2008ApJ...687L.107R


Query : 2008ApJ...687L.107R

2008ApJ...687L.107R - Astrophys. J., 687, L107-L110 (2008/November-2)

Mean motion resonances from planet-planet scattering.

RAYMOND S.N., BARNES R., ARMITAGE P.J. and GORELICK N.

Abstract (from CDS):

Planet-planet scattering is the leading mechanism to explain the large eccentricities of the observed exoplanet population. However, scattering has not been considered important to the production of pairs of planets in mean motion resonances (MMRs). We present results from a large number of numerical simulations of dynamical instabilities in three-planet systems. We show that MMRs arise naturally in about 5% of cases. The most common resonances we populate are the 2:1 and 3:1 MMRs, although a wide variety of MMRs can occur, including high-order MMRs (up to 11th order). MMRs are generated preferentially in systems with uneven mass distributions: the smallest planet is typically ejected after a series of close encounters, leaving the remaining, more massive planets in resonance. The distribution of resonant planets is consistent with the phase-space density of resonant orbits, meaning that planets are randomly thrown into MMRs rather than being slowly pulled into them. It may be possible to distinguish between MMRs created by scattering versus convergent migration in a gaseous disk by considering planetary mass ratios: resonant pairs of planets beyond ∼1 AU with more massive outer planets are likely to have formed by scattering. In addition, scattering may be responsible for pairs of planets in high-order MMRs (3:1 and higher) that are not easily populated by migration. The frequency of MMRs from scattering is comparable to the expected survival rate of MMRs in turbulent disks. Thus, planet-planet scattering is likely to be a major contributor to the population of resonant planets.

Abstract Copyright: ∼

Journal keyword(s): Stars: Planetary Systems: Formation - Methods: {em n}-Body Simulations

Simbad objects: 28

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Number of rows : 28
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 HD 17156 PM* 02 49 44.4871034544 +71 45 11.629235988   8.78 8.16     F9V 195 2
2 HD 17156b Pl 02 49 44.4871034544 +71 45 11.629235988           ~ 197 1
3 HD 73526c Pl 08 37 16.4833548528 -41 19 08.790456324           ~ 45 1
4 HD 73526b Pl 08 37 16.4833548528 -41 19 08.790456324           ~ 56 1
5 HD 73526 PM* 08 37 16.4833548528 -41 19 08.790456324   9.69 9.00     G6V 206 2
6 L 675-81 Pe* 08 40 59.2057867166 -23 27 22.592748045   13.2 11.975 11.637 9.37 M3.5V 180 1
7 NAME L 675-81b Pl 08 40 59.2057867166 -23 27 22.592748045           ~ 40 1
8 HD 82943b Pl 09 34 50.7353072232 -12 07 46.369202196           ~ 102 1
9 HD 82943c Pl 09 34 50.7353072232 -12 07 46.369202196           ~ 88 1
10 HD 82943 PM* 09 34 50.7353072232 -12 07 46.369202196   7.17 6.53     F9VFe+0.5 498 2
11 HD 108874c Pl 12 30 26.8817398344 +22 52 47.377485192           ~ 40 1
12 HD 108874b Pl 12 30 26.8817398344 +22 52 47.377485192           ~ 52 1
13 HD 108874 PM* 12 30 26.8817398344 +22 52 47.377485192   9.49   8.3   G9V 182 1
14 HD 128311b Pl 14 36 00.5602765558 +09 44 47.454573266           ~ 74 1
15 HD 128311 BY* 14 36 00.5602765558 +09 44 47.454573266 9.232 8.441 7.446 6.895 6.425 K3V 338 1
16 HD 128311c Pl 14 36 00.5602765558 +09 44 47.454573266           ~ 63 1
17 * mu. Ara PM* 17 44 08.7031414872 -51 50 02.591603160   5.85 5.15     G3IV-V 578 2
18 * mu. Ara b Pl 17 44 08.7031414872 -51 50 02.591603160           ~ 95 2
19 * mu. Ara d Pl 17 44 08.7031414872 -51 50 02.591603160           ~ 70 2
20 HD 202206c Pl 21 14 57.7686051936 -20 47 21.161521320           ~ 46 1
21 HD 202206b Pl 21 14 57.7686051936 -20 47 21.161521320           ~ 57 1
22 HD 202206 PM* 21 14 57.7686051936 -20 47 21.161521320   8.79 8.07     G6V 246 1
23 HD 208487 PM* 21 57 19.8476861856 -37 45 49.045448556   8.02 7.47     G1/3(V) 138 1
24 HD 208487c Pl? 21 57 19.8476861856 -37 45 49.045448556           ~ 5 1
25 HD 208487b Pl 21 57 19.8476861856 -37 45 49.045448556           ~ 31 1
26 BD-15 6290 BY* 22 53 16.7325836486 -14 15 49.304052185 12.928 11.749 10.192 9.013 7.462 M3.5V 1106 1
27 BD-15 6290b Pl 22 53 16.7325836486 -14 15 49.304052185           ~ 266 1
28 BD-15 6290c Pl 22 53 16.7325836486 -14 15 49.304052185           ~ 202 1

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