论文标题

OGLE-2019-BLG-1470LABC:二进制系统中的另一个微透镜巨星?

OGLE-2019-BLG-1470LABc: Another Microlensing Giant Planet in a Binary System?

论文作者

Kuang, Renkun, Zang, Weicheng, Jung, Youn Kil, Udalski, Andrzej, Yang, Hongjing, Mao, Shude, Albrow, Michael D., Chung, Sun-Ju, Gould, Andrew, Han, Cheongho, Hwang, Kyu-Ha, Ryu, Yoon-Hyun, Shin, In-Gu, Shvartzvald, Yossi, Yee, Jennifer C., Cha, Sang-Mok, Kim, Dong-Jin, Kim, Hyoun-Woo, Kim, Seung- Lee, Lee, Chung-Uk, Lee, Dong-Joo, Lee, Yongseok, Park, Byeong-Gon, Pogge, Richard W., Mróz, Przemek, Skowron, Jan, Poleski, Radoslaw, Szymański, Michał K., Soszyński, Igor, Pietrukowicz, Paweł, Kozłowski, Szymon, Ulaczyk, Krzysztof, Rybicki, Krzysztof A., Iwanek, Patryk, Wrona, Marcin, Gromadzki, Mariusz, Wang, Hanyue, Huang, Shuo, Zhu, Wei

论文摘要

我们报告了候选三镜单源(3L1)微透镜事件的发现和分析,OGLE-2019-BLG-1470。该事件首先被归类为普通的二进制单源单源(2L1)事件,但是仔细的2L1S建模表明,它需要额外的镜头或源以适合观察到的数据。发现3L1S模型提供了最佳拟合度,但是二进制二进制二元源(2L2S)模型仅被$Δχ^2 \ simeq 18 $散布。所有可行的模型都包括一个带有行星至托管质量比例的行星$ 10^{ - 3} \ Lessim Q \ Lessim 10^{ - 2} $。基于银河系模型的贝叶斯分析表明该行星是超级jovian,并且投影的主机 - 行径分离约为3 $ \ mathrm {au} $。具体而言,对于最合适的3L1S模型,两颗星的质量为$ m_1 = 0.57^{+0.43} _ { - 0.32} m _ {\ odot} $,$ m_2 = 0.18^{+0.15^{+0.15} $ 1.3^{+0.5} _ { - 0.5} $ $ $ \ MATHRM {AU} $,行星质量为$ M_3 = 2.2^{+1.8} _ { - 1.3} M _ {\ rm {jupiter}} $。对于2L2S模型,主机之星和行星的质量为$ 0.55^{+0.44} _ { - 0.31} M _ {\ odot} $和$ 4.6^{+3.7} _ { - 2.6} _ { - 2.6} m _ {\ rm _ {\ rm rm {jupiter}} $。通过研究二进制系统中所有已知的微透析行星的特性,我们发现由KMTNET调查发表的二进制系统中的所有行星都位于共振苛性碱内部的范围内,具有$ Q \ gtrsim 2 \ gtrsim 2 \ times 10^{ - 3} $,表明kmtnet样品在bitary Systems中的不满。因此,二进制系统中的行星不能包括在KMTNET质量比率函数的当前研究中,并且需要在KMTNET微透明光曲线中对行星异常进行系统的搜索。

We report the discovery and analysis of a candidate triple-lens single-source (3L1S) microlensing event, OGLE-2019-BLG-1470. This event was first classified as a normal binary-lens single-source (2L1S) event, but a careful 2L1S modelling showed that it needs an additional lens or source to fit the observed data. It is found that the 3L1S model provides the best fit, but the binary-lens binary-source (2L2S) model is only disfavoured by $Δχ^2 \simeq 18$. All of the feasible models include a planet with planet-to-host mass-ratios $10^{-3} \lesssim q \lesssim 10^{-2}$. A Bayesian analysis based on a Galactic model indicates that the planet is super-Jovian, and the projected host-planet separation is about 3 $\mathrm{au}$. Specifically, for the best-fit 3L1S model, the two stars have masses of $M_1=0.57^{+0.43}_{-0.32}M_{\odot}$, and $M_2=0.18^{+0.15}_{-0.10}M_{\odot}$, with projected separation of $1.3^{+0.5}_{-0.5}$ $\mathrm{au}$, and the planetary mass is $M_3=2.2^{+1.8}_{-1.3}M_{\rm{Jupiter}}$. For the 2L2S model, the masses of the host star and the planet are $0.55^{+0.44}_{-0.31}M_{\odot}$ and $4.6^{+3.7}_{-2.6}M_{\rm{Jupiter}}$, respectively. By investigating the properties of all known microlensing planets in binary systems, we find that all planets in binary systems published by the KMTNet survey are located inside the resonant caustics range with $q \gtrsim 2 \times 10^{-3}$, indicating the incompleteness of the KMTNet sample for planets in binary systems. Thus, planets in binary systems cannot be included in the current study of the KMTNet mass-ratio function, and a systematic search for planetary anomalies in KMTNet microlensing light curves of binary systems is needed.

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