Up: A spectroscopic study of family
Themis family is located in the outer part of the main belt with proper
semi-major axis in the region from 3.06 to 3.23 AU. The orbits have
relatively high eccentricities and small inclinations. The Themis family, as
determined by
Zappalà et al. (1995) has 550 members: four - 24 Themis,
90 Antiope, 171 Ophelia, and 268 Adorea - with a diameter greater than
100 km, ten with diameter in the range 50-100 km while the remaining are
smaller than 50 km. The expected size
limit of completeness for this family
corresponds to 20 km (Zappalà & Cellino 1995).
According to
Migliorini et al. (1995),
the expected number of interlopers is relatively low, even if
one or two can be expected at sizes as large as 40 km.
The distributions of the proper elements in the a-e,
and
planes are shown in Fig. 1, using
Milani & Knezevic (1994) proper
elements. In this figure the sizes of the circles are proportional to the
diameter of the objects and the open circles indicate objects observed in
the present work. The two stars indicate objects which might be interlopers as
will be discussed in the next section. A core-halo structure, in which a
dense "core'' is surrounded by a "halo'' of decreasing density, was
initially described by
Williams (1979, 1992). However, more recent studies do
not present such a distribution but mostly a vertical dispersion at the border
coincident with the 2/1 resonance.
Zappalà et al. (1995) even introduce
the denomination of "tribe'' for this family due to its particular space
distribution.
![\begin{figure}
\includegraphics [width=11cm,clip=]{fig1.eps}\end{figure}](/articles/aas/full/1999/03/ds7929/Timg4.gif) |
Figure 1:
Distribution of the Themis family in proper elements
phase space: a) semi-major axis
eccentricity, b) semi-major axis
sine of inclination,
and c) eccentricity sine of
inclination.
The size of the circles is proportional to
the diameter of the objects and the open circles indicate
those observed in the present work (available on-line) |
Since the pioneer work of
Hirayama (1918) it has been assumed that families
of asteroids are the outcome of one, or more, large impact of a body with a
smaller "projectile'' leading to the complete fragmentation or to the erosion
of the parent body. From a statistical point of view this hypothesis is
confirmed by the clustering observed when the planetary perturbations are
removed, i.e., in the proper elements phase space. In this sense Themis
family is undoubtedly one of the most reliable. However, the breakup
mechanism which originated any family, as well as the subsequent evolution
of its fragments, still rely on a wide set of
working hypotheses and initial
parameters which may not be the real ones (see, for example,
Farinella et al. 1982;
Fujiwara 1982;
Zappalà et al. 1984;
Davis et al. 1985;
Farinella & Davis 1992;
Bottke et al. 1994;
Marzari et al. 1995).
Notwithstanding the limitation of these models, some hypotheses on the
Themis family formation are mostly accepted: i) The parent body was
completely disrupted; ii) The family is the outcome of a very energetic
collision, probably unique in all the asteroid belt, with original parent
body and projectile of 380 km and 190 km, respectively
(Marzari et al. 1995);
iii) Such a collision has a very low probability to occur over the age of
the Solar System; iv) The large remnants are probably "rubble-piles'' shaped
by their self-gravitation
(Fujiwara 1982;
Farinella et al. 1982). The
mineralogical characterization of Themis family members' surfaces can,
therefore, help to constrain the collisional model of its formation.
Up: A spectroscopic study of family
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