Damped Lyα Systems at z < 1.65: The Expanded Sloan Digital Sky Survey Hubble Space Telescope Sample
By S. Rao, D. Turnshek, D. Nestor. 2006
315 citations recorded by the source corpus.
Subfields: Astronomy and Astrophysics
View Paper: https://www.semanticscholar.org/paper/d2458d4b6a81795a781bdbe674e8ff24e338bfc0
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Citations in the corpus
- MEASUREMENT OF 21 cm BRIGHTNESS FLUCTUATIONS AT z ∼ 0.8 IN CROSS-CORRELATION (2012, background): “…redshifts are more difficult to measure, and estimates based on Mg-II lines in DLA systems observed with Hubble Space Telescope find ΩHI(z ∼ 1) ≈ (0.97 ± 0.36) × 10−3 (Rao et al. 2006), in rough agreement withz ≈ 0.2 DLA measurements (Meiring et al. 2011) and 21 cm stacking (Lah et al. 2007).”
- The ESO UVES advanced data products quasar sample: II. Cosmological evolution of the neutral gas mass density (2013, methodology): “At low-redshift, results for DLAs come from the Rao et al. (2006) survey of quasars targeted because of known Mgii absorbers.”
- AN EMPIRICAL CHARACTERIZATION OF EXTENDED COOL GAS AROUND GALAXIES USING Mg ii ABSORPTION FEATURES (2010, background): “The large associated HI column density (Rao et al. 2006) suggests that Mg II absorbers are similar to those H I clouds seen around individual galaxies in 21 cm surveys (e.g. Doyle et al. 2005).”
- Evolution of the cosmological mass density of neutral gas from Sloan Digital Sky Survey II - Data Release 7 (2009, methodology): “Rao & Turnshek (2000) and Rao et al. (2006) used a novel technique to measure ΩDLAg at 0.1 < z < 1.6.”
- THE RADIAL AND AZIMUTHAL PROFILES OF Mg ii ABSORPTION AROUND 0.5 < z < 0.9 zCOSMOS GALAXIES OF DIFFERENT COLORS, MASSES, AND ENVIRONMENTS (2011, background): “Mg II absorption originates in photo-ionized gas at temperatures around T∼ 104 K (Bergeron & Stasínska 1986; Charlton et al. 2003) with neutral Hydrogen column densities ofN(HI ) ≈ 1016 − 1022 cm2 (Churchill et al. 2000; Rigby et al. 2002; Rao et al. 2006).”
- THE BIMODAL METALLICITY DISTRIBUTION OF THE COOL CIRCUMGALACTIC MEDIUM AT z ≲ 1 (2013, methodology): “For this cut-off Rao et al. (2006) argued that the DLA sample is essentially complete and therefore free of metallicity bias.”
- ON THE (NON)EVOLUTION OF H i GAS IN GALAXIES OVER COSMIC TIME (2008, methodology): “Before concluding, we comment briefly on current estimates of f(NHI, X) and ρHI at z ∼ 1 where Mg II absorption has been used to identify DLA candidates (Rao & Turnshek 2000; Rao et al. 2006).”
- On the Normalization of the Cosmic Star Formation History (2006, background): “The UV data atz ≤ 1 are “obscuration corrected” 1 Thanks to Sandhya Rao (Rao et al. 2006) for this terminology. by adding the FIR SFR density from Le Floc’h et al. (2005) to each point.”
- A Population of Faint Extended Line Emitters and the Host Galaxies of Optically Thick QSO Absorption Systems (2007, background): “…is more than 14 times larger than that of its contemporary damped Ly systems, as estimated from the Sloan Digital Sky Survey, dN /dz(z ¼ 0:37) ¼ 0:066 (Rao et al. 2006), so even if DLAS were not larger than [O ii] emission regions, and not more numerous, only about 7% of our emitters (i.e., two…”
- RADIATIVE TRANSFER IN A CLUMPY UNIVERSE. IV. NEW SYNTHESIS MODELS OF THE COSMIC UV/X-RAY BACKGROUND (2011, background): “With a power-law exponent β = 2 down to a break column of NHI = 10 21.55 cm−2 (Prochaska & Wolfe 2009), and with an incidence per unit redshift ∝ (1 + z)1.27 (Rao et al. 2006), the parameters for the DLAs becomes (A, β, γ) = (8.7× 1018, 2, 1.27).”
- Four Quasars above Redshift 6 Discovered by the Canada-France High-z Quasar Survey (2007, background): “This set of absorption lines is characteristic of damped Lyα absorbers (DLAs): about 80% of the MgII systems withwrest(2796)> 1.0 Å are DLAs (Rao et al. 2006) and, moreover, all systems withwrest(2852)> 0.7 Å are DLAs (Rao & Turnshek 2000).”
- THE ARECIBO LEGACY FAST ALFA SURVEY. X. THE H i MASS FUNCTION AND FROM THE 40% ALFALFA SURVEY (2010, background): “…with the value inferred from damped Lyman absorber (DLA) systems at z ∼ 2 and that significant evolution is required to reconcile measurements in the two epochs (Noterdaeme et al. 2009; Rao et al. 2006), while providing a tighter constraint on the present-day energy density of cold gas.”