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Astron. Astrophys. 326, L9-L11 (1997)
1. Introduction
It is indeed not a novel idea to suggest that all the distant
objects may be affected by the gravitational lensing of the matter
clumps between the sources and the observer. Three decades ago,
Barnothy and Barnothy (1968) proposed that all the quasars were
nothing but the gravitationally magnified images of Seyfert galactic
nuclei. Press and Gunn (1973) showed that the probability of the
occurrence of gravitational lensing in an
universe is nearly unity. Unlike the previous speculations for which
there was apparently a lack of both convincing observational and
theoretical supports, the current argument is based on the numerous
and unprecedented deep galaxy surveys which have revealed a
considerably large population of faint galaxies (Metcalfe et al. 1996;
references therein). Using the surface number density of faint
galaxies down to , , Fried
(1997) derived a projected mean distance between galaxies to be
, which led him to the conclusion that all the
high redshift ( ) objects are moderately magnified
by a factor of 1.1-1.5 due to gravitational lensing by the intervening
galaxies. Indeed, this was a natural and plausible consequence,
provided that all the faint galaxies were at and
had a mean velocity dispersion -300 km
s-1.
Nonetheless, spectroscopic redshifts have not been available for
most of the faint galaxies to date. Namely, we do not yet know where
these faint galaxies are. For instance, the faint blue galaxies might
be the star-forming galaxies at moderate redshift of
(e.g. Broadhurst et al. 1992) or at high
redshifts of (Metcalfe et al. 1996). While the
dispute regarding the merging rate has existed for several years, it
is generally agreed that galaxy mergers may play an important role in
the formation and evolution of galaxies. At least, the merging model
provides a good fit to the faint galaxy number counts. It is
particularly noted that the merging alters significantly the redshift
and velocity dispersion distributions of galaxies. What is the optical
depth due to gravitational lensing for a distant source if the
redshift and velocity dispersion information for the faint galaxies
according to the prediction of galaxy merging is employed ? Can the
sky be fully covered by the lensing cross-sections of galaxies if
faint galaxies are neither peaked at nor
distributed randomly in redshift space ? We would like to answer these
questions by modeling the galaxy matter distribution as the simplest
singular isothermal sphere and the galaxy evolution as merging. Rix et
al. (1994) and Mao & Kochanek (1994) have presented a
sophisticated treatment of how galaxy mergers affect the various
aspects of statistical lensing. Here we focus on the specific issue of
the lensing covering of galaxies over the sky.
© European Southern Observatory (ESO) 1997
Online publication: April 20, 1998
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