Dust properties of Lyman-break galaxies at z ∼ 3

Context. Since the mid-1990s, the sample of Lyman-break galaxies (LBGs) has been growing thanks to the increasing sensitivities in the optical and in near-infrared telescopes for objects at z > 2.5. However, the dust properties of the LBGs are poorly known because the samples are small and/or biased against far-infrared (far-IR) or submillimeter (submm) observations. Aims. This work explores from a statistical point of view the far-IR and submm properties of a large sample of LBGs at z similar to 3 that cannot be individually detected from current far-IR observations. Methods. We select a sample of 22, 000 LBGs at 2.5 < z < 3.5 in the COSMOS field using the dropout technique. The large number of galaxies included in the sample allows us to split it into several bins as a function of UV luminosity (L-FUV), UV continuum slope (beta(UV)), and stellar mass (M-*) to better sample their variety. We stack in PACS (100 and 160 mu m) images from PACS Evolution Probe survey (PEP), SPIRE (250, 350 and 500 mu m) images from the Herschel Multi-tied Extragalactic Survey (HerMES) programs, and AzTEC (1.1 mm) images from the Atacama Submillimeter Telescope Experiment (ASTE). Our stacking procedure corrects the biases induced by galaxy clustering and incompleteness of our input catalogue in dense regions. Results. We obtain the full infrared spectral energy distributions (SED) of subsamples of LBGs and derive the mean IR luminosity as a function of L-FUV, beta(UV), and M-*. The average IRX (or dust attenuation) is roughly constant over the L-FUV range, with a mean of 7.9 (1.8 mag). However, it is correlated with beta(UV), A(FUV) = (3.15 +/- 0.12) + (1.47 +/- 0.14) beta(UV), and stellar mass, log (IRX) = (0.84 +/- 0.11) log (M-*/10(10.35)) + 1.17 +/- 0.05. We investigate using a statistically controlled stacking analysis as a function of (M-*, beta(UV)), the dispersion of the IRX-beta(UV) and IRX-M-* plane. On the one hand, the dust attenuation shows a departure of up to 2.8 mag above the mean IRX-beta(UV) relation when log(M-* [M-circle dot]) increases from 9.75 to 11.5 in the same beta(UV) bin. This strongly suggests that M-* plays an important role in shaping the IRX-beta(UV) plane. On the other hand, the IRX-M-* plane is less dispersed for variation in the beta(UV). However, the dust attenuation shows a departure of up to 1.3 mag above the mean IRX-M-* relation, when beta(UV) increases from 1.7 to 0.5 in the same M-* bin. The low stellar mass LBGs (log(M-* [M-circle dot]) < 10.5) and red beta(UV) (beta(UV) > -0.7), 15% of the total sample, present a high dust attenuation than the mean IRX-M-*, but they are still in agreement with the mean IRX-beta(UV) relation. We suggest that we have to combine both the IRX-beta(UV) and IRX-M-* relations to obtain the best estimation of the dust attenuation from the UV and NIR properties of the galaxies (L-FUV, beta(UV), M-*). Our results enable us to study the average relation between star formation rate (SFR) and stellar mass, and we show that our LBG sample lies on the main sequence of star formation at z similar to 3. we demonstrate that the SFR is underestimate for LBGs with high stellar mass, but it give a good estimation for LBGs with lower stellar mass when we calculate the SFR by correcting the L-FUV using the IRX-beta(UV) relation.