Table C.3.
Candidates spectroscopically confirmed to not be high-z quasars
| Rejected | RA | Dec | Telescope | Date | CLASS | Rejected | RA | Dec | Telescope | Date | CLASS |
|---|---|---|---|---|---|---|---|---|---|---|---|
| Candidate | (J2000) | (J2000) | Instrument | Candidate | (J2000) | (J2000) | Instrument | ||||
| (1) | (2) | (3) | (4) | (5) | (6) | (7) | (8) | (9) | (10) | (11) | (12) |
| ILT J0010+3239g | 02.5364 | +32.6504 | LBT/MODS | 2023/11/11 | 1 | PSO J003−03 | 03.0822 | −03.7675 | LBT/MODS | 2023/11/12 | 1 |
| PSO J008+04 | 08.3993 | +04.9334 | LBT/MODS | 2023/11/13 | 1 | PSO J010+46 | 10.0308 | +46.4924 | LBT/MODS | 2023/11/12 | 3 |
| PSO J012+36 | 12.0151 | +36.5762 | LBT/MODS | 2023/11/13 | 1 | PSO J027−45a | 27.9230 | −45.5284 | NTT/EFOSC2 | 2024/01/24 | 1 |
| ILT J0157+3042 | 29.3863 | +30.7092 | LBT/MODS | 2023/11/13 | 2 | PSO J039+04 | 39.9339 | +04.4616 | LBT/MODS | 2023/11/13 | 3 |
| MALS J0240+1719 | 40.0717 | +17.3222 | LBT/MODS | 2024/12/05 | 1 | YS J041−29b | 41.1159 | −29.0798 | NTT/EFOSC2 | 2022/12/27 | 3 |
| PSO J047−60 | 47.0409 | −60.8559 | NTT/EFOSC2 | 2024/01/27 | 1 | YS J049−34b | 49.9160 | −34.3035 | NTT/EFOSC2 | 2022/12/27 | 1 |
| PSO J060+03 | 60.2691 | +03.9825 | NTT/EFOSC2 | 2023/12/01 | 3 | YS J066−28b | 66.5230 | −28.7629 | NTT/EFOSC2 | 2023/11/29 | 2 |
| PSO J069−26 | 69.6370 | −26.8314 | NTT/EFOSC2 | 2023/12/02 | 1 | PSO J099+57 | 99.7872 | +57.5060 | LBT/MODS | 2023/11/12 | 1 |
| PSO J117−69 | 117.2528 | −69.6421 | NTT/EFOSC2 | 2024/01/24 | 1 | PSO J112+33 | 112.1840 | +33.2182 | LBT/MODS | 2020/12/25 | 1 |
| PSO J139−04a | 139.7676 | −04.2978 | NTT/EFOSC2 | 2024/01/24 | 1 | PSO J145−27 | 145.5390 | −27.2683 | NTT/EFOSC2 | 2024/01/25 | 1 |
| PSO J153+47 | 153.3546 | +47.6594 | LBT/MODS | 2023/04/19 | 1 | PSO J155+23 | 155.3345 | +23.3206 | LBT/MODS | 2023/04/01 | 1 |
| MALS J1044−1412 | 161.0521 | −14.2127 | NTT/EFOSC2 | 2024/01/24 | 2 | PSO J162−12 | 162.3426 | −12.6113 | NTT/EFOSC2 | 2022/02/04 | 1 |
| NVSS J163−02 | 163.6297 | −02.0645 | NTT/EFOSC2 | 2022/02/04 | 3 | PSO J170−28 | 170.6294 | −28.7200 | NTT/EFOSC2 | 2022/02/05 | 1 |
| PSO J172+16 | 172.0984 | +16.0280 | NTT/EFOSC2 | 2022/02/04 | 1 | ILT J1140+4202 | 175.0467 | +42.0335 | LBT/MODS | 2023/06/13 | 3 |
| PSO J181+30 | 181.2624 | +30.4606 | LBT/MODS | 2023/06/10 | 1 | PSO J182−29 | 182.2378 | −29.9385 | NTT/EFOSC2 | 2022/02/05 | 1 |
| PSO J182−05 | 182.3792 | −05.2293 | LBT/MODS | 2023/06/10 | 1 | PSO J182+11 | 182.7458 | +11.1742 | LBT/MODS | 2023/04/01 | 3 |
| PSO J182+83 | 182.7718 | +83.6176 | LBT/MODS | 2023/03/05 | 1 | PSO J184+64 | 184.1091 | +64.8172 | LBT/MODS | 2023/06/08 | 1 |
| PSO J186+80 | 186.1962 | +80.4875 | LBT/MODS | 2023/04/20 | 1 | PSO J186+60 | 186.2609 | +60.5096 | LBT/MODS | 2023/06/08 | 1 |
| PSO J187+08 | 187.1222 | +08.6590 | LBT/MODS | 2023/06/10 | 1 | MQC J1239+1617 | 189.8990 | +16.2973 | NTT/EFOSC2 | 2024/01/24 | 1 |
| PSO J195−07 | 195.3068 | −07.2171 | NTT/EFOSC2 | 2022/02/04 | 1 | PSO J195+86 | 195.6339 | +86.8951 | LBT/MODS | 2023/04/01 | 1 |
| PSO J195−10 | 195.6990 | −10.0122 | LBT/MODS | 2023/06/10 | 3 | RACS J198+40 | 198.7974 | +40.1505 | LBT/MODS | 2023/06/10 | 2 |
| ILT J1326+5429c | 201.5518 | +54.4944 | LBT/MODS | 2023/06/08 | 1 | RACS J206+40 | 206.9889 | +40.3283 | LBT/MODS | 2023/06/10 | 2 |
| ILT J1407+4252 | 211.9176 | +42.8708 | LBT/MODS | 2023/06/07 | 2 | ILT J1431+4635 | 217.8540 | +46.5862 | LBT/MODS | 2023/06/07 | 1 |
| PSO J222+05 | 222.3130 | +05.7496 | LBT/MODS | 2023/03/28 | 1 | NVSS J225−11 | 225.2889 | −11.9584 | NTT/EFOSC2 | 2022/02/04 | 2 |
| ILT J1504+6258 | 226.1189 | +62.9802 | LBT/MODS | 2023/06/13 | 1 | PSO J227−17 | 227.0505 | −17.3678 | LBT/MODS | 2023/04/01 | 1 |
| PSO J233+05 | 233.2398 | +05.4933 | LBT/MODS | 2023/06/08 | 1 | PSO J234−09 | 234.5534 | −09.4578 | LBT/MODS | 2023/04/21 | 1 |
| RACS J234+40 | 234.6786 | +40.4477 | LBT/MODS | 2023/06/10 | 1 | PSO J245+18 | 245.1485 | +18.6299 | LBT/MODS | 2023/06/08 | 1 |
| ILT J1623+5427 | 245.8994 | +54.4526 | LBT/MODS | 2023/06/13 | 3 | ILT J1629+4156 | 247.4075 | +41.9488 | LBT/MODS | 2023/06/08 | 3 |
| PSO J247+10 | 247.8238 | +10.2805 | LBT/MODS | 2023/06/09 | 3 | PSO J250+00 | 250.5826 | +00.9124 | LBT/MODS | 2023/04/21 | 1 |
| PSO J253+00 | 253.1887 | +00.5648 | LBT/MODS | 2023/06/08 | 3 | PSO J253+07 | 253.5664 | +07.4414 | LBT/MODS | 2023/06/08 | 1 |
| PSO254+25 | 254.7461 | +25.6797 | LBT/MODS | 2023/04/18 | 1 | PSO J262+20 | 262.6972 | +20.9801 | LBT/MODS | 2023/06/08 | 1 |
| PSO J266+54 | 266.5850 | +54.9565 | LBT/MODS | 2023/06/09 | 1 | PSO J269+19 | 269.8055 | +19.6993 | LBT/MODS | 2023/06/10 | 1 |
| RACS J279+40 | 279.1253 | +40.6443 | LBT/MODS | 2023/06/13 | 1 | PSO J281+58 | 281.8065 | +58.8070 | LBT/MODS | 2020/06/06 | 1 |
| PSO J290+58 | 290.3967 | +58.9075 | LBT/MODS | 2023/06/08 | 1 | PSO J331−09 | 331.9305 | −09.3771 | LBT/MODS | 2023/05/28 | 1 |
| PSO J333+29 | 333.0793 | +29.2715 | LBT/MODS | 2022/10/20 | 1 | PSO J350+18 | 350.3733 | +18.8181 | LBT/MODS | 2023/11/11 | 1 |
| PSO J351+07 | 351.4983 | +07.0055 | LBT/MODS | 2023/11/13 | 1 | PSO J353−20 | 353.0240 | −20.3663 | LBT/MODS | 2023/11/12 | 1 |
| PSO J359+28 | 359.2352 | +28.8194 | LBT/MODS | 2023/11/12 | 1 |
Notes. Rejected candidates sorted by R.A. Col (1) and Col (7): Object name; sources named ILT have been selected from the LOFAR LoTSS DR2 catalog (Shimwell et al. 2022); RACS objects are from the RACS 888 MHz radio catalog (McConnell et al. 2020); sources named NVSS have been selected from the NVSS catalog of Condon et al. (1998)); MQC objects have been selected from the Million Quasar Catalog v8 of Flesch (2023); sources named MALS were selected from the MeerKAT Absorption Line Survey DR1 catalog (Deka et al. 2024);
candidates in the Yang & Shen (2023) catalog with pqso large than 99%;
candidate already rejected by Gloudemans et al. (2022);
Col (2), Col (3), Col (8) and Col (9): Coordinates in degrees; Col (4) and Col (10): instrument and telescope used for the spectroscopic follow-up; Col (5) and Col (11): dates of the observation; Col (6) and Col (12): Spectroscopic class: 1=brown dwarf, 2=low-z galaxy, 3 = unknown.
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