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Table 1.

Main properties of the targets observed with VLT/MUSE.

Target RA Dec Redshift FMP Gaia Sep. J G1 G2 Spectrum Texp Observation
(″) source (min:s) date
J0007+0053 00:07:10.02 +00:53:29.0 0.318 12 0.792 15.99 17.68 19.34 SDSS (1) 19:06 11/20/22
J0015–2526 ( * ) 00:15:43.93 −25:26:17.7 0.969 62 15.27 16.27 NTT (2) 19:06 12/20/22
J0052–3045 ( * ) 00:52:37.98 −30:45:52.2 1.462 44 17.63 19.78 2QZ (3) 26:42 12/24/22
J0128–0444 01:28:37.44 −04:44:01.5 1.631 15 17.72 20.42 SDSS1 34:20 08/20/22
J0402–3237 04:02:15.06 −32:37:33.4 1.280 16 0.661 17.19 19.47 20.63 Lemon (4) 27:12 10/19/22
J0525–4153 05:25:35.88 −41:53:46.1 2.155 26 16.95 18.17 Gaia (5) 26:42 12/29/22
J0545–2236 05:45:09.38 −22:36:33.5 2.488 21 0.554 17.31 19.51 20.11 Gaia (5) 26:42 01/15/23
J0840–0529 08:40:04.14 −05:29:11.1 1.393 55 17.01 18.34 Gaia (5) 26:42 01/25/23
J1059+0622( * ) 10:59:26.44 +06:22:27.1 2.199 27 0.592 15.98 17.47 17.95 SDSS (1) 19:06 01/27/23
J2139–4331 21:39:57.14 −43:31:01.7 0.485 10 0.666 16.36 18.57 18.68 NTT2 19:06 11/20/22
J2211–0009 22:11:11.00 −00:09:53.4 0.667 24 17.17 19.26 SDSS (1) 34:20 07/03/22
J2228–3047 22:28:49.43 −30:47:34.5 1.948 28 16.87 18.19 2QZ (3) 34:20 08/21/22

Notes. Separations (in case of multiple objects), G-band magnitude of the primary component (G1), G-band magnitude of the secondary component (G2, in case of multiple objects), and FMP are extracted from the Gaia catalog; J-band are derived from Gaia Bp and Rp photometry, as is described in the appendix. Redshift is obtained from spatially unresolved spectra whose origin is reported in the table. Texp is the total exposure time of the MUSE observations. ( * )Targets on which we applied the decomposition method described in Sect. 2.1. (1): Lyke et al. (2020); (2): our observations at ESO/NTT (Program ID:109.22W4); (3): Croom et al. (2009); (4): Lemon et al. (2020); (5): Gaia quasars candidate catalog, Gaia Collaboration (2023).

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