# VLA Survey results: see http://www.astro.cornell.edu/~shami/psrvlb/vla-x/ # # Name RA (J2000) Dec (J2000) s8400 RMS Major Minor PA R1 R2 # R1, R2 are ratios of minor:major axes, for asec and pixel values. Should match. # # B1508+55.006.ICL001 1 B1508+55.006 15:11:48.06081 55:41:56.2881 24.451 0.212 49.6 x 36.7 @ 109.4 0.740 0.741 # B1541+09.008.ICL001 1 B1541+09.008 15:43:03.70177 09:19:09.7850 21.106 0.476 154.2 x 0.0 @ 63.0 0.000 0.000 # B1541+09.003.ICL001 B1541+09.003 15:43:45.46228 09:15:32.8892 2.306 0.106 280.9 x 184.6 @ 60.6 0.658 0.657 # B1541+09.005.ICL001 B1541+09.005 15:44:51.88232 09:21:42.1646 2.013 0.106 298.2 x 0.0 @ 40.6 0.000 0.000 # B1604-00.003.ICL001 Component 1-Gaussian B1604-00.003 16:07:48.45193 -00:30:25.3863 5.692 0.103 228.3 x 157.2 @ 100.5 0.691 0.689 # B1604-00.004.ICL001 s double ! B1604-00.004 16:08:17.03515 -00:32:15.5460 4.894 0.119 242.0 x 198.1 @ 125.9 0.821 0.819 # B1604-00.011.ICL001 B1604-00.011 16:06:35.55558 -00:32:38.1375 1.441 0.078 160.4 x 91.9 @ 108.1 0.575 0.573 # B1604-00.009.ICL001 B1604-00.009 16:07:39.02613 -00:18:53.2833 1.740 0.106 361.0 x 223.9 @ 160.5 0.621 0.620 # J1643-12.007.ICL001 J1643-12.007 16:43:19.43851 -12:20:15.6982 13.629 0.145 92.6 x 65.3 @ 134.6 0.707 0.705 # B1702-19.002.ICL001 B1702-19.002 17:06:07.40406 -19:00:57.0999 3.315 0.112 52.8 x 0.0 @ 2.3 0.000 0.000 # B1702-19.007.ICL001 B1702-19.007 17:05:45.70871 -19:04:40.4153 4.253 0.121 65.1 x 25.0 @ 140.8 0.383 0.384 # B1702-19.008.ICL001 Component 1-Gaussian B1702-19.008 17:06:02.99436 -19:05:52.0309 0.504 0.086 345.6 x 0.0 @ 114.4 0.000 0.000 # B1702-19.012.ICL001 B1702-19.012 17:04:29.16685 -19:03:35.9717 13.664 0.195 128.2 x 100.5 @ 155.0 0.787 0.783 # B1702-19.003.ICL001 B1702-19.003 17:06:56.48512 -19:09:23.5042 4.472 0.108 281.2 x 113.3 @ 135.6 0.405 0.403 # B1702-19.013.ICL001 B1702-19.013 17:04:41.58686 -18:58:07.3296 27.819 0.282 54.4 x 0.0 @ 127.2 0.000 0.000 # B1706-16.013.ICL001 B1706-16.013 17:09:40.55787 -16:37:35.3791 2.219 0.096 150.5 x 31.2 @ 107.6 0.207 0.207 # J1744-11.015.ICL001 J1744-11.015 17:43:25.18143 -11:17:56.0332 9.644 0.155 79.7 x 0.0 @ 4.2 0.000 0.000 # J1713+07.002.ICL001 J1713+07.002 17:14:08.78695 08:07:24.0619 1.757 0.119 150.9 x 98.5 @ 140.7 0.651 0.653 # J1713+07.005.ICL001 big blob: Component 1-Gaussian J1713+07.005 17:14:58.82457 07:49:57.9958 1.819 0.101 555.3 x 220.5 @ 91.4 0.398 0.397 # J1713+07.008.ICL001 J1713+07.008 17:13:27.09525 07:30:18.9914 12.587 0.234 91.3 x 79.3 @ 35.5 0.868 0.869 # B1800-21.002.ICL001 blob B1800-21.002 18:04:38.02058 -21:47:07.5711 7.688 0.212 418.2 x 108.0 @ 96.0 0.258 0.258 # B1800-21.003.ICL001 about 6 arc sec to the SW of the field center B1800-21.003 18:04:20.40030 -21:31:58.6359 3.269 0.171 164.8 x 0.0 @ 129.4 0.000 0.000 # B1800-21.006.ICL001 B1800-21.006 18:03:38.65393 -21:22:37.3251 4.975 0.199 109.5 x 0.0 @ 140.7 0.000 0.000 # B1821-19.014.ICL001 blob B1821-19.014 18:23:46.63942 -19:46:23.8744 0.753 0.102 861.3 x 501.1 @ 5.1 0.581 0.582 # B1821-19.011.ICL001 B1821-19.011 18:24:22.00872 -19:52:34.8553 6.290 0.190 179.4 x 109.5 @ 159.5 0.612 0.610 # B1821-19.016.ICL001 B1821-19.016 18:22:58.41079 -19:30:02.1575 8.781 0.170 76.8 x 45.8 @ 105.8 0.594 0.596 # B1821-19.007.ICL001 B1821-19.007 18:24:29.58179 -19:36:44.6407 2.191 0.121 0.0 x 0.0 @ 0.0 -1.000 -1.000 # B1826-17.009.ICL001 weak B1826-17.009 18:29:57.80795 -17:46:45.0481 0.726 0.112 244.5 x 0.0 @ 109.8 0.000 0.000 # B1826-17.012.ICL001 weak blob B1826-17.012 18:29:03.25132 -17:59:42.7308 0.528 0.085 640.2 x 407.7 @ 166.2 0.637 0.637 # J1835-11.004.ICL001 note the source is about 5 arc sec to SW of the field center J1835-11.004 18:35:19.57549 -11:15:59.3054 64.045 0.428 49.6 x 26.8 @ 56.6 0.532 0.540 # J1835-11.012.ICL001 J1835-11.012 18:35:25.24992 -11:08:37.0745 3.427 0.116 131.3 x 72.7 @ 132.0 0.555 0.553 # J1835-11.013.ICL001 blob J1835-11.013 18:35:08.40524 -11:11:42.6014 0.755 0.088 370.8 x 254.3 @ 114.1 0.685 0.686 # J1835-11.002.ICL001 big blob J1835-11.002 18:36:21.42227 -11:11:01.3542 0.958 0.112 700.9 x 509.9 @ 80.4 0.727 0.727 # J1835-11.007.ICL001 J1835-11.007 18:36:07.27025 -11:07:45.9080 1.950 0.101 107.1 x 10.7 @ 91.3 0.097 0.100 # J1835-11.009.ICL001 .small double !!!!! seperation is 0.6 or so arc sec J1835-11.009 18:35:55.94897 -11:27:44.1615 2.394 0.105 391.6 x 155.7 @ 132.9 0.398 0.397 # J1835-11.015.ICL001 blob J1835-11.015 18:35:07.84916 -10:55:22.2986 1.098 0.098 400.3 x 157.5 @ 28.5 0.394 0.393 # B1822-09.010.ICL001 blob B1822-09.010 18:24:21.71225 -09:44:33.9812 5.458 0.136 534.8 x 272.5 @ 145.8 0.510 0.510 # B1822-09.005.ICL001 blob B1822-09.005 18:24:50.99719 -09:31:43.3182 0.336 0.093 1139.3 x 548.0 @ 94.4 0.481 0.481 # B1822-09.008.ICL001 looks good B1822-09.008 18:24:32.56547 -09:50:17.6806 34.284 0.348 108.8 x 36.3 @ 164.6 0.331 0.334 # B1822-09.012.ICL001 blob B1822-09.012 18:24:50.99857 -09:31:43.1773 0.584 0.088 619.5 x 342.2 @ 31.1 0.553 0.552 # B1829-08.004.ICL001 one arc sec double, the stronger part of the double B1829-08.004 18:32:32.29644 -08:38:53.5006 11.301 0.174 152.8 x 71.9 @ 149.0 0.471 0.471 # B1829-08.005.ICL001 B1829-08.005 18:32:27.48135 -08:37:18.2364 4.253 0.172 83.4 x 42.3 @ 159.2 0.510 0.507 # B1829-08.007.ICL001 B1829-08.007 18:32:43.76443 -08:30:35.8186 1.284 0.101 259.8 x 183.4 @ 131.1 0.705 0.706 # B1804-08.008.ICL001 1 blob B1804-08.008 18:07:33.71138 -08:50:52.2594 1.098 0.094 567.9 x 239.0 @ 118.4 0.421 0.421 # B1804-08.010.ICL001 blob B1804-08.010 18:07:15.24568 -08:44:59.7122 1.096 0.103 532.7 x 355.0 @ 142.4 0.667 0.666 # B1804-08.003.ICL001 may be 1 arc sec double . this is the stronger component B1804-08.003 18:08:17.68293 -08:52:38.9163 6.275 0.117 121.6 x 45.0 @ 121.0 0.368 0.370 # B1804-08.009.ICL001 B1804-08.009 18:07:34.86720 -08:48:43.3296 1.565 0.107 0.0 x 0.0 @ 0.0 -1.000 -1.000 # B1804-08.002.ICL001 two arc sec e-west double this is the stronger west part B1804-08.002 18:08:13.47497 -09:04:18.8652 3.516 0.127 337.0 x 220.0 @ 163.8 0.653 0.653 # B1804-08.005.ICL001 B1804-08.005 18:07:26.04782 -09:05:47.1842 9.952 0.138 81.6 x 60.4 @ 8.1 0.745 0.740 # B1804-08.011.ICL001 blob B1804-08.011 18:07:57.93373 -08:32:23.7882 2.066 0.119 448.1 x 335.5 @ 166.4 0.748 0.749 # B1804-08.014.ICL001 B1804-08.014 18:06:54.45908 -08:41:08.3209 0.973 0.082 285.6 x 87.5 @ 9.3 0.305 0.307 # B1818-04.005.ICL001 B1818-04.005 18:21:03.91950 -04:26:33.7892 3.382 0.096 30.4 x 0.0 @ 6.1 0.000 0.000 # B1818-04.006.ICL001 great looking source !!!!!! B1818-04.006 18:20:43.39625 -04:24:12.4186 75.350 0.620 57.4 x 44.3 @ 44.8 0.764 0.772 # B1818-04.009.ICL001 strong blob B1818-04.009 18:20:14.10508 -04:25:42.1584 44.817 0.591 365.4 x 222.1 @ 21.4 0.608 0.608 # B1831-04.003.ICL001 blob B1831-04.003 18:35:10.84712 -04:22:14.4379 10.407 0.134 290.5 x 72.8 @ 121.9 0.251 0.250 # B1831-04.004.ICL001 blob B1831-04.004 18:34:11.11571 -04:22:43.6887 1.071 0.075 211.3 x 144.8 @ 177.5 0.686 0.685 # B1831-04.006.ICL001 weak B1831-04.006 18:34:31.02857 -04:15:37.1818 0.584 0.096 110.2 x 0.0 @ 78.6 0.000 0.000 # B1839-04.007.ICL001 great source ! compact and strong B1839-04.007 18:41:27.31409 -03:48:44.3396 106.640 0.927 62.9 x 16.4 @ 10.0 0.266 0.261 # B1839-04.007.ICL001 self cal B1839-04.007 18:41:27.31380 -03:48:44.3345 118.520 0.167 0.9 x 0.0 @ 174.5 0.000 0.000 # B1844-04.008.ICL001 B1844-04.008 18:47:25.32509 -04:05:39.6409 1.780 0.100 0.0 x 0.0 @ 0.0 -1.000 -1.000 # B1844-04.012.ICL001 blob B1844-04.012 18:47:32.21305 -03:53:24.4760 0.752 0.102 322.8 x 142.0 @ 118.1 0.438 0.440 # B1844-04.013.ICL001 blob B1844-04.013 18:47:45.34986 -03:40:50.7641 3.620 0.110 355.5 x 268.2 @ 35.6 0.755 0.754 # B1844-04.017.ICL001 little one arc sec double this is the north east portion B1844-04.017 18:46:26.90112 -04:08:52.2038 3.727 0.117 185.5 x 125.8 @ 156.4 0.677 0.678 # B1845-01.008.ICL001 this is a 2 arc sec shell ! B1845-01.008 18:48:45.04126 -01:33:10.4054 11.454 0.410 2328.1 x 2141.0 @ 80.2 0.920 0.920 # B1845-01.003.ICL001 can be self caled ? B1845-01.003 18:48:51.74014 -01:40:18.0055 13.633 0.170 32.8 x 15.0 @ 41.5 0.463 0.457 # B1845-01.004A.ICL001 8 arcsec double: near field center B1845-01.004A 18:48:40.64240 -01:45:19.0836 4.448 0.122 331.6 x 296.2 @ 141.2 0.894 0.893 # B1845-01.004B.ICL001 next source to the SW B1845-01.004B 18:48:40.14273 -01:45:23.2494 6.841 0.130 62.1 x 45.5 @ 45.4 0.731 0.733 # B1911-04.008.ICL001 6 arcsec double. This is central source B1911-04.008 19:12:56.11807 -04:39:47.7919 2.722 0.107 215.2 x 193.5 @ 90.2 0.900 0.899 # B1911-04.011.ICL001 blob B1911-04.011 19:13:52.02477 -04:35:31.1184 0.340 0.073 1132.6 x 773.4 @ 155.4 0.683 0.683 # B1911-04.012.ICL001 blob B1911-04.012 19:14:19.62517 -04:40:59.0111 0.985 0.096 287.1 x 204.4 @ 49.7 0.713 0.712 # B1911-04.002.ICL001 might be self calib candidate B1911-04.002 19:15:22.12603 -04:34:36.7976 11.560 0.157 133.7 x 97.4 @ 61.7 0.731 0.728 # B1911-04.005.ICL001 can be self caled B1911-04.005 19:14:11.14299 -04:58:44.4351 8.965 0.118 113.3 x 48.0 @ 94.3 0.423 0.423 # B1911-04.009.ICL001 this looks promising. could just be self caled with longer solint B1911-04.009 19:13:21.79433 -04:32:54.0034 6.257 0.120 59.0 x 15.5 @ 177.8 0.257 0.262 # B1855+09.006.ICL001 compact and can be self caled B1855+09.006 18:57:24.77860 09:23:32.3172 11.089 0.186 116.4 x 0.0 @ 46.9 0.000 0.000 # B1839+09.007.ICL001 could be self caled with longer solint. B1839+09.007 18:42:23.59912 09:27:17.8759 5.491 0.089 55.6 x 16.5 @ 21.4 0.304 0.297 # B1839+09.009.ICL001 nice and compact self cal candidate B1839+09.009 18:41:50.02850 08:57:19.6368 17.220 0.156 35.0 x 17.9 @ 79.3 0.500 0.511 # B1839+09.009.ICL001 selfcal fit.solint = 2 min B1839+09.009 18:41:50.02839 08:57:19.6400 17.925 0.123 20.7 x 8.5 @ 97.1 0.423 0.410 # B1839+56.013.ICL001 compact and could be self caled with long solint B1839+56.013 18:41:09.02609 56:38:15.2830 8.545 0.096 43.4 x 0.0 @ 37.7 0.000 0.000 # B1839+56.011.ICL001 B1839+56.011 18:40:13.52424 56:32:01.0263 0.938 0.072 140.0 x 0.0 @ 147.9 0.000 0.000 # B1905+39.017.ICL001 B1905+39.017 19:06:55.76275 39:53:27.1839 4.981 0.102 114.6 x 64.8 @ 21.5 0.566 0.565 # B1905+39.019.ICL001 great looking source B1905+39.019 19:06:11.42710 39:56:10.0581 103.280 0.531 96.6 x 43.6 @ 92.8 0.455 0.452 # B1946+35.010.ICL001 look at this source . 0.3 Jy or so and compact B1946+35.010 19:48:04.51933 35:56:20.6662 296.070 1.040 42.4 x 31.2 @ 3.6 0.736 0.736 # B1946+35.007.ICL001 this is a 0.5 arc sec double B1946+35.007 19:47:43.11283 35:41:59.4507 1.086 0.091 482.1 x 113.2 @ 42.2 0.235 0.235 # B1946+35.008.ICL001 weak ! B1946+35.008 19:48:03.10074 35:30:04.0344 0.637 0.080 57.4 x 0.0 @ 94.0 0.000 0.000 # B1937+21.003.ICL001 a complex source.this is the most compact source. the total size is 1.5 arc sec. the blob is to the N of this source. B1937+21.003 19:40:40.38688 21:40:04.1911 1.097 0.110 544.5 x 301.9 @ 29.9 0.554 0.554 # B1937+21.002.ICL001 0.6 arc sec blob B1937+21.002 19:38:42.82565 21:42:08.2517 0.603 0.091 718.1 x 578.0 @ 88.5 0.805 0.805 # B1919+21.006.ICL001 one arc sec double .n-s this is the most intense compnt and is the one to the N B1919+21.006 19:22:47.60442 21:53:44.5357 1.317 0.091 173.2 x 140.3 @ 43.9 0.810 0.810 # B1933+16.010.ICL001 B1933+16.010 19:35:55.52636 16:17:00.6849 2.763 0.107 107.2 x 52.3 @ 36.4 0.485 0.488 # B1933+16.011.ICL001 blob B1933+16.011 19:35:56.81396 16:14:09.2646 0.570 0.076 349.0 x 226.0 @ 91.0 0.647 0.647 # B1933+16.005.ICL001 extended .... B1933+16.005 19:36:55.85541 16:03:56.8765 1.753 0.084 585.8 x 142.6 @ 67.0 0.243 0.243 # B1933+16.007.ICL001 B1933+16.007 19:36:00.87528 15:56:46.3356 2.461 0.090 104.1 x 25.2 @ 39.4 0.238 0.242 # B1944+17.016.ICL001 may be a double . the weak component is to the SW displaced by about 1.5 arc sec. this source is the stronger component B1944+17.016 19:46:20.93654 18:27:32.7323 25.190 0.235 92.7 x 45.7 @ 51.8 0.491 0.493 # B1944+17.005.ICL001 B1944+17.005 19:47:43.71575 18:17:04.8439 2.033 0.079 136.7 x 0.0 @ 16.7 0.000 0.000 # B1944+17.013.ICL001 one arc sec double this is the strongest SW part . the weak compon is tot he NE B1944+17.013 19:45:45.54691 18:15:14.5061 3.878 0.112 101.8 x 29.1 @ 100.0 0.283 0.286 # B1953+50.016.ICL001 blob B1953+50.016 19:55:35.72096 51:21:29.4334 9.216 0.151 372.6 x 133.8 @ 103.5 0.358 0.359 # B1953+50.021.ICL001 one arc sec double. this is the stronger S component. B1953+50.021 19:53:58.92013 51:18:33.1225 11.262 0.178 71.2 x 65.1 @ 15.1 0.910 0.914 # B2000+40.004.ICL001 can be self caled B2000+40.004 20:03:06.77635 40:29:01.1639 26.274 0.194 30.2 x 20.1 @ 100.3 0.658 0.667 # B2000+40.015.ICL001 may be a small double B2000+40.015 20:01:55.98449 40:40:12.0299 0.962 0.092 175.1 x 139.9 @ 172.3 0.799 0.799 # B2011+38.002.ICL001 great compact source B2011+38.002 20:13:59.27404 38:28:51.9556 77.758 0.463 10.7 x 0.0 @ 29.0 0.000 0.000 # B2011+38.008.ICL001 B2011+38.008 20:13:39.98681 38:37:34.5442 4.458 0.085 70.1 x 0.0 @ 152.6 0.000 0.000 # B2011+38.020.ICL001 seems extended ? B2011+38.020 20:12:27.06420 39:03:19.5647 6.143 0.109 197.0 x 153.1 @ 2.0 0.776 0.777 # B2011+38.021.ICL001 B2011+38.021 20:12:54.33214 38:58:30.4697 2.159 0.081 90.2 x 66.0 @ 176.5 0.726 0.731 # B2045-16.010.ICL001 B2045-16.010 20:48:15.74258 -16:08:08.6186 3.406 0.106 124.4 x 45.6 @ 22.4 0.365 0.366 # B2045-16.011.ICL001 compact-= can be self caled B2045-16.011 20:48:36.69987 -16:09:45.4400 9.161 0.140 61.7 x 0.0 @ 146.0 0.000 0.000 # B2045-16.006.ICL001 blob B2045-16.006 20:48:44.09837 -16:10:41.8099 0.853 0.119 481.5 x 261.6 @ 21.9 0.543 0.543 # B2045-16.008.ICL001 nice strong source . compact- can be self caled B2045-16.008 20:48:49.57188 -16:00:13.9184 76.776 0.630 35.3 x 0.0 @ 28.1 0.000 0.000 # B2045-16.002.ICL001 blob B2045-16.002 20:49:04.01780 -16:32:50.2184 0.334 0.079 708.1 x 361.1 @ 121.0 0.510 0.510 # B2045-16.009.ICL001 B2045-16.009 20:48:08.93113 -16:01:45.2250 3.421 0.093 92.8 x 0.0 @ 0.4 0.000 0.000 # B2053+36.011.ICL001 can be self caled B2053+36.011 20:55:12.22733 36:34:22.6942 17.152 0.126 58.2 x 0.0 @ 176.2 0.000 0.000 # B2053+36.013.ICL001 B2053+36.013 20:55:32.58050 36:37:53.6322 6.176 0.117 51.9 x 12.5 @ 172.6 0.246 0.240 # B2053+36.006.ICL001 extended B2053+36.006 20:55:08.86058 36:06:15.3729 32.600 0.296 245.4 x 143.2 @ 130.7 0.583 0.584 # B2053+36.003.ICL001 6 arc sec triple. this is the NE strong component B2053+36.003 20:57:26.80839 36:27:58.5179 12.107 0.160 150.3 x 109.7 @ 59.6 0.729 0.730 # B2053+36.012.ICL001 blob B2053+36.012 20:55:25.41237 36:40:18.7231 0.594 0.082 252.7 x 151.1 @ 72.0 0.598 0.598 # B2053+36.019.ICL001 B2053+36.019 20:54:14.10850 36:40:30.8534 4.522 0.095 79.3 x 39.2 @ 51.9 0.495 0.494 # B2111+46.002.ICL001 blob B2111+46.002 21:14:22.82751 46:49:10.5968 1.502 0.104 529.1 x 373.2 @ 25.7 0.707 0.705 # B2111+46.005.ICL001 great source can be sel caled B2111+46.005 21:14:32.87520 46:34:39.2880 159.710 1.030 31.7 x 17.9 @ 132.1 0.550 0.564 # B2111+46.011.ICL001 B2111+46.011 21:13:14.25888 46:43:41.4909 2.059 0.093 67.5 x 0.0 @ 42.6 0.000 0.000 # B2111+46.018.ICL001 double size 3 arc sec. this is the stronger west component B2111+46.018 21:11:56.73140 46:37:31.2513 1.301 0.104 600.3 x 414.8 @ 75.3 0.692 0.691 # B2111+46.019.ICL001 B2111+46.019 21:11:52.13387 46:44:53.5221 3.836 0.088 64.6 x 45.3 @ 122.5 0.704 0.702 # B2106+44.009.ICL001 blob B2106+44.009 21:09:46.80817 44:36:13.6269 4.431 0.100 347.4 x 98.8 @ 16.1 0.283 0.284 # B2106+44.002.ICL001 B2106+44.002 21:08:28.85670 44:27:16.7524 0.892 0.083 136.5 x 103.2 @ 164.1 0.754 0.756 # B2106+44.003.ICL001 B2106+44.003 21:08:26.26620 44:29:42.3265 2.382 0.109 137.5 x 0.0 @ 59.8 0.000 0.000 B2106+44.003 21:07:53.04794 44:23:34.0620 1.217 0.099 950.9 x 202.4 @ 69.9 0.213 0.213 # B2106+44.005.ICL001 blob B2106+44.005 21:07:40.56722 44:28:36.8332 1.942 0.097 176.4 x 112.0 @ 9.8 0.633 0.635 # B2106+44.015.ICL001 blob B2106+44.015 21:08:24.70308 44:57:15.0013 2.437 0.109 180.1 x 71.0 @ 11.2 0.396 0.394 # B2106+44.016.ICL001 can self cal good source B2106+44.016 21:08:06.77384 44:56:16.9766 12.090 0.153 63.2 x 48.4 @ 18.8 0.772 0.766 # B2154+40.003.ICL001 can self cal .good source B2154+40.003 21:57:54.02435 40:04:54.6091 19.684 0.265 86.2 x 59.0 @ 108.5 0.685 0.684 # B2154+40.011.ICL001 B2154+40.011 21:57:17.80378 40:12:25.4848 2.374 0.099 48.3 x 0.0 @ 73.9 0.000 0.000 # B2310+42.006.ICL001 extended ? B2310+42.006 23:14:00.74028 42:54:12.7220 1.618 0.104 153.3 x 125.0 @ 11.7 0.813 0.815 # B2310+42.016.ICL001 may be double .blob not at field center - is to the west and north B2310+42.016 23:12:11.22162 42:49:08.6024 6.778 0.239 439.4 x 172.1 @ 60.6 0.392 0.392 # B2310+42.011.ICL001 big blob B2310+42.011 23:13:39.82618 43:01:59.7114 0.436 0.097 588.4 x 553.7 @ 45.9 0.941 0.941 # B2310+42.014.ICL001 can self cal B2310+42.014 23:12:13.49560 42:39:32.3585 18.125 0.238 81.0 x 68.2 @ 64.2 0.842 0.841 # B2310+42.017.ICL001 may be double. size is 6 arc sec. this is the northern portion B2310+42.017 23:11:25.25511 42:54:13.6574 5.205 0.154 217.5 x 155.6 @ 57.6 0.713 0.715 # B2255+58.004.ICL001 1 arc sec double this is the stronger east component B2255+58.004 22:58:01.90675 58:59:15.6779 11.770 0.250 172.1 x 118.1 @ 175.8 0.688 0.686 # B2255+58.003.ICL001 can self cal B2255+58.003 22:59:56.64811 59:11:47.1728 24.933 0.376 98.9 x 44.2 @ 46.2 0.444 0.447 # B2255+58.014.ICL001 blob B2255+58.014 22:57:46.82558 59:24:32.4757 24.933 0.376 172.9 x 77.0 @ 75.2 0.444 0.445 # B2319+60.003.ICL001 B2319+60.003 23:21:40.83344 60:14:43.8933 2.016 0.103 300.7 x 108.2 @ 9.9 0.359 0.360 # B2319+60.002.ICL001 may be double blob B2319+60.002 23:21:37.74266 60:11:10.6734 1.389 0.107 512.4 x 231.7 @ 128.3 0.452 0.452 # B2319+60.004.ICL001 B2319+60.004 23:20:52.84200 60:18:56.0264 1.466 0.104 44.4 x 0.0 @ 174.1 0.000 0.000 # B2319+60.009.ICL001 B2319+60.009 23:19:58.01254 60:26:29.5762 2.520 0.092 56.8 x 0.0 @ 36.0 0.000 0.000 # B2324+60.005.ICL001 blob B2324+60.005 23:27:47.67358 61:16:53.4671 0.688 0.093 441.2 x 369.4 @ 53.4 0.837 0.837 # B2324+60.003.ICL001 B2324+60.003 23:26:32.88767 60:59:31.7402 1.494 0.107 147.3 x 0.0 @ 37.7 0.000 0.000 # B2324+60.004.ICL001 blob B2324+60.004 23:27:58.51541 61:25:20.9155 0.572 0.104 604.8 x 433.7 @ 72.6 0.717 0.717 # B2334+61.002.ICL001 B2334+61.002 23:36:38.89018 61:58:39.1252 2.602 0.175 199.7 x 0.0 @ 156.3 0.000 0.000 # B2351+61.008.ICL001 can be self caled compact B2351+61.008 23:54:40.72552 61:37:36.1183 29.236 0.424 110.5 x 73.8 @ 9.0 0.667 0.668 # B2351+61.008.ICL001 self caled the source may really be extended . B2351+61.008 23:54:40.72452 61:37:36.1156 35.731 0.161 95.7 x 31.3 @ 14.0 0.325 0.327 # B2351+61.016.ICL001 blob B2351+61.016 23:52:56.94807 61:58:53.0811 0.349 0.079 657.1 x 594.5 @ 161.7 0.905 0.905 # B2351+61.020.ICL001 B2351+61.020 23:52:59.30595 62:06:20.9625 7.653 0.161 128.1 x 50.2 @ 54.7 0.394 0.392 # B2351+61.002.ICL001 blob B2351+61.002 23:52:46.60917 61:49:05.1127 1.256 0.094 363.8 x 98.1 @ 54.2 0.270 0.270 # B2351+61.009.ICL001 B2351+61.009 23:53:09.61289 61:38:28.7482 3.316 0.119 119.8 x 29.1 @ 69.2 0.240 0.243 # B0031-07.004.ICL001 blob B0031-07.004 00:34:13.56220 -07:24:31.4751 1.733 0.113 407.5 x 247.7 @ 85.7 0.609 0.608 # B0031-07.005.ICL001 big blob . strong B0031-07.005 00:33:54.69251 -07:30:03.3341 39.270 1.040 399.1 x 228.2 @ 75.4 0.571 0.572 # B0031-07.005.ICL001 now self cal still very extended B0031-07.005 00:33:54.69412 -07:30:03.3304 49.339 0.790 345.2 x 192.6 @ 65.2 0.558 0.558 # B0031-07.003.ICL001 blob B0031-07.003 00:34:55.02346 -07:12:00.1997 4.995 0.211 263.8 x 222.1 @ 79.9 0.842 0.842 # B0031-07.007.ICL001 B0031-07.007 00:33:27.77786 -07:12:38.9802 16.236 0.360 260.2 x 96.1 @ 133.5 0.369 0.369 # B0031-07.007.ICL001 self cal. still extended B0031-07.007 00:33:27.77772 -07:12:38.9767 21.463 0.181 219.5 x 76.8 @ 138.0 0.350 0.350 # J0108-14.005.ICL001 blob J0108-14.005 01:08:29.99397 -14:28:47.0454 3.834 0.186 565.9 x 354.2 @ 2.9 0.627 0.626 # J0108-14.002.ICL001 J0108-14.002 01:09:38.70855 -14:42:35.2357 14.322 0.589 255.0 x 179.7 @ 151.8 0.705 0.704 # J0108-14.002.ICL001 self cal J0108-14.002 01:09:38.70873 -14:42:35.2366 24.553 0.419 145.2 x 87.9 @ 177.6 0.608 0.606 # J0108-14.010.ICL001 big blob J0108-14.010 01:08:36.27528 -14:35:13.8556 0.367 0.084 857.9 x 398.5 @ 85.0 0.465 0.464 # J0108-14.006.ICL001 J0108-14.006 01:07:48.27522 -14:13:45.3725 12.584 0.305 166.5 x 68.7 @ 170.8 0.413 0.413 # J0108-14.006.ICL001 self cal now quite compact J0108-14.006 01:07:48.27484 -14:13:45.3600 18.160 0.168 69.1 x 0.0 @ 20.9 0.000 0.000 # B0149-16.009.ICL001 big blob B0149-16.009 01:51:31.66107 -16:37:08.9422 0.986 0.104 477.2 x 374.5 @ 5.9 0.785 0.785 # B0149-16.006.ICL001 nice compact source but it 10 arc sec or so from field center. nice compact source B0149-16.006 01:53:25.14799 -16:31:13.6879 26.920 0.711 108.8 x 0.0 @ 162.5 0.000 0.000 # B0149-16.014.ICL001 blob B0149-16.014 01:50:57.64067 -16:40:48.1891 0.914 0.097 398.2 x 276.3 @ 145.2 0.693 0.694 # B0149-16.018.ICL001 B0149-16.018 01:51:43.63350 -16:26:37.7007 7.932 0.174 127.9 x 116.5 @ 78.1 0.912 0.911 # B0136+57.005.ICL001 extended ? B0136+57.005 01:40:32.32726 58:11:35.3004 3.891 0.112 180.0 x 124.5 @ 57.7 0.693 0.692 # B0136+57.003.ICL001 big blob B0136+57.003 01:42:04.71766 58:18:45.3798 10.389 0.603 633.3 x 467.8 @ 75.0 0.739 0.739 # B0136+57.006.ICL001 B0136+57.006 01:41:47.91761 58:08:10.5277 7.553 0.183 227.3 x 119.7 @ 106.3 0.528 0.526 # B0136+57.009.ICL001 B0136+57.009 01:38:54.86343 58:21:54.3716 1.021 0.105 171.2 x 74.0 @ 41.1 0.430 0.432 # B0136+57.011.ICL001 great source . nice and compact.could be self caled B0136+57.011 01:39:11.18057 58:35:42.9837 36.773 0.513 43.7 x 0.0 @ 13.8 0.000 0.000 # B0136+57.012.ICL001 another compact source and can be self caled B0136+57.012 01:37:50.47625 58:14:11.2876 69.657 0.899 66.6 x 22.1 @ 89.5 0.337 0.331 B0136+57.012 01:39:30.04724 58:13:32.4339 0.594 0.093 527.1 x 352.5 @ 89.3 0.669 0.669 # B0138+59.014.ICL001 blob B0138+59.014 01:41:57.67083 60:11:07.3715 1.285 0.115 346.7 x 120.8 @ 45.8 0.349 0.348 # B0138+59.016.ICL001 B0138+59.016 01:40:56.30429 60:10:57.2533 4.881 0.187 178.3 x 147.7 @ 178.2 0.830 0.828 # B0138+59.008.ICL001 big blob B0138+59.008 01:41:26.40809 60:17:43.1037 0.748 0.103 573.6 x 204.1 @ 54.7 0.356 0.356 # B0138+59.012.ICL001 blob B0138+59.012 01:40:32.53751 60:13:50.2273 0.462 0.098 699.2 x 503.2 @ 41.1 0.720 0.720 # B0138+59.015.ICL001 blob B0138+59.015 01:41:36.53692 60:12:02.3035 1.219 0.105 482.3 x 341.6 @ 4.7 0.708 0.708 # B0138+59.010.ICL001 B0138+59.010 01:40:12.44514 60:07:45.9803 1.790 0.122 205.0 x 31.3 @ 59.2 0.152 0.153 # B0138+59.011.ICL001 blob B0138+59.011 01:40:07.43777 60:08:38.5484 1.158 0.108 391.3 x 198.9 @ 57.9 0.509 0.508 # B1845-01.003.ICL001 self cal 1 min a&p B1845-01.003 18:48:51.74008 -01:40:18.0075 14.155 0.162 31.1 x 10.6 @ 39.3 0.337 0.341 # B1911-04.002.ICL001 self cal a&p 1 min. slight ext. prob ok B1911-04.002 19:15:22.12592 -04:34:36.8014 13.121 0.117 94.9 x 42.3 @ 67.4 0.446 0.445 # B1911-04.005.ICL001 self cal 1 min a&p. sl. ext B1911-04.005 19:14:11.14288 -04:58:44.4379 10.005 0.101 65.0 x 0.0 @ 178.6 0.000 0.000 # B1911-04.009.ICL001 self cal 2 min a&p reasonably compact! B1911-04.009 19:13:21.79431 -04:32:54.0058 6.863 0.116 58.0 x 0.0 @ 7.0 0.000 0.000 # B1855+09.006.ICL001 self cal 40sec a&p sl. ext. B1855+09.006 18:57:24.77888 09:23:32.3191 13.719 0.089 71.7 x 8.0 @ 22.9 0.113 0.111 # B1839+09.009.ICL001 self cal 1 min a&p compact B1839+09.009 18:41:50.02858 08:57:19.6383 18.121 0.119 7.8 x 0.0 @ 30.5 0.000 0.000 # B1839+56.013.ICL001 self cal 2 min a&p pointlike! B1839+56.013 18:41:09.02612 56:38:15.2841 8.887 0.090 32.8 x 0.0 @ 37.2 0.000 0.000 # B1946+35.010.ICL001 self cal 0.5 min a&p bright! sl. ext. B1946+35.010 19:48:04.51924 35:56:20.6653 303.250 0.174 41.6 x 29.5 @ 179.6 0.705 0.710 # B1944+17.016.ICL001 self cal 1 min a&p AGN core B1944+17.016 19:46:20.93679 18:27:32.7358 27.097 0.098 56.3 x 40.5 @ 21.9 0.718 0.720 # B2000+40.004.ICL001 self cal 1 min a&p pointlike B2000+40.004 20:03:06.77628 40:29:01.1660 27.339 0.112 22.5 x 0.0 @ 139.9 0.000 0.000 # B2011+38.002.ICL001 self cal 1 min a&p fantastic source! B2011+38.002 20:13:59.27394 38:28:51.9562 80.952 0.116 5.0 x 0.0 @ 144.7 0.000 0.000 # B2045-16.011.ICL001 self cal solint 1 a&p B2045-16.011 20:48:36.69994 -16:09:45.4394 9.975 0.121 71.1 x 11.4 @ 31.3 0.160 0.160 # B2045-16.008.ICL001 self cal 1 min a&p Very Nice!!! B2045-16.008 20:48:49.57191 -16:00:13.9195 83.420 0.121 0.0 x 0.0 @ 0.0 -1.000 -1.000 # B2053+36.011.ICL001 self cal 1 a&p nice source B2053+36.011 20:55:12.22739 36:34:22.6929 17.883 0.102 22.3 x 0.0 @ 177.1 0.000 0.000 # B2053+36.013.ICL001 self cal 4 min a&p B2053+36.013 20:55:32.58045 36:37:53.6296 6.668 0.118 35.5 x 0.0 @ 9.5 0.000 0.000 # B2111+46.005.ICL001 self cal solint 1 a&p, compact! B2111+46.005 21:14:32.87532 46:34:39.2864 170.290 0.139 5.4 x 0.0 @ 33.9 0.000 0.000 # B2106+44.016.ICL001 self cal solint 1 a&p B2106+44.016 21:08:06.77400 44:56:16.9776 13.620 0.123 17.9 x 0.0 @ 132.7 0.000 0.000 # B2154+40.003.ICL001 self cal 1 min a&p resolved to ~0.04 arcsec B2154+40.003 21:57:54.02421 40:04:54.6025 23.833 0.121 54.3 x 41.8 @ 2.7 0.768 0.769 # B2255+58.003.ICL001 self cal 1 min a&p B2255+58.003 22:59:56.64761 59:11:47.1650 30.781 0.126 19.1 x 0.0 @ 146.4 0.000 0.000 # B2351+61.008.ICL001 self cal 1 min a&p double B2351+61.008 23:54:40.72504 61:37:36.1130 36.829 0.109 51.8 x 27.1 @ 20.5 0.523 0.523 # B0136+57.011.ICL001 self cal 1 min a&p very compact! B0136+57.011 01:39:11.18090 58:35:42.9875 45.763 0.132 0.0 x 0.0 @ 0.0 -1.000 -1.000 # B0136+57.012.ICL001 self cal 1 min a&p B0136+57.012 01:37:50.47629 58:14:11.2905 85.660 0.141 44.0 x 31.1 @ 30.9 0.707 0.707 # B1508+55.006.ICL001 self cal solint 1 a&p B1508+55.006 15:11:48.06076 55:41:56.2876 25.812 0.126 0.0 x 0.0 @ 0.0 -1.000 -1.000 # B1541+09.008.ICL001 self cal 40 sec a&p bright, compact B1541+09.008 15:43:03.70214 09:19:09.7845 31.063 0.121 35.5 x 0.0 @ 5.0 0.000 0.000 # J1643-12.007.ICL001 self cal 40 sec a&p J1643-12.007 16:43:19.43821 -12:20:15.6969 14.709 0.110 68.2 x 44.2 @ 140.1 0.648 0.648 # B1702-19.012.ICL001 self cal 1 min a&p B1702-19.012 17:04:29.16675 -19:03:35.9759 16.414 0.112 110.0 x 55.2 @ 146.1 0.501 0.502 # B1702-19.013.ICL001 self cal 30 sec a&p bright, fairly compact B1702-19.013 17:04:41.58672 -18:58:07.3331 31.333 0.115 26.4 x 0.0 @ 127.8 0.000 0.000 # J1744-11.015.ICL001 self cal 1 min a&p compact? J1744-11.015 17:43:25.18090 -11:17:56.0366 10.933 0.130 66.4 x 0.0 @ 13.6 0.000 0.000 # J1713+07.008.ICL001 self cal 1 min a&p J1713+07.008 17:13:27.09521 07:30:18.9931 17.144 0.118 39.0 x 22.4 @ 133.3 0.577 0.575 # B1821-19.011.ICL001 self cal 2 min a&p B1821-19.011 18:24:22.00871 -19:52:34.8565 9.928 0.138 56.1 x 0.0 @ 126.1 0.000 0.000 # B1821-19.016.ICL001 self cal 2 min a&p B1821-19.016 18:22:58.41138 -19:30:02.1595 10.819 0.129 55.8 x 0.0 @ 143.7 0.000 0.000 # J1835-11.004.ICL001 self cal 1 min core, probably slightly resolved J1835-11.004 18:35:19.57533 -11:15:59.2894 62.292 0.356 50.9 x 39.0 @ 127.0 0.765 0.766 # B1822-09.008.ICL001 self cal 1 min a&p nice bright point source! B1822-09.008 18:24:32.56566 -09:50:17.6804 39.453 0.114 0.0 x 0.0 @ 0.0 -1.000 -1.000 # B1804-08.003.ICL001 self cal solint 3 a&p core (with jet) B1804-08.003 18:08:17.68320 -08:52:38.9134 6.714 0.098 71.3 x 39.8 @ 165.4 0.559 0.559 # B1804-08.005.ICL001 self cal solint 1 a&p compact? B1804-08.005 18:07:26.04776 -09:05:47.1812 11.315 0.093 34.1 x 0.0 @ 24.0 0.000 0.000 # B1818-04.006.ICL001 self cal 1 min a&p sl. ext.? B1818-04.006 18:20:43.39607 -04:24:12.4164 82.641 0.123 35.6 x 12.1 @ 50.9 0.336 0.340 # B0450-18.003.ICL001 B0450-18.003 04:52:51.14548 -17:53:40.6505 1.524 0.167 270.0 x 95.1 @ 178.1 0.352 0.352 # B0450-18.002.ICL001 self cal 2 min a&p B0450-18.002 04:52:11.97908 -18:16:41.9582 12.026 0.180 180.8 x 0.0 @ 150.1 0.000 0.000 # B0450+55.002.ICL001 self cal 40 sec a&p B0450+55.002 04:54:00.06323 55:36:45.4060 120.730 0.775 78.9 x 0.0 @ 124.7 0.000 0.000 # B0450+55.003.ICL001 brighter (central) component B0450+55.003 04:54:39.55111 55:45:05.4280 1.257 0.135 271.0 x 0.0 @ 28.4 0.000 0.000 # B0450+55.005.ICL001 multiple source, very weak! B0450+55.005 04:55:16.14016 55:50:36.8354 0.530 0.155 228.4 x 199.6 @ 52.5 0.874 0.874 # B0525+21.004.ICL001 weak, multiple B0525+21.004 05:28:48.65463 21:42:30.1766 2.424 0.194 167.5 x 19.7 @ 135.6 0.118 0.118 # # B0525+21.006.ICL001 < 1 mjy # # B0540+23.014.ICL001 1.5 mJy, ext. # # B0540+23.010.ICL001 < 1 mjy # # B0540+23.011.ICL001 1.2 mJy # # B0540+23.015.ICL001 < 1 mjy # B0609+37.008.ICL001 self cal 90 sec a&p compact B0609+37.008 06:12:12.91365 37:25:38.3110 14.686 0.196 53.2 x 0.0 @ 31.6 0.000 0.000 # B0609+37.003.ICL001 1.6 mJy ext? # J0613-02.002.ICL001 self cal 2 min a&p core with skirt? J0613-02.002 06:15:02.38012 -01:58:24.4205 12.258 0.178 125.2 x 46.5 @ 150.9 0.371 0.371 # # J0613-02.003.ICL001 < 1.5 mJy # # J0613-02.017.ICL001 < 2 mJy # J0613-02.008.ICL001 J0613-02.008 06:13:27.79276 -02:14:25.5430 2.124 0.212 182.5 x 93.6 @ 59.9 0.513 0.513 # # J0613-02.009.ICL001 < 1 mJy # # J0613-02.015.ICL001 < 2 mJy # # J0613-02.018.ICL001 not there # B0818-13.002.ICL001 self cal 1 min B0818-13.002 08:20:11.43071 -13:49:12.8558 43.814 0.432 70.5 x 0.0 @ 130.7 0.000 0.000 # # B0818-13.003.ICL001 complicated mess # # J0751+18.010.ICL001 < 2 mJy probl. ext. # J0751+18.005.ICL001 J0751+18.005 07:51:52.28719 17:54:31.5157 2.996 0.278 167.0 x 0.0 @ 23.0 0.000 0.000 # J0751+18.006.ICL001 J0751+18.006 07:52:12.40824 18:10:18.7826 2.445 0.254 199.2 x 161.4 @ 171.3 0.810 0.810 # # J0751+18.010.ICL001 weak multiple and extended # J0751+18.005.ICL001 matches WFB, multiple J0751+18.005 07:51:52.28710 17:54:31.5133 3.617 0.287 107.9 x 0.0 @ 21.0 0.000 0.000 # J0751+18.006.ICL001 matches WFB, double J0751+18.006 07:52:12.40699 18:10:18.7964 2.653 0.288 215.4 x 0.0 @ 33.3 0.000 0.000 # # J0751+18.017.ICL001 no source (<1.3 mJy) # J0751+18.013.ICL001 good source J0751+18.013 07:51:02.04615 17:48:40.2273 3.687 0.279 171.8 x 0.0 @ 18.7 0.000 0.000 # J0751+18.020.ICL001 good source J0751+18.020 07:50:20.38045 18:09:50.5743 3.676 0.259 81.0 x 0.0 @ 35.4 0.000 0.000 # J0751+18.022.ICL001 extnd component (double) J0751+18.022 07:50:38.51860 18:26:28.9680 3.520 0.273 270.1 x 0.0 @ 123.5 0.000 0.000 # J0751+18.023.ICL001 extended? J0751+18.023 07:50:20.65591 18:26:55.5140 3.851 0.404 246.8 x 132.6 @ 136.1 0.537 0.537 # J0751+18.024.ICL001 Bright (150 mJy, RMS 7 mJy) J0751+18.024 07:50:00.33469 18:23:11.2627 141.660 7.040 130.4 x 0.0 @ 64.9 0.000 0.000 # # B0834+06.002.ICL001 Extended, confused mess. 3 mJy peak (ext jet hotspot) # B0834+06.008.ICL001 Compact, excellent B0834+06.008 08:36:35.73231 06:02:43.3238 2.493 0.238 158.9 x 21.8 @ 67.6 0.137 0.137 # B0834+06.010.ICL001 Compact, good source B0834+06.010 08:36:27.17127 06:12:01.9189 3.648 0.288 277.8 x 0.0 @ 30.6 0.000 0.000 # B0834+06.005.ICL001 Good B0834+06.005 08:38:20.02983 06:07:15.2959 3.518 0.211 226.5 x 0.0 @ 19.7 0.000 0.000 # B0834+06.009.ICL001 Double source (1.8, 2.1 mJy, 0.9 asec central sep) -- East comp B0834+06.009 08:36:31.79643 05:59:10.3288 1.815 0.229 97.1 x 0.0 @ 50.6 0.000 0.000 # B0834+06.009.ICL001 Double source (1.8, 2.1 mJy, 0.9 asec central sep) -- West comp B0834+06.009 08:36:31.74770 05:59:10.8400 2.004 0.226 164.5 x 0.0 @ 73.9 0.000 0.000 # J1022+10.007.ICL001 Good, compact. J1022+10.007 10:23:34.06789 10:12:00.1228 30.029 1.260 240.2 x 0.0 @ 54.0 0.000 0.000 # J1022+10.010.ICL001 Good, compact & bright. J1022+10.010 10:23:10.90487 10:01:26.9064 17.759 0.639 181.6 x 0.0 @ 50.1 0.000 0.000 # J1022+10.005.ICL001 J1022+10.005 10:23:26.59566 09:57:21.9062 3.148 0.222 159.0 x 0.0 @ 48.5 0.000 0.000 # # J1022+10.008.ICL001 Weak double 2.1mJy peak # J1022+10.003.ICL001 Somewhat ext. J1022+10.003 10:23:27.31505 09:44:54.8670 1.958 0.209 267.3 x 0.0 @ 58.8 0.000 0.000 # J1022+10.006.ICL001 J1022+10.006 10:24:18.69204 09:55:46.9418 4.988 0.224 189.9 x 0.0 @ 46.4 0.000 0.000 # # J1022+10.012.ICL001 Weak extended <1 mJy # B1039-19.002.ICL001 Triple, not just double? Weak B1039-19.002 10:41:17.81292 -19:52:40.3647 1.705 0.229 162.2 x 80.5 @ 60.8 0.496 0.496 # # B1039-19.004.ICL001 Multiple components, weak # B1039-19.006.ICL001 Extended, multi-comp, bright central comp. Interesting? B1039-19.006 10:40:57.28143 -19:24:03.6841 25.807 1.690 526.2 x 265.1 @ 122.4 0.504 0.504 # B1039-19.003.ICL001 Double: East comp. B1039-19.003 10:42:38.77600 -19:42:09.2728 1.509 0.248 286.9 x 0.0 @ 131.9 0.000 0.000 # B1039-19.003.ICL001 Double: West comp. B1039-19.003 10:42:38.73454 -19:42:09.0389 1.687 0.245 278.8 x 0.0 @ 136.3 0.000 0.000 # J1012+53.017.ICL001 Strong, compact J1012+53.017 10:13:07.29382 53:12:34.3308 3.469 0.218 162.9 x 0.0 @ 60.6 0.000 0.000 # J1012+53.014.ICL001 Ok. J1012+53.014 10:12:30.55368 52:58:25.5316 2.616 0.210 172.6 x 0.0 @ 66.2 0.000 0.000 # J1012+53.018.ICL001 Ok. J1012+53.018 10:13:07.35425 53:04:22.8756 2.301 0.170 178.4 x 0.0 @ 55.3 0.000 0.000 # # J1012+53.019.ICL001 <1 mJy, no clean. # J1012+53.003.ICL001 Ok. J1012+53.003 10:11:28.04108 52:57:26.7611 5.756 0.278 224.6 x 0.0 @ 54.3 0.000 0.000 # J1012+53.006.ICL001 Ok. J1012+53.006 10:13:39.26767 52:57:19.9614 2.038 0.201 318.2 x 0.0 @ 42.8 0.000 0.000 # B1112+50.001.ICL001 4.1 mJy ref source. Also image 12"S for PSR: not seen. B1112+50.001 11:15:38.48095 50:30:25.6254 4.054 0.231 261.1 x 0.0 @ 62.1 0.000 0.000 # B1112+50.004.ICL001 Ok, weak. B1112+50.004 11:16:24.95599 50:28:43.1758 1.169 0.155 231.6 x 0.0 @ 66.2 0.000 0.000 # B1112+50.006.ICL001 B1112+50.006 11:15:13.47113 50:09:01.1887 53.052 1.740 237.5 x 0.0 @ 64.1 0.000 0.000 # # B1112+50.008.ICL001 weak, multiple blobs < 1 mJy # B1112+50.021.ICL001 Ok. B1112+50.021 11:14:50.06499 50:29:17.3066 1.736 0.183 152.8 x 0.0 @ 67.8 0.000 0.000 # B1112+50.003.ICL001 Ok. B1112+50.003 11:16:51.18705 50:36:01.9199 5.734 0.269 197.5 x 0.0 @ 68.3 0.000 0.000 # B1112+50.023.ICL001 Ok. B1112+50.023 11:14:12.55911 50:39:29.7568 6.820 0.298 229.2 x 0.0 @ 50.6 0.000 0.000