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Table 2

Integrated star-forming properties of the sample.

Object Reff L24 μm AV
(1) (2) (3) (4) (5) (6) (7) (8)

IRAS06206-6315 2.5 4.1 ± 0.6 11.0 ± 1.7 ··· 0.53 ± 0.08 1.42 ± 0.22 7.4 ± 2.2
NGC 2369 0.5 0.73 ± 0.11 4.9 ± 0.8 1.7 ± 0.3 2.0 ± 0.3 13.9 ± 2.1 21 ± 6
NGC 3110 1.9 2.4 ± 0.4 5.0 ± 0.8 2.4 ± 0.4 0.93 ± 0.14 2.0 ± 0.3 8 ± 2
NGC 3256 1.0 3.7 ± 0.6 6.7 ± 1.0 10.1 ± 1.5 3.0 ± 0.5 5.4 ± 0.8 6.6 ± 2.0
ESO320-G030 0.7 0.93 ± 0.14 1.58 ± 0.24 1.8 ± 0.3 1.7 ± 0.3 2.8 ± 0.4 6.1 ± 1.8
IRAS12112+0305 2.6 3.8 ± 0.6 11.0 ± 1.7 14.5 ± 0.5 0.46 ± 0.07 1.35 ± 0.20 8.0 ± 2.4
IRASF12115-4656 1.3 1.9 ± 0.3 5.1 ± 0.8 1.40 ± 0.05 0.87 ± 0.13 2.4 ± 0.4 11 ± 3
NGC 5135 0.5 1.35 ± 0.20 3.1 ± 0.5 3.2 ± 0.5 4.1 ± 0.6 9.4 ± 1.4 9 ± 2
IRAS14348-1447 3.8 7.8 ± 1.2 18 ± 3 20.2 ± 0.7 0.44 ± 0.07 1.06 ± 0.16 6.5 ± 2.0
IRASF17138-1017 0.6 1.7 ± 0.3 3.3 ± 0.5 3.60 ± 0.09 4.5 ± 0.7 8.9 ± 1.3 7.6 ± 2.3
IRAS17208-0014 0.9 4.9 ± 0.7 13.2 ± 2.0 15.2 ± 0.4 5.1 ± 0.8 13.7 ± 2.1 7.3 ± 2.2
IC 4687 1.1 4.4 ± 0.7 8.3 ± 1.3 3.7 ± 0.6 3.1 ± 0.5 5.8 ± 0.9 7.2 ± 2.2
IRAS21130-4446 1.6 3.9 ± 0.6 8.3 ± 1.3 ··· 1.23 ± 0.19 2.6 ± 0.4 5.7 ± 1.8
NGC 7130 1.0 1.62 ± 0.25 5.4 ± 0.8 3.3 ± 0.5 1.24 ± 0.19 4.1 ± 0.6 13 ± 4
IC5179 1.6 1.7 ± 0.3 3.2 ± 0.5 1.56 ± 0.23 0.66 ± 0.10 1.25 ± 0.19 7.2 ± 2.2
IRAS22491-1808 1.7 2.3 ± 0.4 5.6 ± 0.9 17.7 ± 0.4 0.65 ± 0.10 1.56 ± 0.24 6.6 ± 2.0
IRAS23128-5919 2.0 11.6 ± 1.7 30 ± 4 18.6 ± 0.5 2.4 ± 0.4 6.3 ± 0.9 7.2 ± 2.2

Notes. Integrated star-forming properties of the sample. Column (2): Hα effective radius in [kpc] from Arribas et al. (2012). Columns (3) and (4): observed (3) and extinction-corrected (4) Paα luminosities measured within Reff, expressed in [×107L]. The Paα luminosities for the LIRGs are obtained from the Brγ fluxes using the case B recombination factor at T = 10 000 K and ne = 104 cm-3 (Osterbrock & Ferland 2006). Column (5): Spitzer/MIPS 24 μm luminosities from Pereira-Santaella et al. (2011) and archival data, in units of [×1010L]. Columns (6) and (7): Observed (6) and extinction-corrected (7) ΣSFR in [M yr-1 kpc-2]. Column (8): AV in magnitudes. All the uncertainties are calculated by a bootstrap method of N = 300 simulations, added in quadrature to the 15% systematic error from the absolute flux calibration.

(†)

Due to the limited FoV of the observations, in these objects the Hα effective radius is greater than our FoV and the luminosities should be considered lower limits.

(‡)

Since the main nucleus of NGC 3256 was not observed, we centred the aperture in the centre of the FoV so the measurements might be inaccurate (see Paper I).

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