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2. Observations and data reduction

2.1. The VLA maps

The 10-kpc "ring'' of M 31 has an angular diameter along the major axis of tex2html_wrap_inline1270 while the beamsize of a single VLA telescope (the primary beam) at tex2html_wrap_inline122820 cm is only tex2html_wrap_inline1274. To cover the whole area, observations of 7 fields ("pointings'') with the VLA-D array were collected during 9 years (Table 1). The angular resolution is 45tex2html_wrap1248 . As the upgrade of the L-band systems took place between 1990 and 1993, only the last 3 pointings could profit from the improved sensitivity. Unfortunately, at the same time the interference situation became worse so that the second IF at 1515 MHz could not be used anymore. The rms noise in the final maps varies between the different pointings due to different observation times, different system sensitivities and a different amount of data affected by interference. In linear polarization, the rms noise is almost the same for all pointings.

Table 1: VLA observations

All data were reduced at the MPIfR Bonn using the standard AIPS package. 3C 48 and 3C 138 were used for absolute flux density and polarization angle calibration, 0038+328 for gain and phase calibration. Self-calibration was performed on each field individually using the AIPS task ASCAL. Comparison of the total flux densities of unresolved background sources in overlapping regions of two (or more) fields yielded good consistency within a few percent, except for field A (the first one observed). Here all flux densities were found to be higher by tex2html_wrap_inline1282, for which the maps in Stokes parameters I(total intensity), Q and U were corrected.

For each Stokes parameter the maps of all fields were combined by applying the AIPS task LPTES which is similar to the standard LTESS, but cuts the individual maps at a chosen radius from the field centre. We chose a radius where the sensitivity is down to tex2html_wrap_inline1290 in order to avoid a large increase of the noise level at the edges of the combined map. The combined maps in Stokes Q and U were transformed into maps of the polarization angle and of the polarized intensity by taking tex2html_wrap_inline1296 where tex2html_wrap_inline1298 (Wardle & Kronberg 1974).

The resulting maps in total and linearly polarized intensities are shown in Figs. 1 (click here) and 2 (click here), respectively. The rms noise within the main regions of M 31 is tex2html_wrap_inline1300 in total power and tex2html_wrap_inline1302 in polarized intensity, increasing to about twice these values at the singly-covered map edges. Hence these maps represent the most sensitive radio continuum survey of M 31 so far and the first one in linear polarization with the VLA.

Figure 1: Mosaic of 7 fields on M 31 showing the total power emission at tex2html_wrap_inline122820.5 cm observed with the VLA-D array. The angular resolution is 45tex2html_wrap1248 . The rms noise generally is tex2html_wrap_inline1300 increasing to tex2html_wrap_inline1310 at the borders of the map

Figure 2: Mosaic of 7 fields on M 31 showing the linearly polarized emission at tex2html_wrap_inline122820.5 cm observed with the VLA-D array. The angular resolution is 45tex2html_wrap1248 . The rms noise generally is tex2html_wrap_inline1302 increasing to tex2html_wrap_inline1318 at the borders of the map. Point sources brighter than 1 mJy in polarized intensity are subtracted. The position of the bright "ring'' is shown by contours of the total emission (see Fig. 4). The contour levels are 0.6, 1.2, 1.8, 2.4, 3.0 and 6.0 mJy/beam

2.2. The Effelsberg map

The largest structure visible to the VLA-D array at tex2html_wrap_inline122820.5 cm is tex2html_wrap_inline1342 due to the lack of short interferometer spacings. To fill these short spacings, observations at 1400 MHz (tex2html_wrap_inline122821.4 cm) were performed with the 100-m Effelsberg telescope of the MPIfR between 1993 and 1995. The bandwidth used was 20 MHz. The system temperature was 26 K and the angular resolution 9tex2html_wrap1368 35. A field of tex2html_wrap_inline1348 in M 31 coordinates (tex2html_wrap_inline1350 position angle of the major axis) was scanned 2 times in tex2html_wrap_inline1228- and 3 times in tex2html_wrap_inline1354-direction, yielding a noise level of tex2html_wrap_inline1356. The scanning effects were removed by a weighted addition of the maps with different scanning angles in the Fourier plane (see Emerson & Gräve (1988) for explanation of the algorithm).

M 31 is located on a spur of Galactic radio continuum emission (Gräve et al. 1981). Subtraction of this foreground emission in total intensity was achieved by a careful application of the BGF algorithm (Sofue & Reich 1979) after subtraction of known background point sources.

The final map in total intensity is shown in Fig. 3 (click here). Unfortunately, at this low angular resolution the polarized emission from M 31 cannot be separated from that from the Galactic foreground.

Figure 3: Total emission (contours) and E-vectors of the polarized emission at tex2html_wrap_inline1358 cm of a tex2html_wrap_inline1348 field containing M 31 observed with the 100-m Effelsberg telescope. The angular resolution is 9tex2html_wrap1368 35. The rms noise is about 5 mJy/beam. Contour levels are 20, 40, ..., 100, 160, 200, 300, ..., 600 mJy/beam. The maximum polarized intensity of 121 mJy/beam corresponds to a vector plotted with 11tex2html_wrap1266\ length

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