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The Clustering of High-Redshift (2.9 \leq z \leq 5.1) Quasars in SDSS Stripe 82

Abstract

We present a measurement of the two-point autocorrelation function of photometrically-selected, high-zz quasars over \sim 100 deg2^2 on the Sloan Digitial Sky Survey Stripe 82 field. Selection is performed using three machine-learning algorithms, trained on known high-zz quasar colors, in a six-dimensional, optical/mid-infrared color space. Optical data from the Sloan Digitial Sky Survey is combined with overlapping deep mid-infrared data from the \emph{Spitzer} IRAC Equatorial Survey and the \emph{Spitzer}-HETDEX Exploratory Large-area survey. The selected quasar sample consists of 1378 objects and contains both spectroscopically-confirmed quasars and photometrically-selected quasar candidates. These objects span a redshift range of 2.9z5.12.9 \leq z \leq 5.1 and are generally fainter than i=20.2i=20.2; a regime which has lacked sufficient number density to perform autocorrelation function measurements of photometrically-classified quasars. We compute the angular correlation function of these data, marginally detecting quasar clustering. We fit a single power-law with an index of δ=1.39±0.618\delta = 1.39 \pm 0.618 and amplitude of θ0=0.71±0.546\theta_0 = 0.71 \pm 0.546 arcmin. A dark-matter model is fit to the angular correlation function to estimate the linear bias. At the average redshift of our survey (z=3.38\langle z \rangle = 3.38) the bias is b=6.78±1.79b = 6.78 \pm 1.79. Using this bias, we calculate a characteristic dark-matter halo mass of 1.70--9.83×1012h1M\times 10^{12}h^{-1} M_{\odot}. Our bias estimate suggests that quasar feedback intermittently shuts down the accretion of gas onto the central super-massive black hole at early times. If confirmed, these results hint at a level of luminosity dependence in the clustering of quasars at high-zz.Comment: 23 Pages, 17 Figure

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