2018A&A...613A..74P


Query : 2018A&A...613A..74P

2018A&A...613A..74P - Astronomy and Astrophysics, volume 613A74-74 (2018/5-1)

Broadband radio spectro-polarimetric observations of high-Faraday-rotation-measure AGN.

PASETTO A., CARRASCO-GONZALEZ C., O'SULLIVAN S., BASU A., BRUNI G., KRAUS A., CURIEL S. and MACK K.-H.

Abstract (from CDS):

We present broadband polarimetric observations of a sample of high-Faraday-rotation-measure (high-RM) active galactic nuclei (AGN) using the Karl. G. Jansky Very Large Array (JVLA) telescope from 1 to 2GHz, and 4 to 12GHz. The sample (14 sources) consists of very compact sources (linear resolution smaller than ~=5kpc) that are unpolarized at 1.4GHz in the NRAO VLA Sky Survey (NVSS). Total intensity data have been modeled using a combination of synchrotron components, revealing complex structure in their radio spectra. Depolarization modeling, through the so-called qu-fitting (the modeling of the fractional quantities of the Stokes Q and U parameters), has been performed on the polarized data using an equation that attempts to simplify the process of fitting many different depolarization models. These models can be divided into two major categories: external depolarization (ED) and internal depolarization (ID) models. Understanding which of the two mechanisms is the most representative would help the qualitative understanding of the AGN jet environment and whether it is embedded in a dense external magneto-ionic medium or if it is the jet-wind that causes the high RM and strong depolarization. This could help to probe the jet magnetic field geometry (e.g., helical or otherwise). This new high-sensitivity data shows a complicated behavior in the total intensity and polarization radio spectrum of individual sources. We observed the presence of several synchrotron components and Faraday components in their total intensity and polarized spectra. For the majority of our targets (12 sources), the depolarization seems to be caused by a turbulent magnetic field. Thus, our main selection criteria (lack of polarization at 1.4GHz in the NVSS) result in a sample of sources with very large RMs and depolarization due to turbulent magnetic fields local to the source. These broadband JVLA data reveal the complexity of the polarization properties of this class of radio sources. We show how the new qu-fitting technique can be used to probe the magnetized radio source environment and to spectrally resolve the polarized components of unresolved radio sources.

Abstract Copyright: © ESO 2018

Journal keyword(s): polarization - radiation mechanisms: non-thermal - techniques: polarimetric - galaxies: active - radio continuum: galaxies

Simbad objects: 21

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Number of rows : 21
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 3C 48 QSO 01 37 41.2996631208 +33 09 35.080388820   16.62 16.20     ~ 2924 2
2 QSO B0237-027 Bla 02 39 45.47227239 -02 34 40.9145702   19.5 21 19.04   ~ 145 1
3 QSO B0240-060 Bla 02 43 12.46947413 -05 50 55.2953784   18.2 19.0 19.11   ~ 67 1
4 NGC 1275 Bla 03 19 48.1599902040 +41 30 42.108850836   13.10 12.48 11.09   ~ 4243 3
5 ICRF J052109.8+163822 Sy1 05 21 09.88596258 +16 38 22.0515459   19.37 18.84 18.480   ~ 910 1
6 QSO B0710+439 QSO 07 13 38.16413557 +43 49 17.2072102   20.7       ~ 256 0
7 QSO J0751+2716 QSO 07 51 41.517 +27 16 31.79     18.7     ~ 86 2
8 ICRF J084517.1+043947 QSO 08 45 17.14370848 +04 39 47.3553476   21.14   19.51   ~ 25 1
9 Ton 469 Bla 09 58 20.9496221568 +32 24 02.208417372   15.88 15.78 15.51   ~ 442 1
10 PKS 1045+019 Rad 10 48 22.86793321 +01 41 48.1139712           ~ 30 1
11 6C 114405+541331 Bla 11 46 44.20434354 +53 56 43.0826910   20.5 20.5 19.82   ~ 72 1
12 QSO J1246-0730 Bla 12 46 04.23211565 -07 30 46.5746985   17.6 18.0 18.2   ~ 198 1
13 [VV2006] J131107.8+141746 Bla 13 11 07.82422420 +14 17 46.6482535   20.11 19.97 19.6   ~ 57 1
14 SDSS J131253.19+554813.2 QSO 13 12 53.1977917080 +55 48 13.115320488           ~ 25 2
15 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4558 2
16 QSO B1402+044 Bla 14 05 01.11981857 +04 15 35.8188818   19.86 19.53 19.22   ~ 204 1
17 Mrk 668 BLL 14 07 00.39441712 +28 27 14.6901341   16.13 15.35 10.29   ~ 826 3
18 QSO B1547+507 Bla 15 49 17.46855793 +50 38 05.7880702   18.89 18.74 18.16   ~ 140 1
19 QSO B1614+051 Bla 16 16 37.55681923 +04 59 32.7365717   19.60 19.17 19.49   ~ 195 2
20 [VV98] J224528.3+032409 Bla 22 45 28.28475081 +03 24 08.8639113   18.5 19.0 17.55   ~ 48 1
21 6C 235239+493337 BLL 23 55 09.45814429 +49 50 08.3394994   21.101   18.400   ~ 284 1

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