![]() | Annu. Rev. Astron. Astrophys. 2005. 43:
861-918 Copyright © 2005 by Annual Reviews. All rights reserved |
On the other hand,
Prochaska et al. (2005)
find that biasing due to gravitational lensing could be important. They
compared the full SDSS sample of damped
Ly systems with
subsamples comprising the brightest 33% of background quasars and the
faintest 33% of background quasars. While the incidence of damped
Ly
systems,
d
/ dX, was
found to be insensitive to quasar magnitude, the mass density,
g(z),
was found to vary significantly. Specifically, the bright subsample
showed sysematically higher values of
g(z)
than the faint subsample. To explain the independence of
d
/ dX on
quasar magnitude, the difference must lie in the incidence of systems
with large N(H I), which is observed to be larger in the bright
subsample.
Prochaska et al. (2005)
argue that gravitational magnification of the background quasars by
massive halos or disks associated with the foreground damped
Ly systems could account
for this systematic effect, which was first detected at the
2
level by
Murphy & Liske (2004).
Whereas obscuration by dust would cause
g(z)
to be lower in the bright subsample, magnification by lensing due to
exponential disks is greatest for damped
Ly
systems with large
values of N(H I)
(Bartelmann & Loeb 1996;
Maller et al. 1997).
Consequently, the values of
g(z)
in Figure 5 may be 10-20% too high,
but the evolution of
g(z) with z is still likely to be
correct. However, the effect could be more important for damped
Ly
system samples with
z < 2
(Rao & Turnshek 2000).