The Dynamics of Three-Planet Systems: an Approach from Dynamical System

TL;DR

This paper investigates the stability and chaotic behavior of three-planet systems using dynamical systems theory, revealing how quasi-stability transitions to chaos through phase space structures like KAM tori and satellite tori.

Contribution

It introduces a detailed analysis of three-planet system dynamics using Lyapunov exponents and power spectra, highlighting the role of phase space structures in quasi-stability and chaos.

Findings

System is nearly non-chaotic initially, then intermittently chaotic.

Power-law distributions for orbital eccentricities and durations of quasi-stable states.

Phase space contains KAM tori, satellite tori, and chaotic regions, explaining observed behaviors.

Abstract

We study in detail the motions of three planets interacting with each other under the influence of a central star. It is known that the system with more than two planets becomes unstable after remaining quasi-stable for long times, leading to highly eccentric orbital motions or ejections of some of the planets. In this paper, we are concerned with the underlying physics for this quasi-stability as well as the subsequent instability and advocate the so-called "stagnant motion" in the phase space, which has been explored in the field of dynamical system. We employ the Lyapunov exponent, the power spectra of orbital elements and the distribution of the durations of quasi-stable motions to analyze the phase space structure of the three-planet system, the simplest and hopefully representative one that shows the instability. We find from the Lyapunov exponent that the system is almost non-chaotic in the initial quasi-stable state whereas it becomes intermittently chaotic thereafter. The non-chaotic motions produce the horizontal dense band in the action-angle plot whereas the voids correspond to the chaotic motions. We obtain power laws for the power spectra of orbital eccentricities. Power-law distributions are also found for the durations of quasi-stable states. All these results combined together, we may reach the following picture: the phase space consists of the so-called KAM tori surrounded by satellite tori and imbedded in the chaotic sea. The satellite tori have a self-similar distribution and are responsible for the scale-free power-law distributions of the duration times. The system is trapped around one of the KAM torus and the satellites for a long time (the stagnant motion) and moves to another KAM torus with its own satellites from time to time, corresponding to the intermittent chaotic behaviors.