A&A 386, 97-113 (2002)
DOI: 10.1051/0004-6361:20020119

The Parkes quarter-Jansky flat-spectrum sample

I. Sample selection and source identifications[*]

C. A. Jackson 1 - J. V. Wall 2 - P. A. Shaver 3 - K. I. Kellermann 4 - I. M. Hook 2 - M. R. S. Hawkins 5


1 - Research School of Astronomy & Astrophysics, The Australian National University, Mount Stromlo Observatory, Canberra, Australia
2 - Department of Astrophysics, University of Oxford, Nuclear and Astrophysics Laboratory, Keble Road,
Oxford OX1 3RH, UK
3 - European Southern Observatory, Karl-Schwarzschild-Str. 2, 85748 Garching bei München, Germany
4 - National Radio Astronomy Observatory, Edgemont Road, Charlottesville, VA 22903-2475, USA
5 - Royal Observatory, Blackford Hill, Edinburgh EH3 9HJ, UK

Received 7 November 2001 / Accepted 22 January 2002

Abstract
We present a new sample of quarter-Jansky flat-spectrum radio sources selected to search for high-redshift quasars and to study the evolution of the flat-spectrum quasar population. The sample comprises 878 radio sources selected from the Parkes catalogues with spectral indices $\alpha^{5 \rm
\thinspace GHz}_{2.7 \rm\thinspace GHz} \ge -$0.4 where $S_{\nu}
\propto \nu^{\alpha}$. The sample covers all right ascensions and the declination range from $-80\hbox{$.\!\!^\circ$ }0$ to $+2\hbox{$.\!\!^\circ$ }5$, excluding low galactic latitudes ( $\mid b \mid < 10^{\circ }$) and the Magellanic Cloud regions. We have obtained improved radio source positions, firstly to reconfirm the majority of the existing identifications, and secondly, using digitized sky-survey data and deep B, Gunn-i and Gunn-z CCD-imaging, to find optical identifications for 223 previously-unidentified sources. We present the final catalogue of 878 flat-spectrum sources: 827 are compact radio sources identified with galaxies, quasars and BLLac objects, 38 have either extended radio structure or are identified with Galactic objects (PN, HII or non-compact radio source), 4 are obscured by Galactic stars, and 9 (1 per cent of the total sample) remain unidentified.

Key words: catalogues - radio continuum: galaxies - BL Lac objects: general - galaxies: general - quasars: general


1 Introduction

This is the first paper in a series of three describing the results of a program to search for high-redshift quasars and study the evolution of the flat-spectrum quasar population.

This paper (Paper I) sets out the sample, discussing its selection and the identification and reconfirmation programme to determine the optical counterparts to the radio sources. Paper II (Hook et al. in preparation) presents new spectroscopic observations and redshift determinations. Paper III (Wall et al. in preparation) considers quasar space distribution, the luminosity function and its epoch dependence. An earlier version of this sample was used by Shaver et al. (1996) to study the evolution of the quasar space density at redshifts greater than 3.

We selected our radio source sample from the machine-readable version of the composite Parkes radio source catalogue (PKSCAT90: Wright & Otrupcek 1990). This catalogue comprises radio and optical data collected for 8264 radio sources for the sky south of +27$^{\circ}$, excluding the Galactic Plane and Magellanic Cloud regions. The catalogue was compiled from major radio surveys at 2.7  GHz undertaken by John Bolton and colleagues over the years 1969 to 1979 (Bolton et al. 1979 and references therein).

Samples extracted from PKSCAT90 contain source-identification information compiled over the last 30 years or more in numerous collaborations, resulting in several complete or near-complete samples, e.g. the 2-Jy sample (Wall & Peacock 1985), the Parkes Selected Regions (Downes et al. 1986; Dunlop et al. 1989, 1991) and the Parkes half-Jansky sample (Drinkwater et al. 1997).

Our goal was to obtain a spectroscopic sample of flat-spectrum radio-selected quasars, free of optical selection effects and complete at high redshifts. Starting with a sample selected from PKSCAT90 and the identifications therein we therefore had to ensure that we (i) identified the remaining PKSCAT90 sources and (ii) obtained redshifts for all candidate quasars in the sample, with priority given to those north of $-40^{\circ}$ declination.

The results of our selection, identification and confirmation programme are described in this paper as follows. Section 2 gives the selection criteria for the sample and some characteristics of the identified and empty field sources. In Sect. 3 we describe the procedure for identifying the PKSCAT90 empty-field sources and in Sect. 4 we analyse the reliability of the complete sample. In Sect. 5 we present the full catalogue and in Sect. 6 we summarise the characteristics of the final sample.

2 Radio source selection

The sample of flat-spectrum radio sources was selected from PKSCAT90 using the following criteria -

1.
$-80\hbox{$.\!\!^\circ$ }0 < \delta$ (B1950) $< +2\hbox{$.\!\!^\circ$ }5$, all right ascensions;

2.
$\alpha_{2.7 \rm\thinspace GHz}^{5.0 \rm\thinspace GHz} >
-0.4$, where $S \propto \nu ^{\alpha }$;

3.
Galactic latitude $\mid b \mid > 10^{\circ}$.

Sources lying within the Magellanic Cloud regions (B1950 RA, Dec = 04 30 hrs to 06 30 hrs, -64$^{\circ}$ to -75$^{\circ}$ for the LMC and 00 hrs to 02 hrs, -69$^{\circ}$ to -76$^{\circ}$ for the SMC) were excluded from our sample. We also checked the 2.7  GHz and 5  GHz flux densities extracted from PKSCAT90 against the original survey papers listed in Table 2. A number of sources have more recent flux density measurements recorded by PKSCAT90; we replaced these with the original survey flux densities for consistency. In addition, we find 10 sources in PKSCAT90 which are not in the original survey papers (Table 1): 3 of these sources lie in regions not covered by the original Parkes surveys. The other 7 sources are within the original survey areas listed in Table 2 but are not in the original survey papers.
 

 
Table 1: PKSCAT90 sources not in original Parkes Survey papers.
Source Region(1)
PKS B0522-030 A
PKS B0528-454 J
PKS B0549-459 J
PKS B1131-115 B
PKS B1150-723 K
PKS B1159-515 H
PKS B1718-649 X
PKS B1730-130 X
PKS B1801+010 X
PKS B2111+015 A


Notes: (1) The original Parkes survey region (see Table 2).


A cut-off value of -0.4 for the spectral index was applied to minimize the number of extended or non-core-dominated radio sources in the sample. However, such sources still contaminate the sample, due to one or more of the following reasons:

1.
Flux density uncertainties: the original Parkes survey flux densities at 2.7  GHz and 5  GHz have uncertainties of ((0.02)2 + (0.03S)2)0.5. Therefore there will be objects with $\alpha^ {5 \rm
\thinspace GHz}_{2.7 \rm\thinspace GHz} < -0.4$ in the sample.

A few nearby sources have a different type of flux-density error, due to diffuse lobe emission that has been poorly mapped and errors in one or both flux densities can result in $\alpha^ {5 \rm
\thinspace GHz}_{2.7 \rm\thinspace GHz} < -0.4$. PKS B0123-016 (3C40) is a case in point.

2.
Confusion: the Parkes beam sizes of 8 arcmin at 2.7  GHz and 4 arcmin at 5  GHz result in occasional instances of source confusion.
3.
Source variability: there are two effects here. The first is due to the time interval between the 2.7  GHz and 5  GHz flux density measurements; a number of steep-spectrum sources are included in our sample whilst a number flat-spectrum sources are missed as the source varied. The second effect is that neither flux density determination measured the mean source flux density, with the result that a number of sources are missed or included depending on their activity at the time of the survey. Drinkwater et al. (1997) analysed the magnitude of these effects for the 0.5-Jy Parkes survey sample which has a steeper spectral-index selection ( $\alpha_{2.7 \rm\thinspace
GHz}^{5.0 \rm\thinspace GHz} > -0.5$) and concluded that 1) the time lag between the surveys includes about 3 per cent steep-spectrum sources and misses a similar proportion of true flat-spectrum sources, and 2) the difference between the Parkes survey flux densities and mean flux densities results in $\sim$11 per cent of the sample having mean flux densities below any survey area's flux density limit, whilst $\sim$8 per cent of sources are missed. The latter bias is inherent in any single-epoch flux-limited sample.

To assess the magnitude of these effects we have compared 694 sources common to our sample and NVSS (Condon et al. 1998). We find that the vast majority - 663 out of 694 (96 per cent) - are either compact (unresolved by NVSS, major axis <15 arcsec) or are extended sources with an obvious dominant radio core so that unambiguous identification is possible. Thus we conclude that the incidence of non-core dominated, steep-spectrum sources in our complete sample is less than 5 per cent.
 

 
Table 2: The Parkes Survey regions.
      $S_{\rm lim,\, 2.7~\rm GHz}$    
Area Dec range RA range / Jy Reference N(1)
A +2 $.\!\!^\circ$5 to -4$^{\circ}$ 7$^{\rm h}$20 to 17$^{\rm h}$50, 19$^{\rm h}$40 to 6$^{\rm h}$ 0.25(2) Wall et al. (1971) 147 (+2)
B -4$^{\circ}$ to -15$^{\circ}$ 10$^{\rm h}$ to 15$^{\rm h}$ 0.25 Bolton et al. (1979) 56 (+1)
C -15$^{\circ}$ to -30$^{\circ}$ 10$^{\rm h}$ to 15$^{\rm h}$ 0.25 Savage et al. (1977) 65
D -4$^{\circ}$ to -30$^{\circ}$ 22$^{\rm h}$ to 5$^{\rm h}$ 0.25 Wall et al. (1976) 157
E -4$^{\circ}$ to -30$^{\circ}$ 5$^{\rm h}$ to 6$^{\rm h}$30, 8$^{\rm h}$ to 10$^{\rm h}$      
    15$^{\rm h}$ to 17$^{\rm h}$, 19$^{\rm h}$ to 22$^{\rm h}$ 0.6 Bolton et al. (1975) 64
F -18 $^{\circ}.8\pm2^{\circ}.6$ 22 $^{\rm h}\pm2\hbox{$.\!\!^\circ$ }6$ 0.10 Wall et al. (1971) 9
G -30$^{\circ}$ to -35$^{\circ}$ 9$^{\rm h}$ to 16$^{\rm h}$30, 18$^{\rm h}$30 to 7$^{\rm h}$15 0.2 Shimmins & Bolton (1974) 91
H -33$^{\circ}$ to -75$^{\circ}$ 3$^{\rm h}$, 11$^{\rm h}$, 19$^{\rm h}$, 23$^{\rm h}$ 0.25 Shimmins (1971) 66 (+1)
I -35$^{\circ}$ to -45$^{\circ}$ 10$^{\rm h}$ to 15$^{\rm h}$, 19$^{\rm h}$ to 7$^{\rm h}$ 0.25 Bolton & Shimmins (1973) 79
J -45$^{\circ}$ to -65$^{\circ}$ 0$^{\rm h}$ to 3$^{\rm h}$, 4$^{\rm h}$ to 8$^{\rm h}$30      
    17$^{\rm h}$30 to 19$^{\rm h}$, 20$^{\rm h}$ to 23$^{\rm h}$ h 0.5 Wall et al. (1975) 74 (+2)
K -65$^{\circ}$ to -75$^{\circ}$ 0$^{\rm h}$ to 24$^{\rm h}$ 0.25 Bolton & Butler (1975) 32 (+1)
L -75$^{\circ}$ to -80$^{\circ}$ 0$^{\rm h}$ to 24$^{\rm h}$ 0.2 Shimmins & Bolton (1972) 28
X all other areas not covered by original Parkes surveys 0.25 PKSCAT90 3


Notes: (1) Number of sources each region contributes to our sample. The number in parenthesis is the number of sources which are in this region but not in the referenced paper (see Table 1). (2) Region A includes 21 sources lying in 5 regions, each of 40 square degrees with $S_{2.7 \rm ~ GHz}$ = 0.1  Jy as shown in Fig. 1.



  \begin{figure}
\par\includegraphics[angle=270,width=18cm,clip]{H3277F1.epsi} %
\end{figure} Figure 1: Sky distribution of the Parkes quarter-Jansky flat-spectrum sources within the Parkes survey regions. Radio sources identified with galaxies and stellar objects are shown as circles with the size of the circle being proportional to the 2.7  GHz flux density. Parkes 2.7  GHz survey limits are shown in shades of grey, from dark to light, equating to $S_{2.7 \rm ~ GHz}$ of 0.10, 0.20, 0.25 and 0.60 Jy. Sources in the Magellanic Cloud regions and near the Galactic equator ( $\mid b \mid < 10^{\circ }$) are excluded from the sample.
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Figure 1 shows the distribution of the 878 quarter-Jansky sample sources within the Parkes survey regions. Of these, 645 have an optical identification given in PKSCAT90, with the majority, 535 (82 per cent), with stellar objects (quasars or BL Lacs). Moreover, it is the brighter radio sources which are identified, leaving the majority of the 247 unidentified (Parkes empty-field) sources with 2.7  GHz flux densities below 0.6  Jy (Fig. 2). In contrast, the distribution of spectral indices between identified and unidentified sources is unbiased (Fig. 3).


  \begin{figure}
\par\includegraphics[angle=270,width=8.8cm,clip]{H3277F2.epsi} %
\end{figure} Figure 2: 2.7  GHz flux density distributions for the quarter-Jansky sample (open histogram). Flux densities for our 223 new identifications shown hatched and the 9 remaining empty fields shown solid fill.
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  \begin{figure}
\par\includegraphics[angle=270,width=8.8cm,clip]{H3277F3.epsi} %
\end{figure} Figure 3: 2.7-5  GHz spectral index distributions for the quarter-Jansky sample ( $S \propto \nu ^{\alpha }$) (open histogram). Spectral indices for our 223 new identifications shown hatched and the 9 remaining empty fields shown solid fill.
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3 The identification procedure

Identification of the PKSCAT90 empty-field sources was carried out as follows:
1.
Accurate radio positions to better than 1 arcsec were obtained for all PKSCAT90 empty-field sources (Sect. 3.1).
2.
The COSMOS digitized sky survey database was interrogated at the new radio positions to find candidate source identifications (Sect. 3.2).
3.
Where no candidate was found from the COSMOS database, deep CCD images were taken through blue and red filters (Sect. 3.3).
4.
We then obtained low-dispersion spectra for all stellar identifications, as these are potential high-redshift (z > 3) quasars (Paper II).
5.
A random subset of COSMOS candidate identifications was also imaged to assess the incidence of blending of faint objects by COSMOS which would otherwise result in mis-identifications.
6.
The reliability of the total sample was then assessed (Sect. 5): (i) for the new identifications; (ii) for the existing PKSCAT90 identifications.

3.1 Radio observations

Refined radio positions are necessary to identify the empty field sources as the original Parkes radio positions are accurate only to $\sim$10-15 arcsec. We obtained these data for 72 of the empty field sources via our own observations with the Very Large Array (VLA) and Australia Telescope Compact Array (ATCA).

For 63 sources south of declination -30$^{\circ}$ the ATCA was used in the "6D'' configuration to obtain accurate radio positions. On 27 September 1993 observations were made at 4.80 and 8.64  GHz with orthogonal linear polarisations and a bandwidth of 128  MHz. The synthesised beam at 4.80  GHz was 2 arcsec FWHM (east-west). Each source was observed in typically three 45-s cuts widely spaced in hour angle, and these one-dimensional cuts were later combined to determine the source position. Secondary position calibrators were interspersed regularly throughout these observations. The flux density scale was based on the ATCA primary calibrator, PKS 1934-638.

In 1994 and 1995 we used the VLA to determine accurate positions of 29 previously unidentified sources. Most of these are are declinations north of $-30^{\circ}$ but a few are as far south as $-41^{\circ}$. The observations were made at 8.4  GHz with the VLA in its "A'' or "B''configuration with corresponding resolutions of 0.4 to 1.2 arcsec. Each programme source was covered with a single "snapshot'' scan typically of about four minutes duration, and each group of snapshots was preceded and followed by scans on a phase calibrator whose rms position uncertainty is not more than 0.1 arcsec in each coordinate. The flux density scale was based on an assumed value of 5.2 Jy for 3C 286.

The VLA data were edited and calibrated using the AIPS software package.

The remainder of the new radio positions were obtained from both previously published and unpublished results. The origin of each position is shown in the final catalogue (Appendix A). All radio positions used in the identification process are accurate to better than 1 arcsec in each coordinate. Throughout, B1950 positions were used, and where necessary the STARLINK SLALIB and COCO routines have been used to convert from other epochs and equinoxes.

Our VLA and ATCA observations revealed four sources with extended radio structures and no well-defined position or obvious optical counterpart. A further five Parkes sources were undetected at the VLA. For these, we found no evidence of any compact structure stronger than 0.5 mJy within 1 arcmin of the Parkes position. They are coded as "NCS'' (non-compact radio sources) in the final catalogue (Appendix A) and no optical identification was attempted.

3.2 Optical identifications using sky survey data

The plates of the ESO/SERC Southern Sky Survey were taken with a IIIa-J emulsion and a GG395 filter to give the photographic blue passband $B_{\rm J}$ (3950 Å-5400 Å), with a limiting magnitude ( $m_{B_{\rm J}}$) of approximately 22.5. These plates were digitized with the COSMOS plate-measuring machine at the Royal Observatory Edinburgh (Yentis et al. 1992). The COSMOS database was used to generate finding charts two arcmin-square centered on the radio position. Details of the COSMOS object nearest to the radio position were recorded.

There is an error in the stored coordinates in the COSMOS database arising from the precession calculations used to construct the database at ROE. The effect of this is that the positions stored in the COSMOS database are not J2000 but are close to B2000 (see Drinkwater et al. 1995 for a full discussion). As a result the "B1950'' positions produced from COSMOS are also incorrect. As the COSMOS positions have been constructed using the "FK4'' catalogue there is no mean systematic offset in the COSMOS positions from the (FK4) SAO catalogue. However, there is a systematic offset between COSMOS and the newer (FK5) Positions and Proper Motions (PPM) catalogue (Roeser et al. 1994). The PPM catalogue is more accurate than the SAO catalogue in that the FK5 system is closer to an inertial reference frame. For the level of astrometric accuracy required by this project, the COSMOS coordinates must be corrected by reference to an FK5 catalogue.

In order to correct the COSMOS "B1950'' positions to true B1950 positions for each field, (x,y) positions for approximately 12 of the faintest PPM stars around each radio position were measured on the ESO R survey plate using the PDS plate-measuring machine at the Royal Greenwich Observatory. The ESO R survey was chosen as the images are smaller, less saturated than deeper surveys, and hence a more accurate determination of the star centres was possible. Where the ESO R survey was not available the UKST IIIa-J survey was used. The (x,y) coordinates were transformed to (RA, Dec) coordinates using a 6-coefficient fit to Schmidt distortion geometry using STARLIB ASTROM. Each COSMOS "B1950'' position was then corrected from the average of the offsets.

With the corrections applied, we initially took the nearest COSMOS-database object to the radio position as the optical counterpart. A Gaussian fitted to the radio - optical offsets revealed an rms scatter of $\sim$1.12 arcsec in each coordinate. We therefore took a maximum offset of 3.6 arcsec ($\sim$3$\sigma$) in each coordinate as the identification criterion.

Objects which were obviously extended or were found to have narrow-line spectra (Paper II) were classified as galaxies, the remainder as stellar objects. If a candidate was close to the sky survey plate limit ($b_{\rm J}$ $\sim22$), in the absence of other data for the object we conservatively classified it as stellar.

Using the COSMOS database, we found identifications for 136 of the PKSCAT90 empty-field sources, comprising 107 stellar objects and 29 galaxies. The galaxy identifications were confirmed via visual inspection of the sky survey plates, as often faint objects in close proximity are merged by the COSMOS digitization process and then erroneously recorded in the database as a single object (usually a "galaxy'').

3.3 CCD Imaging

To identify the 87 sources which had no candidate identification from the COSMOS database we conducted a programme of deep CCD-imaging using the ESO Faint Object Spectrograph and Camera (EFOSC1) at the Cassegrain focus of the ESO 3.6m-telescope. Six observing sessions were undertaken at the telescope, as shown in Table 3.


 

 
Table 3: ESO 3.6-m imaging observations.
  Number of
Dates nights used
20-23 April 1993 3
10-14 November 1993 4
10-12 May 1994 2
5-8 October 1994 3
26-29 April 1995 2
23-25 October 1995 3


ESO filters #552 (B), #614 (Gunn-i) and #615 (Gunn-z) were used for imaging on EFOSC1, using photometric standards from Stobie et al. (1985) and Landolt (1992). Typical integration times were 5 min in B and 10 min in Gunn-i and Gunn-z filters.

The raw FITS-format CCD images obtained with EFOSC1 were reduced using the Image Reduction and Analysis Facility ( IRAF) version 2.10, developed at NOAO. The radio source position (x,y) was aligned onto the CCD frames via the STARLINK ASTROM routine using the positions of approximately 12 faint stellar objects on the CCD frame. The corrected COSMOS B1950 positions of these stellar objects were transformed using a 6-coefficient fit which was accepted when the rms residual reduced to $\mathrel{\mathchoice {\vcenter{\offinterlineskip\halign{\hfil
$\displaystyle ...0.3 arcsecs. In many cases we obtained more than one exposure per radio source so that an (x,y) solution was required for each frame. All frames were then manually examined for candidate objects.

For a source to be accepted as the optical counterpart we adopted the same 3$\sigma$ criterion as for the COSMOS identifications. For the accepted identifications we find that the CCD-based identifications have a wider Gaussian spread of radio - optical offsets as shown in Fig. 4 and Table 4 with the CCD identifications generally associated with fainter optical sources (Fig. 5).


  \begin{figure}
\par\includegraphics[angle=270,width=8.8cm,clip]{H3277F4.epsi} %
\end{figure} Figure 4: Position offsets in RA and dec for the 223 new identifications. Identifications from COSMOS are shown as "1'' and those from CCD imaging as "2''.
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Table 4: Radio-optical position offsets.
    $\langle\Delta {\rm RA}\rangle$ $\sigma_{\rm RA}$ $\langle\Delta {\rm Dec}\rangle$ $\sigma_{\rm Dec}$

Identification

N /arcsec /arcsec /arcsec /arcsec
COSMOS-survey 136 -0.06 0.89 -0.04 0.85

CCD images

87 0.07 1.12 0.03 0.96



  \begin{figure}
\par\includegraphics[angle=270,width=8.8cm,clip]{H3277F5.epsi} %
\end{figure} Figure 5: Position offsets (radial) for the 223 new identifications. Identifications from COSMOS are shown as "1'' and those from CCD imaging as "2''.
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Our CCD-imaging programme resulted in identifications for 87 sources. These identifications comprise 37 stellar objects and 50 galaxies. In Appendix D we show the CCD images, each 2 arcmin square, centred on the new identifications. The classification of type (stellar object/galaxy) was based on observed morphology. For 31 sources (23 stellar objects and 8 galaxies) we have confirmed their classifications via low-resolution spectroscopy (Paper II).

4 Reliability of the new identifications

There is the possibility that erroneous identifications have been made with objects lying close to the line-of-sight of the radio source. The uncertainty in the radio and optical positions and the density of objects on the survey plate or CCD exposure both determine the chance coincidence of a non-radio source being identified in error. Contamination due to foreground objects is fairly obvious where the object is a galactic star but not so obvious when the object is a faint galaxy.

The background faint-galaxy density was determined by examination of the deepest CCD exposures in each of the filters. The count of the galaxy density at the CCD imaging limit ( $m_{\rm B} = 24.5$) is found to be 12 faint galaxies per square arcmin in B, 13 per square arcmin in Gunn-i ( $m_{{\rm Gunn}-i} = 23.5$) and 9 per square arcmin in Gunn-z ( $m_{{\rm Gunn}-z} = 25.0$). There is a 10 per cent chance of a faint galaxy falling within the search area for any one identification. In the majority of identifications the candidate is a far brighter object so that the chance of it being an erroneous identification is remote. However, there are 38 faint galaxy identifications ( $m_{\rm B} \ge 23$), so that 4 are potential spurious identifications. We find that the rms radio minus optical offsets for these 38 faint galaxy identifications is larger (RA, dec: 1.19, 0.92 arcsec) than those for the brighter identifications (RA, Dec: 0.93, 0.89 arcsec).

The new identifications can therefore be considered as being reliable, although this is inevitably a function of magnitude. Additional confidence in the identifications is provided by the histogram of $m_{\rm B}$ magnitudes for the new identifications (Fig. 6). The decline in new identifications occurs around $b_{\rm J}$ =23, i.e. at about one magnitude brighter than the limiting magnitude of our CCD-images.


  \begin{figure}
\par\includegraphics[angle=270,width=8.8cm,clip]{H3277F6.epsi} %
\end{figure} Figure 6: Distribution of optical $b_{\rm J}$ magnitudes for all galaxy, quasar and BL Lac sources in the quarter-Jansky sample, with our new identifications shown hatched.
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5 The sample

5.1 Sample catalogue

The catalogue of the quarter-Jansky sample is presented in Appendix A. Finding charts, images and additional notes on individual sources are given in Appendices B, C and D.

The identification classes in our catalogue, column 8, are as follows. G = galaxy, and in this we have subsumed the PKSCAT90 classes "DB'', "E'' and "Sey'', defining sub-categories of galaxies (double, elliptical and Seyferts respectively). Q = quasar, confirmed spectroscopically or via UVX measurement, while Q* = quasar by virtue of coincidence between the position of a stellar object and an accurate radio position, and Q? is an unconfirmed quasar, a stellar object coincident with a Parkes survey radio position.

5.2 Catalogue reliability

In the course of constructing the final catalogue and subsequent to the analysis of Shaver et al. (1996) we have reassessed the data contained in the entire catalogue. Our primary aim is to ensure that we have not overlooked any z > 5 candidate quasars in the sample, particularly due to errors in PKSCAT90. For the 233 new identifications discussed in Sect. 3 we are confident in that there are no undiscovered high-redshift quasars.

We use digitized material from the UKST IIIa-J and UK SES R surveys along with the best-available radio positions to check every one of the 878 sources in our sample. The overlays of the radio position on the sky survey data is shown in Appendix C.

We find 10 radio sources for which we cannot confirm the identification (see Table 5). Of these 10, one source, PKS B0141-060 lies within an area already covered by the Sydney University Molonglo Sky Survey (SUMSS, Bock et al. 1999) at 843 MHz: This is clearly a complex, extended source so this is classified as a non-compact source (NCS).

Of the remaining 9 sources, 3 have radio positions catalogued by NVSS (Condon et al. 1998): PKS B0225-065, PKS B0415-029 and PKS B0522-030. There is no more recent radio survey data from which to confirm the validity of the other 7 sources. As an interesting point of note, three of the remaining unidentifiable PKSCAT90 sources in Table 5 do not appear in the original Parkes survey papers (Table 2): That such a significant fraction of the non-Parkes survey sources cannot be identified suggests that they are either highly variable or that their existence is questionable.

  \begin{figure}
\par\includegraphics[angle=270,width=18cm,clip]{H3277F7.epsi} %
\par\end{figure} Figure 7: Optical $b_{\rm J}$ magnitudes vs. radio flux densities ($b_{\rm J}$ vs. $S_{2.7 \rm ~ GHz}$) for 150 galaxies ($\bullet $) and 677 stellar objects ($\circ $, quasars and BLLacs) from the quarter-Jansky radio sample.
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Considering the PKSCAT90 identifications we find that two sources, PKS B0225-065 and PKS B1150-723 are identified as galaxies. However, as we find no evidence to support this, we code these sources to "e'' for an elimated PKSCAT90 identification. Another source, PKS B0551-538 is classified as "Xg'' in PKSCAT90, indicating at least one galaxy within the Parkes radio position error box. We code this as an empty-field source (X). Two sources are PKSCAT90 empty-field sources ("Xs'' and "Xsa'') and were overlooked in our identification campaign and remain empty fields (X). The remaining four PKSCAT90-blank coded sources also are coded as empty-fields (X).


 

 
Table 5: PKSCAT90 previously-identified sources de-identified as a result of arcsec-radio positions.
Original          
Parkes PKS B1950 PKSCAT90 $S_{2.7 \rm ~ GHz}$ $S_{\rm lim}$ New
survey name Id / Jy / Jy Id
Y B0141-609 Xg 0.17 0.25 NCS
Y B0225-065 G 0.35 0.25 e
Y B0415-029 Xs 0.16 0.25 X
N B0522-030 Xsa 0.06 0.25 X
N B0528-454 blank 0.39 0.25 X
N B0549-459 blank 0.32 0.25 X
Y B0551-538 Xg 0.27 0.25 X
Y B0619-468 blank 0.43 0.60 X
Y B0715-663 blank 0.43 0.25 X
N B1150-723 G 0.82 0.25 e


For the PKSCAT90 confirmed identifications we have assessed the stellar identifications as follows: Q = quasar, confirmed spectroscopically or via UVX measurement, while Q* = quasar by virtue of coincidence between the position of a stellar object and an accurate radio position, and Q? is an unconfirmed quasar, a stellar object coincident with a Parkes survey ($\sim$10-15 arcsec) radio position.

Furthermore, we have checked all redshifts in the table by searching the original references. Numerous errors in the PKSCAT90 listing were found. Full references for the redshifts appear in Appendix A, and Appendix B gives full details of updates to PKSCAT90 data.

6 Sample characteristics

6.1 Optical magnitude distribution

The distribution of $b_{\rm J}$ magnitudes for the sample is shown in Fig. 6; our new identifications (inevitably) lie at the faint end of the distribution and show that the total distribution is mildy bimodal with a main peak at $b_{\rm J}=19.5$ mag and a subpeak near $b_{\rm J}$  = 22.5 mag.

Figure 7, a plot of the sample in $b_{\rm J}$ magnitude vs. $S_{2.7 \rm ~ GHz}$ with indication of object type, shows that galaxies dominate at faint flux densities and faint $b_{\rm J}$ magnitudes. Considering identification-fraction as a function of $b_{\rm J}$ magnitude (Fig. 8) we see that quasars dominate between $b_{\rm J}=16$ to 22, and that the spectroscopically-confirmed BL Lac objects comprise 5 to 10 per cent of the sample at all $b_{\rm J}$ magnitudes. However, this latter result should be treated as a lower limit only, as we do not have complete spectroscopic measurements for all stellar sources.

6.2 Source types as a function of 2.7 GHz flux density

As a function of flux density (Fig. 9), the galaxies are significant (i) at bright flux densities (the cores of active nearby ellipticals) and (ii) towards the faint flux densities ( $S_{2.7 \rm ~ GHz}$ $\sim$ 0.2  Jy). The increase in the galaxy fraction at fainter flux densities has also been observed in other radio samples (Falco et al. 1998) and probably comprises peaked-spectrum or compact symmetric radio galaxies.

The set of histograms of Fig. 10 shows how the $b_{\rm J}$ magnitude distribution changes with decreasing 2.7  GHz flux density. The brightest radio sources have a peaked distribution around $b_{\rm J}$  = 18.5; there is no hint of bimodality as there is little intrusion of the flat-spectrum population of faint galaxies. As radio flux density decreases and the flat-spectrum galaxies appear, the distribution takes on the bimodal shape, which continues below $S_{2.7 \rm ~ GHz}$ = 0.25  Jy. As first noted by Bolton (1970), the median of the distribution shifts to fainter magnitudes as flux density decreases, an effect seen in subsequent studies (Browne & Wright 1985; Drinkwater et al. 1997).


  \begin{figure}
\par\includegraphics[angle=270,width=8.8cm,clip]{H3277F8.epsi} %
\end{figure} Figure 8: Proportions of identified source types by optical $b_{\rm J}$ magnitude in the quarter-Jansky sample.
Open with DEXTER


  \begin{figure}
\par\includegraphics[angle=270,width=8.8cm,clip]{H3277F9.epsi} %
\end{figure} Figure 9: Proportions of the identified source types by $S_{2.7 \rm ~ GHz}$ in the quarter-Jansky sample.
Open with DEXTER


  \begin{figure}
\par\includegraphics[angle=270,width=8cm,clip]{H3277F10a.epsi}\in...
...c.epsi}\includegraphics[angle=270,width=8cm,clip]{H3277F10d.epsi} %
\end{figure} Figure 10: Optical $b_{\rm J}$ magnitude distributions a) for sources with $S_{2.7 \rm ~ GHz}$ $\ge $ 2.0  Jy b) for sources with $S_{2.7 \rm ~ GHz}$ $\ge $ 0.50  Jy c) for sources with $S_{2.7 \rm ~ GHz}$ $\ge $ 0.25  Jy and d) for sources with $S_{2.7 \rm ~ GHz}$ < 0.25  Jy. Legend: hatched regions indicate galaxy identifications, open histogram regions quasar plus BL Lac identifications.
Open with DEXTER

6.3 Redshift distribution

The redshift distribution is shown in Fig. 11. There is some dependence on flux density in that the distribution for the fainter sources of the sample - those with flux densities in the range 0.25 $\le$ $S_{2.7 \rm ~ GHz}$ < 0.5  Jy - is flatter and biased to significantly higher redshifts than that for all sources with $S_{2.7 \rm ~ GHz}$ $\ge $ 0.25  Jy.

6.4 Spectral index distributions

The distributions of spectral indices for galaxies and stellar objects (quasars and BLLacs) are compared in Fig. 12. A K-S test reveals that there is only a 2.3 per cent probability that the two distributions are drawn from the same population. The galaxy identifications have generally steeper spectra; their distribution is suggestive simply of an extended tail to the classical (low-frequency survey) distribution with its peak around $\sim$-0.8. The quasar plus BLLac distribution gives indication of the bimodality seen so clearly in samples selected at frequencies above 2.7  GHz. In these sources the flat-spectrum peak is identified with beamed emission.


  \begin{figure}
\par\includegraphics[width=8.8cm,clip]{H3277F11.epsi}\par %
\end{figure} Figure 11: Redshift distribution for the quarter-Jansky sample sources $S_{2.7 \rm ~ GHz}$ $\ge $ 0.25  Jy (unfilled histogram). For comparison sources with 0.25 $ \le S_{2.7~ \rm GHz} <$ 0.50  Jy are shown hatched.
Open with DEXTER


  \begin{figure}
\par\includegraphics[angle=270,width=8.8cm,clip]{H3277F12a.epsi}\...
...4mm}
\includegraphics[angle=270,width=8.8cm,clip]{H3277F12b.epsi} %
\end{figure} Figure 12: Spectral index distributions ( $\alpha^{5 \rm
\thinspace GHz}_{2.7 \rm \thinspace GHz}$) by identified source types in the quarter-Jansky sample sources. Left - galaxies; right - quasars and BL Lac objects.
Open with DEXTER

7 Summary

In a sample of 878 flat-spectrum sources selected from PKSCAT90, observations to obtain accurate radio positions and optical imaging data have resulted in optical counterparts for 223 previously unidentified sources. The sample catalogue presented here contains 827 compact radio sources identified with galaxies, quasars and BLLac objects, 38 sources either resolved or identified with Galactic objects, and 4 sources whose fields are optically contaminated by bright stars. Just 9 sources (1 per cent) remain unidentified. From this total sample, complete flux-density limited samples can be selected; for example for sources north of $-40^{\circ}$ declination in regions where the survey limit is $\ge $0.25 Jy there are secure identifications for 418 out of 419 sources (99.8 per cent).

Further to our comprehensive checking of the existing PKSCAT90 data and our new identifications, we conclude that

The sample highlights why completion of optical identifications is difficult even for flat-spectrum compact samples: at faint flux-density levels ( $S_{2.7 \rm ~ GHz}$ < 0.3  Jy) a significant fraction of the host objects are faint red galaxies.

Acknowledgements

We thank Dick Hunstead, Alok Patnaik, John Reynolds, Ann Savage and Niven Tasker for providing radio positions in advance of publication. We also thank Dave McConnell and Bob Sault for assistance with the ATCA observations and analysis, Benoit Germain for his work with the optical data reduction and John Pilkington for carrying out the PDS plate measurements. This work is based on data collected at the European Southern Observatory, the Australia Telescope National Facility and the National Radio Astronomy Observatory. NRAO is operated by Associated Universities Inc. under cooperative agreement with the National Science Foundation.

  
Appendix A: The complete catalogue of the Parkes quarter-Jansky sample

Catalogue column entries:

1. PKSCAT90 B1950 source name.

2. and 3. PKSCAT90 radio source position (B1950).

4. and 5. The best radio source position (B1950).

6. The origin of the radio position given in Cols. 4 and 5:

A

ATCA observation for this project

C

ATCA calibrator (ftp.atnf.csiro.au/pub/atnfdocs/guides/at.cat)

H

R Hunstead, private communication

N

NVSS catalogue (Condon et al. 1998)

P

A Patnaik, private communication

R

J Reynolds, private communication

S

A Savage, private communication

T

N Tasker, private communication

V

VLA observation for this project

W

White (1992)

 

7. Origin of identification:

1: Reconfirmed PKSCAT90 identification based on the following:

1a: Sky survey data and the best radio position available as shown in the table. No offsets (radio - optical) have been determined for these sources.

1b: COSMOS sky survey and the best radio position available as shown in the table. Identification offsets (radio - optical) have been determined for these sources.

1c: CCD imaging and the best radio position available as shown in the table. Identification offsets (radio - optical) have been determined for these sources.

2: A new identification by this project using the COSMOS database.

3: A new identification by this project using CCD-imaging.

8. Identification:

Q: confirmed quasar by spectroscopy or UVX photometry

Q*: stellar object based on positional coincidence with accurate (post-PKSCAT90) radio position, although no spectrum or UVX confirmation.

Q?: PKS radio position coincident with stellar object. No spectroscopy/UVX confirmation.

BL: spectroscopically-confirmed BL Lac object.

G: Galaxy with morphological or spectroscopic confirmation.

G?: probably a galaxy based on optical colour or morphology.

X: no identification, was previously a PKSCAT90 empty-field source.

e: the best radio invalidates the PKSCAT90 identification in that there is no optical source at the best radio position.

Ob: radio position obscured by foreground star.

NCS: Non-compact radio source. The source is either a steep-spectrum or extended radio source. Refer to individual notes for full details (Appendix B).

PN: Planetary nebula.

HII: HII region.

9. and 10. Radio - optical offset of candidate identification (given for identification classes 1c, 2 and 3 in Col. 7).

11. B or $B_{\rm J}$ magnitude. The origin of these magnitudes can be determined from the entry in Col. 7 as follows: for "1'' identifications, the magnitude is from PKSCAT90 and could be B or $B_{\rm J}$, for "2'' identifications the magnitudes is from COSMOS and is a $B_{\rm J}$ magnitude, for "3'' identifications the magnitude is from our CCD-imaging and is a B magnitude.

Magnitudes prefixed with: are either (i) estimated (ii) untraceable in the literature although given in PKSCAT90 or (iii) too close to the DSS plate limit to be reliable.

12. and 13. Gunn-iand Gunn-z (instrumental) magnitudes as determined from our CCD imaging.

14. and 15. Redshift and reference. Those prefixed ":'' are from PKSCAT90 but are untraceable in the literature.

16. to 18. PKSCAT90 $S_{2.7 \rm ~ GHz}$, $S_{5~ \rm GHz}$ and $S_{\rm lim,~2.7~{\rm GHz}}$

19. Exclusion flag. If "X'' then this source is excluded from our complete sample due to one of the following conditions:

Source is non-compact radio source (NCS) as shown in Col. 8 and the individual notes for that source.

Source flux density at 2.7  GHz is below the survey area flux density limit ( $S_{2.7 \rm ~ GHz}$ $< S_{\rm lim, 2.7~{\rm GHz}}$).

Source is steep-spectrum as described in detailed notes for that source.

Source is outside of the original Parkes survey areas (in area "X'' of Table 2). In this case $S_{\rm lim,~2.7~{\rm GHz}}$ is also set to 0.0.


 

 
Table A.1: Parkes radio sources.
  PKSCAT90 B1950 New radio position B1950       Offsets                
Name RA Dec RA Dec   Ident RA Dec B Gunn-i Gunn-z z zRef S2.7 S5 $S_{\rm lim}$
PKS B0000-160 00 00 53.7 -16 03 48 00 00 53.68 -16 03 47.8 P 3 G -0.3 -0.2 22.6 20.1 21.7 0.508 83 0.30 0.26 0.25
PKS B0001-121 00 01 24.0 -12 06 36 00 01 25.89 -12 06 16.2 P 3 G 2.6 1.0 24.0         0.27 0.22 0.25
PKS B0002-170 00 02 43.6 -17 04 45 00 02 44.52 -17 04 46.9 P 1b Q* -0.4 -0.5 18.0         0.14 0.16 0.25 X
PKS B0002-478 00 02 03.0 -47 53 02 00 02 02.94 -47 53 02.1 C 1a Q     19.0         0.63 0.55 0.25
PKS B0003-066 00 03 40.3 -06 40 17 00 03 40.29 -06 40 17.4 P 1b BL -0.5 -0.4 19.5     0.347 1 1.46 1.58 0.25
PKS B0005-239 00 05 27.5 -23 56 00 00 05 27.47 -23 56 00.1 P 1b Q -0.2 -0.8 17.0     1.410 2 0.58 0.53 0.25
PKS B0005-262 00 05 53.5 -26 15 53 00 05 53.48 -26 15 54.0 N 1a Q?     20.0         0.58 0.58 0.25
PKS B0008-222 00 08 21.1 -22 13 49 00 08 21.03 -22 13 45.7 P 2 G? 0.6 0.5 21.8   22.0     0.38 0.39 0.25
PKS B0008-264 00 08 28.9 -26 29 15 00 08 28.89 -26 29 14.9 P 1b Q -0.1 0.1 19.0     1.096 3 0.67 0.81 0.25
PKS B0008-307 00 08 04.4 -30 44 13 00 08 03.58 -30 44 29.1 A 2 Q 0.2 -0.5 19.1     1.189 83 0.31 0.27 0.20
                                   
PKS B0011-046 00 11 20.6 -04 40 33 00 11 20.66 -04 40 33.6 N 1a Q?     19.0         0.21 0.41 0.25 X
PKS B0012-184 00 12 30.0 -18 29 28 00 12 30.06 -18 29 31.5 P 1b Q 0.3 -1.0 20.0     0.743 83 0.48 0.42 0.25
PKS B0013-005 00 13 37.4 -00 31 53 00 13 37.35 -00 31 52.6 P 1b Q -0.1 0.1 19.5     1.575 4 0.80 0.65 0.10
PKS B0013-240 00 13 33.8 -24 00 32 00 13 33.87 -24 00 31.9 N 1a G     17.0         0.25 0.23 0.25
PKS B0014-312 00 14 55.6 -31 14 46       1a NCS               0.15 0.15 0.20 X
PKS B0017-307 00 17 13.0 -30 47 56 00 17 12.15 -30 47 59.0 N 1a Q     19.0     2.666 83 0.34 0.33 0.20
PKS B0022-044 00 22 12.8 -04 28 37 00 22 12.74 -04 28 38.6 P 1b Q -0.3 0.0 20.0     1.946 83 0.29 0.39 0.25
PKS B0026-014 00 26 29.6 -01 29 42 00 26 27.42 -01 30 16.7 P 2 G -0.9 0.5 16.3     0.083 83 0.30 0.26 0.25
PKS B0027-024 00 27 58.9 -02 28 33 00 27 58.41 -02 28 30.2 P 2 Q* 1.1 0.5 19.6         0.22 0.18 0.25 X
PKS B0027-426 00 27 51.8 -42 41 25       1a Q     19.0     0.495 83 0.42 0.43 0.25
                                   
PKS B0028-396 00 28 55.8 -39 39 31 00 28 57.82 -39 39 23.2 A 2 Q* -0.4 -0.4 20.8         0.19 0.19 0.25 X
PKS B0029-414 00 29 01.3 -41 24 39       1a Q     17.0     0.896 5 0.23 0.21 0.25 X
PKS B0035-252 00 35 46.0 -25 15 31 00 35 46.01 -25 15 31.5 P 1b Q -0.6 -0.6 17.5     1.196 6 0.28 0.30 0.25
PKS B0035-595 00 35 09.2 -59 34 27       1a Q     19.0         0.26 0.21 0.25
PKS B0036-216 00 36 00.4 -21 36 33 00 36 00.45 -21 36 33.2 P 1b G 0.0 0.2 19.0         0.53 0.60 0.25
PKS B0038-326 00 38 05.1 -32 41 40 00 38 04.09 -32 41 49.6 S 2 BL 0.8 0.8 21.5       83 0.43 0.69 0.20
PKS B0039-407 00 39 37.6 -40 47 06       1a Q     18.5     2.478 83 0.25 0.34 0.25
PKS B0040+001 00 40 58.6 +00 08 38 00 40 58.91 +00 08 34.3 N 1a Q     19.0     1.127 7 0.08 0.11 0.10 X
PKS B0046-315 00 46 58.3 -31 32 54 00 46 57.68 -31 32 47.0 N 1a Q     16.5     2.718 8 0.15 0.15 0.20 X
PKS B0047+023 00 47 08.8 +02 20 43 00 47 08.87 +02 20 43.0 N 1a BL     18.0       4 0.39 0.39 0.10
                                   
PKS B0047-051 00 47 48.8 -05 08 39 00 47 49.02 -05 08 40.0 P 1b Q* 0.1 -0.2 18.5         0.18 0.27 0.25 X
PKS B0047-579 00 47 48.0 -57 54 47 00 47 48.16 -57 54 47.1 C 1a Q     17.8     1.797 8 1.96 2.48 0.25
PKS B0048-071 00 48 36.2 -07 06 21 00 48 36.22 -07 06 20.9 P 1b Q -0.5 0.0 19.0     1.975 3 0.70 0.67 0.25
PKS B0048-097 00 48 10.0 -09 45 24 00 48 09.98 -09 45 24.3 P 1b BL -0.4 -0.2 17.0       3 1.44 1.92 0.25
PKS B0048-427 00 48 49.0 -42 42 52 00 48 49.02 -42 42 52.0 C 1a Q     18.8     1.749 9 0.68 0.58 0.25
PKS B0051-077 00 51 04.6 -07 43 45 00 51 04.77 -07 43 45.9 P 3 G? 0.6 0.2 >24.5   23.0     0.21 0.19 0.25 X
PKS B0054-006 00 54 43.3 -00 40 46 00 54 43.40 -00 40 45.7 P 1b Q -0.5 -0.2 18.0     2.790 8 0.15 0.19 0.10
PKS B0054-451 00 54 29.0 -45 07 23       1a G     18.5         0.46 0.39 0.25
PKS B0055-328 00 55 42.0 -32 51 17       1a NCS               0.44 0.36 0.20 X
PKS B0056-525 00 56 45.6 -52 35 20 00 56 43.91 -52 35 36.9 A 3 BL -1.2 -1.6 23.6 20.9 23.5   83 0.26 0.26 0.25


   
Appendix B: Notes on individual sources

0000-160 Could be interacting with a fainter galaxy to south.

0001-121 Faint galaxy from CCD imaging, on B frame only. However, the NVSS catalogues 2 bright radio sources, offset 87 and 297 arcsecs respectively with nothing closer to the Parkes or Patnaik position. The nearest NVSS radio source is coincident with a galaxy on DSS, with $B_{\rm J}$ mag approx 21.0. It is probable that this is the correct radio source id, the Parkes beam being confused by 2 close compact radio sources. For the time being we leave the id as the faint galaxy and estimate the B mag.

0005-262 PKSCAT90 galaxy is an incorrect identification: Identified as a stellar object on K-band image by Drinkwater et al. (1997).

0008-222 Classified as galaxy in the COSMOS survey, as probably extended on our Gunn-z image and also brighter on B.

0014-312 Undetected by our VLA observations, nothing in NVSS.

0026-014 A gE galaxy identified in the COSMOS survey, disturbed/interacting. Has smaller companion galaxy at same redshift.

0027-426 The redshift given in NED (from Hewitt et al. 1989) is wrong. New redshift obtained by us (Paper II).

0051-077 Not present on B image. Classed as a galaxy as it is probably extended on Gunn-z image.

0055-328 Double radio source (NVSS). No compact core component at PKSCAT90 position.

0056-525 BL Lac object (Paper II), stellar on Gunn-i and Gunn-z images, very faint on B.

0059-287 Re-observed with VLA 1.4 GHz April 95, showing steep radio spectrum; variable quasar?

0100-760 The correct redshift is given in Wilkes et al. (1983) and is not that of Jauncey et al. (1978).

0111-385 Galaxy identification from CCD frames. Our VLA observations indicate the source has a double radio structure; there is a candidate identification coincident with one component and is a faint diffuse red object. The NVSS survey also catalogues this as a double radio source and thus it is excluded from our complete sample.

0113-310 Original PKS survey catalogues this source as confused with 0112-310. NVSS catalogues this source 84 arcsec offset from the PKS position in RA: it is a compact radio source coincident with a stellar object.

0115-016 Extended (or compound) image appears on the Gunn-i and Gunn-z, stellar on B.

0115-357 Nothing at position in NVSS survey, nearest NVSS source is 250 arcsec offset. Excluded from our complete sample.

0115-368 Extended, probably bent double radio source (NVSS). Excluded from our complete sample.

0123-016 = NGC545/7; it is a very extended FRI radio source, and the apparent flat spectrum only comes about through inaccurate flux-density integration at 2.7 and 5.0 GHz. Excluded from our complete sample.

0128-132 Extended (bent double?) radio source (NVSS). Excluded from our complete sample.

0130-447 Low-surface-brightness galaxy identification from CCD imaging; red and very diffuse.

0143-061 Galaxy identified from the COSMOS survey with narrow-line spectrum (Paper II). Our VLA observations reveal an extended radio structure for the source, agreeing with NVSS. Excluded from our complete sample.

0144-219Low-surface-brightnessgalaxy,mostobviousonGunn-iframe.Possiblyinteractingwithnearby,brighterS0.

0156-144 Faint galaxy, from B frame but not on Gunn-z. Galaxy is actually a steep-spectrum source: the PKSCAT90 2.7 GHz flux density is wrong (0.90 Jy vs. the original PKS survey value of 1.01 Jy). Our VLA observations reveal a steep-spectrum source, thus it is exluded from our complete sample.

0202-337 Scattered light from a nearby bright star creates a ghost ring covering the radio position, but the morphology is reasonably clear.

0203-520 Erroneous redshift given in PKSCAT90. Updated in our table to the correct value and reference.

0215+015 Extremely variable BLLac object (Bolton & Wall 1969; Gaskell 1982).

0215-015 Looks stellar on B and Z; no signal in our optical spectrum (Paper II) and thus unconfirmed quasar.

0218-683 Candidate is very close to bright star and its scattered light makes morphological classification difficult.

0225-065 The NVSS catalogues a compact source 3 arcsec from the PKSCAT90 position, at B1950 $02^{\rm h} 25^{\rm m} 15\hbox{$.\!\!^{\rm s}$ }22$, $-06^{\circ} 34'
32\hbox{$.\!\!^{\prime\prime}$ }3$, 0.513 Jy at 1.4 GHz. DSS shows a very faint object, possibly extended, close to this position; but it cannot be claimed as the identification.

0230-790 A suspect redshift: Browne & Savage (1977) found a single line at 5800 Å and it was pointed out by Jauncey et al. (2000) that if this were identified with MgII $\lambda 2798$ then the redshift is 1.07.

0231+022 Double radio source (NVSS), excluded from our complete sample.

0238-084 NGC1052 LINER-type elliptical with inverted radio spectrum.

0239-553 Faint (possibly double) galaxy based on our ATCA position which notes it as a double radio source. The centroid position is used for the identification. The relatively large radio-optical offset is probably due to the extended radio structure. Excluded from our complete sample.

0240-060 The redshift given in Strittmatter et al. (1974) is wrong. New redshift obtained by us (Paper II).

Appendix C Finding charts for all sources

 

Finding charts for all 878 sources presented in Appendix A. Charts are oriented North up, East left, and the scale is in arcmins. Position of the best radio position is marked (+).


\begin{figure}\par\includegraphics[width=16cm,clip]{H3277fc1.epsi}\end{figure}

   
Appendix D: Newly-identified sources with CCD images

Images are oriented North up, East left, and scale is in arcseconds. Images are 2 arcminutes square, centered on the identification ($\circ $).


\begin{figure}
\par {\includegraphics[width=12cm,clip]{H3277i10.ps} }
\end{figure}

References

 

Online Material


 
Table A.1: continued.
  PKSCAT90 B1950 New radio position B1950       Offsets                
Name RA Dec RA Dec   Ident RA Dec B Gunn-i Gunn-z z zRef S2.7 S5 $S_{\rm lim}$
PKS B0000-160 00 00 53.7 -16 03 48 00 00 53.68 -16 03 47.8 P 3 G -0.3 -0.2 22.6 20.1 21.7 0.508 83 0.30 0.26 0.25
PKS B0001-121 00 01 24.0 -12 06 36 00 01 25.89 -12 06 16.2 P 3 G 2.6 1.0 24.0         0.27 0.22 0.25
PKS B0002-170 00 02 43.6 -17 04 45 00 02 44.52 -17 04 46.9 P 1b Q* -0.4 -0.5 18.0         0.14 0.16 0.25 X
PKS B0002-478 00 02 03.0 -47 53 02 00 02 02.94 -47 53 02.1 C 1a Q     19.0         0.63 0.55 0.25
PKS B0003-066 00 03 40.3 -06 40 17 00 03 40.29 -06 40 17.4 P 1b BL -0.5 -0.4 19.5     0.347 1 1.46 1.58 0.25
PKS B0005-239 00 05 27.5 -23 56 00 00 05 27.47 -23 56 00.1 P 1b Q -0.2 -0.8 17.0     1.410 2 0.58 0.53 0.25
PKS B0005-262 00 05 53.5 -26 15 53 00 05 53.48 -26 15 54.0 N 1a Q?     20.0         0.58 0.58 0.25
PKS B0008-222 00 08 21.1 -22 13 49 00 08 21.03 -22 13 45.7 P 2 G? 0.6 0.5 21.8   22.0     0.38 0.39 0.25
PKS B0008-264 00 08 28.9 -26 29 15 00 08 28.89 -26 29 14.9 P 1b Q -0.1 0.1 19.0     1.096 3 0.67 0.81 0.25
PKS B0008-307 00 08 04.4 -30 44 13 00 08 03.58 -30 44 29.1 A 2 Q 0.2 -0.5 19.1     1.189 83 0.31 0.27 0.20
                                   
PKS B0011-046 00 11 20.6 -04 40 33 00 11 20.66 -04 40 33.6 N 1a Q?     19.0         0.21 0.41 0.25 X
PKS B0012-184 00 12 30.0 -18 29 28 00 12 30.06 -18 29 31.5 P 1b Q 0.3 -1.0 20.0     0.743 83 0.48 0.42 0.25
PKS B0013-005 00 13 37.4 -00 31 53 00 13 37.35 -00 31 52.6 P 1b Q -0.1 0.1 19.5     1.575 4 0.80 0.65 0.10
PKS B0013-240 00 13 33.8 -24 00 32 00 13 33.87 -24 00 31.9 N 1a G     17.0         0.25 0.23 0.25
PKS B0014-312 00 14 55.6 -31 14 46       1a NCS               0.15 0.15 0.20 X
PKS B0017-307 00 17 13.0 -30 47 56 00 17 12.15 -30 47 59.0 N 1a Q     19.0     2.666 83 0.34 0.33 0.20
PKS B0022-044 00 22 12.8 -04 28 37 00 22 12.74 -04 28 38.6 P 1b Q -0.3 0.0 20.0     1.946 83 0.29 0.39 0.25
PKS B0026-014 00 26 29.6 -01 29 42 00 26 27.42 -01 30 16.7 P 2 G -0.9 0.5 16.3     0.083 83 0.30 0.26 0.25
PKS B0027-024 00 27 58.9 -02 28 33 00 27 58.41 -02 28 30.2 P 2 Q* 1.1 0.5 19.6         0.22 0.18 0.25 X
PKS B0027-426 00 27 51.8 -42 41 25       1a Q     19.0     0.495 83 0.42 0.43 0.25
                                   
PKS B0028-396 00 28 55.8 -39 39 31 00 28 57.82 -39 39 23.2 A 2 Q* -0.4 -0.4 20.8         0.19 0.19 0.25 X
PKS B0029-414 00 29 01.3 -41 24 39       1a Q     17.0     0.896 5 0.23 0.21 0.25 X
PKS B0035-252 00 35 46.0 -25 15 31 00 35 46.01 -25 15 31.5 P 1b Q -0.6 -0.6 17.5     1.196 6 0.28 0.30 0.25
PKS B0035-595 00 35 09.2 -59 34 27       1a Q     19.0         0.26 0.21 0.25
PKS B0036-216 00 36 00.4 -21 36 33 00 36 00.45 -21 36 33.2 P 1b G 0.0 0.2 19.0         0.53 0.60 0.25
PKS B0038-326 00 38 05.1 -32 41 40 00 38 04.09 -32 41 49.6 S 2 BL 0.8 0.8 21.5       83 0.43 0.69 0.20
PKS B0039-407 00 39 37.6 -40 47 06       1a Q     18.5     2.478 83 0.25 0.34 0.25
PKS B0040+001 00 40 58.6 +00 08 38 00 40 58.91 +00 08 34.3 N 1a Q     19.0     1.127 7 0.08 0.11 0.10 X
PKS B0046-315 00 46 58.3 -31 32 54 00 46 57.68 -31 32 47.0 N 1a Q     16.5     2.718 8 0.15 0.15 0.20 X
PKS B0047+023 00 47 08.8 +02 20 43 00 47 08.87 +02 20 43.0 N 1a BL     18.0       4 0.39 0.39 0.10
                                   
PKS B0047-051 00 47 48.8 -05 08 39 00 47 49.02 -05 08 40.0 P 1b Q* 0.1 -0.2 18.5         0.18 0.27 0.25 X
PKS B0047-579 00 47 48.0 -57 54 47 00 47 48.16 -57 54 47.1 C 1a Q     17.8     1.797 8 1.96 2.48 0.25
PKS B0048-071 00 48 36.2 -07 06 21 00 48 36.22 -07 06 20.9 P 1b Q -0.5 0.0 19.0     1.975 3 0.70 0.67 0.25
PKS B0048-097 00 48 10.0 -09 45 24 00 48 09.98 -09 45 24.3 P 1b BL -0.4 -0.2 17.0       3 1.44 1.92 0.25
PKS B0048-427 00 48 49.0 -42 42 52 00 48 49.02 -42 42 52.0 C 1a Q     18.8     1.749 9 0.68 0.58 0.25
PKS B0051-077 00 51 04.6 -07 43 45 00 51 04.77 -07 43 45.9 P 3 G? 0.6 0.2 >24.5   23.0     0.21 0.19 0.25 X
PKS B0054-006 00 54 43.3 -00 40 46 00 54 43.40 -00 40 45.7 P 1b Q -0.5 -0.2 18.0     2.790 8 0.15 0.19 0.10
PKS B0054-451 00 54 29.0 -45 07 23       1a G     18.5         0.46 0.39 0.25
PKS B0055-328 00 55 42.0 -32 51 17       1a NCS               0.44 0.36 0.20 X
PKS B0056-525 00 56 45.6 -52 35 20 00 56 43.91 -52 35 36.9 A 3 BL -1.2 -1.6 23.6 20.9 23.5   83 0.26 0.26 0.25


 
Table A.1: continued.
  PKSCAT90 B1950 New radio position B1950       Offsets                
Name RA Dec RA Dec   Ident RA Dec B Gunn-i Gunn-z z zRef S2.7 S5 $S_{\rm lim}$
PKS B0056-572 00 56 38.9 -57 15 21 00 56 38.58 -57 15 22.4 C 1a Q     18.3         0.77 1.07 0.25
PKS B0059-287 00 59 28.3 -28 47 30 00 59 28.18 -28 47 27.9 P 3 Q 0.6 -0.1 23.2 21.0 22.7 1.694 83 0.44 0.36 0.25
PKS B0059-628 00 59 14.6 -62 49 14       1a Q     19.3         0.28 0.25 0.25
PKS B0100-270 01 00 31.5 -27 02 42 01 00 31.62 -27 02 42.8 P 1b Q -0.3 0.7 17.5     1.597 5 0.26 0.24 0.25
PKS B0100-413 01 00 58.5 -41 20 38       1a Q     18.5         0.15 0.13 0.25 X
PKS B0100-760 01 00 55.8 -76 02 59       1a Q     18.2     1.015 10 0.43 0.55 0.20
PKS B0102-245 01 02 32.8 -24 32 33 01 02 32.78 -24 32 32.3 P 1b Q* -0.9 0.0 18.5         0.24 0.22 0.25 X
PKS B0104-275 01 04 02.1 -27 34 14 01 04 02.07 -27 34 13.9 P 1b Q -0.8 0.0 19.0     2.492 11 0.29 0.37 0.25
PKS B0104-408 01 04 27.6 -40 50 21       1a Q     19.0     0.584 9 0.57 0.85 0.25
PKS B0106+013 01 06 04.5 +01 19 01 01 06 04.50 +01 18 59.6 N 1a Q     18.0     2.094 7 4.24 4.76 0.25
                                   
PKS B0107-395 01 07 26.3 -39 34 27 01 07 27.83 -39 34 35.3 A 3 G? -0.5 -0.5 23.5         0.19 0.15 0.25 X
PKS B0107-610 01 07 16.8 -61 05 46 01 07 17.16 -61 05 46.9 C 1a Q     21.4         0.28 0.37 0.25
PKS B0108-079 01 08 19.0 -07 57 38 01 08 19.01 -07 57 37.6 P 1b Q -1.2 -0.1 19.0     1.776 3 1.02 0.89 0.25
PKS B0108-635 01 08 22.9 -63 31 49 01 08 22.86 -63 31 53.9 T 1c Q -1.3 1.1 19.4         0.29 0.24 0.25
PKS B0110-668 01 10 32.6 -66 50 36       1a Q     17.7         0.34 0.31 0.25
PKS B0111+021 01 11 08.6 +02 06 25 01 11 08.57 +02 06 24.6 P 1b G -1.4 0.0 16.3     0.047 2 0.63 0.65 0.25
PKS B0111-256 01 11 18.7 -25 39 51 01 11 18.77 -25 39 51.9 P 1b Q -0.7 0.5 19.5     1.030 83 0.26 0.23 0.25
PKS B0111-385 01 11 58.5 -38 33 21 01 12 01.79 -38 34 11.8 V 1a NCS -1.2 -0.1   22.9 24.9     0.23 0.18 0.25 X
PKS B0112-017 01 12 43.9 -01 42 55 01 12 43.93 -01 42 55.0 P 1b Q -0.1 -0.3 18.0     1.365 7 0.94 1.10 0.25
PKS B0113-118 01 13 43.2 -11 52 05 01 13 43.22 -11 52 04.6 P 1b Q -1.3 -0.1 18.5     0.670 3 1.78 1.88 0.25
                                   
PKS B0113-283 01 13 01.6 -28 20 45 01 13 01.53 -28 20 45.5 P 1b Q -0.8 -0.5 19.0     2.555 83 0.29 0.43 0.25
PKS B0113-310 01 13 19.0 -31 05 04 01 13 25.56 -31 05 9.1 N 1a Q?     20.2         0.39 0.32 0.20
PKS B0114-351 01 14 17.7 -35 11 35 01 14 18.35 -35 12 49.7 A 2 Q* -0.6 -0.3 18.7         0.07 0.07 0.25 X
PKS B0115-016 01 15 42.2 -01 36 15 01 15 42.21 -01 36 16.6 P 3 Q -0.2 0.4 22.5 20.9 22.6 1.162 83 0.64 0.56 0.25
PKS B0115-342 01 15 25.6 -34 12 53 01 15 25.75 -34 12 54.0 N 1a Q     19.0     0.647 83 0.27 0.26 0.20
PKS B0115-357 01 15 46.0 -35 44 27       1a NCS               0.07 0.09 0.25 X
PKS B0115-368 01 15 45.3 -36 53 57       1a NCS               0.08 0.07 0.25 X
PKS B0116-219 01 16 32.4 -21 57 15 01 16 32.41 -21 57 15.4 P 1b Q -0.4 -0.2 19.0     1.165 3 0.57 0.51 0.25
PKS B0118-272 01 18 09.5 -27 17 07 01 18 09.54 -27 17 07.6 P 1b BL 0.3 -0.2 16.5       83 0.96 1.18 0.25
PKS B0120-078 01 20 24.0 -07 49 30 01 20 23.23 -07 49 15.4 N 1a Q?     19.0         0.11 0.12 0.25 X
                                   
PKS B0122-003 01 22 55.2 -00 21 31 01 22 55.18 -00 21 31.3 P 1b Q -0.4 -0.4 17.0     1.08 12 1.19 1.29 0.25
PKS B0122-005 01 22 43.6 -00 34 04 01 22 43.58 -00 34 04.6 P 1b Q -0.4 0.0 18.5     2.280 13 0.28 0.23 0.25
PKS B0122-042 01 22 03.2 -04 16 33 01 22 02.78 -04 16 41.8 N 1a Q     18.0     0.561 31 0.14 0.25 0.25 X
PKS B0122-514 01 22 53.5 -51 28 50       1a Q     19.2         0.35 0.29 0.25
PKS B0123-016 01 23 27.2 -01 36 17 01 23 27.47 -01 36 27.1 N 1a NCS     13.0     0.018 14 2.17 1.78 0.25 X
PKS B0123-226 01 23 51.2 -22 38 07 01 23 51.29 -22 38 07.7 P 1b Q 0.0 -0.8 18.5     0.720 26 0.48 0.40 0.25
PKS B0124-249 01 24 16.5 -24 55 45 01 24 15.88 -24 55 56.3 P 1b G 0.1 -0.9 18.0         0.22 0.19 0.25 X
PKS B0128-132 01 28 36.7 -13 17 01       1a NCS               0.28 0.22 0.25 X
PKS B0130-106 01 30 56.9 -10 41 21 01 30 57.01 -10 41 40.1 N 1a G     16.5         0.24 0.19 0.25 X
PKS B0130-171 01 30 17.7 -17 10 12 01 30 17.69 -17 10 12.0 P 1b Q 0.0 0.3 19.0     1.020 3 0.99 0.97 0.25


 
Table A.1: continued.
  PKSCAT90 B1950 New radio position B1950       Offsets                
Name RA Dec RA Dec   Ident RA Dec B Gunn-i Gunn-z z zRef S2.7 S5 $S_{\rm lim}$
PKS B0130-447 01 30 54.5 -44 46 25 01 30 52.90 -44 46 05.9 A 3 G -0.6 -1.2 24.3   22.9     0.59 0.49 0.25
PKS B0131-522 01 31 05.6 -52 15 26 01 31 05.61 -52 15 26.6 C 1a Q     20.3         1.09 1.18 0.25
PKS B0133-204 01 33 13.6 -20 24 04 01 33 13.64 -20 24 04.3 P 1b Q -0.3 -0.5 18.0     1.144 3 0.68 0.63 0.25
PKS B0135-247 01 35 17.1 -24 46 09 01 35 17.11 -24 46 08.8 P 1b Q 0.2 -0.4 16.9     0.837 3 1.37 1.65 0.25
PKS B0136-059 01 36 20.9 -05 55 21 01 36 20.90 -05 55 21.0 P 1b Q -0.4 -0.9 20.0     2.004 83 0.30 0.36 0.25
PKS B0136-231 01 36 35.2 -23 09 57 01 36 35.47 -23 09 59.9 P 1b Q -0.7 -1.0 18.0     1.893 31 0.33 0.28 0.25
PKS B0138-097 01 38 56.9 -09 43 52 01 38 56.86 -09 43 51.7 P 1b BL -0.1 -0.4 18.0       83 0.71 1.19 0.25
PKS B0140-059 01 40 08.0 -05 59 12 01 40 08.06 -05 59 07.3 P 1b BL -0.6 -0.4 18.5       83 0.27 0.25 0.25
PKS B0141-609 01 41 17.6 -60 59 56       1a NCS               0.17 0.15 0.25 X
PKS B0142-278 01 42 45.0 -27 48 35 01 42 44.97 -27 48 35.9 N 1b Q     18.5     1.155 3 0.82 0.90 0.25
                                   
PKS B0143-061 01 43 46.5 -06 06 18 01 43 45.56 -06 06 09.8 V 1a NCS -0.1 0.6 21.8     0.499 83 0.28 0.23 0.25 X
PKS B0144-219 01 44 45.7 -21 59 43 01 44 45.56 -21 59 39.7 P 3 G -0.4 -0.2 :24.0 18.7 23.0 0.262 83 0.28 0.22 0.25
PKS B0150-144 01 50 06.1 -14 27 22 01 50 06.23 -14 27 25.8 P 2 Q -0.7 0.3 19.8     1.349 83 0.39 0.37 0.25
PKS B0150-334 01 50 57.0 -33 25 11 01 50 56.97 -33 25 10.1 N 1a Q     16.5     0.610 15 0.92 0.86 0.20
PKS B0152-513 01 52 25.4 -51 22 32       1a Q     18.8     1.581 16 0.29 0.38 0.25
PKS B0153-663 01 53 09.7 -66 18 57       1a Q     18.2         0.37 0.40 0.25
PKS B0155-549 01 55 02.0 -54 54 14       1a G     19.5         0.48 0.47 0.25
PKS B0156-144 01 56 18.1 -14 27 37 01 56 18.34 -14 27 40.5 P 3 G 0.3 -0.6 23.6         0.90 0.73 0.25 X
PKS B0157+011 01 57 29.5 +01 10 43 01 57 29.44 +01 10 41.4 N 1a Q     18.5     1.170 2 0.38 0.40 0.25
PKS B0158-519 01 58 04.3 -51 58 06       1a Q     18.5     2.390 17 0.17 0.15 0.25 X
                                   
PKS B0200-127 02 00 36.8 -12 47 02 02 00 38.38 -12 47 34.8 N 1a G     18.5         0.21 0.17 0.25 X
PKS B0202-172 02 02 34.5 -17 15 39 02 02 34.52 -17 15 39.5 P 1b Q 0.0 -0.4 18.0     1.740 3 1.40 1.38 0.25
PKS B0202-337 02 02 18.6 -33 43 14 02 02 17.67 -33 43 11.0 A 3 G -0.1 -0.4 23.1         0.34 0.31 0.20
PKS B0203-520 02 03 00.8 -52 01 14       1a Q     18.0     1.420 17 0.12 0.16 0.25 X
PKS B0206-688 02 06 47.7 -68 52 06 02 06 47.88 -68 52 06.4 A 1c Q 0.3 -0.4 19.6         0.31 0.32 0.25
PKS B0207-149 02 07 58.8 -14 59 05 02 07 58.90 -14 59 06.3 P 3 G -1.7 0.7 24.1   24.6     0.37 0.50 0.25
PKS B0208-512 02 08 57.1 -51 15 06 02 08 56.96 -51 15 07.8 C 1a Q     17.6     1.003 8 3.56 3.21 0.25
PKS B0213-026 02 13 09.9 -02 36 52 02 13 09.88 -02 36 51.5 P 3 Q -0.1 0.1 21.6   20.9 1.177 83 0.54 0.77 0.25
PKS B0214-085 02 14 34.3 -08 34 43 02 14 34.46 -08 34 43.7 P 1b BL 0.0 -0.4 17.5       83 0.43 0.34 0.25
PKS B0214-330 02 14 38.5 -33 01 35 02 14 38.55 -33 01 32.4 N 1a Q     18.0     1.331 83 0.25 0.24 0.20
                                   
PKS B0214-522 02 14 17.2 -52 14 05 02 14 17.21 -52 14 05.5 W 3 G 1.2 0.6 23.0         0.70 0.55 0.25
PKS B0215+015 02 15 14.1 +01 31 00 02 15 14.14 +01 31 00.0 P 1b BL -0.2 -0.1 18.5     1.715 18 0.73 1.06 0.25
PKS B0215-015 02 15 22.0 -01 35 39 02 15 22.22 -01 35 40.1 P 3 Q* -1.3 -0.2 22.9   21.9     0.27 0.22 0.25
PKS B0216+011 02 16 32.5 +01 07 13 02 16 32.43 +01 07 12.9 N 1a Q     20.0     1.623 19 0.62 0.73 0.25
PKS B0217-189 02 17 00.2 -18 56 24 02 17 00.33 -18 56 24.4 P 1b BL 0.0 -0.3 19.5       83 0.40 0.46 0.25
PKS B0218-220 02 18 16.8 -22 04 54 02 18 16.80 -22 04 54.6 P 1b Q* 0.1 0.1 18.5         0.22 0.21 0.25 X
PKS B0218-683 02 18 44.0 -68 20 02 02 18 43.48 -68 20 01.4 A 3 G 0.7 -0.3 23.1         0.30 0.29 0.25
PKS B0219-164 02 19 38.2 -16 28 55 02 19 38.29 -16 28 55.5 P 1b Q -0.7 -0.9 19.0     0.70 31 0.33 0.38 0.25
PKS B0219-474 02 19 37.0 -47 26 37       1a Q?     18.0         0.33 0.31 0.25
PKS B0219-637 02 19 37.8 -63 43 59       1a Q     18.3         0.51 0.46 0.25


 
Table A.1: continued.
  PKSCAT90 B1950 New radio position B1950       Offsets                
Name RA Dec RA Dec   Ident RA Dec B Gunn-i Gunn-z z zRef S2.7 S5 $S_{\rm lim}$
PKS B0220-349 02 20 49.6 -34 55 04 02 20 49.59 -34 55 4.5 N 1a Q     22.0     1.49 20 0.60 0.61 0.20
PKS B0221-171 02 21 21.7 -17 10 06 02 21 21.96 -17 10 12.3 P 1b Q* -0.5 -1.1 19.5         0.22 0.23 0.25 X
PKS B0222+000 02 22 34.1 +00 03 37 02 22 34.17 +00 03 35.7 N 1a Q     19.0     0.523 8 0.14 0.11 0.10
PKS B0223+012 02 23 34.9 +01 16 03 02 23 35.02 +01 15 58.0 N 1a Q     19.0     1.369 4 0.21 0.17 0.10
PKS B0225-065 02 25 15.2 -06 34 35 02 25 15.22 -06 34 32.3 N 1a e               0.35 0.28 0.25
PKS B0226-038 02 26 22.0 -03 50 57 02 26 22.08 -03 50 58.5 P 1b Q -0.4 -0.3 17.5     2.064 21 0.77 0.71 0.25
PKS B0226-559 02 26 46.8 -55 59 25       1a Q     17.6         0.43 0.45 0.25
PKS B0227-369 02 27 24.9 -36 57 03 02 27 24.85 -36 57 17.1 N 1a Q     19.0     2.115 83 0.25 0.27 0.25
PKS B0229-398 02 29 52.0 -39 48 59 02 29 52.07 -39 48 58.5 N 1a Q     22.3     1.646 20 0.64 0.68 0.25
PKS B0230-790 02 30 28.9 -79 00 59 02 30 28.73 -79 01 00.9 C 1a Q     18.6     :1.07 22 0.57 0.77 0.20
                                   
PKS B0231+022 02 31 13.3 +02 15 48 02 31 13.51 +02 16 16.3 N 1a NCS     17.5     0.322 23 0.07 0.11 0.10 X
PKS B0233-478 02 33 18.7 -47 50 12 02 33 18.49 -47 50 12.7 A 2 Q* 0.4 -2.2 17.3         0.46 0.37 0.25
PKS B0234-301 02 34 21.5 -30 06 56 02 34 21.61 -30 06 56.1 N 1a Q     18.0     2.102 8 0.42 0.53 0.20
PKS B0235-618 02 35 37.6 -61 49 14 02 35 37.76 -61 49 13.5 C 1a Q     17.8         0.55 0.59 0.25
PKS B0237-027 02 37 13.7 -02 47 33 02 37 13.72 -02 47 32.9 P 1b Q -0.8 -0.1 19.0     1.116 24 0.68 1.16 0.25
PKS B0238-052 02 38 26.2 -05 17 30 02 38 26.32 -05 17 30.8 P 1b BL -0.9 -0.5 18.5       83 0.33 0.41 0.25
PKS B0238-084 02 38 37.3 -08 28 09 02 38 37.36 -08 28 09.0 P 1b G 0.4 -0.9 11.6     0.004 3 0.58 1.40 0.25
PKS B0239-553 02 39 15.0 -55 21 00 02 39 16.84 -55 20 30.9 A 1a NCS -1.7 -2.3 23.7         0.16 0.16 0.25 X
PKS B0240-021 02 40 15.0 -02 10 12 02 40 15.45 -02 10 33.1 N 1a Q     19.0     0.617 4 0.12 0.10 0.10
PKS B0240-060 02 40 43.2 -06 03 38 02 40 43.25 -06 03 37.5 P 1b Q -1.0 -0.5 19.0     1.805 83 0.53 0.52 0.25
                                   
PKS B0240-217 02 40 19.3 -21 45 10 02 40 19.34 -21 45 09.7 P 1b G 0.2 -0.6 17.0     0.314 3 0.97 0.82 0.25
PKS B0241-513 02 41 33.8 -51 17 56 02 41 34.06 -51 17 57.3 A 1c Q 0.3 -1.4 20.1         0.40 0.56 0.25
PKS B0244-128 02 44 34.7 -12 49 02 02 44 34.70 -12 49 02.2 P 1b Q -0.9 -0.2 18.5     2.201 6 0.32 0.32 0.25
PKS B0244-297 02 44 12.9 -29 47 38 02 44 12.88 -29 47 38.7 P 1a NCS -0.4 -0.4 22.5         0.36 0.34 0.25 X
PKS B0244-470 02 44 13.4 -47 03 50       1a Q?     18.5         0.73 0.59 0.25
PKS B0245-167 02 45 47.2 -16 44 15 02 45 47.28 -16 44 14.2 P 1b BL -1.0 0.2 20.0       83 0.34 0.32 0.25
PKS B0248-266 02 48 24.2 -26 40 02 02 48 24.34 -26 40 03.1 P 1b Q* 0.5 0.2 19.0         0.21 0.28 0.25 X
PKS B0248-412 02 48 51.0 -41 15 56       1a Q     19.0         0.23 0.22 0.25 X
PKS B0250-602 02 50 11.2 -60 12 19       1a Q     19.0         0.28 0.32 0.25
PKS B0252-549 02 52 00.2 -54 54 02 02 52 00.26 -54 54 02.4 C 1a Q     17.9     0.537 5 0.76 0.80 0.25
                                   
PKS B0253-218 02 53 57.5 -21 49 35 02 53 57.51 -21 49 32.9 P 1b Q -0.7 0.4 18.5     1.470 31 0.30 0.25 0.25
PKS B0253-754 02 53 32.3 -75 25 26       1a Q     21.6         0.34 0.28 0.20
PKS B0254-334 02 54 39.2 -33 27 12 02 54 39.41 -33 27 23.0 N 1a Q     17.0     1.915 8 0.37 0.42 0.20
PKS B0256-005 02 56 55.4 -00 31 52 02 56 55.12 -00 31 54.2 P 1b Q -1.3 -1.0 17.5     1.998 25 0.27 0.23 0.25
PKS B0256-393 02 56 18.9 -39 21 44 02 56 18.47 -39 21 37.8 A 2 Q -0.5 -0.2 19.6     3.449 83 0.32 0.36 0.25
PKS B0257-128 02 57 32.0 -12 48 29 02 57 32.13 -12 48 27.7 P 1b G -0.3 0.3 17.0         0.30 0.24 0.25
PKS B0257-510 02 57 02.5 -51 03 58       1a Q     20.8         0.45 0.39 0.25
PKS B0258+011 02 58 49.0 +01 06 52 02 58 48.85 +01 06 47.2 N 1a Q     20.5     1.221 83 0.37 0.32 0.25
PKS B0258-018 02 58 24.8 -01 51 10 02 58 24.59 -01 51 09.4 P 1b G 0.2 -2.2 19.0         0.16 0.14 0.25 X
PKS B0258-184 02 58 48.5 -18 24 06 02 58 48.60 -18 24 06.7 P 1b Q 0.1 -0.2 19.0     1.627 83 0.25 0.31 0.25


 
Table A.1: continued.
  PKSCAT90 B1950 New radio position B1950       Offsets                
Name RA Dec RA Dec   Ident RA Dec B Gunn-i Gunn-z z zRef S2.7 S5 $S_{\rm lim}$
PKS B0258-344 02 58 34.7 -34 25 58 02 58 34.61 -34 25 54.9 N 1a Q     18.0     1.704 83 0.35 0.33 0.20
PKS B0259-316 02 59 11.5 -31 38 29 02 59 11.50 -31 38 5.2 N 1a G     18.5         0.39 0.42 0.20
PKS B0300-186 03 00 34.0 -18 36 07 03 00 33.97 -18 36 14.5 N 1a G     17.0     0.089 26 0.20 0.17 0.25 X
PKS B0301-721 03 01 31.4 -72 08 17 03 01 31.52 -72 08 18.0 A 1c Q 1.0 -0.9 18.6         0.39 0.40 0.25
PKS B0302-623 03 02 48.0 -62 23 03 03 02 48.14 -62 23 04.1 C 1a Q     19.1         1.11 1.47 0.25
PKS B0305-131 03 05 00.9 -13 09 47 03 05 01.12 -13 09 51.1 N 1a NCS     18.5         0.47 0.38 0.25 X
PKS B0308-611 03 08 51.2 -61 09 57 03 08 51.29 -61 09 58.3 C 1a Q     18.6         0.85 1.32 0.25
PKS B0310+013 03 10 08.7 +01 22 11 03 10 08.55 +01 22 4.7 N 1a Q     18.5     0.660 27 0.42 0.46 0.25
PKS B0312-770 03 12 56.4 -77 02 59       1a Q     17.2     0.223 5 0.50 0.59 0.20
PKS B0313-107 03 13 32.5 -10 42 43 03 13 32.53 -10 42 41.1 P 1b Q* -0.5 -0.1 18.5         0.23 0.19 0.25 X
                                   
PKS B0313-171 03 13 09.1 -17 07 32 03 13 09.28 -17 07 32.9 P 2 Q* -0.1 0.0 18.4         0.22 0.25 0.25 X
PKS B0315-282 03 15 26.9 -28 14 14 03 15 26.88 -28 14 13.5 N 1b Q     20.0     1.166 83 0.40 0.41 0.25
PKS B0318-388 03 18 53.4 -38 48 15 03 18 53.70 -38 48 14.9 A 3 Q* -0.1 1.4 20.7         0.38 0.31 0.25
PKS B0320+015 03 20 34.6 +01 35 13 03 20 34.62 +01 35 12.5 P 3 G 0.5 0.4 23.5 22.9 23.4     0.49 0.42 0.25
PKS B0323-244 03 23 03.2 -24 26 22 03 23 03.11 -24 26 18.4 P 2 Q -0.1 0.2 21.6     1.161 83 0.29 0.26 0.25
PKS B0324-489 03 24 18.0 -48 57 47 03 24 17.87 -48 58 00.8 A 3 G 0.0 0.2 :24.5 22.3 23.8     0.26 0.23 0.25
PKS B0325-222 03 25 47.5 -22 12 26 03 25 47.50 -22 12 27.3 P 1b Q -0.3 -0.3 19.0     2.220 10 0.40 0.41 0.25
PKS B0327-241 03 27 43.9 -24 07 23 03 27 43.88 -24 07 23.1 P 2 Q -0.1 0.3 18.8     0.888 20 0.63 0.73 0.25
PKS B0328-469 03 28 41.5 -46 58 10       1a Q?     18.0         0.18 0.18 0.25 X
PKS B0329-255 03 29 00.5 -25 34 53 03 29 00.46 -25 34 53.2 P 1b Q -0.4 -0.6 17.1     2.685 5 0.41 0.38 0.25
                                   
PKS B0331-448 03 31 55.6 -44 48 57 03 31 54.95 -44 49 01.9 A 3 G 1.5 1.8 23.2 21.5 22.6     0.28 0.22 0.25
PKS B0331-654 03 31 07.1 -65 28 12 03 31 06.89 -65 28 14.4 A 1c Q 1.0 4.1 20.1         0.73 0.59 0.25
PKS B0332-403 03 32 25.2 -40 18 24 03 32 25.24 -40 18 23.8 C 1a Q     18.5     :1.445   1.96 2.60 0.25
PKS B0333-729 03 33 03.2 -72 59 04 03 33 03.25 -72 59 04.4 A 1c Q 0.6 -0.7 19.3         0.43 0.65 0.25
PKS B0334-131 03 34 13.7 -13 11 55 03 34 13.86 -13 11 55.0 N 1a Q     19.0     1.303 83 0.33 0.42 0.25
PKS B0334-546 03 34 35.9 -54 40 17 03 34 36.04 -54 40 17.1 C 1a Q     20.4         0.56 0.63 0.25
PKS B0335-122 03 35 33.5 -12 13 59 03 35 33.37 -12 13 51.1 P 2 Q -0.8 -0.6 21.5   21.8 3.450 28 0.34 0.38 0.25
PKS B0335-364 03 35 00.0 -36 25 55 03 35 00.02 -36 25 54.4 N 1a Q     18.0     1.537 29 0.46 0.46 0.25
PKS B0336-019 03 36 58.9 -01 56 17 03 36 58.96 -01 56 16.9 P 1b Q -1.0 -0.8 18.4     0.852 7 2.58 2.75 0.25
PKS B0338-214 03 38 23.3 -21 29 08 03 38 23.29 -21 29 07.9 P 1b BL -0.5 -0.3 17.5       10 0.82 0.94 0.25
                                   
PKS B0340-600 03 40 24.0 -60 03 43 03 40 22.86 -60 03 40.8 A 2 Q* 0.0 0.3 18.6         0.25 0.26 0.25
PKS B0341-256 03 41 12.0 -25 39 44 03 41 12.16 -25 39 44.3 P 1b Q 0.0 -0.3 19.0     1.419 83 0.40 0.38 0.25
PKS B0342-528 03 42 29.5 -52 50 43       1a G     18.5         0.37 0.31 0.25
PKS B0346-163 03 46 21.8 -16 19 25 03 46 21.83 -16 19 25.6 P 1b BL -0.1 -1.4 18.0       83 0.54 0.55 0.25
PKS B0346-279 03 46 34.0 -27 58 21 03 46 34.03 -27 58 21.0 P 1b Q 0.5 -0.4 19.5     0.991 9 1.10 0.96 0.25
PKS B0347-211 03 47 45.7 -21 11 47 03 47 45.78 -21 11 50.5 P 2 Q 0.3 0.0 21.1     2.944 83 0.37 0.52 0.25
PKS B0348-120 03 48 49.2 -12 02 21 03 48 49.17 -12 02 21.4 P 1b Q -0.7 -0.1 19.5     1.520 3 0.50 0.54 0.25
PKS B0348-326 03 48 45.2 -32 41 57 03 48 45.39 -32 41 58.8 S 3 G 2.9 -0.6 22.9 21.0 23.1 0.927 83 0.27 0.23 0.20
PKS B0350-518 03 50 06.1 -51 51 50       1a Q     20.2         0.36 0.41 0.25
PKS B0351-701 03 51 52.7 -70 08 30 03 51 52.69 -70 08 27.1 A 3 Q 0.8 0.1 22.4   20.5 0.455 83 0.32 0.29 0.25



 
Table A.1: continued.
  PKSCAT90 B1950 New radio position B1950       Offsets                
Name RA Dec RA Dec   Ident RA Dec B Gunn-i Gunn-z z zRef S2.7 S5 $S_{\rm lim}$
PKS B0352-153 03 52 13.7 -15 23 01 03 52 14.77 -15 23 01.1 P 1b G -0.3 0.2 18.0         0.29 0.25 0.25
PKS B0352-164 03 52 07.9 -16 25 09 03 52 07.96 -16 25 09.0 P 1b Q -0.9 -0.1 19.0     1.187 6 0.40 0.40 0.25
PKS B0352-255 03 52 00.2 -25 31 04 03 51 57.26 -25 31 39.8 N 1a Q?     19.5         0.18 0.15 0.25 X
PKS B0353-474 03 53 30.9 -47 27 46 03 53 31.66 -47 27 47.4 A 2 Q* 1.2 0.5 21.6         0.22 0.22 0.25 X
PKS B0354-263 03 54 46.1 -26 21 29 03 54 46.13 -26 21 21.6 N 1a G     18.5         0.23 0.20 0.25 X
PKS B0355-079 03 55 17.5 -07 59 49 03 55 17.53 -07 59 48.9 P 1b Q -1.0 -0.7 18.0     1.050 31 0.34 0.43 0.25
PKS B0355-483 03 55 52.5 -48 20 49 03 55 52.51 -48 20 49.2 C 1a Q     17.5     1.016 30 0.61 0.57 0.25
PKS B0355-669 03 55 27.8 -66 54 12 03 55 27.83 -66 54 12.1 C 1a Q     18.7         0.74 0.62 0.25
PKS B0357-264 03 57 28.4 -26 23 58 03 57 28.47 -26 23 58.1 P 2 BL -0.2 -0.1 21.7       83 0.58 0.47 0.25
PKS B0400-319 04 00 23.6 -31 55 42 04 00 23.61 -31 55 42.0 C 1c Q 0.3 -0.5 19.5     1.288 83 1.14 1.03 0.20
                                   
PKS B0402-362 04 02 02.6 -36 13 12 04 02 02.62 -36 13 11.5 N 1a Q     16.5     1.417 8 1.04 1.29 0.25
PKS B0403-132 04 03 14.0 -13 16 19 04 03 13.99 -13 16 18.2 P 1b Q -0.7 -0.5 17.1     0.571 21 3.15 3.24 0.25
PKS B0403-179 04 03 57.4 -17 58 00 04 03 57.43 -17 57 59.7 P 1b Q -0.7 0.0 19.0     1.640 10 0.38 0.32 0.25
PKS B0405-331 04 05 38.5 -33 11 42 04 05 38.50 -33 11 41.8 N 1a Q     19.0     2.562 20 0.70 0.63 0.20
PKS B0405-385 04 05 12.1 -38 34 25 04 05 11.95 -38 34 26.1 N 1a Q     18.0     1.285 32 1.02 1.06 0.25
PKS B0405-712 04 04 19.2 -71 17 15       1a Q     19.0         0.31 0.25 0.25
PKS B0406-056 04 06 31.7 -05 37 32 04 06 31.65 -05 37 32.0 P 1b G -0.6 -0.2 18.5     0.304 83 0.41 0.34 0.25
PKS B0406-127 04 06 45.3 -12 46 39 04 06 45.33 -12 46 39.1 P 1b Q 0.1 -0.8 18.5     1.563 33 0.59 0.61 0.25
PKS B0406-311 04 06 27.5 -31 08 33 04 06 27.63 -31 08 44.0 S 1a NCS 0.8 -0.9 23.7 22.6       0.55 0.55 0.20 X
PKS B0409-045 04 09 22.0 -04 32 02 04 09 20.54 -04 31 56.6 N 1a Q?     19.5         0.14 0.15 0.25 X
                                   
PKS B0410-519 04 10 19.1 -51 57 01       1a Q     17.5         0.48 0.59 0.25
PKS B0410-756 04 10 47.8 -75 41 33 04 10 49.34 -75 41 32.3 A 3 G -0.6 0.8 23.3 21.6 22.8     0.25 0.21 0.20
PKS B0411-462 04 11 17.4 -46 12 32 04 11 18.53 -46 12 24.4 A 2 Q -0.4 -0.3 20.4     2.223 83 0.42 0.33 0.25
PKS B0414-189 04 14 23.3 -18 58 30 04 14 23.36 -18 58 29.7 P 1b Q -0.6 -0.5 18.0     1.536 26 1.18 1.31 0.25
PKS B0414-467 04 14 27.8 -46 45 05 04 14 28.63 -46 45 11.5 T 2 G 1.7 -0.4 :23.0         0.45 0.36 0.25
PKS B0415-029 04 15 26.5 -02 57 30 04 15 27.51 -02 57 35.8 N 1a X               0.16 0.14 0.25 X
PKS B0418-151 04 18 00.8 -15 08 33 04 18 00.93 -15 08 33.7 P 1b Q* -0.5 0.3 20.5         0.16 0.28 0.25 X
PKS B0420+022 04 20 16.1 +02 12 29 04 20 16.04 +02 12 30.0 N 1a Q     19.5     2.277 83 0.33 0.67 0.25
PKS B0420-014 04 20 43.5 -01 27 29 04 20 43.54 -01 27 28.7 P 1b Q -0.8 -0.3 18.0     0.914 7 2.14 4.15 0.25
PKS B0420-484 04 20 01.0 -48 25 15 04 20 01.95 -48 25 05.9 A 2 Q 0.2 -0.1 17.5     0.527 83 0.29 0.29 0.25
                                   
PKS B0421+019 04 21 32.7 +01 57 33 04 21 32.69 +01 57 33.0 N 1a Q     17.5     2.048 34 0.83 0.73 0.25
PKS B0422+004 04 22 12.5 +00 29 17 04 22 12.50 +00 29 17.1 N 1a BL     16.0     :0.31 35 1.28 1.60 0.25
PKS B0422-380 04 22 56.2 -38 03 09 04 22 56.29 -38 03 09.9 N 1a Q     16.5     0.780 15 0.49 0.81 0.25
PKS B0422-389 04 22 49.1 -38 55 30 04 22 49.10 -38 55 30.9 N 1a Q     18.0     2.346 83 0.47 0.37 0.25
PKS B0423-163 04 23 37.6 -16 19 24 04 23 37.66 -16 19 25.1 P 3 Q* -0.8 -1.6 24.6 21.8 23.3     0.55 0.44 0.25
PKS B0426-380 04 26 54.7 -38 02 52 04 26 54.67 -38 02 52.3 N 1a BL     18.0       83 1.04 1.14 0.25
PKS B0427-435 04 27 49.7 -43 35 02       1a Q     18.0     1.423 83 0.30 0.25 0.25
PKS B0431-512 04 31 04.2 -51 15 44       1a Q     17.7     0.557 30 0.68 0.57 0.25
PKS B0432-440 04 32 30.2 -44 02 03 04 32 29.42 -44 01 58.2 A 2 Q -0.7 0.3 19.6     2.649 83 0.29 0.25 0.25
PKS B0432-606 04 32 50.3 -60 36 25       1a Q     19.0         0.43 0.39 0.25


 
Table A.1: continued.
  PKSCAT90 B1950 New radio position B1950       Offsets                
Name RA Dec RA Dec   Ident RA Dec B Gunn-i Gunn-z z zRef S2.7 S5 $S_{\rm lim}$
PKS B0434-188 04 34 49.0 -18 50 48 04 34 48.97 -18 50 48.2 P 1b Q -0.3 -0.5 20.0     2.702 3 1.05 1.19 0.25
PKS B0435-083 04 35 43.8 -08 23 24 04 35 43.13 -08 24 44.9 V 3 G -0.7 -0.9 >24.0   24.4     0.20 0.22 0.25 X
PKS B0436-089 04 36 13.8 -08 54 14 04 36 13.88 -08 54 14.8 P 1b G -0.6 -0.1 20.0         0.35 0.31 0.25
PKS B0436-129 04 36 15.5 -12 56 56 04 36 15.60 -12 56 56.8 P 1b Q -0.4 -0.3 19.0     1.277 31 0.40 0.43 0.25
PKS B0436-203 04 36 39.6 -20 18 14 04 36 39.84 -20 18 18.5 P 3 Q -1.8 1.4 22.8   23.1 2.146 83 0.36 0.30 0.25
PKS B0437-454 04 37 30.6 -45 28 12 04 37 30.64 -45 28 12.4 W 2 Q* 0.0 -0.2 20.8         1.22 1.37 0.25
PKS B0438-436 04 38 43.2 -43 38 53 04 38 43.19 -43 38 53.5 C 1a Q     19.5     2.863 36 6.50 7.00 0.25
PKS B0439-299 04 39 21.9 -29 58 17 04 39 21.93 -29 58 17.8 P 1b G -0.5 -1.0 19.5         0.41 0.33 0.25
PKS B0439-433 04 39 43.6 -43 19 10       1a Q     16.5     0.593 31 0.32 0.30 0.25
PKS B0439-501 04 39 52.4 -50 09 50 04 39 53.69 -50 09 44.4 A 2 Q* -0.7 -0.1 20.6         0.25 0.21 0.25
                                   
PKS B0440-285 04 40 38.0 -28 31 06 04 40 38.06 -28 31 07.0 P 1b Q -0.3 -1.4 19.0     1.952 9 0.34 0.45 0.25
PKS B0440-520 04 40 45.0 -52 00 34       1a Q?     17.5         0.32 0.33 0.25
PKS B0445-019 04 45 11.6 -01 58 01 04 45 11.00 -01 58 03.5 P 1b Q -0.2 0.1 19.0         0.23 0.18 0.25 X
PKS B0446-175 04 46 50.8 -17 34 25 04 46 50.53 -17 34 23.8 P 2 G -0.2 0.2 23.3   22.1     0.24 0.19 0.25 X
PKS B0446-212 04 46 08.4 -21 15 02 04 46 08.27 -21 14 57.8 P 1b Q 0.0 0.1 19.5     1.971 37 0.29 0.28 0.25
PKS B0446-370 04 46 30.1 -37 04 29 04 46 29.19 -37 04 14.3 A 2 Q 0.1 -0.9 18.9     0.561 83 0.27 0.26 0.25
PKS B0447-010 04 47 10.4 -01 02 28 04 47 10.27 -01 02 30.2 P 1b Q -0.9 -0.8 19.5     0.487 83 0.41 0.35 0.25
PKS B0448-187 04 48 23.8 -18 42 07 04 48 23.68 -18 42 03.9 P 1b Q 0.1 -0.7 19.0     2.05 31 0.43 0.43 0.25
PKS B0448-392 04 48 00.4 -39 16 15 04 48 00.47 -39 16 15.4 N 1a Q     17.5     1.288 15 0.89 0.89 0.25
PKS B0450-230 04 50 37.7 -23 03 10 04 50 38.31 -23 03 00.6 N 2 Q? -1.0 2.4 21.2         0.23 0.19 0.25 X
                                   
PKS B0450-469 04 50 27.8 -46 58 16 04 50 27.91 -46 58 16.2 C 1a Q?     19.0         0.69 0.58 0.25
PKS B0451-282 04 51 15.1 -28 12 29 04 51 15.14 -28 12 29.4 P 1b Q 0.5 -1.1 19.0     2.564 24 2.38 2.50 0.25
PKS B0454-234 04 54 57.3 -23 29 28 04 54 57.31 -23 29 28.3 P 1b Q 0.0 0.5 18.5     1.003 1 1.76 2.00 0.25
PKS B0455-395 04 55 47.0 -39 32 05 04 55 48.02 -39 32 09.9 T 2 Q -0.2 -0.1 18.6     0.570 9 0.15 0.14 0.25 X
PKS B0458-020 04 58 41.3 -02 03 34 04 58 41.35 -02 03 33.9 P 1b Q -1.2 0.2 20.0     2.286 27 1.89 2.19 0.25
PKS B0459-308 04 59 12.1 -30 51 50 04 59 11.75 -30 51 55.9 N 1a Q?     19.0         0.17 0.14 0.20 X
PKS B0500+019 05 00 45.2 +01 58 54 05 00 45.18 +01 58 53.9 W 3 G -0.3 -0.8 22.8 19.5 21.3 0.584 83 2.46 2.04 0.25
PKS B0503-608 05 03 24.0 -60 53 57       1a Q     19.3         0.58 0.74 0.25
PKS B0509+011 05 09 23.0 +01 07 10 05 09 22.54 +01 07 16.1 N 1a G     18.0         0.39 0.35 0.25
PKS B0510-006 05 10 29.5 -00 36 00 05 10 29.44 -00 35 54.2 N 1a G     19.4         0.33 0.31 0.25
                                   
PKS B0511-220 05 11 41.8 -22 02 41 05 11 41.82 -22 02 41.2 P 1b Q -0.6 -0.6 19.5     1.296 1 1.21 1.27 0.60
PKS B0512-013 05 12 39.0 -01 22 57 05 12 38.97 -01 23 22.4 P 1b Q* -0.3 0.4 18.5         0.15 0.13 0.25 X
PKS B0514-161 05 14 01.1 -16 06 23 05 14 01.08 -16 06 22.6 P 1b Q -0.6 -0.2 18.0     1.278 2 0.80 0.76 0.60
PKS B0516-621 05 16 15.4 -62 10 13 05 16 15.38 -62 10 14.4 A 1c Q 0.4 -0.8 21.0         0.38 0.44 0.25
PKS B0519+011 05 19 42.3 +01 10 41 05 19 42.36 +01 10 41.9 N 2 G? 0.0 -0.8 :22.2         0.55 0.55 0.25
PKS B0522-030 05 22 08.8 -03 03 35 05 22 08.11 -03 03 40.0 N 1a X               0.06 0.11 0.25 X
PKS B0522-611 05 22 00.2 -61 10 42 05 22 00.39 -61 10 41.4 C 1a Q     19.0     1.400 33 0.71 0.67 0.25
PKS B0524-433 05 24 23.0 -43 20 35       1a Q     18.0     2.164 83 0.29 0.27 0.25
PKS B0524-460 05 24 06.0 -46 00 28       1a Q     17.3     1.479 38 0.91 0.99 0.25
PKS B0524-485 05 24 56.5 -48 33 06       1a Q?     20.0         0.45 0.48 0.25


 
Table A.1: continued.
  PKSCAT90 B1950 New radio position B1950       Offsets                
Name RA Dec RA Dec   Ident RA Dec B Gunn-i Gunn-z z zRef S2.7 S5 $S_{\rm lim}$
PKS B0525-127 05 25 09.4 -12 44 16 05 25 09.39 -12 44 17.0 N 1a PN     10.0         1.63 1.78 0.60
PKS B0528-250 05 28 05.2 -25 05 44 05 28 05.21 -25 05 44.6 P 1b Q -0.4 -0.9 19.0     2.813 15 1.32 1.13 0.60
PKS B0528-454 05 28 58.5 -45 26 45       1a X               0.39 0.34 0.25
PKS B0529-305 05 29 20.5 -30 34 16 05 29 20.62 -30 34 23.6 S 2 G 2.6 -1.4 22.4         0.38 0.31 0.20
PKS B0532-378 05 32 35.2 -37 49 22 05 32 35.26 -37 49 21.4 C 1c Q -1.1 0.1 19.5     1.668 20 0.70 0.59 0.25
PKS B0533-120 05 33 13.1 -12 04 31 05 33 13.74 -12 04 14.2 P 1b G -0.3 -0.5 17.8     0.157 39 0.80 0.64 0.60
PKS B0534-340 05 34 39.6 -34 02 58 05 34 39.57 -34 02 58.1 W 2 Q -0.3 -0.3 18.3     0.683 83 0.41 0.73 0.20
PKS B0534-611 05 34 02.4 -61 07 59       1a Q     18.8         0.42 0.47 0.25
PKS B0537-158 05 37 17.1 -15 52 05 05 37 17.17 -15 52 04.6 P 1b Q -0.6 0.0 18.0     0.947 33 0.63 0.61 0.60
PKS B0537-286 05 37 56.9 -28 41 28 05 37 56.94 -28 41 28.0 P 1b Q -0.7 -0.5 20.0     3.110 40 0.74 0.99 0.60
                                   
PKS B0537-441 05 37 21.1 -44 06 45 05 37 21.08 -44 06 44.6 C 1a Q     15.0     0.894 8 3.84 3.80 0.25
PKS B0539-057 05 39 11.0 -05 43 15 05 39 11.00 -05 43 15.0 P 1b Q -0.3 0.0 20.0     0.893 41 0.65 1.51 0.60
PKS B0549-459 05 49 52.3 -45 56 54       1a X               0.32 0.31 0.25
PKS B0549-575 05 49 20.8 -57 33 11       1a Q     19.5         0.35 0.41 0.25
PKS B0551-538 05 51 33.8 -53 50 07       1a X               0.27 0.22 0.25
PKS B0557-454 05 57 45.0 -45 28 27 05 57 45.79 -45 29 47.0 A 2 Q -0.4 0.1 17.9     0.687 67 0.24 0.19 0.25 X
PKS B0601-172 06 01 44.8 -17 16 19 06 01 44.77 -17 16 15.8 P 1b Q -0.4 -0.8 20.0     2.711 83 0.40 0.55 0.60 X
PKS B0602-424 06 02 52.4 -42 25 14 06 02 52.49 -42 25 14.1 C 1a Q     19.0     0.611 83 0.35 0.84 0.25
PKS B0605-063 06 05 19.2 -06 22 38 06 05 19.80 -06 22 34.3 N 1a HII               5.60 6.94 0.60
PKS B0605-085 06 05 36.0 -08 34 20 06 05 36.03 -08 34 20.2 P 1b Q -1.6 -2.6 18.0     0.872 38 2.90 3.39 0.60
                                   
PKS B0606-223 06 06 53.4 -22 19 46 06 06 53.39 -22 19 46.2 P 1b Q -0.6 0.4 20.0     1.926 33 1.00 1.36 0.60
PKS B0607-157 06 07 26.0 -15 42 03 06 07 25.99 -15 42 03.3 P 1b Q 2.3 -2.9 18.0     0.324 26 2.20 1.77 0.60
PKS B0607-605 06 07 19.5 -60 31 18 06 07 19.56 -60 31 18.7 A 1c Q 0.0 0.3 18.2         0.34 0.45 0.60 X
PKS B0610-316 06 10 37.0 -31 38 07 06 10 36.98 -31 38 06.6 N 1a Q     18.5     0.873 83 0.47 0.51 0.20
PKS B0610-436 06 10 58.3 -43 36 58 06 10 58.46 -43 36 57.1 C 1a Q     19.0     3.461 83 0.35 0.64 0.25
PKS B0613-312 06 13 27.0 -31 16 23 06 13 26.02 -31 16 18.8 N 1a BL     17.0       83 0.32 0.33 0.20
PKS B0615-305 06 15 45.7 -30 30 16 06 15 45.97 -30 30 18.0 A 3 G -1.5 1.5 23.6   23.4     0.27 0.23 0.20
PKS B0618-252 06 18 29.7 -25 13 53 06 18 29.77 -25 13 52.2 P 1b Q -0.4 -0.5 18.2     :1.90   0.81 0.73 0.60
PKS B0619-468 06 19 50.0 -46 50 30       1a X               0.43 0.56 0.60 X
PKS B0621-786 06 21 29.7 -78 41 33       1a Q     17.5     0.942 5 0.16 0.18 0.20 X
                                   
PKS B0622-441 06 22 02.7 -44 11 23       1a Q     17.5     0.688 15 0.77 0.89 0.60
PKS B0625-401 06 25 17.3 -40 11 57 06 25 17.19 -40 10 57.9 T 3 G -0.2 -0.8 23.4 20.3 22.1     0.25 0.23 0.25
PKS B0627-199 06 27 14.1 -19 57 16 06 27 14.12 -19 57 16.2 P 2 BL -0.1 0.0 21.1       83 0.57 0.75 0.60 X
PKS B0628-627 06 28 32.7 -62 46 40 06 28 32.76 -62 46 39.4 A 1c G? -0.2 0.3 21.5         0.37 0.44 0.60 X
PKS B0629-418 06 29 37.7 -41 52 14 06 29 37.67 -41 52 14.3 C 1a Q     17.0     1.416 6 0.53 0.74 0.25
PKS B0630-261 06 30 05.0 -26 11 45 06 30 05.37 -26 11 58.4 P 3 Q 2.7 0.1 20.5 19.0 20.2 0.717 83 0.44 0.44 0.60 X
PKS B0637-337 06 37 31.2 -33 43 12 06 37 31.16 -33 43 12.8 N 1a BL     20.5       83 0.54 0.70 0.20
PKS B0637-752 06 37 23.3 -75 13 37       1a Q     17.2     0.651 30 5.90 5.49 0.20
PKS B0642-349 06 42 37.4 -34 56 33 06 42 37.45 -34 56 34.0 N 1a Q     18.5     2.165 15 0.94 0.99 0.20
PKS B0644-390 06 44 50.4 -39 00 06 06 44 50.25 -39 00 22.0 N 1a Q     18.5     0.681 83 0.28 0.26 0.25


 
Table A.1: continued.
  PKSCAT90 B1950 New radio position B1950       Offsets                
Name RA Dec RA Dec   Ident RA Dec B Gunn-i Gunn-z z zRef S2.7 S5 $S_{\rm lim}$
PKS B0644-671 06 44 30.3 -67 09 44       1a G?     21.7         0.32 0.41 0.25
PKS B0646-306 06 46 19.2 -30 40 54 06 46 19.22 -30 40 54.3 W 2 Q -0.2 -0.9 20.4     1.153 83 0.95 1.06 0.20
PKS B0700-465 07 00 07.5 -46 30 14 07 00 08.86 -46 30 13.5 R 2 Q 0.0 0.0 19.5     0.822 83 0.55 0.64 0.60 X
PKS B0700-661 07 00 23.6 -66 06 26 07 00 23.46 -66 06 23.6 T 1c Q -1.4 -1.8 19.2         0.25 0.45 0.25
PKS B0715-663 07 15 06.5 -66 22 44       1a X               0.43 0.36 0.25
PKS B0726-476 07 26 57.3 -47 39 13 07 26 57.91 -47 39 02.5 T 3 Q 0.1 -0.3 22.4   22.2 2.282 83 0.38 0.30 0.60 X
PKS B0731-465 07 31 16.3 -46 33 53 07 31 15.66 -46 33 45.7 C 2 Q?     22.0         0.83 0.76 0.60
PKS B0736+017 07 36 42.5 +01 44 00 07 36 42.52 +01 44 00.2 P 1b Q 0.2 -0.2 18.0     0.191 21 2.24 1.85 0.25
PKS B0736-770 07 36 37.3 -77 04 28 07 36 37.07 -77 04 27.3 T 1c Q 0.4 -0.1 21.6         0.26 0.21 0.20
PKS B0738-674 07 38 49.7 -67 28 50       1a Q     19.8     1.663 31 0.45 0.56 0.25
                                   
PKS B0743-006 07 43 21.0 -00 36 56 07 43 21.05 -00 36 55.7 P 1b Q -0.2 -0.8 18.0     0.994 9 1.01 1.31 0.25
PKS B0744-691 07 44 25.4 -69 11 47       1a Q     21.5         0.38 0.43 0.25
PKS B0748-006 07 48 37.0 -00 39 09 07 48 37.21 -00 39 08.6 P 1b Q 0.1 -0.2 20.5         0.20 0.23 0.25 X
PKS B0800-098 08 00 16.1 -09 49 44 08 00 08.76 -09 49 06.3 N 1a NCS     18.5         1.20 0.99 0.60 X
PKS B0802-010 08 02 42.9 -01 02 50 08 02 40.26 -01 02 37.8 P 1b NCS -0.3 0.0 17.5     0.088 43 0.33 0.33 0.25 X
PKS B0805-077 08 05 49.5 -07 42 22 08 05 49.56 -07 42 22.3 P 1b Q -0.2 -0.4 19.0     1.837 9 1.10 1.01 0.60
PKS B0805-119 08 05 14.4 -11 58 59 08 05 14.41 -11 58 58.4 P 1a NCS -0.1 0.0 19.1         0.51 0.44 0.60 X
PKS B0806-710 08 06 46.3 -71 03 30 08 06 46.59 -71 03 26.9 A 1c Q -0.2 0.4 20.0     0.330 83 0.44 0.40 0.25
PKS B0808+019 08 08 51.1 +01 55 51 08 08 51.14 +01 55 51.2 P 1b BL 0.0 -0.6 17.0     :0.93   0.40 0.59 0.25
PKS B0813-741 08 13 14.2 -74 11 07 08 13 15.57 -74 11 05.2 A 1a NCS -4.3 -1.0 23.2         0.40 0.38 0.25 X
                                   
PKS B0818-128 08 18 36.2 -12 49 25 08 18 36.26 -12 49 25.0 P 1b BL -0.7 -0.1 18.0         0.87 0.81 0.60
PKS B0819+012 08 19 01.1 +01 12 28 08 19 00.37 +01 12 08.4 N 2 G 1.0 2.7 17.0         0.10 0.08 0.25 X
PKS B0819-032 08 19 09.5 -03 13 39 08 19 09.46 -03 13 36.2 P 1b Q -0.8 -0.8 18.2     2.352 15 0.37 0.30 0.25
PKS B0834-201 08 34 24.6 -20 06 30 08 34 24.64 -20 06 29.6 N 1b Q     19.0     2.752 24 4.15 3.42 0.60
PKS B0834-223 08 34 38.5 -22 22 40 08 34 38.52 -22 22 40.1 P 2 Q 0.0 -1.4 18.0     0.837 83 0.50 0.47 0.60 X
PKS B0837+012 08 37 14.6 +01 15 04 08 37 14.81 +01 15 06.3 N 1a Q     19.0     1.123 44 0.45 0.39 0.25
PKS B0845-051 08 45 29.5 -05 09 28 08 45 29.52 -05 09 27.7 N 1a Q     19.5     1.242 33 0.49 0.40 0.60 X
PKS B0855-716 08 55 04.1 -71 37 31       1a Q     19.3         0.33 0.38 0.25
PKS B0858-004 08 58 52.8 -00 25 12 08 58 52.50 -00 25 13.6 N 1a Q     20.0         0.24 0.19 0.25 X
PKS B0858-771 08 58 39.5 -77 07 42       1a Q     18.0     0.489 31 0.42 0.33 0.20
                                   
PKS B0859-140 08 59 54.9 -14 03 39 08 59 54.95 -14 03 38.7 P 1b Q -0.2 -0.1 16.6     1.333 31 2.93 2.29 0.60
PKS B0902-256 09 02 40.9 -25 40 51 09 02 40.89 -25 40 51.3 P 1b Q -0.2 -0.1 18.0     1.635 33 0.50 0.47 0.60 X
PKS B0906+015 09 06 35.2 +01 33 48 09 06 35.19 +01 33 48.2 P 1b Q 0.0 -1.0 18.0     1.020 15 0.97 1.20 0.25
PKS B0907+022 09 07 04.1 +02 12 19 09 07 04.42 +02 12 19.3 N 1a BL     19.0       83 0.26 0.43 0.25
PKS B0909-745 09 09 33.2 -74 32 49       1a Q     21.0         0.31 0.28 0.25
PKS B0913+003 09 13 18.0 +00 19 55 09 13 17.78 +00 19 45.4 N 2 Q -0.8 0.0 21.7     3.074 83 0.27 0.25 0.25
PKS B0915-213 09 15 10.3 -21 18 57 09 15 10.44 -21 18 57.0 P 1b Q -0.4 -0.5 18.5     0.847 33 0.59 0.54 0.60 X
PKS B0919-260 09 19 16.7 -26 05 55 09 19 16.71 -26 05 54.4 P 1b Q -0.2 -1.0 19.0     2.300 33 1.15 1.28 0.60
PKS B0921-213 09 21 21.8 -21 22 47 09 21 21.83 -21 22 52.2 P 1b G -0.1 -0.5 16.5     0.052 45 0.53 0.42 0.60 X
PKS B0922+005 09 22 33.7 +00 32 12 09 22 33.68 +00 32 12.9 N 1a Q     18.5     1.720 23 0.82 0.70 0.25


 
Table A.1: continued.
  PKSCAT90 B1950 New radio position B1950       Offsets                
Name RA Dec RA Dec   Ident RA Dec B Gunn-i Gunn-z z zRef S2.7 S5 $S_{\rm lim}$
PKS B0925-203 09 25 33.5 -20 21 45 09 25 33.55 -20 21 44.8 P 1b Q 0.2 -0.8 16.3     0.348 45 0.81 0.70 0.60
PKS B0926-039 09 26 01.8 -03 55 52 09 26 02.61 -03 56 02.2 V 2 Q* 0.3 0.5 20.3         0.14 0.13 0.60 X
PKS B0928+008 09 28 18.1 +00 48 12 09 28 17.99 +00 48 12.6 N 1a Q     19.0     0.505 6 0.30 0.33 0.25
PKS B0930-338 09 30 29.0 -33 52 31 09 30 30.03 -33 52 38.6 S 2 Q -1.7 -0.8 19.5     0.936 83 0.34 0.31 0.20
PKS B0931-114 09 31 08.8 -11 26 03 09 31 08.91 -11 26 04.0 P 3 G -2.9 -1.0 23.0 20.7 22.1     0.45 0.44 0.60 X
PKS B0933-333 09 33 01.1 -33 19 08 09 33 01.71 -33 19 12.0 V 2 Q -0.8 -0.3 20.0   20.8 2.906 83 0.31 0.32 0.20
PKS B0938-002 09 38 07.3 -00 14 56 09 38 06.96 -00 14 21.6 P 2 Q* -0.3 0.6 20.4   21.5     0.24 0.22 0.25 X
PKS B0945-321 09 45 58.9 -32 09 49 09 45 58.86 -32 09 48.5 N 1a Q     19.0     2.14 9 0.58 0.83 0.20
PKS B0952-691 09 52 20.0 -69 10 12 09 52 19.88 -69 10 12.7 A 1c Q 0.8 -0.2 19.1         0.27 0.22 0.25
PKS B0958-314 09 58 27.4 -31 25 26 09 58 27.69 -31 25 23.9 N 1a G     12.7         0.48 0.51 0.20
                                   
PKS B0959-307 09 59 26.1 -30 44 07 09 59 26.07 -30 43 59.7 N 1a NCS               0.61 0.49 0.20 X
PKS B1004-018 10 04 31.7 -01 52 31 10 04 31.72 -01 52 30.5 P 1b Q -0.2 0.1 19.2     1.212 7 0.59 0.53 0.25
PKS B1004-217 10 04 25.8 -21 44 39 10 04 25.50 -21 44 40.3 P 1b Q 0.0 -0.2 16.4     0.330 22 0.30 0.30 0.25
PKS B1005-333 10 05 17.5 -33 18 15 10 05 18.54 -33 18 26.9 N 1a Q     18.0     1.837 83 0.27 0.31 0.20
PKS B1005-739 10 05 22.6 -73 55 03 10 05 22.16 -73 55 04.0 A 1c Q 1.0 0.3 20.1         0.40 0.48 0.25
PKS B1008+013 10 08 41.6 +01 21 28 10 08 41.19 +01 21 31.1 N 1a BL     19.0       83 0.27 0.23 0.25
PKS B1008-041 10 08 58.0 -04 08 41 10 08 58.79 -04 08 38.2 P 1b Q -0.1 -0.4 18.5         0.17 0.21 0.25 X
PKS B1009-321 10 09 41.8 -32 08 44 10 09 41.78 -32 08 44.0 N 1a Q     18.1     1.742 30 0.32 0.27 0.20
PKS B1009-328 10 09 53.1 -32 49 30 10 09 51.97 -32 49 25.4 V 2 Q -0.4 -0.5 19.0   20.0 1.745 83 0.26 0.22 0.20
PKS B1010-255 10 10 54.0 -25 32 20 10 10 53.92 -25 32 01.5 V 2 G 0.3 0.7 21.9   24.1     0.21 0.17 0.25 X
                                   
PKS B1010-427 10 10 32.3 -42 43 39       1a Q     17.5     2.954 83 0.38 0.43 0.25
PKS B1016-268 10 16 50.3 -26 53 46 10 16 49.41 -26 53 50.9 P 2 BL 0.0 -0.1 18.3       83 0.29 0.36 0.25
PKS B1016-311 10 16 12.6 -31 08 51 10 16 12.53 -31 08 51.3 N 1a Q     18.5     0.794 20 0.62 0.65 0.20
PKS B1021-323 10 21 45.6 -32 18 58 10 21 44.13 -32 19 1.6 N 1a Q     19.5     1.568 83 0.46 0.37 0.20
PKS B1022-102 10 22 29.6 -10 16 25 10 22 27.60 -10 16 27.9 P 1b Q -0.4 -0.8 16.8     2.00 46 0.27 0.27 0.25
PKS B1022-183 10 22 21.5 -18 23 03 10 22 21.47 -18 23 17.4 N 1a PN     9.0         0.92 0.81 0.25
PKS B1026-084 10 26 09.3 -08 29 15 10 26 09.03 -08 29 16.9 P 2 Q 0.5 0.4 21.4     4.276 47 0.27 0.22 0.25
PKS B1027-186 10 27 08.3 -18 37 29 10 27 08.18 -18 37 27.0 P 1b Q 0.2 -0.7 19.0     1.784 83 0.26 0.21 0.25
PKS B1029-222 10 29 28.1 -22 13 12 10 29 29.00 -22 12 57.8 P 3 G 1.4 2.6 >23.0   22.6     0.34 0.27 0.25
PKS B1030-357 10 30 52.1 -35 46 27 10 30 51.80 -35 46 31.1 N 1a Q     20.5     1.455 6 0.66 0.57 0.25
                                   
PKS B1031-019 10 31 51.9 -01 55 36 10 31 51.56 -01 55 31.6 V 2 G -0.6 -0.9 20.7         0.14 0.14 0.25 X
PKS B1032-199 10 32 37.4 -19 56 02 10 32 37.37 -19 56 02.0 P 1b Q -0.2 -0.6 18.5     2.198 33 1.10 1.15 0.25
PKS B1034-058 10 34 16.4 -05 50 07 10 34 16.34 -05 50 06.2 P 1b G? -0.5 -0.6 20.0         0.46 0.58 0.25
PKS B1034-293 10 34 55.8 -29 18 27 10 34 55.83 -29 18 26.8 P 1b Q 0.2 -0.1 17.0     0.312 1 1.33 1.51 0.25
PKS B1034-374 10 34 38.2 -37 28 40 10 34 38.16 -37 28 35.1 N 1a Q     18.5     1.821 6 0.54 0.44 0.25
PKS B1035-728 10 35 57.0 -72 49 55 10 35 56.69 -72 49 54.9 A 1c Q* -1.3 -0.8 19.5         0.43 0.39 0.25
PKS B1036-154 10 36 39.5 -15 25 28 10 36 39.48 -15 25 28.0 P 1b Q -0.3 -0.7 19.5     0.525 20 0.75 0.78 0.25
PKS B1036-431 10 36 03.5 -43 09 39 10 36 03.06 -43 10 08.8 S 2 Q 1.8 0.4 18.5     1.356 83 0.42 0.39 0.25
PKS B1044-128 10 44 35.6 -12 52 41 10 44 35.09 -12 52 42.1 P 1b Q -0.4 -0.7 18.0     1.288 48 0.28 0.33 0.25
PKS B1045+019 10 45 48.4 +01 57 40 10 45 48.43 +01 57 40.0 V 3 G -0.1 -0.5 >24.5 22.4       0.49 0.43 0.25


 
Table A.1: continued.
  PKSCAT90 B1950 New radio position B1950       Offsets                
Name RA Dec RA Dec   Ident RA Dec B Gunn-i Gunn-z z zRef S2.7 S5 $S_{\rm lim}$
PKS B1045-188 10 45 40.1 -18 53 44 10 45 40.10 -18 53 43.9 P 1b Q -0.1 -0.5 19.0     0.595 38 0.94 1.11 0.25
PKS B1046-222 10 46 58.6 -22 15 01 10 46 56.61 -22 15 13.9 P 2 Q 0.5 -0.2 21.7   21.1 1.609 83 0.29 0.24 0.25
PKS B1048-313 10 48 43.4 -31 22 19 10 48 43.39 -31 22 18.5 W 2 Q -0.4 -0.1 18.5     1.429 20 0.80 0.73 0.20
PKS B1049-349 10 49 09.4 -34 58 00 10 49 12.07 -34 58 06.3 V 3 G -1.1 -2.2 21.8   21.7     0.30 0.24 0.20
PKS B1049-726 10 49 16.7 -72 38 36 10 49 16.33 -72 38 36.5 A 1c Q -0.3 0.0 20.4         0.27 0.22 0.25
PKS B1055+018 10 55 55.3 +01 50 04 10 55 55.32 +01 50 03.6 P 1b Q 0.5 -0.9 18.2     0.888 7 3.15 3.16 0.25
PKS B1055-243 10 55 29.9 -24 17 45 10 55 29.94 -24 17 44.5 P 2 Q -0.4 0.1 19.9     1.086 20 0.77 0.61 0.25
PKS B1055-248 10 55 29.6 -24 53 50 10 55 28.89 -24 53 24.6 P 2 Q 0.0 0.4 18.7   19.8 0.593 83 0.32 0.31 0.25
PKS B1055-301 10 55 38.3 -30 08 57 10 55 37.28 -30 08 51.0 N 1a Q     19.5     2.523 83 0.36 0.43 0.20
PKS B1056-113 10 56 42.3 -11 18 17 10 56 42.30 -11 18 17.0 P 1b BL -0.4 -0.5 17.5       83 0.37 0.61 0.25
                                   
PKS B1057-797 10 57 50.0 -79 47 48 10 57 49.73 -79 47 47.7 C 1c Q 0.5 0.5 19.0         1.13 1.57 0.20
PKS B1101-325 11 01 07.8 -32 35 01 11 01 08.43 -32 35 8.1 N 1a Q     15.4     0.355 15 0.93 0.73 0.20
PKS B1102-242 11 02 19.8 -24 15 14 11 02 19.81 -24 15 13.7 P 1b Q -0.3 -0.7 19.3     1.666 20 0.50 0.57 0.25
PKS B1104-445 11 04 50.4 -44 32 53 11 04 50.38 -44 32 52.8 C 1a Q     18.0     1.598 45 1.84 2.03 0.25
PKS B1105-304 11 05 18.8 -30 27 12 11 05 19.45 -30 27 21.0 S 2 Q 0.6 1.7 20.2     0.740 83 0.26 0.26 0.20
PKS B1106-227 11 06 43.3 -22 45 28 11 06 43.34 -22 45 28.6 P 2 Q 0.5 -0.1 20.8     1.875 83 0.32 0.29 0.25
PKS B1110-217 11 10 21.7 -21 42 10 11 10 21.71 -21 42 09.2 P 2 G 0.4 0.1 22.5         0.94 0.76 0.25
PKS B1110-355 11 10 37.6 -35 33 30 11 10 37.70 -35 33 23.1 N 1a Q     19.0     1.695 83 0.26 0.34 0.25
PKS B1112-080 11 12 00.8 -08 00 25 11 12 00.74 -08 00 17.4 P 3 G -1.1 1.2 22.6   21.9     0.26 0.34 0.25
PKS B1115-122 11 15 46.1 -12 16 29 11 15 46.13 -12 16 29.5 P 1b Q -0.3 -1.0 19.0     1.739 20 0.67 0.63 0.25
                                   
PKS B1115-306 11 15 55.9 -30 38 12 11 15 54.25 -30 38 34.2 N 1a Q?     18.5         0.22 0.18 0.20
PKS B1117-124 11 17 41.4 -12 27 14 11 17 40.99 -12 27 11.5 P 2 G 0.3 -0.2 22.1   21.4     0.26 0.29 0.25
PKS B1117-270 11 17 48.8 -27 02 59 11 17 48.54 -27 02 39.9 P 1b Q 1.6 -0.2 19.0     1.881 83 0.42 0.34 0.25
PKS B1118-056 11 18 52.1 -05 38 30 11 18 52.52 -05 37 29.2 P 2 Q -0.6 -0.4 19.4     1.297 20 0.66 0.57 0.25
PKS B1118-140 11 18 24.8 -14 04 02 11 18 24.77 -14 04 03.0 P 1b Q -0.3 -0.3 17.5     1.114 83 0.34 0.59 0.25
PKS B1119-069 11 19 09.9 -06 54 52 11 19 09.79 -06 54 39.0 P 2 BL 0.0 -0.6 20.3   20.1   83 0.34 0.42 0.25
PKS B1124-073 11 24 39.3 -07 18 41 11 24 39.98 -07 18 40.9 P 3 Q* 0.8 -0.3 :23.0   21.8     0.37 0.49 0.25
PKS B1124-186 11 24 34.1 -18 40 46 11 24 34.02 -18 40 46.2 P 1b Q 0.0 -0.9 19.0     1.048 20 0.61 0.84 0.25
PKS B1124-382 11 24 18.8 -38 12 05 11 24 18.38 -38 12 13.8 V 2 G -0.1 -0.1 22.0   22.1     0.26 0.26 0.25
PKS B1127-145 11 27 35.7 -14 32 54 11 27 35.67 -14 32 54.3 P 1b Q -1.3 -0.1 16.9     1.184 31 5.97 5.46 0.25
                                   
PKS B1128-047 11 28 57.5 -04 43 46 11 28 57.50 -04 43 45.8 P 1b G -0.3 -0.6 20.0     0.266 20 0.74 0.90 0.25
PKS B1131-088 11 31 03.0 -08 48 52 11 31 03.51 -08 48 48.3 P 2 Q* 1.0 0.5 21.5   21.7     0.35 0.31 0.25
PKS B1131-115 11 31 25.4 -11 34 52       1a NCS               0.27 0.25 0.25 X
PKS B1133-032 11 33 51.3 -03 13 51 11 33 51.25 -03 13 53.1 P 1b Q -0.1 -0.5 19.5     1.648 83 0.26 0.39 0.25
PKS B1133-172 11 33 31.6 -17 16 36 11 33 31.60 -17 16 36.4 P 2 Q -0.1 -0.5 22.4     1.024 20 0.65 0.52 0.25
PKS B1133-739 11 34 01.4 -73 59 09 11 34 01.43 -73 59 08.7 W 2 Q* 0.4 0.1 21.6         0.80 0.63 0.25
PKS B1136-135 11 36 38.6 -13 34 09 11 36 38.52 -13 34 05.9 P 1b Q -0.5 -0.4 16.0     0.557 31 2.76 2.22 0.25
PKS B1136-156 11 36 57.7 -15 36 22 11 36 57.61 -15 36 13.8 P 1b Q -0.2 -1.0 20.0     2.625 83 0.34 0.51 0.25
PKS B1141+011 11 41 34.8 +01 11 18 11 41 34.79 +01 11 14.9 N 1a G     19.4         0.34 0.27 0.25
PKS B1142-225 11 42 50.2 -22 33 52 11 42 50.23 -22 33 51.3 P 3 Q 0.2 0.5 22.3   22.1 1.141 20 0.54 0.63 0.25


 
Table A.1: continued.
  PKSCAT90 B1950 New radio position B1950       Offsets                
Name RA Dec RA Dec   Ident RA Dec B Gunn-i Gunn-z z zRef S2.7 S5 $S_{\rm lim}$
PKS B1143-245 11 43 36.4 -24 30 53 11 43 36.37 -24 30 52.7 P 1b Q -0.3 -0.2 18.0     1.940 20 1.32 1.18 0.25
PKS B1143-287 11 43 54.8 -28 42 39 11 43 54.81 -28 42 38.2 P 1b Q 1.0 -0.6 20.0     0.45 10 0.43 0.60 0.25
PKS B1144-379 11 44 30.9 -37 55 31 11 44 30.83 -37 55 31.0 N 1a BL     18.0     1.048 1 1.03 0.90 0.25
PKS B1145-071 11 45 18.3 -07 08 01 11 45 18.30 -07 08 00.5 P 1b Q 0.6 -1.5 18.5     1.342 31 1.09 1.21 0.25
PKS B1146-037 11 46 22.4 -03 47 30 11 46 22.38 -03 47 28.7 P 1b Q -0.5 -1.0 16.4     0.340 15 0.42 0.34 0.25
PKS B1147-192 11 47 59.3 -19 14 29 11 47 58.88 -19 14 08.2 P 2 Q -0.3 0.0 19.4   22.4 2.489 83 0.28 0.27 0.25
PKS B1148-001 11 48 10.1 -00 07 13 11 48 10.13 -00 07 13.0 P 1b Q -0.2 -0.4 17.6     1.978 49 2.40 1.90 0.25
PKS B1148-171 11 48 30.4 -17 07 19 11 48 30.38 -17 07 18.4 P 1b Q -0.3 -0.5 19.0     1.751 33 0.60 0.50 0.25
PKS B1149-084 11 49 43.5 -08 24 23 11 49 43.83 -08 24 22.5 N 1b Q     18.5     2.370 83 0.39 0.56 0.25
PKS B1149-480 11 49 07.5 -48 05 28 11 49 07.23 -48 05 24.0 T 3 G? 3.0 -0.2 23.8         0.25 0.24 0.25
                                   
PKS B1150-723 11 50 30.7 -72 22 43       1a e     19.0         0.82 0.65 0.25
PKS B1156-094 11 56 39.1 -09 24 10 11 56 39.06 -09 24 09.8 P 2 Q* -0.5 -0.1 22.0         0.75 0.66 0.25
PKS B1156-221 11 56 37.8 -22 11 55 11 56 37.76 -22 11 54.5 P 1b Q -0.2 -0.4 20.0     0.565 33 0.71 0.78 0.25
PKS B1157-215 11 57 18.3 -21 32 12 11 57 18.32 -21 32 11.3 P 1b Q -0.4 -0.3 18.5     0.927 30 0.49 0.66 0.25
PKS B1159-515 11 59 09.2 -51 33 53 11 59 09.36 -51 33 51.9 C 1a Q     20.3         0.33 0.54 0.25
PKS B1200-051 12 00 00.4 -05 11 20 12 00 00.43 -05 11 20.2 P 1b Q -0.1 -0.4 18.0     0.381 33 0.50 0.46 0.25
PKS B1203+011 12 03 14.8 +01 10 24 12 03 14.82 +01 10 25.7 N 1a Q     18.0     0.933 7 0.13 0.14 0.10
PKS B1205+011 12 05 59.8 +01 11 05 12 05 59.94 +01 11 03.6 P 3 G 0.4 0.3 >22.5   21.8     0.25 0.25 0.10
PKS B1205-008 12 05 07.8 -00 49 55 12 05 07.89 -00 49 54.8 P 1b Q -0.4 -0.5 18.5     1.002 15 0.22 0.20 0.10
PKS B1206-202 12 06 39.5 -20 16 09 12 06 39.99 -20 15 57.2 P 3 G 1.7 0.2 22.1 19.0 20.3 0.404 83 0.38 0.65 0.25
                                   
PKS B1206-238 12 06 27.7 -23 49 39 12 06 27.68 -23 49 38.9 P 1b Q 0.1 -0.2 18.0     1.299 83 0.49 0.71 0.25
PKS B1206-399 12 06 59.4 -39 59 30       1a Q     16.1     0.966 5 0.59 0.53 0.25
PKS B1207-319 12 07 04.8 -31 58 03 12 07 04.79 -31 58 11.5 V 3 Q* 1.0 2.3 24.1   23.7     0.32 0.28 0.20
PKS B1209-191 12 09 22.0 -19 09 32 12 09 22.89 -19 09 26.4 P 3 G 1.0 0.1 23.6   21.7     0.21 0.36 0.25 X
PKS B1210-097 12 10 49.1 -09 46 48 12 10 48.56 -09 46 44.3 P 3 BL -1.1 0.8 21.5   21.7   83 0.27 0.28 0.25
PKS B1213-102 12 13 51.0 -10 16 48 12 13 49.83 -10 16 35.4 P 3 Q -0.7 0.0 21.8   21.6 0.636 83 0.29 0.31 0.25
PKS B1213-172 12 13 11.7 -17 15 05 12 13 11.76 -17 15 6.0 N 1a Ob               1.33 1.28 0.25
PKS B1215-002 12 15 24.8 -00 13 08 12 15 24.94 -00 13 06.7 P 1b G -0.4 0.2 18.5     0.417 4 0.33 0.28 0.10
PKS B1216-010 12 16 01.1 -01 03 14 12 16 01.07 -01 03 14.9 P 1b Q -0.2 -0.1 17.7     0.415 50 0.15 0.16 0.10
PKS B1217+023 12 17 38.3 +02 20 21 12 17 38.77 +02 20 20.5 N 1a Q     16.5     0.240 51 0.51 0.44 0.10
                                   
PKS B1218-136 12 18 56.0 -13 37 29 12 18 55.90 -13 37 23.2 P 1b G 0.6 -1.3 17.0         0.18 0.16 0.25 X
PKS B1224-443 12 24 45.3 -44 20 10 12 24 45.57 -44 19 56.9 T 2 BL 1.4 1.0 21.5 20.5 22.1   83 0.32 0.36 0.25
PKS B1226+023 12 26 33.2 +02 19 43 12 26 32.96 +02 19 40.0 N 1a Q     12.8     0.158 52 40.90 36.70 0.25
PKS B1226-028 12 26 02.5 -02 48 06 12 26 02.75 -02 48 04.1 P 1b Q 0.2 -0.4 19.0         0.18 0.16 0.25 X
PKS B1226-062 12 26 18.0 -06 15 02 12 26 17.54 -06 15 11.2 N 1a Ob               0.24 0.22 0.25 X
PKS B1228-113 12 28 20.1 -11 22 36 12 28 20.04 -11 22 35.8 P 2 Q -0.5 -0.8 22.0     3.528 20 0.55 0.46 0.25
PKS B1228-310 12 28 05.7 -31 04 39 12 28 06.03 -31 04 49.8 N 1a Q     19.0     2.276 9 0.29 0.27 0.20
PKS B1229-439 12 29 59.6 -43 54 55 12 30 00.39 -43 55 00.6 A 3 G 0.4 -0.3 24.0   21.1     0.27 0.23 0.25
PKS B1230-101 12 30 37.4 -10 08 53 12 30 37.72 -10 08 45.8 P 2 Q -0.2 -0.7 19.8     2.394 83 0.43 0.34 0.25
PKS B1237-101 12 37 07.3 -10 07 01 12 37 07.28 -10 07 00.4 P 1b Q -0.5 -0.5 18.0     0.753 2 1.35 1.13 0.25


 
Table A.1: continued.
  PKSCAT90 B1950 New radio position B1950       Offsets                
Name RA Dec RA Dec   Ident RA Dec B Gunn-i Gunn-z z zRef S2.7 S5 $S_{\rm lim}$
PKS B1240-059 12 40 58.4 -05 57 02 12 40 59.61 -05 56 56.9 V 3 G -0.1 -0.7 14.4 17.0 18.3 0.139 83 0.20 0.16 0.25 X
PKS B1240-394 12 40 50.1 -39 25 33 12 40 50.29 -39 25 27.0 S 2 Q -0.2 -0.6 21.0     1.387 83 0.26 0.26 0.25
PKS B1241-399 12 41 45.0 -39 56 21 12 41 45.07 -39 56 21.6 S 2 Q -2.4 -1.3 17.2     0.191 83 0.26 0.21 0.25
PKS B1243-072 12 43 28.8 -07 14 23 12 43 28.79 -07 14 23.3 P 1b Q -0.3 -0.8 18.0     1.286 10 0.79 1.11 0.25
PKS B1243-160 12 43 16.1 -16 00 18 12 43 16.24 -16 00 22.3 P 2 G? 0.6 -0.6 22.5         0.30 0.36 0.25
PKS B1244-255 12 44 06.7 -25 31 27 12 44 06.72 -25 31 26.5 P 1b Q 0.3 -1.2 17.0     0.633 30 1.34 1.55 0.25
PKS B1245-062 12 45 47.4 -06 15 25 12 45 47.69 -06 15 48.6 P 2 Q 0.1 -0.8 19.5   21.3 0.762 83 0.41 0.33 0.25
PKS B1248-350 12 48 55.5 -35 02 13 12 48 55.06 -35 02 21.9 S 2 Q 1.9 0.4 21.2     0.410 83 0.37 0.32 0.25
PKS B1250-330 12 50 14.9 -33 03 42 12 50 14.90 -33 03 42.0 N 1c Q -1.0 -1.2 21.4     0.859 83 0.52 0.49 0.20
PKS B1251-407 12 51 12.8 -40 43 11 12 51 12.62 -40 43 14.7 V 3 Q -0.5 0.1 23.7 19.3 22.9 4.464 83 0.25 0.22 0.25
                                   
PKS B1252-441 12 52 09.2 -44 08 39       1a G     15.5         0.32 0.35 0.25
PKS B1253-055 12 53 35.8 -05 31 08 12 53 35.84 -05 31 07.8 P 1b Q -0.5 -0.9 17.8     0.536 53 12.00 13.00 0.25
PKS B1254+006 12 54 30.8 +00 40 46 12 54 29.74 +00 40 50.8 N 1a Q     18.0     1.257 9 0.13 0.13 0.25 X
PKS B1255-316 12 55 15.2 -31 39 05 12 55 15.20 -31 39 03.5 N 1a Q     18.5     1.924 6 1.49 1.68 0.20
PKS B1256-015 12 56 32.3 -01 34 46 12 56 32.35 -01 34 47.8 P 3 G -0.9 -0.2 :22.5   23.4     0.25 0.20 0.25
PKS B1256-177 12 56 00.2 -17 43 42 12 55 59.21 -17 43 52.1 V 3 Q -0.7 0.2 20.2   21.3 1.956 83 0.45 0.45 0.25
PKS B1256-220 12 56 13.9 -22 03 20 12 56 13.94 -22 03 20.2 P 1b Q 0.0 -0.6 20.0     1.306 54 0.65 0.79 0.25
PKS B1256-229 12 56 27.6 -22 54 28 12 56 27.61 -22 54 27.9 P 1b Q -0.5 -0.5 18.0     1.365 20 0.50 0.54 0.25
PKS B1256-243 12 56 31.3 -24 19 55 12 56 31.27 -24 19 54.9 P 1b Q -0.4 -0.4 19.5     2.263 55 0.44 0.36 0.25
PKS B1258-321 12 58 16.2 -32 10 20 12 58 15.89 -32 10 19.3 N 1a G     13.0     0.017 56 0.92 0.79 0.20
                                   
PKS B1259-312 12 59 41.3 -31 14 45 12 59 41.13 -31 14 36.7 V 3 G -0.2 -2.7 >22.5 21.6 23.0     0.25 0.21 0.20
PKS B1300-105 13 00 37.0 -10 35 27 13 00 36.73 -10 35 11.2 P 3 BL 0.2 1.1 22.9 20.6 22.2   83 0.32 0.36 0.25
PKS B1302-034 13 02 08.7 -03 29 59 13 02 08.72 -03 29 58.4 P 1b Q -0.2 -1.1 19.4     1.250 7 0.60 0.54 0.25
PKS B1302-102 13 02 55.8 -10 17 16 13 02 55.85 -10 17 16.2 P 1b Q -0.2 -0.3 15.2     0.286 12 0.89 1.00 0.25
PKS B1302-208 13 02 18.5 -20 50 40 13 02 18.29 -20 50 38.5 P 2 Q* -1.6 -0.4 21.8         0.49 0.43 0.25
PKS B1302-285 13 02 24.2 -28 34 40 13 02 24.66 -28 34 38.3 P 2 Q* -0.7 -0.5 22.5   24.5     0.30 0.30 0.25
PKS B1306-241 13 06 01.3 -24 07 16 13 05 59.59 -24 06 59.8 N 1a G     16.0     0.014 57 0.28 0.22 0.25
PKS B1307+010 13 07 54.9 +01 00 10 13 07 54.99 +01 00 7.1 N 1a Q?     20.0         0.21 0.25 0.25 X
PKS B1313-333 13 13 20.0 -33 23 10 13 13 20.05 -33 23 09.5 P 1b Q 0.0 -0.3 19.5     1.21 58 1.00 1.32 0.20
PKS B1316-120 13 16 34.0 -12 01 42 13 16 33.51 -12 01 47.1 P 1b Q* 0.0 -0.5 18.0         0.32 0.41 0.25
                                   
PKS B1317+019 13 17 53.7 +01 56 20 13 17 53.72 +01 56 19.6 N 1a Q     19.5     1.232 20 0.59 0.59 0.25
PKS B1318-263 13 18 28.9 -26 20 29 13 18 28.91 -26 20 28.2 P 2 Q 1.2 0.0 20.4     2.027 20 0.65 0.64 0.25
PKS B1319-093 13 19 59.8 -09 22 57 13 19 59.27 -09 21 57.8 P 1b Q -0.4 -0.4 18.0     1.864 83 0.37 0.53 0.25
PKS B1320-338 13 20 28.0 -33 51 28 13 20 27.79 -33 51 33.9 N 1a Q     20.0     1.346 83 0.31 0.36 0.20
PKS B1321-105 13 21 48.4 -10 34 51 13 21 47.65 -10 33 46.6 N 1a Q     18.5     0.872 83 0.34 0.64 0.25
PKS B1324-047 13 24 19.4 -04 45 27 13 24 18.76 -04 45 25.8 P 1b Q -0.2 -0.6 19.0     1.882 83 0.30 0.28 0.25
PKS B1325-222 13 25 54.6 -22 16 00 13 25 53.86 -22 16 01.8 P 2 G -1.9 -0.8 20.6         0.25 0.21 0.25
PKS B1327-311 13 27 30.0 -31 07 31 13 27 29.97 -31 07 31.0 N 1a Q     18.5     1.326 45 0.52 0.56 0.20
PKS B1328-034 13 28 53.6 -03 25 53 13 28 53.81 -03 25 48.4 P 1b Q -0.4 -0.2 19.0     1.352 7 0.35 0.29 0.10
PKS B1328-263 13 28 25.3 -26 23 57 13 28 25.19 -26 23 43.1 P 1b Q 0.3 -0.4 17.4     0.883 22 0.34 0.37 0.25


 
Table A.1: continued.
  PKSCAT90 B1950 New radio position B1950       Offsets                
Name RA Dec RA Dec   Ident RA Dec B Gunn-i Gunn-z z zRef S2.7 S5 $S_{\rm lim}$
PKS B1329-137 13 29 50.7 -13 46 47 13 29 50.75 -13 46 49.1 P 2 Q* 0.6 0.2 22.1   21.7     0.25 0.30 0.25
PKS B1330-143 13 30 44.0 -14 20 40 13 30 43.34 -14 20 59.0 N 1a BL     19.0       83 0.31 0.42 0.25
PKS B1331-115 13 31 25.5 -11 34 52 13 31 24.97 -11 34 52.9 P 2 Q -0.3 0.0 20.5   20.5 1.402 83 0.27 0.25 0.25
PKS B1333-049 13 33 21.2 -04 56 20 13 33 20.33 -04 56 23.6 P 3 BL 2.2 0.3 21.8 19.4 21.3   83 0.39 0.31 0.25
PKS B1333-082 13 33 30.5 -08 14 34 13 33 30.54 -08 14 34.1 P 1b G -0.8 -0.2 13.0     0.023 59 0.50 0.59 0.25
PKS B1334+008 13 34 58.0 +00 50 43 13 34 57.98 +00 50 43.1 N 1a G     19.0     0.299 4 0.10 0.11 0.25 X
PKS B1334-127 13 34 59.8 -12 42 10 13 34 59.81 -12 42 09.6 P 1b Q -0.6 -0.9 18.5     0.541 6 2.01 2.18 0.25
PKS B1335+023 13 35 07.0 +02 22 09 13 35 06.97 +02 22 12.5 N 1a Q     17.5     1.353 7 0.10 0.10 0.10
PKS B1336-000 13 36 59.7 -00 01 12 13 37 00.66 -00 01 17.4 N 1a NCS     19.0     1.808 31 0.12 0.12 0.10 X
PKS B1336-237 13 36 15.7 -23 46 01 13 36 15.75 -23 46 01.2 P 1b Q 0.0 -0.6 19.0     0.657 83 0.38 0.41 0.25
                                   
PKS B1336-260 13 36 32.5 -26 05 18 13 36 32.49 -26 05 18.2 P 1b Q 0.1 -0.2 20.5     1.51 20 0.71 0.77 0.25
PKS B1337-013 13 37 30.1 -01 22 36 13 37 30.12 -01 22 35.9 P 1b Q 0.2 0.0 19.1     1.619 7 0.35 0.37 0.10
PKS B1339-206 13 39 20.1 -20 36 28 13 39 20.21 -20 36 22.4 P 1b Q -0.1 -0.3 19.0     1.582 83 0.33 0.31 0.25
PKS B1339-287 13 39 25.6 -28 45 40 13 39 25.88 -28 45 34.7 P 1b Q 0.0 -0.6 19.5     1.442 83 0.37 0.53 0.25
PKS B1339-299 13 39 30.5 -29 55 09 13 39 28.72 -29 55 09.0 N 1a NCS               0.25 0.20 0.25 X
PKS B1346-113 13 46 51.3 -11 18 01 13 46 51.54 -11 18 01.1 P 1b Q 0.0 -0.4 17.5     0.34 60 0.42 0.58 0.25
PKS B1346-139 13 46 34.0 -13 58 48 13 46 34.64 -13 58 23.6 P 2 G 1.5 -1.1 21.0   20.0 0.253 83 0.21 0.17 0.25 X
PKS B1348+007 13 48 31.1 +00 46 06 13 48 31.04 +00 46 08.7 V 3 Q -0.9 0.3 22.7   22.9 2.084 4 0.21 0.17 0.10
PKS B1348-289 13 48 55.7 -28 57 29 13 48 55.86 -28 57 29.0 P 1b Q -0.1 -0.7 20.0     1.034 83 0.48 0.40 0.25
PKS B1349-145 13 49 10.8 -14 34 27 13 49 10.76 -14 34 27.2 N 1a Ob               1.04 0.93 0.25
                                   
PKS B1349-439 13 49 52.5 -43 57 54 13 49 52.53 -43 57 54.0 C 1a BL     :18.0         0.54 0.76 0.25
PKS B1351+021 13 51 18.8 +02 06 36 13 51 18.91 +02 06 38.1 N 1a Q     19.0     1.606 7 0.33 0.26 0.10
PKS B1351-018 13 51 32.0 -01 51 20 13 51 32.04 -01 51 19.9 P 1b Q -1.0 -0.3 20.9     3.709 4 1.00 0.82 0.10
PKS B1351-237 13 51 44.5 -23 43 27 13 51 42.68 -23 43 06.0 P 3 G 0.0 -0.6 21.5   21.7     0.27 0.22 0.25
PKS B1352-104 13 52 06.8 -10 26 21 13 52 06.83 -10 26 20.6 P 1b Q -0.9 -0.3 17.5     0.332 12 0.79 0.98 0.25
PKS B1353-341 13 53 09.8 -34 06 31 13 53 09.84 -34 06 30.6 N 1a G     18.5     0.223 9 0.64 0.67 0.20
PKS B1354-107 13 54 07.3 -10 47 05 13 54 06.85 -10 46 51.4 P 3 Q 1.0 0.2 19.2   19.9 3.006 83 0.26 0.27 0.25
PKS B1356+022 13 56 54.7 +02 14 26 13 56 54.60 +02 14 26.4 P 1b Q -0.2 0.0 18.3     1.329 7 0.75 0.68 0.25
PKS B1358-090 13 58 26.6 -09 02 08 13 58 26.19 -09 02 03.0 P 2 Q -0.1 0.4 19.8   20.0 0.667 83 0.41 0.33 0.25
PKS B1358-298 13 58 41.3 -29 50 05 13 58 41.90 -29 50 09.0 P 2 Q -0.2 0.3 19.7 18.7 20.6 0.689 83 0.32 0.28 0.25
                                   
PKS B1359-281 13 59 10.7 -28 08 00 13 59 10.60 -28 07 58.3 P 2 Q -1.7 1.2 20.9   21.3 0.803 20 0.82 0.67 0.25
PKS B1401+000 14 01 38.2 +00 00 55 14 01 38.29 +00 00 56.3 P 1b Q -0.1 -0.4 19.0     1.221   0.42 0.47 0.25
PKS B1402-012 14 02 11.3 -01 16 02 14 02 11.30 -01 16 01.6 P 1b Q -0.2 -0.7 18.2     2.518 7 0.73 0.60 0.25
PKS B1402-144 14 02 51.1 -14 25 49 14 02 50.15 -14 25 59.5 P 1b Q* -0.7 -0.3 17.5         0.19 0.20 0.25 X
PKS B1403-085 14 03 21.7 -08 33 50 14 03 21.65 -08 33 49.3 P 1b Q -0.4 -0.4 18.5     1.763 33 0.71 0.58 0.25
PKS B1404-267 14 04 37.9 -26 46 52 14 04 38.28 -26 46 49.7 P 1b G -1.6 2.5 13.5     0.022 62 0.50 0.40 0.25
PKS B1404-342 14 04 57.1 -34 17 15 14 04 57.20 -34 17 14.2 S 2 Q -0.4 -1.1 17.7     1.122 9 0.67 0.60 0.20
PKS B1405-287 14 05 56.3 -28 46 08 14 05 56.39 -28 46 12.0 P 1b Q 0.2 -0.2 18.5     0.575 33 0.34 0.29 0.25
PKS B1406-076 14 06 17.9 -07 38 16 14 06 17.90 -07 38 15.8 P 1b Q -0.2 -0.2 20.0     1.494 45 0.96 1.05 0.25
PKS B1406-230 14 06 23.0 -23 01 37 14 06 23.09 -23 01 39.1 P 1b G     17.5         0.44 0.35 0.25


 
Table A.1: continued.
  PKSCAT90 B1950 New radio position B1950       Offsets                
Name RA Dec RA Dec   Ident RA Dec B Gunn-i Gunn-z z zRef S2.7 S5 $S_{\rm lim}$
PKS B1406-267 14 06 58.4 -26 43 28 14 06 58.43 -26 43 27.7 P 1b Q     21.8     2.43 20 0.57 0.90 0.25
PKS B1407+022 14 07 32.2 +02 17 16 14 07 32.24 +02 17 14.9 P 1b BL -0.4 -0.8 18.7         0.39 0.35 0.25
PKS B1412-096 14 12 39.1 -09 41 53 14 12 40.68 -09 42 02.5 P 1b Q -0.8 -0.4 17.5     2.001 83 0.33 0.35 0.25
PKS B1412-368 14 12 24.8 -36 51 49 14 12 25.12 -36 51 49.5 A 3 G -0.5 0.5 >22.5   23.8     0.39 0.56 0.25
PKS B1413-168 14 13 50.5 -16 51 25 14 13 49.25 -16 51 53.1 N 2 Q? 1.7 -0.2 20.0         0.26 0.22 0.25
PKS B1415-349 14 15 58.8 -34 55 56 14 15 58.71 -34 55 54.4 N 1a Q     19.5     1.544 83 0.43 0.49 0.25
PKS B1418-064 14 18 29.1 -06 29 56 14 18 29.55 -06 30 14.8 P 1b Q -0.1 0.1 18.5     3.689 83 0.38 0.34 0.25
PKS B1422-250 14 22 29.3 -25 00 13 14 22 30.87 -24 59 35.9 P 2 Q 0.2 -0.2 19.6 18.5 20.5 1.884 83 0.31 0.25 0.25
PKS B1424-418 14 24 46.7 -41 52 54 14 24 46.72 -41 52 54.4 C 1a Q     18.0     1.522 9 2.63 2.12 0.25
PKS B1427-448 14 27 53.0 -44 48 02 14 27 46.33 -44 47 44.5 A 2 BL -1.3 0.0 19.9   20.7   83 0.43 0.34 0.25
                                   
PKS B1427-742 14 27 22.5 -74 14 25       1a G     15.5         0.37 0.34 0.25
PKS B1430-155 14 30 36.1 -15 35 35 14 30 36.12 -15 35 34.7 P 3 Q -0.5 0.3 22.8 21.6 22.8 1.583 83 0.55 0.66 0.25
PKS B1430-178 14 30 10.7 -17 48 24 14 30 10.65 -17 48 24.2 P 1b Q -0.6 -0.4 19.0     2.331 33 1.00 0.93 0.25
PKS B1434-325 14 34 14.0 -32 31 44 14 34 13.85 -32 31 40.8 V 1a NCS -1.5 -3.7   23.5       0.22 0.20 0.20 X
PKS B1435-218 14 35 18.7 -21 51 58 14 35 18.66 -21 51 57.7 P 1b Q 0.1 0.2 17.9     1.194 30 0.79 0.81 0.25
PKS B1435-311 14 35 11.4 -31 09 29 14 35 11.35 -31 09 30.3 N 1a Q     20.0     1.287 58 0.30 0.25 0.20
PKS B1437-153 14 37 11.2 -15 18 59 14 37 11.34 -15 18 58.7 P 1b BL -0.3 -0.4 19.0       82 0.72 0.64 0.25
PKS B1438-328 14 38 19.3 -32 50 39 14 38 18.17 -32 50 37.9 S 3 Q 1.5 1.0 19.5   19.6 1.479 83 0.30 0.29 0.20
PKS B1438-347 14 38 20.3 -34 43 57 14 38 20.39 -34 43 56.9 N 1a Q     18.0     1.159 58 0.50 0.45 0.20
PKS B1440-389 14 40 45.7 -38 55 33 14 40 48.15 -38 55 58.2 T 2 G -1.2 +1.0 17.0         0.20 0.19 0.25 X
                                   
PKS B1443-032 14 43 06.1 -03 17 21 14 43 06.08 -03 17 23.8 P 2 Q* -0.2 0.1 20.8         0.21 0.18 0.25 X
PKS B1446-005 14 46 42.3 -00 32 36 14 46 42.31 -00 32 54.4 P 2 G? 0.1 -0.4 22.7   22.7     0.40 0.40 0.25
PKS B1449-012 14 49 12.6 -01 15 18 14 49 12.57 -01 15 17.8 P 1b Q -0.2 -0.2 18.0     1.319 7 0.46 0.42 0.25
PKS B1451-248 14 51 51.5 -24 52 59 14 51 51.56 -24 53 03.3 P 2 Q -0.9 -2.4 21.7     1.216 83 0.33 0.32 0.25
PKS B1451-375 14 51 18.3 -37 35 22 14 51 18.47 -37 35 24.2 N 1a Q     16.4     0.321 12 1.51 1.84 0.25
PKS B1451-400 14 51 20.6 -40 00 22 14 51 20.58 -40 00 21.1 C 1c Q 0.3 -1.2 18.5     :1.81   0.71 0.61 0.25
PKS B1452-168 14 52 15.3 -16 48 01 14 52 15.08 -16 48 05.8 P 2 Q* -2.2 -0.5 21.1   21.7     0.31 0.28 0.25
PKS B1452-367 14 52 01.1 -36 43 47 14 52 01.60 -36 42 59.5 V 3 G 0.4 0.6 17.2