Abstract

Abstract High-eccentricity migration is a possible formation channel for hot Jupiters. However, in order for it to be consistent with the observed population of planets, tides must circularize the orbits in an efficient manner. A potential mechanism for such rapid circularization is the diffusive growth of the tidally driven planetary f-mode. Such growth occurs if the f-mode phase at pericenter varies chaotically from one pericenter passage to the next. Previous studies focused on the variation of the orbital period due to tidal back-reaction on the orbit as the source of chaos. Here we show that nonlinear mode interactions can also be an important source. Specifically, we show that nonlinear interactions between a parent f-mode and daughter f-/p-modes induce an energy-dependent shift in the oscillation frequency of the parent. This frequency shift varies randomly from orbit to orbit because the parents’ energy varies. As a result, the parents’ phase at pericenter varies randomly, which we find can trigger it to grow diffusively. We show that the phase shift induced by nonlinear mode interactions in fact dominates the shift induced by tidal back-reaction and lowers the one-kick energy threshold for diffusive growth by about a factor of 5 compared to the prediction from the linear theory. For a given pericenter distance, this reduces the semimajor axis needed to trigger diffusive growth from ≳2 au to ≃1 au. Nonlinear interactions could thus enhance the formation rate of hot Jupiters through the high-eccentricity migration channel and potentially mitigate the discrepancy between the observed and predicted occurrence rates for close-in gas giants as compared to those farther from the star.

Highlights

  • More than 25 yr after the first detection of a hot Jupiter (Mayor & Queloz 1995), we still do not know their dominant formation channel

  • We extend the work of Wu (2018) and Vick & Lai (2018) by considering the effects of weakly nonlinear mode interactions on the f-mode’s diffusive growth

  • We show that the random changes in mode phase induced by three-wave nonlinear interactions act in concert with tidal back-reaction on the orbit in order to lower the threshold for diffusive growth

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Summary

Introduction

More than 25 yr after the first detection of a hot Jupiter (Mayor & Queloz 1995), we still do not know their dominant formation channel. Wu (2018) showed that the diffusive growth of the planet’s l = 2 f-mode during high-eccentricity migration could lead to very rapid orbit circularization (see Vick & Lai 2018; Vick et al 2019). This process was first considered in the hot Jupiter context by Ivanov & Papaloizou (2004) and has been considered in a number of other high-eccentricity systems, e.g., in tidal capture binaries (Kochanek 1992; Mardling 1995) and eccentric neutron star binaries (Vick & Lai 2018).

Linear Problem
Iterative Map Including Only Linear Effects
Orbital and Spin Angular Momentum
Nonlinear Problem
Nonlinear Frequency Shift and Effective Damping Rate
Evolution of the Nonlinear Oscillator
Values of Ω and Γ for a Jupiter Model
Iterative Map Including Nonlinear Effects
Triggering Diffusive Growth
16 We estimate that one would need from evolving into the wave-breaking
Significance of Nonlinear Effects in Other Types of Eccentric
Early Orbital Evolution Following the Onset of Diffusive Growth
Including Spin Effects
Threshold Expressed in Terms of Semimajor Axis Rather Than One-kick Energy
Findings
Conclusion and Discussion
Full Text
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