Polarization Surveys with the DRAO 26-m Telescope at 1.4 GHz Maik Wolleben, T. Landecker, O. Davison Dominion Radio Astrophysical Observatory W. Reich,

Slides:



Advertisements
Similar presentations
Jeroen Stil Department of Physics & Astronomy University of Calgary Stacking of Radio Surveys.
Advertisements

Fundamentals of Radio Astronomy Lyle Hoffman, Lafayette College ALFALFA Undergraduate Workshop Arecibo Observatory, 2009 Jan. 12.
The Ability of Planck to Measure Unresolved Sources Bruce Partridge Haverford College For the Planck Consortium.
S-PASS, a new view of the polarized sky Gianni Bernardi SKA SA On behalf of the S-PASS team CMB2013, Okinawa, June th 2013.
Primary results of polarization survey of large-SNRs at 6cm Li Xiao, XiaoHui Sun, Chen Wang, WeiBin Shi, Wolfgang Reich, JinLin Han Partner Group of MPIfR.
Cambridge CMB meeting 20 th July 2009 CMB B-modes: Foregrounds Paddy Leahy, Clive Dickinson, Mike Preece, Mike Peel (Manchester)
Jo-Anne Brown Observations of the Galactic Magnetic Field from the International Galactic Plane Survey.
Controversies in radio astronomy, observational mistakes, false priority claims overinterpretation Richard Wielebinski Max-Planck-Institut für Radioastronomie.
Mehreen Mahmud Denise Gabuzda University College Cork, Ireland Searching for Helical Magnetic Fields in Several BL Lac Objec ts.
The Sino-German 6cm polarization survey of the Galactic plane Total intensity Polarized intensity Xiaohui Sun NAOC.
HI from z ~ 0 – 1 with FAST D.J. Pisano West Virginia University NRAO.
Contamination of the CMB Planck data by galactic polarized emissions L. Fauvet, J.F. Macίas-Pérez.
Radio Telescopes Large metal dish acts as a mirror for radio waves. Radio receiver at prime focus. Surface accuracy not so important, so easy to make.
Polarization 2005, Orsay, 13/09/2005 Depolarization canals in Milky Way radio maps Anvar Shukurov and Andrew Fletcher School of Mathematics and Statistics,
Fundamentals of Radio Astronomy Lyle Hoffman, Lafayette College ALFALFA Undergraduate Workshop Union College, 2005 July 06.
Zeldovich-Sakharov program at RATAN-600 “Cosmological Gene” project Ground based support of the Space CMB Missions Y.Parijskij et al Special Astrophysical.
T.G.Arshakian MPI für Radioastronomie (Bonn) Exploring the weak magnetic fields with LOFAR.
Contour statistics, depolarization canals and interstellar turbulence Anvar Shukurov School of Mathematics and Statistics, Newcastle, U.K.
Galactic Magnetic Field Research with LOFAR Wolfgang Reich Max-Planck-Institut für Radioastronomie Bonn, Germany.
Low frequency sky surveys with the Murchison Widefield Array (MWA) Gianni Bernardi Harvard-Smithsonian Center for Astrophysics SKA SA project/MeerKAT observatory.
4/19/2017 7:18 PM Linear and circular radio and optical polarization studies as a probe of AGN physics I. Myserlis E. Angelakis (PhD advisor), L. Fuhrmann,
The Solar Corona Steven R. Spangler Department of Physics and Astronomy University of Iowa.
Aristeidis Noutsos The Galactic Magnetic Field from Pulsar RMs and the Low-Frequency Arrays Aristeidis Noutsos Jodrell Bank Centre for Astrophysics, Manchester,
The "26-m Polarization Survey" ( ) MAIK WOLLEBEN.
P olarized R adiation I maging and S pectroscopy M ission Probing cosmic structures and radiation with the ultimate polarimetric spectro-imaging of the.
“First Light” From New Probes of the Dark Ages and Reionization Judd D. Bowman (Caltech) Hubble Fellows Symposium 2008.
Chen, Yi-Ping Supervisor: Hirano, Naomi 12 CO J=2-1 Observation Of M51 With SMA Physical Department of Tamkang University August,27, 2002 Summer Student.
Random Media in Radio Astronomy Atmospherepath length ~ 6 Km Ionospherepath length ~100 Km Interstellar Plasma path length ~ pc (3 x Km)
Maser Polarization and Magnetic fields during Massive Star Formation W. H. T. Vlemmings ASP Conference Series, Vol. 387, 2008 Do-Young Byun.
Science with a Rover-based Low-frequency Dipole Array A multi-configuration rover-borne dipole array for Low-frequency RadioAstronomy from the Moon Ettore.
Designing Experiments T. Venturi Istituto di Radioastronomia, Bologna, INAF ERIS, Manchester, 9 September 2005.
Australia Telescope 20 GHz survey (AT20G): An Update Ron Ekers (ATNF, PI),Sarah Burke(Haverford-Swinburne), Mark Calabretta (ATNF), Gianfranco De Zotti.
Galactic Radioemission – a problem for precision cosmology ? Absolute Temperatures at Short CM-Waves with a Lunar Radio Telescope Wolfgang Reich Max-Planck-Institut.
First Result of Urumqi 6cm Polarization Observations: Xiaohui Sun, Wolfgang Reich JinLin Han, Patricia Reich, Richard Wielebinski Partner Group of MPIfR.
The Galactic Plane Infrared Polarization Survey (GPIPS) Current Members: Michael Pavel Dan Clemens (PI) Lauren Cashman Sadia Hoq Jordan Montgomory Ian.
Magnetic fields in the Galaxy via Faraday effect: Future prospects with ASKAP and the SKA Lisa Harvey-Smith Collaborators: Bryan CSIRO SKA Project ScientistGaensler.
Conference Summary Ue-Li Pen
Cosmic magnetism ( KSP of the SKA)‏ understand the origin and evolution of magnetism in the Galaxy, extragalactic objects, clusters and inter-galactic/-cluster.
Kashi1 Radio continuum observations of the Sombrero galaxy NGC4594 (M104) and other edge-on spirals Marita Krause MPIfR, Bonn Michael Dumke ESO,
EBEx foregrounds and band optimization Carlo Baccigalupi, Radek Stompor.
The low frequency Galactic polarisation foreground Xiaohui Sun & Wolfang Reich MPIfR
Aristeidis Noutsos University of Manchester. The LOFAR Ionosphere See Ger’s talk, in Hamburg last year. Variations of ~3 rad m –2 were observed in the.
Weibin Shi, Xiaohui Sun, Wolfgang Reich Jinlin Han, Patricia Reich, Richard Wielebinski Partner Group of MPIfR at NAOC Primary results for 6cm polarization.
Observation and Data Analysis Activityin SPOrt and BaR-SPOrt Exp.s Ettore Carretti Bologna 7-9 January 2004.
Radio Sounding of the Near-Sun Plasma Using Polarized Pulsar Pulses I.V.Chashei, T.V.Smirnova, V.I.Shishov Pushchino Radio Astronomy Obsertvatory, Astrospace.
Dependence of the Integrated Faraday Rotations on Total Flux Density in Radio Sources Chen Y.J, Shen Z.-Q.
Measuring the Near-Nothingness of Interstellar Space with Radio Astronomy Steven R. Spangler University of Iowa.
Galactic Legacy Projects Naomi McClure-Griffiths Australia Telescope National Facility, CSIRO NRAO Legacy Projects Meeting, 17 May 2006.
150GHz 100GHz 220GHz Galactic Latitude (Deg) A Millimeter Wave Galactic Plane Survey with the BICEP Polarimeter Evan Bierman (U.C. San Diego) and C. Darren.
GALFA GALACTIC ASTRONOMY WITH ALFA Three Major Science Areas: CON Radio Continuum (incl. Polarimetry) RRL Radio Recombination Line (Spectroscopy) HI (Spectroscopy)
Searching for the Synchrotron Cosmic Web with the Murchison Widefield Array Bryan Gaensler Centre for All-sky Astrophysics / The University of Sydney Natasha.
UPDATE ON GALACTIC NOISE CORRECTION Joe Tenerelli SMOS Quality Working Group #9 ESA ESRIN 24 October 2012.
Is the Inner Radio Jet of BL Lac Precessing? R. L. Mutel University of Iowa Astrophysics Seminar 17 September 2003.
Observations of SNR G at 6cm JianWen Xu, Li Xiao, XiaoHui Sun, Chen Wang, Wolfgang Reich, JinLin Han Partner Group of MPIfR at NAOC.
Cosmic Microwave Background Carlo Baccigalupi, SISSA CMB lectures at TRR33, see the complete program at darkuniverse.uni-hd.de/view/Main/WinterSchoolLecture5.
On the Doorstep of Reionization Judd D. Bowman (Caltech) March 11, 2009 DIY 21 cm cosmology.
Effelsberg-Bonn HI Survey (EBHIS) Jürgen Kerp 1,Benjamin Winkel 2, Nadya Ben Bekhti 1, Shahram Faridani 1, Lars Flöer 1, Peter Kalberla 1, Daniel Lenz.
The large-scale structure of the Galactic magnetic field & Faraday tomography --desh Raman Research Institute, Bangalore.
Imaging issues Full beam, full bandwidth, full Stokes noise limited imaging Algorithmic Requirements: –PB corrections: Rotation, Freq. & Poln. dependence,
Eyes on the Polarized Sky, Feet on the Ground
SARA Conference Meter Dish Demo
EDGES: The ‘Global’ Perspective
Observing and Data Reduction
Molecular Gas Distribution of our Galaxy: NANTEN Galactic Plane Survey
Surrounding effects and sensitivity of the CODALEMA experiment
T.G.Arshakian MPI für Radioastronomie (Bonn)
Polarization Properties of an Eclipsing Pulsar
Polarization Properties of the John A. Galt 26-m Radio Telescope
1.4 GHz Source Counts Melanie Gendre Walter Max-Moerbeck
SKADS Polarization Simulations The MPIfR team (Milky Way & star-forming galaxies): Tigran Arshakian, Rainer Beck, Marita Krause, Wolfgang Reich, XiaoHui.
Presentation transcript:

Polarization Surveys with the DRAO 26-m Telescope at 1.4 GHz Maik Wolleben, T. Landecker, O. Davison Dominion Radio Astrophysical Observatory W. Reich, R. Wielebinski Max-Planck-Institut für Radioastronomie

Outline 1)- The DRAO 26-m Polarization Survey (finished) - Brief Representation of Data 2)- The DRAO/MPI Rotation Measure Survey (ongoing )

Specifications TELESCOPE PARAMETER diameter: 25.6m polar mounting resolution: 37 arcmin aperture efficiency: 55 % hard limits: -34 to 90 deg system temperature: 125 K SURVEY PARAMETER frequency:1410 MHz bandwidth:12 MHz observing mode:drift scanning pixel-size:15 arcmin integration time:60 s / pixel First observing period: Nov 2002 – May 2003, coverage 17% Second observing period: Jun 2004 – Mar 2005, coverage 42%

Coverage - about 350 Meridian drift scans - about 350 Meridian drift scans - carried out by night (to avoid solar interference and ionospheric FR) - carried out by night (to avoid solar interference and ionospheric FR) - fully sampled along right ascension - fully sampled along right ascension - incomplete sampling along declination - incomplete sampling along declination

Calibration After correction: ● Effelsberg-MB scale ● Agrees with southern sky survey (Parkes-MB) ● Pole temperature 80mK Stokes U'Stokes Q' this response pattern (above) is not calibrated (max %pol roughly 6%) 1. ¼ of the observed signal is coming through the side lobes 2. instrumental polarization: side lobes are polarized → ground radiation correction

Calibration Observing & Calibration Strategy about 1000 pointings congruent with the Leiden/Dwingeloo 1 polarization survey: → provides zero-levels in Stokes U and Q (absolute levels) → used for the gain calibration of the receiving system (Müller matrix) ground radiation profiles: → required to extrapolate absolute zero-levels below 0° declination comparison with Effelsberg Medium Latitude Survey: → refines the (relative) temperature scale - includes correction for main-beam instrumental polarization - residual side lobe polarization visible along the Galactic plane (l ≈0° - 60°) - systematic errors due to scanning effects (system temperature variations) 1 A survey of linear polarization at 1415 MHz: Spoelstra, T. A. Th., A&AS, 1972

Errors correlation coefficients r U =0.89, r Q =0.86: → rms-noise: 12 mK (U), 33 mK (Q) NCP-measurement gives: → rms-noise of 12 mK in U and Q

Map of Polarized Intensity combined with southern sky polarization survey at 1.4 GHz (Testori, J. C.; Reich, P.; Reich, W., in The Magnetized Interstellar Medium, 2004 the ultimate goal: all-sky polarization map preliminary version

The l=140° Region HαHα PI HαHα HαHα VTSS & WHAM

The l=140° Region HαHαPI H II regions can be used to: - derive the distance to the origin of polarized emission - derive local synchrotron emissivity towards H II regions > more complicated if there is depolarization and Faraday rotation < apparently, some H II regions do not cause depolarization: - the role of magnetic fields in HII regions? - H II regions with/without B-field?

The l=140° Region B-star dist: ≈ pc S 203 dist: ≈3.8 kpc S 185 dist: ≈210 pc O-star dist: ≈1.2 kpc

The “Depolarization Patch“ observation - low PI and %pol towards inner Galaxy - small scale structure - striking sharp upper and lower boundaries intuitive statements Either caused by: - depolarization along the line-of-sight (depth depolarization) pro: symmetry about Galactic plane total power or - depolarization by a local Faraday screen pro: explains lack of polarized emission from the North-Polar Spur (dist. ≈150 pc)

Data Availability data available within the next two months! then, interpolated data can be downloaded as: J2000 fits format - interpolated U, Q - coverage mask (to retrieve original coverage) - anything else (if requested) Galactic

Future: The DRAO/MPI Rotation Measure Survey frequency range: 1300 MHz – 1800 MHz # channels: about 1,000 – 10,000 fully Nyquist sampled between declination -30° and +90° scans along the Meridian (not drift scanning) rms per 500 MHz band: 0.3 mK observing time: 1.5 years What's next? Digital Polarimetry!

Future: The DRAO/MPI Rotation Measure Survey RM..... RM 25x n e = 0.05 cm -3 L = 150 pc B ║ = μG RM = rad/m 2 Example 1

Future: The DRAO/MPI Rotation Measure Survey n e = 0.04 cm -3 B ║ = 3 μG d = kpc RM = 0.81·n e ·B ║ ·d Example 2

Future: The DRAO/MPI Rotation Measure Survey the observed polarization angle will probably not depend linearly on λ 2 → observed RM depends on frequency! RM-survey products: Stokes U & Q data cubes Stokes I data cube Rotation Measure Synthesis RM-cube (pol. int. vs. Faraday depth)

Summary 1) DRAO 26-m Polarization Survey 2) DRAO/MPI Rotation Measure Survey (data will be released soon) - receiving system currently under development - survey start scheduled for May total observing time required: 1.5 years