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The Global Jet Structure of the Archetypical Quasar 3C 273
galaxies Article The Global Jet Structure of the Archetypical Quasar 3C 273 Kazunori Akiyama 1,2,3,*, Keiichi Asada 4, Vincent L. Fish 2 ID , Masanori Nakamura 4, Kazuhiro Hada 3 ID , Hiroshi Nagai 3 and Colin J. Lonsdale 2 1 National Radio Astronomy Observatory, 520 Edgemont Rd, Charlottesville, VA 22903, USA 2 Massachusetts Institute of Technology, Haystack Observatory, 99 Millstone Rd, Westford, MA 01886, USA; vfi[email protected] (V.L.F.); [email protected] (C.J.L.) 3 National Astronomical Observatory of Japan, 2-21-1 Osawa, Mitaka, Tokyo 181-8588, Japan; [email protected] (K.H.); [email protected] (H.N.) 4 Institute of Astronomy and Astrophysics, Academia Sinica, P.O. Box 23-141, Taipei 10617, Taiwan; [email protected] (K.A.); [email protected] (M.N.) * Correspondence: [email protected] Received: 16 September 2017; Accepted: 8 January 2018; Published: 24 January 2018 Abstract: A key question in the formation of the relativistic jets in active galactic nuclei (AGNs) is the collimation process of their energetic plasma flow launched from the central supermassive black hole (SMBH). Recent observations of nearby low-luminosity radio galaxies exhibit a clear picture of parabolic collimation inside the Bondi accretion radius. On the other hand, little is known of the observational properties of jet collimation in more luminous quasars, where the accretion flow may be significantly different due to much higher accretion rates. In this paper, we present preliminary results of multi-frequency observations of the archetypal quasar 3C 273 with the Very Long Baseline Array (VLBA) at 1.4, 15, and 43 GHz, and Multi-Element Radio Linked Interferometer Network (MERLIN) at 1.6 GHz. -
Radio Astronomy & Radio Telescopes
Radio Astronomy & Radio Telescopes Tasso Tzioumis ([email protected]) Australia Telescope National Facility (ATNF) sms2020, Stellenbosch 2-6 March 2020 CSIRO ASTRONOMY AND SPACE SCIENCE Radio Astronomy – ITU definition 1.13 radio astronomy: Astronomy based on the reception of radio waves of cosmic origin. 1.5 radio waves or hertzian waves: Electromagnetic waves of frequencies arbitrarily lower than 3 000 GHz, propagated in space without artificial guide. • Astronomy covers the whole electromagnetic spectrum • Radio astronomy is the “low energy” part of the spectrum é 3 000 GHz Radioastronomy & Radio telescopes | Tasso Tzioumis Radio Astronomy “special” characteristics Technical challenges • Very faint signals – measured in 10-26 W/m2/Hz (-260 dBW) • “Power collected by all radiotelescopes since the start of radio astronomy would light a 1W bulb for less than 1 second” • à Need “sensitivity” i.e. large antennas and/or arrays of many antennas • à Very susceptible to intereference • Celestial structures at all scales: from very large to very small • à Need “spatial resolution” i.e. ability to see the details at all scales • à Need large antennas and/or arrays of many antennas • Astronomical events at all timescales(from < 1ms to > millions years) & and at all spectral resolutions (from < 1 Hz to GHz) • à Need very high time and frequency resolution • à Sensitive telescopes and arrays & extreme technical challenges Radioastronomy & Radio telescopes | Tasso Tzioumis Radio Astronomy “special” characteristics Scientific challenges • Radio -
EDGES Memo #054
EDGES MEMO #054 MASSACHUSETTS INSTITUTE OF TECHNOLOGY HAYSTACK OBSERVATORY WESTFORD, MASSACHUSETTS 01886 December 1, 2009 Telephone: 781-981-5407 Fax: 781-981-0590 To: EDGES Group From: Alan E.E. Rogers Subject: Meteor scatter rates Since all the World’s designated radio quiet zones are les than 2000 km from strong radio transmitters they are subject to RFI from meteor scatter. The key parameters of meteor scatter are poorly determined. For example, theory suggests that the radar cross-section (RCS) should decrease by 20 dB per decade from head echoes but measurements typically have an even faster decline with frequency. The frequency range for significant scatter and the range of concern to radio astronomy is about 50 to 300 MHz. Some papers claim that 1012 meteors enter the Earth’s atmosphere each day while others suggest a number more like 109. In practice we observed a rate of about 1 per minute when located in a canyon (see memo #52) with sky coverage limited to elevations greater than about 25 degrees. Based on the geometry of Figure 1 this corresponds to a worldwide rate of about 107/day. Figure 2 shows the estimated burst rate as a function of elevation cut-off angle. This very sharp curve shows the advantage of limiting the low elevation response of the antenna or using the terrain to limit the elevation angle. Potential locations for EDGES are on route 205 in the canyon just before 205 enters the Catlow Valley, Oregon or about 1km West of route 205 on Skull creek road. 1 h R To solve: theta=acos( ( (R+ h)*(R+ h)+ R*R-r*r) / (2*(R+ h)*R)) a 1 b -2*R*cos(elev+90) c = -(R+h)*(R+h)+R*R r = ((- b+sqrt(b*b-4*a*c) / (2*a) ; R earth radius = 6357 km r = region where meteors form ions ,-..J 100 km Figure 1. -
CASKAR: a CASPER Concept for the SKA Phase 1 Signal Processing Sub-System
CASKAR: A CASPER concept for the SKA phase 1 Signal Processing Sub-system Francois Kapp, SKA SA Outline • Background • Technical – Architecture – Power • Cost • Schedule • Challenges/Risks • Conclusions Background CASPER Technology MeerKAT Who is CASPER? • Berkeley Wireless Research Center • Nancay Observatory • UC Berkeley Radio Astronomy Lab • Oxford University Astrophysics • UC Berkeley Space Sciences Lab • Metsähovi Radio Observatory, Helsinki University of • Karoo Array Telescope / SKA - SA Technology • NRAO - Green Bank • New Jersey Institute of Technology • NRAO - Socorro • West Virginia University Department of Physics • Allen Telescope Array • University of Iowa Department of Astronomy and • MIT Haystack Observatory Physics • Harvard-Smithsonian Center for Astrophysics • Ohio State University Electroscience Lab • Caltech • Hong Kong University Department of Electrical and Electronic Engineering • Cornell University • Hartebeesthoek Radio Astronomy Observatory • NAIC - Arecibo Observatory • INAF - Istituto di Radioastronomia, Northern Cross • UC Berkeley - Leuschner Observatory Radiotelescope • Giant Metrewave Radio Telescope • University of Manchester, Jodrell Bank Centre for • Institute of Astronomy and Astrophysics, Academia Sinica Astrophysics • National Astronomical Observatories, Chinese Academy of • Submillimeter Array Sciences • NRAO - Tucson / University of Arizona Department of • CSIRO - Australia Telescope National Facility Astronomy • Parkes Observatory • Center for Astrophysics and Supercomputing, Swinburne University -
Next Generation Radio Arrays
NextNext GenerationGeneration RadioRadio ArraysArrays Dr.Dr. FrankFrank D.D. LindLind MITMIT HaystackHaystack ObservatoryObservatory (with acknowledgement to my colleagues who contribute to these efforts...) [McKay-Bukowski, et al., 2014] contact info : Frank D. Lind MIT Haystack Observatory Route 40 Westford MA, 01886 email - [email protected] DeepDeep MemoryMemory Solid state memory capacity will exceed our data storage requirements. Deep memory instruments will become possible. Store all data from every element for the life of a radio array... Intel + Micron 3D Flash Intel XPoint memory Keon Jae Lee of the Korea Advanced Institute of Science and Technology (KAIST) ConnectedConnected WorldWorld Wireless networks will be global and even replace the wires. Disconnected, self networking, and software realized instrumentation Sparse global radio arrays, deployable dense arrays, and ad-hoc arrays DisappearingDisappearing SensorsSensors Integration will become extreme and include quantum referenced sensors Receivers in connectors, cloud computers on a chip, really good clocks Energy harvesting and low power near field wireless data Self coherent arrays, personal passive radar, the ionosphere as a sensor Deployable Low Power Radio Platforms Instruments in ~ 10W power envelopes. Future systems will use ~ 1W of power total. Zero infrastructure radio science instrumentation Software radio and radar technology Solar and battery power Low power computing for data acquisition Intelligent control software Mahali Array (during build out) Deep -
Real-Time High Volume Data Transfer and Processing for E-VLBI
Real-time high volume data transfer and processing for e-VLBI Yasuhiro Koyama, Tetsuro Kondo, Hiroshi Takeuchi, Moritaka Kimura (Kashima Space Research Center, NICT, Japan) and Masaki Hirabaru (New Generation Network Research Center, NICT, Japan) OutlineOutline What is e-VLBI? Why e-VLBI is necessary? How? – K5 VLBI System ~ Standardization – Network Test Experiments – June 2004 : Near-Realtime UT1 Estimation – January 2005 : Realtime Processing Demo Future Plan Traditional VLBI The Very-Long Baseline Interferometry (VLBI) Technique (with traditional data recording) The Global VLBI Array (up to ~20 stations can be used simultaneously) WhatWhat isis ee--VVLBI?LBI? VLBI=Very Long Baseline Interferometry Correlator Radio Telescope Network Correlator Radio Telescope Shipping Data Media e-VLBI (Tapes/Disks) Conventional VLBI VLBIVLBI ApplicationsApplications Geophysics and Plate Tectonics Kashima-Kauai鹿島-ハワイの基線長変化 Baseline Length -63.5 ± 0.5 mm/year 400 200 0 -200 基線長(mm) -400 5400km 5400km Fairbanksアラスカ 1984 1986 1988 1990 1992 1994 Fairbanks-Kauaiアラスカ-ハワイの基線長変化年 Baseline Length 4700km 4700km -46.1 ± 0.3 mm/year Kashima鹿島 400 5700km 200 Kauaiハワイ 0 -200 基線長(mm) -400 1984 1986 1988 1990 1992 1994 Kashima-Fairbanks鹿島-アラスカの基線長変化年 Baseline Length 1.3 ± 0.5 mm/year 400 200 0 -200 基線長(mm) -400 1984 1986 1988 1990 1992 1994 年 VLBIVLBI ApplicationsApplications (2)(2) Radio Astronomy : High Resolution Imaging, Astro-dynamics Reference Frame : Celestial / Terrestrial Reference Frame Earth Orientation Parameters, Dynamics of Earth’s Inner Core -
Istituto Di Radioastronomia Inaf
ISTITUTO DI RADIOASTRONOMIA INAF STATUS REPORT October 2007 http://www.ira.inaf.it/ Chapter 1. STRUCTURE AND ORGANIZATION The Istituto di Radioastronomia (IRA) is presently the only INAF structure with divisions distributed over the national territory. Such an organization came about because IRA was originally a part of the National Council of Research (CNR), which imposed the first of its own reforms in 2001. The transition from CNR to INAF began in 2004 and was completed on January 1st , 2005. The Institute has its headquarters in Bologna in the CNR campus area, and two divisions in Firenze and Noto. The Medicina station belongs to the Bologna headquarters. A fourth division is foreseen in Cagliari at the Sardinia Radiotelescope site. The IRA operates 3 radio telescopes: the Northern Cross Radio Telescope (Medicina), and two 32-m dishes (Medicina and Noto), which are used primarily for Very Long Baseline Interferometry (VLBI) observations. The IRA leads the construction of the Sardinia Radio Telescope (SRT), a 64-m dish of new design. This is one of the INAF large projects nowadays. The aims of the Institute comprise: - the pursuit of excellence in many research areas ranging from observational radio astronomy, both galactic and extragalactic, to cosmology, to geodesy and Earth studies; - the design and management of the Italian radio astronomical facilities; - the design and fabrication of instrumentation operating in bands from radio to infrared and visible. Main activities of the various sites include: Bologna: The headquarters are responsible for the institute management and act as interface with the INAF central headquarters in Roma. Much of the astronomical research is done in Bologna, with major areas in cosmology, extragalactic astrophysics, star formation and geodesy. -
EVGA2021 Making VLBI Great Again!
25th European VLBI Group for Geodesy and Astronomy Working Meeting 14-18 March 2021 Cyberspace Information and book of abstracts 2021-03-03 EVGA2021 Making VLBI Great Again! European VLBI Group For Geodesy and Astrometry This page is intentionally left blank. II EVGA2021 information Scientific Organizing Committee (SOC) Simone Bernhart (Reichert GmbH/BKG/MPIfR Bonn) • Sigrid B¨ohm(Technische Universit¨atWien) • Susana Garcia-Espada (Kartverket) • Anastasiia Girdiuk (BKG Frankfurt) • R¨udigerHaas (Chalmers University of Technology) • Karine Le Bail (Chalmers University of Technology) • Nataliya Zubko (Finnish Geospatial Research Institute) • Virtual Organizing Committee (VOC) Periklis-Konstantinos Diamantidis (Chalmers University of Technology) • Susana Garcia-Espada (Kartverket) • R¨udigerHaas (Chalmers University of Technology) • Karine Le Bail (Chalmers University of Technology) • Series of events during the EVGA2021 Date Time Event 14 March UT 16:00-18:00 Icebreaker party 15 March UT 10:50-17:00 EVGA2021-day-1 16 March UT 11:00-17:00 EVGA2021-day-2 17 March UT 11:00-17:00 EVGA2021-day-3 18 March UT 11:00-14:45 EVGA2021-day-4 18 March UT 14:45-18:30 IVS Analysis Workshop All events will be in Cyberspace, i.e. virtually, and the corresponding information to access the virtual events will be provided via email to the participants. Interested persons not presenting themselves at the EVGA2021, but still interested in attending the oral presentations, are asked to get in to contact with the VOC via email to receive further instructions. III -
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. -
The NRAO Program Operating Plan
NATIONAL RADIO ASTRONOMY OBSERVATORY PROGRAM OPERATING PLAN FY 20 12 Associated Univ rsities. Inc. '>1> . r " " , " " , " r 'rr. '°S 9 g[[5 44 t " - , The NRAO Program Operating Plan FY 2012 Revised: March 2012 The National Radio Astronomy Observatory is a facility of the National Science Foundation operated under cooperative agreement by Associated Universities, Inc. Table of Contents Executive Summary .......................................................................................................................................... 1 1. Overview ..................................................................................................................................................... 3 1.1 Introduction to the Plan .............................................................................................................................. 3 1.2 Structure of the POP ................................................................................................................................... 4 1.3 Financial and Budget Considerations ........................................................................................................ 4 2. Science Programs FY 2012 ...................................................................................................................... 6 3. Optimizing Science Impact: Observatory Science Operations ........................................................ 9 3.1 Shared Services ............................................................................................................................................. -
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. -
Table of Contents - 1 - - 2
Table of contents - 1 - - 2 - Table of Contents Foreword 5 1. The European Consortium for VLBI 7 2. Scientific highlights on EVN research 9 3. Network Operations 35 4. VLBI technical developments and EVN operations support at member institutes 47 5. Joint Institute for VLBI in Europe (JIVE) 83 6. EVN meetings 105 7. EVN publications in 2007-2008 109 - 3 - - 4 - Foreword by the Chairman of the Consortium The European VLBI Network (EVN) is the result of a collaboration among most major radio observatories in Europe, China, Puerto Rico and South Africa. The large radio telescopes hosted by these observatories are operated in a coordinated way to perform very high angular observations of cosmic radio sources. The data are then correlated by using the EVN correlator at the Joint Institute for VLBI in Europe (JIVE). The EVN, when operating as a single astronomical instrument, is the most sensitive VLBI array and constitutes one of the major scientific facilities in the world. The EVN also co-observes with the Very Long Baseline Array (VLBA) and other radio telescopes in the U.S., Australia, Japan, Russia, and with stations of the NASA Deep Space Network to form a truly global array. In the past, the EVN also operated jointly with the Japanese space antenna HALCA in the frame of the VLBI Space Observatory Programme (VSOP). The EVN plans now to co-observe with the Japanese space 10-m antenna ASTRO-G, to be launched by 2012, within the frame of the VSOP-2 project. With baselines in excess of 25.000 km, the space VLBI observations provide the highest angular resolution ever achieved in Astronomy.