TY - JOUR
T1 - Conditions of dynamical stability for the HD 160691 planetary system
AU - Bois, Eric
AU - Rambaux, Nicolas
AU - Pilat-Lohinger, Elke
N1 - Affiliations: Observatoire de Bordeaux, 2 rue d'Observatoire, F-33270 Floirac, France; Deptartment of Mathematics, School of Science, St. Mary's College of California, Moraga, CA 94575; Institute of Astronomy, University of Vienna, Türkenschanzstrasse 17, A-1180 Vienna, Austria
Adressen: Bois, E.; Observatoire de Bordeaux; 2 rue d'Observatoire F-33270 Floirac, France; email: [email protected]
Source-File: AstroScopus.csv
Import aus Scopus: 2-s2.0-0346969595
Importdatum: 14.12.2006 13:56:49
PY - 2003
Y1 - 2003
N2 - In our previous paper we showed that the currently determined orbital
parameters placed four recently announced planetary systems (HD 12661,
HD 38529, HD 37124, and HD 160691) in very different situations from the
point of view of dynamical stability. In the present paper we deal with
the last of these systems, whose orbital parameters of the outer planet
are yet uncertain. We discover a stabilizing mechanism that could be
the key to its existence. The paper is devoted to the study of this
mechanism by a global dynamics analysis in the orbital parameter space
related to the HD 160691 system. We obtained our results using a new
technique called the mean exponential growth factor of nearby orbits
(MEGNO), and verified them with the fast Lyapunov indicator technique
(FLI). In order to be dynamically stable, the HD 160691 planetary system
has to satisfy the following conditions: (1) it should have a 2 : 1
mean motion resonance, (2) combined with an apsidal secular resonance,
(3) in a configuration Pc(ap)-S-Pb(ap) (which means that the planets c and b may be considered as initially located at their apoastron around the central star S),
and (4) it must satisfy specific conditions for the respective sizes of
the eccentricities. High eccentricity for the outer orbit (ec > 0.52) is the most probable necessary condition, while the eccentricity of the inner orbit eb becomes relatively unimportant when ec
> 0.7. We also show that there is an upper limit for planetary
masses (in the interval permitted by the undetermined line-of-sight
inclination factor sin il) due to the dynamical stability mechanism. More generally, in this original orbital topology, where the resonance variables θ1 and θ3 librate about 180° while θ2
librates about 0°, the HD 160691 system and its mechanism have revealed
aspects of the 2 : 1 orbital resonances that have not been observed nor
analyzed before. The present topology with antialigned apsidal lines,
combined with the 2 : 1 resonance, is indeed more wide-ranging than the
particular case of the HD 160691 planetary system. It is a new
theoretical possibility that is suitable for a stable regime despite
relatively small semimajor axes with respect to the important masses in
interactions.
AB - In our previous paper we showed that the currently determined orbital
parameters placed four recently announced planetary systems (HD 12661,
HD 38529, HD 37124, and HD 160691) in very different situations from the
point of view of dynamical stability. In the present paper we deal with
the last of these systems, whose orbital parameters of the outer planet
are yet uncertain. We discover a stabilizing mechanism that could be
the key to its existence. The paper is devoted to the study of this
mechanism by a global dynamics analysis in the orbital parameter space
related to the HD 160691 system. We obtained our results using a new
technique called the mean exponential growth factor of nearby orbits
(MEGNO), and verified them with the fast Lyapunov indicator technique
(FLI). In order to be dynamically stable, the HD 160691 planetary system
has to satisfy the following conditions: (1) it should have a 2 : 1
mean motion resonance, (2) combined with an apsidal secular resonance,
(3) in a configuration Pc(ap)-S-Pb(ap) (which means that the planets c and b may be considered as initially located at their apoastron around the central star S),
and (4) it must satisfy specific conditions for the respective sizes of
the eccentricities. High eccentricity for the outer orbit (ec > 0.52) is the most probable necessary condition, while the eccentricity of the inner orbit eb becomes relatively unimportant when ec
> 0.7. We also show that there is an upper limit for planetary
masses (in the interval permitted by the undetermined line-of-sight
inclination factor sin il) due to the dynamical stability mechanism. More generally, in this original orbital topology, where the resonance variables θ1 and θ3 librate about 180° while θ2
librates about 0°, the HD 160691 system and its mechanism have revealed
aspects of the 2 : 1 orbital resonances that have not been observed nor
analyzed before. The present topology with antialigned apsidal lines,
combined with the 2 : 1 resonance, is indeed more wide-ranging than the
particular case of the HD 160691 planetary system. It is a new
theoretical possibility that is suitable for a stable regime despite
relatively small semimajor axes with respect to the important masses in
interactions.
U2 - 10.1086/378796
DO - 10.1086/378796
M3 - Article
SN - 0004-637X
VL - 598
SP - 1312
EP - 1320
JO - The Astrophysical Journal: an international review of astronomy and astronomical physics
JF - The Astrophysical Journal: an international review of astronomy and astronomical physics
IS - 2 I
ER -