论文标题

通过出色的活动建模重新访问HD 21749行星系统

Revisiting the HD 21749 Planetary System with Stellar Activity Modeling

论文作者

Gan, Tianjun, Wang, Sharon Xuesong, Teske, Johanna K., Mao, Shude, Howard, Ward S., Law, Nicholas M., Batalha, Natasha E., Vanderburg, Andrew, Dragomir, Diana, Huang, Chelsea X., Feng, Fabo, Butler, R. Paul, Crane, Jeffrey D., Shectman, Stephen A., Beletsky, Yuri, Shporer, Avi, Montet, Benjamin T., Burt, Jennifer A., Feinstein, Adina D., Flowers, Erin, Nandakumar, Sangeetha, Barbieri, Mauro, Corbett, Hank, Ratzloff, Jeffrey K., Galliher, Nathan, Chavez, Ramses Gonzalez, Vasquez, Alan, Glazier, Amy, Haislip, Joshua

论文摘要

HD 21749是一个明亮的($ v = 8.1 $ mag)K矮人16 PC,已知可容纳内部陆地行星HD 21749C以及外部亚北北图21749b,均由TESS提供。后续光谱观测测量HD 21749B的质量为$ 22.7 \ pm2.2 \ m _ {\ oplus} $,密度为$ 7.0^{+1.6} _ { - 1.6} _ { - 1.3} $ g〜cm $ $ g〜cm $^{ - 3} $,使其成为一个密集的Sub-Nessess of sub-NeSest sub-Nestepteptepteptept。但是,怀疑质量测量受到恒星旋转的影响。在这里,我们提出了新的高环境PFS RV数据,以将恒星活动信号从行星信号中解散。我们发现HD 21749具有与行星轨道周期相似的旋转时间尺度,并且估计行星轨道轨道RV信号的幅度估计与恒星活性信号的幅度相似。我们在从竖琴和PFS的光度法和RV上执行高斯过程(GP)回归,以建模恒星活动信号。我们的新型号显示,HD 21749b的半径为$ 2.86 \ pm0.20 \ r _ {\ oplus} $,轨道周期为$ 35.6133 \ pm0.0005 $ d,质量为$ M_ {b} = 20.0 \ pm2.7 \ pm2.7 \ m _ \ m_ { $ 4.8^{+2.0} _ { - 1.4} $ g〜cm $^{ - 3} $在带有$ e = 0.16 \ pm0.06 $的偏心轨道上,这与此系统发布的最新值一致。 HD 21749C的轨道周期为$ 7.7902 \ pm0.0006 $ d,半径为$ 1.13 \ pm0.10 \ r _ {\ oplus} $,以及3 $σ$质量上限的上限为$ 3.5 \ m _ {\ m _ {\ oplus} $。我们的蒙特卡洛模拟证实,如果不正确考虑出色的活动信号,HD 21749B的质量测量可能会明显低估。

HD 21749 is a bright ($V=8.1$ mag) K dwarf at 16 pc known to host an inner terrestrial planet HD 21749c as well as an outer sub-Neptune HD 21749b, both delivered by TESS. Follow-up spectroscopic observations measured the mass of HD 21749b to be $22.7\pm2.2\ M_{\oplus}$ with a density of $7.0^{+1.6}_{-1.3}$ g~cm$^{-3}$, making it one of the densest sub-Neptunes. However, the mass measurement was suspected to be influenced by stellar rotation. Here we present new high-cadence PFS RV data to disentangle the stellar activity signal from the planetary signal. We find that HD 21749 has a similar rotational timescale as the planet's orbital period, and the amplitude of the planetary orbital RV signal is estimated to be similar to that of the stellar activity signal. We perform Gaussian Process (GP) regression on the photometry and RVs from HARPS and PFS to model the stellar activity signal. Our new models reveal that HD 21749b has a radius of $2.86\pm0.20\ R_{\oplus}$, an orbital period of $35.6133\pm0.0005$ d with a mass of $M_{b}=20.0\pm2.7\ M_{\oplus}$ and a density of $4.8^{+2.0}_{-1.4}$ g~cm$^{-3}$ on an eccentric orbit with $e=0.16\pm0.06$, which is consistent with the most recent values published for this system. HD 21749c has an orbital period of $7.7902\pm0.0006$ d, a radius of $1.13\pm0.10\ R_{\oplus}$, and a 3$σ$ mass upper limit of $3.5\ M_{\oplus}$. Our Monte Carlo simulations confirm that without properly taking stellar activity signals into account, the mass measurement of HD 21749b is likely to arrive at a significantly underestimated error bar.

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