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A Signature of Planetary Migration: The Origin of Asymmetric Capture in the 2:1 Resonance

机译:行星迁移的标志:2:1共振中不对称捕获的起源

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The spatial distribution of Kuiper Belt objects (KBOs) in 2?:?1 exterior resonance with Neptune constrains that planet's migration history. Numerical simulations demonstrate that fast planetary migration generates a larger population of KBOs trailing rather than leading Neptune in orbital longitude. This asymmetry corresponds to a greater proportion of objects caught into asymmetric resonance such that their resonance angles librate about values greater than π (trailing) as opposed to less than π (leading). We provide, for the first time, an explanation of this phenomenon, using physical, analytic, and semianalytic arguments. Central to our understanding is how planetary migration shifts the equilibrium points of the superposed direct and indirect potentials. Symmetric libration, in which librates about ~π, precedes capture into asymmetric resonance. As a particle transitions from symmetric to asymmetric libration, if exceeds the value ψ at the unstable point of asymmetric resonance, then the particle is caught into trailing resonance, while if ψ, the particle is caught into leading resonance. The probability that the KBO is caught into trailing resonance is determined by the fraction of time it spends with ψ while in symmetric libration. This fractional time increases with faster migration because migration not only shifts ψ to values less than π but also shifts the stable point of symmetric libration to values greater than π. Smaller eccentricities prior to capture strengthen the effect of these shifts. Large capture asymmetries appear for exponential timescales of migration τ shorter than ~107 yr. The observed distribution of 2?:?1 KBOs (two trailing and seven leading) excludes τ ≤ 106 yr with 99.65% confidence.
机译:海王星在2?:?1外部共振中与海王星的柯伊伯带天体(KBOs)的空间分布限制了该行星的迁移历史。数值模拟表明,快速的行星迁移会产生更大的KBO尾迹,而不是在轨道经度上领先海王星。这种不对称性对应于陷入非对称共振的物体比例更大,从而使物体的共振角在大于π(后移)的值附近释放,而小于小于π(超前)的值。我们首次使用物理,解析和半解析论证对此现象进行了解释。我们理解的中心是行星迁移如何改变叠加的直接和间接势能的平衡点。对称解放在大约〜π的时间内解放,先于捕获进入非对称共振。当粒子从对称释放转变为非对称释放时,如果在非对称共振的不稳定点处超过值ψ,则粒子将陷入尾随共振,而如果<ψ,粒子将陷入前导共振。 KBO陷入尾随共振的可能性由它在对称释放时花费大于ψ的时间分数确定。随着迁移的加快,该分数时间增加,因为迁移不仅将ψ偏移到小于π的值,而且还将对称解放的稳定点偏移到大于π的值。捕获之前较小的离心率会增强这些偏移的影响。对于迁移时间τ小于约107年的指数时间尺度,会出现较大的捕获不对称性。所观察到的2?:?1 KBO(两个尾随和七个前导)的分布排除了τ≤106年,置信度为99.65%。

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