This high redshift object was first identified and
studied by Chambers et
al 1988. Infrared spectroscopy has been obtained by Rawlings and
Eales 1993. A small
4" double, 4C40.36 is remarkable for the very high degree of asymmetry
in the radio
polarization properties of the two lobes (Figure 7). In this and other
respects it is quite similar to 4C24.28 discussed above.
The eastern lobe B is completely depolarized at all frequencies. At high spatial resolution A has a bright extension to the north and faint lobe emission to the south. The polarization image at 20 cm (Fig 7c) is extended to the south, at 6 cm the polarization peaks at the extremity of the lobe, and at 2 cm it is (marginally) extended and peaks north of the total intensity image. If the depolarization of 4C40.36 is due to an enveloping medium as suggested by the Laing-Garrington effect then this structure suggests that we are seeing the southwestern lobe A in the foreground, and the we see it through the northeastern edge of the lobe.
Redshifted Ly emission is in the U band, so this image
(Figure 7b) is part line and
part ultraviolet continuum. It is extended and aligned with the
radio axis. The morphology
in this band has a slight opening to the west. In V band the peak
is X compared to the
radio source. Towards the red the peak becomes more compact. In the
R and I band the
aligned continuum westward of the peak is has become quite faint.
Since the emission lines
in 4C40.36 are bright, some of the features in the broad band images
may be contaminated
by different emission lines. The continuum emission is the most
compact in the I band (Fig
7e), but still has an aligned component. The K band image is of
poor quality, it is not clear
if the misaligned structure is real or not.
A faint diffuse object can be seen 2" to the southeast of the eastern lobe. It is detected in all the optical bands and possibly in the K band. It has very similar colors to 4C40.36 and is an excellent candidate for a companion (or subcomponent) of 4C40.36.