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The Photoeccentric Effect and Proto-hot Jupiters. III. A Paucity of Proto-hot Jupiters on Super-eccentric Orbits

机译:光偏心效应和原始热木星。三,超偏心轨道上缺乏原始热木星。

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摘要

Gas giant planets orbiting within 0.1 AU of their host stars are unlikely to have formed in situ and are evidence for planetary migration. It is debated whether the typical hot Jupiter smoothly migrated inward from its formation location through the proto-planetary disk, or was perturbed by another body onto a highly eccentric orbit, which tidal dissipation subsequently shrank and circularized during close stellar passages. Socrates and collaborators predicted that the latter model should produce a population of super-eccentric proto-hot Jupiters readily observable by Kepler. We find a paucity of such planets in the Kepler sample, which is inconsistent with the theoretical prediction with 96.9% confidence. Observational effects are unlikely to explain this discrepancy. We find that the fraction of hot Jupiters with an orbital period P > 3 days produced by the star-planet Kozai mechanism does not exceed (at two-sigma) 44%. Our results may indicate that disk migration is the dominant channel for producing hot Jupiters with P > 3 days. Alternatively, the typical hot Jupiter may have been perturbed to a high eccentricity by interactions with a planetary rather than stellar companion, and began tidal circularization much interior to 1 AU after multiple scatterings. A final alternative is that early in the tidal circularization process at high eccentricities tidal circularization occurs much more rapidly than later in the process at low eccentricities, although this is contrary to current tidal theories.
机译:在其主恒星0.1 AU之内运行的天然气巨型行星不太可能在原地形成,并且是行星迁移的证据。有争议的是,典型的热木星是否会从其形成位置顺利地向内迁移通过原行星盘,还是被另一个天体扰动到一个高度偏心的轨道上,潮汐消散随后在恒星通过时收缩并环化了。苏格拉底和合作者预测,后一种模型应能产生开普勒容易观察到的超偏心原始热木星。我们在开普勒样本中发现这种行星很少,这与96.9%的置信度的理论预测不一致。观察效果不太可能解释这种差异。我们发现,由恒星行星Kozai机制产生的,轨道周期P> 3天的热木星所占比例不超过44%(在2σ时)。我们的结果可能表明,磁盘迁移是生产P> 3天的热木星的主要渠道。或者,典型的热木星可能已通过与行星而不是恒星伴星的相互作用而被扰动到很高的偏心率,并在多次散射之后在1 AU内部开始进行潮汐环化。最终的选择是,在高偏心率的潮汐环化过程的早期,比在低偏心率的潮汐环化过程的后期,发生潮环化的速度要快得多,尽管这与当前的潮汐理论相反。

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