The Magnetic Milky Way Bryan Gaensler Centre of Excellence for All-sky Astrophysics www.caastro.org Brown (2010)

Slides:



Advertisements
Similar presentations
Activity: The Galactic Centre
Advertisements

Magnetic Field Puzzles From Our Own Backyard Jo-Anne Brown & Russ Taylor.
Radio and Gamma-Ray Beams from Pulsars R. N. Manchester CSIRO Astronomy and Space Science Australia Telescope National Facility, Sydney Summary Pulse profiles.
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.
Observations of turbulence in the magneto-ionized ISM on subparsec scales Marijke Haverkorn.
Cambridge CMB meeting 20 th July 2009 CMB B-modes: Foregrounds Paddy Leahy, Clive Dickinson, Mike Preece, Mike Peel (Manchester)
Early Polarisation Science with ASKAP Bryan Gaensler, Tom Landecker, Russ Taylor and the POSSUM team askap.org/possum.
Study of Cosmic Magnetic Fields with Square Kilometer Array Keitaro Takahashi Nagoya University workshop 2010.
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.
3-D Simulations of Magnetized Super Bubbles J. M. Stil N. D. Wityk R. Ouyed A. R. Taylor Department of Physics and Astronomy, The University of Calgary,
Multiwavelength Sky by NASA. Radio Continuum (408 MHz). Intensity of radio continuum emission from surveys with ground- based radio telescopes (Jodrell.
Galactic Diffuse Gamma-ray Emission, the EGRET Model, and GLAST Science Stanley D. Hunter NASA/GSFC Code 661
Radio Astronomy And The Spiral Structure Of The Milky Way Jess Broderick Supervisor: Dr George Warr.
The Mass of the Galaxy We can use the orbital velocity to deduce the mass of the Galaxy (interior to our orbit): v orb 2 =GM/R. This comes out about 10.
T.G.Arshakian MPI für Radioastronomie (Bonn) Exploring the weak magnetic fields with LOFAR.
Magnetic fields in our Galaxy How much do we know JinLin Han National Astronomical Observatories Chinese Academy of Sciences Beijing, China
WG7.4: Modelling the Galactic Magnetic Field Paddy Leahy (for Althea Wilkinson and Tony Banday)
Galactic Magnetic Field Research with LOFAR Wolfgang Reich Max-Planck-Institut für Radioastronomie Bonn, Germany.
Synchrotron Radiation, continued Rybicki & Lightman Chapter 6 Also Course notes for “Essential Radio Astronomy” at NRAO, Condon & Ransom
Radio Diagnostics of Turbulence in the Interstellar & Intergalactic media J. M. Cordes, Cornell University URSI 20 August 2002.
The Milky Way Center, Shape Globular cluster system
Cosmic Rays Discovery of cosmic rays Local measurements Gamma-ray sky (and radio sky) Origin of cosmic rays.
ASTR112 The Galaxy Lecture 6 Prof. John Hearnshaw 10. Galactic spiral structure 11. The galactic nucleus and central bulge 11.1 Infrared observations Galactic.
THE CAASTRO TEAM IS PURSUING THREE INTERLINKED SCIENCE PROGRAMS: THE EVOLVING UNIVERSE When did the first galaxies form, and how have they then evolved?
The Effect of Solar Wind on Pulsar Observations Xiaopeng YOU Southwest University, Chongqing, China.
Aristeidis Noutsos The Galactic Magnetic Field from Pulsar RMs and the Low-Frequency Arrays Aristeidis Noutsos Jodrell Bank Centre for Astrophysics, Manchester,
Molecular absorption in Cen A on VLBI scales Huib Jan van Langevelde, JIVE Ylva Pihlström, NRAO Tony Beasley, CARMA.
Magnetic fields in our Galaxy JinLin Han National Astronomical Observatories Chinese Academy of Sciences Beijing, China Thanks for cooperation.
The Canadian Galactic Plane Survey Mapping the Ecology Of the Milky Way Galaxy.
Nebular Astrophysics.
The Swedish contribution to EU-HOU: A Hands-On Radio Astronomy exercise Mapping the Galaxy using hydrogen Daniel Johansson Christer Andersson.
Cosmic magnetism ( KSP of the SKA) understand the origin and evolution of magnetism in the Galaxy, extragalactic objects, clusters and inter-galactic/-cluster.
The Milky Way Galaxy.
Polarization Surveys with the DRAO 26-m Telescope at 1.4 GHz Maik Wolleben, T. Landecker, O. Davison Dominion Radio Astrophysical Observatory W. Reich,
The Interstellar Medium and Interstellar Molecules Ronald Maddalena National Radio Astronomy Observatory.
The Canadian Galactic Plane Survey What is the CGPS? Status and some results What’s next? Mapping the Ecology of the Milky Way Galaxy.
Galactic Radioemission – a problem for precision cosmology ? Absolute Temperatures at Short CM-Waves with a Lunar Radio Telescope Wolfgang Reich Max-Planck-Institut.
Interstellar Scattering Joseph Lazio (Naval Research Laboratory) J. Cordes, A. Fey, S. Spangler, B. Dennison, B. Rickett, M. Goss, E. Waltman, M. Claussen,
JinLin Han National Astronomical Observatories Chinese Academy of Sciences Beijing , China P. Demorest Grateful to cooperators Pulsar.
Magnetic fields in the Galaxy via Faraday effect: Future prospects with ASKAP and the SKA Lisa Harvey-Smith Collaborators: Bryan CSIRO SKA Project ScientistGaensler.
ASTR112 The Galaxy Lecture 7 Prof. John Hearnshaw 11. The galactic nucleus and central bulge 11.1 Infrared observations (cont.) 11.2 Radio observations.
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,
Tsunefumi Mizuno 1 Fermi_Diffuse_ASJ_2010Mar.ppt Fermi-LAT Study of Galactic Cosmic-Ray Distribution -- CRs in the Outer Galaxy -- Tsunefumi Mizuno Hiroshima.
Lecture 30: The Milky Way. topics: structure of our Galaxy structure of our Galaxy components of our Galaxy (stars and gas) components of our Galaxy (stars.
The low frequency Galactic polarisation foreground Xiaohui Sun & Wolfang Reich MPIfR
Astronomy 404/CSI 769 Extragalactic Astronomy
UNIT 1 The Milky Way Galaxy.
Our Milky Way Galaxy. The Milky Way Almost everything we see in the night sky belongs to the Milky Way. We see most of the Milky Way as a faint band of.
ISM X-ray Astrophysics Randall K. Smith Chandra X-ray Center.
Galactic Legacy Projects Naomi McClure-Griffiths Australia Telescope National Facility, CSIRO NRAO Legacy Projects Meeting, 17 May 2006.
The Planck Satellite Matthew Trimble 10/1/12. Useful Physics Observing at a redshift = looking at light from a very distant object that was emitted a.
Searching for the Synchrotron Cosmic Web with the Murchison Widefield Array Bryan Gaensler Centre for All-sky Astrophysics / The University of Sydney Natasha.
(history of radio polarization)
Fermi LAT Observations of Galactic and Extragalactic Diffuse Emission Jean-Marc Casandjian, on behalf of the Fermi LAT collaboration 7 questions addressed.
Cosmic Microwave Background Carlo Baccigalupi, SISSA CMB lectures at TRR33, see the complete program at darkuniverse.uni-hd.de/view/Main/WinterSchoolLecture5.
Milky Way Galaxy. Galaxy A group of stars, dust and gases held together by gravity. 170 billion galaxies in the universe 200 billion stars in a galaxy.
Cosmic Masers Chris Phillips CSIRO / ATNF. What is a Maser? Microwave Amplification by Stimulated Emission of Radiation Microwave version of a LASER Occur.
1 ASTRON is part of the Netherlands Organisation for Scientific Research (NWO) Netherlands Institute for Radio Astronomy Astronomy at ASTRON George Heald.
Eyes on the Polarized Sky, Feet on the Ground
A Turbulent Local Environment
Spiral Arms.
Our Milky Way Galaxy.
Arecibo Radio Telescope Puerto Rico World's largest radio telescope
T.G.Arshakian MPI für Radioastronomie (Bonn)
Xinjiang Astronomical Observatory,CAS
Shane O’Sullivan University College Cork
SKADS Polarization Simulations The MPIfR team (Milky Way & star-forming galaxies): Tigran Arshakian, Rainer Beck, Marita Krause, Wolfgang Reich, XiaoHui.
Presentation transcript:

The Magnetic Milky Way Bryan Gaensler Centre of Excellence for All-sky Astrophysics Brown (2010)

The Centre for All-sky Astrophysics The CAASTRO Vision: To be the international leader in wide-field astronomy, positioning Australia to address fundamental unsolved questions about the Universe with the dramatic capabilities of next-generation telescopes and advanced instrumentation. → DISCOVER: Ground-breaking advances in understanding the Universe → INNOVATE: New ways of processing & visualising complex data sets → PERFORM: High-impact discoveries using SKA pathfinders → UNITE: A new network of talented researchers → EDUCATE: Exciting opportunities for students and young scientists

Overview 1.Early History 2.Faraday Rotation 3.The Galactic Magnetic Field 4.Challenges and recent progress -Electron density models -Coherence -Fluctuations -The vertical magnetic field 5.Conclusions & Future Work

Magnets in the Sky? ›Alfvén (1937): cosmic ray confinement implies “the existence of a magnetic field in interstellar space” ›Fermi (Jan 1949): “the main process of acceleration [of cosmic rays] is due to magnetic fields which occupy interstellar spaces … the magnetic field in the dilute matter is of the order of 5x10 -6 gauss, while its intensity is probably greater in the heavier clouds” ›Hall, Hiltner (Feb 1949): starlight is polarised ›Davis & Greenstein (Mar 1949): “the polarisation is not a property of the star but is produced while the light is traversing extensive regions of interstellar space … non-spherical dust grains produce [this if] there exists a general galactic magnetic field” ›Kiepenheuer (June 1950): Galactic radio emission comes from cosmic rays gyrating in magnetic fields Hall (1949) Lowell Observatory Archives / ASP / Yerkes Observatory

The Dawn of Radio Polarimetry ›Razin (1956, 1958), Thompson (1957), Pawsey & Harting (1960): attempts to detect polarisation & Faraday rotation in Galactic radio emission ›Bolton & Wild (1957): “large radio reflectors [offer] the possibility of determining longitudinal fields in localised interstellar regions by observing the Zeeman splitting of the 21-cm line” ›Westerhout et al. (1962), Wielebinski et al. (1962): detection of polarisation of diffuse Galactic radio emission ›Cooper & Price (1962): Detection of interstellar Faraday rotation against lobes of Centaurus A ›Verschuur (1968): Detection of H I Zeeman splitting; “Fields of the order of 2x10 -5 G exist in the Perseus spiral arm in the direction of the radio source Cassiopeia A.” (shortest abstract of all time?) Parkes polarimetry of Centaurus A (Cooper & Price 1962)

Pulsar B (Gaensler et al. 1998) RM = +495 ± 6 rad m -2  (degrees) [ (metres)] 2 › Optical starlight polarisation › Synchrotron emission / polarisation B ┴ (orientation, but not direction) › Infrared dust polarisation › Zeeman splitting B ║ (weak effect, long observations) › Faraday rotation & rotation measure (RM) are powerful probes of B ║ -provides direction of B -radio wavelengths: no attenuation of radiation Superconductivity Lab, Oslo University Mapping Magnetic Fields }

Faraday Rotation Philipp Kronberg / Physics Today

The Galactic Magnetic Field ›Large- and small-scale components ›Concentrated in disk; follows arms? -local field is clockwise (Manchester 1972) -field in Sagittarius arm is counterclockwise (Thomson & Nelson 1980; Simard & Kronberg 1980)  reversal between arms … but overall geometry unclear (Noutsos et al. 2008; Men et al. 2008; Vallée 2008; Nota & Katgert 2010; Pshirkov et al. 2011) Han (2009) M. Thévenot (1644) / National Library of Australia Starlight polarisation (Fosalba 2001; Han & Wielebinski 2002) Brown (2010)

› Need to assume model for n e (l) - “NE2001” (Cordes & Lazio 2002, 2003)  n e (x, y, z) ; disk, arms, clumps, voids - for extragalactic RMs,  B  depends on n e (l) - for pulsar RMs,  B   RM/DM, but distance is inferred from DM =  n e (l)dl, and so depends on n e (l) also! Faraday Rotation & Electron Models Cordes & Lazio (2002)

In the Thrall of NE2001 Sun, Reich, Waelkens & Enßlin (2008)

›NE2001: thick disk with H DM = 950 pc -implies B halo ≈ 10 μG, CRs truncated at z = 1 kpc (Sun et al. 2008) ›NE2001 calibrated using 112 PSR distances - test of a model is its predictive power - new parallaxes don’t match NE2001 › Example : PSR B d predicted = 1.0 ± 0.2 kpc (NE2001) ; d parallax = 2.1 ± 0.1 kpc (Chatterjee et al. 2009) › A new look at n e vs. z (Gaensler et al. 2008) PSRs w. accurate distances  revised scale height H DM = 1.8 kpc  double previous estimates  implies B halo ≈ 2 μG & H CR ≈ 0.8 kpc (Sun & Reich 2010) How Reliable Is NE2001? NE2001 model Gaensler et al. (2008)

Sampling of Background RMs ›Han et al. (1997): 557 extragalactic RMs › Taylor et al. (2009): extragalactic RMs (reprocessing of NVSS data) - simultaneously shows large-scale coherence & small-scale fluctuations

Blue= axisymmetric ring Red= axisymmetric spiral Green= bisymmetric spiral Sun, Reich, Waelkens & Enßlin (2008) › VLA polarimetry observations of 194 new extragalactic RMs, 17 o < l < 63 o and 205 o < l < 253 o (Van Eck, Brown, Gaensler et al. 2011) Han (2009) New Insights: Coherence Van Eck et al. (2011)

› B random > B ordered, plus many identified & unidentified regions of anomalous RM (Mitra et al. 2003; McClure-Griffiths, Gaensler et al. 2010; Harvey-Smith, Madsen & Gaensler 2011) -impossible to differentiate between models for large-scale field only via χ 2 of RMs (Men et al. 2008; Nota & Katgert 2010) -approaches needed that simultaneously incorporate large- + small-scale B, plus coherent, random & ordered B (Jaffe et al. 2010; Jansson & Farrar 2011) New Insights: Fluctuations Harvey-Smith et al. (2011)McClure-Griffiths et al. (2010)

›Field symmetry is a vital diagnostic ›Han et al. (1994, 1997, 1999): behaviour of RMs at high |b| -B z = +0.4 ± 0.2 μG from S to N  A0 symmetry ›Wolleben, Gaensler et al. (2010): behaviour of RMs at high |b|  RM feature at l > 0 o, b > 0 o seen also in H I : local magnetised bubble ›Mao, Gaensler et al. (2010): RMs of 1000 xgal sources, |b| > 77 o -B z, south = ± 0.03 μG -B z, north = 0.00 ± 0.02 μG  no coherent vertical field at Sun  not pure dipole or quadrupole  overlapping disk/halo dynamos? Mao, Gaensler et al. (2010)Han et al. (1997) The Vertical Field Brown (2010) NORTHSOUTH

Conclusions ›Galactic B is clockwise in outer disk, counterclockwise in (parts of) inner disk (Van Eck et al. 2011; Jansson & Farrar 2011) ›No coherent vertical field structure (Mao et al. 2010) ›No simple fit for large-scale B (Men et al. 2008)  No match to any simple theoretical model ›The future: -new & improved n e model (“NE2008”; Cordes et al., in prep) -GALFACTS, GMIMS, Planck, Auger, LOFAR, MWA, ASKAP-POSSUM, SKA Hall (1949) Brown (2010) CSIRO / Swinburne © Frank R. Paul estate askap.org/possum