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A&A 414, 79-93 (2004)
DOI: 10.1051/0004-6361:20034003
The sizes and kinematic structure of absorption systems towards the lensed quasar APM08279+5255
S. L. Ellison1, 2, 3, R. Ibata4, M. Pettini5, G. F. Lewis6, B. Aracil7, P. Petitjean7 and R. Srianand81 P. Universidad Católica de Chile, Casilla 306, Santiago 22, Chile
2 European Southern Observatory, Casilla 19001, Santiago 19, Chile
3 Current address: University of Victoria, Department of Physics and Astronomy, Elliott Building, 3800 Finnerty Rd., Victoria, BC, V8P 1A1, Canada
e-mail: sarae@uvic.ca
4 Observatoire de Strasbourg, 11 rue de l'Université, 67000, Strasbourg, France
5 Institute of Astronomy, Madingley Rd, Cambridge, CB3 0HA, UK
6 Institute of Astronomy, School of Physics, A 29, University of Sydney, NSW 2006, Australia
7 Institut d'Astrophysique de Paris - CNRS, 98bis boulevard Arago, 75014 Paris, France
8 IUCAA, Post Bag 4, Ganeshkhind, Pune 411 007, India
(Received 25 June 2003 / Accepted 6 October 2003)
Abstract
We have obtained spatially resolved spectra of the
triply imaged
QSO APM08279+5255 using the Space Telescope Imaging Spectrograph (STIS)
on board the Hubble Space Telescope (HST).
We study the line of sight equivalent width (
EW)
differences and velocity shear of high and low ionization
absorbers (including a damped Lyman alpha [DLA] system identified
in a spatially unresolved ground based spectrum) in the three
lines of sight. The combination of
a particularly rich spectrum and three sight-lines
allow us to study 27 intervening absorption systems
over a redshift range
,
probing proper transverse dimensions of 30
h70-1 pc up to
2.7
h70-1 kpc.
We find that high ionization systems (primarily C IV absorbers) do not
exhibit strong
EW variations on scales
<
0.4
h70-1 kpc; their fractional
EW differences
are typically less than 30%.
When combined with previous work on other QSO pairs,
we find that the fractional variation increases steadily
with separation out to at least ~
100
h70-1 kpc. Conversely, low
ionization systems (primarily Mg II absorbers) show strong
variations (often
>
80%) over kpc scales. A minimum radius for
strong (
EW > 0.3 Å) Mg II systems of
>
1.4
h70-1 kpc
is inferred from absorption coincidences in all lines of sight.
For weak Mg II absorbers (
EW
< 0.3 Å),
a maximum likelihood analysis indicates a most probable coherence
scale of
2.0
h70-1 kpc for a uniform spherical geometry, with 95% confidence limits
ranging between 1.5 and 4.4
h70-1 kpc.
The weak Mg II absorbers may therefore represent a distinct population
of smaller galaxies compared with the strong Mg II systems which
we know to be associated with
luminous galaxies whose halos extend over tens of kpc. Alternatively,
the weak systems may reside in the outer parts of larger galaxies,
where their filling factor may be lower.
By cross-correlating spectra along different lines of sight, we infer shear
velocities of typically less than 20 km s
-1 for both high and low
ionization absorbers. Finally, for systems with
weak absorption that can be confidently converted to column densities,
we find constant
N(C IV)/
N(Si IV) across the three lines of sight.
Similarly, the [Al/Fe] ratios in the
DLA
are consistent with solar relative abundances
over a transverse distance of ~
0.35
h70-1 kpc.
Key words: quasars: absorption lines -- quasars: individual: APM08279+5255 -- galaxies: ISM -- galaxies: kinematics and dynamics -- gravitational lensing
Offprint request: S. Ellison, sarae@uvic.ca
SIMBAD Objects
© ESO 2004
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