Table 2:

Table of HerMES SDP number counts at 250, 350 and 500 $\mu $m.
  Bin 1 Bin 2 Bin 3 Bin 4 Bin 5 Bin 6
$S_{\rm min}$ 20 29 51 69 111 289
$S_{\rm max}$ 29 51 69 111 289 511
$S_{\rm euc}$ 23.8 37.5 58.9 85.9 166.2 374.1
250 $\mu $m
$\frac{{\rm d}N}{{\rm d}S}$ $2.0 \times 10^8$ $6.4\times 10^7$ $1.2\times 10^7$ $3.1 \times 10^6$ $2.1\times 10^5$ $1.7\times 10^4$
err1 38 22 28 35 23 6
err2 10 6 7 6 4 19
err3 4 3 7 4 7 23
err4 11 19 30 28 30 8
350 $\mu $m
$\frac{{\rm d}N}{{\rm d}S}$ $1.1\times 10^8$ 3.5 $\times 10^7$ $5.3\times 10^6$ $1.1\times 10^6$ $6.2\times 10^4$ $4.7\times 10^3$
err1 49 34 44 56 25 129
err2 18 14 17 6 5 12
err3 7 4 10 7 15 43
err4 23 13 33 8 12 64
500 $\mu $m
$\frac{{\rm d}N}{{\rm d}S}$ $3.6\times 10^7$ $1.1\times 10^7$ $1.6\times 10^6$ $2.3\times 10^5$ $1.3\times 10^4$ $1.3\times 10^3$
err1 83 50 62 56 45 0
err2 31 18 25 15 18 7
err3 10 6 18 14 33 50
err4 5 17 48 27 20 0

Notes. Bin limits and Euclidian weighted central fluxes are given in mJy. Counts are in $/{\rm sr}^{-1}{\rm Jy}^{-1}$. Errors 1-4 are fractional errors in percentages arising from: flux-deboosting, completeness corrections, Poisson statistics and field-field variations respectively.


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