52 research outputs found

    The Extremely Luminous Quasar Survey (ELQS) in the SDSS footprint I.: Infrared Based Candidate Selection

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    Studies of the most luminous quasars at high redshift directly probe the evolution of the most massive black holes in the early Universe and their connection to massive galaxy formation. However, extremely luminous quasars at high redshift are very rare objects. Only wide area surveys have a chance to constrain their population. The Sloan Digital Sky Survey (SDSS) has so far provided the most widely adopted measurements of the quasar luminosity function (QLF) at z>3z>3. However, a careful re-examination of the SDSS quasar sample revealed that the SDSS quasar selection is in fact missing a significant fraction of z≳3z\gtrsim3 quasars at the brightest end. We have identified the purely optical color selection of SDSS, where quasars at these redshifts are strongly contaminated by late-type dwarfs, and the spectroscopic incompleteness of the SDSS footprint as the main reasons. Therefore we have designed the Extremely Luminous Quasar Survey (ELQS), based on a novel near-infrared JKW2 color cut using WISE AllWISE and 2MASS all-sky photometry, to yield high completeness for very bright (mi<18.0m_{\rm{i}} < 18.0) quasars in the redshift range of 3.0≤z≤5.03.0\leq z\leq5.0. It effectively uses random forest machine-learning algorithms on SDSS and WISE photometry for quasar-star classification and photometric redshift estimation. The ELQS will spectroscopically follow-up ∼230\sim 230 new quasar candidates in an area of ∼12000 deg2\sim12000\,\rm{deg}^2 in the SDSS footprint, to obtain a well-defined and complete quasars sample for an accurate measurement of the bright-end quasar luminosity function at 3.0≤z≤5.03.0\leq z\leq5.0. In this paper we present the quasar selection algorithm and the quasar candidate catalog.Comment: 16 pages, 8 figures, 9 tables; ApJ in pres

    Quasar Photometric Redshifts and Candidate Selection: A New Algorithm Based on Optical and Mid-Infrared Photometric Data

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    We present a new algorithm to estimate quasar photometric redshifts (photo-zzs), by considering the asymmetries in the relative flux distributions of quasars. The relative flux models are built with multivariate Skew-t distributions in the multi-dimensional space of relative fluxes as a function of redshift and magnitude. For 151,392 quasars in the SDSS, we achieve a photo-zz accuracy, defined as the fraction of quasars with the difference between the photo-zz zpz_p and the spectroscopic redshift zsz_s, ∣Δz∣=∣zs−zp∣/(1+zs)|\Delta z| = |z_s-z_p|/(1+z_s) within 0.1, of 74%. Combining the WISE W1 and W2 infrared data with the SDSS data, the photo-zz accuracy is enhanced to 87%. Using the Pan-STARRS1 or DECaLS photometry with WISE W1 and W2 data, the photo-zz accuracies are 79% and 72%, respectively. The prior probabilities as a function of magnitude for quasars, stars and galaxies are calculated respectively based on (1) the quasar luminosity function; (2) the Milky Way synthetic simulation with the Besan\c{c}on model; (3) the Bayesian Galaxy Photometric Redshift estimation. The relative fluxes of stars are obtained with the Padova isochrones, and the relative fluxes of galaxies are modeled through galaxy templates. We test our classification method to select quasars using the DECaLS gg, rr, zz, and WISE W1 and W2 photometry. The quasar selection completeness is higher than 70% for a wide redshift range 0.5<z<4.50.5<z<4.5, and a wide magnitude range 18<r<21.518<r<21.5 mag. Our photo-zz regression and classification method has the potential to extend to future surveys. The photo-zz code will be publicly available.Comment: 22 pages, 17 figure, accepted by AJ. The code is available at https://doi.org/10.5281/zenodo.101440

    The Extremely Luminous Quasar Survey in the Pan-STARRS 1 Footprint (PS-ELQS)

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    We present the results of the Extremely Luminous Quasar Survey in the 3π3\pi survey of the Panoramic Survey Telescope and Rapid Response System (Pan-STARRS; PS1). This effort applies the successful quasar selection strategy of the Extremely Luminous Survey in the Sloan Digital Sky Survey footprint (∼12,000 deg2\sim12,000\,\rm{deg}^2) to a much larger area (∼21486 deg2\sim\rm{21486}\,\rm{deg}^2). This spectroscopic survey targets the most luminous quasars (M1450≤−26.5M_{1450}\le-26.5; mi≤18.5m_{i}\le18.5) at intermediate redshifts (z≥2.8z\ge2.8). Candidates are selected based on a near-infrared JKW2 color cut using WISE AllWISE and 2MASS photometry to mainly reject stellar contaminants. Photometric redshifts (zregz_{\rm{reg}}) and star-quasar classifications for each candidate are calculated from near-infrared and optical photometry using the supervised machine learning technique random forests. We select 806 quasar candidates at zreg≥2.8z_{\rm{reg}}\ge2.8 from a parent sample of 74318 sources. After exclusion of known sources and rejection of candidates with unreliable photometry, we have taken optical identification spectra for 290 of our 334 good PS-ELQS candidates. We report the discovery of 190 new z≥2.8z\ge2.8 quasars and an additional 28 quasars at lower redshifts. A total of 44 good PS-ELQS candidates remain unobserved. Including all known quasars at z≥2.8z\ge2.8, our quasar selection method has a selection efficiency of at least 77%77\%. At lower declinations −30≤Decl.≤0-30\le\rm{Decl.}\le0 we approximately triple the known population of extremely luminous quasars. We provide the PS-ELQS quasar catalog with a total of 592 luminous quasars (mi≤18.5m_{i}\le18.5, z≥2.8z\ge2.8). This unique sample will not only be able to provide constraints on the volume density and quasar clustering of extremely luminous quasars, but also offers valuable targets for studies of the intergalactic medium.Comment: 34 pages, 10 figures, accepted to ApJ

    A Closer Look at Two of the Most Luminous Quasars in the Universe

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    Ultra-luminous quasars (M1450≤−29M_{1450} \leq -29) provide us with a rare view into the nature of the most massive and most rapidly accreting supermassive black holes (SMBHs). Following the discovery of two of these extreme sources, J0341+{+}1720 (M1450=−29.56M_{1450}=-29.56, z=3.71z=3.71) and J2125−{-}1719 (M1450=−29.39M_{1450}=-29.39, z=3.90z=3.90), in the Extremely Luminous Quasar Survey (ELQS) and its extension to the Pan-STARRS\,1 footprint (PS-ELQS), we herein present an analysis of their rest-frame UV to optical spectroscopy. Both quasars harbor very massive SMBHs with MBH=6.73−0.83+0.75×109 M⊙M_{\rm{BH}}=6.73_{-0.83}^{+0.75}\times10^{9}\,M_{\odot} and MBH=5.45−0.55+0.60×109 M⊙M_{\rm{BH}}=5.45_{-0.55}^{+0.60}\times10^{9}\,M_{\odot}, respectively, showing evidence of accretion above the Eddington limit (Lbol/LEdd=2.74−0.27+0.39L_{\rm{bol}}/L_{\rm{Edd}}=2.74_{-0.27}^{+0.39} and Lbol/LEdd=3.01−0.30+0.34L_{\rm{bol}}/L_{\rm{Edd}}=3.01_{-0.30}^{+0.34}). NOEMA 3 millimeter observations of J0341+{+}1720 reveal a highly star-forming (SFR≈1500 M⊙ yr−1\rm{SFR}\approx1500\,M_{\odot}\,\rm{yr}^{-1}), ultra-luminous infrared galaxy (LTIR≈1.0×1013 L⊙L_{\rm{TIR}}\approx1.0\times10^{13}\,L_{\odot}) host, which, based on an estimate of its dynamical mass, is only ∼30{\sim}30 times more massive than the SMBH it harbors at its center. As examples of luminous super-Eddington accretion, these two quasars provide support for theories, which explain the existence of billion solar mass SMBHs ∼700{\sim}700 million years after the Big Bang by moderate super-Eddington growth from standard SMBH seeds.Comment: Accepted for publication in the Astrophysical Journal (ApJ

    X-Ray Observations of a z ∼ 6.2 Quasar/Galaxy Merger

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    Quasars at early redshifts (z > 6) with companion galaxies offer unique insights into the growth and evolution of the first supermassive black holes. Here, we report on a 150 ks Chandra observation of PSO.J308.0416-21.2339, a z = 6.23 quasar with a merging companion galaxy identified in [C II] and rest-frame UV emission. With 72.3(-8.6)(+9.6) net counts, we find that PSO.J308.0416-21.2339 is powerful (L-X = 2.31(-0.76)(+1.14) x 10(45) erg s(-1) cm(-2) in rest-frame 2.0-10.0 keV) yet soft (spectral power-law index Gamma = 2.39(-0.36)(+0.37) and optical-to-X-ray slope alpha(OX) = -1.41 +/- 0.11). In addition, we detect three hard-energy photons 2 ''.0 to the west of the main quasar, cospatial with the brightest UV emission of the merging companion. As no soft-energy photons are detected in the same area, this is potentially indicative of a highly obscured source. With conservative assumptions, and accounting for both background fluctuations and the extended wings of the quasar's emission, these photons only have a probability P = 0.021 of happening by chance. If confirmed by deeper observations, this system is the first high-redshift quasar and companion individually detected in X-rays and is likely a dual active galactic nucleus.STSCI/NASAThis item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at [email protected]

    The Discovery of A Luminous Broad Absorption Line Quasar at A Redshift of 7.02

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    Despite extensive efforts, only two quasars have been found at z>7z>7 to date due to a combination of low spatial density and high contamination from more ubiquitous Galactic cool dwarfs in quasar selection. This limits our current knowledge of the super-massive black hole (SMBH) growth mechanism and reionization history. In this letter, we report the discovery of a luminous quasar at z=7.021z=7.021, DELS J003836.10−-152723.6 (hereafter J0038−-1527), selected using photometric data from DESI Legacy imaging Survey (DELS), Pan-STARRS1 (PS1) imaging Survey, as well as Wide-field Infrared Survey Explore (WISEWISE) mid-infrared all-sky survey. With an absolute magnitude of M1450M_{1450}=−-27.1 and bolometric luminosity of LBolL_{\rm Bol}=5.6×\times1013^{13} L⊙L_\odot, J0038−-1527 is the most luminous quasar known at z>7z>7. Deep optical to near infrared spectroscopic observations suggest that J0038-1527 hosts a 1.3 billion solar mass BH accreting at the Eddington limit, with an Eddington ratio of 1.25±\pm0.19. The CIV broad emission line of J0038−-1527 is blue-shifted by more than 3000 km s−1^{-1} to the systemic redshift. More detailed investigations of the high quality spectra reveal three extremely high velocity CIV broad absorption lines (BALs) with velocity from 0.08 to 0.14 times the speed of light and total balnicity index of more than 5000 km s−1^{-1}, suggesting the presence of relativistic outflows. J0038−-1527 is the first quasar found at the epoch of reionization (EoR) with such strong outflows and provides a unique laboratory to investigate AGN feedback on the formation and growth of the most massive galaxies in the early universe.Comment: ApJL in pres

    Detecting and Characterizing Young Quasars I: Systemic Redshifts and Proximity Zones Measurements

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    In a multi-wavelength survey of 1313 quasars at 5.8≲z≲6.55.8\lesssim z\lesssim6.5, that were pre-selected to be potentially young, we find five objects with extremely small proximity zone sizes that may imply UV-luminous quasar lifetimes of ≲100,000\lesssim 100,000 years. Proximity zones are regions of enhanced transmitted flux in the vicinity of the quasars that are sensitive to the quasars' lifetimes because the intergalactic gas has a finite response time to their radiation. We combine sub-mm observations from the Atacama Large Millimetre Array (ALMA) and the NOrthern Extended Millimeter Array (NOEMA), as well as deep optical and near-infrared spectra from medium-resolution spectrograph on the Very Large Telescope (VLT) and on the Keck telescopes, in order to identify and characterize these new young quasars, which provide valuable clues about the accretion behavior of supermassive black holes (SMBHs) in the early universe, and pose challenges on current black hole formation models to explain the rapid formation of billion solar mass black holes. We measure the quasars' systemic redshifts, black hole masses, Eddington ratios, emission line luminosities, and star formation rates of their host galaxies. Combined with previous results we estimate the fraction of young objects within the high-redshift quasar population at large to be 5%≲fyoung≲10%5\%\lesssim f_{\rm young}\lesssim 10\%. One of the young objects, PSO J158-14, shows a very bright dust continuum flux (Fcont=3.46±0.02 mJyF_{\rm cont}=3.46\pm 0.02\,\rm mJy), indicating a highly star-bursting host galaxy with a star formation rate of approximately 1420 M⊙ yr−11420\,M_{\odot}\,\rm yr^{-1}.Comment: Accepted for publication in Ap

    No Redshift Evolution in the Broad Line Region Metallicity up to z=7.54: Deep NIR Spectroscopy of ULAS J1342+0928

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    We present deep (9 hours) Gemini-N/GNIRS near-infrared spectroscopic observations of ULAS J1342+0928, a luminous quasar at z=7.54. Various broad emission lines were detected, as well as the underlying continuum and iron forests over the rest-frame wavelength 970-2930A. There is a clear trend that higher-ionization emission lines show larger blueshifts with CIV1549 exhibiting 5510^{+240}_{-110} km s-1 blueshift with respect to the systematic redshift from the far-infrared [CII] 158um emission line. Those high ionization lines have wide profiles with FWHM more than 10000 km s-1. A modest blueshift of 340^{+110}_{-80} km s-1 is also seen in MgII, the lowest ionization line identified in the spectrum. The updated MgII-based black hole mass of M_BH=9.1_{-1.3}^{+1.4} x 10^8 M_sun and the Eddington ratio of L_bol/L_Edd=1.1_{-0.2}^{+0.2} confirm that ULAS J1342+0928 is powered by a massive and actively accreting black hole. There is no significant difference in the emission line ratios such as SiIV/CIV and AlIII/CIV when compared to lower-redshift quasars in a similar luminosity range, which suggests early metal pollution of the broad-line-region clouds. This trend also holds for the FeII/MgII line ratio, known as a cosmic clock that traces the iron enrichment in the early universe. Different iron templates and continuum fitting ranges were used to explore how the FeII/MgII measurement changes as a function of spectral modeling. Quasars at even higher redshift or at fainter luminosity range (L_bol<10^46 erg s-1) are needed to probe the sites of early metal enrichment and a corresponding change in the FeII/MgII ratio.Comment: 21 pages, 8 figures, 3 tables, accepted for publication in Ap
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