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首页> 外文期刊>The Astrophysical journal >MOA 2010-BLG-477Lb: CONSTRAINING THE MASS OF A MICROLENSING PLANET FROM MICROLENSING PARALLAX, ORBITAL MOTION, AND DETECTION OF BLENDED LIGHT
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MOA 2010-BLG-477Lb: CONSTRAINING THE MASS OF A MICROLENSING PLANET FROM MICROLENSING PARALLAX, ORBITAL MOTION, AND DETECTION OF BLENDED LIGHT

机译:MOA 2010-BLG-477Lb:由微透镜的视差,轨道运动和混合光的检测构成微透镜的质量

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摘要

Microlensing detections of cool planets are important for the construction of an unbiased sample to estimate the frequency of planets beyond the snow line, which is where giant planets are thought to form according to the core accretion theory of planet formation. In this paper, we report the discovery of a giant planet detected from the analysis of the light curve of a high-magnification microlensing event MOA 2010-BLG-477. The measured planet-star mass ratio is q = (2.181 ± 0.004) × 10–3 and the projected separation is s = 1.1228 ± 0.0006 in units of the Einstein radius. The angular Einstein radius is unusually large θE = 1.38 ± 0.11 mas. Combining this measurement with constraints on the "microlens parallax" and the lens flux, we can only limit the host mass to the range 0.13 M/M ☉ 1.0. In this particular case, the strong degeneracy between microlensing parallax and planet orbital motion prevents us from measuring more accurate host and planet masses. However, we find that adding Bayesian priors from two effects (Galactic model and Keplerian orbit) each independently favors the upper end of this mass range, yielding star and planet masses of M * = 0.67+0.33 – 0.13 M ☉ and mp = 1.5+0.8 – 0.3 M JUP at a distance of D = 2.3 ± 0.6?kpc, and with a semi-major axis of a = 2+3 – 1?AU. Finally, we show that the lens mass can be determined from future high-resolution near-IR adaptive optics observations independently from two effects, photometric and astrometric.
机译:对冷行星的微透镜检测对于构建无偏样本以估计超出雪线的行星的频率非常重要,根据积雪形成的核心积淀理论,认为积雪线是超大行星形成的地方。在本文中,我们报告了通过对高倍微透镜事件MOA 2010-BLG-477的光曲线分析发现的一个巨大行星的发现。测得的恒星质量比为q =(2.181±0.004)×10–3,预计的分离度为s = 1.1228±0.0006,以爱因斯坦半径为单位。爱因斯坦角半径异常大,θE= 1.38±0.11 mas。将此测量与“微透镜视差”和透镜通量的约束条件相结合,我们只能将主体质量限制在0.13
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