#################### #Euclidean normalized differential source counts at 8.4 GHz. # col. 1 = log(S [Jy]) # col. 2 = S^2.5dN/dS[Jy^1.5/sr] # col. 3-4 = positive and negative errors on the counts. # col. 5 = For surveys covering less than 25 deg^2 the contribution to such errors # due to the sampling variance [eq.(6) in De Zotti et al. (2009)]; # such contributions are negligible for larger areas. # col. 6 = references (see the list below) # Reference codes. # fo02: 2002AJ....123.2402F # hp05: 2005ApJ...635..950H # wi93: 1993ApJ...405..498W ################## -4.863 0.231 0.050 0.050 - fo02 -4.717 0.520 0.385 0.385 0.106 wi93 -4.611 0.192 0.043 0.043 - fo02 -4.480 0.530 0.263 0.263 0.108 wi93 -4.348 0.288 0.064 0.064 - fo02 -4.192 1.320 0.577 0.577 0.270 wi93 -3.710 0.441 0.096 0.096 - fo02 -3.678 0.834 0.352 0.352 0.089 hp05 -3.481 1.190 0.547 0.547 0.244 wi93 -2.745 2.787 1.125 1.125 0.296 hp05 -2.699 8.716 3.107 3.107 0.393 hp05 -2.474 20.374 11.961 11.961 2.165 hp05 -2.360 10.123 4.550 4.550 0.457 hp05 -2.160 10.809 5.426 5.426 0.488 hp05 -2.034 20.953 9.918 9.918 2.227 hp05 -1.901 18.039 8.108 8.108 0.814 hp05 -1.654 19.820 3.769 4.360 - wi93 -1.618 41.222 20.695 20.695 1.860 hp05 -1.457 40.823 8.986 6.514 - wi93 -1.348 92.022 65.202 65.202 4.153 hp05 -1.250 55.132 15.549 13.185 - wi93 -1.052 31.982 6.081 5.758 - wi93 -0.855 43.182 8.211 9.492 - wi93 -0.658 62.820 11.945 11.321 - wi93 -0.461 62.951 19.796 17.368 - wi93 -0.263 82.912 23.387 19.831 - wi93 -0.056 61.674 9.908 2.992 - wi93 0.122 63.343 6.625 7.380 - wi93 0.320 58.911 6.161 5.566 - wi93 0.527 43.823 8.309 7.898 - wi93 0.726 24.797 10.319 9.330 - wi93