2009ApJ...693....1O


Query : 2009ApJ...693....1O

2009ApJ...693....1O - Astrophys. J., 693, 1-7 (2009/March-1)

Can the cosmic ray driven dynamo model explain the observations of the polarized emission of edge-on galaxies?

OTMIANOWSKA-MAZUR K., SOIDA M., KULESZA-ZYDZIK B., HANASZ M. and KOWAL G.

Abstract (from CDS):

In the present paper, we construct maps of polarized synchrotron radio emission of a whole galaxy, based on local models of the cosmic ray driven dynamo. We perform numerical simulations of the dynamo in local Cartesian domains, with shear-periodic boundary conditions, placed at the different galactocentric radii. Those local solutions are concatenated together to construct the synchrotron images of the whole galaxy. The aim of the paper is to compare the model results with the observed radio continuum emission from nearly edge-on spiral galaxy. On the basis of the modeled evolution of the magnetic field structure, the polarization maps can be calculated at different time steps and at any orientation of the modeled galaxy. For the first time, a selfconsistent cosmic ray electron distribution is used to integrate synchrotron emissivity along the line of sight. Finally, our maps are convolved with the given radiotelescope beam. We show that it is possible to reconstruct the extended magnetic halo structures of the edge-on galaxies (so-called X-shaped structures).

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Journal keyword(s): galaxies: magnetic fields - MHD

Simbad objects: 7

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Number of rows : 7
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 NGC 253 SyG 00 47 33.134 -25 17 19.68   8.03   6.94 8.1 ~ 3588 2
2 NGC 891 H2G 02 22 32.907 +42 20 53.95 11.08 10.81 9.93 7.86   ~ 1741 2
3 NGC 3628 LIN 11 20 17.018 +13 35 22.16   10.42 9.48 9.22   ~ 853 3
4 NGC 4217 GiG 12 15 50.900 +47 05 30.44   12.4       ~ 324 2
5 NGC 4631 GiC 12 42 08.009 +32 32 29.44   9.78 9.19 9.10   ~ 1154 3
6 NGC 4666 AGN 12 45 08.676 -00 27 42.88   11.7   11.5 10.7 ~ 421 1
7 NGC 5775 GiG 14 53 57.653 +03 32 40.10   13.0 11.34     ~ 460 2

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