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Explore the definition, measurement techniques, and future potential of Coronal Faraday Rotation in radio astronomy using various radio sources and spacecraft data. Discover the impact of solar phenomena on Faraday Rotation variations over different time scales.
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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