日本地球惑星科学連合2014年大会

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ポスター発表

セッション記号 U (ユニオン) » ユニオン

[U-06_28PO1] 太陽系小天体研究の新展開

2014年4月28日(月) 18:15 〜 19:30 3階ポスター会場 (3F)

コンビーナ:*荒川 政彦(神戸大学大学院理学研究科)、中本 泰史(東京工業大学)、渡邊 誠一郎(名古屋大学大学院環境学研究科地球環境科学専攻)、安部 正真(宇宙航空研究開発機構宇宙科学研究所)、石黒 正晃(ソウル大学物理天文学科)

18:15 〜 19:30

[U06-P01] Hayabusa 2探査候補天体1999 JU3の光学特性

*石黒 正晃1黒田 大介2長谷川 直3Hayabusa 2 地上観測グループ 4 (1.ソウル大学物理天文学科、2.国立天文台岡山天体物理観 測所、3.宇宙航空研究開発機構宇宙科学研究所、4.宇宙航空研究開発機構)

キーワード:はやぶさ2, 1999 JU3, 地上観測

A near-Earth asteroid, (162173) 1999 JU3 (hereafter 1999 JU3), is a primary target asteroid for Hayabusa 2 sample return mission. We conducted a worldwide campaign to make photometric observations of the asteroid to determine the physical properties. 1999 JU3 is classified into C-type asteroid having a nearly spherical shape and the synodic rotational period of 7.6312±0.0010 hr.

In this presentation, we will report further information about 1999 JU3 determined since last JpGU meeting in 2013. We investigated the magnitude-phase angle relation. We obtained the parameters for IAU H-G formalism, H =19.20±0.12 and G=0.077±0.011 (V-band, 550nm), respectively. In combination of our result with infrared photometry, the geometric albedo is updated to be 0.05 (Mueller et al. in preparation), which is typical to but slightly smaller than the average of C-type asteroids in main-belt. We found that the magnitude-phase angle relation has a linear behavior in a wide range of the phase angles (5-80 degree) and show a possible non-linear opposition brightening within the phase angle of 5 degree. The phase slope is consistent to those of tens-km C-type asteroids, that is, 0.04 mag degree-1. The opposition effect amplitude, ≈10% or less, is slightly weaker than that of a precursor C-type mission target body, (253) Mathilde, but the difference seems to reflect the diversity of C-type asteroids. Recently, Shevchenko & Belskaya (2010) reported that ~20% of all studied low albedo asteroids did not show detectable opposition effect. We explore the significance of 1999 JU3 data with remote-sensing devices in terms of the opposition effect.