Polarimetric structure in the first Galactic quadrant from the 2.695 GHz Effelsberg survey

Astronomy and Astrophysics – Astrophysics

Scientific paper

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Techniques: Polarimetric, Surveys, Ism: Magnetic Fields, Galaxy: General, Radio Continuum: General

Scientific paper

Polarimetric data from the 2.695 GHz Effelsberg survey of the Galactic Plane have been reduced, resulting in images of the Stokes Q and U emission components over Galactic longitudes given by 74degr >= l >= 4fdg9 , at a resolution of 4\farcm3. This extends the earlier work of Junkes et al. (1987a) out to the latitude limit of the survey observations (b = +/- 5degr ). Patchy, diffuse polarised emission is seen to extend to high latitudes (|b| = 5degr ), with generally brighter polarisation detected above |b| >~ 2degr . The distributions of both the polarised intensities and polarisation position-angles are shown, as a function of Galactic longitude, and compared with similar data from the southern Galactic Plane. These data will assist in higher resolution studies of the Galactic magnetic field and the magneto-ionic properties of the interstellar medium. Between longitudes of 20degr - 45degr , bright patches of polarised emission are detected, which exhibit quasi-periodic variations of the polarisation angles with scale-sizes of approximately 7degr . Both the characteristics and the possible origins of these structures are discussed. This bright emission appears to originate from the Sagittarius spiral arm, between distances of approximately 2.5 and 8 kpc. An anticorrelation between polarised intensities and regions of enhanced H I gas density (lying at kinematic distances of 2-2.5 kpc) is found. Possible mechanisms are suggested to account for this anticorrelation, arising through the action of a Faraday ``screen'' associated with the Sagittarius arm. The structured, quasi-periodic nature of the polarisation position-angles over this region of the Plane most likely results from a peculiar magnetic field geometry associated with the Sagittarius arm. With scale-sizes of between 200 and 600 pc, such magnetic field geometries may be produced by a mechanism similar to the Parker instability.

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