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Astron. Astrophys. 338, 777-780 (1998)
4. Results and discussions
Knowing the analytic expressions for the lensing cross-sections in
general FLRW cosmologies, we can explore in detail the influences of
cosmological parameters by numerical computation. We compute the
probability so as to investigate whether the
background objects (like quasars) counts are significantly
contaminated. Eq. 18contains three factors, namely, the
µ-dependent term, the galaxies term and the cosmological
term, associated with . Here we concentrate on
the cosmological term by adopting the maximum value
(Kochanek 1996) and a moderate magnification of
.
Fig. 1 shows how the probability
depends on the normalized cosmological parameters
and for an open
( , ) and a flat
( ) universe respectively. In our calculations,
the source has been set at or
respectively, and a moderate magnification of
has been used. Indeed, the probability
depends sensitively on cosmological parameters
and . However, even for a
-dominated ( ) flat
universe, only a small fraction ( ) of the sky
can be moderately ( ) lensed by galaxies.
![[FIGURE]](img76.gif) |
Fig. 1a and b. The probability, , that the sources located at (solid-lines) and (dashed-lines) are magnified by the factor greater than as a function of for a an open universe with , , and b a flat universe with .
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Of course, by taking somewhat lower value for µ the
probability of the magnification can siginificantly increase. In order
to get a more robust conclusion, we now estimate what value of
magnification would affect the current observations of quasar count,
i.e., we calculate the value of which makes
. The resulting magnification, which depends on
both the cosmological model and the source redshift, is shown in
Fig. 2. Since the magnification is generally much lower than 1.1,
our result reinforces the hypothesis that the quasar counts are not
seriously contaminated by the galactic lenses.
![[FIGURE]](img79.gif) |
Fig. 2a and b. The magnification , which makes the probability of the sources located at (solid-lines) and (dashed-lines) , as a function of for a an open universe with , , and b a flat universe with .
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© European Southern Observatory (ESO) 1998
Online publication: September 17, 1998
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