- Palanque-Delabrouille, N;
- Magneville, Ch;
- Yèche, Ch;
- Eftekharzadeh, S;
- Myers, AD;
- Petitjean, P;
- Pâris, I;
- Aubourg, E;
- McGreer, I;
- Fan, X;
- Dey, A;
- Schlegel, D;
- Bailey, S;
- Bizayev, D;
- Bolton, A;
- Dawson, K;
- Ebelke, G;
- Ge, J;
- Malanushenko, E;
- Malanushenko, V;
- Oravetz, D;
- Pan, K;
- Ross, NP;
- Schneider, DP;
- Sheldon, E;
- Simmons, A;
- Tinker, J;
- White, M;
- Willmer, Ch
We present a measurement of the quasar luminosity function in the range 0.68 < z < 4 down to extinction corrected magnitude gdered = 22.5, using a simple and well understood target selection technique based on the time-variability of quasars. The completeness of our sample was derived directly from a control sample of quasars, without requiring complex simulations of quasar light-curves or colors. A total of 1877 quasar spectra were obtained from dedicated programs on the Sloan telescope (as part of the SDSS-III/BOSS survey) and on the Multiple Mirror Telescope. They allowed us to derive the quasar luminosity function. It agrees well with results previously published in the redshift range 0.68 < z < 2.6. Our deeper data allow us to extend the measurement to z = 4. We measured quasar densities to gdered < 22.5, obtaining 30 QSO per deg2 at z < 1, 99 QSO per deg 2 for 1 < z < 2.15, and 47 QSO per deg2 at z > 2.15. Using pure luminosity evolution models, we fitted our LF measurements and predicted quasar number counts as a function of redshift and observed magnitude. These predictions are useful inputs for future cosmology surveys such as those relying on the observation of quasars to measure baryon acoustic oscillations. © 2013 ESO.