CO 80309, USA jIN2P3, CNRS, Laboratoire APC, Universit´ede Paris, 75013 Paris, France kIRFU, CEA, Universit´eParis-Saclay, 91191 Gif-sur-Yvette, France lBeijing Normal University, Beijing 100875 mAnhui University, Hefei 230039 nArizona State University, Tempe, AZ 85004, USA oShanghai Jiao Tong University, Shanghai 200240 pSun Yat-Sen University, Zhuhai 519082 ABSTRACT Ali CMB Polarization Telescope (AliCPT-1) is the first CMB degree-scale polarimeter to be deployed on the Tibetan plateau at 5,250 m above sea level. -
The B3-VLA CSS Sample⋆
A&A 528, A110 (2011) Astronomy DOI: 10.1051/0004-6361/201015379 & c ESO 2011 Astrophysics The B3-VLA CSS sample VIII. New optical identifications from the Sloan Digital Sky Survey The ultraviolet-optical spectral energy distribution of the young radio sources C. Fanti1,R.Fanti1, A. Zanichelli1, D. Dallacasa1,2, and C. Stanghellini1 1 Istituto di Radioastronomia – INAF, via Gobetti 101, 40129 Bologna, Italy e-mail: [email protected] 2 Dipartimento di Astronomia, Università di Bologna, via Ranzani 1, 40127 Bologna, Italy Received 12 July 2010 / Accepted 22 December 2010 ABSTRACT Context. Compact steep-spectrum radio sources and giga-hertz peaked spectrum radio sources (CSS/GPS) are generally considered to be mostly young radio sources. In recent years we studied at many wavelengths a sample of these objects selected from the B3-VLA catalog: the B3-VLA CSS sample. Only ≈60% of the sources were optically identified. Aims. We aim to increase the number of optical identifications and study the properties of the host galaxies of young radio sources. Methods. We cross-correlated the CSS B3-VLA sample with the Sloan Digital Sky Survey (SDSS), DR7, and complemented the SDSS photometry with available GALEX (DR 4/5 and 6) and near-IR data from UKIRT and 2MASS. Results. We obtained new identifications and photometric redshifts for eight faint galaxies and for one quasar and two quasar candi- dates. Overall we have 27 galaxies with SDSS photometry in five bands, for which we derived the ultraviolet-optical spectral energy distribution (UV-O-SED). We extended our investigation to additional CSS/GPS selected from the literature. -
Cosmography of the Local Universe SDSS-III Map of the Universe
Cosmography of the Local Universe SDSS-III map of the universe Color = density (red=high) Tools of the Future: roBotic/piezo fiBer positioners AstroBot FiBer Positioners Collision-avoidance testing Echidna (for SuBaru FMOS) Las Campanas Redshift Survey The first survey to reach the quasi-homogeneous regime Large-scale structure within z<0.05, sliced in Galactic plane declination “Zone of Avoidance” 6dF Galaxy Survey, Jones et al. 2009 Large-scale structure within z<0.1, sliced in Galactic plane declination “Zone of Avoidance” 6dF Galaxy Survey, Jones et al. 2009 Southern Hemisphere, colored By redshift 6dF Galaxy Survey, Jones et al. 2009 SDSS-BOSS map of the universe Image credit: Jeremy Tinker and the SDSS-III collaBoration SDSS-III map of the universe Color = density (red=high) Millenium Simulation (2005) vs Galaxy Redshift Surveys Image Credit: Nina McCurdy and Joel Primack/University of California, Santa Cruz; Ralf Kaehler and Risa Wechsler/Stanford University; Klypin et al. 2011 Sloan Digital Sky Survey; Michael Busha/University of Zurich Trujillo-Gomez et al. 2011 Redshift-space distortion in the 2D correlation function of 6dFGS along line of sight on the sky Beutler et al. 2012 Matter power spectrum oBserved by SDSS (Tegmark et al. 2006) k-3 Solid red lines: linear theory (WMAP) Dashed red lines: nonlinear corrections Note we can push linear approx to a Bit further than k~0.02 h/Mpc Baryon acoustic peaks (analogous to CMB acoustic peaks; standard rulers) keq SDSS-BOSS map of the universe Color = distance (purple=far) Image credit: -
Clover: Measuring Gravitational-Waves from Inflation
ClOVER: Measuring gravitational-waves from Inflation Executive Summary The existence of primordial gravitational waves in the Universe is a fundamental prediction of the inflationary cosmological paradigm, and determination of the level of this tensor contribution to primordial fluctuations is a uniquely powerful test of inflationary models. We propose an experiment called ClOVER (ClObserVER) to measure this tensor contribution via its effect on the geometric properties (the so-called B-mode) of the polarization of the Cosmic Microwave Background (CMB) down to a sensitivity limited by the foreground contamination due to lensing. In order to achieve this sensitivity ClOVER is designed with an unprecedented degree of systematic control, and will be deployed in Antarctica. The experiment will consist of three independent telescopes, operating at 90, 150 or 220 GHz respectively, and each of which consists of four separate optical assemblies feeding feedhorn arrays arrays of superconducting detectors with phase as well as intensity modulation allowing the measurement of all three Stokes parameters I, Q and U in every pixel. This project is a combination of the extensive technical expertise and experience of CMB measurements in the Cardiff Instrumentation Group (Gear) and Cavendish Astrophysics Group (Lasenby) in UK, the Rome “La Sapienza” (de Bernardis and Masi) and Milan “Bicocca” (Sironi) CMB groups in Italy, and the Paris College de France Cosmology group (Giraud-Heraud) in France. This document is based on the proposal submitted to PPARC by the UK groups (and funded with 4.6ML), integrated with additional information on the Dome-C site selected for the operations. This document has been prepared to obtain an endorsement from the INAF (Istituto Nazionale di Astrofisica) on the scientific quality of the proposed experiment to be operated in the Italian-French base of Dome-C, and to be submitted to the Commissione Scientifica Nazionale Antartica and to the French INSU and IPEV. -
Searching for the Missing Baryons in Clusters
Searching for the missing baryons in clusters Bilhuda Rasheed, Neta Bahcall1, and Paul Bode Department of Astrophysical Sciences, 4 Ivy Lane, Peyton Hall, Princeton University, Princeton, NJ 08544 Edited by Marc Davis, University of California, Berkeley, CA, and approved January 10, 2011 (received for review July 8, 2010) Observations of clusters of galaxies suggest that they contain few- fraction in the richest clusters, it is still systematically below er baryons (gas plus stars) than the cosmic baryon fraction. This the cosmic value. This baryon discrepancy, especially the gas frac- “missing baryon” puzzle is especially surprising for the most mas- tion, is observed to increase with decreasing cluster mass (14, 15). sive clusters, which are expected to be representative of the cosmic This raises the questions: Where are the missing baryons? Why matter content of the universe (baryons and dark matter). Here we are they “missing”? show that the baryons may not actually be missing from clusters, Attempted explanations for the missing baryons in clusters but rather are extended to larger radii than typically observed. The range from preheating or other energy inputs that expel gas from baryon deficiency is typically observed in the central regions of the system (16–22, and references therein), to the suggestion of clusters (∼0.5 the virial radius). However, the observed gas-density additional baryonic components not yet detected [e.g., cool gas, profile is significantly shallower than the mass-density profile, faint stars (10, 23)]. Simulations, which do suggest a depletion of implying that the gas is more extended than the mass and that cluster gas in the inner regions of clusters, do not yet contain all the gas fraction increases with radius. -
The 6Df Galaxy Survey: Z ≈ 0 Measurements of the Growth Rate and Σ 8
Mon. Not. R. Astron. Soc. 423, 3430–3444 (2012) doi:10.1111/j.1365-2966.2012.21136.x The 6dF Galaxy Survey: z ≈ 0 measurements of the growth rate and σ 8 Florian Beutler,1 Chris Blake,2 Matthew Colless,3 D. Heath Jones,4 Lister Staveley-Smith,1,5 Gregory B. Poole,2 Lachlan Campbell,6 Quentin Parker,3,7 Will Saunders3 and Fred Watson3 1International Centre for Radio Astronomy Research (ICRAR), University of Western Australia, 35 Stirling Highway, Crawley, WA 6009, Australia 2Centre for Astrophysics & Supercomputing, Swinburne University of Technology, PO Box 218, Hawthorn, VIC 3122, Australia 3Australian Astronomical Observatory, PO Box 296, Epping, NSW 1710, Australia 4School of Physics, Monash University, Clayton, VIC 3800, Australia 5ARC Centre of Excellence for All-sky Astrophysics (CAASTRO), Australia 6Western Kentucky University, Bowling Green, KY 42101, USA 7Department of Physics and Astronomy, Faculty of Sciences, Macquarie University, NSW 2109, Sydney, Australia Accepted 2012 April 19. Received 2012 March 16; in original form 2011 November 14 ABSTRACT We present a detailed analysis of redshift-space distortions in the two-point correlation function of the 6dF Galaxy Survey (6dFGS). The K-band selected subsample which we employ in this 2 study contains 81 971 galaxies distributed over 17 000 degree with an effective redshift zeff = 0.067. By modelling the 2D galaxy correlation function, ξ(rp, π), we measure the parameter = ± γ combination f (zeff)σ 8(zeff) 0.423 0.055, where f m(z) is the growth rate of cosmic −1 structure and σ 8 is the rms of matter fluctuations in 8 h Mpc spheres.