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Table 1.

Basic CARS sample characteristics from the literature.

Target Other name (a) α (J2000) δ (J2000) z(b) MBJ f1.4 GHz(c) f0.1 − 2.4 keV(d) ICO(1 − 0)(e) IH I(f)
[h:m:s] [°:′:″] [mag] [mJy] [10−12 erg s−1 cm−2] [K km s−1] [Jy km s−1]
HE0021–1810 00:23:39.4 −17:53:54 0.0537 −20.44 40.0 ± 1.3 1.2 ± 0.2 < 0.1 ...
HE0021–1819 00:23:55.4 −18:02:51 0.0533 −20.18 < 2.5 1.0 ± 0.1 0.4 ± 0.0 < 2.0
HE0040−1105 RBS101 00:42:36.9 −10:49:22 0.0419 −19.38 < 2.5 7.4 ± 0.8 1.0 ± 0.1 < 1.6
HE0045−2145 MCG-04-03-014 00:47:41.2 −21:29:28 0.0214 −20.09 8.0 ± 0.5 ... 8.2 ± 0.2 3.3 ± 0.1
HE0108−4743 RBS162 01:11:09.7 −47:27:37 0.0239 −19.92 < 2.5 6.2 ± 0.6 2.2 ± 0.1 ...
HE0114−0015 RBS175 01:17:03.6 00:00:27 0.0458 −20.29 1.3 ± 0.1 3.7 ± 0.4 0.9 ± 0.1 < 1.8
HE0119−0118 Mrk1503 01:21:59.8 −01:02:24 0.0548 −21.35 4.2 ± 0.5 7.8 ± 1.1 2.4 ± 0.1 < 1.4
HE0150−0344 01:53:01.5 −03:29:23 0.0480 −20.02 3.2 ± 0.5 ... 0.9 ± 0.1 2.7 ± 0.3
HE0203−0031 Mrk1018 02:06:16.0 −00:17:29 0.0425 −21.59 4.2 ± 0.4 3.6 ± 0.3 < 0.2 ...
HE0212−0059 Mrk590 02:14:33.6 −00:46:00 0.0264 −21.17 16.2 ± 0.6 25.5 ± 0.8 3.5 ± 0.1 2.0 ± 0.2
HE0224−2834 AM0224-283 02:26:25.9 −28:21:01 0.0602 −20.84 2.6 ± 0.5 0.8 ± 0.3 0.7 ± 0.1 2.6 ± 0.3
HE0227−0913 Mrk1044 02:30:05.5 −08:59:53 0.0165 −19.86 2.4 ± 0.5 83.4 ± 3.4 1.9 ± 0.2 2.6 ± 0.2
HE0232−0900 NGC985 02:34:37.8 −08:47:15 0.0427 −22.04 15.3 ± 1.0 38.7 ± 2.1 6.9 ± 0.3 3.3 ± 0.4
HE0253−1641 02:56:02.6 −16:29:15 0.0319 −20.09 14.2 ± 1.0 2.6 ± 0.6 2.9 ± 0.1 < 2.6
HE0345+0056 03:47:40.2 01:05:14 0.0310 −21.26 32.0 ± 1.0 1.9 ± 0.8 < 0.1 ...
HE0351+0240 RBS489 03:54:09.5 02:49:31 0.0354 −19.09 3.7 ± 0.5 4.1 ± 0.4 < 0.2 ...
HE0412−0803 04:14:52.7 −07:55:40 0.0380 −20.69 8.9 ± 0.5 2.7 ± 0.2 < 0.1 ...
HE0429−0247 RBS550 04:31:37.1 −02:41:24 0.0423 −19.49 < 2.5 29.0 ± 3.1 < 0.3 ...
HE0433−1028 Mrk618 04:36:22.2 −10:22:34 0.0355 −20.76 17.0 ± 0.7 61.9 ± 4.2 9.4 ± 0.3 < 2.2
HE0853−0126 08:56:17.8 −01:38:08 0.0596 −20.85 2.5 ± 0.5 18.4 ± 2.9 1.3 ± 0.1 < 1.0
HE0853+0102 08:55:54.2 00:51:11 0.0527 −20.32 0.9 ± 0.2 ... < 0.2 ...
HE0934+0119 Mrk707 09:37:01.0 01:05:43 0.0507 −20.70 < 2.5 14.5 ± 1.1 < 0.1 ...
HE0949−0122 Mrk1239 09:52:19.2 −01:36:43 0.0197 −20.12 62.2 ± 1.9 1.5 ± 0.4 1.2 ± 0.1 5.9 ± 0.5
HE1011−0403 PG1011-040 10:14:20.6 −04:18:40 0.0587 −22.26 < 2.5 0.1 ± 0.0 1.4 ± 0.1 < 0.6
HE1017−0305 Mrk1253 10:19:32.9 −03:20:14 0.0491 −20.80 < 2.5 5.4 ± 0.6 1.2 ± 0.1 < 1.2
HE1029−1831 10:31:57.4 −18:46:34 0.0405 −20.99 10.3 ± 0.6 5.6 ± 0.9 4.2 ± 0.2 1.1 ± 0.1
HE1107−0813 11:09:48.5 −08:30:15 0.0585 −21.44 7.3 ± 1.2 ... 0.8 ± 0.1 < 1.0
HE1108−2813 ESO438-9 11:10:48.0 −28:30:04 0.0240 −20.88 15.2 ± 0.6 2.9 ± 0.3 8.3 ± 0.3 < 0.5
HE1126−0407 PG1126-041 11:29:16.6 −04:24:08 0.0605 −22.69 1.2 ± 0.1 ... 1.5 ± 0.1 < 1.8
HE1237−0504 NGC4593 12:39:39.4 −05:20:39 0.0083 −19.16 4.4 ± 0.5 40.5 ± 2.0 7.5 ± 0.6 7.5 ± 0.4
HE1248−1356 IC3834 12:51:32.4 −14:13:17 0.0145 −16.99 2.9 ± 0.6 ... 3.0 ± 0.2 0.8 ± 0.0
HE1310−1051 PG1310-109 13:13:05.8 −11:07:42 0.0343 −20.29 < 2.5 4.1 ± 0.4 < 0.2 ...
HE1330−1013 MCG-02-35-001 13:32:39.1 −10:28:53 0.0225 −19.30 < 2.5 119.0 ± 10.7 1.8 ± 0.2 1.8 ± 0.3
HE1338−1423 RBS1303 13:41:13.0 −14:38:41 0.0413 −21.32 5.3 ± 0.6 33.2 ± 3.1 < 0.1 ...
HE1353−1917 ES O578-9 13:56:36.7 −19:31:45 0.0348 −19.36 12.6 ± 0.6 2.9 ± 0.7 3.2 ± 0.2 < 2.4
HE1417−0909 14:20:06.2 −09:23:14 0.0437 −20.06 < 2.5 2.2 ± 0.3 < 0.1 ...
HE2128−0221 21:30:49.9 −02:08:15 0.0527 −19.76 < 2.5 7.2 ± 1.7 < 0.1 ...
HE2211−3903 ESO344-16 22:14:42.0 −38:48:23 0.0397 −20.62 3.5 ± 0.6 16.9 ± 1.4 1.9 ± 0.1 ...
HE2222−0026 22:24:35.3 −00:11:04 0.0581 −19.97 < 2.5 ... 0.2 ± 0.0 < 1.2
HE2233+0124 22:35:42.0 01:39:33 0.0567 −20.67 < 2.5 1.6 ± 0.5 0.9 ± 0.1 < 2.9
HE2302−0857 Mrk926 23:04:43.4 −08:41:09 0.0470 −20.91 32.6 ± 1.1 30.9 ± 1.3 2.3 ± 0.2 1.9 ± 0.2

Notes.

(a)

Most common alternative target identifier for targets if available.

(b)

Accurate systemic redshift of the host galaxies based on the stellar continuum in our observed IFU data.

(c)

Flux density at 1.4GHz as measured by the NRAO VLA sky survey (NVSS) and the VLA FIRST survey if undetected in NVSS. For non-detection we assume the completeness limit of NVSS at 2.5 mJy as the upper limit for the source.

(d)

Soft X-ray flux as seen by ROSAT.

(e)

CO(1-0) line fluxes and upper limits for non-detection as reported in Bertram et al. (2007).

(f)

H I line fluxes and upper limits for non-detection as reported in König et al. (2009).

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