Table C.1.
Outflow and AGN properties of galaxies with molecular outflows
Galaxy | z | Vout | Ṁout | log(LAGN) | F1.4GHz | log(Pjet) |
---|---|---|---|---|---|---|
km s−1 | M⊙ yr−1 | erg s−1 | Jy | erg s−1 | ||
NGC1377 | 0.00578 | 110 | 5 | 42.93 | < 0.0015 1 | < 42.46 |
NGC1068 | 0.00379 | 150 | 28 | 43.94 | 4.85 2 | 43.56 |
4C12.50 | 0.1217 | 800 3 | 652 3 | 45.7 | 5.14 | 44.62 * |
NGC1433 | 0.0036 | 100 | 0.7 | 42.24 | 0.0034 5 | 42.45 |
Mrk231 | 0.04217 | 700 | 350 | 45.72 | 0.314 | ... |
IC5063 | 0.011 | 300 | 10 | 44.3 | 1.87 2 | 43.74 |
M51 | 0.002 | 100 | 11 | 43.79 | 1.4 6 | 43.17 ** |
Mrk1014 | 0.16311 | 268 | 93 | 45.29 | 0.0225 1 | 43.84 |
NGC1266 | 0.00719 | 177 | 11 | 43.31 | 0.115 4 | 43.18 |
NGC5643 | 0.003999 | 500 | 85 | 42.91 | 0.2037 | 42.96 |
IRASF08572+3915 | 0.04311 | 800 | 403 | 45.72 | 0.0049 1 | ... |
IRASF10565+2448 | 0.189 | 450 | 100 | 44.81 | 0.0576 1 | ... |
IRASF11119+3257 | 0.06438 | 1000 | 203 | 46.2 | 0.106 8 | 43.77 |
IRASF23365+3604 | 0.02448 | 450 | 57 | 44.67 | 0.0287 4 | ... |
NGC6240 | 0.123 | 400 | 267 | 45.38 | 0.4272 | ... |
SDSSJ1356+1026 | 0.04256 | 500 | 118 | 46 | 0.499 | ... |
IRAS05189-2524 | 0.007268 | 491 | 219 | 44.47 | 0.0291 1 | ... |
NGC4418 | 0.06764 | 134 | 19 | 43.81 | 0.04144 | ... |
IRASF14378-3651 | 0.030761 | 425 | 180 | 45.12 | 0.0349 1 | ... |
IRAS13120-5453 | 0.08257 | 549 | 1115 | 44.35 | 0.065 2 | ... |
IRASF14348-1447 | 0.04295 | 450 | 420 | 44.59 | 0.018 1011 | ... |
NGC613 | 0.00495 | 300 12 | 19 12 | 42.6 13 | 0.223 2 | 43.18 |
ESO420-613 | 0.01205 | 379 14 | 14 14 | 44.0 14 | 0.1 14 | 43.25 |
PKS1549-79 | 0.15 | 600 15 | 1733 15 | 44.7 25 | 5.36 16 | 44.69 |
3C273 | 0.15834 | 245 24 | 439 24 | 46.06 26 | 55 1 | 45.06 *** |
HE1353-1917 | 0.03502 | 145 17 | 22 17 | 43.42 18 | 0.0128 1 | |
NGC6764 | 0.00807 | 170 | 1 | 42.23 | 0.113 19 | 43.15 |
Circinus | 0.0014 | 150 | 1 | 43.57 | 1.2 2 | 42.89 |
Mrk273 | 0.03777 | 620 | 200 | 44.16 | 0.145 1 | 43.62 |
NGC3256S | 0.00926 | 140021 | 19 21 | 42.04 20 | 0.0168 **** | 42.97 |
NGC3100 | 0.0088 | 200 22 | 0.12 22 | 42.78 22 | 0.5 23 | 43 22 |
NGC6328 | 0.014 | 150 | 3.1 | 42.11 | 0.32 | 42.35 |
Notes. are from Allison et al. (2014), unless otherwise indicated. For 4C12.50, properties are presented for the nuclear outflow component, as the extended components add little to the energetics (Fotopoulou et al. 2019). Likewise, the infrared luminosity fraction of the southern nucleus comes from resolved SF rates (Lira et al. 2002). The radio power, Pjet, (for the sources with a certain radio jet detection) is calculated as in Bîrzan et al. (2008) after the subtraction of the starburst contribution, as indicated in the text. Alternative radio power (Pjet) computations are as follows:
43.96 for the synchrotron radiation (Fotopoulou et al. 2019),
39.3 for the X-ray cavity (Urquhart et al. 2018), and
an averaged value of 43.86 Punsly & Kharb (2016).
To find the 1.4GHz flux fraction assigned to the southern nucleus of this galaxy merger, we used the information from spatially resolved 5 GHz data (Neff et al. 2003).
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