TY - JOUR
T1 - Faraday rotation structure on kiloparsec scales in the radio lobes of Centaurus A
AU - Feain, I. J.
AU - Ekers, R. D.
AU - Murphy, T.
AU - Gaensler, B. M.
AU - MacQuart, J.-P.
AU - Norris, R. P.
AU - Cornwell, T. J.
AU - Johnston-Hollitt, M.
AU - Ott, J.
AU - Middelberg, E.
PY - 2009
Y1 - 2009
N2 - We present the results of an Australia Telescope Compact Array 1.4 GHz spectropolarimetric aperture synthesis survey of 34 deg2 centered on Centaurus A-NGC 5128. A catalog of 1005 extragalactic compact radio sources in the field to a continuum flux density of 3 mJy beam-1 is provided along with a table of Faraday rotation measures (RMs) and linear polarized intensities for the 28% of sources with high signal to noise in linear polarization. We use the ensemble of 281 background polarized sources as line-of-sight probes of the structure of the giant radio lobes of Centaurus A. This is the first time such a method has been applied to radio galaxy lobes and we explain how it differs from the conventional methods that are often complicated by depth and beam depolarization effects. Assuming a magnetic field strength in the lobes of 1.3 B 1 μG, where B 1 = 1 is implied by equipartition between magnetic fields and relativistic particles, the upper limit we derive on the maximum possible difference between the average RM of 121 sources behind Centaurus A and the average RM of the 160 sources along sightlines outside Centaurus A implies an upper limit on the volume-averaged thermal plasma density in the giant radio lobes of 〈ne 〉 < 5 ÃÂ 10-5 B -1 1 cm-3. We use an RM structure function analysis and report the detection of a turbulent RM signal, with rms σRM = 17 rad m-2 and scale size 03, associated with the southern giant lobe. We cannot verify whether this signal arises from turbulent structure throughout the lobe or only in a thin skin (or sheath) around the edge, although we favor the latter. The RM signal is modeled as possibly arising from a thin skin with a thermal plasma density equivalent to the Centaurus intragroup medium density and a coherent magnetic field that reverses its sign on a spatial scale of 20 kpc. For a thermal density of n 1 10-3 cm-3, the skin magnetic field strength is 0.8 n -1 1 μG.
AB - We present the results of an Australia Telescope Compact Array 1.4 GHz spectropolarimetric aperture synthesis survey of 34 deg2 centered on Centaurus A-NGC 5128. A catalog of 1005 extragalactic compact radio sources in the field to a continuum flux density of 3 mJy beam-1 is provided along with a table of Faraday rotation measures (RMs) and linear polarized intensities for the 28% of sources with high signal to noise in linear polarization. We use the ensemble of 281 background polarized sources as line-of-sight probes of the structure of the giant radio lobes of Centaurus A. This is the first time such a method has been applied to radio galaxy lobes and we explain how it differs from the conventional methods that are often complicated by depth and beam depolarization effects. Assuming a magnetic field strength in the lobes of 1.3 B 1 μG, where B 1 = 1 is implied by equipartition between magnetic fields and relativistic particles, the upper limit we derive on the maximum possible difference between the average RM of 121 sources behind Centaurus A and the average RM of the 160 sources along sightlines outside Centaurus A implies an upper limit on the volume-averaged thermal plasma density in the giant radio lobes of 〈ne 〉 < 5 ÃÂ 10-5 B -1 1 cm-3. We use an RM structure function analysis and report the detection of a turbulent RM signal, with rms σRM = 17 rad m-2 and scale size 03, associated with the southern giant lobe. We cannot verify whether this signal arises from turbulent structure throughout the lobe or only in a thin skin (or sheath) around the edge, although we favor the latter. The RM signal is modeled as possibly arising from a thin skin with a thermal plasma density equivalent to the Centaurus intragroup medium density and a coherent magnetic field that reverses its sign on a spatial scale of 20 kpc. For a thermal density of n 1 10-3 cm-3, the skin magnetic field strength is 0.8 n -1 1 μG.
UR - http://handle.uws.edu.au:8081/1959.7/546902
U2 - 10.1088/0004-637X/707/1/114
DO - 10.1088/0004-637X/707/1/114
M3 - Article
SN - 0004-637X
VL - 707
SP - 114
EP - 125
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 1
ER -