{"title":"超级泡芙行星开普勒-51d的缓慢自转","authors":"Caleb Lammers, Joshua N. Winn","doi":"arxiv-2409.06697","DOIUrl":null,"url":null,"abstract":"Super-puffs are low-density planets of unknown origin and composition. If\nthey form by accreting nebular gas through a circumplanetary disk, one might\nexpect super-puffs to be spinning quickly. Here, we derive upper limits on the\nrotational oblateness of the super-puff Kepler-51d, based on precise transit\nobservations with the NIRSpec instrument aboard the James Webb Space Telescope.\nThe absence of detectable oblateness-related anomalies in the light curve leads\nto an upper limit of about $0.15$ on the planet's sky-projected oblateness.\nAssuming the sky-projected oblateness to be representative of the true\noblateness, the rotation period of Kepler-51d is $\\gtrsim 40$ hours, or\nequivalently, its rotation speed is $\\lesssim 42\\%$ of the breakup speed.\nAlternatively, if the apparently low density of Kepler-51d is due to an opaque\nplanetary ring, the ring must be oriented within $27\\deg$ of face-on and have\nan inner radius smaller than $1.2$ times the planet's radius. The lack of\nanomalies exceeding $0.01\\%$ in the ingress and egress portions of the light\ncurve also places a constraint on the model of Wang & Dai, in which the\nplanet's apparently low density is due to a dusty outflowing atmosphere.","PeriodicalId":501209,"journal":{"name":"arXiv - PHYS - Earth and Planetary Astrophysics","volume":"403 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Slow Rotation for the Super-Puff Planet Kepler-51d\",\"authors\":\"Caleb Lammers, Joshua N. Winn\",\"doi\":\"arxiv-2409.06697\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Super-puffs are low-density planets of unknown origin and composition. If\\nthey form by accreting nebular gas through a circumplanetary disk, one might\\nexpect super-puffs to be spinning quickly. Here, we derive upper limits on the\\nrotational oblateness of the super-puff Kepler-51d, based on precise transit\\nobservations with the NIRSpec instrument aboard the James Webb Space Telescope.\\nThe absence of detectable oblateness-related anomalies in the light curve leads\\nto an upper limit of about $0.15$ on the planet's sky-projected oblateness.\\nAssuming the sky-projected oblateness to be representative of the true\\noblateness, the rotation period of Kepler-51d is $\\\\gtrsim 40$ hours, or\\nequivalently, its rotation speed is $\\\\lesssim 42\\\\%$ of the breakup speed.\\nAlternatively, if the apparently low density of Kepler-51d is due to an opaque\\nplanetary ring, the ring must be oriented within $27\\\\deg$ of face-on and have\\nan inner radius smaller than $1.2$ times the planet's radius. The lack of\\nanomalies exceeding $0.01\\\\%$ in the ingress and egress portions of the light\\ncurve also places a constraint on the model of Wang & Dai, in which the\\nplanet's apparently low density is due to a dusty outflowing atmosphere.\",\"PeriodicalId\":501209,\"journal\":{\"name\":\"arXiv - PHYS - Earth and Planetary Astrophysics\",\"volume\":\"403 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-10\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - Earth and Planetary Astrophysics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.06697\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Earth and Planetary Astrophysics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.06697","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
超级泡芙是起源和成分不明的低密度行星。如果它们是通过环行星盘吸积星云气体形成的,那么人们可能会期待超级泡芙快速旋转。这里,我们根据詹姆斯-韦伯太空望远镜(James Webb Space Telescope)上的近红外望远镜(NIRSpec)的精确凌日观测,推导出了超级泡芙 Kepler-51d 的旋转扁圆度上限。另外,如果开普勒-51d表面上的低密度是由于一个不透明的行星环造成的,那么这个行星环的方向必须在面朝上的27deg以内,并且其内半径小于行星半径的1.2倍。在光曲线的入口和出口部分缺乏超过0.01美元/%$的异常,这也对Wang和Dai的模型施加了限制,在他们的模型中,行星明显的低密度是由于尘埃外流大气造成的。
Slow Rotation for the Super-Puff Planet Kepler-51d
Super-puffs are low-density planets of unknown origin and composition. If
they form by accreting nebular gas through a circumplanetary disk, one might
expect super-puffs to be spinning quickly. Here, we derive upper limits on the
rotational oblateness of the super-puff Kepler-51d, based on precise transit
observations with the NIRSpec instrument aboard the James Webb Space Telescope.
The absence of detectable oblateness-related anomalies in the light curve leads
to an upper limit of about $0.15$ on the planet's sky-projected oblateness.
Assuming the sky-projected oblateness to be representative of the true
oblateness, the rotation period of Kepler-51d is $\gtrsim 40$ hours, or
equivalently, its rotation speed is $\lesssim 42\%$ of the breakup speed.
Alternatively, if the apparently low density of Kepler-51d is due to an opaque
planetary ring, the ring must be oriented within $27\deg$ of face-on and have
an inner radius smaller than $1.2$ times the planet's radius. The lack of
anomalies exceeding $0.01\%$ in the ingress and egress portions of the light
curve also places a constraint on the model of Wang & Dai, in which the
planet's apparently low density is due to a dusty outflowing atmosphere.