2011ApJ...728...57L


Query : 2011ApJ...728...57L

2011ApJ...728...57L - Astrophys. J., 728, 57 (2011/February-2)

Spectropolarimetry with the allen telescope array: Faraday rotation toward bright polarized radio galaxies.

LAW C.J., GAENSLER B.M., BOWER G.C., BACKER D.C., BAUERMEISTER A., CROFT S., FORSTER R., GUTIERREZ-KRAYBILL C., HARVEY-SMITH L., HEILES C., HULL C., KEATING G., MacMAHON D., WHYSONG D., WILLIAMS P.K.G. and WRIGHT M.

Abstract (from CDS):

We have observed 37 bright, polarized radio sources with the Allen Telescope Array (ATA) to present a novel analysis of their Faraday rotation properties. Each source was observed during the commissioning phase with two to four 100 MHz bands at frequencies ranging from 1 to 2 GHz. These observations demonstrate how the continuous frequency coverage of the ATA's log-periodic receiver can be applied to the study of Faraday rotation measures (RMs). We use RM synthesis to show that wide-bandwidth data can find multiple RM components toward a single source. Roughly a quarter of the sources studied have extra RM components with high confidence (brighter than ~40 mJy), when observing with an RM resolution of roughly 100 rad/m2. These extra components contribute 10%-70% of the total polarized flux. This is the first time multiple RM components have been identified in a large sample of point sources. For our observing configuration, these extra RM components bias the measurement of the peak RM by 10-15 rad/m2; more generally, the peak RM cannot be determined more precisely than the RM beam size. Comparing our 1-2 GHz RM spectra to Very Long Baseline Array (VLBA) polarimetric maps shows that both techniques can identify complicated Faraday structures in the sources. However, the RM values and fractional polarization are generally smaller at lower frequencies than in the higher frequency VLBA maps. With a few exceptions, the RMs from this work are consistent with that of earlier, narrow-bandwidth, all-sky surveys. This work also describes the polarimetry calibration procedure and that on-axis ATA observations of linear polarization can be calibrated to an accuracy of 0.2% of Stokes I. Future research directions include studying the time-dependent RM structure in active galactic nuclei and enabling accurate, wide-area RM surveys to test models of Galactic and extragalactic magnetic fields.

Abstract Copyright: ∼

Journal keyword(s): galaxies: magnetic fields - radio continuum: galaxies - surveys - techniques: polarimetric

Nomenclature: Table 5: [LGB2011] JHHMMSS+DDMMSS N=5.

Simbad objects: 45

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Number of rows : 45
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 8C 0052+681 Sy2 00 56 01.122 +68 22 29.53           ~ 74 1
2 Z 384-48 rG 00 57 34.90446247 -01 23 27.5469897   14.07 15.10     ~ 269 1
3 2C 94 Sy2 01 08 52.8701830824 +13 20 14.262799812   15.19       ~ 494 2
4 [LGB2011] J010855+132214 Rad 01 08 55.0 +13 22 14           ~ 1 0
5 3C 41.0 rG 01 26 44.388 +33 13 11.22   21       ~ 172 1
6 3C 61.1 Sy2 02 23 13.4857575951 +86 19 13.422392083     19.0     ~ 210 1
7 NGC 1218 Sy1 03 08 26.22380005 +04 06 39.3007808   12.84       ~ 413 0
8 2MASSI J0352305-071102 Sy1 03 52 30.5518280976 -07 11 02.326141644   17.02 16.67     ~ 163 1
9 ICRF J052109.8+163822 Sy1 05 21 09.88596258 +16 38 22.0515459   19.37 18.84 18.480   ~ 910 1
10 LEDA 19313 Sy2 06 36 32.2509554376 -20 34 53.181243300   18.27 17.58     ~ 139 2
11 4C 56.16 rG 07 49 48.077 +55 54 19.45           ~ 176 1
12 4C 71.07 Bla 08 41 24.36528508 +70 53 42.1730435     17.30 16.8   ~ 818 1
13 ATO J146.9381+07.4223 Sy1 09 47 45.1433922288 +07 25 20.595729756   17.37 16.95     ~ 389 1
14 4C 12.37 QSO 10 42 44.6052783816 +12 03 31.263917976   18.03 17.77     ~ 448 2
15 QSO J1130-1449 Bla 11 30 07.0523452128 -14 49 27.388021944   17.17 16.90 16 16.97 ~ 739 1
16 3C 273 BLL 12 29 06.6998257176 +02 03 08.597629980   13.05 14.830 14.11   ~ 6022 1
17 [LGB2011] J123049+122323 Rad 12 30 49.0 +12 23 23           ~ 1 0
18 NAME M87 Jet Rad 12 30 49.423 +12 23 28.04           ~ 315 1
19 M 87 AGN 12 30 49.42338414 +12 23 28.0436859 10.16 9.59 8.63   7.49 ~ 7815 3
20 3C 274.1 rG 12 35 22.97 +21 20 18.3   20       ~ 144 0
21 [LGB2011] J123530+212048 Rad 12 35 30.0 +21 20 48           ~ 1 0
22 3C 279 Bla 12 56 11.16657958 -05 47 21.5251510   18.01 17.75 15.87   ~ 3205 2
23 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4558 2
24 3C 321 Sy1 15 31 43.46520 +24 04 18.9948   16.0   15.40   ~ 341 1
25 IRAS 15599+0206 Sy1 16 02 27.3724911037 +01 57 56.238625559   17.70 16.31     ~ 250 1
26 NAME 3C 330G2 Sy2 16 09 34.92456720 +65 56 37.8351240   20.33       ~ 280 1
27 3C 341 rG 16 28 04.049 +27 41 43.07   19       ~ 146 1
28 3C 345 Bla 16 42 58.80997043 +39 48 36.9939552   16.81 16.59 16.84   ~ 1808 3
29 MCG+01-43-006 SyG 16 51 07.9886687784 +04 59 35.547131472     18.25     ~ 502 1
30 4C -00.67 Sy2 17 20 28.1680537512 -00 58 46.582453920   15.36       ~ 345 1
31 [LGB2011] J172034-005843 Rad 17 20 34.0 -00 58 43           ~ 1 0
32 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
33 [LGB2011] J184150+794728 Rad 18 41 50.0 +79 47 28           ~ 1 0
34 3C 390.3 Bla 18 42 08.9904975672 +79 46 17.127835104   16.06 15.38     ~ 1381 1
35 QSO B1921-293 BLL 19 24 51.05595254 -29 14 30.1210248   18.71 18.21 15.07   ~ 918 1
36 PKS J1941-1524 Sy1 19 41 14.9996710393 -15 24 31.311811663           ~ 83 1
37 NVSS J195904+393805 Rad 19 59 04.92 +39 38 05.7           ~ 2 0
38 NVSS J200259+410150 Rad 20 02 59.80 +41 01 50.0           ~ 2 0
39 4C 33.50 Rad 20 17 13.149 +33 45 46.67           ~ 11 1
40 PKS 2113-21 rG 21 16 36.0876 -20 55 43.924           ~ 29 1
41 3C 433.0 Sy2 21 23 44.5778423928 +25 04 27.670672416   17.660 16.350     ~ 338 1
42 3C 446 BLL 22 25 47.25929101 -04 57 01.3907626   18.83 18.39 16.3   ~ 863 1
43 3C 454.3 Bla 22 53 57.7480438728 +16 08 53.561508864   16.57 16.10 15.22   ~ 3004 2
44 PKS J2319-2728 rG 23 19 56.2948629696 -27 28 12.172353060   17.5       ~ 30 1
45 NAME Cas A SNR 23 23 26.0 +58 48 41     14.30     ~ 3033 1

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