Table D.1.
Summary of the phenomenological final best-fitting continuum model parameters of each observation of the SUBWAYS sample
Baseline Model: Continuum parameters | |||||||||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
power-law | bbodylow | bbodyhigh | XABS | Stats | Cross-cal. | ||||||||||||
Source | XMM ObsID | Γ | norm | F4 − 10 keV, obs | kTlow | normlow | kThigh | normhigh | NH | log(ξ) | fcov | 𝒞pn/ζ | 𝒞mos1/ζ | 𝒞mos2/ζ | 𝒞tot/ν | MOS 1 | MOS 2 |
10−3 | 10−12 | eV | 10−5 | eV | 10−5 | 1021 cm−2 | erg cm s−1 | % | |||||||||
PG0052+251 | 0841480101 |
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125.7/102 | 124.4/119 | 127.0/127 | 377.1/335 |
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PG0953+414 | 0841480201 |
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100f | 109.7/106 | 109.7/114 | 152.5/120 | 371.8/324 |
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PG1626+554 | 0841480401 |
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100f | 79.0/90 | 125.2/115 | 115.1/120 | 320.1/311 |
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PG1202+281 | 0841480501 |
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92.1/108 | 112.6/118 | 127.0/124 | 331.8/333 |
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PG1435−067 | 0841480601 |
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– | – | – | 86.8/83 | 124.5/104 | 159.4/112 | 370.7/287 |
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SDSS J144414+0633⊞ | 0841480701 |
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– | – | – | 117.3/91 | 117.4/118 | 124.2/124 | 358.9/321 |
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2MASS J165315+2349† | 0841480801 |
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– | – | – | – | – | – | – | 74.2/82 | 83.2/100 | 105.7/107 | 263.1/273 |
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PG1216+069 | 0841480901 |
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100f | 83.2/89 | 122.4/114 | 141.8/121 | 347.4/311 |
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PG0947+396 (Obs 1) | 0841481001 |
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– | – | – | 96.8/82 | 102.0/100 | 108.2/109 | 307.0/277 |
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PG0947+396 (Obs 2) | 0841482301 |
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– | – | – | 81.1/84 | 112.5/107 | 99.7/112 | 293.2/293 |
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WISE J053756−0245 | 0841481101 |
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– | – |
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– | – | – | 96.1/86 | 121.8/109 | 121.1/114 | 339.0/301 |
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HB 891529+050 | 0841481301 |
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100f | 84.3/86 | 112.1/113 | 129.4/118 | 325.7/304 |
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PG1307+085 | 0841481401 |
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100f | 114.8/94 | 116.1/119 | 186.5/126 | 399.4/327 |
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PG1425+267 | 0841481501 |
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100f | 97.8/88 | 102.4/115 | 107.5/120 | 307.6/307 |
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PG1352+183 | 0841481601 |
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– | – | – | 119.9/88 | 128.8/115 | 112.9/119 | 361.7/311 |
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2MASS J105144+3539‡ | 0841481701 |
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– | – | – | – | – | – | – | 94.7/80 | 87.2/94 | 122.3/102 | 304.3/263 |
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2MASS J0220−0728 | 0841481901 |
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– | – |
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79.7/78 | 149.7/114 | 117.6/119 | 347.0/311 |
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LBQS 1338−0038 | 0841482101 |
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100f | 101.5/92 | 128.8/119 | 100.1/125 | 330.4/320 |
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PG0804+761 | 0102040401 |
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– | – | – | 88.8/92 | 137.6/112 | 131.1/112 | 357.6/302 |
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0605110101 |
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– | – | – | 116.2/106 | 153.0/121 | 131.9/126 | 401.0/333 |
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|
0605110201 |
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– | – | – | 129.9/103 | 133.6/124 | 139.6/120 | 403.0/30 |
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|
PG1416−129⋆ | 0203770201 |
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– | – |
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100f | 132.5/109 | 120.5/118 | 136.5/118 | 389.6/335 |
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PG1402+261 | 0400200101 |
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– | – | – | 94.7/99 | 90.0/106 | 117.2/108 | 301.9/301 |
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0830470101 |
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– | – | – | 122/104 | 136.4/116 | 107.0/121 | 365.3/329 |
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|
HB89 1257+286 | 0204040101 |
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117.2/98 | 121.7/119 | 137.5/120 | 376.4/322 |
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0204040201 |
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100f | 111.0/96 | 151.3/117 | 157.8/117 | 420.1/318 |
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|
0204040301 |
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85.4/96 | 165.7/119 | 130.7/119 | 381.8/319 |
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|
0304320201 |
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100f | 93.9/94 | 104.5/115 | 91.4/116 | 289.9/312 |
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|
0304320301 |
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– | – | – | 78.7/91 | 107.4/112 | 119.9/113 | 305.1/306 |
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|
0304320801 |
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– | – | – | 101.2/93 | 100.0/112 | 110.7/112 | 311.9/307 |
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|
PG1114+445 | 0109080801 |
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– | – |
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100f | 118.7/104 | 110.5/108 | 122.0/99 | 351.1/297 |
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0651330101 |
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– | – |
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100f | 88.0/95 | 92.8/97 | 107.5/101 | 288.3/278 |
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0651330301 |
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– | – |
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100f | 86.0/96 | 92.2/91 | 112.2/95 | 290.3/268 |
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0651330401 |
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– | – |
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100f | 113.1/96 | 103.1/96 | 106.4/106 | 323.1/288 |
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|
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0651330501 |
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– | – |
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100f | 95.0/96 | 115.8/97 | 127.4/101 | 338.2/286 |
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|
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0651330601 |
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– | – |
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100f | 112.0/98 | 135.3/106 | 122.3/109 | 369.7/300 |
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0651330701 |
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– | – |
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100f | 113.0/97 | 102.9/101 | 123.3/105 | 339.4/291 |
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0651330801 |
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– | – |
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100f | 85.6/96 | 83.8/100 | 134.6/104 | 304.0/288 |
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0651330901 |
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– | – |
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100f | 96.0/96 | 65.3/101 | 113.2/105 | 274.2/290 |
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0651331001 |
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– | – |
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100f | 92.4/95 | 91.1/98 | 78.7/103 | 262.2/284 |
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0651331101 |
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– | – |
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100f | 112.2/94 | 72.7/98 | 122.0/102 | 306.9/282 |
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|
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Notes. In the best-fit models the iron K emission and absorption lines, with their Gaussians model parameters are included and reported separately in Table 2. The 𝒩ℋℳ used in Sect. 4.4 consist of the best-fitting models reported here minus the Gaussian absorption components. Flux in the 4–10 keV band in units of (erg cm−2 s−1). Reduced 𝒞stat and number of degrees of freedom (ν) for the final best-fit model. All the WA components are required at PF > 99%. 𝒞−stat using the number of bins (ζ) in each EPIC detector and the total 𝒞−stat with the degree of freedoms (ν) corresponding to the final best-fit model. ⊞ A narrow (10 eV) Gaussian absorption line of rest-frame energy of E = 3.51 ± 0.06 keV was required at 3σ (99.7%) confidence level. † Seyfert 2 target with an intrinsic neutral absorber with column density of . The soft X-ray band < 2 keV was modelled with two thermal emission components with apec yielding
eV,
and
eV,
with normalisations in unit of
where DA is the angular diameter distance to the source in cm, ne and nH are the electron and H densities (cm−3), respectively. A narrow/strong Gaussian emission line of E = 2.35 ± 0.04 keV was required at 3.6σ (> 99.9%) confidence level. ‡ Intrinsic neutral absorber with
required at PF > 99.99% and two narrow soft X-ray emission at
keV and
keV both at PF > 99.99%.
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