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Table 1.

Physical parameters of the mergers.

Minor
Major
Source z1 z2 Δv rp μ[CII] μK FWHM re S/N FWHM re S/N
[km s−1] [kpc] [km s−1] [kpc] [km s−1] [kpc]
(1) (2) (3) (4) (5) (6) (7) (8) (9) (10) (11) (12) (13)
CG_38 5.5731 5.5698 152.3 2.7 1.8 96.9 1.4 3.8 165.9 2.0 3.9
DC_308643 4.5238 4.5221 92.3 3.0 1.2 85.4 1.0 4.5 85.6 1.4 5.3
DC_372292 5.1345 5.1374 144.0 1.8 2.7 2.9 82.8 2.2 4.1 157.9 3.7 5.7
DC_378903 5.4311 5.4293 94.5 0.9 1.9 70.0 4.4 (*) 3.6 111.2 1.3 4.2
DC_417567 5.6676 5.6700 106.7 5.3 2.1 84.8 1.0 3.1 163.9 4.0 3.4
DC_422677 4.4361 4.4378 92.8 0.0 1.4 95.7 1.0 4.7 93.1 0.5 6.7
DC_434239 4.4914 4.4876 206.1 5.5 6.9 103.5 3.9 4.5 441.8 3.4 7.2
DC_493583 4.5122 4.5141 103.4 1.0 4.7 64.8 3.3 3.6 139.5 1.0 8.0
DC_519281 5.5731 5.5765 158.0 0.9 4.5 95.7 0.9 3.1 163.8 2.3 8.3
DC_536534 5.6834 5.6886 234.6 4.4 2.7 113.9 1.9 3.6 228.5 2.6 4.9
DC_665509 4.5244 4.5261 95.9 1.0 2.0 70.5 4.5 (*) 3.0 107.0 2.4 4.0
DC_680104 4.5288 4.5308 106.4 0.0 1.0 89.5 0.5 3.7 111.6 8.7 (*) 4.7
DC_773957 5.6802 5.6770 141.2 3.0 1.6 5.6 118.0 1.3 5.9 179.5 1.7 6.2
DC_814483 4.5823 4.5796 145.5 7.9 2.4 128.1 1.1 3.3 192.7 2.8 4.2
DC_818760 4.5626 4.5609 92.3 9.9 1.3 2.6 127.1 2.4 10.4 271.0 2.9 18.3
DC_834764 4.5076 4.5055 119.0 1.0 1.7 96.2 1.4 (*) 5.1 143.8 3.1 5.8
DC_842313 4.5547 4.5406 751.5 11.6 32.9 1.5 229.9 4.3 (*) 5.1 1089.7 1.7 5.9
DC_859732 4.5353 4.5315 205.2 4.9 3.9 55.4 1.7 (*) 3.0 176.4 3.3 (*) 3.7
DC_873321 5.1545 5.1544 4.5 6.5 1.2 3.1 171.2 1.3 4.9 219.3 2.8 7.6
vc_5100541407 4.5628 4.5628 1.9 13.8 1.6 1.4 203.8 4.4 (*) 3.5 166.5 1.2 6.9
vc_5100822662 4.5210 4.5205 22.3 10.9 1.6 1.7 189.6 4.0 5.1 192.7 2.0 8.0
vc_5101209780 4.5724 4.5684 217.3 10.8 4.1 2.5 126.1 2.3 4.4 303.9 6.6 7.4
vc_5180966608 4.5294 4.5293 8.9 7.2 3.0 3.7 243.6 1.8 3.4 231.6 4.3 10.9

Notes. The right side of the table shows the measurements of FWHM (in km s−1), [CII] emission size (in kpc), and S/N for both the minor and major components, intended as such in terms of their integrated [CII] fluxes. The asterisk near the size of some of the sources indicates a bad re estimate from the best-fit parameters of the 2D Gaussian fit on the moment-0 maps of the individual components.

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