Table 1
Truncation factors for median-filtered sources (,
) and filaments (ℱG, ℱP) using sliding windows with different radii W = R/H, corresponding to the images described in Sect. 2.1 and their profiles plotted in Fig. 1.
W |
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ℱG |
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ℱP |
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1 | 4 | 4 | 4 | 3 | 3 | 3 | 1.6 | 1.6 | 1.6 | 1.7 | 1.7 | 1.7 |
2 | 260 | 200 | 130 | 9 | 9 | 9 | 6.8 | 6.8 | 6.8 | 3.5 | 3.6 | 3.6 |
4 | 4 × 109 | 2000 | 720 | 33 | 33 | 30 | 1000 | 240 | 160 | 11 | 11 | 11 |
8 | – | – | – | 130 | 110 | 84 | 108 | 710 | 220 | 44 | 43 | 40 |
16 | – | – | – | 510 | 340 | 250 | 5 × 109 | 1700 | 350 | 170 | 140 | 55 |
Notes. The factors are defined as the ratio fT = IP/IF of the original peak intensity to the filtered peak intensity. For the images with background, fT were computed in background-subtracted images. Some entries for the largest windows present additional information with respect to the plots in Fig. 1.
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