Alma Mater Studiorum Universit`a degli Studi di Bologna ... - Inaf
Alma Mater Studiorum Universit`a degli Studi di Bologna ... - Inaf
Alma Mater Studiorum Universit`a degli Studi di Bologna ... - Inaf
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6.2. Two-<strong>di</strong>mensional analysis: rotation measure and depolarization 115<br />
IMAGE: 0755.RM.4.0_BLANK.FITS<br />
DECLINATION (J2000)<br />
37 48 00<br />
37 47 30<br />
37 47 00<br />
37 46 30<br />
;20 ;10 0 10 20<br />
RAD/M/M<br />
07 58 36<br />
07 58 32 07 58 28 07 58 24<br />
RIGHT ASCENSION (J2000)<br />
10 kpc<br />
DECLINATION (J2000)<br />
37 48 00<br />
37 47 30<br />
37 47 00<br />
37 46 30<br />
IMAGE: 0755.RM.1.3_BLANK.FITS<br />
;20 ;10 0 10 20<br />
RAD/M/M<br />
07 58 36<br />
07 58 32 07 58 28 07 58 24<br />
RIGHT ASCENSION (J2000)<br />
10 kpc<br />
07 58 20<br />
Figure 6.4: Images of the rotation measure for 0755+37, computed from weighted least-squares<br />
fits to the position angle –λ 2 relation at frequencies of 1385.1, 1469.1 and 4860.1 MHz. The<br />
angular resolutions are 4.0 arcsec FWHM (left) and 1.3 arcsec FWHM (right).<br />
IMAGE: 0755_K;BURN_4ARCSEC_4SIGMAP.FITS<br />
0 100 200 300 400<br />
rad^2/m^4<br />
IMAGE: 0755_K;BURN_1.3ARCSEC.FITS<br />
0 100 200 300 400<br />
rad^2/m^4<br />
37 48 00<br />
37 48 00<br />
DECLINATION (J2000)<br />
37 47 30<br />
37 47 00<br />
37 46 30<br />
DECLINATION (J2000)<br />
37 47 30<br />
37 47 00<br />
37 46 30<br />
07 58 36<br />
07 58 32 07 58 28 07 58 24<br />
RIGHT ASCENSION (J2000)<br />
07 58 36<br />
07 58 32 07 58 28 07 58 24<br />
RIGHT ASCENSION (J2000)<br />
07 58 20<br />
Figure 6.5: Images of Burn law k for 0755+37 computed from weighted least-squares fits to the<br />
relation p(λ)= p(0)exp(−kλ 4 ) at frequencies of 1385.1, 1469.1 and 4860.1 MHz. The angular<br />
resolutions are 4.0 arcsec FWHM (left) and 1.3 arcsec FWHM (right).<br />
This scenario is confirmed by the profiles of〈k〉 across the source (Fig. 6.6): at lower resolution<br />
the profile is asymmetrical, with less depolarization at a given <strong>di</strong>stance from the core in the E lobe<br />
and a peak which is <strong>di</strong>splaced slightly W of the nucleus. In contrast, the〈k〉 profile at 1.3 arcsec<br />
resolution is symmetrical and lies significantly below that at 4.0 arcsec.<br />
The high k values in the W lobe at the lower resolution are mostly seen in a cone-like structure<br />
(Fig. 6.5 left), as was already pointed out by Bon<strong>di</strong> et al. (2000). It is possible that the origin of<br />
such structure may be gas and field compression or the development of a mixing layer as <strong>di</strong>scussed<br />
for M 84 and 3C 270 (Sec. 5.8.5). To confirm this picture, higher resolution X-ray observations are<br />
needed. In contrast, a region with very low and almost constant depolarization is observed at the<br />
lea<strong>di</strong>ng edge of the W lobe, beyond the end of the approaching jet.<br />
115