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Table 1:

VIMOS LIRG sample: for each pointing, the total number of data points, mean value and standard deviation for the different line ratios and velocity dispersion are given.

Galaxy
$\log L_{\rm ir}^{(1)}$ D Scale [N II]$\lambda $6584/H$\alpha $ [S II] $\lambda \lambda $6717,6731/H$\alpha $ [O I]$\lambda $6300/H$\alpha $ $\sigma^{(2)} $ (km s-1)
(IRAS number) ($L_\odot$) (Mpc) (pc/ $^{\prime\prime}$) n $\overline x\pm\sigma (x)$ n $\overline x\pm\sigma (x)$ n $\overline x\pm\sigma (x)$ n $\overline x\pm\sigma (x)$
Class 0
F06295-1735 11.27 92.7 431 998 0.38 $\pm$ 0.07 486 0.31 $\pm$ 0.06 194 0.05 $\pm$ 0.04 1118 33 $\pm$ 11
F06592-6313 11.91 100.0 464 199 0.82 $\pm$ 0.32 ... ... ... ... 266 54 $\pm$ 33
F07027-6011 N 11.64 137.4 626 342 0.40 $\pm$ 0.09 94 0.30 $\pm$ 0.06 92 0.07 $\pm$ 0.04 387 32 $\pm$ 11
F07027-6011 S   137.4 626 163 0.61 $\pm$ 0.17 74 0.24 $\pm$ 0.05 49 0.03 $\pm$ 0.02 177 72 $\pm$ 17
F07160-6215 11.16 46.7 221 755 0.92 $\pm$ 0.61 189 0.33 $\pm$ 0.16 ... ... 888 69 $\pm$ 37
F10015-0614 11.77 73.1 343 1298 0.41 $\pm$ 0.10 850 0.31 $\pm$ 0.08 137 0.03 $\pm$ 0.01 1312 51 $\pm$ 13
F10409-4556 11.26 91.4 425 928 0.49 $\pm$ 0.25 ... ... ... ... 1083 39 $\pm$ 16
F10567-4310 11.07 74.6 350 1154 0.44 $\pm$ 0.15 270 0.25 $\pm$ 0.06 ... ... 1153 29 $\pm$ 11
F11255-4120 11.04 70.9 333 759 0.58 $\pm$ 0.28 173 0.28 $\pm$ 0.06 ... ... 782 33 $\pm$ 20
F11506-3851 11.30 46.6 221 887 0.67 $\pm$ 0.23 434 0.33 $\pm$ 0.13 327 0.04 $\pm$ 0.03 914 41 $\pm$ 14
F12115-4656 11.11 80.3 375 724 0.52 $\pm$ 0.18 462 0.31 $\pm$ 0.08 274 0.03 $\pm$ 0.02 847 41 $\pm$ 12
F13229-2934 11.29 59.3 280 865 1.21 $\pm$ 0.71 295 0.42 $\pm$ 0.19 146 0.07 $\pm$ 0.06 932 65 $\pm$ 24
F22132-3705 11.22 49.3 234 1706 0.41 $\pm$ 0.08 1490 0.29 $\pm$ 0.08 712 0.03 $\pm$ 0.02 1714 32 $\pm$ 8
Class 1
F01159-4443 11.48 99.8 462 558 0.45 $\pm$ 0.12 170 0.29 $\pm$ 0.06 97 0.07 $\pm$ 0.05 646 48 $\pm$ 20
ESO 297-G011 11.18 75.0 352 1339 0.45 $\pm$ 0.11 627 0.32 $\pm$ 0.08 109 0.03 $\pm$ 0.03 1404 32 $\pm$ 10
ESO 297-G012   75.0 352 223 0.54 $\pm$ 0.15 97 0.38 $\pm$ 0.10 80 0.10 $\pm$ 0.08 226 91 $\pm$ 31
F06076-2139 11.67 165.0 743 274 0.63 $\pm$ 0.45 ... ... ... ... 313 40 $\pm$ 25
F06259-4708 P1 11.91 171.1 769 443 0.48 $\pm$ 0.24 221 0.27 $\pm$ 0.10 149 0.04 $\pm$ 0.04 550 81 $\pm$ 40
F06259-4708 P2   171.1 769 279 0.30 $\pm$ 0.08 201 0.36 $\pm$ 0.11 163 0.06 $\pm$ 0.05 404 59 $\pm$ 20
08424-3130 11.04 70.1 329 241 0.80 $\pm$ 0.47 108 0.38 $\pm$ 0.15 56 0.05 $\pm$ 0.03 392 73 $\pm$ 32
F08520-6850 11.83 205.4 909 196 0.34 $\pm$ 0.10 103 0.39 $\pm$ 0.10 39 0.05 $\pm$ 0.03 318 72 $\pm$ 31
IC 563(3,4) 11.21 89.0 415 873 0.36 $\pm$ 0.08 491 0.33 $\pm$ 0.10 264 0.04 $\pm$ 0.02 1007 38 $\pm$ 9
IC 564 P1(3,4)   89.0 415 727 0.42 $\pm$ 0.12 163 0.35 $\pm$ 0.12 ... ... 843 33 $\pm$ 10
IC 564 P2 (3,4)   89.0 415 495 0.37 $\pm$ 0.08 77 0.27 $\pm$ 0.09 ... ... 635 36 $\pm$ 14
12042-3140 11.37 101.1 468 540 0.58 $\pm$ 0.23 246 0.33 $\pm$ 0.13 176 0.08 $\pm$ 0.06 611 85 $\pm$ 46
12596-1529 11.07 69.0 324 433 0.42 $\pm$ 0.13 226 0.41 $\pm$ 0.14 35 0.03 $\pm$ 0.02 487 64 $\pm$ 34
F14544-4255 E 11.11 68.2 320 322 0.45 $\pm$ 0.19 53 0.21 $\pm$ 0.06 ... ... 370 55 $\pm$ 15
F14544-4255 W   68.2 320 356 0.70 $\pm$ 0.26 165 0.68 $\pm$ 0.27 87 0.15 $\pm$ 0.09 392 66 $\pm$ 24
18093-5744 N 11.57 75.3 353 804 0.41 $\pm$ 0.12 528 0.36 $\pm$ 0.09 105 0.03 $\pm$ 0.02 886 46 $\pm$ 13
18093-5744 C   75.3 353 373 0.23 $\pm$ 0.07 204 0.23 $\pm$ 0.11 61 0.02 $\pm$ 0.01 634 80 $\pm$ 35
18093-5744 S   75.3 353 316 0.46 $\pm$ 0.10 185 0.33 $\pm$ 0.06 28 0.03 $\pm$ 0.02 359 47 $\pm$ 16
Class 2
F04315-0840 11.69 69.1 325 763 0.58 $\pm$ 0.24 398 0.42 $\pm$ 0.13 407 0.10 $\pm$ 0.08 759 66 $\pm$ 32
08355-4944 11.60 113.1 521 260 0.32 $\pm$ 0.07 121 0.25 $\pm$ 0.06 108 0.03 $\pm$ 0.02 347 59 $\pm$ 20
F10038-3338 11.77 149.9 679 172 0.60 $\pm$ 0.29 58 0.44 $\pm$ 0.18 42 0.13 $\pm$ 0.09 303 55 $\pm$ 28
10257-4338 11.69 40.4 192 1698 0.45 $\pm$ 0.11 1573 0.39 $\pm$ 0.13 1403 0.06 $\pm$ 0.05 1744 61 $\pm$ 19
12116-5615(3) 11.61 80.3 375 90 0.84 $\pm$ 0.29 33 0.34 $\pm$ 0.13 ... ... 114 70 $\pm$ 15
13001-2339(3) 11.48 94.5 439 320 0.78 $\pm$ 0.28 80 0.63 $\pm$ 0.16 96 0.21 $\pm$ 0.07 388 117 $\pm$ 54
17138-1017(3) 11.41 75.2 352 235 0.53 $\pm$ 0.15 87 0.38 $\pm$ 0.10 ... ... 257 63 $\pm$ 18
21453-3511 11.41 70.0 329 1112 0.61 $\pm$ 0.41 476 0.23 $\pm$ 0.11 63 0.04 $\pm$ 0.05 1136 43 $\pm$ 19

Notes. (1) Logarithm of the infrared luminosity, $L_{\rm ir} = L(8{-}1000~\mu$m), in units of solar bolometric luminosity, calculated using the fluxed in the four IRAS bands as given in Sanders et al. (2003), when available. Otherwise from the IRAS fluxes given in IRAS Point Source and Faint Source catalogs Moshir et al. (1990). When a system of more than one galaxy is observed using several VIMOS pointings, the infrared luminosity of the entire system is indicated in the data corresponding to the first galaxy of the system.
(2) Velocity dispersion derived from the H$\alpha $ line.
(3) Classification uncertain. Not used in the analysis of systems grouped by interaction class.
(4) Members of IRAS 09437+0317.


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