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Table 3.

Main properties of the [O III] fits from the nuclear spectra of the QSO2s.

ID Line FWHM vs Flux ×10−15
[O III] [km s−1] [km s−1] [erg cm−2 s−1]
J1010 (n) 238 ± 10 61 ± 3 3.45 ± 0.23
λc = 5499.5 Å (n) 175 ± 6 −153 ± 6 1.35 ± 0.08
(i) 892 ± 30  − 21 ± 2 16.70 ± 0.71
(b) 2164 ± 80  − 55 ± 7 14.19 ± 1.73

J1100 (n) 429 ± 1 0 ± 1 54.62 ± 0.22
λc = 5510.0 Å (n) 420 594 ± 2 5.77 ± 0.07
(i) 664 ± 5 −366 ± 3 18.66 ± 0.31
(b) 2241 ± 13  − 40 ± 2 32.74 ± 0.83

J1356 (n) 226 ± 1 0 ± 1 15.46 ± 0.10
λc = 5627.3 Å (n) 250 ± 4  − 281 ± 3 3.31 ± 0.05
(i) 338 ± 5 280 ± 2 8.00 ± 0.14
(i) 483 ± 5  − 351 ± 2 12.03 ± 0.16
(b) 1325 ± 25  − 85 ± 4 11.50 ± 0.47

J1430 (n) 151 ± 5 97 ± 2 6.97 ± 0.24
λc = 5433.4 Å (n) 181 ± 6  − 102 ± 3 6.70 ± 0.22
(i) 590 ± 7 26 ± 2 46.59 ± 1.06
(b) 1296 ± 23  − 98 ± 8 25.58 ± 2.06

J1509 (n) 458 ± 4 0 ± 1 5.10 ± 0.06
λc = 5558.9 Å (b) 1536 ± 7 −431 ± 1 9.57 ± 0.11

Notes. Column description: (1) object ID followed by the observed wavelength of [O III] (λc); (2) kinematic component: narrow (n), intermediate (i) or broad (b); (3) FWHM corrected from instrumental broadening; (4) velocity shifts (vs) measured from λc; (5) integrated line flux. Measurements without errors correspond to parameters that have been fixed.

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