Table 1.
Properties of the 20 Type 1 SUPER targets presented in this paper.
| Target | RA | Dec | zopt | log M* | SFR | log Lbol | log L[2 − 10 keV] | log NH | log MBH |
|---|---|---|---|---|---|---|---|---|---|
| (1) | (2) | (3) | (4) | (5) | (6) | (7) | (8) | (9) | |
| (h:m:s) | (d:m:s) | (M⊙) | (M⊙ yr−1) | (erg s−1) | (erg s−1) | (cm−2) | (M⊙) | ||
| X_N_160_22 | 02:04:53.81 | −06:04:07.82 | 2.445 | – | – | 46.74 ± 0.02 | 44.77 |
< 22.32 | 9.05 ± 0.30 |
| X_N_81_44 | 02:17:30.95 | −04:18:23.66 | 2.311 | 11.04 ± 0.37 | 229 ± 103 | 46.80 ± 0.03 | 44.77 |
< 21.86 | 9.02 ± 0.30 |
| X_N_53_3 | 02:20:29.84 | −02:56:23.41 | 2.434 | – | 686 ± 178 | 46.21 ± 0.03 | 44.80 |
22.77 |
8.51 ± 0.30 |
| X_N_66_23 | 02:22:33.64 | −05:49:02.73 | 2.386 | 10.96 ± 0.29 | < 268 | 46.04 ± 0.02 | 44.71 |
< 21.51 | 8.92 ± 0.30 |
| X_N_35_20 | 02:24:02.71 | −05:11:30.82 | 2.261 | – | – | 45.44 ± 0.02 | 44.00 |
< 22.27 | 8.38 ± 0.37 |
| X_N_12_26 | 02:25:50.09 | −03:06:41.16 | 2.471 | – | – | 46.52 ± 0.02 | 44.56 |
< 20.90 | 8.84 ± 0.30 |
| X_N_44_64 | 02:27:01.46 | −04:05:06.73 | 2.252 | 11.09 ± 0.25 | 229 ± 80 | 45.51 ± 0.07 | 44.21 |
< 21.97 | 8.74 ± 0.31 |
| X_N_4_48 | 02:27:44.63 | −03:42:05.46 | 2.317 | – | – | 46.16 ± 0.02 | 44.52 |
< 21.85 | 8.88 ± 0.31 |
| X_N_102_35 | 02:29:05.94 | −04:02:42.99 | 2.190 | – | – | 46.82 ± 0.02 | 45.37 |
< 22.17 | 8.82 ± 0.30 |
| X_N_115_23 | 02:30:05.66 | −05:08:14.10 | 2.342 | – | – | 46.49 ± 0.02 | 44.93 |
< 22.26 | 9.08 ± 0.30 |
| cid_166 | 09:58:58.68 | +02:01:39.22 | 2.448 | 10.38 ± 0.22 | < 224 | 46.93 ± 0.02 | 45.15 |
< 21.25 | 9.30 ± 0.30 |
| cid_1605 | 09:59:19.82 | +02:42:38.73 | 2.121 | – | < 94 | 46.03 ± 0.02 | 44.69 |
21.77 |
8.52 ± 0.31 |
| cid_346 | 09:59:43.41 | +02:07:07.44 | 2.219 | 11.01 ± 0.22 | 362 ± 49 | 46.66 ± 0.02 | 44.47 |
23.05 |
9.15 ± 0.30 |
| cid_1205 | 10:00:02.57 | +02:19:58.68 | 2.255 | 11.20 ± 0.10 | 384 ± 33 | 45.75 ± 0.17 | 44.25 |
23.50 ± 0.27 | 8.94 ± 0.31 |
| cid_467 | 10:00:24.48 | +02:06:19.76 | 2.288 | 10.10 ± 0.29 | < 147 | 46.53 ± 0.04 | 44.87 |
22.31 |
9.26 ± 0.31 |
| J1333+1649 | 13:33:35.79 | +16:49:03.96 | 2.089 | – | – | 47.91 ± 0.02 | 45.81 |
21.81 |
9.96 ± 0.30 |
| J1441+0454 | 14:41:05.54 | +04:54:54.96 | 2.059 | – | – | 47.55 ± 0.02 | 44.77 |
22.77 |
9.24 ± 0.30 |
| J1549+1245 | 15:49:38.73 | +12:45:09.20 | 2.365 | – | – | 47.73 ± 0.04 | 45.38 |
22.69 |
10.66 ± 0.30 |
| S82X1905 | 23:28:56.35 | −00:30:11.74 | 2.263 | – | – | 46.50 ± 0.02 | 44.91 |
22.95 |
8.87 ± 0.30 |
| S82X1940 | 23:29:40.28 | −00:17:51.68 | 2.351 | – | – | 46.03 ± 0.02 | 44.72 |
< 20.50 | 8.33 ± 0.30 |
| S82X2058 | 23:31:58.62 | −00:54:10.44 | 2.308 | – | – | 46.39 ± 0.02 | 44.67 |
< 20.50 | 9.09 ± 0.30 |
Notes. (1) and (2): Right ascension and declination of the optical counterpart of the target (J2000). (3): Spectroscopic redshift obtained from archival optical spectra. (4): Galaxy stellar mass obtained from SED fitting, wherever applicable. (5): Star formation rate derived from the far-infrared (8–1000 μm) luminosity. (6): AGN bolometric luminosity derived from SED fitting. (7): Hard-band (2–10 keV) X-ray luminosity corrected for absorption with a 90% confidence level error. (8): Absorbing hydrogen column density with 90% confidence limits. (9): Latest black hole mass estimates from the SINFONI data. All the error values (except NH) are 1σ uncertainties. Further details about the derivation of these properties is given in Circosta et al. (2018) and Vietri et al. (in prep.).
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