论文标题

非主要轴旋转器(5247)Krylov的形状模型和自旋状态

Shape model and spin state of non-principal axis rotator (5247) Krylov

论文作者

Lee, H. -J., Ďurech, J., Kim, M. -J., Moon, H. -K., Kim, C. -H., Choi, Y. -J., Galád, A., Pray, D., Marciniak, A., Kaplan, M., Erece, O., Duffard, R., Gajdoš, Š., Világi, J., Lehký, M.

论文摘要

语境。非主要轴(NPA)旋转器的研究可以为小行星旋转状态的演变提供重要的线索。但是,到目前为止,很少有研究集中于NPA旋转的主要皮带小行星(MBA)。已知处于激发旋转状态的MBA之一是小行星(5247)Krylov。目标。通过使用磁盘集成的光度数据,我们构建了(5247)Krylov的物理模型,包括形状和自旋状态。方法。我们采用光曲线凸反转方法,采用了通过在2006年,2016年和2017年使用地面望远镜在三种幻影中获得的光光曲线,以及2010年宽场红外调查Explorer(Wise)卫星获得的红外光曲线在2010年在2010年获得。小行星(5247)〜Krylov以短轴模式(SAM)旋转,其特征分别为368.7小时和67.27小时。发现Krylov的角动量向量方向为$λ_{l} = 298^\ circ $和$β_{l} = -58^\ circ $。与主轴(PA)旋转状态相比,旋转动能与基本旋转状态能$ e/e_ {0} \ simeq 1.02 $的比率大约是(5247)Krylov激发态。 (5247)Krylov的形状可以通过细长的pr酸椭圆形近似,其惯性矩的比例为$ i_ {a}:i_ {b}:i_ {c} = 0.36:0.96:0.96:1 $。这是MBA中NPA旋转器的第一个物理模型。导致当前NPA旋转的物理过程不能明确地重建。

Context. The study of non-principal axis (NPA) rotators can provide important clues to the evolution of the spin state of asteroids. However, so far, very few studies have focused on NPA-rotating main-belt asteroids (MBAs). One of MBAs that are known to be in an excited rotation state is asteroid (5247) Krylov. Aims. By using disk-integrated photometric data, we construct a physical model of (5247) Krylov including shape and spin state. Methods. We apply the light curve convex inversion method employing optical light curves obtained by using ground-based telescopes in three apparitions during 2006, 2016, and 2017, along with infrared light curves obtained by the Wide-field Infrared Survey Explorer (WISE) satellite in 2010. Results. Asteroid (5247)~Krylov is spinning in a short axis mode (SAM) characterized by rotation and precession periods of 368.7 hr and 67.27 hr, respectively. The angular momentum vector orientation of Krylov is found to be $λ_{L} = 298^\circ$ and $β_{L} = -58^\circ$. The ratio of the rotational kinetic energy to the basic spin state energy $E/E_{0} \simeq 1.02$ shows that the (5247) Krylov is about 2% excited state compared to the Principal Axis (PA) rotation state. The shape of (5247) Krylov can be approximated by an elongated prolate ellipsoid with a ratio of moments of inertia of $I_{a}:I_{b}:I_{c}=0.36:0.96:1$. This is the first physical model of NPA rotator among MBAs. The physical processes that led to the current NPA rotation cannot be unambiguously reconstructed.

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