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Spitzer IRS spectra
PKS0442-28
(Top) 5GHz
(Middle) Image of 0442-28 at 6-cm. The contour levels are: , 1, 2, 3, 4, 6, 8, 10, 15, 20, 25, 30, 50, 100, 200, 400 mJy beam-1. The peak flux is 197.0 mJy beam-1. (Bottom) Zoom-in of the southern (Right) and of the northern lobe (Left) of 0442-28 at 6-cm. with superimposed vectors indicating the projected electric field direction. The vectors are proportional in length to the fractional polarisation (1 arcsec = 1.0 ratio). The contour levels are: , 1, 2, 4, 8, 10, 15, 20, 25, 30, 40, 50 mJy beam-1
PKS0442-28
Spitzer IRS spectra
Dicken et al. (in preperation)
PKS0442-28
Spitzer MIPS infrared photometric observations. Left to right: 24 microns, 70 microns and 160 microns (when available). FOV are 5x5 arcmins for 24 microns, 5x2.5 arcmins for 70 microns and 0.5x5 arcmins for 160 microns.
Other name:
Redshift:
RA (j2000):
Dec (j2000):
Optical class:
Radio Class:
0.147
04 44 37.67
-28 09 54.6
NLRG
FRII
OF-271
N
E
Notes
The radio observations for this NLRG/FRII galaxy (Morganti et al. 1999) shows a complex morphology for its radio lobes. A core has been detected but no radio jets.
This object has strong, narrow optical emission lines [O III] λλ5007, 4959 and [O II] λ3727 (Tadhunter et al. 1993). The optical continuum colours may be slightly bluer than those of typical early type-galaxies and there are no clear detections of stellar absorption features. It is also detected in X-rays (Siebert et al. 1996), where it appears to be extended, even though this source is not known to be associated with a cluster.
The optical image shows a faint, but sharply defined shell ∼50 kpc to SW of its nucleus in our GMOS-S image (Ramos Almeida et al. 2011a). This shell has a surface brightness μ_V = 25.7 mag arcsec^−2. There are several galaxies within ∼20 arcsec, any of them possibly interacting with the radio galaxy.
Gemini/GMOS-S: median filtered image
5 GHz VLA radio map
PKS0442-28
Spectral energy distribution. The blue solid line is fitted to the data from 109 to 1010 Hz. Extrapolating this line from the radio to the infrared SED tests whether non-thermal synchrotron emission from the lobes can contaminate the Spitzer mid-infrared flux. In this case the lobes emission lies out of the Spitzer beam so cannot contaminate the Spitzer data. The weak, flat spectrum, non-thermal radio core emission is also not likely to contaminate the Spitzer infrared flux data for this object.