Figure 3.
Rest-frame absorption equivalent width ${W_{\rm r}(2796)}$ versus projected distance d for LRGs with sufficiently high S/N background QSO spectra for detecting Mg ii absorbers as weak as W0 = 0.3 Å. Absorption observations for passive LRGs are shown in the left-hand panel. Observations of [O ii]-emitting LRGs are shown in the right-hand panel. LRGs with detected Mg ii absorbers are shown in filled circles with error bars representing measurement uncertainties. For non-detections, we use light grey circles to indicate the 2σ upper limits. Note that a significant fraction of the original SDSS LRG sample have poor-quality QSO spectra, which result in upper limits exceeding 0.3 Å. These LRG-QSO pairs offer few or no constraints for the underlying absorber strengths in LRG haloes and are therefore excluded from the plots for clarity.

Rest-frame absorption equivalent width |${W_{\rm r}(2796)}$| versus projected distance d for LRGs with sufficiently high S/N background QSO spectra for detecting Mg ii absorbers as weak as W0 = 0.3 Å. Absorption observations for passive LRGs are shown in the left-hand panel. Observations of [O ii]-emitting LRGs are shown in the right-hand panel. LRGs with detected Mg ii absorbers are shown in filled circles with error bars representing measurement uncertainties. For non-detections, we use light grey circles to indicate the 2σ upper limits. Note that a significant fraction of the original SDSS LRG sample have poor-quality QSO spectra, which result in upper limits exceeding 0.3 Å. These LRG-QSO pairs offer few or no constraints for the underlying absorber strengths in LRG haloes and are therefore excluded from the plots for clarity.

Close
This Feature Is Available To Subscribers Only

Sign In or Create an Account

Close

This PDF is available to Subscribers Only

View Article Abstract & Purchase Options

For full access to this pdf, sign in to an existing account, or purchase an annual subscription.

Close