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Coronal Faraday Rotation of Occulted Radio Signals. M. K. Bird Argelander-Institut für Astronomie, Universität Bonn. International Colloquium on Scattering and Scintillation in Radio Astronomy Pushchino, Russia Monday, 19 June 2006 . Coronal Faraday Rotation – Definition
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Coronal Faraday Rotation of Occulted Radio Signals M. K. Bird Argelander-Institut für Astronomie, Universität Bonn International Colloquium on Scattering and Scintillation in Radio Astronomy Pushchino, Russia Monday, 19 June 2006
Coronal Faraday Rotation – Definition Coronal FR using Various Radio Sources Pulsars Extended Continuum Sources Spacecraft (Helios E12: 1975-1984) FR Variations over Different Time Scales Background Coronal Magnetic Field FR Signature of Coronal Mass Ejections FR Fluctuations: Alfvén Waves & Quasi-harmonic Oscillations Coronal FR Mapping – the Future? Summary Outline
Faraday Rotation : Definition radians with 2.36∙104 in MKS or cgs units radio frequency (Helios: 2.3 GHz) electron density mag field proj. along ray path
Interplanetary Electron Column Density from Earth I = ∫Ne(s) ds “Dispersion Measure” Units: hexems 1 hexem = 1016 el/m2 Earth Sun analogous plot for Faraday Rotation does not exist!
Polarization Angle Measurement Electric Vectors (semi-major axis of polarization ellipse): E0 = Source (transmitted) E= Measured (received) Angle definitions: q = locally measured polarization angle p = parallactic angle = Faraday rotation
Rotation Measure RM: A rotation measure of RM = 1 rad m-2 yields: • = 0.97° at 2.3 GHz (=0.13 m) • = 57.3° at 300 MHz (=1.0 m) • = 1432° at 60 MHz (=5.0 m)
can be positive or negative (from polarity of interplanetary magnetic field) Angle ambiguity ( ± m·180°) Contributions from electron density and magnetic field cannot be separated without independent measurements Correction for variable ionosphere necessary if solar offset R > 10 RS Coronal Faraday Rotation Measurement
Pulsars at Conjunction 1978-79 [Bird et al., Nature 283, 459-460, 1980]
Pulsar Pulse Profiles: Measurement Technique intrinsic profile modified profile p-angle: intrinsic & modified PSR 0540+23 PSR 0525+21
Coronal FR with Extended ContinuumSources 3C228 A [Spangler, 2005] 1' B C
Coronal FR at VLA: 21 Aug 2003 3C228 R = 7.1…6.2 RS RM: 62.5 rad/m2
SOHO/LASCO: 16 AUG 2003 3C228 3C228 Venus Jupiter
Coronal FR with Helios • Helios – 1 • Launch: 10 Dec 1974 • EOM: 15 Mar 1986 • q = 0.31 AU (P = 190 d) • i = 0°, "spin up" • Helios – 2 • Launch: 15 Jan 1976 • EOM: 08 Jan 1981 • q = 0.29 AU (P = 186 d) • i = 0°, "spin down"
Coronal Faraday Rotation: Helios Observations <FR> = 35.4° FR = 2.1°
Coronal FR: Helios-1, Dec 1981 180 ambiguity
FR Variations over Different Time Scales …Background Coronal Magnetic Field
Mean Absolute FR: 1975-1976 |max| R-4.15
Mean Coronal Magnetic Field 1975-76 [Pätzold et al., Solar Phys. 109, 91, 1987] 3 RS < R < 10 RS: Br = 7.9 R-2.7 G (17) or Br = 6 R-3 + 1.2 R-2 G (18)
FR Variations over Different Time Scales … FR Fluctuations: Alfvén Waves & Quasi-harmonic Oscillations
FR Spectra for Various Solar Offset Distances Andreev et al., [1996]
Rapid Sequence of FR Spectra QHC comes… … and goes! [Chashei et al., 1999]
FR Variations over Different Time Scales … FR Signature of Coronal Mass Ejections
CME Passing through Helios-2 Ray Path Solwind Coronagraph Images recorded during Helios Solar Occultations In Oct/Nov 1979 [Bird et al., 1985]
Simulated Coronal FR for CR 1751 [J. Kasper, priv. comm, 2004.]
Transient Simulations: October 2003 CMEs CME! Large FR in 20 sources CME not yet detected