2017ApJ...834...55G


Query : 2017ApJ...834...55G

2017ApJ...834...55G - Astrophys. J., 834, 55-55 (2017/January-1)

P-type planet-planet scattering: Kepler close binary configurations.

GONG Y.-X.

Abstract (from CDS):

A hydrodynamical simulation shows that a circumbinary planet will migrate inward to the edge of the disk cavity. If multiple planets form in a circumbinary disk, successive migration will lead to planet-planet scattering (PPS). PPS of Kepler-like circumbinary planets is discussed in this paper. The aim of this paper is to answer how PPS affects the formation of these planets. We find that a close binary has a significant influence on the scattering process. If PPS occurs near the unstable boundary of a binary, about 10% of the systems can be completely destroyed after PPS. In more than 90% of the systems, there is only one planet left. Unlike the eccentricity distribution produced by PPS in a single star system, the surviving planets generally have low eccentricities if PPS take place near the location of the currently found circumbinary planets. In addition, the ejected planets are generally the innermost of two initial planets. The above results depend on the initial positions of the two planets. If the initial positions of the planets are moved away from the binary, the evolution tends toward statistics similar to those around single stars. In this process, the competition between the planet-planet force and the planet-binary force makes the eccentricity distribution of surviving planets diverse. These new features of P-type PPS will deepen our understanding of the formation of these circumbinary planets.

Abstract Copyright: © 2016. The American Astronomical Society. All rights reserved.

Journal keyword(s): binaries: close - methods: numerical - planets and satellites: dynamical evolution and stability - planets and satellites: individual: Kepler circumbinary planets - planets and satellites: individual: Kepler circumbinary planets

Simbad objects: 20

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Number of rows : 20
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 Kepler-453 EB* 18 52 57.9087897864 +46 22 42.553340616           G5 90 0
2 Kepler-453b Pl 18 52 57.9087897864 +46 22 42.553340616           ~ 35 0
3 Kepler-38b Pl 19 07 19.2812772264 +42 16 45.121212624           ~ 60 1
4 Kepler-38 EB* 19 07 19.2812772264 +42 16 45.121212624           ~ 107 1
5 Kepler-413 EB* 19 14 02.5619727768 +51 09 45.019100160           ~ 89 0
6 Kepler-413b Pl 19 14 02.5619727768 +51 09 45.019100160           ~ 66 0
7 Kepler-16b Pl 19 16 18.1758378936 +51 45 26.782726104           ~ 178 1
8 Kepler-16 SB* 19 16 18.1758378936 +51 45 26.782726104   12.1   11.90   K7V 274 1
9 Kepler-35b Pl 19 37 59.2726213344 +46 41 22.952695956           ~ 99 1
10 Kepler-35 EB* 19 37 59.2726213344 +46 41 22.952695956           ~ 146 1
11 Kepler-47b Pl 19 41 11.4983203032 +46 55 13.707336288           ~ 86 1
12 Kepler-47 EB* 19 41 11.4983203032 +46 55 13.707336288           ~ 185 1
13 Kepler-47d Pl 19 41 11.4983203032 +46 55 13.707336288           ~ 32 0
14 Kepler-47c Pl 19 41 11.4983203032 +46 55 13.707336288           ~ 79 1
15 Kepler-34b Pl 19 45 44.5974898536 +44 38 29.610983076           ~ 115 1
16 Kepler-34 EB* 19 45 44.5974898536 +44 38 29.610983076           ~ 181 1
17 Kepler-1647 EB* 19 52 36.0203935200 +40 39 22.342749552           F5 84 0
18 Kepler-1647b Pl 19 52 36.0203935200 +40 39 22.342749552           ~ 52 0
19 Kepler-64b Pl 19 52 51.6169691968 +39 57 18.370395541           ~ 55 1
20 Kepler-64 EB* 19 52 51.6169691968 +39 57 18.370395541           F0 107 1

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