Table 1: Description of the distant LIRGs sample. The technique used to compute the equivalent widths of H$\delta $, H8, H9, H10 and the 4000 Å break (D4000) is described in Sect. 2.3. $L_{\rm IR}$ and SFR$_{\rm IR}$ were derived using the Chary & Elbaz (2001) technique.

Object		 RA Dec z H8 H $\delta _{\rm A}$ D4000 $F_{\nu}^{15~\mu{\rm m}}$ $F_{\nu}^{24~\mu{\rm m}}$ log( $\frac{L_{\rm IR}}{L_{\odot}}$) SFR$_{\rm IR}$
Slit (J2000) (J2000)         $\mu$Jy $\mu$Jy   $M_{\odot }$ yr-1
(1) (2) (3) (4) (5) (6) (7) (8) (9) (10) (11)
UDSR08 3 14 55.20 -55 20 31.0 0.7291 3.8 $\pm$ 0.5 4.2  $\pm$ 0.9 1.11 $\pm$ 0.02 236 $\pm$ 75 - 11.44 $\pm$ 0.24 46.7
UDSR09 3 14 56.10 -55 20 08.0 0.3884 1.4 $\pm$ 0.4 - 1.74 $\pm$ 0.03 609 $\pm$ 87 - 11.20 $\pm$ 0.08 27.2
UDSR10 3 14 43.90 -55 21 35.0 0.6798 4.3 $\pm$ 0.6 8.4 $\pm$ 0.7 1.25 $\pm$ 0.03 495 $\pm$ 91 - 11.78 $\pm$ 0.13 102.9
UDSR14 3 14 43.30 -55 20 11.0 0.8150 4.7 $\pm$ 0.4 3.9 $\pm$ 0.4 1.15 $\pm$ 0.02 200 $\pm$ 69 - 11.48 $\pm$ 0.27 52.0
UDSR20 3 14 41.10 -55 18 40.0 0.7660 6.9 $\pm$ 0.5 6.5 $\pm$ 0.8 1.19 $\pm$ 0.02 214 $\pm$ 72 - 11.44 $\pm$ 0.25 47.0
UDSR23 3 14 32.10 -55 19 02.0 0.7094 4.9 $\pm$ 0.4 4.7 $\pm$ 0.3 1.15 $\pm$ 0.02 271 $\pm$ 80 - 11.48 $\pm$ 0.22 51.8
UDSF06 3 13 30.20 -55 04 04.0 0.6928 4.3 $\pm$ 1.3 - 1.27 $\pm$ 0.06 150 $\pm$ 75 180 $\pm$ 22 11.09 $\pm$ 0.49 21.0
UDSF07 3 13 17.30 -55 05 16.0 0.7014 3.6 $\pm$ 0.9 4.2 $\pm$ 0.7 1.17 $\pm$ 0.04 154 $\pm$ 32 198 $\pm$ 27 11.12 $\pm$ 0.15 22.6
UDSF12 3 13 07.70 -55 05 26.0 0.7388 7.6 $\pm$ 0.9 - 1.29 $\pm$ 0.06 331 $\pm$ 58 420 $\pm$ 30 11.64 $\pm$ 0.11 74.7
UDSF16 3 13 08.0 -55 04 18.0 0.4548 - 3.7 $\pm$ 0.6 1.25 $\pm$ 0.01 138 $\pm$ 29 205 $\pm$ 26 10.55 $\pm$ 0.11 6.0
UDSF17 3 13 08.60 -55 03 57.0 0.8100 6.2 $\pm$ 0.3 6.7 $\pm$ 0.4 1.22 $\pm$ 0.02 257 $\pm$ 47 343 $\pm$ 23 11.62 $\pm$ 0.12 72.0
UDSF18 3 13 16.5 -55 02 27.0 0.4620 - 4.7 $\pm$ 0.8 1.17 $\pm$ 0.01 170 $\pm$ 44 - 10.68 $\pm$ 0.10 8.2
UDSF19 3 13 09.80 -55 03 08.0 0.5476 4.8 $\pm$ 1.0 3.9 $\pm$ 1.2 1.32 $\pm$ 0.05 611 $\pm$ 90 778 $\pm$ 40 11.62 $\pm$ 0.09 71.4
UDSF28 3 12 51.80 -55 02 57.0 0.6612 2.9 $\pm$ 0.6 -- 1.47 $\pm$ 0.04 321 $\pm$ 35 861 $\pm$ 37 11.49 $\pm$ 0.06 53.1
UDSF29 3 12 50.20 -55 02 59.0 0.6619 4.1 $\pm$ 1.3 -- 1.37 $\pm$ 0.06 354 $\pm$ 66 568 $\pm$ 28 11.54 $\pm$ 0.11 59.6
UDSF20 3 13 19.00 -55 01 42.0 0.8424 2.8 $\pm$ 0.7 - 1.33 $\pm$ 0.04 117 $\pm$ 25 248 $\pm$ 21 11.19 $\pm$ 0.16 26.7
UDSF31 3 12 44.00 -55 03 21.0 0.6868 4.5 $\pm$ 1.1 5.6 $\pm$ 1.1 1.44 $\pm$ 0.06 193 $\pm$ 38 174 $\pm$ 28 11.24 $\pm$ 0.14 29.9

CFRS02

 3 02 52.01 +00 10 33.0 0.6172 6.9 $\pm$ 1.0 5.9 $\pm$ 1.2 1.30 $\pm$ 0.10 582 $\pm$ 114 - 11.75 $\pm$ 0.12 95.8
CFRS06 3 02 49.08 +00 10  1.8 0.6169 3.8 $\pm$ 0.4 5.0 $\pm$ 0.3 1.21 $\pm$ 0.02 370 $\pm$ 95 - 11.50 $\pm$ 0.17 53.5
CFRS08 3 02 46.29 +00 13 53.6 0.7154 4.0 $\pm$ 0.3 5.9 $\pm$ 0.9 1.24 $\pm$ 0.03 360 $\pm$ 95 - 11.65 $\pm$ 0.17 75.7
CFRS10 3 02 44.57 +00 12 20.1 0.5276 5.6 $\pm$ 0.6 5.9 $\pm$ 1.2 1.03 $\pm$ 0.04 220 $\pm$ 95 - 11.01 $\pm$ 0.40 17.7
CFRS11 3 02 42.31 +00 12 9.5 0.6895 - 2.5 $\pm$ 0.7 1.15 $\pm$ 0.04 425 $\pm$ 110 - 11.70 $\pm$ 0.16 85.4
CFRS14 3 02 40.44 +00 14  3.8 0.4652 4.6 $\pm$ 0.5 6.5 $\pm$ 0.5 1.10 $\pm$ 0.02 172 $\pm$ 117 - 10.69 $\pm$ 0.58 8.4
CFRS16 3 02 38.80 +00 14 17.5 0.8274 3.3 $\pm$ 1.0 - 1.30 $\pm$ 0.05 444 $\pm$ 100 - 11.99 $\pm$ 0.15 166.7
CFRS29 3 02 29.41 +00 12 59.8 0.8804 7.3 $\pm$ 1.4 - 1.13 $\pm$ 0.05 370 $\pm$ 103 - 11.98 $\pm$ 0.20 163.6


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