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Table 3.

IR fractions.

No. Galaxy in system % Ref.
(1) (2) (3)
47 CGCG 436−030 (W) 100 5
52 NGC 6670 (W) 62 1
53 UGC 02369 (S) 98 2
56 NGC 5331 (S) 81 1
57 IRAS F06076−2139 (N) 88 2
60 IC 2810 (NW) 68 1
63 IRAS 18090+0130 (E) 81 1
64 III Zw 035 (N) 100 5
67 IRAS F16399−0937 (N) 90 3
69 IC 4687 (N,S)* 66,22 1
75 NGC 6090 (NE) 90 4
79 NGC 5256 (SW) 63 2
80 IRAS F03359+1523 (E) 100 5
81 ESO 550−IG025 (N) 59 1
83 MCG+12−02−001 (E,W)* 90,10 2
95 ESO 440−IG058 (S) 89 1
104 NGC 7771 90 1
105 NGC 7592 (E,S)* 63,0 2
106 NGC 6286 87 1
107 NGC 4922 (N) 99 2
110 NGC 3110 (NE) 91 1
117 MCG+08−18−013 (E) 97 1
127 MCG−03−34−064 75 1
141 IC 0564 54 1
157 MCG−02−33−098/9 (W) 69 2
163 NGC 4418 99 1
169 ESO 343−IG013 (N) 78 2
179 NGC 7591 94 1
194 ESO 432−IG006 (SW) 63 1
196 NGC 7753 64 1

Notes. Column (1): Name of the galaxy (galaxies) that emits most of the IR luminosity in a double (triple) system. Column (2): Percentage of IR emission originating in the dominant component. Column (3): Reference from which the contribution to the IR luminosity is derived. 1: Derived from Herschel data (as in Chu et al. 2017). 2: Derived from MIPS 24 data (as in Díaz-Santos et al. 2010). 3: MIR determination from Haan et al. (2011). 4: Predicted IR emission from radio continuum in Hattori et al. (2004). 5: We refer to the notes on individual objects in Appendix A.

(*)

Triple-component galaxy.

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