论文标题
在恒星簇中制作热木星:二进制交易的重要性
Making hot Jupiters in stellar clusters: the importance of binary exchange
论文作者
论文摘要
有人提出,开放群集中热木星(HJS)的发生率可能达到数%,大大高于该领域($ \ sim $ a%)。在一个出色的群集中,当行星系统以恒星二进制散射时,它可能会获得同伴恒星,该星星可能会激发地球轨道偏心中的大幅度von Zeipel-lidov-kozai振荡,从而触发高分子迁移和HJ的形成。我们通过在带有二元恒星和单颗恒星的连续散射的影响下对气体巨星周围的气体巨星的演化进行建模来量化这种机制的效率。我们表明,(1,10)$ au中的行星$ \在一群恒星密度$ n _*= 50 $ pc $^{ - 3} $和二进制分数$ f_ \ mathrm {bin} = 0.5 = 0.5 $ iS ty 2 \%cy conters and conspers contrult of Comperion contrull offers contrull offer Ondion conters contrull of Compers of Compers of Compersion conters contrull of Compers Oull,经验拟合表明,这些结果的总百分比渐近地达到了上限,仅由$ f_ \ mathrm {bin} $确定(例如,$ 10 \%$ at $ f_ \ f_ \ mathrm {bin {bin} = 0.3 $ an ($ n _**\ sim100 $ pc $^{ - 3} $)($ \ sim $ gyr for $ n _*\ sim100 $)。碰撞与潮汐破坏的比率大约有一些,并取决于潮汐模型。因此,如果巨型行星的发生率为10〜%,我们的机制意味着GYR中的HJ发生率为几次0.1〜%,因此可以解释观察到的速率的很大一部分。
It has been suggested that the occurrence rate of hot Jupiters (HJs) in open clusters might reach several per cent, significantly higher than that of the field ($\sim$ a per cent). In a stellar cluster, when a planetary system scatters with a stellar binary, it may acquire a companion star which may excite large amplitude von Zeipel-Lidov-Kozai oscillations in the planet's orbital eccentricity, triggering high-eccentricity migration and the formation of an HJ. We quantify the efficiency of this mechanism by modelling the evolution of a gas giant around a solar mass star under the influence of successive scatterings with binary and single stars. We show that the chance that a planet $\in(1,10)$ au becomes an HJ in a Gyr in a cluster of stellar density $n_*=50$ pc$^{-3}$ and binary fraction $f_\mathrm{bin}=0.5$ is about 2\% and an additional 4\% are forced by the companion star into collision with or tidal disruption by the central host. An empirical fit shows that the total percentage of those outcomes asymptotically reaches an upper limit determined solely by $f_\mathrm{bin}$ (e.g., $10\%$ at $f_\mathrm{bin}=0.3$ and 18\% at $f_\mathrm{bin}=1$) on a timescale inversely proportional to $n_*$ ($\sim$ Gyr for $n_*\sim100$ pc$^{-3}$). The ratio of collisions to tidal disruptions is roughly a few, and depends on the tidal model. Therefore, if the giant planet occurrence rate is 10~\%, our mechanism implies an HJ occurrence rate of a few times 0.1~\% in a Gyr and can thus explain a substantial fraction of the observed rate.