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Table A.4.

Spectral fitting results of Compton-thick sources only using the UXCLUMPY model.

Source name Mission1 PHABSGAL * (PO + APEC + UXCLUMPY) model parameters

Γsoft Nsoft kT NAPEC Γ NHeq NHlos θinc (σtorus) NUXCLUMPY χ2/dof
×10−5 keV ×10−5 ×1022 cm−2 ×1022 cm−2 deg. ×10−3
ESO420-013 C,N 3 . 35 0.24 + 0.40 $ 3.35^{+0.40}_{-0.24} $ 5 . 14 2.43 + 2.06 $ 5.14^{+2.06}_{-2.43} $ 0 . 86 0.07 + 0.08 $ 0.86^{+0.08}_{-0.07} $ 2 . 55 1.21 + 0.44 $ 2.55^{+0.44}_{-1.21} $ 1 . 53 0.28 + 0.27 $ 1.53^{+0.27}_{-0.28} $ - > 292 90(f) 30(f) 0 . 89 0.11 + 1.42 $ 0.89^{+1.42}_{-0.11} $ 100.83/95
UGC01214 X,N 3 . 61 0.16 + 0.20 $ 3.61^{+0.20}_{-0.16} $ 9 . 61 1.01 + 0.91 $ 9.61^{+0.91}_{-1.01} $ 0 . 88 0.09 + 0.10 $ 0.88^{+0.10}_{-0.09} $ 1 . 58 0.58 + 0.60 $ 1.58^{+0.60}_{-0.58} $ 2 . 33 0.22 + 0.31 $ 2.33^{+0.31}_{-0.22} $ - > 345 90(f) 30(f) 16 . 46 7.91 + 21.70 $ 16.46^{+21.70}_{-7.91} $ 85.17/72
2MASXJ04405494-0822221 X,N - - 0 . 38 0.12 + 0.33 $ 0.38^{+0.33}_{-0.12} $ 0.22 0.14 + 0.18 $ ^{+0.18}_{-0.14} $ 2 . 17 0.21 + 0.20 $ 2.17^{+0.20}_{-0.21} $ - > 298 90(f) 30(f) 18.57 6.90 + 11.21 $ ^{+11.21}_{-6.90} $ 80.91/58
IC4769 X - - 0.75 0.10 + 0.10 $ ^{+0.10}_{-0.10} $ 0.38 0.11 + 0.11 $ ^{+0.11}_{-0.11} $ 2 . 01 0.32 + 0.34 $ 2.01^{+0.34}_{-0.32} $ - > 142 90(f) 30(f) 5.12 2.97 + 6.47 $ ^{+6.47}_{-2.97} $ 71.42/55
IC4995 X,N 5.53 1.62 + 3.15 $ ^{+3.15}_{-1.62} $ 0.81 0.69 + 1.41 $ ^{+1.41}_{-0.69} $ 0.79 0.14 + 0.16 $ ^{+0.16}_{-0.14} $ 0.73 0.42 + 0.44 $ ^{+0.44}_{-0.42} $ 2.38 0.11 + 0.27 $ ^{+0.27}_{-0.11} $ - > 363 90(f) 30(f) 36 . 6 11.53 + 28.17 $ 36.6^{+28.17}_{-11.53} $ 86.72/53

Notes.(1)X:XMM-Newton data have been used , C: Chandra data have been used, N: NuSTAR data have been used

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