2003ApJ...592.1201L


Query : 2003ApJ...592.1201L

2003ApJ...592.1201L - Astrophys. J., 592, 1201-1216 (2003/August-1)

Secular evolution of hierarchical planetary systems.

LEE M.H. and PEALE S.J.

Abstract (from CDS):

We investigate the dynamical evolution of coplanar, hierarchical, two-planet systems where the ratio of the orbital semimajor axes α=a1/a2is small. Hierarchical two-planet systems are likely to be ubiquitous among extrasolar planetary systems. We show that the orbital parameters obtained from a multiple-Kepler fit to the radial velocity variations of a host star are best interpreted as Jacobi coordinates and that Jacobi coordinates should be used in any analyses of hierarchical planetary systems. An approximate theory that can be applied to coplanar, hierarchical, two-planet systems with a wide range of masses and orbital eccentricities is the octopole-level secular perturbation theory, which is based on an expansion to order α3 and orbit averaging. It reduces the coplanar problem to 1 degree of freedom, with e1(or e2) and {piv}1-{piv}2as the relevant phase-space variables (where e1,2are the orbital eccentricities of the inner and outer orbits, respectively, and {piv}1,2are the longitudes of periapse). The octopole equations show that if the ratio of the maximum orbital angular momenta, λ=L1/L2~(m1/m2)α1/2, for given semimajor axes is approximately equal to a critical value λcrit, then libration of {piv}1-{piv}2about either 0° or 180° is almost certain, with possibly large amplitude variations of both eccentricities. From a study of the HD 168443 and HD 12661 systems and their variants using both the octopole theory and direct numerical orbit integrations, we establish that the octopole theory is highly accurate for systems with α≲0.1 and reasonably accurate even for systems with α as large as (1)/(3), provided that α is not too close to a significant mean-motion commensurability or above the stability boundary. The HD 168443 system is not in a secular resonance, and its {piv}1-{piv}2circulates. The HD 12661 system is the first extrasolar planetary system found to have {piv}1-{piv}2librating about 180°. The secular resonance means that the lines of apsides of the two orbits are on average antialigned, although the amplitude of libration of {piv}1-{piv}2is large. The libration of {piv}1-{piv}2and the large amplitude variations of both eccentricities in the HD 12661 system are consistent with the analytic results on systems with λ~λcrit. The evolution of the HD 12661 system with the best-fit orbital parameters and sini=1 (i is the inclination of the orbital plane from the plane of the sky) is affected by the close proximity to the 11:2 mean-motion commensurability, but small changes in the orbital period of the outer planet within the uncertainty can result in configurations that are not affected by mean-motion commensurabilities. The stability of the HD 12661 system requires sini>0.3.

Abstract Copyright: ∼

Journal keyword(s): Celestial Mechanics - Stars: Planetary Systems - Planets and Satellites: General

Errata: erratum vol. 597, p. 644 (2003)

Simbad objects: 24

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Number of rows : 24
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 * ups And c Pl 01 36 47.8415443907 +41 24 19.651368029           ~ 163 1
2 * ups And d Pl 01 36 47.8415443907 +41 24 19.651368029           ~ 171 1
3 * ups And PM* 01 36 47.8415443907 +41 24 19.651368029 4.70 4.64 4.10 3.64 3.35 F9V 1017 1
4 * ups And b Pl 01 36 47.8415443907 +41 24 19.651368029           ~ 284 1
5 HD 12661 PM* 02 04 34.2881404104 +25 24 51.513637932   8.16   7.0   K0V 278 1
6 HD 12661b Pl 02 04 34.2881404104 +25 24 51.513637932           ~ 73 1
7 HD 12661c Pl 02 04 34.2881404104 +25 24 51.513637932           ~ 61 1
8 * rho01 Cnc b Pl 08 52 35.8111044043 +28 19 50.954994470           ~ 267 1
9 * rho01 Cnc d Pl 08 52 35.8111044043 +28 19 50.954994470           ~ 163 1
10 * rho01 Cnc c Pl 08 52 35.8111044043 +28 19 50.954994470           ~ 154 1
11 * rho01 Cnc PM* 08 52 35.8111044043 +28 19 50.954994470 7.45 6.82   5.4   K0IV-V 1223 1
12 HD 82943c Pl 09 34 50.7353072232 -12 07 46.369202196           ~ 88 1
13 HD 82943b Pl 09 34 50.7353072232 -12 07 46.369202196           ~ 102 1
14 HD 82943 PM* 09 34 50.7353072232 -12 07 46.369202196   7.17 6.53     F9VFe+0.5 498 2
15 HD 83443 PM* 09 37 11.8275201048 -43 16 19.933774320   9.03 8.24     K0/1V+G(III) 250 1
16 * 47 UMa c Pl 10 59 27.9727514012 +40 25 48.920572724           ~ 105 1
17 * 47 UMa PM* 10 59 27.9727514012 +40 25 48.920572724   5.66   4.7   G1-VFe-0.5 824 1
18 * 47 UMa b Pl 10 59 27.9727514012 +40 25 48.920572724           ~ 165 1
19 HD 168443c Pl 18 20 03.9332862096 -09 35 44.614653900           ~ 96 1
20 HD 168443b Pl 18 20 03.9332862096 -09 35 44.614653900           ~ 100 1
21 HD 168443 PM* 18 20 03.9332862096 -09 35 44.614653900   7.62 6.92     G6V 334 1
22 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
23 BD-15 6290b Pl 22 53 16.7325836486 -14 15 49.304052185           ~ 266 1
24 BD-15 6290c Pl 22 53 16.7325836486 -14 15 49.304052185           ~ 202 1

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