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Table 2.

Observational parameters derived from the optical spectra.

Source S/N [O III] χrange2 FWHM(Hβ) FWHM(Hβb) σ F(Hβ) F(Hβb) Fcont FSDSS R4570 A(V)
(1) (2) (3) (4) (5) (6) (7) (8) (9) (10) (11) (12)
J1029 12 −2/+1 2132 2320 2856 1.39 1.38 2.74 4.85 1.34
J1228 65 −3/+2 971 1360 1807 1.97 1.88 13.96 14.66 2.81 3.590
J1232 33 −2/+1 1518 1700 1631 8.14 8.01 17.67 15.95 1.58 1.826
J1509 26 −2/+1 1744 1861 2193 2.20 2.18 5.77 8.19 1.06 3.067
J1510 14 −3/+2 1031 1193 2307 1.99 1.87 8.09 12.97 2.37 3.764
J1522 42 −2/+1 886 1181 1.34 1.13 17.48 33.87 3.285
J1641 25 −1/+1 1140 4050 1767 0.90 0.79 10.48 21.23 2.58

Notes. Columns: (1) Source name; (2) S/N measured in the 5100 Å continuum; (3) values multiplied to the FWHMs of [O III]λλ4959,5007 for the χ2 calculation; (4) FWHM of the Hβ profile [km s−1]; (5) FWHM of the Hβ broad component [km s−1]; (6) square root of the second-order moment as in Eq. (1) [km s−1]; (7) Hβ flux [×10−15 erg s−1 cm−2]; (8) Hβ broad flux [× − 10−15 erg s−1 cm−2]; (9) flux density at 5100 Å [×10−17 erg s−1 cm−2 Å−1]; (10) flux density at 5100 Å on SDSS spectra [×10−17 erg s−1 cm−2 Å−1]; (11) flux ratio between Fe IIλ4570 multiplets and Hβ; (12) internal extinction as in Eq. (2).

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