Table 1: Radio emission data of the sources in the three epochs of the observations (a = 22 Aug. 1998; b = 10 Sep. 1998; c = 21 Sep. 1998). Column [1], IAU name; Col. [2] optical id.; Col. [3] redshift (values in parentheses are photometric redshifts, using the GPS galaxy Hubble diagram); Cols. [4]-[7] flux density of the arc second core and any additional radio emission at 1.36 and 1.66 GHz (values in parentheses indicate that in our judgment, the radio emission likely comes from an unrelated object). Flux density errors for compact strong components are dominated by the calibration uncertainties estimated around 3$\%$, while for extended weak components the flux density errors are dominated by the limits of the self-cal/imaging process in the presence of a strong source nearby, and the flux densities given can be considered only rough estimates. *  It accounts for the region South of the arcsecond core only.
  1.36 GHz 1.66 GHz
Name id z Peak Extended Peak Extended
      mJy mJy mJy mJy
B0019-000a G 0.305 2932 - 2652 -
B0108+388ac G 0.669 414 9.3 595 6.0
B0237-233a Q 2.223 6282 (62.0) 5950 (51.5)
B0248+430a Q 1.310 1197 (26.2) 1281 (25.1)
B0316+162a G (1.57) 7820 (25.0) 7167 (21.9)
B0428+205a G 0.219 3720 - 3665 -
B0457+024a Q 2.384 2242 - 2417 -
B0457+024c Q 2.384 2248 - 2232 -
B0500+019a G 0.583 2144 (42.1) 2341 (30.5)
B0710+439a G 0.518 1953 -    
B0738+313a Q 0.631 2036 86 2461 57
B0742+103a Q 2.624 3308 - 3795 -
B0743-006a Q 0.994 690 (25.2) 841 (17.9)
B0941-080ab G 0.228 2725 31.1 2401 24.4
B1031+567a G 0.460 1791 - 1741 -
B1117+146a G 0.362 2445 - 2153 -
B1127-145b Q 1.187 5448 96.2 5371 75.4
B1143-245b Q 1.940 1557 - 1676 -
B1245-197b Q 1.273 5322 (54.6) 4708 (45.4)
B1323+321a G 0.369 4855 - 4339 -
B1345+125ac G 0.122 5262 35.4 4734 32.1
B1358+624c G 0.431 4357 - 3860 -
B1404+286a G 0.077 792 (7.3) 1070 (5.8)
B1442+101a Q 3.522 2432 - 2220 -
B1518+047a Q 1.296 3963 (243) 3457 (211)
B1600+335a G (1.10) 2914 - 2834 -
B1607+268a G 0.473 4875 - 4387 -
B2008-068a G (0.70) 2576 (55.4) 2523 (58.3)
B2126-158a Q 3.270 562 - 684 -
B2128+048a G 0.990 3970 (19.2) 3747 (18.5)
B2134+004a Q 1.932 3412 11.0* 4608 7.1*
B2210+016a G (0.68) 2823 - 2522 -
B2342+821a Q 0.735 3797 - 3286 -
B2352+495a G 0.237 2532 - 2390 -


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