The data were obtained during two runs with the ESO 2.2 m telescope
with IRAC2B in 1996. The detector was a NICMOS-3 array with pixels of
size m, a Read Out Noise of 46 e- and a Gain of
6.6 e-/ADU. We used lenses B (0.278''/pix) and
C (0.507''/pix), that
give field sizes of
and
respectively. The
observing strategy for each object was the following: we first
obtained a J image with lense C and if it showed any hint of an
extension we changed to lense B
and obtained the K' image. Details on
the observations are given in Table 1.
For every target,
we obtained a number of images
(less than 1 minute exposure each)
shifting the quasar position by about 15''-20'' until the total
exposure time was attained. For the flux calibration we measured the
following standard stars: HD 29250, HD 56189, HD 84503, HD 105116 (first
run), HD 84090, HD 1148951, DM 597287, HD 177619 and SJ 9149 (second
run). The data reduction and calibration was performed, following the
standard procedures with the IRAF
software and SQIID package. We
used dome flat-fields by subtracting
the images taken with the lamps off from those taken with the lamps
on. We compute the median of object images to obtain the corresponding
sky frame. Sky-subtracted images were used to obtain the final
mosaics. We reach a photometric accuracy of about 10%. In Col. 9
of Table 1 we give the isophotal magnitude/arcsec2 corresponding to
2
of the background for the regions close to the quasar (where
the S/N is the highest). Total magnitudes given in Table 2 were
measured in circular apertures.
Deconvolution from the point spread function was performed using the
Lucy algorithm in the stsdas.analysis.restore package. We estimated
the shape of the PSF by using starlike objects in the field. Average
isophotal profiles were determined using the IRAF task ellipse
in the stsdas.analysis.isophote package.
We have computed the host galaxy contribution by subtracting the PSF profile
(for the images with suitable stars to compute the PSF) from that of
the quasar, forcing that the resulting profile has no central hole
(Aretxaga et al. 1995;
Rönnback et al. 1996); the magnitudes of the
host galaxies are given in Table 3. Since the
deconvolution procedure does not conserve calibrated fluxes, we have
deconvolved sky-subtracted non-calibrated images. This explains why
the deconvolved images are given with fluxes in arbitrary units
(Figs. 2, 12, 14 and 15).
Table 2 lists for every object detected in our images: (1)
our order number (mentioned in the text with a # symbol); (2) and (3)
abridged and
coordinates; (4) and (5)
and
positions relative to the quasar (the quasar coordinates were
taken from the Simbad database, in order to have more accurate values
than those written in the image headers); (6) and (7) our J and K'
magnitude measurements (note that the spatial coverage is smaller for
the higher resolution scale of the K' images); (8) R magnitudes from
published optical photometry; (9) references; (10) numbering in the
corresponding reference; (11) type of the object (1 = galaxy,
2 = probable
galaxy, 3 = star) given by the reference or, when no reference was
given, type assigned by us. When available, we also give the redshift
in Col. 11 in parentheses, with the corresponding reference; (12)
Yes for radio-loud, No for radio-quiet objects.
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To calculate absolute magnitudes we have used
|
A few of the objects closest to the quasar are indicated in the various plots (Figs. 1 to 16) with their corresponding numbers as given in Table 2, Col. 1. Whenever they are mentioned in the text we use the #number; when we mention the numbering given by other authors we just use the number.
We compare the infra-red images with optical HST images (Figs. 17 to 23) from the public archive when available to verifiy in particular that the extensions that we detect are not a consequence of the presence of close companions.
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Figure 2: Image of PKS 0812+020 in the J band after deconvolution for seeing effects. Contour levels are 0.075, 0.1, 0.2, 1 and 10 (in arbitrary units) |
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Figure 3: Image of PKS 0837-120 in the J band. Contour levels are 1.0 10-9, 2.2 10-9, 4.1 10-9, 8.0 10-9, 2.0 10-8 and 1.2 10-7 erg s-1 arcsec-2 |
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Figure 4: Image of 3C 215 in the J band. Contour levels are 2.4 10-9, 3.4 10-9, 5.3 10-9, 2.1 10-8 and 7.9 10-8 erg s-1 arcsec-2 |
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Figure 5: Image of IRAS 09149-6206 in the J band. Contour levels are 1.7 10-8, 1.9 10-8, 2.3 10-8, 3.5 10-8, 5.4 10-8 and 2.1 10-7 erg s-1 arcsec-2 |
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Figure 6: Image of PKS 1011-282 in the J band. Contour levels are 9.6 10-10, 1.7 10-9, 3.7 10-9, 1.9 10-8 and 1.9 10-7 erg s-1 arcsec-2 |
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Figure 7: Image of 3C 275.1 in the J band. Contour levels are 1.0 10-9, 1.7 10-9, 8.0 10-9 and 2.0 10-8 erg s-1 arcsec-2 |
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Figure 8: Image of PKS 1302-102 in the J band. Contour levels are 3.0 10-10, 8.9 10-10, 2.8 10-9, 6.7 10-9, 3.8 10-8 and 1.9 10-7 erg s-1 arcsec-2 |
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Figure 9: Image of 3C 281 in the J band. Contour levels are 9.9 10-10, 1.4 10-9, 2.2 10-9, 3.7 10-9, 2.9 10-9 and 2.2 10-8 erg s-1 arcsec-2 |
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Figure 10: Image of 4C 20.33 in the J band. Contour levels are 6.6 10-10, 1.2 10-9, 3.2 10-9, 1.9 10-8 and 1.9 10-7 erg s-1 arcsec-2 |
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Figure 11: Image of 4C 11.50 in the J band. Contour levels are 8.9 10-10, 2.1 10-9 and 9.8 10-9 erg s-1 arcsec-2 |
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Figure 12: Image of 4C 11.50 in the K' band corrected for seeing effects. Contour levels are 1, 1.5, 2, 5, 10 and 20 (in arbitrary units) |
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Figure 13: Image of MRK 877 in the J band. Contour levels are 2.8 10-9, 3.6 10-9, 5.1 10-9, 1.0 10-8, 3.0 10-8 and 2.0 10-7 erg s-1 arcsec-2 |
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Figure 14: Image of 3C 334 in the J band after deconvolution for seeing effects. Contour levels are 0.8, 1.0, 1.2, 2.0, 10 and 100 (in arbitrary units) |
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Figure 15: Image of MC 1745+163 in the J band. Contour levels are 3, 5, 7.5, 50 and 200 (in arbitrary units) |
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Figure 16: Image of 4C 11.72 in the J band. Contour levels are 7.4 10-10, 1.3 10-9, 2.5 10-9, 4.4 10-9, 1.1 10-8, 4.2 10-8 and 2.0 10-7 erg s-1 arcsec-2 |
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