Difference imaging and multi-channel Clean
|
|
- Cori Bruce
- 5 years ago
- Views:
Transcription
1 Difference imaging and multi-channel Clean Olaf Wucknitz Algorithms 2008, Oxford, 1 3 Dezember 2008
2 Finding gravitational lenses through variability [ Kochanek et al. (2006) ] small field in SDSS: one candidate, no lens [ Lacki et al. (2008) ] titlepage introduction summary contents back forward previous next fullscreen 1
3 Optical difference imaging difference original image convolution kernel reference image [ Alard & Lupton (1998) ] titlepage introduction summary contents back forward previous next fullscreen 2
4 Radio difference imaging UV epoch 1 CLEAN convolve crap UV epoch 2 CLEAN convolve UV epoch 1 CLEAN convolve crap UV epoch 2 UV epoch 1 difference + convolve mean UV epoch 2 CLEAN convolve difference titlepage introduction summary contents back forward previous next fullscreen 3
5 Related problem: combining different arrays UV epoch 1 CLEAN convolve + crap UV epoch 2 CLEAN convolve UV epoch 1 + CLEAN convolve crap UV epoch 2 UV epoch 1 difference + convolve mean UV epoch 2 CLEAN convolve difference titlepage introduction summary contents back forward previous next fullscreen 4
6 Notation sky brightness distribution I(l, m) I visibilities Ĩ(u, v) Ĩ perfect measurement Fourier transform vectors Ĩ µ = j A µ j I j A µ j = e 2πi(l,m) j (u,v) µ Ĩ = AI residuals R 2 = (AI Ĩ) W(AI Ĩ) natural weighting W = diag(σ 2 j ) R 2 = χ 2 titlepage introduction summary contents back forward previous next fullscreen 5
7 Lazy interferometrists do it in image space expand R 2 = Ĩ WĨ + I A WAI 2I A WĨ define (using w = Tr W) dirty beam dirty map B = A WA w I D = A WĨ w residuals derived in image space R 2 = const + w(i BI 2I I D ) minimum BI = I D } {{ } R 2 titlepage introduction summary contents back forward previous next fullscreen 6
8 CLEAN as maximum likelihood fitting add components to the model I minimize residuals in each step empty model plus component I j optimal flux R 2 = I 2 j 2I j I D j I j = I D j residuals for optimal flux R 2 = I D 2 j optimal position: peak in dirty map subtract shifted beam from dirty map, start over titlepage introduction summary contents back forward previous next fullscreen 7
9 Simultaneous CLEANing two epochs Ĩ 1 and Ĩ2 two models/maps I 1 and I 2 combined residuals R 2 = const + w 1 (I 1 B 1 I 1 2I 1 I D1 ) + w 2 (I 2 B 2 I 2 2I 2 I D2 ) next component at same position in 1 and 2 fluxes independent optimal fluxes I D1 and I D2 optimal position maximum of w 1 I D w 2 I D 2 2 titlepage introduction summary contents back forward previous next fullscreen 8
10 Need for difference-clean disadvantages of simultaneous CLEANing deconvolution errors still independent no control over mean and difference alternative approach two channels I + and I I + = 1 2 (I 1 + I 2 ) I = 1 2 (I 1 I 2 ) dirty maps I D+ = w 1 I D1 + w 2 I D2 w 1 + w 2 I D = w 1 I D1 w 2 I D2 w 1 + w 2 titlepage introduction summary contents back forward previous next fullscreen 9
11 D-CLEAN procedure next component in either I + or I { 2 ID residuals R 2 = const (w 1 + w 2 ) + for + for I D 2 subtract according to ( ID+ I D ) = ( B B )( I+ B B I ) I + and I not independent dirty beams B = w 1 B 1 + w 2 B 2 w 1 + w 2 B = w 1 B 1 w 2 B 2 w 1 + w 2 titlepage introduction summary contents back forward previous next fullscreen 10
12 An experiment: VLA-like uv coverage, scale 1:4 input convolved CLEAN 1 2 titlepage introduction summary contents back forward previous next fullscreen 11
13 Alternative methods CLEAN simultaneous D-CLEAN + titlepage introduction summary contents back forward previous next fullscreen 12
14 Alternative methods: residual errors CLEAN simultaneous D-CLEAN + titlepage introduction summary contents back forward previous next fullscreen 13
15 Combining different arrays: input input convolved CLEAN 1 2 titlepage introduction summary contents back forward previous next fullscreen 14
16 Combining different arrays: output combined simultaneous D-CLEAN + + titlepage introduction summary contents back forward previous next fullscreen 15
17 Two-channel CLEANing of real data target lens B two bright images Einstein ring two VLA-A observations with Pie Town use 1 IF titlepage introduction summary contents back forward previous next fullscreen 16
18 Differencing images of B CLEAN simultaneous D-CLEAN titlepage introduction summary contents back forward previous next fullscreen 17
19 Combined images of B CLEAN combined simultaneous D-CLEAN titlepage introduction summary contents back forward previous next fullscreen 18
20 Test with simulated VLBA data uv coverage and model from real observations of Virgo A (thanks to Yuri Kovalev) [ details in Kovalev et al. (2007) ] following slides: simulation without/with noise, two epochs, slightly different uv coverage titlepage introduction summary contents back forward previous next fullscreen 19
21 Results for simulated data: no noise difference of Clean maps difference-clean mean Clean map titlepage introduction summary contents back forward previous next fullscreen 20
22 Results for simulated data: with noise difference of Clean maps difference-clean mean Clean map titlepage introduction summary contents back forward previous next fullscreen 21
23 Alternative bases so far: two epochs constant part (sum) variable part (difference) many epochs constant part one additional part for each epoch continuous observation (or ν instead of t) constant part linear slope higher derivatives or general orthogonal polynomials, or... titlepage introduction summary contents back forward previous next fullscreen 22
24 Constant + linear in frequency dirty maps I D (n) = ν w(ν)ν n I D (ν) ν w(ν) dirty beams B (n) = ν w(ν)ν n B(ν) ν w(ν) convolution equation up to linear order ( ID (0) I D (1) ) = ( ) (I B (0) B (1) ) (0) B (1) B (2) I (1) previous MFS methods only use I D (0) = B (0) I (0) + B (1) I (1) [ Conway et al. (1990), Sault & Wieringa (1994) ] titlepage introduction summary contents back forward previous next fullscreen 23
25 ATCA observations of Pictor-A 4800 / 4928 MHz [ data from Emil Lenc ] titlepage introduction summary contents back forward previous next fullscreen 24
26 Pictor-A: difference MHz difference of Clean maps difference channel of D-Clean titlepage introduction summary contents back forward previous next fullscreen 25
27 Pictor-A: correct for variability with AIPS (4800 MHz) five epochs with ATCA (different configurations) common model + variable parts titlepage introduction summary contents back forward previous next fullscreen 26
28 Summary etc these tasks difference imaging, variability combine different arrays / epochs wide-band imaging with spectral indices multi-resolution / multi-scale Clean have in common that multi-channel output is needed channels do not always correspond to parts of the data want Clean regularisation for output channels need to deconvolve everything simultaneously developing multi-channel Clean first tests encouraging work in progress titlepage introduction summary contents back forward previous next fullscreen 27
29 Contents 1 Finding gravitational lenses through variability 2 Optical difference imaging 3 Radio difference imaging 4 Related problem: combining different arrays 5 Notation 6 Lazy interferometrists do it in image space 7 CLEAN as maximum likelihood fitting 8 Simultaneous CLEANing 9 Need for difference-clean 10 D-CLEAN procedure 11 An experiment: VLA-like uv coverage, scale 1:4 12 Alternative methods 13 Alternative methods: residual errors 14 Combining different arrays: input 15 Combining different arrays: output 16 Two-channel CLEANing of real data 17 Differencing images of B titlepage introduction summary contents back forward previous next fullscreen 28
30 18 Combined images of B Test with simulated VLBA data 20 Results for simulated data: no noise 21 Results for simulated data: with noise 22 Alternative bases 23 Constant + linear in frequency 24 ATCA observations of Pictor-A 4800 / 4928 MHz 25 Pictor-A: difference MHz 26 Pictor-A: correct for variability with AIPS (4800 MHz) 27 Summary etc 28 Contents titlepage introduction summary contents back forward previous next fullscreen 29
The Source and Lens of B
The Source and Lens of B0218+357 New Polarization Radio Data to Constrain the Source Structure and H 0 with LensCLEAN Olaf Wucknitz Astrophysics Seminar Potsdam University, Germany 5 July 2004 The source
More informationE-MERLIN and EVN/e-VLBI Capabilities, Issues & Requirements
E-MERLIN and EVN/e-VLBI Capabilities, Issues & Requirements e-merlin: capabilities, expectations, issues EVN/e-VLBI: capabilities, development Requirements Achieving sensitivity Dealing with bandwidth,
More informationPrinciples of Interferometry. Hans-Rainer Klöckner IMPRS Black Board Lectures 2014
Principles of Interferometry Hans-Rainer Klöckner IMPRS Black Board Lectures 2014 acknowledgement Mike Garrett lectures James Di Francesco crash course lectures NAASC Lecture 5 calibration image reconstruction
More informationNon-Imaging Data Analysis
Outline 2 Non-Imaging Data Analysis Greg Taylor Based on the original lecture by T.J. Pearson Introduction Inspecting visibility data Model fitting Some applications Superluminal motion Gamma-ray bursts
More informationImaging Capability of the LWA Phase II
1 Introduction Imaging Capability of the LWA Phase II Aaron Cohen Naval Research Laboratory, Code 7213, Washington, DC 2375 aaron.cohen@nrl.navy.mil December 2, 24 The LWA Phase I will consist of a single
More informationThe magnification theorem
The magnification theorem Olaf Wucknitz wucknitz@astro.uni-bonn.de Three decades of gravitational lenses, JENAM, 21 April 2009 2.5 decades of the magnification theorem General theorems in lensing odd image
More informationThe Australia Telescope. The Australia Telescope National Facility. Why is it a National Facility? Who uses the AT? Ray Norris CSIRO ATNF
The Australia Telescope National Facility The Australia Telescope Ray Norris CSIRO ATNF Why is it a National Facility? Funded by the federal government (through CSIRO) Provides radio-astronomical facilities
More informationRadio Interferometry and Aperture Synthesis
Radio Interferometry and Aperture Synthesis Phil gave a detailed picture of homodyne interferometry Have to combine the light beams physically for interference Imposes many stringent conditions on the
More informationIs there a magnification paradox in gravitational lensing?
Is there a magnification paradox in gravitational lensing? Olaf Wucknitz wucknitz@astro.uni-bonn.de Astrophysics seminar/colloquium, Potsdam, 26 November 2007 Is there a magnification paradox in gravitational
More informationNon-Closing Offsets on the VLA. R. C. Walker National Radio Astronomy Observatory Charlottesville VA.
VLA SCIENTIFIC MEMORANDUM NO. 152 Non-Closing Offsets on the VLA R. C. Walker National Radio Astronomy Observatory Charlottesville VA. March 1984 Recent efforts to obtain very high dynamic range in VLA
More informationImaging with the SKA: Comparison to other future major instruments
1 Introduction Imaging with the SKA: Comparison to other future major instruments A.P. Lobanov Max-Planck Institut für Radioastronomie, Bonn, Germany The Square Kilometer Array is going to become operational
More informationNew calibration sources for very long baseline interferometry in the 1.4-GHz band
New calibration sources for very long baseline interferometry in the 1.4-GHz band M K Hailemariam 1,2, M F Bietenholz 2, A de Witt 2, R S Booth 1 1 Department of Physics, University of Pretoria, South
More informationDeconvolving Primary Beam Patterns from SKA Images
SKA memo 103, 14 aug 2008 Deconvolving Primary Beam Patterns from SKA Images Melvyn Wright & Stuartt Corder University of California, Berkeley, & Caltech, Pasadena, CA. ABSTRACT In this memo we present
More informationRadio Interferometry Fundamentals. John Conway Onsala Space Obs and Nordic ALMA ARC-node
Radio Interferometry Fundamentals John Conway Onsala Space Obs and Nordic ALMA ARC-node So far discussed only single dish radio/mm obs Resolution λ/d, for D=20m, is 30 at mm-wavelengths and 30 (diameter
More informationMerging Single-Dish Data
Lister Staveley-Smith Narrabri Synthesis Workshop 15 May 2003 1 Merging Single-Dish Data!Bibliography!The short-spacing problem!examples Images Power spectrum!fourier (or UV) plane.v. sky (or image) plane
More information2-D Images in Astronomy
2-D Images in Astronomy ZTF camera FOV is 50 square degrees. Largest camera on >1m telescope by area in the world. Or, to make a little clearer, here s Orion. The white box is the ZTF imaging area. The
More informationFundamentals of radio astronomy
Fundamentals of radio astronomy Sean Dougherty National Research Council Herzberg Institute for Astrophysics Apologies up front! Broad topic - a lot of ground to cover (the first understatement of the
More informationInformation Field Theory. Torsten Enßlin MPI for Astrophysics Ludwig Maximilian University Munich
Information Field Theory Torsten Enßlin MPI for Astrophysics Ludwig Maximilian University Munich Information Field Theory signal field: degrees of freedom data set: finite additional information needed
More informationHughes et al., 1998 ApJ, 505, 732 : ASCA. Westerlund, 1990 A&ARv, 2, 29 : Distance to LMC 1 ) ) (ergs s F X L X. 2 s 1. ) (ergs cm
1 SUMMARY 1 SNR 0525-66.1 1 Summary Common Name: N 49 Distance: 50 kpc (distance to LMC, Westerlund(1990) ) Position of Central Source (J2000): ( 05 25 59.9, -66 04 50.8 ) X-ray size: 85 x 65 Description:??
More information1. INTRODUCTION 2. SOURCE SELECTION
THE ASTROPHYSICAL JOURNAL SUPPLEMENT SERIES, 124:285È381, 1999 October ( 1999. The American Astronomical Society. All rights reserved. Printed in U.S.A. VLA IMAGES AT 5 GHz OF 212 SOUTHERN EXTRAGALACTIC
More informationWide-Field Imaging: I
Wide-Field Imaging: I S. Bhatnagar NRAO, Socorro Twelfth Synthesis Imaging Workshop 010 June 8-15 Wide-field imaging What do we mean by wide-field imaging W-Term: D Fourier transform approximation breaks
More informationCompressed Sensing: Extending CLEAN and NNLS
Compressed Sensing: Extending CLEAN and NNLS Ludwig Schwardt SKA South Africa (KAT Project) Calibration & Imaging Workshop Socorro, NM, USA 31 March 2009 Outline 1 Compressed Sensing (CS) Introduction
More informationVLBI long and wide. AIfA The far side of Bonn LOFAR. VLBI long and wide. LOFAR is VLBI. LOFAR resolution. International LOFAR stations
VLBI long and wide International LOFAR and efficient wide-field mapping Olaf Wucknitz wucknitz@astro.uni-bonn.de ICRAR, Curtin University of Technology, 22nd October 2010 AIfA The far side of Bonn If we
More informationFARADAY ROTATION MEASURE SYNTHESIS OF UGC 10288, NGC 4845, NGC 3044
FARADAY ROTATION MEASURE SYNTHESIS OF UGC 10288, NGC 4845, NGC 3044 PATRICK KAMIENESKI DYLAN PARÉ KENDALL SULLIVAN PI: DANIEL WANG July 21, 2016 Madison, WI OUTLINE Overview of RM Synthesis: Benefits Basic
More informationCan we do this science with SKA1-mid?
Can we do this science with SKA1-mid? Let s start with the baseline design SKA1-mid expected to go up to 3.05 GHz Proposed array configuration: 133 dishes in ~1km core, +64 dishes out to 4 km, +57 antennas
More informationExtending and Exploring the 2cm Survey Sample. Eduardo Ros (MPIfR) and the 2cm Survey Team 7th EVN Symposium Toledo (not in Ohio) 2004/10/12
Extending and Exploring the 2cm Survey Sample Eduardo Ros (MPIfR) and the 2cm Survey Team 7th EVN Symposium Toledo (not in Ohio) 2004/10/12 The 2cm Survey Collaboration Team Members NRAO: Ken I. Kellermann,
More informationImage Processing in Astronomy: Current Practice & Challenges Going Forward
Image Processing in Astronomy: Current Practice & Challenges Going Forward Mario Juric University of Washington With thanks to Andy Connolly, Robert Lupton, Ian Sullivan, David Reiss, and the LSST DM Team
More informationarxiv:astro-ph/ v2 6 Nov 2005
Astronomy & Astrophysics manuscript no. paper October, 8 (DOI: will be inserted by hand later) VLBI phase reference observations of the gravitational lens JVAS B8+57 Rupal Mittal, Richard Porcas, Olaf
More informationCentral image detection with VLBI
Central image detection with VLBI Zhang Ming Xinjiang Astronomical Observatory, Chinese Academy of Sciences RTS meeting, Manchester, 2012.04.19 Strong lensing nomenclature Structure formation at subgalactic
More informationSolar System Objects. Bryan Butler National Radio Astronomy Observatory
Solar System Objects Bryan Butler National Radio Astronomy Observatory Atacama Large Millimeter/submillimeter Array Expanded Very Large Array Robert C. Byrd Green Bank Telescope Very Long Baseline Array
More informationShort-Spacings Correction From the Single-Dish Perspective
Short-Spacings Correction From the Single-Dish Perspective Snezana Stanimirovic & Tam Helfer (UC Berkeley) Breath and depth of combining interferometer and single-dish data A recipe for observing extended
More informationBINGO simulations and updates on the performance of. the instrument
BINGO simulations and updates on the performance of BINGO telescope the instrument M.-A. Bigot-Sazy BINGO collaboration Paris 21cm Intensity Mapping Workshop June 2014 21cm signal Observed sky Credit:
More informationarxiv: v1 [astro-ph.ga] 22 Nov 2018
Preprint 26 November 2018 Compiled using MNRAS LATEX style file v3.0 arxiv:1811.09152v1 [astro-ph.ga] 22 Nov 2018 A novel search for gravitationally lensed radio sources in wide-field VLBI imaging from
More informationNext Generation VLA Memo. 41 Initial Imaging Tests of the Spiral Configuration. C.L. Carilli, A. Erickson March 21, 2018
Next Generation VLA Memo. 41 Initial Imaging Tests of the Spiral Configuration C.L. Carilli, A. Erickson March 21, 2018 Abstract We investigate the imaging performance of the Spiral214 array in the context
More informationSequence Obs ID Instrument Exposure uf Exposure f Date Observed Aimpoint (J2000) (ks) (ks) (α, δ)
1 SUMMARY 1 G120.1+01.4 1 Summary Common Name: Tycho s Distance: 2.4 kpc ( Chevalier et al., 1980 ) Center of X-ray emission (J2000): ( 00 25 19.9, 64 08 18.2 ) X-ray size: 8.7 x8.6 Description: 1.1 Summary
More informationVery Large Array Sky Survey
1 Very Large Array Sky Survey Technical Implementation & Test Plan Casey Law, UC Berkeley Galactic Center (Survey) Multiwavelength Image Credit: X-ray: NASA/UMass/D.Wang et al., Radio: N RAO/AUI/NSF/NRL/N.Kassim,
More informationRadio Astronomy Project. VLA and VLBA Observations of AGN
Astronomy-423: Radio Astronomy Professor: Greg Taylor Spring 2006 Radio Astronomy Project VLA and VLBA Observations of AGN Adam Johnson Cristina Rodríguez Introduction It is important to observe radio
More informationForegrounds for observations of the high redshift global 21 cm signal
Foregrounds for observations of the high redshift global 21 cm signal Geraint Harker 28/10/2010 Fall Postdoc Symposium 1 The hydrogen 21cm line The hydrogen 21cm (1420MHz) transition is a forbidden transition
More informationInterferometry of Solar System Objects
Interferometry of Solar System Objects Bryan Butler National Radio Astronomy Observatory Atacama Large Millimeter/submillimeter Array Expanded Very Large Array Robert C. Byrd Green Bank Telescope Very
More informationGravitational lensing at the highest angular resolution
Gravitational lensing at the highest angular resolution John McKean! (SHARP) Matus Rybak, Cristiana Spingola, Simona Vegetti, Matt Auger, Chris Fassnacht, Neal Jackson, David Lagattuta, Leon Koopmans!
More informationAn Accurate, All-Sky, Absolute, Low Frequency Flux Density Scale
An Accurate, All-Sky, Absolute, Low Frequency Flux Density Scale Rick Perley, Bryan Butler (NRAO) Joe Callingham (U. Sydney) Atacama Large Millimeter/submillimeter Array Expanded Very Large Array Robert
More information=> most distant, high redshift Universe!? Consortium of international partners
LOFAR LOw Frequency Array => most distant, high redshift Universe!? Consortium of international partners Dutch ASTRON USA Haystack Observatory (MIT) USA Naval Research Lab `best site = WA Novel `technology
More informationImage Reconstruction in Radio Interferometry
Draft January 28, 2008 Image Reconstruction in Radio Interferometry S.T. Myers National Radio Astronomy Observatory, P.O. Box O, Socorro, NM 87801 and Los Alamos National Laboratory, Los Alamos, NM 87545
More informationConfusion, the sky model and realistic simulations
Confusion, the sky model and realistic simulations Randall Wayth (CfA) with team Greenhill (Greenhill, Mitchell, Sault) team MAPS (Doeleman, Bhat) Ashes Update: England all out for 350. Australia wins
More informationStatistical inversion of the LOFAR Epoch of Reionization experiment data model
Statistical inversion of the LOFAR Epoch of Reionization experiment data model ASTRON, Oude Hoogeveensedijk 4, 7991 PD, Dwingeloo, the Netherlands Kapteyn Astronomical Institute, Landleven 12, 9747 AD,
More informationImaging, Deconvolution & Image Analysis I. Theory. (IRAM/Obs. de Paris) 7 th IRAM Millimeter Interferometry School Oct. 4 - Oct.
Imaging, Deconvolution & Image Analysis I. Theory Jérôme PETY (IRAM/Obs. de Paris) 7 th IRAM Millimeter Interferometry School Oct. 4 - Oct. 8 2010, Grenoble Scientific Analysis of a mm Interferometer Output
More information154 MHz detection of faint, polarised flares from UV Ceti
154 MHz detection of faint, polarised flares from UV Ceti Christene Lynch University of Sydney/CAASTRO Collaborators: Emil Lenc, University of Sydney/CAASTRO Tara Murphy, University of Sydney/CAASTRO David
More informationMulti-frequency imaging of Cygnus A with LOFAR
Netherlands Institute for Radio Astronomy Multi-frequency imaging of Cygnus A with LOFAR John McKean (ASTRON) and all the imaging busy week team! ASTRON is part of the Netherlands Organisation for Scientific
More informationPoS(11th EVN Symposium)084
Analysis of Potential VLBI Southern Hemisphere Radio Calibrators and Michael Bietenholz Hartebeesthoek Radio Astronomy Observatory P.O. Box 443 Krugersdorp 174 South Africa E-mail: alet@hartrao.ac.za The
More informationProbing a massive radio galaxy with gravitational lensing
Mon. Not. R. Astron. Soc. 384, 1701 1710 (2008) doi:10.1111/j.1365-2966.2007.12831.x Probing a massive radio galaxy with gravitational lensing A. More, 1 J. P. McKean, 1 T. W. B. Muxlow, 2 R. W. Porcas,
More informationQuantifying and mitigating correlated noise between formed beams on the ASKAP Phased Array Feeds
Quantifying and mitigating correlated noise between formed beams on the ASKAP Phased Array Feeds Ian Heywood,PaoloSerra,AidanHotan,DavidMcConnell CSIRO Astronomy & Space Science Abstract Pairs of beams
More informationRadio Afterglows. What Good are They? Dale A. Frail. National Radio Astronomy Observatory. Gamma Ray Bursts: The Brightest Explosions in the Universe
Radio Afterglows What Good are They? Dale A. Frail National Radio Astronomy Observatory Gamma Ray Bursts: The Brightest Explosions in the Universe The 2 nd Harvard-Smithsonian Conference on Theoretical
More informationASTR240: Radio Astronomy
ASTR240: Radio Astronomy HW#3 Due Feb 27, 2013 Problem 1 (4 points) (Courtesy J. J. Condon & S. M. Ransom) The GBT (Green Bank Telescope, a steerable radio telescope roughly the size of a football field
More informationThe Radio Sky at Meter Wavelengths:
: Foregrounds for 21-cm Cosmology Michael W. Eastwood (Caltech) on behalf of the OVRO-LWA collaboration Cosmological Signals from Cosmic Dawn to the Present February 8, 2018 N 1 / 21 Caltech Gregg Hallinan
More informationarxiv:astro-ph/ v1 27 Mar 2004
Future Directions in High Resolution Astronomy: The 10th Anniversary of the VLBA ASP Conference Series, Vol. ***, 2004 J. D. Romney & M. J. Reid (eds.) 21st Century VLBI: Deep Wide-Field Surveys arxiv:astro-ph/0403642v1
More informationarxiv:astro-ph/ v1 27 Aug 2001
AMiBA 2001: High-z Clusters, Missing Baryons, and CMB Polarization ASP Conference Series, Vol. 999, 2002 L-W Chen, C-P Ma, K-W Ng and U-L Pen, eds ATCA and CMB anisotropies arxiv:astro-ph/0108409v1 27
More informationIntroduction to Interferometry
Introduction to Interferometry Ciro Pappalardo RadioNet has received funding from the European Union s Horizon 2020 research and innovation programme under grant agreement No 730562 Radioastronomy H.Hertz
More informationThe imaging capabilities of the Frequency Agile Solar Radiotelescope
The imaging capabilities of the Frequency Agile Solar Radiotelescope Stephen M. White a, Jeongwoo Lee b, Markus J. Aschwanden c, and Timothy S. Bastian d a Dept. of Astronomy, Univ. of Maryland, College
More informationMethanol absorption in PKS B at milliarcsecond scales
Advance Access publication 2016 December 19 doi:10.1093/mnras/stw3295 Methanol absorption in PKS B1830 211 at milliarcsecond scales M. A. Marshall, 1 S. P. Ellingsen, 1 J. E. J. Lovell, 1 J. M. Dickey,
More informationSquare Kilometre Array Science Data Challenge 1
Square Kilometre Array Science Data Challenge 1 arxiv:1811.10454v1 [astro-ph.im] 26 Nov 2018 Anna Bonaldi & Robert Braun, for the SKAO Science Team SKA Organization, Jodrell Bank, Lower Withington, Macclesfield,
More informationEnergy Sources of the Far IR Emission of M33
Energy Sources of the Far IR Emission of M33 Hinz, Reike et al., ApJ 154: S259 265 (2004). Presented by James Ledoux 24 µm 70 µm 160 µm Slide 1 M33 Properties Distance 840kpc = 2.7 Mlyr (1'' ~ 4 pc) Also
More informationTHE VLA GALACTIC PLANE SURVEY
Accepted for publication in The Astronomical Journal Preprint typeset using L A TEX style emulateapj v. 11/26/04 THE VLA GALACTIC PLANE SURVEY J. M. Stil 1 and A. R. Taylor 1, J. M. Dickey 2,3 and D. W.
More informationReduction procedure of long-slit optical spectra. Astrophysical observatory of Asiago
Reduction procedure of long-slit optical spectra Astrophysical observatory of Asiago Spectrograph: slit + dispersion grating + detector (CCD) It produces two-dimension data: Spatial direction (x) along
More informationAnalysis of the Hydrogen Gas Distribution in the Galaxy HIZSS 3
Analysis of the Hydrogen Gas Distribution in the Galaxy HIZSS 3 Lance Edens Advisor: Dr. Patricia Henning Honors Thesis University of New Mexico Department of Physics and Astronomy April 21, 2006 Abstract
More informationThe highest redshift radio quasar as seen with
The highest redshift radio quasar as seen with the EVN & the VLA S. Frey (FÖMI SGO, H) Z. Paragi (JIVE, NL) L. Mosoni (Konkoly Obs., H) L.I. Gurvits (JIVE, NL) 7th EVN Symposium, 12-15 Oct 2004, Toledo
More informationFourier phase analysis in radio-interferometry
Fourier phase analysis in radio-interferometry François Levrier Ecole Normale Supérieure de Paris In collaboration with François Viallefond Observatoire de Paris Edith Falgarone Ecole Normale Supérieure
More informationLow-frequency radio astronomy and wide-field imaging
Low-frequency radio astronomy and wide-field imaging James Miller-Jones (NRAO Charlottesville/Curtin University) ITN 215212: Black Hole Universe Many slides taken from NRAO Synthesis Imaging Workshop (Tracy
More informationCelestial Reference Systems:
Celestial Reference Systems: Stability and Alignment G. Bourda Laboratoire d Astrophysique de Bordeaux (LAB) Observatoire Aquitain des Sciences de l Univers (OASU) Université Bordeaux 1 Floirac FRANCE
More informationDetection of hot gas in multi-wavelength datasets. Loïc Verdier DDAYS 2015
Detection of hot gas in multi-wavelength datasets Loïc Verdier SPP DDAYS 2015 Loïc Verdier (SPP) Detection of hot gas in multi-wavelength datasets DDAYS 2015 1 / 21 Cluster Abell 520; Credit: X-ray: NASA/CXC/UVic./A.Mahdavi
More informationMulti-Frequency VLBI Telescopes & Synergy with ALMA Taehyun Jung
Multi-Frequency VLBI Telescopes & Synergy with ALMA Taehyun Jung Korean VLBI Network (KVN) Korea Astronomy & Space Science Institute (KASI) Workshop on mm-vlbi with ALMA @ Istituto di Radioastronomia Bologna,
More information258 of the Hipparcos Catalogue (ESA 1997). What follows is an overview of these data as pertaining to this project. The Hipparcos split-mirror telesco
257 USING HIPPARCOS TRANSIT DATA FOR APERTURE SYNTHESIS IMAGING Carl Fredrik Quist, Lennart Lindegren, Staan Soderhjelm Lund Observatory, Box 43, SE-221 00 Lund, Sweden ABSTRACT The ESA Hipparcos astrometry
More informationSensitivity. Bob Zavala US Naval Observatory. Outline
Sensitivity Bob Zavala US Naval Observatory Tenth Synthesis Imaging Summer School University of New Mexico, June 13-20, 2006 Outline 2 What is Sensitivity? Antenna Performance Measures Interferometer Sensitivity
More informationTECHNICAL REPORT NO. 86 fewer points to average out the noise. The Keck interferometry uses a single snapshot" mode of operation. This presents a furt
CHARA Technical Report No. 86 1 August 2000 Imaging and Fourier Coverage: Mapping with Depleted Arrays P.G. Tuthill and J.D. Monnier 1. INTRODUCTION In the consideration of the design of a sparse-pupil
More informationStrong gravitational lensing
Strong gravitational lensing Olaf Wucknitz, JIVE, Dwingeloo, NL Mike Garrett, JIVE, Dwingeloo, NL Neal Jackson, Jodrell Bank, UK Dieter Engels, Hamburger Sternwarte, Germany 1 Introduction The gravitational
More informationDeconvolution in sythesis imaging an introduction
Chapter 12 Deconvolution in sythesis imaging an introduction Rajaram Nityananda 12.1 Preliminaries These lectures describe the two main tools used for deconvolution in the context of radio aperture synthesis.
More informationTesting the MCS Deconvolution Algorithm on Infrared Data. Michael P. Egan National Geospatial-Intelligence Agency Basic and Applied Research Office
Testing the MCS Deconvolution Algorithm on Infrared Data Michael P. Egan ational Geospatial-Intelligence Agency Basic and Applied Research Office ABSTRACT Magain, Courbin, and Sohy (MCS, 1998) [1] proposed
More informationMulti-frequency polarimetry of a complete sample of faint PACO sources. INAF-IRA (Bologna)
Multi-frequency polarimetry of a complete sample of faint PACO sources. Vincenzo Galluzzi Marcella Massardi DiFA (University of Bologna) INAF-IRA (Bologna) INAF-IRA & Italian ARC The state-of-the-art The
More informationAlan Turing Building, Oxford Road, Manchester M13 9PL, UK; * Correspondence:
galaxies Article Gravitational Lens Time Delays Using Polarization Monitoring Andrew Biggs 1, * ID and Ian Browne 2 1 European Southern Observatory, Karl-Schwarzschild-Straße 2, D-85748 Garching bei München,
More informationArray signal processing for radio-astronomy imaging and future radio telescopes
Array signal processing for radio-astronomy imaging and future radio telescopes School of Engineering Bar-Ilan University Amir Leshem Faculty of EEMCS Delft University of Technology Joint wor with Alle-Jan
More informationAn Introduction to Radio Astronomy
An Introduction to Radio Astronomy Second edition Bernard F. Burke and Francis Graham-Smith CAMBRIDGE UNIVERSITY PRESS Contents Preface to the second edition page x 1 Introduction 1 1.1 The role of radio
More informationThe data model. Panos Labropoulos. Kapteyn Instituut
The data model Panos Labropoulos " Challenges The actual 21-cm signal is several times weaker than the foregrounds and sits below the telescope noise Foregrounds: galactic and extragalactic (polarization?)
More informationThe Square Kilometre Array & High speed data recording
The Square Kilometre Array & High speed Astrophysics Group, Cavendish Laboratory, University of Cambridge http://www.mrao.cam.ac.uk/ bn204/ CRISP Annual Meeting FORTH, Crete, Greece March 2012 Outline
More informationSingle-dish antenna at (sub)mm wavelengths
Single-dish antenna at (sub)mm wavelengths P. Hily-Blant Institut de Planétologie et d Astrophysique de Grenoble Université Joseph Fourier October 15, 2012 Introduction A single-dish antenna Spectral surveys
More informationCLASS B : last of the Cosmic Lens All-Sky Survey lenses
Mon. Not. R. Astron. Soc. 361, 259 271 (2005) doi:10.1111/j.1365-2966.2005.09170.x CLASS B0631+519: last of the Cosmic Lens All-Sky Survey lenses T. York, 1 N. Jackson, 1 I. W. A. Browne, 1 L. V. E. Koopmans,
More informationGeraint Harker. Kapteyn Astronomical Institute, Groningen. Wed. 17th Sept Hamburg LOFAR Workshop
Geraint Harker Kapteyn Astronomical Institute, Groningen Wed. 17th Sept. 2008 Hamburg LOFAR Workshop 1 Extract a cosmological signal from a datacube, the three axes of which are x and y positions, and
More informationSolar System Objects. Bryan Butler NRAO. Planetary Radio Astronomy. Solar System Bodies. Why Interferometry? A Bit of History. 45% - Extragalactic
Solar System Objects Bryan Butler NRAO )+*, -/.0 1 24365 7-'*80 1 9436285;:6< 5= 3>
More informationCentral parsec(s) of the quasar
Central parsec(s) of the quasar 0850+581 Yuri Kovalev MPIfR, Bonn ASC Lebedev, Moscow In collaboration with: Andrei Lobanov, Alexander Pushkarev (MPIfR, Bonn) 5 June, 2008 Arecibo Observatory Library Colloquium
More informationBlake Stauffer. A senior thesis submitted to the faculty of Brigham Young University in partial fulfillment of the requirements for the degree of
H 2 O Maser Observations of Planetary Nebula K3-35 Blake Stauffer A senior thesis submitted to the faculty of Brigham Young University in partial fulfillment of the requirements for the degree of Bachelor
More informationACIS ( , ) Total e e e e-10 4.
1 SUMMARY 1 G21.5-0.9 1 Summary Distance: 5 kpc ( Safi-Harb et al., 2001 ) Position of Central Source (J2000): ( 18 33 34.0, -10 34 15.3 ) X-ray size: 4.7 x4.6 Description: 1.1 Summary of Chandra Observations
More informationRestarting activity. in the nucleus of PBC J Lorena Hernández García
Restarting activity in the nucleus of PBC J2333.9-2343 Lorena Hernández García Collaborators: Francesca Panessa Marcello Giroletti Gabriele Ghisellini Loredana Bassani Nicola Masetti Mirjana Povic Angela
More informationHigh-resolution observations and mass modelling of the CLASS gravitational lens B
Mon. Not. R. Astron. Soc. 330, 205 211 (2002) High-resolution observations and mass modelling of the CLASS gravitational lens B11521199 D. Rusin, 1P M. Norbury, 2 A. D. Biggs, 2 D. R. Marlow, 2 N. J. Jackson,
More informationFourier Analysis and Imaging Ronald Bracewell L.M. Terman Professor of Electrical Engineering Emeritus Stanford University Stanford, California
Fourier Analysis and Imaging Ronald Bracewell L.M. Terman Professor of Electrical Engineering Emeritus Stanford University Stanford, California 4u Springer Contents fa 1 PREFACE INTRODUCTION xiii 1 11
More informationVLBA IMAGING OF SOURCES AT 24 AND 43 GHZ
VLBA IMAGING OF SOURCES AT 24 AND 43 GHZ D.A. BOBOLTZ 1, A.L. FEY 1, P. CHARLOT 2,3 & THE K-Q VLBI SURVEY COLLABORATION 1 U.S. Naval Observatory 3450 Massachusetts Ave., NW, Washington, DC, 20392-5420,
More informationStrong gravitational lenses in the 2020s
Strong gravitational lenses in the 2020s Masamune Oguri University of Tokyo 2014/7/18 TMT science forum @ Tucson Strong gravitational lenses are rare wide-field surveys find strong gravitational lenses
More informationClassifying Galaxy Morphology using Machine Learning
Julian Kates-Harbeck, Introduction: Classifying Galaxy Morphology using Machine Learning The goal of this project is to classify galaxy morphologies. Generally, galaxy morphologies fall into one of two
More informationarxiv: v1 [astro-ph.ga] 12 Aug 2009
Mon. Not. R. Astron. Soc. 000, 1 17 (2005) Printed 12 August 2009 (MN LATEX style file v2.2) AMI observations of Lynds Dark Nebulae: further evidence for anomalous cm-wave emission arxiv:0908.1655v1 [astro-ph.ga]
More informationDual frequency VLBI polarimetric observations of 3C138
Astron. Astrophys. 325, 493 51 (1997) ASTRONOMY AND ASTROPHYSICS Dual frequency VLBI polarimetric observations of 3C138 W.D. Cotton 1, D. Dallacasa 2, C. Fanti 2,3, R. Fanti 2,3, A.R. Foley 4, R.T. Schilizzi
More informationarxiv: v1 [astro-ph.ga] 11 Oct 2018
**Volume Title** ASP Conference Series, Vol. **Volume Number** **Author** c **Copyright Year** Astronomical Society of the Pacific Imaging Molecular Gas at High Redshift arxiv:1810.05053v1 [astro-ph.ga]
More informationAn IDL Based Image Deconvolution Software Package
An IDL Based Image Deconvolution Software Package F. Városi and W. B. Landsman Hughes STX Co., Code 685, NASA/GSFC, Greenbelt, MD 20771 Abstract. Using the Interactive Data Language (IDL), we have implemented
More informationThe shapes of faint galaxies: A window unto mass in the universe
Lecture 15 The shapes of faint galaxies: A window unto mass in the universe Intensity weighted second moments Optimal filtering Weak gravitational lensing Shear components Shear detection Inverse problem:
More information