Issue |
A&A
Volume 414, Number 1, January IV 2004
|
|
---|---|---|
Page(s) | 53 - 67 | |
Section | Extragalactic astronomy | |
DOI | https://doi.org/10.1051/0004-6361:20034133 | |
Published online | 12 January 2004 |
The magnetic field of M 31 from multi-wavelength radio polarization observations*
1
Max-Planck-Institut für Radioastronomie, Auf dem Hügel 69, 53121 Bonn, Germany
2
School of Mathematics and Statistics, University of Newcastle, Newcastle upon Tyne, NE1 7RU, UK
Corresponding author: A. Fletcher, fletcher@mpifr-bonn.mpg.de
Received:
29
July
2003
Accepted:
6
October
2003
The configuration of the regular magnetic field in M 31 is
deduced from radio polarization observations at the wavelengths
and
. By fitting the observed
azimuthal distribution of polarization angles, we find that the
regular magnetic field, averaged over scales 1–3 kpc, is almost
perfectly axisymmetric in the radial range 8 to
, and
follows a spiral pattern with pitch angles of
to
. In the ring between 6 and
a
perturbation of the dominant axisymmetric mode may be present,
having the azimuthal wave number
. A systematic analysis of
the observed depolarization allows us to identify the main mechanism
for wavelength dependent depolarization – Faraday rotation measure
gradients arising in a magneto-ionic screen above the synchrotron
disk. Modelling of the depolarization leads to constraints on the
relative scale heights of the thermal and synchrotron emitting
layers in M 31; the thermal layer is found to be up to three times
thicker than the synchrotron disk. The regular magnetic field must
be coherent over a vertical scale at least similar to the scale
height of the thermal layer, estimated to be
.
Faraday effects offer a powerful method to detect thick
magneto-ionic disks or halos around spiral galaxies.
Key words: galaxies: magnetic fields / galaxies: individual: M 31 / galaxies: spiral / ISM: magnetic fields / radio continuum: galaxies / polarization
© ESO, 2004
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