2019 UO14:土星的一颗瞬变木马

Man-To Hui, 文韜 許, Paul A. Wiegert, Robert Weryk, Marco Micheli, David J. Tholen, Sam Deen, Andrew J. Walker and Richard Wainscoat
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摘要

长期以来,土星一直是太阳系中唯一没有已知木马成员的巨行星。在这封信中,通过偶然的档案观测和精细的轨道测定,我们报告说 2019 UO14 是这颗气体巨行星的特洛伊木马。然而,该天体只是一个瞬态特洛伊木马,目前正在围绕太阳-土星系统的前沿拉格朗日点L4进行周期为0.7千年的天体运动。我们的N-body数值模拟显示,2019 UO14很可能是作为一颗半人马星被捕获的,并在2千年前从一个马蹄形共轨轨道被困在L4附近。目前的特洛伊状态还将维持一千年左右,然后再过渡回马蹄形状态。此外,我们还描述了 2019 年 UO14 的物理特性。假定线性相位斜率为 0.06 ± 0.01 磁格-1,该天体的平均 r 波段绝对星等被测定为 Hr = 13.11 ± 0.07,其颜色与木星和海王星特洛伊木马的颜色一致,与半人马的颜色没有统计学差异。虽然在观测中,这颗短命的土星特洛伊木马没有表现出令人信服的活动证据,但我们倾向于它可能是一颗活动的特洛伊木马。如果得到证实,2019 UO14 将成为太阳系中第一颗活跃的特洛伊木马。如果尘粒的物理性质与半人马座 29P/Schwassmann-Wachmann 1 类似,我们保守地将测光孔径内尘粒的光学深度定为≲10-7,对应的尘粒质量损失率为≲1 kg s-1。
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2019 UO14: A Transient Trojan of Saturn
Saturn has long been the only giant planet in our solar system without any known Trojan members. In this Letter, with serendipitous archival observations and refined orbit determination, we report that 2019 UO14 is a Trojan of the gas giant. However, the object is only a transient Trojan currently librating around the leading Lagrange point L4 of the Sun–Saturn system in a period of ∼0.7 kyr. Our N-body numerical simulation shows that 2019 UO14 was likely captured as a Centaur and became trapped around L4 ∼ 2 kyr ago from a horseshoe co-orbital. The current Trojan state will be maintained for another millennium or thereabouts before transitioning back to a horseshoe state. Additionally, we characterize the physical properties of 2019 UO14. Assuming a linear phase slope of 0.06 ± 0.01 mag deg−1, the mean r-band absolute magnitude of the object was determined to be Hr = 13.11 ± 0.07, with its color measured to be consistent with that of Jupiter and Neptune Trojans and not statistically different from Centaurs. Although the short-lived Saturn Trojan exhibited no compelling evidence of activity in the observations, we favor the possibility that it could be an active Trojan. If confirmed, 2019 UO14 would be marked as the first active Trojan in our solar system. We conservatively determine the optical depth of dust within our photometric aperture to be ≲10−7, corresponding to a dust mass-loss rate to be ≲1 kg s−1, provided that the physical properties of dust grains resemble Centaur 29P/Schwassmann–Wachmann 1.
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