A. Gould, Y. Ryu, S. Novati, W. Zang, M. Albrow, Sun-Ju Chung, C. Han, K. Hwang, Y. Jung, I. Shin, Y. Shvartzvald, J. Yee, S. Cha, Dong-Jin Kim, Hyoun-Woo Kim, Seung-Lee Kim, Chung-Uk Lee, Dong-Joo Lee, Yongseok Lee, Byeong-Gon Park, R. Pogge, C. Beichman, G. Bryden, S. Carey, B. Gaudi, C. Henderson, Wei Zhu, P. Fouqu'e, M. Penny, A. Petric, T. Burdullis, S. Mao
{"title":"KMT-2018-BLG-0029Lb:非常低质量比斯皮策微透镜行星","authors":"A. Gould, Y. Ryu, S. Novati, W. Zang, M. Albrow, Sun-Ju Chung, C. Han, K. Hwang, Y. Jung, I. Shin, Y. Shvartzvald, J. Yee, S. Cha, Dong-Jin Kim, Hyoun-Woo Kim, Seung-Lee Kim, Chung-Uk Lee, Dong-Joo Lee, Yongseok Lee, Byeong-Gon Park, R. Pogge, C. Beichman, G. Bryden, S. Carey, B. Gaudi, C. Henderson, Wei Zhu, P. Fouqu'e, M. Penny, A. Petric, T. Burdullis, S. Mao","doi":"10.5303/JKAS.2020.53.1.9","DOIUrl":null,"url":null,"abstract":"At $q=1.81\\pm 0.20 \\times 10^{-5}$, KMT-2018-BLG-0029Lb has the lowest planet-host mass ratio $q$ of any microlensing planet to date by more than a factor of two. Hence, it is the first planet that probes below the apparent \"pile-up\" at $q=5$--10 $\\times 10^{-5}$. The event was observed by {\\it Spitzer}, yielding a microlens-parallax $\\pi_{\\rm E}$ measurement. Combined with a measurement of the Einstein radius $\\theta_{\\rm E}$ from finite-source effects during the caustic crossings, these measurements imply masses of the host $M_{\\rm host}=1.14^{+0.10}_{-0.12}\\, M_\\odot$ and planet $M_{\\rm planet} = 7.59^{+0.75}_{-0.69}\\,M_\\oplus$, system distance $D_L = 3.38^{+0.22}_{-0.26}\\,\\,{\\rm kpc}$ and projected separation $a_\\perp = 4.27^{+0.21}_{-0.23}\\,{\\rm au}$. The blended light, which is substantially brighter than the microlensed source, is plausibly due to the lens and could be observed at high resolution immediately.","PeriodicalId":8428,"journal":{"name":"arXiv: Earth and Planetary Astrophysics","volume":"21 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2019-06-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"14","resultStr":"{\"title\":\"KMT-2018-BLG-0029Lb: A Very Low Mass-Ratio Spitzer Microlens Planet\",\"authors\":\"A. Gould, Y. Ryu, S. Novati, W. Zang, M. Albrow, Sun-Ju Chung, C. Han, K. Hwang, Y. Jung, I. Shin, Y. Shvartzvald, J. Yee, S. Cha, Dong-Jin Kim, Hyoun-Woo Kim, Seung-Lee Kim, Chung-Uk Lee, Dong-Joo Lee, Yongseok Lee, Byeong-Gon Park, R. Pogge, C. Beichman, G. Bryden, S. Carey, B. Gaudi, C. Henderson, Wei Zhu, P. Fouqu'e, M. Penny, A. Petric, T. Burdullis, S. Mao\",\"doi\":\"10.5303/JKAS.2020.53.1.9\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"At $q=1.81\\\\pm 0.20 \\\\times 10^{-5}$, KMT-2018-BLG-0029Lb has the lowest planet-host mass ratio $q$ of any microlensing planet to date by more than a factor of two. Hence, it is the first planet that probes below the apparent \\\"pile-up\\\" at $q=5$--10 $\\\\times 10^{-5}$. The event was observed by {\\\\it Spitzer}, yielding a microlens-parallax $\\\\pi_{\\\\rm E}$ measurement. Combined with a measurement of the Einstein radius $\\\\theta_{\\\\rm E}$ from finite-source effects during the caustic crossings, these measurements imply masses of the host $M_{\\\\rm host}=1.14^{+0.10}_{-0.12}\\\\, M_\\\\odot$ and planet $M_{\\\\rm planet} = 7.59^{+0.75}_{-0.69}\\\\,M_\\\\oplus$, system distance $D_L = 3.38^{+0.22}_{-0.26}\\\\,\\\\,{\\\\rm kpc}$ and projected separation $a_\\\\perp = 4.27^{+0.21}_{-0.23}\\\\,{\\\\rm au}$. The blended light, which is substantially brighter than the microlensed source, is plausibly due to the lens and could be observed at high resolution immediately.\",\"PeriodicalId\":8428,\"journal\":{\"name\":\"arXiv: Earth and Planetary Astrophysics\",\"volume\":\"21 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-06-26\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"14\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv: Earth and Planetary Astrophysics\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.5303/JKAS.2020.53.1.9\",\"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: Earth and Planetary Astrophysics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.5303/JKAS.2020.53.1.9","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
KMT-2018-BLG-0029Lb: A Very Low Mass-Ratio Spitzer Microlens Planet
At $q=1.81\pm 0.20 \times 10^{-5}$, KMT-2018-BLG-0029Lb has the lowest planet-host mass ratio $q$ of any microlensing planet to date by more than a factor of two. Hence, it is the first planet that probes below the apparent "pile-up" at $q=5$--10 $\times 10^{-5}$. The event was observed by {\it Spitzer}, yielding a microlens-parallax $\pi_{\rm E}$ measurement. Combined with a measurement of the Einstein radius $\theta_{\rm E}$ from finite-source effects during the caustic crossings, these measurements imply masses of the host $M_{\rm host}=1.14^{+0.10}_{-0.12}\, M_\odot$ and planet $M_{\rm planet} = 7.59^{+0.75}_{-0.69}\,M_\oplus$, system distance $D_L = 3.38^{+0.22}_{-0.26}\,\,{\rm kpc}$ and projected separation $a_\perp = 4.27^{+0.21}_{-0.23}\,{\rm au}$. The blended light, which is substantially brighter than the microlensed source, is plausibly due to the lens and could be observed at high resolution immediately.