arXiv:2004.11175 [astro-ph.GA]AbstractReferencesReviewsResources
Differences and similarities of stellar populations in LAEs and LBGs at $z\sim$ 3.4 - 6.8
P. Arrabal Haro, J. M. Rodríguez Espinosa, C. Muñoz-Tuñón, D. Sobral, A. Lumbreras-Calle, M. Boquien, A. Hernán-Caballero, L. Rodríguez-Muñoz, B. Alcalde Pampliega
Published 2020-04-23Version 1
The differences between the inherent stellar populations (SPs) of LAEs and LBGs are a key factor in understanding early galaxy formation and evolution. We have run a set of SP burst-like models for a sample of 1,558 sources at $3.4<z<6.8$ from the Survey for High-$z$ Absorption Red and Dead Sources (SHARDS) over the GOODS-N field. This work focuses on the differences between the three different observational subfamilies of our sample: LAE-LBGs, no-Ly$\alpha$ LBGs and pure LAEs. Single and double SP synthetic spectra were used to model the SEDs, adopting a Bayesian information criterion to analyse under which situations a second SP is required. We find that the sources are well modelled using a single SP in $\sim79\%$ of the cases. The best models suggest that pure LAEs are typically young low mass galaxies ($t\sim26^{+41}_{-25}$ Myr; $M_{\mathrm{star}}\sim5.6^{+12.0}_{-5.5}\times10^{8}\ M_{\odot}$), undergoing one of their first bursts of star formation. On the other hand, no-Ly$\alpha$ LBGs require older SPs ($t\sim71\pm12$ Myr), and they are substantially more massive ($M_{\mathrm{star}}\sim3.5\pm1.1\times10^{9}\ M_{\odot}$). LAE-LBGs appear as the subgroup that more frequently needs the addition of a second SP, representing an old and massive galaxy caught in a strong recent star-forming episode. The relative number of sources found from each subfamily at each $z$ supports an evolutionary scenario from pure LAEs and single SP LAE-LBGs to more massive LBGs. Stellar Mass Functions are also derived, finding an increase of $M^{*}$ with cosmic time and a possible steepening of the low mass slope from $z\sim6$ to $z\sim5$ with no significant change to $z\sim4$. Additionally, we have derived the SFR-$M_{\mathrm{star}}$ relation, finding a $\mathrm{SFR}\propto M_{\mathrm{star}}^{\beta}$ behaviour with negligible evolution from $z\sim4$ to $z\sim6$.