Table 1.
Target galaxies and their properties, ordered by increasing redshift.
| Source | RA & Dec | zs | zL | ![]() |
![]() |
FWHM CO(1−0) | μFIR |
|---|---|---|---|---|---|---|---|
| [J2000] | [1012 L⊙] | [1010 K km s−1 pc−2] | [km/s] | ||||
| SDP.9 | 09:07:40.0 –00:41:59.8 | 1.575 | 0.613 | 66 ± 1O17 | 13 ± 3O17 | 370 ± 10a | 8.8 ± 2.2B13 |
| SDP.11 | 09:10:43.1 –00:03:22.8 | 1.786 | 0.793 | 64 ± 1O17 | 13 ± 1O17 | 500 ± 100O17 | 10.9 ± 1.3B13 |
| G09v1.40 | 08:53:58.9 +01:55:37.7 | 2.092 | ?b | 66 ± 25Y17 | 30 ± 8Y17 | 310 ± 90Y17,c | 15.3 ± 3.5B13 |
| SDP.17 | 09:03:03.0 –01:41:27.1 | 2.305 | 0.23 | 71 ± 26Y17 | 26 ± 3H12 | 1000 ± 130H12 | 4.9 ± 0.7B13 |
| J1202 | 12:02:07.6 +53:34:39 | 2.442 | 0.21 | 81 ± 4H21 | 142 ± 50H21 | 600 ± 20d | 25.0H21,d |
| G15v2.235 | 14:13:52.1 –00:00:24.4 | 2.478 | 0.547 | 28 ± 7Y17 | 43 ± 5H12 | 500 ± 40H12 | 1.8 ± 0.3B13 |
| J0209 | 02:09:41.3 +00:15:59 | 2.553 | 0.20 | 133 ± 4H21 | 84 ± 11R | 410 ± 20e | 14.7 ± 0.3 |
| G09v1.326 | 09:18:40.9 +02:30:45.9 | 2.581 | – | 40 ± 5H12 | 33 ± 8H12 | 680 ± 140H12 | 1 |
| SDP.130 | 09:13:05.4 –00:53:41 | 2.625 | 0.22 | 32 ± 3B13 | 25 ± 4F11 | 360 ± 40F11 | 8.6 ± 0.4F18 |
| NAv1.195 | 13:26:30.2 +33:44:07.6 | 2.951 | 0.785 | 75 ± 20Y17 | 57 ± 20H21 | 266 ± 19H21 | 4.1 ± 0.3F18 |
| SDP.81 | 09:03:11.6 +00:39:07 | 3.042 | 0.299 | 43 ± 1R20 | 54 ± 9V11 | 435 ± 54V11 | 18.2 ± 1.2R20 |
| G12v2.43 | 11:35:26.3 –01:46:06.6 | 3.128 | ?b | 90 ± 2Y17 | 15 ± 3H12 | 350 ± 80H12 | 9.2 ± 3.2G23,f |
Notes. Individual columns list the source position, source and lens redshift (zS, zL), sky-plane (lensed) FIR and CO(1–0) luminosities, CO(1–0) FWHM and FIR continuum magnification. LFIR is inferred from modified black-body fits integrated over 8−1000 μm. For completeness, we also include SDP.81 from Paper II (Rybak et al. 2023).
– Mean magnification for ALMA Bands 6, 7, and 8 continuum (Giulietti et al. 2023).
References: B13 – Bussmann et al. (2013), F11 – Frayer et al. (2011), F17 – Falgarone et al. (2017), G23 – Giulietti et al. (2023), H12 – Harris et al. (2012), H21 – Harrington et al. (2021), I12 – Iono et al. (2012), O17 – Oteo et al. (2017), R – Riechers et al. (in prep.); R20 – Rybak et al. (2020), V11 – Valtchanov et al. (2011), Y17 – Yang et al. (2017).
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