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Table B.3

Deconvolution accuracy ratios A = Dj/H (left) and power-law slopes γ (right) for the finite Gaussian and power-law sources 𝒮 and filaments ℱ (Sect. 4.6) with profiles {𝒢|𝒫{A|B|C|D}} from Fig. 1, convolved with the Gaussian kernels 𝒪j and power-law kernels 𝒦j· of half maximum sizes Oj (cf. Fig. 13), without any background. These results correspond to those presented in Sect. 3 for a perfectly subtracted flat background (∈l = 0).

Oj 𝒢 𝒫A 𝒫B 𝒫C 𝒫D 𝒢 𝒫A 𝒫B 𝒫C 𝒫D
(″)
𝒮 4 1.00 1.10 1.10 1.39 1.00 1.12 1.02 1.17 1.00 1.11 2.0 2.0 2.0 2.0 2.0
4 1.00 1.23 1.08 1.55 1.00 1.26 1.02 1.31 1.00 1.24 1.0 1.3 1.3 1.3 1.3
𝒮 32 1.00 1.10 3.53 4.01 2.35 2.63 2.11 2.35 1.47 1.63 2.0 2.0 2.0 2.0 2.0
32 1.00 2.10 2.50 3.72 1.59 2.67 1.59 2.65 1.19 2.27 1.0 1.3 1.3 1.3 1.3
𝒮 256 1.00 1.10 5.16 5.69 4.52 4.98 3.60 3.96 2.71 2.98 2.0 2.0 2.0 2.0 2.0
256 1.00 13.24 4.04 14.09 2.82 13.64 2.34 13.50 1.62 13.33 1.0 1.2 1.2 1.2 1.2

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