Table 1.
Targeted quasar pair.
ID | SDSS name | RA | Dec | zsystemic(a) | zpeakLyα(b) | i(c) | M1450 | Radio flux (d) |
---|---|---|---|---|---|---|---|---|
(J2000) | (J2000) | SDSS (this work) | (mJy beam−1) | |||||
QSO1 | SDSS J113502.03−022110.9 | 11:35:02.030 | −02:21:10.93 | 3.020 ± 0.001 (3.019 ± 0.003) | 3.011 | 21.84 ± 0.02 | −23.44 | <0.44 |
QSO2 | SDSS J113502.50−022120.1 | 11:35:02.500 | −02:21:20.14 | 3.008 ± 0.001 (3.008 ± 0.003) | 3.003 | 22.15 ± 0.02 | −23.12 | <0.44 |
Notes.
Quasar systemic redshift from the SDSS catalog and, in brackets, from the peak of the [C III] complex (i.e., [C III] is a doublet 1906.7, 1908.7 Å; and [Si III]λ1892 could be blended), after correcting for the expected shift (Shen et al. 2016). The intrinsic uncertainty on this correction is ∼233 km s−1 and dominates the error budget (Δz ≈ 0.003).
i magnitude extracted from our data using the SDSS filter transmission curve and a circular aperture with a radius of 2″. The SDSS i magnitudes for the two quasars are iQSO1 = 21.50 ± 0.08 and iQSO2 = 22.05 ± 0.12.
3× rms at 1.4 GHz from the Very Large Array survey: Faint Images of the Radio Sky at Twenty-Centimeters (VLA FIRST; Becker et al. 1994).
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