2019
DOI: 10.1093/mnras/stz354
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Chaotic Tides in Migrating Gas Giants: Forming Hot and Transient Warm Jupiters via Lidov-Kozai Migration

Abstract: High-eccentricity migration is an important channel for the formation of hot Jupiters (HJs). In particular, Lidov-Kozai (LK) oscillations of orbital eccentricity/inclination induced by a distant planetary or stellar companion, combined with tidal friction, have been shown to produce HJs on Gyr timescales, provided that efficient tidal dissipation operates in the planet. We re-examine this scenario with the inclusion of dynamical tides. When the planet's orbit is in a high-eccentricity phase, the tidal force fr… Show more

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Cited by 66 publications
(77 citation statements)
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References 69 publications
(112 reference statements)
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“…For planets that are formed at large semimajor axes and have been undergoing high-eccentricity tidal migration, we would expect to observe them only in the gray region if they are decoupled from their perturber. We also show the constant angular momentum track for planets with periapses small enough that they could excite planetary f-mode dissipation (Wu 2018;Vick et al 2019). Above the dashed line, the planet's periapse is close enough to the host star to excite f-mode oscillation which leads to rapid orbital decay from a "cold" Jupiter to a "warm" Jupiter, so we expect an absence of highly elliptical Jupiters (i.e., e > 0.9) above that line.…”
Section: Discussion and Future Workmentioning
confidence: 93%
“…For planets that are formed at large semimajor axes and have been undergoing high-eccentricity tidal migration, we would expect to observe them only in the gray region if they are decoupled from their perturber. We also show the constant angular momentum track for planets with periapses small enough that they could excite planetary f-mode dissipation (Wu 2018;Vick et al 2019). Above the dashed line, the planet's periapse is close enough to the host star to excite f-mode oscillation which leads to rapid orbital decay from a "cold" Jupiter to a "warm" Jupiter, so we expect an absence of highly elliptical Jupiters (i.e., e > 0.9) above that line.…”
Section: Discussion and Future Workmentioning
confidence: 93%
“…This is because gravitational scattering in the dense environment near SgrA* causes stochastic change in orbital period of the captured star, with a fractional change per orbit ∆P/P ∼ P/t rel , where t rel is the local relaxation time. For typical mode frequency ω ∼ 3GM * /R 3 * , we find ω∆P ∼ 30(P/20 yr) 3/2 (t rel /1 Gyr) −1/2 (M * /3M ) −1 1 for all cases considered in this work, so the system is in the chaotic tide regime where mode energy can stochastically grow (by ∆E nlm on average in each orbit) and is then rapidly dissipated by non-linear effects (Mardling 1995a,b;Ivanov & Papaloizou 2004;Vick et al 2019).…”
Section: Cumulative Tidal Heatingmentioning
confidence: 78%
“…(i) As an outcome of binary/planetary formation, the primordial density of binaries in the P-M 2 plane was flat, with no BDD. The desert was formed by some later mechanism that caused objects found in the BDD to 'move away' from the 'restricted area' (e.g., Armitage & Bonnell 2002;Damiani & Díaz 2016;Grunblatt et al 2018;Vick et al 2019). This could happen by…”
Section: Discussionmentioning
confidence: 99%