Radio Astronomy & Radio Telescopes
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History of Radio Astronomy
History of Radio Astronomy Reading for High School Students Getsemary Báez Introduction form of radiation involved (soon known as electro- Radio Astronomy, a field that has strongly magnetic waves). Nevertheless, it was Oliver Heavi- evolved since the end of World War II, has become side who in conjunction with Willard Gibbs in 1884 one of the most important tools of astronomical ob- modified the equations and put them into modern servations. Radio astronomy has been responsible for vector notation. a great part of our understanding of the universe, its A few years later, Heinrich Hertz (1857- formation, composition, interactions, and even pre- 1894) demonstrated the existence of electromagnetic dictions about its future path. This article intends to waves by constructing a device that had the ability to inform the public about the history of radio astron- transmit and receive electromagnetic waves of about omy, its evolution, connection with solar studies, and 5m wavelength. This was actually the first radio the contribution the STEREO/WAVES instrument on wave transmitter, which is what we call today an LC the STEREO spacecraft will have on the study of oscillator. Just like Maxwell’s theory predicted, the this field. waves were polarized. The radiation emissions were detected using a 1mm thin circle of copper wire. Pre-history of Radio Waves Now that there is evidence of electromag- It is almost impossible to depict the most im- netic waves, the physicist Max Planck (1858-1947) portant facts in the history of radio astronomy with- was responsible for a breakthrough in physics that out presenting a sneak peak where everything later developed into the quantum theory, which sug- started, the development and understanding of the gests that energy had to be emitted or absorbed in electromagnetic spectrum. -
Interferometry and Aperture Synthesis in Order to Understand the Re
Summer Student Lecture Notes INTERFEROMETRY AND APERTURE SYNTHESIS Bruce Balick July 1973 The following pages are reprinted (with corrections) from Balick, B. 1972, thesis (Cornell University) CHAPTER II INTERFEROMETRY AND APERTURE SYNTHESIS Electromagnetic radiation is a wave phenomena, consequently in- struments used to observe this radiation are subject to diffraction limi- tations on their resolution. The angular limit, A, is given approxi- mately by AS6 D/A, where D is the aperture dimension and X is the obscwrving wavelcngth; for radio work - _____A - 140 B/cm) min -arc [D/feet] Thus the 300-foot telescope has a maximum resolution of 6' .arc at XAll cm, whereas a 10-cm aperture optical telescope has a diffraction limit of 1" are at optical wavelengths. (The same high resolution would require ap- ertures 1-1000 km in diameter at radio wavelengths.) To obtain high resolution at radio wavelengths, partially fill- ed apertures of large diameter can be synthesized. For this, two tele- scopes separated by a baseline B can be used to simulate the response of a nearly circular annulus of diameter IB. The telescope pair is con- figured in such a manner that it is best described as an interferometer in the ordinary optical sense. By moving the telescopes to obtain inter- ferometers of different spacings, annuli of different sizes can be simu- lated. The results obtained on the various spacings can be added appropriately to synthesize the response of a single telescope of very large diameter, and thereby yield maps of high resolution. For example, the interferometer of the National Radio Astronomy Observatory (NRAO) can 10 S. -
Cross-Correlator Implementations Enabling Aperture Synthesis for Geostationary-Based Remote Sensing
THESIS FOR THE DEGREE OF DOCTOR OF PHILOSOPHY Cross-Correlator Implementations Enabling Aperture Synthesis for Geostationary-Based Remote Sensing ERIK RYMAN Division of Computer Engineering Department of Computer Science and Engineering CHALMERS UNIVERSITY OF TECHNOLOGY Göteborg, Sweden 2018 Cross-Correlator Implementations Enabling Aperture Synthesis for Geostationary-Based Remote Sensing Erik Ryman ISBN 978-91-7597-751-5 Copyright © Erik Ryman, 2018. Doktorsavhandlingar vid Chalmers tekniska högskola Ny serie Nr 4432 ISSN 0346-718X Technical report No. 156D Department of Computer Science and Engineering VLSI Research Group Department of Computer Science and Engineering Chalmers University of Technology SE-412 96 GÖTEBORG, Sweden Phone: +46 (0)31-772 10 00 Author e-mail: [email protected] Cover: A 64-channel cross-correlator unit, including chip photos of digital correlator and analog-to-digital converter. Printed by Chalmers Reproservice Göteborg, Sweden 2018 Cross-Correlator Implementations Enabling Aperture Synthesis for Geostationary-Based Remote Sensing Erik Ryman Department of Computer Science and Engineering, Chalmers University of Technology ABSTRACT An ever-increasing demand for weather prediction and high climate modelling ac- curacy drives the need for better atmospheric data collection. These demands in- clude better spatial and temporal coverage of mainly humidity and temperature distributions in the atmosphere. A new type of remote sensing satellite technol- ogy is emerging, originating in the field of radio astronomy where telescope aper- ture upscaling could not keep up with the increasing demand for higher resolution. Aperture synthesis imaging takes an array of receivers and emulates apertures ex- tending way beyond what is possible with any single antenna. In the field of Earth remote sensing, the same idea could be used to construct satellites observing in the microwave region at a high resolution with foldable antenna arrays. -
Book of Abstracts
Dissecting the Universe - Workshop on Results from High-Resolution VLBI Monday 30 November 2015 - Wednesday 02 December 2015 Max-Planck-Institut für Radioastronomie, Bonn, Germany Book of Abstracts Contents GMVA Observations of M87 and Status Report of the GLT Project . 1 Water megamasers at high resolution . 1 Millimeter VLBI Observations of the Twin-Jet-System in NGC1052 . 1 First 3mm-VLBI imaging of the two-sided jet in Cygnus A: zooming into the launching region . 2 New insight into AGN-jets: they are alive! . 2 The connection between the mm VLBI jet and the gamma-ray emission in the blazar CTA102 and the radio galaxy 3C120 . 2 New Developments with the Event Horizon Telescope . 3 Dissecting TeV blazars: Space VLBI study of the BL Lac source Markarian 501 . 3 VLBI Studies of Star Forming Regions using Molecular Masers . 4 The farthest view with overterrestrial baselines . 4 Probing the innermost regions of AGN jets and their magnetic fields with RadioAstron 4 What has VLBI at the highest resolutions taught us about the VLBI "core"? . 5 The most compact H2O maser spots and their locations in W3 IRS5 . 5 A physical model for the radio and GeV emission from the microquasar LS I +61◦303 6 Detection and Implications of Horizon-Scale Polarization in Sgr A* . 7 The Discovery and Implications of Refractive Substructure for VLBI at the Highest Angular Resolutions . 7 Microarcsecond Structure of the Parsec Scale Jet of the Quasar 3C454.3 . 7 Jets from Water-Disk-Megamaser Galaxies . 8 Unlocking the secrets of PKS 1502+106. Synergies between mm-VLBI and single-dish monitoring . -
REBER CIRCLE, GROTE REBER RADIO TELESCOPE SITE HAER No
REBER CIRCLE, GROTE REBER RADIO TELESCOPE SITE HAER No. HI-118 (Haleakala High Observatory Site) Pukalani Vicinity Maui County Hawaii PHOTOGRAPHS WRITTEN HISTORICAL AND DESCRIPTIVE DATA HISTORIC AMERICAN ENGINEERING RECORD U.S. Department of the Interior National Park Service San Francisco, California HISTORIC AMERICAN ENGINEERING RECORD REBER CIRCLE, GROTE REBER RADIO TELESCOPE SITE HAER No. HI-118 Location: Haleakala High Altitude Observatory Site (on Pu‘u Kolekole hill) Pukalani Vicinity Maui, Hawaii U.S.G.S. Topographic map, Kilohana Quadrangle 1991 (7.5 minute series) Universal Transverse Mercator Coordinates NAD 83: 04.785505. 2292557 Present Owner: University of Hawaii Institute for Astronomy Present Use: None Significance: Reber Circle is a significant resource in the history of the development of Haleakala for astronomical observation, as well as the development of Radio Astronomy generally. Reber’s telescope was the first to make use of Haleakala’s peak for the observation of celestial objects. It was also an important early radio telescope; guiding radio astronomers toward better placement of receiving antennas, with data gathered through it leading to Reber’s discoveries that modified ionospheric theory. Historian: Lesleigh Jones Mason Architects, Inc. 119 Merchant Street, Suite 501 Honolulu, HI 96813 Project Information: This report is part of a mitigation measure for the construction of the Advanced Technology Solar Telescope (ATST). This documentation was required under Section I.H. (2-7) of the Advanced Technology Solar Telescope Project Programmatic Agreement (PA), which was signed by the National Science Foundation, the National Park Service, the Advisory Council on Historic Preservation, the Hawaii State Historic Preservation Officer, The Association of Universities for Research In Astronomy, and the University of Hawai‘i (for the benefit of its Institute for Astronomy. -
IAU-RT-Full Text.Pages
IAU General Assembly 2018 - Vienna - Session on 27 August 2018, 13:30 - 17:00 Commission B4 - IAU/URSI Working Group on Historic Radio Astronomy The history of large single dish projects and lessons learned ————————————————————————————————————- Review of the evolution of large single dishes Jaap Baars, Max-Planck-Institut für Radioastronomie, Bonn, Germany Slide 1 - Archimedes’ Burning Mirror at Syracuse 1. Introduction Here is a picture of a mural by Giulio Pangi (~1599) in the Galleria degli Uffizi in Florence with the title “Specchi Ustori di Archimede”, in English, “Archimede’s Burning Glasses”. Most historians believe it never happened. If it did it was the first application of the focussing properties of the paraboloidal reflector; not for astronomy but for military action. You will already have noticed that the artist did not know about focus. The Suns’ light concentrates on the mirror and is reflected in a divergent beam towards the ship. It would be hard to get anything burning! It is however interesting to note that for a successful attack the mirror would have been an offset paraboloid, a geometry that receives increasing interest from current radio telescope designers and users. HISTORY OF LARGE SINGLE DISHES !1 Astro Tech Talk 17.11.2017 Hans Jürgen Kärcher Haus der Astronomie Heidelberg Actual ELT’s use all rocking chair mounts 39m E-ELT 30m TMT 24.5m GMT Slide 2. Reber with his dish at NRAO, Green Bank and ESO ELT model, both with “rocking chair” elevation drive. After Jansky detected radio radiation from the direction to the Galactic Center in 1932 at a wavelength of about 15 m, radio astronomy was started in earnest by Grote Reber, an engineer and radio Ham, not an astronomer. -
Aperture Synthesis James Di Francesco National Research Council of Canada North American ALMA Regional Center – Victoria
A Crash Course in ! Radio Astronomy and Interferometry:! 2. Aperture Synthesis James Di Francesco National Research Council of Canada North American ALMA Regional Center – Victoria (thanks to S. Dougherty, C. Chandler, D. Wilner & C. Brogan) Aperture Synthesis Output of a Filled Aperture • Signals at each point in the aperture are brought together in phase at the antenna output (the focus) • Imagine the aperture to be subdivided into N smaller elementary areas; the voltage, V(t), at the output is the sum of the contributions ΔVi(t) from the N individual aperture elements: V(t) = ∑ΔVi (t) € Aperture Synthesis Aperture Synthesis: Basic Concept • The radio power measured by a receiver attached to the telescope is proportional to a running time average of the square of the output voltage: 2 P V V V ∝ (∑Δ i ) = ∑∑ (Δ iΔ k ) 2 = ∑ ΔVi + ∑∑ ΔViΔVk i≠k • Any€ measurement with the large filled-aperture telescope can be written as a sum, in which each term depends on contributions from only two of the N aperture€ elements • Each term 〈ΔViΔVk〉 can be measured with two small antennas, if we place them at locations i and k and measure the average product of their output voltages with a correlation (multiplying) receiver Aperture Synthesis Aperture Synthesis: Basic Concept • If the source emission is unchanging, there is no need to measure all the pairs at one time • One could imagine sequentially combining pairs of signals. For N sub-apertures there will be N(N-1)/2 pairs to combine • Adding together all the terms effectively “synthesizes” one measurement -
H I Observations of Two New Dwarf Galaxies: Pisces a and B with the SKA Pathfinder KAT-7? C
A&A 587, L3 (2016) Astronomy DOI: 10.1051/0004-6361/201527910 & c ESO 2016 Astrophysics Letter to the Editor H I observations of two new dwarf galaxies: Pisces A and B with the SKA Pathfinder KAT-7? C. Carignan1;2, Y. Libert1, D. M. Lucero1;4, T. H. Randriamampandry1, T. H. Jarrett1, T. A. Oosterloo3;4, and E. J. Tollerud5 1 Department of Astronomy, University of Cape Town, Private Bag X3, 7701 Rondebosch, South Africa e-mail: [email protected] 2 Observatoire d’Astrophysique de l’Université de Ouagadougou, BP 7021, Ouagadougou 03, Burkina Faso 3 Netherlands Institute for Radio Astronomy (ASTRON), Postbus 2, 7990 AA Dwingeloo, The Netherlands 4 Kapteyn Astronomical Institute, University of Groningen, PO Box 800, 9700 AV Groningen, The Netherlands 5 Space Telescope Science Institute, 3700 San Martin Dr, Baltimore, MD 21218, USA Received 7 December 2015 / Accepted 3 January 2016 ABSTRACT Context. Pisces A and Pisces B are the only two galaxies found via optical imaging and spectroscopy out of 22 Hi clouds identified in the GALFAHI survey as dwarf galaxy candidates. Aims. We derive the Hi content and kinematics of Pisces A and B. Methods. Our aperture synthesis Hi observations used the seven-dish Karoo Array Telescope (KAT-7), which is a pathfinder instru- ment for MeerKAT, the South African precursor to the mid-frequency Square Kilometre Array (SKA-MID). Results. The low rotation velocities of ∼5 km s−1 and ∼10 km s−1 in Pisces A and B, respectively, and their Hi content show that they are really dwarf irregular galaxies (dIrr). -
Fundamentals of Radio Astronomy
• 4.85 GHz radio image The Radio Sky at 4.85 GHz • 45 degrees wide • brightest irregular sources are clouds of ionized hydrogen The Radio Universe Dr. Chuck Higgins Middle Tennessee State University • Supernovae remnants appear as faint radio rings • Radio "stars" scattered over the sky - most are luminous radio galaxies 9 (c) National Radio Astronomy Observatory / Associated or quasars (average distance > 5 x 10 ly) Universities, Inc. / National Science Foundation • 4.85 GHz radio image The Radio Sky at 4.85 GHz • 45 degrees wide • brightest irregular sources are clouds of ionized hydrogen Outline 1.The Radio Sky and the EM Spectrum 2.Radio Telescopes 3.What We Learn and Major Discoveries 4.Sources of Radio Emission 5.Examples – Sun, Planets, Stars, Pulsars, Galaxies, etc. 6.Radio JOVE • Supernovae remnants appear as faint radio rings • Radio "stars" scattered over the sky - most are luminous radio galaxies 9 (c) National Radio Astronomy Observatory / Associated or quasars (average distance > 5 x 10 ly) Universities, Inc. / National Science Foundation Radio Astronomy the study of radio waves originating outside Earth’s atmosphere Radio Window 1 THz – 10 MHz 0.3 mm – 30 m Credit: Adapted from STScI/JHU/NASA Radio Telescopes Concept Drawing of the Square Kilometer Array, Australia Green Bank Telescope (NRAO, NSF) Fast Radio Telescope (China) 500 m dish VLA, New Mexico (NRAO, NSF) Itty Bitty Radio Telescope Radio Telescopes Radio Waves Image Credit: Windows to the Universe Radio waves = electromagnetic waves generally caused by moving charged -
First Results from the Event Horizon Telescope
First results from the Event Horizon Telescope Dom Pesce On behalf of the Event Horizon Telescope collaboration March 10, 2020 EDSU conference The goal (ca. 2017) The goal is to take a picture of a black hole The goal (ca. 2017) Subrahmanyan Chandrasekhar The goal is to take a picture of a black hole • General relativity makes a prediction for the apparent shape of a black hole “It is conceptually interesting, if not astrophysically very important, to calculate the precise apparent shape of the black hole… Unfortunately, there seems to be no hope of observing this effect.” - James Bardeen, 1973 James Bardeen Photon ring and black hole shadow The warped spacetime around a black hole causes photon trajectories to bend event horizon b photon orbit Photon ring and black hole shadow The warped spacetime around a black hole causes photon trajectories to bend The closer these trajectories get to a critical impact parameter, the more tightly wound they become Photon ring and black hole shadow The warped spacetime around a black hole causes photon trajectories to bend The closer these trajectories get to a critical impact parameter, the more tightly wound they become Photon ring and black hole shadow The warped spacetime around a black hole causes photon trajectories to bend The closer these trajectories get to a critical impact parameter, the more tightly wound they become The trajectories interior to this critical impact parameter intersect the horizon, and these collectively form the black hole “shadow” (Falcke, Melia, & Agol 2000) while the bright surrounding region constitutes the “photon ring” Adapted from: Asada et al. -
ATNF News Issue No
ATNF News Issue No. 70, April 2011 ISSN 1323-6326 CSIRO Astronomy and Space Science – undertaking world leading astronomical research and operator of the Australia Telescope National Facility. The Parkes Phased Array Feed (PAF) package, partially rotated, showing the chequerboard array minus the weather cover. The ability to invert the PAF package during and after assembly enables efficient final construction and, most importantly, safe transport and readiness for sky testing. Credit: Russ Bolton, CSIRO Cover page image Australian Square Kilometre Array Pathfinder (ASKAP) antenna construction. Credit: Antony Schinckel, CSIRO 2 Issue No. 70, April 2011 Contents From the Chief of CSIRO Astronomy and Space Science ..........................................................................................4 New Deputy Chief for CASS ........................................................................................................................................................5 Distinguished Visitors ..........................................................................................................................................................................6 Graduate Student Program.............................................................................................................................................................7 Grote Reber Gold Medal Awarded ..........................................................................................................................................8 CSIRO Chief Visits -
Jive Virtual Radio Interferometer Interferometers
Radio Astronomy an introduction Marta Burgay Overview • The birth of radio astronomy • The role of radio astronomy in astrophysics • Basic principles and instrumentation • FRBs: an (intriguing) operational example The birth of radio Astronomy 1931-1933 Karl Jansky The birth of radio Astronomy 1931-1933 Karl Jansky The first radio astronomer 1937-1947: Grote Reber built his own 9-m-diameter parabolic dish antenna in his backyard in Wheaton, Illinois The first spectral maps Reber's multi-frequency observations revealed the non-thermal nature of radio emission (UNEXPECTED!) Radio astronomy milestones 1945: Oort and Van de Hulst Radio astronomy milestones HI emission at 21 cm on 25 march 1951 with a horn antenna installed at Harvard E.M. Purcell & H.W. Ewen (Nobel 1952 for Purcell) Radio astronomy milestones HI emission at 21 cm on 25 march 1951 with a horn antenna installed at Harvard E.M. Purcell & H.W. Ewen (Nobel 1952 for Purcell) 1964: Penzias & Wilson Radio astronomy milestones HI emission at 21 cm on 25 march 1951 with a horn antenna installed at Harvard E.M. Purcell & H.W. Ewen (Nobel 1952 for Purcell) ? 1964: Penzias & Wilson Radio astronomy milestones HI emission at 21 cm on 25 march 1951 with a horn antenna installed at Harvard E.M. Purcell & H.W. Ewen (Nobel 1952 for Purcell) Robert Dickie was predicting a background signal associated with the cooling of radiation from the Big Bang Radio astronomy milestones HI emission at 21 cm on 25 march 1951 with a horn antenna installed at Harvard E.M. Purcell & H.W. Ewen (Nobel 1952 for Purcell) Cosmic Microwave Background in 1965 with a horn antenna installed at Bell’s Labs A.A.