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Table 1.

CO properties of the 66 CO-ARC sample sources.

Galaxy Line Beam size σrms SCOΔv FWHM vres log(MH2) log()
(“×”) (mJy/beam) (Jy km s−1) ( km s−1) ( km s−1) (M⊙) (K km s−1 pc2)
J1000–3139 CO(2–1) 0.97 × 0.71 0.40 18.38 ± 0.59 368.53 20.00 7.85 ± 6.87 7.21 ± 6.22
J1109–3732 CO(2–1) 0.6 × 0.5 0.46 6.93 ± 0.35 452.27 20.00 7.56 ± 6.61 6.92 ± 5.97
J1336–3357 CO(2–1) 0.63 × 0.57 0.34 1.89 ± 0.29 781.79 20.00 7.17 ± 6.33 6.52 ± 5.68
J1723–6500 CO(2–1) 0.27 × 0.19 0.24 93.80 ± 2.15 533.90 20.00 8.98 ± 7.98 8.34 ± 7.34
J1945–5520 CO(1–0) 1.8 × 1.6 2.20 < 17.99 300.00 100.00 < 8.91 < 8.28
J0057+3021 CO(2–1) 0.5 × 0.32 0.18 13.52 ± 0.20 582.32 20.00 8.27 ± 7.29 7.63 ± 6.64
J1301–3226 CO(2–1) 0.68 × 0.65 0.31 < 5.15 300.00 100.00 < 7.87 < 7.22
J2131–3837 CO(2–1) 0.67 × 0.61 0.51 1.08 ± 0.18 540.65 20.00 7.27 ± 6.56 6.62 ± 5.92
J1407–2701 CO(2–1) 0.69 × 0.59 0.32 3.75 ± 0.50 147.77 20.00 7.96 ± 7.00 7.31 ± 6.35
J2009–4849 CO(2–1) 0.64 × 0.58 0.40 6.17 ± 1.03 448.41 22.00 9.20 ± 8.26 8.56 ± 7.61
J1008+0029 CO(1–0) 2.21 × 1.95 0.64 < 0.74 300.00 100.00 < 9.16 < 8.52
J1221+2813 CO(1–0) 2.14 × 1.39 0.07 < 0.11 300.00 180.00 < 8.40 < 7.76
J0623–6436 CO(1–0) 0.79 × 0.6 0.28 4.68 ± 0.91 671.67 100.00 10.21 ± 9.33 9.57 ± 8.69
J1217+3007 CO(1–0) 2.56 × 1.51 0.23 < 0.21 300.00 100.00 < 8.88 < 8.24
J1427+2348 CO(1–0) 1.78 × 1.32 0.27 < 0.28 300.00 100.00 < 9.18 < 8.55
J1332+0200 CO(1–0) 2.74 × 2.24 0.75 < 0.39 300.00 100.00 < 9.59 < 8.95
J1356–3421 CO(1–0) 1.1 × 0.88 0.28 < 0.34 300.00 100.00 < 9.56 < 8.93
J0943–0819 CO(1–0) 4.78 × 2.19 0.69 < 0.36 300.00 100.00 < 9.60 < 8.96
J1220+0203 CO(1–0) 0.34 × 0.26 0.36 < 1.39 300.00 102.00 < 10.24 < 9.60
J1547+2052 CO(1–0) 0.23 × 0.21 0.58 < 2.83 300.00 100.00 < 10.63 < 9.99
J2341+0018 CO(1–0) 0.7 × 0.57 0.55 4.16 ± 0.56 350.00 20.00 10.84 ± 9.93 10.20 ± 9.29
J1305–1033 CO(1–0) 0.47 × 0.42 0.14 0.67 ± 0.17 173.67 100.00 10.06 ± 9.25 9.42 ± 8.61
J0242–2132 CO(1–0) 0.74 × 0.63 0.30 < 0.41 300.00 100.00 < 9.95 < 9.31
J0006–0623 CO(1–0) 2.27 × 1.3 44.60 < 23.17 300.00 100.00 < 11.79 < 11.15
J1505+0326 CO(3–2) 0.81 × 0.44 0.81 3.28 ± 0.26 376.56 20.00 10.15 ± 9.31 9.50 ± 8.66
J0748+2400 CO(3–2) 1.22 × 0.99 0.61 < 0.44 300.00 100.00 < 9.28 < 8.63
J0510+1800 CO(3–2) 0.65 × 0.46 0.41 < 0.26 300.00 20.00 < 9.07 < 8.42
J2349+0534 CO(3–2) 7.77 × 5.09 3.13 < 1.63 300.00 100.00 < 9.87 < 9.22
J2141–3729 CO(3–2) 1.4 × 1.04 0.96 0.73 ± 0.24 255.50 20.00 9.53 ± 8.99 8.88 ± 8.34
J0914+0245 CO(3–2) 0.05 × 0.04 0.16 < 3.34 300.00 100.00 < 10.20 < 9.55
J1038+0512 CO(2–1) 2.26 × 1.94 0.95 < 0.49 300.00 100.00 < 9.80 < 9.16
J0940+2603 CO(3–2) 0.11 × 0.09 0.68 < 3.58 300.00 60.00 < 10.37 < 9.71
J1610–3958 CO(3–2) 1.02 × 0.81 0.53 < 0.41 300.00 100.00 < 9.46 < 8.80
J2239–5701 CO(3–2) 6.96 × 5.44 5.18 < 2.69 300.00 100.00 < 10.36 < 9.71
J1058–8003 CO(3–2) 1.66 × 1.09 0.89 < 0.46 300.00 100.00 < 9.61 < 8.96
J0106–4034 CO(4–3) 7.07 × 3.59 7.73 < 4.02 300.00 100.00 < 10.36 < 9.66
J0217–0820 CO(2–1) 1.91 × 1.46 0.58 < 0.30 300.00 100.00 < 9.81 < 9.17
J2320+0513 CO(2–1) 1.2 × 1.19 0.48 < 0.25 300.00 100.00 < 9.76 < 9.12
J2000–1748 CO(2–1) 0.4 × 0.27 0.36 < 0.68 300.00 100.00 < 10.23 < 9.59
J1010–0200 CO(4–3) 1.17 × 0.74 0.63 < 0.37 300.00 100.00 < 9.70 < 9.00
J0329–2357 CO(4–3) 0.43 × 0.33 0.54 < 0.80 300.00 100.00 < 10.03 < 9.33
J0946+1017 CO(2–1) 0.39 × 0.34 1.98 < 2.92 300.00 100.00 < 11.24 < 10.59
J0909+0121 CO(2–1) 0.71 × 0.66 1.12 < 0.89 300.00 100.00 < 10.74 < 10.09
J1351–2912 CO(2–1) 2.32 × 1.87 0.38 < 0.20 300.00 100.00 < 10.10 < 9.45
J1743–0350 CO(4–3) 0.72 × 0.55 0.06 2.26 ± 0.04 145.99 80.00 10.62 ± 9.65 9.92 ± 8.95
J0125–0005 CO(2–1) 3.26 × 2.52 0.42 < 0.21 300.00 90.00 < 10.15 < 9.51
J0239–0234 CO(4–3) 0.4 × 0.32 0.47 < 0.70 300.00 100.00 < 10.16 < 9.46
J0837+2454 CO(2–1) 0.9 × 0.79 0.66 < 0.42 300.00 100.00 < 10.49 < 9.84
J0118–2141 CO(4–3) 0.6 × 0.53 0.77 < 0.72 300.00 100.00 < 10.21 < 9.51
J0112–6634 CO(2–1) 0.54 × 0.47 0.61 < 0.64 300.00 100.00 < 10.72 < 10.08
J1304–0346 CO(2–1) 0.71 × 0.65 0.31 < 0.23 300.00 100.00 < 10.33 < 9.68
J2134–0153 CO(2–1) 1.52 × 1.25 0.47 < 0.24 300.00 100.00 < 10.37 < 9.72
J1359+0159 CO(2–1) 0.7 × 0.55 0.31 < 0.26 300.00 100.00 < 10.41 < 9.77
J0529–7245 CO(2–1) 2.38 × 2.16 0.89 < 0.21 300.00 20.00 < 10.33 < 9.69
J1147–0724 CO(4–3) 0.55 × 0.37 0.58 < 0.66 300.00 100.00 < 10.29 < 9.59
J0343–2530 CO(2–1) 1.47 × 1.19 0.38 < 0.19 300.00 100.00 < 10.35 < 9.71
J1419+0628 CO(3–2) 0.39 × 0.3 0.17 0.98 ± 0.18 410.76 100.00 10.72 ± 9.95 10.07 ± 9.30
J0954+1743 CO(4–3) 0.87 × 0.78 0.46 0.58 ± 0.09 193.30 20.00 10.31 ± 9.61 9.61 ± 8.91
J2056–4714 CO(2–1) 2.23 × 1.77 0.23 < 0.12 300.00 100.00 < 10.18 < 9.54
J1520+2016 CO(3–2) 0.47 × 0.32 0.13 < 0.17 300.00 100.00 < 10.03 < 9.38
J1107–4449 CO(2–1) 0.97 × 0.8 0.91 4.98 ± 0.15 43.74 20.00 11.86 ± 10.90 11.21 ± 10.26
J0219+0120 CO(2–1) 0.86 × 0.65 0.66 < 0.45 300.00 100.00 < 10.82 < 10.18
J1136–0330 CO(2–1) 2.49 × 2.19 0.55 < 0.29 300.00 100.00 < 10.64 < 10.00
J1146–2447 CO(4–3) 2.3 × 1.47 0.49 < 0.25 300.00 100.00 < 10.17 < 9.47
J0403+2600 CO(4–3) 0.06 × 0.04 0.11 < 1.07 300.00 100.00 < 10.86 < 10.16
J0106–2718 CO(3–2) 1.43 × 1.09 0.59 < 0.31 300.00 100.00 < 10.64 < 9.99

Notes. Note that, even for targets with available multiple-J CO observations, only the properties of lowest-J CO transitions are listed here and used for the luminosity function computations.

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