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Related papers: Updating quasar bolometric luminosity corrections

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We present a measurement of the quasar luminosity function in the range 0.68<z<4 down to extinction corrected magnitude g_dered=22.5, using a simple and well understood target selection technique based on the time-variability of quasars.…

The measurement of small-angle Bhabha scattering is used to determine the luminosity at the OPAL interaction point for the LEP I data recorded between 1993 and 1995. The measurement is based on the OPAL Silicon-Tungsten Luminometer which is…

High Energy Physics - Experiment · Physics 2019-08-17 The OPAL collaboration , G. Abbiendi

We present new observations of the highest-redshift quasar known, ULAS J1120+0641, redshift $z=7.084$, obtained in the optical, at near-, mid-, and far-infrared wavelengths, and in the sub-mm. We combine these results with published X-ray…

Astrophysics of Galaxies · Physics 2015-02-18 R. Barnett , S. J. Warren , M. Banerji , R. G. McMahon , P. C. Hewett , D. J. Mortlock , C. Simpson , B. P. Venemans , K. Ota , T. Shibuya

We present an investigation of the low-frequency radio and ultraviolet properties of a sample of $\simeq$10,500 quasars from the Sloan Digital Sky Survey Data Release 14, observed as part of the first data release of the Low-Frequency-Array…

Astrophysics of Galaxies · Physics 2021-03-03 Amy L. Rankine , James H. Matthews , Paul C. Hewett , Manda Banerji , Leah K. Morabito , Gordon T. Richards

We present an updated determination of the z ~ 4 QSO luminosity function (QLF), improving the quality of the determination of the faint end of the QLF presented in Glikman et al. (2010). We have observed an additional 43 candidates from our…

Cosmology and Nongalactic Astrophysics · Physics 2015-05-20 Eilat Glikman , S. G. Djorgovski , Daniel Stern , Arjun Dey , Buell T. Jannuzi , Kyoung-Soo Lee

Interferometric calibration always yields non unique solutions. It is therefore essential to remove these ambiguities before the solutions could be used in any further modeling of the sky, the instrument or propagation effects such as the…

Instrumentation and Methods for Astrophysics · Physics 2013-07-19 Sarod Yatawatta

The future missions for astrophysical studies in the submillimeter region will need detectors with very high sensitivity and large field of view. Bolometer arrays can fulfill these requirements over a very broad band. We describe a…

Instrumentation and Methods for Astrophysics · Physics 2015-05-20 Vincent Revéret , Louis Rodriguez , Patrick Agnèse

Experiment E158 at SLAC can measure an azimuthal asymmetry in single-spin, transversely polarized Moller scattering, e^{-\uparrow} e^- -> e^- e^-, which arises from a QED rescattering phase. We recompute the leading-order (one-loop)…

High Energy Physics - Phenomenology · Physics 2014-11-17 Lance Dixon , Marc Schreiber

For 15 bright (V<17.5), high redshift (z>3) quasars, we have obtained IR spectra and photometry, and optical spectrophotometry and photometry, which we use to construct their rest-frame 1285-5100 AA spectral energy distributions (SEDs).…

Astrophysics · Physics 2009-11-06 Olga Kuhn , Martin Elvis , Jill Bechtold , Richard Elston

We use MARCS model atmosphere fluxes to compute synthetic colours, bolometric corrections and reddening coefficients for the Hipparcos/Tycho, Pan-STARRS1, SkyMapper and JWST systems. Tables and interpolation subroutines are provided to…

Solar and Stellar Astrophysics · Physics 2018-01-31 Luca Casagrande , Don A. VandenBerg

Weak emission-line quasars (WLQs) are a subset of Type 1 quasars that exhibit extremely weak Ly$\alpha +$N V $\lambda$1240 and/or C IV $\lambda$1549 emission lines. We investigate the relationship between emission-line properties and…

High precision astrometry requires an accurate geometric distortion solution. In this work, we present an average correction for the Blue Camera of the Large Binocular Telescope which enables a relative astrometric precision of ~15 mas for…

Instrumentation and Methods for Astrophysics · Physics 2010-05-07 A. Bellini , L. R. Bedin

We describe the first results from the All-sky BRIght, Complete Quasar Survey (AllBRICQS), which aims to discover the last remaining optically bright quasars. We present 156 spectroscopically confirmed quasars (140 newly identified) having…

Astrophysics of Galaxies · Physics 2023-03-29 Christopher A. Onken , Christian Wolf , Wei Jeat Hon , Samuel Lai , Patrick Tisserand , Rachel Webster

The POLARBEAR-2 CosmicMicrowave Background (CMB) experiment aims to observe B-mode polarization with high sensitivity to explore gravitational lensing of CMB and inflationary gravitational waves. POLARBEAR-2 is an upgraded experiment based…

With the advent of large-scale weak lensing surveys there is a need to understand how realistic, scale-dependent systematics bias cosmic shear and dark energy measurements, and how they can be removed. Here we describe how spatial…

Cosmology and Nongalactic Astrophysics · Physics 2016-05-31 A. N. Taylor , T. D. Kitching

The black hole (BH) mass and luminosity are key factors in determining how a quasar interacts with its environment. In this study, we utilise data from the European Southern Observatory Large Programme XQ-100, a high-quality sample of 100…

Astrophysics of Galaxies · Physics 2023-10-03 Samuel Lai , Christopher A. Onken , Christian Wolf , Fuyan Bian , Guido Cupani , Sebastian Lopez , Valentina D'Odorico

Current and future Cosmic Microwave Background (CMB) Radiation experiments are targeting the polarized $B$-mode signal. The small amplitude of this signal makes a successful measurement challenging for current technologies. Therefore, very…

Instrumentation and Methods for Astrophysics · Physics 2020-11-18 Tommaso Ghigna , Tomotake Matsumura , Guillaume Patanchon , Hirokazu Ishino , Masashi Hazumi

The COSmic Monopole Observer (COSMO) is an experiment to measure low-level spectral distortions in the isotropic component of the Cosmic Microwave Background (CMB). Deviations from a pure blackbody spectrum are expected at low level ($<$ 1…

We present a new method of modelling time-series data based on the running optimal average (ROA). By identifying the effective number of parameters for the ROA model, in terms of the shape and width of its window function and the times and…

Instrumentation and Methods for Astrophysics · Physics 2021-10-13 Fergus R. Donnan , Keith Horne , Juan V. Hernández Santisteban