The absorbing haloes around high-redshift radio galaxies: the UVES view

We summarise the properties of the absorbing haloes around two high-redshift radio galaxies studied with the VLT-UVES echelle spectrograph. The absorbers in 0943 - 242 (z = 2.92) exhibit little further structure compared with previous data-the main absorber still has N(HI) similar or equal to 10(19)...

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Main Authors: Wilman, R, Jarvis, M, Rottgering, H, Binette, L
Format: Conference item
Published: 2003
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author Wilman, R
Jarvis, M
Rottgering, H
Binette, L
author_facet Wilman, R
Jarvis, M
Rottgering, H
Binette, L
author_sort Wilman, R
collection OXFORD
description We summarise the properties of the absorbing haloes around two high-redshift radio galaxies studied with the VLT-UVES echelle spectrograph. The absorbers in 0943 - 242 (z = 2.92) exhibit little further structure compared with previous data-the main absorber still has N(HI) similar or equal to 10(19) cm(-2)-reinforcing the picture in which the absorbing gas occupies a smooth shell beyond the emission line halo. In 0200+015 (z = 2.23) the main absorber now splits into two spatially-resolved systems with N(HI) = 4 x 10(14) cm(-2), one of which has strong CIV absorption, implying a metallicity of Z similar or equal to 10 Zcircle dot. We explain the differences between the two sources with an evolutionary scenario, invoking interaction with the expanding radio source and metal enrichment via a starburst superwind. (C) 2003 Elsevier B.V. All rights reserved.
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spelling oxford-uuid:09f2a4ff-68d8-426b-a390-dca7351f86fb2022-03-26T09:21:08ZThe absorbing haloes around high-redshift radio galaxies: the UVES viewConference itemhttp://purl.org/coar/resource_type/c_5794uuid:09f2a4ff-68d8-426b-a390-dca7351f86fbSymplectic Elements at Oxford2003Wilman, RJarvis, MRottgering, HBinette, LWe summarise the properties of the absorbing haloes around two high-redshift radio galaxies studied with the VLT-UVES echelle spectrograph. The absorbers in 0943 - 242 (z = 2.92) exhibit little further structure compared with previous data-the main absorber still has N(HI) similar or equal to 10(19) cm(-2)-reinforcing the picture in which the absorbing gas occupies a smooth shell beyond the emission line halo. In 0200+015 (z = 2.23) the main absorber now splits into two spatially-resolved systems with N(HI) = 4 x 10(14) cm(-2), one of which has strong CIV absorption, implying a metallicity of Z similar or equal to 10 Zcircle dot. We explain the differences between the two sources with an evolutionary scenario, invoking interaction with the expanding radio source and metal enrichment via a starburst superwind. (C) 2003 Elsevier B.V. All rights reserved.
spellingShingle Wilman, R
Jarvis, M
Rottgering, H
Binette, L
The absorbing haloes around high-redshift radio galaxies: the UVES view
title The absorbing haloes around high-redshift radio galaxies: the UVES view
title_full The absorbing haloes around high-redshift radio galaxies: the UVES view
title_fullStr The absorbing haloes around high-redshift radio galaxies: the UVES view
title_full_unstemmed The absorbing haloes around high-redshift radio galaxies: the UVES view
title_short The absorbing haloes around high-redshift radio galaxies: the UVES view
title_sort absorbing haloes around high redshift radio galaxies the uves view
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