OVERSTABLE LIBRATIONS CAN ACCOUNT FOR THE PAUCITY OF MEAN MOTION RESONANCES AMONG EXOPLANET PAIRS

被引:161
作者
Goldreich, Peter [1 ,2 ]
Schlichting, Hilke E. [3 ]
机构
[1] CALTECH, Pasadena, CA 91125 USA
[2] Inst Adv Study, Princeton, NJ 08540 USA
[3] MIT, Cambridge, MA 02139 USA
关键词
celestial mechanics; methods: analytical; methods: numerical; planet-disk interactions; planets and satellites: dynamical evolution and stability; planets and satellites: formation; DENSITY WAVES; CAPTURE; PLANET; DISK; EVOLUTION; DYNAMICS; OVERLAP; ORIGIN;
D O I
10.1088/0004-6256/147/2/32
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We assess the multi-planet systems discovered by the Kepler satellite in terms of current ideas about orbital migration and eccentricity damping due to planet-disk interactions. Our primary focus is on mean motion resonances. Only a few percent of planet pairs are in close proximity to a resonance. However, predicted migration rates (parameterized by tau(n)=n/vertical bar(n)vertical bar) over dot imply that during convergent migration most planets would have been captured into first order resonances. Eccentricity damping (parameterized by tau(e)=e/vertical bar(e) over dot vertical bar) offers a plausible resolution. Estimates suggest tau(e)/tau(n) similar to (h/a)(2) similar to 10(-2), where $h/a$ is the ratio of disk thickness to radius. Together, eccentricity damping and orbital migration give rise to an equilibrium eccentricity, e(eq) similar to (tau(e)/tau(n))(1/2). Capture is permanent provided e(eq) < mu(1/3), where mu denotes the planet to star mass ratio. But for e(eq) less than or similar to mu(1/3), capture is only temporary because librations around equilibrium are overstable and lead to passage through resonance on timescale tau(e). Most Kepler planet pairs have e(eq)>mu(1/3). Since tau(n)>>tau(e) is the timescale for migration between neighboring resonances, only a modest percentage of pairs end up trapped in resonances after the disk disappears. Planet pairs close to a mean motion resonance typically exhibit period ratios 1-2% larger than those for exact resonance. The direction of this shift undoubtedly reflects the same asymmetry that requires convergent migration for resonance capture. Permanent resonance capture at these separations from exact resonance would demand mu (tau(n)/tau(e))(1/2) greater than or similar to 0.01, a value that estimates of $\mu$ from transit data and (tau(e)/tau(n))(1/2) from theory are insufficient to match. Plausible alternatives involve eccentricity damping during or after disk dispersal. (Abridged)
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