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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Prochaska, J. X.
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Topics
Publications (3/3 displayed)
- 2009Dust Extinction in High-z Galaxies with Gamma-Ray Burst Afterglow Spectroscopy: The 2175 Å Feature at z = 2.45citations
- 2008Probing feedback in protogalaxies: multiphase gas in a DLA at z ~ 2.4citations
- 2006When Do Internal Shocks End and External Shocks Begin? Early-Time Broadband Modeling of GRB 051111citations
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article
Probing feedback in protogalaxies: multiphase gas in a DLA at z ~ 2.4
Abstract
We investigate the physical processes occurring in the multiphase gas of a damped Lyα absorber (DLA). We base our analysis on a high-quality Keck High-Resolution Echelle Spectrometer (HIRES) spectrum of the QSO J1211+0422 in which a DLA is detected at z ~= 2.377. There is little contamination of the high-ion (OVI, NV, CIV, SiIV) absorption, allowing us to explore the properties of the highly ionized gas and its connection to other gas phases. The metallicity ([Z/H] = -1.41 +/- 0.08), HI column density [], full-width velocity (∆v<SUB>neut</SUB> ~= 70 kms<SUP>-1</SUP>) and relative abundances ([Si/Fe] = +0.23 +/- 0.05 and [N/Si] = -0.88 +/- 0.07) of this DLA are not unusual. However, we derive the lowest CII* cooling rate in a DLA, l<SUB>c</SUB> < 10<SUP>-27.8</SUP>ergs<SUP>-1</SUP> per H atom (3σ). Using this stringent limit, we show that the neutral gas (confined at |v| < +39kms<SUP>-1</SUP>) must be warm and the star formation rate is <7.1 × 10<SUP>-3</SUP>M<SUB>solar</SUB>yr<SUP>-1</SUP>kpc<SUP>-2</SUP>. Surprisingly, the gas shows strong, complex absorption profiles from highly ionized gas whose kinematics appear connected to each other and the low ions. The total amount of highly and weakly ionized gas is very large with >~ 1.5. At |v| >~ +39kms<SUP>-1</SUP>, the gas is fully and highly ionized []. Based on ionization models, OVI and NV are generally difficult to produce by hard photons, while SiIV and CIV can be photoionized to a large extent. There is, however, no evidence of OVI-bearing gas at T ~ 10<SUP>6</SUP> K associated with this DLA. In contrast, there is some evidence for narrow OVI, NV and CIV components (unexplained by photoionization), implying too low temperatures (T < 10<SUP>5</SUP> K) for simple collisional ionization models to produce their observed column densities. Stellar feedback is a possible source for producing the high ions, but we cannot rule out accretion of non-pristine material on to the protogalaxy....