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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

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