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Table 4

Fits results of the average spectrum of the full sample and subsamples using gsmooth ⊗  [pha × (pex+laor)+gaus)] .

Sample /ν χ2/ν 1 − Pν,Δχ2) N H Γ Re l refl E W rel E W na /ν E W one−rel
1022 cm-2 eV eV eV
(0) (1) (2) (3) (4) (5) (6) (7) (8) (9) (10)

Full 87.0/94 82.6/93 3.6 × 10-2(2.1σ) 0.24 ± 0.24 1.61 ± 0.06 140 ± 120 67 ± 28 98.4/94 347 ± 105
Unabs 108.7/94 108.7/93 1(0σ) <0.82 1.87 ± 0.03 138.9/94
Abs 94.2/94 92.6/93 0.2(1.3σ) 2.84 ± 0.60 1.29 ± 0.08 404 ± 140 <1000 92.6/94 404 ± 140
z < 1 97.0/94 95.2/93 0.2(1.3σ) 0.68 ± 0.40 1.55 ± 0.09 173 ± 173 104 ± 93 99.7/94 362 ± 210
z ≥ 1 78.5/94 77.6/93 0.3(1σ) <0.3 1.58 ± 0.04 84 ± 84 94.6/94 318 ± 119
Sey 93.9/94 92.2/93 0.2(1.3σ) 1.57 ± 0.07 118 ± 118 107.6/94 380 ± 130
QSO 178.2/94 166.7/93 7 × 10-4(3.4σ) <0.138 1.58 ± 0.08 228 ± 70 49 ± 45 169.7/94 316 ± 82

Notes. In all fits we have fixed Ri ≡ 6, β ≡ −2, θ ≡ 30. Columns: (0) sample; (1) χ2/d.o.f. of the fit with the Gaussian with Efixed − σfixed only, repeated from Table 3 for reference; (2) χ2/d.o.f. with the two-component model (see text); (3) Significance of the laor (expressed in 1 − Pν,Δχ2) and in σ); (4) intrinsic column density of the neutral absorber. (5) powerlaw slope. (6) reflection factor; (7) laor EW measured from the two-component model; (8) EW of the narrow component; (9) χ2/d.o.f. of the fit after having fixed the flux of the narrow line component to zero; (10) laor EW measured from the same fit of Col. 9.

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