The inflated, eccentric warm Jupiter TOI-4914 b orbiting a metal-poor star, and the hot Jupiters TOI-2714 b and TOI-2981 b

G. Mantovan, T. G. Wilson, L. Borsato, T. Zingales, K. Biazzo, D. Nardiello, L. Malavolta, S. Desidera, F. Marzari, A. Collier Cameron, V. Nascimbeni, F. Z. Majidi, M. Montalto, G. Piotto, K. G. Stassun, J. N. Winn, J. M. Jenkins, L. Mignon, A. Bieryla, D. W. Latham, K. Barkaoui, K. A. Collins, P. Evans, M. M. Fausnaugh, V. Granata, V. Kostov, A. W. Mann, F. J. Pozuelos, D. J. Radford, H. M. Relles, P. Rowden, S. Seager, T. -G. Tan, M. Timmermans, C. N. Watkins
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Abstract

Recent observations of giant planets have revealed unexpected bulk densities. Hot Jupiters, in particular, appear larger than expected for their masses compared to planetary evolution models, while warm Jupiters seem denser than expected. These differences are often attributed to the influence of the stellar incident flux, but could they also result from different planet formation processes? Is there a trend linking the planetary density to the chemical composition of the host star? In this work we present the confirmation of three giant planets in orbit around solar analogue stars. TOI-2714 b ($P \simeq 2.5$ d, $R_{\rm p} \simeq 1.22 R_{\rm J}$, $M_{\rm p} = 0.72 M_{\rm J}$) and TOI-2981 b ($P \simeq 3.6$ d, $R_{\rm p} \simeq 1.2 R_{\rm J}$, $M_{\rm p} = 2 M_{\rm J}$) are hot Jupiters on nearly circular orbits, while TOI-4914 b ($P \simeq 10.6$ d, $R_{\rm p} \simeq 1.15 R_{\rm J}$, $M_{\rm p} = 0.72 M_{\rm J}$) is a warm Jupiter with a significant eccentricity ($e = 0.41 \pm 0.02$) that orbits a star more metal-poor ([Fe/H]$~= -0.13$) than most of the stars known to host giant planets. Our radial velocity (RV) follow-up with the HARPS spectrograph allows us to detect their Keplerian signals at high significance (7, 30, and 23$\sigma$, respectively) and to place a strong constraint on the eccentricity of TOI-4914 b (18$\sigma$). TOI-4914 b, with its large radius and low insolation flux ($F_\star < 2 \times 10^8~{\rm erg~s^{-1}~cm^{-2}}$), appears to be more inflated than what is supported by current theoretical models for giant planets. Moreover, it does not conform to the previously noted trend that warm giant planets orbiting metal-poor stars have low eccentricities. This study thus provides insights into the diverse orbital characteristics and formation processes of giant exoplanets, in particular the role of stellar metallicity in the evolution of planetary systems.
围绕一颗贫金属恒星运行的膨胀偏心暖木星TOI-4914 b,以及热木星TOI-2714 b和TOI-2981 b
与行星演化模型相比,热木星的质量似乎比预期的要大,而暖木星的密度似乎比预期的要大。这些差异通常归因于恒星入射通量的影响,但它们是否也可能是不同的行星形成过程造成的呢?是否存在行星密度与宿主恒星化学成分相关联的趋势?在这项工作中,我们证实了三颗围绕太阳类似恒星运行的巨行星。TOI-2714 b ($P\simeq 2.5$ d, $R_{\rm p}\1.22 R_{\rm J}$,$M_{\rm p} = 0.72 M_{\rm J}$)和TOI-2981 b($P \simeq 3.6$ d, $R_{\rm p}1.2 R_{\rm J}$,$M_{\rm p}= 2 M_{\rm J})都是运行在近圆形轨道上的热木星,而TOI-4914 b($P\simeq 10.6$ d, $R_{\rm p}= 1.15 M_{\rm J})则是运行在近圆形轨道上的热木星。而TOI-4914 b($P\simeq 10.6$ d, $R_{\rm p}$ 1.15 R_{\rm J}$, $M_{\rm p} = 0.72 M_{\rmJ}$)是一颗温暖的木星,它的偏心率很大($e = 0.41 \pm 0.02$),与已知的大多数孕育巨行星的恒星相比,它的金属含量更低([Fe/H]$~= -0.13$)。我们利用HARPS光谱仪进行的径向速度(RV)跟踪使我们能够探测到它们高显著性(分别为7、30和23$\sigma$)的开普勒信号,并对TOI-4914 b的同心度(18$\sigma$)进行了强有力的约束。TOI-4914 b的半径很大,日照通量很低($F_\star < 2 \times 10^8~{\rm erg~s^{-1}~cm^{-2}}$ ),似乎比目前的巨行星理论模型所支持的更膨胀。此外,它也不符合之前提到的趋势,即围绕贫金属恒星运行的暖巨行星具有较低的中心距。因此,这项研究为了解巨型系外行星的不同轨道特征和形成过程,特别是恒星金属性在行星系统演化中的作用提供了启示。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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