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The low frequency Galactic polarisation foreground

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The low frequency Galactic polarisation foreground ... An emission feature? NO! -- the intrinsic ~0 -- only appear at certain Properties of the ring structure ... – PowerPoint PPT presentation

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Title: The low frequency Galactic polarisation foreground


1
The low frequency Galactic polarisation foreground
Xiaohui Sun Wolfang Reich MPIfR23.05.2011
2
foreground polarisation causes trouble
Galactic foreground
1 rad m-2 ? 229 deg at 150 MHz
0.15 Leakage of PI to I (dotted) reionisation
(solid)
Jelic et al. 2010
3
WSRT observations at 150MHz
  • Fan region
  • 8 bands
  • 139.3 141.5 143.7
  • 145.9 148.1 150.3
  • 152.5 154.7
  • bandwidth
  • 2.5 MHz
  • Frequency resolution
  • 9.8 kHz (tapering)
  • Resolution (PI)
  • 4.2 arcmin
  • 1 mJy/beam 1 K
  • rms fluctuation 7 K

Bernardi et al. 2009
4
learn from observations RM synthesis
from Heald
Brentjens de Bruyn 2005
5
  • data
  • Bernardi et al. (2009)
  • RM synthesis software
  • Brentjens
  • clean software
  • Heald
  • f
  • -9 2 rad m-2
  • resolution
  • 3.44 rad m-2
  • max f extent
  • 0.85 rad m-2

6
Missing large-scale components
  • 2 4 K at 408 MHz
  • (Brouw Spoelstra 1976)
  • spectral index of 2.5
  • ? 24 49 K at 150 MHz
  • Faraday depth very small
  • (Spoelstra 1984)
  • flt0.8 rad m-2
  • otherwise depolarisation
  • ? assuming f0

Structures not influenced if fgt2 rad
m-2
7
A ring structure!
8
Properties of the ring structure --
centre-filled to ring-like -- intensity twice as
the surrounding -- inner radius about 1 degree --
outer radius of about 2 degree
An emission feature? NO! -- the intrinsic
f0 -- only appear at certain f
9
HAMMURABI code (Waelkens et al. 2009)
Understanding observations by simulations
3D-emssion models Sun et al. 2008 Sun
Reich 2009 Sun Reich 2010
pixel
  • Code modifications
  • Cartesian coordinates
  • Output RM cubes directly
  • Add faraday screens
  • Zoom-in of a patch

10
Observations imply a Faraday screen
  • FD from Simulations
  • negative
  • monotonously decreasing
  • versus distance
  • Constrains on FS
  • positive
  • smaller at centre
  • FD
  • too large
  • too small
  • distance
  • too far
  • too near

11
FS facts
D 200-250 pc R 6.4 pc Shell 2 pc F 1.5--3.7
rad m-2
-- RM synthesis 1/?2min maximal FD extent
0.85 rad m-2 needs frequency gt 400 MHz
(Effelsberg 300-800 MHz GMIMS survey) --
Geometry of the FS multi-FSs? (Bernardi et
al. 2009)
12
Previous observations
Haverkorn et al. 2003
Schnitzeler et al. 2007
Difficulties observations
influence of large-scale
emission simulations add local emission
13
Summary
  • Nature of the FS
  • related with the star HD 20336
  • -- B2V
  • -- D 24637 pc (parallax)
  • -- wind-blow bubble?
  • although disfavored by Haverkorn et al.
    (2003)
  • not clear
  • -- a magnetic structure (Haverkorn et al.
    2003)
  • need 300-800MHz observations (GMIMS)
  • RM synthesis simulations can constrain
    distance
  • and other parameters!
  • nature of FSs remains unclear

14
Thank you!??!
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