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ejected subsequently by the planet as it migrates further inward. This allows the planet to migrate a substantial fraction of its<br />

initial semimajor axis by ejecting planetesimals.<br />

Author<br />

Extrasolar Planets; Protoplanets; Planetary Orbits; Orbital Mechanics<br />

20040074152 Naval Observatory, Washington, DC, USA, National Radio Astronomy Observatory, Socorro, NM, USA<br />

Ground-State SiO Maser Emission Toward Evolved Stars<br />

Boboltz, D. A.; Claussen, M. J.; Feb. 20, 2004; 18 pp.; In English; Original contains color illustrations<br />

Report No.(s): AD-A422690; No Copyright; Avail: CASI; A03, Hardcopy<br />

We have made the first unambiguous detection of vibrational ground-state maser emission from 28SiO toward six evolved<br />

stars. Using the Very Large Array, we simultaneously observed the v = 0,J = 1-0, 43.4-GHz, groundstate <strong>and</strong> the v = 1,J = 1-0,<br />

43.1-GHz, first excited-state transitions of 28SiO toward the oxygen-rich evolved stars IRC+10011, o Ceti, W Hya, RX Boo,<br />

NML Cyg, <strong>and</strong> R Cas <strong>and</strong> the S-type star chi Cyg. We detected at least one v=0SiOmaser feature from six of the seven<br />

stars observed, with peak maser brightness temperatures ranging from 10000 K to 108800 K. In fact, four of the seven v =<br />

0 spectra show multiple maser peaks, a phenomenon which has not been previously observed. Ground-state thermal emission<br />

was detected for one of the stars, RX Boo, with a peak brightness temperature of 200 K. Comparing the v=0<strong>and</strong>thev=<br />

1 transitions, we find that the ground-state masers are much weaker with spectral characteristics different from those of the<br />

first excited-state masers. For four of the seven stars the velocity dispersion is smaller for the v=0emission than for the v<br />

= 1 emission, for one star the dispersions are roughly equivalent, <strong>and</strong> for two stars (one of which is RX Boo) the velocity<br />

spread of the v=0emission is larger. In most cases, the peak flux density in the v = 0 emission spectrum does not coincide<br />

with the v=1maser peak. Although the angular resolution of these VLA observations were insufficient to completely resolve<br />

the spatial structure of the SiO emission, the SiO spot maps produced from the interferometric image cubes suggest that the<br />

v = 0 masers are more extended than their v=1counterparts.<br />

DTIC<br />

Ground State; Interferometry; Masers; Radio Astronomy<br />

20040074164 Harvard-Smithsonian Center for Astrophysics, Cambridge, MA, USA<br />

Long-Term Stability of Planets in Binary Systems<br />

Holman, Matthew J.; Wiegert, Paul A.; The Astronomical Journal; 1′999; Volume 117, pp. 621-628; In English<br />

Contract(s)/Grant(s): NAG5-10365; No Copyright; Avail: Other Sources; Abstract Only<br />

A simple question of celestial mechanics is investigated: in what regions of phase space near a binary system can planets<br />

persist for long times? The planets are taken to be test particles moving in the field of an eccentric binary system. A range of<br />

values of the binary eccentricity <strong>and</strong> mass ratio is studied, <strong>and</strong> both the case of planets orbiting close to one of the stars, <strong>and</strong><br />

that of planets outside the binary orbiting the systems center of mass, are examined. From the results, empirical expressions<br />

are developed for both (1) the largest orbit around each of the stars <strong>and</strong> (2) the smallest orbit around the binary system as a<br />

whole, in which test particles survive the length of the integration (10A4 binary periods). The empirical expressions<br />

developed, which are roughly linear in both the mass ratio mu <strong>and</strong> the binary eccentricity e, are determined for the range<br />

0.0=e=0.7-0.8 <strong>and</strong> 0.1=mu=0.9 in both regions <strong>and</strong> can be used to guide searches for planets in binary systems. After<br />

considering the case of a single low-mass planet in binary systems, the stability of a mutually interacting system of planets<br />

orbiting one star of a binary system is examined, though in less detail.<br />

Author<br />

Planets; Center of Mass; Eccentricity; Celestial Mechanics; Systems Stability<br />

20040074165 Harvard-Smithsonian Center for Astrophysics, Cambridge, MA, USA<br />

On the Origin of Chaos in the Asteroid Belt<br />

Murray, N.; Holman, M.; Potter, M.; The Astronomical Journal; 1998; Volume 116, pp. 2583-2589; In English<br />

Contract(s)/Grant(s): NAG5-10365; No Copyright; Avail: Other Sources; Abstract Only<br />

We consider the effect of gravitational perturbations from Jupiter on the dynamics of asteroids, when Jupiter is itself<br />

perturbed by Saturn. The presence of Saturn introduces a number of additional frequencies into Jupiters orbit. These<br />

frequencies in turn produce chaos in narrow regions on either side of the chaotic zones associated with the mean motion<br />

resonances between the asteroids <strong>and</strong> Jupiter. The resonant arguments of these three-body resonances contain the longitudes<br />

of Jupiter <strong>and</strong> the asteroid together with either the secular frequency 9-6, or the longitude of Saturn. Resonances involving<br />

the longitude of Saturn are analogs of the Laplace resonance in the Jovian satellite system. We show that many three-body<br />

296

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