The clustering of H$β$+[OIII] and [OII] emitters since $z \sim 5$: dependencies with line luminosity and stellar mass (1705.01101v1)
Abstract: We investigate the clustering properties of $\sim 7000$ H$\beta$+[OIII] and [OII] narrowband-selected emitters at $z \sim 0.8 - 4.7$ from the High-$z$ Emission Line Survey. We find clustering lengths, $r_0$, of $1.5 - 4.0h{-1}$ Mpc and minimum dark matter halo masses of $10{10.7 - 12.1}\rm{M}\odot$ for our $z = 0.8 - 3.2$ H$\beta$+[OIII] emitters and $r_0 \sim 2.0 - 8.3h{-1}$ Mpc and halo masses of $10{11.5 - 12.6}\rm{M}\odot$ for our $z = 1.5 - 4.7$ [OII] emitters. We find $r_0$ to strongly increase both with increasing line luminosity and redshift. By taking into account the evolution of the characteristic line luminosity, $L\star(z)$, and using our model predictions of halo mass given $r_0$, we find a strong, redshift-independent increasing trend between $L/L\star(z)$ and minimum halo mass. The faintest H$\beta$+[OIII] emitters are found to reside in $10{9.5}\rm{M}_\odot$ halos and the brightest emitters in $10{13.0}\rm{M}_\odot$ halos. For [OII] emitters, the faintest emitters are found in $10{10.5} \rm{M}\odot$ halos and the brightest emitters in $10{12.6}\rm{M}\odot$ halos. A redshift-independent stellar mass dependency is also observed where the halo mass increases from $10{11}\rm{M}_\odot$ to $10{12.5} \rm{M}\odot$ for stellar masses of $10{8.5}\rm{M}\odot$ to $10{11.5}\rm{M}_\odot$, respectively. We investigate the interdependencies of these trends by repeating our analysis in a $L_\textrm{line} - \rm{M}\textrm{star}$ grid space for our most populated samples (H$\beta$+[OIII] $z = 0.84$ and [OII] $z = 1.47$) and find that the line luminosity dependency is stronger than the stellar mass dependency on halo mass. For $L > L\star$ emitters at all epochs, we find a relatively flat trend with halo masses of $10{12.5 - 13}\rm{M}\odot$ which may be due to quenching mechanisms in massive halos which is consistent with a transitional halo mass predicted by models.
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