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Home All issues Volume 502 / No 1 (July IV 2009) A&A, 502 1 (2009) 61-65 Full HTML
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Table 2:

Flux densities and polarised flux densities from Effelsberg 100-m and NVSS measurements.
Name S1.4 S2.64 S4.85 S8.35 S10.45 $S_{\rm p 1.4}$ $S_{\rm p 2.64}$ $S_{\rm p 4.85}$ $S_{\rm p 8.35}$ $S_{\rm p 10.45}$  
  [mJy] [mJy] [mJy] [mJy] [mJy] [mJy] [mJy] [mJy] [mJy] [mJy]  
3C 43  0127+23 29 414 $\pm$ 88 1787 $\pm$ 37 1109 $\pm$ 22 698 $\pm$ 14 578 $\pm$ 12 <10.8 <38.4 <6.6 14.7 $\pm$ 4.1 12.2 $\pm$ 2.3
3C 48  0134+32 16 018 $\pm$ 481 9373 $\pm$ 191 5534 $\pm$ 113 3243 $\pm$ 65 2495 $\pm$ 52 70.8 $\pm$ 57.6 <195.0 185.5 $\pm$ 43.1 160.5 $\pm$ 18.8 139.5 $\pm$ 5.6
3C 49  0138+13 2740 $\pm$ 82 1552 $\pm$ 33 878 $\pm$ 18 494 $\pm$ 10 376 $\pm$ 8 <9.9 <34.5 <20.4 <8.7 <6.3
3C 67  0221+27 3024 $\pm$ 91 1757 $\pm$ 36 997 $\pm$ 20 575 $\pm$ 12 419 $\pm$ 9 17.0 $\pm$ 10.9 <37.8 <23.4 22.3 $\pm$ 3.4 15.7 $\pm$ 1.9
4C 34.07  0223+34 2894 $\pm$ 87 2483 $\pm$ 51 2234 $\pm$ 46 1452 $\pm$ 30 1212 $\pm$ 25 <10.5 <51.6 <52.2 <24.9 <13.2
4C 16.09  0316+16 8028 $\pm$ 241 5038 $\pm$ 103 2937 $\pm$ 60 1563 $\pm$ 32 1187 $\pm$ 25 <28.9 <103.5 <6.9 <27.0 <12.9
   0319+12 1907 $\pm$ 67 1704 $\pm$ 35 1791 $\pm$ 37 1527 $\pm$ 31 1549 $\pm$ 32 71.8 $\pm$ 7.0 95.3 $\pm$ 12.3 113.0 $\pm$ 14.1 88.9 $\pm$ 8.9 77.2 $\pm$ 5.7
3C 93.1  0345+33 2365 $\pm$ 71 1390 $\pm$ 29 926 $\pm$ 19 477 $\pm$ 10 383 $\pm$ 8 <8.6 <30.0 <21.6 <8.4 9.1 $\pm$ 1.6
4C 76.03  0404+76 5619 $\pm$ 169 4042 $\pm$ 83 3355 $\pm$ 69 2087 $\pm$ 42 1648 $\pm$ 34 <20.3 < 83.4 <78.3 <36.0 <18.0
   0428+20 3755 $\pm$ 112 3166 $\pm$ 65 2761 $\pm$ 57 1542 $\pm$ 31 1289 $\pm$ 26 <13.6 <65.7 <64.5 <26.7 <14.1
3C 119  0429+41 9832 $\pm$ 295 6126 $\pm$ 126 4722 $\pm$ 97 2677 $\pm$ 54 2260 $\pm$ 47 <35.4 <125.4 <110.1 157.9 $\pm$ 15.7 200.6 $\pm$ 8.9
3C 138  0518+165 8603 $\pm$ 258 5780 $\pm$ 119 4119 $\pm$ 84 2552 $\pm$ 53 2160 $\pm$ 45 619.0 $\pm$ 31.0 595.5 $\pm$ 41.0 411.6 $\pm$ 32.8 297.8 $\pm$ 17.6 218.8 $\pm$ 8.8
3C 147  0538+49 22 880 $\pm$ 686 13 436 $\pm$ 276 10 120 $\pm$ 207 4735 $\pm$ 96 3823 $\pm$ 80 <82.3 <274.5 <236.1 <81.6 47.3 $\pm$ 13.6
3C 186  0740+38 1236 $\pm$ 37 615 $\pm$ 14 271 $\pm$ 8 114 $\pm$ 3 85 $\pm$ 3 <4.6 <15.3 <6.3 <2.4 <3.0
3C 190  0758+14 2734 $\pm$ 82 1359 $\pm$ 28 746 $\pm$ 16 426 $\pm$ 10 360 $\pm$ 8 <9.9 <31.5 <17.4 <7.8 <5.1
3C 216  0906+43 4239 $\pm$ 127 1446 $\pm$ 50 1731 $\pm$ 35 1413 $\pm$ 29 1337 $\pm$ 29 <15.3 <52.5 <40.5 <24.3 <14.7
3C 237  1005+07 6522 $\pm$ 196 3608 $\pm$ 74 1971 $\pm$ 42 1034 $\pm$ 21 823 $\pm$ 17 <23.5 <76.5 <45.9 <18.0 9.7 $\pm$ 3.2
3C 241  1019+22 1686 $\pm$ 51 799 $\pm$ 17 350 $\pm$ 7 161 $\pm$ 33 112 $\pm$ 3 <6.2 <19.5 <8.1 <3.0 < 1.2
4C 31.38  1153+31 2978 $\pm$ 89 1751 $\pm$ 36 1030 $\pm$ 21 545 $\pm$ 11 441 $\pm$ 10 <10.8 <45.0 <24.0 <9.6 8.6 $\pm$ 1.8
3C 268.3  1203+64 3719 $\pm$ 112 1947 $\pm$ 39 1153 $\pm$ 23 618 $\pm$ 13 479 $\pm$ 10 <13.4 <40.8 <27.0 17.2 $\pm$ 3.7 14.2 $\pm$ 2.1
   1225+36 2098 $\pm$ 63 1434 $\pm$ 30 753 $\pm$ 16 353 $\pm$ 9 239 $\pm$ 5 <7.7 <31.5 <17.7 <6.3 <2.4
3C 277.1  1250+56 2288 $\pm$ 69 1343 $\pm$ 30 790 $\pm$ 16 481 $\pm$ 10 384 $\pm$ 8 <8.3 <29.4 <18.3 14.3 $\pm$ 2.9 9.9 $\pm$ 1.8
4C 32.44  1323+32 4862 $\pm$ 146 3369 $\pm$ 70 2293 $\pm$ 47 1540 $\pm$ 31 1293 $\pm$ 28 <17.5 17.3 $\pm$ 2.3 <53.4 <26.7 <14.1
3C 286  1328+30 14 902 $\pm$ 447 10 607 $\pm$ 219 7430 $\pm$ 152 5179 $\pm$ 104 4474 $\pm$ 94 999.9 $\pm$ 53.7 1152.7 $\pm$ 74.1 776.7 $\pm$ 59.4 607.4 $\pm$ 31.5 525.8$\pm$ 18.4
3C 287  1328+27 7052 $\pm$ 212 4697 $\pm$ 97 3130 $\pm$ 64 2050 $\pm$ 42 1748 $\pm$ 36 45.6 $\pm$ 25.4 168.7 $\pm$ 32.3 116.6 $\pm$ 24.4 65.2 $\pm$ 11.8 58.6 $\pm$ 6.4
4C 62.22  1358+62 4308 $\pm$ 129 2765 $\pm$ 57 1701 $\pm$ 35 1080 $\pm$ 22 888 $\pm$ 18 <15.6 <57.3 <39.6 <18.6 <9.9
   1413+34 1864 $\pm$ 56 1488 $\pm$ 30 1059 $\pm$ 22 735 $\pm$ 15 621 $\pm$ 14 <6.8 45.8 $\pm$ 11.2 <24.6 <12.9 <7.5
3C 298  1416+06 6100 $\pm$ 183 2888 $\pm$ 60 1432 $\pm$ 30 789 $\pm$ 17 616 $\pm$ 14 <22.0 <60.0 <33.3 14.6 $\pm$ 4.6 12.8 $\pm$ 2.6
3C 299  1419+41 3147 $\pm$ 111 1721 $\pm$ 35 922 $\pm$ 20 502 $\pm$ 10 400 $\pm$ 9 <11.4 <40.8 <21.6 <9.0 <6.6
OQ172  1442+10 2418 $\pm$ 72 1398 $\pm$ 38 1032 $\pm$ 21 641 $\pm$ 14 516 $\pm$ 11 31.7 $\pm$ 8.8 63.2 $\pm$ 12.0 26.5 $\pm$ 8.0 14.2 $\pm$ 3.8 <8.7
3C 303.1  1443+77 1880 $\pm$ 66 882 $\pm$ 19 413 $\pm$ 8 199 $\pm$ 4 128 $\pm$ 3 <6.9 <20.1 <9.6 <3.9 <2.4
3C 305.1  1447+77 1666 $\pm$ 50 837 $\pm$ 18 412 $\pm$ 9 208 $\pm$ 4 154 $\pm$ 3 <6.2 <20.1 <9.6 <11.7 <3.9
3C 309.1  1458+71 7468 $\pm$ 224 5129 $\pm$ 105 3552 $\pm$ 73 2568 $\pm$ 52 2196 $\pm$ 46 91.1 $\pm$ 26.9 188.3 $\pm$ 35.2 8.5 $\pm$ 2.8 70.8 $\pm$ 14.8 55.5 $\pm$ 8.8
3C 318  1517+20 2688 $\pm$ 81 1417 $\pm$ 29 764 $\pm$ 16 417 $\pm$ 8 322 $\pm$ 7 <9.8 <30.9 25.8 $\pm$ 6.0 27.6 $\pm$ 2.6 29.6 $\pm$ 1.8
   1600+33 2991 $\pm$ 90 1980 $\pm$ 41 1433 $\pm$ 29 1049 $\pm$ 21 915 $\pm$ 20 <10.8 <42.3 <33.3 <18.3 <10.5
OS111  1607+26 4908 $\pm$ 147 3140 $\pm$ 65 1728 $\pm$ 35 902 $\pm$ 18 681 $\pm$ 15 <17.7 <98.7 <40.2 <15.6 <8.1
3C 343  1634+62 5002 $\pm$ 150 2858 $\pm$ 59 1503 $\pm$ 31 808 $\pm$ 16 622 $\pm$ 13 <18.0 <59.1 <35.1 <14.1 8.4 $\pm$ 2.5
3C 343.1  1637+62 4611 $\pm$ 138 2384 $\pm$ 49 1190 $\pm$ 24 631 $\pm$ 13 479 $\pm$ 10 <16.6 <49.2 <27.9 <11.1 <6.0
3C 346  1641+17 3666 $\pm$ 110 2260 $\pm$ 47 1426 $\pm$ 29 915 $\pm$ 19 773 $\pm$ 17 80.6 $\pm$ 13.3 <47.7 <33.3 <45.9 13.8 $\pm$ 3.0
4C 39.56  1819+39 3507 $\pm$ 105 1871 $\pm$ 42 938 $\pm$ 19 463 $\pm$ 10 337 $\pm$ 7 <12.7 <39.9 <21.9 <8.1 <4.5
3C 380  1828+48 13 573 $\pm$ 413 8139 $\pm$ 167 5073 $\pm$ 105 3523 $\pm$ 71 3055 $\pm$ 63 62.2 $\pm$ 49.5 <166.5 <118.2 <60.6 <32.7
4C 29.56  1829+29 2924 $\pm$ 88 1945 $\pm$ 40 1168 $\pm$ 24 679 $\pm$ 14 533 $\pm$ 12 <10.6 <40.8 <27.3 <12.0 <6.9
4C 11.69 2230+11 7202 $\pm$ 216 5695 $\pm$ 118 4135 $\pm$ 85 3396 $\pm$ 69 3209 $\pm$ 67 114.0 $\pm$ 26.0 229.6 $\pm$ 39.1 147.6 $\pm$ 32.3 127.3 $\pm$ 19.6 116.4 $\pm$ 11.6
3C 454  2249+18 2133 $\pm$ 64 1265 $\pm$ 26 761 $\pm$ 16 469 $\pm$ 10 383 $\pm$ 8 77.4 $\pm$ 7.8 73.6 $\pm$ 9.1 71.0 $\pm$ 6.1 52.7 $\pm$ 2.9 42.8 $\pm$ 1.9
3C 454.1  2248+71 1555 $\pm$ 47 696 $\pm$ 15 287 $\pm$ 6 119 $\pm$ 3 87 $\pm$ 2 <5.8 <16.8 <6.9 <3.6 <0.9
3C 455  2252+12 2706 $\pm$ 81 1491 $\pm$ 30 772 $\pm$ 16 421 $\pm$ 93 312 $\pm$ 7 55.8 $\pm$ 9.9 50.5 $\pm$ 10.9 <18.0 <7.8 4.7 $\pm$ 1.5
   2342+82 3777 $\pm$ 113 2275 $\pm$ 47 1308 $\pm$ 27 747 $\pm$ 15 579 $\pm$ 12 <13.7 <47.4 <30.6 <13.2 <6.6
The values at the various observing frequencies (in GHz) are organised as follows: Col. 1, source name; Col. 2, other name; Cols. 3 to 7, flux density S; Cols. 8 to 12, polarised flux density $S_{\rm p}$.

Source LaTeX | All tables | In the text

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