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Astron. Astrophys. 343, 916-922 (1999)
4. Probability of detection
From the above modeling, we can evaluate the probability to detect a
photometric stellar variation due to an extra-solar comet. We assume a
survey of a given number of stars at a given accuracy. We carried out
a large number of simulations of cometary occultations in all
directions.
4.1. Orbital parameters
The characteristics of the comets are given by their distribution
in the parameter space. Concerning the orbital parameters, the
periastron density distribution is chosen to be the same as the one
observed in the solar system: with
AU AU
(A'Hearn et al., 1995). Many sun-grazing comets have been discovered
by SOHO with perihelion AU
(Kohl et al. 1997; see also the numerous IAU Circulars). But it is
still difficult to infer the distribution for these small periastrons.
The above distribution is thus likely biased by an underestimate of
the number of comets with small periastron, because such comets are
difficult to observe. These star-grazing comets give a larger
photometric variation. Therefore, we possibly slightly underestimate
the probabilities of detection.
We fixed all the apoastrons at 20 AU, the longitudes of
periastron, the ascending nodes and the inclinations are chosen
randomly.
4.2. Dust production rate
One of the most important parameter is the dust production rate.
Because, it dictates the mass of dust in the tail, and constrains the
detectability of the comet. The amplitude of the photometric variation
is roughly proportional to that parameter.
We consider that the dust production rate (P) is
proportional to the area of the comet's nucleus, and that the
distribution of the comets' radii ( )
is similar to the distribution observed for the comets, asteroids, and
Kuiper belt objects of the solar system. We assume that the number
density of objects with radius in the range
to
is
.
is a positive number, typically in the range 3 to 4 (Luu 1995). It is
constrained to be 3-3.5 for the
comets' nuclei observed with
km km
(Fernández 1982, Hughes & Daniels 1982, Brandt et al. 1997)
The same distribution is consistent with the observation of the Kuiper
belt objects: with
km km
(Jewitt 1996), or with theoretical models for the formation of these
objects: for
km (Kenyon & Luu, 1998).
With the assumption that , the
number of comets with a production rate between P and
is
. We adopt
. Changing
to 3 or 4 would change the
probability of detection by less than a factor of two.
Finally, this distribution is normalized by
, the number of comets per unit of
time passing through the periastron with a production rate larger than
. Hence, we have
. Thus,
![[EQUATION]](img142.gif)
4.3. Results
Using a large number of various comets, we calculate the
probability of detection at a given photometric accuracy. Then, the
number of possible detections is simply this probability multiplied by
, the duration of the observation
and the number of stars surveyed
.
We suppose that the time scale between each measurement is small
enough ( hour) that each
variation above the detection limit will effectively be detected. As
an example, we take year and
, which is the order of magnitude
for the future space mission COROT.
The expected number of detections is plotted in Fig. 5. We
considered two types of planetary systems. The first one is similar to
the solar system with comets per
year with
kg s-1 at
AU. We see that few dozens of
comets could be detected at an accuracy of
. We consider it as the pessimistic
case.
![[FIGURE]](img181.gif) |
Fig. 5. Plot of the number of detections of cometary occultations as a function of the photometric accuracy. Two cases are considered: the "pessimistic case" which is a survey of sun-like stars, during year ( , kg s-1), and the "optimistic case" where among the 30000 stars, 1% ( ) have a Pictoris-like activity ( , kg s-1). With an accuracy of , about 10 to 103 detections can be expected. The large difference between the two cases shows that this kind of survey will also give information on the planetary evolution. For comparison, the dotted histogram gives the number of detection of planets assuming that each star has a planetary system like the solar system. With an accuracy larger than , this gives the number of detection of giant planets, and mainly Jupiter-like planets. With an accuracy better than , Earth-like planets will be detected. Each step in the histogram represents the possibility to detect successively the Earth ( ), Venus ( ), Mars ( ) and Mercury ( ). We see that accurate photometric survey should detect more comets than planets.
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The second type of planetary system is supposed to be a young
planetary system with a large cometary activity as during the youth of
the solar system. The typical example is the well-known star
Pictoris where comets' infalls
are commonly observed through UV and optical spectroscopy (see e.g.,
Ferlet et al. 1987, Lagrange et al. 1988, Beust et al. 1990,
Vidal-Madjar et al. 1994, 1998). For such a planetary system,
comets per year with
kg s-1 at
AU (Beust 1995, Beust et al.
1996). Note that Pictoris is
young but on the main sequence (Crifo et al. 1997), its age is few
percents of the age of the solar system. Therefore, in a set of 30 000
stars there should be about stars
with about the same activity as
Pictoris. Thus, few thousands
comets could be expected with a survey at
accuracy. We consider it as the
optimistic case.
The solar system is likely not exceptional. The bottom-line in
Fig. 5 is a good estimate of the lower limit of the expected number of
detections. Younger stars may have a higher level of activity, with a
larger number of comets; but, although infrared excess have been
observed around many main sequence stars,
Pictoris is certainly a very
peculiar case (Vidal-Madjar et al. 1998). Thus, the top-line in Fig. 5
gives a good estimate of the upper limit of the expected number of
detections.
Note that the major assumption that the dust production rates in
the solar system can be extrapolated to large values is realistic. A
large rate has effectively been observed in the recent comet Hale-Bopp
where it reached of few times
kg s-1 at
about 1 AU (Rauer H. et al., 1997, Schleicher et al., 1997, Senay
et al. 1997, Weaver et al., 1997).
It is very likely that in the near future a large number of
extra-solar comets will be detected through occultations.
For comparison, we also evaluate the probability to detect planets
assuming that each star has a planetary system like the solar system.
With an accuracy better than ,
Jupiter can be detected. Below ,
other giant planets are also detectable. But because of their large
orbital periods, their contribution to the number of detections is
smaller than the one from Jupiter. With a total probability of
to detect a giant planet in one
year, the survey of 30000 stars will give
planets. With an accuracy better
than , Earth-like planets start to be
detectable. Because of their smaller distance to the star, they have
larger contribution to the probability of planet detection. The Earth
and Venus can be detected with a probability of
in one year. Mars and Mercury,
which are detectable with an accuracy of
, give a total probability of
. The comparison with the number of
detection of comets shows that accurate photometric surveys should
detect more comets than planets.
© European Southern Observatory (ESO) 1999
Online publication: March 1, 1999
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