日本地球惑星科学連合2025年大会

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[E] 口頭発表

セッション記号 P (宇宙惑星科学) » P-AE 天文学・太陽系外天体

[P-AE18] 系外惑星

2025年5月30日(金) 13:45 〜 15:15 304 (幕張メッセ国際会議場)

コンビーナ:小玉 貴則(地球生命研究所、東京科学大学)、川島 由依(京都大学)、野津 翔太(東京大学 大学院理学系研究科 地球惑星科学専攻 地球惑星システム科学講座)、森 万由子(アストロバイオロジーセンター)、座長:野津 翔太(東京大学 大学院理学系研究科 地球惑星科学専攻 地球惑星システム科学講座)、大野 和正(国立天文台)


14:15 〜 14:30

[PAE18-15] Validation of an Eccentric Hot Jupiter Transiting the Edge of a Mid-A-type star TOI-1355

*渡辺 紀治1成田 憲保1,2福井 暁彦1、佐藤 文衛3、磯貝 桂介1,4リビングストン ジョン2,5、デ・レオン ジェローム1河合 優悟1大宮 正士2,5、泉浦 秀行5、田實 晃人5日下部 展彦2,5田村 元秀1,2,5 (1.東京大学、2.アストロバイオロジーセンター、3.東京科学大学、4.京都大学、5.国立天文台)

キーワード:系外惑星、高温星、ホットジュピター

Hot Jupiter, a gas giant orbiting with a short period of less than 10 days, is a difficult planet to form in situ. Thus, some orbital evolution models have been proposed, such as the disk migration and the high eccentricity migration. The disk migration involves a gas giant dropping near its host star through disk-planet interaction and aligning the orbit with the stellar spin. In contrast, the high eccentricity migration is a model in which a gas giant with a high eccentric and misaligned orbit approaches its host star due to the circularization from the tides of planetary deformation. High eccentricities and misalignments can arise from interactions with other giant planets or outer companions. Because a hot star, whose effective temperature is above 7000K, has no convective zones in its envelopes and hardly undergoes realignment, the system with a hot Jupiter and a hot star is favorable to research orbital evolution.

In this study, we discovered a massive hot Jupiter around TOI-1355, one of the A-type stars, from the TESS transit survey, and the follow-up observations such as the high-resolution spectrograph Seimei/GAOES-RV and the multi-band camera LOCGT(2m)/MuSCAT3. This is the first discovery of an eccentric hot Jupiter around a hot star, which suggests that this hot Jupiter has undergone the high eccentricity migration. We also detected the nodal precession, a phenomenon that the orbital axis precesses relative to the stellar rotational axis, by measuring the change in its impact parameter (an apparent distance between the transit trajectory and the center of the host star). This implies that the orbital axis is almost perpendicular to the stellar rotational axis and we cannot observe its transit since 2028 CE.