Science
Nugget—Exosolar Planetesimals
Charles
M. Telesco, Department of Astronomy, University of Florida
The
impressive progress in discovering exoplanets, now numbering
over 200, has resulted quite remarkably in our beginning to view
these as complex "systems" with
many interacting components. The several stars that have multiple
planets clearly fall into this category, with enough information
in some cases (e.g., GJ876; Fischer et al. 2003) to indicate,
for example, resonant interactions among them. But a planetary
system consists of more than the star and its planetary entourage.
Gas, dust, asteroids, and comets percolate around and among the
planets, and they have a fascinating story to tell. The evolving
configuration of planetesimals so intimate to the formation of
the planets determines, in non-trivial ways that are apparently
heavily stochastic (Gomes et al. 2007), key planetary properties
such as water content (and therefore life) in the habitable zone
and the occurrence of global catastrophic events like the Solar
System's Late Heavy Bombardment. Determining the nature and distribution
of planetesimals in a young system is therefore a key constraint
guiding our assessment of the multiple possible outcomes of the
planet formation process.
Particularly
at mid-IR (3-30 µm) wavelengths, TMT will have
an enormous impact on the detailed study of these early asteroid
and Kuiper-Belt analogs around other stars, as illustrated by the
recent resolution, the first ever, of a probable asteroid-belt
analog orbiting the 230 million year-old A star Zeta Leporis located
21 pc away (Moerchen et al. 2007). The excess IR thermal emission
at 18 μm from Zeta Lep arises in warm starlight-heated dust
particles apparently generated by grinding collisions among a population
of planetesimals located about 3 AU from the star, a distribution
comparable in size to our asteroid belt (see Figure 1). Simple
modeling of the azimuthally averaged brightness profile (Figure
2) suggests that there are two dust annuli, the outer perhaps associated
with the smaller-sized, "higher-ß" particles, which
have periastrons within the inner annulus and apastons in the outer
one. But this source is barely resolved at 18 μm with an 8-m
telescope, so this model is highly speculative.
The
nearly four-times better angular resolution of TMT (Figure 3)
would reveal not only the radial structure of the emitting particles
around Ζ Lep, but also the azimuthal structure, which holds
clues to the actual origin of the particles. Their azimuthal distribution
(and therefore that of their parent bodies) might be uniform and
indicative of steady grinding of a vast ring full of planetesimals
the dynamical stability of which reflects an intimate balancing
act with an ensemble of planets. Such appears to be the case for
the unresolved asteroidal dust ring (Beichman et al. 2005) orbiting
at about 1 AU in the triple Neptune system associated with the
K0 V star HD69830 (Lovis et al 2006).
But
the "ring" may,
instead, be clumpy. Clumpiness could result, for example, from
resonant trapping of the planetesimals, as is the case for the
Trojan asteroids at Jupiter's L4 and L5 points, or it might hint
at a single, more catastrophic event, as may have been observed
in the thermal IR in the central part of the Kuiper Belt surrounding
the 10-20 million-year-old A star Beta Pictoris (Telesco et al.
2005). If the emitting region is highly structured, with many
unresolved features, rather than uniform, the mid-IR integration
time needed to probe this texture will be nearly 200 times less
with TMT than with the largest groundbased telescopes now in
operation. These stunning gains will open the door dramatically
to the exploration of exosolar planetesimals.

Figure 1.
Azimuthally
averaged profiles at 18.3 µm made at Gemini
South of Ζ Lep (red dots) and a PSF star (black dots). Ζ Lep
is wider, and the excess thermal IR emission appears associated
with dust particles orbiting at 3.0 ± 0.3 AU (Moerchen et
al. 2007)

Figure 2.
A best-fit model to the profile of Ζ Lep. The two model annuli
represent flux levels to the profile in Figure 1. The inner and
out annuli, which are suggestive only, have widths of 2-4 AU and
4-8 AU, respectively.

Figure 3.
A cross-section of the model (Figure 2) compared to the actual
point-spread-function (PSF) profile at 18.3 µm with the
8-m Gemini telescope (broad Gaussian-like curve) and that expected
with the TMT (narrow Gaussian-like curve).
References
Beichman C. A., et al. 2005, ApJ, 626, 1061.
Fischer, D. A., et al. 2003, ApJ, 586, 1394.
Gomes, R., Levison, H. F., Tsiganis, K., & Morbidelli, A. 2007,
Nature, 435, 466.
Lovis C., et al 2006, Nature, 441, 305.
Moerchen, M. M., Telesco, C. M., Packham, C., & Kehoe, T. J.
J. 2007, ApJ, 655, L109.
Telesco, C. M., et al. 2005, Nature, 433, 133.
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